Abstract:We here apply the recently developed initiator density matrix quantum Monte Carlo (i-DMQMC) to a wide range of chemical environments using atoms and molecules in vacuum. i-DMQMC samples the exact density matrix of a Hamiltonian at finite temperature and combines the accuracy of full configuration interaction quantum Monte Carlo (FCIQMC) full configuration interaction (FCI) or exact energies in a finite basis set with finite temperature. By way of exploring the applicability of i-DMQMC for molecular systems, we… Show more
“…In a recent study, we showed that the density matrix quantum Monte Carlo (DMQMC) method could be applied to molecular systems, extending it beyond original applications to model systems in condensed matter physics. 1 The use of finite temperature electronic structure methods are becoming increasingly important in applications such as plasmonic catalysis, 2,3 the study of planetary interiors, 4 and solid-state materials 5 , where the temperature dependence is key in obtaining physical and chemical properties, such as phase diagrams and excitation energies. The inclusion of temperature in quantum chemistry methods is difficult because at finite temperatures, more than one state is often occupied, increasing the difficulty of solving the Schrodinger equation.…”
Section: Introductionmentioning
confidence: 99%
“…The development of the initiator approximation in DMQMC achieved a similar outcome allowing for our previous work on the uniform electron gas and ab initio molecular systems. 1,34 Subsequently, there were also a wide variety of FCIQMC or FCIQMC-like methods developments which are beyond the scope of this work to review in detail. [35][36][37][38][39][40][41][42][43][44][45][46][47][48][49][50] Large scale implementations of the FCIQMC method and related methods have also been developed and these papers review current challenges and developments for the interested reader.…”
“…In a recent study, we showed that the density matrix quantum Monte Carlo (DMQMC) method could be applied to molecular systems, extending it beyond original applications to model systems in condensed matter physics. 1 The use of finite temperature electronic structure methods are becoming increasingly important in applications such as plasmonic catalysis, 2,3 the study of planetary interiors, 4 and solid-state materials 5 , where the temperature dependence is key in obtaining physical and chemical properties, such as phase diagrams and excitation energies. The inclusion of temperature in quantum chemistry methods is difficult because at finite temperatures, more than one state is often occupied, increasing the difficulty of solving the Schrodinger equation.…”
Section: Introductionmentioning
confidence: 99%
“…The development of the initiator approximation in DMQMC achieved a similar outcome allowing for our previous work on the uniform electron gas and ab initio molecular systems. 1,34 Subsequently, there were also a wide variety of FCIQMC or FCIQMC-like methods developments which are beyond the scope of this work to review in detail. [35][36][37][38][39][40][41][42][43][44][45][46][47][48][49][50] Large scale implementations of the FCIQMC method and related methods have also been developed and these papers review current challenges and developments for the interested reader.…”
“…62 This will enable the study of low temperature Bose and Bose-Fermi condensates 62 as well as superconductors 91 with the high accuracy typical of AFQMC techniques. In addition, our algorithm will enable apples-to-apples, canonical ensemble comparisons between FT-AFQMC and other canonical ensemble finite temperature electronic structure techniques, such as Density Matrix QMC 92 and finite temperature coupled cluster approaches, [18][19][20][21] for the first time. Some of these comparisons will necessitate generalizing our formalism to arbitrary ab initio Hamiltonians, which is an ongoing effort.…”
Finite temperature auxiliary field-based Quantum Monte Carlo methods, including Determinant Quantum Monte Carlo (DQMC) and Auxiliary Field Quantum Monte Carlo (AFQMC), have historically assumed pivotal roles in the investigation of the finite temperature phase diagrams of a wide variety of multidimensional lattice models and materials. Despite their utility, however, these techniques are typically formulated in the grand canonical ensemble, which makes them difficult to apply to condensates like superfluids and difficult to benchmark against alternative methods that are formulated in the canonical ensemble. Working in the grand canonical ensemble is furthermore accompanied by the increased overhead associated with having to determine the chemical potentials that produce desired fillings. Given this backdrop, in this work, we present a new recursive approach for performing AFQMC simulations in the canonical ensemble that does not require knowledge of chemical potentials. To derive this approach, we exploit the convenient fact that AFQMC solves the many-body problem by decoupling many-body propagators into integrals over one-body problems to which non-interacting theories can be applied. We benchmark the accuracy of our technique on illustrative Bose and Fermi Hubbard models and demonstrate that it can converge more quickly to the ground state than grand canonical AFQMC simulations. We believe that our novel use of HS-transformed operators to implement algorithms originally derived for non-interacting systems will motivate the development of a variety of other methods and anticipate that our technique will enable direct performance comparisons against other many-body approaches formulated in the canonical ensemble.
“…After being developed to use the initiator approach, 65 which was also adapted from the groundstate FCIQMC version 66 , IP-DMQMC benchmarked the warm dense electron gas alongside path integral Monte Carlo approaches to obtain a finite-temperature local density approximation functional. [67][68][69] In addition to these successes, IP-DMQMC showed promise in initial applications to molecular systems 70 and its sign problem showed to be similar to that of FCIQMC. 71 In this work we seek to extend IP-DMQMC by continuing the simulation after the target inverse temperature is reached.…”
The density matrix quantum Monte Carlo (DMQMC) set of methods stochastically samples the exact Nbody density matrix for interacting electrons at finite temperature. We introduce a simple modification to the interaction picture DMQMC method (IP-DMQMC) which overcomes the limitation of only sampling one inverse temperature point at a time. At the target inverse temperature, instead of ending the simulation, we incorporate a change of picture away from the interaction picture. The result is a propagator that is a piecewise function, which uses the interaction picture in the first phase of a simulation, followed by the application of the Bloch equation once the target inverse temperature is reached. We find that the performance of this method is similar to or better than the DMQMC and IP-DMQMC algorithms in a variety of molecular test systems.
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