Classical Particle in a Box with Random Potential: exploiting rotational symmetry of replicated Hamiltonian
arXiv:cond-mat/0610035 · doi:10.1016/j.nuclphysb.2006.11.029
Abstract
We investigate thermodynamics of a single classical particle placed in a spherical box of a finite radius and subject to a superposition of a dimensional Gaussian random potential and the parabolic potential with the curvature . Earlier solutions of version of this model were based on combining the replica trick with the Gaussian Variational Ansatz (GVA) for free energy, and revealed a possibility of a glassy phase at low temperatures. For a general , we show how to utilize instead the underlying rotational symmetry of the replicated partition function and to arrive to a compact expression for the free energy in the limit directly, without any need for intermediate variational approximations. This method reveals striking similarity with the much-studied spherical model of spin glasses. Depending on the value of and the three types of disorder - short-ranged, long-ranged, and logarithmic - the phase diagram of the system in the plane undergoes considerable modifications. In the limit of infinite confinement radius our analysis confirms all previous results obtained by GVA.
46 pages, 4 figures; This version corrects a few more typos discovered in the published version
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