Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S2056989014028047/sj5435sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S2056989014028047/sj5435Isup2.hkl |
CCDC reference: 1040897
Key indicators
- Single-crystal synchrotron study
- T = 100 K
- Mean (C-C) = 0.003 Å
- R factor = 0.034
- wR factor = 0.091
- Data-to-parameter ratio = 21.0
checkCIF/PLATON results
No syntax errors found
Alert level B PLAT029_ALERT_3_B _diffrn_measured_fraction_theta_full Low ....... 0.943 Note
Alert level C PLAT430_ALERT_2_C Short Inter D...A Contact O1 .. O1 .. 2.89 Ang. PLAT911_ALERT_3_C Missing # FCF Refl Between THmin & STh/L= 0.600 125 Report
Alert level G ABSMU01_ALERT_1_G Calculation of _exptl_absorpt_correction_mu not performed for this radiation type. PLAT007_ALERT_5_G Number of Unrefined Donor-H Atoms .............. 2 Report PLAT066_ALERT_1_G Predicted and Reported Tmin&Tmax Range Identical ? Check PLAT154_ALERT_1_G The su's on the Cell Angles are Equal .......... 0.03000 Degree PLAT180_ALERT_4_G Check Cell Rounding: # of Values Ending with 0 = 3 PLAT232_ALERT_2_G Hirshfeld Test Diff (M-X) Cu1 -- O2 .. 8.1 su PLAT793_ALERT_4_G The Model has Chirality at N1 ............. S Verify PLAT793_ALERT_4_G The Model has Chirality at N2 ............. R Verify PLAT794_ALERT_5_G Tentative Bond Valency for Cu1 (II) ..... 2.17 Note PLAT912_ALERT_4_G Missing # of FCF Reflections Above STh/L= 0.600 120 Note PLAT984_ALERT_1_G The Cu-f'= 0.355 Deviates from the B&C-Value 0.338 Check
0 ALERT level A = Most likely a serious problem - resolve or explain 1 ALERT level B = A potentially serious problem, consider carefully 2 ALERT level C = Check. Ensure it is not caused by an omission or oversight 11 ALERT level G = General information/check it is not something unexpected 4 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 2 ALERT type 2 Indicator that the structure model may be wrong or deficient 2 ALERT type 3 Indicator that the structure quality may be low 4 ALERT type 4 Improvement, methodology, query or suggestion 2 ALERT type 5 Informative message, check
Coordination compounds with macrocyclic ligands have attracted considerable attention in chemistry, biological chemistry and materials science (Lehn, 1995). In particular, macrocyclic CuII complexes with vacant sites in the axial positions are good building blocks for assembling multi-dimensional frameworks (Ko et al., 2002), with potential applications as metal extractants, radiotherapeutic materials and as medical imaging agents (Sowen et al., 2013). For example, CuII complexes with tetra-azamacrocyclic ligands have been studied with various auxiliary anionic ligands such as ferricyanide and hexacyanochromate and their biological redox-sensing and magnetic properties (Xiang et al., 2009) have been investigated. Moreover, the perchlorate ion is a versatile anion which can easily bridge two transition metal complexes, allowing the assembly of multi-dimensional compounds (Kwak et al., 2001). Here, we report the synthesis and crystal structure of a CuII azamacrocyclic complex, trans-diperchlorato(1,8-dibutyl-1,3,6,8,10,13-hexaazacyclotetradecane)copper(II), which has two perchlorate ions coordinated in the axial positions in the six-coordinate complex.
In the title compound, the coordination environment around the CuII ion, which lies on an inversion centre, is tetragonally distorted octahedral. The copper(II) ion binds to the four secondary N atoms of the azamacrocyclic ligand in a square-planar fashion in the equatorial plane, with two O atoms from the perchlorate anions in axial positions as shown in Fig. 1. The bonds to the two axially located perchlorate anions are significantly longer than those to the donor N atoms in the equatorial plane. This can be attributed either to a rather large Jahn–Teller distortion of the CuII ion and/or to a considerable ring contraction of the azamacrocyclic ligand (Halcrow, 2013). The six-membered chelate rings adopt chair conformations and the five-membered chelate rings assume gauche conformations (Min & Suh, 2001). Intramolecular N—H···O hydrogen bonds between the secondary amine groups of the azamacrocyclic ligand and an O atom of each perchlorate ion contribute to the molecular conformation (Fig. 1 and Table 1).
