dc.contributor.author |
Cornwall, JM |
en |
dc.contributor.author |
Tiktopoulos, G |
en |
dc.date.accessioned |
2014-03-01T01:06:31Z |
|
dc.date.available |
2014-03-01T01:06:31Z |
|
dc.date.issued |
1986 |
en |
dc.identifier.issn |
0370-2693 |
en |
dc.identifier.uri |
https://dspace.lib.ntua.gr/xmlui/handle/123456789/9433 |
|
dc.relation.uri |
http://www.scopus.com/inward/record.url?eid=2-s2.0-0001767626&partnerID=40&md5=0d22d64a0dd0f2d24048a6576ecbadd7 |
en |
dc.subject.classification |
Physics, Multidisciplinary |
en |
dc.title |
Three-dimensional gauge configurations and their properties in QCD |
en |
heal.type |
journalArticle |
en |
heal.language |
English |
en |
heal.publicationDate |
1986 |
en |
heal.abstract |
Two important properties are discussed of three-dimensional gauge-field configurations which are expected to arise in QCD, beyond the classical level, as a vacuum condensate. First, these configurations have fermion zero modes normalizable in three dimensions, which are responsible for chiral symmetry breakdown. Second, they form a natural dynamical realization of the semi-infinite branch line which necessarily begins on any localized gauge configuration with fractional topological charge. Other properties of these configurations (e.g., as glueballs) are briefly mentioned. © 1986. |
en |
heal.publisher |
ELSEVIER SCIENCE BV |
en |
heal.journalName |
Physics Letters B |
en |
dc.identifier.isi |
ISI:A1986F162300035 |
en |
dc.identifier.volume |
181 |
en |
dc.identifier.issue |
3-4 |
en |
dc.identifier.spage |
353 |
en |
dc.identifier.epage |
358 |
en |