2022
DOI: 10.3390/computation10020030
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Kinetic Energy Density Functionals Based on a Generalized Screened Coulomb Potential: Linear Response and Future Perspectives

Abstract: We consider kinetic energy functionals that depend, beside the usual semilocal quantities (density, gradient, Laplacian of the density), on a generalized Yukawa potential, that is the screened Coulomb potential of the density raised to some power. These functionals, named Yukawa generalized gradient approximations (yGGA), are potentially efficient real-space semilocal methods that include significant non-local effects and can describe different important exact properties of the kinetic energy. In this work, we… Show more

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Cited by 12 publications
(9 citation statements)
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References 92 publications
(112 reference statements)
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“…Thus, both classes of functionals have positive and negative features. Recently, we have introduced a new class of KE functionals, named Yukawa‐Generalized Gradient Approximation (yGGA), with the following general form [61,62]: TsyGGA=τTF(r)Fs[p(r),q(r),yα(r)]d3r, where τTF(r)=(3/10)n(r)kF(r)2 [with kF(r)=(3π2n(r))1/3 and n(r) being the Fermi wave vector and the electron density, respectively] is the Thomas‐Fermi (TF) kinetic energy density (KED), Fs is the enhancement factor, p=|n|2/(4kF2n2) is the reduced gradient, q=2n/(4kF2n) is the reduced Laplacian, and …”
Section: Introductionmentioning
confidence: 99%
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“…Thus, both classes of functionals have positive and negative features. Recently, we have introduced a new class of KE functionals, named Yukawa‐Generalized Gradient Approximation (yGGA), with the following general form [61,62]: TsyGGA=τTF(r)Fs[p(r),q(r),yα(r)]d3r, where τTF(r)=(3/10)n(r)kF(r)2 [with kF(r)=(3π2n(r))1/3 and n(r) being the Fermi wave vector and the electron density, respectively] is the Thomas‐Fermi (TF) kinetic energy density (KED), Fs is the enhancement factor, p=|n|2/(4kF2n2) is the reduced gradient, q=2n/(4kF2n) is the reduced Laplacian, and …”
Section: Introductionmentioning
confidence: 99%
“…A key point of the reduced Yukawa potential yα is that it yields a non‐linear contribution to the linear response function of the HEG, so that the Lindhard function can be well reproduced [61,62]. This is a fundamental improvement with respect to conventional KE functionals based only on semilocal ingredients (such as p and q), which yield an incorrect polynomial linear response function [36,61,62].…”
Section: Introductionmentioning
confidence: 99%
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“…This quantity has long been associated with proper electronic shell structure [15,30,31]. Recently, shell-structure-based functionals are also showing promises [32,33].…”
Section: Introductionmentioning
confidence: 99%
“…We can notice the large panel of scientific topics covered by Karlheinz's knowledge. We deeply acknowledge the following contributions related to spectroscopy by Manuel Yañez et al [12], Juan-Carlos Sancho-García and Emilio San-Fabián [13]; excited states by Ágnes Nagy [14], Kalidas Sen et al [15] and Fabrizia Negri et al [16]; DFT developments by Fabio Della Sala et al [17], Mathias Rapacioli and Nathalie Tarrat [18], Emmanuel Fromager et al [19], José Manuel García de la Vega et al [20] and Harry Ramanantoanina [21]; results analysis by Andreas Savin et al [22] and Manuel Richter et al [23]; and, of course, the solid state and surfaces by Leila Kalantari and Fabien Tran et al [24], Denis Salahub et al [25], Peter Blaha et al [26], Samuel B. Trickey [27], William Lafargue-Dit-Hauret and Xavier Rocquefelte [28], Tzonka Mineva and Hazar Guesmi et al [29]. (H.C.)…”
mentioning
confidence: 99%