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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2010 Apr 17;66(Pt 5):m527. doi: 10.1107/S1600536810012997

catena-Poly[[[aqua­copper(II)]bis­[μ-bis(3,5-dimethyl-1H-pyrazol-4-yl) selenide]] bis­(tetra­fluorido­borate) bis­(triphenyl­phosphine oxide) monohydrate]

Maksym Seredyuk a,*, Kateryna O Znovjyak a, Yurii S Moroz a, Vadim A Pavlenko a, Igor O Fritsky a
PMCID: PMC2979014  PMID: 21579021

Abstract

The title compound, {[Cu(C10H14N4Se)2(H2O)](BF4)2·2C18H15PO·H2O}n, has a polymeric structure where each CuII ion adopts a square-pyramidal coordination constituted by four N atoms of pyrazole moieties in the equatorial plane and an axial O atom of a water mol­ecule. A pair of bis­(3,5-dimethyl-1H-pyrazol-4-yl) selenide ligands bridges the CuII centres into a chain extending along the c axis. The water mol­ecules, anions and triphenyl­phosphine oxide mol­ecules are involved in inter­molecular hydrogen bonding, which links the chains into a three-dimensional network.

Related literature

For general background, see: Farha et al. (2009); Shibahara et al. (2007); Zhang et al. (2009). For related structures, see: Seredyuk et al. (2007, 2009).graphic file with name e-66-0m527-scheme1.jpg

Experimental

Crystal data

  • [Cu(C10H14N4Se)2(H2O)](BF4)2·2C18H15OP·H2O

  • M r = 1386.17

  • Monoclinic, Inline graphic

  • a = 21.4560 (4) Å

  • b = 15.3590 (4) Å

  • c = 18.4910 (6) Å

  • β = 97.74 (2)°

  • V = 6038.0 (3) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 1.70 mm−1

  • T = 100 K

  • 0.09 × 0.07 × 0.04 mm

Data collection

  • Kuma KM4 CCD area-detector diffractometer

  • 34362 measured reflections

  • 6876 independent reflections

  • 6210 reflections with I > 2σ(I)

  • R int = 0.045

Refinement

  • R[F 2 > 2σ(F 2)] = 0.043

  • wR(F 2) = 0.082

  • S = 1.16

  • 6876 reflections

  • 384 parameters

  • H-atom parameters constrained

  • Δρmax = 0.63 e Å−3

  • Δρmin = −0.38 e Å−3

Data collection: KM-4-CCD (Kuma, 1999); cell refinement: KM-4-CCD; data reduction: KM-4-CCD; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999).

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810012997/ds2023sup1.cif

e-66-0m527-sup1.cif (28.5KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810012997/ds2023Isup2.hkl

e-66-0m527-Isup2.hkl (329.8KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
O1W—H1W⋯F2 0.90 2.14 3.002 (3) 161
O1W—H1W⋯F3 0.90 2.51 3.115 (3) 125
O1W—H2W⋯O2 0.95 1.90 2.785 (3) 155
O1—H1O⋯O2 0.81 1.95 2.752 (2) 173
N1—H1N⋯F4i 0.88 2.06 2.861 (3) 152
N4—H4N⋯O1Wii 0.88 1.86 2.730 (3) 170

Symmetry codes: (i) Inline graphic; (ii) Inline graphic.

Acknowledgments

The authors thank the Ministry of Education and Science of Ukraine for financial support (grant No. M/263-2008)

supplementary crystallographic information

Comment

Study of organometallic polymers is a well elaborated research area in coordination chemistry. Infinite molecular polymeric arrays are potentially applicable as specifically ordered crystalline substances with reversible selective sorption (Farha et al., 2009; Zhang et al., 2009), electrical conductivity (Zhang et al., 2009) and molecular magnetism functionality (Shibahara et al., 2007).

