English

On maximal multiplicities for Hamiltonians with separable variables

Combinatorics 2019-08-09 v1 Mathematical Physics Functional Analysis math.MP

Abstract

For N:=N{0}\mathbb N^*:=\mathbb N \setminus \{0\}, we consider the collection M(N)\mathfrak M(N) of all the NN rows, for which, for n=1,,Nn=1,\cdots,N, the nthn-th row consists of an increasing sequence (ajn)j(a_j^n)_j of real numbers. For AM(N)\mathfrak A \in \mathfrak M(N), we define its spectrum σ(A)\sigma(\mathfrak A) by σ(A)={λR    λ=n=1Najnn},\sigma(\mathfrak A)=\{\lambda\in \mathbb R \;|\; \lambda=\sum_{n=1}^Na_{j_n}^n\}\,, where (j1,j2,,jN)(N)N(j_1,j_2,\dots,j_N)\in (\mathbb N^*)^N. This spectrum is discrete and consists of an infinite sequence that can be ordered as a strictly increasing sequence λk(A)\lambda_k(\mathfrak A). For λσ(A)\lambda \in \sigma (\mathfrak A) we denote by m(λ,A)m(\lambda,\mathfrak A) the number of representations of such a λ\lambda, hence the multiplicity of λ\lambda.\\ In this paper we investigate for given NNN\in \mathbb N^* and kNk\in \mathbb N^* the highest possible multiplicity (denoted by mk(N)\mathfrak m_k(N)) of λk(A)\lambda_k(\mathfrak A) for AM(N)\mathfrak A \in \mathfrak M(N). We give the exact result for N=2N=2 and for N=3N=3 prove a lower bound which appears, according to numerical experiments, as a "good" conjecture. For the general case, we give examples demonstrating that the problem is quite difficult. \\ This problem is equivalent to the analogue eigenvalue multiplicity questions for Schr\"odinger operators describing a system of N non-interacting one-dimensional particles.

Keywords

Cite

@article{arxiv.1908.02752,
  title  = {On maximal multiplicities for Hamiltonians with separable variables},
  author = {B. Helffer and T. Hoffmann-Ostenhof and P. Marquetand},
  journal= {arXiv preprint arXiv:1908.02752},
  year   = {2019}
}
R2 v1 2026-06-23T10:42:19.974Z