Each complex molecule forms three N—H···O and two C—H···O hydrogen bonds (Steed & Atwood, 2009), as shown in Table 1, Fig. 2. Sheets of complex molecules form in the ab plane, Fig. 3, and additional C6—H6B···O3 contacts link these sheets into a three-dimensional network.
A search of the Cambridge Structural Database (Version 5.35, May 2014 with three updates; Groom & Allen 2014) indicated that 51 azamacrocyclic CuII complexes with pendant alkyl groups had been reported previously. These complexes have been studied as good building blocks for supramolecular chemistry and contain a variety of pendant alkyl groups (Cho et al., 2003). Their magnetic properties and guest-exchange effects with cyano groups and carboxylic acid groups as ligands have also been investigated (Ko et al., 2002; Zhou et al., 2014). No corresponding azamacrocyclic CuII complex with pendant butyl groups has been reported and the title compound was newly synthesized for this research.
The title compound was prepared as follows. Ethylenediamine (3.4 ml, 0.05 mol), paraformaldehyde (3.0 g, 0.10 mol), and butylamine (3.7 g, 0.05 mol) were slowly added to a stirred solution of CuCl2·2H2O (4.26 g, 0.025 mol) in MeOH (50 ml). The mixture was heated to reflux for 1 day. The solution was filtered and cooled at room temperature. HClO4 (70%, 15 ml) was added to the purple solution. A bright-purple precipitate formed and was filtered off, washed with H2O, MeOH, and diethyl ether, and dried in air. Purple crystals of the title compound were obtained by diffusion of diethyl ether into the purple solution over several days. Yield: 2.38g (17%). FT–IR (ATR, cm-1): 3240, 2936, 1443, 1053, 995, 962, 746. Safety note: Although we have experienced no problems with the compound reported in this study, perchlorate salts of metal complexes are often explosive and should be handled with great caution.
Crystal data, data collection and structure refinement details are summarized in Table 3. All H atoms were placed in geometrically idealized positions and constrained to ride on their parent atoms, with C—H distances of 0.98–0.99 Å and an N—H distance of 1.0 Å with Uiso(H) values of 1.2 or 1.5 Ueq of the parent atoms.
Data collection: PAL ADSC Quantum-210 ADX (Arvai & Nielsen, 1983); cell refinement: HKL3000sm (Otwinowski & Minor, 1997); data reduction: HKL3000sm (Otwinowski & Minor, 1997); program(s) used to solve structure: SHELXT2014 (Sheldrick, 2008); program(s) used to refine structure: SHELXL2014 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 2012); software used to prepare material for publication: publCIF (Westrip, 2010).
