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The reaction between the metal diphosphine [Ag(PPh3)2(MeCN)](SbF6) and the metal acetyl­ide compound Pt(dmbpy)(C2Ph)2 (dmbpy is 4,4'-di­methyl-2,2'-bi­pyridine) gave the title compound, Pt(dmbpy)(C2Ph)·SbF6 or [Pt(C8H5)(C18H15P)(C12H12N2)](SbF6). The Pt center is four-coordinated and exhibits a distorted square-planar coordin­ation geometry.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536803006834/lh6047sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536803006834/lh6047Isup2.hkl
Contains datablock I

CCDC reference: 209904

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](C-C) = 0.013 Å
  • R factor = 0.041
  • wR factor = 0.110
  • Data-to-parameter ratio = 14.2

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry


Yellow Alert Alert Level C:
PLAT_371 Alert C Long C(sp2)-C(sp1) Bond C(2) - C(3) = 1.43 Ang. PLAT_601 Alert C Structure Contains Solvent Accessible VOIDS of 36.00 A   3
0 Alert Level A = Potentially serious problem
0 Alert Level B = Potential problem
2 Alert Level C = Please check

Comment top

Transition metal acetylide complexes are of considerable interest because of their potential applications in many fields of materials chemistry, including luminiscent materials and conducting polymers (Chan et al., 2001). We are interested in the design of photoluminescent heterometallic cluster complexes by self-assembly between two metal components, one with alkynyl ligands and the other with vacant coordination sites. Thus, the reaction between Pt(dmbpy)(C2Ph)2, with two alkynyl ligands, and [Ag(PPh3)2(MeCN)]+, with a vacant coordination site, was expected to afford a Pt–Ag heteronuclear species. However, the product isolated from the reaction was the title compound, (I). A perspective drawing of the complex with atomic numbering scheme is depicted in Fig. 1 and selected geometric parameters are presented in Table 1.

The Pt atom is located in a distorted square-planar coordination geometry. The Pt—P distance is 2.246 (2) Å, which is slighlty shorter than that observed in the complex of PtCuCl(C2Bu)2(PMe2Ph)2 [2.300 (3) Å; Yamazaki & Deeming, 1993]. The Pt—N distances are 2.068 (6) and 2.094 (6) Å, which are similar to those observed in the complex of Pt(1,10-phenanthroline)(C9H7)2 (Hissler et al., 2000).

Experimental top

The starting compounds Pt(dmbpy)(C2Ph)2 (Chan et al., 2001) and [Ag(PPh3)2(MeCN)](SbF6) were prepared according to literature procedures (Bachman et al., 1998). Pt(dmbpy)(C2Ph)2 and [Ag(PPh3)2(MeCN)](SbF6) were reacted, in an equimolar ratio, in dichloromethane under anaerobic conditions for 24 h. The solvent was then reduced in vacuo. Well shaped yellow crystals suitable for X-ray diffraction analysis were grown by slow diffusion of diethyl ether into the dichloromethane solution.

Refinement top

All H atoms were included in calculated positions with C—H distances of 0.93 and 0.96 Å (methyl). They were included in the refinement in riding-motion approximation, with Uiso = 1.2Ueq (1.5Ueq for methyl) of the carrier atom.

Computing details top

Data collection: SMART (Siemens, 1996); cell refinement: SMART and SAINT (Siemens, 1994); data reduction: XPREP (Siemens, 1994); program(s) used to solve structure: SHELXTL (Siemens, 1994); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.

