research communications
trans-(1,8-dibutyl-1,3,6,8,10,13-hexaazacyclotetradecane-κ4N3,N6,N10,N13)bis(thiocyanato-κN)nickel(II) from synchrotron data
ofaDepartment of Chemistry and Green-Nano Materials Research Center, Kyungpook National University, Daegu, 702-701, Republic of Korea, bDepartment of Applied Chemistry, College of Engineering, Kyungpook National University, Daegu, 702-701, Republic of Korea, and cBeamline Department, Pohang Accelerator Laboratory 80, Jigokro-127-beongil, Nam-Gu Pohang, Gyeongbuk 790-784, South Korea
*Correspondence e-mail: dmoon@postech.ac.kr
The 2(C16H38N6)], has been determined from synchrotron data. The consists of two halves of the complex molecules which have their NiII atoms located on inversion centres. The NiII ions show a tetragonally distorted octahedral coordination geometry, with four secondary amine N atoms of the azamacrocyclic ligand in the equatorial plane and two N atoms of the thiocyanate anions in the axial positions. The average equatorial Ni—N bond length [2.070 (5) Å] is shorter than the average axial Ni—N bond length [2.107 (18) Å]. Only half of the macrocyclic ligand N—H groups are involved in hydrogen bonding. The complex molecules are connected via intermolecular N—H⋯S hydrogen bonds into two symmetry-independent one-dimensional polymeric structures extending along the b-axis direction. One of the n-butyl substituents of the macrocycle exhibits with a refined occupancy ratio of 0.630:0.370.
of the title compound, [Ni(NCS)Keywords: crystal structure; azamacrocyclic ligand; Jahn–Teller distortion; sodium thiocyanate; hydrogen bonding; synchrotron data.
CCDC reference: 1405450
1. Chemical context
Coordination compounds, including those formed by macrocyclic ligands, have attracted wide interest of material sciences, because of their potential applications (Lehn, 1995; Zhou et al., 2012). In particular, NiII macrocyclic complexes having vacant sites in the axial positions have been used for the synthesis of new supramolecular materials with interesting properties, including chiral recognition (Ryoo et al., 2010) and gas storage (Suh et al., 2012). For example, NiII complexes with alkyl-substituted tetra-azamacrocyclic ligands and anionic tetrazole derivatives, metal cyanide and azide (Shen et al., 2012; Kim et al., 2015) have been studied as magnetic materials and substrates for crystal engineering. The thiocyanate ion is a versatile anionic ligand which can easily bind to a transition metal ion as a terminal or bridging ligand through the nitrogen and/or the sulfur atoms, thus allowing the assembly of multi-dimensional compounds or heterometallic complexes (Safarifard & Morsali, 2012; Wang & Wang, 2015). Here, we report the synthesis and of an NiII complex with an azamacrocycle ligand and two thiocyanate anions, trans-(1,8-dibutyl-1,3,6,8,10,13-hexaazacyclotetradecane-κ4N3,N6,N10,N13)bis(thiocyanato-κN)nickel(II) (I).
2. Structural commentary
The title compound (I) contains two crystallographically independent complex molecules that are centrosymmetric. Each NiII ion lies on an inversion centre and is coordinated by four secondary amine N atoms of the azamacrocyclic ligand in a square-planar fashion in the equatorial plane, and by two N atoms from the thiocyanate anions at the axial positions, resulting in a tetragonally distorted octahedral geometry, as shown in Fig. 1. The average equatorial bond lengths, Ni1A—Neq and Ni1B—Neq, are 2.070 (8) and 2.070 (3) Å, respectively. The axial bond lengths, Ni1A—Nax and Ni1B—Nax are 2.119 (1) and 2.093 (1) Å, respectively. The axial bonds are longer than the equatorial bonds, which can be attributed either to a large Jahn–Teller distortion effect of the NiII ion and/or to a ring contraction of the azamacrocyclic ligand (Halcrow, 2013; Kim et al., 2015). The average N—C and C—S bond lengths of the thiocyanate ligands are 1.157 (1) and 1.627 (11) Å, respectively. The former is very similar to a C≡N triple-bond length, while the latter is slightly shorter than reported C—S single-bond lengths (Bradforth et al., 1993; Shin et al., 2010). The six-membered chelate rings involving C2A, C3A and C2B, C3B atoms adopt a chair conformation, whereas the five-membered chelate rings involving C1A, C4A and C1B, C4B assume a gauche conformation (Min & Suh, 2001; Kim et al., 2015).
3. Supramolecular features
The S atoms of the thiocyanate groups form intermolecular N—H⋯S hydrogen bonds with adjacent secondary amine groups of the azamacrocyclic ligand, giving rise to two symmetry-independent one-dimensional polymeric chains propagating along the b-axis direction (Fig. 2 and Table 1).
4. Database survey
A search of the Cambridge Structural Database (Version 5.36, Feb 2015 with two updates; Groom & Allen, 2014) indicated one complex of NiII with the same azamaclocyclic ligand having an anionic tetrazole derivative at the axial positions (Kim et al., 2015).
5. Synthesis and crystallization
The title compound (I) was prepared as follows. The starting complex, [Ni(C16H38N6)](ClO4)2, was prepared by a slightly modified method reported by Jung et al. (1989). To a MeCN solution (10 mL) of [Ni(C16H38N6)](ClO4)2 (0.15 g, 0.26 mmol) was slowly added a MeCN solution (5 mL) containing sodium thiocyanate (0.042 g, 0.52 mmol) at room temperature. A pale-pink precipitate was formed, which was filtered off, washed with MeCN, and diethyl ether, and dried in air. Single crystals of the title compound were obtained by layering of the MeCN solution of sodium thiocyanate on the MeCN solution of [Ni(C16H38N6)](ClO4)2 for several days. Yield: 0.062 g (49%). FT–IR (KBr, cm−1): 3304, 3243, 2929, 2867, 2069, 1468, 1386, 1273, 1204, 1070, 925.
Safety note: Although we have experienced no problem with the compounds reported in this study, perchlorate salts of metal complexes are often explosive and should be handled with great caution.
