2024
DOI: 10.1039/d3cp05471c
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The accuracy limit of chemical shift predictions for species in aqueous solution

Stefan Maste,
Bikramjit Sharma,
Tim Pongratz
et al.

Abstract: Accurate predictions of chemical shifts of species in aqueous solution are possible by combining ab initio molecular dynamics simulations for ensembles of locally solvated target and reference compound (DSS) with quantum-mechanical solvation models.

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Cited by 4 publications
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“…These first-principles simulations dynamically solve the Schrödinger equation, explicitly incorporating electronic many-body effects and solute–solvent interactions without relying on predefined parameters . Despite their high computational cost, these simulations have been widely adopted to incorporate dynamical effects in predicting NMR properties, including 1 H, 13 C, and 15 N chemical shifts. Throughout the AIMD simulations, TPB maintains its structural characteristics observed in the crystal phase with the H1 and H3 atoms proximal to the aromatic rings and the H2 and H4 atoms close to the O atoms in the tosylate groups. To characterize the configuration of TPB, we use d HX and d HO as geometric parameters and calculate the free energies as F = prefix− k B T ln P ( d H O , d H X ) P max Here, k B is the Boltzmann constant and T is the simulation temperature.…”
Section: Resultsmentioning
confidence: 99%
“…These first-principles simulations dynamically solve the Schrödinger equation, explicitly incorporating electronic many-body effects and solute–solvent interactions without relying on predefined parameters . Despite their high computational cost, these simulations have been widely adopted to incorporate dynamical effects in predicting NMR properties, including 1 H, 13 C, and 15 N chemical shifts. Throughout the AIMD simulations, TPB maintains its structural characteristics observed in the crystal phase with the H1 and H3 atoms proximal to the aromatic rings and the H2 and H4 atoms close to the O atoms in the tosylate groups. To characterize the configuration of TPB, we use d HX and d HO as geometric parameters and calculate the free energies as F = prefix− k B T ln P ( d H O , d H X ) P max Here, k B is the Boltzmann constant and T is the simulation temperature.…”
Section: Resultsmentioning
confidence: 99%