Skip to main navigation Skip to search Skip to main content

Phaseless auxiliary field quantum Monte Carlo with projector-augmented wave method for solids

  • Amir Taheridehkordi (Corresponding author)
  • , Martin Schlipf
  • , Zoran Sukurma
  • , Moritz Humer
  • , Andreas Grüneis
  • , Georg Kresse

Publications: Contribution to journal › Article › Peer Reviewed

Abstract

We implement the phaseless auxiliary field quantum Monte Carlo method using the plane-wave based projector augmented wave method and explore the accuracy and the feasibility of applying our implementation to solids. We use a singular value decomposition to compress the two-body Hamiltonian and, thus, reduce the computational cost. Consistent correlation energies from the primitive-cell sampling and the corresponding supercell calculations numerically verify our implementation. We calculate the equation of state for diamond and the correlation energies for a range of prototypical solid materials. A down-sampling technique along with natural orbitals accelerates the convergence with respect to the number of orbitals and crystal momentum points. We illustrate the competitiveness of our implementation in accuracy and computational cost for dense crystal momentum point meshes compared to a well-established quantum-chemistry approach, the coupled-cluster ansatz including singles, doubles, and perturbative triple particle-hole excitation operators.
Original languageEnglish
Article number044109
Number of pages14
JournalJournal of Chemical Physics
Volume159
Issue number4
DOIs
Publication statusPublished - 28 Jul 2023

Funding

Funding by the Austrian Science Foundation (FWF) within the project P 33440 is gratefully acknowledged. Parts of the presented computational results have been obtained using the Vienna Scientific Cluster (VSC).

Austrian Fields of Science 2012

  • 103006 Chemical physics

Fingerprint

Dive into the research topics of 'Phaseless auxiliary field quantum Monte Carlo with projector-augmented wave method for solids'. Together they form a unique fingerprint.

Cite this