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The title compound, [Pt(C12H27P)2(C14H8N)2], is a mononuclear PtII di-yne exhibiting π-conjugation along the molecular backbone. It is used as a model species for rigid-rod platinum poly yne compounds of which it is a precursor. Such compounds are of interest due to the extended π-conjugation through the hetero-aromatic linker unit in the backbone.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536803017872/ww6109sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536803017872/ww6109Isup2.hkl
Contains datablock I

CCDC reference: 222816

Key indicators

  • Single-crystal X-ray study
  • T = 150 K
  • Mean [sigma](C-C) = 0.005 Å
  • R factor = 0.024
  • wR factor = 0.062
  • Data-to-parameter ratio = 16.2

checkCIF/PLATON results

No syntax errors found



Alert level C ABSTM02_ALERT_3_C The ratio of expected to reported Tmax/Tmin(RR) is > 1.10 Tmin and Tmax reported: 0.538 0.683 Tmin and Tmax expected: 0.414 0.674 RR = 1.284 Please check that your absorption correction is appropriate. PLAT060_ALERT_3_C Ratio Tmax/Tmin (Exp-to-Rep) (too) Large ....... 1.27 PLAT125_ALERT_4_C No _symmetry_space_group_name_Hall Given ....... ? PLAT128_ALERT_4_C Non-standard setting of Space group P21/c .... P21/a PLAT220_ALERT_2_C Large Non-Solvent C Ueq(max)/Ueq(min) ... 2.78 Ratio PLAT222_ALERT_3_C Large Non-Solvent H Ueq(max)/Ueq(min) ... 3.48 Ratio PLAT232_ALERT_2_C Hirshfeld Test Diff (M-X) Pt1 - C14 = 7.64 su PLAT371_ALERT_2_C Long C(sp2)-C(sp1) Bond C10 - C13 = 1.45 Ang. PLAT420_ALERT_2_C D-H Without Acceptor N1 - H1A ... ? PLAT710_ALERT_4_C Delete 1-2-3 or 2-3-4 Linear Torsion Angle ... # 29 C11 -C10 -C13 -C14 -153.00 6.00 1.555 1.555 1.555 1.555 PLAT710_ALERT_4_C Delete 1-2-3 or 2-3-4 Linear Torsion Angle ... # 30 C9 -C10 -C13 -C14 26.00 6.00 1.555 1.555 1.555 1.555 PLAT710_ALERT_4_C Delete 1-2-3 or 2-3-4 Linear Torsion Angle ... # 31 C10 -C13 -C14 -PT1 31.00 11.00 1.555 1.555 1.555 1.555 PLAT710_ALERT_4_C Delete 1-2-3 or 2-3-4 Linear Torsion Angle ... # 51 C13 -C14 -PT1 -C14 92.00 72.00 1.555 1.555 1.555 3.555 PLAT710_ALERT_4_C Delete 1-2-3 or 2-3-4 Linear Torsion Angle ... # 52 C13 -C14 -PT1 -P1 -170.00 7.00 1.555 1.555 1.555 1.555 PLAT710_ALERT_4_C Delete 1-2-3 or 2-3-4 Linear Torsion Angle ... # 53 C13 -C14 -PT1 -P1 10.00 7.00 1.555 1.555 1.555 3.555 PLAT710_ALERT_4_C Delete 1-2-3 or 2-3-4 Linear Torsion Angle ... # 60 C23 -P1 -PT1 -P1 85.00 31.00 1.555 1.555 1.555 3.555 PLAT710_ALERT_4_C Delete 1-2-3 or 2-3-4 Linear Torsion Angle ... # 61 C15 -P1 -PT1 -P1 -154.00 31.00 1.555 1.555 1.555 3.555 PLAT710_ALERT_4_C Delete 1-2-3 or 2-3-4 Linear Torsion Angle ... # 62 C19 -P1 -PT1 -P1 -36.00 31.00 1.555 1.555 1.555 3.555
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 18 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 4 ALERT type 2 Indicator that the structure model may be wrong or deficient 3 ALERT type 3 Indicator that the structure quality may be low 11 ALERT type 4 Improvement, methodology, query or suggestion