The title compound, [Cu(H2O)(C10H14N4Se)2][(BF4)2.(Ph3PO)2.H2O, was prepared in a water–methanolic medium by mixing solutions of Cu(BF4)2.6H2O and the mixture of the ligand bis(3,5-dimethyl-1H-pyrazolyl)selenide (L) and trisphenylphosphine oxide. It has similar structure to the copper compounds reported recently (Seredyuk et al., 2007, 2009). A pyramidal environment of the CuII ion is constituted by four non-coplanar N atoms of pyrazolyl cycles (distances Cu—N are 1.997 (2) and 2.040 (2) Å, distance Cu—O is 2.222 (2) Å). Symmetrically equivalent ligand molecules in cis-bonding configuration are linked to CuII ion in a double-stranded bridge fashion (Fig. 1). Formed one-dimensional linear chain is running along the c axis where each Cu atom deviates from the average position by a value of ±0.279 (0) Å (Fig. 2). One of the pyrazole cycles of the ligand molecule is involved in hydrogen bonding with F atom of the tetrafluoroborate anion (N···F 2.861 (3) Å) which additionally forms a hydrogen bond with the free water molecule (F···OW 3.002 (3) Å). Further, the coordinated water molecule is connected through hydrogen bonds with the free water molecule (O···OW 2.785 (3) Å) and the Ph3PO molecule (O···O 3.115 (3) Å).

Experimental

Bis(3,5-dimethyl-1H-pyrazolyl)selenide was prepared according to early reported method (Seredyuk et al., 2007). Copper(II) tetrafluoroborate hexahydrate (0.065 g, 0.19 mmol) in water (5 ml) was added to 5 ml of hot methanol solution of the ligand (0.100 g, 0.37 mmol) and thisphenylphosphine oxide (0.052 g, 0.19 mmol). After several days green crystals of the title compound suitable for X-ray analysis were isolated. Found: C 49.06, H 4.43, N 8.22; C56H62B2CuF8N8O4P2Se2 requires: C 49.16, H 4.57, N 8.19.

Refinement

The H atoms were located from the difference Fourier map and were constrained to ride on their parent atoms with Uiso = 1.2–1.5Ueq(parent atom). The highest peak is located 0.90 Å from atom F3 and the deepest hole is located 0.67 Å from atom F2.

Figures

Fig. 1.

Fig. 1.

A portion of the crystal structure of the title compound showing the labeling scheme and 80% probability displacement ellipsoids [(i) 1.5 - x, 1.5 - y, 1 - z; (ii) 1.5 - x, 0.5 + y, 1.5 - z; (iii) -0.5 + x, 1.5 - y, 0.5 + z; (iv) 1 - x, 1 + y, 1.5 - z]. Hydrogen bonds are indicated by dashed lines. H atoms are omitted for clarity.

Fig. 2.

Fig. 2.

A packing diagram of the title compound. H atoms are omitted for clarity.

Crystal data

[Cu(C10H14N4Se)2(H2O)](BF4)2·2C18H15OP·H2O F(000) = 2820
Mr = 1386.17 Dx = 1.525 Mg m3
Monoclinic, C2/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -C 2yc Cell parameters from 34362 reflections
a = 21.4560 (4) Å θ = 3.1–28.5°
b = 15.3590 (4) Å µ = 1.70 mm1
c = 18.4910 (6) Å T = 100 K
β = 97.74 (2)° Needle, green
V = 6038.0 (3) Å3 0.09 × 0.07 × 0.04 mm
Z = 4

Data collection

Kuma KM4 CCD area-detector diffractometer 6210 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tube Rint = 0.045
graphite θmax = 27.5°, θmin = 3.1°
ω scans h = −27→27
34362 measured reflections k = −19→18
6876 independent reflections l = −24→22

Refinement

Refinement on F2 Primary atom site location: structure-invariant direct methods
Least-squares matrix: full Secondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.043 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.082 H-atom parameters constrained
S = 1.16 w = 1/[σ2(Fo2) + (0.0323P)2 + 9.8106P] where P = (Fo2 + 2Fc2)/3
6876 reflections (Δ/σ)max = 0.002
384 parameters Δρmax = 0.63 e Å3
0 restraints Δρmin = −0.38 e Å3

Special details

Experimental. The H atoms were located from the difference Fourier map and were constrained to ride on their parent atoms with Uiso = 1.2–1.5Ueq(parent atom). The highest peak is located 0.90 Å from atom F3 and the deepest hole is located 0.67 Å from atom F2.
Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'s involving l.s. planes.
Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > 2σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)

