{"status":"ok","message-type":"work","message-version":"1.0.0","message":{"indexed":{"date-parts":[[2022,3,30]],"date-time":"2022-03-30T01:10:38Z","timestamp":1648602638682},"reference-count":8,"publisher":"World Scientific Pub Co Pte Lt","issue":"08n10","content-domain":{"domain":[],"crossmark-restriction":false},"short-container-title":["Int. J. Mod. Phys. D"],"published-print":{"date-parts":[[2010,8]]},"abstract":"<jats:p> An effective Lagrangian for quark pairing in nonlinear chromodielectric models (CDM) is derived in the leading order. The effective pairing coupling depends explicitly on the confinement field, \u03c7, of the CDM manifesting a confinement effect on color superconductivity. The self-consistent gap equations are constructed and solved for the color-flavor locked phase. The pairing coupling, for the quartic \u03c7 potential used in the calculations, is inversely proportional to the second power of the \u03c7 field and to the \u03c7 mass squared. In the chiral solution the quarks do not pair, but in the chiral breaking solution, where \u03c7 is small and the effective pairing interaction is stronger, it does show pairing. Our results indicate that the vector channel of the gap is weaker than the scalar one. <\/jats:p>","DOI":"10.1142\/s0218271810017792","type":"journal-article","created":{"date-parts":[[2010,8,26]],"date-time":"2010-08-26T20:54:39Z","timestamp":1282856079000},"page":"1737-1741","source":"Crossref","is-referenced-by-count":0,"title":["THE EFFECT OF CONFINEMENT ON THE CFL QUARK PAIRING IN THE CHROMODIELECTRIC MODEL"],"prefix":"10.1142","volume":"19","author":[{"given":"S. M.","family":"DE CARVALHO","sequence":"first","affiliation":[{"name":"Departamento de F\u00edsica, Instituto Tecnol\u00f3gico de Aeron\u00e1utica, S\u00e3o Jos\u00e9 dos Campos, SP, Brazil"}]},{"given":"M.","family":"MALHEIRO","sequence":"additional","affiliation":[{"name":"Departamento de F\u00edsica, Instituto Tecnol\u00f3gico de Aeron\u00e1utica, S\u00e3o Jos\u00e9 dos Campos, SP, Brazil"}]},{"given":"T.","family":"FREDERICO","sequence":"additional","affiliation":[{"name":"Departamento de F\u00edsica, Instituto Tecnol\u00f3gico de Aeron\u00e1utica, S\u00e3o Jos\u00e9 dos Campos, SP, Brazil"}]},{"given":"B. V.","family":"CARLSON","sequence":"additional","affiliation":[{"name":"Departamento de F\u00edsica, Instituto Tecnol\u00f3gico de Aeron\u00e1utica, S\u00e3o Jos\u00e9 dos Campos, SP, Brazil"}]},{"given":"M.","family":"FIOLHAIS","sequence":"additional","affiliation":[{"name":"Departamento F\u00edsica and Centro de F\u00edsica Computacional, Universidade Coimbra, P-3004-516 Coimbra, Portugal"}]},{"given":"N.","family":"SCOCCOLA","sequence":"additional","affiliation":[{"name":"CONICET, Rivadavia 1917, (1033) Buenos Aires, Argentina"},{"name":"Physics Department, Comisi\u00f3n National de Energia Atomica, Buenos Aires, Argentina"},{"name":"Universidad Favaloro, Sol\u00eds 453, (1078) Buenos Aires, Argentina"}]},{"given":"A. G.","family":"GRUNFELD","sequence":"additional","affiliation":[{"name":"CONICET, Rivadavia 1917, (1033) Buenos Aires, Argentina"},{"name":"Department of Physics, Sultan Qaboos University, P. O. Box: 36 Al-Khode 123 Muscat, Oman"}]}],"member":"219","published-online":{"date-parts":[[2012,1,25]]},"reference":[{"key":"rf1","doi-asserted-by":"publisher","DOI":"10.1016\/0146-6410(92)90003-K"},{"key":"rf2","doi-asserted-by":"publisher","DOI":"10.1088\/0954-3899\/29\/6\/307"},{"key":"rf3","doi-asserted-by":"publisher","DOI":"10.1103\/RevModPhys.80.1455"},{"key":"rf4","doi-asserted-by":"publisher","DOI":"10.1016\/j.nuclphysa.2007.03.095"},{"key":"rf5","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevD.70.074026"},{"key":"rf6","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevC.56.3097"},{"key":"rf8","first-page":"505","volume":"34","author":"Gorkov L. P.","journal-title":"Sov. Phys. J. Exp. Theor. Phys."},{"key":"rf9","doi-asserted-by":"publisher","DOI":"10.1016\/0375-9474(95)00076-D"}],"container-title":["International Journal of Modern Physics D"],"original-title":[],"language":"en","link":[{"URL":"https:\/\/www.worldscientific.com\/doi\/pdf\/10.1142\/S0218271810017792","content-type":"unspecified","content-version":"vor","intended-application":"similarity-checking"}],"deposited":{"date-parts":[[2019,8,7]],"date-time":"2019-08-07T10:39:47Z","timestamp":1565174387000},"score":1,"resource":{"primary":{"URL":"https:\/\/www.worldscientific.com\/doi\/abs\/10.1142\/S0218271810017792"}},"subtitle":[],"short-title":[],"issued":{"date-parts":[[2010,8]]},"references-count":8,"journal-issue":{"issue":"08n10","published-online":{"date-parts":[[2012,1,25]]},"published-print":{"date-parts":[[2010,8]]}},"alternative-id":["10.1142\/S0218271810017792"],"URL":"https:\/\/doi.org\/10.1142\/s0218271810017792","relation":{},"ISSN":["0218-2718","1793-6594"],"issn-type":[{"value":"0218-2718","type":"print"},{"value":"1793-6594","type":"electronic"}],"subject":[],"published":{"date-parts":[[2010,8]]}}}