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IUCrJ
Volume 8| Part 2| March 2021| Pages 178-185
ISSN: 2052-2525

Quaternary and quinary molecular solids based on structural inequivalence and combinatorial approaches: 2-nitro­resorcinol and 4,6-di­chloro­resorcinol

aSolid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore 560 012, India
*Correspondence e-mail: gdesiraju@iisc.ac.in

Edited by C.-Y. Su, Sun Yat-Sen University, China (Received 3 November 2020; accepted 22 December 2020; online 11 January 2021)

A synthetic strategy for the formation of stoichiometric quaternary and non­stoichiometric quinary solids is outlined. A series of 2-nitro­resorcinol-based quaternary cocrystals were developed from binary precursors in two conceptual stages. In the first stage, ternary solids are synthesized based on the structural inequivalence at two recognition sites in the binary. In the second stage, the ternary is homologated into a stoichiometric quaternary based on the same concept. Any cocrystal without an inequivalence becomes a synthetic dead end. The combinatorial approach involves lower cocrystal systems with different structural environments and preferred synthon selection from a synthon library in solution. Such are the stepping stones for the isolation of higher cocrystals. In addition, a quaternary cocrystal of 4,6-di­chloro­resorcinol is described wherein an unusual synthon is observed with two resorcinol molecules in a closed loop with two different ditopic bases. The concept of the virtual synthon in binaries with respect to isolated ternaries is validated for the 4,6-di­chloro­resorcinol system. It is possible that only some binary systems are amenable to homologation into higher cocrystals. The reasons for this could have to do with the existence of preferred synthon modules, in other words, the critical components of the putative higher assembly that cannot be altered. Addition of the third and fourth component might be more flexible, and the choices of these com­ponents, possible from a larger pool of chemically related molecules.

1. Introduction

The design of higher-order multicomponent cocrystals (Bond, 2007[Bond, A. D. (2007). CrystEngComm, 9, 833-834.]; Bolla & Nangia, 2015[Bolla, G. & Nangia, A. (2015). Chem. Commun. 51, 15578-15581.]), especially ternaries and quater­naries, is a challenging synthetic exercise (Mir et al., 2019[Mir, N. A., Dubey, R. & Desiraju, G. R. (2019). Acc. Chem. Res. 52, 2210-2220.]) requiring a proper knowledge of the robustness of specific supramolecular synthons (Desiraju, 1995[Desiraju, G. R. (1995). Angew. Chem. Int. Ed. Engl. 34, 2311-2327.]; Shattock et al., 2008[Shattock, T. R., Arora, K. K., Vishweshwar, P. & Zaworotko, M. J. (2008). Cryst. Growth Des. 8, 4533-4545.]). Any synthetic strategy towards higher cocrystals should be of high supramolecular yield and without contamination from by-products such as binaries and pure compounds. A very limited number of stoichiometric quaternaries (less than 20) have been obtained to date (Bhogala & Nangia, 2008[Bhogala, B. R. & Nangia, A. (2008). New J. Chem. 32, 800-807.]; Dandela et al., 2018[Dandela, R., Tothadi, S., Marelli, U. K. & Nangia, A. (2018). IUCrJ, 5, 816-822.]; Dubey et al., 2016[Dubey, R., Mir, N. A. & Desiraju, G. R. (2016). IUCrJ, 3, 102-107.]; Mir et al., 2016[Mir, N. A., Dubey, R. & Desiraju, G. R. (2016). IUCrJ, 3, 96-101.]; Paul et al., 2018[Paul, M., Chakraborty, S. & Desiraju, G. R. (2018). J. Am. Chem. Soc. 140, 2309-2315.]; Paul & Desiraju, 2019[Paul, M. & Desiraju, G. R. (2019). Angew. Chem. Int. Ed. 58, 12027-12031.]). All quaternary cocrystals thus far obtained by our group are based on either structural inequivalences or a combinatorial approach. These higher cocrystal experiments suggest that combinations of resorcinols and methyl­ated pyrazines could be the way forward for general synthetic strategies (Dubey et al., 2016[Dubey, R., Mir, N. A. & Desiraju, G. R. (2016). IUCrJ, 3, 102-107.]; Mir et al., 2016[Mir, N. A., Dubey, R. & Desiraju, G. R. (2016). IUCrJ, 3, 96-101.]; Paul et al., 2018[Paul, M., Chakraborty, S. & Desiraju, G. R. (2018). J. Am. Chem. Soc. 140, 2309-2315.]; Paul & Desiraju, 2019[Paul, M. & Desiraju, G. R. (2019). Angew. Chem. Int. Ed. 58, 12027-12031.]). The inclusion of a fifth component stoichiometrically within the same crystal still remains an open challenge because with an increasing number of components and functional groups, the number of possible permutations creates very difficult synthetic challenges (Gunawardana & Aakeröy, 2018[Gunawardana, C. A. & Aakeröy, C. B. (2018). Chem. Commun. 54, 14047-14060.]). In this article, we report seven quaternary and two quinary molecular solids to further strengthen the generality of our synthetic strategy towards higher cocrystals.

The structural inequivalence strategy (Mir et al., 2016[Mir, N. A., Dubey, R. & Desiraju, G. R. (2016). IUCrJ, 3, 96-101.]) is an outcome of molecule selection by the chemist in that if any particular molecule is bound at two distinct crystallographic environments in a (lower) cocrystal structure, this distinction can be exploited to homologate into a higher cocrystal by substituting a new, but similar, molecule at the more loosely bound site. This structural inequivalence is always integrated with a graded interaction hierarchy (Aakeröy et al., 2001[Aakeröy, C. B., Beatty, A. M. & Helfrich, B. A. (2001). Angew. Chem. Int. Ed. 40, 3240-3242.]). On the other hand, the combinatorial strategy (Dubey & Desiraju, 2014[Dubey, R. & Desiraju, G. R. (2014). Angew. Chem. Int. Ed. 53, 13178-13182.]) depends on the fact that if a molecule persists in many forms (polymorphs and/or pseudopolymorphs, the latter being essentially stoichiometric variants), crystallization of such a molecule with another component can lead to a higher cocrystal which is anticipated with a selection of the fittest interactions that are possible from a pool of multiple competing interactions for this particular molecule.

2. Results and discussion

Our approach to the design of quaternary and quinary molecular solids of 2-nitro­resorcinol (NRES) is based on the simultaneous use of chemical (interaction-based) and geometrical (shape- and size-based) recognition information (Aakeröy et al., 2007[Aakeröy, C. B., Desper, J. & Smith, M. M. (2007). Chem. Commun. pp. 3936-3938.]; Moorthy et al., 2010[Moorthy, J. N., Natarajan, P. & Venugopalan, P. (2010). Chem. Commun. 46, 3574-3576.]). The compounds used in this study with acronyms are given in Fig. 1[link] and the synthetic strategy involved in the quaternary cocrystal synthesis for NRES:TMP:PYR:ACR and NRES:TMP:PYR:4DMAP is presented in Fig. 2[link]. In these quaternaries, the binary cocrystal of NRES with tetra­methyl­pyrazine (TMP) is the basic template. In our hands, this binary cocrystal was obtained in two pseudopolymorphic variants. The first is a 2:1 form that crystallizes in the space group P1. The second is a 2:3 form which crystallizes in the space group P[\overline 1]. Details of these two cocrystals are given in the supporting information. Because the TMP molecules are located on pseudocentres of symmetry in the noncentrosymmetric 2:1 form, adequate care was taken in the space-group assignment.

[Figure 1]
Figure 1
Compounds used in this study with acronyms.
[Figure 2]
Figure 2
Synthetic strategy for the preparation of the NRES:TMP:PYR:ACR and NRES:TMP:PYR:4DMAP quaternary cocrystals. Colour coding and shapes represent distinct chemical and geometrical features of the molecules.

In any event, the connectivity of the TMP and NRES molecules is the same in both of these cocrystals and, most significantly, the TMP molecule is found in two distinct crystallographic environments in both cases. Of the two TMP molecules, one is connected to NRES only via O—H⋯N hydrogen bonds to give an infinite one-dimensional (1D) chain, while the other is additionally involved in weak C—H⋯O, C—H⋯π and ππ interactions with adjacent NRES molecules. As C—H⋯O, C—H⋯π and ππ interactions are comparable in strength, a PYR molecule, which has the capability of forming a C—H⋯π interaction with TMP, may be incorporated as the third component (replacing the NRES that bonds weakly via C—H⋯O). In this ternary, and as prescribed, the PYR molecule is connected with one of the two TMP molecules through C—H⋯π interactions, while the other is still unaffected; accordingly, a fourth component, which may be either ACR or 4DMAP, may be introduced with interaction substitution to homologate to the quaternaries NRES:TMP:PYR:ACR and NRES:TMP:PYR:4DMAP (Fig. 3[link]). In both cases, the monotopic bases ACR and 4DAMAP are connected at the two ends of the assembly but these become synthetic dead ends for homologation into quinaries. In other words, since inequivalences were not found in any of the quaternaries we isolated, stoichiometric inclusion of a fifth component with this strategy is not possible.

[Figure 3]
Figure 3
The development of the NRES:TMP:PYR:ACR and NRES:TMP:PYR:4DMAP quaternaries from the NRES:TMP:PYR ternary in which one of the TMP molecules is replaced by a fourth component, ACR or 4DMAP, using O—H⋯N hydrogen bonding.

While developing these quaternaries, two ternaries were simultaneously obtained, namely, NRES:4DMAP:PYR and NRES:TMP:DPE-I. Let us first consider the former. Crystallization of NRES with 4DMAP gave a 1:1 cocrystal and a 1:1 binary salt (from MeOH and MeCN, respectively). In the cocrystal, the two components are connected via O—H⋯.N hydrogen bonding at each hydroxy-group end of NRES; in the salt, the NRES molecules are linked to one another via O—H⋯O hydrogen bonds to form a chain, while 4DMAP molecules are connected to them via N—H⋯O hydrogen bonds. In the next step, PYR is added to the binary mixture to obtain a ternary in which PYR is stacked with 4DMAP through a C—H⋯π interaction. The other ternary, NRES:TMP:DPE-I, was obtained when the ternary mixture NRES:TMP:PYR was crystallized with DPE-I (to obtain a quaternary). This procedure removed the PYR molecule and an entirely different supramolecular topology was obtained in the resulting ternary. In this cocrystal, DPE-I is O—H⋯N hydrogen bonded at its two ends to NRES, which uses its other hy­droxy group to connect with TMPs, which terminates the sequence (the second heterocyclic N atom of TMP is `free'). Employing the structural inequivalence approach, Komisarek et al. (2020[Komisarek, D., Schauerte, C. & Merz, K. (2020). Chemistry, 2, 93-100.]) have reported this kind of synthon in the system 2-methyl­resorcinol--TMP--DPE-I. In both of these ternaries (NRES:4DMAP:PYR and NRES:TMP:DPE-I), no inequivalences are observed at any of the chemically identical sites and therefore these cannot be exploited for further homologation. Both ternaries are synthetic dead ends.

Let us next consider the synthetic strategy towards quinary cocrystals from quaternaries (Fig. 4[link]). Here, the binary NRES:TMP (mentioned previously) is crystallized with either 2,2′-bi­pyridine (22BP) or 2,2′-bi­thio­phene (22TBP) to give the ternaries NRES:TMP:22BP and NRES:TMP:22TBP in 1:2:2 and 1:2:4 stoichiometries, respectively. In these ternary systems, it is found that the two TMP molecules flanking NRES are in different crystallographic environments (as seen previously with PYR). In NRES:TMP:22BP, of the two TMP molecules, one forms C—H⋯π interactions with 22BP, while the other is not involved in any such interaction; accordingly, the latter may be replaced by other ditopic N-atom donors. In NRES:TMP:22TBP, there is a similar situation. These differences are sufficient for the replacement of such `free' molecules by another N-atom donor. Accordingly, in the next homologation step, each of these ternaries was crystallized with DPE-I or DPE-II, so that we successfully obtained four 1:1:1:1 quaternaries, namely, NRES:TMP:22BP:DPE-I and NRES:TMP:22BP:DPE-II with 22BP, and cor­respondingly NRES:TMP:22TBP:DPE-I and NRES:TMP:22TBP:DPE-II with 22TBP. These quaternaries are, however, syn­thetic dead ends and structural inequivalences may no longer be used to homologate to the quinary stage.

[Figure 4]
Figure 4
Proposed schemes for the construction of five-component systems.

A careful analysis of these quaternary structures paved the way to include a fifth component in these systems. In this context, the phenyl/thiophenyl exchange rule is relevant (Thallapally et al., 2000[Thallapally, P. K., Chakraborty, K., Carrell, H., Kotha, S. & Desiraju, G. (2000). Tetrahedron, 56, 6721-6728.]; Tothadi et al., 2011[Tothadi, S., Mukherjee, A. & Desiraju, G. R. (2011). Chem. Commun. 47, 12080-12082.]). According to this concept, 2,2′-bi­thio­phene, 2,2′-bi­phenyl and 2,2′-bi­pyridine are volume equivalents (–S– ≃ –CH=CH– ≃ –CH=N–) and so are mutually exchangeable in a crystal structure. The question arises therefore as to whether it might be possible to obtain quinary cocrystals if both 2,2′-bi­thio­phene and 2,2′-bi­pyridine are taken together along with the other three components NRES:TMP:DPE-I. Accordingly, we ground NRES, TMP and DPE-I with 0.5:0.5 ratios of 22BP and 22TBP, and isolated a five-component solid-solution cocrystal (Fig. 5[link]). We carried out a similar crystallization experiment with DPE-II and obtained the corresponding five-component solid-solution cocrystal NRES:TMP:22BP:22TBP:DPE-II.

[Figure 5]
Figure 5
Quinaries NRES:TMP:22TBP:22BP:DPE-I and NRE:TMP:22TBP:22BP:DPE-II. Note that the fourth and fifth components are included in a solid-solution manner.

To confirm the existence of five different organic molecules in the same crystal, we carried out GC–MS (gas chromatography–mass spectrometry) analysis. For this, single crystals of the quinary system were dissolved in MeOH. We observed five different peaks at different retention times (Fig. 6[link]; the very small peak is an unknown impurity, possibly from stopcock grease).

[Figure 6]
Figure 6
GCMS spectra of five-component systems.

We now discuss the combinatorial synthetic strategy based on long-range synthon Aufbau modules (LSAM) in the higher cocrystals of 4,6-di­chloro­resorcinol. The modular nature of the interactions may be utilized to obtain higher cocrystals by adding and/or exchanging a new molecule in the LSAM of the lower cocrystals. A putative supramolecular synthon of 4,6-di­chloro­resorcinol with complementary N-atom donors is illustrated in Fig. 7[link] and a schematic representation of the synthesis of quaternary cocrystals is shown in Fig. 8[link].

[Figure 7]
Figure 7
Possible supramolecular synthons of the 4,6-di­chloro­resorcinol system with N-atom donors. CRES is shown in green and blue and red are ditopic bases. Note that synthon A (seen elsewhere) is not observed in this study. Synthon D, which is unsymmetrical, is rarely seen with resorcinols in general (Paul & Desiraju, 2019[Paul, M. & Desiraju, G. R. (2019). Angew. Chem. Int. Ed. 58, 12027-12031.]).
[Figure 8]
Figure 8
A cartoon representation of the synthetic strategy for the CRES quaternary. Distinct chemical species are given with different shapes and in different colours.

In this attempt, we obtained three each of the binary and ternary cocrystals, and one quaternary cocrystal. Crystallization of CRES with (one of) TMP, PHE or DMP resulted in a stoichiometric binary cocrystal. In the 1:1 CRES:TMP cocrystal, the TMP molecules form discrete synthon C (closed CRES:TMP tetramer synthons, the so-called MacGillivray synthon) (Papaefstathiou et al., 2001[Papaefstathiou, G. S., Kipp, A. J. & MacGillivray, L. R. (2001). Chem. Commun. pp. 2462-2463.]; Ghorai et al., 2013[Ghorai, S., Sumrak, J. C., Hutchins, K. M., Bučar, D.-K., Tivanski, A. V. & MacGillivray, L. R. (2013). Chem. Sci. 4, 4304-4308.]) that are laterally offset with respect to one another. Next, we observed the formation of an unusual open synthon in the 1:3 CRES:PHE binary in which one hydroxy group of the CRES molecule is connected to two PHE molecules through O—H⋯N hydrogen bonding, followed by C—H⋯N interactions, while the second hydroxy group of CRES is linked to three PHE molecules so as to form a continuous 1D LSAM (Fig. 9[link]). These open synthons are further stacked with ππ interactions between PHE molecules. The CRES:DMP binary forms another kind of continuous 1D LSAM in which the two DMP molecules that are connected to CRES are perpendicular to each other, leading to C—H⋯π interactions. In all these binaries, we found that there are some weak interactions (C—H⋯O, ππ and C—H⋯π) which may be opened further to obtain higher cocrystals.

[Figure 9]
Figure 9
Binary cocrystals with synthons B and C. Note that CRES:PHE shows an unusual open synthon.

Accordingly, in the next homologation experiment, the PYR molecule was incorporated within these binaries and this resulted in three distinct ternaries. Interestingly, although binaries with closed synthon C were not isolated (say in CRES:PHE and CRES:DMP), all ternaries in this system have the closed synthon C wherein both bases are the same (Fig. 10[link]). This suggests the idea of a virtual synthon which, while it exists in solution, is only manifested in some isolated cocrystals in the entire system. Such a synthon is virtual with respect to binary crystallization and becomes real with respect to ternary systems (Dubey & Desiraju, 2014[Dubey, R. & Desiraju, G. R. (2014). Angew. Chem. Int. Ed. 53, 13178-13182.]). Exploiting the similarities of the synthons in these ternary systems, three attempts at homologation were made: (i) CRES:TMP:PYR with PHE; (ii) CRES:TMP:PYR with DMP; and (iii) CRES:DMP:PYR with PHE. In the process of crystallizing CRES:TMP:PYR with PHE, two distinguishable crystals differing in colour (red and yellow) were obtained from the same solution. The red crystal was identified as the ternary CRES:PHE:PYR and the yellow crystal as the quaternary CRES:TMP:PYR:PHE (Fig. 11[link]). This quaternary cocrystal contains the anomalous MacGillivray synthon (Paul & Desiraju, 2019[Paul, M. & Desiraju, G. R. (2019). Angew. Chem. Int. Ed. 58, 12027-12031.]) (synthon D) with two different bases (TMP and PHE). Crystallization according to protocols (ii) and (iii) above did not prove fruitful. The crystallographic details of all the cocrystals used are provided in the supporting information.

[Figure 10]
Figure 10
The 2:2:1 stoichiometric ternary cocrystals with synthon C, i.e. (a) CRES:TMP:PYR, (b) CRES:PHE:PYR and (c) CRES:DMP:PYR.
[Figure 11]
Figure 11
The structure of the quaternary cocrystal CRES:PHE:TMP:PYR with the unusual synthon D. The inset photograph shows the simultaneous growth of the quaternary (red) and ternary (yellow) crystals from a solution containing CRES, PHE, TMP and PYR.

3. Conclusions

The results obtained in this work validate the structural inequivalence and combinatorial approaches for the isolation of quaternary molecular solids and the use of such approaches combined with solid-solution methods for the achieving of quinary solids, providing more synthetic generality. In the present study, six stoichiometric quaternaries and two non­stoichiometric quinary cocrystals are reported based on the structural inequivalence approach. The two-component combinations of TMP:PYR, TMP:22BP and TMP:22TBP play a pivotal role in the formation of quaternary cocrystals in which there are C—H⋯π interactions. In the case of the NRES:TMP:PYR ternary, monotopic N-atom donors are required for the formation of quaternary cocrystals, whereas in the case of NRES:TMP:22BP and NRES:TMP:22TBP, symmetrical ditopic N-atom donors are required. After reaching synthetic dead ends at the quaternary level, the concept of shape–size similarity was utilized as a synthetic tool for obtaining five-component systems. In addition, an interesting quaternary cocrystal was obtained based on the combinatorial approach in which an unusual tetramer synthon, containing two different bases, was obtained. Finally, a closed supramolecular synthon, which was not observed in binary cocrystals, appears at the ternary and quaternary levels, strengthening the concept of virtual synthons in solution.

The formation of higher cocrystals (ternary and higher) poses restrictions on exactly what molecular precursors are chosen, and on what exactly are the experimental conditions of the crystallization experiment. Many of these choices may be, in the end, arbitrary, especially regarding the solvents chosen and the temperatures and cooling rates employed. Of course, the latter experimental variables are critical in many crystallizations, including in some of the simplest single-substance experiments, as they depend on the details of the relevant solvent–solute phase diagrams. What is of relevance here is to ascertain if certain compounds or types of compounds are more amenable to the formation of higher cocrystals than others. Expectedly, polyfunctional compounds such as diphenols, triphenols and ditopic bases were found to be suitable. In the course of our work in this area over the past decade, we have found that a combination of a 2-substituted (or other) resorcinol with TMP is generally required to form ternary and higher cocrystals. There are a few exceptions but the above is largely true across many crystallization experiments that have led to the isolation and characterization of around 75 ternaries and 20 quaternaries. The present study is no exception to these general trends. There is some latitude in the nature of the 2-substituent in the resorcinol component (or the other substituents) for higher cocrystals to be formed but TMP seems to be necessary. It is seen that both tri­methyl­pyrazine and 2,5-di­methyl­pyrazine form binaries with 2-sub­stituted resorcinols, but these cannot be homologated. On the other hand, there is considerable flexibility in the choice of the third and fourth component once resorcinol and TMP are selected as two of the components in the crystallization experiment. These can be chosen from several heterocyclic and nonheterocyclic bases, and from condensed ring hydro­carbons that are usually C—H⋯π stacked on the TMP.

These results suggest the relevance of the resorcinol–TMP association, which seems to be the basic building block of higher architectures through synthons of types A through D (Fig. 7[link]). Why such synthons are important for homologation is not clear, and especially why TMP itself seems to be so important is unknown. It is possible that these small synthons can expand easily into LSAMs that incorporate the third and fourth component, but again the specificity of synthons A through D is not easy to rationalize. More high-throughput crystallizations involving combinatorial and robotic methods may prove to be the route to expanding the structural space occupied by stoichiometric ternary and quaternary cocrystals. However, what seems clear enough is that there exist a vast number of higher cocrystals that remain to be discovered.

Supporting information


Computing details top

Program(s) used to solve structure: SHELXT 2014/5 (Sheldrick, 2014) for 2NRES-TMP, 5NRES-9AACR, 8NRES-DPE-I, 9NRES-DPE-II, 10NRES-44AZO, 12NRES-4DMAP-II, 13NRES-TMP-PYR, 14NRES-4DMAP-PYR, 15NRES-TMP-DPE-I, 17NRE-TMP-22TBP, 20NRES-TMP-22BP-DPE-I, 26CRES-TMP, 27CRES-PHE, 28CRES-DMP, 30CRES-PHE-PYR, 31CRES-DMP-PYR, 32CRES-TMP-PHE-PYR; SHELXT 2014/4 (Sheldrick, 2014) for 25NRES-TMP-22BP-22TBP-DPE-II. Program(s) used to refine structure: SHELXL2014 (Sheldrick, 2014) for 1NRES-TMP; SHELXL2018/3 (Sheldrick, 2018) for 2NRES-TMP, 3NRES-ACR, 4NRES-DMP, 5NRES-9AACR, 6NRES-33BP, 7NRES-44BP, 8NRES-DPE-I, 9NRES-DPE-II, 10NRES-44AZO, 11NRES-4DMAP, 12NRES-4DMAP-II, 13NRES-TMP-PYR, 14NRES-4DMAP-PYR, 15NRES-TMP-DPE-I, 16NRES-TMP-22BP, 17NRE-TMP-22TBP, 18NRES-TMP-PYR-ACR, 19NTES-TMP-PYR-4DMAP, 20NRES-TMP-22BP-DPE-I, 21NRES-TMP-22BP-DPE-II, 22NRES-TMP-22TBP-DPE-I, 23NRES-TMP-22TBP-DPE-II, 24NRES-TMP-22BP-22TBP-DPE-I, 25NRES-TMP-22BP-22TBP-DPE-II, 26CRES-TMP, 27CRES-PHE, 28CRES-DMP, 29CRES-TMP-PYR, 30CRES-PHE-PYR, 31CRES-DMP-PYR, 32CRES-TMP-PHE-PYR.