x y z Uiso*/Ueq
C1 0.76965 (12) 0.52259 (18) 0.58609 (14) 0.0230 (6)
H1A 0.7463 0.4882 0.6180 0.035*
H1B 0.7520 0.5126 0.5351 0.035*
H1C 0.7664 0.5845 0.5977 0.035*
C2 0.83728 (11) 0.49578 (16) 0.59738 (12) 0.0161 (5)
C3 0.87223 (11) 0.44383 (15) 0.55608 (12) 0.0150 (5)
C4 0.93294 (11) 0.43713 (15) 0.59578 (12) 0.0140 (5)
C5 0.98757 (11) 0.38947 (16) 0.57328 (13) 0.0163 (5)
H5A 1.0132 0.4296 0.5485 0.025*
H5B 0.9724 0.3421 0.5400 0.025*
H5C 1.0131 0.3653 0.6165 0.025*
C6 0.97077 (12) 0.35740 (16) 0.37061 (14) 0.0199 (5)
H6A 0.9845 0.3431 0.3236 0.030*
H6B 0.9494 0.3070 0.3885 0.030*
H6C 1.0075 0.3725 0.4059 0.030*
C7 0.92668 (11) 0.43281 (15) 0.36128 (12) 0.0142 (5)
C8 0.87522 (11) 0.45220 (15) 0.39826 (12) 0.0134 (5)
C9 0.84777 (11) 0.52685 (16) 0.36613 (12) 0.0156 (5)
C10 0.78973 (12) 0.57463 (17) 0.37889 (14) 0.0207 (5)
H10A 0.7855 0.6274 0.3489 0.031*
H10B 0.7926 0.5906 0.4305 0.031*
H10C 0.7530 0.5372 0.3656 0.031*
C11 0.93216 (12) 0.04009 (16) 0.84170 (13) 0.0172 (5)
C12 0.97655 (13) −0.02714 (16) 0.84964 (13) 0.0204 (5)
H12 1.0177 −0.0166 0.8740 0.024*
C13 0.96033 (14) −0.10957 (17) 0.82184 (15) 0.0264 (6)
H13 0.9906 −0.1551 0.8269 0.032*
C14 0.90039 (15) −0.12532 (19) 0.78687 (15) 0.0326 (7)
H14 0.8894 −0.1818 0.7683 0.039*
C15 0.85628 (15) −0.0592 (2) 0.77881 (15) 0.0328 (7)
H15 0.8151 −0.0704 0.7547 0.039*
C16 0.87171 (13) 0.02374 (18) 0.80581 (14) 0.0252 (6)
H16 0.8413 0.0690 0.7999 0.030*
C17 0.89479 (12) 0.09403 (16) 0.99831 (13) 0.0192 (5)
H17 0.9065 0.0365 0.9869 0.023*
C18 0.86575 (12) 0.10921 (18) 1.06015 (14) 0.0234 (6)
H18 0.8580 0.0620 1.0909 0.028*
C19 0.84825 (13) 0.19234 (19) 1.07704 (15) 0.0263 (6)
H19 0.8285 0.2024 1.1193 0.032*
C20 0.90673 (11) 0.16311 (15) 0.95319 (13) 0.0151 (5)
C21 1.07652 (13) 0.14666 (17) 0.86366 (15) 0.0234 (6)
H21 1.0631 0.1465 0.8126 0.028*
C22 1.11652 (13) 0.14863 (17) 1.01317 (15) 0.0236 (6)
H22 1.1304 0.1496 1.0642 0.028*
C23 1.05261 (12) 0.14969 (16) 0.98780 (13) 0.0183 (5)
H23 1.0228 0.1510 1.0215 0.022*
C24 1.03194 (12) 0.14881 (15) 0.91255 (13) 0.0160 (5)
C25 1.16016 (13) 0.14610 (17) 0.96428 (16) 0.0262 (6)
H25 1.2038 0.1453 0.9819 0.031*
C26 0.88851 (13) 0.24716 (17) 0.97001 (15) 0.0244 (6)
H26 0.8959 0.2945 0.9392 0.029*
C27 0.85963 (14) 0.26146 (19) 1.03183 (16) 0.0311 (7)
H27 0.8476 0.3188 1.0434 0.037*
C28 1.14020 (13) 0.14472 (19) 0.88991 (16) 0.0283 (6)
H28 1.1703 0.1424 0.8567 0.034*
N1 0.87644 (9) 0.51791 (13) 0.65756 (10) 0.0159 (4)
H1N 0.8655 0.5510 0.6926 0.019*
N2 0.93546 (9) 0.48303 (13) 0.65830 (10) 0.0132 (4)
N3 0.93111 (9) 0.49421 (12) 0.30991 (10) 0.0130 (4)
N4 0.88268 (9) 0.55081 (13) 0.31437 (10) 0.0140 (4)
H4N 0.8752 0.5973 0.2867 0.017*
O1 1.0000 0.33717 (15) 0.7500 0.0184 (5)
H1O 0.9810 0.3047 0.7736 0.028*
O2 0.93330 (8) 0.21702 (11) 0.81896 (9) 0.0200 (4)
O1W 0.84524 (9) 0.31134 (11) 0.72590 (10) 0.0238 (4)
H1W 0.8041 0.2973 0.7207 0.036*
H2W 0.8687 0.2652 0.7505 0.036*
Cu1 1.0000 0.48181 (3) 0.7500 0.01134 (9)
Se1 0.841882 (11) 0.382203 (16) 0.468941 (12) 0.01567 (7)
P1 0.94959 (3) 0.14841 (4) 0.87644 (3) 0.01450 (13)
B1 0.71450 (15) 0.1759 (2) 0.75026 (17) 0.0261 (7)
F4 0.65217 (8) 0.17089 (10) 0.76495 (9) 0.0292 (4)
F3 0.75223 (9) 0.21024 (12) 0.81081 (10) 0.0423 (5)
F1 0.73540 (9) 0.09284 (12) 0.73760 (10) 0.0459 (5)