Figures top
[Figure 1] Fig. 1. A view of the compound with the atomic numbering scheme. Displacement ellipsoids are drawn at the 30% probability level.
(4,4'-dimethyl-2,2'-bipyridine)(ethynylbenzene)(triphenylphosphine)platinum(II) hexafluoroantimonate top
Crystal data top
[Pt(C8H5)(C18H15P)(C12H12N2)](SbF6)F(000) = 1888
Mr = 978.47Dx = 1.814 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 4988 reflections
a = 14.4131 (4) Åθ = 1.5–25.1°
b = 10.1848 (2) ŵ = 4.76 mm1
c = 24.7099 (7) ÅT = 293 K
β = 98.915 (1)°Block, yellow
V = 3583.46 (16) Å30.50 × 0.30 × 0.25 mm
Z = 4
Data collection top
Siemens SMART CCD
diffractometer
6291 independent reflections
Radiation source: fine-focus sealed tube4473 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.024
ω scansθmax = 25.1°, θmin = 1.5°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 717
Tmin = 0.194, Tmax = 0.304k = 912
10524 measured reflectionsl = 2929
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.041Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.110H-atom parameters constrained
S = 1.19 w = 1/[σ2(Fo2) + (0.0387P)2 + 9.8193P]
where P = (Fo2 + 2Fc2)/3
6291 reflections(Δ/σ)max = 0.002
442 parametersΔρmax = 1.04 e Å3
0 restraintsΔρmin = 0.61 e Å3
Crystal data top
[Pt(C8H5)(C18H15P)(C12H12N2)](SbF6)V = 3583.46 (16) Å3
Mr = 978.47Z = 4
Monoclinic, P21/nMo Kα radiation
a = 14.4131 (4) ŵ = 4.76 mm1
b = 10.1848 (2) ÅT = 293 K
c = 24.7099 (7) Å0.50 × 0.30 × 0.25 mm
β = 98.915 (1)°
Data collection top
Siemens SMART CCD
diffractometer
6291 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
4473 reflections with I > 2σ(I)
Tmin = 0.194, Tmax = 0.304Rint = 0.024
10524 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0410 restraints
wR(F2) = 0.110H-atom parameters constrained
S = 1.19Δρmax = 1.04 e Å3
6291 reflectionsΔρmin = 0.61 e Å3
442 parameters
Special details top

