scholarly journals Hard gluon damping in hot QCD

2004 ◽  
Vol 70 (3) ◽  
Author(s):  
André Peshier
Keyword(s):  

Proceedings ◽  
2019 ◽  
Vol 10 (1) ◽  
pp. 11
Author(s):  
Fabio Dominguez ◽  
Jose Guilherme Milhano ◽  
Carlos A. Salgado ◽  
Konrad Tywoniuk ◽  
Victor Vila

In the first part of this work we study the color coherence phenomenon by considering the well-known quark-antiquark antenna with an in-medium hard gluon emission and an extra very soft emission outside it—double antenna. By discussing the coherence effects in terms of the survival probability, we generalize previous studies of the antenna radiation to the case of more than two emitters. After providing support to the jet quenching picture with effective emitters in the QCD cascade, we present a novel setup of an antenna splitting inside the medium taking into account the finite formation time of the dipole, which turns out to be an important scale. We read into the role of coherence and the relevant time scales which control the scenario, while also providing theoretical support for vacuum-like emissions early in the medium. Finally, by mapping the spectrum of in-medium splittings through the corresponding kinematical Lund diagram, we appreciate regimes of a close correspondence to a semi-classical description.





1999 ◽  
Vol 1999 (07) ◽  
pp. 013-013 ◽  
Author(s):  
Probir Roy ◽  
K Sridhar


1995 ◽  
Vol 10 (19) ◽  
pp. 2799-2818 ◽  
Author(s):  
A.N. MITRA ◽  
ANJU SHARMA

The total width of a [Formula: see text] hadron is modeled by the rate at which it dissociates into a pair of quasifree quarks brought about by “soft” and “hard” gluon exchanges, under the ansatz of a short time zone for the existence of such a state. A crucial ingredient in this regard is the quark’s mass function for which a nonperturbative formula is obtained via dynamical breaking of the chiral symmetry of an input vector-exchange-like four-fermion Lagrangian, facilitated by the knowledge that for a chirally invariant Lagrangian this quantity is also equal to the pion-quark vertex function in the chiral limit (Mπ⇒0). The mass function so employed is based on a Bethe-Salpeter (BS) model with a vectorexchange-like kernel (chirally invariant) which is precalibrated to the spectroscopy of [Formula: see text] and qqq hadrons, and also predicts a value of [Formula: see text] fully consistent with QCD sum rules. The predicted widths show a good overlap with available data from L>1 to J=5, while limitations of phase space resist applicability of the said mechanism due to the onset of hadronic selection rules for certain L≤1 states.



1985 ◽  
Vol 157 (5-6) ◽  
pp. 430-436 ◽  
Author(s):  
F. Herzog ◽  
Z. Kunszt


1981 ◽  
Vol 47 (8) ◽  
pp. 556-560 ◽  
Author(s):  
H. C. Ballagh ◽  
H. H. Bingham ◽  
W. B. Fretter ◽  
T. Lawry ◽  
G. R. Lynch ◽  
...  


1995 ◽  
Vol 348 (1-2) ◽  
pp. 196-200 ◽  
Author(s):  
Bodo Lampe
Keyword(s):  




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