2018
DOI: 10.1021/acs.jctc.8b00988
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Combining Pair-Density Functional Theory and Variational Two-Electron Reduced-Density Matrix Methods

Abstract: Complete active space self-consistent field (CASSCF) computations can be realized at polynomial cost via the variational optimization of the active-space two-electron reduced-density matrix (2-RDM). Like conventional approaches to CASSCF, variational 2-RDM (v2RDM)-driven CASSCF captures nondynamical electron correlation in the active space, but it lacks a description of the remaining dynamical correlation effects. Such effects can be modeled through a combination of v2RDM-CASSCF and on-top pair-density functio… Show more

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Cited by 33 publications
(43 citation statements)
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References 153 publications
(298 reference statements)
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“…The existence of a spin‐contaminated, spin‐unrestricted solution of the Hartree–Fock (HF) [11, 12] or Kohn–Sham (KS) equations [13] for acenes suggests that strong nondynamic (also called static) correlation effects are present and that a single determinant description (as provided by HF and KS‐DFT) of the ground state is qualitatively insufficient. Nonetheless, the singlet ground‐state nature of larger acenes finds general support from studies that employ a wide variety of computational methods, including multiconfiguration treatments that are deemed more appropriate for systems with strong static correlation [14, 108–122] …”
Section: Theoretical Studiesmentioning
confidence: 99%
“…The existence of a spin‐contaminated, spin‐unrestricted solution of the Hartree–Fock (HF) [11, 12] or Kohn–Sham (KS) equations [13] for acenes suggests that strong nondynamic (also called static) correlation effects are present and that a single determinant description (as provided by HF and KS‐DFT) of the ground state is qualitatively insufficient. Nonetheless, the singlet ground‐state nature of larger acenes finds general support from studies that employ a wide variety of computational methods, including multiconfiguration treatments that are deemed more appropriate for systems with strong static correlation [14, 108–122] …”
Section: Theoretical Studiesmentioning
confidence: 99%
“…A partitioning of the matrix elements 2Dfalse˜jlik according to the well‐known Coulomb, exchange, and correlation components [ 38,39 ] and a subsequent formulation of the last two ones within the PDFT framework [ 2,22 ] allow one to express the energy as Enormalv2RDMDOCIPDFTg=i,j0.5emvji0.25em1Dfalse˜ji+i,j,k,l0.5emwitalicjlitalicik0.25em1trueD˜ji0.25em1Dfalse˜lk+Eot[],ρ()rnormalΠ()r where E ot is a functional of the total DOCI density ρ()r=false∑i,j1Dfalse˜ji0.5emϕi*()rϕj()r and on‐top pair density normalΠ()r=false∑i,j,k,l2Dfalse˜jlik0.5emϕi*()rϕk*()rϕj()rϕl()r . [ 40,41 ] In this work, we will evaluate the quantity E ot by means of the procedure described in ref.…”
Section: Theorymentioning
confidence: 99%
“…[ 40,41 ] In this work, we will evaluate the quantity E ot by means of the procedure described in ref. [22] 15.5emlefttrueEotρboldrΠboldr=EXCρboldr{}ρ()r1Rboldr12if1emR()r10if1emR()r>1ρboldr{}ρ()r1Rboldr12if1emR()r10if1emR()r>1 where R()r=40.5emnormalΠ()rρboldr2 defines the spin polarization factor 1Rboldr12, [2,22 ] and E XC is the translated functional of the corresponding quantities, where no dependence on |∇ Π( r )| is assumed. Notwithstanding, in order to avoid the known shortcomings derived from the double counting of the correlation, we follow ref.…”
Section: Theorymentioning
confidence: 99%
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