Umebayashi Yasuhiro, Mitsugi Takushi, Fukuda Shuhei, Fujimori Takao, Fujii Kenta, Kanzaki Ryo, Takeuchi Munetaka, Ishiguro Shin-Ichi
Department of Chemistry, Faculty of Science, Kyushu University, Hakozaki, Higashi-ku, Fukuoka, 812-8581, Japan.
J Phys Chem B. 2007 Nov 15;111(45):13028-32. doi: 10.1021/jp076869m. Epub 2007 Oct 19.
The solvation structure of the lithium ion in room-temperature ionic liquids 1-ethyl-3-methylimidazolium bis(trifluoromethanesulfonyl) imide (EMI(+)TFSI(-)) and N-butyl-N-methylpyrrolidinium bis(trifluoromethanesulfonyl) imide (BMP(+0TFSI(-)) has been studied by Raman spectroscopy and DFT calculations. Raman spectra of EMI(+)TFSI(-) and BMP(+)TFSI(-) containing Li(+)TFSI(-) over the range 0.144-0.589 and 0.076-0.633 mol dm(-3), respectively, were measured at 298 K. A strong 744 cm-1 band of the free TFSI(-) ion in the bulk weakens with increasing concentration of the lithium ion, and it revealed by analyzing the intensity decrease that the two TFSI(-) ions bind to the metal ion. The lithium ion may be four-coordinated through the O atoms of two bidentate TFSI(-) ions. It has been established in our previous work that the TFSI(-) ion involves two conformers of C(1) (cis) and C(2) (trans) symmetries in equilibrium, and the dipole moment of the C(1) conformer is significantly larger than that of the C(2) conformer. On the basis of these facts, the geometries and SCF energies of possible solvate ion clusters Li(C(1)-TFSI(-))(2), Li(C(1)-TFSI(-))(C(2)-TFSI(-)), and Li(C(2)-TFSI(-))(2) were examined using the theoretical DFT calculations. It is concluded that the C(1) conformer is more preferred to the C(2) conformer in the vicinity of the lithium ion.
通过拉曼光谱和密度泛函理论(DFT)计算研究了锂离子在室温离子液体1-乙基-3-甲基咪唑双(三氟甲磺酰)亚胺(EMI(+)TFSI(-))和N-丁基-N-甲基吡咯烷双(三氟甲磺酰)亚胺(BMP(+0TFSI(-))中的溶剂化结构。分别在0.144 - 0.589和0.076 - 0.633 mol dm(-3)范围内,于298 K下测量了含有Li(+)TFSI(-)的EMI(+)TFSI(-)和BMP(+)TFSI(-)的拉曼光谱。本体中自由TFSI(-)离子的744 cm-1强峰随着锂离子浓度的增加而减弱,通过分析强度降低表明两个TFSI(-)离子与金属离子结合。锂离子可能通过两个双齿TFSI(-)离子的O原子形成四配位。在我们之前的工作中已经确定,TFSI(-)离子涉及处于平衡状态的C(1)(顺式)和C(2)(反式)对称的两种构象,并且C(1)构象的偶极矩明显大于C(2)构象。基于这些事实,使用理论DFT计算研究了可能的溶剂化离子簇Li(C(1)-TFSI(-))(2)、Li(C(1)-TFSI(-))(C(2)-TFSI(-))和Li(C(2)-TFSI(-))(2)的几何结构和自洽场能量。得出的结论是,在锂离子附近,C(1)构象比C(2)构象更受青睐。