Structural investigation of homonuclear Pt2 and heteronuclear PdPt complexes containing a metal-metal bond bridged by hydrido and sulfido ligands

270 Acta Cryst. (1996). B52, 270-276 Structural Investigation of Homonuclear Pt2 and Heteronuclear PdPt Complexes Containing a Metal-Metal Bond Bridged by Hydrido and Suifido Ligands WILLIAM CLEGG, a* MERCI~ CAPDEVILA, b PILAR GONZ,~,LEZ-DUARTE b AND JOAN SOLA b aDepartment of Chemistry, University of Newcastle, Newcastle upon Tyne NE1 7RU, England, and bDepartamento de Qu[mica, Universitat Autrnoma de Barcelona, 08193 Bellaterra, Barcelona, Spain. E-maih [email protected] (Received 2 December 1994; accepted 28 July 1995) Abstract The complex [Pt2(/.t-H)(#-S)(dppe)2](PF6) undergoes a displacive order-disorder transformation at ca 230 K. The low-temperature structure is ordered with one cation-anion pair as the asymmetric unit in space group P2Jn. At room temperature the b axis is halved and the space group is P2/n, imposing crystallographic twofold rotation symmetry on both ions; the anion shows major disorder and there is probably minor disorder in the cation, but its internal geometry remains essentially unchanged. The heteronuclear complex [PdPt(ft-H)(/.t-S)(dppe)2](PF6) is isostructural with the Pt2 complex at room temperature. All three structures have been determined crystallographically and both complexes have been extensively characterized by NMR spectroscopy, unambiguously confirming the genuine heteronuclear nature of the mixed-metal complex and the presence of the bridging hydride ligand. 1. Introduction As part of a wide-ranging programme of research in the coordination chemistry of aminoalkanethiolates (aliphatic mercaptoamines), we have prepared and structurally characterized palladium(II) and platinum(II) complexes of various aminoalkanethiolato ligands (Capdevila, Clegg, Gonz~ilez-Duarte & Mira, 1992; Capdevila, Clegg, Gonz~ilez-Duarte, Harris, Mira, Sola & Taylor, 1992; Capdevila, Gonz~ilez-Duarte, Foces-Foces, Hemandez Cano & Martfnez-Ripoll, 1990; Capdevila, Clegg, Gonz~ilez-Duarte, Jarid & Lled6s, 1996). Reaction of the two mononuclear platinum complexes [Pt(SCsH9NMe)2(dppe)] and [PtC12(dppe)] in organic solvents gives the dinuclear cationic species [Pt2(#- SCsH9NMe)2(dppe)2] 2+, obtained as its PF6- or BPh4- salt, the latter being fully characterized by single-crystal diffraction [dppe = bis(diphenylphosphino)ethane, Ph2PCH2CH2PPh2 (Capdevila, Clegg, Gonz~ilez-Duarte, Harris, Mira, Sola & Taylor, 1992)]. More detailed examination of this reaction showed that, on some occasions, even though the experimental procedures and conditions were apparently the same, a completely different result was obtained, and the only platinum-containing product identified was [Pt2(#- H)(#-S)(dppe)2] +, isolated in ca 20% yield as its PF6- © 1996 International Union of Crystallography Printed in Great Britain - all rights reserved salt (1). The nature of this product was established by a combination of X-ray crystallography and NMR spectroscopy (Capdevila, Gonz~ilez-Duarte, Mira, Sola & Clegg, 1992). From the room-temperature diffraction data the bridging hydride ligand could not be located and the structure included a disordered PF6- anion on a twofold rotation axis. Ph Ph Ph Phx.x I S \ / p,/\M/P\ /x /\ Ph Ph Ph Ph pF 6 - (I)M = Pt (2) M = Pd We subsequently prepared a fresh sample of (1) and undertook a low-temperature diffraction study with the aim of modelling the disorder better and possibly locating the hydride. We discovered that the complex undergoes a reversible phase transition on cooling below 230K, to give an ordered structure in a unit cell of doubled volume, and were able to locate and refine the hydride position. We report here a comparison of the room-temperature and low-temperature structures, together with an account of the analogous mixed-metal PdPt complex (2), obtained in a similar way and characterized both crystallographically and spectroscopically. 