F2 0.71809 (9) 0.22853 (14) 0.68996 (10) 0.0503 (5)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0159 (13) 0.0333 (15) 0.0200 (13) 0.0052 (11) 0.0030 (10) −0.0026 (11)
C2 0.0145 (12) 0.0212 (12) 0.0127 (11) 0.0000 (10) 0.0028 (9) 0.0022 (9)
C3 0.0155 (12) 0.0189 (12) 0.0111 (11) −0.0018 (9) 0.0037 (9) 0.0021 (9)
C4 0.0172 (12) 0.0148 (11) 0.0107 (11) −0.0012 (9) 0.0045 (9) 0.0027 (9)
C5 0.0153 (12) 0.0201 (12) 0.0134 (11) 0.0030 (10) 0.0014 (9) −0.0025 (9)
C6 0.0209 (13) 0.0201 (13) 0.0197 (12) 0.0031 (10) 0.0064 (10) 0.0033 (10)
C7 0.0136 (12) 0.0179 (12) 0.0111 (11) −0.0026 (9) 0.0016 (9) −0.0020 (9)
C8 0.0115 (11) 0.0179 (12) 0.0107 (10) −0.0023 (9) 0.0015 (9) −0.0026 (9)
C9 0.0154 (12) 0.0197 (12) 0.0116 (11) −0.0007 (10) 0.0019 (9) −0.0018 (9)
C10 0.0175 (13) 0.0262 (14) 0.0191 (12) 0.0042 (10) 0.0045 (10) −0.0011 (10)
C11 0.0211 (13) 0.0197 (12) 0.0118 (11) −0.0025 (10) 0.0053 (9) 0.0012 (9)
C12 0.0236 (14) 0.0201 (13) 0.0184 (12) −0.0010 (10) 0.0062 (10) 0.0004 (10)
C13 0.0363 (16) 0.0205 (13) 0.0245 (13) −0.0015 (12) 0.0119 (12) −0.0022 (11)
C14 0.048 (2) 0.0277 (15) 0.0234 (14) −0.0133 (14) 0.0115 (13) −0.0091 (12)
C15 0.0329 (17) 0.0432 (18) 0.0210 (14) −0.0154 (14) −0.0015 (12) −0.0022 (12)
C16 0.0229 (14) 0.0309 (15) 0.0213 (13) −0.0015 (11) 0.0017 (11) 0.0016 (11)
C17 0.0187 (13) 0.0180 (12) 0.0218 (13) 0.0002 (10) 0.0063 (10) 0.0014 (10)
C18 0.0212 (14) 0.0280 (14) 0.0223 (13) −0.0012 (11) 0.0078 (11) 0.0063 (11)
C19 0.0238 (14) 0.0356 (16) 0.0217 (13) −0.0007 (12) 0.0114 (11) −0.0048 (11)
C20 0.0120 (11) 0.0172 (12) 0.0164 (11) 0.0012 (9) 0.0030 (9) 0.0016 (9)
C21 0.0234 (14) 0.0269 (14) 0.0213 (13) 0.0021 (11) 0.0084 (11) 0.0038 (11)
C22 0.0214 (14) 0.0227 (13) 0.0252 (14) 0.0010 (11) −0.0020 (11) 0.0023 (11)
C23 0.0180 (13) 0.0175 (12) 0.0201 (12) 0.0005 (10) 0.0056 (10) 0.0008 (9)
C24 0.0166 (12) 0.0127 (11) 0.0194 (12) 0.0010 (9) 0.0045 (10) 0.0016 (9)
C25 0.0141 (13) 0.0231 (13) 0.0408 (16) 0.0011 (10) 0.0019 (11) 0.0076 (12)
C26 0.0254 (14) 0.0187 (13) 0.0318 (15) 0.0015 (11) 0.0140 (12) 0.0033 (11)
C27 0.0348 (17) 0.0221 (14) 0.0398 (17) 0.0035 (12) 0.0177 (14) −0.0056 (12)
C28 0.0199 (14) 0.0318 (15) 0.0359 (16) 0.0044 (11) 0.0137 (12) 0.0100 (12)
N1 0.0150 (10) 0.0210 (10) 0.0121 (9) 0.0046 (8) 0.0032 (8) −0.0002 (8)
N2 0.0113 (10) 0.0175 (10) 0.0113 (9) 0.0021 (8) 0.0029 (7) 0.0013 (7)
N3 0.0120 (10) 0.0157 (10) 0.0114 (9) 0.0017 (8) 0.0018 (7) 0.0006 (7)
N4 0.0138 (10) 0.0151 (10) 0.0135 (9) 0.0026 (8) 0.0028 (8) 0.0017 (7)
O1 0.0212 (13) 0.0162 (12) 0.0203 (12) 0.000 0.0111 (10) 0.000
O2 0.0196 (9) 0.0212 (9) 0.0195 (9) 0.0008 (7) 0.0038 (7) 0.0072 (7)
O1W 0.0204 (10) 0.0215 (9) 0.0283 (10) −0.0019 (8) −0.0006 (8) −0.0022 (8)
Cu1 0.0110 (2) 0.0155 (2) 0.00792 (18) 0.000 0.00246 (14) 0.000
Se1 0.01537 (13) 0.02050 (13) 0.01152 (11) −0.00501 (10) 0.00324 (8) −0.00052 (9)
P1 0.0146 (3) 0.0151 (3) 0.0144 (3) 0.0005 (2) 0.0040 (2) 0.0027 (2)
B1 0.0247 (17) 0.0276 (16) 0.0271 (16) −0.0012 (13) 0.0066 (13) −0.0015 (13)
F4 0.0275 (9) 0.0238 (8) 0.0369 (9) −0.0034 (7) 0.0066 (7) 0.0056 (7)
F3 0.0413 (11) 0.0443 (11) 0.0420 (10) −0.0186 (9) 0.0080 (8) −0.0179 (8)
F1 0.0429 (11) 0.0384 (10) 0.0501 (12) 0.0178 (9) −0.0167 (9) −0.0192 (9)
F2 0.0476 (12) 0.0625 (13) 0.0447 (11) 0.0072 (10) 0.0209 (9) 0.0234 (10)

