Structural analysis of [Bmim]2CuCl4 ionic liquids in the presence of water and ethanol by XAFS technique JIANG FangLing1,2, LI Cheng1, FU HaiYing1, Wang YaXing1, GUO XiaoJing1 & WU GuoZhong1,* 1 Shanghai Institute of Applied Physics, Chinese Academy of Sciences, Shanghai 201800, China 2 Graduate University of Chinese Academy of Sciences, Beijing 100049, China Supporting information Computational method The calculations were performed with the Gaussian 09 program using density functional theory (DFT) at B3LYP [1] level with LANL2DZ [2] and 6-311G** [3] basis sets. LANL2DZ basis set is being widely utilized in the investigation on transition metal to calculate the equilibrium geometries of Cu(II) complexes. 6-311G** basis sets were used for chlorine atoms. The frequency calculations were employed to confirm the resulting geometry as minima. XAFS analysis proved the formation of the octahedral configuration compound. And then a series of DFT calculations for these compounds [CuCln(H2O)6-n]2-n (n=1,2,3,4,5) were performed in our work. DFT calculations confirmed the stable structure, which involves two Cu–Cl bonds and four Cu–O bonds, as seen in Figure S1. It was not possible to locate a minimum corresponding to these compounds [CuCln(H2O)6-n]2-n (n=1,3,4,5). Figure S1 Structure of CuCl2(H2O)4, band length: Cu-Cl1 2.32461Å, Cu-Cl2 2.32474 Å, Cu-O1 2.15807Å, Cu-O2 2.28196Å, Cu-O3 2.28155Å, Cu-O4 2.15801 Å; bond angle: Cl1-Cu-Cl2 179.982°, O1-Cu-Cl1 90.278°, O2-Cu-Cl1 89.464°, O1-Cu-O2 92.657°, O2-Cu-O4 87.32436°, O1-Cu-O4 179.921°, O2-Cu-O3 179.855°. [1] Lee C, Yang W, Parr RG, Development of the Colic-Salvetti correlation-energy formula into a functional of the electron density, Phys. Rev. B17 (1988) 785–789. [2] Hay PJ, Wadt WR, Ab initio effective core potentials for molecular calculations. Potentials for the transition metal atoms Sc to Hg, Chem. Phys. 82 (1985) 270–284. [3] Frisch MJ, Trucks GW, Schlegel HB, Scuseria GE, Robb MA, Cheeseman JR, Scalmani G, Barone V, Mennucci B, Petersson GA, Nakatsuji H, Caricato M, Li X, Hratchian HP, Izmaylov AF, Bloino J, Zheng G, Sonnenberg JL, Hada M, Ehara M, Toyota K, Fukuda R, Hasegawa J, Ishida M, Nakajima T, Honda Y, Kitao O, Nakai H, Vreven T, Montgomery JA, Peralta JE, Ogliaro F, Bearpark M, Heyd JJ, Brothers E, Kudin KN, Staroverov VN, Kobayashi R, Normand J, Raghavachari K, Rendell A, Burant JC, Iyengar SS, Tomasi J, Cossi M, Rega N, Millam JM, Klene M, Knox JE, Cross JB, Bakken V, Adamo C, Jaramillo J, Gomperts R, Stratmann RE, Yazyev O, Austin AJ, Cammi R, Pomelli C, Ochterski JW, Martin RL, Morokuma K, Zakrzewski VG, Voth GA, Salvador P, Dannenberg PP, Dapprich S, Daniels AD, Farkas, Foresman JB, Ortiz JV, Cioslowski J and Fox DJ, Gaussian 09, Revision C.01; Gaussian, Inc., Wallingford CT, 2009.