6. Refinement
Crystal data, data collection and structure . 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 1.5Ueq of the parent atoms. The C7A and C8A atoms of the macrocyclic ligand were refined as disordered over two sets of sites (C71A, C72A and C81A, C82A) with refined occupancies of 0.630 and 0.370, respectively. The bond lengths and angles of the disordered part were restrained to ensure proper geometry using DFIX and DANG instructions of SHELXL2014 (Sheldrick, 2015b).
details are summarized in Table 2Supporting information
CCDC reference: 1405450
10.1107/S205698901501110X/gk2635sup1.cif
contains datablock I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S205698901501110X/gk2635Isup2.hkl
Coordination compounds, including those formed by macrocyclic ligands, have attracted wide interest of material sciences, because of their potential applications (Lehn, 1995; Zhou et al., 2012). In particular, NiII macrocyclic complexes having vacant sites in the axial positions have been used for the synthesis of new supramolecular materials with interesting properties, including chiral recognition (Ryoo et al., 2010) and gas storage (Suh et al., 2012). For example, NiII complexes with alkyl-substituted tetra-azamacrocyclic ligands and anionic tetrazole derivatives, metal cyanide and azide (Shen et al., 2012; Kim et al., 2015) have been studied as magnetic materials and substrates for crystal engineering. The thiocyanate ion is a versatile anionic ligand which can easily bind to a transition metal ion as a terminal or bridging ligand through the nitrogen and/or the sulfur atoms, thus allowing the assembly of multi-dimensional compounds or heterometallic complexes (Safarifard & Morsali, 2012; Wang & Wang 2015). Here, we report the synthesis and κ4N3,N6,N10,N13)bis(thiocyanato-κN)nickel(II) (I).
of an NiII complex with azamacrocycle and two thiocyanate anions, trans-(1,8-dibutyl-1,3,6,8,10,13-hexaazacyclotetradecane-The title compound (I) contains two crystallographically independent complex molecules that are centrosymmetric. Each NiII ion lies on an inversion centre and is coordinated by four secondary amine N atoms of the azamacrocyclic ligand in a square-planar fashion in the equatorial plane, and by two N atoms from the thiocyanate anions at the axial positions, resulting in a tetragonally distorted octahedral geometry, as shown in Fig. 1. The average equatorial bond lengths, Ni1A—Neq and Ni1B—Neq, are 2.070 (1) and 2.070 (1) Å, respectively. The axial bond lengths, Ni1A—Nax and Ni1B—Nax are 2.119 (1) and 2.093 (1) Å, respectively. The axial bonds are longer than the equatorial bonds, which can be attributed either to a large Jahn–Teller distortion effect of the NiII ion and/or to a ring contraction of the azamacrocyclic ligand (Halcrow, 2013; Kim et al., 2015). The average N—C and C—S bond lengths of the coordinated thiocyanate ions are 1.157 (1) and 1.627 (1) Å, respectively. The former is very similar to a C≡N triple-bond distance, while the latter is slightly shorter than reported C—S single-bond distances (Bradforth et al., 1993; Shin et al., 2010). The six-membered chelate rings involving C2A, C3A and C2B, C3B atoms adopt a chair conformation, whereas the five-membered chelate rings involving C1A, C4A and C1B, C4B assume a conformation (Min & Suh, 2001; Kim et al., 2015).
The S atoms of the thiocyanate groups form intermolecular N—H···S hydrogen bonds with adjacent secondary amine groups of the azamacrocyclic ligand, giving rise to two symmetry-independent one-dimensional polymeric chains propagating along the b-axis direction (Fig. 2 and Table 1).
A search of the Cambridge Structural Database (Version 5.36, Feb 2015 with two updates; Groom & Allen, 2014) indicated one complex of NiII with the same azamaclocyclic ligand having an anionic tetrazole derivative at the axial positions (Kim et al., 2015).
The title compound (I) was prepared as follows. The starting complex, [Ni(C16H38N6)](ClO4)2, was prepared by a slightly modified method reported by Jung et al. (1989). To a MeCN solution (10 mL) of [Ni(C16H38N6)] (ClO4)2 (0.15 g, 0.26 mmol) was slowly added a MeCN solution (5 mL) containing sodium thiocyanate (0.042 g, 0.52 mmol) at room temperature. A pale-pink precipitate was formed, which was filtered off, washed with MeCN, and diethyl ether, and dried in air. Single crystals of the title compound were obtained by layering of the MeCN solution of sodium thiocyanate on the MeCN solution of [Ni(C16H38N6)] (ClO4)2 for several days. Yield: 0.062 g (49%). FT–IR (KBr, cm-1): 3304, 3243, 2929, 2867, 2069, 1468, 1386, 1273, 1204, 1070, 925.
Safety note: Although we have experienced no problem with the compounds 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
details are summarized in Table 2. 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 1.5Ueq of the parent atoms. The C7A and C8A atoms of the macrocyclic ligand were refined as disordered over two sets of sites (C71A, C72A and C81A, C82A) with refined occupancies of 0.630 and 0.370, respectively. The bond distances and angles of the disordered part were restrained to ensure proper geometry using DFIX and DANG instructions of SHELXL2014/7 (Sheldrick, 2015b).Coordination compounds, including those formed by macrocyclic ligands, have attracted wide interest of material sciences, because of their potential applications (Lehn, 1995; Zhou et al., 2012). In particular, NiII macrocyclic complexes having vacant sites in the axial positions have been used for the synthesis of new supramolecular materials with interesting properties, including chiral recognition (Ryoo et al., 2010) and gas storage (Suh et al., 2012). For example, NiII complexes with alkyl-substituted tetra-azamacrocyclic ligands and anionic tetrazole derivatives, metal cyanide and azide (Shen et al., 2012; Kim et al., 2015) have been studied as magnetic materials and substrates for crystal engineering. The thiocyanate ion is a versatile anionic ligand which can easily bind to a transition metal ion as a terminal or bridging ligand through the nitrogen and/or the sulfur atoms, thus allowing the assembly of multi-dimensional compounds or heterometallic complexes (Safarifard & Morsali, 2012; Wang & Wang 2015). Here, we report the synthesis and κ4N3,N6,N10,N13)bis(thiocyanato-κN)nickel(II) (I).