Comment top

In this paper, we report the structural characterization of the title compound, (I), which is a mononuclear platinum(II) di-yne species, trans-[Pt(PnBu3)2(—CCR)2] (R = carbazol-3-yl). Such platinum-containing species form the building blocks for rigid-rod organometallic poly-ynes of general formula trans-[Pt(PnBu3)2—CC—R—CC—] (R = aromatic or heteroaromatic linker unit). Platinum(II) poly-ynes are of immense current interest due to π-electron conjugation along the backbone, donor–acceptor metal–ligand interactions and novel photophysical properties (Wittmann et al., 1994; Beljonne et al., 1996; Younus et al., 1998; Chawdhury et al., 1998, 1999; Khan et al., 2002, 2003). They possess interesting optoelectronic properties useful for application in light-emitting diodes and photocells (Wilson et al., 2000, 2001). Precursors to these species, such as the title compound, are studied as models of the molecular and electronic properties and structure-property relationships in the metal poly-ynes.

The structure of (I) exhibits a C—H···N close contact between alkynyl atom H25a and N1, with a C25···N1 distance of 3.674 (5) Å (Table 2).

Experimental top

The title compound was synthesized by the following procedure. To a stirred solution of trans-[(PnBu3)2PtCl2] (0.38 g, 0.5 mmol) and 3-ethynylcarbazole (0.19 g, 1.0 mmol) in CH2Cl2/iPr2NH (50 ml, 1:1 v/v) under nitrogen was added a catalytic amount of CuI (5 mg). The yellow solution was stirred at room temperature for 15 h, after which all volatile components were removed under reduced pressure. The residue was dissolved in CH2Cl2 and passed through a silica column eluting with hexane/CH2Cl2 (1:1, v/v). Removal of the solvents under vacuo gave the title complex as a pale-yellow solid in 72% yield.

Refinement top

Aromatic, methylene and methyl H atom types were constrained as riding atoms fixed to the parent atoms with distances of 0.95, 0.99 and 0.98 Å, respectively. The isotropic displacement parameters were fixed to 120% of that of the parent atom for aromatic and methylene H atoms and 150% for methyl H atoms.

Structure description top

In this paper, we report the structural characterization of the title compound, (I), which is a mononuclear platinum(II) di-yne species, trans-[Pt(PnBu3)2(—CCR)2] (R = carbazol-3-yl). Such platinum-containing species form the building blocks for rigid-rod organometallic poly-ynes of general formula trans-[Pt(PnBu3)2—CC—R—CC—] (R = aromatic or heteroaromatic linker unit). Platinum(II) poly-ynes are of immense current interest due to π-electron conjugation along the backbone, donor–acceptor metal–ligand interactions and novel photophysical properties (Wittmann et al., 1994; Beljonne et al., 1996; Younus et al., 1998; Chawdhury et al., 1998, 1999; Khan et al., 2002, 2003). They possess interesting optoelectronic properties useful for application in light-emitting diodes and photocells (Wilson et al., 2000, 2001). Precursors to these species, such as the title compound, are studied as models of the molecular and electronic properties and structure-property relationships in the metal poly-ynes.

The structure of (I) exhibits a C—H···N close contact between alkynyl atom H25a and N1, with a C25···N1 distance of 3.674 (5) Å (Table 2).

Computing details top

Data collection: COLLECT (Nonius, 1997); cell refinement: HKL SCALEPACK (Otwinowski & Minor, 1997); data reduction: HKL DENZO (Otwinowski & Minor, 1997) and SCALEPACK; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997), X-SEED (Barbour, 1999) and POV-RAY for Windows (Cason, 1999); software used to prepare material for publication: WinGX publication routines (Farrugia, 1999).

