000062006 001__ 62006
000062006 005__ 20170907131843.0
000062006 0247_ $$2doi$$a10.1016/j.nuclphysb.2010.11.004
000062006 0248_ $$2sideral$$a72550
000062006 037__ $$aART-2011-72550
000062006 041__ $$aeng
000062006 100__ $$aAguado, M.
000062006 245__ $$aTheta-vacuum and large N limit in CPN-1   models
000062006 260__ $$c2011
000062006 5060_ $$aAccess copy available to the general public$$fUnrestricted
000062006 5203_ $$aThe ¿ dependence of the vacuum energy density in models is re-analysed in the semiclassical approach, the expansion and arguments based on the nodal structure of vacuum wavefunctionals. The expansion is shown not to be in contradiction with instanton physics at finite (spacetime) volume V. The interplay of large volume V and large N parameter gives rise to two regimes with different ¿ dependence, one behaving as a dilute instanton gas and the other dominated by the traditional large N picture, where instantons reappear as resonances of the one-loop effective action, even in the absence of regular instantonic solutions. The realms of the two regimes are given in terms of the mass gap m by and , respectively. The small volume regime is relevant for physical effects associated to the physics of the boundary, like the leading rôle of edge states in the quantum Hall effect, which, however, do not play any rôle in the thermodynamic limit at large N. Depending on the order in which the limits and are taken, two different theories are obtained; this is the hallmark of a phase transition at .
000062006 536__ $$9info:eu-repo/grantAgreement/ES/DGA/E24-2$$9info:eu-repo/grantAgreement/ES/MICINN/FPA2009-09638
000062006 540__ $$9info:eu-repo/semantics/openAccess$$aby$$uhttp://creativecommons.org/licenses/by/3.0/es/
000062006 590__ $$a4.661$$b2011
000062006 591__ $$aPHYSICS, PARTICLES & FIELDS$$b5 / 27 = 0.185$$c2011$$dQ1$$eT1
000062006 655_4 $$ainfo:eu-repo/semantics/article$$vinfo:eu-repo/semantics/publishedVersion
000062006 700__ $$0(orcid)0000-0003-3669-6241$$aAsorey, M.$$uUniversidad de Zaragoza
000062006 7102_ $$12004$$2405$$aUniversidad de Zaragoza$$bDepartamento de Física Teórica$$cFísica Teórica
000062006 773__ $$g844, 2 (2011), 243-265$$pNucl. phys., B$$tNUCLEAR PHYSICS B$$x0550-3213
000062006 8564_ $$s294691$$uhttps://zaguan.unizar.es/record/62006/files/texto_completo.pdf$$yVersión publicada
000062006 8564_ $$s57017$$uhttps://zaguan.unizar.es/record/62006/files/texto_completo.jpg?subformat=icon$$xicon$$yVersión publicada
000062006 909CO $$ooai:zaguan.unizar.es:62006$$particulos$$pdriver
000062006 951__ $$a2017-09-07-09:54:46
000062006 980__ $$aARTICLE