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NSR database version of April 26, 2024.

Search: Author = Y.Kucuk

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2022DA12      Eur.Phys.J. A 58, 85 (2022)

H.Dapo, Y.Kucuk, I.Boztosun

A realistic numerical treatment of Coulomb potential in comparison with the analytical approximations

doi: 10.1140/epja/s10050-022-00728-4
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2022KU22      Eur.Phys.J. A 58, 97 (2022)

Y.Kucuk, T.K.Zholdybayev, B.Canbula, Zh.Mukan, B.M.Sadykov, M.Nassurlla, K.M.Ismailov, M.B.Yucel, I.Boztosun

A new proton spectra for ^natCu(p, xp) reaction at E_p = 7 and 30 MeV

NUCLEAR REACTIONS Cu(p, xp), E=7, 30 MeV; measured reaction products, Ep, Ip; deduced σ(θ), σ(E). Comparison with theoretical calculations. Isochronous cyclotron U-150M, at the Institute of Nuclear Physics of Kazakhstan.

doi: 10.1140/epja/s10050-022-00740-8
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD8049.

2021KU05      Eur.Phys.J. A 57, 37 (2021)

Y.Kucuk, M.Karakoc, A.Vitturi

The macroscopic analysis of α-α scattering for the population of the monopole "breathing" mode

NUCLEAR REACTIONS ⁴He(α, α'), E=64 MeV; calculated σ(θ) for the inelastic scattering to the "breathing" mode at different values of the normalization coefficients, macroscopic form factor. Comparison with available data.

doi: 10.1140/epja/s10050-021-00362-6
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2021KU12      Eur.Phys.J. A 57, 87 (2021)

Y.Kucuk, V.Guimaraes, B.V.Carlson

Towards a systematic optical model potential for A = 8 projectiles

NUCLEAR STRUCTURE ⁸B, ⁸Li, ⁸He; analyzed available data; deduced potential set using a Woods-Saxon potential shape; calculated σ(θ).

doi: 10.1140/epja/s10050-021-00405-y
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2021NA14      Eur.Phys.J. A 57, 231 (2021)

M.Nassurlla, N.Burtebayev, B.K.Karakozov, S.B.Sakuta, I.Boztosun, N.Amangeldi, A.K.Morzabayev, G.Yergaliuly, D.K.Alimov, J.Burtebayeva, M.Nassurlla, B.Mauyey, Y.Kucuk, Sh.Hamada, A.Sabidolda, R.Khojayev

New measurements and analysis of elastic scattering of ¹³C by ⁹Be nuclei in a wide energy range

NUCLEAR REACTIONS ⁹Be(¹³C, ¹³C), E=16.25, 19.5, 22.75, 28.12, 36.15, 57.77, 72.88 MeV; measured reaction products; deduced σ, σ(θ). OM and DWBA method, FRESCO program.

doi: 10.1140/epja/s10050-021-00539-z
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2020BE05      Phys.Rev.Lett. 124, 132301 (2020)

Carl.A.Bertulani, Y.Kucuk, R.Lozeva

Fission of Relativistic Nuclei with Fragment Excitation and Reorientation

NUCLEAR REACTIONS ²⁰⁸Pb(²³⁸U, F), E=1 GeV/nucleon; analyzed available data; calculated fission and fragmentation σ in relativistic heavy ion collisions.

doi: 10.1103/PhysRevLett.124.132301
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2020KU04      Nucl.Phys. A994, 121665 (2020)

Y.Kucuk, A.Soylu, L.C.Chamon

Role of the dynamical polarization potential in explaining the α+¹²C system at low energies

doi: 10.1016/j.nuclphysa.2019.121665
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2020MU03      Acta Phys.Pol. B51, 783 (2020)

Y.Mukhamejanov, G.Alieva, D.Alimov, G.D.Kabdrakhimova, M.Nassurlla, N.Saduyev, B.M.Sadykov, T.K.Zholdybayev, K.M.Ismailov, Y.Kucuk

Investigation of (p, xp) and (p, xα) Reactions of 30-MeV Protons with the ¹⁰3Rh Nucleus

doi: 10.5506/APhysPolB.51.783
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD8020.

