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Acta Crystallographica Section E: Crystallographic Communications logoLink to Acta Crystallographica Section E: Crystallographic Communications
. 2015 Feb 7;71(Pt 3):m54. doi: 10.1107/S2056989015002169

Crystal structure of [1-(2,6-diiso­propyl­phen­yl)-2,4-bis­(di­methyl­amino)-5-tri­methyl­silyl-1,3,5-tri­aza­penta­dienyl-κ2 N 1,N 5](tri­phenyl­phosphane-κP)copper(I)

Feiguang Li a, Lei Yan a, Hongbo Tong a, Meisu Zhou a,*
PMCID: PMC4350696  PMID: 25844205

Abstract

The title complex, [Cu(C21H38N5Si)(C18H15P)], was obtained from the one-pot reaction between (Dipp)N(Li)SiMe3 (Dipp = 2,6-diiso­propyl­phen­yl), Me2NCN, CuCl and PPh3. The CuI atom has a distorted trigonal–planar coordination sphere. The tri­aza­penta­dienyl ligand acts as a κ2-donor. The N—Cu—N bond angle is 95.88 (14)°. In the tri­aza­penta­dienyl fragment, the C—N bond lengths are in the range 1.328 (5)–1.349 (5) Å, which indicates delocalization of the π-electrons in the NCNCN system.

Keywords: crystal structure, tri­aza­penta­dien­yl, copper(I) complex

Related literature  

For reviews of related ligands and metals, see: Dias & Singh (2004); Flores et al. (2009); Xie et al. (2014); Zhou et al. (2008, 2011); Liu et al. (2013).graphic file with name e-71-00m54-scheme1.jpg

Experimental  

Crystal data  

  • [Cu(C21H38N5Si)(C18H15P)]

  • M r = 714.46

  • Triclinic, Inline graphic

  • a = 9.7935 (16) Å

  • b = 11.2141 (18) Å

  • c = 19.570 (3) Å

  • α = 103.601 (4)°

  • β = 90.867 (3)°

  • γ = 108.240 (4)°

  • V = 1974.8 (6) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.66 mm−1

  • T = 195 K

  • 0.32 × 0.31 × 0.28 mm

Data collection  

  • Bruker APEXII CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2000) T min = 0.818, T max = 0.838

  • 11084 measured reflections

  • 6988 independent reflections

  • 3246 reflections with I > 2σ(I)

  • R int = 0.077

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.051

  • wR(F 2) = 0.089

  • S = 0.75

  • 6988 reflections

  • 435 parameters

  • 12 restraints

  • H-atom parameters constrained

  • Δρmax = 0.35 e Å−3

  • Δρmin = −0.24 e Å−3

Data collection: APEX2 (Bruker, 2000); cell refinement: SAINT (Bruker, 2000); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL.

Supplementary Material

Crystal structure: contains datablock(s) I, New_Global_Publ_Block. DOI: 10.1107/S2056989015002169/lx2294sup1.cif

e-71-00m54-sup1.cif (437.1KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989015002169/lx2294Isup2.hkl

e-71-00m54-Isup2.hkl (341.9KB, hkl)

Supporting information file. DOI: 10.1107/S2056989015002169/lx2294Isup3.txt

e-71-00m54-Isup3.txt (92.6KB, txt)

. DOI: 10.1107/S2056989015002169/lx2294fig1.tif

The mol­ecular structure of (I), showing the atom-numbering scheme. Displacement ellipsoids are drawn at the 30% probability level. H atoms are presented as a small spheres of arbitrary radius.

CCDC reference: 1046645

Additional supporting information: crystallographic information; 3D view; checkCIF report

Acknowledgments

The authors acknowledge the financial support of the Natural Science Foundation of China (grant No. 21371111), the Shanxi Functional Organometallic Compound Information Net Project (grant No. 2013091022) and the Shanxi Scholarship Council of China (grant No. 2013–025).

supplementary crystallographic information

S1. Synthesis and crystallization

Me2NCN (0.41 mL, 5.06 mmol) was added to a solution of (Dipp)N(Li)SiMe3 (0.65 g, 2.53 mmol) in Et2O (30 cm3) at -78°C. The resulting mixture was warmed to ca. 25°C and stirred overnight. CuCl (0.25 g, 2.53 mmol) and PPh3 (0.66 g, 2.53 mmol) were added at -78°C. The resulting mixture was allowed to warm to ca. 25°C and stirred overnight. Filtered and the filtrate was concentrated in vacuo and stored at 25°C for 4 d, yielding colorless crystals of the title compound (0.62 g, 34 %).

