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NSR database version of May 10, 2024.

Search: Author = N.Buyukcizmeci

Found 28 matches.

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2024KI09      Phys.Rev. C 109, 044913 (2024)

A.Kittiratpattana, T.Reichert, N.Buyukcizmeci, A.Botvina, A.Limphirat, Ch.Herold, J.Steinheimer, M.Bleicher

Production of nuclei and hypernuclei in pion-induced reactions near threshold energies

doi: 10.1103/PhysRevC.109.044913
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2024OG01      Few-Body Systems 65, 22 (2024)

R.Ogul, A.S.Botvina, M.Bleicher, N.Buyukcizmeci, A.Ergun, H.Imal

Isospin Correlations in Isotope Yields at Intermediate and High Energy Heavy-Ion Collisions

NUCLEAR REACTIONS 48Ca(80Kr, X), E=35 MeV/nucleon; Pb(136Xe, X), 124Sn(124Sn, X), E=1 GeV/nucleon; analyzed FAZIA and FRS experiments data; deduced relative isotopic yields in the framework of the statistical multifragmentation model for an ensemble of excited both projectile and midrapidity sources.

doi: 10.1007/s00601-024-01885-6
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2023BU11      Phys.Rev. C 108, 054904 (2023)

N.Buyukcizmeci, T.Reichert, A.S.Botvina, M.Bleicher

Nucleosynthesis of light nuclei and hypernuclei in central Au + Au collisions at √ sNN = 3 GeV

doi: 10.1103/PhysRevC.108.054904
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2023OG01      Phys.Rev. C 107, 054606 (2023)

R.Ogul, A.S.Botvina, M.Bleicher, N.Buyukcizmeci, A.Ergun, H.Imal, Y.Leifels, W.Trautmann

Isospin compositions of correlated sources in the Fermi energy domain

NUCLEAR REACTIONS 40,48Ca(80Kr, X), E=35 MeV/nucleon; calculated isotope yield distributions of reaction products at forward angles with Z=1-4 (N=0-8) and Z=19-24 (N=19-31), neutron-to-proton ratio of the fragments, mean multiplicity of the fragments. Statistical Multifragmentation Model (SMM) calculations using the ensemble method previously established for reactions at higher energy with relation to the nuclear liquid-gas phase transition. Inferred on the isotopic compositions of the projectile residues, the isospin exchange between the reaction partners, and the origin of the experimentally identified groups of Z=1-4 fragments and the neck-like emitted Z=2-11 fragments. Comparison to the data reported in 2021PI02: Phys.Rev. C 103, 014603 (2021). Obtained satisfactory reproduction of the experimental results with two correlated and statistically decaying sources, a projectile source and a neck source with enhanced neutron content.

doi: 10.1103/PhysRevC.107.054606
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2023PA34      Phys.Rev. C 108, 044610 (2023)

P.Pawlowski, J.Brzychczyk, N.Buyukcizmeci, H.T.Johansson, W.Trautmann, A.Wieloch, P.Adrich, T.Aumann, T.Barczyk, S.Bianchin, K.Boretzky, A.S.Botvina, A.Chbihi, J.Cibor, B.Czech, H.Emling, J.D.Frankland, M.Heil, A.Le Fevre, Y.Leifels, J.Luhning, J.Lukasik, U.Lynen, Z.Majka, I.N.Mishustin, W.F.J.Muller, R.Ogul, H.Orth, R.Palit, D.Rossi, C.Schwarz, C.Sfienti, H.Simon, K.Summerer, H.Weick, B.Zwieglinski

Neutrons from projectile fragmentation at 600 MeV/nucleon

doi: 10.1103/PhysRevC.108.044610
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2022BO11      Phys.Rev. C 106, 014607 (2022)

A.S.Botvina, N.Buyukcizmeci, M.Bleicher

Evolution of the statistical disintegration of finite nuclei toward high energy

NUCLEAR REACTIONS Ni(Ni, X)H/He/Li/Be/B/C/N/O/F/Ne/Na/Mg, E=150, 250 MeV/nucleon; Au(Au, X)H/He/Li/Be/B/C/N/O/F/Ne/Na/Mg, E=90, 120, 150, 250 MeV/nucleon; calculated production of the nuclear clusters with defined Z, average excitation energy per nucleon of local clusters. Statistical approach. Comparison to experimental data.

doi: 10.1103/PhysRevC.106.014607
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2021BO16      Phys.Rev. C 103, 064602 (2021)

