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Anderson localisation for an interacting two-particle quantum system on \mathbb Z

2007/05/04 by Victor Chulaevsky, Chulaevsky, Victor, Yuri Suhov +1
Computer Science · Mathematics · Physics and Astronomy · #Advanced Mathematical Modeling in Engineering #FOS: Physical sciences #Mathematical Physics (math-ph) #Quantum chaos and dynamical systems #Spectral Theory in Mathematical Physics #math-ph #math.MP

paper · pdf · doi:10.48550/arxiv.0705.0657

38 pages; main results have been reported earlier on international conferences

arxiv created 2007/05/04 · openalex publication_date 2007/05/04 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/28

Abstract

We study spectral properties of a system of two quantum particles on an integer lattice with a bounded short-range two-body interaction, in an external random potential field V(x,ω) with independent, identically distributed values. The main result is that if the common probability density f of random variables V(x,ω) is analytic in a strip around the real line and the amplitude constant g is large enough (i.e. the system is at high disorder), then, with probability one, the spectrum of the two-particle lattice Schroedinger operator H(ω) (bosonic or fermionic) is pure point, and all eigen-functions decay exponentially. The proof given in this paper is based on a refinement of a multiscale analysis (MSA) scheme proposed by von Dreifus and Klein, adapted to incorporate lattice systems with interaction.

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