of an NiII complex with azamacrocycle and two thiocyanate anions, trans-(1,8-dibutyl-1,3,6,8,10,13-hexaazacyclotetradecane-The title compound (I) contains two crystallographically independent complex molecules that are centrosymmetric. Each NiII ion lies on an inversion centre and is coordinated by four secondary amine N atoms of the azamacrocyclic ligand in a square-planar fashion in the equatorial plane, and by two N atoms from the thiocyanate anions at the axial positions, resulting in a tetragonally distorted octahedral geometry, as shown in Fig. 1. The average equatorial bond lengths, Ni1A—Neq and Ni1B—Neq, are 2.070 (1) and 2.070 (1) Å, respectively. The axial bond lengths, Ni1A—Nax and Ni1B—Nax are 2.119 (1) and 2.093 (1) Å, respectively. The axial bonds are longer than the equatorial bonds, which can be attributed either to a large Jahn–Teller distortion effect of the NiII ion and/or to a ring contraction of the azamacrocyclic ligand (Halcrow, 2013; Kim et al., 2015). The average N—C and C—S bond lengths of the coordinated thiocyanate ions are 1.157 (1) and 1.627 (1) Å, respectively. The former is very similar to a C≡N triple-bond distance, while the latter is slightly shorter than reported C—S single-bond distances (Bradforth et al., 1993; Shin et al., 2010). The six-membered chelate rings involving C2A, C3A and C2B, C3B atoms adopt a chair conformation, whereas the five-membered chelate rings involving C1A, C4A and C1B, C4B assume a conformation (Min & Suh, 2001; Kim et al., 2015).
The S atoms of the thiocyanate groups form intermolecular N—H···S hydrogen bonds with adjacent secondary amine groups of the azamacrocyclic ligand, giving rise to two symmetry-independent one-dimensional polymeric chains propagating along the b-axis direction (Fig. 2 and Table 1).
A search of the Cambridge Structural Database (Version 5.36, Feb 2015 with two updates; Groom & Allen, 2014) indicated one complex of NiII with the same azamaclocyclic ligand having an anionic tetrazole derivative at the axial positions (Kim et al., 2015).
For related literature, see: Bradforth et al. (1993); Groom & Allen (2014); Halcrow (2013); Jung et al. (1989); Kim et al. (2015); Lehn (1995); Min & Suh (2001); Ryoo et al. (2010); Safarifard & Morsali (2012); Shen et al. (2012); Shin et al. (2010); Steed & Atwood (2009); Suh et al. (2012); Wang & Wang (2015); Zhou et al. (2012).
The title compound (I) was prepared as follows. The starting complex, [Ni(C16H38N6)](ClO4)2, was prepared by a slightly modified method reported by Jung et al. (1989). To a MeCN solution (10 mL) of [Ni(C16H38N6)] (ClO4)2 (0.15 g, 0.26 mmol) was slowly added a MeCN solution (5 mL) containing sodium thiocyanate (0.042 g, 0.52 mmol) at room temperature. A pale-pink precipitate was formed, which was filtered off, washed with MeCN, and diethyl ether, and dried in air. Single crystals of the title compound were obtained by layering of the MeCN solution of sodium thiocyanate on the MeCN solution of [Ni(C16H38N6)] (ClO4)2 for several days. Yield: 0.062 g (49%). FT–IR (KBr, cm-1): 3304, 3243, 2929, 2867, 2069, 1468, 1386, 1273, 1204, 1070, 925.
Safety note: Although we have experienced no problem with the compounds reported in this study, perchlorate salts of metal complexes are often explosive and should be handled with great caution.
detailsCrystal data, data collection and structure
details are summarized in Table 2. 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 1.5Ueq of the parent atoms. The C7A and C8A atoms of the macrocyclic ligand were refined as disordered over two sets of sites (C71A, C72A and C81A, C82A) with refined occupancies of 0.630 and 0.370, respectively. The bond distances and angles of the disordered part were restrained to ensure proper geometry using DFIX and DANG instructions of SHELXL2014/7 (Sheldrick, 2015b).Data collection: PAL ADSC Quantum-210 ADX (Arvai & Nielsen, 1983); cell