A.S.Botvina, N.Buyukcizmeci, M.Bleicher

Coupling dynamical and statistical mechanisms for baryonic cluster production in nucleus collisions of intermediate and high energies

doi: 10.1103/PhysRevC.103.064602
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2020BU04      Phys.Scr. 95, 075311 (2020)

N.Buyukcizmeci, R.Ogul, A.S.Botvina, M.Bleicher

On the survey of nuclei and hypernuclei in multifragmentation

NUCLEAR STRUCTURE H, C, O; analyzed available data; deduced hyperon yields.

doi: 10.1088/1402-4896/ab978f
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2020BU10      Eur.Phys.J. A 56, 210 (2020)

N.Buyukcizmeci, A.S.Botvina, R.Ogul, M.Bleicher

Evaluation of hypernuclei in relativistic ion collisions

doi: 10.1140/epja/s10050-020-00217-6
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2020IM01      Eur.Phys.J. A 56, 110 (2020)

H.Imal, N.Buyukcizmeci, R.Ogul, A.S.Botvina

Isospin dependence of fragment yields in peripheral heavy ion collisions

doi: 10.1140/epja/s10050-020-00114-y
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2019BU05      Eur.Phys.J. A 55, 2 (2019)

N.Buyukcizmeci, A.S.Botvina, R.Ogul, A.Ergun, M.Bleicher

Production of Λ-hypernuclei and evaluation of their binding energies via the double yield ratio

NUCLEAR STRUCTURE 200Hg; calculated yields of fragments and hyperfragments from excited 3Λ-hypernucleus, calculated yield of the isotopes vs neutron number, hyperons binding energy, Q vs fragment mass for several temperatures (T=0, 2, 3, 4, 6 MeV) using hyper-fragment formulas, temperature vs E* for single- and double-hypernuclei.

doi: 10.1140/epja/i2019-12672-y
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2018BU17      Phys.Rev. C 98, 064603 (2018)

N.Buyukcizmeci, A.S.Botvina, A.Ergun, R.Ogul, M.Bleicher

Statistical production and binding energy of hypernuclei

NUCLEAR STRUCTURE 20,21O, 24,25Mg, 32,33P, 40,41S, 49,50Ca, 59,60Cr, 80,81Ge, 100,101Zr, 124,125Sn; calculated yield ratios of hypernuclei with hyperon number of 1, 2 or 3 to 12C, 13C hyperons. 13C, 21O, 25Mg, 33P, 41S, 50Ca, 60Cr, 81Ge, 101Zr, 125Sn; calculated difference of binding energies of hyperons versus A using the double ratio method, temperature versus the excitation energy for disintegration of the hypernuclear system, Influence of the secondary deexcitation on the difference of binding energies of hyperons for (13ΛC/12C)/(21ΛO/20O), (13ΛC/12C)/(25ΛMg/24Mg), (13ΛC/12C)/(33ΛP/32P), (13ΛC/12C)/(41ΛS/40S), (13ΛC/12C)/(50ΛCa/49Ca), (13ΛC/12C)/(60ΛCr/59Cr), (13ΛC/12C)/(81ΛGe/80Ge), (13ΛC/12C)/(101ΛZr/100Zr), and (13ΛC/12C)/(125ΛSn/124Sn). Statistical model calculations. Relevance to production of all kinds of hypernuclei with large cross sections in multifragmentation process in relativistic ion-ion and hadron-ion collisions.

doi: 10.1103/PhysRevC.98.064603
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2016BO28      Phys.Rev. C 94, 054615 (2016)

A.S.Botvina, N.Buyukcizmeci, A.Ergun, R.Ogul, M.Bleicher, J.Pochodzalla

Formation of hypernuclei in evaporation and fission processes

NUCLEAR STRUCTURE 112,124Sn, 165Ho, 209Bi, 238U; calculated fragment mass distributions, probabilities of nuclear and hypernuclear fission, and evaporation of light hypernuclei, average mass numbers, charges, yields, excitation energies and the fission barriers of the fissioning hypernuclei. Generalization of nuclear evaporation and fission models applied to excited hot hypernuclei.

doi: 10.1103/PhysRevC.94.054615
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2015ER04      Phys.Rev. C 92, 014610 (2015)

A.Ergun, H.Imal, N.Buyukcizmeci, R.Ogul, A.S.Botvina

Influence of angular momentum and Coulomb interaction of colliding nuclei on their multifragmentation