2. Experimental The synthesis of complex (1) has already been described (Capdevila, Gonz~ilez-Duarte, Mira, Sola & Clegg, 1992). The mixed-metal complex (2) was prepared in an analogous reaction with [PdC12(dppe)] instead of [PtC12(dppe)] as one of the metal-containing starting materials. Crystals suitable for diffraction study were obtained from solution in acetonitrile. Satisfactory analyses (for C, S and H) were obtained for both complexes. Experimental details are summarized in Table 1. Acta Crystallographica Section B ISSN 0108-7681 © 1996 WILLIAM CLEGG et al. 271 Crystal data Chemical formula Chemical formula weight Crystal system Space group a (A) b (A) c (h) ~(o) v (A 3) Z Dx (Mg m -3) Radiation type Wavelength (,~,) No. of reflections for cell parameters 0 range (o) /z (mm q) Temperature (K) Crystal form Crystal size (mm) Crystal colour Data collection Diffractometer Data collection method Absorption correction Tmin Tm~x No. of measured reflections No. of independent reflections No. of observed reflections Criterion for observed reflections Rint 0max (o) Range of h, k, 1 No. of standard reflections Frequency of standard reflections (min) Intensity decay (%) Refinement Refinement on R[F 2 > 2o.(F) 2] wR(all data, F 2) S(all data) No. of reflections used in refinement No. of parameters refined H-atom treatment Weighting scheme (A/o')rnax Apmax (e A -3) Apmin (e /~-3) Source of atomic scattering factors Computer programs Data collection Cell refinement Data reduction Structure solution Structure refinement Preparation of material for publication Table 1. Experimental details (1) at room temperature [Pt2 (C26 H24 P2)2 (H)(S)](PF6) 1365.00 Monoclinic P2/n 13.742 (2) 11.0580 (7) 16.7504 (14) 96.644 (11 ) 2528.3 (4) 2 1.793 Mo Kc~ 0.71073 32 10.16-11.82 5.784 295 (2) Block 0.20 x 0.18 × 0.12 Yellow Stoe-Siemens diffractometer w/O scans with on-line profile fitting (Clegg, 1981) ~p scans (SHELXTL) 0.283 0.314 5397 4447 3239 1 > 2,7(/) 0.0531 25.01 --16--~ h ~ 16 --11 ~ k ~ 13 --18 ~ 1 ~ 19 3 60 (1) at low temperature [Pt2 (C26H24P2)2 (H)(S)] (PF6) 1365.00 Monoclinic P21/n 13.689 (4) 21.857 (7) 16.662 (5) 95.92 (3) 4958.7 (26) 4 1.828 Mo Ko~ 0.71073 32 10.20-12.25 5.898 160.0 (10) Block 0.25 x 0.25 x 0.25 Yellow Stoe-Siemens diffractometer ~/8 scans with on-line profile fitting (Clegg, 1981) ~b scans (SHELXTL) 0.144 0.225 10 478 8708 5497 I > 2o'(/) 0.0307 25.00 --16 ~ h ~ 16 -3 ----~ k --~ 25 -19--~l~ 19 4 60 None F 2 0.0295 0.0683 1.063 4437 312 See text w = 1/[a2(Fo 2) + (0.0295P) 2 + 2.8898P], where P = (Fo 2 + 2Fc2)/3 0.001 0.580 --0.475 International Tables for Crystallography (1992, Vol. C, Tables 4.2.6.8 and 6.1.1.4) I F 2 0.0385 0.0850 1.054 8679 599 See text w = 1][o.2(Fo 2) + (0.0254P) 2 + 58.7745P], where P = (Fo 2 + 2Fc2)/3 2.821 2.097 e A -3 ,,~ 1.1 A from Pt -1.204 e/~-3 ~,1.1 /~ from Pt International Tables for Crystallography (1992, Vol. C, Tables 4.2.6.8 and 6.1.1.4) DIF4 (Stoe & Cie, 1988) DIF4 Local programs SHELXTL/PC (Sheldrick, 1990) SHELXL93 (Sheldrick, 1994) SHELXL93 and local programs DIF4 (Stoe & Cie, 1988) DIF4 Local programs SHELXTL/PC (Sheldrick, 1990) SHELXL93 (Sheldrick, 1994) SHELXL93 and local programs (2) [PdPt(C26 H24P2)2 (H)(S)](PF6) 1276.31 Monoclinic P2/n 13.724 (4) 11.097 (2) 16.740 (4) 96.77 (3) 2531.6 (11) 2 1.674 Mo Kc~ 0.71073 32 10.19-11.80 3.372 295 (2) Block 0.24 X 0.20 X 0.16 Yellow Stoe-Siemens diffractometer w/O scans with on-line profile fitting (Clegg, 1981) ~b scans (SHELXTL) 0.191 0.250 5166 3295 2199 1 > 2o.