HKL3000sm (Otwinowski & Minor, 1997); data reduction: HKL3000sm (Otwinowski & Minor, 1997); program(s) used to solve structure: SHELXT2014 (Sheldrick, 2015a); program(s) used to refine structure: SHELXL2014 (Sheldrick, 2015b); molecular graphics: DIAMOND (Putz & Brandenburg, 2007); software used to prepare material for publication: publCIF (Westrip, 2010).Fig. 1. View of the molecular structure of the title compound, showing the atom-labelling scheme, with displacement ellipsoids drawn at the 30% probability level. H atoms have been omitted for clarity. The minor position of the n-butyl substituent in the A molecule is not shown. | |
Fig. 2. View of the crystal packing, with N—H···S hydrogen bonds drawn as red dashed lines. H atoms have been omitted for clarity. |
[Ni(NCS)2(C16H38N6)] | Z = 2 |
Mr = 489.39 | F(000) = 524 |
Triclinic, P1 | Dx = 1.348 Mg m−3 |
a = 8.6610 (17) Å | Synchrotron radiation, λ = 0.630 Å |
b = 12.027 (2) Å | Cell parameters from 49914 reflections |
c = 12.560 (3) Å | θ = 0.4–33.6° |
α = 94.66 (3)° | µ = 0.72 mm−1 |
β = 97.99 (3)° | T = 180 K |
γ = 110.04 (3)° | Block, pale pink |
V = 1205.4 (5) Å3 | 0.25 × 0.15 × 0.13 mm |
ADSC Q210 CCD area-detector diffractometer | 6243 reflections with I > 2σ(I) |
Radiation source: PLSII 2D bending magnet | Rint = 0.014 |
ω scan | θmax = 26.0°, θmin = 1.6° |
Absorption correction: empirical (using intensity measurements) (HKL3000sm SCALEPACK; Otwinowski & Minor, 1997) | h = −12→12 |
Tmin = 0.841, Tmax = 0.916 | k = −16→16 |
12812 measured reflections | l = −17→17 |
6583 independent reflections |
Refinement on F2 | 11 restraints |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.042 | H-atom parameters constrained |
wR(F2) = 0.111 | w = 1/[σ2(Fo2) + (0.0541P)2 + 0.7946P] where P = (Fo2 + 2Fc2)/3 |
S = 1.06 | (Δ/σ)max = 0.002 |
6583 reflections | Δρmax = 1.58 e Å−3 |
287 parameters | Δρmin = −1.11 e Å−3 |
[Ni(NCS)2(C16H38N6)] | γ = 110.04 (3)° |
Mr = 489.39 | V = 1205.4 (5) Å3 |
Triclinic, P1 | Z = 2 |
a = 8.6610 (17) Å | Synchrotron radiation, λ = 0.630 Å |
b = 12.027 (2) Å | µ = 0.72 mm−1 |
c = 12.560 (3) Å | T = 180 K |
α = 94.66 (3)° | 0.25 × 0.15 × 0.13 mm |
β = 97.99 (3)° |
ADSC Q210 CCD area-detector diffractometer | 6583 independent reflections |
Absorption correction: empirical (using intensity measurements) (HKL3000sm SCALEPACK; Otwinowski & Minor, 1997) | 6243 reflections with I > 2σ(I) |
Tmin = 0.841, Tmax = 0.916 | Rint = 0.014 |
12812 measured reflections |
R[F2 > 2σ(F2)] = 0.042 | 11 restraints |
wR(F2) = 0.111 | H-atom parameters constrained |
S = 1.06 | Δρmax = 1.58 e Å−3 |
6583 reflections | Δρmin = −1.11 e Å−3 |
287 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 | Occ. (<1) | |
Ni1A | 0.0000 | 0.0000 | 0.5000 | 0.02295 (8) | |
S1A | −0.39772 (6) | 0.09973 (6) | 0.68745 (4) | 0.05126 (15) | |
N1A | 0.20720 (17) | 0.11708 (13) | 0.60541 (11) | 0.0301 (3) | |
H1A | 0.3083 | 0.1069 | 0.5828 | 0.036* | |
N2A | 0.02319 (18) | 0.10693 (13) | 0.37714 (12) | 0.0321 (3) | |
H2A | 0.1105 | 0.0955 | 0.3377 | 0.039* | |
N3A | 0.2318 (2) | 0.27979 (15) | 0.49597 (17) | 0.0460 (4) | |
N4A | −0.16012 (18) | 0.07346 (14) | 0.56843 (13) | 0.0343 (3) | |
C1A | 0.1944 (2) | 0.07739 (18) | 0.71320 (14) | 0.0373 (4) | |
H1A1 | 0.1128 | 0.1036 | 0.7459 | 0.045* | |
H1A2 | 0.3042 | 0.1129 | 0.7621 | 0.045* | |
C2A | 0.2242 (3) | 0.24393 (17) | 0.60232 (18) | 0.0426 (4) | |
H2A1 | 0.1280 | 0.2567 | 0.6285 | 0.051* | |
H2A2 | 0.3269 | 0.2957 | 0.6528 | 0.051* | |
C3A | 0.0780 (3) | 0.23584 (17) | 0.41904 (19) | 0.0431 (4) | |
H3A1 | 0.0916 | 0.2821 | 0.3571 | 0.052* | |
H3A2 | −0.0106 | 0.2499 | 0.4539 | 0.052* | |
C4A | −0.1381 (2) | 0.05792 (19) | 0.30124 (15) | 0.0387 (4) | |