(1NRES-TMP) top
Crystal data top
C20H22N4O8Z = 2
Mr = 446.41F(000) = 468
Triclinic, P1Dx = 1.410 Mg m3
a = 7.7162 (8) ÅMo Kα radiation, λ = 0.71073 Å
b = 8.9727 (9) ÅCell parameters from 10074 reflections
c = 16.9089 (17) Åθ = 3.0–27.6°
α = 86.559 (6)°µ = 0.11 mm1
β = 78.838 (6)°T = 150 K
γ = 66.314 (5)°Block, yellow
V = 1051.59 (19) Å30.20 × 0.20 × 0.20 mm
Data collection top
Rigaku Mercury375R (2x2 bin mode)
diffractometer
7362 reflections with I > 2σ(I)
Radiation source: Sealed TubeRint = 0.017
Absorption correction: multi-scan
Jacobson, R. (1998) Private communication
θmax = 27.5°, θmin = 3.0°
Tmin = 0.846, Tmax = 1.000h = 910
10971 measured reflectionsk = 1111
9240 independent reflectionsl = 2121
Refinement top
Refinement on F2Hydrogen site location: mixed
Least-squares matrix: fullH atoms treated by a mixture of independent and constrained refinement
R[F2 > 2σ(F2)] = 0.048 w = 1/[σ2(Fo2) + (0.0388P)2 + 0.8048P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.127(Δ/σ)max < 0.001
S = 1.05Δρmax = 0.27 e Å3
9240 reflectionsΔρmin = 0.24 e Å3
612 parametersAbsolute structure: Refined as an inversion twin.
3 restraintsAbsolute structure parameter: 0.6 (15)
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Refinement. Refined as a 2-component inversion twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O130.2403 (5)0.7004 (4)0.0925 (2)0.0295 (7)
O140.2482 (5)1.1162 (4)0.0863 (2)0.0330 (8)
O150.0087 (5)0.9269 (4)0.0605 (2)0.0341 (8)
O160.0640 (5)1.0132 (5)0.0624 (2)0.0497 (11)
N20.0530 (5)0.9533 (4)0.0011 (2)0.0237 (8)
C120.3460 (6)0.7766 (5)0.0508 (3)0.0228 (9)
C80.3528 (6)0.9931 (5)0.0441 (3)0.0224 (9)
C90.5491 (6)0.9460 (6)0.0430 (3)0.0253 (10)
H90.61801.00110.07320.030*
C70.2572 (6)0.9049 (5)0.0029 (3)0.0215 (9)
C110.5414 (6)0.7308 (6)0.0500 (3)0.0285 (10)
H110.60670.64350.08040.034*
C100.6379 (6)0.8167 (6)0.0036 (3)0.0274 (10)
H100.76810.78550.00390.033*
O10.9754 (6)0.6516 (5)0.7402 (3)0.0526 (11)
O21.0996 (8)0.0875 (5)0.6836 (3)0.0672 (13)
H21.15330.10530.63950.101*
O31.1866 (5)0.4996 (5)0.6081 (2)0.0493 (10)
O41.2108 (7)0.2629 (5)0.5789 (3)0.0688 (13)
N41.1520 (6)0.3796 (6)0.6272 (3)0.0411 (11)
C191.0447 (7)0.3712 (6)0.7054 (3)0.0377 (11)
C200.9642 (8)0.5062 (7)0.7585 (3)0.0431 (14)
C220.8506 (9)0.3498 (11)0.8565 (4)0.067 (2)
H220.78520.34270.90800.080*
C210.8662 (8)0.4932 (9)0.8349 (3)0.0566 (17)
H210.81170.58150.87080.068*
C230.9266 (9)0.2149 (9)0.8063 (4)0.0622 (18)
H230.91170.11970.82350.075*
C241.0248 (9)0.2230 (7)0.7301 (4)0.0499 (15)
O50.7411 (5)0.6261 (4)0.6045 (2)0.0300 (8)
O60.7682 (5)1.0207 (4)0.4128 (2)0.0310 (8)
O80.9636 (5)0.8369 (4)0.58108 (19)0.0300 (7)
O71.0709 (5)0.7287 (4)0.4619 (2)0.0351 (8)
N30.9395 (5)0.7946 (4)0.5183 (2)0.0222 (8)
C30.4588 (6)0.7747 (5)0.5461 (3)0.0251 (10)
H30.38900.72030.57650.030*
C20.6454 (6)0.7394 (5)0.5556 (3)0.0213 (9)
C60.6616 (6)0.9427 (5)0.4541 (3)0.0233 (9)
C10.7433 (6)0.8259 (5)0.5087 (2)0.0196 (9)
C50.4746 (7)0.9750 (6)0.4458 (3)0.0276 (10)
H5A0.41601.05250.40960.033*
C40.3755 (7)0.8906 (6)0.4918 (3)0.0286 (10)
H40.25020.91250.48600.034*
O100.0478 (6)0.0879 (5)0.2066 (3)0.0436 (9)
O120.0521 (8)0.3087 (6)0.1000 (3)0.0713 (14)
O110.0531 (7)0.5450 (6)0.1136 (3)0.0694 (14)
O90.0419 (7)0.6486 (5)0.2502 (3)0.0676 (13)
H9A0.06740.66190.20470.101*
N10.0378 (7)0.4107 (6)0.1414 (3)0.0468 (12)
C150.0203 (7)0.4565 (7)0.3504 (4)0.0490 (15)
H150.01530.53640.38440.059*
C160.0572 (7)0.3014 (7)0.3783 (3)0.0411 (13)
H160.07650.27820.43110.049*
C180.0351 (6)0.2127 (6)0.2507 (3)0.0304 (11)
C130.0041 (7)0.3726 (6)0.2227 (3)0.0355 (11)
C170.0661 (7)0.1784 (6)0.3289 (3)0.0370 (11)
H170.09280.07400.34850.044*
C140.0094 (7)0.4948 (6)0.2724 (4)0.0412 (13)
N50.5430 (5)0.4698 (4)0.6985 (2)0.0228 (8)
N60.4206 (5)0.2833 (4)0.8119 (2)0.0219 (8)
C320.6938 (8)0.2482 (6)0.5993 (3)0.0326 (11)
H32A0.61010.23250.56840.049*
H32B0.79810.14590.60440.049*
H32C0.74420.32360.57260.049*
C280.2633 (8)0.5079 (6)0.9097 (3)0.0351 (11)
H28A0.14740.59920.90330.053*
H28B0.33800.54250.93780.053*
H28C0.23090.42590.94010.053*
C290.5649 (8)0.0434 (6)0.7240 (3)0.0379 (12)
H29A0.69820.02130.72500.057*
H29B0.53810.03170.67210.057*
H29C0.48590.00770.76500.057*
C250.3960 (8)0.7096 (6)0.7856 (3)0.0355 (12)
H25A0.45280.75220.73900.053*
H25B0.44800.71890.83130.053*
H25C0.25910.77020.79610.053*
C310.5828 (6)0.3145 (5)0.6814 (3)0.0238 (9)
C270.3785 (6)0.4391 (5)0.8282 (3)0.0226 (9)
C260.4401 (6)0.5343 (5)0.7703 (3)0.0229 (9)
C300.5220 (6)0.2188 (5)0.7393 (3)0.0233 (9)
N80.4285 (5)0.4716 (4)0.1947 (2)0.0251 (8)
N70.5741 (5)0.2446 (4)0.3074 (2)0.0235 (8)
C370.4592 (8)0.2652 (6)0.0994 (3)0.0342 (11)
H37A0.39270.36140.07140.051*
H37B0.38660.19830.10770.051*
H37C0.58410.20550.06780.051*
C360.3792 (8)0.6985 (6)0.2802 (3)0.0380 (12)
H36A0.35300.75530.23110.057*
H36B0.47850.71880.29820.057*
H36C0.26430.73600.32070.057*
C330.5342 (7)0.4498 (6)0.4038 (3)0.0317 (11)
H33A0.40920.49110.43780.047*
H33B0.58530.53210.39770.047*
H33C0.61860.35570.42780.047*
C380.4811 (6)0.3123 (5)0.1793 (3)0.0230 (9)
C340.5176 (6)0.4036 (5)0.3229 (3)0.0228 (9)
C350.4445 (6)0.5192 (5)0.2654 (3)0.0242 (10)
C390.5556 (6)0.1978 (5)0.2366 (3)0.0226 (9)
C400.6157 (8)0.0185 (6)0.2227 (3)0.0348 (12)
H40A0.70300.04190.25780.052*
H40B0.67830.00990.16760.052*
H40C0.50400.00720.23390.052*
H50.656 (9)0.569 (7)0.636 (4)0.058 (19)*
H60.714 (8)1.079 (6)0.382 (3)0.031 (15)*
H130.321 (10)0.617 (8)0.125 (4)0.07 (2)*
H140.302 (7)1.165 (6)0.107 (3)0.027 (14)*
H10A0.017 (10)0.117 (8)0.164 (4)0.06 (2)*
H11.026 (8)0.645 (7)0.694 (3)0.032 (16)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O130.0295 (18)0.0290 (17)0.0341 (18)0.0167 (14)0.0090 (14)0.0161 (14)
O140.0281 (18)0.0293 (18)0.044 (2)0.0163 (15)0.0083 (15)0.0221 (16)
O150.0290 (17)0.045 (2)0.0342 (19)0.0177 (15)0.0150 (15)0.0076 (15)
O160.0210 (17)0.075 (3)0.043 (2)0.0109 (18)0.0048 (16)0.018 (2)
N20.0191 (18)0.0221 (18)0.032 (2)0.0102 (15)0.0079 (16)0.0102 (16)
C120.023 (2)0.022 (2)0.025 (2)0.0114 (18)0.0055 (18)0.0048 (18)
C80.024 (2)0.018 (2)0.024 (2)0.0090 (18)0.0022 (18)0.0035 (17)
C90.023 (2)0.030 (2)0.027 (2)0.0165 (19)0.0017 (18)0.0059 (19)
C70.019 (2)0.019 (2)0.027 (2)0.0084 (17)0.0048 (18)0.0007 (17)
C110.023 (2)0.030 (2)0.032 (2)0.0072 (19)0.0107 (19)0.0083 (19)
C100.017 (2)0.032 (2)0.035 (2)0.0104 (19)0.0075 (18)0.003 (2)
O10.056 (3)0.048 (2)0.049 (3)0.010 (2)0.021 (2)0.005 (2)
O20.081 (3)0.040 (2)0.085 (3)0.019 (2)0.040 (3)0.009 (2)
O30.038 (2)0.048 (2)0.056 (2)0.0126 (18)0.0074 (18)0.0117 (19)
O40.082 (3)0.054 (3)0.052 (3)0.012 (2)0.001 (2)0.016 (2)
N40.031 (2)0.044 (3)0.037 (2)0.002 (2)0.0123 (19)0.005 (2)
C190.028 (2)0.044 (3)0.036 (3)0.006 (2)0.016 (2)0.006 (2)
C200.033 (3)0.053 (4)0.041 (3)0.010 (3)0.018 (2)0.003 (3)
C220.045 (4)0.109 (6)0.042 (4)0.027 (4)0.019 (3)0.036 (4)
C210.040 (3)0.085 (5)0.034 (3)0.009 (3)0.015 (2)0.004 (3)
C230.050 (4)0.075 (5)0.067 (4)0.026 (3)0.033 (3)0.037 (4)
C240.048 (3)0.051 (4)0.055 (4)0.016 (3)0.034 (3)0.019 (3)
O50.0271 (17)0.0297 (17)0.0368 (19)0.0145 (14)0.0122 (14)0.0172 (14)
O60.0261 (17)0.0343 (19)0.0366 (19)0.0168 (15)0.0100 (15)0.0191 (15)
O80.0289 (17)0.0364 (18)0.0282 (17)0.0136 (14)0.0113 (14)0.0023 (14)
O70.0214 (16)0.045 (2)0.0341 (18)0.0106 (15)0.0026 (14)0.0053 (15)
N30.0205 (19)0.0224 (18)0.0254 (19)0.0099 (15)0.0065 (15)0.0061 (15)
C30.023 (2)0.025 (2)0.030 (2)0.0144 (19)0.0039 (19)0.0062 (19)
C20.023 (2)0.020 (2)0.023 (2)0.0103 (17)0.0046 (17)0.0016 (17)
C60.025 (2)0.023 (2)0.023 (2)0.0112 (18)0.0035 (18)0.0029 (17)
C10.017 (2)0.018 (2)0.023 (2)0.0067 (17)0.0035 (17)0.0029 (16)
C50.024 (2)0.028 (2)0.030 (2)0.0097 (19)0.0104 (18)0.0130 (19)
C40.022 (2)0.034 (3)0.033 (2)0.013 (2)0.0102 (19)0.003 (2)
O100.049 (2)0.038 (2)0.047 (2)0.0184 (18)0.0138 (19)0.0005 (18)
O120.092 (4)0.081 (3)0.059 (3)0.044 (3)0.042 (3)0.022 (2)
O110.061 (3)0.067 (3)0.098 (4)0.037 (2)0.042 (3)0.051 (3)
O90.050 (3)0.026 (2)0.120 (4)0.0109 (18)0.012 (3)0.003 (2)
N10.031 (2)0.054 (3)0.058 (3)0.018 (2)0.018 (2)0.019 (2)
C150.030 (3)0.048 (3)0.065 (4)0.015 (2)0.007 (3)0.021 (3)
C160.028 (3)0.054 (3)0.040 (3)0.015 (2)0.003 (2)0.005 (3)
C180.019 (2)0.032 (3)0.041 (3)0.0111 (19)0.005 (2)0.000 (2)
C130.024 (2)0.034 (3)0.048 (3)0.011 (2)0.007 (2)0.007 (2)
C170.026 (2)0.038 (3)0.043 (3)0.010 (2)0.005 (2)0.003 (2)
C140.024 (3)0.033 (3)0.063 (4)0.008 (2)0.005 (2)0.002 (3)
N50.029 (2)0.0194 (17)0.0234 (19)0.0110 (15)0.0102 (15)0.0076 (14)
N60.0261 (19)0.0200 (17)0.0211 (18)0.0111 (15)0.0050 (15)0.0044 (14)
C320.045 (3)0.026 (2)0.024 (2)0.015 (2)0.001 (2)0.0002 (18)
C280.051 (3)0.036 (3)0.019 (2)0.023 (2)0.005 (2)0.0006 (19)
C290.055 (3)0.018 (2)0.040 (3)0.019 (2)0.001 (2)0.001 (2)
C250.046 (3)0.022 (2)0.041 (3)0.016 (2)0.006 (2)0.003 (2)
C310.028 (2)0.023 (2)0.023 (2)0.0120 (19)0.0084 (18)0.0055 (17)
C270.027 (2)0.021 (2)0.021 (2)0.0105 (18)0.0064 (17)0.0037 (17)
C260.029 (2)0.020 (2)0.024 (2)0.0127 (18)0.0074 (18)0.0049 (17)
C300.029 (2)0.018 (2)0.026 (2)0.0112 (18)0.0082 (18)0.0032 (17)
N80.026 (2)0.0213 (19)0.0237 (19)0.0064 (16)0.0022 (15)0.0042 (15)
N70.0187 (18)0.0241 (19)0.0246 (19)0.0072 (15)0.0013 (15)0.0050 (15)
C370.036 (3)0.032 (3)0.028 (2)0.005 (2)0.009 (2)0.000 (2)
C360.052 (3)0.023 (2)0.039 (3)0.015 (2)0.008 (2)0.003 (2)
C330.032 (3)0.036 (3)0.025 (2)0.011 (2)0.009 (2)0.001 (2)
C380.021 (2)0.020 (2)0.026 (2)0.0077 (18)0.0011 (18)0.0015 (17)
C340.018 (2)0.025 (2)0.022 (2)0.0068 (18)0.0010 (17)0.0017 (17)
C350.023 (2)0.021 (2)0.026 (2)0.0089 (18)0.0011 (18)0.0027 (17)
C390.019 (2)0.022 (2)0.023 (2)0.0075 (18)0.0002 (17)0.0070 (17)
C400.039 (3)0.023 (2)0.036 (3)0.010 (2)0.000 (2)0.005 (2)
Geometric parameters (Å, º) top
O13—C121.341 (6)N1—C131.443 (7)
O13—H130.98 (7)C15—C161.377 (8)
O14—C81.339 (5)C15—C141.380 (8)
O14—H140.75 (5)C15—H150.9300
O15—N21.220 (5)C16—C171.396 (7)
O16—N21.222 (5)C16—H160.9300
N2—C71.463 (5)C18—C171.384 (7)
C12—C71.386 (6)C18—C131.414 (7)
C12—C111.392 (6)C13—C141.405 (7)
C8—C71.403 (6)C17—H170.9300
C8—C91.403 (6)N5—C261.334 (6)
C9—C101.377 (6)N5—C311.339 (5)
C9—H90.9300N6—C271.334 (5)
C11—C101.388 (7)N6—C301.343 (6)
C11—H110.9300C32—C311.497 (6)
C10—H100.9300C32—H32A0.9600
O1—C201.355 (7)C32—H32B0.9600
O1—H10.79 (5)C32—H32C0.9600
O2—C241.343 (8)C28—C271.502 (6)
O2—H20.8200C28—H28A0.9600
O3—N41.222 (6)C28—H28B0.9600
O4—N41.244 (6)C28—H28C0.9600
N4—C191.433 (7)C29—C301.500 (6)
C19—C201.405 (7)C29—H29A0.9600
C19—C241.428 (8)C29—H29B0.9600
C20—C211.388 (8)C29—H29C0.9600
C22—C211.362 (10)C25—C261.497 (6)
C22—C231.375 (10)C25—H25A0.9600
C22—H220.9300C25—H25B0.9600
C21—H210.9300C25—H25C0.9600
C23—C241.376 (9)C31—C301.400 (6)
C23—H230.9300C27—C261.400 (6)
O5—C21.340 (5)N8—C351.338 (6)
O5—H51.04 (6)N8—C381.346 (6)
O6—C61.355 (5)N7—C341.340 (6)
O6—H60.78 (5)N7—C391.343 (6)
O8—N31.219 (5)C37—C381.499 (6)
O7—N31.224 (5)C37—H37A0.9600
N3—C11.465 (5)C37—H37B0.9600
C3—C21.384 (6)C37—H37C0.9600
C3—C41.384 (6)C36—C351.501 (6)
C3—H30.9300C36—H36A0.9600
C2—C11.402 (6)C36—H36B0.9600
C6—C51.387 (6)C36—H36C0.9600
C6—C11.388 (6)C33—C341.496 (6)
C5—C41.389 (7)C33—H33A0.9600
C5—H5A0.9300C33—H33B0.9600
C4—H40.9300C33—H33C0.9600
O10—C181.343 (6)C38—C391.396 (6)
O10—H10A0.80 (7)C34—C351.399 (6)
O12—N11.236 (6)C39—C401.504 (6)
O11—N11.236 (6)C40—H40A0.9600
O9—C141.344 (6)C40—H40B0.9600
O9—H9A0.8200C40—H40C0.9600
C12—O13—H13108 (4)C14—C13—N1119.4 (5)
C8—O14—H14113 (4)C18—C13—N1119.5 (5)
O15—N2—O16123.4 (4)C18—C17—C16119.7 (5)
O15—N2—C7118.5 (4)C18—C17—H17120.1
O16—N2—C7118.1 (4)C16—C17—H17120.1
O13—C12—C7118.0 (4)O9—C14—C15116.6 (5)
O13—C12—C11124.1 (4)O9—C14—C13124.9 (6)
C7—C12—C11117.9 (4)C15—C14—C13118.5 (5)
O14—C8—C7117.0 (4)C26—N5—C31119.5 (4)
O14—C8—C9125.3 (4)C27—N6—C30119.4 (4)
C7—C8—C9117.7 (4)C31—C32—H32A109.5
C10—C9—C8118.8 (4)C31—C32—H32B109.5
C10—C9—H9120.6H32A—C32—H32B109.5
C8—C9—H9120.6C31—C32—H32C109.5
C12—C7—C8123.4 (4)H32A—C32—H32C109.5
C12—C7—N2119.0 (4)H32B—C32—H32C109.5
C8—C7—N2117.6 (4)C27—C28—H28A109.5
C10—C11—C12119.3 (4)C27—C28—H28B109.5
C10—C11—H11120.3H28A—C28—H28B109.5
C12—C11—H11120.3C27—C28—H28C109.5
C9—C10—C11122.9 (4)H28A—C28—H28C109.5
C9—C10—H10118.6H28B—C28—H28C109.5
C11—C10—H10118.6C30—C29—H29A109.5
C20—O1—H1106 (4)C30—C29—H29B109.5
C24—O2—H2109.5H29A—C29—H29B109.5
O3—N4—O4120.1 (5)C30—C29—H29C109.5
O3—N4—C19120.5 (5)H29A—C29—H29C109.5
O4—N4—C19119.4 (5)H29B—C29—H29C109.5
C20—C19—C24119.9 (5)C26—C25—H25A109.5
C20—C19—N4120.3 (5)C26—C25—H25B109.5
C24—C19—N4119.7 (5)H25A—C25—H25B109.5
O1—C20—C21116.8 (6)C26—C25—H25C109.5
O1—C20—C19124.0 (5)H25A—C25—H25C109.5
C21—C20—C19119.2 (6)H25B—C25—H25C109.5
C21—C22—C23123.4 (6)N5—C31—C30120.2 (4)
C21—C22—H22118.3N5—C31—C32117.9 (4)
C23—C22—H22118.3C30—C31—C32121.9 (4)
C22—C21—C20119.3 (6)N6—C27—C26120.4 (4)
C22—C21—H21120.4N6—C27—C28118.0 (4)
C20—C21—H21120.4C26—C27—C28121.6 (4)
C22—C23—C24119.1 (7)N5—C26—C27120.3 (4)
C22—C23—H23120.5N5—C26—C25117.3 (4)
C24—C23—H23120.5C27—C26—C25122.4 (4)
O2—C24—C23117.1 (6)N6—C30—C31120.1 (4)
O2—C24—C19123.8 (6)N6—C30—C29117.3 (4)
C23—C24—C19119.1 (6)C31—C30—C29122.6 (4)
C2—O5—H5111 (3)C35—N8—C38119.8 (4)
C6—O6—H6111 (4)C34—N7—C39119.1 (4)
O8—N3—O7123.5 (4)C38—C37—H37A109.5
O8—N3—C1118.8 (4)C38—C37—H37B109.5
O7—N3—C1117.7 (4)H37A—C37—H37B109.5
C2—C3—C4120.3 (4)C38—C37—H37C109.5
C2—C3—H3119.8H37A—C37—H37C109.5
C4—C3—H3119.8H37B—C37—H37C109.5
O5—C2—C3125.0 (4)C35—C36—H36A109.5
O5—C2—C1117.6 (4)C35—C36—H36B109.5
C3—C2—C1117.4 (4)H36A—C36—H36B109.5
O6—C6—C5123.6 (4)C35—C36—H36C109.5
O6—C6—C1118.1 (4)H36A—C36—H36C109.5
C5—C6—C1118.3 (4)H36B—C36—H36C109.5
C6—C1—C2123.0 (4)C34—C33—H33A109.5
C6—C1—N3118.0 (4)C34—C33—H33B109.5
C2—C1—N3119.0 (4)H33A—C33—H33B109.5
C6—C5—C4119.5 (4)C34—C33—H33C109.5
C6—C5—H5A120.3H33A—C33—H33C109.5
C4—C5—H5A120.3H33B—C33—H33C109.5
C3—C4—C5121.5 (4)N8—C38—C39119.7 (4)
C3—C4—H4119.2N8—C38—C37117.8 (4)
C5—C4—H4119.2C39—C38—C37122.5 (4)
C18—O10—H10A112 (5)N7—C34—C35120.6 (4)
C14—O9—H9A109.5N7—C34—C33117.0 (4)
O12—N1—O11120.2 (5)C35—C34—C33122.5 (4)
O12—N1—C13119.7 (5)N8—C35—C34120.1 (4)
O11—N1—C13120.1 (5)N8—C35—C36117.5 (4)
C16—C15—C14120.8 (5)C34—C35—C36122.4 (4)
C16—C15—H15119.6N7—C39—C38120.8 (4)
C14—C15—H15119.6N7—C39—C40117.3 (4)
C15—C16—C17121.2 (5)C38—C39—C40121.9 (4)
C15—C16—H16119.4C39—C40—H40A109.5
C17—C16—H16119.4C39—C40—H40B109.5
O10—C18—C17116.3 (5)H40A—C40—H40B109.5
O10—C18—C13125.0 (5)C39—C40—H40C109.5
C17—C18—C13118.7 (5)H40A—C40—H40C109.5
C14—C13—C18121.1 (5)H40B—C40—H40C109.5
O14—C8—C9—C10179.9 (4)C2—C3—C4—C50.3 (7)
C7—C8—C9—C100.1 (6)C6—C5—C4—C30.1 (7)
O13—C12—C7—C8179.3 (4)C14—C15—C16—C170.1 (8)
C11—C12—C7—C81.9 (7)O10—C18—C13—C14178.2 (4)
O13—C12—C7—N21.2 (6)C17—C18—C13—C140.8 (7)
C11—C12—C7—N2178.6 (4)O10—C18—C13—N11.3 (7)
O14—C8—C7—C12178.8 (4)C17—C18—C13—N1179.7 (4)
C9—C8—C7—C121.1 (7)O12—N1—C13—C14172.9 (5)
O14—C8—C7—N20.7 (6)O11—N1—C13—C146.8 (7)
C9—C8—C7—N2179.5 (4)O12—N1—C13—C187.6 (7)
O15—N2—C7—C12110.4 (5)O11—N1—C13—C18172.7 (5)
O16—N2—C7—C1267.3 (6)O10—C18—C17—C16179.4 (5)
O15—N2—C7—C870.1 (5)C13—C18—C17—C160.3 (7)
O16—N2—C7—C8112.2 (5)C15—C16—C17—C180.8 (7)
O13—C12—C11—C10178.9 (4)C16—C15—C14—O9179.2 (5)
C7—C12—C11—C101.6 (7)C16—C15—C14—C131.0 (7)
C8—C9—C10—C110.3 (7)C18—C13—C14—O9178.7 (4)
C12—C11—C10—C90.6 (7)N1—C13—C14—O90.8 (7)
O3—N4—C19—C205.3 (7)C18—C13—C14—C151.5 (7)
O4—N4—C19—C20175.0 (5)N1—C13—C14—C15179.0 (5)
O3—N4—C19—C24172.7 (4)C26—N5—C31—C301.9 (6)
O4—N4—C19—C246.9 (7)C26—N5—C31—C32178.3 (4)
C24—C19—C20—O1179.8 (5)C30—N6—C27—C260.3 (6)
N4—C19—C20—O12.1 (7)C30—N6—C27—C28179.4 (4)
C24—C19—C20—C210.1 (7)C31—N5—C26—C271.7 (6)
N4—C19—C20—C21177.9 (5)C31—N5—C26—C25178.6 (4)
C23—C22—C21—C200.4 (9)N6—C27—C26—N50.6 (6)
O1—C20—C21—C22179.9 (5)C28—C27—C26—N5179.7 (4)
C19—C20—C21—C220.1 (8)N6—C27—C26—C25179.8 (4)
C21—C22—C23—C240.4 (9)C28—C27—C26—C250.1 (7)
C22—C23—C24—O2178.8 (5)C27—N6—C30—C310.0 (6)
C22—C23—C24—C190.2 (8)C27—N6—C30—C29179.8 (4)
C20—C19—C24—O2179.0 (5)N5—C31—C30—N61.1 (6)
N4—C19—C24—O21.0 (7)C32—C31—C30—N6179.2 (4)
C20—C19—C24—C230.1 (8)N5—C31—C30—C29179.1 (4)
N4—C19—C24—C23178.0 (5)C32—C31—C30—C290.7 (7)
C4—C3—C2—O5177.8 (4)C35—N8—C38—C391.3 (6)
C4—C3—C2—C10.4 (6)C35—N8—C38—C37179.6 (4)
O6—C6—C1—C2179.0 (4)C39—N7—C34—C351.5 (6)
C5—C6—C1—C20.1 (7)C39—N7—C34—C33177.7 (4)
O6—C6—C1—N30.1 (6)C38—N8—C35—C340.6 (6)
C5—C6—C1—N3178.9 (4)C38—N8—C35—C36178.5 (4)
O5—C2—C1—C6178.1 (4)N7—C34—C35—N80.8 (6)
C3—C2—C1—C60.3 (6)C33—C34—C35—N8178.4 (4)
O5—C2—C1—N33.0 (6)N7—C34—C35—C36179.9 (4)
C3—C2—C1—N3178.6 (4)C33—C34—C35—C360.7 (7)
O8—N3—C1—C6110.2 (5)C34—N7—C39—C380.9 (6)
O7—N3—C1—C668.9 (5)C34—N7—C39—C40178.3 (4)
O8—N3—C1—C268.8 (5)N8—C38—C39—N70.5 (6)
O7—N3—C1—C2112.1 (5)C37—C38—C39—N7179.6 (4)
O6—C6—C5—C4178.9 (4)N8—C38—C39—C40179.7 (4)
C1—C6—C5—C40.0 (7)C37—C38—C39—C401.2 (7)
(2NRES-TMP) top
Crystal data top
C6H5NO4·1.5(C8H12N2)Z = 2
Mr = 359.40F(000) = 382
Triclinic, P1Dx = 1.246 Mg m3
a = 7.658 (2) ÅMo Kα radiation, λ = 0.71075 Å
b = 9.277 (3) ÅCell parameters from 5527 reflections
c = 15.152 (5) Åθ = 3.0–27.7°
α = 79.304 (6)°µ = 0.09 mm1
β = 82.008 (6)°T = 150 K
γ = 65.214 (5)°Block, yellow
V = 957.9 (5) Å30.20 × 0.20 × 0.20 mm
Data collection top
Rigaku Mercury375R (2x2 bin mode)
diffractometer
1894 reflections with I > 2σ(I)
Radiation source: Sealed TubeRint = 0.059
profile data from ω–scansθmax = 25.0°, θmin = 3.0°
Absorption correction: multi-scan
Jacobson, R. (1998) Private communication
h = 99
Tmin = 0.683, Tmax = 1.000k = 1111
6882 measured reflectionsl = 1818
3305 independent reflections
Refinement top
Refinement on F2Hydrogen site location: mixed
Least-squares matrix: fullH atoms treated by a mixture of independent and constrained refinement
R[F2 > 2σ(F2)] = 0.078 w = 1/[σ2(Fo2) + (0.122P)2 + 0.3342P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.253(Δ/σ)max < 0.001
S = 1.11Δρmax = 0.27 e Å3
3305 reflectionsΔρmin = 0.25 e Å3
247 parametersExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.020 (8)
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O20.0736 (4)0.6091 (4)0.6982 (2)0.0558 (9)
H20.0637490.6944710.6674920.084*
O10.4591 (5)0.1968 (4)0.9072 (2)0.0594 (10)
N10.8110 (5)0.0571 (4)0.9808 (2)0.0460 (10)
N20.0330 (5)0.8706 (4)0.5667 (2)0.0417 (9)
N40.1161 (5)0.3582 (4)0.8311 (3)0.0454 (9)
O40.0012 (6)0.4247 (5)0.8885 (3)0.0847 (13)
N30.4585 (5)0.1495 (4)0.4485 (3)0.0499 (10)
C20.2505 (6)0.5352 (5)0.7326 (3)0.0396 (10)
C60.4516 (6)0.3189 (5)0.8416 (3)0.0413 (10)
C120.0183 (5)0.8559 (5)0.4815 (3)0.0382 (10)
C10.2772 (6)0.4050 (5)0.8002 (2)0.0374 (10)
C130.0167 (6)1.0116 (5)0.5863 (3)0.0404 (10)
C160.4877 (6)0.1261 (5)0.5365 (3)0.0449 (11)
C170.4700 (6)0.0246 (5)0.4112 (3)0.0453 (11)
C30.4047 (6)0.5778 (5)0.7036 (3)0.0449 (11)
H30.3911610.6636190.6582060.054*
C80.9390 (6)0.0818 (5)0.9550 (3)0.0444 (11)
O30.1069 (6)0.2522 (6)0.7987 (3)0.1051 (16)
C50.6034 (6)0.3644 (5)0.8106 (3)0.0487 (11)
H50.7219080.3088640.8357660.058*
C90.8692 (6)0.1410 (5)1.0252 (3)0.0466 (11)
C40.5787 (6)0.4918 (5)0.7427 (3)0.0502 (12)
H40.6817370.5205210.7227360.060*
C70.8639 (8)0.1719 (6)0.9075 (3)0.0601 (13)
H7A0.8682050.2677500.9460880.090*
H7B0.9425360.1998020.8530170.090*
H7C0.7332390.1052450.8932410.090*
C140.0339 (8)1.0218 (6)0.6825 (3)0.0583 (13)
H14A0.0885961.0913220.7073490.087*
H14B0.1281551.0639020.6846490.087*
H14C0.0730840.9167790.7169900.087*
C110.0387 (7)0.6950 (5)0.4640 (3)0.0583 (13)
H11A0.1683280.6361300.4413920.087*
H11B0.0493260.7098530.4204060.087*
H11C0.0100150.6362550.5190750.087*
C180.4373 (8)0.0547 (7)0.3141 (3)0.0669 (14)
H18A0.3160310.0522840.3069020.100*
H18B0.5392090.0266010.2839640.100*
H18C0.4354950.1580600.2884690.100*
C100.7187 (7)0.2954 (6)1.0520 (4)0.0674 (15)
H10A0.5987380.3172961.0284050.101*
H10B0.7586250.3811311.0284070.101*
H10C0.7023530.2867121.1165170.101*
C150.4711 (8)0.2696 (6)0.5761 (4)0.0678 (15)
H15A0.4648010.3555210.5285040.102*
H15B0.5816340.2408660.6094110.102*
H15C0.3563110.3037080.6156120.102*
H10.568 (11)0.138 (9)0.920 (5)0.12 (3)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O20.0542 (19)0.0488 (19)0.058 (2)0.0181 (16)0.0192 (15)0.0132 (15)
O10.047 (2)0.057 (2)0.065 (2)0.0204 (17)0.0196 (16)0.0234 (17)
N10.045 (2)0.042 (2)0.041 (2)0.0081 (18)0.0099 (16)0.0015 (16)
N20.044 (2)0.034 (2)0.041 (2)0.0117 (16)0.0088 (15)0.0013 (15)
N40.040 (2)0.039 (2)0.057 (2)0.0149 (18)0.0116 (18)0.0026 (17)
O40.078 (3)0.089 (3)0.097 (3)0.048 (2)0.038 (2)0.035 (2)
N30.048 (2)0.046 (2)0.056 (2)0.0190 (19)0.0014 (18)0.0108 (18)
C20.046 (2)0.034 (2)0.036 (2)0.012 (2)0.0081 (18)0.0050 (17)
C60.040 (2)0.042 (2)0.038 (2)0.013 (2)0.0095 (18)0.0004 (18)
C120.033 (2)0.035 (2)0.044 (2)0.0104 (18)0.0065 (17)0.0036 (17)
C10.038 (2)0.038 (2)0.036 (2)0.0160 (19)0.0020 (17)0.0038 (17)
C130.035 (2)0.040 (2)0.043 (2)0.0121 (19)0.0055 (18)0.0034 (18)
C160.039 (2)0.045 (3)0.055 (3)0.019 (2)0.004 (2)0.020 (2)
C170.042 (2)0.050 (3)0.048 (3)0.021 (2)0.0012 (19)0.013 (2)
C30.052 (3)0.040 (2)0.043 (2)0.021 (2)0.000 (2)0.0038 (19)
C80.051 (3)0.043 (2)0.034 (2)0.014 (2)0.0093 (19)0.0013 (18)
O30.092 (3)0.124 (4)0.145 (4)0.075 (3)0.022 (3)0.072 (3)
C50.036 (2)0.055 (3)0.054 (3)0.017 (2)0.009 (2)0.004 (2)
C90.053 (3)0.041 (2)0.036 (2)0.009 (2)0.007 (2)0.0026 (18)
C40.044 (3)0.048 (3)0.063 (3)0.024 (2)0.007 (2)0.012 (2)
C70.076 (3)0.057 (3)0.047 (3)0.024 (3)0.016 (2)0.007 (2)
C140.075 (3)0.058 (3)0.045 (3)0.027 (3)0.017 (2)0.004 (2)
C110.066 (3)0.044 (3)0.070 (3)0.024 (2)0.010 (3)0.013 (2)
C180.070 (3)0.084 (4)0.054 (3)0.036 (3)0.013 (3)0.009 (3)
C100.063 (3)0.051 (3)0.072 (3)0.002 (3)0.006 (3)0.017 (2)
C150.069 (3)0.055 (3)0.082 (4)0.020 (3)0.006 (3)0.027 (3)
Geometric parameters (Å, º) top
O2—C21.365 (5)C8—C9iii1.390 (6)
O2—H20.8200C8—C71.513 (6)
O1—C61.348 (5)C5—C41.380 (6)
O1—H10.81 (7)C5—H50.9300
N1—C81.340 (5)C9—C101.499 (6)
N1—C91.352 (6)C4—H40.9300
N2—C131.346 (5)C7—H7A0.9600
N2—C121.347 (5)C7—H7B0.9600
N4—O31.207 (5)C7—H7C0.9600
N4—O41.209 (5)C14—H14A0.9600
N4—C11.464 (5)C14—H14B0.9600
N3—C161.344 (5)C14—H14C0.9600
N3—C171.347 (5)C11—H11A0.9600
C2—C31.388 (6)C11—H11B0.9600
C2—C11.393 (5)C11—H11C0.9600
C6—C51.391 (6)C18—H18A0.9600
