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NSR database version of May 19, 2024.

Search: Author = A.Mirjalili

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2021SH32      Nucl.Phys. A1015, 122303 (2021)

J.Sheibani, R.Gharaei, A.Mirjalili, K.Javidan

Heavy-ion fusion cross sections in the barrier and high-energy regions: Signature of energy dependence in the repulsive core potential

NUCLEAR REACTIONS ²⁴⁸Cm(²⁸Mg, X), ²³⁸U(³⁶S, X), ²⁰⁸Pb(⁴⁸Ca, X), ²⁰⁹Bi(⁵⁰Ti, X), ²³⁸U(⁴⁰Ca, X), (⁴⁸Ca, X), E=190-240 MeV; analyzed available data; deduced effect of incompressibility of cold nuclear matter (CNM) on the high-energy fusion data.

doi: 10.1016/j.nuclphysa.2021.122303
Citations: PlumX Metrics

2020MO02      Nucl.Phys. A993, 121643 (2020)

M.Mottaghizadeh, A.Mirjalili

The impact of QED corrections on heavy quarks structure functions at LHC energies, within the xFitter framework

doi: 10.1016/j.nuclphysa.2019.121643
Citations: PlumX Metrics

2018SH34      Phys.Rev. C 98, 045211 (2018)

J.Sheibani, A.Mirjalili, S.A.Tehrani

EMC effect in the next-to-leading order approximation based on the Laplace transformation

NUCLEAR REACTIONS ²H, ⁴He, ¹²C, ⁴⁰Ca, ⁵⁶Fe(μ, X) at Q²=4 GeV²; calculated nuclear structure functions through an analytical solution using Laplace transformation for the DGLAP evolution equation at the next-to-leading order of perturbative QCD; deduced separate nuclear parton distributions for all parton including valence quark densities, the anti-quark and strange sea parton distribution functions (PDFs), and gluon distributions. Phenomenological quark models.

doi: 10.1103/PhysRevC.98.045211
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2017KH04      Phys.Rev. C 95, 035201 (2017)

H.Khanpour, A.Mirjalili, S.A.Tehrani

Analytic derivation of the next-to-leading order proton structure function F^p₂ (x, Q²) based on the Laplace transformation

doi: 10.1103/PhysRevC.95.035201
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2012MI19      Eur.Phys.J. A 47, 71 (2012); Erratum Eur.Phys.J. A 48, 106 (2012)

A.Mirjalili, M.M.Yazdanpanah

Target mass correction on the ³He polarized structure function

NUCLEAR STRUCTURE ³He; calculated polarized structure function using convolution of the light cone momentum distribution and target-mass correction. Polarized proton structure function compared with data.

doi: 10.1140/epja/i2012-12071-0
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2009YA22      Nucl.Phys. A831, 243 (2009)

M.M.Yazdanpanah, A.Mirjalili, S.A.Tehrani, F.Taghavi-Shahri

³He and ³H polarized structure functions, using the constituent quark model

NUCLEAR STRUCTURE ³H, ³He; calculated polarized structure functions using the constituent quark model. Comparison with data.

doi: 10.1016/j.nuclphysa.2009.10.080
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2007KH01      Nucl.Phys. B(Proc.Supp.) S164, 34 (2007)

A.N.Khorramian, S.A.Tehrani, A.Mirjalili

Non-singlet structure function in the NNLO approximation

doi: 10.1016/j.nuclphysbps.2006.11.109
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2007MI08      Nucl.Phys. B(Proc.Supp.) S167, 34 (2007)

A.Mirjalili, A.N.Khorramian, S.A.Tehrani

QCD analysis of heavy quarks production in hadronic collisions

NUCLEAR REACTIONS ¹H(p-bar, X), E(cm)=1.8 TeV; analyzed heavy quark production σ. Complete renormalization group improvement.

doi: 10.1016/j.nuclphysbps.2006.12.040
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2007TE01      Nucl.Phys. B(Proc.Supp.) S164, 30 (2007)

S.A.Tehrani, A.Mirjalili, A.N.Khorramian

EMC effect and nuclear structure functions

NUCLEAR STRUCTURE ⁴He, ¹²C, ⁴⁰Ca; analyzed structure function ratios, related data.

doi: 10.1016/j.nuclphysbps.2006.11.092
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2006MI12      Nucl.Phys. B(Proc.Supp.) S152, 136 (2006)

A.Mirjalili, A.N.Khorramian, S.A.Tehrani

Analysis of b(b-bar) production in proton-antiproton collisions, using the approach of complete RG-improvement

doi: 10.1016/j.nuclphysbps.2005.08.025
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