dc.contributor.author |
Gersdorff, G |
en |
dc.contributor.author |
Irges, N |
en |
dc.contributor.author |
Quirós, M |
en |
dc.date.accessioned |
2014-03-01T01:52:51Z |
|
dc.date.available |
2014-03-01T01:52:51Z |
|
dc.date.issued |
2003 |
en |
dc.identifier.uri |
https://dspace.lib.ntua.gr/xmlui/handle/123456789/26745 |
|
dc.subject |
Fixed Point |
en |
dc.subject |
Gauge Field |
en |
dc.subject |
Gauge Invariance |
en |
dc.subject |
Gauge Theory |
en |
dc.subject |
Space Time |
en |
dc.title |
Radiative brane-mass terms in D>5 orbifold gauge theories |
en |
heal.type |
journalArticle |
en |
heal.identifier.primary |
10.1016/S0370-2693(02)03039-3 |
en |
heal.identifier.secondary |
http://dx.doi.org/10.1016/S0370-2693(02)03039-3 |
en |
heal.publicationDate |
2003 |
en |
heal.abstract |
A gauge theory with gauge group G defined in D>4 space–time dimensions can be broken to a subgroup H on four-dimensional fixed point branes, when compactified on an orbifold. Mass terms for extra-dimensional components of gauge fields Ai (brane scalars) might acquire (when allowed by the brane symmetries) quadratically divergent radiative masses and thus jeopardize the stability of the four-dimensional |
en |
heal.journalName |
Physics Letters B |
en |
dc.identifier.doi |
10.1016/S0370-2693(02)03039-3 |
en |