Pt Complexes of Z Configuration Iminoether Ligands
crystalline solid was collected by filtration of the mother liquor,
washed with hexane, and dried in a stream of dry air. Yield: 80%.
Anal. Calcd for C24H28NOCl2PPt: C, 44.8; H, 4.4; N, 2.2. Found:
C, 45.1; H, 4.4; N, 2.0. 1H NMR in CDCl3 (δ): 0.80 (s, 9H, CBut),
4.85 (s, 3H, OMe), 6.09 (s, br, 1H, NH), 7.44 (m, 9H, meta +
para PPh), 7.76 (m, 6H, ortho PPh).
cis-[PtCl2(PPh3)2]. trans-[PtCl2{Z-HNdC(OMe)But}2] (0.06 g,
0.12 mmol) and an excess of PPh3 (0.15 g, 0.6 mmol) were
dissolved in CHCl3 (20 mL), and the solution was kept under stirring
for 20 h at room temperature. After evaporation of the solvent under
reduced pressure, the white residue was transferred on a filter,
washed carefully with diethyl ether (which removes excess PPh3),
and dried in a stream of dry air. Yield: 80%. Anal. Calcd for C36H30-
Cl2P2Pt: C, 54.7; H, 3.8. Found: C, 54.7; H, 3.9. 1H NMR in CD2-
Cl2 (δ): 7.48 (m, 2H, ortho PPh), 7.21 (m, 2H, meta PPh) 7.37
(m, 1H, para PPh). The cis configuration of the compound was
deduced on the basis of spectral features already reported for this
compound22,23
least-squares cycles. The hydrogen atoms for the methyl groups
were located in computed positions and allowed to ride on the
carbon atoms to which they are linked. All the hydrogen atoms
were refined isotropically, and their thermal parameters were
restrained to 1.2 times those (U(eq)) of the atoms to which they
are bound. The agreement factors converged to R1 ) 0.0160 and
wR2 ) 0.0400 over the independent observed reflections with
I > 2σ(I).
All the calculations were carried out using XSCANS,24 XEMP,25
SHELXS 97,26 SHELXL 97,27 PARST 97,28 PLATON 98,29
XPMA-ZORTEP,30 and ORTEP 331 computer programs imple-
mented on Pentium machines.
trans-[PtIVCl4{Z-HNdC(OMe)But}2], 2. (a) Data Collection.
A yellow prism of 2 (dimensions 0.10 × 0.15 × 0.20 mm) was
used for the X-ray analysis through the techniques and the devices
already reported above for 1. The cell constants (see Table 1) were
determined from the values of 42 carefully centered randomly
selected reflections in the range 11° e 2θ e 44°. The data were
collected at 293 ( 2 K and then corrected for Lorentz-polarization
and absorption effects (ψ-scan technique). The independent ob-
served reflections (I > 2σ(I)) were 1445 out of a total of 2334
collected reflections (R(int) ) 0.0345). The space group (P21/c,
No. 14) is in agreement with the systematic extinctions and with
the structure solution and refinement (see below). Three standard
reflections were monitored periodically (97 reflections) during the
data collection; no appreciable decay was observed.
(b) Structure Solution and Refinement. The structure was
solved through the Patterson and Fourier techniques. The Pt atom
is located on an inversion center. Two chloride ligands and a
Z-HNdC(OMe)But ligand, which complete the asymmetric unit,
are in general positions. As a consequence the structure of the
complex molecule is pseudooctahedral. All the non-hydrogen atoms
were treated as anisotropic during the subsequent 12 cycles of least-
squares refinement. All the hydrogen atoms for the Z-HNdC(OMe)-
But group were located in computed positions, allowed to ride on
the atoms to which they are linked, and refined isotropically. The
agreement factors converged to R1 ) 0.0274 and wR2 ) 0.0714
over the independent observed reflections with I > 2σ(I).
All the calculations were carried out using the packages and
machines described above for 1.
Physical Measurements. IR spectra in the range 4000-400
cm-1 were recorded as KBr pellets; spectra in the range 400-200
cm-1 were recorded as polythene pellets on a Perkin-Elmer FT 1600
1
spectrophotometer. H NMR spectra were obtained with a Bruker
Avance DPX 300WB spectrometer.