C6—C11.402 (5)C18—H18B0.9600
C12—C13i1.404 (6)C18—H18C0.9600
C12—C111.504 (6)C10—H10A0.9600
C13—C141.506 (6)C10—H10B0.9600
C16—C17ii1.404 (6)C10—H10C0.9600
C16—C151.511 (6)C15—H15A0.9600
C17—C181.482 (6)C15—H15B0.9600
C3—C41.385 (6)C15—H15C0.9600
C3—H30.9300
C2—O2—H2109.5C8iii—C9—C10123.1 (4)
C6—O1—H1113 (5)C5—C4—C3121.7 (4)
C8—N1—C9119.8 (4)C5—C4—H4119.1
C13—N2—C12120.0 (3)C3—C4—H4119.1
O3—N4—O4122.3 (4)C8—C7—H7A109.5
O3—N4—C1118.3 (4)C8—C7—H7B109.5
O4—N4—C1119.3 (4)H7A—C7—H7B109.5
C16—N3—C17118.6 (4)C8—C7—H7C109.5
O2—C2—C3124.8 (3)H7A—C7—H7C109.5
O2—C2—C1116.7 (4)H7B—C7—H7C109.5
C3—C2—C1118.4 (4)C13—C14—H14A109.5
O1—C6—C5125.4 (4)C13—C14—H14B109.5
O1—C6—C1117.1 (4)H14A—C14—H14B109.5
C5—C6—C1117.5 (4)C13—C14—H14C109.5
N2—C12—C13i119.8 (4)H14A—C14—H14C109.5
N2—C12—C11117.3 (4)H14B—C14—H14C109.5
C13i—C12—C11122.9 (4)C12—C11—H11A109.5
C2—C1—C6122.5 (4)C12—C11—H11B109.5
C2—C1—N4119.0 (3)H11A—C11—H11B109.5
C6—C1—N4118.5 (3)C12—C11—H11C109.5
N2—C13—C12i120.2 (4)H11A—C11—H11C109.5
N2—C13—C14117.9 (3)H11B—C11—H11C109.5
C12i—C13—C14121.9 (4)C17—C18—H18A109.5
N3—C16—C17ii121.3 (4)C17—C18—H18B109.5
N3—C16—C15116.9 (4)H18A—C18—H18B109.5
C17ii—C16—C15121.8 (4)C17—C18—H18C109.5
N3—C17—C16ii120.2 (4)H18A—C18—H18C109.5
N3—C17—C18117.1 (4)H18B—C18—H18C109.5
C16ii—C17—C18122.7 (4)C9—C10—H10A109.5
C4—C3—C2119.6 (4)C9—C10—H10B109.5
C4—C3—H3120.2H10A—C10—H10B109.5
C2—C3—H3120.2C9—C10—H10C109.5
N1—C8—C9iii120.3 (4)H10A—C10—H10C109.5
N1—C8—C7117.2 (4)H10B—C10—H10C109.5
C9iii—C8—C7122.4 (4)C16—C15—H15A109.5
C4—C5—C6120.2 (4)C16—C15—H15B109.5
C4—C5—H5119.9H15A—C15—H15B109.5
C6—C5—H5119.9C16—C15—H15C109.5
N1—C9—C8iii119.9 (4)H15A—C15—H15C109.5
N1—C9—C10117.1 (4)H15B—C15—H15C109.5
C13—N2—C12—C13i0.9 (6)C12—N2—C13—C14179.9 (4)
C13—N2—C12—C11179.7 (4)C17—N3—C16—C17ii0.2 (7)
O2—C2—C1—C6179.8 (4)C17—N3—C16—C15179.3 (4)
C3—C2—C1—C62.0 (6)C16—N3—C17—C16ii0.2 (7)
O2—C2—C1—N41.4 (6)C16—N3—C17—C18179.9 (4)
C3—C2—C1—N4179.6 (4)O2—C2—C3—C4178.8 (4)
O1—C6—C1—C2178.9 (4)C1—C2—C3—C40.6 (6)
C5—C6—C1—C22.2 (6)C9—N1—C8—C9iii0.8 (6)
O1—C6—C1—N40.5 (6)C9—N1—C8—C7178.6 (4)
C5—C6—C1—N4179.4 (4)O1—C6—C5—C4179.9 (4)
O3—N4—C1—C296.0 (5)C1—C6—C5—C41.1 (6)
O4—N4—C1—C285.0 (5)C8—N1—C9—C8iii0.8 (6)
O3—N4—C1—C685.6 (5)C8—N1—C9—C10180.0 (4)
O4—N4—C1—C693.5 (5)C6—C5—C4—C30.1 (7)
C12—N2—C13—C12i0.9 (6)C2—C3—C4—C50.4 (7)
Symmetry codes: (i) x, y+2, z+1; (ii) x+1, y, z+1; (iii) x+2, y, z+2.
(3NRES-ACR) top
Crystal data top
C32H23N3O3.99Z = 4
Mr = 513.33F(000) = 1072
Triclinic, P1Dx = 1.370 Mg m3
a = 9.2447 (9) ÅMo Kα radiation, λ = 0.71073 Å
b = 14.4694 (13) ÅCell parameters from 20527 reflections
c = 19.3202 (18) Åθ = 3.0–27.6°
α = 93.232 (7)°µ = 0.09 mm1
β = 102.634 (7)°T = 150 K
γ = 97.795 (7)°Block, yellow
V = 2488.6 (4) Å30.29 × 0.22 × 0.17 mm
Data collection top
Rigaku Mercury375R (2x2 bin mode)
diffractometer
7523 reflections with I > 2σ(I)
Radiation source: Sealed TubeRint = 0.045
profile data from ω–scansθmax = 27.5°, θmin = 3.0°
Absorption correction: multi-scan
Jacobson, R. (1998) Private communication
h = 1112
Tmin = 0.762, Tmax = 1.000k = 1818
25721 measured reflectionsl = 2425
11355 independent reflections
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.057H-atom parameters constrained
wR(F2) = 0.159 w = 1/[σ2(Fo2) + (0.0665P)2 + 0.7465P]
where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max < 0.001
11355 reflectionsΔρmax = 0.58 e Å3
729 parametersΔρmin = 0.40 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
N11.02767 (19)0.09475 (10)0.43919 (8)0.0241 (4)
C400.8842 (2)0.11091 (13)0.42520 (10)0.0249 (4)
C410.7959 (3)0.09336 (15)0.35405 (11)0.0346 (5)
H410.8381300.0716410.3179460.041*
C420.6510 (3)0.10808 (16)0.33857 (13)0.0426 (6)
H420.5948620.0962230.2919240.051*
C430.5838 (3)0.14139 (16)0.39269 (14)0.0428 (6)
H430.4845240.1515220.3811170.051*
C440.6635 (2)0.15847 (14)0.46098 (12)0.0346 (5)
H440.6179950.1797190.4959800.042*
C450.8163 (2)0.14427 (13)0.47990 (11)0.0260 (4)
C460.9031 (2)0.16090 (13)0.54892 (10)0.0254 (4)
H460.8615470.1818980.5854910.031*
C471.0527 (2)0.14621 (12)0.56374 (10)0.0232 (4)
C481.1477 (2)0.16304 (14)0.63360 (10)0.0297 (5)
H481.1107340.1850290.6714510.036*
C491.2923 (3)0.14686 (15)0.64478 (11)0.0336 (5)
H491.3538790.1583720.6903420.040*
C501.3504 (2)0.11272 (14)0.58791 (11)0.0322 (5)
H501.4492530.1017020.5967080.039*
C511.2635 (2)0.09588 (13)0.52075 (11)0.0275 (4)
H511.3032980.0735110.4839940.033*
C521.1117 (2)0.11231 (12)0.50630 (10)0.0227 (4)
N20.48018 (18)0.41106 (10)0.42076 (8)0.0223 (3)
C270.2460 (2)0.41349 (14)0.33878 (11)0.0304 (5)
H270.2965030.4377340.3055780.037*
C280.0938 (3)0.39716 (16)0.32272 (12)0.0389 (5)
H280.0411580.4105270.2785550.047*
C290.0137 (3)0.35985 (15)0.37253 (13)0.0382 (5)
H290.0905880.3484140.3605550.046*
C300.0887 (2)0.34108 (14)0.43700 (12)0.0316 (5)
H300.0352300.3174680.4693410.038*
C310.2486 (2)0.35680 (13)0.45651 (10)0.0244 (4)
C320.3311 (2)0.33894 (13)0.52234 (10)0.0253 (4)
H320.2817160.3163030.5564180.030*
C330.4875 (2)0.35472 (12)0.53763 (10)0.0223 (4)
C340.5787 (2)0.33647 (14)0.60361 (10)0.0293 (5)
H340.5337170.3131360.6389370.035*
C350.7306 (2)0.35284 (14)0.61534 (11)0.0315 (5)
H350.7887680.3401830.6584570.038*
C360.8013 (2)0.38928 (13)0.56201 (11)0.0293 (5)
H360.9054460.4001510.5707190.035*
C370.7189 (2)0.40834 (13)0.49872 (10)0.0257 (4)
H370.7669970.4326580.4646960.031*
C380.5595 (2)0.39142 (12)0.48398 (10)0.0210 (4)
C390.3287 (2)0.39374 (13)0.40614 (10)0.0234 (4)
C200.4392 (2)0.83894 (13)0.06174 (10)0.0263 (4)
H200.3957320.8156630.0975400.032*
C140.5947 (2)0.86094 (13)0.07412 (10)0.0251 (4)
C150.6928 (3)0.85036 (14)0.13999 (11)0.0329 (5)
H150.6533140.8282990.1773260.040*
C160.8440 (3)0.87223 (15)0.14890 (12)0.0372 (5)
H160.9071720.8656280.1923720.045*
C170.9055 (3)0.90497 (14)0.09224 (12)0.0352 (5)
H171.0091060.9184990.0987390.042*
C180.8162 (2)0.91702 (13)0.02857 (11)0.0300 (5)
H180.8589660.9392150.0077710.036*
C190.6569 (2)0.89577 (12)0.01715 (10)0.0233 (4)
N30.57066 (19)0.90952 (10)0.04613 (8)0.0238 (4)
C210.4200 (2)0.88807 (12)0.05718 (10)0.0233 (4)
C220.3286 (2)0.90207 (13)0.12401 (10)0.0290 (5)
H220.3727670.9265440.1592290.035*
C230.1772 (3)0.87994 (14)0.13671 (12)0.0355 (5)
H230.1188210.8889210.1808370.043*
C240.1063 (3)0.84330 (15)0.08377 (13)0.0377 (5)
H240.0024230.8278990.0937200.045*
C250.1887 (2)0.83067 (13)0.01910 (12)0.0316 (5)
H250.1409460.8082730.0155970.038*
C260.3487 (2)0.85138 (12)0.00342 (10)0.0239 (4)
C70.0092 (2)0.66044 (13)0.08920 (10)0.0264 (4)
H70.0215950.6812850.1292850.032*
C10.1535 (2)0.63897 (13)0.09619 (10)0.0255 (4)
C20.2603 (3)0.64742 (14)0.16295 (11)0.0318 (5)
H20.2341090.6683520.2042700.038*
C30.4002 (3)0.62507 (15)0.16655 (12)0.0349 (5)
H30.4683240.6300230.2103320.042*
C40.4423 (3)0.59434 (15)0.10392 (12)0.0347 (5)
H40.5385780.5802510.1069950.042*
C50.3440 (2)0.58507 (13)0.03918 (11)0.0294 (5)
H50.3737740.5646710.0013030.035*
C60.1963 (2)0.60636 (12)0.03313 (10)0.0236 (4)
N40.10118 (19)0.59591 (10)0.03158 (8)0.0245 (4)
C80.0382 (2)0.61774 (13)0.03747 (10)0.0251 (4)
C90.1382 (2)0.60792 (14)0.10569 (11)0.0305 (5)
H90.1069340.5865000.1454640.037*
C100.2794 (3)0.62957 (14)0.11335 (12)0.0343 (5)
H100.3433850.6228310.1583470.041*
C110.3302 (3)0.66231 (14)0.05352 (13)0.0360 (5)
H110.4266230.6772620.0596380.043*
C120.2386 (2)0.67184 (14)0.01249 (12)0.0312 (5)
H120.2736060.6921960.0514330.037*
C130.0892 (2)0.65104 (13)0.02297 (10)0.0250 (4)
O10.85130 (18)0.49834 (9)0.14411 (8)0.0352 (4)
H10.8579000.4638800.1101210.053*
O20.63299 (17)0.51091 (9)0.34051 (7)0.0309 (3)
H2A0.5828440.4791500.3632100.046*
O50.9096 (2)0.61645 (12)0.31244 (10)0.0618 (6)
O60.7650 (2)0.65495 (10)0.22096 (9)0.0475 (4)
N60.80915 (18)0.59709 (11)0.25947 (8)0.0232 (4)
C530.7414 (2)0.49862 (12)0.24225 (9)0.0194 (4)
C540.7690 (2)0.44999 (13)0.18366 (9)0.0221 (4)
C550.7147 (2)0.35471 (13)0.17041 (10)0.0262 (4)
H550.7326340.3201260.1319340.031*
C560.6337 (2)0.31216 (13)0.21537 (10)0.0270 (4)
H560.5985970.2482690.2068260.032*
C570.6031 (2)0.36130 (13)0.27243 (10)0.0258 (4)
H570.5461800.3309550.3009690.031*
C580.6578 (2)0.45657 (13)0.28712 (9)0.0215 (4)
O30.14648 (19)0.00245 (10)0.35063 (7)0.0354 (4)
H3A0.1068870.0301860.3748300.053*
O40.32772 (18)0.00928 (9)0.14213 (7)0.0328 (4)
H4A0.3552960.0242940.1132140.049*
N50.26203 (19)0.09878 (11)0.25486 (9)0.0246 (4)
C590.2409 (2)0.00080 (12)0.24754 (9)0.0200 (4)
C600.1845 (2)0.04575 (13)0.29861 (9)0.0221 (4)
C610.1745 (2)0.14063 (13)0.29335 (10)0.0256 (4)
H610.1383290.1739020.3268140.031*
C620.2188 (2)0.18499 (13)0.23793 (10)0.0273 (4)
H620.2131930.2484060.2351510.033*
C630.2712 (2)0.13734 (13)0.18670 (10)0.0253 (4)
H630.2983890.1684040.1495630.030*
C640.2831 (2)0.04297 (13)0.19076 (9)0.0216 (4)
O80.1573 (2)0.15747 (13)0.25752 (16)0.0356 (9)0.770 (7)
O70.3913 (2)0.11700 (14)0.26010 (18)0.0427 (10)0.800 (8)
O120.1801 (11)0.1557 (5)0.2054 (6)0.047 (4)0.203 (8)
O110.3353 (15)0.1184 (6)0.3042 (7)0.058 (5)0.202 (9)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0306 (10)0.0211 (8)0.0224 (8)0.0024 (7)0.0106 (7)0.0042 (6)
C400.0292 (11)0.0195 (9)0.0257 (10)0.0010 (8)0.0077 (9)0.0044 (8)
C410.0399 (13)0.0348 (12)0.0257 (11)0.0017 (10)0.0042 (10)0.0066 (9)
C420.0403 (14)0.0416 (13)0.0378 (13)0.0041 (11)0.0044 (11)0.0132 (10)
C430.0279 (12)0.0360 (13)0.0609 (16)0.0031 (10)0.0018 (12)0.0113 (11)
C440.0290 (12)0.0274 (11)0.0487 (14)0.0036 (9)0.0110 (11)0.0074 (10)
C450.0277 (11)0.0193 (10)0.0329 (11)0.0017 (8)0.0107 (9)0.0071 (8)
C460.0343 (12)0.0182 (9)0.0278 (10)0.0041 (8)0.0154 (9)0.0034 (8)
C470.0312 (11)0.0166 (9)0.0234 (10)0.0019 (8)0.0102 (9)0.0045 (7)
C480.0396 (13)0.0267 (10)0.0234 (10)0.0035 (9)0.0099 (9)0.0016 (8)
C490.0366 (13)0.0348 (12)0.0264 (11)0.0015 (10)0.0015 (10)0.0072 (9)
C500.0271 (11)0.0286 (11)0.0413 (12)0.0044 (9)0.0067 (10)0.0107 (9)
C510.0297 (11)0.0247 (10)0.0316 (11)0.0058 (8)0.0127 (9)0.0050 (8)
C520.0298 (11)0.0156 (9)0.0245 (10)0.0015 (8)0.0103 (9)0.0043 (7)
N20.0263 (9)0.0210 (8)0.0216 (8)0.0059 (7)0.0088 (7)0.0005 (6)
C270.0361 (12)0.0308 (11)0.0241 (10)0.0093 (9)0.0047 (9)0.0014 (8)
C280.0381 (14)0.0389 (13)0.0345 (12)0.0119 (10)0.0046 (11)0.0032 (10)
C290.0248 (12)0.0357 (12)0.0510 (14)0.0067 (9)0.0028 (11)0.0047 (10)
C300.0254 (11)0.0252 (10)0.0445 (13)0.0029 (8)0.0103 (10)0.0002 (9)
C310.0265 (11)0.0176 (9)0.0307 (10)0.0035 (8)0.0105 (9)0.0004 (8)
C320.0301 (11)0.0202 (10)0.0290 (10)0.0028 (8)0.0150 (9)0.0019 (8)
C330.0294 (11)0.0166 (9)0.0224 (9)0.0029 (8)0.0098 (8)0.0001 (7)
C340.0386 (13)0.0265 (11)0.0244 (10)0.0053 (9)0.0105 (9)0.0031 (8)
C350.0351 (13)0.0322 (11)0.0245 (10)0.0081 (9)0.0001 (9)0.0010 (8)
C360.0248 (11)0.0271 (11)0.0349 (11)0.0046 (8)0.0055 (9)0.0037 (9)
C370.0260 (11)0.0231 (10)0.0291 (10)0.0026 (8)0.0102 (9)0.0003 (8)
C380.0259 (10)0.0164 (9)0.0220 (9)0.0035 (7)0.0088 (8)0.0017 (7)
C390.0278 (11)0.0200 (9)0.0233 (10)0.0053 (8)0.0077 (8)0.0011 (7)
C200.0386 (12)0.0176 (9)0.0294 (11)0.0075 (8)0.0189 (10)0.0058 (8)
C140.0377 (12)0.0181 (9)0.0232 (10)0.0080 (8)0.0123 (9)0.0016 (7)
C150.0476 (14)0.0283 (11)0.0263 (11)0.0129 (10)0.0103 (10)0.0073 (8)
C160.0436 (14)0.0349 (12)0.0298 (11)0.0100 (10)0.0012 (10)0.0031 (9)
C170.0296 (12)0.0295 (11)0.0433 (13)0.0057 (9)0.0020 (10)0.0010 (9)
C180.0346 (12)0.0222 (10)0.0350 (11)0.0026 (9)0.0132 (10)0.0006 (8)
C190.0323 (11)0.0167 (9)0.0231 (10)0.0060 (8)0.0099 (9)0.0006 (7)
N30.0320 (10)0.0198 (8)0.0225 (8)0.0052 (7)0.0121 (7)0.0010 (6)
C210.0330 (11)0.0168 (9)0.0227 (9)0.0057 (8)0.0108 (9)0.0004 (7)
C220.0397 (13)0.0225 (10)0.0252 (10)0.0064 (9)0.0077 (10)0.0006 (8)
C230.0410 (14)0.0278 (11)0.0335 (12)0.0083 (10)0.0015 (10)0.0001 (9)
C240.0287 (12)0.0284 (11)0.0542 (15)0.0045 (9)0.0058 (11)0.0023 (10)
C250.0333 (12)0.0220 (10)0.0440 (13)0.0057 (9)0.0171 (10)0.0057 (9)
C260.0313 (11)0.0156 (9)0.0279 (10)0.0052 (8)0.0120 (9)0.0026 (7)
C70.0388 (12)0.0180 (9)0.0265 (10)0.0022 (8)0.0177 (9)0.0016 (7)
C10.0345 (12)0.0183 (9)0.0261 (10)0.0025 (8)0.0132 (9)0.0032 (8)
C20.0443 (14)0.0273 (11)0.0251 (10)0.0025 (9)0.0126 (10)0.0016 (8)
C30.0376 (13)0.0345 (12)0.0306 (11)0.0043 (10)0.0041 (10)0.0047 (9)
C40.0347 (13)0.0305 (11)0.0406 (13)0.0068 (9)0.0100 (11)0.0068 (9)
C50.0377 (12)0.0236 (10)0.0317 (11)0.0057 (9)0.0170 (10)0.0052 (8)
C60.0320 (11)0.0160 (9)0.0251 (10)0.0016 (8)0.0123 (9)0.0038 (7)
N40.0320 (10)0.0194 (8)0.0250 (8)0.0033 (7)0.0131 (8)0.0036 (6)
C80.0329 (11)0.0182 (9)0.0266 (10)0.0003 (8)0.0132 (9)0.0051 (7)
C90.0383 (13)0.0272 (11)0.0274 (11)0.0009 (9)0.0121 (10)0.0057 (8)
C100.0370 (13)0.0293 (11)0.0335 (12)0.0001 (9)0.0037 (10)0.0068 (9)
C110.0293 (12)0.0267 (11)0.0533 (14)0.0045 (9)0.0114 (11)0.0062 (10)
C120.0345 (12)0.0226 (10)0.0399 (12)0.0028 (9)0.0171 (10)0.0011 (9)
C130.0299 (11)0.0173 (9)0.0305 (10)0.0013 (8)0.0140 (9)0.0029 (8)
O10.0527 (10)0.0264 (8)0.0320 (8)0.0033 (7)0.0285 (8)0.0036 (6)
O20.0443 (9)0.0262 (7)0.0269 (7)0.0019 (6)0.0213 (7)0.0011 (6)
O50.0529 (12)0.0384 (10)0.0695 (13)0.0036 (8)0.0314 (10)0.0011 (9)
O60.0646 (12)0.0254 (8)0.0443 (9)0.0064 (8)0.0065 (9)0.0091 (7)
N60.0245 (9)0.0229 (8)0.0225 (8)0.0036 (7)0.0061 (7)0.0016 (7)
C530.0195 (10)0.0188 (9)0.0188 (9)0.0023 (7)0.0024 (8)0.0010 (7)
C540.0220 (10)0.0265 (10)0.0189 (9)0.0021 (8)0.0075 (8)0.0039 (7)
C550.0329 (11)0.0239 (10)0.0227 (10)0.0035 (8)0.0102 (9)0.0025 (8)
C560.0328 (12)0.0190 (9)0.0295 (10)0.0003 (8)0.0109 (9)0.0007 (8)
C570.0310 (11)0.0234 (10)0.0262 (10)0.0024 (8)0.0133 (9)0.0055 (8)
C580.0252 (10)0.0230 (10)0.0178 (9)0.0058 (8)0.0068 (8)0.0017 (7)
O30.0590 (11)0.0288 (8)0.0286 (8)0.0119 (7)0.0271 (8)0.0078 (6)
O40.0506 (10)0.0275 (8)0.0295 (8)0.0105 (7)0.0258 (7)0.0053 (6)
N50.0276 (10)0.0260 (9)0.0221 (9)0.0060 (8)0.0088 (8)0.0022 (7)
C590.0191 (10)0.0205 (9)0.0196 (9)0.0024 (7)0.0032 (8)0.0016 (7)
C600.0240 (10)0.0239 (10)0.0189 (9)0.0014 (8)0.0076 (8)0.0012 (7)
C610.0314 (11)0.0256 (10)0.0224 (10)0.0064 (8)0.0114 (9)0.0011 (8)
C620.0345 (12)0.0217 (10)0.0275 (10)0.0039 (8)0.0110 (9)0.0023 (8)
C630.0290 (11)0.0255 (10)0.0238 (10)0.0033 (8)0.0105 (9)0.0065 (8)
C640.0194 (10)0.0278 (10)0.0175 (9)0.0018 (8)0.0056 (8)0.0003 (7)
O80.0362 (13)0.0214 (11)0.051 (2)0.0010 (8)0.0158 (11)0.0047 (9)
O70.0306 (13)0.0431 (13)0.058 (2)0.0179 (9)0.0085 (11)0.0116 (11)
O120.052 (6)0.021 (4)0.053 (8)0.003 (4)0.016 (5)0.003 (4)
O110.069 (9)0.049 (6)0.045 (8)0.033 (5)0.024 (6)0.005 (4)
Geometric parameters (Å, º) top
N1—C521.348 (2)C23—C241.420 (3)
N1—C401.350 (3)C23—H230.9300
C40—C411.426 (3)C24—C251.350 (3)
C40—C451.435 (3)C24—H240.9300
C41—C421.356 (3)C25—C261.429 (3)
C41—H410.9300C25—H250.9300
C42—C431.421 (3)C7—C131.386 (3)
C42—H420.9300C7—C11.391 (3)
C43—C441.354 (3)C7—H70.9300
C43—H430.9300C1—C21.430 (3)
C44—C451.425 (3)C1—C61.435 (3)
C44—H440.9300C2—C31.363 (3)
C45—C461.387 (3)C2—H20.9300
C46—C471.398 (3)C3—C41.416 (3)
C46—H460.9300C3—H30.9300
C47—C481.428 (3)C4—C51.363 (3)
C47—C521.430 (3)C4—H40.9300
C48—C491.362 (3)C5—C61.422 (3)
C48—H480.9300C5—H50.9300
C49—C501.417 (3)C6—N41.349 (2)
C49—H490.9300N4—C81.350 (3)
C50—C511.358 (3)C8—C91.422 (3)
C50—H500.9300C8—C131.435 (3)
C51—C521.425 (3)C9—C101.362 (3)
C51—H510.9300C9—H90.9300
N2—C381.347 (2)C10—C111.420 (3)
N2—C391.352 (2)C10—H100.9300
C27—C281.357 (3)C11—C121.356 (3)
C27—C391.423 (3)C11—H110.9300
C27—H270.9300C12—C131.427 (3)
C28—C291.424 (3)C12—H120.9300
C28—H280.9300O1—C541.350 (2)
C29—C301.348 (3)O1—H10.8200
C29—H290.9300O2—C581.340 (2)
C30—C311.427 (3)O2—H2A0.8200
C30—H300.9300O5—N61.212 (2)
C31—C321.390 (3)O6—N61.205 (2)
C31—C391.431 (3)N6—C531.465 (2)
C32—C331.394 (3)C53—C541.388 (2)
C32—H320.9300C53—C581.394 (2)
C33—C341.426 (3)C54—C551.391 (3)
C33—C381.438 (2)C55—C561.384 (3)
C34—C351.358 (3)C55—H550.9300
C34—H340.9300C56—C571.380 (3)
C35—C361.425 (3)C56—H560.9300
C35—H350.9300C57—C581.393 (3)
C36—C371.356 (3)C57—H570.9300
C36—H360.9300O3—C601.337 (2)
C37—C381.423 (3)O3—H3A0.8200
C37—H370.9300O4—C641.341 (2)
C20—C261.387 (3)O4—H4A0.8200
C20—C141.393 (3)N5—O111.118 (8)
C20—H200.9300N5—O81.210 (2)
C14—C151.421 (3)N5—O71.242 (3)
C14—C191.434 (3)N5—O121.262 (8)
C15—C161.361 (3)N5—C591.467 (2)
C15—H150.9300C59—C601.394 (2)
C16—C171.416 (3)C59—C641.398 (2)
C16—H160.9300C60—C611.396 (3)
C17—C181.358 (3)C61—C621.387 (3)
C17—H170.9300C61—H610.9300
C18—C191.428 (3)C62—C631.383 (3)
C18—H180.9300C62—H620.9300
C19—N31.347 (2)C63—C641.390 (3)
N3—C211.352 (3)C63—H630.9300
C21—C221.422 (3)O8—O121.074 (12)
C21—C261.436 (3)O8—O111.698 (11)
C22—C231.357 (3)O7—O111.090 (15)
C22—H220.9300
C52—N1—C40119.35 (16)C25—C24—C23120.4 (2)
N1—C40—C41119.31 (18)C25—C24—H24119.8
N1—C40—C45122.12 (18)C23—C24—H24119.8
C41—C40—C45118.57 (19)C24—C25—C26120.67 (19)
C42—C41—C40120.6 (2)C24—C25—H25119.7
C42—C41—H41119.7C26—C25—H25119.7
C40—C41—H41119.7C20—C26—C25123.25 (18)
C41—C42—C43120.9 (2)C20—C26—C21118.00 (18)
C41—C42—H42119.6C25—C26—C21118.74 (18)
C43—C42—H42119.6C13—C7—C1120.53 (17)
C44—C43—C42120.4 (2)C13—C7—H7119.7
C44—C43—H43119.8C1—C7—H7119.7
C42—C43—H43119.8C7—C1—C2123.21 (18)
C43—C44—C45120.8 (2)C7—C1—C6118.02 (18)
C43—C44—H44119.6C2—C1—C6118.77 (18)
C45—C44—H44119.6C3—C2—C1120.58 (19)
C46—C45—C44123.18 (19)C3—C2—H2119.7
C46—C45—C40118.07 (18)C1—C2—H2119.7
C44—C45—C40118.75 (19)C2—C3—C4120.3 (2)
C45—C46—C47120.26 (18)C2—C3—H3119.9
C45—C46—H46119.9C4—C3—H3119.9
C47—C46—H46119.9C5—C4—C3121.1 (2)
C46—C47—C48122.68 (18)C5—C4—H4119.4
C46—C47—C52118.21 (18)C3—C4—H4119.4
C48—C47—C52119.10 (18)C4—C5—C6120.47 (18)
C49—C48—C47119.96 (19)C4—C5—H5119.8
C49—C48—H48120.0C6—C5—H5119.8
C47—C48—H48120.0N4—C6—C5119.12 (17)
C48—C49—C50120.9 (2)N4—C6—C1122.11 (18)
C48—C49—H49119.6C5—C6—C1118.78 (18)
C50—C49—H49119.6C6—N4—C8119.08 (16)
C51—C50—C49120.9 (2)N4—C8—C9119.31 (17)
C51—C50—H50119.6N4—C8—C13122.16 (18)
C49—C50—H50119.6C9—C8—C13118.53 (18)
C50—C51—C52120.32 (19)C10—C9—C8120.66 (19)
C50—C51—H51119.8C10—C9—H9119.7
C52—C51—H51119.8C8—C9—H9119.7
N1—C52—C51119.18 (17)C9—C10—C11120.9 (2)
N1—C52—C47121.96 (18)C9—C10—H10119.6
C51—C52—C47118.86 (18)C11—C10—H10119.6
C38—N2—C39119.52 (16)C12—C11—C10120.3 (2)
C28—C27—C39120.4 (2)C12—C11—H11119.9
C28—C27—H27119.8C10—C11—H11119.9
C39—C27—H27119.8C11—C12—C13120.84 (19)
C27—C28—C29120.9 (2)C11—C12—H12119.6
C27—C28—H28119.5C13—C12—H12119.6
C29—C28—H28119.5C7—C13—C12123.07 (18)
C30—C29—C28120.1 (2)C7—C13—C8118.09 (18)
C30—C29—H29119.9C12—C13—C8118.83 (19)
C28—C29—H29119.9C54—O1—H1109.5
C29—C30—C31121.2 (2)C58—O2—H2A109.5
C29—C30—H30119.4O6—N6—O5122.75 (17)
C31—C30—H30119.4O6—N6—C53119.65 (16)
C32—C31—C30123.40 (18)O5—N6—C53117.60 (16)
C32—C31—C39118.10 (18)C54—C53—C58122.76 (16)
C30—C31—C39118.50 (18)C54—C53—N6118.42 (15)
C31—C32—C33120.47 (17)C58—C53—N6118.75 (15)
C31—C32—H32119.8O1—C54—C53117.34 (16)
C33—C32—H32119.8O1—C54—C55124.06 (17)
C32—C33—C34123.30 (17)C53—C54—C55118.57 (16)
C32—C33—C38118.00 (17)C56—C55—C54118.99 (17)
C34—C33—C38118.70 (18)C56—C55—H55120.5
C35—C34—C33120.65 (18)C54—C55—H55120.5
C35—C34—H34119.7C57—C56—C55122.22 (18)
C33—C34—H34119.7C57—C56—H56118.9
C34—C35—C36120.41 (19)C55—C56—H56118.9
C34—C35—H35119.8C56—C57—C58119.72 (17)
C36—C35—H35119.8C56—C57—H57120.1
C37—C36—C35120.92 (19)C58—C57—H57120.1
C37—C36—H36119.5O2—C58—C57124.49 (16)
C35—C36—H36119.5O2—C58—C53117.79 (16)
C36—C37—C38120.50 (18)C57—C58—C53117.71 (16)
C36—C37—H37119.8C60—O3—H3A109.5
C38—C37—H37119.8C64—O4—H4A109.5
N2—C38—C37119.35 (16)O11—N5—O893.5 (8)
N2—C38—C33121.82 (17)O11—N5—O754.7 (8)
C37—C38—C33118.82 (17)O8—N5—O7122.64 (19)
N2—C39—C27119.09 (17)O11—N5—O12125.3 (6)
N2—C39—C31122.06 (17)O8—N5—O1251.5 (5)
C27—C39—C31118.85 (18)O7—N5—O12105.6 (5)
C26—C20—C14120.69 (17)O11—N5—C59120.2 (5)
C26—C20—H20119.7O8—N5—C59120.36 (17)
C14—C20—H20119.7O7—N5—C59116.97 (17)
C20—C14—C15123.11 (18)O12—N5—C59114.1 (4)
C20—C14—C19117.72 (18)C60—C59—C64122.66 (16)
C15—C14—C19119.17 (19)C60—C59—N5118.86 (15)
C16—C15—C14120.58 (19)C64—C59—N5118.44 (16)
C16—C15—H15119.7O3—C60—C59118.15 (16)
C14—C15—H15119.7O3—C60—C61123.83 (16)
C15—C16—C17120.2 (2)C59—C60—C61118.01 (16)
C15—C16—H16119.9C62—C61—C60119.63 (17)
C17—C16—H16119.9C62—C61—H61120.2
C18—C17—C16121.3 (2)C60—C61—H61120.2
C18—C17—H17119.4C63—C62—C61121.70 (18)
C16—C17—H17119.4C63—C62—H62119.2
C17—C18—C19120.32 (19)C61—C62—H62119.2
C17—C18—H18119.8C62—C63—C64119.94 (17)
C19—C18—H18119.8C62—C63—H63120.0
N3—C19—C18119.18 (17)C64—C63—H63120.0
N3—C19—C14122.43 (18)O4—C64—C63123.84 (16)
C18—C19—C14118.40 (18)O4—C64—C59118.09 (16)
C19—N3—C21119.08 (16)C63—C64—C59118.03 (16)
N3—C21—C22119.29 (17)O12—O8—N566.7 (4)
N3—C21—C26122.07 (17)O12—O8—O1196.9 (7)
C22—C21—C26118.64 (18)N5—O8—O1141.1 (4)
C23—C22—C21120.39 (19)O11—O7—N556.8 (4)
C23—C22—H22119.8O8—O12—N561.8 (6)
C21—C22—H22119.8O7—O11—N568.5 (8)
C22—C23—C24121.1 (2)O7—O11—O898.7 (7)
C22—C23—H23119.4N5—O11—O845.4 (4)
C24—C23—H23119.4
C52—N1—C40—C41179.26 (16)C7—C1—C2—C3179.82 (19)
C52—N1—C40—C451.5 (3)C6—C1—C2—C30.1 (3)
N1—C40—C41—C42179.34 (18)C1—C2—C3—C40.9 (3)
C45—C40—C41—C420.1 (3)C2—C3—C4—C51.0 (3)
C40—C41—C42—C430.1 (3)C3—C4—C5—C60.1 (3)
C41—C42—C43—C440.4 (3)C4—C5—C6—N4179.56 (17)
C42—C43—C44—C450.6 (3)C4—C5—C6—C10.9 (3)
C43—C44—C45—C46179.82 (19)C7—C1—C6—N40.3 (3)
C43—C44—C45—C400.4 (3)C2—C1—C6—N4179.46 (17)
N1—C40—C45—C460.6 (3)C7—C1—C6—C5179.31 (17)
C41—C40—C45—C46179.86 (17)C2—C1—C6—C51.0 (3)
N1—C40—C45—C44179.19 (17)C5—C6—N4—C8178.82 (16)
C41—C40—C45—C440.0 (3)C1—C6—N4—C80.7 (3)
C44—C45—C46—C47179.50 (17)C6—N4—C8—C9179.25 (16)
C40—C45—C46—C470.7 (3)C6—N4—C8—C130.5 (3)
C45—C46—C47—C48179.36 (17)N4—C8—C9—C10179.87 (17)
C45—C46—C47—C521.1 (3)C13—C8—C9—C100.1 (3)
C46—C47—C48—C49179.60 (18)C8—C9—C10—C110.1 (3)
C52—C47—C48—C490.1 (3)C9—C10—C11—C120.5 (3)
C47—C48—C49—C500.5 (3)C10—C11—C12—C131.2 (3)
C48—C49—C50—C510.5 (3)C1—C7—C13—C12179.90 (17)
C49—C50—C51—C520.0 (3)C1—C7—C13—C80.7 (3)
C40—N1—C52—C51179.49 (16)C11—C12—C13—C7179.40 (18)
C40—N1—C52—C471.1 (3)C11—C12—C13—C81.4 (3)
C50—C51—C52—N1179.79 (17)N4—C8—C13—C70.2 (3)
C50—C51—C52—C470.4 (3)C9—C8—C13—C7179.95 (17)
C46—C47—C52—N10.2 (3)N4—C8—C13—C12179.44 (16)
C48—C47—C52—N1179.77 (16)C9—C8—C13—C120.8 (3)