Geometric parameters (Å, °)

C1—C2 1.496 (3) C17—H17 0.9500
C1—H1A 0.9800 C18—C19 1.378 (4)
C1—H1B 0.9800 C18—H18 0.9500
C1—H1C 0.9800 C19—C27 1.393 (4)
C2—N1 1.345 (3) C19—H19 0.9500
C2—C3 1.392 (3) C20—C26 1.396 (3)
C3—C4 1.410 (3) C20—P1 1.806 (2)
C3—Se1 1.906 (2) C21—C28 1.387 (4)
C4—N2 1.349 (3) C21—C24 1.402 (3)
C4—C5 1.488 (3) C21—H21 0.9500
C5—H5A 0.9800 C22—C25 1.387 (4)
C5—H5B 0.9800 C22—C23 1.388 (4)
C5—H5C 0.9800 C22—H22 0.9500
C6—C7 1.491 (3) C23—C24 1.402 (3)
C6—H6A 0.9800 C23—H23 0.9500
C6—H6B 0.9800 C24—P1 1.803 (3)
C6—H6C 0.9800 C25—C28 1.384 (4)
C7—N3 1.351 (3) C25—H25 0.9500
C7—C8 1.407 (3) C26—C27 1.389 (4)
C8—C9 1.386 (3) C26—H26 0.9500
C8—Se1 1.905 (2) C27—H27 0.9500
C9—N4 1.344 (3) C28—H28 0.9500
C9—C10 1.491 (3) N1—N2 1.373 (3)
C10—H10A 0.9800 N1—H1N 0.8800
C10—H10B 0.9800 N2—Cu1 2.0397 (19)
C10—H10C 0.9800 N3—N4 1.366 (3)
C11—C16 1.398 (4) N3—Cu1i 1.9971 (19)
C11—C12 1.399 (4) N4—H4N 0.8800
C11—P1 1.804 (2) O1—Cu1 2.222 (2)
C12—C13 1.393 (4) O1—H1O 0.8082
C12—H12 0.9500 O2—P1 1.5040 (17)
C13—C14 1.381 (4) O1W—H1W 0.9003
C13—H13 0.9500 O1W—H2W 0.9489
C14—C15 1.383 (4) Cu1—N3ii 1.9971 (19)
C14—H14 0.9500 Cu1—N3i 1.9971 (19)
C15—C16 1.391 (4) Cu1—N2iii 2.0397 (19)
C15—H15 0.9500 B1—F1 1.383 (4)
C16—H16 0.9500 B1—F2 1.387 (4)
C17—C18 1.394 (3) B1—F3 1.394 (4)
C17—C20 1.395 (3) B1—F4 1.402 (4)
C2—C1—H1A 109.5 C18—C19—H19 120.2
C2—C1—H1B 109.5 C27—C19—H19 120.2
H1A—C1—H1B 109.5 C17—C20—C26 119.4 (2)
C2—C1—H1C 109.5 C17—C20—P1 121.94 (18)
H1A—C1—H1C 109.5 C26—C20—P1 118.57 (18)
H1B—C1—H1C 109.5 C28—C21—C24 120.0 (2)
N1—C2—C3 106.0 (2) C28—C21—H21 120.0
N1—C2—C1 122.2 (2) C24—C21—H21 120.0
C3—C2—C1 131.7 (2) C25—C22—C23 120.2 (2)
C2—C3—C4 106.5 (2) C25—C22—H22 119.9
C2—C3—Se1 126.91 (18) C23—C22—H22 119.9
C4—C3—Se1 126.17 (17) C22—C23—C24 120.1 (2)
N2—C4—C3 109.6 (2) C22—C23—H23 120.0
N2—C4—C5 123.7 (2) C24—C23—H23 120.0
C3—C4—C5 126.7 (2) C21—C24—C23 119.2 (2)
C4—C5—H5A 109.5 C21—C24—P1 118.74 (19)
C4—C5—H5B 109.5 C23—C24—P1 122.04 (19)