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) top
xyzUiso*/Ueq
Pt0.11648 (2)0.00002 (3)0.094070 (11)0.04068 (11)
Sb0.49147 (5)0.18053 (7)0.10878 (3)0.06338 (19)
P0.06876 (14)0.0455 (2)0.17434 (8)0.0424 (5)
F10.4859 (4)0.0352 (6)0.0637 (3)0.101 (2)
F20.6135 (6)0.1462 (11)0.1340 (6)0.227 (7)
F30.5005 (5)0.3269 (7)0.1539 (2)0.104 (2)
F40.3707 (6)0.2193 (13)0.0842 (5)0.219 (6)
F50.4544 (11)0.0870 (10)0.1626 (4)0.229 (7)
F60.5241 (11)0.2795 (10)0.0542 (4)0.219 (6)
N10.1700 (4)0.0471 (6)0.0236 (3)0.0418 (15)
N20.2270 (4)0.1346 (6)0.0971 (2)0.0416 (15)
C10.0150 (6)0.1284 (8)0.0793 (3)0.0470 (19)
C20.0466 (6)0.2070 (8)0.0645 (3)0.050 (2)
C30.1147 (5)0.3057 (8)0.0450 (3)0.047 (2)
C40.1952 (6)0.3232 (9)0.0678 (4)0.063 (2)
H4A0.20670.26770.09590.075*
C50.2598 (7)0.4219 (12)0.0500 (5)0.081 (3)
H5A0.31330.43420.06610.098*
C60.2414 (9)0.5006 (11)0.0074 (6)0.094 (4)
H6A0.28450.56560.00560.113*
C70.1622 (10)0.4866 (11)0.0166 (5)0.084 (3)
H7A0.15130.54140.04500.101*
C80.0995 (7)0.3899 (9)0.0026 (4)0.063 (2)
H8A0.04530.38010.01310.076*
C110.1695 (5)0.0594 (8)0.2290 (3)0.0410 (18)
C120.1662 (6)0.1371 (8)0.2743 (3)0.051 (2)
H12A0.11140.18250.27760.061*
C130.2437 (6)0.1483 (9)0.3150 (3)0.057 (2)
H13A0.24030.19960.34570.069*
C140.3252 (6)0.0837 (9)0.3098 (4)0.057 (2)
H14A0.37750.09240.33680.069*
C150.3297 (6)0.0068 (9)0.2654 (4)0.063 (2)
H15A0.38490.03810.26240.075*
C160.2525 (6)0.0054 (8)0.2242 (3)0.054 (2)
H16A0.25650.05690.19360.065*
C210.0079 (6)0.0718 (8)0.2017 (3)0.049 (2)
C220.0280 (7)0.1662 (9)0.2385 (4)0.063 (2)
H22A0.09260.17180.24940.076*
C230.0314 (9)0.2547 (11)0.2598 (4)0.084 (3)
H23A0.00640.31780.28510.101*
C240.1256 (9)0.2478 (12)0.2434 (5)0.081 (3)
H24A0.16490.30680.25740.097*
C250.1635 (7)0.1547 (12)0.2062 (5)0.080 (3)
H25A0.22820.14970.19560.095*
C260.1043 (6)0.0682 (10)0.1846 (4)0.066 (3)
H26A0.12950.00710.15840.079*
C310.0069 (5)0.2006 (8)0.1732 (3)0.0453 (19)
C320.0498 (6)0.2332 (10)0.2123 (4)0.061 (2)
H32A0.05750.17390.23990.073*
C330.0944 (6)0.3540 (10)0.2100 (4)0.067 (3)
H33A0.13180.37540.23610.081*
C340.0838 (7)0.4421 (11)0.1695 (4)0.070 (3)
H34A0.11320.52350.16870.084*
C350.0305 (6)0.4107 (9)0.1308 (4)0.061 (2)
H35A0.02460.47000.10290.073*
C360.0155 (6)0.2903 (8)0.1325 (3)0.050 (2)
H36A0.05240.27020.10590.060*
C420.2498 (5)0.0163 (7)0.0162 (3)0.0397 (18)
C430.2982 (6)0.0174 (8)0.0258 (3)0.052 (2)
H43A0.35290.02740.02990.063*
C440.2660 (6)0.1170 (9)0.0618 (3)0.050 (2)
C450.1851 (6)0.1797 (9)0.0541 (3)0.053 (2)
H45A0.16140.24750.07740.064*
C460.1388 (6)0.1427 (8)0.0120 (3)0.052 (2)
H46A0.08340.18580.00800.063*
C470.3179 (7)0.1593 (11)0.1071 (4)0.078 (3)
H47A0.37210.10450.10720.118*
H47B0.33740.24900.10150.118*
H47C0.27740.15130.14170.118*
C520.2799 (5)0.1199 (7)0.0564 (3)0.0433 (18)
C530.3537 (5)0.2008 (8)0.0522 (4)0.051 (2)
H53A0.38870.18690.02410.062*
C540.3782 (6)0.3034 (8)0.0887 (4)0.056 (2)
C550.3234 (6)0.3164 (9)0.1299 (4)0.055 (2)
H55A0.33670.38300.15570.066*
C560.2498 (6)0.2325 (8)0.1332 (3)0.051 (2)
H56A0.21460.24380.16140.061*
C570.4592 (7)0.3934 (10)0.0842 (5)0.076 (3)
H57A0.46500.45690.11320.114*
H57B0.51610.34310.08690.114*
H57C0.44840.43790.04950.114*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Pt0.04262 (17)0.04339 (18)0.03631 (16)0.00069 (16)0.00701 (11)0.00109 (15)
Sb0.0604 (4)0.0776 (4)0.0557 (4)0.0025 (3)0.0203 (3)0.0065 (4)
P0.0424 (11)0.0477 (12)0.0370 (11)0.0083 (9)0.0059 (9)0.0027 (9)
