{ "id": "2006.15465", "version": "v1", "published": "2020-06-27T23:22:24.000Z", "updated": "2020-06-27T23:22:24.000Z", "title": "Dirty bosons on the Cayley tree: Bose-Einstein condensation versus ergodicity breaking", "authors": [ "Maxime Dupont", "Nicolas Laflorencie", "Gabriel LemariƩ" ], "comment": "21 pages, 16 figures", "categories": [ "cond-mat.dis-nn", "cond-mat.str-el" ], "abstract": "Building on large-scale quantum Monte Carlo simulations, we investigate the zero-temperature phase diagram of hard-core bosons in a random potential on site-centered Cayley trees with branching number $K=2$. In order to follow how the Bose-Einstein condensate (BEC) is affected by the disorder, we focus on both the zero-momentum density, probing the quantum coherence, and the one-body density matrix (1BDM) whose largest eigenvalue monitors the off-diagonal long-range order. We further study its associated eigenstate which brings useful information about the real-space properties of this leading eigenmode. Upon increasing randomness, we find that the system undergoes a quantum phase transition at finite disorder strength between a long-range ordered BEC state, fully ergodic at large scale, and a new disordered Bose glass regime showing conventional localization for the coherence fraction while the 1BDM displays a non-trivial algebraic vanishing BEC density together with a non-ergodic occupation in real-space. These peculiar properties can be analytically captured by a simple toy-model on the Cayley tree which provides a physical picture of the Bose glass regime.", "revisions": [ { "version": "v1", "updated": "2020-06-27T23:22:24.000Z" } ], "analyses": { "keywords": [ "cayley tree", "bose-einstein condensation", "dirty bosons", "algebraic vanishing bec density", "glass regime showing conventional" ], "note": { "typesetting": "TeX", "pages": 21, "language": "en", "license": "arXiv", "status": "editable" } } }