{ "id": "nucl-th/0304084", "version": "v2", "published": "2003-04-30T08:51:26.000Z", "updated": "2003-06-30T12:29:50.000Z", "title": "The 2p-2h electromagnetic response in the quasielastic peak and beyond", "authors": [ "A. De Pace", "M. Nardi", "W. M. Alberico", "T. W. Donnelly", "A. Molinari" ], "comment": "27 pages, 12 figures, revtex4; minor modifications in the discussion of the results, references added", "journal": "Nucl.Phys. A726 (2003) 303-326", "doi": "10.1016/S0375-9474(03)01625-7", "categories": [ "nucl-th" ], "abstract": "The contribution to the nuclear transverse response function R_T arising from two particle-two hole (2p-2h) states excited through the action of electromagnetic meson exchange currents (MEC) is computed in a fully relativistic framework. The MEC considered are those carried by the pion and by Delta degrees of freedom, the latter being viewed as a virtual nucleonic resonance. The calculation is performed in the relativistic Fermi gas model in which Lorentz covariance can be maintained. All 2p-2h many-body diagrams containing two pionic lines that contribute to R_T are taken into account and the relative impact of the various components of the MEC on R_T is addressed. The non-relativistic limit of the MEC contributions is also discussed and compared with the relativistic results to explore the role played by relativity in obtaining the 2p-2h nuclear response.", "revisions": [ { "version": "v2", "updated": "2003-06-30T12:29:50.000Z" } ], "analyses": { "subjects": [ "25.30.Rw", "24.30.Gd", "24.10.Jv" ], "keywords": [ "2p-2h electromagnetic response", "quasielastic peak", "nuclear transverse response function", "electromagnetic meson exchange currents", "relativistic fermi gas model" ], "tags": [ "journal article" ], "publication": { "publisher": "Elsevier", "journal": "Nucl. Phys. A" }, "note": { "typesetting": "RevTeX", "pages": 27, "language": "en", "license": "arXiv", "status": "editable", "inspire": 617908 } } }