Nuclear quantum effects in molecular dynamics simulations

• Published in: Journal of physics. Conference series Vol. 1136; no. 1; pp. 12014 - 12022
• Main Authors: Dammak, H, Hayoun, M, Brieuc, F, Geneste, G
• Format: Journal Article
• Language: English
• Published: Bristol IOP Publishing 01.12.2018; IOP Science
• Subjects: Access time; Anharmonicity; Centroids; Chemical Sciences; Classical mechanics; Computational Physics; Computing time; Condensed Matter; Cristallography; Energy distribution; Harmonic oscillators; Material chemistry; Molecular dynamics; Physics; Power spectral density; Quantum mechanics; Quantum Physics; Statistical Mechanics; Thermal baths; Time correlation functions; White noise; Zero point energy
• ISSN: 1742-6588; 1742-6596
• DOI: 10.1088/1742-6596/1136/1/012014

To take into account nuclear quantum effects on the dynamics of atoms, the path integral molecular dynamics (PIMD) method used since 1980s is based on the formalism developed by R. P. Feynman. However, the huge computation time required for the PIMD reduces its range of applicability. Another drawback is the requirement of additional techniques to access time correlation functions (ring polymer MD or centroid MD). We developed an alternative technique based on a quantum thermal bath (QTB) which reduces the computation time by a factor of ∼20. The QTB approach consists in a classical Langevin dynamics in which the white noise random force is replaced by a Gaussian random force having the power spectral density given by the quantum fluctuation-dissipation theorem. The method has yielded satisfactory results for weakly anharmonic systems: the quantum harmonic oscillator, the heat capacity of a MgO crystal, and isotope effects in 7LiH and 7LiD. Unfortunately, the QTB is subject to the problem of zero-point energy leakage (ZPEL) in highly anharmonic systems, which is inherent in the use of classical mechanics. Indeed, a part of the energy of the high-frequency modes is transferred to the low-frequency modes leading to a wrong energy distribution. We have shown that in order to reduce or even eliminate ZPEL, it is sufficient to increase the value of the frictional coefficient. Another way to solve the ZPEL problem is to combine the QTB and PIMD techniques. It requires the modification of the power spectral density of the random force within the QTB. This combination can also be seen as a way to speed up the PIMD.