TY - JOUR
T1 - Bi-layering at ionic liquid surfaces
T2 - a sum-frequency generation vibrational spectroscopy- And molecular dynamics simulation-based study
AU - Iwahashi, Takashi
AU - Ishiyama, Tatsuya
AU - Sakai, Yasunari
AU - Morita, Akihiro
AU - Kim, Doseok
AU - Ouchi, Yukio
N1 - Funding Information:
This work is supported in part by KAKENHI; Grant-in-Aid for Scientific Research (A) (No. 26248004) and Grant-in-Aid for Scientific Research (B) (No. 16H04095) from the Ministry of Education, Culture, Sports, Science and Technology (MEXT) of Japan. Some of the MD calculations were performed using the supercomputers at the Research Center for Computational Science, Okazaki, Japan. D. K. acknowledges National Research Foundation (NRF) grant no. 2019R1A2C1004292 of the Republic of Korea.
Publisher Copyright:
© the Owner Societies 2020.
PY - 2020/6/14
Y1 - 2020/6/14
N2 - Room-temperature ionic liquids (RTILs) are being increasingly employed as novel solvents in several fields, including chemical engineering, electrochemistry, and synthetic chemistry. To further increase their usage potential, a better understanding of the structure of their surface layer is essential. Bi-layering at the surfaces of RTILs consisting of 1-alkyl-3-methylimidazolium ([Cnmim]+;n= 4, 6, 8, 10, and 12) cations and bis(trifluoromethanesulfonyl)amide ([TFSA]−) anions was demonstratedviainfrared-visible sum-frequency generation (IV-SFG) vibrational spectroscopy and molecular dynamics (MD) simulations. It was found that the sum-frequency (SF) signal from the [TFSA]−anions decreases as the alkyl chain length increases, whereas the SF signal from the r+mode (the terminal CH3group) of the [Cnmim]+cations is almost the same regardless of chain length. MD simulations show the formation of a bi-layered structure consisting of the outermost first layer and a submerged second layer in a “head-to-head” molecular arrangement. The decrease in the SF signals of the normal modes of the [TFSA]−anions is caused by destructive and out-of-phase interference of vibrations of corresponding molecular moieties oriented toward each other in the first and second layers. In contrast, the r+mode of [Cnmim]+does not experience destructive interference because the peak position of the r+mode differs marginally at the surface and in the bulk. Our conclusions are not limited to the system presented here. Similar bi-layered structures can be expected for the surfaces of conventional RTILs, which necessitates the consideration of bi-layering in the design and application.
AB - Room-temperature ionic liquids (RTILs) are being increasingly employed as novel solvents in several fields, including chemical engineering, electrochemistry, and synthetic chemistry. To further increase their usage potential, a better understanding of the structure of their surface layer is essential. Bi-layering at the surfaces of RTILs consisting of 1-alkyl-3-methylimidazolium ([Cnmim]+;n= 4, 6, 8, 10, and 12) cations and bis(trifluoromethanesulfonyl)amide ([TFSA]−) anions was demonstratedviainfrared-visible sum-frequency generation (IV-SFG) vibrational spectroscopy and molecular dynamics (MD) simulations. It was found that the sum-frequency (SF) signal from the [TFSA]−anions decreases as the alkyl chain length increases, whereas the SF signal from the r+mode (the terminal CH3group) of the [Cnmim]+cations is almost the same regardless of chain length. MD simulations show the formation of a bi-layered structure consisting of the outermost first layer and a submerged second layer in a “head-to-head” molecular arrangement. The decrease in the SF signals of the normal modes of the [TFSA]−anions is caused by destructive and out-of-phase interference of vibrations of corresponding molecular moieties oriented toward each other in the first and second layers. In contrast, the r+mode of [Cnmim]+does not experience destructive interference because the peak position of the r+mode differs marginally at the surface and in the bulk. Our conclusions are not limited to the system presented here. Similar bi-layered structures can be expected for the surfaces of conventional RTILs, which necessitates the consideration of bi-layering in the design and application.
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U2 - 10.1039/d0cp01219j
DO - 10.1039/d0cp01219j
M3 - Article
C2 - 32452479
AN - SCOPUS:85086347011
SN - 1463-9076
VL - 22
SP - 12565
EP - 12576
JO - Physical Chemistry Chemical Physics
JF - Physical Chemistry Chemical Physics
IS - 22
ER -