NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = B.Yilmaz Found 23 matches. 2023AY01 Phys.Rev. C 107, 014609 (2023) S.Ayik, M.Arik, O.Yilmaz, B.Yilmaz, A.S.Umar Multinucleon transfer mechanism in 250Cf + 232Th collisions using the quantal transport description based on the stochastic mean-field approach NUCLEAR REACTIONS 232Th(250Cf, X), E(cm)=950; calculated drift path of Cf-like fragments in the head-on collision, total kinetic energy, fragments mass and charge distribution yields for different combinations of 250Cf and 232Th orientations, primary and secondary production σ, mean values of neutron and proton numbers of Cf-like fragments, diffusion coefficients. Stochastic mean field approach which provides an extension to the standard time-dependent Hartree-Fock theory by including mean-field fluctuations.
doi: 10.1103/PhysRevC.107.014609
2021AY06 Phys.Rev. C 104, 054614 (2021) S.Ayik, M.Arik, E.C.Karanfil, O.Yilmaz, B.Yilmaz, A.S.Umar Quantal diffusion description of isotope production via the multinucleon transfer mechanism in 48Ca + 238U collisions NUCLEAR REACTIONS 238U(48Ca, X), E(cm)=193 MeV; calculated neutron and proton diffusion coefficients, mean drift path of the projectile-like fragments, neutron, proton, and mixed variances as a functions of time and initial orbital angular momentum, orbital angular momentum, final average total kinetic energy (TKE), average total excitation energy, and scattering angles, mean values of mass and charge numbers of initial and final fragments, combined primary yield of multi-nucleon transfer and binary fission as function fragment mass, isotopic production σ for 238U(48Ca, X), E(cm)=193.1 MeV; calculated production σ for primary and secondary isotopes of A=150-200 Tb, Dy, Ho and Er, A=160-210 Tm, Yb, Lu and Hf, A=170-220 Ta, W, Re and Os, and A=180-230 Ir, Pt, Au and Hg. Methods involved quantal diffusion from stochastic mean-field approach, and transport properties from time-dependent single-particle wave functions of the time-dependent Hartree-Fock theory using statistical GEMINI++ code.
doi: 10.1103/PhysRevC.104.054614
2020AY06 Phys.Rev. C 102, 024619 (2020) S.Ayik, B.Yilmaz, O.Yilmaz, A.S.Umar Merging of transport theory with the time-dependent Hartree-Fock approach: Multinucleon transfer in U + U collisions NUCLEAR REACTIONS 238U(238U, X), E(cm)=833 MeV; calculated density profile and the geometry of the collisions, values of final masses and charges of the projectile-like and target-like fragments, final orbital angular momentum, total kinetic energy (TKE), total excitation energy, center of mass angle, laboratory scattering angles for tip-tip and side-side collisions, asymptotic values of the neutron, the proton and the mixed dispersions, neutron and proton diffusion coefficients, production σ(N, Z), σ(A), σ(Z) for primary fragments, production σ(A) of gold isotopes averaged over tip-tip and side-side geometries as a function of the mass numbers, and compared with experimental data. 240Cm(236Ra, X), E(cm)=833 MeV; calculated drift path of the radium-like fragments in central collisions, neutron and proton numbers of radium-like fragments as function of time, neutron and proton diffusion coefficients. Multinucleon transfer mechanism treated in the framework of quantal diffusion description based on the stochastic mean-field (SMF) properties derived from the time-dependent Hartree-Fock (TDHF) wave functions.
doi: 10.1103/PhysRevC.102.024619
2020YI01 Eur.Phys.J. A 56, 37 (2020) Quasi-fission and fusion-fission reactions in 48Ca+208Pb collisions at Ec.m=190 MeV
doi: 10.1140/epja/s10050-020-00053-8
2019AY02 Phys.Rev. C 100, 014609 (2019) S.Ayik, B.Yilmaz, O.Yilmaz, A.S.Umar Quantal diffusion approach for multinucleon transfers in Xe + Pb collisions NUCLEAR REACTIONS 136Xe(208Pb, X), 130Te(214Po, X), 138Ce(206Pt, X), E(cm)=526 MeV; calculated distribution of projectile-like and target-like reaction product by mass number and charge for 208Pb+136Xe reaction, neutron and proton diffusion coefficients and drift paths using quantal diffusion approach.
