Comprehensive relativistic ab initio and density functional theory studies on PtH, PtF, PtCl, and Pt(NH3)2Cl2

Platinum monohydride is taken as an example to compare the performance of various relativistic and correlation approaches, such as all‐electron DPT (direct perturbation theory), ECP (effective core potential); RSPT2, RSPT3 (second‐ and third‐order multireference Rayleigh–Schrödinger perturbation theory), CCSD(T) (coupled‐cluster with singles, doubles, and perturbative triples), as well as the four‐component relativistic density functional theory. It is shown that first‐order DPT performs significantly better than the (first‐order) Breit–Pauli Hamiltonian. The performance of different approaches for the excitation energies of the platinum diatomics is discussed critically. The molecular spectroscopic constants for PtF and PtCl are predicted for the first time. The geometric data for several isomers of cis‐ and trans‐Pt(NH3)2Cl2 are reported. The corresponding energetic data are calculated at relativistic all‐electron and ECP‐CCSD(T) as well as four‐component relativistic density functional levels of theory. Contrary to previous results, it is found that the two C2v isomers of cis‐Pt(NH3)2Cl2 are marginally separated in energy, which could be ascribed to Cl—H interactions. © 2002 Wiley Periodicals, Inc. J Comput Chem 23: 564–575, 2002; DOI 10.1002/jcc.10030

[1]  W. Kutzelnigg,et al.  Relativistic Hartree–Fock by means of stationary direct perturbation theory. I. General theory , 1995 .

[2]  R. Franke Numerical study of the iterative solution of the one-electron Dirac equation based on ‘direct perturbation theory’ , 1997 .

[3]  Pekka Pyykkö,et al.  Relativistic effects in structural chemistry , 1988 .

[4]  Paolo Carloni,et al.  Key Steps of the cis-Platin-DNA Interaction: Density Functional Theory-Based Molecular Dynamics Simulations , 2000 .

[5]  Wenjian Liu,et al.  Fully relativistic density functional calculations of the ground and excited states of Yb, YbH, YbF, and YbO , 1998 .

[6]  K. Pitzer,et al.  The ground and excited states of PtH and PtH+ by relativistic ab initio electronic structure calculations: A model study for hydrogen chemisorption on platinum surfaces and related photoemission properties , 1983 .

[7]  W. Schwarz,et al.  Effective Hamiltonian for near-degenerate states in direct relativistic perturbation theory. I. Formalism , 1996 .

[8]  D. Lide Handbook of Chemistry and Physics , 1992 .

[9]  L. Visscher,et al.  The electronic structure of the PtH molecule: Fully relativistic configuration interaction calculations of the ground and excited states , 1993 .

[10]  W. Klopper Simple recipe for implementing computation of first‐order relativistic corrections to electron correlation energies in framework of direct perturbation theory , 1997 .

[11]  J. Almlöf,et al.  Relativistic calculations on platinum hydride using effective core potentials and first‐order perturbation theory , 1992 .

[12]  Johannes Grotendorst,et al.  Modern methods and algorithms of quantum chemistry , 2000 .

[13]  Wang,et al.  Accurate and simple analytic representation of the electron-gas correlation energy. , 1992, Physical review. B, Condensed matter.

[14]  Hess,et al.  Applicability of the no-pair equation with free-particle projection operators to atomic and molecular structure calculations. , 1985, Physical review. A, General physics.

[15]  W. Kutzelnigg Perturbation theory of relativistic corrections , 1989 .

[16]  B. Rosenberg Platinum coordination complexes in cancer chemotherapy , 1973, Naturwissenschaften.

[17]  K. Jankowski,et al.  Correlation and relativistic effects for many-electron systems , 1987 .

[18]  Marvin Douglas,et al.  Quantum electrodynamical corrections to the fine structure of helium , 1971 .

[19]  Wojciech Cencek,et al.  Accurate relativistic energies of one‐ and two‐electron systems using Gaussian wave functions , 1996 .

[20]  R. Franke,et al.  First‐order relativistic corrections to MP2 energy from standard gradient codes: Comparison with results from density functional theory , 1998 .

[21]  Robert J. Gdanitz,et al.  The averaged coupled-pair functional (ACPF): A size-extensive modification of MR CI(SD) , 1988 .

[22]  H. Stoll,et al.  Correlation energies in the spin-density functional formalism , 1980 .

[23]  Hans-Joachim Werner,et al.  Third-order multireference perturbation theory The CASPT3 method , 1996 .

[24]  M. Klobukowski,et al.  Well-tempered gaussian basis set expansions of Roothaan-Hartree-Fock atomic wavefunctions for lithium through mercury , 1988 .

[25]  Hans W. Horn,et al.  ELECTRONIC STRUCTURE CALCULATIONS ON WORKSTATION COMPUTERS: THE PROGRAM SYSTEM TURBOMOLE , 1989 .

[26]  Ingvar Lindgren,et al.  Diagonalisation of the Dirac Hamiltonian as a basis for a relativistic many-body procedure , 1986 .

[27]  H. Stoll,et al.  Energy-adjustedab initio pseudopotentials for the second and third row transition elements , 1990 .

[28]  Wenjian Liu,et al.  A small-core multiconfiguration Dirac–Hartree–Fock-adjusted pseudopotential for Tl – application to TlX (X = F, Cl, Br, I) , 2000 .