Figures top
[Figure 1] Fig. 1. The molecular structure of (I), showing the atom-numbering scheme. Displacement ellipsoids are drawn at the 50% probability level.
[Figure 2] Fig. 2. Packing diagram of compound (I), showing the close intermolecular contact between atoms N1 and H25a.
(I) top
Crystal data top
[Pt(C12H27P)2(C14H8N)2]F(000) = 1008
Mr = 980.13Dx = 1.359 Mg m3
Monoclinic, P21/aMo Kα radiation, λ = 0.71073 Å
a = 9.2860 (1) ÅCell parameters from 25483 reflections
b = 19.4330 (3) Åθ = 2.9–27.5°
c = 13.6980 (2) ŵ = 3.03 mm1
β = 104.238 (1)°T = 150 K
V = 2395.94 (6) Å3Block, white
Z = 20.33 × 0.25 × 0.13 mm
Data collection top
Bruker–Nonius KappaCCD
diffractometer
3270 reflections with I > 2σ(I)
φ and ω scansRint = 0.070
Absorption correction: multi-scan
(SORTAV; Blessing, 1995)
θmax = 25.0°, θmin = 3.9°
Tmin = 0.538, Tmax = 0.683h = 1111
35095 measured reflectionsk = 2323
4221 independent reflectionsl = 1616
Refinement top
Refinement on F2H-atom parameters constrained
Least-squares matrix: full w = 1/[σ2(Fo2) + (0.0312P)2 + 0.9277P]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.024(Δ/σ)max < 0.001
wR(F2) = 0.062Δρmax = 0.70 e Å3
S = 1.03Δρmin = 1.32 e Å3
4221 reflectionsExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
260 parametersExtinction coefficient: 0.0016 (3)
0 restraints
Crystal data top
[Pt(C12H27P)2(C14H8N)2]V = 2395.94 (6) Å3
Mr = 980.13Z = 2
Monoclinic, P21/aMo Kα radiation
a = 9.2860 (1) ŵ = 3.03 mm1
b = 19.4330 (3) ÅT = 150 K
c = 13.6980 (2) Å0.33 × 0.25 × 0.13 mm
β = 104.238 (1)°
Data collection top
Bruker–Nonius KappaCCD
diffractometer
4221 independent reflections
Absorption correction: multi-scan
(SORTAV; Blessing, 1995)
3270 reflections with I > 2σ(I)
Tmin = 0.538, Tmax = 0.683Rint = 0.070
35095 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0240 restraints
wR(F2) = 0.062H-atom parameters constrained
S = 1.03Δρmax = 0.70 e Å3
4221 reflectionsΔρmin = 1.32 e Å3
260 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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.9298 (4)0.1955 (2)0.5822 (3)0.0479 (10)
H11.00710.20580.640.057*
C20.9142 (4)0.23525 (19)0.4978 (3)0.0439 (10)
H20.97950.27260.49610.053*
C30.7997 (4)0.21912 (16)0.4149 (2)0.0319 (8)
C40.7016 (3)0.16412 (15)0.4165 (2)0.0277 (7)
C50.7203 (4)0.12433 (18)0.5033 (2)0.0371 (8)
H50.65520.0870.50590.044*
C60.8352 (4)0.1400 (2)0.5858 (3)0.0449 (9)
H60.84980.1130.64520.054*
C70.6357 (3)0.21772 (15)0.2628 (2)0.0264 (7)
C80.5550 (4)0.23210 (15)0.1652 (2)0.0298 (8)
H80.58140.26930.12810.036*
C90.4354 (4)0.19049 (15)0.1244 (2)0.0291 (7)
H90.37920.19970.05780.035*
C100.3925 (3)0.13462 (15)0.1770 (2)0.0260 (7)
C110.4738 (3)0.12194 (15)0.2752 (2)0.0240 (7)
H110.44620.08520.31250.029*
C120.5956 (3)0.16302 (15)0.3189 (2)0.0247 (7)