H4A1 | −0.1251 | 0.0872 | 0.2304 | 0.046* | |
H4A2 | −0.2223 | 0.0840 | 0.3307 | 0.046* | |
C5A | 0.3770 (3) | 0.2784 (3) | 0.4483 (3) | 0.0632 (7) | |
H5A1 | 0.3705 | 0.3095 | 0.3778 | 0.076* | |
H5A2 | 0.3693 | 0.1945 | 0.4332 | 0.076* | |
C6A | 0.5445 (3) | 0.3493 (3) | 0.5164 (4) | 0.0870 (11) | |
H6A1 | 0.5622 | 0.3131 | 0.5829 | 0.104* | |
H6A2 | 0.5534 | 0.4327 | 0.5378 | 0.104* | |
C71A | 0.6816 (5) | 0.3457 (6) | 0.4395 (4) | 0.084 (2) | 0.63 |
H71A | 0.6781 | 0.2628 | 0.4233 | 0.100* | 0.63 |
H71B | 0.6563 | 0.3747 | 0.3701 | 0.100* | 0.63 |
C81A | 0.8493 (5) | 0.4237 (4) | 0.4995 (4) | 0.0654 (11) | 0.63 |
H81A | 0.8483 | 0.5035 | 0.5213 | 0.098* | 0.63 |
H81B | 0.9324 | 0.4296 | 0.4525 | 0.098* | 0.63 |
H81C | 0.8780 | 0.3895 | 0.5642 | 0.098* | 0.63 |
C72A | 0.7095 (11) | 0.3319 (9) | 0.5052 (9) | 0.077 (2) | 0.37 |
H72A | 0.8005 | 0.3782 | 0.5662 | 0.093* | 0.37 |
H72B | 0.6971 | 0.2465 | 0.4991 | 0.093* | 0.37 |
C82A | 0.7346 (11) | 0.3790 (12) | 0.4057 (7) | 0.090 (3) | 0.37 |
H82A | 0.6498 | 0.3254 | 0.3461 | 0.135* | 0.37 |
H82B | 0.8460 | 0.3857 | 0.3921 | 0.135* | 0.37 |
H82C | 0.7255 | 0.4582 | 0.4107 | 0.135* | 0.37 |
C9A | −0.2607 (2) | 0.08368 (15) | 0.61628 (13) | 0.0304 (3) | |
Ni2B | 1.0000 | 0.5000 | 0.0000 | 0.02474 (8) | |
S1B | 0.48562 (7) | 0.51503 (7) | −0.18976 (6) | 0.0654 (2) | |
N1B | 0.90438 (18) | 0.33335 (13) | −0.09357 (12) | 0.0319 (3) | |
H1B | 0.7910 | 0.3226 | −0.1338 | 0.038* | |
N2B | 0.86585 (17) | 0.44340 (13) | 0.12179 (11) | 0.0293 (3) | |
H2B | 0.7493 | 0.4404 | 0.0979 | 0.035* | |
N3B | 0.7849 (2) | 0.23013 (14) | 0.05324 (14) | 0.0368 (3) | |
N4B | 0.79629 (19) | 0.53663 (16) | −0.07763 (14) | 0.0384 (3) | |
C1B | 1.0161 (2) | 0.34041 (17) | −0.17379 (16) | 0.0395 (4) | |
H1B1 | 0.9614 | 0.2749 | −0.2350 | 0.047* | |
H1B2 | 1.1210 | 0.3322 | −0.1394 | 0.047* | |
C2B | 0.8871 (3) | 0.23310 (16) | −0.02905 (18) | 0.0401 (4) | |
H2B1 | 0.8377 | 0.1568 | −0.0789 | 0.048* | |
H2B2 | 0.9997 | 0.2392 | 0.0065 | 0.048* | |
C3B | 0.8572 (2) | 0.32257 (17) | 0.14559 (15) | 0.0363 (3) | |
H3B1 | 0.9715 | 0.3258 | 0.1735 | 0.044* | |
H3B2 | 0.7904 | 0.3008 | 0.2037 | 0.044* | |
C4B | 0.9457 (2) | 0.53919 (17) | 0.21515 (14) | 0.0366 (4) | |
H4B1 | 1.0503 | 0.5321 | 0.2515 | 0.044* | |
H4B2 | 0.8700 | 0.5320 | 0.2685 | 0.044* | |
C5B | 0.6079 (2) | 0.20371 (17) | 0.00919 (15) | 0.0366 (4) | |
H5B1 | 0.5718 | 0.1390 | −0.0530 | 0.044* | |
H5B2 | 0.5956 | 0.2756 | −0.0184 | 0.044* | |
C6B | 0.4936 (2) | 0.16605 (17) | 0.09165 (15) | 0.0382 (4) | |
H6B1 | 0.5143 | 0.0997 | 0.1253 | 0.046* | |
H6B2 | 0.5206 | 0.2340 | 0.1498 | 0.046* | |
C7B | 0.3107 (3) | 0.12633 (19) | 0.04111 (16) | 0.0413 (4) | |
H7B1 | 0.2794 | 0.0511 | −0.0089 | 0.050* | |
H7B2 | 0.2932 | 0.1877 | −0.0020 | 0.050* | |
C8B | 0.1979 (3) | 0.1066 (2) | 0.12585 (18) | 0.0456 (4) | |
H8B1 | 0.2212 | 0.0508 | 0.1725 | 0.068* | |
H8B2 | 0.0808 | 0.0734 | 0.0895 | 0.068* | |
H8B3 | 0.2190 | 0.1831 | 0.1701 | 0.068* | |
C9B | 0.6659 (2) | 0.52684 (14) | −0.12328 (13) | 0.0294 (3) |
U11 | U22 | U33 | U12 | U13 | U23 | |
Ni1A | 0.02036 (13) | 0.02643 (14) | 0.02328 (13) | 0.00930 (10) | 0.00718 (9) | 0.00057 (9) |
S1A | 0.0351 (2) | 0.0888 (4) | 0.0415 (3) | 0.0343 (3) | 0.01563 (19) | 0.0052 (3) |
N1A | 0.0239 (6) | 0.0347 (7) | 0.0292 (6) | 0.0085 (5) | 0.0064 (5) | −0.0031 (5) |
N2A | 0.0294 (6) | 0.0369 (7) | 0.0333 (7) | 0.0130 (5) | 0.0111 (5) | 0.0087 (5) |
N3A | 0.0402 (8) | 0.0320 (7) | 0.0611 (11) | 0.0053 (6) | 0.0126 (8) | 0.0082 (7) |
N4A | 0.0292 (6) | 0.0389 (7) | 0.0376 (7) | 0.0161 (6) | 0.0098 (5) | −0.0021 (6) |
C1A | 0.0309 (8) | 0.0535 (10) | 0.0258 (7) | 0.0150 (7) | 0.0046 (6) | −0.0020 (7) |
C2A | 0.0391 (9) | 0.0315 (8) | 0.0492 (10) | 0.0061 (7) | 0.0071 (8) | −0.0078 (7) |