Anal. calcd. for C39H53N5PSiCu (%): C, 65.56; H, 7.48; N, 9.80. Found: C, 65.59; H, 7.50; N, 9.76. All manipulations were performed under argon using standard Schlenk and vacuum line techniques. Et2O was dried and distilled over Na under argon prior to use. Elemental analysis is completely in agreement with the structure of the compound.

S2. Refinement

All H atoms were positioned geometrically and refined using a riding model, with C—H = 0.95 Å for aryl, 1.00 Å for methine and 0.98 Å for methyl H atoms, respectively. Uiso(H) = 1.2Ueq(C) for aryl and methine, and 1.5Ueq(C) for methyl H atoms. The positions of methyl hydrogens were optimized using the SHELXL-97's command AFIX 137 (Sheldrick, 2008).

S3. Results and discussion

1,3,5–Tri­aza­penta­dienyl ligands are one of the most useful nitro­gen-based ligands in coordination chemistry and organometallic chemistry due to their structural features and stronger coordination properties(Dias & Singh, 2004; Flores et al., 2009). Our group has developed a series of 2,4–N,N'–substituted–1,3,5–tri­aza­penta­dienyl ligands and obtained their Fe,Co,Mg,Cu(I) complexes (Xie et al. , 2014; Zhou et al., 2011; Liu et al., 2013).The title compound is polymorph of C39H53N5PSiCu which was reported in 2008(Zhou et al., 2008).This article will provide a new set of unit cell data on the 1,3,5– tri­aza­penta­dienyl (tri­phenyl­phosphane) copper(I) compound C39H53N5PSiCu.

Its molecular structure is shown in Fig. 1. In the monomeric molecular structure of title compound, the dihedral angle between N1C13C16N3 and C13N2C16 is 14.16(0.65)°, and the dihedral angle between N1C13C16N3 and N1CuN3 is 3.30(0.33)°. The bond angles of N5—C16—N3, C16—N3—C13, and N3—C13—N1 are 127.8 (4), 125.8 (4), and 124.6 (4)°, respectively. The N1C13C16N3 plane is twisted by about 26.47(0.28)° from the N1N5CuP plane. The tri­aza­penta­dienyl ligand acts as a κ2-donor. The bond angle of N1—Cu—N5 is 95.88 (14)°. In the tri­aza­penta­dienyl fragment, the C—N bond distances are in the range of 1.328 (5)–1.349 (5) Å, which indicates the delocalization of the π-electrons as a η5 anion in the NCNCN system.Cu located above 0.172 (2) Å from P1–N1–N5 triangular plane.

Figures

Fig. 1.

Fig. 1.

The molecular structure of (I), showing the atom-numbering scheme. Displacement ellipsoids are drawn at the 30% probability level. H atoms are presented as a small spheres of arbitrary radius.

Crystal data

[Cu(C21H38N5Si)(C18H15P)] Z = 2
Mr = 714.46 F(000) = 760
Triclinic, P1 Dx = 1.202 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 9.7935 (16) Å Cell parameters from 1276 reflections
b = 11.2141 (18) Å θ = 2.5–18.7°
c = 19.570 (3) Å µ = 0.66 mm1
α = 103.601 (4)° T = 195 K
β = 90.867 (3)° Block, colorless
γ = 108.240 (4)° 0.32 × 0.31 × 0.28 mm
V = 1974.8 (6) Å3

Data collection

Bruker APEXII CCD diffractometer 6988 independent reflections
Radiation source: fine-focus sealed tube 3246 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.077
φ and ω scans θmax = 25.1°, θmin = 1.1°
Absorption correction: multi-scan (SADABS; Bruker, 2000) h = −11→9
Tmin = 0.818, Tmax = 0.838 k = −11→13
11084 measured reflections l = −23→23

