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NSR database version of April 11, 2024.

Search: Author = M.Karakoc

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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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2020NA30      Chin.Phys.C 44, 104103 (2020)

M.Nassurlla, N.Burtebayev, T.Kh.Sadykov, I.Boztosun, N.Amangeldi, D.Alimov, Z.Kerimkulov, J.Burtebayeva, M.Nassurlla, A.Kurakhmedov, S.B.Sakuta, M.Karakoc, A.A.Ibraheem, K.W.Kemper, S.Hamada

New measurements and reanalysis of 14N elastic scattering on 10B target

NUCLEAR REACTIONS 10B(14N, 14N), E= 38-94.0 MeV; measured reaction products; deduced σ(θ), possible contribution of the α-cluster exchange mechanism, spectroscopic amplitudes using the optical model and the distorted waves Born approximation method.

doi: 10.1088/1674-1137/abab89
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2014BO01      Turk.J.Phys. 38, 1 (2014)

I.Boztosun, H.Dapo, S.F.Ozmen, Y.Cecen, M.Karakoc, A.Coban, A.Cesur, T.Caner, E.Bayram, G.B.Keller, B.Kucuk, A.Guvendi, M.Derman, D.Kaya

The results of the first photonuclear reaction performed in Turkey: the zinc example

RADIOACTIVITY 63,65Zn(EC), 69Zn, 67Cu(β-); measured decay products, Eγ, Iγ; deduced T1/2. Comparison with available data.

doi: 10.3906/fiz-1305-19
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2014KA27      Phys.Rev. C 89, 064313 (2014)

M.Karakoc, R.G.T.Zegers, B.A.Brown, Y.Fujita, T.Adachi, I.Boztosun, H.Fujita, M.Csatlos, J.M.Deaven, C.J.Guess, J.Gulyas, K.Hatanaka, K.Hirota, D.Ishikawa, A.Krasznahorkay, H.Matsubara, R.Meharchand, F.Molina, H.Okamura, H.J.Ong, G.Perdikakis, C.Scholl, Y.Shimbara, G.Susoy, T.Suzuki, A.Tamii, J.H.Thies, J.Zenihiro

Gamow-Teller transitions in the A=40 isoquintet of relevance for neutrino captures in 40Ar

NUCLEAR REACTIONS 40Ar(3He, t), E=140 MeV/nucleon; measured triton spectra, σ using Grand-Raiden spectrometer at RCNP facility. 40K; deduced levels, J, π, B(GT) DWBA analysis. Main focus on 1+ states at 2290 and 2730 keV. Other details to appear in a future publication. 40Ar(p, n)40K; 40Ti(β+), (EC); analyzed previous experimental results, and compared Gamow-Teller B(GT) strengths in all three studies. Comparison with shell-model calculations in the sd-pf shell with a new interaction (WBMB-C) to study differences between structure of transitions from 40Ar and 40Ti. Discussed ratio of the cross sections for low-lying 1+ states populated in 40Ar(p, n) and 40Ar(3He, t) reactions. Relevance of 40Ar in the use of liquid argon as a medium for neutrino detection.

doi: 10.1103/PhysRevC.89.064313
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2014MA26      Acta Phys.Pol. B45, 229 (2014)

J.Marganiec, F.Wamers, F.Aksouh, Y.Aksyutina, H.Alvarez-Pol, T.Aumann, S.Beceiro, C.Bertulani, K.Boretzky, M.J.G.Borge, M.Chartier, A.Chatillon, L.Chulkov, D.Cortina-Gil, I.Egorova, H.Emling, O.Ershova, C.Forssen, L.M.Fraile, H.Fynbo, D.Galaviz, H.Geissel, L.Grigorenko, M.Heil, D.H.H.Hoffmann, J.Hoffmann, H.Johansson, B.Jonson, M.Karakoc, C.Karagiannis, O.Kiselev, J.V.Kratz, R.Kulessa, N.Kurz, C.Langer, M.Lantz, K.Larsson, T.Le Bleis, R.Lemmon, Yu.A.Litvinov, K.Mahata, C.Muntz, T.Nilsson, C.Nociforo, G.Nyman, W.Ott, V.Panin, Yu.Parfenova, S.Paschalis, A.Perea, R.Plag, R.Reifarth, A.Richter, K.Riisager, C.Rodriguez-Tajes, D.Rossi, G.Schrieder, N.Shulgina, H.Simon, J.Stroth, K.Summerer, J.Taylor, O.Tengblad, E.Tengborn, H.Weick, M.Wiescher, C.Wimmer, M.Zhukov