[Cu(ClO4)2(C16H38N6)] | Z = 1 |
Mr = 576.96 | F(000) = 303 |
Triclinic, P1 | Dx = 1.571 Mg m−3 |
a = 8.2230 (16) Å | Synchrotron radiation, λ = 0.62998 Å |
b = 8.3600 (17) Å | Cell parameters from 16838 reflections |
c = 10.039 (2) Å | θ = 0.4–33.6° |
α = 92.87 (3)° | µ = 0.84 mm−1 |
β = 96.12 (3)° | T = 100 K |
γ = 116.60 (3)° | Plate, purple |
V = 609.8 (3) Å3 | 0.10 × 0.10 × 0.03 mm |
ADSC Q210 CCD area-detector diffractometer | 2536 reflections with I > 2σ(I) |
Radiation source: PLSII 2D bending magnet | Rint = 0.025 |
ω scans | θmax = 26.0°, θmin = 1.8° |
Absorption correction: empirical (using intensity measurements) (HKL3000sm SCALEPACK; Otwinowski & Minor, 1997) | h = −11→11 |
Tmin = 0.921, Tmax = 0.975 | k = −11→11 |
6292 measured reflections | l = −13→13 |
3195 independent reflections |
Refinement on F2 | 0 restraints |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.034 | H-atom parameters constrained |
wR(F2) = 0.091 | w = 1/[σ2(Fo2) + (0.0574P)2] where P = (Fo2 + 2Fc2)/3 |
S = 1.02 | (Δ/σ)max = 0.001 |
3195 reflections | Δρmax = 0.29 e Å−3 |
152 parameters | Δρmin = −0.86 e Å−3 |
[Cu(ClO4)2(C16H38N6)] | γ = 116.60 (3)° |
Mr = 576.96 | V = 609.8 (3) Å3 |
Triclinic, P1 | Z = 1 |
a = 8.2230 (16) Å | Synchrotron radiation, λ = 0.62998 Å |
b = 8.3600 (17) Å | µ = 0.84 mm−1 |
c = 10.039 (2) Å | T = 100 K |
α = 92.87 (3)° | 0.10 × 0.10 × 0.03 mm |
β = 96.12 (3)° |
ADSC Q210 CCD area-detector diffractometer | 3195 independent reflections |
Absorption correction: empirical (using intensity measurements) (HKL3000sm SCALEPACK; Otwinowski & Minor, 1997) | 2536 reflections with I > 2σ(I) |
Tmin = 0.921, Tmax = 0.975 | Rint = 0.025 |
6292 measured reflections |
R[F2 > 2σ(F2)] = 0.034 | 0 restraints |
wR(F2) = 0.091 | H-atom parameters constrained |
S = 1.02 | Δρmax = 0.29 e Å−3 |
3195 reflections | Δρmin = −0.86 e Å−3 |
152 parameters |
Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes. |
x | y | z | Uiso*/Ueq | ||
Cu1 | 0.5000 | 0.5000 | 0.5000 | 0.01063 (10) | |
N1 | 0.7678 (2) | 0.6261 (2) | 0.57656 (16) | 0.0119 (3) | |
H1 | 0.8221 | 0.5443 | 0.5535 | 0.014* | |
N2 | 0.4291 (2) | 0.3507 (2) | 0.65492 (16) | 0.0123 (3) | |
H2 | 0.4599 | 0.2490 | 0.6389 | 0.015* | |
N3 | 0.7247 (2) | 0.5222 (2) | 0.80108 (16) | 0.0152 (3) | |
C1 | 0.8525 (2) | 0.7860 (2) | 0.5034 (2) | 0.0155 (4) | |
H1A | 0.9876 | 0.8328 | 0.5156 | 0.019* | |
H1B | 0.8242 | 0.8821 | 0.5385 | 0.019* | |
C2 | 0.8084 (3) | 0.6731 (3) | 0.7267 (2) | 0.0164 (4) | |