C130.2679 (4)0.09229 (16)0.1272 (2)0.0268 (7)
C140.1660 (4)0.05812 (16)0.0815 (2)0.0281 (7)
C150.3196 (3)0.07956 (16)0.0225 (2)0.0304 (7)
H15A0.36950.05180.03680.036*
H15B0.39130.08610.06450.036*
C160.2821 (4)0.15066 (16)0.0146 (2)0.0349 (8)
H16A0.37630.17590.04120.042*
H16B0.22420.17680.04410.042*
C170.1956 (4)0.15002 (19)0.0951 (3)0.0428 (9)
H17A0.09150.13670.06390.051*
H17B0.23860.11470.1460.051*
C180.1964 (6)0.2188 (2)0.1472 (3)0.0672 (14)
H18A0.1390.21520.19820.101*
H18B0.15180.25380.09750.101*
H18C0.2990.23180.17970.101*
C190.2441 (4)0.04446 (15)0.1407 (2)0.0278 (7)
H19A0.30050.07060.08150.033*
H19B0.16250.07450.17740.033*
C200.3479 (4)0.03028 (19)0.2099 (2)0.0319 (7)
H20A0.29440.00210.26770.038*
H20B0.43420.00330.17230.038*
C210.4034 (4)0.09568 (17)0.2492 (3)0.0371 (8)
H21A0.31750.1220.28880.044*
H21B0.45420.12460.19140.044*
C220.5103 (4)0.0809 (2)0.3149 (3)0.0497 (10)
H22A0.54320.12430.33850.075*
H22B0.59660.05560.27550.075*
H22C0.45990.0530.37290.075*
C230.0899 (4)0.08302 (16)0.2067 (2)0.0283 (7)
H23A0.04050.1240.18690.034*
H23B0.17480.09940.23210.034*
C240.0199 (4)0.04668 (17)0.2924 (2)0.0333 (8)
H24A0.02860.00590.31370.04*
H24B0.10610.03050.26820.04*
C250.0734 (5)0.0940 (2)0.3816 (3)0.0507 (10)
H25A0.11470.13620.35840.061*
H25B0.0130.10790.40750.061*
C260.1896 (5)0.0629 (2)0.4668 (3)0.0650 (12)
H26A0.21850.09660.52150.098*
H26B0.27690.05020.44260.098*
H26C0.14910.02180.49180.098*
N10.7591 (3)0.25035 (14)0.3214 (2)0.0336 (7)
H1A0.80490.28560.30210.04*
P10.16139 (9)0.03072 (5)0.09511 (6)0.02533 (19)
Pt10000.02389 (8)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.034 (2)0.074 (3)0.034 (2)0.011 (2)0.0037 (17)0.0149 (19)
C20.033 (2)0.055 (2)0.046 (2)0.0192 (18)0.0154 (18)0.0157 (18)
C30.0259 (19)0.0358 (19)0.0375 (19)0.0058 (15)0.0141 (16)0.0086 (15)
C40.0228 (18)0.0307 (17)0.0322 (18)0.0022 (14)0.0117 (15)0.0055 (14)
C50.031 (2)0.045 (2)0.038 (2)0.0060 (16)0.0135 (17)0.0011 (16)
C60.037 (2)0.063 (3)0.035 (2)0.005 (2)0.0087 (18)0.0016 (18)
C70.0235 (18)0.0253 (17)0.0337 (18)0.0048 (14)0.0132 (15)0.0081 (14)
C80.033 (2)0.0269 (17)0.0342 (19)0.0013 (15)0.0181 (16)0.0000 (14)
C90.031 (2)0.0305 (18)0.0275 (17)0.0075 (15)0.0104 (15)0.0005 (14)
C100.0216 (18)0.0267 (17)0.0332 (18)0.0030 (14)0.0137 (15)0.0064 (14)
C110.0224 (18)0.0226 (16)0.0310 (18)0.0005 (13)0.0144 (15)0.0023 (13)
C120.0215 (18)0.0257 (16)0.0297 (17)0.0009 (13)0.0118 (14)0.0052 (13)
C130.0231 (19)0.0319 (18)0.0282 (17)0.0034 (15)0.0114 (15)0.0057 (14)
C140.0260 (19)0.0338 (18)0.0275 (17)0.0059 (15)0.0124 (15)0.0023 (14)
C150.0191 (18)0.0376 (19)0.0351 (18)0.0028 (14)0.0078 (15)0.0057 (15)
C160.034 (2)0.0377 (19)0.0315 (19)0.0022 (16)0.0050 (16)0.0011 (15)
C170.040 (2)0.050 (2)0.040 (2)0.0012 (18)0.0136 (18)0.0040 (17)
