English

Complex complex landscapes

Statistical Mechanics 2021-04-28 v2 Disordered Systems and Neural Networks High Energy Physics - Lattice High Energy Physics - Theory Mathematical Physics math.MP

Abstract

We study the saddle-points of the pp-spin model -- the best understood example of a `complex' (rugged) landscape -- when its NN variables are complex. These points are the solutions to a system of NN random equations of degree p1p-1. We solve for N\overline{\mathcal N}, the number of solutions averaged over randomness in the NN\to\infty limit. We find that it saturates the B\'ezout bound logNNlog(p1)\log\overline{\mathcal N}\sim N\log(p-1). The Hessian of each saddle is given by a random matrix of the form CCC^\dagger C, where CC is a complex symmetric Gaussian matrix with a shift to its diagonal. Its spectrum has a transition where a gap develops that generalizes the notion of `threshold level' well-known in the real problem. The results from the real problem are recovered in the limit of real parameters. In this case, only the square-root of the total number of solutions are real. In terms of the complex energy, the solutions are divided into sectors where the saddles have different topological properties.

Keywords

Cite

@article{arxiv.2012.06299,
  title  = {Complex complex landscapes},
  author = {Jaron Kent-Dobias and Jorge Kurchan},
  journal= {arXiv preprint arXiv:2012.06299},
  year   = {2021}
}
R2 v1 2026-06-23T20:54:00.064Z