(/) 0.0429 22.50 --14 ---* h ---* 14 -11 ~ k ---* 11 --18 ---* l ---* 18 3 60 None F 2 0.0366 0.0810 1.082 3288 315 See text w = 1/[o-2(Fo 2) + (0.0409P) 2 + 2.1952P], where P = (Fo 2 + 2Fc2)/3 <0.001 0.600 --0.431 International Tables for Crystallography (1992, Vol. C, Tables 4.2.6.8 and 6.1.1.4) DIF4 (Stoe & Cie, 1988) DIF4 Local programs SHELXTL/PC (Sheldrick, 1990) SHELXL93 (Sheldrick, 1994) SHELXL93 and local programs 2.1. Room-temperature structure of (1) The bridging hydride could not be located in difference syntheses. Its presence was deduced at this stage from the charge balance of the complex and confirmed by NMR spectroscopy (see §3). The PF6- anion was found to be disordered over a twofold rotation axis, with a well defined central position for P and a total 272 HOMONUCLEAR Pt2 AND HETERONUCLEAR PdPt COMPLEXES of eight peaks (including symmetry equivalents) in a diffuse region of significant electron density at a suitable distance from the central atom. The disorder could not be resolved into alternative orientations of an idealized octahedral PF6- group. Instead, partial F atoms were refined with anisotropic displacement parameters and with initial positions taken from the difference density map, the total occupancy of all F-atom sites being restrained to 6. The refinement leading to the results presented here was made subsequent to the preliminary communication of this structure (Capdevila, Gonz~ilez-Duarte, Mira, Sola & Clegg, 1992) and with different software. The structure is a little more precisely described, but there are no significant changes. H atoms other than the bridging hydride were refined with a riding model for coordinates and with U(H) = 1.2Ueq(C); this applies to all three structures. 2.2. Low-temperature structure of (1) Preliminary cell determination at 160K revealed a b axis doubled relative to the room-temperature cell and systematic absences for 0k0 with odd k indicated a change of space group from P2/n to P21/n. The doubled cell volume and loss of the twofold rotation axis imply general rather than special positions for the cations and anions (assuming a simple structural relationship between the room-temperature and lowtemperature phases, thus rendering unlikely the migration of anions to centres of symmetry), lifting the crystallographic symmetry imposed on both ions at room temperature. Small but significant positional and orientational changes were detected in the ions as a result of the two structure determinations and the anion was found to be ordered, with six clear fluorine positions; refinement required no restraints or constraints. The bridging hydride was also located in a difference synthesis and its position freely refined; the isotropic displacement parameter was fixed at 0.05/~2 after attempted refinement gave an anomolously low value with an extremely high e.s.d. The largest .4/0- ratio is for the z coordinate of the bridging H atom, which showed oscillation in alternate cycles. Following intensity data collection, the phase transition was investigated by monitoring a reflection which has moderate intensity for the low-temperature phase but is absent (with non-integral k index) for the roomtemperature phase, while varying the temperature with the Cryostream device employed in these experiments (Cosier & Glazer, 1986). On warming from 160 K, the reflection peak intensity declined slowly and steadily, then dropped rapidly around 230 K to give no signal significantly above background at higher temperatures. The effect was reversible, the reflection reappearing on cooling through 230 K, to be restored to its initial intensity at 160 K. Several cycles of warming and cooling through the phase transition gave no apparent deterioration of the quality of the crystal and its diffraction properties. 2.3. Room-temperature structure of (2) Refinement was as for the room-temperature structure of (1) except for the bridging hydride and the metal atoms. The hydride was located in a difference synthesis and was refined freely with its own isotropic displacement parameter. The crystallographically unique single metal atom was treated as a composite of Pd and Pt, and the relative occupancy factors of these atoms were refined as a check on the chemical composition; the final Pt:Pd values obtained are 0.513:0.487 (7). NMR spectra were measured with a Bruker AM- 400 spectrometer, for samples in d6-DMSO solution. External standards were 85% phosphoric acid and 1 M H2PtC16/D20. 