{ "id": "0907.2413", "version": "v1", "published": "2009-07-14T17:19:51.000Z", "updated": "2009-07-14T17:19:51.000Z", "title": "Collapse of the random phase approximation: examples and counter-examples from the shell model", "authors": [ "Calvin W. Johnson", "Ionel Stetcu" ], "comment": "8 pages, 7 figures", "journal": "Phys.Rev.C80:024320,2009", "doi": "10.1103/PhysRevC.80.024320", "categories": [ "nucl-th" ], "abstract": "The Hartree-Fock approximation to the many-fermion problem can break exact symmetries, and in some cases by changing a parameter in the interaction one can drive the Hartree-Fock minimum from a symmetry-breaking state to a symmetry-conserving state (also referred to as a ``phase transition'' in the literature). The order of the transition is important when one applies the random phase approximation (RPA) to the of the Hartree-Fock wavefunction: if first order, RPA is stable through the transition, but if second-order, then the RPA amplitudes become large and lead to unphysical results. The latter is known as ``collapse'' of the RPA. While the difference between first- and second-order transitions in the RPA was first pointed out by Thouless, we present for the first time non-trivial examples of both first- and second-order transitions in a uniform model, the interacting shell-model, where we can compare to exact numerical results.", "revisions": [ { "version": "v1", "updated": "2009-07-14T17:19:51.000Z" } ], "analyses": { "subjects": [ "21.60.Cs", "21.60.Jz" ], "keywords": [ "random phase approximation", "shell model", "first time non-trivial examples", "second-order transitions", "counter-examples" ], "tags": [ "journal article" ], "publication": { "publisher": "APS", "journal": "Physical Review C", "year": 2009, "month": "Aug", "volume": 80, "number": 2, "pages": "024320" }, "note": { "typesetting": "TeX", "pages": 8, "language": "en", "license": "arXiv", "status": "editable", "inspire": 825654, "adsabs": "2009PhRvC..80b4320J" } } }