C180.112 (4)0.054 (3)0.043 (2)0.009 (3)0.036 (3)0.006 (2)
C190.0244 (19)0.0306 (19)0.0323 (18)0.0010 (14)0.0144 (15)0.0044 (14)
C200.0264 (19)0.0387 (18)0.0328 (18)0.0046 (16)0.0119 (15)0.0058 (16)
C210.032 (2)0.044 (2)0.037 (2)0.0052 (16)0.0118 (17)0.0017 (16)
C220.046 (3)0.064 (3)0.045 (2)0.012 (2)0.024 (2)0.000 (2)
C230.0248 (19)0.0322 (18)0.0297 (17)0.0006 (14)0.0101 (15)0.0075 (14)
C240.027 (2)0.041 (2)0.0347 (19)0.0006 (15)0.0129 (16)0.0026 (15)
C250.050 (3)0.050 (2)0.043 (2)0.002 (2)0.005 (2)0.0085 (18)
C260.060 (3)0.079 (3)0.046 (2)0.002 (2)0.006 (2)0.010 (2)
N10.0332 (17)0.0329 (15)0.0386 (17)0.0138 (13)0.0162 (14)0.0040 (13)
P10.0195 (4)0.0297 (4)0.0283 (4)0.0002 (4)0.0089 (4)0.0053 (4)
Pt10.01673 (11)0.03025 (12)0.02588 (12)0.00045 (8)0.00753 (7)0.00580 (8)
Geometric parameters (Å, º) top
C1—C21.369 (5)C17—H17B0.99
C1—C61.398 (5)C18—H18A0.98
C1—H10.95C18—H18B0.98
C2—C31.388 (5)C18—H18C0.98
C2—H20.95C19—C201.534 (4)
C3—N11.383 (4)C19—P11.830 (3)
C3—C41.408 (4)C19—H19A0.99
C4—C51.393 (4)C19—H19B0.99
C4—C121.453 (4)C20—C211.519 (5)
C5—C61.384 (5)C20—H20A0.99
C5—H50.95C20—H20B0.99
C6—H60.95C21—C221.522 (5)
C7—N11.381 (4)C21—H21A0.99
C7—C81.391 (4)C21—H21B0.99
C7—C121.414 (4)C22—H22A0.98
C8—C91.376 (4)C22—H22B0.98
C8—H80.95C22—H22C0.98
C9—C101.414 (4)C23—C241.525 (4)
C9—H90.95C23—P11.819 (3)
C10—C111.393 (4)C23—H23A0.99
C10—C131.447 (4)C23—H23B0.99
C11—C121.393 (4)C24—C251.513 (4)
C11—H110.95C24—H24A0.99
C13—C141.199 (4)C24—H24B0.99
C14—Pt12.013 (3)C25—C261.508 (5)
C15—C161.541 (4)C25—H25A0.99
C15—P11.825 (3)C25—H25B0.99
C15—H15A0.99C26—H26A0.98
C15—H15B0.99C26—H26B0.98
C16—C171.516 (5)C26—H26C0.98
C16—H16A0.99N1—H1A0.88
C16—H16B0.99P1—Pt12.2935 (8)
C17—C181.514 (5)Pt1—C14i2.013 (3)
C17—H17A0.99Pt1—P1i2.2935 (8)
C2—C1—C6121.9 (3)C20—C19—H19A108.1
C2—C1—H1119.1P1—C19—H19A108.1
C6—C1—H1119.1C20—C19—H19B108.1
C1—C2—C3117.7 (3)P1—C19—H19B108.1
C1—C2—H2121.2H19A—C19—H19B107.3
C3—C2—H2121.2C21—C20—C19112.8 (3)
N1—C3—C2129.7 (3)C21—C20—H20A109
N1—C3—C4108.5 (3)C19—C20—H20A109
C2—C3—C4121.8 (3)C21—C20—H20B109
C5—C4—C3119.3 (3)C19—C20—H20B109
C5—C4—C12133.8 (3)H20A—C20—H20B107.8
C3—C4—C12106.9 (3)C20—C21—C22112.2 (3)
C6—C5—C4118.9 (3)C20—C21—H21A109.2
C6—C5—H5120.5C22—C21—H21A109.2
C4—C5—H5120.5C20—C21—H21B109.2
C5—C6—C1120.4 (3)C22—C21—H21B109.2
C5—C6—H6119.8H21A—C21—H21B107.9
C1—C6—H6119.8C21—C22—H22A109.5
N1—C7—C8129.8 (3)C21—C22—H22B109.5
N1—C7—C12108.7 (3)H22A—C22—H22B109.5
C8—C7—C12121.5 (3)C21—C22—H22C109.5
C9—C8—C7117.6 (3)H22A—C22—H22C109.5
C9—C8—H8121.2H22B—C22—H22C109.5
C7—C8—H8121.2C24—C23—P1115.1 (2)
C8—C9—C10123.0 (3)C24—C23—H23A108.5
C8—C9—H9118.5P1—C23—H23A108.5
C10—C9—H9118.5C24—C23—H23B108.5
C11—C10—C9118.3 (3)P1—C23—H23B108.5
C11—C10—C13122.4 (3)H23A—C23—H23B107.5