2018KU02      Turk.J.Phys. 42, 33 (2018)

Y.Kucuk

Surface effect in explaining the elastic scattering of the α + ¹²C system at low energies

NUCLEAR REACTIONS ¹²C(α, α), E=13-172.5 MeV; analyzed available data; calculated σ(θ); deduced optical model parameters.

doi: 10.3906/fiz-1706-22
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2016KU07      Eur.Phys.J. A 52, 98 (2016)

Y.Kucuk, E.Aciksoz

Target-charge dependence of the breakup coupling effects in the elastic scattering of ⁸B

NUCLEAR REACTIONS ²⁷Al(⁸B, ⁸B), E=16.0, 22.0 MeV;⁴⁰Ca(⁸B, ⁸B), E=21.0, 26.5 MeV;⁵⁸Ni(⁸B, ⁸B), E=26.0, 31.2 MeV;¹²⁰Sn(⁸B, ⁸B), E=37.8 MeV; ²⁰⁸Pb(⁸B, ⁸B), E=54 MeV; calculated full σ(θ) and breakup σ(θ) using full coupling and no-coupling CDCC; deduced specific features of Coulomb-nuclear interface for proton halo nuclei.

doi: 10.1140/epja/i2016-16098-9
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2014KU05      Phys.Rev. C 89, 034607 (2014)

Y.Kucuk, J.A.Tostevin

Intermediate-energy four-body breakup calculations for ²²C

NUCLEAR REACTIONS ¹²C(²²C, X), E=300 MeV/nucleon; calculated reaction σ, point-nucleon matter rms radii, three-body binding energy, n+²⁰C 2_s1/2 virtual state scattering length. Four-body (three-body projectile plus target) reaction model calculations using fast adiabatic approximation with and without eikonal approximation for Borromean ²⁰C+n+n three-body interpretation for ²²C. Comparison with Glauber few-body model calculations, and with experimental data.

doi: 10.1103/PhysRevC.89.034607
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2014KU09      Nucl.Phys. A927, 195 (2014)

Y.Kucuk

Folding model analysis of the ⁶He elastic scattering using No-core Shell model: Indication of the breakup threshold anomal

NUCLEAR REACTIONS ¹²C(⁶He, ⁶He), E=5.9, 8.79, 9.18, 9.9, 18.0, 229.0, 249.6 MeV;²⁷Al(⁶He, ⁶He), E=9.5, 11.0, 12.0, 13.4 MeV;⁵⁸Ni(⁶He, ⁶He), E=9.0, 10.0 MeV;⁶⁴Zn(⁶He, ⁶He), E=10.0, 13.6 MeV;⁶⁵Cu(⁶He, ⁶He), E=19.5, 22.6, 30.0 MeV;¹⁹⁷Au(⁶He, ⁶He), E=27.0, 29.0, 40.0 MeV;²⁰⁸Pb(⁶He, ⁶He), E=14.0, 16.0, 18.0, 22.0, 27.0 MeV;²⁰⁹Bi(⁶He, ⁶He), E=17.8, 19.0, 22.5 MeV; calculated σ(θ) using new version of NCSM (no-core shell model); deduced potential parameters. Results compared with data and with global potential calculations.

doi: 10.1016/j.nuclphysa.2014.04.020
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2014UN04      Phys.Rev. C 89, 057605 (2014)

A.Un, Y.Kucuk, T.Caner, I.Boztosun

Role of the surface potential in explaining the ¹¹Li+²⁸Si system

NUCLEAR REACTIONS ²⁸Si(¹¹Li, ¹¹Li), E=29 MeV/nucleon; analyzed elastic and quasielastic σ(θ) data in the framework of the coupled-channels model using double-folding potential with a Woods-Saxon type of imaginary part, and modified shape of the real and imaginary potentials simultaneously in the surface region.

doi: 10.1103/PhysRevC.89.057605
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2012KU25      Phys.Rev. C 86, 034601 (2012)

Y.Kucuk, A.M.Moro

Exclusive breakup of ¹⁷F on ⁵⁸Ni and ²⁰⁸Pb within the continuum-discretized coupled-channels method

NUCLEAR REACTIONS ⁵⁸Ni, ²⁰⁸Pb(¹⁷F, ¹⁷F), (¹⁷F, X), E=10, 65 MeV/nucleon; calculated elastic σ(θ), differential and integrated breakup σ, σ(θ) angular distribution of protons and ¹⁶O fragments following the ¹⁷F dissociation, effect of different multipoles, role of Coulomb and nuclear couplings in the breakup cross sections. Continuum-discretized coupled-channels (CDCC) method, assuming ¹⁶O+p model for the projectile. Comparison with recent experimental data.

doi: 10.1103/PhysRevC.86.034601
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2012KU37      J.Phys.:Conf.Ser. 381, 012109 (2012)

Y.Kucuk, J.A.Tostevin

Three-body-model calculations for ²²C

NUCLEAR REACTIONS ¹²C(²²C, X), E=300 MeV/nucleon; calculated σ using different three-body model wave functions.

