NSR Query Results
Output year order : Descending NSR database version of May 19, 2024. Search: Author = G.R.Boroun Found 21 matches. 2024BO02 Phys.Lett. B 849, 138440 (2024) A simple model for the charm structure function of nuclei
doi: 10.1016/j.physletb.2023.138440
2024BO07 Eur.Phys.J. A 60, (2024) The unintegrated gluon distribution from the GBW and BGK models
doi: 10.1140/epja/s10050-024-01255-0
2023BO03 Phys.Rev. C 107, 025209 (2023) Parametrization of the nuclear structure function NUCLEAR STRUCTURE 12C, 40Ca, 131Xe, 208Pb; calculated nuclear structure function dependence on the scaling variable. Parametrization of the nuclear structure function obtained from the proton experimental data by relying on a Froissart-bounded parametrization of the proton structure function. Comparison with available data from NMC, EMC and E665.
doi: 10.1103/PhysRevC.107.025209
2021BO01 Nucl.Phys. A1006, 122062 (2021) The study of the gluon distribution function and reduced cross section behavior using the proton structure function
doi: 10.1016/j.nuclphysa.2020.122062
2021BO17 Phys.Rev. C 103, 065202 (2021) Color dipole model bounds with the gluon-gluon recombination correction
doi: 10.1103/PhysRevC.103.065202
2021BO19 Eur.Phys.J. A 57, 219 (2021) Physical limits in the color-dipole model bounds
doi: 10.1140/epja/s10050-021-00517-5
2020RE07 Phys.Rev. C 101, 045202 (2020) Color dipole picture and extracting the ratio of structure functions at small x
doi: 10.1103/PhysRevC.101.045202
2020RE15 Eur.Phys.J. A 56, 262 (2020) Longitudinal structure function from the parton parameterization
doi: 10.1140/epja/s10050-020-00267-w
2019BO11 Nucl.Phys. A990, 244 (2019) Ratio of the structure functions and the color dipole model bound
doi: 10.1016/j.nuclphysa.2019.07.011 Get
2019HE05 Nucl.Phys. A986, 195 (2019) S.Heidari, B.Rezaei, J.K.Sarma, G.R.Boroun The non-singlet structure function of light and heavy nuclei up to next-to-leading order analysis at low χ region
doi: 10.1016/j.nuclphysa.2019.03.005
2019RE05 Eur.Phys.J. A 55, 66 (2019) The behavior of the structure function by using the effective exponent at low x
doi: 10.1140/epja/i2019-12734-2
2018BO04 Phys.Rev. C 97, 015206 (2018) Longitudinal structure function from logarithmic slopes of F2 at low x
doi: 10.1103/PhysRevC.97.015206
2016BO15 Nucl.Phys. A953, 21 (2016) G.R.Boroun, S.Zarrin, S.Dadfar Laplace method for the evolution of the fragmentation function of Bc mesons
doi: 10.1016/j.nuclphysa.2016.03.032
2014BO07 Eur.Phys.J. A 50, 69 (2014) Dynamical behavior connection of the gluon distribution and the proton structure function at small x NUCLEAR STRUCTURE 1H; calculated gluon distribution, proton structure function, form factor. Compared to other calculations.
doi: 10.1140/epja/i2014-14069-x
2014BO16 Nucl.Phys. A929, 119 (2014) Geometrical scaling in charm structure function ratios
doi: 10.1016/j.nuclphysa.2014.06.002
2011RE07 Nucl.Phys. A857, 42 (2011) Analytical solution of the longitudinal structure function FL in the leading and next-to-leading-order analysis at low χ with respect to Laguerre polynomials method
doi: 10.1016/j.nuclphysa.2011.03.012
2010BO09 Eur.Phys.J. A 43, 335 (2010) Nonlinear correction to the longitudinal structure function at small x
doi: 10.1140/epja/i2010-10919-9
2009BO29 Eur.Phys.J. A 42, 251 (2009) Shadowing correction to the gluon distribution behavior at small x
doi: 10.1140/epja/i2009-10871-9
2006BO05 Chin.Phys.Lett. 23, 324 (2006) A Solution of the DGLAP Equation for Gluon Distribution as a Function of F2 and dF2/dlnQ2 at Low x: the Next-to-Leading Order Analysis NUCLEAR STRUCTURE A=1; analyzed data; deduced gluon distribution.
doi: 10.1088/0256-307X/23/2/014
2006BO38 Acta Phys.Slovaca 56, 463 (2006) Calculation of the exponent λg(x, t) based on the behavior of steeply rising gluon distribution function at low-x
2002GH01 Phys.Lett. 528B, 239 (2002) Extraction of the Structure Function F2(x, Q2) at Low-x from the Cross Section Derivative NUCLEAR REACTIONS 1H(e, e'X), E=high; analyzed data; deduced structure function F2(x, Q2).
doi: 10.1016/S0370-2693(02)01227-3
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