C9—C10—C13119.3 (3)C25—C24—C23111.4 (3)
C10—C11—C12120.2 (3)C25—C24—H24A109.4
C10—C11—H11119.9C23—C24—H24A109.4
C12—C11—H11119.9C25—C24—H24B109.4
C11—C12—C7119.4 (3)C23—C24—H24B109.4
C11—C12—C4134.3 (3)H24A—C24—H24B108
C7—C12—C4106.3 (3)C26—C25—C24114.3 (3)
C14—C13—C10176.7 (3)C26—C25—H25A108.7
C13—C14—Pt1177.5 (3)C24—C25—H25A108.7
C16—C15—P1115.4 (2)C26—C25—H25B108.7
C16—C15—H15A108.4C24—C25—H25B108.7
P1—C15—H15A108.4H25A—C25—H25B107.6
C16—C15—H15B108.4C25—C26—H26A109.5
P1—C15—H15B108.4C25—C26—H26B109.5
H15A—C15—H15B107.5H26A—C26—H26B109.5
C17—C16—C15115.8 (3)C25—C26—H26C109.5
C17—C16—H16A108.3H26A—C26—H26C109.5
C15—C16—H16A108.3H26B—C26—H26C109.5
C17—C16—H16B108.3C7—N1—C3109.5 (3)
C15—C16—H16B108.3C7—N1—H1A125.2
H16A—C16—H16B107.4C3—N1—H1A125.2
C18—C17—C16113.2 (3)C23—P1—C15104.23 (14)
C18—C17—H17A108.9C23—P1—C19104.85 (15)
C16—C17—H17A108.9C15—P1—C19104.61 (15)
C18—C17—H17B108.9C23—P1—Pt1117.91 (11)
C16—C17—H17B108.9C15—P1—Pt1112.13 (11)
H17A—C17—H17B107.8C19—P1—Pt1111.94 (10)
C17—C18—H18A109.5C14i—Pt1—C14180.0 (3)
C17—C18—H18B109.5C14i—Pt1—P186.70 (8)
H18A—C18—H18B109.5C14—Pt1—P193.30 (8)
C17—C18—H18C109.5C14i—Pt1—P1i93.30 (8)
H18A—C18—H18C109.5C14—Pt1—P1i86.70 (8)
H18B—C18—H18C109.5P1—Pt1—P1i180.00 (5)
C20—C19—P1116.6 (2)
C6—C1—C2—C30.4 (6)P1—C15—C16—C1768.8 (3)
C1—C2—C3—N1179.9 (3)C15—C16—C17—C18165.1 (3)
C1—C2—C3—C40.3 (5)P1—C19—C20—C21176.4 (2)
N1—C3—C4—C5179.8 (3)C19—C20—C21—C22178.1 (3)
C2—C3—C4—C50.5 (5)P1—C23—C24—C25179.9 (3)
N1—C3—C4—C120.6 (3)C23—C24—C25—C26176.4 (3)
C2—C3—C4—C12179.0 (3)C8—C7—N1—C3178.6 (3)
C3—C4—C5—C60.0 (5)C12—C7—N1—C30.9 (3)
C12—C4—C5—C6179.4 (3)C2—C3—N1—C7178.7 (3)
C4—C5—C6—C10.7 (5)C4—C3—N1—C71.0 (3)
C2—C1—C6—C50.9 (6)C24—C23—P1—C15166.1 (2)
N1—C7—C8—C9179.8 (3)C24—C23—P1—C1956.4 (3)
C12—C7—C8—C90.8 (4)C24—C23—P1—Pt168.9 (2)
C7—C8—C9—C100.1 (5)C16—C15—P1—C2363.2 (3)
C8—C9—C10—C111.0 (4)C16—C15—P1—C19173.0 (2)
C8—C9—C10—C13178.2 (3)C16—C15—P1—Pt165.5 (2)
C9—C10—C11—C121.0 (4)C20—C19—P1—C2347.9 (3)
C13—C10—C11—C12178.2 (3)C20—C19—P1—C1561.4 (3)
C10—C11—C12—C70.1 (4)C20—C19—P1—Pt1176.9 (2)
C10—C11—C12—C4180.0 (3)C13—C14—Pt1—C14i92 (72)
N1—C7—C12—C11179.7 (3)C13—C14—Pt1—P1170 (7)
C8—C7—C12—C110.8 (4)C13—C14—Pt1—P1i10 (7)
N1—C7—C12—C40.5 (3)C23—P1—Pt1—C14i174.09 (15)
C8—C7—C12—C4179.0 (3)C15—P1—Pt1—C14i64.87 (14)
C5—C4—C12—C110.3 (6)C19—P1—Pt1—C14i52.35 (15)
C3—C4—C12—C11179.7 (3)C23—P1—Pt1—C145.91 (15)
C5—C4—C12—C7179.6 (3)C15—P1—Pt1—C14115.13 (14)
C3—C4—C12—C70.1 (3)C19—P1—Pt1—C14127.65 (15)
C11—C10—C13—C14153 (6)C23—P1—Pt1—P1i85 (31)
C9—C10—C13—C1426 (6)C15—P1—Pt1—P1i154 (31)
C10—C13—C14—Pt131 (11)C19—P1—Pt1—P1i36 (31)
Symmetry code: (i) x, y, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C25—H25A···N1ii0.992.693.674 (5)171
Symmetry code: (ii) x+1/2, y+1/2, z.

