@article {417,
	title = {Mechanism of Fast Proton Transport along One-Dimensional Water Chains Confined in Carbon Nanotubes},
	journal = {J. Am. Chem. Soc.},
	volume = {132},
	year = {2010},
	pages = {11395{\textendash}11397},
	doi = {10.1021/ja1046704},
	author = {Cao, Z. and Peng, Y. and T. Yan and Li, S. and Li, A. and G. A. Voth}
}
@article {720,
	title = {Structure of the Liquid-Vacuum Interface of Room-Temperature Ionic Liquids:  A Molecular Dynamics Study},
	journal = {J Phys Chem B},
	volume = {110},
	number = {4},
	year = {2006},
	note = {Yan, Tianying Li, Shu Jiang, Wei Gao, Xueping Xiang, Bing Voth, Gregory A United States The journal of physical chemistry. B J Phys Chem B. 2006 Feb 2;110(4):1800-6.},
	pages = {1800-6},
	abstract = {<p>Molecular dynamics simulations for the liquid-vacuum interface of the ionic liquid 1-ethyl-3-methylimidazolium nitrate (EMIM+/NO3-) were performed for both electronically polarizable and nonpolarizable potential energy surfaces. The interfacial structural properties, such as the oscillation in the number density profile, the orientational ordering, and the local clustering in the interfacial region, were calculated. The simulations with both the polarizable and nonpolarizable model demonstrate the existence of an inhomogeneous interfacial structure normal to the surface layer. It was found for both models that the ethyl tail group on EMIM+ is likely to protrude outward from the surface. In the outmost surface layer, the cation is likely to lie on the surface with the imidazolium ring parallel to the interface, while there is a second region with enhanced density from that in the bulk where the cation preferably slants with the imidazolium ring tending to be perpendicular to the surface. The results also reveal that the electronic polarization effect is important for the ionic liquid interface. It is found that the cation is likely to be segregated at the ionic liquid surface for the polarizable model, while for the nonpolarizable model, the anion is found to be more likely to exhibit such behavior. The surface tension of the polarizable model (58.5 +/- 0.5 mN/m) is much smaller than that of the nonpolarizable model (82.7 +/- 0.6 mN/m), in better agreement with extrapolated experimental measurements on similar ionic liquid systems.</p>},
	doi = {10.1021/jp055890p},
	author = {T. Yan and Li, S. and Jiang, W. and Gao, X. and Xiang, B. and G. A. Voth}
}
