The high-frequency finite-temperature quark dispersion relation

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dc.creatorSeibert, David
dc.date1993-10-07
dc.date.accessioned2026-07-07T05:41:19Z
dc.date.available2026-07-07T05:41:19Z
dc.descriptionI calculate the dispersion relation for quarks of mass $m$ and momentum $k$ in a quark gluon plasma at temperature $T$, in the limit $m^2+k^2 \gg (gT)^2$, where $g$ is the strong coupling constant. I find three contributions to the dispersion relation: one that depends on $T$ but not $m$ or $k$, one that depends on $m$ and $T$ but not $k$, and third contribution that depends on all three (and is opposite in sign to the other two).
dc.descriptionlatex, 5 pages, CERN-TH.7034/93
dc.identifierhttps://arxiv.org/abs/nucl-th/9310008
dc.identifierhttp://arxiv.org/abs/nucl-th/9310008
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/82529
dc.subjectNuclear Theory
dc.subjectHigh Energy Physics - Phenomenology
dc.titleThe high-frequency finite-temperature quark dispersion relation
dc.typetext

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