NUCLEAR REACTIONS 84Kr(84Kr, X), E=35 MeV/nucleon; calculated total and specific charge yields, mean neutron-to-proton ratios, and velocity distributions of Z<40 primary hot fragments. Microcanonical Markov chain calculations within the statistical multifragmentation model, including angular momentum and long-range Coulomb interaction between projectile and target residues. Discussed connection between dynamical and statistical phenomena in nuclear reactions.

doi: 10.1103/PhysRevC.92.014610
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2015IM01      Phys.Rev. C 91, 034605 (2015)

H.Imal, A.Ergun, N.Buyukcizmeci, R.Ogul, A.S.Botvina, W.Trautmann

Theoretical study of projectile fragmentation in the 112Sn + 112Sn and 124Sn + 124Sn reactions at 1 GeV/nucleon

NUCLEAR REACTIONS 112Sn(112Sn, X), 124Sn(124Sn, X), E=600, 1000 MeV/nucleon; analyzed experimental data for the production cross sections of projectile fragments as a function of fragment atomic number Z, isotopic σ(Z) and symmetry-energy coefficient for final fragments with atomic numbers Z=10-21, 22-33, 34-45. Statistical multifragmentation model (SMM) calculations. Experimental data from measurements using FRS at GSI.

doi: 10.1103/PhysRevC.91.034605
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2013BU08      Nucl.Phys. A907, 13 (2013)

N.Buyukcizmeci, A.S.Botvina, I.N.Mishustin, R.Ogul, M.Hempel, J.Schaffner-Bielich, F.-K.Thielemann, S.Furusawa, K.Sumiyoshi, S.Yamada, H.Suzuki

A comparative study of statistical models for nuclear equation of state of stellar matter

doi: 10.1016/j.nuclphysa.2013.03.010
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2013BU11      Phys.Rev. C 88, 014611 (2013); Erratum Phys.Rev. C 93, 019902 (2016)

N.Buyukcizmeci, A.S.Botvina, J.Pochodzalla, M.Bleicher

Mechanisms for the production of hypernuclei beyond the neutron and proton drip lines

doi: 10.1103/PhysRevC.88.014611
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2013ER05      Eur.Phys.J. A 49, 48 (2013)

N.Eren, N.Buyukcizmeci, R.OguL, A.S.Botvina

Mass distribution in the disintegration of heavy nuclei

NUCLEAR REACTIONS 232Th(p, F), E=12 MeV;232Th, 235,238U(n, F), E=14 MeV; calculated fission mass distribution. Compared to data. 235U(X, F), (X, X'), E*=0.05-5 MeV/nucleon; calculated fission, evaporation, multifragmentation mass distributions. Compared to data.

COMPILATION Os, Ir, Pt, Au, Hg, Tl, Pb, Bi, Po, At(p, F), (d, F), (3He, F), (α, F), (12C, F), (16O, F), E*≈10-90 MeV; compiled symmetric mass distribution variance; deduced simple trend. Ac, Th, Pa, U, Np, Pu, Am, Cm(n, F), (p, F), (d, F), (α, F), E*≈5-60 MeV; compiled symmetric to asymmetric fission peak ratio; deduced simple trend.

doi: 10.1140/epja/i2013-13048-1
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2012BU13      J.Phys.(London) G39, 115102 (2012)

N.Buyukcizmeci, H.Imal, R.Ogul, A.S.Botvina, I.N.Mishustin

Isotopic yields and symmetry energy in nuclear multifragmentation reactions

NUCLEAR REACTIONS 124Sn(124Sn, X), 112Sn(112Sn, X), E=50 MeV/nucleon; analyzed available data; calculated charge and isotope yields, isotope distributions. Statistical multifragmentation model, comparison with available data.

doi: 10.1088/0954-3899/39/11/115102
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2011BU02      Acta Phys.Pol. B42, 697 (2011)

N.Buyukcizmeci, F.Bulut, M.Erdogan, H.Imal, R.Ogul, A.S.Botvina, I.N.Mishustin, W.Trautmann

Investigating the Isotopic Effects in Nuclear Fragmentation

NUCLEAR REACTIONS 124Sn(124Sn, X), 112Sn(112Sn, X), E not given; analyzed experimental data; deduced mean N/Z ratio for light fragments, symmetry term coefficient.

doi: 10.5506/APhysPolB.42.697
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2011OG01      Phys.Rev. C 83, 024608 (2011); Erratum Phys.Rev. C 85, 019903 (2012)