C46—C47—C52—C51179.22 (16)O6—N6—C53—C5469.9 (2)
C48—C47—C52—C510.3 (3)O5—N6—C53—C54109.5 (2)
C39—C27—C28—C290.2 (3)O6—N6—C53—C58113.0 (2)
C27—C28—C29—C300.7 (3)O5—N6—C53—C5867.6 (2)
C28—C29—C30—C310.8 (3)C58—C53—C54—O1179.89 (17)
C29—C30—C31—C32179.75 (19)N6—C53—C54—O13.1 (3)
C29—C30—C31—C390.4 (3)C58—C53—C54—C552.0 (3)
C30—C31—C32—C33179.15 (17)N6—C53—C54—C55175.02 (17)
C39—C31—C32—C331.5 (3)O1—C54—C55—C56178.88 (19)
C31—C32—C33—C34178.97 (17)C53—C54—C55—C560.9 (3)
C31—C32—C33—C381.2 (3)C54—C55—C56—C570.9 (3)
C32—C33—C34—C35179.69 (18)C55—C56—C57—C581.6 (3)
C38—C33—C34—C350.4 (3)C56—C57—C58—O2179.09 (19)
C33—C34—C35—C360.5 (3)C56—C57—C58—C530.5 (3)
C34—C35—C36—C370.0 (3)C54—C53—C58—O2177.42 (17)
C35—C36—C37—C380.6 (3)N6—C53—C58—O25.6 (3)
C39—N2—C38—C37178.99 (16)C54—C53—C58—C571.3 (3)
C39—N2—C38—C331.8 (3)N6—C53—C58—C57175.71 (17)
C36—C37—C38—N2179.91 (17)O11—N5—C59—C6057.5 (11)
C36—C37—C38—C330.6 (3)O8—N5—C59—C6057.6 (3)
C32—C33—C38—N20.5 (3)O7—N5—C59—C60120.4 (2)
C34—C33—C38—N2179.37 (16)O12—N5—C59—C60115.7 (7)
C32—C33—C38—C37179.75 (16)O11—N5—C59—C64120.4 (10)
C34—C33—C38—C370.1 (3)O8—N5—C59—C64124.5 (2)
C38—N2—C39—C27179.11 (16)O7—N5—C59—C6457.5 (3)
C38—N2—C39—C311.4 (3)O12—N5—C59—C6466.4 (7)
C28—C27—C39—N2179.74 (18)C64—C59—C60—O3179.56 (18)
C28—C27—C39—C310.2 (3)N5—C59—C60—O32.6 (3)
C32—C31—C39—N20.2 (3)C64—C59—C60—C611.9 (3)
C30—C31—C39—N2179.61 (17)N5—C59—C60—C61175.88 (17)
C32—C31—C39—C27179.26 (17)O3—C60—C61—C62179.04 (19)
C30—C31—C39—C270.1 (3)C59—C60—C61—C620.6 (3)
C26—C20—C14—C15179.46 (17)C60—C61—C62—C630.9 (3)
C26—C20—C14—C190.6 (3)C61—C62—C63—C641.2 (3)
C20—C14—C15—C16179.43 (19)C62—C63—C64—O4177.61 (19)
C19—C14—C15—C160.5 (3)C62—C63—C64—C590.0 (3)
C14—C15—C16—C170.6 (3)C60—C59—C64—O4176.14 (17)
C15—C16—C17—C181.2 (3)N5—C59—C64—O46.0 (3)
C16—C17—C18—C190.6 (3)C60—C59—C64—C631.7 (3)
C17—C18—C19—N3179.11 (17)N5—C59—C64—C63176.18 (17)
C17—C18—C19—C140.5 (3)O11—N5—O8—O12133.7 (8)
C20—C14—C19—N31.5 (3)O7—N5—O8—O1284.1 (6)
C15—C14—C19—N3178.52 (17)C59—N5—O8—O1298.0 (5)
C20—C14—C19—C18178.86 (17)O7—N5—O8—O1149.6 (6)
C15—C14—C19—C181.1 (3)O12—N5—O8—O11133.7 (8)
C18—C19—N3—C21179.04 (16)C59—N5—O8—O11128.3 (7)
C14—C19—N3—C211.4 (3)O8—N5—O7—O1168.7 (7)
C19—N3—C21—C22179.72 (16)O12—N5—O7—O11122.6 (8)
C19—N3—C21—C260.3 (3)C59—N5—O7—O11109.3 (6)
N3—C21—C22—C23179.15 (17)O11—O8—O12—N528.6 (4)
C26—C21—C22—C230.8 (3)O11—N5—O12—O862.1 (13)
C21—C22—C23—C240.6 (3)O7—N5—O12—O8119.6 (4)
C22—C23—C24—C250.7 (3)C59—N5—O12—O8110.6 (4)
C23—C24—C25—C261.8 (3)N5—O7—O11—O834.4 (2)
C14—C20—C26—C25179.57 (17)O8—N5—O11—O7128.2 (4)
C14—C20—C26—C210.4 (3)O12—N5—O11—O784.3 (11)
C24—C25—C26—C20179.34 (18)C59—N5—O11—O7103.3 (5)
C24—C25—C26—C211.5 (3)O7—N5—O11—O8128.2 (4)
N3—C21—C26—C200.6 (3)O12—N5—O11—O843.9 (9)
C22—C21—C26—C20179.39 (16)C59—N5—O11—O8128.5 (6)
N3—C21—C26—C25179.82 (16)O12—O8—O11—O75.7 (7)
C22—C21—C26—C250.2 (3)N5—O8—O11—O747.7 (6)
C13—C7—C1—C2179.84 (17)O12—O8—O11—N542.0 (7)
C13—C7—C1—C60.5 (3)
(4NRES-DMP) top
Crystal data top
C12H13N3O4F(000) = 552
Mr = 263.25Dx = 1.392 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
a = 8.7482 (14) ÅCell parameters from 4346 reflections
b = 14.926 (3) Åθ = 3.5–27.6°
c = 10.2464 (17) ŵ = 0.11 mm1
β = 110.165 (8)°T = 150 K
V = 1255.9 (4) Å3Block, brown
Z = 40.26 × 0.21 × 0.17 mm
Data collection top
Rigaku Mercury375R (2x2 bin mode)
diffractometer
859 reflections with I > 2σ(I)
Radiation source: Sealed TubeRint = 0.065
profile data from ω–scansθmax = 27.5°, θmin = 3.5°
Absorption correction: multi-scan
Jacobson, R. (1998) Private communication
h = 1111
Tmin = 0.793, Tmax = 1.000k = 1919
6402 measured reflectionsl = 1313
1441 independent reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.057 w = 1/[σ2(Fo2) + (0.1096P)2]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.199(Δ/σ)max < 0.001
S = 1.02Δρmax = 0.34 e Å3
1441 reflectionsΔρmin = 0.22 e Å3
90 parametersExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.019 (5)
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
N10.0000000.44224 (18)0.2500000.0487 (8)
O10.28383 (18)0.35093 (11)0.34731 (19)0.0559 (6)
H10.3643900.3184730.3715990.084*
C60.7062 (3)0.33684 (14)0.4823 (2)0.0418 (6)
C30.1487 (3)0.30020 (15)0.3006 (2)0.0415 (6)
N20.5878 (2)0.27505 (13)0.43909 (18)0.0440 (6)
C10.0000000.1629 (2)0.2500000.0554 (9)
H1A0.0000000.1005850.2500000.066*
C70.8662 (3)0.31027 (14)0.5418 (2)0.0452 (6)
H70.9461050.3543020.5700730.054*
C40.0000000.34430 (19)0.2500000.0385 (7)
C20.1472 (3)0.20758 (16)0.3021 (2)0.0509 (7)
H20.2440260.1756660.3377740.061*
O20.0475 (3)0.48063 (13)0.1684 (2)0.0884 (8)
C80.6575 (3)0.43299 (15)0.4621 (3)0.0655 (8)
H8A0.7526960.4700490.4970640.098*
H8B0.6039020.4446970.3648190.098*
H8C0.5846850.4461460.5113690.098*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0235 (14)0.0466 (17)0.0668 (19)0.0000.0038 (14)0.000
O10.0243 (9)0.0519 (11)0.0802 (13)0.0051 (7)0.0035 (9)0.0034 (8)
C60.0324 (12)0.0406 (13)0.0506 (13)0.0046 (10)0.0121 (11)0.0037 (9)
C30.0329 (13)0.0469 (14)0.0403 (12)0.0001 (10)0.0070 (10)0.0002 (9)
N20.0325 (11)0.0429 (11)0.0521 (12)0.0056 (8)0.0090 (9)0.0028 (8)
C10.056 (2)0.0394 (18)0.066 (2)0.0000.016 (2)0.000
C70.0306 (12)0.0410 (13)0.0591 (14)0.0003 (10)0.0093 (11)0.0063 (10)
C40.0311 (16)0.0391 (17)0.0424 (17)0.0000.0089 (14)0.000
C20.0425 (15)0.0503 (15)0.0564 (15)0.0107 (11)0.0125 (13)0.0051 (11)
O20.0965 (17)0.0601 (13)0.1218 (18)0.0156 (12)0.0547 (15)0.0375 (11)
C80.0460 (17)0.0444 (15)0.101 (2)0.0097 (12)0.0185 (16)0.0035 (13)
Geometric parameters (Å, º) top
N1—O2i1.200 (2)C6—C81.491 (3)
N1—O21.200 (2)C3—C21.383 (3)
N1—C41.462 (4)C3—C41.389 (3)
O1—C31.345 (3)N2—C7ii1.330 (3)
C6—N21.343 (3)C1—C21.383 (3)
C6—C71.378 (3)C1—C2i1.383 (3)
O2i—N1—O2123.0 (3)C2—C3—C4117.8 (2)
O2i—N1—C4118.52 (16)C7ii—N2—C6116.69 (19)
O2—N1—C4118.52 (16)C2—C1—C2i122.3 (3)
N2—C6—C7119.9 (2)N2ii—C7—C6123.4 (2)
N2—C6—C8117.7 (2)C3—C4—C3i123.4 (3)
C7—C6—C8122.4 (2)C3—C4—N1118.29 (14)
O1—C3—C2124.7 (2)C3i—C4—N1118.29 (14)
O1—C3—C4117.5 (2)C3—C2—C1119.3 (2)
Symmetry codes: (i) x, y, z+1/2; (ii) x+3/2, y+1/2, z+1.
(5NRES-9AACR) top
Crystal data top
C19H15N3O4Z = 2
Mr = 349.34F(000) = 364
Triclinic, P1Dx = 1.475 Mg m3
a = 7.7638 (14) ÅMo Kα radiation, λ = 0.71075 Å
b = 8.5897 (15) ÅCell parameters from 5658 reflections
c = 12.723 (2) Åθ = 3.4–27.6°
α = 105.585 (7)°µ = 0.11 mm1
β = 102.978 (7)°T = 150 K
γ = 95.062 (7)°Block, yellow
V = 786.3 (2) Å30.20 × 0.20 × 0.20 mm
Data collection top
Rigaku Mercury375R (2x2 bin mode)
diffractometer
2234 reflections with I > 2σ(I)
Radiation source: Sealed TubeRint = 0.039
profile data from ω–scansθmax = 27.5°, θmin = 3.4°
Absorption correction: multi-scan
Jacobson, R. (1998) Private communication
h = 1010
Tmin = 0.744, Tmax = 1.000k = 1111
7168 measured reflectionsl = 1616
3538 independent reflections
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.053H-atom parameters constrained
wR(F2) = 0.177 w = 1/[σ2(Fo2) + (0.0982P)2]
where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max < 0.001
3538 reflectionsΔρmax = 0.31 e Å3
236 parametersΔρmin = 0.36 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O10.5554 (2)0.10015 (18)0.27152 (12)0.0271 (4)
O20.7822 (2)0.22913 (19)0.02638 (13)0.0326 (4)
H20.8724740.1606780.0052700.049*
O30.9559 (2)0.0378 (2)0.10529 (14)0.0427 (5)
N10.2317 (2)0.6350 (2)0.55075 (14)0.0228 (4)
H10.2365360.7153730.6092910.027*
N30.8378 (2)0.0623 (2)0.15944 (15)0.0265 (4)
O40.8673 (2)0.1826 (2)0.24322 (15)0.0479 (6)
N20.2836 (2)0.2822 (2)0.27473 (14)0.0261 (5)
H2A0.3349620.2004560.2842680.031*
H2B0.2541180.2950550.2086440.031*
C130.2875 (3)0.4950 (2)0.56593 (17)0.0209 (5)
C190.2503 (3)0.3873 (3)0.36111 (17)0.0209 (5)
C180.2996 (3)0.3662 (2)0.47215 (17)0.0198 (5)
C120.1689 (3)0.6527 (3)0.44704 (17)0.0218 (5)
C10.6759 (3)0.0486 (2)0.12276 (16)0.0208 (5)
C70.1683 (3)0.5280 (3)0.34856 (17)0.0210 (5)
C20.5357 (3)0.0162 (2)0.17994 (17)0.0215 (5)
C60.6514 (3)0.1911 (3)0.02691 (17)0.0235 (5)
C170.3608 (3)0.2233 (3)0.49234 (18)0.0247 (5)
H170.3697520.1376890.4319920.030*
C90.0338 (3)0.6917 (3)0.2342 (2)0.0302 (5)
H90.0144180.7042750.1636540.036*
C140.3363 (3)0.4786 (3)0.67554 (18)0.0255 (5)
H140.3283800.5627680.7370990.031*
C150.3951 (3)0.3398 (3)0.69155 (19)0.0291 (5)
H150.4279840.3305930.7643000.035*
C50.4916 (3)0.2950 (3)0.01254 (18)0.0317 (6)
H50.4761960.3896430.0724570.038*
C40.3512 (3)0.2580 (3)0.03798 (19)0.0330 (6)
H40.2415680.3269530.0084830.040*
C110.1083 (3)0.7995 (3)0.43761 (19)0.0287 (5)
H110.1132440.8839520.5023190.034*
C80.0968 (3)0.5510 (3)0.24207 (18)0.0267 (5)
H80.0928560.4687090.1764720.032*
C160.4067 (3)0.2101 (3)0.59960 (19)0.0275 (5)
H160.4455910.1154630.6117380.033*
C30.3702 (3)0.1246 (3)0.12860 (19)0.0297 (5)
H30.2723790.1035740.1579480.036*
C100.0420 (3)0.8178 (3)0.3331 (2)0.0319 (6)
H100.0018790.9148820.3273860.038*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0261 (8)0.0255 (8)0.0258 (8)0.0022 (7)0.0108 (7)0.0017 (7)
O20.0392 (10)0.0329 (10)0.0232 (8)0.0083 (8)0.0119 (8)0.0003 (7)
O30.0274 (10)0.0594 (12)0.0320 (10)0.0035 (8)0.0169 (8)0.0060 (9)
N10.0263 (10)0.0196 (9)0.0197 (9)0.0057 (8)0.0069 (8)0.0002 (7)
N30.0245 (10)0.0286 (10)0.0235 (10)0.0032 (8)0.0089 (8)0.0013 (8)
O40.0324 (10)0.0390 (11)0.0518 (11)0.0100 (8)0.0209 (9)0.0236 (9)
N20.0288 (10)0.0261 (10)0.0205 (9)0.0074 (8)0.0050 (8)0.0022 (8)
C130.0176 (11)0.0188 (11)0.0233 (11)0.0002 (9)0.0069 (9)0.0008 (9)
C190.0159 (10)0.0217 (11)0.0205 (11)0.0026 (8)0.0057 (9)0.0006 (8)
C180.0176 (10)0.0177 (10)0.0223 (11)0.0007 (8)0.0062 (9)0.0030 (8)
C120.0188 (11)0.0209 (11)0.0243 (11)0.0006 (9)0.0075 (9)0.0037 (9)
C10.0243 (11)0.0161 (10)0.0204 (11)0.0037 (9)0.0043 (9)0.0041 (9)
C70.0175 (10)0.0213 (11)0.0231 (11)0.0003 (8)0.0065 (9)0.0046 (9)
C20.0239 (11)0.0190 (11)0.0235 (11)0.0054 (9)0.0078 (9)0.0076 (9)
C60.0308 (12)0.0243 (11)0.0166 (10)0.0096 (10)0.0064 (9)0.0061 (9)
C170.0231 (12)0.0225 (11)0.0276 (12)0.0040 (9)0.0104 (10)0.0026 (9)
C90.0300 (13)0.0359 (13)0.0274 (12)0.0050 (11)0.0066 (10)0.0145 (10)
C140.0273 (12)0.0248 (12)0.0208 (11)0.0024 (9)0.0066 (10)0.0009 (9)
C150.0297 (12)0.0320 (13)0.0243 (12)0.0011 (10)0.0077 (10)0.0068 (10)
C50.0468 (15)0.0218 (12)0.0188 (11)0.0011 (11)0.0018 (11)0.0003 (9)
C40.0305 (13)0.0296 (13)0.0297 (13)0.0081 (11)0.0027 (11)0.0068 (10)
C110.0309 (13)0.0234 (12)0.0313 (12)0.0054 (10)0.0106 (10)0.0049 (10)
C80.0251 (12)0.0296 (12)0.0222 (11)0.0023 (10)0.0054 (10)0.0035 (9)
C160.0275 (12)0.0236 (12)0.0334 (13)0.0069 (10)0.0099 (11)0.0094 (10)
C30.0240 (12)0.0313 (13)0.0330 (13)0.0016 (10)0.0091 (10)0.0078 (10)
C100.0337 (13)0.0288 (13)0.0363 (14)0.0081 (10)0.0107 (11)0.0125 (11)
Geometric parameters (Å, º) top
O1—C21.283 (2)C2—C31.425 (3)
O2—C61.359 (3)C6—C51.368 (3)
O2—H20.8200C17—C161.369 (3)
O3—N31.264 (2)C17—H170.9300
N1—C121.354 (3)C9—C81.363 (3)
N1—C131.360 (3)C9—C101.408 (3)
N1—H10.8600C9—H90.9300
N3—O41.230 (2)C14—C151.362 (3)
N3—C11.411 (3)C14—H140.9300
N2—C191.314 (2)C15—C161.408 (3)
N2—H2A0.8600C15—H150.9300
N2—H2B0.8600C5—C41.403 (3)
C13—C141.409 (3)C5—H50.9300
C13—C181.420 (3)C4—C31.359 (3)
C19—C181.443 (3)C4—H40.9300
C19—C71.444 (3)C11—C101.370 (3)
C18—C171.420 (3)C11—H110.9300
C12—C71.411 (3)C8—H80.9300
C12—C111.410 (3)C16—H160.9300
C1—C61.440 (3)C3—H30.9300
C1—C21.446 (3)C10—H100.9300
C7—C81.417 (3)
C6—O2—H2109.5C16—C17—C18120.8 (2)
C12—N1—C13122.56 (17)C16—C17—H17119.6
C12—N1—H1118.7C18—C17—H17119.6
C13—N1—H1118.7C8—C9—C10119.8 (2)
O4—N3—O3118.99 (18)C8—C9—H9120.1
O4—N3—C1121.52 (18)C10—C9—H9120.1
O3—N3—C1119.48 (17)C15—C14—C13120.2 (2)
C19—N2—H2A120.0C15—C14—H14119.9
C19—N2—H2B120.0C13—C14—H14119.9
H2A—N2—H2B120.0C14—C15—C16121.0 (2)
N1—C13—C14119.86 (18)C14—C15—H15119.5
N1—C13—C18120.37 (19)C16—C15—H15119.5
C14—C13—C18119.8 (2)C6—C5—C4119.6 (2)
N2—C19—C18120.2 (2)C6—C5—H5120.2
N2—C19—C7121.42 (19)C4—C5—H5120.2
C18—C19—C7118.35 (18)C3—C4—C5122.2 (2)
C13—C18—C17118.3 (2)C3—C4—H4118.9
C13—C18—C19118.46 (19)C5—C4—H4118.9
C17—C18—C19123.19 (19)C10—C11—C12120.0 (2)
N1—C12—C7120.83 (19)C10—C11—H11120.0
N1—C12—C11119.48 (18)C12—C11—H11120.0
C7—C12—C11119.7 (2)C9—C8—C7121.1 (2)
N3—C1—C6119.22 (18)C9—C8—H8119.4
N3—C1—C2119.85 (17)C7—C8—H8119.4
C6—C1—C2120.92 (18)C17—C16—C15119.9 (2)
C12—C7—C8118.5 (2)C17—C16—H16120.0
C12—C7—C19118.39 (19)C15—C16—H16120.0
C8—C7—C19122.96 (19)C4—C3—C2121.9 (2)
O1—C2—C3120.8 (2)C4—C3—H3119.0
O1—C2—C1123.67 (19)C2—C3—H3119.0
C3—C2—C1115.49 (19)C11—C10—C9120.9 (2)
O2—C6—C5117.70 (19)C11—C10—H10119.6
O2—C6—C1122.68 (19)C9—C10—H10119.6
C5—C6—C1119.6 (2)
(6NRES-33BP) top
Crystal data top
C26H21N5O4Z = 2
Mr = 467.48F(000) = 488
Triclinic, P1Dx = 1.391 Mg m3
a = 7.3217 (8) ÅMo Kα radiation, λ = 0.71073 Å
b = 11.6513 (13) ÅCell parameters from 10398 reflections
c = 13.9987 (16) Åθ = 3.1–27.6°
α = 105.915 (7)°µ = 0.10 mm1
β = 102.665 (7)°T = 150 K
γ = 91.242 (6)°Block, yellow
V = 1116.2 (2) Å30.20 × 0.20 × 0.20 mm
Data collection top
Rigaku Mercury375R (2x2 bin mode)
diffractometer
4075 reflections with I > 2σ(I)
Radiation source: Sealed TubeRint = 0.023
profile data from ω–scansθmax = 27.5°, θmin = 3.1°
Absorption correction: multi-scan
Jacobson, R. (1998) Private communication
h = 99
Tmin = 0.888, Tmax = 1.000k = 1515
11717 measured reflectionsl = 1818
5120 independent reflections
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.040H-atom parameters constrained
wR(F2) = 0.104 w = 1/[σ2(Fo2) + (0.0504P)2 + 0.2648P]
where P = (Fo2 + 2Fc2)/3
S = 1.05(Δ/σ)max < 0.001
5120 reflectionsΔρmax = 0.25 e Å3
318 parametersΔρmin = 0.23 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O20.62535 (13)0.01397 (8)0.37342 (7)0.0223 (2)
H20.6411700.0548600.3707260.033*
O10.93638 (13)0.34882 (8)0.41651 (7)0.0224 (2)
H11.0201570.3885300.3981650.034*
O40.51596 (14)0.30008 (10)0.32253 (8)0.0337 (3)
O30.58962 (15)0.22002 (11)0.48531 (8)0.0372 (3)
N20.65425 (16)0.19231 (10)0.32435 (9)0.0227 (3)
N10.62009 (15)0.23644 (10)0.40083 (8)0.0187 (2)
N30.77484 (17)0.01404 (11)0.07001 (9)0.0284 (3)
N40.15102 (16)0.48877 (10)0.33818 (8)0.0217 (2)
C70.65747 (19)0.31084 (12)0.36573 (10)0.0224 (3)
H70.6526920.3396920.4339270.027*
N50.26793 (17)0.47096 (11)0.05175 (9)0.0262 (3)
C20.95337 (18)0.24026 (11)0.40054 (9)0.0169 (3)
C50.95771 (19)0.01179 (12)0.37179 (9)0.0198 (3)
H50.9618420.0638360.3618270.024*
C80.66768 (19)0.39178 (12)0.31041 (10)0.0225 (3)
H80.6686430.4735140.3409600.027*
C250.2032 (2)0.37109 (13)0.12776 (10)0.0255 (3)
H250.2091810.3706820.1935310.031*
C60.78975 (18)0.06454 (12)0.37842 (9)0.0175 (3)
C31.11915 (18)0.18578 (12)0.39408 (10)0.0208 (3)
H31.2289180.2246850.3990550.025*
C170.16363 (19)0.38823 (13)0.36748 (10)0.0230 (3)
H170.1584150.3923560.4341120.028*
C220.18462 (18)0.37099 (12)0.06467 (9)0.0184 (3)
C230.11819 (19)0.26859 (13)0.01687 (10)0.0235 (3)
H230.0676160.2007790.0058050.028*
C180.18402 (19)0.27911 (12)0.30256 (10)0.0226 (3)
H180.1934010.2113120.3255950.027*
C200.17866 (17)0.37416 (12)0.17056 (9)0.0170 (3)
C120.68266 (18)0.17468 (12)0.05662 (10)0.0189 (3)
C140.60805 (19)0.22874 (13)0.01910 (10)0.0228 (3)
H140.5533230.3006520.0026370.027*
C10.79311 (17)0.17821 (11)0.39235 (9)0.0156 (3)
C210.15935 (18)0.48038 (12)0.24181 (10)0.0197 (3)
H210.1517360.5499020.2212420.024*
C100.67462 (17)0.22681 (12)0.16446 (10)0.0184 (3)
C190.19042 (18)0.27104 (12)0.20308 (10)0.0200 (3)
H190.2024430.1976840.1582890.024*
C160.6994 (2)0.06804 (13)0.14041 (11)0.0280 (3)
H160.7032880.0317770.2078850.034*
C110.66194 (18)0.15294 (12)0.22636 (10)0.0207 (3)
H110.6586100.0706710.1975190.025*
C260.25837 (19)0.46885 (12)0.04215 (10)0.0229 (3)
H260.3040920.5373770.0959480.027*
C41.11832 (18)0.07265 (13)0.38011 (9)0.0214 (3)
H41.2295860.0361730.3761620.026*
C150.6164 (2)0.17415 (14)0.11897 (11)0.0277 (3)
H150.5668570.2084590.1706660.033*
C90.67644 (18)0.34953 (12)0.20903 (10)0.0207 (3)
H90.6834890.4028170.1709330.025*
C240.1283 (2)0.26893 (13)0.11444 (10)0.0263 (3)
H240.0853670.2014930.1697660.032*
C130.7658 (2)0.06833 (12)0.02637 (11)0.0241 (3)
H130.8186200.0325350.0765180.029*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O20.0210 (5)0.0210 (5)0.0294 (5)0.0051 (4)0.0066 (4)0.0135 (4)
O10.0235 (5)0.0202 (5)0.0288 (5)0.0089 (4)0.0127 (4)0.0100 (4)
O40.0251 (5)0.0351 (6)0.0335 (6)0.0103 (5)0.0057 (5)0.0001 (5)
O30.0282 (6)0.0646 (8)0.0261 (5)0.0016 (5)0.0114 (4)0.0213 (5)
N20.0242 (6)0.0224 (6)0.0251 (6)0.0034 (5)0.0069 (5)0.0115 (5)
N10.0168 (5)0.0199 (6)0.0232 (6)0.0045 (4)0.0062 (4)0.0110 (5)
N30.0301 (7)0.0244 (7)0.0273 (6)0.0022 (5)0.0078 (5)0.0011 (5)
N40.0238 (6)0.0228 (6)0.0205 (6)0.0059 (5)0.0084 (5)0.0066 (5)
C70.0213 (7)0.0251 (7)0.0207 (6)0.0013 (6)0.0047 (5)0.0065 (6)
N50.0334 (7)0.0274 (7)0.0207 (6)0.0017 (5)0.0077 (5)0.0104 (5)
C20.0197 (6)0.0176 (6)0.0123 (6)0.0018 (5)0.0039 (5)0.0023 (5)
C50.0245 (7)0.0184 (7)0.0164 (6)0.0028 (5)0.0049 (5)0.0054 (5)
C80.0238 (7)0.0172 (7)0.0252 (7)0.0003 (5)0.0050 (5)0.0046 (5)
C250.0283 (7)0.0328 (8)0.0171 (6)0.0049 (6)0.0062 (6)0.0092 (6)
C60.0183 (6)0.0203 (7)0.0140 (6)0.0022 (5)0.0035 (5)0.0055 (5)
C30.0167 (6)0.0275 (7)0.0180 (6)0.0042 (5)0.0058 (5)0.0050 (5)
C170.0232 (7)0.0303 (8)0.0202 (6)0.0064 (6)0.0084 (5)0.0118 (6)
C220.0165 (6)0.0207 (7)0.0186 (6)0.0039 (5)0.0049 (5)0.0060 (5)
C230.0239 (7)0.0228 (7)0.0235 (7)0.0022 (6)0.0058 (5)0.0061 (6)
C180.0234 (7)0.0221 (7)0.0271 (7)0.0044 (5)0.0074 (6)0.0134 (6)
C200.0139 (6)0.0192 (7)0.0189 (6)0.0013 (5)0.0048 (5)0.0062 (5)
C120.0158 (6)0.0188 (7)0.0226 (6)0.0006 (5)0.0041 (5)0.0072 (5)
C140.0227 (7)0.0220 (7)0.0244 (7)0.0027 (5)0.0048 (5)0.0084 (6)
C10.0151 (6)0.0183 (6)0.0129 (6)0.0013 (5)0.0033 (5)0.0039 (5)
C210.0203 (6)0.0189 (7)0.0218 (6)0.0044 (5)0.0068 (5)0.0075 (5)
C100.0137 (6)0.0197 (7)0.0229 (7)0.0015 (5)0.0038 (5)0.0084 (5)
C190.0192 (6)0.0166 (7)0.0233 (7)0.0020 (5)0.0053 (5)0.0040 (5)
C160.0292 (8)0.0298 (8)0.0207 (7)0.0043 (6)0.0063 (6)0.0004 (6)
C110.0214 (7)0.0168 (7)0.0255 (7)0.0028 (5)0.0059 (5)0.0081 (5)
C260.0283 (7)0.0203 (7)0.0192 (6)0.0001 (6)0.0050 (5)0.0048 (5)
C40.0188 (6)0.0287 (7)0.0156 (6)0.0046 (5)0.0051 (5)0.0041 (5)
C150.0279 (7)0.0325 (8)0.0227 (7)0.0003 (6)0.0027 (6)0.0104 (6)
C90.0190 (6)0.0200 (7)0.0256 (7)0.0010 (5)0.0047 (5)0.0111 (5)
C240.0272 (7)0.0281 (8)0.0179 (6)0.0026 (6)0.0023 (6)0.0000 (6)
C130.0252 (7)0.0216 (7)0.0249 (7)0.0021 (6)0.0048 (6)0.0061 (6)
Geometric parameters (Å, º) top
O2—C61.3481 (15)C25—C241.375 (2)
O1—C21.3512 (15)C6—C11.3905 (18)
O4—N11.2231 (15)C3—C41.384 (2)
O3—N11.2159 (14)C17—C181.378 (2)
N2—C111.3361 (17)C22—C261.3914 (19)
N2—C71.3406 (18)C22—C231.3955 (19)
N1—C11.4669 (16)C22—C201.4829 (17)
N3—C161.3373 (19)C23—C241.3850 (19)
N3—C131.3408 (18)C18—C191.3811 (18)
N4—C211.3405 (16)C20—C211.3925 (18)
N4—C171.3419 (17)C20—C191.3949 (18)
C7—C81.3847 (19)C12—C131.3940 (19)
N5—C251.3367 (19)C12—C141.3949 (18)
N5—C261.3383 (17)C12—C101.4796 (18)
C2—C31.3895 (18)C14—C151.384 (2)
C2—C11.3913 (17)C10—C91.3929 (19)
C5—C41.3859 (19)C10—C111.3932 (18)
C5—C61.3954 (18)C16—C151.377 (2)
C8—C91.3851 (19)
C11—N2—C7117.82 (11)C21—C20—C19117.00 (12)
O3—N1—O4123.75 (12)C21—C20—C22121.34 (12)
O3—N1—C1118.21 (11)C19—C20—C22121.66 (12)
O4—N1—C1118.02 (10)C13—C12—C14117.02 (12)
C16—N3—C13116.48 (12)C13—C12—C10120.95 (12)
C21—N4—C17117.55 (11)C14—C12—C10122.03 (12)
N2—C7—C8122.26 (13)C15—C14—C12119.25 (13)
C25—N5—C26116.79 (12)C6—C1—C2123.66 (12)
O1—C2—C3124.80 (12)C6—C1—N1118.95 (11)
O1—C2—C1117.02 (11)C2—C1—N1117.38 (11)
C3—C2—C1118.17 (12)N4—C21—C20124.14 (12)
C4—C5—C6119.68 (12)C9—C10—C11116.65 (12)
C7—C8—C9119.20 (13)C9—C10—C12122.89 (12)
N5—C25—C24123.86 (12)C11—C10—C12120.45 (12)
O2—C6—C1117.43 (11)C18—C19—C20119.24 (12)
O2—C6—C5125.41 (12)N3—C16—C15123.93 (13)
C1—C6—C5117.15 (12)N2—C11—C10124.43 (12)
C4—C3—C2118.95 (12)N5—C26—C22124.39 (13)
N4—C17—C18122.47 (12)C3—C4—C5122.39 (12)
C26—C22—C23117.01 (12)C16—C15—C14118.77 (13)
C26—C22—C20121.78 (12)C8—C9—C10119.64 (12)
C23—C22—C20121.20 (12)C25—C24—C23118.59 (13)
C24—C23—C22119.35 (13)N3—C13—C12124.55 (13)
C17—C18—C19119.59 (12)
(7NRES-44BP) top
Crystal data top
C42H34N8O8Z = 1
Mr = 778.77F(000) = 406
Triclinic, P1Dx = 1.408 Mg m3
a = 7.4323 (10) ÅMo Kα radiation, λ = 0.71073 Å
b = 9.1138 (12) ÅCell parameters from 8552 reflections
c = 14.562 (2) Åθ = 3.0–27.5°
α = 106.397 (7)°µ = 0.10 mm1
β = 103.133 (7)°T = 150 K
γ = 90.486 (6)°Block, yellow
V = 918.7 (2) Å30.20 × 0.20 × 0.20 mm
Data collection top
Rigaku Mercury375R (2x2 bin mode)
diffractometer
3376 reflections with I > 2σ(I)
Radiation source: Sealed TubeRint = 0.024
profile data from ω–scansθmax = 27.5°, θmin = 3.0°
Absorption correction: multi-scan
Jacobson, R. (1998) Private communication
h = 99
Tmin = 0.829, Tmax = 1.000k = 1111
9526 measured reflectionsl = 1818
4200 independent reflections
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.045H-atom parameters constrained
wR(F2) = 0.142 w = 1/[σ2(Fo2) + (0.0807P)2 + 0.2379P]
where P = (Fo2 + 2Fc2)/3
S = 1.07(Δ/σ)max < 0.001
4200 reflectionsΔρmax = 0.33 e Å3
264 parametersΔρmin = 0.37 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O10.21704 (15)0.14715 (12)0.88284 (9)0.0252 (3)
H10.3199350.1924230.8970800.038*
O20.10204 (15)0.34219 (11)0.74466 (8)0.0248 (3)
H20.0968500.4272160.7070490.037*
O30.15821 (16)0.08161 (13)0.90132 (9)0.0295 (3)
N40.10142 (16)0.03893 (13)0.83987 (9)0.0186 (3)
O40.17775 (15)0.05119 (13)0.79823 (9)0.0284 (3)
C200.0598 (2)0.25839 (16)0.76464 (11)0.0194 (3)
C240.2264 (2)0.00238 (16)0.83693 (11)0.0198 (3)
C210.2204 (2)0.31727 (17)0.73899 (12)0.0246 (3)
H210.2203090.4206930.7057500.029*
N10.54938 (18)0.30714 (15)0.93048 (10)0.0253 (3)
C160.9057 (2)0.45992 (16)0.98543 (10)0.0199 (3)
C190.06763 (19)0.10135 (16)0.81344 (11)0.0180 (3)
C230.3858 (2)0.06496 (18)0.81172 (12)0.0249 (3)
H230.4949290.0029440.8271730.030*
C220.3799 (2)0.22061 (19)0.76339 (13)0.0272 (4)
H220.4864860.2613090.7468400.033*
C140.5828 (2)0.43088 (19)0.90304 (12)0.0284 (4)
H140.4843980.4658250.8648400.034*
C170.8703 (2)0.33113 (18)1.01360 (12)0.0254 (3)
H170.9659290.2928111.0514180.030*
