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Published August 14, 2018 | Submitted
Journal Article Open

A Perturbative Density Matrix Renormalization Group Algorithm for Large Active Spaces

Abstract

We describe a low cost alternative to the standard variational DMRG (density matrix renormalization group) algorithm that is analogous to the combination of the selected configuration interaction plus perturbation theory (SCI+PT). We denote the resulting method p-DMRG (perturbative DMRG) to distinguish it from the standard variational DMRG. p-DMRG is expected to be useful for systems with very large active spaces, for which variational DMRG becomes too expensive. Similar to SCI+PT, in p-DMRG, a zeroth-order wave function is first obtained by a standard DMRG calculation but with a small bond dimension. Then, the residual correlation is recovered by a second-order perturbative treatment. We discuss the choice of partitioning for perturbation theory, which is crucial for its accuracy and robustness. To circumvent the problem of a large bond dimension in the first-order wave function, we use a sum of matrix product states to expand the first-order wave function, yielding substantial savings in computational cost and memory. We also propose extrapolation schemes to reduce the errors in the zeroth- and first-order wave functions. Numerical results for Cr2 with a (28e, 76o) active space and 1,3-butadiene with an (22e, 82o) active space reveal that p-DMRG provides ground state energies of a similar quality to variational DMRG with very large bond dimensions but at a significantly lower computational cost. This suggests that p-DMRG will be an efficient tool for benchmark studies in the future.

Additional Information

© 2018 American Chemical Society. Received: March 17, 2018; Published: June 21, 2018. This work was supported by the U.S. National Science Foundation through CHE 1665333. Additional support for development of the Block program used in this work was provided by OAC 1657286. Z.L. is supported by the Simons Collaboration on the Many-Electron Problem. G.K.-L.C. is a Simons Investigator in Physics. The authors declare no competing financial interest.

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