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)] = 0.051 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.089 H-atom parameters constrained
S = 0.75 w = 1/[σ2(Fo2) + (0.P)2] where P = (Fo2 + 2Fc2)/3
6988 reflections (Δ/σ)max < 0.001
435 parameters Δρmax = 0.35 e Å3
12 restraints Δρmin = −0.24 e Å3

Special details

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.
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 > σ(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
Cu1 0.21585 (5) 0.98646 (5) 0.27053 (3) 0.04164 (17)
P1 0.09334 (12) 0.97196 (11) 0.17417 (6) 0.0438 (3)
N1 0.3161 (3) 0.8786 (3) 0.30319 (17) 0.0404 (9)
N2 0.4998 (4) 0.8723 (4) 0.3817 (2) 0.0611 (11)
N3 0.5058 (3) 1.0667 (3) 0.36417 (17) 0.0472 (9)
N4 0.5552 (4) 1.2786 (4) 0.3743 (2) 0.0625 (11)
N5 0.3128 (4) 1.1463 (3) 0.34393 (16) 0.0425 (9)
Si1 0.21254 (13) 1.22563 (12) 0.39437 (6) 0.0481 (3)
C1 0.2675 (4) 0.7442 (4) 0.2716 (2) 0.0368 (10)
C2 0.3404 (5) 0.6878 (4) 0.2203 (2) 0.0436 (11)
C3 0.2818 (5) 0.5576 (4) 0.1869 (2) 0.0602 (13)
H3 0.3326 0.5185 0.1524 0.072*
C4 0.1516 (6) 0.4838 (5) 0.2026 (3) 0.0649 (14)
H4 0.1118 0.3947 0.1783 0.078*
C5 0.0795 (5) 0.5377 (4) 0.2528 (3) 0.0602 (14)
H5 −0.0098 0.4855 0.2641 0.072*
C6 0.1343 (5) 0.6682 (4) 0.2878 (2) 0.0496 (12)
C7 0.0520 (5) 0.7255 (5) 0.3453 (3) 0.0779 (17)
H7 0.1096 0.8188 0.3657 0.093*
C8 0.0293 (7) 0.6572 (7) 0.4055 (3) 0.148 (3)
H8A −0.0164 0.7020 0.4427 0.222*
H8B 0.1228 0.6589 0.4250 0.222*
H8C −0.0331 0.5669 0.3873 0.222*
C9 −0.0938 (6) 0.7191 (6) 0.3153 (3) 0.128 (2)
H9A −0.1489 0.6290 0.2913 0.192*
H9B −0.0806 0.7728 0.2814 0.192*
H9C −0.1464 0.7513 0.3536 0.192*
C10 0.4816 (5) 0.7661 (4) 0.1990 (3) 0.0612 (13)
H10 0.5233 0.8474 0.2375 0.073*
C11 0.5904 (6) 0.6964 (5) 0.1891 (4) 0.153 (3)
H11A 0.6046 0.6690 0.2319 0.230*
H11B 0.6823 0.7545 0.1799 0.230*
H11C 0.5555 0.6199 0.1489 0.230*
C12 0.4540 (6) 0.8046 (6) 0.1327 (3) 0.137 (3)
H12A 0.5463 0.8468 0.1161 0.205*
H12B 0.3987 0.8650 0.1427 0.205*
H12C 0.3989 0.7271 0.0961 0.205*
C13 0.4329 (5) 0.9383 (4) 0.3489 (2) 0.0437 (11)
C14 0.6398 (5) 0.9422 (5) 0.4222 (3) 0.106 (2)
H14A 0.6997 1.0021 0.3968 0.159*
H14B 0.6876 0.8801 0.4283 0.159*
H14C 0.6260 0.9912 0.4685 0.159*
C15 0.4316 (6) 0.7524 (5) 0.3966 (3) 0.110 (2)
H15A 0.3271 0.7272 0.3851 0.164*
H15B 0.4521 0.7599 0.4469 0.164*
H15C 0.4681 0.6864 0.3683 0.164*
C16 0.4503 (5) 1.1592 (4) 0.3590 (2) 0.0458 (11)
C17 0.7011 (5) 1.3023 (4) 0.4024 (3) 0.0821 (17)
H17A 0.7025 1.2352 0.4264 0.123*
H17B 0.7363 1.3877 0.4362 0.123*
H17C 0.7635 1.3002 0.3638 0.123*