3. Discussion Fractional atomic coordinates and equivalent isotropic displacement parameters for the three structures are reported in Tables 2, 4 and 6; Tables 3, 5 and 7 give selected geometric parameters.* 3.1. Room-temperature structure of (1) A preliminary account of this has already been given (Capdevila, Gonztilez-Duarte, Mira, Sola & Clegg, 1992). Further refinement on F 2 rather than F marginally improves the precision of the structure, but gives no significant difference. It was not possible to locate the bridging hydride ligand crystallographically, but the evidence from ill, 31p and 195pt NMR spectroscopy was clear and unambiguous, and the position indicated spectroscopically for this hydride is consistent with the crystallographic results and with results previously obtained both spectroscopically and crystallographically for [Pt2(#-H)(#-CO)(dppe)2](BF4) (Minghetti, Bandini, Banditelli, Bonati, Szostak, Strouse, Knobler & Kaesz, 1983). The identity of the other bridging ligand as S 2- is supported by successful structure refinement (in terms of electron density a bridging chloride would be equally acceptable, but this can be ruled out on the grounds of overall charge balance) and satisfactory elemental analysis, which included quantitative determination of sulfur and chlorine, the latter being recorded as negligible. This ligand is presumably derived from S--C bond cleavage of the original mercaptoamine ligands in the synthesis of the starting materials, but the source of the bridging hydride is obscure. The apparent geometry of the disordered PF6- anion is essentially meaningless; the anisotropic displacement parameters of the partial F atoms are large, indicating * Lists of atomic coordinates, anisotropic displacement parameters and structure factors have been deposited with the IUCr (Reference: FG0001). Copies may be obtained through The Managing Editor, International Union of Crystallography, 5 Abbey Square, Chester CH1 2HU, England. WILLIAM CLEGG et al. 273 Table 2. Fractional atomic coordinates and equivalent isotropic displacement parameters (~[2)for (1) at room temperature x y z Ueq Pt 0.22373 (2) 0.38855 (2) 0.32750 (2) 0.04434 (10) S 1/4 0.2233 (2) 1/4 0.0669 (8) P1 0.20559 (12) 0.5617 (2) 0.39580 (11) 0.0450 (4) P2 0.17441 (12) 0.2916 (2) 0.43374 (11) 0.0463 (4) CI 0.3210 (5) 0.6148 (6) 0.4480 (4) 0.050 (2) C2 0.4025 (6) 0.6201 (8) 0.4055 (6) 0.076 (2) C3 0.4925 (6) 0.6541 (I0) 0.4434 (8) 0.097 (3) C4 0.5034 (7) 0.6777 (9) 0.5242 (7) 0.090 (3) C5 0.4253 (7) 0.6701 (8) 0.5676 (6) 0.082 (3) C6 0.3326 (6) 0.6416 (7) 0.5279 (5) 0.065 (2) C7 0.1445 (5) 0.6916 (6) 0.3454 (4) 0.051 (2) C8 0.1884 (7) 0.8032 (8) 0.3438 (6) 0.096 (3) C9 0.1368 (9) 0.8994 (8) 0.3060 (8) 0.125 (5) C10 0.0436 (8) 0.8837 (9) 0.2716 (7) 0.109 (4) Cll 0.0007 (7) 0.7737 (9) 0.2713 (6) 0.096 (3) C12 0.0503 (6) 0.6779 (9) 0.3094 (5) 0.081 (3) C13 0.1267 (5) 0.5240 (6) 0.4738 (4) 0.056 (2) C14 0.1621 (5) 0.4038 (6) 0.5114 (4) 0.052 (2) C15 0.0522 (5) 0.2275 (6) 0.4105 (4) 0.053 (2) C16 0.0015 (6) 0.2441 (8) 0.3359 (6) 0.076 (2) C17 -0.0940 (7) 0.2035 (10) 0.3189 (7) 0.107 (4) C18 -0.1384 (6) 0.1477 (10) 0.3769 (9) 0.106 (4) C!9 -0.0893 (8) 0.1280 (8) 0.4511 (7) 0.094 (3) C20 0.0070 (6) 0.1706 (8) 0.4693 (6) 0.076 (2) C21 0.2518 (5) 0.1741 (6) 0.4855 (4) 0.050 (2) C22 0.2620 (6) 0.1671 (8) 0.5683 (5) 0.068 (2) C23 0.3238 (7) 0.0787 (9) 0.6076 (6) 0.080 (3) C24 0.3718 (7) 0.0002 (9) 0.5643 (7) 0.085 (3) C25 0.3607 (6) 0.0042 (8) 0.4815 (7) 0.080 (2) C26 0.3017 (6) 0.0917 (6) 0.4427 (5) 0.062 (2) P3 !