TY - JOUR
T1 - Path integral molecular dynamics for hydrogen adsorption site of zeolite-templated carbon with semi-empirical PM3 potential
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 - 2011/11/15
Y1 - 2011/11/15
N2 - To evaluate the adsorption sites of hydrogen atom on buckybowl-like molecule (C36H12), which is a model fragment structure of zeolite-templated carbon (ZTC), we have performed path integral molecular dynamics (PIMD) simulation including thermal and nuclear quantum fluctuations under the semi-empirical PM3 potential. Here we have picked up ten carbons as the adsorption sites of additional hydrogen atom (H*), which are labeled as α-, β1-, β2-, γ-, and δ-carbon from edge to bottom carbon for inside and outside of C36H12, respectively. In the static PM3 calculation and conventional MD simulation the ten stable adsorption sites of H* are obtained both inside and outside of C36H12. In PIMD simulation, on the other hand, the nine stable adsorption sites are obtained, except for δ-carbon for inside of C36H12. This result is due to the fact that the thermal effect and zero point vibration of δ-carbon and H* stretching motion make adsorbed hydrogen atom go over potential barrier from δ- and β1-carbon for inside of C36H12 more readily. The thermal and nuclear quantum effects are important to evaluate the hydrogen adsorption site on carbon materials.
AB - To evaluate the adsorption sites of hydrogen atom on buckybowl-like molecule (C36H12), which is a model fragment structure of zeolite-templated carbon (ZTC), we have performed path integral molecular dynamics (PIMD) simulation including thermal and nuclear quantum fluctuations under the semi-empirical PM3 potential. Here we have picked up ten carbons as the adsorption sites of additional hydrogen atom (H*), which are labeled as α-, β1-, β2-, γ-, and δ-carbon from edge to bottom carbon for inside and outside of C36H12, respectively. In the static PM3 calculation and conventional MD simulation the ten stable adsorption sites of H* are obtained both inside and outside of C36H12. In PIMD simulation, on the other hand, the nine stable adsorption sites are obtained, except for δ-carbon for inside of C36H12. This result is due to the fact that the thermal effect and zero point vibration of δ-carbon and H* stretching motion make adsorbed hydrogen atom go over potential barrier from δ- and β1-carbon for inside of C36H12 more readily. The thermal and nuclear quantum effects are important to evaluate the hydrogen adsorption site on carbon materials.
KW - Carbon materials
KW - Nuclear quantum effect
KW - Path integral simulation
KW - Zeolite-templated carbon
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U2 - 10.1016/j.comptc.2010.12.028
DO - 10.1016/j.comptc.2010.12.028
M3 - Article
AN - SCOPUS:84555197130
SN - 2210-271X
VL - 975
SP - 128
EP - 133
JO - Computational and Theoretical Chemistry
JF - Computational and Theoretical Chemistry
IS - 1-3
ER -