C3A | 0.0437 (10) | 0.0344 (9) | 0.0555 (11) | 0.0155 (8) | 0.0138 (8) | 0.0144 (8) |
C4A | 0.0354 (8) | 0.0551 (11) | 0.0305 (8) | 0.0204 (8) | 0.0076 (6) | 0.0118 (7) |
C5A | 0.0370 (11) | 0.0618 (15) | 0.0824 (18) | −0.0004 (10) | 0.0211 (11) | 0.0257 (13) |
C6A | 0.0414 (13) | 0.0560 (16) | 0.147 (3) | −0.0010 (11) | 0.0047 (17) | 0.0253 (19) |
C71A | 0.042 (2) | 0.129 (4) | 0.055 (2) | −0.011 (2) | 0.0025 (17) | 0.067 (3) |
C81A | 0.051 (2) | 0.062 (2) | 0.076 (3) | 0.0168 (18) | 0.0036 (19) | −0.003 (2) |
C72A | 0.062 (5) | 0.074 (5) | 0.098 (7) | 0.026 (4) | 0.016 (5) | 0.019 (5) |
C82A | 0.083 (7) | 0.129 (10) | 0.054 (5) | 0.049 (7) | −0.015 (5) | −0.011 (6) |
C9A | 0.0253 (7) | 0.0374 (8) | 0.0300 (7) | 0.0144 (6) | 0.0043 (5) | −0.0002 (6) |
Ni2B | 0.02097 (13) | 0.02802 (14) | 0.02616 (14) | 0.01142 (10) | 0.00207 (9) | 0.00079 (10) |
S1B | 0.0371 (3) | 0.0927 (5) | 0.0605 (4) | 0.0332 (3) | −0.0185 (2) | −0.0201 (3) |
N1B | 0.0280 (6) | 0.0312 (6) | 0.0350 (7) | 0.0090 (5) | 0.0090 (5) | −0.0017 (5) |
N2B | 0.0241 (6) | 0.0333 (6) | 0.0283 (6) | 0.0093 (5) | 0.0025 (5) | 0.0009 (5) |
N3B | 0.0358 (7) | 0.0314 (7) | 0.0425 (8) | 0.0102 (6) | 0.0093 (6) | 0.0065 (6) |
N4B | 0.0285 (7) | 0.0482 (9) | 0.0418 (8) | 0.0189 (6) | 0.0019 (6) | 0.0083 (7) |
C1B | 0.0345 (8) | 0.0373 (9) | 0.0424 (9) | 0.0079 (7) | 0.0145 (7) | −0.0086 (7) |
C2B | 0.0419 (9) | 0.0297 (8) | 0.0524 (11) | 0.0152 (7) | 0.0153 (8) | 0.0037 (7) |
C3B | 0.0341 (8) | 0.0393 (9) | 0.0347 (8) | 0.0119 (7) | 0.0039 (6) | 0.0102 (7) |
C4B | 0.0299 (8) | 0.0446 (9) | 0.0289 (7) | 0.0070 (7) | 0.0060 (6) | −0.0040 (7) |
C5B | 0.0354 (8) | 0.0332 (8) | 0.0363 (8) | 0.0054 (6) | 0.0084 (7) | 0.0042 (6) |
C6B | 0.0386 (9) | 0.0371 (8) | 0.0339 (8) | 0.0067 (7) | 0.0089 (7) | 0.0046 (7) |
C7B | 0.0397 (9) | 0.0445 (10) | 0.0339 (8) | 0.0069 (8) | 0.0105 (7) | 0.0029 (7) |
C8B | 0.0434 (10) | 0.0489 (11) | 0.0440 (10) | 0.0125 (8) | 0.0158 (8) | 0.0083 (8) |
C9B | 0.0283 (7) | 0.0303 (7) | 0.0309 (7) | 0.0131 (6) | 0.0055 (6) | 0.0003 (6) |
Ni1A—N1Ai | 2.0640 (17) | C82A—H82A | 0.9800 |
Ni1A—N1A | 2.0640 (17) | C82A—H82B | 0.9800 |
Ni1A—N2Ai | 2.0754 (15) | C82A—H82C | 0.9800 |
Ni1A—N2A | 2.0754 (15) | Ni2B—N2Bii | 2.0675 (15) |
Ni1A—N4Ai | 2.1190 (15) | Ni2B—N2B | 2.0675 (15) |
Ni1A—N4A | 2.1190 (15) | Ni2B—N1Bii | 2.0719 (16) |
S1A—C9A | 1.6339 (17) | Ni2B—N1B | 2.0719 (16) |
N1A—C1A | 1.478 (2) | Ni2B—N4Bii | 2.0933 (16) |
N1A—C2A | 1.486 (2) | Ni2B—N4B | 2.0933 (16) |
N1A—H1A | 1.0000 | S1B—C9B | 1.6190 (18) |
N2A—C4A | 1.477 (2) | N1B—C1B | 1.479 (2) |
N2A—C3A | 1.483 (3) | N1B—C2B | 1.484 (2) |
N2A—H2A | 1.0000 | N1B—H1B | 1.0000 |
N3A—C3A | 1.436 (3) | N2B—C4B | 1.480 (2) |
N3A—C2A | 1.440 (3) | N2B—C3B | 1.486 (2) |
N3A—C5A | 1.470 (3) | N2B—H2B | 1.0000 |
N4A—C9A | 1.158 (2) | N3B—C3B | 1.444 (3) |
C1A—C4Ai | 1.517 (3) | N3B—C2B | 1.446 (2) |
C1A—H1A1 | 0.9900 | N3B—C5B | 1.469 (3) |
C1A—H1A2 | 0.9900 | N4B—C9B | 1.156 (2) |
C2A—H2A1 | 0.9900 | C1B—C4Bii | 1.523 (3) |
C2A—H2A2 | 0.9900 | C1B—H1B1 | 0.9900 |
C3A—H3A1 | 0.9900 | C1B—H1B2 | 0.9900 |
C3A—H3A2 | 0.9900 | C2B—H2B1 | 0.9900 |
C4A—C1Ai | 1.517 (3) | C2B—H2B2 | 0.9900 |
C4A—H4A1 | 0.9900 | C3B—H3B1 | 0.9900 |
C4A—H4A2 | 0.9900 | C3B—H3B2 | 0.9900 |
C5A—C6A | 1.501 (4) | C4B—C1Bii | 1.522 (3) |
C5A—H5A1 | 0.9900 | C4B—H4B1 | 0.9900 |
C5A—H5A2 | 0.9900 | C4B—H4B2 | 0.9900 |
C6A—C72A | 1.537 (9) | C5B—C6B | 1.520 (3) |
C6A—C71A | 1.641 (6) | C5B—H5B1 | 0.9900 |
C6A—H6A1 | 0.9900 | C5B—H5B2 | 0.9900 |
C6A—H6A2 | 0.9900 | C6B—C7B | 1.514 (3) |
C71A—C81A | 1.485 (5) | C6B—H6B1 | 0.9900 |
C71A—H71A | 0.9900 | C6B—H6B2 | 0.9900 |
C71A—H71B | 0.9900 | C7B—C8B | 1.522 (3) |
C81A—H81A | 0.9800 | C7B—H7B1 | 0.9900 |
C81A—H81B | 0.9800 | C7B—H7B2 | 0.9900 |
C81A—H81C | 0.9800 | C8B—H8B1 | 0.9800 |
C72A—C82A | 1.427 (12) | C8B—H8B2 | 0.9800 |
