scholarly journals Study of small x behaviour of unintegrated gluon distribution constraining gluon evolution in MD-BFKL equation

2019 ◽  
Vol 1330 ◽  
pp. 012017
Author(s):  
P Phukan ◽  
M Lalung ◽  
J K Sarma
2004 ◽  
Vol 742 (1-2) ◽  
pp. 182-252 ◽  
Author(s):  
E. Iancu ◽  
K. Itakura ◽  
D.N. Triantafyllopoulos

2011 ◽  
Vol 705 (1-2) ◽  
pp. 106-111 ◽  
Author(s):  
Fabio Dominguez ◽  
A.H. Mueller ◽  
Stéphane Munier ◽  
Bo-Wen Xiao
Keyword(s):  

2020 ◽  
Vol 72 (2) ◽  
pp. 025201
Author(s):  
Pragyan Phukan ◽  
Madhurjya Lalung ◽  
Jayanta Kumar Sarma
Keyword(s):  

2015 ◽  
Vol 39 ◽  
pp. 1560115
Author(s):  
A. A. Grinyuk ◽  
A. V. Lipatov ◽  
G. I. Lykasov

We study the role of the non-perturbative input to the transverse momentum dependent (TMD) gluon density in hard processes at the LHC. We derive the TMD gluon distribution from the fit of the inclusive hadron spectra measured at low transverse momenta in [Formula: see text] collisions at the LHC and demonstrate that the best description of these spectra for larger hadron transverse momenta can be achieved by matching the derived TMD gluon distribution with the exact solution of the Balitsky-Fadin-Kuraev-Lipatov (BFKL) equation obtained at small transverse momenta outside the saturation region. A special attention is put to the phenomenological applications of presented TMD parton densities to some LHC processes, which are sensitive to the quark and gluon content of a proton.


1993 ◽  
Vol 317 (1-2) ◽  
pp. 200-204 ◽  
Author(s):  
Wei Zhu ◽  
Dali Xue ◽  
Kangmin Chai ◽  
Zaixin Xu
Keyword(s):  

1990 ◽  
Vol 243 (4) ◽  
pp. 421-426 ◽  
Author(s):  
P.N. Harriman ◽  
A.D. Martin ◽  
W.J. Stirling ◽  
R.G. Roberts

2007 ◽  
Vol 22 (02n03) ◽  
pp. 667-671 ◽  
Author(s):  
ANTONI SZCZUREK

I discuss double-diffractive (double-elastic) production of the η′ and ηc mesons in the pp → pXp reaction within the formalism of unintegrated gluon distribution functions (UGDF). The contribution of γ*γ* → η′ fusion is estimated. The distributions in the Feynman xF (or rapidity), transferred four-momenta squared between initial and final protons (t1, t2) and azimuthal angle difference between outgoing protons (Φ) are calculated and discussed. The results are compared with the WA102 data. Predictions at higher energies are presented.


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