Literature DB >> 21577472

Bromido(2,2':6',2''-terpyridine)platinum(II) dibromidoaurate(I) dimethyl sulfoxide solvate.

Michael I Kahn, James A Golen, Arnold L Rheingold, Linda H Doerrer.   

Abstract

The crystal structure of the title compound, [PtBr(C(15)H(11)N(3))][AuBr(2)]·(CH(3))(2)SO, exhibits infinite chains of {PtAuPt}(∞) metallophilic inter-actions along the b axis. Two cations and one anion stack in a trimer with a unique PtAu distance of 3.3361 (5) Å and PtPt contacts of 3.4335 (6) Å. The remaining [AuBr(2)](-) anion forms no close contacts.

Entities:  

Year:  2009        PMID: 21577472      PMCID: PMC2970032          DOI: 10.1107/S1600536809033248

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For the related chloride structure, [Pt(tpy)Cl][AuCl2] (tpy=2,2′:6′,2"-terpyridine), see Hayoun et al. (2006 ▶). For the related [Pt(tpy)I][AuI2] complex, see Angle et al. (2007 ▶). For a review of double salts with metallophilic inter­actions, see Doerrer (2008 ▶). The synthesis of [Pt(tpy)X]X complexes (X = Cl, Br, I) is discussed in Annibale et al. (2004 ▶), and the preparation of [AuX 2]− in Braunstein & Clark (1973 ▶). For background to metallophilic inter­actions, see: Pyykkö (1997 ▶). For a description of the Cambridge Structural Database, see: Allen (2002 ▶).

Experimental

Crystal data

[PtBr(C15H11N3)][AuBr2]·C2H6OS M = 943.18 Triclinic, a = 8.1463 (11) Å b = 10.0930 (14) Å c = 13.9624 (19) Å α = 81.905 (2)° β = 87.675 (2)° γ = 68.532 (3)° V = 1057.6 (3) Å3 Z = 2 Mo Kα radiation μ = 19.31 mm−1 T = 208 K 0.30 × 0.20 × 0.15 mm

Data collection

Bruker SMART CCD area-detector diffractometer Absorption correction: multi-scan (SADABS; Sheldrick, 2000 ▶) T min = 0.068, T max = 0.160 7511 measured reflections 4826 independent reflections 4312 reflections with I > 2σ(I) R int = 0.019

