By James B. Anderson, Stuart M. Rothstein
content material: 1. Quantum Monte Carlo Calculations for Helium Dimers and Trimers - Matthew C. Wilson and James B. Anderson; 2. Energies and homes of the Hydrogen Molecular Ion - S. A. Alexander and R. L. Coldwell; three. Accuracy of a Random stroll dependent method within the choice of Equilibrium Bond Lengths and Harmonic Frequencies for a few Doublet First-Row Diatomic Radicals - Shih-I Lu; four. Rydberg States with Quantum Monte Carlo - Annika Bande and Arne Luchow; five. Linear-Scaling evaluate of the neighborhood power in Quantum Monte Carlo - Brian Austin, Alan Aspuru-Guzik, Romelia Salmon-Ferrer, and William A. Lester, Jr; 6. digital Quantum Monte Carlo Calculations of Energies and Atomic Forces for Diatomic and Polyatomic Molecules - Myung gained Lee, Massimo Mella, and Andrew M. Rappe; 7. The fastened Hypernode technique for the answer of the various physique Schroedinger Equation - F. Pederiva, M. H. Kalos, F. Reboredo, D. Bressanini, D. Guclu, L. Colletti, C. J. Umrigar; eight. contemporary growth in Fermion Monte Carlo - M. H. Kalos and F. Pederiva; nine. Quantum results in Loosely sure Complexes - Meredith J. T. Jordan, Deborah L. Crittenden and Keiran C. Thompson; 10. Ab Initio Biomolecular Calculations utilizing Quantum Monte Carlo mixed with the Fragment Molecular Orbital strategy - Ryo Maezona, Hirofumi Watanabe, and Shigenori Tanaka; eleven. Vibrational Excited States via DMC - Anne B. McCoy; 12. Rotations and trade in Doped Helium Clusters: perception from Imaginary-Time Correlation capabilities - Nicholas Blinov and Pierre-Nicholas Roy
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Additional info for Advances in Quantum Monte Carlo
Recently Beran et al. (J) reported some sophisticated coupled-cluster based results using the basis sets of cc-pVTZ and cc-pVQZ for the same set of molecules that are C H , O H , F H , B O , C N , C O , N , CF, N O , 0 , OF, and F . The random walk based method employed in this work is the fixed-node (FN) diffusion quantum Monte Carlo (DQMC) method (2-5) implemented with the Ornstein-Uhlenbeck (OU) random walks guided by a trial wave function constructed from floating spherical Gaussian orbitals (FSGO) and spherical Gaussian geminals (SGG).
J. Chem. Phys. 1970, 53, 36813690. O. Atomic Data and Nuclear Data Tables 1974, 14, 11-20. M. Phys. Rev. A. 1977, 16, 640-645. ; Orlikowski, T. Mol. Phys. 1991, 74, 103-111. E. Mol. Phys. 1993, 80, 1541-1554. M. Mol. Phys. 1978, 36, 501-507. ; Shertzer, J. Chem. Phys. Lett. 1992, 189, 287-290. ; ACS Symposium Series; American Chemical Society: Washington, DC, 2006. ch003 Accuracy of a Random Walk-Based Approach in the Determination of Equilibrium Bond Lengths and Harmonic Frequencies for Some Doublet First-Row Diatomic Radicals Shih-I L u Department of Applied Chemistry, Fooyin University, 151 Chinhsueh Road, Ta-Liao Hsiang, Kaohsiung Hsien, 831 Taiwan The accuracy of equilibrium bond lengths and harmonic frequencies for 12 doublet first-row diatomic radicals is presented as predicted by the fixed-node diffusion quantum Monte Carlo method based on the Ornstein-Uhlenbeck random walk guided by a floating-spherical-Gaussian-orbital and spherical-Gaussian-geminal-type of trial wave function.
7 - the integration error and the error caused by our interpolation procedure. We evaluated the energy of each optimized wavefunction using 1,024,000 Monte Carlo integration points. This resulted in a set of energies that had a very low statistical error. We can estimate the grid error by omitting one point in V(R), reoptimizing the trial wavefunction and then recalculating E . This process was repeated until each point in V(R) had been omitted. The grid error in each rotational-vibrational energy level is just the standard deviation between our original value and these new energies.
Advances in Quantum Monte Carlo by James B. Anderson, Stuart M. Rothstein