Experimental details

Crystal data
Chemical formula[Pt(C12H27P)2(C14H8N)2]
Mr980.13
Crystal system, space groupMonoclinic, P21/a
Temperature (K)150
a, b, c (Å)9.2860 (1), 19.4330 (3), 13.6980 (2)
β (°) 104.238 (1)
V3)2395.94 (6)
Z2
Radiation typeMo Kα
µ (mm1)3.03
Crystal size (mm)0.33 × 0.25 × 0.13
Data collection
DiffractometerBruker–Nonius KappaCCD
Absorption correctionMulti-scan
(SORTAV; Blessing, 1995)
Tmin, Tmax0.538, 0.683
No. of measured, independent and
observed [I > 2σ(I)] reflections
35095, 4221, 3270
Rint0.070
(sin θ/λ)max1)0.595
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.024, 0.062, 1.03
No. of reflections4221
No. of parameters260
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.70, 1.32

Computer programs: COLLECT (Nonius, 1997), HKL SCALEPACK (Otwinowski & Minor, 1997), HKL DENZO (Otwinowski & Minor, 1997) and SCALEPACK, SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), ORTEP-3 for Windows (Farrugia, 1997), X-SEED (Barbour, 1999) and POV-RAY for Windows (Cason, 1999), WinGX publication routines (Farrugia, 1999).

Selected geometric parameters (Å, º) top
C3—N11.383 (4)C13—C141.199 (4)
C3—C41.408 (4)C14—Pt12.013 (3)
C4—C121.453 (4)C15—P11.825 (3)
C7—N11.381 (4)C19—P11.830 (3)
C7—C121.414 (4)C23—P11.819 (3)
C10—C131.447 (4)P1—Pt12.2935 (8)
N1—C3—C4108.5 (3)C7—N1—C3109.5 (3)
C3—C4—C12106.9 (3)C23—P1—Pt1117.91 (11)
N1—C7—C12108.7 (3)C15—P1—Pt1112.13 (11)
C7—C12—C4106.3 (3)C19—P1—Pt1111.94 (10)
C14—C13—C10176.7 (3)C14—Pt1—P193.30 (8)
C13—C14—Pt1177.5 (3)
N1—C3—C4—C120.6 (3)C4—C3—N1—C71.0 (3)
C8—C9—C10—C13178.2 (3)C13—C14—Pt1—P1170 (7)
N1—C7—C12—C40.5 (3)C23—P1—Pt1—C145.91 (15)
C3—C4—C12—C70.1 (3)C15—P1—Pt1—C14115.13 (14)
C12—C7—N1—C30.9 (3)C19—P1—Pt1—C14127.65 (15)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C25—H25A···N1i0.992.693.674 (5)171
Symmetry code: (i) x+1/2, y+1/2, z.
 

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