Refinement

R[F 2 > 2σ(F 2)] = 0.039 wR(F 2) = 0.103 S = 1.01 4826 reflections 249 parameters H-atom parameters constrained Δρmax = 2.01 e Å−3 Δρmin = −4.14 e Å−3 Data collection: SMART (Bruker, 2005 ▶); cell refinement: SAINT (Bruker, 2005 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 (Farrugia, 1997 ▶); software used to prepare material for publication: SHELXTL (Sheldrick, 2008 ▶). Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809033248/cv2602sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536809033248/cv2602Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
[PtBr(C15H11N3)][AuBr2]·C2H6OSZ = 2
Mr = 943.18F(000) = 852
Triclinic, P1Dx = 2.962 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 8.1463 (11) ÅCell parameters from 5521 reflections
b = 10.0930 (14) Åθ = 2.5–28.2°
c = 13.9624 (19) ŵ = 19.31 mm1
α = 81.905 (2)°T = 208 K
β = 87.675 (2)°Block, red
γ = 68.532 (3)°0.30 × 0.20 × 0.15 mm
V = 1057.6 (3) Å3
Bruker SMART CCD area-detector diffractometer4826 independent reflections
Radiation source: fine-focus sealed tube4312 reflections with I > 2σ(I)
graphiteRint = 0.019
φ and ω scansθmax = 28.2°, θmin = 1.5°
Absorption correction: multi-scan (SADABS; Sheldrick, 2000)h = −8→10
Tmin = 0.068, Tmax = 0.160k = −13→10
7511 measured reflectionsl = −18→17
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.039Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.103H-atom parameters constrained
S = 1.01w = 1/[σ2(Fo2) + (0.0756P)2] P = (Fo2 + 2Fc2)/3
4826 reflections(Δ/σ)max = 0.001
249 parametersΔρmax = 2.01 e Å3
0 restraintsΔρmin = −4.13 e Å3
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 F^2^ against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F^2^, conventional R-factors R are based on F, with F set to zero for negative F^2^. The threshold expression of F^2^ > σ(F^2^) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F^2^ are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.
xyzUiso*/Ueq
Au11.00000.50001.00000.03631 (12)
Au20.50000.50000.50000.03754 (12)
Pt10.01155 (3)0.82805 (2)−0.005856 (15)0.02023 (9)
Br1−0.25578 (8)0.87221 (7)0.08893 (5)0.03042 (15)
Br20.98737 (9)0.44194 (7)1.17203 (6)0.03918 (18)
Br30.75978 (12)0.32173 (10)0.45033 (6)0.0514 (2)
S10.3410 (3)1.1786 (2)0.55776 (14)0.0477 (5)
N10.1935 (6)0.7291 (5)0.1004 (4)0.0220 (10)
N3−0.0990 (6)0.9177 (5)−0.1372 (4)0.0212 (9)
N20.2244 (6)0.7937 (5)−0.0823 (4)0.0196 (9)
O10.3110 (10)1.0395 (7)0.5756 (6)0.079 (2)
C10.1657 (9)0.6989 (7)0.1947 (5)0.0292 (13)
H1A0.04930.72570.21720.035*
C20.3038 (10)0.6292 (8)0.2598 (5)0.0363 (15)
H2A0.28090.60860.32560.044*
C30.4751 (10)0.5900 (8)0.2277 (5)0.0356 (15)
H3A0.57000.54200.27130.043*
C40.5057 (9)0.6221 (7)0.1305 (5)0.0313 (14)
H4A0.62160.59760.10720.038*
C50.3634 (8)0.6908 (6)0.0682 (4)0.0239 (12)
C60.3808 (8)0.7276 (7)−0.0365 (5)0.0275 (13)
C70.5327 (8)0.7028 (6)−0.0895 (5)0.0274 (13)
H7A0.64400.6568−0.05920.033*
C80.5184 (8)0.7467 (7)−0.1880 (5)0.0307 (14)
H8A0.62150.7295−0.22490.037*
C90.3560 (8)0.8153 (7)−0.2337 (4)0.0270 (12)
H9A0.34750.8453−0.30080.032*
C100.2060 (8)0.8385 (6)−0.1780 (4)0.0237 (12)
C110.0209 (8)0.9105 (6)−0.2094 (4)0.0241 (12)
C12−0.0334 (9)0.9673 (7)−0.3032 (5)0.0306 (14)
H12A0.05080.9637−0.35190.037*
C13−0.2089 (9)1.0288 (7)−0.3261 (5)0.0344 (15)
H13A−0.24701.0662−0.39030.041*
C14−0.3288 (9)1.0348 (8)−0.2530 (5)0.0356 (15)
H14A−0.45021.0775−0.26720.043*
C15−0.2725 (8)0.9788 (6)−0.1592 (5)0.0270 (13)
H15A−0.35590.9833−0.11000.032*
C160.2828 (11)1.2500 (9)0.4364 (5)0.0473 (19)
H16A0.35721.18380.39450.071*
H16B0.29871.34140.42220.071*
H16C0.16031.26420.42550.071*
C170.1620 (13)1.3074 (11)0.6114 (7)0.063 (3)
H17A0.17991.29240.68090.094*
H17B0.05251.29650.59690.094*
H17C0.15601.40350.58560.094*
U11U22U33U12U13U23
Au10.02295 (18)0.0324 (2)0.0533 (3)−0.00747 (15)−0.00103 (16)−0.01197 (17)
Au20.0434 (2)0.0484 (2)0.0243 (2)−0.02176 (18)−0.00643 (16)0.00001 (16)
Pt10.01865 (13)0.02448 (13)0.01805 (14)−0.00871 (9)0.00074 (9)−0.00222 (9)