C18 0.5366 (5) 1.3833 (4) 0.3462 (3) 0.0809 (17)
H18A 0.6148 1.4108 0.3169 0.121*
H18B 0.5392 1.4569 0.3854 0.121*
H18C 0.4436 1.3521 0.3176 0.121*
C19 0.3128 (5) 1.3379 (4) 0.4780 (2) 0.0682 (14)
H19A 0.3866 1.3053 0.4936 0.102*
H19B 0.2455 1.3434 0.5143 0.102*
H19C 0.3592 1.4242 0.4703 0.102*
C20 0.0592 (4) 1.1020 (4) 0.4188 (2) 0.0745 (15)
H20A 0.0047 1.0390 0.3759 0.112*
H20B −0.0043 1.1445 0.4453 0.112*
H20C 0.0962 1.0571 0.4483 0.112*
C21 0.1368 (5) 1.3199 (4) 0.3466 (2) 0.0824 (17)
H21A 0.2157 1.3913 0.3371 0.124*
H21B 0.0710 1.3551 0.3757 0.124*
H21C 0.0839 1.2628 0.3018 0.124*
C22 −0.0030 (4) 0.8179 (4) 0.1131 (2) 0.0485 (12)
C23 0.0152 (5) 0.7052 (5) 0.1226 (3) 0.0733 (16)
H23 0.0821 0.7099 0.1596 0.088*
C24 −0.0622 (6) 0.5870 (5) 0.0792 (3) 0.103 (2)
H24 −0.0520 0.5104 0.0881 0.124*
C25 −0.1539 (6) 0.5771 (5) 0.0233 (3) 0.098 (2)
H25 −0.2046 0.4949 −0.0074 0.117*
C26 −0.1713 (6) 0.6880 (5) 0.0125 (3) 0.0842 (17)
H26 −0.2359 0.6826 −0.0256 0.101*
C27 −0.0970 (5) 0.8055 (5) 0.0559 (2) 0.0651 (14)
H27 −0.1096 0.8813 0.0470 0.078*
C28 −0.0413 (4) 1.0544 (4) 0.1788 (2) 0.0423 (11)
C29 −0.1412 (5) 1.0359 (4) 0.2284 (2) 0.0566 (13)
H29 −0.1351 0.9835 0.2593 0.068*
C30 −0.2476 (5) 1.0912 (5) 0.2337 (3) 0.0728 (15)
H30 −0.3143 1.0777 0.2681 0.087*
C31 −0.2577 (5) 1.1664 (5) 0.1893 (3) 0.0782 (17)
H31 −0.3317 1.2051 0.1927 0.094*
C32 −0.1605 (6) 1.1860 (4) 0.1393 (3) 0.0721 (16)
H32 −0.1671 1.2388 0.1087 0.087*
C33 −0.0545 (5) 1.1292 (4) 0.1340 (2) 0.0505 (12)
H33 0.0107 1.1415 0.0988 0.061*
C34 0.2300 (4) 1.0584 (5) 0.1248 (2) 0.0475 (12)
C35 0.3147 (5) 1.1830 (5) 0.1584 (2) 0.0566 (13)
H35 0.2973 1.2218 0.2046 0.068*
C36 0.4241 (5) 1.2518 (5) 0.1258 (3) 0.0685 (15)
H36 0.4825 1.3370 0.1500 0.082*
C37 0.4500 (6) 1.1987 (6) 0.0585 (3) 0.0771 (18)
H37 0.5257 1.2464 0.0360 0.093*
C38 0.3649 (6) 1.0763 (6) 0.0250 (3) 0.0772 (17)
H38 0.3819 1.0386 −0.0215 0.093*
C39 0.2543 (5) 1.0056 (5) 0.0570 (3) 0.0612 (14)
H39 0.1953 0.9209 0.0323 0.073*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Cu1 0.0472 (3) 0.0362 (3) 0.0419 (3) 0.0148 (3) −0.0030 (3) 0.0093 (3)
P1 0.0514 (8) 0.0412 (7) 0.0408 (7) 0.0192 (6) −0.0039 (6) 0.0088 (6)
N1 0.045 (2) 0.026 (2) 0.050 (2) 0.0119 (18) −0.0095 (18) 0.0103 (19)
N2 0.058 (3) 0.049 (3) 0.078 (3) 0.020 (2) −0.021 (2) 0.018 (2)
N3 0.039 (2) 0.041 (2) 0.055 (3) 0.011 (2) −0.0054 (18) 0.004 (2)
N4 0.053 (3) 0.040 (3) 0.081 (3) 0.003 (2) −0.006 (2) 0.009 (2)
N5 0.039 (2) 0.038 (2) 0.044 (2) 0.0099 (18) −0.0058 (18) 0.0034 (19)