C150.7546 (2)0.50992 (19)0.92796 (13)0.0277 (4)
H150.7698510.5954600.9068520.033*
C180.6935 (2)0.25988 (18)0.98557 (13)0.0282 (4)
H180.6735640.1745681.0060830.034*
N30.0849 (2)0.62517 (14)0.36843 (11)0.0289 (3)
C10.0862 (2)0.81472 (17)0.52020 (12)0.0256 (3)
H1A0.1111780.8403480.5885980.031*
C60.0181 (2)0.92136 (15)0.47266 (11)0.0208 (3)
C70.4756 (2)1.08148 (17)0.51344 (12)0.0233 (3)
N20.3854 (2)1.38947 (17)0.56473 (12)0.0370 (4)
C120.4143 (3)1.15596 (19)0.44372 (13)0.0343 (4)
H120.4011191.1049820.3772350.041*
C20.1174 (2)0.66986 (17)0.46629 (13)0.0277 (4)
H2A0.1633540.6003420.5001640.033*
C110.3720 (3)1.3080 (2)0.47285 (15)0.0383 (4)
H110.3312621.3553180.4238560.046*
C40.0213 (4)0.7274 (2)0.32252 (15)0.0535 (6)
H40.0014960.6987250.2541090.064*
C80.4930 (4)1.1663 (3)0.61003 (15)0.0623 (8)
H80.5356631.1228230.6608000.075*
C50.0132 (4)0.8747 (2)0.37083 (14)0.0517 (6)
H50.0572950.9421430.3349930.062*
C90.4463 (4)1.3175 (3)0.63100 (16)0.0680 (8)
H90.4590661.3719180.6968930.082*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0182 (6)0.0186 (5)0.0343 (6)0.0017 (4)0.0061 (5)0.0008 (4)
O20.0243 (6)0.0168 (5)0.0297 (6)0.0010 (4)0.0085 (5)0.0002 (4)
O30.0283 (6)0.0330 (6)0.0353 (7)0.0068 (5)0.0182 (5)0.0140 (5)
N40.0147 (6)0.0175 (6)0.0212 (6)0.0010 (5)0.0037 (5)0.0026 (5)
O40.0222 (6)0.0309 (6)0.0366 (7)0.0109 (5)0.0076 (5)0.0160 (5)
C200.0210 (8)0.0185 (7)0.0189 (7)0.0027 (6)0.0046 (6)0.0059 (5)
C240.0182 (7)0.0204 (7)0.0204 (7)0.0020 (6)0.0040 (6)0.0056 (6)
C210.0270 (8)0.0207 (7)0.0265 (8)0.0081 (6)0.0098 (7)0.0048 (6)
N10.0209 (7)0.0250 (6)0.0258 (7)0.0032 (5)0.0058 (6)0.0008 (5)
C160.0210 (8)0.0213 (7)0.0166 (7)0.0011 (6)0.0055 (6)0.0034 (6)
C190.0152 (7)0.0199 (7)0.0192 (7)0.0039 (5)0.0051 (6)0.0055 (5)
C230.0142 (7)0.0298 (8)0.0302 (8)0.0011 (6)0.0065 (6)0.0072 (6)
C220.0217 (8)0.0315 (8)0.0316 (8)0.0111 (6)0.0117 (7)0.0096 (7)
C140.0204 (8)0.0340 (8)0.0278 (8)0.0000 (6)0.0000 (7)0.0093 (7)
C170.0218 (8)0.0265 (8)0.0283 (8)0.0001 (6)0.0028 (7)0.0113 (6)
C150.0242 (8)0.0307 (8)0.0298 (8)0.0007 (6)0.0016 (7)0.0152 (7)
C180.0274 (9)0.0246 (8)0.0332 (9)0.0019 (6)0.0068 (7)0.0098 (7)
N30.0347 (8)0.0171 (6)0.0330 (8)0.0028 (5)0.0102 (6)0.0026 (5)
C10.0317 (9)0.0211 (7)0.0230 (8)0.0063 (6)0.0041 (7)0.0068 (6)
C60.0237 (8)0.0157 (7)0.0233 (7)0.0025 (6)0.0070 (6)0.0052 (6)
C70.0166 (7)0.0260 (8)0.0279 (8)0.0031 (6)0.0061 (6)0.0080 (6)
N20.0380 (9)0.0292 (7)0.0429 (9)0.0115 (6)0.0102 (7)0.0084 (7)
C120.0462 (11)0.0276 (8)0.0268 (9)0.0054 (8)0.0052 (8)0.0071 (7)
C20.0312 (9)0.0190 (7)0.0331 (9)0.0058 (6)0.0071 (7)0.0085 (6)
C110.0476 (11)0.0292 (9)0.0384 (10)0.0101 (8)0.0056 (9)0.0140 (8)
C40.105 (2)0.0294 (9)0.0247 (9)0.0249 (11)0.0170 (11)0.0042 (8)
C80.120 (2)0.0444 (12)0.0273 (10)0.0459 (14)0.0207 (12)0.0142 (9)
C50.105 (2)0.0269 (9)0.0246 (9)0.0272 (11)0.0142 (11)0.0094 (7)
C90.125 (2)0.0471 (13)0.0298 (11)0.0469 (15)0.0198 (13)0.0059 (9)
Geometric parameters (Å, º) top
O1—C241.3482 (17)C14—C151.381 (2)
O2—C201.3473 (18)C17—C181.381 (2)
O3—N41.2229 (17)N3—C41.325 (2)
N4—O41.2234 (16)N3—C21.330 (2)
N4—C191.4692 (17)C1—C61.382 (2)
C20—C211.397 (2)C1—C21.384 (2)
C20—C191.4009 (19)C6—C51.385 (2)
C24—C191.396 (2)C6—C6ii1.490 (3)
C24—C231.398 (2)C7—C121.372 (2)
C21—C221.386 (2)C7—C81.376 (2)
N1—C141.337 (2)C7—C7iii1.495 (3)
N1—C181.337 (2)N2—C111.315 (2)
C16—C171.390 (2)N2—C91.315 (3)
C16—C151.403 (2)C12—C111.391 (2)
C16—C16i1.488 (3)C4—C51.384 (2)
C23—C221.390 (2)C8—C91.390 (3)
O3—N4—O4124.08 (12)C18—C17—C16120.15 (15)
O3—N4—C19117.95 (12)C14—C15—C16119.34 (15)
O4—N4—C19117.96 (12)N1—C18—C17123.44 (15)
O2—C20—C21124.38 (13)C4—N3—C2116.85 (14)
O2—C20—C19117.99 (12)C6—C1—C2120.17 (15)
C21—C20—C19117.63 (13)C1—C6—C5116.28 (14)
O1—C24—C19118.12 (12)C1—C6—C6ii122.20 (17)
O1—C24—C23124.08 (14)C5—C6—C6ii121.52 (17)
C19—C24—C23117.80 (13)C12—C7—C8116.15 (15)
C22—C21—C20119.59 (14)C12—C7—C7iii122.13 (18)
C14—N1—C18116.63 (14)C8—C7—C7iii121.71 (19)
C17—C16—C15116.45 (14)C11—N2—C9115.06 (15)
C17—C16—C16i121.67 (17)C7—C12—C11119.76 (16)
C15—C16—C16i121.88 (17)N3—C2—C1123.24 (15)
C24—C19—C20123.30 (13)N2—C11—C12124.66 (17)
C24—C19—N4118.95 (12)N3—C4—C5123.56 (17)
C20—C19—N4117.74 (12)C7—C8—C9119.39 (19)
C22—C23—C24119.42 (14)C4—C5—C6119.90 (17)
C21—C22—C23122.24 (14)N2—C9—C8124.97 (19)
N1—C14—C15123.98 (16)
Symmetry codes: (i) x+2, y+1, z+2; (ii) x, y+2, z+1; (iii) x+1, y+2, z+1.
(8NRES-DPE-I) top
Crystal data top
C18H17N3O4F(000) = 712
Mr = 339.34Dx = 1.337 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71075 Å
a = 17.802 (3) ÅCell parameters from 13038 reflections
b = 7.5355 (11) Åθ = 3.1–27.7°
c = 12.5671 (19) ŵ = 0.10 mm1
β = 91.187 (6)°T = 150 K
V = 1685.5 (4) Å3Block, yellow
Z = 40.20 × 0.20 × 0.20 mm
Data collection top
Rigaku Mercury375R (2x2 bin mode)
diffractometer
2673 reflections with I > 2σ(I)
Radiation source: Sealed TubeRint = 0.074
profile data from ω–scansθmax = 27.5°, θmin = 3.2°
Absorption correction: multi-scan
Jacobson, R. (1998) Private communication
h = 2323
Tmin = 0.752, Tmax = 1.000k = 99
16334 measured reflectionsl = 1616
3859 independent reflections
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.074H-atom parameters constrained
wR(F2) = 0.199 w = 1/[σ2(Fo2) + (0.0721P)2 + 1.9128P]
where P = (Fo2 + 2Fc2)/3
S = 1.09(Δ/σ)max < 0.001
3859 reflectionsΔρmax = 0.51 e Å3
228 parametersΔρmin = 0.40 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O20.83534 (12)0.1880 (3)0.77910 (16)0.0330 (5)
H20.8601900.2774020.7919150.050*
O10.66069 (13)0.0619 (3)0.53742 (17)0.0393 (6)
H10.6358830.0416370.4830710.059*
O40.70962 (13)0.0781 (3)0.80485 (17)0.0406 (6)
O30.77914 (14)0.2170 (3)0.6928 (2)0.0478 (6)
N30.74516 (14)0.0852 (3)0.72221 (19)0.0287 (5)
N20.90735 (15)0.4803 (3)0.8462 (2)0.0349 (6)
N10.58340 (14)0.0297 (4)0.3534 (2)0.0334 (6)
C60.79470 (15)0.2120 (4)0.6882 (2)0.0261 (6)
C10.74767 (15)0.0740 (4)0.6550 (2)0.0253 (6)
C20.70453 (16)0.0795 (4)0.5608 (2)0.0284 (6)
C110.96895 (17)0.7614 (4)0.9644 (2)0.0303 (6)
C70.98037 (18)0.5232 (4)0.8398 (2)0.0326 (7)
H71.0105900.4568600.7953060.039*
C50.79792 (16)0.3626 (4)0.6242 (2)0.0308 (6)
H50.8276600.4585040.6448980.037*
C101.01236 (16)0.6613 (4)0.8965 (2)0.0312 (6)
H101.0630610.6873260.8892390.037*
C30.71006 (16)0.2306 (4)0.4967 (2)0.0309 (6)
H30.6829190.2383970.4328110.037*
C40.75657 (17)0.3687 (4)0.5297 (2)0.0322 (7)
H40.7601190.4688620.4868110.039*
C130.62871 (18)0.0466 (4)0.2708 (2)0.0348 (7)
H130.6803310.0461440.2837390.042*
C90.89352 (18)0.7174 (4)0.9702 (3)0.0376 (7)
H90.8620060.7812711.0141960.045*
C121.00254 (19)0.9110 (4)1.0297 (2)0.0359 (7)
H12A1.0548090.8845291.0463060.043*
H12B0.9762150.9204431.0962930.043*
C140.50914 (18)0.0266 (4)0.3326 (3)0.0375 (7)
H140.4765690.0149940.3891250.045*
C170.52625 (19)0.0622 (4)0.1450 (3)0.0381 (8)
C80.86558 (18)0.5780 (5)0.9100 (3)0.0405 (8)
H80.8147540.5510330.9143740.049*
C150.60292 (18)0.0646 (5)0.1674 (3)0.0394 (8)
H150.6367890.0782550.1126610.047*
C160.47917 (18)0.0401 (4)0.2306 (3)0.0395 (8)
H160.4274270.0343860.2193800.047*
C180.4975 (3)0.0832 (5)0.0314 (3)0.0561 (11)
H18A0.5263680.1750110.0032180.067*
H18B0.4455310.1217590.0321960.067*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O20.0394 (12)0.0294 (11)0.0299 (11)0.0083 (9)0.0114 (9)0.0000 (9)
O10.0474 (13)0.0394 (13)0.0305 (11)0.0143 (10)0.0137 (10)0.0019 (10)
O40.0520 (13)0.0449 (14)0.0252 (11)0.0102 (11)0.0048 (10)0.0008 (10)
O30.0630 (16)0.0295 (12)0.0512 (15)0.0079 (11)0.0096 (12)0.0048 (11)
N30.0334 (12)0.0273 (13)0.0252 (12)0.0064 (10)0.0044 (10)0.0007 (10)
N20.0452 (15)0.0277 (13)0.0314 (13)0.0085 (11)0.0088 (11)0.0007 (11)
N10.0376 (14)0.0350 (14)0.0273 (13)0.0009 (11)0.0067 (10)0.0039 (11)
C60.0276 (13)0.0268 (14)0.0239 (13)0.0002 (11)0.0008 (11)0.0030 (11)
C10.0282 (13)0.0237 (14)0.0240 (13)0.0003 (11)0.0001 (11)0.0007 (11)
C20.0304 (14)0.0294 (15)0.0253 (14)0.0015 (12)0.0002 (11)0.0045 (12)
C110.0404 (16)0.0240 (14)0.0261 (14)0.0033 (12)0.0060 (12)0.0022 (11)
C70.0417 (17)0.0310 (16)0.0249 (14)0.0026 (13)0.0007 (12)0.0003 (12)
C50.0325 (15)0.0250 (14)0.0348 (16)0.0026 (12)0.0022 (12)0.0007 (12)
C100.0300 (14)0.0312 (15)0.0323 (15)0.0069 (12)0.0008 (12)0.0026 (12)
C30.0317 (14)0.0361 (16)0.0246 (14)0.0053 (13)0.0053 (11)0.0008 (12)
C40.0381 (16)0.0283 (15)0.0304 (15)0.0046 (13)0.0009 (12)0.0040 (12)
C130.0341 (15)0.0346 (17)0.0354 (17)0.0026 (13)0.0076 (13)0.0004 (13)
C90.0370 (16)0.0350 (17)0.0409 (18)0.0015 (13)0.0016 (14)0.0067 (14)
C120.0493 (18)0.0264 (16)0.0317 (16)0.0069 (14)0.0089 (14)0.0009 (13)
C140.0386 (17)0.0398 (18)0.0341 (16)0.0004 (14)0.0025 (13)0.0050 (14)
C170.0493 (18)0.0334 (17)0.0312 (16)0.0114 (14)0.0127 (14)0.0065 (13)
C80.0321 (16)0.0434 (19)0.0460 (19)0.0077 (14)0.0015 (14)0.0006 (15)
C150.0427 (17)0.0451 (19)0.0304 (16)0.0050 (15)0.0000 (13)0.0001 (14)
C160.0340 (16)0.0370 (17)0.0470 (19)0.0024 (14)0.0148 (14)0.0033 (15)
C180.075 (3)0.053 (2)0.039 (2)0.024 (2)0.0249 (19)0.0108 (17)
Geometric parameters (Å, º) top
O2—C61.352 (3)C10—H100.9300
O2—H20.8200C3—C41.388 (4)
O1—C21.350 (4)C3—H30.9300
O1—H10.8200C4—H40.9300
O4—N31.228 (3)C13—C151.376 (4)
O3—N31.224 (3)C13—H130.9300
N3—C11.469 (4)C9—C81.382 (5)
N2—C81.328 (4)C9—H90.9300
N2—C71.343 (4)C12—C12i1.537 (6)
N1—C131.334 (4)C12—H12A0.9700
N1—C141.342 (4)C12—H12B0.9700
C6—C51.392 (4)C14—C161.382 (5)
C6—C11.394 (4)C14—H140.9300
C1—C21.398 (4)C17—C161.388 (5)
C2—C31.400 (4)C17—C151.388 (5)
C11—C101.386 (4)C17—C181.514 (4)
C11—C91.386 (4)C8—H80.9300
C11—C121.511 (4)C15—H150.9300
C7—C101.378 (4)C16—H160.9300
C7—H70.9300C18—C18ii1.486 (7)
C5—C41.386 (4)C18—H18A0.9700
C5—H50.9300C18—H18B0.9700
C6—O2—H2109.5N1—C13—C15123.3 (3)
C2—O1—H1109.5N1—C13—H13118.3
O3—N3—O4123.9 (3)C15—C13—H13118.3
O3—N3—C1117.9 (2)C8—C9—C11119.4 (3)
O4—N3—C1118.2 (2)C8—C9—H9120.3
C8—N2—C7117.2 (3)C11—C9—H9120.3
C13—N1—C14117.3 (3)C11—C12—C12i111.6 (3)
O2—C6—C5124.7 (2)C11—C12—H12A109.3
O2—C6—C1117.5 (2)C12i—C12—H12A109.3
C5—C6—C1117.8 (2)C11—C12—H12B109.3
C6—C1—C2123.2 (3)C12i—C12—H12B109.3
C6—C1—N3117.5 (2)H12A—C12—H12B108.0
C2—C1—N3119.2 (2)N1—C14—C16122.6 (3)
O1—C2—C1117.8 (3)N1—C14—H14118.7
O1—C2—C3124.3 (3)C16—C14—H14118.7
C1—C2—C3117.9 (3)C16—C17—C15116.8 (3)
C10—C11—C9117.1 (3)C16—C17—C18123.1 (3)
C10—C11—C12121.4 (3)C15—C17—C18120.1 (3)
C9—C11—C12121.5 (3)N2—C8—C9123.6 (3)
N2—C7—C10122.8 (3)N2—C8—H8118.2
N2—C7—H7118.6C9—C8—H8118.2
C10—C7—H7118.6C13—C15—C17119.9 (3)
C4—C5—C6119.7 (3)C13—C15—H15120.1
C4—C5—H5120.2C17—C15—H15120.1
C6—C5—H5120.2C14—C16—C17120.0 (3)
C7—C10—C11120.0 (3)C14—C16—H16120.0
C7—C10—H10120.0C17—C16—H16120.0
C11—C10—H10120.0C18ii—C18—C17112.9 (4)
C4—C3—C2119.1 (3)C18ii—C18—H18A109.0
C4—C3—H3120.4C17—C18—H18A109.0
C2—C3—H3120.4C18ii—C18—H18B109.0
C5—C4—C3122.3 (3)C17—C18—H18B109.0
C5—C4—H4118.9H18A—C18—H18B107.8
C3—C4—H4118.9
Symmetry codes: (i) x+2, y+2, z+2; (ii) x+1, y, z.
(9NRES-DPE-II) top
Crystal data top
C18H15N3O4F(000) = 704
Mr = 337.33Dx = 1.385 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71075 Å
a = 17.9122 (13) ÅCell parameters from 13763 reflections
b = 7.4259 (5) Åθ = 3.2–27.6°
c = 12.1765 (8) ŵ = 0.10 mm1
β = 92.337 (7)°T = 150 K
V = 1618.30 (19) Å3Block, yellow
Z = 40.20 × 0.20 × 0.20 mm
Data collection top
Rigaku Mercury375R (2x2 bin mode)
diffractometer
2933 reflections with I > 2σ(I)
Radiation source: sealed tubeRint = 0.040
profile data from ω–scansθmax = 27.5°, θmin = 3.2°
Absorption correction: multi-scan
Jacobson, R. (1998) Private communication
h = 2323
Tmin = 0.818, Tmax = 1.000k = 99
16284 measured reflectionsl = 1515
3707 independent reflections
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.043H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.108 w = 1/[σ2(Fo2) + (0.0487P)2 + 0.5466P]
where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max = 0.001
3707 reflectionsΔρmax = 0.25 e Å3
236 parametersΔρmin = 0.26 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O0010.84598 (6)0.14176 (14)0.79383 (8)0.0263 (3)
H0010.8705660.2327850.8074360.039*
O0020.65923 (6)0.10196 (14)0.55885 (8)0.0265 (3)
H0020.6339430.0837700.5022800.040*
O0030.71992 (6)0.12122 (15)0.82946 (8)0.0322 (3)
O0040.78070 (7)0.26443 (15)0.70767 (10)0.0378 (3)
N30.75081 (7)0.12920 (16)0.74151 (10)0.0225 (3)
N10.91348 (7)0.44416 (17)0.86049 (10)0.0249 (3)
N20.57684 (7)0.05617 (18)0.37171 (10)0.0257 (3)
C20.70284 (8)0.04221 (19)0.58097 (11)0.0200 (3)
C10.75126 (8)0.03328 (18)0.67354 (11)0.0192 (3)
C60.79998 (8)0.17128 (19)0.70537 (11)0.0201 (3)
C110.94985 (8)0.7850 (2)0.94646 (11)0.0225 (3)
C30.70334 (8)0.1996 (2)0.51904 (11)0.0235 (3)
H30.6718660.2110370.4567790.028*
C170.51532 (8)0.02266 (19)0.15729 (11)0.0219 (3)
C50.79905 (8)0.32735 (19)0.64239 (12)0.0227 (3)
H50.8304230.4230210.6616770.027*
C40.75089 (8)0.3393 (2)0.55045 (12)0.0242 (3)
H40.7505150.4441010.5086610.029*
C180.48157 (8)0.0022 (2)0.04614 (12)0.0249 (3)
C130.61992 (8)0.0417 (2)0.28507 (12)0.0247 (3)
H130.6714870.0417380.2976320.030*
C150.59230 (8)0.0269 (2)0.17836 (12)0.0251 (3)
H150.6247530.0198160.1208070.030*
C101.00089 (8)0.6850 (2)0.88797 (12)0.0250 (3)
H101.0482930.7307470.8766810.030*
C160.47049 (8)0.0365 (2)0.24730 (12)0.0265 (3)
H160.4187530.0334000.2373710.032*
C70.98076 (8)0.5181 (2)0.84698 (12)0.0257 (3)
H71.0155240.4536500.8080900.031*
C90.88026 (8)0.7079 (2)0.96030 (13)0.0270 (3)
H90.8442270.7691460.9985780.032*
C120.96634 (9)0.9640 (2)0.99265 (12)0.0251 (3)
C80.86502 (8)0.5400 (2)0.91682 (13)0.0280 (3)
H80.8181620.4905180.9273780.034*
C140.50289 (9)0.0549 (2)0.35165 (12)0.0285 (3)
H140.4718520.0669200.4105970.034*
H120.9231 (10)1.034 (3)1.0122 (14)0.036 (5)*
H180.4281 (10)0.008 (2)0.0447 (13)0.030 (4)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O0010.0305 (6)0.0203 (5)0.0273 (5)0.0064 (4)0.0105 (4)0.0001 (4)
O0020.0302 (6)0.0258 (6)0.0227 (5)0.0062 (5)0.0090 (4)0.0008 (4)
O0030.0429 (7)0.0338 (6)0.0201 (5)0.0103 (5)0.0030 (5)0.0014 (5)
O0040.0538 (8)0.0202 (6)0.0397 (7)0.0082 (5)0.0047 (6)0.0019 (5)
N30.0263 (6)0.0192 (6)0.0215 (6)0.0042 (5)0.0048 (5)0.0001 (5)
N10.0260 (6)0.0223 (6)0.0260 (6)0.0038 (5)0.0039 (5)0.0015 (5)
N20.0263 (7)0.0298 (7)0.0206 (6)0.0016 (5)0.0028 (5)0.0027 (5)
C20.0195 (7)0.0214 (7)0.0192 (7)0.0004 (6)0.0012 (5)0.0033 (6)
C10.0219 (7)0.0168 (7)0.0188 (7)0.0007 (6)0.0017 (5)0.0003 (5)
C60.0205 (7)0.0197 (7)0.0201 (7)0.0018 (6)0.0000 (5)0.0031 (5)
C110.0245 (7)0.0218 (7)0.0209 (7)0.0030 (6)0.0024 (6)0.0006 (6)
C30.0247 (7)0.0259 (8)0.0196 (7)0.0049 (6)0.0015 (6)0.0012 (6)
C170.0240 (7)0.0222 (7)0.0192 (7)0.0001 (6)0.0014 (6)0.0018 (6)
C50.0228 (7)0.0172 (7)0.0284 (8)0.0009 (6)0.0027 (6)0.0024 (6)
C40.0266 (8)0.0181 (7)0.0280 (8)0.0044 (6)0.0033 (6)0.0049 (6)
C180.0220 (7)0.0306 (8)0.0220 (7)0.0005 (6)0.0019 (6)0.0006 (6)
C130.0198 (7)0.0276 (8)0.0265 (7)0.0033 (6)0.0030 (6)0.0026 (6)
C150.0230 (7)0.0303 (8)0.0221 (7)0.0008 (6)0.0021 (6)0.0002 (6)
C100.0209 (7)0.0284 (8)0.0258 (7)0.0067 (6)0.0023 (6)0.0034 (6)
C160.0200 (7)0.0363 (9)0.0231 (7)0.0008 (6)0.0006 (6)0.0028 (6)
C70.0243 (7)0.0260 (8)0.0269 (8)0.0008 (6)0.0002 (6)0.0057 (6)
C90.0223 (7)0.0273 (8)0.0315 (8)0.0006 (6)0.0021 (6)0.0056 (7)
C120.0253 (7)0.0239 (8)0.0260 (7)0.0009 (6)0.0013 (6)0.0037 (6)
C80.0213 (7)0.0299 (8)0.0329 (8)0.0073 (6)0.0002 (6)0.0006 (7)
C140.0251 (8)0.0389 (9)0.0215 (7)0.0007 (7)0.0023 (6)0.0023 (7)
Geometric parameters (Å, º) top
O001—C61.3472 (16)C17—C151.393 (2)
O001—H0010.8200C17—C181.468 (2)
O002—C21.3460 (17)C5—C41.388 (2)
O002—H0020.8200C5—H50.9300
O003—N31.2267 (16)C4—H40.9300
O004—N31.2178 (16)C18—C18i1.327 (3)
N3—C11.4634 (18)C18—H180.960 (17)
N1—C81.334 (2)C13—C151.376 (2)
N1—C71.3404 (19)C13—H130.9300
N2—C131.3366 (19)C15—H150.9300
N2—C141.3370 (19)C10—C71.379 (2)
C2—C31.391 (2)C10—H100.9300
C2—C11.3954 (19)C16—C141.382 (2)
C1—C61.391 (2)C16—H160.9300
C6—C51.389 (2)C7—H70.9300
C11—C91.388 (2)C9—C81.378 (2)
C11—C101.396 (2)C9—H90.9300
C11—C121.469 (2)C12—C12ii1.325 (3)
C3—C41.386 (2)C12—H120.971 (18)
C3—H30.9300C8—H80.9300
C17—C161.389 (2)C14—H140.9300
C6—O001—H001109.5C18i—C18—C17125.67 (18)
C2—O002—H002109.5C18i—C18—H18120.9 (10)
O004—N3—O003123.74 (13)C17—C18—H18113.5 (10)
O004—N3—C1118.42 (12)N2—C13—C15123.70 (13)
O003—N3—C1117.84 (12)N2—C13—H13118.1
C8—N1—C7116.86 (13)C15—C13—H13118.1
C13—N2—C14117.05 (13)C13—C15—C17119.41 (14)
O002—C2—C3125.18 (12)C13—C15—H15120.3
O002—C2—C1117.41 (12)C17—C15—H15120.3
C3—C2—C1117.41 (13)C7—C10—C11119.74 (14)
C6—C1—C2123.53 (13)C7—C10—H10120.1
C6—C1—N3117.89 (12)C11—C10—H10120.1
C2—C1—N3118.58 (12)C14—C16—C17119.89 (14)
O001—C6—C5124.76 (13)C14—C16—H16120.1
O001—C6—C1117.34 (13)C17—C16—H16120.1
C5—C6—C1117.88 (13)N1—C7—C10123.15 (14)
C9—C11—C10116.92 (13)N1—C7—H7118.4
C9—C11—C12119.61 (14)C10—C7—H7118.4
C10—C11—C12123.47 (13)C8—C9—C11119.42 (14)
C4—C3—C2119.77 (13)C8—C9—H9120.3
C4—C3—H3120.1C11—C9—H9120.3
C2—C3—H3120.1C12ii—C12—C11125.78 (19)
C16—C17—C15116.94 (13)C12ii—C12—H12118.8 (11)
C16—C17—C18120.38 (13)C11—C12—H12115.4 (11)
C15—C17—C18122.68 (13)N1—C8—C9123.90 (14)
C4—C5—C6119.43 (13)N1—C8—H8118.0
C4—C5—H5120.3C9—C8—H8118.0
C6—C5—H5120.3N2—C14—C16122.99 (14)
C3—C4—C5121.98 (13)N2—C14—H14118.5
C3—C4—H4119.0C16—C14—H14118.5
C5—C4—H4119.0
Symmetry codes: (i) x+1, y, z; (ii) x+2, y+2, z+2.
(10NRES-44AZO) top
Crystal data top
C16H13N5O4F(000) = 704
Mr = 339.31Dx = 1.422 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71075 Å
a = 18.213 (3) ÅCell parameters from 12104 reflections
b = 7.2967 (13) Åθ = 3.0–27.6°
c = 11.940 (2) ŵ = 0.11 mm1
β = 92.967 (7)°T = 150 K
V = 1584.7 (5) Å3Block, red
Z = 40.20 × 0.20 × 0.20 mm
Data collection top
Rigaku Mercury375R (2x2 bin mode)
diffractometer
2782 reflections with I > 2σ(I)
Radiation source: sealed tubeRint = 0.054
profile data from ω–scansθmax = 27.5°, θmin = 3.0°
Absorption correction: multi-scan
Jacobson, R. (1998) Private communication
h = 2323
Tmin = 0.686, Tmax = 1.000k = 99
14469 measured reflectionsl = 1515
3639 independent reflections
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.058H-atom parameters constrained
wR(F2) = 0.149 w = 1/[σ2(Fo2) + (0.0606P)2 + 1.0262P]
where P = (Fo2 + 2Fc2)/3
S = 1.04(Δ/σ)max < 0.001
3639 reflectionsΔρmax = 0.69 e Å3
228 parametersΔρmin = 0.27 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O10.14931 (8)0.1420 (2)0.20812 (12)0.0332 (4)
H10.1258780.2356810.1932800.050*
O20.34443 (8)0.0912 (2)0.43735 (12)0.0355 (4)
H20.3660960.0781450.4987500.053*
O30.28655 (10)0.1186 (2)0.17188 (13)0.0467 (4)
N50.24990 (10)0.1257 (2)0.25486 (14)0.0315 (4)
O40.21592 (11)0.2609 (2)0.28178 (16)0.0527 (5)
N20.08673 (9)0.4601 (2)0.13670 (15)0.0308 (4)
N10.42295 (10)0.0529 (2)0.63618 (14)0.0327 (4)
N30.51978 (10)0.0326 (3)0.96381 (14)0.0336 (4)
N40.02702 (9)0.9600 (2)0.01889 (15)0.0328 (4)
C20.19633 (11)0.1729 (3)0.29705 (16)0.0262 (4)
C10.24772 (11)0.0378 (3)0.32621 (16)0.0260 (4)
C60.29771 (10)0.0504 (3)0.41804 (16)0.0270 (4)
C150.48363 (11)0.0370 (3)0.85373 (17)0.0297 (4)
C160.40835 (12)0.0288 (3)0.83389 (18)0.0321 (5)
H160.3771590.0186480.8928380.039*
C50.29578 (11)0.2091 (3)0.48352 (17)0.0301 (4)
H50.3282520.2228380.5456500.036*
C110.04509 (11)0.7909 (3)0.03891 (17)0.0296 (4)
C30.19550 (11)0.3302 (3)0.36400 (18)0.0301 (4)
H30.1619040.4235010.3473870.036*
C40.24534 (11)0.3454 (3)0.45548 (18)0.0322 (5)
H40.2448180.4507090.4993260.039*
C120.38071 (12)0.0361 (3)0.72449 (18)0.0332 (5)
H120.3300400.0290030.7110100.040*
C90.00082 (11)0.7028 (3)0.10984 (18)0.0318 (5)
H90.0461030.7530170.1254210.038*
C140.52882 (12)0.0556 (3)0.76363 (18)0.0338 (5)
H140.5796330.0630690.7750310.041*
C130.49569 (12)0.0625 (3)0.65663 (18)0.0351 (5)
H130.5255010.0744990.5961270.042*
C80.02203 (12)0.5383 (3)0.15724 (18)0.0338 (5)
H80.0087300.4791780.2054520.041*
C70.13056 (12)0.5487 (3)0.0683 (2)0.0354 (5)
H70.1758480.4968900.0543740.042*
C100.11191 (12)0.7128 (3)0.01741 (19)0.0365 (5)
H100.1436200.7696740.0303300.044*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0379 (8)0.0255 (7)0.0349 (8)0.0070 (6)0.0103 (6)0.0001 (6)
O20.0384 (8)0.0384 (9)0.0288 (8)0.0107 (7)0.0082 (6)0.0016 (6)
O30.0650 (11)0.0457 (10)0.0299 (9)0.0174 (9)0.0089 (8)0.0015 (7)
N50.0379 (10)0.0297 (9)0.0262 (9)0.0067 (8)0.0052 (7)0.0008 (7)
O40.0689 (12)0.0306 (9)0.0596 (12)0.0140 (9)0.0130 (9)0.0109 (8)
N20.0340 (9)0.0245 (9)0.0333 (9)0.0033 (7)0.0051 (7)0.0002 (7)
N10.0351 (9)0.0336 (10)0.0287 (9)0.0029 (8)0.0038 (7)0.0030 (7)
N30.0356 (10)0.0373 (10)0.0276 (9)0.0043 (8)0.0021 (7)0.0007 (7)
N40.0325 (9)0.0270 (9)0.0388 (10)0.0059 (7)0.0015 (7)0.0018 (7)
C20.0286 (10)0.0233 (10)0.0267 (10)0.0019 (8)0.0001 (7)0.0028 (7)
C10.0295 (10)0.0238 (10)0.0246 (10)0.0007 (8)0.0004 (7)0.0009 (7)
C60.0269 (10)0.0297 (11)0.0244 (10)0.0013 (8)0.0014 (7)0.0015 (8)
C150.0343 (11)0.0272 (10)0.0271 (10)0.0006 (9)0.0018 (8)0.0022 (8)
C160.0342 (11)0.0307 (11)0.0317 (11)0.0016 (9)0.0035 (8)0.0012 (8)
C50.0312 (10)0.0311 (11)0.0277 (10)0.0051 (9)0.0024 (8)0.0005 (8)
C110.0338 (11)0.0217 (10)0.0328 (11)0.0024 (8)0.0031 (8)0.0020 (8)
C30.0317 (10)0.0208 (10)0.0376 (11)0.0005 (8)0.0005 (8)0.0003 (8)
C40.0364 (11)0.0251 (10)0.0352 (11)0.0061 (9)0.0029 (8)0.0055 (8)
C120.0302 (10)0.0333 (12)0.0358 (12)0.0045 (9)0.0021 (8)0.0027 (9)
C90.0309 (10)0.0285 (11)0.0358 (11)0.0065 (9)0.0008 (8)0.0003 (8)
C140.0310 (10)0.0396 (13)0.0304 (11)0.0031 (9)0.0005 (8)0.0015 (9)
C130.0363 (11)0.0420 (13)0.0270 (11)0.0001 (10)0.0020 (8)0.0026 (9)
C80.0349 (11)0.0321 (11)0.0345 (11)0.0046 (9)0.0019 (8)0.0062 (9)
C70.0286 (10)0.0309 (12)0.0467 (13)0.0070 (9)0.0023 (9)0.0018 (9)
C100.0342 (11)0.0324 (11)0.0431 (13)0.0019 (9)0.0053 (9)0.0044 (9)
Geometric parameters (Å, º) top
O1—C21.348 (2)C15—C141.395 (3)
O1—H10.8200C16—C121.376 (3)
O2—C61.351 (2)C16—H160.9300
O2—H20.8200C5—C41.384 (3)
O3—N51.224 (2)C5—H50.9300
N5—O41.216 (2)C11—C91.379 (3)
N5—C11.468 (3)C11—C101.380 (3)
N2—C71.338 (3)C3—C41.388 (3)
N2—C81.343 (3)C3—H30.9300
N1—C131.337 (3)C4—H40.9300
N1—C121.343 (3)C12—H120.9300
N3—N3i1.248 (3)C9—C81.382 (3)
N3—C151.440 (3)C9—H90.9300
N4—N4ii1.249 (3)C14—C131.385 (3)
