dc.contributor.author |
Alexandre, J |
en |
dc.contributor.author |
Farakos, K |
en |
dc.contributor.author |
Koutsoumbas, G |
en |
dc.date.accessioned |
2014-03-01T01:49:28Z |
|
dc.date.available |
2014-03-01T01:49:28Z |
|
dc.date.issued |
2000 |
en |
dc.identifier.uri |
https://dspace.lib.ntua.gr/xmlui/handle/123456789/25793 |
|
dc.subject |
Finite Temperature |
en |
dc.subject |
Magnetic Field |
en |
dc.subject |
Phase Diagram |
en |
dc.subject |
schwinger dyson equation |
en |
dc.subject |
Strong Magnetic Field |
en |
dc.subject |
The Critical Temperature |
en |
dc.title |
Magnetic catalysis in QED_3 at finite temperature: beyond the constant mass approximation |
en |
heal.type |
journalArticle |
en |
heal.identifier.primary |
10.1103/PhysRevD.63.065015 |
en |
heal.identifier.secondary |
http://dx.doi.org/10.1103/PhysRevD.63.065015 |
en |
heal.publicationDate |
2000 |
en |
heal.abstract |
We solve the Schwinger-Dyson equations for (2+1)-dimensional QED in thepresence of a strong external magnetic field. The calculation is done at finitetemperature and the fermionic self energy is not supposed to bemomentum-independent, which is the usual simplification in such calculations.The phase diagram in the temperature-magnetic field plane is determined. Forintermediate magnetic fields the critical temperature |
en |
heal.journalName |
Physical Review D |
en |
dc.identifier.doi |
10.1103/PhysRevD.63.065015 |
en |