/4 0.4701 (4) 3/4 0.0900 (11) Fi 0.3435 (5) 0.4747 (9) 0.8131 (4) 0.141 (4) F2 0.3204 (6) 0.4487 (14) 0.6840 (4) 0.161 (7) F3 0.259 (2) 0.3392 (15) 0.7800 (9) 0.196 (12) F4 0.2730 (13) 0.5935 (13) 0.7115 (9) 0.180 (9) Table 3. Selected geometric parameters (/[, °)for (1) at room temperature Pt--Pt i 2.7742 (5) Pt--P1 2.259 (2) Pt--S 2.294 (2) Pt--P2 2.248 (2) Pt--S--Pt i 74.41 (8) S--Pt--Pt i 52.79 (4) P1--Pt--P2 86.69 (6) P1--Pt--Pt ~ 122.00 (4) P1--Pt--S 174.56 (6) p2--Pt--Pt i 151.13 (4) P2--Pt--S 98.61 (6) Symmetry code: (i) 1 _ x, y, ½ - z. that the disorder is more complex and extensive than the simple model with a relatively small number of partial atoms. The disorder is largely orientational rather than displacive, since the central P atom appears to be well ordered. Relatively high displacement parameters for some of the C atoms may indicate minor unresolved disorder in the cation (Fig. 1). 3.2. Low-temperature structure of (1) On cooling, the b-axis length doubles and the space group changes from P2/n to P21/n. The structural implications of this phase change are: (a) cations (and also anions) which are related by one unit-cell translation along b at room temperature are now related by a Table 4. Fractional atomic coordinates and equivalent isotropic displacement parameters (/[2)for (1) at low temperature x y z Ueq Ptl 0.22971 (3) 0.19255 (2) 0.34739 (2) 0.0248 (2) Pt2 0.28116 (3) 0.19439 (2) 0.19058 (2) 0.0249 (2) S 0.2600 (2) 0.11008 (11) 0.2684 (2) 0.039 (2) P1 0.1814 (2) 0.14328 (11) 0.4549 (2) 0.0252 (13) P2 0.2079 (2) 0.27962 (11) 0.4158 (2) 0.0249 (13) P3 0.2959 (2) 0.28283 (11) 0.1223 (2) 0.0243 (12) P4 0.3296 (2) 0.14664 (11) 0.0821 (2) 0.0254 (14) C1 0.0566 (7) 0.1132 (4) 0.4335 (7) 0.032 (5) C2 0.0058 (9) 0.1216 (6) 0.3599 (9) 0.052 (7) C3 -0.0906 (10) 0.1034 (7) 0.3463 (11) 0.070 (7) C4 -0.1356 (10) 0.0760 (7) 0.4057 (14) 0.081 (7) C5 -0.0848 (10) 0.0659 (6) 0.4794 (12) 0.066 (8) C6 0.0122 (8) 0.0841 (5) 0.4951 (8) 0.042 (7) C7 0.2578 (7) 0.0823 (4) 0.5050 (6) 0.027 (5) C8 0.2705 (8) 0.0798 (5) 0.5885 (7) 0.037 (7) C9 0.3318 (9) 0.0352 (5) 0.6256 (8) 0.045 (7) C10 0.3805 (8) -0.0059 (5) 0.5795 (7) 0.040 (6) Cll 0.3662 (8) -0.0031 (5) 0.4977 (7) 0.038 (5) C12 0.3050 (7) 0.0407 (5) 0.4582 (7) 0.033 (5) C13 0.1710 (7) 0.1992 (5) 0.5333 (6) 0.032 (5) C14 0.1326 (7) 0.2591 (5) 0.4965 (6) 0.029 (5) C15 0.3235 (7) 0.3089 (5) 0.4659 (7) 0.030 (5) C16 0.3353 (8) 0.3236 (5) 0.5462 (7) 0.039 (5) C17 0.4269 (10) 0.3370 (6) 0.5847 (9) 0.055 (8) C!8 0.5075 (9) 0.3388 (6) 0.5415 (11) 0.059 (7) C 19 0.4954 (9) 0.3267 (6) 0.4599 (11) 0.057 (7) C20 0.4056 (8) 0.3106 (6) 0.4222 (8) 0.047 (6) C21 0.1441 (7) 0.3443 (4) 0.3651 (6) 0.028 (6) C22 0.0464 (8) 0.3347 (5) 0.3328 (7) 0.036 (6) C23 -0.0078 (9) 0.3843 (6) 0.2958 (8) 0.049 (7) C24 0.0368 (10) 0.4398 (5) 0.2899 (8) 0.051 (8) C25 0.1339 (11) 0.4476 (5) 0.3196 (9) 0.061 (10) C26 0.1889 (9) 0.4007 (5) 0.3576 (7) 0.042 (7) C27 0.3539 (7) 0.3483 (5) 0.1725 (6) 0.028 (5) C28 0.3106 (9) 0.4065 (5) 0.1729 (7) 0.041 (7) C29 0.3631 (10) 0.4547 (6) 0.2080 (8) 0.055 (9) C30 0.4564 (11) 0.4479 (6) 0.2451 (8) 0.057 (10) C31 0.5010 (9) 0.3907 (6) 0.2462 (8) 0.054 (7) C32 0.4505 (8) 0.3419 (5) 0.2114 (7) 0.041 (6) C33 0.1795 (7) 0.3082 (5) 0.0716 (6) 0.030 (5) C34 0.1637 (8) 0.3189 (5) -0.0104 (7) 0.034 (6) C35 0.0705 (9) 0.3334 (5) -0.0462 (8) 0.044 (7) C36 -0.0059 (9) 0.3372 (6) -0.0012 (10) 0.053 (6) C37 0.0079 (9) 0.3279 (6) 0.0809 (9) 0.050 (7) C38 0.0987 (7) 0.3122 (6) 0.1175 (7) 0.041 (5) C39 0.3756 (7) 0.2653 (4) 0.0438 (6) 0.026 (5) C40 0.3438 (7) 0.2043 (4) 0.0064 (6) 0.029 (4) C41 0.4519 (7) 0.1137 (4) 0.1027 (6) 0.028 (6) C42 0.5038 (8) 0.1208 (5) 0.1774 (7) 0.037 (6) C43 0.5987 (9) 0.1002 (5) 0.1924 (8) 0.045 (7) C44 0.6436 (9) 0.0711 (6) 0.1317 (8) 0.051 (6) C45 0.5924 (9) 0.0623 (5) 0.0581 (8) 0.047 (8) C46 0.4961 (7) 0.0834 (5) 0.0414 (7) 0.032 (6) C47 0.2520 (7) 0.0881 (4) 0.0291 (6) 0.027 (5) C48 0.1965 (7) 0.0490 (5) 0.0724 (7) 0.036 (5) C49 0.1371 (9) 0.0057 (5) 0.0316 (8) 0.046 (7) C50 0.1303 (8) 0.0008 (6) -0.0505 (8) 0.048 (6) C51 0.1829 (9) 0.0415 (5) -0.0943 (7) 0.040 (7) C52 0.2436 (8) 0.0848 (5) -0.0544 (7) 0.037 (6) P5 0.7410 (3) 0.2619 (2) 0.2685 (2) 0.049 (2) FI 0.6734 (7) 0.2845 (6) 0.3351 (6) 0.100 (7) F2 0.6442 (6) 0.2556 (4) 0.2059 (5) 0.066 (5) F3 0.7447 (10) 0.3323 (5) 0.2443 (9) 