N4—C111.444 (3)C14—H140.9300
C2—C11.391 (3)C13—H130.9300
C2—C31.399 (3)C8—H80.9300
C1—C61.392 (3)C7—C101.377 (3)
C6—C51.398 (3)C7—H70.9300
C15—C161.381 (3)C10—H100.9300
C2—O1—H1109.5C10—C11—N4116.45 (19)
C6—O2—H2109.5C4—C3—C2119.30 (19)
O4—N5—O3123.70 (19)C4—C3—H3120.4
O4—N5—C1118.44 (17)C2—C3—H3120.4
O3—N5—C1117.86 (18)C5—C4—C3122.12 (19)
C7—N2—C8117.60 (18)C5—C4—H4118.9
C13—N1—C12117.66 (18)C3—C4—H4118.9
N3i—N3—C15112.8 (2)N1—C12—C16123.55 (19)
N4ii—N4—C11113.0 (2)N1—C12—H12118.2
O1—C2—C1118.06 (17)C16—C12—H12118.2
O1—C2—C3124.17 (18)C11—C9—C8118.47 (19)
C1—C2—C3117.74 (18)C11—C9—H9120.8
C2—C1—C6123.68 (18)C8—C9—H9120.8
C2—C1—N5117.97 (17)C13—C14—C15117.95 (19)
C6—C1—N5118.35 (17)C13—C14—H14121.0
O2—C6—C1117.68 (17)C15—C14—H14121.0
O2—C6—C5124.87 (17)N1—C13—C14123.1 (2)
C1—C6—C5117.45 (18)N1—C13—H13118.4
C16—C15—C14119.50 (19)C14—C13—H13118.4
C16—C15—N3123.98 (19)N2—C8—C9122.9 (2)
C14—C15—N3116.50 (18)N2—C8—H8118.6
C12—C16—C15118.18 (19)C9—C8—H8118.6
C12—C16—H16120.9N2—C7—C10123.2 (2)
C15—C16—H16120.9N2—C7—H7118.4
C4—C5—C6119.72 (18)C10—C7—H7118.4
C4—C5—H5120.1C7—C10—C11118.5 (2)
C6—C5—H5120.1C7—C10—H10120.8
C9—C11—C10119.37 (19)C11—C10—H10120.8
C9—C11—N4124.15 (18)
Symmetry codes: (i) x+1, y, z+2; (ii) x, y+2, z.
(11NRES-4DMAP) top
Crystal data top
C20H25N5O4Z = 2
Mr = 399.45F(000) = 424
Triclinic, P1Dx = 1.322 Mg m3
a = 7.7563 (12) ÅMo Kα radiation, λ = 0.71073 Å
b = 8.1082 (13) ÅCell parameters from 9048 reflections
c = 16.240 (3) Åθ = 3.0–27.6°
α = 97.387 (7)°µ = 0.09 mm1
β = 95.164 (7)°T = 150 K
γ = 95.007 (7)°Block, brown
V = 1003.7 (3) Å30.20 × 0.20 × 0.20 mm
Data collection top
Rigaku Mercury375R (2x2 bin mode)
diffractometer
3549 reflections with I > 2σ(I)
Radiation source: Sealed TubeRint = 0.026
profile data from ω–scansθmax = 27.5°, θmin = 3.0°
Absorption correction: multi-scan
Jacobson, R. (1998) Private communication
h = 1010
Tmin = 0.863, Tmax = 1.000k = 1010
10336 measured reflectionsl = 2121
4570 independent reflections
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.056H-atom parameters constrained
wR(F2) = 0.144 w = 1/[σ2(Fo2) + (0.0522P)2 + 0.7433P]
where P = (Fo2 + 2Fc2)/3
S = 1.08(Δ/σ)max < 0.001
4570 reflectionsΔρmax = 0.36 e Å3
264 parametersΔρmin = 0.36 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O40.60341 (17)0.02852 (17)0.16535 (9)0.0287 (3)
H40.6306810.0558720.1381490.043*
O10.50221 (19)0.43882 (17)0.24905 (9)0.0350 (4)
N10.5560 (2)0.31112 (19)0.27075 (9)0.0236 (3)
N30.6784 (2)0.7554 (2)1.07806 (11)0.0308 (4)
O30.83865 (19)0.51870 (18)0.34057 (10)0.0380 (4)
H30.9299510.5762770.3581130.057*
N20.7794 (2)0.31238 (19)0.93565 (10)0.0256 (3)
C60.7478 (2)0.1239 (2)0.20101 (11)0.0212 (4)
O20.47029 (19)0.2152 (2)0.30746 (10)0.0389 (4)
C100.6845 (2)0.5902 (2)0.94444 (12)0.0261 (4)
H100.6638630.5819470.8866790.031*
C31.0388 (2)0.3430 (2)0.27584 (12)0.0257 (4)
H3A1.1362880.4135070.2999440.031*
C10.7303 (2)0.2721 (2)0.25282 (10)0.0200 (4)
C110.7526 (2)0.4583 (2)0.98166 (11)0.0222 (4)
C20.8724 (2)0.3844 (2)0.29101 (11)0.0234 (4)
C41.0583 (3)0.1971 (2)0.22495 (12)0.0277 (4)
H4A1.1698040.1711060.2153560.033*
C80.6490 (3)0.7307 (2)0.99419 (13)0.0286 (4)
H80.6014790.8145470.9682220.034*
C50.9167 (3)0.0879 (2)0.18762 (12)0.0273 (4)
H50.9343730.0092500.1536500.033*
C90.7880 (2)0.4862 (2)1.06950 (12)0.0268 (4)
H90.8377200.4061611.0975180.032*
C70.7484 (3)0.6320 (3)1.11318 (12)0.0299 (4)
H70.7716570.6465311.1709820.036*
C120.8386 (3)0.1750 (3)0.97629 (14)0.0339 (5)
H12A0.8506950.0822500.9348030.051*
H12B0.9489810.2103031.0081240.051*
H12C0.7552950.1416761.0127840.051*
C130.7482 (3)0.2896 (3)0.84495 (12)0.0336 (5)
H13A0.7738230.1797030.8230690.050*
H13B0.6285810.3023810.8286810.050*
H13C0.8217690.3716450.8233020.050*
N40.0777 (2)0.7367 (2)0.41400 (11)0.0322 (4)
N50.3475 (2)1.1630 (2)0.55655 (11)0.0347 (4)
C160.2623 (2)1.0245 (2)0.50966 (13)0.0279 (4)
C170.2203 (4)0.8794 (3)0.54327 (17)0.0655 (10)
H170.2530320.8743800.5993450.079*
C150.3870 (5)1.3135 (4)0.51993 (17)0.0702 (10)
H15A0.4472371.3983950.5618150.105*
H15B0.4591261.2902050.4756580.105*
H15C0.2807821.3516760.4979880.105*
C140.3956 (4)1.1664 (3)0.64494 (17)0.0589 (8)
H14A0.4545921.2738530.6677270.088*
H14B0.2928501.1464990.6724530.088*
H14C0.4714001.0812510.6533080.088*
C200.1307 (5)0.7429 (3)0.49415 (18)0.0678 (10)
H200.1054260.6477850.5190410.081*
C190.1177 (4)0.8749 (3)0.38177 (14)0.0524 (7)
H190.0821560.8755150.3255760.063*
C180.2075 (4)1.0174 (3)0.42506 (14)0.0587 (8)
H180.2321101.1095810.3978970.070*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O40.0236 (7)0.0250 (7)0.0331 (8)0.0016 (5)0.0006 (5)0.0081 (6)
O10.0323 (8)0.0271 (7)0.0444 (9)0.0119 (6)0.0076 (6)0.0019 (6)
N10.0245 (8)0.0255 (8)0.0185 (7)0.0042 (6)0.0037 (6)0.0020 (6)
N30.0277 (9)0.0272 (8)0.0337 (9)0.0040 (7)0.0049 (7)0.0073 (7)
O30.0289 (8)0.0304 (8)0.0464 (9)0.0042 (6)0.0090 (7)0.0185 (7)
N20.0303 (9)0.0241 (8)0.0230 (8)0.0057 (6)0.0051 (6)0.0013 (6)
C60.0244 (9)0.0200 (8)0.0181 (8)0.0004 (7)0.0009 (7)0.0014 (6)
O20.0297 (8)0.0508 (9)0.0423 (9)0.0107 (7)0.0125 (7)0.0183 (7)
C100.0278 (10)0.0262 (9)0.0226 (9)0.0008 (8)0.0001 (7)0.0015 (7)
C30.0223 (9)0.0270 (9)0.0256 (9)0.0030 (7)0.0019 (7)0.0020 (7)
C10.0208 (9)0.0221 (8)0.0173 (8)0.0041 (7)0.0001 (6)0.0032 (6)
C110.0187 (9)0.0234 (9)0.0234 (9)0.0022 (7)0.0041 (7)0.0010 (7)
C20.0282 (10)0.0196 (8)0.0207 (9)0.0028 (7)0.0033 (7)0.0002 (7)
C40.0217 (9)0.0325 (10)0.0290 (10)0.0027 (8)0.0057 (7)0.0016 (8)
C80.0273 (10)0.0208 (9)0.0358 (11)0.0013 (7)0.0006 (8)0.0003 (8)
C50.0281 (10)0.0249 (9)0.0275 (10)0.0031 (8)0.0059 (8)0.0042 (7)
C90.0257 (10)0.0296 (10)0.0239 (9)0.0029 (8)0.0017 (7)0.0036 (7)
C70.0292 (10)0.0342 (11)0.0225 (9)0.0068 (8)0.0027 (8)0.0035 (8)
C120.0387 (12)0.0283 (10)0.0369 (11)0.0075 (9)0.0092 (9)0.0059 (8)
C130.0409 (12)0.0336 (11)0.0248 (10)0.0042 (9)0.0056 (8)0.0033 (8)
N40.0268 (9)0.0303 (9)0.0348 (9)0.0020 (7)0.0037 (7)0.0087 (7)
N50.0290 (9)0.0302 (9)0.0392 (10)0.0018 (7)0.0030 (7)0.0130 (7)
C160.0170 (9)0.0285 (10)0.0347 (10)0.0042 (7)0.0031 (7)0.0104 (8)
C170.113 (3)0.0211 (11)0.0499 (15)0.0047 (13)0.0536 (16)0.0006 (10)
C150.096 (2)0.0549 (16)0.0479 (15)0.0504 (16)0.0369 (15)0.0175 (13)
C140.0777 (19)0.0304 (12)0.0560 (16)0.0180 (12)0.0405 (14)0.0168 (11)
C200.118 (3)0.0193 (11)0.0535 (16)0.0030 (13)0.0471 (17)0.0047 (10)
C190.0704 (18)0.0576 (16)0.0208 (10)0.0310 (13)0.0101 (11)0.0051 (10)
C180.087 (2)0.0544 (15)0.0255 (12)0.0436 (15)0.0177 (12)0.0032 (10)
Geometric parameters (Å, º) top
O4—C61.343 (2)C3—C21.397 (3)
O1—N11.230 (2)C1—C21.409 (2)
N1—O21.226 (2)C11—C91.413 (3)
N1—C11.461 (2)C4—C51.389 (3)
N3—C71.344 (3)C9—C71.372 (3)
N3—C81.347 (3)N4—C191.321 (3)
O3—C21.328 (2)N4—C201.322 (3)
N2—C111.358 (2)N5—C161.356 (2)
N2—C121.453 (3)N5—C151.445 (3)
N2—C131.456 (2)N5—C141.446 (3)
C6—C51.396 (3)C16—C171.385 (3)
C6—C11.400 (2)C16—C181.393 (3)
C10—C81.373 (3)C17—C201.372 (3)
C10—C111.413 (3)C19—C181.370 (3)
C3—C41.381 (3)
O2—N1—O1122.91 (17)O3—C2—C1117.80 (17)
O2—N1—C1118.27 (15)C3—C2—C1117.26 (16)
O1—N1—C1118.82 (16)C3—C4—C5122.17 (18)
C7—N3—C8116.00 (16)N3—C8—C10124.41 (19)
C11—N2—C12120.43 (16)C4—C5—C6120.10 (17)
C11—N2—C13120.95 (16)C7—C9—C11119.59 (19)
C12—N2—C13118.62 (16)N3—C7—C9124.40 (18)
O4—C6—C5124.13 (16)C19—N4—C20115.08 (19)
O4—C6—C1118.81 (16)C16—N5—C15120.7 (2)
C5—C6—C1117.02 (16)C16—N5—C14121.1 (2)
C8—C10—C11119.49 (18)C15—N5—C14118.23 (19)
C4—C3—C2119.81 (17)N5—C16—C17122.0 (2)
C6—C1—C2123.64 (16)N5—C16—C18123.1 (2)
C6—C1—N1118.64 (15)C17—C16—C18114.88 (19)
C2—C1—N1117.69 (15)C20—C17—C16120.3 (2)
N2—C11—C10121.79 (16)N4—C20—C17124.8 (2)
N2—C11—C9122.17 (17)N4—C19—C18124.8 (2)
C10—C11—C9116.03 (17)C19—C18—C16120.2 (2)
O3—C2—C3124.91 (16)
(12NRES-4DMAP-II) top
Crystal data top
C13H15N3O4F(000) = 584
Mr = 277.28Dx = 1.404 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71075 Å
a = 10.1301 (13) ÅCell parameters from 11747 reflections
b = 12.6967 (17) Åθ = 3.1–27.5°
c = 10.3338 (14) ŵ = 0.11 mm1
β = 99.170 (7)°T = 150 K
V = 1312.1 (3) Å3Block, brown
Z = 40.20 × 0.20 × 0.20 mm
Data collection top
Rigaku Mercury375R (2x2 bin mode)
diffractometer
2568 reflections with I > 2σ(I)
Radiation source: Sealed TubeRint = 0.027
profile data from ω–scansθmax = 27.5°, θmin = 3.1°
Absorption correction: multi-scan
Jacobson, R. (1998) Private communication
h = 1313
Tmin = 0.873, Tmax = 1.000k = 1616
13192 measured reflectionsl = 1313
3009 independent reflections
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.038H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.094 w = 1/[σ2(Fo2) + (0.041P)2 + 0.5219P]
where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max < 0.001
3009 reflectionsΔρmax = 0.24 e Å3
189 parametersΔρmin = 0.29 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O10.83809 (9)0.26442 (7)0.32904 (8)0.0225 (2)
O20.53573 (9)0.15051 (7)0.04164 (9)0.0222 (2)
O30.62117 (11)0.04678 (7)0.20127 (10)0.0323 (2)
O40.56850 (12)0.18141 (9)0.30863 (11)0.0442 (3)
N30.62215 (10)0.14152 (8)0.22227 (10)0.0210 (2)
N10.70849 (11)0.36971 (9)0.50172 (10)0.0224 (2)
N20.56869 (11)0.54280 (8)0.78994 (11)0.0235 (2)
C90.79649 (11)0.27240 (9)0.20174 (11)0.0173 (2)
C80.68854 (11)0.21079 (9)0.14036 (11)0.0163 (2)
C130.63845 (12)0.21410 (9)0.00593 (12)0.0174 (2)
C50.61419 (12)0.48747 (9)0.69533 (12)0.0189 (3)
C100.85602 (12)0.33926 (10)0.11860 (12)0.0206 (3)
H100.9293360.3802010.1531580.025*
C120.69836 (13)0.28344 (10)0.07127 (12)0.0214 (3)
H120.6665610.2890030.1605280.026*
C110.80628 (13)0.34450 (10)0.01405 (13)0.0228 (3)
H110.8461770.3902130.0665750.027*
C30.53614 (13)0.40670 (10)0.62492 (12)0.0217 (3)
H30.4509700.3921750.6430220.026*
C20.58557 (13)0.35063 (10)0.53120 (12)0.0228 (3)
H20.5334180.2978550.4863360.027*
C40.74202 (12)0.50577 (10)0.66002 (12)0.0212 (3)
H40.7967600.5583380.7020580.025*
C10.78489 (13)0.44663 (10)0.56476 (12)0.0223 (3)
H10.8688850.4596620.5427250.027*
C60.43747 (14)0.51932 (11)0.82476 (14)0.0281 (3)
H6A0.4205880.5657770.8935830.042*
H6B0.3698210.5290970.7493840.042*
H6C0.4358290.4476890.8541880.042*
C70.64904 (16)0.62614 (11)0.86083 (15)0.0327 (3)
H7A0.6008750.6567880.9242880.049*
H7B0.7317090.5971000.9046770.049*
H7C0.6674130.6793640.8001540.049*
H2A0.469 (2)0.1849 (18)0.100 (2)0.064 (6)*
H1A0.7412 (18)0.3302 (14)0.4382 (17)0.040 (5)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0193 (4)0.0294 (5)0.0174 (4)0.0024 (4)0.0008 (3)0.0039 (4)
O20.0190 (4)0.0215 (4)0.0228 (4)0.0000 (3)0.0064 (4)0.0004 (4)
O30.0436 (6)0.0203 (5)0.0324 (5)0.0034 (4)0.0044 (5)0.0047 (4)
O40.0512 (7)0.0455 (7)0.0443 (6)0.0131 (5)0.0335 (6)0.0117 (5)
N30.0184 (5)0.0255 (6)0.0182 (5)0.0032 (4)0.0002 (4)0.0004 (4)
N10.0266 (6)0.0231 (5)0.0182 (5)0.0014 (4)0.0060 (4)0.0003 (4)
N20.0248 (6)0.0217 (5)0.0256 (5)0.0003 (4)0.0087 (4)0.0020 (4)
C90.0146 (5)0.0181 (5)0.0189 (6)0.0030 (4)0.0016 (4)0.0038 (5)
C80.0148 (5)0.0162 (5)0.0180 (6)0.0017 (4)0.0028 (4)0.0008 (4)
C130.0151 (5)0.0168 (6)0.0196 (6)0.0042 (4)0.0002 (4)0.0029 (4)
C50.0214 (6)0.0176 (6)0.0177 (6)0.0023 (5)0.0035 (5)0.0040 (4)
C100.0163 (6)0.0180 (6)0.0279 (6)0.0010 (4)0.0049 (5)0.0038 (5)
C120.0263 (7)0.0217 (6)0.0158 (6)0.0054 (5)0.0018 (5)0.0018 (5)
C110.0245 (6)0.0194 (6)0.0266 (7)0.0017 (5)0.0102 (5)0.0024 (5)
C30.0197 (6)0.0228 (6)0.0228 (6)0.0024 (5)0.0038 (5)0.0039 (5)
C20.0263 (7)0.0209 (6)0.0205 (6)0.0039 (5)0.0013 (5)0.0008 (5)
C40.0208 (6)0.0204 (6)0.0221 (6)0.0032 (5)0.0027 (5)0.0005 (5)
C10.0203 (6)0.0244 (6)0.0231 (6)0.0005 (5)0.0056 (5)0.0041 (5)
C60.0256 (7)0.0316 (7)0.0291 (7)0.0051 (6)0.0110 (6)0.0007 (6)
C70.0378 (8)0.0287 (7)0.0334 (8)0.0035 (6)0.0110 (6)0.0107 (6)
Geometric parameters (Å, º) top
O1—C91.3197 (14)C10—C111.3846 (18)
O2—C131.3467 (14)C10—H100.9300
O2—H2A0.94 (2)C12—C111.3927 (18)
O3—N31.2220 (14)C12—H120.9300
O4—N31.2259 (14)C11—H110.9300
N3—C81.4573 (15)C3—C21.3601 (18)
N1—C11.3478 (17)C3—H30.9300
N1—C21.3502 (17)C2—H20.9300
N1—H1A0.928 (18)C4—C11.3630 (18)
N2—C51.3437 (16)C4—H40.9300
N2—C71.4591 (18)C1—H10.9300
N2—C61.4622 (17)C6—H6A0.9600
C9—C101.4098 (17)C6—H6B0.9600
C9—C81.4102 (16)C6—H6C0.9600
C8—C131.4015 (16)C7—H7A0.9600
C13—C121.3907 (17)C7—H7B0.9600
C5—C41.4194 (17)C7—H7C0.9600
C5—C31.4222 (17)
C13—O2—H2A113.1 (14)C10—C11—C12122.06 (12)
O3—N3—O4122.95 (11)C10—C11—H11119.0
O3—N3—C8118.84 (10)C12—C11—H11119.0
O4—N3—C8118.21 (11)C2—C3—C5120.27 (12)
C1—N1—C2120.01 (11)C2—C3—H3119.9
C1—N1—H1A119.4 (11)C5—C3—H3119.9
C2—N1—H1A120.6 (11)N1—C2—C3121.61 (12)
C5—N2—C7121.06 (11)N1—C2—H2119.2
C5—N2—C6120.21 (11)C3—C2—H2119.2
C7—N2—C6118.72 (11)C1—C4—C5120.28 (12)
O1—C9—C10123.64 (11)C1—C4—H4119.9
O1—C9—C8120.49 (11)C5—C4—H4119.9
C10—C9—C8115.86 (11)N1—C1—C4121.58 (12)
C13—C8—C9124.16 (11)N1—C1—H1119.2
C13—C8—N3117.78 (10)C4—C1—H1119.2
C9—C8—N3118.04 (10)N2—C6—H6A109.5
O2—C13—C12123.55 (11)N2—C6—H6B109.5
O2—C13—C8118.72 (11)H6A—C6—H6B109.5
C12—C13—C8117.74 (11)N2—C6—H6C109.5
N2—C5—C4122.29 (11)H6A—C6—H6C109.5
N2—C5—C3121.47 (11)H6B—C6—H6C109.5
C4—C5—C3116.24 (11)N2—C7—H7A109.5
C11—C10—C9120.58 (11)N2—C7—H7B109.5
C11—C10—H10119.7H7A—C7—H7B109.5
C9—C10—H10119.7N2—C7—H7C109.5
C13—C12—C11119.58 (11)H7A—C7—H7C109.5
C13—C12—H12120.2H7B—C7—H7C109.5
C11—C12—H12120.2
(13NRES-TMP-PYR) top
Crystal data top
C29H26N3O4F(000) = 506
Mr = 480.53Dx = 1.322 Mg m3
Monoclinic, P21Mo Kα radiation, λ = 0.71075 Å
a = 7.7925 (13) ÅCell parameters from 9438 reflections
b = 12.885 (2) Åθ = 3.1–27.6°
c = 12.398 (2) ŵ = 0.09 mm1
β = 104.054 (7)°T = 150 K
V = 1207.6 (4) Å3Block, yellow
Z = 20.20 × 0.20 × 0.20 mm
Data collection top
Rigaku Mercury375R (2x2 bin mode)
diffractometer
3193 reflections with I > 2σ(I)
Radiation source: Sealed TubeRint = 0.057
profile data from ω–scansθmax = 27.5°, θmin = 3.1°
Absorption correction: multi-scan
Jacobson, R. (1998) Private communication
h = 1010
Tmin = 0.710, Tmax = 1.000k = 1616
12163 measured reflectionsl = 1616
5506 independent reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.091 w = 1/[σ2(Fo2) + (0.1152P)2 + 1.4802P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.276(Δ/σ)max < 0.001
S = 1.05Δρmax = 0.47 e Å3
5506 reflectionsΔρmin = 0.35 e Å3
340 parametersAbsolute structure: Flack x determined using 988 quotients [(I+)-(I-)]/[(I+)+(I-)] (Parsons, Flack and Wagner, Acta Cryst. B69 (2013) 249-259).
1 restraintAbsolute structure parameter: 1.5 (10)
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
O10.8237 (8)0.4406 (4)0.3005 (5)0.0487 (15)
O40.5663 (6)0.5084 (6)0.4455 (3)0.0445 (14)
H40.5080790.5283460.4883950.067*
N30.4249 (7)0.5172 (6)0.3740 (4)0.0327 (12)
O30.5609 (7)0.5250 (6)0.0685 (4)0.0499 (14)
H30.4969330.5193350.0056390.075*
N10.7422 (7)0.5218 (6)0.2834 (4)0.0326 (13)
N20.4071 (8)0.5266 (5)0.1548 (4)0.0329 (13)
C130.4217 (11)0.6113 (5)0.2110 (6)0.0318 (17)
O20.8155 (10)0.6067 (5)0.2897 (6)0.064 (2)
C120.4317 (10)0.6079 (5)0.3214 (6)0.0285 (16)
C20.4640 (9)0.5088 (6)0.3406 (5)0.0341 (16)
C10.5497 (8)0.5152 (6)0.2554 (5)0.0278 (13)
C60.4624 (9)0.5178 (7)0.1434 (5)0.0359 (15)
C90.4048 (10)0.4289 (6)0.3188 (6)0.0312 (17)
C50.2754 (11)0.5088 (8)0.1164 (6)0.048 (2)
H50.2118160.5069230.0424960.058*
C30.2789 (10)0.5020 (7)0.3122 (6)0.0391 (18)
H3A0.2169780.4969700.3674110.047*
C140.4315 (13)0.7138 (6)0.1487 (7)0.046 (2)
H14A0.5455430.7447970.1423880.069*
H14B0.3412560.7598070.1887610.069*
H14C0.4137160.7015880.0758390.069*
C110.4503 (15)0.7040 (6)0.3851 (7)0.052 (2)
H11A0.5677530.7312190.3593030.078*
H11B0.4289860.6876310.4628120.078*
H11C0.3659680.7547950.3742460.078*
C40.1889 (10)0.5028 (7)0.2007 (6)0.0436 (19)
H4A0.0660540.4992590.1824140.052*
C80.3979 (11)0.4331 (6)0.2066 (6)0.0365 (18)
C270.9393 (15)0.4332 (10)0.5939 (9)0.067 (3)
H270.9544600.4260950.5221590.080*
C300.8851 (12)0.4578 (8)0.8089 (8)0.052 (2)
C290.9149 (11)0.5494 (7)0.7506 (8)0.051 (2)
C100.4009 (14)0.3274 (7)0.3810 (9)0.052 (2)
H10A0.5006230.2857160.3451060.078*
H10B0.2935440.2908420.3810420.078*
H10C0.4062050.3412140.4562030.078*
C210.8578 (14)0.4716 (8)0.9155 (9)0.065 (3)
C70.3668 (18)0.3399 (7)0.1442 (8)0.067 (3)
H7A0.4721340.2983080.1265400.101*
H7B0.3368340.3608260.0767510.101*
H7C0.2713940.3002280.1888700.101*
C260.9154 (14)0.3495 (9)0.6492 (9)0.064 (3)
H260.9184430.2840340.6181090.076*
C280.9430 (12)0.5378 (8)0.6422 (8)0.060 (3)
C250.8831 (15)0.3611 (9)0.7625 (10)0.066 (3)
C220.8393 (18)0.3783 (10)0.9768 (9)0.082 (4)
H220.8230460.3834131.0484710.099*
C150.9712 (15)0.6252 (9)0.5852 (11)0.075 (3)
H150.9896900.6195930.5140830.090*
C240.871 (2)0.2724 (10)0.8226 (13)0.108 (6)
H240.8799800.2072570.7922290.129*
C230.846 (3)0.2819 (10)0.9293 (12)0.120 (6)
H230.8325800.2224810.9692680.144*
C0AA0.9213 (15)0.6473 (10)0.7960 (11)0.070 (4)
C2AA0.9435 (19)0.7298 (11)0.7447 (14)0.102 (6)
H2AA0.9416150.7944170.7778250.123*
C1AA0.9717 (17)0.7216 (10)0.6345 (15)0.095 (5)
H1AA0.9902840.7810790.5963680.114*
C3AA0.861 (2)0.5829 (13)0.9426 (14)0.046 (4)0.5
H3AA0.8483850.5991571.0133230.055*0.5
C4AA0.879 (3)0.6604 (14)0.881 (3)0.094 (11)0.5
H4AA0.8584390.7273300.9036810.112*0.5
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.039 (3)0.041 (3)0.065 (4)0.014 (3)0.011 (3)0.008 (3)
O40.039 (3)0.078 (4)0.019 (2)0.007 (3)0.0121 (18)0.001 (3)
N30.036 (3)0.042 (3)0.020 (2)0.003 (3)0.006 (2)0.001 (3)
O30.058 (3)0.075 (4)0.020 (2)0.017 (4)0.015 (2)0.003 (3)
N10.042 (3)0.038 (3)0.023 (2)0.017 (3)0.018 (2)0.011 (3)
N20.044 (3)0.037 (3)0.018 (2)0.006 (3)0.007 (2)0.001 (3)
C130.042 (4)0.027 (4)0.026 (4)0.002 (3)0.006 (3)0.006 (3)
O20.072 (5)0.043 (4)0.082 (5)0.018 (3)0.031 (4)0.011 (3)
C120.028 (4)0.032 (4)0.025 (4)0.004 (3)0.005 (3)0.004 (3)
C20.042 (4)0.041 (4)0.017 (3)0.002 (4)0.004 (3)0.001 (3)
C10.035 (3)0.025 (3)0.023 (3)0.005 (3)0.009 (2)0.000 (3)
C60.050 (4)0.039 (4)0.019 (3)0.002 (4)0.010 (3)0.002 (4)
C90.039 (4)0.031 (4)0.024 (4)0.005 (3)0.008 (3)0.000 (3)
C50.056 (5)0.061 (5)0.025 (3)0.008 (5)0.006 (3)0.000 (4)
C30.041 (4)0.051 (5)0.031 (3)0.001 (4)0.017 (3)0.005 (4)
C140.063 (6)0.039 (5)0.032 (4)0.001 (4)0.007 (4)0.015 (3)
C110.082 (7)0.038 (5)0.032 (5)0.001 (4)0.008 (4)0.010 (4)
C40.034 (4)0.060 (6)0.038 (4)0.007 (4)0.012 (3)0.001 (4)
C80.049 (5)0.039 (4)0.021 (4)0.010 (4)0.008 (3)0.003 (3)
C270.063 (7)0.091 (8)0.046 (6)0.006 (6)0.013 (5)0.013 (6)
C300.047 (5)0.059 (6)0.053 (5)0.008 (4)0.015 (4)0.003 (5)
C290.037 (5)0.049 (6)0.062 (5)0.002 (4)0.002 (4)0.002 (4)
C100.060 (6)0.041 (5)0.058 (6)0.002 (4)0.019 (5)0.015 (4)
C210.057 (6)0.068 (7)0.067 (7)0.002 (5)0.010 (5)0.004 (5)
C70.114 (10)0.048 (6)0.038 (5)0.024 (6)0.016 (6)0.001 (4)
C260.051 (6)0.077 (7)0.065 (7)0.005 (5)0.016 (5)0.004 (6)
C280.048 (5)0.066 (7)0.058 (5)0.001 (5)0.005 (4)0.000 (5)
C250.058 (7)0.066 (7)0.067 (7)0.005 (5)0.005 (5)0.027 (6)
C220.109 (10)0.091 (9)0.056 (7)0.050 (8)0.040 (7)0.014 (6)
C150.047 (6)0.072 (8)0.089 (8)0.006 (5)0.017 (6)0.020 (6)
C240.178 (17)0.055 (7)0.110 (11)0.025 (8)0.075 (11)0.020 (7)
C230.22 (2)0.068 (8)0.094 (10)0.047 (11)0.076 (12)0.007 (7)
C0AA0.046 (6)0.071 (9)0.077 (8)0.022 (6)0.014 (5)0.036 (6)
C2AA0.087 (10)0.053 (8)0.132 (14)0.003 (7)0.038 (9)0.018 (8)
C1AA0.061 (8)0.069 (8)0.127 (13)0.015 (6)0.031 (8)0.000 (8)
C3AA0.050 (11)0.037 (10)0.041 (9)0.025 (8)0.006 (8)0.009 (7)
C4AA0.044 (12)0.015 (9)0.22 (4)0.002 (8)0.038 (17)0.008 (14)
Geometric parameters (Å, º) top
O1—N11.216 (8)C27—H270.9300
O4—C21.350 (7)C30—C251.371 (15)
O4—H40.8200C30—C211.400 (14)
N3—C121.333 (10)C30—C291.433 (12)
N3—C91.356 (10)C29—C0AA1.377 (14)
O3—C61.343 (8)C29—C281.421 (13)
O3—H30.8200C10—H10A0.9600
N1—O21.227 (9)C10—H10B0.9600
N1—C11.458 (8)C10—H10C0.9600
N2—C131.313 (10)C21—C221.447 (16)
N2—C81.359 (10)C21—C3AA1.473 (18)
C13—C121.391 (11)C7—H7A0.9600
C13—C141.523 (10)C7—H7B0.9600
C12—C111.495 (11)C7—H7C0.9600
C2—C11.382 (8)C26—C251.493 (16)
C2—C31.402 (10)C26—H260.9300
C1—C61.391 (8)C28—C151.375 (15)
C6—C51.419 (11)C25—C241.380 (17)
C9—C81.407 (10)C22—C231.381 (18)
C9—C101.515 (11)C22—H220.9300
C5—C41.376 (10)C15—C1AA1.383 (18)
C5—H50.9300C15—H150.9300
C3—C41.390 (10)C24—C231.390 (18)
C3—H3A0.9300C24—H240.9300
C14—H14A0.9600C23—H230.9300
C14—H14B0.9600C0AA—C4AA1.20 (3)
C14—H14C0.9600C0AA—C2AA1.27 (2)
C11—H11A0.9600C2AA—C1AA1.44 (2)
C11—H11B0.9600C2AA—H2AA0.9300
C11—H11C0.9600C1AA—H1AA0.9300
C4—H4A0.9300C3AA—C4AA1.28 (3)
C8—C71.479 (12)C3AA—H3AA0.9300
C27—C261.315 (15)C4AA—H4AA0.9300
C27—C281.472 (16)
C2—O4—H4109.5C0AA—C29—C28119.0 (11)
C12—N3—C9119.0 (5)C0AA—C29—C30122.9 (11)
C6—O3—H3109.5C28—C29—C30118.2 (8)
O1—N1—O2122.7 (6)C9—C10—H10A109.5
O1—N1—C1117.1 (7)C9—C10—H10B109.5
O2—N1—C1120.2 (7)H10A—C10—H10B109.5
C13—N2—C8119.2 (5)C9—C10—H10C109.5
N2—C13—C12121.9 (6)H10A—C10—H10C109.5
N2—C13—C14116.9 (7)H10B—C10—H10C109.5
C12—C13—C14121.2 (7)C30—C21—C22116.6 (10)
N3—C12—C13120.3 (6)C30—C21—C3AA109.9 (11)
N3—C12—C11117.7 (7)C22—C21—C3AA133.4 (13)
C13—C12—C11122.0 (7)C8—C7—H7A109.5
O4—C2—C1117.0 (6)C8—C7—H7B109.5
O4—C2—C3124.9 (6)H7A—C7—H7B109.5
C1—C2—C3118.1 (5)C8—C7—H7C109.5
C2—C1—C6123.7 (6)H7A—C7—H7C109.5
C2—C1—N1118.8 (5)H7B—C7—H7C109.5
C6—C1—N1117.5 (5)C27—C26—C25119.1 (11)
O3—C6—C1118.0 (6)C27—C26—H26120.5
O3—C6—C5124.7 (5)C25—C26—H26120.5
C1—C6—C5117.3 (6)C15—C28—C29118.7 (10)
N3—C9—C8120.3 (6)C15—C28—C27122.1 (10)
N3—C9—C10117.3 (7)C29—C28—C27119.2 (9)
C8—C9—C10122.4 (7)C30—C25—C24121.4 (11)
C4—C5—C6119.3 (6)C30—C25—C26119.9 (9)
C4—C5—H5120.3C24—C25—C26118.4 (11)
C6—C5—H5120.3C23—C22—C21120.3 (11)
C4—C3—C2119.2 (6)C23—C22—H22119.8
C4—C3—H3A120.4C21—C22—H22119.8
C2—C3—H3A120.4C28—C15—C1AA119.5 (14)
C13—C14—H14A109.5C28—C15—H15120.3
C13—C14—H14B109.5C1AA—C15—H15120.3
H14A—C14—H14B109.5C25—C24—C23119.1 (12)
C13—C14—H14C109.5C25—C24—H24120.4
H14A—C14—H14C109.5C23—C24—H24120.4
H14B—C14—H14C109.5C22—C23—C24120.8 (11)
C12—C11—H11A109.5C22—C23—H23119.6
C12—C11—H11B109.5C24—C23—H23119.6
H11A—C11—H11B109.5C4AA—C0AA—C2AA115.2 (15)
C12—C11—H11C109.5C4AA—C0AA—C29120.1 (17)
H11A—C11—H11C109.5C2AA—C0AA—C29123.8 (15)
H11B—C11—H11C109.5C0AA—C2AA—C1AA118.9 (14)
C5—C4—C3122.3 (7)C0AA—C2AA—H2AA120.5
C5—C4—H4A118.9C1AA—C2AA—H2AA120.5
C3—C4—H4A118.9C15—C1AA—C2AA120.0 (13)