[29]  Evert Jan Baerends,et al.  Relativistic regular two‐component Hamiltonians , 1993 .

[30]  J. Olsen,et al.  Spin–orbit and correlation effects in platinum hydride (PtH) , 1998 .

[31]  Wenjian Liu,et al.  Relativistic ab initio and density functional theory calculations on the mercury fluorides: Is HgF4 thermodynamically stable? , 1999 .

[32]  A. Becke,et al.  Density-functional exchange-energy approximation with correct asymptotic behavior. , 1988, Physical review. A, General physics.

[33]  Michael Dolg,et al.  The Beijing four-component density functional program package (BDF) and its application to EuO, EuS, YbO and YbS , 1997 .

[34]  Wenjian Liu,et al.  Relativistic MCSCF by means of quasidegenerate direct perturbation theory. II. Preliminary applications , 2000 .

[35]  K. Dyall Relativistic effects on the bonding and properties of the hydrides of platinum , 1993 .

[36]  W. Kutzelnigg,et al.  Perturbative relativistic calculations for one-electron systems in a Gaussian basis , 1992 .

[37]  C. Marian,et al.  Relativistic all-electron ab initio calculations on the platinum hydride molecule , 1994 .

[38]  G. Gustafsson,et al.  Rotational analysis of the 2Δ3/2-X 2Δ3/2 and 2Φ7/2-X 2Δ5/2 sub-systems of PtD , 1989 .

[39]  N. Hush,et al.  Homogeneous Conversion of Methane to Methanol. 1. Catalytic Activation and Functionalization of Methane by cis-Platin in Sulfuric Acid: A Density Functional Study of the Thermochemistry , 1999 .

[40]  M. Parrinello,et al.  STRUCTURE AND BONDING IN CISPLATIN AND OTHER PT(II) COMPLEXES , 1995 .

[41]  T. H. Dunning Gaussian basis sets for use in correlated molecular calculations. I. The atoms boron through neon and hydrogen , 1989 .

[42]  Ph. Durand,et al.  Regular Two-Component Pauli-Like Effective Hamiltonians in Dirac Theory , 1986 .

[43]  A. Schäfer,et al.  Fully optimized contracted Gaussian basis sets of triple zeta valence quality for atoms Li to Kr , 1994 .

[44]  U. Wahlgren,et al.  A new mean-field and ECP-based spin-orbit method. Applications to Pt and PtH , 1996 .

[45]  R. Franke,et al.  Effective Hamiltonian for near-degenerate states in relativistic direct perturbation theory. II. H2+-like systems , 1998 .

[46]  Peddaiahgari Seetharamulu,et al.  Comprehensive ab initio quantum mechanical and molecular orbital (MO) analysis of cisplatin: Structure, bonding, charge density, and vibrational frequencies , 1999, J. Comput. Chem..

[47]  W. Kutzelnigg Effective Hamiltonians for degenerate and quasidegenerate direct perturbation theory of relativistic effects , 1999 .

[48]  A. Rutkowski Iterative solution of the one-electron Dirac equation based on the Bloch equation of the `direct perturbation theory' , 1999 .

[49]  P. Hay,et al.  An effective core potential investigation of Ni, Pd, and Pt and their monohydrides , 1986 .

[50]  P. Bernath,et al.  Laser and Fourier Transform Spectroscopy of PtH and PtD , 1993 .

[51]  J. A. Webster,et al.  The Addition of Silicon Hydrides to Olefinic Double Bonds. Part II. The Use of Group VIII Metal Catalysts , 1957 .

[52]  W. Kutzelnigg,et al.  Direct perturbation theory of relativistic effects for explicitly correlated wave functions: The He isoelectronic series , 1997 .

[53]  A. Rutkowski Relativistic perturbation theory. I. A new perturbation approach to the Dirac equation , 1986 .

[54]  Wenjian Liu,et al.  Relativistic MCSCF by means of quasidegenerate direct perturbation theory. I. Theory , 2000 .

[55]  Christoph van Wüllen,et al.  Relativistic all-electron density functional calculations , 1999, J. Comput. Chem..

[56]  S. H. Vosko,et al.  Accurate spin-dependent electron liquid correlation energies for local spin density calculations: a critical analysis , 1980 .

[57]  N. N. Greenwood,et al.  Chemistry of the elements , 1984 .

[58]  K. Balasubramanian,et al.  Potential‐energy surfaces for Pt2+H and Pt+H interactions , 1990 .

[59]  W. Kutzelnigg,et al.  Relativistic Hartree-Fock by means of stationary direct perturbation theory. II. Ground states of rare gas atoms , 1995 .

[60]  Rafa Wysokiski,et al.  The performance of different density functional methods in the calculation of molecular structures and vibrational spectra of platinum(II) antitumor drugs: cisplatin and carboplatin , 2001, J. Comput. Chem..

[61]  G. Herzberg,et al.  Constants of diatomic molecules , 1979 .

[62]  E. D. Cyan Handbook of Chemistry and Physics , 1970 .

[63]  J. Perdew,et al.  Density-functional approximation for the correlation energy of the inhomogeneous electron gas. , 1986, Physical review. B, Condensed matter.