Br10.0254 (3)0.0345 (3)0.0311 (3)−0.0109 (3)0.0069 (2)−0.0054 (3)
Br20.0306 (3)0.0323 (3)0.0542 (5)−0.0095 (3)−0.0011 (3)−0.0097 (3)
Br30.0499 (5)0.0579 (5)0.0436 (5)−0.0160 (4)−0.0025 (4)−0.0072 (4)
S10.0383 (9)0.0678 (13)0.0308 (10)−0.0188 (9)−0.0043 (8)0.0137 (9)
N10.021 (2)0.027 (2)0.019 (2)−0.0096 (19)−0.0004 (19)−0.0027 (19)
N30.017 (2)0.022 (2)0.022 (2)−0.0041 (18)−0.0033 (18)−0.0013 (19)
N20.018 (2)0.021 (2)0.020 (2)−0.0077 (18)0.0020 (18)−0.0030 (19)
O10.081 (5)0.057 (4)0.079 (5)−0.020 (4)0.013 (4)0.033 (4)
C10.034 (3)0.035 (3)0.021 (3)−0.017 (3)0.003 (3)−0.002 (3)
C20.042 (4)0.045 (4)0.023 (3)−0.020 (3)−0.001 (3)0.005 (3)
C30.039 (4)0.038 (4)0.029 (4)−0.015 (3)−0.012 (3)0.006 (3)
C40.030 (3)0.034 (3)0.032 (4)−0.013 (3)−0.004 (3)−0.004 (3)
C50.023 (3)0.025 (3)0.024 (3)−0.011 (2)0.000 (2)−0.001 (2)
C60.024 (3)0.030 (3)0.028 (3)−0.010 (2)−0.001 (2)−0.003 (3)
C70.023 (3)0.029 (3)0.029 (3)−0.008 (2)−0.002 (2)−0.004 (3)
C80.024 (3)0.036 (3)0.032 (4)−0.011 (3)0.007 (3)−0.005 (3)
C90.027 (3)0.035 (3)0.020 (3)−0.013 (3)0.002 (2)−0.002 (2)
C100.025 (3)0.023 (3)0.025 (3)−0.010 (2)0.001 (2)−0.003 (2)
C110.022 (3)0.026 (3)0.025 (3)−0.008 (2)−0.001 (2)−0.007 (2)
C120.036 (3)0.029 (3)0.026 (3)−0.013 (3)−0.003 (3)0.001 (3)
C130.035 (3)0.036 (3)0.029 (4)−0.010 (3)−0.009 (3)0.001 (3)
C140.027 (3)0.042 (4)0.035 (4)−0.010 (3)−0.010 (3)0.002 (3)
C150.022 (3)0.030 (3)0.029 (3)−0.009 (2)−0.003 (2)−0.003 (3)
C160.057 (5)0.060 (5)0.028 (4)−0.025 (4)0.001 (3)−0.001 (3)
C170.070 (6)0.084 (7)0.049 (5)−0.040 (5)0.016 (5)−0.025 (5)
Au1—Br2i2.3981 (9)C4—H4A0.9400
Au1—Br22.3981 (9)C5—C61.471 (9)
Au2—Br32.3753 (9)C6—C71.375 (9)
Au2—Br3ii2.3753 (9)C7—C81.381 (9)
Pt1—N21.944 (5)C7—H7A0.9400
Pt1—N32.015 (5)C8—C91.383 (9)
Pt1—N12.018 (5)C8—H8A0.9400
Pt1—Br12.4320 (7)C9—C101.385 (8)
S1—O11.497 (7)C9—H9A0.9400
S1—C161.757 (8)C10—C111.468 (8)
S1—C171.782 (9)C11—C121.376 (9)
N1—C11.338 (8)C12—C131.365 (9)
N1—C51.369 (7)C12—H12A0.9400
N3—C151.348 (7)C13—C141.376 (10)
N3—C111.366 (8)C13—H13A0.9400
N2—C61.342 (7)C14—C151.376 (9)
N2—C101.345 (8)C14—H14A0.9400
C1—C21.382 (10)C15—H15A0.9400
C1—H1A0.9400C16—H16A0.9700
C2—C31.379 (10)C16—H16B0.9700
C2—H2A0.9400C16—H16C0.9700
C3—C41.385 (9)C17—H17A0.9700
C3—H3A0.9400C17—H17B0.9700
C4—C51.380 (9)C17—H17C0.9700
Br2i—Au1—Br2180.0C6—C7—H7A120.7
Br3—Au2—Br3ii180.000 (1)C8—C7—H7A120.7
N2—Pt1—N380.7 (2)C7—C8—C9121.5 (6)
N2—Pt1—N180.8 (2)C7—C8—H8A119.2
N3—Pt1—N1161.5 (2)C9—C8—H8A119.2
N2—Pt1—Br1179.63 (16)C8—C9—C10118.2 (6)
N3—Pt1—Br198.95 (14)C8—C9—H9A120.9
N1—Pt1—Br199.58 (14)C10—C9—H9A120.9
O1—S1—C16107.0 (4)N2—C10—C9118.9 (5)
O1—S1—C17106.8 (4)N2—C10—C11113.0 (5)
C16—S1—C1797.3 (4)C9—C10—C11128.2 (6)
C1—N1—C5118.9 (5)N3—C11—C12120.8 (6)
C1—N1—Pt1127.8 (4)N3—C11—C10114.7 (5)
C5—N1—Pt1113.3 (4)C12—C11—C10124.4 (6)
C15—N3—C11119.1 (5)C13—C12—C11120.3 (7)
C15—N3—Pt1127.2 (4)C13—C12—H12A119.8
C11—N3—Pt1113.6 (4)C11—C12—H12A119.8
C6—N2—C10123.9 (5)C12—C13—C14118.4 (6)
C6—N2—Pt1118.2 (4)C12—C13—H13A120.8
C10—N2—Pt1117.9 (4)C14—C13—H13A120.8
N1—C1—C2121.7 (6)C13—C14—C15120.6 (6)
N1—C1—H1A119.2C13—C14—H14A119.7
C2—C1—H1A119.2C15—C14—H14A119.7
C3—C2—C1119.7 (6)N3—C15—C14120.7 (6)
C3—C2—H2A120.1N3—C15—H15A119.7
C1—C2—H2A120.1C14—C15—H15A119.7
C2—C3—C4119.2 (6)S1—C16—H16A109.5
C2—C3—H3A120.4S1—C16—H16B109.5
C4—C3—H3A120.4H16A—C16—H16B109.5
C5—C4—C3118.9 (6)S1—C16—H16C109.5
C5—C4—H4A120.5H16A—C16—H16C109.5
C3—C4—H4A120.5H16B—C16—H16C109.5
N1—C5—C4121.6 (6)S1—C17—H17A109.5
N1—C5—C6115.0 (5)S1—C17—H17B109.5
C4—C5—C6123.4 (6)H17A—C17—H17B109.5
N2—C6—C7119.0 (6)S1—C17—H17C109.5
N2—C6—C5112.7 (5)H17A—C17—H17C109.5
C7—C6—C5128.3 (6)H17B—C17—H17C109.5
C6—C7—C8118.6 (6)
ClBrI
Au—Pt3.2684 (1)3.3361 (5)4.2546 (4)
Pt—X2.305 (3)2.4319 (8)2.5930 (5)
Au—X2.271 (3)2.3984 (9)2.5581 (5)
Pt—Pt3.4535 (7)3.4335 (6)3.5278 (3)
ClBr
X2—Au1—Pt188.63 (7)81.70 (2)
91.37 (7)98.30 (2)
X1—Pt1—Au197.62 (7)84.08 (2)
Au1—Pt1—Pt1(1-x, 2-y, -z)165.10 (2)173.94 (1)
Table 1