Si1 0.0529 (8) 0.0398 (8) 0.0497 (9) 0.0188 (7) −0.0053 (7) 0.0034 (7)
C1 0.035 (3) 0.033 (3) 0.048 (3) 0.013 (2) −0.004 (2) 0.016 (2)
C2 0.045 (3) 0.042 (3) 0.048 (3) 0.019 (2) 0.001 (2) 0.013 (3)
C3 0.071 (4) 0.045 (3) 0.066 (4) 0.026 (3) 0.005 (3) 0.008 (3)
C4 0.081 (4) 0.036 (3) 0.076 (4) 0.022 (3) −0.001 (3) 0.009 (3)
C5 0.057 (3) 0.041 (3) 0.083 (4) 0.009 (3) 0.006 (3) 0.025 (3)
C6 0.047 (3) 0.043 (3) 0.064 (3) 0.019 (3) 0.001 (3) 0.017 (3)
C7 0.064 (4) 0.049 (3) 0.126 (5) 0.019 (3) 0.036 (4) 0.031 (4)
C8 0.187 (7) 0.198 (8) 0.106 (6) 0.102 (6) 0.073 (5) 0.069 (6)
C9 0.093 (5) 0.145 (6) 0.187 (7) 0.072 (5) 0.050 (5) 0.072 (6)
C10 0.058 (3) 0.058 (3) 0.071 (4) 0.021 (3) 0.014 (3) 0.018 (3)
C11 0.076 (5) 0.116 (6) 0.289 (10) 0.050 (4) 0.067 (5) 0.066 (6)
C12 0.118 (5) 0.187 (7) 0.098 (5) 0.003 (5) 0.015 (4) 0.085 (5)
C13 0.042 (3) 0.046 (3) 0.046 (3) 0.019 (3) 0.009 (2) 0.011 (3)
C14 0.082 (4) 0.087 (5) 0.149 (6) 0.030 (4) −0.054 (4) 0.029 (4)
C15 0.120 (5) 0.078 (4) 0.122 (5) 0.006 (4) −0.054 (4) 0.046 (4)
C16 0.052 (3) 0.038 (3) 0.037 (3) 0.005 (3) 0.007 (2) 0.003 (2)
C17 0.053 (3) 0.062 (4) 0.101 (4) −0.008 (3) −0.012 (3) 0.001 (3)
C18 0.093 (4) 0.045 (3) 0.085 (4) −0.005 (3) 0.003 (3) 0.017 (3)
C19 0.078 (4) 0.064 (3) 0.058 (3) 0.028 (3) 0.000 (3) 0.002 (3)
C20 0.060 (3) 0.075 (4) 0.078 (4) 0.017 (3) 0.011 (3) 0.006 (3)
C21 0.099 (4) 0.064 (4) 0.093 (4) 0.047 (3) −0.019 (3) 0.011 (3)
C22 0.058 (3) 0.048 (3) 0.041 (3) 0.024 (3) −0.010 (2) 0.006 (2)
C23 0.096 (4) 0.051 (3) 0.073 (4) 0.030 (3) −0.031 (3) 0.009 (3)
C24 0.151 (6) 0.046 (4) 0.100 (5) 0.035 (4) −0.059 (4) −0.004 (3)
C25 0.122 (5) 0.052 (4) 0.097 (5) 0.025 (4) −0.055 (4) −0.014 (4)
C26 0.100 (4) 0.069 (4) 0.076 (4) 0.039 (4) −0.042 (3) −0.008 (3)
C27 0.082 (4) 0.052 (3) 0.057 (3) 0.030 (3) −0.023 (3) −0.001 (3)
C28 0.043 (3) 0.036 (3) 0.047 (3) 0.014 (2) −0.004 (2) 0.006 (2)
C29 0.054 (3) 0.057 (3) 0.061 (3) 0.022 (3) 0.004 (3) 0.014 (3)
C30 0.058 (4) 0.074 (4) 0.086 (4) 0.028 (3) 0.018 (3) 0.010 (4)
C31 0.057 (4) 0.064 (4) 0.114 (5) 0.035 (3) −0.008 (4) 0.004 (4)
C32 0.070 (4) 0.062 (4) 0.095 (4) 0.033 (3) −0.010 (3) 0.024 (3)
C33 0.057 (3) 0.046 (3) 0.053 (3) 0.025 (3) 0.000 (2) 0.012 (3)
C34 0.046 (3) 0.062 (3) 0.047 (3) 0.033 (3) 0.002 (2) 0.018 (3)
C35 0.050 (3) 0.062 (4) 0.053 (3) 0.015 (3) 0.003 (3) 0.010 (3)
C36 0.052 (3) 0.070 (4) 0.085 (4) 0.013 (3) 0.000 (3) 0.033 (4)
C37 0.067 (4) 0.101 (5) 0.084 (5) 0.034 (4) 0.020 (4) 0.053 (4)
C38 0.083 (4) 0.114 (5) 0.055 (4) 0.051 (4) 0.024 (3) 0.032 (4)
C39 0.073 (4) 0.068 (4) 0.054 (3) 0.036 (3) 0.008 (3) 0.017 (3)