H2A | 0.9432 | 0.7303 | 0.7541 | 0.020* | |
H2B | 0.7654 | 0.7626 | 0.7508 | 0.020* | |
C3 | 0.5278 (3) | 0.4466 (3) | 0.7910 (2) | 0.0158 (4) | |
H3A | 0.4948 | 0.5445 | 0.8119 | 0.019* | |
H3B | 0.4855 | 0.3612 | 0.8594 | 0.019* | |
C4 | 0.2256 (2) | 0.2705 (3) | 0.6448 (2) | 0.0156 (4) | |
H4A | 0.1894 | 0.3598 | 0.6819 | 0.019* | |
H4B | 0.1786 | 0.1649 | 0.6964 | 0.019* | |
C5 | 0.8000 (3) | 0.3919 (3) | 0.7910 (2) | 0.0169 (4) | |
H5A | 0.9359 | 0.4586 | 0.8041 | 0.020* | |
H5B | 0.7593 | 0.3265 | 0.6992 | 0.020* | |
C6 | 0.7409 (3) | 0.2567 (3) | 0.8931 (2) | 0.0177 (4) | |
H6A | 0.6067 | 0.1782 | 0.8721 | 0.021* | |
H6B | 0.7662 | 0.3217 | 0.9840 | 0.021* | |
C7 | 0.8401 (3) | 0.1406 (3) | 0.8937 (2) | 0.0221 (4) | |
H7A | 0.9723 | 0.2171 | 0.9266 | 0.026* | |
H7B | 0.8289 | 0.0888 | 0.8003 | 0.026* | |
C8 | 0.7636 (3) | −0.0116 (3) | 0.9822 (2) | 0.0215 (4) | |
H8A | 0.7749 | 0.0390 | 1.0749 | 0.032* | |
H8B | 0.8328 | −0.0812 | 0.9806 | 0.032* | |
H8C | 0.6338 | −0.0904 | 0.9481 | 0.032* | |
Cl1 | 0.32457 (6) | 0.78356 (6) | 0.65025 (4) | 0.01406 (11) | |
O1 | 0.1610 (2) | 0.6610 (2) | 0.56090 (18) | 0.0282 (4) | |
O2 | 0.48300 (19) | 0.77847 (19) | 0.60352 (16) | 0.0221 (3) | |
O3 | 0.3102 (3) | 0.7249 (2) | 0.78200 (16) | 0.0319 (4) | |
O4 | 0.3413 (2) | 0.96148 (19) | 0.65392 (18) | 0.0285 (4) |
U11 | U22 | U33 | U12 | U13 | U23 | |
Cu1 | 0.00685 (15) | 0.00798 (15) | 0.01599 (17) | 0.00179 (11) | 0.00383 (11) | 0.00327 (12) |
N1 | 0.0092 (7) | 0.0080 (6) | 0.0180 (8) | 0.0032 (5) | 0.0030 (5) | 0.0031 (6) |
N2 | 0.0091 (6) | 0.0114 (7) | 0.0184 (8) | 0.0053 (5) | 0.0054 (6) | 0.0044 (6) |
N3 | 0.0152 (7) | 0.0159 (8) | 0.0170 (8) | 0.0091 (6) | 0.0028 (6) | 0.0022 (6) |
C1 | 0.0082 (8) | 0.0091 (8) | 0.0275 (10) | 0.0015 (6) | 0.0051 (7) | 0.0069 (7) |
C2 | 0.0143 (8) | 0.0125 (8) | 0.0208 (10) | 0.0052 (7) | 0.0009 (7) | 0.0000 (7) |
C3 | 0.0156 (9) | 0.0176 (9) | 0.0176 (9) | 0.0100 (7) | 0.0050 (7) | 0.0034 (8) |
C4 | 0.0094 (8) | 0.0141 (8) | 0.0253 (10) | 0.0047 (7) | 0.0096 (7) | 0.0101 (8) |
C5 | 0.0148 (8) | 0.0199 (9) | 0.0202 (9) | 0.0112 (7) | 0.0039 (7) | 0.0046 (8) |
C6 | 0.0197 (9) | 0.0191 (9) | 0.0194 (10) | 0.0124 (8) | 0.0057 (7) | 0.0059 (8) |
C7 | 0.0186 (9) | 0.0242 (10) | 0.0295 (11) | 0.0133 (8) | 0.0081 (8) | 0.0100 (9) |
C8 | 0.0242 (10) | 0.0202 (10) | 0.0244 (11) | 0.0133 (8) | 0.0050 (8) | 0.0054 (8) |
Cl1 | 0.0128 (2) | 0.0121 (2) | 0.0198 (2) | 0.00762 (17) | 0.00396 (16) | 0.00067 (18) |
O1 | 0.0152 (7) | 0.0258 (8) | 0.0420 (10) | 0.0115 (6) | −0.0050 (6) | −0.0127 (7) |
