J. Hansen and I. R. Mcdonald, Theory of Simple Liquids, Adv. Chem. Phys, vol.139, issue.1, 2008.

M. Mézard and G. Parisi, A tentative replica study of the glass transition, Journal of Physics A: Mathematical and General, vol.29, issue.20, pp.6515-1076, 1996.
DOI : 10.1088/0305-4470/29/20/009

B. Coluzzi, G. Parisi, and P. Verrochio, Lennard-Jones binary mixture: A thermodynamical approach to glass transition, The Journal of Chemical Physics, vol.31, issue.6, p.2933, 2000.
DOI : 10.1080/00268979809483145

URL : http://arxiv.org/abs/cond-mat/9904124

S. Franz and G. Parisi, Effective potential in glassy systems: theory and simulations, Physica A: Statistical Mechanics and its Applications, vol.261, issue.3-4, p.317, 1998.
DOI : 10.1016/S0378-4371(98)00315-X

URL : http://arxiv.org/abs/cond-mat/9711215

F. J. Rogers and D. A. Young, New, thermodynamically consistent, integral equation for simple fluids, Physical Review A, vol.30, issue.2, p.999, 1984.
DOI : 10.1103/PhysRevA.30.999

M. J. Gillan, A new method of solving the liquid structure integral equations, Molecular Physics, vol.38, issue.6, p.1781, 1979.
DOI : 10.1016/0031-8914(64)90054-0

N. P. Bailey, U. R. Pedersen, N. Gnan, T. B. Schroder, and J. C. Dyre, Pressure-energy correlations in liquids. I. Results from computer simulations, The Journal of Chemical Physics, vol.129, issue.18, p.184507, 2008.
DOI : 10.1021/ja00334a030

Y. Singh, J. P. Stoessel, and P. G. Wolynes, Hard-Sphere Glass and the Density-Functional Theory of Aperiodic Crystals, Physical Review Letters, vol.54, issue.10, p.1059, 1985.
DOI : 10.1103/PhysRevLett.54.1059

G. Zerah and J. Hansen, Self???consistent integral equations for fluid pair distribution functions: Another attempt, The Journal of Chemical Physics, vol.54, issue.4, p.2336, 1986.
DOI : 10.1098/rspa.1964.0233

D. M. Duh and D. Henderson, Integral equation theory for Lennard???Jones fluids: The bridge function and applications to pure fluids and mixtures, The Journal of Chemical Physics, vol.104, issue.17, p.6742, 1996.
DOI : 10.1080/00268977200100031