2023
DOI: 10.1021/acs.jctc.3c00659
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Streamlining and Optimizing Strategies of Electrostatic Parameterization

Qiang Zhu,
Yongxian Wu,
Shiji Zhao
et al.

Abstract: Accurate characterization of electrostatic interactions is crucial in molecular simulation. Various methods and programs have been developed to obtain electrostatic parameters for additive or polarizable models to replicate electrostatic properties obtained from experimental measurements or theoretical calculations. Electrostatic potentials (ESPs), a set of physically well-defined observables from quantum mechanical (QM) calculations, are well suited for optimization efforts due to the ease of collecting a lar… Show more

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Cited by 3 publications
(11 citation statements)
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“…The components f e and f t represent distance-dependent damping functions that modify T ij to circumvent the problem termed the “polarization catastrophe”, where induced dipole moments become divergent due to cooperative induction between closely positioned dipoles. , Several damping schemes proposed by Thole have been integrated into the AMBER ff12pol force field. However, Thole’s approaches have a drawback in that they solely address interactions between induced dipoles, leading to an inconsistent treatment of polarizations arising from fixed charges and permanent multipoles. Elking et al proposed an alternative damping scheme for modeling atomic electric multipoles using Gaussian density profiles, which was later named the polarizable Gaussian Multipole (pGM) model. The pGM model rectifies the limitation of Thole’s strategies by uniformly screening all short-range electrostatic interactions in a physically consistent manner, including interactions of charge–charge, charge–dipole, charge–quadrupole, dipole–dipole, etc. The formulas for damping functions f e and f t in the pGM model are as follows .25ex2ex S italicij = r ij 2 ( R i 2 + R j 2 ) f normale = erf false( S ij false) 2 π S italicij exp false( prefix− S italicij 2 false) f normalt = erf false( S ij false) 2 π S italicij exp false( prefix− S …”
Section: Introductionmentioning
confidence: 99%
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“…The components f e and f t represent distance-dependent damping functions that modify T ij to circumvent the problem termed the “polarization catastrophe”, where induced dipole moments become divergent due to cooperative induction between closely positioned dipoles. , Several damping schemes proposed by Thole have been integrated into the AMBER ff12pol force field. However, Thole’s approaches have a drawback in that they solely address interactions between induced dipoles, leading to an inconsistent treatment of polarizations arising from fixed charges and permanent multipoles. Elking et al proposed an alternative damping scheme for modeling atomic electric multipoles using Gaussian density profiles, which was later named the polarizable Gaussian Multipole (pGM) model. The pGM model rectifies the limitation of Thole’s strategies by uniformly screening all short-range electrostatic interactions in a physically consistent manner, including interactions of charge–charge, charge–dipole, charge–quadrupole, dipole–dipole, etc. The formulas for damping functions f e and f t in the pGM model are as follows .25ex2ex S italicij = r ij 2 ( R i 2 + R j 2 ) f normale = erf false( S ij false) 2 π S italicij exp false( prefix− S italicij 2 false) f normalt = erf false( S ij false) 2 π S italicij exp false( prefix− S …”
Section: Introductionmentioning
confidence: 99%
“…Recently, the programs PyRESP_GEN and PyRESP have been developed for pGM model electrostatic parametrizations, , which extends the RESP program to accommodate both permanent and induced atomic dipoles and has been integrated into the AmberTools package. , An efficient simulation algorithm for the pGM model has also been incorporated into the SANDER program and is presently being adapted for utilization on parallel platforms through the PMEMD program. ,, Numerous previous studies have highlighted the efficacy of the pGM models in terms of accuracy in modeling molecular properties, including molecular polarizability anisotropy, ESPs surrounding molecules, molecular electric moments, interaction energies, and many-body interaction energies . Furthermore, the pGM model has been shown to possess transferability from training molecules and conformations to testing molecules (such as oligomers, molecule complexes, or polymers) and different conformations …”
Section: Introductionmentioning
confidence: 99%
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