| dc.contributor.author |
Phan, Hong Lien |
|
| dc.date.accessioned |
2011-04-20T03:23:08Z |
|
| dc.date.available |
2011-04-20T03:23:08Z |
|
| dc.date.issued |
2008 |
|
| dc.identifier.citation |
VNU Journal of Science, Mathematics - Physics 24 (2008) 145-154 |
vi |
| dc.identifier.issn |
0866-8612 |
|
| dc.identifier.uri |
http://hdl.handle.net/123456789/844 |
|
| dc.description |
VNU Journal of Science, Mathematics - Physics. Vol. 24 (2008), No 3 (M.P), P. 145-154 |
vi |
| dc.description.abstract |
Within the framework of the Walecka model (QHD-I)[1] the renormalized effective
Dirac equation and the kinetic equation for fermion are presented. In fact, the fermion propa-
gator in the medium is dramatically different from that in the vacuum. The main feature is the
treating of the fermion distribution in non equilibrium, which depends on the interaction rate
involving temperature. |
vi |
| dc.language.iso |
en |
vi |
| dc.publisher |
ĐHQGHN |
vi |
| dc.subject |
field Theory |
vi |
| dc.subject |
nuclear Theory |
vi |
| dc.title |
Quantum kinetic equation in the quantum hadrondynamics (QHD-I) model |
vi |
| dc.type |
Article |
vi |