Geometric parameters (Å, º)

Cu1—N5 1.964 (3) C14—H14C 0.9800
Cu1—N1 1.980 (3) C15—H15A 0.9800
Cu1—P1 2.1651 (12) C15—H15B 0.9800
P1—C22 1.811 (4) C15—H15C 0.9800
P1—C28 1.824 (4) C17—H17A 0.9800
P1—C34 1.824 (4) C17—H17B 0.9800
N1—C13 1.328 (5) C17—H17C 0.9800
N1—C1 1.409 (4) C18—H18A 0.9800
N2—C13 1.379 (5) C18—H18B 0.9800
N2—C15 1.403 (5) C18—H18C 0.9800
N2—C14 1.457 (5) C19—H19A 0.9800
N3—C16 1.335 (5) C19—H19B 0.9800
N3—C13 1.349 (5) C19—H19C 0.9800
N4—C16 1.371 (5) C20—H20A 0.9800
N4—C17 1.444 (5) C20—H20B 0.9800
N4—C18 1.464 (5) C20—H20C 0.9800
N5—C16 1.329 (5) C21—H21A 0.9800
N5—Si1 1.702 (3) C21—H21B 0.9800
Si1—C19 1.853 (4) C21—H21C 0.9800
Si1—C20 1.854 (4) C22—C23 1.384 (5)
Si1—C21 1.865 (4) C22—C27 1.390 (5)
C1—C2 1.387 (5) C23—C24 1.369 (6)
C1—C6 1.404 (5) C23—H23 0.9500
C2—C3 1.379 (5) C24—C25 1.365 (6)
C2—C10 1.512 (5) C24—H24 0.9500
C3—C4 1.370 (6) C25—C26 1.369 (6)
C3—H3 0.9500 C25—H25 0.9500
C4—C5 1.356 (6) C26—C27 1.357 (6)
C4—H4 0.9500 C26—H26 0.9500
C5—C6 1.386 (5) C27—H27 0.9500
C5—H5 0.9500 C28—C33 1.380 (5)
C6—C7 1.531 (6) C28—C29 1.392 (5)
C7—C9 1.510 (6) C29—C30 1.363 (5)
C7—C8 1.533 (6) C29—H29 0.9500
C7—H7 1.0000 C30—C31 1.368 (6)
C8—H8A 0.9800 C30—H30 0.9500
C8—H8B 0.9800 C31—C32 1.382 (6)
C8—H8C 0.9800 C31—H31 0.9500
C9—H9A 0.9800 C32—C33 1.371 (5)
C9—H9B 0.9800 C32—H32 0.9500
C9—H9C 0.9800 C33—H33 0.9500
C10—C11 1.497 (6) C34—C35 1.378 (5)
C10—C12 1.506 (6) C34—C39 1.378 (5)
C10—H10 1.0000 C35—C36 1.372 (5)
C11—H11A 0.9800 C35—H35 0.9500
C11—H11B 0.9800 C36—C37 1.374 (6)
C11—H11C 0.9800 C36—H36 0.9500
C12—H12A 0.9800 C37—C38 1.362 (6)
C12—H12B 0.9800 C37—H37 0.9500
C12—H12C 0.9800 C38—C39 1.382 (6)
C14—H14A 0.9800 C38—H38 0.9500
C14—H14B 0.9800 C39—H39 0.9500
N5—Cu1—N1 95.88 (14) N2—C15—H15B 109.5
N5—Cu1—P1 126.26 (10) H15A—C15—H15B 109.5
N1—Cu1—P1 135.59 (11) N2—C15—H15C 109.5
C22—P1—C28 100.94 (18) H15A—C15—H15C 109.5
C22—P1—C34 105.5 (2) H15B—C15—H15C 109.5
C28—P1—C34 103.48 (19) N5—C16—N3 127.8 (4)
C22—P1—Cu1 122.58 (14) N5—C16—N4 121.1 (4)
C28—P1—Cu1 119.03 (14) N3—C16—N4 111.1 (4)
C34—P1—Cu1 103.22 (14) N4—C17—H17A 109.5
C13—N1—C1 123.6 (3) N4—C17—H17B 109.5
C13—N1—Cu1 118.2 (3) H17A—C17—H17B 109.5