Selected geometric parameters (Å, °) in [Pt(tpy)X][AuX 2], X = Cl, Br, I

 ClBrI  
Au—Pt3.2684 (1)3.3361 (5)4.2546 (4)  
Pt—X2.305 (3)2.4319 (8)2.5930 (5)  
Au—X2.271 (3)2.3984 (9)2.5581 (5)  
Pt—Pt3.4535 (7)3.4335 (6)3.5278 (3)  
      
 ClBr   
X2—Au1—Pt188.63 (7)81.70 (2)   
 91.37 (7)98.30 (2)   
X1—Pt1—Au197.62 (7)84.08 (2)   
Au1—Pt1—Pt1(1 − x, 2 − y, −z)165.10 (2)173.94 (1)   
  5 in total

1.  Strong Closed-Shell Interactions in Inorganic Chemistry.

Authors:  Pekka Pyykkö
Journal:  Chem Rev       Date:  1997-05-08       Impact factor: 60.622

2.  The Cambridge Structural Database: a quarter of a million crystal structures and rising.

Authors:  Frank H Allen
Journal:  Acta Crystallogr B       Date:  2002-05-29

3.  A short history of SHELX.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr A       Date:  2007-12-21       Impact factor: 2.290

4.  Gold(III) and platinum(II) polypyridyl double salts and a general metathesis route to metallophilic interactions.

Authors:  Rebecca Hayoun; Diane K Zhong; Arnold L Rheingold; Linda H Doerrer
Journal:  Inorg Chem       Date:  2006-08-07       Impact factor: 5.165

5.  Metallophilic interactions in iodido(2,2':6',2''-terpyridine)platinum(II) diiodidoaurate(I).

Authors:  Christina S Angle; Kathryn J Woolard; Michael I Kahn; James A Golen; Arnold L Rheingold; Linda H Doerrer
Journal:  Acta Crystallogr C       Date:  2007-05-11       Impact factor: 1.172

  5 in total

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