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Fitting Potential Energy Surfaces by Learning the Charge Density Matrix with Permutationally Invariant Polynomials
[Image: see text] The electronic energy in the Hartree–Fock (HF) theory is the trace of the product of the charge density matrix (CDM) with the one-electron and two-electron matrices represented in an atomic orbital basis, where the two-electron matrix is also a function of the same CDM. In this wor...
Autores principales: | , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical Society
2023
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10501011/ https://www.ncbi.nlm.nih.gov/pubmed/37561135 http://dx.doi.org/10.1021/acs.jctc.3c00586 |
Sumario: | [Image: see text] The electronic energy in the Hartree–Fock (HF) theory is the trace of the product of the charge density matrix (CDM) with the one-electron and two-electron matrices represented in an atomic orbital basis, where the two-electron matrix is also a function of the same CDM. In this work, we examine a formalism of analytic representation of a generic molecular potential energy surface (PES) as a sum of a linearly parameterized HF and a correction term, the latter formally representing the electron correlation energy, also linearly parameterized, by expressing the elements of CDM using permutationally invariant polynomials (PIPs). We show on a variety of numerical examples, ranging from exemplary two-electron systems HeH(+) and H(3)(+) to the more challenging cases of methanium (CH(5)(+)) fragmentation and high-energy tautomerization of formamide to formimidic acid that such a formulation requires significantly fewer, 10–20% of PIPs, to accomplish the same accuracy of the fit as the conventional representation at practically the same computational cost. |
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