{ "id": "1211.3578", "version": "v2", "published": "2012-11-15T11:28:49.000Z", "updated": "2014-04-13T06:32:26.000Z", "title": "Chiral Perturbation Theory and the $\\bar B \\bar B$ Strong Interaction", "authors": [ "Zhan-Wei Liu", "Ning Li", "Shi-Lin Zhu" ], "comment": "14 pages, 8 figures, 4 tables; discussion extended, references added, version published in Phys. Rev. D", "journal": "Phys. Rev. D 89, 074015 (2014)", "doi": "10.1103/PhysRevD.89.074015", "categories": [ "hep-ph", "hep-ex", "hep-lat", "nucl-th" ], "abstract": "We have calculated the potentials of the heavy (charmed or bottomed) pseudoscalar mesons up to $O(\\epsilon^2)$ with the heavy meson chiral perturbation theory. We take into account the contributions from the football, triangle, box, and crossed diagrams with the 2$\\phi$ exchange and one-loop corrections to the contact terms. We notice that the total 2$\\phi$-exchange potential alone is attractive in the small momentum region in the channel ${\\bar B \\bar B}^{I=1}$, ${\\bar B_s \\bar B_s}^{I=0}$, or ${\\bar B \\bar B_s}^{I=1/2}$, while repulsive in the channel ${\\bar B \\bar B}^{I=0}$. Hopefully the analytical chiral structures of the potentials may be useful in the extrapolation of the heavy meson interaction from lattice QCD simulation.", "revisions": [ { "version": "v2", "updated": "2014-04-13T06:32:26.000Z" } ], "analyses": { "subjects": [ "12.39.Fe", "14.40.Lb", "34.20.Gj", "14.40.Nd" ], "keywords": [ "strong interaction", "heavy meson chiral perturbation theory", "lattice qcd simulation", "heavy meson interaction", "small momentum region" ], "tags": [ "journal article" ], "publication": { "publisher": "APS", "journal": "Phys. Rev. D" }, "note": { "typesetting": "TeX", "pages": 14, "language": "en", "license": "arXiv", "status": "editable", "inspire": 1202879, "adsabs": "2012arXiv1211.3578L" } } }