Bi-layering at ionic liquid surfaces: a sum-frequency generation vibrational spectroscopy- and molecular dynamics simulation-based study

被引:14
作者
Iwahashi, Takashi [1 ]
Ishiyama, Tatsuya [2 ]
Sakai, Yasunari [1 ]
Morita, Akihiro [3 ,4 ]
Kim, Doseok [5 ]
Ouchi, Yukio [1 ]
机构
[1] Tokyo Inst Technol, Sch Mat & Chem Technol, Dept Mat Sci & Engn, Meguro Ku, Tokyo 1528552, Japan
[2] Univ Toyama, Dept Environm Appl Chem, Fac Engn, Toyama, Toyama 9308555, Japan
[3] Tohoku Univ, Grad Sch Sci, Dept Chem, Aoba Ku, Sendai, Miyagi 9808578, Japan
[4] Kyoto Univ, Elements Strategy Initiat Catalysts & Batteries E, Kyoto 6158520, Japan
[5] Sogang Univ, Dept Phys, Seoul 04107, South Korea
基金
新加坡国家研究基金会;
关键词
PARTICLE MESH EWALD; AIR/LIQUID INTERFACE; ALKYL CHAIN; TEMPERATURE; HYSTERESIS; ANION; WATER; RAMAN;
D O I
10.1039/d0cp01219j
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
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 ([C(n)mim](+);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 CH(3)group) of the [C(n)mim](+)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 [C(n)mim](+)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.
引用
收藏
页码:12565 / 12576
页数:12
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