O2 | 0.0132 (6) | 0.0216 (7) | 0.0332 (8) | 0.0088 (6) | 0.0086 (6) | −0.0005 (6) |
O3 | 0.0450 (10) | 0.0412 (10) | 0.0225 (8) | 0.0280 (8) | 0.0144 (7) | 0.0124 (8) |
O4 | 0.0297 (8) | 0.0123 (7) | 0.0490 (11) | 0.0132 (6) | 0.0101 (7) | 0.0047 (7) |
Cu1—N1 | 2.0073 (17) | C4—C1i | 1.518 (3) |
Cu1—N1i | 2.0073 (17) | C4—H4A | 0.9900 |
Cu1—N2i | 2.0131 (17) | C4—H4B | 0.9900 |
Cu1—N2 | 2.0131 (17) | C5—C6 | 1.515 (3) |
N1—C1 | 1.478 (2) | C5—H5A | 0.9900 |
N1—C2 | 1.501 (3) | C5—H5B | 0.9900 |
N1—H1 | 1.0000 | C6—C7 | 1.522 (3) |
N2—C4 | 1.487 (2) | C6—H6A | 0.9900 |
N2—C3 | 1.496 (3) | C6—H6B | 0.9900 |
N2—H2 | 1.0000 | C7—C8 | 1.523 (3) |
N3—C2 | 1.432 (2) | C7—H7A | 0.9900 |
N3—C3 | 1.440 (2) | C7—H7B | 0.9900 |
N3—C5 | 1.478 (2) | C8—H8A | 0.9800 |
C1—C4i | 1.518 (3) | C8—H8B | 0.9800 |
C1—H1A | 0.9900 | C8—H8C | 0.9800 |
C1—H1B | 0.9900 | Cl1—O4 | 1.4293 (15) |
C2—H2A | 0.9900 | Cl1—O3 | 1.4318 (17) |
C2—H2B | 0.9900 | Cl1—O1 | 1.4420 (17) |
C3—H3A | 0.9900 | Cl1—O2 | 1.4481 (14) |
C3—H3B | 0.9900 | ||
N1—Cu1—N1i | 180.00 (9) | H3A—C3—H3B | 107.7 |
N1—Cu1—N2i | 86.45 (7) | N2—C4—C1i | 107.28 (15) |
N1i—Cu1—N2i | 93.55 (7) | N2—C4—H4A | 110.3 |
N1—Cu1—N2 | 93.55 (7) | C1i—C4—H4A | 110.3 |
N1i—Cu1—N2 | 86.45 (7) | N2—C4—H4B | 110.3 |
N2i—Cu1—N2 | 180.0 | C1i—C4—H4B | 110.3 |
C1—N1—C2 | 112.37 (15) | H4A—C4—H4B | 108.5 |
C1—N1—Cu1 | 106.33 (11) | N3—C5—C6 | 113.14 (15) |
C2—N1—Cu1 | 115.28 (12) | N3—C5—H5A | 109.0 |
C1—N1—H1 | 107.5 | C6—C5—H5A | 109.0 |
C2—N1—H1 | 107.5 | N3—C5—H5B | 109.0 |
Cu1—N1—H1 | 107.5 | C6—C5—H5B | 109.0 |
C4—N2—C3 | 113.49 (15) | H5A—C5—H5B | 107.8 |
C4—N2—Cu1 | 106.73 (11) | C5—C6—C7 | 112.19 (16) |
C3—N2—Cu1 | 115.29 (12) | C5—C6—H6A | 109.2 |
C4—N2—H2 | 107.0 | C7—C6—H6A | 109.2 |
C3—N2—H2 | 107.0 | C5—C6—H6B | 109.2 |
Cu1—N2—H2 | 107.0 | C7—C6—H6B | 109.2 |
C2—N3—C3 | 114.81 (15) | H6A—C6—H6B | 107.9 |
C2—N3—C5 | 114.08 (15) | C6—C7—C8 | 112.45 (16) |
C3—N3—C5 | 116.15 (16) | C6—C7—H7A | 109.1 |
N1—C1—C4i | 107.87 (15) | C8—C7—H7A | 109.1 |
N1—C1—H1A | 110.1 | C6—C7—H7B | 109.1 |
C4i—C1—H1A | 110.1 | C8—C7—H7B | 109.1 |
N1—C1—H1B | 110.1 | H7A—C7—H7B | 107.8 |
C4i—C1—H1B | 110.1 | C7—C8—H8A | 109.5 |
H1A—C1—H1B | 108.4 | C7—C8—H8B | 109.5 |
N3—C2—N1 | 114.03 (15) | H8A—C8—H8B | 109.5 |
N3—C2—H2A | 108.7 | C7—C8—H8C | 109.5 |
N1—C2—H2A | 108.7 | H8A—C8—H8C | 109.5 |
N3—C2—H2B | 108.7 | H8B—C8—H8C | 109.5 |
N1—C2—H2B | 108.7 | O4—Cl1—O3 | 110.11 (11) |
H2A—C2—H2B | 107.6 | O4—Cl1—O1 | 109.74 (10) |
N3—C3—N2 | 113.39 (15) | O3—Cl1—O1 | 108.36 (11) |
