scholarly journals Zγγproduction with leptonic decays and triple photon production at next-to-leading order QCD

2011 ◽  
Vol 84 (7) ◽  
Author(s):  
G. Bozzi ◽  
F. Campanario ◽  
M. Rauch ◽  
D. Zeppenfeld
2012 ◽  
Vol 86 (3) ◽  
Author(s):  
Zhang Shi-Ming ◽  
Zhang Ren-You ◽  
Ma Wen-Gan ◽  
Guo Lei

1996 ◽  
Vol 54 (11) ◽  
pp. 7081-7081 ◽  
Author(s):  
A. P. Contogouris ◽  
B. Kamal ◽  
Z. Merebashvili ◽  
F. V. Tkachov

1993 ◽  
Vol 48 (9) ◽  
pp. 4092-4102 ◽  
Author(s):  
A. P. Contogouris ◽  
B. Kamal ◽  
Z. Merebashvili ◽  
F. V. Tkachov

2007 ◽  
Vol 16 (07n08) ◽  
pp. 2350-2355 ◽  
Author(s):  
GUANG-YOU QIN ◽  
CHARLES GALE ◽  
ABHIJIT MAJUMDER

A new channel of direct photon production from a quark gluon plasma (QGP) is explored in the framework of high-temperature QCD. This process appears at next-to-leading order, in the presence of a charge asymmetry in the excited matter. The photon production rate from this new mechanism is suppressed compared to the QCD annihilation and Compton scattering at low baryon density but assumes importance in baryon-rich matter.


2011 ◽  
Vol 83 (11) ◽  
Author(s):  
G. Bozzi ◽  
F. Campanario ◽  
M. Rauch ◽  
D. Zeppenfeld

2008 ◽  
Vol 17 (03) ◽  
pp. 519-530
Author(s):  
SHASHANK BHATNAGAR

Two photon decays of pion are studied in the framework of the Bethe–Salpeter equation under Covariant Instantaneous Ansatz where the structure of hadron-quark vertex function Γ is generalized to include various Dirac covariants (other than γ5) from their complete set. These covariants are incorporated in accordance with a power counting rule (which was recently employed to calculate leptonic decays constants of pseudoscalar mesons and vector mesons) order by order in powers of the inverse of the meson mass. Pion-photon coupling constant Fπ is calculated with the incorporation of leading order covariants.


2004 ◽  
Vol 19 (01) ◽  
pp. 149-158 ◽  
Author(s):  
NIKOLAOS KIDONAKIS ◽  
J. F. OWENS

Previous work on soft-gluon resummation for direct photon production is extended to include additional subleading logarithmic terms through [Formula: see text] and some representative comparisons are made to experimental results from the E-706 and UA-6 Collaborations. The additional terms are small in magnitude, indicating good convergence properties to the level of accuracy calculated. The scale dependence remains much smaller than that of the next-to-leading-order calculation.


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