F L structure function and heavy quark contributions

2009 ◽  
Vol 194 (1-3) ◽  
pp. 341-345 ◽  
Author(s):  
Ali N. Khorramian ◽  
S. Atashbar Tehrani ◽  
M. Soleymaninia ◽  
S. Batebi
EXA/LEAP 2008 ◽  
2009 ◽  
pp. 689-693
Author(s):  
Ali N. Khorramian ◽  
S. Atashbar Tehrani ◽  
M. Soleymaninia ◽  
S. Batebi

2017 ◽  
Vol 32 (33) ◽  
pp. 1750197 ◽  
Author(s):  
G. R. Boroun ◽  
B. Rezaei ◽  
S. Heidari

The nucleon and nuclear longitudinal structure functions are determined by the Kharzeev–Levin–Nardin (KLN) model of the low-[Formula: see text] gluon distribution. The behavior of the gluon distribution ratio [Formula: see text] and the ratio [Formula: see text] in [Formula: see text] processes are shown in this paper. The heavy longitudinal structure function ratios in [Formula: see text] processes at the LHeC region are discussed. Heavy contributions to the ratio of the total longitudinal structure function are considerable and should not be neglected especially at smaller [Formula: see text] of the LHeC project. In the KLN model, the new geometrical scaling for transition from the linear to nonlinear regions in accordance with the LHeC processes is used, whose results intensively depended on the heavy quark mass effect.


2006 ◽  
Vol 755 (1-3) ◽  
pp. 272-285 ◽  
Author(s):  
J. Blümlein ◽  
A. De Freitas ◽  
W.L. van Neerven ◽  
S. Klein

2004 ◽  
Vol 135 ◽  
pp. 56-60
Author(s):  
H. Kawamura ◽  
J. Kodaira ◽  
K. Tanaka

2018 ◽  
Vol 175 ◽  
pp. 13006 ◽  
Author(s):  
Shoji Hashimoto ◽  
Brian Colquhoun ◽  
Taku Izubuchi ◽  
Takashi Kaneko ◽  
Hiroshi Ohki

First-principle lattice calculation of inclusive B meson semileptonic decays is possible for a certain class of moments that is connected to the structure function at unphysical kinematics by analytic continuation. We present an exploratory lattice calculation and a comparison with the heavy quark expansion technique.


2009 ◽  
Vol 186 ◽  
pp. 379-382 ◽  
Author(s):  
Ali N. Khorramian ◽  
S. Atashbar Tehrani ◽  
A. Mirjalili

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