N2—C8—C9119.4 (6)C15—C1AA—H1AA120.0
N2—C8—C7118.0 (7)C2AA—C1AA—H1AA120.0
C9—C8—C7122.5 (7)C4AA—C3AA—C21129 (2)
C26—C27—C28122.0 (10)C4AA—C3AA—H3AA115.7
C26—C27—H27119.0C21—C3AA—H3AA115.7
C28—C27—H27119.0C0AA—C4AA—C3AA120 (2)
C25—C30—C21121.5 (9)C0AA—C4AA—H4AA119.8
C25—C30—C29121.6 (9)C3AA—C4AA—H4AA119.8
C21—C30—C29116.9 (9)
(14NRES-4DMAP-PYR) top
Crystal data top
C58H50N6O8Z = 2
Mr = 959.04F(000) = 1008
Triclinic, P1Dx = 1.304 Mg m3
a = 13.337 (3) ÅMo Kα radiation, λ = 0.71075 Å
b = 13.504 (3) ÅCell parameters from 14998 reflections
c = 16.069 (3) Åθ = 3.1–28.2°
α = 75.831 (5)°µ = 0.09 mm1
β = 66.422 (5)°T = 150 K
γ = 67.934 (5)°Block, colorless
V = 2442.9 (8) Å30.20 × 0.20 × 0.20 mm
Data collection top
Rigaku Mercury375R (2x2 bin mode)
diffractometer
4435 reflections with I > 2σ(I)
Radiation source: Sealed TubeRint = 0.062
profile data from ω–scansθmax = 27.5°, θmin = 3.1°
Absorption correction: multi-scan
Jacobson, R. (1998) Private communication
h = 1717
Tmin = 0.804, Tmax = 1.000k = 1717
25588 measured reflectionsl = 2020
11144 independent reflections
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.087H-atom parameters constrained
wR(F2) = 0.284 w = 1/[σ2(Fo2) + (0.1128P)2 + 0.737P]
where P = (Fo2 + 2Fc2)/3
S = 1.04(Δ/σ)max < 0.001
11144 reflectionsΔρmax = 0.36 e Å3
655 parametersΔρmin = 0.25 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O600.7180 (2)0.06012 (17)0.31313 (16)0.0517 (6)
O610.6864 (2)0.43167 (18)0.27054 (18)0.0576 (7)
O630.5142 (2)0.3393 (2)0.37148 (19)0.0691 (8)
N710.6024 (3)0.2651 (2)0.3728 (2)0.0485 (7)
O640.7690 (3)0.5800 (2)0.18932 (18)0.0692 (8)
H640.7456160.5292370.2185280.104*
O620.6068 (3)0.2053 (2)0.44286 (19)0.0870 (10)
O670.7839 (3)0.9091 (2)0.2175 (2)0.0860 (10)
H670.7501070.9582790.2499420.129*
N720.7881 (3)0.0097 (2)0.4547 (2)0.0572 (8)
H720.7470510.0176880.4198790.069*
N690.3246 (3)0.6258 (2)0.0293 (2)0.0590 (8)
C10.7020 (3)0.2466 (3)0.2910 (2)0.0414 (8)
N680.5099 (3)0.5050 (3)0.2037 (2)0.0628 (9)
H680.5482260.4799020.2405630.075*
C20.7411 (3)0.3356 (3)0.2427 (2)0.0416 (8)
C60.7565 (3)0.1418 (3)0.2641 (2)0.0423 (8)
N700.8315 (5)0.7604 (4)0.1113 (3)0.0870 (13)
N730.9842 (3)0.1401 (3)0.6204 (3)0.0693 (10)
C30.8410 (3)0.3140 (3)0.1655 (3)0.0512 (9)
H30.8718930.3689580.1325020.061*
C80.7452 (3)0.6500 (3)0.2463 (2)0.0475 (9)
C70.7733 (3)0.7439 (3)0.2103 (2)0.0508 (9)
C50.8521 (3)0.1282 (3)0.1847 (3)0.0546 (10)
H50.8882380.0613000.1628560.066*
C40.8941 (3)0.2123 (3)0.1379 (3)0.0543 (10)
H40.9601150.2002230.0862870.065*
C120.7494 (3)0.8239 (3)0.2615 (3)0.0551 (10)
C170.3856 (3)0.5860 (3)0.0856 (3)0.0507 (9)
C150.4754 (3)0.6232 (3)0.0764 (3)0.0594 (10)
H150.4944010.6764400.0296700.071*
C210.7470 (4)0.0177 (3)0.5394 (3)0.0621 (11)
H210.6737970.0668370.5600570.075*
C200.8927 (4)0.0797 (3)0.4246 (3)0.0630 (11)
H200.9203550.0981970.3655360.076*
C240.9206 (4)0.0980 (3)0.5664 (3)0.0547 (10)
C130.5343 (3)0.5816 (3)0.1356 (3)0.0613 (10)
H130.5933500.6071250.1285260.074*
C220.8088 (4)0.0239 (3)0.5955 (3)0.0608 (11)
H220.7776070.0035880.6542410.073*
C90.6920 (4)0.6361 (3)0.3395 (3)0.0648 (11)
H90.6727460.5734950.3670770.078*
C110.6958 (4)0.8070 (3)0.3537 (3)0.0674 (12)
H110.6784970.8586660.3906670.081*
C230.9609 (4)0.1253 (3)0.4770 (3)0.0640 (11)
H231.0336360.1740730.4538780.077*
C100.6672 (4)0.7144 (4)0.3921 (3)0.0735 (13)
H100.6303800.7043550.4549300.088*
C160.3628 (4)0.5045 (3)0.1589 (3)0.0636 (11)
H160.3045600.4765460.1685350.076*
C140.4255 (4)0.4680 (3)0.2138 (3)0.0680 (12)
H140.4095050.4145060.2612480.082*
C190.3476 (4)0.7086 (3)0.0449 (3)0.0700 (12)
H19A0.3259390.7748760.0207360.105*
H19B0.3040070.7179830.0830340.105*
H19C0.4282920.6880480.0803740.105*
C580.2295 (4)0.8100 (4)0.2191 (4)0.0800 (14)
C570.2657 (4)0.7396 (4)0.2898 (4)0.0797 (14)
C410.3115 (5)0.2338 (4)0.2316 (4)0.0864 (16)
C180.2284 (4)0.5884 (4)0.0428 (3)0.0812 (14)
H18A0.2572270.5138690.0332980.122*
H18B0.1902730.6298440.0000030.122*
H18C0.1747110.5970700.1039260.122*
O650.9323 (5)0.7146 (6)0.0804 (3)0.177 (3)
C420.2039 (5)0.3076 (4)0.2650 (5)0.0901 (16)
C480.1379 (5)0.8067 (5)0.1978 (5)0.0988 (17)
C261.0995 (4)0.2161 (4)0.5898 (4)0.0931 (16)
H26A1.0951010.2811370.5793450.140*
H26B1.1338100.2320060.6358300.140*
H26C1.1455650.1853290.5341290.140*
O660.7767 (7)0.8176 (4)0.0666 (3)0.186 (3)
C270.3381 (8)0.2142 (6)0.3795 (6)0.116 (2)
H270.3813140.1834920.4179140.139*
C590.2068 (5)0.6636 (4)0.3404 (4)0.0969 (17)
C540.3576 (5)0.7435 (5)0.3108 (5)0.0994 (18)
C250.9397 (5)0.1098 (4)0.7124 (3)0.0919 (16)
H25A0.9264620.0342280.7093010.138*
H25B0.9947720.1495940.7425270.138*
H25C0.8686820.1255730.7461530.138*
C440.2888 (6)0.8845 (5)0.1660 (5)0.111 (2)
C290.1611 (7)0.3349 (6)0.3576 (5)0.1032 (18)
C360.3550 (8)0.2048 (6)0.1416 (6)0.111 (2)
C330.1297 (7)0.3602 (6)0.2144 (6)0.116 (2)
C340.1763 (9)0.3278 (7)0.1198 (7)0.139 (3)
H340.1315110.3576880.0825500.167*
C490.0815 (5)0.7310 (6)0.2510 (6)0.115 (2)
H490.0196050.7282900.2394380.138*
C500.1144 (6)0.6634 (6)0.3172 (6)0.115 (2)
H500.0756280.6136510.3498170.137*
C400.3839 (6)0.1849 (5)0.2867 (6)0.111 (2)
C560.3830 (7)0.8853 (6)0.1897 (6)0.130 (3)
H560.4215630.9353030.1577880.156*
C280.2331 (9)0.2859 (7)0.4086 (6)0.132 (3)
H280.2065240.3040840.4676460.158*
C350.2821 (10)0.2560 (8)0.0876 (6)0.139 (3)
H350.3085740.2393330.0281160.166*
C370.4607 (9)0.1330 (7)0.1064 (6)0.141 (3)
H370.4876620.1151680.0472070.169*
C390.4856 (8)0.1156 (7)0.2551 (8)0.139 (3)
H390.5309350.0847030.2918730.167*
C530.3889 (7)0.6712 (8)0.3827 (6)0.126 (2)
H530.4478760.6726470.3988380.152*
C450.2531 (9)0.9546 (6)0.0967 (6)0.151 (3)
H450.2911961.0043310.0620400.181*
C550.4151 (6)0.8162 (7)0.2560 (7)0.139 (3)
H550.4788320.8165660.2661850.167*
C510.2425 (8)0.5935 (6)0.4097 (5)0.137 (3)
H510.2057360.5425710.4434460.164*
C320.0256 (8)0.4308 (7)0.2436 (10)0.161 (4)
H320.0200910.4628370.2071770.193*
C460.1627 (10)0.9510 (7)0.0792 (7)0.152 (4)
H460.1393861.0000500.0334770.183*
C380.5283 (9)0.0864 (7)0.1644 (9)0.158 (4)
H380.6008930.0366030.1430370.190*
C470.1048 (7)0.8780 (7)0.1262 (6)0.129 (3)
H470.0452930.8755200.1113090.155*
C520.3300 (9)0.5991 (8)0.4279 (6)0.151 (3)
H520.3519260.5505920.4744450.181*
C300.0562 (8)0.4056 (6)0.3904 (7)0.136 (3)
H300.0281510.4225220.4499340.163*
C310.0104 (10)0.4536 (8)0.3343 (10)0.173 (5)
H310.0823760.5033400.3578720.208*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O600.0781 (18)0.0322 (13)0.0549 (15)0.0257 (12)0.0287 (14)0.0015 (11)
O610.0679 (17)0.0312 (14)0.0784 (18)0.0189 (12)0.0267 (15)0.0059 (12)
O630.0545 (17)0.0562 (18)0.0702 (19)0.0035 (14)0.0138 (15)0.0026 (14)
N710.055 (2)0.0371 (17)0.0495 (19)0.0144 (15)0.0152 (16)0.0027 (14)
O640.102 (2)0.0521 (17)0.0652 (17)0.0451 (16)0.0168 (17)0.0135 (13)
O620.082 (2)0.077 (2)0.0531 (18)0.0034 (16)0.0129 (17)0.0130 (15)
O670.143 (3)0.0513 (18)0.0713 (19)0.057 (2)0.018 (2)0.0092 (14)
N720.078 (2)0.0455 (19)0.060 (2)0.0232 (17)0.038 (2)0.0065 (15)
N690.065 (2)0.054 (2)0.062 (2)0.0207 (16)0.0275 (19)0.0001 (16)
C10.049 (2)0.0350 (19)0.046 (2)0.0166 (15)0.0199 (18)0.0022 (15)
N680.071 (2)0.047 (2)0.068 (2)0.0036 (17)0.033 (2)0.0094 (17)
C20.054 (2)0.0326 (19)0.051 (2)0.0200 (16)0.0279 (19)0.0011 (15)
C60.054 (2)0.0329 (19)0.050 (2)0.0130 (16)0.0279 (19)0.0043 (15)
N700.140 (4)0.075 (3)0.056 (3)0.064 (3)0.017 (3)0.004 (2)
N730.088 (3)0.061 (2)0.085 (3)0.030 (2)0.056 (2)0.0051 (19)
C30.054 (2)0.051 (2)0.054 (2)0.0255 (18)0.022 (2)0.0054 (18)
C80.057 (2)0.038 (2)0.054 (2)0.0226 (17)0.017 (2)0.0065 (16)
C70.072 (3)0.043 (2)0.046 (2)0.0320 (19)0.016 (2)0.0037 (16)
C50.067 (3)0.041 (2)0.056 (2)0.0075 (18)0.023 (2)0.0144 (17)
C40.051 (2)0.061 (3)0.048 (2)0.0205 (19)0.0135 (19)0.0015 (19)
C120.075 (3)0.041 (2)0.056 (2)0.0298 (19)0.018 (2)0.0078 (17)
C170.053 (2)0.037 (2)0.055 (2)0.0085 (17)0.014 (2)0.0094 (16)
C150.060 (3)0.051 (2)0.062 (3)0.0184 (19)0.016 (2)0.0058 (19)
C210.073 (3)0.046 (2)0.066 (3)0.013 (2)0.026 (2)0.0063 (19)
C200.088 (3)0.050 (2)0.057 (2)0.028 (2)0.027 (3)0.0020 (19)
C240.071 (3)0.041 (2)0.066 (3)0.0252 (19)0.035 (2)0.0027 (18)
C130.055 (2)0.054 (3)0.072 (3)0.0134 (19)0.019 (2)0.013 (2)
C220.081 (3)0.052 (2)0.056 (2)0.023 (2)0.031 (2)0.0017 (19)
C90.084 (3)0.059 (3)0.058 (3)0.045 (2)0.012 (2)0.000 (2)
C110.084 (3)0.060 (3)0.061 (3)0.029 (2)0.011 (2)0.025 (2)
C230.067 (3)0.054 (3)0.070 (3)0.018 (2)0.023 (2)0.007 (2)
C100.100 (4)0.075 (3)0.049 (2)0.051 (3)0.002 (2)0.013 (2)
C160.075 (3)0.049 (2)0.072 (3)0.023 (2)0.034 (3)0.006 (2)
C140.076 (3)0.051 (3)0.073 (3)0.020 (2)0.029 (3)0.005 (2)
C190.083 (3)0.057 (3)0.067 (3)0.020 (2)0.030 (3)0.003 (2)
C580.061 (3)0.054 (3)0.102 (4)0.013 (2)0.008 (3)0.040 (3)
C570.071 (3)0.063 (3)0.093 (4)0.016 (3)0.005 (3)0.038 (3)
C410.097 (4)0.081 (4)0.107 (5)0.064 (3)0.045 (4)0.021 (3)
C180.077 (3)0.089 (3)0.089 (3)0.035 (3)0.038 (3)0.002 (3)
O650.153 (5)0.243 (7)0.090 (3)0.095 (5)0.038 (3)0.027 (4)
C420.094 (4)0.077 (4)0.126 (5)0.056 (3)0.049 (4)0.010 (3)
C480.077 (4)0.077 (4)0.114 (5)0.000 (3)0.006 (4)0.048 (4)
C260.090 (4)0.074 (3)0.137 (5)0.026 (3)0.071 (4)0.006 (3)
O660.359 (9)0.130 (4)0.091 (3)0.074 (5)0.123 (5)0.024 (3)
C270.174 (8)0.119 (6)0.116 (6)0.100 (5)0.090 (6)0.038 (4)
C590.095 (4)0.069 (4)0.095 (4)0.021 (3)0.005 (4)0.028 (3)
C540.081 (4)0.088 (4)0.113 (5)0.016 (3)0.002 (4)0.055 (4)
C250.138 (5)0.086 (4)0.089 (4)0.048 (3)0.076 (4)0.010 (3)
C440.120 (5)0.054 (3)0.119 (5)0.022 (3)0.006 (4)0.028 (3)
C290.115 (5)0.092 (5)0.123 (6)0.073 (4)0.032 (5)0.003 (4)
C360.132 (6)0.095 (5)0.125 (6)0.082 (5)0.028 (5)0.004 (4)
C330.119 (6)0.099 (5)0.170 (7)0.078 (4)0.087 (6)0.051 (5)
C340.185 (9)0.135 (7)0.172 (9)0.113 (7)0.117 (8)0.051 (6)
C490.082 (4)0.113 (6)0.146 (6)0.025 (4)0.011 (5)0.063 (5)
C500.091 (5)0.103 (5)0.136 (6)0.052 (4)0.013 (4)0.044 (4)
C400.095 (5)0.090 (4)0.177 (8)0.061 (4)0.073 (5)0.034 (4)
C560.108 (6)0.085 (5)0.174 (8)0.058 (5)0.020 (5)0.051 (5)
C280.176 (8)0.120 (6)0.151 (7)0.106 (6)0.077 (7)0.029 (5)
C350.208 (9)0.152 (8)0.130 (6)0.137 (7)0.094 (8)0.050 (6)
C370.133 (7)0.115 (6)0.165 (8)0.086 (6)0.005 (6)0.017 (6)
C390.102 (6)0.111 (6)0.221 (10)0.061 (5)0.079 (7)0.040 (6)
C530.103 (5)0.142 (7)0.119 (6)0.001 (5)0.028 (5)0.064 (5)
C450.155 (8)0.064 (5)0.153 (8)0.015 (5)0.011 (6)0.014 (5)
C550.092 (5)0.116 (6)0.205 (10)0.038 (5)0.001 (6)0.089 (6)
C510.149 (7)0.110 (6)0.109 (6)0.031 (5)0.010 (5)0.014 (4)
C320.099 (6)0.094 (6)0.309 (15)0.046 (5)0.095 (8)0.014 (7)
C460.151 (8)0.082 (6)0.158 (8)0.030 (6)0.033 (7)0.040 (5)
C380.127 (7)0.113 (6)0.217 (11)0.071 (6)0.028 (8)0.013 (7)
C470.117 (6)0.103 (6)0.133 (6)0.023 (5)0.043 (5)0.046 (5)
C520.142 (8)0.156 (9)0.111 (6)0.009 (6)0.027 (6)0.031 (6)
C300.112 (6)0.103 (6)0.190 (9)0.057 (5)0.017 (6)0.030 (6)
C310.140 (9)0.114 (7)0.272 (15)0.056 (6)0.057 (10)0.028 (9)
Geometric parameters (Å, º) top
O60—C61.333 (4)C57—C541.417 (8)
O61—C21.314 (4)C57—C591.421 (7)
O63—N711.230 (4)C41—C421.383 (8)
N71—O621.222 (4)C41—C361.420 (8)
N71—C11.439 (4)C41—C401.439 (7)
O64—C81.343 (4)C18—H18A0.9600
O64—H640.8200C18—H18B0.9600
O67—C121.332 (4)C18—H18C0.9600
O67—H670.8200C42—C331.406 (8)
N72—C201.329 (5)C42—C291.451 (8)
N72—C211.338 (5)C48—C491.407 (9)
N72—H720.8600C48—C471.410 (9)
N69—C171.339 (5)C26—H26A0.9600
N69—C191.442 (5)C26—H26B0.9600
N69—C181.470 (5)C26—H26C0.9600
C1—C61.412 (4)C27—C281.340 (10)
C1—C21.418 (4)C27—C401.460 (10)
N68—C141.334 (5)C27—H270.9300
N68—C131.337 (5)C59—C511.390 (9)
N68—H680.8600C59—C501.424 (9)
C2—C31.400 (5)C54—C551.389 (10)
C6—C51.386 (5)C54—C531.410 (9)
N70—O661.170 (6)C25—H25A0.9600
N70—O651.195 (6)C25—H25B0.9600
N70—C71.467 (5)C25—H25C0.9600
N73—C241.336 (5)C44—C451.390 (10)
N73—C261.454 (6)C44—C561.455 (10)
N73—C251.456 (6)C29—C301.342 (9)
C3—C41.379 (5)C29—C281.385 (9)
C3—H30.9300C36—C371.361 (9)
C8—C91.376 (5)C36—C351.432 (9)
C8—C71.380 (5)C33—C321.326 (10)
C7—C121.383 (5)C33—C341.501 (11)
C5—C41.376 (5)C34—C351.354 (11)
C5—H50.9300C34—H340.9300
C4—H40.9300C49—C501.325 (8)
C12—C111.367 (5)C49—H490.9300
C17—C151.408 (5)C50—H500.9300
C17—C161.421 (5)C40—C391.305 (10)
C15—C131.357 (5)C56—C551.329 (10)
C15—H150.9300C56—H560.9300
C21—C221.344 (5)C28—H280.9300
C21—H210.9300C35—H350.9300
C20—C231.362 (5)C37—C381.427 (11)
C20—H200.9300C37—H370.9300
C24—C231.407 (5)C39—C381.433 (11)
C24—C221.412 (5)C39—H390.9300
C13—H130.9300C53—C521.366 (11)
C22—H220.9300C53—H530.9300
C9—C101.376 (5)C45—C461.363 (11)
C9—H90.9300C45—H450.9300
C11—C101.372 (6)C55—H550.9300
C11—H110.9300C51—C521.343 (10)
C23—H230.9300C51—H510.9300
C10—H100.9300C32—C311.415 (13)
C16—C141.338 (5)C32—H320.9300
C16—H160.9300C46—C471.372 (11)
C14—H140.9300C46—H460.9300
C19—H19A0.9600C38—H380.9300
C19—H19B0.9600C47—H470.9300
C19—H19C0.9600C52—H520.9300
C58—C571.411 (7)C30—C311.393 (12)
C58—C481.413 (7)C30—H300.9300
C58—C441.416 (8)C31—H310.9300
O62—N71—O63121.0 (3)H18A—C18—H18B109.5
O62—N71—C1118.9 (3)N69—C18—H18C109.5
O63—N71—C1120.1 (3)H18A—C18—H18C109.5
C8—O64—H64109.5H18B—C18—H18C109.5
C12—O67—H67109.5C41—C42—C33124.0 (7)
C20—N72—C21119.5 (3)C41—C42—C29120.1 (6)
C20—N72—H72120.2C33—C42—C29115.9 (7)
C21—N72—H72120.2C49—C48—C47122.1 (8)
C17—N69—C19122.0 (3)C49—C48—C58117.4 (6)
C17—N69—C18120.7 (3)C47—C48—C58120.5 (7)
C19—N69—C18117.2 (3)N73—C26—H26A109.5
C6—C1—C2123.7 (3)N73—C26—H26B109.5
C6—C1—N71118.9 (3)H26A—C26—H26B109.5
C2—C1—N71117.4 (3)N73—C26—H26C109.5
C14—N68—C13119.2 (4)H26A—C26—H26C109.5
C14—N68—H68120.4H26B—C26—H26C109.5
C13—N68—H68120.4C28—C27—C40119.2 (7)
O61—C2—C3123.0 (3)C28—C27—H27120.4
O61—C2—C1121.1 (3)C40—C27—H27120.4
C3—C2—C1115.9 (3)C51—C59—C57118.3 (7)
O60—C6—C5121.9 (3)C51—C59—C50123.6 (7)
O60—C6—C1121.4 (3)C57—C59—C50118.1 (6)
C5—C6—C1116.7 (3)C55—C54—C53123.7 (8)
O66—N70—O65123.5 (6)C55—C54—C57117.3 (7)
O66—N70—C7118.3 (6)C53—C54—C57118.9 (7)
O65—N70—C7118.2 (5)N73—C25—H25A109.5
C24—N73—C26121.8 (4)N73—C25—H25B109.5
C24—N73—C25120.4 (4)H25A—C25—H25B109.5
C26—N73—C25117.8 (4)N73—C25—H25C109.5
C4—C3—C2120.9 (3)H25A—C25—H25C109.5
C4—C3—H3119.6H25B—C25—H25C109.5
C2—C3—H3119.6C45—C44—C58119.4 (8)
O64—C8—C9124.4 (3)C45—C44—C56123.4 (8)
O64—C8—C7118.8 (3)C58—C44—C56117.1 (7)
C9—C8—C7116.8 (3)C30—C29—C28122.7 (9)
C8—C7—C12124.2 (3)C30—C29—C42120.1 (8)
C8—C7—N70118.1 (3)C28—C29—C42117.2 (7)
C12—C7—N70117.7 (3)C37—C36—C41122.8 (8)
C4—C5—C6120.9 (3)C37—C36—C35120.5 (10)
C4—C5—H5119.5C41—C36—C35116.7 (8)
C6—C5—H5119.5C32—C33—C42126.2 (10)
C5—C4—C3121.8 (4)C32—C33—C34119.7 (9)
C5—C4—H4119.1C42—C33—C34114.1 (8)
C3—C4—H4119.1C35—C34—C33121.4 (8)
O67—C12—C11125.4 (3)C35—C34—H34119.3
O67—C12—C7117.5 (3)C33—C34—H34119.3
C11—C12—C7117.0 (3)C50—C49—C48121.5 (7)
N69—C17—C15122.0 (4)C50—C49—H49119.2
N69—C17—C16122.0 (4)C48—C49—H49119.2
C15—C17—C16116.0 (4)C49—C50—C59122.7 (7)
C13—C15—C17120.1 (4)C49—C50—H50118.6
C13—C15—H15119.9C59—C50—H50118.6
C17—C15—H15119.9C39—C40—C41120.9 (9)
N72—C21—C22121.7 (4)C39—C40—C27121.6 (9)
N72—C21—H21119.2C41—C40—C27117.5 (7)
C22—C21—H21119.2C55—C56—C44121.5 (7)
N72—C20—C23122.4 (4)C55—C56—H56119.2
N72—C20—H20118.8C44—C56—H56119.2
C23—C20—H20118.8C27—C28—C29125.0 (8)
N73—C24—C23121.9 (4)C27—C28—H28117.5
N73—C24—C22122.1 (4)C29—C28—H28117.5
C23—C24—C22116.0 (4)C34—C35—C36122.5 (9)
N68—C13—C15121.9 (4)C34—C35—H35118.7
N68—C13—H13119.0C36—C35—H35118.7
C15—C13—H13119.0C36—C37—C38117.0 (9)
C21—C22—C24120.7 (4)C36—C37—H37121.5
C21—C22—H22119.6C38—C37—H37121.5
C24—C22—H22119.6C40—C39—C38120.8 (9)
C10—C9—C8120.2 (4)C40—C39—H39119.6
C10—C9—H9119.9C38—C39—H39119.6
C8—C9—H9119.9C52—C53—C54118.1 (8)
C12—C11—C10120.5 (4)C52—C53—H53120.9
C12—C11—H11119.8C54—C53—H53120.9
C10—C11—H11119.8C46—C45—C44120.4 (9)
C20—C23—C24119.6 (4)C46—C45—H45119.8
C20—C23—H23120.2C44—C45—H45119.8
C24—C23—H23120.2C56—C55—C54122.9 (8)
C11—C10—C9121.3 (4)C56—C55—H55118.5
C11—C10—H10119.3C54—C55—H55118.5
C9—C10—H10119.3C52—C51—C59120.1 (9)
C14—C16—C17119.7 (4)C52—C51—H51119.9
C14—C16—H16120.1C59—C51—H51119.9
C17—C16—H16120.1C33—C32—C31114.8 (11)
N68—C14—C16123.0 (4)C33—C32—H32122.6
N68—C14—H14118.5C31—C32—H32122.6
C16—C14—H14118.5C45—C46—C47122.7 (10)
N69—C19—H19A109.5C45—C46—H46118.7
N69—C19—H19B109.5C47—C46—H46118.7
H19A—C19—H19B109.5C37—C38—C39120.7 (10)
N69—C19—H19C109.5C37—C38—H38119.7
H19A—C19—H19C109.5C39—C38—H38119.7
H19B—C19—H19C109.5C46—C47—C48118.3 (8)
C57—C58—C48122.2 (5)C46—C47—H47120.9
C57—C58—C44119.1 (6)C48—C47—H47120.9
C48—C58—C44118.7 (7)C51—C52—C53124.4 (9)
C58—C57—C54121.9 (6)C51—C52—H52117.8
C58—C57—C59118.0 (6)C53—C52—H52117.8
C54—C57—C59120.2 (6)C29—C30—C31119.5 (10)
C42—C41—C36121.3 (6)C29—C30—H30120.3
C42—C41—C40120.9 (7)C31—C30—H30120.3
C36—C41—C40117.8 (7)C30—C31—C32123.5 (11)
N69—C18—H18A109.5C30—C31—H31118.3
N69—C18—H18B109.5C32—C31—H31118.3
(15NRES-TMP-DPE-I) top
Crystal data top
C40H46N8O8Z = 1
Mr = 766.85F(000) = 406
Triclinic, P1Dx = 1.338 Mg m3
a = 7.5319 (7) ÅMo Kα radiation, λ = 0.71075 Å
b = 8.6425 (8) ÅCell parameters from 9035 reflections
c = 15.3925 (14) Åθ = 3.0–27.5°
α = 78.729 (6)°µ = 0.10 mm1
β = 75.782 (5)°T = 150 K
γ = 89.099 (6)°Block, yellow
V = 951.99 (15) Å30.20 × 0.20 × 0.20 mm
Data collection top
Rigaku Mercury375R (2x2 bin mode)
diffractometer
3565 reflections with I > 2σ(I)
Radiation source: Sealed TubeRint = 0.023
profile data from ω–scansθmax = 27.5°, θmin = 3.0°
Absorption correction: multi-scan
Jacobson, R. (1998) Private communication
h = 99
Tmin = 0.887, Tmax = 1.000k = 1111
9956 measured reflectionsl = 1919
4348 independent reflections
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.043H-atom parameters constrained
wR(F2) = 0.124 w = 1/[σ2(Fo2) + (0.0593P)2 + 0.3903P]
where P = (Fo2 + 2Fc2)/3
S = 1.07(Δ/σ)max = 0.032
4348 reflectionsΔρmax = 0.34 e Å3
257 parametersΔρmin = 0.33 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O20.74232 (14)0.39058 (12)0.11433 (7)0.0209 (2)
H20.6561140.3542330.1000210.031*
O41.09634 (15)0.60447 (14)0.10504 (8)0.0295 (3)
O10.90113 (15)0.72439 (14)0.28963 (8)0.0291 (3)
H10.8610900.7836120.3249820.044*
O31.05902 (15)0.42111 (14)0.22552 (8)0.0319 (3)
N41.00179 (16)0.52678 (14)0.17525 (8)0.0187 (3)
N20.79637 (17)0.90020 (14)0.41860 (9)0.0212 (3)
N30.70851 (17)1.09154 (15)0.54523 (9)0.0217 (3)
N10.47151 (17)0.22009 (15)0.08590 (9)0.0223 (3)
C20.80734 (18)0.56332 (16)0.20322 (9)0.0172 (3)
C30.7619 (2)0.66648 (17)0.26358 (10)0.0202 (3)
C10.67929 (19)0.49019 (16)0.17162 (9)0.0176 (3)
C60.4957 (2)0.52497 (18)0.20210 (10)0.0216 (3)
H60.4055320.4786850.1827060.026*
C80.80473 (19)0.84553 (17)0.50524 (10)0.0209 (3)
C90.76027 (19)0.94317 (18)0.56908 (10)0.0208 (3)
C190.15438 (19)0.08327 (18)0.06372 (10)0.0195 (3)
C150.3473 (2)0.30740 (18)0.05113 (10)0.0232 (3)
H150.3687150.4160890.0340770.028*
C170.2838 (2)0.00883 (18)0.09885 (10)0.0229 (3)
H170.2665330.1179470.1155580.027*
C40.5774 (2)0.70031 (18)0.29286 (10)0.0229 (3)
H40.5415600.7695340.3327440.028*
C50.4486 (2)0.62885 (18)0.26140 (11)0.0235 (3)
H50.3257960.6516040.2809080.028*
C160.4379 (2)0.06370 (19)0.10860 (10)0.0236 (3)
H160.5229130.0005990.1321770.028*
C130.74639 (19)1.04844 (17)0.39377 (10)0.0201 (3)
C120.70169 (19)1.14479 (17)0.45881 (10)0.0203 (3)
C180.1893 (2)0.24508 (18)0.03924 (10)0.0226 (3)
H180.1071410.3109150.0150440.027*
C200.0153 (2)0.01207 (19)0.04939 (10)0.0225 (3)
H20A0.1169160.0811970.0626920.027*
H20B0.0467700.0886780.0911950.027*
C140.7450 (2)1.1043 (2)0.29547 (11)0.0291 (4)
H14A0.7910681.0238000.2616460.044*
H14B0.8210611.1984640.2707020.044*
H14C0.6218351.1266060.2910930.044*
C110.6494 (2)1.31371 (18)0.43376 (12)0.0293 (4)
H11A0.5991141.3533130.4884620.044*
H11B0.5597101.3188300.3985590.044*
H11C0.7561461.3765760.3982950.044*
C70.8638 (2)0.67898 (19)0.52806 (13)0.0311 (4)
H7A0.7598320.6076220.5416230.047*
H7B0.9147170.6670030.5802840.047*
H7C0.9546210.6557640.4768800.047*
C100.7688 (2)0.8892 (2)0.66667 (11)0.0327 (4)
H10A0.7429640.9756510.6981460.049*
H10B0.8890080.8524940.6684990.049*
H10C0.6797460.8048710.6958200.049*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O20.0170 (5)0.0256 (5)0.0241 (5)0.0004 (4)0.0073 (4)0.0118 (4)
O40.0213 (6)0.0337 (6)0.0277 (6)0.0007 (5)0.0005 (5)0.0004 (5)
O10.0238 (6)0.0347 (6)0.0364 (6)0.0000 (5)0.0096 (5)0.0225 (5)
O30.0214 (6)0.0353 (7)0.0361 (7)0.0064 (5)0.0110 (5)0.0045 (5)
N40.0172 (6)0.0195 (6)0.0219 (6)0.0010 (5)0.0072 (5)0.0072 (5)
N20.0203 (6)0.0205 (6)0.0241 (7)0.0016 (5)0.0063 (5)0.0061 (5)
N30.0206 (6)0.0223 (6)0.0215 (6)0.0002 (5)0.0034 (5)0.0047 (5)
N10.0192 (6)0.0288 (7)0.0216 (6)0.0025 (5)0.0066 (5)0.0092 (5)
C20.0143 (6)0.0182 (7)0.0194 (7)0.0007 (5)0.0044 (5)0.0040 (5)
C30.0218 (7)0.0192 (7)0.0212 (7)0.0007 (5)0.0072 (6)0.0051 (5)
C10.0183 (7)0.0179 (7)0.0170 (7)0.0003 (5)0.0058 (5)0.0026 (5)
C60.0168 (7)0.0241 (7)0.0250 (7)0.0007 (5)0.0077 (6)0.0043 (6)
C80.0171 (7)0.0190 (7)0.0264 (8)0.0020 (5)0.0066 (6)0.0021 (6)
C90.0161 (7)0.0241 (7)0.0215 (7)0.0007 (5)0.0046 (5)0.0028 (6)
C190.0183 (7)0.0254 (7)0.0167 (7)0.0036 (5)0.0043 (5)0.0081 (5)
C150.0232 (7)0.0225 (7)0.0245 (8)0.0048 (6)0.0063 (6)0.0049 (6)
C170.0257 (8)0.0215 (7)0.0230 (7)0.0016 (6)0.0081 (6)0.0056 (6)
C40.0240 (8)0.0209 (7)0.0242 (8)0.0033 (6)0.0040 (6)0.0079 (6)
C50.0161 (7)0.0264 (8)0.0256 (8)0.0027 (6)0.0021 (6)0.0033 (6)
C160.0229 (7)0.0284 (8)0.0226 (7)0.0023 (6)0.0092 (6)0.0082 (6)
C130.0184 (7)0.0203 (7)0.0223 (7)0.0034 (5)0.0066 (6)0.0032 (6)
C120.0167 (7)0.0191 (7)0.0241 (7)0.0006 (5)0.0046 (6)0.0026 (6)
C180.0225 (7)0.0246 (8)0.0224 (7)0.0018 (6)0.0089 (6)0.0046 (6)
C200.0190 (7)0.0277 (8)0.0224 (8)0.0066 (6)0.0060 (6)0.0071 (6)
C140.0338 (9)0.0302 (8)0.0246 (8)0.0026 (7)0.0120 (7)0.0019 (6)
C110.0308 (9)0.0201 (8)0.0365 (9)0.0048 (6)0.0090 (7)0.0036 (6)
C70.0316 (9)0.0210 (8)0.0417 (10)0.0047 (6)0.0128 (7)0.0037 (7)
C100.0347 (9)0.0388 (10)0.0237 (8)0.0008 (7)0.0099 (7)0.0003 (7)
Geometric parameters (Å, º) top
O2—C11.3500 (17)C15—H150.9300
O2—H20.8200C17—C161.381 (2)
O4—N41.2162 (16)C17—H170.9300
O1—C31.3465 (17)C4—C51.387 (2)
O1—H10.8200C4—H40.9300
O3—N41.2223 (16)C5—H50.9300
N4—C21.4693 (18)C16—H160.9300
N2—C131.3391 (19)C13—C121.400 (2)
N2—C81.3415 (19)C13—C141.498 (2)
N3—C121.3331 (19)C12—C111.507 (2)