0.142 (10) F4 0.8372 (6) 0.2673 (5) 0.3300 (4) 0.087 (5) F5 0.7252 (9) 0.1972 (5) 0.3023 (8) 0.142 (11) F6 0.8030 (8) 0.2455 (11) 0.2028 (6) 0.239 (7) 21 screw axis and so are no longer aligned strictly collinear; (b) the crystallographic twofold rotation symmetry is no longer imposed on the cations and anions, so that the asymmetric unit of the low-temperature 274 HOMONUCLEAR Pt2 AND HETERONUCLEAR PdPt COMPLEXES Table 5. Selected geometric parameters (f[, °)for (1) at low temperature Ptl--Pt2 2.776 (2) Pt2--H1 1.88 (11) Ptl--H1 1.96 (11) Pt2---S 2.289 (3) Ptl---S 2.295 (3) Pt2--P3 2.263 (3) Ptl--P1 2.248 (3) Pt2--P4 2.246 (3) Pt l--P2 2.254 (3) Ptl--H1--Pt2 93 (5) S--Ptl--Pt2 52.64 (7) Ptl---S--Pt2 74.54 (8) H1--Pt2--P3 77 (3) H1--PtlIP1 165 (3) H1--Pt2--P4 163 (3) H1--PtlIP2 79 (3) P3--Pt2--P4 86.74 (9) P1--Ptl--P2 86.33 (10) H1--Pt2--S 98 (3) H1--Ptl---S 95 (3) P3IPt2--S 174.76 (9) P1--Ptl---S 99.57 (10) P4---Pt2--S 98.46 (10) P2--Ptl---S 173.99 (9) H1--Pt2--Ptl 45 (3) H1--Ptl--Pt2 43 (3) P3--Pt2--Ptl 122.03 (7) P1--Ptl--Pt2 151.82 (7) P4---Pt2--Ptl 151.11 (7) P2--Ptl--Pt2 121.58 (7) S--Pt2--Ptl 52.82 (7) Table 6. Fractional atomic coordinates and equivalent isotropic displacement parameters (,~2 ) for (2) x y z Ueq Pt 0.22353 (3) 0.38918 (4) 0.32693 (3) 0.0539 (2) Pd 0.22353 (3) 0.38918 (4) 0.32693 (3) 0.0539 (2) S 1/4 0.2239 (3) 1/4 0.0821 (12) P1 0.2053 (2) 0.5619 (2) 0.39586 (14) 0.0570 (7) P2 0.1749 (2) 0.2912 (2) 0.43317 (14) 0.0605 (7) C1 0.3207 (6) 0.6151 (8) 0.4480 (5) 0.063 (2) C2 0.4018 (7) 0.6207 (10) 0.4064 (7) 0.090 (3) C3 0.4921 (8) 0.6547 (12) 0.4429 (9) 0.111 (4) C4 0.5047 (9) 0.6773 (I0) 0.5242 (9) 0.103 (4) C5 0.4261 (10) 0.6708 (I0) 0.5667 (7) 0.099 (3) C6 0.3325 (8) 0.6408 (9) 0.5288 (7) 0.081 (3) C7 0.1444 (7) 0.6902 (8) 0.3463 (5) 0.064 (2) C8 0.1889 (10) 0.8031 (10) 0.3423 (8) 0.118 (4) C9 0.1352 (14) 0.8973 (12) 0.3047 (10) 0.154 (7) C10 0.0425 (12) 0.8833 (13) 0.2723 (9) 0.129 (5) Cll -0.0005 (10) 0.7728 (13) 0.2722 (8) 0.121 (4) C12 0.0515 (8) 0.6796 (10) 0.3099 (7) 0.095 (3) C13 0.1273 (7) 0.5235 (8) 0.4739 (6) 0.071 (3) C14 0.1632 (7) 0.4029 (7) 0.5099 (5) 0.065 (2) C15 0.0506 (7) 0.2280 (8) 0.4094 (6) 0.066 (2) C16 0.0014 (8) 0.2449 (10) 0.3357 (7) 0.094 (3) C17 -0.0932 (10) 0.2046 (12) 0.3164 (9) 0.126 (5) C18 -0.1373 (9) 0.1491 (13) 0.3727 (11) 0.123 (5) C19 -0.0921 (10) 0.1294 (10) 0.4476 (10) 0.107 (4) C20 0.0060 (8) 0.1700 (9) 0.4681 (7) 0.089 (3) C21 0.2512 (6) 0.1739 (8) 0.4856 (6) 0.067 (2) C22 0.2620 (8) 0.1657 (9) 0.5684 (6) 0.079 (3) C23 0.3220 (10) 0.0800 (11) 0.6065 (8) 0.099 (4) C24 0.3708 (9) -0.0010 (12) 0.5654 (9) 0.101 (4) C25 0.3591 (8) 0.0029 (10) 0.4837 (9) 0.100 (4) C26 0.2998 (7) 0.0921 (8) 0.4418 (6) 0.077 (3) P3 1/4 0.4687 (6) 3/4 0.113 (2) F1 0.3428 (7) 0.4757 (11) 0.8123 (4) 0.167 (6) F2 0.3205 (9) 0.4501 (18) 0.6841 (5) 0.190 (9) F3 0.258 (2) 0.3449 (18) 0.7835 (11) 0.219 (16) F4 0.2727 (16) 0.5916 (16) 0.7106 (i 1) 0.184 (11) Table 7. Selected geometric parameters low temperature M M i 2.7574 (11) M--P1 M--H1 1.94 (7) M--P2 M--S 2.295 (3) M--H 1----~ 91 (4) P1--M--S ML-S--M 73.85 (10) P2--M--S H1--M--P2 164 (2) H1 M M 4 H1--M--P1 78 (2) PI M M ~ P1--M--P2 86.87 (8) P2 M M ~ H1--M---S 98(2) S M M ~ Symmetry code: (i) ½ - x, y, ½ - z. (,~, °)for (2) at 2.266 (2) 2.252 (2) 174.97 (7) 97.96 (8) 45 (2) 122.19 (6) 150.81 (6) 53.08 (5) structure is one complete pair of ions instead of half a cation and half an anion. Comparison of the roomtemperature and low-temperature structures shows that the removal of the symmetry constraint is marked by a small displacement of the cations away from their roomtemperature symmetry-imposed position, the centroid of the Pt2SH ring lying about 0.31 A from the line 1/4, y, 1/4 in the low-temperature form; the S...H vector remains almost parallel with this line, at an angle of only 0.8 °. There is a very marked reduction, by about half their values, in the equivalent isotropic displacement parameters of the cation atoms. As well as reduced dynamic freedom (thermal vibration), this may also be due to the removal of minor unresolved static disorder in the room-temperature structure. At low temperature the bridging hydride is clearly located and could be 018 02s C20 ~t'~'~C17 S .