H5A—C5—H5B 109.5 C28—C25—C22 120.2 (3)
C4—C5—H5C 109.5 C28—C25—H25 119.9
H5A—C5—H5C 109.5 C22—C25—H25 119.9
H5B—C5—H5C 109.5 C27—C26—C20 119.9 (2)
C7—C6—H6A 109.5 C27—C26—H26 120.0
C7—C6—H6B 109.5 C20—C26—H26 120.0
H6A—C6—H6B 109.5 C26—C27—C19 120.5 (3)
C7—C6—H6C 109.5 C26—C27—H27 119.8
H6A—C6—H6C 109.5 C19—C27—H27 119.8
H6B—C6—H6C 109.5 C25—C28—C21 120.4 (2)
N3—C7—C8 109.2 (2) C25—C28—H28 119.8
N3—C7—C6 121.3 (2) C21—C28—H28 119.8
C8—C7—C6 129.5 (2) C2—N1—N2 112.47 (19)
C9—C8—C7 106.4 (2) C2—N1—H1N 123.8
C9—C8—Se1 125.73 (18) N2—N1—H1N 123.8
C7—C8—Se1 127.30 (18) C4—N2—N1 105.36 (18)
N4—C9—C8 106.6 (2) C4—N2—Cu1 130.69 (16)
N4—C9—C10 122.4 (2) N1—N2—Cu1 122.26 (14)
C8—C9—C10 130.9 (2) C7—N3—N4 105.99 (18)
C9—C10—H10A 109.5 C7—N3—Cu1i 130.26 (16)
C9—C10—H10B 109.5 N4—N3—Cu1i 122.83 (14)
H10A—C10—H10B 109.5 C9—N4—N3 111.75 (19)
C9—C10—H10C 109.5 C9—N4—H4N 124.1
H10A—C10—H10C 109.5 N3—N4—H4N 124.1
H10B—C10—H10C 109.5 Cu1—O1—H1O 128.2
C16—C11—C12 119.5 (2) H1W—O1W—H2W 108.7
C16—C11—P1 118.0 (2) N3ii—Cu1—N3i 158.75 (11)
C12—C11—P1 122.53 (19) N3ii—Cu1—N2 89.38 (8)
C13—C12—C11 120.0 (3) N3i—Cu1—N2 90.43 (8)
C13—C12—H12 120.0 N3ii—Cu1—N2iii 90.43 (8)
C11—C12—H12 120.0 N3i—Cu1—N2iii 89.38 (8)
C14—C13—C12 120.2 (3) N2—Cu1—N2iii 178.95 (11)
C14—C13—H13 119.9 N3ii—Cu1—O1 100.62 (6)
C12—C13—H13 119.9 N3i—Cu1—O1 100.62 (6)
C13—C14—C15 120.2 (3) N2—Cu1—O1 90.53 (6)
C13—C14—H14 119.9 N2iii—Cu1—O1 90.53 (6)
C15—C14—H14 119.9 C8—Se1—C3 100.52 (10)
C14—C15—C16 120.5 (3) O2—P1—C24 112.46 (11)
C14—C15—H15 119.7 O2—P1—C11 112.16 (11)
C16—C15—H15 119.7 C24—P1—C11 106.30 (11)
C15—C16—C11 119.7 (3) O2—P1—C20 111.92 (11)
C15—C16—H16 120.2 C24—P1—C20 106.62 (11)
C11—C16—H16 120.2 C11—P1—C20 106.98 (11)
C18—C17—C20 120.1 (2) F1—B1—F2 110.3 (2)
C18—C17—H17 119.9 F1—B1—F3 108.6 (3)
C20—C17—H17 119.9 F2—B1—F3 109.7 (3)
C19—C18—C17 120.4 (2) F1—B1—F4 108.7 (2)
C19—C18—H18 119.8 F2—B1—F4 110.2 (2)
C17—C18—H18 119.8 F3—B1—F4 109.3 (2)
C18—C19—C27 119.7 (2)
N1—C2—C3—C4 0.3 (3) C3—C4—N2—N1 0.2 (2)