doi: 10.1103/PhysRevC.100.014609
2019AY06 Phys.Rev. C 100, 044614 (2019) S.Ayik, O.Yilmaz, B.Yilmaz, A.S.Umar Heavy-isotope production in 136Xe 208Pb collisions at Ec.m. = 514 MeV NUCLEAR REACTIONS 208Pb(136Xe, X)210Po/222Rn/224Ra, E(cm)=514 MeV; calculated TKE, excitation energy, scattering angles, mass dispersions toward asymmetry and symmetry directions, production σ for A=110-230 isotopes, and for primary isotopes of Z=84, 86 and 88 as a function of mass number using stochastic mean field (SMF) approach. Comparison with experimental data.
doi: 10.1103/PhysRevC.100.044614
2019UL01 Phys.Rev. C 100, 054603 (2019) Impact of initial fluctuations on the dissipative dynamics of interacting Fermi systems: A model case study
doi: 10.1103/PhysRevC.100.054603
2018AY03 Phys.Rev. C 97, 054618 (2018) S.Ayik, B.Yilmaz, O.Yilmaz, A.S.Umar Quantal diffusion description of multinucleon transfers in heavy-ion collisions NUCLEAR REACTIONS 238U(48Ca, X), E(cm)=193 MeV; calculated collision density profile, neutron and proton mean-drift path, drift and diffusion coefficients, curvature parameters, covariance of fragment mass distribution, impact parameter, final orbital angular momentum, final average total kinetic energy TKE, average total excitation energy, scattering angles, mass and charge numbers of final fragments, yield and production cross section of primary fragments. Stochastic mean-field (SMF) approach with a quantal diffusion description of the multi-nucleon transfer in heavy-ion collisions at finite impact parameters. Comparison with experimental data.
doi: 10.1103/PhysRevC.97.054618
2018YI04 Phys.Rev. C 98, 034604 (2018) B.Yilmaz, S.Ayik, O.Yilmaz, A.S.Umar Multinucleon transfer in 58Ni + 60Ni and 60Ni + 60Ni in a stochastic mean-field approach NUCLEAR REACTIONS 60Ni(58Ni, X), (60Ni, X), E(cm)=135.6 MeV; calculated density profiles, neutron and proton diffusion coefficients, one-sided mean drift paths, collision covariances, dispersion per unit mass, and fragment mass distribution using stochastic mean-field (SMF) approach. Comparison with experimental values and time-dependent random-phase approximation (TDRPA) calculations.
doi: 10.1103/PhysRevC.98.034604
2017AY05 Phys.Rev. C 96, 024611 (2017) S.Ayik, B.Yilmaz, O.Yilmaz, A.S.Umar, G.Turan Multinucleon transfer in central collisions of 238U + 238U NUCLEAR REACTIONS 238U(238U, X), E(cm)=900, 1050 MeV; calculated density profiles in the reaction plane, and mean drift path of the projectile-like fragments using time-dependent Hartree-Fock (TDHF) approach, quantal neutron and proton diffusion coefficients, memory effects and covariances, primary fragment mass distributions using stochastic mean-field (SMF) approach.
doi: 10.1103/PhysRevC.96.024611
2016AY06 Phys.Rev. C 94, 044624 (2016) S.Ayik, O.Yilmaz, B.Yilmaz, A.S.Umar Quantal nucleon diffusion: Central collisions of symmetric nuclei NUCLEAR REACTIONS 28O(28O, X), E(cm)=8.7 MeV; 40Ca(40Ca, X), E(cm)=52.7 MeV; 48Ca(48Ca, X), E(cm)=50.7 MeV; 56Ni(56Ni, X), E(cm)=100.0 MeV; calculated quantal and semiclassical neutron and proton diffusion coefficients, effect of Pauli blocking on fragment neutron and proton variances using stochastic mean-field (SMF) approach.
