{ "id": "1404.0968", "version": "v1", "published": "2014-04-03T15:28:35.000Z", "updated": "2014-04-03T15:28:35.000Z", "title": "Distributional approach to point interactions in one-dimensional quantum mechanics", "authors": [ "Marcos Calçada", "José T. Lunardi", "Luiz A. Manzoni", "Wagner Monteiro" ], "comment": "Open Access link: http://journal.frontiersin.org/Journal/10.3389/fphy.2014.00023/abstract", "journal": "Frontiers in Physics 2:23 (2014)", "doi": "10.3389/fphy.2014.00023", "categories": [ "quant-ph", "hep-th", "math-ph", "math.MP" ], "abstract": "We consider the one-dimensional quantum mechanical problem of defining interactions concentrated at a single point in the framework of the theory of distributions. The often ill-defined product which describes the interaction term in the Schr\\\"odinger and Dirac equations is replaced by a well-defined distribution satisfying some simple mathematical conditions and, in addition, the physical requirement of probability current conservation is imposed. A four-parameter family of interactions thus emerges as the most general point interaction both in the non-relativistic and in the relativistic theories (in agreement with results obtained by self-adjoint extensions). Since the interaction is given explicitly, the distributional method allows one to carry out symmetry investigations in a simple way, and it proves to be useful to clarify some ambiguities related to the so-called $\\delta^\\prime$ interaction.", "revisions": [ { "version": "v1", "updated": "2014-04-03T15:28:35.000Z" } ], "analyses": { "keywords": [ "one-dimensional quantum mechanics", "distributional approach", "one-dimensional quantum mechanical problem", "probability current conservation", "general point interaction" ], "tags": [ "journal article" ], "publication": { "journal": "Frontiers in Physics", "year": 2014, "month": "Apr", "volume": 2, "pages": 23 }, "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable", "inspire": 1288529, "adsabs": "2014FrP.....2...23C" } } }