F10.080 (4)0.101 (5)0.119 (5)0.007 (3)0.011 (4)0.046 (4)
F20.090 (6)0.221 (11)0.335 (15)0.051 (6)0.076 (7)0.166 (11)
F30.142 (6)0.099 (5)0.076 (4)0.014 (4)0.036 (4)0.026 (4)
F40.097 (6)0.292 (14)0.250 (12)0.068 (7)0.030 (7)0.151 (11)
F50.43 (2)0.149 (9)0.139 (8)0.116 (11)0.137 (11)0.009 (7)
F60.412 (18)0.148 (8)0.132 (8)0.053 (10)0.159 (10)0.022 (6)
N10.042 (4)0.046 (4)0.039 (4)0.002 (3)0.009 (3)0.006 (3)
N20.045 (4)0.043 (4)0.036 (3)0.001 (3)0.006 (3)0.002 (3)
C10.053 (5)0.051 (5)0.038 (4)0.003 (4)0.011 (4)0.004 (4)
C20.054 (5)0.045 (5)0.051 (5)0.001 (4)0.012 (4)0.005 (4)
C30.042 (4)0.050 (5)0.046 (5)0.003 (4)0.004 (4)0.008 (4)
C40.049 (5)0.054 (6)0.084 (7)0.002 (5)0.005 (5)0.006 (5)
C50.056 (6)0.078 (8)0.106 (9)0.008 (6)0.001 (6)0.016 (7)
C60.091 (9)0.055 (6)0.119 (10)0.014 (7)0.044 (8)0.017 (8)
C70.104 (9)0.068 (7)0.072 (7)0.000 (7)0.011 (7)0.005 (6)
C80.070 (6)0.063 (6)0.055 (6)0.003 (5)0.003 (5)0.003 (5)
C110.044 (4)0.040 (4)0.040 (4)0.008 (4)0.008 (3)0.002 (4)
C120.053 (5)0.059 (5)0.042 (5)0.017 (4)0.010 (4)0.002 (4)
C130.063 (6)0.071 (6)0.038 (5)0.005 (5)0.006 (4)0.004 (4)
C140.049 (5)0.067 (6)0.052 (5)0.008 (5)0.006 (4)0.004 (5)
C150.049 (5)0.060 (6)0.079 (6)0.019 (5)0.009 (5)0.002 (6)
C160.059 (5)0.053 (5)0.048 (5)0.014 (5)0.004 (4)0.002 (5)
C210.053 (5)0.052 (5)0.046 (5)0.003 (4)0.022 (4)0.005 (4)
C220.072 (6)0.056 (6)0.059 (6)0.001 (5)0.004 (5)0.010 (5)
C230.121 (10)0.064 (7)0.068 (7)0.008 (7)0.017 (7)0.012 (6)
C240.083 (8)0.091 (8)0.075 (8)0.020 (7)0.036 (6)0.004 (7)
C250.050 (6)0.111 (9)0.083 (7)0.013 (6)0.029 (5)0.005 (7)
C260.049 (5)0.077 (7)0.072 (6)0.005 (5)0.016 (5)0.008 (6)
C310.044 (4)0.049 (5)0.040 (4)0.006 (4)0.001 (4)0.002 (4)
C320.057 (6)0.072 (6)0.051 (5)0.020 (5)0.002 (4)0.006 (5)
C330.057 (6)0.083 (7)0.060 (6)0.028 (5)0.004 (5)0.022 (6)
C340.075 (7)0.060 (6)0.065 (7)0.022 (5)0.017 (5)0.009 (6)
C350.069 (6)0.052 (6)0.053 (5)0.005 (5)0.017 (5)0.000 (4)
C360.049 (5)0.049 (5)0.047 (5)0.006 (4)0.005 (4)0.001 (4)
C420.038 (4)0.048 (5)0.033 (4)0.001 (4)0.005 (3)0.003 (4)
C430.049 (5)0.059 (6)0.051 (5)0.008 (4)0.016 (4)0.003 (4)
C440.052 (5)0.058 (5)0.040 (5)0.004 (4)0.004 (4)0.006 (4)
C450.055 (5)0.059 (5)0.046 (5)0.007 (4)0.008 (4)0.022 (4)
C460.050 (5)0.056 (5)0.052 (5)0.010 (4)0.011 (4)0.009 (4)
C470.068 (6)0.096 (8)0.078 (7)0.010 (6)0.036 (5)0.040 (6)
C520.045 (4)0.039 (4)0.044 (4)0.005 (4)0.001 (4)0.008 (4)
C530.041 (4)0.056 (5)0.059 (5)0.010 (4)0.014 (4)0.003 (4)
C540.058 (5)0.044 (5)0.063 (6)0.007 (4)0.003 (4)0.001 (5)
C550.060 (5)0.045 (5)0.056 (5)0.001 (4)0.003 (4)0.004 (4)
C560.049 (5)0.053 (5)0.050 (5)0.001 (4)0.004 (4)0.008 (4)
C570.072 (7)0.057 (6)0.097 (8)0.026 (5)0.004 (6)0.009 (6)
Geometric parameters (Å, º) top
Pt—C11.954 (9)C22—C231.401 (13)
Pt—N12.068 (6)C22—H22A0.9300
Pt—N22.094 (6)C23—C241.357 (15)
Pt—P2.246 (2)C23—H23A0.9300
Sb—F51.783 (8)C24—C251.372 (15)
Sb—F41.797 (8)C24—H24A0.9300
Sb—F61.803 (9)C25—C261.389 (13)
Sb—F21.807 (7)C25—H25A0.9300
Sb—F11.847 (6)C26—H26A0.9300
Sb—F31.854 (6)C31—C361.378 (11)
P—C311.812 (8)C31—C321.400 (11)
P—C211.827 (8)C32—C331.385 (12)
P—C111.828 (8)C32—H32A0.9300
N1—C461.341 (10)C33—C341.369 (14)
N1—C421.356 (9)C33—H33A0.9300
N2—C561.343 (9)C34—C351.356 (13)
N2—C521.362 (9)C34—H34A0.9300
C1—C21.209 (11)C35—C361.391 (11)
C2—C31.435 (11)C35—H35A0.9300
C3—C41.378 (11)C36—H36A0.9300
C3—C81.397 (12)C42—C431.380 (11)
