Abstract:We describe further details of the stochastic coupled cluster method and a diagnostic of such calculations, the shoulder height, akin to the plateau found in full configuration interaction quantum Monte Carlo. We describe an initiator modification to stochastic coupled cluster theory and show that initiator calculations can at times be extrapolated to the unbiased limit. We apply this method to the 3D 14-electron uniform electron gas and present complete basis set limit values of the coupled cluster singles an… Show more
“…The extrapolated energy is 91.6% ± 0.5% of the GFMC energy, which is in agreement with similar previous findings for 3D electron gases. 43,46 Repeating this procedure gives E = −0.257 ± 0.004 Ry and E = −0.140 ± 0.001 Ry for r s = 0.5 and 2.0, respectively.…”
mentioning
confidence: 99%
“…The power-laws derived were used in the years leading up to that study and then subsequently to achieve complete basis set results for a variety of systems [37][38][39] and in particular the uniform electron gas. [40][41][42][43][44][45][46][47][48][49][50][51] In recent times, several further major developments addressing plane wave basis set incompleteness error have been made. In particular, explicit correlation has been applied to a planewave basis, including F12 methods [52][53][54] and transcorrelation; 55 corrections have been derived for a semi-analytical correction which has been found for the direct term MP2 and for dRPA; 56 and hybrid basis sets of plane-wave derived occupied orbitals and Gaussian virtual orbitals have been implemented.…”
Basis set incompleteness error and finite size error can manifest concurrently in systems for which the two effects are phenomenologically well-separated in length scale. When this is true, we need not necessarily remove the two sources of error simultaneously. Instead, the errors can be found and remedied in different parts of the basis set. This would be of great benefit to a method such as coupled cluster theory since the combined cost of n 6 occ n 4 virt could be separated into n 6 occ and n 4 virt costs with smaller prefactors. In this Communication, we present analysis on a data set due to Baardsen and coworkers, containing coupled cluster doubles energies for the 2DEG for r s = 0.5, 1.0 and 2.0 a.u. at a wide range of basis set sizes and particle numbers. In obtaining complete basis set limit thermodynamic limit results, we find that within a small and removable error the above assertion is correct for this simple system. This approach allows for the combination of methods which separately address finite size effects and basis set incompleteness error.
“…The extrapolated energy is 91.6% ± 0.5% of the GFMC energy, which is in agreement with similar previous findings for 3D electron gases. 43,46 Repeating this procedure gives E = −0.257 ± 0.004 Ry and E = −0.140 ± 0.001 Ry for r s = 0.5 and 2.0, respectively.…”
mentioning
confidence: 99%
“…The power-laws derived were used in the years leading up to that study and then subsequently to achieve complete basis set results for a variety of systems [37][38][39] and in particular the uniform electron gas. [40][41][42][43][44][45][46][47][48][49][50][51] In recent times, several further major developments addressing plane wave basis set incompleteness error have been made. In particular, explicit correlation has been applied to a planewave basis, including F12 methods [52][53][54] and transcorrelation; 55 corrections have been derived for a semi-analytical correction which has been found for the direct term MP2 and for dRPA; 56 and hybrid basis sets of plane-wave derived occupied orbitals and Gaussian virtual orbitals have been implemented.…”
Basis set incompleteness error and finite size error can manifest concurrently in systems for which the two effects are phenomenologically well-separated in length scale. When this is true, we need not necessarily remove the two sources of error simultaneously. Instead, the errors can be found and remedied in different parts of the basis set. This would be of great benefit to a method such as coupled cluster theory since the combined cost of n 6 occ n 4 virt could be separated into n 6 occ and n 4 virt costs with smaller prefactors. In this Communication, we present analysis on a data set due to Baardsen and coworkers, containing coupled cluster doubles energies for the 2DEG for r s = 0.5, 1.0 and 2.0 a.u. at a wide range of basis set sizes and particle numbers. In obtaining complete basis set limit thermodynamic limit results, we find that within a small and removable error the above assertion is correct for this simple system. This approach allows for the combination of methods which separately address finite size effects and basis set incompleteness error.
“…2(c) shows the quasiparticle energies as function of the electron wave vector, i.e. the energy dispersion relation, for the 114 electron system with results extrapolated to the complete basis set limit 51 . The inferred bandwidths are 2.96 eV for CCSD, 3.79 eV for HF+GW, 2.77 eV for LDA+GW, and 2.56 eV for LDA+GW xc ; selfconsistency treated within the quasiparticle self-consistent GW scheme gives only a minor bandwidth narrowing compared to LDA+G 0 W 0 .…”
Section: Resultsmentioning
confidence: 99%
“…Since the submission of this article, two relevant articles have been published: Spencer and Thom have applied a stochastic implementation of CCSDT to the 14-electron UEG for r s ≤ 2 59 and Bhaskaran-Nair et al have calculated the CCSD Green's function for small molecules at a few frequency values. 60 …”
Section: Discussionmentioning
confidence: 99%
“…CCSDT calculations were performed using a modified version of the CFOUR code. 62 Dynamical DMRG calculations were done with the BLOCK code. …”
We use, for the first time, ab initio coupled-cluster theory to compute the spectral function of the uniform electron gas at a Wigner-Seitz radius of r s = 4. The coupled-cluster approximations we employ go significantly beyond the diagrammatic content of state-of-the-art GW theory. We compare our calculations extensively to GW and GW-plus-cumulant theory, illustrating the strengths and weaknesses of these methods in capturing the quasiparticle and satellite features of the electron gas. Our accurate calculations further allow us to address the long-standing debate over the occupied bandwidth of metallic sodium. Our findings indicate that the future application of coupled-cluster theory to condensed phase material spectra is highly promising.
We review the current state of reduced-scaling electron correlation methods, particularly coupled-cluster theory for the simulation and prediction of molecular response properties. The successes of local-coupled-cluster and related approaches are well known for reaction energies, thermodynamic constants, dipole moments, and so forth-properties that depend primarily on the quality of the ground-state wave function. However, much more challenging are higher-order properties such as polarizabilities, hyperpolarizabilities, optical rotations, magnetizabilities, and others that also require accurate representation of the derivative of the wave function to external electromagnetic fields. We discuss a range of methods for improving the correlation domains of such perturbed wave functions, including the use of "perturbation-aware" natural orbitals that are customized for the property of interest. In addition, we consider the viability and potential of promising, but stillemerging methods such as stochastic and real-time coupled-cluster approaches, for which the localizability of the field-dependent wave function may be more controllable than for conventional response theory.
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