Abstract

We determine the correlation energy of BN, SiO$_2$ and ice polymorphs employing a recently developed RPAx (random phase approximation with exchange) approach. The RPAx provides larger and more accurate polarizabilities as compared to the RPA, and captures effects of anisotropy. In turn, the correlation energy, defined as an integral over the density-density response function, gives improved binding energies without the need for error cancellation. Here, we demonstrate that these features are crucial for predicting the relative energies between low- and high-pressure polymorphs of different coordination number as, e.g., between $\alpha$-quartz and stishovite in SiO$_2$, or layered and cubic BN. Furthermore, a reliable (H$_2$O)$_2$ potential energy surface is obtained, necessary for describing the various phases of ice. The RPAx gives results comparable to other high-level methods such as coupled cluster and quantum Monte Carlo, also in cases where the RPA breaks down. Although higher computational cost than RPA we observe a faster convergence with respect to the number of eigenvalues in the response function.

Highlights

  • The development of an accurate, yet computationally efficient, electronic structure approach able to treat electron correlation in solids remains an important task in condensed matter physics

  • The random phase approximation with exchange (RPAx) approximation for the correlation energy is based on the adiabatic connection fluctuation-dissipation (ACFD) formula, in which the exact correlation energy is expressed in terms of the linear density response function, χλ, multiplied by the Coulomb interaction, v, and integrated over the frequency and the interaction strength λ

  • In this work we analyzed some of these cases and demonstrated how exact-exchange in the response function provides a theoretically well-defined, accurate, and reliable improvement

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Summary

INTRODUCTION

The development of an accurate, yet computationally efficient, electronic structure approach able to treat electron correlation in solids remains an important task in condensed matter physics. Within an approach that combines many-body perturbation theory (MBPT) and TDDFT the first step beyond RPA is to include the full Fock exchange term in the density response function via the nonlocal and frequency-dependent exactexchange (EXX) kernel. This generates the random phase approximation with exchange (RPAx) that exactly includes the second-order exchange diagram as well as higher-order exchange effects, in addition to the RPA ring series of diagrams [25,26,27,28,29]. The RPAx stays within the simple computational framework of the RPA, but has an accuracy comparable with more sophisticated methods such as quantum Monte Carlo (QMC) and coupled cluster (CC)

RPA WITH EXCHANGE
NOBLE GAS SOLIDS
BORON NITRIDE AND SILICA
ICE POLYMORPHISM
Findings
CONCLUSION
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