Temperature effects in first-principles solid state calculations of the chemical shielding tensor made simple

被引:27
|
作者
Monserrat, Bartomeu [1 ]
Needs, Richard J. [1 ]
Pickard, Chris J. [2 ]
机构
[1] Univ Cambridge, Cavendish Lab, TCM Grp, Cambridge CB3 0HE, England
[2] UCL, Dept Phys & Astron, London WC1E 6BT, England
来源
JOURNAL OF CHEMICAL PHYSICS | 2014年 / 141卷 / 13期
基金
英国工程与自然科学研究理事会;
关键词
DENSITY-FUNCTIONAL THEORY; 1ST PRINCIPLES; NMR PARAMETERS; AB-INITIO; L-ALANINE; VIBRATIONAL CORRECTIONS; MAGNETIC-RESONANCE; MOLECULAR-DYNAMICS; O-17; SPECTROSCOPY;
D O I
10.1063/1.4897261
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
We study the effects of atomic vibrations on the solid-state chemical shielding tensor using first principles density functional theory calculations. At the harmonic level, we use a Monte Carlo method and a perturbative expansion. The Monte Carlo method is accurate but computationally expensive, while the perturbative method is computationally more efficient, but approximate. We find excellent agreement between the two methods for both the isotropic shift and the shielding anisotropy. The effects of zero-point quantum mechanical nuclear motion are important up to relatively high temperatures: at 500 K they still represent about half of the overall vibrational contribution. We also investigate the effects of anharmonic vibrations, finding that their contribution to the zero-point correction to the chemical shielding tensor is small. We exemplify these ideas using magnesium oxide and the molecular crystals L-alanine and beta-aspartyl-L-alanine. We therefore propose as the method of choice to incorporate the effects of temperature in solid state chemical shielding tensor calculations using the perturbative expansion within the harmonic approximation. This approach is accurate and requires a computational effort that is about an order of magnitude smaller than that of dynamical or Monte Carlo approaches, so these effects might be routinely accounted for. (C) 2014 AIP Publishing LLC.
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页数:13
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