Product representation of potential energy surfaces. II

An efficient method was recently introduced [J. Chem. Phys. 102, 5605 (1995); 104, 7974 (1996)] to represent multidimensional potential energy surfaces as a linear combination of products of one-dimensional functions, so-called natural potentials. Weight functions were shown to be easily implemented in the product representation scheme as long as they are separable, i.e., defined as a product of one-dimensional weight functions. Here the constraint imposed by the special product form of the separable weights is removed. Nonseparable weights are emulated by dividing the potential energy surface in arbitrary regions of minor and major physical relevance and by utilizing a so-called relevant region iteration procedure. Maintaining the advantageous computational scaling properties of the product representation scheme, this relevant region iteration procedure allows the stepwise improvement of the surface representation in the regions of major relevance. The quality of the product representation in the regions...

[1]  H. Meyer,et al.  Reactive scattering using the multiconfiguration time‐dependent Hartree approximation: General aspects and application to the collinear H+H2→H2+H reaction , 1995 .

[2]  Donald G. Truhlar,et al.  A double many‐body expansion of the two lowest‐energy potential surfaces and nonadiabatic coupling for H3 , 1987 .

[3]  C. Cerjan,et al.  Numerical grid methods and their application to Schrödinger's equation , 1993 .

[4]  C. Horowitz,et al.  Functional representation of Liu and Siegbahn’s accurate ab initio potential energy calculations for H+H2 , 1978 .

[5]  E. Schmidt Zur Theorie der linearen und nichtlinearen Integralgleichungen , 1907 .

[6]  Bin Liu,et al.  An accurate three‐dimensional potential energy surface for H3 , 1978 .

[7]  U. Manthe,et al.  Iterative diagonalization within the multi-configurational time-dependent Hartree approach: calculation of vibrationally excited states and reaction rates , 1996 .

[8]  M. Baer,et al.  The time‐dependent Schrödinger equation: Application of absorbing boundary conditions , 1989 .

[9]  Uwe V. Riss,et al.  Calculation of resonance energies and widths using the complex absorbing potential method , 1993 .

[10]  William H. Press,et al.  Numerical recipes , 1990 .

[11]  M. R. Peterson,et al.  An improved H3 potential energy surface , 1991 .

[12]  U. Manthe,et al.  A multi-configurational time-dependent Hartree approach to the direct calculation of thermal rate constants , 1997 .

[13]  U. Manthe,et al.  Wave‐packet dynamics within the multiconfiguration Hartree framework: General aspects and application to NOCl , 1992 .

[14]  M. Nonella,et al.  Photodissociation of ClNO in the S1 state: A quantum‐mechanical ab initio study , 1990 .

[15]  H. Meyer,et al.  Time‐dependent calculation of reactive flux employing complex absorbing potentials: General aspects and application within the multiconfiguration time‐dependent Hartree wave approach , 1996 .

[16]  M. R. Peterson,et al.  A refined H3 potential energy surface , 1996 .

[17]  U. Manthe,et al.  The multi-configurational time-dependent Hartree approach , 1990 .

[18]  Jan Broeckhove,et al.  Time-dependent quantum molecular dynamics , 1992 .

[19]  R. Kosloff,et al.  A fourier method solution for the time dependent Schrödinger equation as a tool in molecular dynamics , 1983 .

[20]  Uwe V. Riss,et al.  Investigation on the reflection and transmission properties of complex absorbing potentials , 1996 .

[21]  D. Kouri,et al.  L2 amplitude density method for multichannel inelastic and rearrangement collisions , 1988 .

[22]  Hans-Dieter Meyer,et al.  An efficient and robust integration scheme for the equations of motion of the multiconfiguration time-dependent Hartree (MCTDH) method , 1997 .

[23]  Carl de Boor,et al.  A Practical Guide to Splines , 1978, Applied Mathematical Sciences.

[24]  D. Neuhauser,et al.  The application of wave packets to reactive atom–diatom systems: A new approach , 1989 .