X-ray Structure Determinations. trans-[PtIICl2{Z-HNdC-
(OMe)But}2], 1. (a) Data Collection. A pale yellow prism of 1
(dimensions 0.10 × 0.15 × 0.20 mm) was selected at the polarizing
microscope and mounted on a glass fiber. The diffraction data were
collected through a four-circle automatic Siemens P4 diffractometer,
by using graphite-monochromatized Mo KR radiation (λ, 0.710 73
Å). The cell constants (see Table 1) were determined via full-matrix
least-squares refinement of the values of 26 carefully centered
randomly selected reflections in the range 11° e 2θ e 42°. The
data were collected at 293 ( 2 K and then corrected for Lorentz-
polarization and absorption effects (ψ-scan technique). The inde-
pendent observed reflections (I > 2σ(I)) were 1369 out of a total
of 1636 collected reflections ([R(int) ) 0.0130]). The space group
(C2/m, No. 12) is in agreement with the systematic extinctions and
with the structure solution and refinement (see below). Three
standard reflections were monitored periodically (97 reflections)
during the data collection; no appreciable decay was observed.
Acknowledgment. This work was supported by the
Ministero della Universita` e della Ricerca Scientifica e
Tecnologica (Italy), the Italian National Research Council
(Italy), the Ministerio de Education y Cultura (Spain), and
the European Community (COST D8 97/007 and COST D20
01/001). The authors gratefully acknowledge Mr. F. Berrettini
(b) Structure Solution and Refinement. The structure was
solved through the Patterson and Fourier techniques. The Pt atom
is located on a mirror plane and on a 2-fold crystallographic axis,
whereas the chlorine atom is located on the mirror plane. All the
other atoms are located in general position. As a consequence, the
structure is disordered as regard to the iminoether ligands. The
occupancy of atoms N(1), C(1), C(2), O(1), and C(6) was fixed to
0.5. Two sets of three peaks each was generated by the Fourier-
difference synthesis around C(2). This was interpreted as a further
statistical disorder of the tert-butyl group. The two sets of peaks
were assigned as carbon atoms (namely, C(3), C(4), and C(5) and
C(3A), C(4A), and C(5A)) at the occupancy of 0.25 each. All the
non-hydrogen atoms were treated as anisotropic during the subse-
quent 12 cycles of least-squares refinement. The Fourier-difference
synthesis performed at this stage showed a low intensity new peak,
close to the N(1) atom. This peak was assigned to a hydrogen atom
linked to N(1), and its position was refined freely in the subsequent
(24) XSCANS Users Manual; Siemens Analytical X-ray Instruments Inc.:
Madison, WI, 1994.
(25) Xemp Empirical Absorption Correction Program; Siemens Analytical
X-ray Instruments Inc.: Madison, WI, 1994
(26) Sheldrick, G. M. SHELXS 97, Program for the Solution of Crystal
Structures; University of Go¨ttingen: Go¨ttingen, Germany, 1997.
(27) Sheldrick, G. M. SHELXL 97, Program for the Refinement of Crystal
Structures; University of Go¨ttingen: Go¨ttingen, Germany, 1997.
(28) Nardelli, M. PARST 97, A System of Computer Routines for Calculating
Molecular Parameters from Results of Crystal Structure Analyses;
University of Parma: Parma, Italy, 1997.
(29) Spek, A. L. PLATON 98; Utrecht University: Utrecht, The Nether-
lands, 1998. Windows Implementation by L. J. Farrugia, University
of Glasgow, 1998.
(30) Zsolnai, L. XPMA-ZORTEP 98; University of Heidelberg: Heidelberg,
Germany, 1998.
(31) Johnson, C. K.; Burnett, M. N. ORTEP-3 for Windows; Oak Ridge
National Laboratory: Oak Ridge, TN, 1998. 32-bit Implementation
by L. J.Farrugia, University of Glasgow.
(22) Gillard, R. D.; Pilbrow, M. F. J. Chem. Soc., Dalton Trans. 1974,
2320.
(23) Bracher, G.; Grove, D. M.; Venanzi, L. M.; Bachechi, F.; Mura, P.;
Zambonelli, L. HelV. Chim. Acta 1980, 63, 2519.
Inorganic Chemistry, Vol. 41, No. 3, 2002 477