TY - JOUR
T1 - Nuclear quantum effect on hydrogen adsorption site of zeolite-templated carbon model using path integral molecular dynamics
AU - Suzuki, Kimichi
AU - Kayanuma, Megumi
AU - Tachikawa, Masanori
AU - Ogawa, Hiroshi
AU - Nishihara, Hirotomo
AU - Kyotani, Takashi
AU - Nagashima, Umpei
N1 - Funding Information:
K. S., M. T., and U. N. thank to Dr M. Shiga at the Japan Atomic Energy Agency (JAEA) for useful discussions. This work has been supported by New Energy and Industrial Technology Development Organization (NEDO) under “Advanced Fundamental Research Project on Hydrogen Storage Materials”.
PY - 2011/9
Y1 - 2011/9
N2 - To settle the hydrogen adsorption sites on buckybowl C36H 12, which is picked up from zeolite-templated carbon (ZTC), we have performed path integral molecular dynamics (PIMD) simulation including thermal and nuclear quantum fluctuations under semi-empirical PM3 method. In the static PM3 calculation and classical simulation the five stable adsorption sites of hydrogen atom are optimized inside a buckybowl C36H12, which are labeled as α-, β1-, β2-, γ-, and δ-carbons from edge to innermost carbon. In PIMD simulation, meanwhile, stable adsorption site is not appeared on δ-carbon, but on only α-, β1-, β2-, and γ-carbons. This result is due to the fact that the adsorbed hydrogen atom can easily go over the barrier for hydrogen transferring from δ- to β1- carbons by thermal and nuclear quantum fluctuations. The thermal and nuclear quantum effects are key role to settle the hydrogen adsorption sites on carbon materials.
AB - To settle the hydrogen adsorption sites on buckybowl C36H 12, which is picked up from zeolite-templated carbon (ZTC), we have performed path integral molecular dynamics (PIMD) simulation including thermal and nuclear quantum fluctuations under semi-empirical PM3 method. In the static PM3 calculation and classical simulation the five stable adsorption sites of hydrogen atom are optimized inside a buckybowl C36H12, which are labeled as α-, β1-, β2-, γ-, and δ-carbons from edge to innermost carbon. In PIMD simulation, meanwhile, stable adsorption site is not appeared on δ-carbon, but on only α-, β1-, β2-, and γ-carbons. This result is due to the fact that the adsorbed hydrogen atom can easily go over the barrier for hydrogen transferring from δ- to β1- carbons by thermal and nuclear quantum fluctuations. The thermal and nuclear quantum effects are key role to settle the hydrogen adsorption sites on carbon materials.
KW - Carbon material
KW - Nuclear quantum effect
KW - Zeolite-templated carbon
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U2 - 10.1016/j.jallcom.2010.10.066
DO - 10.1016/j.jallcom.2010.10.066
M3 - Article
AN - SCOPUS:80052811133
SN - 0925-8388
VL - 509
SP - S868-S871
JO - Journal of Alloys and Compounds
JF - Journal of Alloys and Compounds
IS - SUPPL. 2
ER -