C1—C2—C3—C4 −176.6 (3) C5—C4—N2—N1 178.7 (2)
N1—C2—C3—Se1 173.45 (17) C3—C4—N2—Cu1 165.24 (16)
C1—C2—C3—Se1 −3.4 (4) C5—C4—N2—Cu1 −16.2 (3)
C2—C3—C4—N2 −0.3 (3) C2—N1—N2—C4 0.0 (3)
Se1—C3—C4—N2 −173.53 (16) C2—N1—N2—Cu1 −166.62 (16)
C2—C3—C4—C5 −178.8 (2) C8—C7—N3—N4 −0.5 (2)
Se1—C3—C4—C5 8.0 (3) C6—C7—N3—N4 177.6 (2)
N3—C7—C8—C9 1.3 (3) C8—C7—N3—Cu1i 168.54 (16)
C6—C7—C8—C9 −176.6 (2) C6—C7—N3—Cu1i −13.4 (3)
N3—C7—C8—Se1 173.23 (16) C8—C9—N4—N3 1.3 (3)
C6—C7—C8—Se1 −4.7 (4) C10—C9—N4—N3 −176.2 (2)
C7—C8—C9—N4 −1.6 (3) C7—N3—N4—C9 −0.5 (2)
Se1—C8—C9—N4 −173.66 (16) Cu1i—N3—N4—C9 −170.57 (15)
C7—C8—C9—C10 175.6 (2) C4—N2—Cu1—N3ii −146.4 (2)
Se1—C8—C9—C10 3.5 (4) N1—N2—Cu1—N3ii 16.47 (17)
C16—C11—C12—C13 0.0 (4) C4—N2—Cu1—N3i 54.8 (2)
P1—C11—C12—C13 179.83 (19) N1—N2—Cu1—N3i −142.28 (17)
C11—C12—C13—C14 −0.5 (4) C4—N2—Cu1—O1 −45.8 (2)
C12—C13—C14—C15 0.5 (4) N1—N2—Cu1—O1 117.09 (17)
C13—C14—C15—C16 −0.1 (4) C9—C8—Se1—C3 −84.4 (2)
C14—C15—C16—C11 −0.4 (4) C7—C8—Se1—C3 105.1 (2)
C12—C11—C16—C15 0.4 (4) C2—C3—Se1—C8 106.5 (2)
P1—C11—C16—C15 −179.4 (2) C4—C3—Se1—C8 −81.6 (2)
C20—C17—C18—C19 0.4 (4) C21—C24—P1—O2 −51.1 (2)
C17—C18—C19—C27 0.1 (4) C23—C24—P1—O2 130.0 (2)
C18—C17—C20—C26 −0.9 (4) C21—C24—P1—C11 72.0 (2)
C18—C17—C20—P1 175.1 (2) C23—C24—P1—C11 −106.8 (2)
C25—C22—C23—C24 −0.4 (4) C21—C24—P1—C20 −174.10 (19)
C28—C21—C24—C23 0.5 (4) C23—C24—P1—C20 7.0 (2)
C28—C21—C24—P1 −178.4 (2) C16—C11—P1—O2 −52.4 (2)
C22—C23—C24—C21 0.2 (4) C12—C11—P1—O2 127.8 (2)
C22—C23—C24—P1 179.02 (19) C16—C11—P1—C24 −175.71 (19)
C23—C22—C25—C28 0.1 (4) C12—C11—P1—C24 4.5 (2)
C17—C20—C26—C27 0.9 (4) C16—C11—P1—C20 70.7 (2)
P1—C20—C26—C27 −175.2 (2) C12—C11—P1—C20 −109.1 (2)
C20—C26—C27—C19 −0.5 (4) C17—C20—P1—O2 155.2 (2)
C18—C19—C27—C26 −0.1 (5) C26—C20—P1—O2 −28.8 (2)
C22—C25—C28—C21 0.6 (4) C17—C20—P1—C24 −81.5 (2)
C24—C21—C28—C25 −0.9 (4) C26—C20—P1—C24 94.6 (2)
C3—C2—N1—N2 −0.2 (3) C17—C20—P1—C11 31.9 (2)
C1—C2—N1—N2 177.0 (2) C26—C20—P1—C11 −152.0 (2)

