dc.contributor.author |
Metaxas, D |
en |
dc.date.accessioned |
2014-03-01T01:19:01Z |
|
dc.date.available |
2014-03-01T01:19:01Z |
|
dc.date.issued |
2003 |
en |
dc.identifier.issn |
0295-5075 |
en |
dc.identifier.uri |
https://dspace.lib.ntua.gr/xmlui/handle/123456789/15329 |
|
dc.subject |
Effective Action |
en |
dc.subject |
Finite Temperature |
en |
dc.subject |
Gauge Invariance |
en |
dc.subject |
Lorentz Invariance |
en |
dc.subject |
Hard Thermal Loop |
en |
dc.subject.classification |
Physics, Multidisciplinary |
en |
dc.subject.other |
QUARK-GLUON PLASMA |
en |
dc.subject.other |
TEMPERATURE |
en |
dc.title |
Hard thermal loops with a background plasma velocity |
en |
heal.type |
journalArticle |
en |
heal.identifier.primary |
10.1209/epl/i2003-00113-x |
en |
heal.identifier.secondary |
http://dx.doi.org/10.1209/epl/i2003-00113-x |
en |
heal.language |
English |
en |
heal.publicationDate |
2003 |
en |
heal.abstract |
I consider the calculation of the two- and three-point functions for QED at finite temperature in the presence of a background plasma velocity. The final expressions are consistent with Lorentz invariance, gauge invariance and current conservation, pointing to a straightforward generalization of the hard-thermal-loop formalism to this physical situation. I also give the resulting expression for the effective action and identify the various terms. |
en |
heal.publisher |
E D P SCIENCES |
en |
heal.journalName |
Europhysics Letters |
en |
dc.identifier.doi |
10.1209/epl/i2003-00113-x |
en |
dc.identifier.isi |
ISI:000181080600004 |
en |
dc.identifier.volume |
61 |
en |
dc.identifier.issue |
5 |
en |
dc.identifier.spage |
599 |
en |
dc.identifier.epage |
605 |
en |