C4—C51.395 (13)C42—C521.468 (10)
C4—H4A0.9300C43—C441.381 (11)
C5—C61.381 (17)C43—H43A0.9300
C5—H5A0.9300C44—C451.368 (11)
C6—C71.373 (18)C44—C471.505 (11)
C6—H6A0.9300C45—C461.372 (11)
C7—C81.370 (14)C45—H45A0.9300
C7—H7A0.9300C46—H46A0.9300
C8—H8A0.9300C47—H47A0.9600
C11—C121.378 (10)C47—H47B0.9600
C11—C161.387 (11)C47—H47C0.9600
C12—C131.387 (11)C52—C531.363 (10)
C12—H12A0.9300C53—C541.390 (11)
C13—C141.370 (11)C53—H53A0.9300
C13—H13A0.9300C54—C551.387 (12)
C14—C151.359 (12)C54—C571.503 (12)
C14—H14A0.9300C55—C561.375 (11)
C15—C161.392 (12)C55—H55A0.9300
C15—H15A0.9300C56—H56A0.9300
C16—H16A0.9300C57—H57A0.9600
C21—C221.367 (12)C57—H57B0.9600
C21—C261.389 (12)C57—H57C0.9600
C1—Pt—N193.0 (3)C21—C22—H22A119.6
C1—Pt—N2171.2 (3)C23—C22—H22A119.6
N1—Pt—N278.6 (2)C24—C23—C22119.7 (10)
C1—Pt—P88.9 (2)C24—C23—H23A120.1
N1—Pt—P175.58 (18)C22—C23—H23A120.1
N2—Pt—P99.68 (18)C23—C24—C25120.8 (10)
F5—Sb—F489.0 (7)C23—C24—H24A119.6
F5—Sb—F6177.4 (7)C25—C24—H24A119.6
F4—Sb—F688.6 (7)C24—C25—C26119.4 (10)
F5—Sb—F291.6 (7)C24—C25—H25A120.3
F4—Sb—F2178.4 (5)C26—C25—H25A120.3
F6—Sb—F290.7 (7)C21—C26—C25120.7 (10)
F5—Sb—F191.8 (4)C21—C26—H26A119.6
F4—Sb—F191.3 (4)C25—C26—H26A119.6
F6—Sb—F189.3 (4)C36—C31—C32118.4 (8)
F2—Sb—F190.1 (4)C36—C31—P119.3 (6)
F5—Sb—F389.0 (4)C32—C31—P122.3 (6)
F4—Sb—F390.0 (4)C33—C32—C31119.9 (9)
F6—Sb—F389.9 (4)C33—C32—H32A120.0
F2—Sb—F388.5 (4)C31—C32—H32A120.0
F1—Sb—F3178.4 (3)C34—C33—C32120.6 (9)
C31—P—C21104.6 (4)C34—C33—H33A119.7
C31—P—C11106.1 (4)C32—C33—H33A119.7
C21—P—C11103.5 (4)C35—C34—C33120.0 (9)
C31—P—Pt112.5 (3)C35—C34—H34A120.0
C21—P—Pt118.6 (3)C33—C34—H34A120.0
C11—P—Pt110.6 (3)C34—C35—C36120.4 (9)
C46—N1—C42117.6 (7)C34—C35—H35A119.8
C46—N1—Pt126.1 (5)C36—C35—H35A119.8
C42—N1—Pt116.0 (5)C31—C36—C35120.7 (8)
C56—N2—C52117.7 (7)C31—C36—H36A119.7
C56—N2—Pt128.0 (5)C35—C36—H36A119.7
C52—N2—Pt114.2 (5)N1—C42—C43121.4 (7)
C2—C1—Pt173.2 (7)N1—C42—C52114.8 (7)
C1—C2—C3175.7 (9)C43—C42—C52123.8 (7)
C4—C3—C8117.9 (8)C42—C43—C44120.5 (8)
C4—C3—C2121.9 (8)C42—C43—H43A119.7
C8—C3—C2120.2 (8)C44—C43—H43A119.7
C3—C4—C5121.8 (10)C45—C44—C43117.5 (8)
C3—C4—H4A119.1C45—C44—C47120.2 (8)
C5—C4—H4A119.1C43—C44—C47122.2 (8)
C6—C5—C4117.5 (11)C44—C45—C46120.1 (8)
C6—C5—H5A121.3C44—C45—H45A119.9
C4—C5—H5A121.3C46—C45—H45A119.9
C7—C6—C5122.6 (11)N1—C46—C45122.9 (8)
C7—C6—H6A118.7N1—C46—H46A118.6
C5—C6—H6A118.7C45—C46—H46A118.6
C8—C7—C6118.3 (11)C44—C47—H47A109.5
C8—C7—H7A120.8C44—C47—H47B109.5
C6—C7—H7A120.8H47A—C47—H47B109.5
C7—C8—C3121.9 (10)C44—C47—H47C109.5
C7—C8—H8A119.1H47A—C47—H47C109.5
C3—C8—H8A119.1H47B—C47—H47C109.5
C12—C11—C16118.7 (7)N2—C52—C53121.5 (7)
C12—C11—P121.4 (6)N2—C52—C42116.0 (7)
C16—C11—P119.8 (6)C53—C52—C42122.4 (7)
C11—C12—C13120.7 (8)C52—C53—C54121.9 (8)
C11—C12—H12A119.6C52—C53—H53A119.1
C13—C12—H12A119.6C54—C53—H53A119.1
C14—C13—C12119.9 (8)C55—C54—C53115.6 (8)
C14—C13—H13A120.0C55—C54—C57122.3 (8)
C12—C13—H13A120.0C53—C54—C57122.2 (9)
C15—C14—C13120.1 (8)C56—C55—C54121.1 (8)
C15—C14—H14A120.0C56—C55—H55A119.4
C13—C14—H14A120.0C54—C55—H55A119.4
C14—C15—C16120.5 (8)N2—C56—C55122.2 (8)
C14—C15—H15A119.7N2—C56—H56A118.9
C16—C15—H15A119.7C55—C56—H56A118.9
C11—C16—C15119.9 (8)C54—C57—H57A109.5
C11—C16—H16A120.0C54—C57—H57B109.5
C15—C16—H16A120.0H57A—C57—H57B109.5
C22—C21—C26118.6 (8)C54—C57—H57C109.5
C22—C21—P121.2 (7)H57A—C57—H57C109.5
C26—C21—P120.2 (7)H57B—C57—H57C109.5
C21—C22—C23120.8 (10)