doi: 10.1103/PhysRevC.94.044624
2016LA12 Eur.Phys.J. A 52, 94 (2016) D.Lacroix, Y.Tanimura, S.Ayik, B.Yilmaz A simplified BBGKY hierarchy for correlated fermions from a stochastic mean-field approach
doi: 10.1140/epja/i2016-16094-1
2015AY03 Phys.Rev. C 91, 054601 (2015) S.Ayik, O.Yilmaz, B.Yilmaz, A.S.Umar, A.Gokalp, G.Turan, D.Lacroix Quantal description of nucleon exchange in a stochastic mean-field approach NUCLEAR REACTIONS 40Ca(40Ca, X), E(cm)=52.7 MeV; 48Ca(48Ca, X), E(cm)=50.7 MeV; 56Ni(56Ni, X), E(cm)=99.9 MeV; calculated quantal diffusion coefficient and variance of fragment mass distribution as a function of time in central collision. Stochastic mean-field approach. Comparison with other theoretical calculations.
doi: 10.1103/PhysRevC.91.054601
2015AY08 Phys.Rev. C 92, 064615 (2015) Multinucleon exchange in quasifission reactions NUCLEAR REACTIONS 238U(40Ca, X), E(cm)=202.0 MeV; 238U(48Ca, X), E(cm)=198.7 MeV; calculated mean drift paths of projectile-like fragments, proton and neutron drift coefficients, diffusion coefficients for proton and neutron exchange, and mass dispersion of the fragment distributions. Dinuclear structure. Stochastic mean-field (SMF) approach with time-dependent Hartree-Fock (TDHF) calculations for systems near the quasifission regime.
doi: 10.1103/PhysRevC.92.064615
2014GH01 Phys.Rev. C 89, 014301 (2014) F.Ghazi Moradi, C.Qi, B.Cederwall, A.Atac, T.Back, R.Liotta, M.Doncel, A.Johnson, G.de France, E.Clement, A.Dijon, R.Wadsworth, T.W.Henry, A.J.Nichols, H.Al-Azri, J.Nyberg, A.Gengelbach, T.Huyuk, B.M.Nyako, J.Timar, D.Sohler, Zs.Dombradi, I.Kuti, K.Juhasz, M.Palacz, G.Jaworski, S.M.Lenzi, P.R.John, D.R.Napoli, A.Gottardo, V.Modamio, A.Di Nitto, B.Yilmaz, O.Aktas, E.Ideguchi Character of particle-hole excitations in γ-ray angular correlation and linear polarization measurements NUCLEAR REACTIONS 58Ni(40Ca, 4p)94Ru, E=125 MeV; measured Eγ, Iγ, γγ-, γγ(particle)-coin, γγ(θ)(DCO), γγ(linear polarization) using EXOGAM array for γ rays and DIAMANT array for particles at GANIL facility. 94Ru; deduced high-spin levels, J, π, multipolarity, configurations, hindrance factors for E1 transitions. Comparison with large-scale shell-model (LSSM) calculations.