N3—C91.3423 (19)C18—H180.9300
N1—C161.340 (2)C20—C20i1.536 (3)
N1—C151.341 (2)C20—H20A0.9700
C2—C31.390 (2)C20—H20B0.9700
C2—C11.3914 (19)C14—H14A0.9600
C3—C41.397 (2)C14—H14B0.9600
C1—C61.395 (2)C14—H14C0.9600
C6—C51.384 (2)C11—H11A0.9600
C6—H60.9300C11—H11B0.9600
C8—C91.394 (2)C11—H11C0.9600
C8—C71.501 (2)C7—H7A0.9600
C9—C101.500 (2)C7—H7B0.9600
C19—C181.387 (2)C7—H7C0.9600
C19—C171.394 (2)C10—H10A0.9600
C19—C201.5090 (19)C10—H10B0.9600
C15—C181.380 (2)C10—H10C0.9600
C1—O2—H2109.5N1—C16—H16118.2
C3—O1—H1109.5C17—C16—H16118.2
O4—N4—O3124.07 (13)N2—C13—C12119.62 (13)
O4—N4—C2118.56 (12)N2—C13—C14117.43 (13)
O3—N4—C2117.36 (12)C12—C13—C14122.94 (14)
C13—N2—C8119.87 (13)N3—C12—C13121.07 (13)
C12—N3—C9118.73 (13)N3—C12—C11117.26 (13)
C16—N1—C15116.70 (13)C13—C12—C11121.65 (14)
C3—C2—C1123.72 (13)C15—C18—C19119.34 (14)
C3—C2—N4116.85 (12)C15—C18—H18120.3
C1—C2—N4119.38 (12)C19—C18—H18120.3
O1—C3—C2116.59 (13)C19—C20—C20i110.92 (15)
O1—C3—C4125.43 (13)C19—C20—H20A109.5
C2—C3—C4117.97 (13)C20i—C20—H20A109.5
O2—C1—C2117.47 (12)C19—C20—H20B109.5
O2—C1—C6125.16 (13)C20i—C20—H20B109.5
C2—C1—C6117.37 (13)H20A—C20—H20B108.0
C5—C6—C1119.55 (13)C13—C14—H14A109.5
C5—C6—H6120.2C13—C14—H14B109.5
C1—C6—H6120.2H14A—C14—H14B109.5
N2—C8—C9119.78 (13)C13—C14—H14C109.5
N2—C8—C7117.04 (14)H14A—C14—H14C109.5
C9—C8—C7123.18 (14)H14B—C14—H14C109.5
N3—C9—C8120.93 (13)C12—C11—H11A109.5
N3—C9—C10116.87 (14)C12—C11—H11B109.5
C8—C9—C10122.20 (14)H11A—C11—H11B109.5
C18—C19—C17117.45 (13)C12—C11—H11C109.5
C18—C19—C20120.28 (13)H11A—C11—H11C109.5
C17—C19—C20122.23 (13)H11B—C11—H11C109.5
N1—C15—C18123.69 (14)C8—C7—H7A109.5
N1—C15—H15118.2C8—C7—H7B109.5
C18—C15—H15118.2H7A—C7—H7B109.5
C16—C17—C19119.28 (14)C8—C7—H7C109.5
C16—C17—H17120.4H7A—C7—H7C109.5
C19—C17—H17120.4H7B—C7—H7C109.5
C5—C4—C3118.84 (14)C9—C10—H10A109.5
C5—C4—H4120.6C9—C10—H10B109.5
C3—C4—H4120.6H10A—C10—H10B109.5
C6—C5—C4122.54 (14)C9—C10—H10C109.5
C6—C5—H5118.7H10A—C10—H10C109.5
C4—C5—H5118.7H10B—C10—H10C109.5
N1—C16—C17123.52 (14)
Symmetry code: (i) x, y, z.
(16NRES-TMP-22BP) top
Crystal data top
C38H42N8O8Z = 1
Mr = 738.79F(000) = 390
Triclinic, P1Dx = 1.318 Mg m3
a = 7.4104 (7) ÅMo Kα radiation, λ = 0.71073 Å
b = 8.8964 (9) ÅCell parameters from 8594 reflections
c = 15.7722 (15) Åθ = 3.0–27.5°
α = 95.531 (7)°µ = 0.10 mm1
β = 101.446 (7)°T = 150 K
γ = 111.676 (8)°Block, yellow
V = 930.47 (17) Å30.20 × 0.20 × 0.20 mm
Data collection top
Rigaku Mercury375R (2x2 bin mode)
diffractometer
3261 reflections with I > 2σ(I)
Radiation source: Sealed TubeRint = 0.027
profile data from ω–scansθmax = 27.5°, θmin = 3.0°
Absorption correction: multi-scan
Jacobson, R. (1998) Private communication
h = 99
Tmin = 0.850, Tmax = 1.000k = 1111
9757 measured reflectionsl = 2020
4270 independent reflections
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.052H-atom parameters constrained
wR(F2) = 0.150 w = 1/[σ2(Fo2) + (0.0713P)2 + 0.439P]
where P = (Fo2 + 2Fc2)/3
S = 1.06(Δ/σ)max < 0.001
4270 reflectionsΔρmax = 0.64 e Å3
248 parametersΔρmin = 0.29 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O10.6072 (2)0.54850 (19)0.39526 (11)0.0435 (4)
O20.6668 (2)0.75298 (18)0.32810 (11)0.0417 (4)
O30.33133 (19)0.37213 (15)0.21274 (9)0.0304 (3)
H30.2545440.2975270.1718920.046*
O40.36697 (18)0.80485 (15)0.41924 (8)0.0280 (3)
H40.3006360.8520080.4362260.042*
N40.5521 (2)0.63146 (17)0.34811 (9)0.0228 (3)
C150.3358 (2)0.5858 (2)0.31408 (11)0.0204 (3)
C160.2297 (3)0.4542 (2)0.24416 (11)0.0221 (4)
C170.2482 (2)0.6802 (2)0.35159 (11)0.0214 (4)
C180.0265 (3)0.4174 (2)0.20989 (12)0.0261 (4)
H180.0487870.3308660.1627320.031*
C190.0623 (3)0.5108 (2)0.24662 (12)0.0260 (4)
H190.1978320.4853790.2233930.031*
C200.0443 (3)0.6404 (2)0.31671 (12)0.0252 (4)
H200.0192110.7005730.3403900.030*
N10.0879 (2)0.12529 (19)0.07224 (10)0.0289 (4)
C70.2525 (3)0.3251 (2)0.01269 (15)0.0401 (5)
H7A0.2665130.4011100.0381380.060*
H7B0.1930970.3545560.0648170.060*
H7C0.3822170.3288670.0156180.060*
C80.1197 (3)0.1531 (2)0.00606 (13)0.0294 (4)
C90.0316 (3)0.0262 (2)0.08106 (13)0.0271 (4)
C100.0658 (3)0.0514 (3)0.16873 (13)0.0362 (5)
H10A0.0042280.0524020.2088020.054*
H10B0.0079920.1251670.1901180.054*
H10C0.2074220.0976570.1642420.054*
N20.5635 (2)1.1208 (2)0.10899 (11)0.0312 (4)
C10.4262 (3)0.9491 (3)0.20808 (13)0.0331 (4)
H10.4135470.9383800.2649240.040*
C20.3378 (3)0.8147 (3)0.14009 (14)0.0377 (5)
H20.2600650.7121030.1500720.045*
C30.3657 (3)0.8337 (2)0.05689 (13)0.0315 (4)
H3A0.3078940.7442010.0104360.038*
C40.4808 (2)0.9877 (2)0.04417 (11)0.0240 (4)
C50.5335 (3)1.0991 (2)0.18930 (13)0.0313 (4)
H50.5884331.1907280.2344470.038*
N30.1436 (2)0.94649 (17)0.48337 (9)0.0216 (3)
C110.0386 (3)0.7194 (2)0.56171 (14)0.0334 (4)
H11A0.1542650.7081070.5481740.050*
H11B0.0791370.6223770.5331870.050*
H11C0.0545730.7332420.6242500.050*
C120.0171 (3)0.8669 (2)0.52969 (11)0.0223 (4)
C130.1294 (3)1.0790 (2)0.45359 (11)0.0221 (4)
C140.2786 (3)1.1669 (2)0.40453 (13)0.0307 (4)
H14A0.3581031.2773340.4361100.046*
H14B0.2086991.1699200.3469600.046*
H14C0.3643761.1098190.3991340.046*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0278 (7)0.0473 (9)0.0535 (9)0.0152 (7)0.0007 (7)0.0215 (7)
O20.0198 (7)0.0404 (8)0.0657 (10)0.0089 (6)0.0138 (7)0.0195 (7)
O30.0257 (7)0.0276 (7)0.0330 (7)0.0119 (6)0.0022 (5)0.0106 (5)
O40.0212 (6)0.0301 (7)0.0296 (7)0.0118 (5)0.0032 (5)0.0084 (5)
N40.0187 (7)0.0233 (7)0.0253 (7)0.0093 (6)0.0047 (6)0.0022 (6)
C150.0156 (7)0.0214 (8)0.0228 (8)0.0068 (6)0.0038 (6)0.0020 (6)
C160.0224 (8)0.0200 (8)0.0237 (8)0.0083 (7)0.0067 (7)0.0013 (6)
C170.0199 (8)0.0204 (8)0.0228 (8)0.0074 (7)0.0061 (7)0.0011 (6)
C180.0220 (8)0.0221 (8)0.0274 (9)0.0049 (7)0.0011 (7)0.0002 (7)
C190.0158 (8)0.0271 (9)0.0318 (9)0.0064 (7)0.0035 (7)0.0043 (7)
C200.0201 (8)0.0270 (9)0.0310 (9)0.0119 (7)0.0076 (7)0.0033 (7)
N10.0267 (8)0.0291 (8)0.0291 (8)0.0123 (7)0.0039 (6)0.0016 (6)
C70.0453 (12)0.0266 (10)0.0401 (12)0.0048 (9)0.0136 (10)0.0016 (8)
C80.0274 (9)0.0350 (10)0.0320 (10)0.0175 (8)0.0098 (8)0.0095 (8)
C90.0209 (8)0.0246 (9)0.0354 (10)0.0115 (7)0.0027 (7)0.0026 (7)
C100.0387 (11)0.0426 (12)0.0296 (10)0.0198 (10)0.0075 (8)0.0044 (9)
N20.0270 (8)0.0310 (8)0.0308 (8)0.0078 (7)0.0038 (7)0.0065 (7)
C10.0324 (10)0.0416 (11)0.0300 (10)0.0167 (9)0.0117 (8)0.0117 (8)
C20.0415 (11)0.0325 (11)0.0373 (11)0.0096 (9)0.0120 (9)0.0155 (9)
C30.0358 (10)0.0255 (9)0.0296 (10)0.0085 (8)0.0073 (8)0.0058 (7)
C40.0176 (8)0.0269 (9)0.0280 (9)0.0091 (7)0.0045 (7)0.0091 (7)
C50.0310 (10)0.0346 (10)0.0272 (9)0.0132 (8)0.0047 (8)0.0057 (8)
N30.0237 (7)0.0212 (7)0.0189 (7)0.0095 (6)0.0041 (5)0.0009 (5)
C110.0394 (11)0.0293 (10)0.0372 (11)0.0188 (9)0.0097 (9)0.0111 (8)
C120.0248 (8)0.0211 (8)0.0185 (8)0.0082 (7)0.0032 (6)0.0005 (6)
C130.0253 (8)0.0205 (8)0.0181 (8)0.0083 (7)0.0042 (6)0.0011 (6)
C140.0331 (10)0.0319 (10)0.0291 (10)0.0117 (8)0.0136 (8)0.0079 (8)
Geometric parameters (Å, º) top
O1—N41.213 (2)C8—C9i1.412 (3)
O2—N41.218 (2)C9—C101.478 (3)
O3—C161.353 (2)N2—C41.344 (2)
O4—C171.349 (2)N2—C51.348 (2)
N4—C151.469 (2)C1—C51.374 (3)
C15—C161.390 (2)C1—C21.380 (3)
C15—C171.392 (2)C2—C31.385 (3)
C16—C181.394 (2)C3—C41.379 (3)
C17—C201.396 (2)C4—C4ii1.497 (3)
C18—C191.386 (3)N3—C121.340 (2)
C19—C201.382 (3)N3—C131.342 (2)
N1—C81.332 (2)C11—C121.502 (2)
N1—C91.350 (2)C12—C13iii1.398 (2)
C7—C81.509 (3)C13—C141.500 (2)
O1—N4—O2123.57 (15)N1—C9—C8i118.63 (17)
O1—N4—C15118.77 (15)N1—C9—C10118.49 (17)
O2—N4—C15117.65 (14)C8i—C9—C10122.88 (18)
C16—C15—C17123.10 (15)C4—N2—C5117.49 (16)
C16—C15—N4118.63 (14)C5—C1—C2118.02 (18)
C17—C15—N4118.23 (14)C1—C2—C3119.53 (19)
O3—C16—C15117.79 (15)C4—C3—C2118.79 (18)
O3—C16—C18124.29 (15)N2—C4—C3122.52 (17)
C15—C16—C18117.91 (15)N2—C4—C4ii117.07 (19)
O4—C17—C15117.56 (14)C3—C4—C4ii120.4 (2)
O4—C17—C20124.41 (15)N2—C5—C1123.59 (18)
C15—C17—C20118.03 (15)C12—N3—C13119.53 (15)
C19—C18—C16119.51 (16)N3—C12—C13iii120.24 (15)
C20—C19—C18122.07 (16)N3—C12—C11117.65 (15)
C19—C20—C17119.37 (16)C13iii—C12—C11122.11 (16)
C8—N1—C9120.16 (16)N3—C13—C12iii120.23 (16)
N1—C8—C9i121.21 (18)N3—C13—C14117.49 (15)
N1—C8—C7118.12 (17)C12iii—C13—C14122.27 (16)
C9i—C8—C7120.67 (18)
Symmetry codes: (i) x, y, z; (ii) x+1, y+2, z; (iii) x, y+2, z+1.
(17NRE-TMP-22TBP) top
Crystal data top
C22H23N3O4S2Z = 2
Mr = 457.55F(000) = 480
Triclinic, P1Dx = 1.371 Mg m3
a = 7.6512 (11) ÅMo Kα radiation, λ = 0.71075 Å
b = 8.9495 (13) ÅCell parameters from 9432 reflections
c = 18.121 (3) Åθ = 3.0–27.7°
α = 87.883 (6)°µ = 0.27 mm1
β = 78.725 (6)°T = 150 K
γ = 65.728 (5)°Block, colorless
V = 1108.0 (3) Å30.20 × 0.20 × 0.20 mm
Data collection top
Rigaku Mercury375R (2x2 bin mode)
diffractometer
3698 reflections with I > 2σ(I)
Radiation source: Sealed TubeRint = 0.039
profile data from ω–scansθmax = 27.5°, θmin = 3.0°
Absorption correction: multi-scan
Jacobson, R. (1998) Private communication
h = 99
Tmin = 0.805, Tmax = 1.000k = 1111
11118 measured reflectionsl = 2323
5059 independent reflections
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.067H-atom parameters constrained
wR(F2) = 0.206 w = 1/[σ2(Fo2) + (0.1022P)2 + 1.3547P]
where P = (Fo2 + 2Fc2)/3
S = 1.07(Δ/σ)max < 0.001
5059 reflectionsΔρmax = 0.93 e Å3
286 parametersΔρmin = 0.79 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S21.09372 (13)0.15221 (11)0.59467 (5)0.0363 (3)
S10.77371 (16)0.24729 (13)1.00457 (7)0.0509 (3)
O10.3983 (3)0.3740 (3)0.64814 (13)0.0288 (5)
H10.4019610.3149660.6137820.043*
O20.0179 (3)0.7223 (3)0.85409 (12)0.0285 (5)
H20.1296660.7586990.8789930.043*
O40.4648 (3)0.4560 (3)0.79685 (15)0.0378 (6)
N20.3433 (3)0.5694 (3)0.77070 (13)0.0195 (5)
N10.6362 (3)0.8868 (3)0.94558 (13)0.0184 (5)
O30.3512 (4)0.7021 (3)0.76095 (17)0.0431 (7)
N30.4442 (3)0.1301 (3)0.55041 (13)0.0219 (5)
C201.0204 (4)0.0623 (3)0.89161 (16)0.0204 (6)
H201.1183170.0257640.8616180.024*
C20.1796 (4)0.5466 (3)0.75046 (15)0.0171 (5)
C90.5137 (4)1.0333 (3)0.92630 (16)0.0197 (6)
C10.0056 (4)0.6289 (3)0.79521 (16)0.0196 (6)
C80.6242 (4)0.8510 (3)1.01825 (15)0.0187 (6)
C60.1620 (4)0.6081 (3)0.77621 (16)0.0214 (6)
H60.2873710.6608460.8049630.026*
C30.2144 (4)0.4446 (3)0.68839 (16)0.0209 (6)
C130.4317 (4)0.1561 (4)0.47811 (16)0.0226 (6)
C120.5110 (4)0.0244 (4)0.57306 (16)0.0227 (6)
C40.0552 (4)0.4263 (4)0.66999 (17)0.0247 (6)
H40.0726580.3598180.6285180.030*
C50.1288 (4)0.5080 (4)0.71407 (17)0.0236 (6)
H50.2340870.4951670.7014430.028*
C160.8646 (5)0.1493 (4)0.58579 (18)0.0286 (7)
H160.7923470.2499060.5676100.034*
C70.7596 (4)0.6845 (4)1.03695 (17)0.0260 (6)
H7A0.8327410.6199460.9912350.039*
H7B0.6849220.6315261.0664190.039*
H7C0.8480530.6952771.0651960.039*
C150.9822 (4)0.0104 (4)0.54077 (18)0.0257 (6)
C170.8665 (5)0.1210 (4)0.6639 (2)0.0326 (7)
H170.7938500.2012640.7022550.039*
C100.5312 (5)1.0644 (4)0.84435 (17)0.0302 (7)
H10A0.6369320.9718500.8160760.045*
H10B0.5563331.1606980.8350040.045*
H10C0.4114051.0806730.8292040.045*
C180.9843 (5)0.0340 (4)0.6762 (2)0.0339 (7)
H181.0037020.0721420.7236780.041*
C110.5196 (5)0.0479 (4)0.65492 (17)0.0329 (7)
H11A0.4904470.0553160.6793650.049*
H11B0.6482680.1247840.6596180.049*
H11C0.4255080.0893000.6781300.049*
C140.3532 (5)0.3308 (4)0.4552 (2)0.0363 (8)
H14A0.3206840.4031310.4983950.054*
H14B0.2382480.3542300.4349750.054*
H14C0.4506520.3468310.4176410.054*
C190.9611 (5)0.0636 (4)0.9744 (2)0.0327 (7)
C220.7748 (7)0.3176 (5)0.9174 (3)0.0617 (14)
H220.6893730.4213020.9066090.074*
C210.9102 (9)0.2096 (7)0.8658 (3)0.0670 (15)
H210.9291190.2325680.8150780.080*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S20.0316 (4)0.0284 (4)0.0374 (5)0.0022 (3)0.0046 (3)0.0073 (3)
S10.0463 (6)0.0443 (6)0.0662 (7)0.0189 (5)0.0213 (5)0.0113 (5)
O10.0197 (10)0.0316 (12)0.0296 (12)0.0081 (9)0.0050 (8)0.0168 (9)
O20.0180 (10)0.0364 (13)0.0264 (11)0.0090 (9)0.0044 (8)0.0162 (9)
O40.0313 (12)0.0367 (13)0.0522 (15)0.0157 (11)0.0229 (11)0.0196 (11)
N20.0152 (11)0.0206 (12)0.0189 (12)0.0047 (9)0.0003 (9)0.0004 (9)
N10.0172 (11)0.0172 (11)0.0180 (12)0.0054 (9)0.0000 (9)0.0030 (9)
O30.0330 (13)0.0276 (13)0.079 (2)0.0184 (11)0.0216 (13)0.0135 (13)
N30.0209 (12)0.0235 (12)0.0184 (12)0.0070 (10)0.0013 (9)0.0039 (9)
C200.0359 (16)0.0151 (13)0.0201 (13)0.0192 (12)0.0077 (12)0.0007 (10)
C20.0134 (12)0.0179 (13)0.0187 (13)0.0058 (10)0.0020 (10)0.0005 (10)
C90.0193 (13)0.0195 (13)0.0199 (14)0.0082 (11)0.0016 (10)0.0024 (11)
C10.0180 (13)0.0164 (13)0.0204 (14)0.0043 (10)0.0003 (10)0.0023 (10)
C80.0150 (12)0.0178 (13)0.0205 (14)0.0045 (10)0.0016 (10)0.0024 (10)
C60.0137 (12)0.0201 (14)0.0258 (15)0.0038 (11)0.0004 (11)0.0008 (11)
C30.0167 (13)0.0201 (14)0.0218 (14)0.0055 (11)0.0012 (10)0.0021 (11)
C130.0219 (14)0.0238 (15)0.0203 (14)0.0078 (11)0.0036 (11)0.0007 (11)
C120.0210 (14)0.0287 (15)0.0187 (14)0.0107 (12)0.0031 (11)0.0009 (12)
C40.0236 (14)0.0259 (15)0.0237 (15)0.0097 (12)0.0018 (11)0.0083 (12)
C50.0192 (13)0.0247 (15)0.0280 (15)0.0094 (12)0.0059 (11)0.0011 (12)
C160.0267 (15)0.0244 (15)0.0343 (17)0.0099 (13)0.0067 (13)0.0014 (13)
C70.0240 (15)0.0206 (14)0.0270 (16)0.0026 (12)0.0051 (12)0.0001 (12)
C150.0187 (14)0.0252 (15)0.0331 (17)0.0085 (12)0.0069 (12)0.0067 (12)
C170.0359 (18)0.0313 (17)0.0335 (18)0.0170 (14)0.0058 (14)0.0006 (14)
C100.0334 (17)0.0317 (17)0.0190 (15)0.0082 (14)0.0023 (12)0.0002 (12)
C180.0335 (17)0.0350 (18)0.0341 (18)0.0153 (15)0.0070 (14)0.0073 (14)
C110.0452 (19)0.0401 (19)0.0172 (15)0.0203 (16)0.0089 (13)0.0020 (13)
C140.044 (2)0.0275 (17)0.0332 (18)0.0086 (15)0.0116 (15)0.0019 (14)
C190.0405 (18)0.0281 (17)0.0420 (19)0.0208 (15)0.0223 (15)0.0093 (14)
C220.067 (3)0.037 (2)0.107 (4)0.028 (2)0.063 (3)0.029 (3)
C210.119 (5)0.069 (3)0.054 (3)0.066 (4)0.053 (3)0.029 (3)
Geometric parameters (Å, º) top
S2—C181.705 (4)C13—C141.502 (4)
S2—C151.732 (3)C12—C111.501 (4)
S1—C221.678 (5)C4—C51.382 (4)
S1—C191.697 (4)C4—H40.9300
O1—C31.346 (3)C5—H50.9300
O1—H10.8200C16—C151.374 (4)
O2—C11.345 (3)C16—C171.431 (5)
O2—H20.8200C16—H160.9300
O4—N21.216 (3)C7—H7A0.9600
N2—O31.219 (3)C7—H7B0.9600
N2—C21.463 (3)C7—H7C0.9600
N1—C81.338 (4)C15—C15iii1.454 (6)
N1—C91.342 (4)C17—C181.347 (5)
N3—C131.337 (4)C17—H170.9300
N3—C121.342 (4)C10—H10A0.9600
C20—C211.365 (6)C10—H10B0.9600
C20—C191.479 (5)C10—H10C0.9600
C20—H200.9300C18—H180.9300
C2—C31.389 (4)C11—H11A0.9600
C2—C11.394 (4)C11—H11B0.9600
C9—C8i1.400 (4)C11—H11C0.9600
C9—C101.491 (4)C14—H14A0.9600
C1—C61.390 (4)C14—H14B0.9600
C8—C71.497 (4)C14—H14C0.9600
C6—C51.382 (4)C19—C19iv1.446 (6)
C6—H60.9300C22—C211.322 (8)
C3—C41.396 (4)C22—H220.9300
C13—C12ii1.392 (4)C21—H210.9300
C18—S2—C1592.07 (16)C17—C16—H16124.0
C22—S1—C1993.1 (2)C8—C7—H7A109.5
C3—O1—H1109.5C8—C7—H7B109.5
C1—O2—H2109.5H7A—C7—H7B109.5
O4—N2—O3122.8 (3)C8—C7—H7C109.5
O4—N2—C2118.9 (2)H7A—C7—H7C109.5
O3—N2—C2118.3 (2)H7B—C7—H7C109.5
C8—N1—C9119.6 (2)C16—C15—C15iii128.5 (4)
C13—N3—C12119.1 (3)C16—C15—S2110.7 (2)
C21—C20—C19109.9 (3)C15iii—C15—S2120.8 (3)
C21—C20—H20125.0C18—C17—C16113.0 (3)
C19—C20—H20125.0C18—C17—H17123.5
C3—C2—C1123.0 (3)C16—C17—H17123.5
C3—C2—N2119.1 (2)C9—C10—H10A109.5
C1—C2—N2117.9 (2)C9—C10—H10B109.5
N1—C9—C8i120.4 (3)H10A—C10—H10B109.5
N1—C9—C10117.1 (2)C9—C10—H10C109.5
C8i—C9—C10122.5 (3)H10A—C10—H10C109.5
O2—C1—C6125.1 (2)H10B—C10—H10C109.5
O2—C1—C2116.7 (2)C17—C18—S2112.2 (3)
C6—C1—C2118.2 (3)C17—C18—H18123.9
N1—C8—C9i120.0 (2)S2—C18—H18123.9
N1—C8—C7117.8 (2)C12—C11—H11A109.5
C9i—C8—C7122.2 (3)C12—C11—H11B109.5
C5—C6—C1119.2 (3)H11A—C11—H11B109.5
C5—C6—H6120.4C12—C11—H11C109.5
C1—C6—H6120.4H11A—C11—H11C109.5
O1—C3—C2118.0 (2)H11B—C11—H11C109.5
O1—C3—C4124.0 (3)C13—C14—H14A109.5
C2—C3—C4117.9 (2)C13—C14—H14B109.5
N3—C13—C12ii120.4 (3)H14A—C14—H14B109.5
N3—C13—C14117.5 (3)C13—C14—H14C109.5
C12ii—C13—C14122.1 (3)H14A—C14—H14C109.5
N3—C12—C13ii120.5 (3)H14B—C14—H14C109.5
N3—C12—C11117.4 (3)C19iv—C19—C20129.2 (4)
C13ii—C12—C11122.1 (3)C19iv—C19—S1122.2 (4)
C5—C4—C3119.3 (3)C20—C19—S1108.5 (2)
C5—C4—H4120.3C21—C22—S1112.7 (3)
C3—C4—H4120.3C21—C22—H22123.6
C6—C5—C4122.4 (3)S1—C22—H22123.6
C6—C5—H5118.8C22—C21—C20115.7 (4)
C4—C5—H5118.8C22—C21—H21122.2
C15—C16—C17112.1 (3)C20—C21—H21122.2
C15—C16—H16124.0
Symmetry codes: (i) x+1, y+2, z+2; (ii) x+1, y, z+1; (iii) x+2, y, z+1; (iv) x+2, y, z+2.
(18NRES-TMP-PYR-ACR) top
Crystal data top
C62H50N6O8Z = 1
Mr = 1007.08F(000) = 528
Triclinic, P1Dx = 1.379 Mg m3
a = 7.6840 (18) ÅMo Kα radiation, λ = 0.71073 Å
b = 9.266 (2) ÅCell parameters from 8502 reflections
c = 18.043 (4) Åθ = 3.0–28.2°
α = 96.343 (7)°µ = 0.09 mm1
β = 94.419 (7)°T = 150 K
γ = 107.054 (7)°Block, yellow
V = 1212.6 (5) Å30.20 × 0.20 × 0.20 mm
Data collection top
Rigaku Mercury375R (2x2 bin mode)
diffractometer
2857 reflections with I > 2σ(I)
Radiation source: Sealed TubeRint = 0.092
profile data from ω–scansθmax = 27.5°, θmin = 3.0°
Absorption correction: multi-scan
Jacobson, R. (1998) Private communication
h = 99
Tmin = 0.600, Tmax = 1.000k = 1212
12080 measured reflectionsl = 2323
5501 independent reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.086 w = 1/[σ2(Fo2) + (0.1336P)2]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.254(Δ/σ)max < 0.001
S = 0.95Δρmax = 0.60 e Å3
5501 reflectionsΔρmin = 0.52 e Å3
348 parametersExtinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.008 (3)
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C120.3986 (4)0.0782 (4)0.62510 (17)0.0294 (8)
H120.4721910.0007070.6606980.035*
C40.1211 (5)0.2104 (4)0.35485 (18)0.0328 (8)
H40.0731860.2366070.3112090.039*
N10.3446 (3)0.1032 (3)0.54927 (13)0.0231 (6)
C230.4342 (5)0.1425 (4)0.85978 (18)0.0332 (8)
H230.4593980.2338100.8398400.040*
O20.8896 (3)0.6054 (3)0.86315 (12)0.0344 (6)
H2A0.8798970.6765270.8921980.052*
O10.6141 (3)0.2941 (3)0.63979 (12)0.0317 (6)
H10.5161770.2510940.6138580.048*
N30.9075 (3)0.4172 (3)0.73826 (13)0.0249 (6)
C280.1367 (5)0.0178 (4)0.84754 (17)0.0352 (8)
H28A0.1735190.1222670.8245300.053*
H28B0.0438040.0422020.8212570.053*
H28C0.2406610.0197250.8453780.053*
C310.0661 (5)0.2799 (4)0.94073 (18)0.0361 (8)
H31A0.1172290.3622620.9809530.054*
H31B0.0460560.2889710.9173770.054*
H31C0.1514630.2837020.9043060.054*
N20.0884 (3)0.1366 (3)0.95681 (14)0.0281 (6)
C50.0873 (4)0.0624 (4)0.36312 (17)0.0311 (8)
H50.0152530.0122160.3252280.037*
O31.0112 (3)0.5027 (3)0.70384 (15)0.0510 (8)
O40.9380 (3)0.3068 (3)0.75920 (15)0.0472 (7)
C130.3170 (4)0.0428 (4)0.55916 (16)0.0241 (7)
C270.4649 (4)0.0021 (4)0.96269 (16)0.0248 (7)
C70.1316 (4)0.1305 (4)0.43997 (16)0.0256 (7)
H70.0598280.2084830.4034790.031*
C300.0283 (4)0.1321 (4)0.97105 (16)0.0270 (7)
C290.0624 (4)0.0071 (4)0.92751 (17)0.0267 (7)
C220.5044 (4)0.1417 (4)0.93314 (17)0.0274 (7)
C190.5855 (4)0.3765 (3)0.70048 (16)0.0236 (7)
C10.2699 (4)0.1364 (4)0.48630 (17)0.0246 (7)
C90.1869 (4)0.3169 (4)0.51880 (18)0.0307 (8)
H90.1181810.3980060.4831940.037*
C80.2082 (4)0.1667 (4)0.50465 (17)0.0251 (7)
C180.4211 (4)0.4007 (4)0.71390 (17)0.0276 (7)
H180.3160170.3540340.6805210.033*
C60.1596 (4)0.0185 (4)0.42869 (16)0.0247 (7)
C20.3011 (4)0.2905 (4)0.47550 (18)0.0284 (7)
H20.3718730.3678650.5124930.034*
C110.3724 (5)0.2223 (4)0.63741 (18)0.0348 (8)
H110.4251750.2422260.6817540.042*
C140.7368 (4)0.4466 (3)0.75300 (16)0.0217 (7)
C30.2289 (5)0.3264 (4)0.41188 (18)0.0306 (8)
H30.2502770.4281190.4055680.037*
C150.7318 (4)0.5427 (3)0.81698 (16)0.0261 (7)
C260.3542 (4)0.1348 (4)0.91779 (17)0.0285 (7)
C170.4155 (5)0.4958 (4)0.77792 (18)0.0309 (8)
H170.3045750.5119240.7868420.037*
C250.2879 (4)0.1268 (4)0.84461 (17)0.0323 (8)
H250.2155340.2153790.8145090.039*
C100.2642 (5)0.3454 (4)0.58304 (19)0.0359 (8)
H100.2468340.4454830.5917750.043*
C160.5679 (4)0.5676 (4)0.82901 (17)0.0296 (8)
H160.5597350.6320030.8710550.036*
C200.6839 (4)0.2734 (4)1.05002 (19)0.0330 (8)
H200.7576350.3634331.0785880.040*
C210.6163 (5)0.2772 (4)0.97978 (19)0.0331 (8)
H210.6426400.3697970.9609940.040*
C240.3273 (5)0.0089 (4)0.81623 (18)0.0356 (8)
H240.2817280.0111480.7672460.043*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C120.0340 (18)0.0346 (19)0.0188 (15)0.0101 (15)0.0031 (14)0.0007 (14)
C40.043 (2)0.038 (2)0.0195 (16)0.0155 (16)0.0005 (15)0.0070 (15)
N10.0268 (13)0.0226 (14)0.0168 (12)0.0053 (11)0.0003 (11)0.0019 (11)
C230.039 (2)0.035 (2)0.0276 (18)0.0142 (16)0.0049 (16)0.0071 (16)
O20.0346 (13)0.0311 (14)0.0281 (12)0.0077 (10)0.0128 (10)0.0179 (10)
O10.0302 (12)0.0329 (13)0.0220 (12)0.0029 (10)0.0049 (10)0.0144 (10)
N30.0306 (15)0.0227 (14)0.0164 (13)0.0049 (12)0.0050 (11)0.0039 (11)
C280.045 (2)0.034 (2)0.0226 (17)0.0120 (16)0.0039 (15)0.0069 (15)
C310.050 (2)0.0283 (19)0.0254 (17)0.0076 (16)0.0003 (16)0.0011 (15)
N20.0332 (15)0.0264 (15)0.0182 (13)0.0042 (12)0.0029 (12)0.0073 (11)
C50.0325 (18)0.036 (2)0.0199 (16)0.0072 (15)0.0015 (14)0.0032 (15)
O30.0393 (15)0.0627 (19)0.0620 (18)0.0193 (14)0.0224 (14)0.0327 (16)
O40.0473 (15)0.0385 (16)0.0638 (18)0.0222 (13)0.0077 (14)0.0155 (14)
C130.0288 (17)0.0245 (17)0.0169 (15)0.0076 (13)0.0012 (13)0.0034 (13)
C270.0273 (16)0.0281 (18)0.0194 (16)0.0102 (14)0.0043 (14)0.0007 (14)
C70.0265 (16)0.0246 (17)0.0199 (15)0.0035 (13)0.0011 (13)0.0070 (13)
C300.0313 (17)0.0305 (18)0.0175 (15)0.0092 (14)0.0017 (13)0.0020 (14)
C290.0331 (18)0.0275 (18)0.0165 (15)0.0086 (14)0.0011 (13)0.0059 (13)
C220.0300 (17)0.0298 (18)0.0226 (16)0.0096 (14)0.0056 (14)0.0013 (14)
C190.0308 (17)0.0180 (16)0.0178 (15)0.0051 (13)0.0021 (13)0.0049 (12)
C10.0251 (16)0.0273 (17)0.0195 (15)0.0069 (13)0.0020 (13)0.0023 (13)
C90.0359 (18)0.0226 (17)0.0306 (18)0.0052 (14)0.0085 (15)0.0025 (14)
C80.0270 (16)0.0232 (17)0.0217 (16)0.0051 (13)0.0036 (13)0.0048 (13)
C180.0294 (17)0.0234 (17)0.0242 (16)0.0040 (14)0.0078 (13)0.0027 (13)
C60.0256 (16)0.0280 (17)0.0168 (15)0.0053 (13)0.0011 (13)0.0038 (13)
C20.0314 (17)0.0251 (17)0.0256 (17)0.0054 (14)0.0038 (14)0.0009 (14)
C110.044 (2)0.042 (2)0.0243 (17)0.0197 (17)0.0061 (16)0.0101 (16)
C140.0229 (15)0.0186 (15)0.0193 (15)0.0021 (12)0.0008 (12)0.0018 (12)
C30.0405 (19)0.0250 (18)0.0282 (17)0.0120 (15)0.0058 (15)0.0052 (14)
C150.0299 (17)0.0211 (16)0.0205 (16)0.0032 (13)