R.Ogul, A.S.Botvina, U.Atav, N.Buyukcizmeci, I.N.Mishustin, P.Adrich, T.Aumann, C.O.Bacri, T.Barczyk, R.Bassini, S.Bianchin, C.Boiano, A.Boudard, J.Brzychczyk, A.Chbihi, J.Cibor, B.Czech, M.De Napoli, J.-E.Ducret, H.Emling, J.D.Frankland, M.Hellstrom, D.Henzlova, G.Imme, I.Iori, H.Johansson, K.Kezzar, A.Lafriakh, A.Le Fevre, E.Le Gentil, Y.Leifels, J.Luhning, J.Lukasik, W.G.Lynch, Z.Majka, M.Mocko, W.F.J.Muller, A.Mykulyak, H.Orth, A.N.Otte, R.Palit, P.Pawlowski, A.Pullia, G.Raciti, E.Rapisarda, H.Sann, C.Schwarz, C.Sfienti, H.Simon, K.Summerer, W.Trautmann, M.B.Tsang, G.Verde, C.Volant, M.Wallace, H.Weick, J.Wiechula, A.Wieloch, B.Zwieglinski

Isospin-dependent multifragmentation of relativistic projectiles

NUCLEAR REACTIONS Sn(107Sn, X), (124Sn, X), (124La, X), [107Sn, 124La secondary beams from 9Be(142Nd, X), E=900 MeV/nucleon primary reaction], E=600 MeV/nucleon; measured charge (Z) spectra and fragment trajectories according to Z number, σ as function of Z and A numbers, yields, mass distributions and correlations, multiplicity of mass fragments, neutron-to-proton ratio for fragments using ALADIN spectrometer. Comparison with statistical multifragmentation model (SMM) calculations.

doi: 10.1103/PhysRevC.83.024608
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2010BU15      J.Phys.:Conf.Ser. 202, 012003 (2010)

N.Buyukcizmeci, A.S.Botvina, I.N.Mishustin, R.Ogul

Towards the equation of state for dense stellar matter

doi: 10.1088/1742-6596/202/1/012003
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2009OG05      J.Phys.(London) G36, 115106 (2009)

R.Ogul, U.Atav, F.Bulut, N.Buyukcizmeci, M.Erdogan, H.Imal, A.S.Botvina, I.N.Mishustin

Surface and symmetry energies in isoscaling for multifragmentation reactions

NUCLEAR REACTIONS Sn(112Sn, X), (124Sn, X), E not given; calculated isoscaling parameters, neutron and proton ratios for light fragments. Markov chain calculations, comparison with MSU experimental data.

doi: 10.1088/0954-3899/36/11/115106
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2008BU06      Phys.Rev. C 77, 034608 (2008)

N.Buyukcizmeci, A.S.Botvina, I.N.Mishustin, R.Ogul

Role of bulk energy in nuclear multifragmentation

doi: 10.1103/PhysRevC.77.034608
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2006BO25      Phys.Rev. C 74, 044609 (2006)

A.S.Botvina, N.Buyukcizmeci, M.Erdogan, J.Lukasik, I.N.Mishustin, R.Ogul, W.Trautmann

Modification of surface energy in nuclear multifragmentation

NUCLEAR REACTIONS Be, C, Al, Cu, In, Au(139Xe, X), (197Au, X), (238U, X), E=600 MeV/nucleon; analyzed fragments yields, related data; deduced isospin dependence of surface energy coefficient.

doi: 10.1103/PhysRevC.74.044609
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2006BU23      Phys.Scr. T125, 182 (2006)

N.Buyukcizmeci, R.Ogul

Bimodality in multifragmentation of finite nuclei

NUCLEAR STRUCTURE 124La, 124Sn, 197Au; calculated relative mass probabilities, temperature for fragmentation of excited systems.

doi: 10.1088/0031-8949/2006/T125/041
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2005BU27      Eur.Phys.J. A 25, 57 (2005)

N.Buyukcizmeci, R.Ogul, A.S.Botvina

Isospin and symmetry energy effects on nuclear fragment production in liquid-gas-type phase transition region

NUCLEAR STRUCTURE 78Kr, 124La, 124Sn, 197Au; calculated fragment mass yields vs excitation energy; deduced isospin and symmetry energy effects. Statistical multifragmentation model.

doi: 10.1140/epja/i2004-10281-7
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2005OG01      Nucl.Phys. A749, 126c (2005)

R.Ogul, N.Buyukcizmeci, A.S.Botvina

Nuclear fragmentation and critical temperature for the liquid-gas phase transition region

NUCLEAR STRUCTURE 124La, 124Sn, 197Au; calculated fragment mass yields vs excitation energy; deduced phase transition features. Statistical multifragmentation model.

doi: 10.1016/j.nuclphysa.2004.12.020
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