__~~ 014% o T-- C13C6( ~ C2 011W ° Cl0~J, C9 Fig. 1. The room-temperature structure of the cation of (1), with 50% probability ellipsoids and atom labelling. H atoms are omitted. Cll C10 C50 C49 C 4 6~.(~23 43 S C3 C 4.--'~~ ~- c C42 .e. C 39 ~",,,,,,,,,,,,,;.~ ,-..~ o H1 ___ 1}~,~,,"'~'<~ C 14 C35 ~ 3~-~(~r ~ C19#~C17 C 29((~C 30 C25 Fig. 2. The low-temperature structure of the cation of (1), with 50% probability ellipsoids and atom labelling. H atoms arc omitted, except for the bridging hydride. WILLIAM CLEGG et al. 275 successfully refined with acceptable geometry, albeit with not very high precision. Apart from the hydride, the internal geometry of the cation remains essentially identical to that at room temperature (Fig. 2). In the low-temperature phase the PF6- anion, not constrained by the crystallographic twofold rotation symmetry, is ordered and its refinement proceeded smoothly to give essentially octahedral geometry. The atomic shifts involved in the interconversion of the two structures are small and the phase transition is readily characterized as a displacive order-disorder transformation. It is fully reversible on heating and a Fig. 3. A section through the crystal structure of (1) at room temperature. Only half the depth of the unit-cell contents are shown. cooling through the transition temperature of ca 230 K. The packing of the ions in the two structures is shown in Figs. 3 and 4. 3.3. Room-temperature structure of (2) The mixed-metal PdPt complex (2) was found to be isomorphous with the pure Pt complex (1) at room temperature, with almost identical cell parameters. Full structure determination shows that the complexes are isostructural. The major difference experimentally is that the bridging hydride can be located and refined for complex (2), with observed results which are entirely consistent with those obtained for the low-temperature structure of (1) (Fig. 5). The two metal sites in the cation are equivalent by crystallographic symmetry. In the refinement the unique metal site was treated as a composite of Pd and Pt, which have very different X-ray scattering factors, allowing a reliable refinement of the relative site occupancy factors to give a Pt:Pd ratio of 0.513:0.487 (7), representing a small and insignificant excess of Pt over Pd. A metal site disorder of equal proportions could have two interpretations, which cannot be distinguished by purely crystallographic methods: (a) genuine heteronuclear PdPt complex ions adopting two possible orientations (Pt- Pd and Pd-Pt) at random or (b) a random mixture of equal mole proportions of homonuclear PtPt and PdPd complexes. Indeed, both types of disorder could be present together, resulting from a mixture of PtPt, PtPd and PdPd complexes in the one structure. The question is resolved by NMR spectroscopy (IH and 31p), which also unambiguously confirms the presence of the bridging hydride ligand. The range between -2.0 and --6.0 p.p.m, of the 1H NMR spectrum (dimethyl sulfoxide solution) shows a triplet with Pt satellites Fig. 4. A section through the crystal structure of (1) at low tcmperature, comparable with Fig. 3. 024 c2s C19 (,~~..~,.~ C 26 '~..~ s c10(~ C9 Fig. 5. The room-temperature structure of the cation of (2), with 50% probability ellipsoids and atom labelling on the assumption of a mixed-metal species, as indicated by NMR spectroscopy. H atoms are omitted, except for the bridging hydride. 