N3—C3—H3A | 108.9 | O4—Cl1—O2 | 110.65 (10) |
N2—C3—H3A | 108.9 | O3—Cl1—O2 | 108.82 (10) |
N3—C3—H3B | 108.9 | O1—Cl1—O2 | 109.12 (9) |
N2—C3—H3B | 108.9 | ||
C2—N1—C1—C4i | −169.53 (14) | C4—N2—C3—N3 | 179.24 (14) |
Cu1—N1—C1—C4i | −42.53 (15) | Cu1—N2—C3—N3 | −57.23 (18) |
C3—N3—C2—N1 | −69.8 (2) | C3—N2—C4—C1i | 168.24 (15) |
C5—N3—C2—N1 | 67.8 (2) | Cu1—N2—C4—C1i | 40.14 (16) |
C1—N1—C2—N3 | 178.48 (14) | C2—N3—C5—C6 | 167.34 (16) |
Cu1—N1—C2—N3 | 56.43 (18) | C3—N3—C5—C6 | −55.6 (2) |
C2—N3—C3—N2 | 70.2 (2) | N3—C5—C6—C7 | −172.24 (17) |
C5—N3—C3—N2 | −66.5 (2) | C5—C6—C7—C8 | −172.38 (18) |
Symmetry code: (i) −x+1, −y+1, −z+1. |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1···O1ii | 1.00 | 2.50 | 3.136 (2) | 121 |
N2—H2···O4iii | 1.00 | 2.17 | 3.000 (2) | 139 |
C1—H1A···O1ii | 0.99 | 2.46 | 3.160 (2) | 127 |
N1—H1···O1i | 1.00 | 2.08 | 3.018 (2) | 155 |
C6—H6B···O3iv | 0.99 | 2.50 | 3.338 (3) | 142 |
Symmetry codes: (i) −x+1, −y+1, −z+1; (ii) x+1, y, z; (iii) x, y−1, z; (iv) −x+1, −y+1, −z+2. |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1···O1i | 1.00 | 2.50 | 3.136 (2) | 121.3 |
N2—H2···O4ii | 1.00 | 2.17 | 3.000 (2) | 139.0 |
C1—H1A···O1i | 0.99 | 2.46 | 3.160 (2) | 127.1 |
N1—H1···O1iii | 1.00 | 2.08 | 3.018 (2) | 154.9 |
C6—H6B···O3iv | 0.99 | 2.50 | 3.338 (3) | 142.1 |
Symmetry codes: (i) x+1, y, z; (ii) x, y−1, z; (iii) −x+1, −y+1, −z+1; (iv) −x+1, −y+1, −z+2. |
Experimental details
Crystal data | |
Chemical formula | [Cu(ClO4)2(C16H38N6)] |
Mr | 576.96 |
Crystal system, space group | Triclinic, P1 |
Temperature (K) | 100 |
a, b, c (Å) | 8.2230 (16), 8.3600 (17), 10.039 (2) |
α, β, γ (°) | 92.87 (3), 96.12 (3), 116.60 (3) |
V (Å3) | 609.8 (3) |
Z | 1 |
Radiation type | Synchrotron, λ = 0.62998 Å |
µ (mm−1) | 0.84 |
Crystal size (mm) | 0.10 × 0.10 × 0.03 |
Data collection | |
Diffractometer | ADSC Q210 CCD area-detector diffractometer |
Absorption correction | Empirical (using intensity measurements) (HKL3000sm SCALEPACK; Otwinowski & Minor, 1997) |
Tmin, Tmax | 0.921, 0.975 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 6292, 3195, 2536 |
Rint | 0.025 |
(sin θ/λ)max (Å−1) | 0.696 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.034, 0.091, 1.02 |
No. of reflections | 3195 |
No. of parameters | 152 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.29, −0.86 |
Computer programs: PAL ADSC Quantum-210 ADX (Arvai & Nielsen, 1983), HKL3000sm (Otwinowski & Minor, 1997), SHELXT2014 (Sheldrick, 2008), SHELXL2014 (Sheldrick, 2008), ORTEP-3 for Windows (Farrugia, 2012), publCIF (Westrip, 2010).