TY - JOUR
T1 - Electronic and Nuclear Contributions to Vibrational Stark Shifts of Hydroxyl Stretching Frequencies of Water Clusters
AU - Lim, Jong Hyeon
AU - Cho, Daeheum
AU - Kang, Heon
AU - Lee, Jin Yong
N1 - Publisher Copyright:
© 2018 American Chemical Society.
PY - 2018/6/21
Y1 - 2018/6/21
N2 - In spite of the importance of vibrational Stark effect (VSE) and many attempts, origin of VSE is still unclear in molecular level. Here, we studied on origin of VSE of hydroxyl stretching vibration in small water clusters (monomer, dimer, and tetramer) assuming that VSE can be separated by nuclear and electronic contribution. We calculated total Stark tuning rate (Δμtot) and its nuclear contribution (Δμgeom) using the ab initio method, then the electronic contribution (Δμelec) was simply obtained by the difference, Δμtot - Δμgeom. In all cases, the nuclear contribution has dominant contribution to VSE. The hydroxyl stretching mode with neighboring hydrogen acceptor showed larger Δμgeom than that of dangling bonds. Furthermore, the calculated Δμgeom became larger in larger cluster due to the hydrogen bond network. The comparison between Stark tuning rates including and excluding anharmonicity supports the importance of potential anharmonicity in VSE, as previously reported. Interestingly, a good linear relationship is observed between the hydroxyl stretch frequency (νgeom) and hydroxyl bond length and also between the Stark tuning rate (Δμgeom) and the change of hydroxyl bond length. Similarly, the electronic contribution of calculated frequencies and Stark tuning rate (Δμelec) showed a good linear relationship with atomic charge derived by electronic perturbation (Δqelec) and change of that (Δ(Δqelec)), respectively.
AB - In spite of the importance of vibrational Stark effect (VSE) and many attempts, origin of VSE is still unclear in molecular level. Here, we studied on origin of VSE of hydroxyl stretching vibration in small water clusters (monomer, dimer, and tetramer) assuming that VSE can be separated by nuclear and electronic contribution. We calculated total Stark tuning rate (Δμtot) and its nuclear contribution (Δμgeom) using the ab initio method, then the electronic contribution (Δμelec) was simply obtained by the difference, Δμtot - Δμgeom. In all cases, the nuclear contribution has dominant contribution to VSE. The hydroxyl stretching mode with neighboring hydrogen acceptor showed larger Δμgeom than that of dangling bonds. Furthermore, the calculated Δμgeom became larger in larger cluster due to the hydrogen bond network. The comparison between Stark tuning rates including and excluding anharmonicity supports the importance of potential anharmonicity in VSE, as previously reported. Interestingly, a good linear relationship is observed between the hydroxyl stretch frequency (νgeom) and hydroxyl bond length and also between the Stark tuning rate (Δμgeom) and the change of hydroxyl bond length. Similarly, the electronic contribution of calculated frequencies and Stark tuning rate (Δμelec) showed a good linear relationship with atomic charge derived by electronic perturbation (Δqelec) and change of that (Δ(Δqelec)), respectively.
UR - http://www.scopus.com/inward/record.url?scp=85048234308&partnerID=8YFLogxK
U2 - 10.1021/acs.jpcc.8b03936
DO - 10.1021/acs.jpcc.8b03936
M3 - Article
AN - SCOPUS:85048234308
SN - 1932-7447
VL - 122
SP - 12970
EP - 12974
JO - Journal of Physical Chemistry C
JF - Journal of Physical Chemistry C
IS - 24
ER -