{ "id": "1403.7771", "version": "v2", "published": "2014-03-30T15:15:57.000Z", "updated": "2014-08-04T14:47:38.000Z", "title": "Resonance chains in open systems, generalized zeta functions and clustering of the length spectrum", "authors": [ "Sonja Barkhofen", "Frédéric Faure", "Tobias Weich" ], "journal": "Nonlinearity 27 (2014) 1829-1858", "categories": [ "math-ph", "cond-mat.mes-hall", "math.DS", "math.MP", "math.SP" ], "abstract": "In many non-integrable open systems in physics and mathematics resonances have been found to be surprisingly ordered along curved lines in the complex plane. In this article we provide a unifying approach to these resonance chains by generalizing dynamical zeta functions. By means of a detailed numerical study we show that these generalized zeta functions explain the mechanism that creates the chains of quantum resonance and classical Ruelle resonances for 3-disk systems as well as geometric resonances on Schottky surfaces. We also present a direct system-intrinsic definition of the continuous lines on which the resonances are strung together as a projection of an analytic variety. Additionally, this approach shows that the existence of resonance chains is directly related to a clustering of the classical length spectrum on multiples of a base length. Finally, this link is used to construct new examples where several different structures of resonance chains coexist.", "revisions": [ { "version": "v2", "updated": "2014-08-04T14:47:38.000Z" } ], "analyses": { "subjects": [ "35P25", "47A40", "58J50", "81Q50", "81Q05" ], "keywords": [ "open systems", "clustering", "resonance chains coexist", "direct system-intrinsic definition", "generalized zeta functions explain" ], "tags": [ "journal article" ], "publication": { "doi": "10.1088/0951-7715/27/8/1829", "journal": "Nonlinearity", "year": 2014, "month": "Aug", "volume": 27, "number": 8, "pages": 1829 }, "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2014Nonli..27.1829B" } } }