C72A—H72A | 0.9900 | C8B—H8B3 | 0.9800 |
C72A—H72B | 0.9900 | ||
N1Ai—Ni1A—N1A | 180.00 (7) | C72A—C82A—H82B | 109.5 |
N1Ai—Ni1A—N2Ai | 95.00 (7) | H82A—C82A—H82B | 109.5 |
N1A—Ni1A—N2Ai | 85.00 (6) | C72A—C82A—H82C | 109.5 |
N1Ai—Ni1A—N2A | 85.00 (6) | H82A—C82A—H82C | 109.5 |
N1A—Ni1A—N2A | 95.00 (6) | H82B—C82A—H82C | 109.5 |
N2Ai—Ni1A—N2A | 180.00 (8) | N4A—C9A—S1A | 178.09 (16) |
N1Ai—Ni1A—N4Ai | 91.75 (6) | N2Bii—Ni2B—N2B | 180.0 |
N1A—Ni1A—N4Ai | 88.25 (6) | N2Bii—Ni2B—N1Bii | 93.91 (6) |
N2Ai—Ni1A—N4Ai | 92.85 (6) | N2B—Ni2B—N1Bii | 86.09 (6) |
N2A—Ni1A—N4Ai | 87.15 (6) | N2Bii—Ni2B—N1B | 86.09 (6) |
N1Ai—Ni1A—N4A | 88.25 (6) | N2B—Ni2B—N1B | 93.91 (6) |
N1A—Ni1A—N4A | 91.75 (6) | N1Bii—Ni2B—N1B | 180.0 |
N2Ai—Ni1A—N4A | 87.15 (6) | N2Bii—Ni2B—N4Bii | 88.26 (6) |
N2A—Ni1A—N4A | 92.85 (6) | N2B—Ni2B—N4Bii | 91.74 (6) |
N4Ai—Ni1A—N4A | 180.0 | N1Bii—Ni2B—N4Bii | 88.42 (7) |
C1A—N1A—C2A | 114.56 (15) | N1B—Ni2B—N4Bii | 91.58 (7) |
C1A—N1A—Ni1A | 106.14 (11) | N2Bii—Ni2B—N4B | 91.74 (6) |
C2A—N1A—Ni1A | 112.51 (12) | N2B—Ni2B—N4B | 88.26 (6) |
C1A—N1A—H1A | 107.8 | N1Bii—Ni2B—N4B | 91.58 (7) |
C2A—N1A—H1A | 107.8 | N1B—Ni2B—N4B | 88.42 (7) |
Ni1A—N1A—H1A | 107.8 | N4Bii—Ni2B—N4B | 180.0 |
C4A—N2A—C3A | 115.13 (15) | C1B—N1B—C2B | 114.04 (15) |
C4A—N2A—Ni1A | 105.93 (11) | C1B—N1B—Ni2B | 104.88 (11) |
C3A—N2A—Ni1A | 112.70 (12) | C2B—N1B—Ni2B | 113.56 (11) |
C4A—N2A—H2A | 107.6 | C1B—N1B—H1B | 108.0 |
C3A—N2A—H2A | 107.6 | C2B—N1B—H1B | 108.0 |
Ni1A—N2A—H2A | 107.6 | Ni2B—N1B—H1B | 108.0 |
C3A—N3A—C2A | 116.46 (17) | C4B—N2B—C3B | 114.37 (14) |
C3A—N3A—C5A | 113.3 (2) | C4B—N2B—Ni2B | 104.95 (10) |
C2A—N3A—C5A | 116.6 (2) | C3B—N2B—Ni2B | 112.98 (11) |
C9A—N4A—Ni1A | 161.18 (15) | C4B—N2B—H2B | 108.1 |
N1A—C1A—C4Ai | 108.32 (14) | C3B—N2B—H2B | 108.1 |
N1A—C1A—H1A1 | 110.0 | Ni2B—N2B—H2B | 108.1 |
C4Ai—C1A—H1A1 | 110.0 | C3B—N3B—C2B | 115.91 (15) |
N1A—C1A—H1A2 | 110.0 | C3B—N3B—C5B | 115.92 (16) |
C4Ai—C1A—H1A2 | 110.0 | C2B—N3B—C5B | 113.83 (16) |
H1A1—C1A—H1A2 | 108.4 | C9B—N4B—Ni2B | 163.23 (16) |
N3A—C2A—N1A | 113.64 (16) | N1B—C1B—C4Bii | 108.49 (15) |
N3A—C2A—H2A1 | 108.8 | N1B—C1B—H1B1 | 110.0 |
N1A—C2A—H2A1 | 108.8 | C4Bii—C1B—H1B1 | 110.0 |
N3A—C2A—H2A2 | 108.8 | N1B—C1B—H1B2 | 110.0 |
N1A—C2A—H2A2 | 108.8 | C4Bii—C1B—H1B2 | 110.0 |
H2A1—C2A—H2A2 | 107.7 | H1B1—C1B—H1B2 | 108.4 |
N3A—C3A—N2A | 113.85 (16) | N3B—C2B—N1B | 113.94 (15) |
N3A—C3A—H3A1 | 108.8 | N3B—C2B—H2B1 | 108.8 |
N2A—C3A—H3A1 | 108.8 | N1B—C2B—H2B1 | 108.8 |
N3A—C3A—H3A2 | 108.8 | N3B—C2B—H2B2 | 108.8 |
N2A—C3A—H3A2 | 108.8 | N1B—C2B—H2B2 | 108.8 |
H3A1—C3A—H3A2 | 107.7 | H2B1—C2B—H2B2 | 107.7 |
N2A—C4A—C1Ai | 108.23 (15) | N3B—C3B—N2B | 114.19 (14) |
N2A—C4A—H4A1 | 110.1 | N3B—C3B—H3B1 | 108.7 |
C1Ai—C4A—H4A1 | 110.1 | N2B—C3B—H3B1 | 108.7 |
N2A—C4A—H4A2 | 110.1 | N3B—C3B—H3B2 | 108.7 |
C1Ai—C4A—H4A2 | 110.1 | N2B—C3B—H3B2 | 108.7 |
H4A1—C4A—H4A2 | 108.4 | H3B1—C3B—H3B2 | 107.6 |
N3A—C5A—C6A | 115.5 (3) | N2B—C4B—C1Bii | 108.66 (15) |
N3A—C5A—H5A1 | 108.4 | N2B—C4B—H4B1 | 110.0 |
C6A—C5A—H5A1 | 108.4 | C1Bii—C4B—H4B1 | 110.0 |
N3A—C5A—H5A2 | 108.4 | N2B—C4B—H4B2 | 110.0 |
C6A—C5A—H5A2 | 108.4 | C1Bii—C4B—H4B2 | 110.0 |
H5A1—C5A—H5A2 | 107.5 | H4B1—C4B—H4B2 | 108.3 |
C5A—C6A—C72A | 125.6 (5) | N3B—C5B—C6B | 113.59 (16) |
C5A—C6A—C71A | 105.5 (3) | N3B—C5B—H5B1 | 108.8 |
C5A—C6A—H6A1 | 110.6 | C6B—C5B—H5B1 | 108.8 |
C71A—C6A—H6A1 | 110.6 | N3B—C5B—H5B2 | 108.8 |
C5A—C6A—H6A2 | 110.6 | C6B—C5B—H5B2 | 108.8 |
C71A—C6A—H6A2 | 110.6 | H5B1—C5B—H5B2 | 107.7 |
H6A1—C6A—H6A2 | 108.8 | C7B—C6B—C5B | 112.38 (16) |
C81A—C71A—C6A | 107.8 (4) | C7B—C6B—H6B1 | 109.1 |
C81A—C71A—H71A | 110.2 | C5B—C6B—H6B1 | 109.1 |
C6A—C71A—H71A | 110.2 | C7B—C6B—H6B2 | 109.1 |
C81A—C71A—H71B | 110.2 | C5B—C6B—H6B2 | 109.1 |
C6A—C71A—H71B | 110.2 | H6B1—C6B—H6B2 | 107.9 |