276 HOMONUCLEAR Pt2 AND HETERONUCLEAR PdPt COMPLEXES due to coupling of the hydride bridge with the WSpt nucleus [6 = -4.57 p.p.m., 1J(Pt--H) = 647.3 Hz] and with two P atoms [2J(P--H) = 68.3 Hz]. The central resonance is in fact a set of three doublets, which indicates that the hydride is additionally coupled to a third P atom [2J(p--H) = 8.2Hz]. As previously reported for the PtPt analogue (1), the larger 2j(p__ H) has been assigned to the P atoms trans to H and the smaller 2J(P--H) to those cis to H. However, in the heterodinuclear complex all four P atoms are nonequivalent and thus the observed pattern requires that both trans 2J(p--H) have very similar values, while those corresponding to cis 2J(P--H) are quite different, only the higher one of these being observed in the spectrum, the smaller coupling remaining unresolved. In addition, the ~H NMR spectrum reveals that the heterodinuclear complex is somewhat contaminated (ca 20% for the particular solution studied) with the PtPt homodinuclear analogue as shown by a group of signals centred at -3.35p.p.m. corresponding to the central triplet of triplets of the quintet reported for the latter complex (Capdevila, Gonz~ilez-Duarte, Mira, Sola & Clegg, 1992); this result is consistent with the refined site occupancy factors for the two metals in the crystal structure. The four non-equivalent phosphorus nuclei are clearly seen in the proton-decoupled 31p NMR spectrum, which shows two signals at 6 47.38 [P(cis) bonded to Pd] and 64.23 p.p.m. [P(trans) bonded to Pd] and two signals with 195pt satellites (1:4:1) at 6 46.37 [P(cis) bonded to Pt] and 60.87 p.p.m. [P(trans) bonded to Pt] with 1J(Pt-- P) couplings of 2625.4 and 3550Hz, respectively, as well as the signals corresponding to the minor presence of the PtPt analogue (at 6 43.7 and 54.9 p.p.m.). Also, the pattem of this spectrum indicates the genuine heteronuclearity of the PdPt complex, further corroborated by the fact that all the phosphorus chemical shifts differ from those observed in the PtPt analogue. By selective decoupling of the diphosphine protons (i.e. with the hydride still coupled), all signals except that for P(cis)--Pt split, displaying either P--P or P(trans)--H couplings. The 2J[P(cis)--H] coupling is not observed because it is much smaller. Accordingly, P(cis)--Pd appears as a doublet [2j(p__p) = 32.9 Hz], P(trans)-- Pt as a doublet with Pt satellites [2J(P--H) = 67.8 Hz] and P(trans)--Pd as a doublet of doublets [2J(P--H) = 65.7 Hz, 2j(p__p) = 33.8 Hz]. These assignments require that the 2j(p__p) coupling constant is greater when P atoms are bonded to Pd than when they are bonded to Pt, which agrees with the fact that no measurable 2j(p__ P) was observed in the homonuclear PtPt analogue. All coupling constants of the two spectra reported here are consistent among themselves and also with those corresponding to the PtPt complex. The genuine heteronuclear nature of complex (2) contrasts with the results obtained for the mixed-metal PdPt product from the normal course of the synthesis, which contains two metal ions, each chelated by a dppe ligand, bridged by two mercaptoamine ligands (Capdevila, Clegg, Gonz~ilez-Duarte, Harris, Mira, Sola & Taylor, 1992). In that case, the evidence from crystallography, spectroscopy and chemical analysis indicated that the mixed-metal product was essentially a solid solution of the diplatinum and dipalladium complexes, with only a minor amount of the heteronuclear complex. In all previously reported structures containing both palladium and platinum in chemically equivalent positions, the metals are disordered and crystallographic study cannot distinguish between genuine heteronuclear complexes and mixtures of homonuclear products (Clark, Ferguson, Jain & Parvez, 1985, 1986; Clark, Ferguson, Kapoor & Parvez, 1985; Suzuki, Iitaka, Kurachi, Kita, Kashiwavara, Ohba & Fujita, 1992). In some of these cases, the presence of a genuine heteronuclear complex was confirmed by NMR and mass spectrometry. This work was supported by the UK Science and Engineering Research Council, the Comisi6n Interministerial de Ciencia y Tecnologia, the Ministerio de Educaci6n y Ciencia and the British Council. 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