doi: 10.1103/PhysRevC.89.014301
2014GH02 Phys.Rev. C 89, 044310 (2014) F.Ghazi Moradi, B.Cederwall, C.Qi, T.Back, A.Atac, R.Liotta, M.Doncel, A.Johnson, G.de France, E.Clement, J.Nyberg, A.Gengelbach, B.M.Nyako, J.Gal, G.Kalinka, J.Molnar, J.Timar, D.Sohler, Zs.Dombradi, I.Kuti, K.Juhasz, D.R.Napoli, A.Gottardo, V.Modamio, R.Wadsworth, T.W.Henry, A.J.Nichols, H.Al-Azri, M.Palacz, E.Ideguchi, O.Aktas, A.Di Nitto, A.Dijon, T.Huyuk, G.Jaworski, P.R.John, B.Yilmaz Spectroscopy of the neutron-deficient N = 50 nucleus 95Rh NUCLEAR REACTIONS 58Ni(40Ca, 3p), E=125 MeV; measured Eγ, Iγ, γγ-, nγ-, (particle)γ-coin, γγ(θ)(DCO), γ(linear polarization) using EXOGAM Ge detector array, Neutron Wall and DIAMANT CsI(Tl) detector arrays at GANIL facility. 95Rh; deduced high-spin levels, J, π, multipolarity, configurations, E1 transition strengths and hindrance factors. Comparison with large-scale shell model (LSSM) calculations in fpg and fpgd model spaces.
doi: 10.1103/PhysRevC.89.044310
2014YI03 Phys.Rev. C 90, 024613 (2014) B.Yilmaz, S.Ayik, D.Lacroix, O.Yilmaz Nucleon exchange in heavy-ion collisions within a stochastic mean-field approach NUCLEAR REACTIONS 40Ca(40Ca, X), E(cm)=110 MeV; 90Zr(90Zr, X), E(cm)=300 MeV; calculated diffusion coefficients for nucleon exchange, widths of fragment mass distributions, and asymptotic values of cross sections as a function of orbital angular momentum in deep-inelastic symmetric heavy-ion collisions. Stochastic mean-field (SMF) approach. Comparison with predictions of phenomenological nucleon exchange model, and available experimental data.
doi: 10.1103/PhysRevC.90.024613
2014YI05 Phys.Rev. C 90, 054617 (2014) B.Yilmaz, D.Lacroix, R.Curebal Importance of realistic phase-space representations of initial quantum fluctuations using the stochastic mean-field approach for fermions
doi: 10.1103/PhysRevC.90.054617
2012LA09 Phys.Rev. C 85, 041602 (2012) Symmetry breaking and fluctuations within stochastic mean-field dynamics: Importance of initial quantum fluctuations
doi: 10.1103/PhysRevC.85.041602
2011YI02 Phys.Rev. C 83, 064615 (2011) B.Yilmaz, S.Ayik, D.Lacroix, K.Washiyama Nucleon exchange mechanism in heavy-ion collisions at near-barrier energies NUCLEAR REACTIONS 90Zr(40Ca, X), E(cm)=97 MeV; calculated nucleon density profiles, number of nucleon transfer to the target, nucleon drift coefficients, nucleon diffusion coefficients, fragment mass distributions in frameworks of the standard mean-field provided by the TDHF equations and the stochastic mean-field (SMF) approaches.
doi: 10.1103/PhysRevC.83.064615
2010AY03 Phys.Rev. C 81, 034605 (2010) Stochastic semi-classical description of fusion at near-barrier energies NUCLEAR REACTIONS 58Ni(58Ni, X), 58,64Ni(64Ni, X), E(cm)=85-110 MeV; calculated fusion cross sections using stochastic semi-classical model. Comparison with experimental data and other theoretical calculations.
doi: 10.1103/PhysRevC.81.034605
2007AB08 Int.J.Mod.Phys. E16, 491 (2007) Y.Abe, A.Marchix, C.Shen, B.Yilmaz, G.Kosenko, D.Boilley, B.G.Giraud Dynamics of massive systems and synthesis of superheavy elements NUCLEAR REACTIONS 208Pb(58Fe, n), E(cm)=210-235 MeV; 132Sn, 160Gd(132Sn, n), (132Sn, 2n), (132Sn, 3n), (132Sn, 4n), E(cm)=265-295 MeV; calculated fusion and evaporation residue σ.
doi: 10.1142/S0218301307005922
2005AY01 Phys.Rev. C 71, 054611 (2005) S.Ayik, B.Yilmaz, A.Gokalp, O.Yilmaz, N.Takigawa Quantum statistical effects on fusion dynamics of heavy ions
doi: 10.1103/PhysRevC.71.054611
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