H71A—C71A—H71B | 108.5 | C6B—C7B—C8B | 112.29 (17) |
C71A—C81A—H81A | 109.5 | C6B—C7B—H7B1 | 109.1 |
C71A—C81A—H81B | 109.5 | C8B—C7B—H7B1 | 109.1 |
H81A—C81A—H81B | 109.5 | C6B—C7B—H7B2 | 109.1 |
C71A—C81A—H81C | 109.5 | C8B—C7B—H7B2 | 109.1 |
H81A—C81A—H81C | 109.5 | H7B1—C7B—H7B2 | 107.9 |
H81B—C81A—H81C | 109.5 | C7B—C8B—H8B1 | 109.5 |
C82A—C72A—C6A | 99.0 (7) | C7B—C8B—H8B2 | 109.5 |
C82A—C72A—H72A | 112.0 | H8B1—C8B—H8B2 | 109.5 |
C6A—C72A—H72A | 112.0 | C7B—C8B—H8B3 | 109.5 |
C82A—C72A—H72B | 112.0 | H8B1—C8B—H8B3 | 109.5 |
C6A—C72A—H72B | 112.0 | H8B2—C8B—H8B3 | 109.5 |
H72A—C72A—H72B | 109.6 | N4B—C9B—S1B | 178.44 (17) |
C72A—C82A—H82A | 109.5 | ||
C2A—N1A—C1A—C4Ai | 167.05 (14) | C5A—C6A—C72A—C82A | 71.8 (8) |
Ni1A—N1A—C1A—C4Ai | 42.27 (15) | C2B—N1B—C1B—C4Bii | −167.20 (15) |
C3A—N3A—C2A—N1A | 73.7 (2) | Ni2B—N1B—C1B—C4Bii | −42.36 (16) |
C5A—N3A—C2A—N1A | −64.4 (2) | C3B—N3B—C2B—N1B | −71.3 (2) |
C1A—N1A—C2A—N3A | −178.39 (15) | C5B—N3B—C2B—N1B | 66.9 (2) |
Ni1A—N1A—C2A—N3A | −57.03 (18) | C1B—N1B—C2B—N3B | 176.89 (15) |
C2A—N3A—C3A—N2A | −73.1 (2) | Ni2B—N1B—C2B—N3B | 56.80 (19) |
C5A—N3A—C3A—N2A | 66.4 (2) | C2B—N3B—C3B—N2B | 72.1 (2) |
C4A—N2A—C3A—N3A | 177.61 (16) | C5B—N3B—C3B—N2B | −65.2 (2) |
Ni1A—N2A—C3A—N3A | 55.96 (19) | C4B—N2B—C3B—N3B | −177.77 (14) |
C3A—N2A—C4A—C1Ai | −167.20 (15) | Ni2B—N2B—C3B—N3B | −57.79 (17) |
Ni1A—N2A—C4A—C1Ai | −41.95 (15) | C3B—N2B—C4B—C1Bii | 166.62 (14) |
C3A—N3A—C5A—C6A | 166.0 (2) | Ni2B—N2B—C4B—C1Bii | 42.25 (15) |
C2A—N3A—C5A—C6A | −54.7 (3) | C3B—N3B—C5B—C6B | −58.2 (2) |
N3A—C5A—C6A—C72A | 159.1 (5) | C2B—N3B—C5B—C6B | 163.62 (16) |
N3A—C5A—C6A—C71A | −173.6 (3) | N3B—C5B—C6B—C7B | −173.67 (16) |
C5A—C6A—C71A—C81A | 175.0 (4) | C5B—C6B—C7B—C8B | −171.39 (18) |
Symmetry codes: (i) −x, −y, −z+1; (ii) −x+2, −y+1, −z. |
D—H···A | D—H | H···A | D···A | D—H···A |
N1A—H1A···S1Aiii | 1.00 | 2.73 | 3.5154 (17) | 136 |
N2B—H2B···S1Biv | 1.00 | 2.66 | 3.4556 (17) | 137 |
Symmetry codes: (iii) x+1, y, z; (iv) −x+1, −y+1, −z. |
D—H···A | D—H | H···A | D···A | D—H···A |
N1A—H1A···S1Ai | 1.00 | 2.73 | 3.5154 (17) | 135.6 |
N2B—H2B···S1Bii | 1.00 | 2.66 | 3.4556 (17) | 137.0 |
Symmetry codes: (i) x+1, y, z; (ii) −x+1, −y+1, −z. |
Experimental details
Crystal data | |
Chemical formula | [Ni(NCS)2(C16H38N6)] |
Mr | 489.39 |
Crystal system, space group | Triclinic, P1 |
Temperature (K) | 180 |
a, b, c (Å) | 8.6610 (17), 12.027 (2), 12.560 (3) |
α, β, γ (°) | 94.66 (3), 97.99 (3), 110.04 (3) |
V (Å3) | 1205.4 (5) |
Z | 2 |
Radiation type | Synchrotron, λ = 0.630 Å |
µ (mm−1) | 0.72 |
Crystal size (mm) | 0.25 × 0.15 × 0.13 |
Data collection | |
Diffractometer | ADSC Q210 CCD area-detector |
Absorption correction | Empirical (using intensity measurements) (HKL3000sm SCALEPACK; Otwinowski & Minor, 1997) |
Tmin, Tmax | 0.841, 0.916 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 12812, 6583, 6243 |
Rint | 0.014 |
(sin θ/λ)max (Å−1) | 0.696 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.042, 0.111, 1.06 |
No. of reflections | 6583 |
No. of parameters | 287 |
No. of restraints | 11 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 1.58, −1.11 |
Computer programs: PAL ADSC Quantum-210 ADX (Arvai & Nielsen, 1983), HKL3000sm (Otwinowski & Minor, 1997), SHELXT2014 (Sheldrick, 2015a), SHELXL2014 (Sheldrick, 2015b), DIAMOND (Putz & Brandenburg, 2007), publCIF (Westrip, 2010).
Acknowledgements
This work was supported by Basic Science Research Program through the National Research Foundation of Korea (NRF) funded by the Ministry of Education, Science and Technology (NRF-2014R1A1A2058815) and supported by the Institute for Basic Science (IBS, IBS-R007-D1–2015 − a01). The X-ray crystallography BL2D-SMC beamline at PLS-II was supported in part by MSIP and POSTECH.
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