C1—N1—Cu1 118.0 (2) N4—C17—H17C 109.5
C13—N2—C15 125.5 (4) H17A—C17—H17C 109.5
C13—N2—C14 119.3 (4) H17B—C17—H17C 109.5
C15—N2—C14 112.9 (4) N4—C18—H18A 109.5
C16—N3—C13 125.8 (4) N4—C18—H18B 109.5
C16—N4—C17 123.6 (4) H18A—C18—H18B 109.5
C16—N4—C18 120.5 (4) N4—C18—H18C 109.5
C17—N4—C18 114.1 (4) H18A—C18—H18C 109.5
C16—N5—Si1 126.4 (3) H18B—C18—H18C 109.5
C16—N5—Cu1 111.5 (3) Si1—C19—H19A 109.5
Si1—N5—Cu1 119.71 (19) Si1—C19—H19B 109.5
N5—Si1—C19 113.54 (19) H19A—C19—H19B 109.5
N5—Si1—C20 107.65 (19) Si1—C19—H19C 109.5
C19—Si1—C20 106.9 (2) H19A—C19—H19C 109.5
N5—Si1—C21 112.7 (2) H19B—C19—H19C 109.5
C19—Si1—C21 107.8 (2) Si1—C20—H20A 109.5
C20—Si1—C21 107.9 (2) Si1—C20—H20B 109.5
C2—C1—C6 119.4 (4) H20A—C20—H20B 109.5
C2—C1—N1 121.7 (4) Si1—C20—H20C 109.5
C6—C1—N1 118.6 (4) H20A—C20—H20C 109.5
C3—C2—C1 119.4 (4) H20B—C20—H20C 109.5
C3—C2—C10 119.0 (4) Si1—C21—H21A 109.5
C1—C2—C10 121.6 (4) Si1—C21—H21B 109.5
C4—C3—C2 121.1 (5) H21A—C21—H21B 109.5
C4—C3—H3 119.4 Si1—C21—H21C 109.5
C2—C3—H3 119.4 H21A—C21—H21C 109.5
C5—C4—C3 120.0 (5) H21B—C21—H21C 109.5
C5—C4—H4 120.0 C23—C22—C27 117.0 (4)
C3—C4—H4 120.0 C23—C22—P1 119.7 (3)
C4—C5—C6 120.8 (5) C27—C22—P1 123.3 (4)
C4—C5—H5 119.6 C24—C23—C22 120.6 (4)
C6—C5—H5 119.6 C24—C23—H23 119.7
C5—C6—C1 119.3 (4) C22—C23—H23 119.7
C5—C6—C7 119.6 (4) C25—C24—C23 121.3 (5)
C1—C6—C7 121.1 (4) C25—C24—H24 119.4
C9—C7—C6 111.2 (5) C23—C24—H24 119.4
C9—C7—C8 108.4 (5) C24—C25—C26 118.7 (5)
C6—C7—C8 112.8 (4) C24—C25—H25 120.6
C9—C7—H7 108.1 C26—C25—H25 120.6
C6—C7—H7 108.1 C27—C26—C25 120.5 (5)
C8—C7—H7 108.1 C27—C26—H26 119.7
C7—C8—H8A 109.5 C25—C26—H26 119.7
C7—C8—H8B 109.5 C26—C27—C22 121.8 (4)
H8A—C8—H8B 109.5 C26—C27—H27 119.1
C7—C8—H8C 109.5 C22—C27—H27 119.1
H8A—C8—H8C 109.5 C33—C28—C29 117.8 (4)
H8B—C8—H8C 109.5 C33—C28—P1 123.9 (4)
C7—C9—H9A 109.5 C29—C28—P1 118.2 (3)
C7—C9—H9B 109.5 C30—C29—C28 121.6 (4)
H9A—C9—H9B 109.5 C30—C29—H29 119.2
C7—C9—H9C 109.5 C28—C29—H29 119.2
H9A—C9—H9C 109.5 C29—C30—C31 119.7 (5)
H9B—C9—H9C 109.5 C29—C30—H30 120.2
C11—C10—C12 110.3 (5) C31—C30—H30 120.2
C11—C10—C2 113.1 (4) C30—C31—C32 120.1 (5)
C12—C10—C2 109.7 (4) C30—C31—H31 120.0
