Analytic Derivation of the Longitudinal Proton Structure Function FL(x, Q2) and the Reduced Cross Section σr(x, Q2) at the Leading Order and the Next-to-leading Order Approximations
We present a set of formulas to extract the longitudinal proton structure function F L ( x , Q 2 ) and the reduced cross section σ r ( x , Q 2 ) by using Dokshitzer–Gribov–Lipatov–Altarelli–Parisi (DGLAP) evolution equations and Altarelli-Martinelli equation at the leading order (LO) and the next-to...
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Published in | International journal of theoretical physics Vol. 60; no. 10; pp. 3822 - 3849 |
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Main Authors | , |
Format | Journal Article |
Language | English |
Published |
New York
Springer US
01.10.2021
Springer Nature B.V |
Subjects | |
Online Access | Get full text |
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Summary: | We present a set of formulas to extract the longitudinal proton structure function
F
L
(
x
,
Q
2
) and the reduced cross section
σ
r
(
x
,
Q
2
) by using Dokshitzer–Gribov–Lipatov–Altarelli–Parisi (DGLAP) evolution equations and Altarelli-Martinelli equation at the leading order (LO) and the next-to-leading order (NLO) approximations in perturbative quantum chromodynamics (QCD). These formulas are obtained by the Laplace transform method at the virtualities higher than
Q
0
2
. We show that, the obtained equations for
F
L
and
σ
r
depend only on the parton distribution functions (PDF’s) at the initial scale
Q
0
2
. We obtain the corresponding numerical results in a range of the virtuality
Q
0
2
≤
Q
2
≤
800
G
e
V
2
and Bjorken scale 10
− 4
≤
x
≤ 1 and compare them with the results achieved by MSTW2008 (Martin et al. Eur. Phys. J
63
(2), 189–285,
2009
), WT (White and Thorne Phy. Rev. D
75
(3), 034005,
2007
) and Dipole (b-Sat) model (H. Kowalski, L. Motyka, G. Watt, Phys. Rev. D
74
(7), 074016,
2006
) predictions and also with data released by the Hadron Electron Ring Accelerator (HERA). Our numerical results show an acceptable agreement with the deep inelastic scattering (DIS) experimental data throughout over a wide range of the Bjorken scale
x
and the virtuality
Q
2
, and then can be applied in analyses of the Large Hadron Collider and Future Circular Collider projects. |
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ISSN: | 0020-7748 1572-9575 |
DOI: | 10.1007/s10773-021-04947-1 |