NUCLEAR STRUCTURE ²²C; calculated ground-state wavefunction using three-body model code EFADDY. Discussed four-body model.

doi: 10.1088/1742-6596/381/1/012109
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2010AY08      Nucl.Phys. A848, 245 (2010)

M.Aygun, Y.Kucuk, I.Boztosun, Awad A.Ibraheem

Microscopic few-body and Gaussian-shaped density distributions for the analysis of the ⁶He exotic nucleus with different target nuclei

NUCLEAR REACTIONS ¹²C(⁶He, ⁶He), E=5.9, 9.9 MeV; ²⁷Al(⁶He, ⁶He), E=9.5, 11, 12, 13.4 MeV; ⁵⁸Ni(⁶He, ⁶He), E=9, 10 MeV; ⁶⁴Zn(⁶He, ⁶He), E=10, 13.6 MeV; ⁶⁵Cu(⁶He, ⁶He), E=19.5, 30 MeV; ¹⁹⁷Au(⁶He, ⁶He), E=27, 29, 40 MeV; ²⁰⁸Pb(⁶He, ⁶He), E=14, 16, 18, 22, 27 MeV; ²⁰⁹Bi(⁶He, ⁶He), E=16.25, 17.8, 19, 22.01, 22.5 MeV; calculated σ(θ) using few body and Gaussian density distributions within a double-folding model. Comparison with data.

doi: 10.1016/j.nuclphysa.2010.09.005
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2009KU11      Phys.Rev. C 79, 067601 (2009)

Y.Kucuk, I.Boztosun, N.Keeley

Onset of nuclear structure effects in near-barrier elastic scattering of weakly bound nuclei: ⁶He and ⁶Li compared

NUCLEAR REACTIONS ⁵⁸Ni(⁶He, ⁶He), E=11.0, 16.0 MeV; ²⁰⁸Pb(⁶He, ⁶He), (⁶Li, ⁶Li), E=22.0, 33.0 MeV; ⁵⁸Ni(⁶Li, ⁶Li), E not given; ¹²⁰Sn, ¹⁴⁴Sm, ¹⁸¹Ta(⁶He, ⁶He), (⁶Li, ⁶Li), E not given; calculated σ(θ) using continuum discretized coupled channels calculations. Comparison with experimental data.

doi: 10.1103/PhysRevC.79.067601
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2009KU25      Phys.Rev. C 80, 054602 (2009)

Y.Kucuk, I.Boztosun, T.Topel

Global optical potential for the elastic scattering of ⁶He at low energies

NUCLEAR REACTIONS ¹²C(⁶He, ⁶He), E=8.79, 9.18, 18.0 MeV; ²⁷Al(⁶He, ⁶He), E=9.5, 11.0, 12.0, 13.4 MeV; ⁵⁸Ni(⁶He, ⁶He), E=9.0 MeV; ⁶⁴Zn(⁶He, ⁶He), E=10.0 MeV; ⁶⁵Cu(⁶He, ⁶He), E=22.6 MeV; ¹⁹⁷Au(⁶He, ⁶He), E=27.0, 29, 40.0 MeV; ²⁰⁸Pb(⁶He, ⁶He), E=14.0, 16.0, 18.0, 22.0, 27.0 MeV; ²⁰⁹Bi(⁶He, ⁶He), E=14.7, 16.3, 17.8, 19.0, 22.5 MeV; analyzed elastic scattering σ and angular distributions using optical model analysis; deduced global optical model potential parameters. Comparison with experimental data.

doi: 10.1103/PhysRevC.80.054602
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2008BO19      Phys.Rev. C 77, 064608 (2008)

I.Boztosun, M.Karakoc, Y.Kucuk

Microscopic double folding potential description of the ⁶He+¹²C reaction

NUCLEAR REACTIONS ¹²C(⁶He, ⁶He), (⁶He, ⁶He'), (⁶He, α), E=18.0 MeV; calculated proton and neutron density distributions, real and imaginary potentials and deformations, σ. Coupled-channel Born approximation. Comparison with experimental data.

doi: 10.1103/PhysRevC.77.064608
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2006KU06      Nucl.Phys. A764, 160 (2006)

Y.Kucuk, I.Boztosun

Global examination of the ¹²C + ¹²C reaction data at low and intermediate energies

NUCLEAR REACTIONS ¹²C(¹²C, ¹²C), E=32-70.7 MeV; analyzed σ(θ, E). Coupled channels and optical models compared.

doi: 10.1016/j.nuclphysa.2005.09.013
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2005ER05      J.Phys.(London) G31, S1837 (2005)

S.Erturk, I.Boztosun, Y.Kucuk, M.Karakoc, S.Aydin

Failure of the standard coupled-channels method in describing inelastic reaction data: on the use of a new shape for the coupling potential

NUCLEAR REACTIONS ¹²C(¹²C, ¹²C), (¹²C, ¹²C'), E=73.4, 93.8, 126.7 MeV; analyzed σ(θ); deduced coupling potential features.

doi: 10.1088/0954-3899/31/10/083
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