C11—C10—H10 107.9 C32—C31—H31 120.0
C12—C10—H10 107.9 C33—C32—C31 119.9 (5)
C2—C10—H10 107.9 C33—C32—H32 120.1
C10—C11—H11A 109.5 C31—C32—H32 120.1
C10—C11—H11B 109.5 C32—C33—C28 121.0 (4)
H11A—C11—H11B 109.5 C32—C33—H33 119.5
C10—C11—H11C 109.5 C28—C33—H33 119.5
H11A—C11—H11C 109.5 C35—C34—C39 118.6 (4)
H11B—C11—H11C 109.5 C35—C34—P1 117.5 (4)
C10—C12—H12A 109.5 C39—C34—P1 123.9 (4)
C10—C12—H12B 109.5 C36—C35—C34 120.8 (5)
H12A—C12—H12B 109.5 C36—C35—H35 119.6
C10—C12—H12C 109.5 C34—C35—H35 119.6
H12A—C12—H12C 109.5 C35—C36—C37 120.8 (5)
H12B—C12—H12C 109.5 C35—C36—H36 119.6
N1—C13—N3 124.6 (4) C37—C36—H36 119.6
N1—C13—N2 122.7 (4) C38—C37—C36 118.5 (5)
N3—C13—N2 112.5 (4) C38—C37—H37 120.8
N2—C14—H14A 109.5 C36—C37—H37 120.8
N2—C14—H14B 109.5 C37—C38—C39 121.6 (5)
H14A—C14—H14B 109.5 C37—C38—H38 119.2
N2—C14—H14C 109.5 C39—C38—H38 119.2
H14A—C14—H14C 109.5 C34—C39—C38 119.8 (5)
H14B—C14—H14C 109.5 C34—C39—H39 120.1
N2—C15—H15A 109.5 C38—C39—H39 120.1

Footnotes

Supporting information for this paper is available from the IUCr electronic archives (Reference: LX2294).

References

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Associated Data

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

Supplementary Materials

Crystal structure: contains datablock(s) I, New_Global_Publ_Block. DOI: 10.1107/S2056989015002169/lx2294sup1.cif

e-71-00m54-sup1.cif (437.1KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989015002169/lx2294Isup2.hkl

e-71-00m54-Isup2.hkl (341.9KB, hkl)

Supporting information file. DOI: 10.1107/S2056989015002169/lx2294Isup3.txt

e-71-00m54-Isup3.txt (92.6KB, txt)

. DOI: 10.1107/S2056989015002169/lx2294fig1.tif

The mol­ecular structure of (I), showing the atom-numbering scheme. Displacement ellipsoids are drawn at the 30% probability level. H atoms are presented as a small spheres of arbitrary radius.

CCDC reference: 1046645

Additional supporting information: crystallographic information; 3D view; checkCIF report


Articles from Acta Crystallographica Section E: Crystallographic Communications are provided here courtesy of International Union of Crystallography

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