Study of the 15O(2p, γ)17Ne Cross Section by Coulomb Dissociation of 17Ne for the rp Process of Nucleosynthesis

NUCLEAR REACTIONS Pb(17Ne, 2p)15O, E=500 MeV/nucleon; measured reaction products, Eγ, Iγ, Ep, Ip; deduced σ, σ(E), resonances. Comparison with theoretical calculations, R3BROOT package.

doi: 10.5506/APhysPolB.45.229
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2013KA09      Phys.Rev. C 87, 024607 (2013)

M.Karakoc, A.Banu, C.A.Bertulani, L.Trache

Coulomb distortion and medium corrections in nucleon-removal reactions

NUCLEAR REACTIONS 12C, 9Be, 7Li, 4He, 1H(17C, 16B), 12C(23Al, 22Mg), E=35 MeV/nucleon; 12C(23Al, 22Mg), E=50 MeV/nucleon; 12C(17C, 16B), E=100, 200, 400, 800, 1000 MeV/nucleon; 9Be(15O, 14N), E=56 MeV/nucleon; 9Be(11Be, 10Be), E=60 MeV/nucleon; 12C(24O, 23O), E=920 MeV/nucleon; 12C(33Mg, 32Mg), E=898 MeV/nucleon; calculated nucleon removal cross sections, Coulomb scattering effects, shapes and magnitude of longitudinal and transverse momentum distributions with Coulomb corrections, and with medium modifications of nucleon-nucleon interactions. State-of-the-art eikonal method. Comparison with experimental data, including previous experimental data for 12C(p, X), E=20-100 MeV.

doi: 10.1103/PhysRevC.87.024607
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2012BE30      J.Phys.:Conf.Ser. 337, 012007 (2012)

C.A.Bertulani, M.Karakoc

Medium Effects in Reactions with Rare Isotopes

NUCLEAR REACTIONS 9Be(15C, 14C), E=10-500 MeV/nucleon; analyzed data; deduced σ, dσ data of halo neutron knockout. 9Be(14O, 13O), (14O, 13N), E≈50, 300 MeV/nucleon; 9Be(36Ca, 35Ca), (36Ca, 35K), E=70.5, 300 MeV/nucleon; calculated spectroscopic factors using NuShell code, σ using modified MOMDIS code to solve Bethe-Goldstone equation considering medium effects via effective interaction.

doi: 10.1088/1742-6596/337/1/012007
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2010KO07      Phys.Rev. C 81, 024615 (2010)

G.Kocak, M.Karakoc, I.Boztosun, A.B.Balantekin

Effects of α-cluster potentials for the 16O+16O fusion reaction and S factor

NUCLEAR REACTIONS 16O(16O, 16O), E(cm)=2-15 MeV; analyzed σ and S-factors. 16O(16O, 16O), E(cm)=12.5, 14, 15.5, 20.5, 24.5, 29.5 MeV; analyzed σ(θ). Optical model using Woods-Saxon and α-α double folding α-cluster potentials for fusion reactions.

doi: 10.1103/PhysRevC.81.024615
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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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2007KO15      Phys.Atomic Nuclei 70, 290 (2007)

G.Kocak, M.Karakoc, I.Boztosun

Examination of the 16O + 28Si system with microscopic and phenomenological potentials

NUCLEAR REACTIONS 28Si(16O, 16O), E=29-44 MeV; calculated σ(θ). Results for microscopic and phenomenological potentials compared with data.

doi: 10.1134/S106377880702010X
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2006KA23      Phys.Rev. C 73, 047601 (2006)

M.Karakoc, I.Boztosun

α-α double folding cluster potential description of the 12C + 24Mg system

NUCLEAR REACTIONS 24Mg(12C, 12C), E=20, 21, 22 MeV; 24Mg(12C, X), E(cm) ≈ 13-16 MeV; analyzed elastic σ(θ) and fusion σ. α-α double folding cluster potential.

doi: 10.1103/PhysRevC.73.047601
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2006KA43      Int.J.Mod.Phys. E15, 1317 (2006)

M.Karakoc, I.Boztosun

Microscopic potential description of the elastic scattering and fusion cross-section data of the 12C + 24Mg system

NUCLEAR REACTIONS 24Mg(12C, 12C), E=20, 21, 22, 23, 24 MeV; calculated σ(θ). 24Mg(12C, X), E=20, 21, 22, 23, 24 MeV; calculated fusion σ. Microscopic potential, comparison with data.

doi: 10.1142/S0218301306004867
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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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