Experimental details

Crystal data
Chemical formula[Pt(C8H5)(C18H15P)(C12H12N2)](SbF6)
Mr978.47
Crystal system, space groupMonoclinic, P21/n
Temperature (K)293
a, b, c (Å)14.4131 (4), 10.1848 (2), 24.7099 (7)
β (°) 98.915 (1)
V3)3583.46 (16)
Z4
Radiation typeMo Kα
µ (mm1)4.76
Crystal size (mm)0.50 × 0.30 × 0.25
Data collection
DiffractometerSiemens SMART CCD
diffractometer
Absorption correctionMulti-scan
(SADABS; Sheldrick, 1996)
Tmin, Tmax0.194, 0.304
No. of measured, independent and
observed [I > 2σ(I)] reflections
10524, 6291, 4473
Rint0.024
(sin θ/λ)max1)0.596
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.041, 0.110, 1.19
No. of reflections6291
No. of parameters442
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)1.04, 0.61

Computer programs: SMART (Siemens, 1996), SMART and SAINT (Siemens, 1994), XPREP (Siemens, 1994), SHELXTL (Siemens, 1994), SHELXTL.

Selected geometric parameters (Å, º) top
Pt—C11.954 (9)Pt—N22.094 (6)
Pt—N12.068 (6)Pt—P2.246 (2)
C1—Pt—N193.0 (3)C1—Pt—P88.9 (2)
C1—Pt—N2171.2 (3)N1—Pt—P175.58 (18)
N1—Pt—N278.6 (2)N2—Pt—P99.68 (18)
 

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