A. Zee, Quantum Field Theory in a Nutshell · Problem VI.7.2

Field Theory Redux

Physics — QFT

Problem

As another example from the literature on disorder, consider the following problem. Place NN points randomly in a DD-dimensional Euclidean space of volume VV. Denote the locations of the points by x⃗i\vec{x}_i (i=1,…,N)(i = 1, \ldots, N). Let f(x⃗)=(−)∫dDk(2π)Deik⃗⋅x⃗k2+m2f(\vec{x}) = (-)\int \frac{d^D k}{(2\pi)^D} \frac{e^{i \vec{k} \cdot \vec{x}}}{k^2 + m^2}. Consider the NN by NN matrix Hij=f(x⃗i−x⃗j)H_{ij} = f(\vec{x}_i - \vec{x}_j). Calculate ρ(E)\rho(E), the density of eigenvalues of HH, averaged over the ensemble of matrices, in the limit N→∞N \to \infty, V→∞V \to \infty, with the density of points ρe=N/V\rho_e = N/V (not to be confused with ρ(E)\rho(E) of course) held fixed. [Hint: Use the replica method and arrive at the field theory action S(ϕ)=∫dDx[∑a=1n(∣∇ϕa∣2+m2∣ϕa∣2)−ρee−(1/z)∑a=1n∣ϕa∣2]S(\phi) = \int d^D x \left[ \sum_{a=1}^n (|\nabla \phi_a|^2 + m^2 |\phi_a|^2) - \rho_e e^{-(1/z) \sum_{a=1}^n |\phi_a|^2} \right]. This problem is not entirely trivial; if you need help consult M. M\'ezard et al., Nucl. Phys. B559: 689, 2000, cond-mat/9906135.]

Browse the problem library