{
  "id": "1805.00079",
  "version": "v1",
  "published": "2018-04-30T19:59:35.000Z",
  "updated": "2018-04-30T19:59:35.000Z",
  "title": "Coherence, entanglement and quantumness in closed and open systems with conserved charge, with an application to many-body localisation",
  "authors": [
    "Katarzyna Macieszczak",
    "Emanuele Levi",
    "Tommaso Macrì",
    "Igor Lesanovsky",
    "Juan P. Garrahan"
  ],
  "comment": "28 pages, 11 figures",
  "categories": [
    "cond-mat.stat-mech",
    "cond-mat.dis-nn",
    "cond-mat.quant-gas",
    "quant-ph"
  ],
  "abstract": "The usefulness of a quantum system as a sensor is given by the quantum Fisher information (QFI) which quantifies the sensitivity of its quantum states to perturbations. In particular, for unitary perturbations useful quantum states are necessarily coherent. Quantum enhanced sensing with many-body states relies on multipartite entanglement (MPE), and therefore QFI is used as an entanglement witness. Here we show that for systems with a fixed local charge (for example fixed density) the connection between QFI and MPE simplifies. In this case, QFI can become a faithful witness of MPE, as a consequence of the emerging direct relation between MPE and coherence in a quantum state, and coherence (as quantified by relative entropy) becomes a faithful upper bound for the relative entropy MPE. When the local charge is not fixed but conserved, QFI becomes a faithful witness of multipartite quantum discord (i.e. quantumness) and coherence becomes its faithful upper bound. Analogously, we show how the bipartite entanglement (BPE) of a fixed-charge state can be witnessed by the QFI related to unitary perturbations of the bipartition, while the corresponding block coherence (i.e., charge asymmetry between partitions) serves as a lower bound on BPE of formation. As estimating QFI is difficult for mixed states of open quantum systems, we adapt a recently introduced protocol that measures QFI of pure states and provides a lower bound for the QFI in open systems. When conservation laws are present, this lower bound can also be a faithful witness of MPE, and furthermore a lower bound of a BPE measure. We illustrate these general results with an application to the problem of detecting the growth of entanglement in a many-body localised system with and without dissipation.",
  "revisions": [
    {
      "version": "v1",
      "updated": "2018-04-30T19:59:35.000Z"
    }
  ],
  "analyses": {
    "keywords": [
      "open systems",
      "many-body localisation",
      "lower bound",
      "entanglement",
      "conserved charge"
    ],
    "note": {
      "typesetting": "TeX",
      "pages": 28,
      "language": "en",
      "license": "arXiv",
      "status": "editable"
    }
  }
}