Symmetry codes: (i) −x+2, −y+1, −z+1; (ii) x, −y+1, z+1/2; (iii) −x+2, y, −z+3/2.

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
O1W—H1W···F2 0.90 2.14 3.002 (3) 161
O1W—H1W···F3 0.90 2.51 3.115 (3) 125
O1W—H2W···O2 0.95 1.90 2.785 (3) 155
O1—H1O···O2 0.81 1.95 2.752 (2) 173
N1—H1N···F4iv 0.88 2.06 2.861 (3) 152
N4—H4N···O1Wv 0.88 1.86 2.730 (3) 170

Symmetry codes: (iv) −x+3/2, y+1/2, −z+3/2; (v) x, −y+1, z−1/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: DS2023).

References

  1. Farha, O. K., Spokoyny, A. M., Mulfort, K. L., Galli, S., Hupp, J. T. & Mirkin, C. A. (2009). Small, 5, 1727–1731. [DOI] [PubMed]
  2. Farrugia, L. J. (1997). J. Appl. Cryst.30, 565.
  3. Farrugia, L. J. (1999). J. Appl. Cryst.32, 837–838.
  4. Kuma (1999). KM-4-CCD Software Kuma Diffraction, Wrocław, Poland.
  5. Seredyuk, M., Haukka, M., Fritsky, I. O., Kozłowski, H., Krämer, R., Pavlenko, V. A. & Gütlich, P. (2007). Dalton Trans. pp. 3183–3194. [DOI] [PubMed]
  6. Seredyuk, M., Haukka, M., Pavlenko, V. A. & Fritsky, I. O. (2009). Acta Cryst. E65, m1396. [DOI] [PMC free article] [PubMed]
  7. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  8. Shibahara, S., Kitagawa, H., Kubo, T. & Nakasuji, K. (2007). Inorg. Chem. Commun.10, 860–862. [DOI] [PubMed]
  9. Zhang, Y.-B., Zhang, W.-X., Feng, F.-Y., Zhang, J.-P. & Chen, X.-M. (2009). Angew. Chem. Int. Ed. Engl.48, 5287–5290. [DOI] [PubMed]

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810012997/ds2023sup1.cif

e-66-0m527-sup1.cif (28.5KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810012997/ds2023Isup2.hkl

e-66-0m527-Isup2.hkl (329.8KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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