NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = S.Shlomo Found 140 matches. Showing 1 to 100. [Next]2024MA02 Eur.Phys.J. A 60, 6 (2024) A.G.Magner, A.I.Sanzhur, S.N.Fedotkin, A.I.Levon, U.V.Grygoriev, S.Shlomo Pairing correlations within the micro-macroscopic approach for the level density NUCLEAR STRUCTURE 40,48Ca, 52,54Fe, 56Ni, 115Sn, 144Sm, 208Pb; calculated level densities for low-energy states within the microscopic-macroscopic approach (MMA). Comparison with available data.
doi: 10.1140/epja/s10050-023-01222-1
2023GO08 Phys.Rev. C 108, 014328 (2023) M.L.Gorelik, S.Shlomo, B.A.Tulupov, M.H.Urin Semimicroscopic description of isoscalar giant multipole resonances in medium-mass closed-shell nuclei NUCLEAR STRUCTURE 48Ca, 90Zr, 132Sn, 208Pb; calculated isoscalar giant multipole resonances (up to L=3, including L=0 and 2 overtones) parameters, relative energy-weighted strength functions for isoscalar giant monopole, dipole, quadrupole, and octupole resonances (ISGMR, ISGDR, ISGQR and ISGOR), projected transition densities for isoscalar giant multipole resonances, partial branching ratio of direct one-nucleon decay. Particle-hole dispersive optical model (PHDOM). Comparison to experimental data.
doi: 10.1103/PhysRevC.108.014328
2023MA40 Iader.Fiz.Enerh. 24, 175 (2023) A.G.Magner, A.I.Sanzhur, S.N.Fedotkin, A.I.Levon, U.V.Grygoriev, S.Shlomo Nuclear level density in the statistical semiclassical micro-macroscopic approach NUCLEAR STRUCTURE 140,142,145Nd, 144,150Sm, 166Ho, 208Pb, 230Th, 240Pu; analyzed available data; deduced level density parameters using Least Mean-Square (LMS) fit.
doi: 10.15407/jnpae2023.03.175
2022MA14 Nucl.Phys. A1021, 122423 (2022) A.G.Magner, A.I.Sanzhur, S.N.Fedotkin, A.I.Levon, S.Shlomo Level density within a micro-macroscopic approach NUCLEAR STRUCTURE 240Pu, 150Sm, 166Ho; analyzed available data; deduced statistical level density for nucleonic system with a given energy E, particle number A and other integrals of motion in the micro-macroscopic approximation beyond the standard saddle-point method of the Fermi gas model.
doi: 10.1016/j.nuclphysa.2022.122423
2021BO09 Nucl.Phys. A1010, 122159 (2021) G.Bonasera, S.Shlomo, D.H.Youngblood, Y.-W.Lui, J.Button, X.Chen Isoscalar and isovector giant resonances in 44Ca, 54Fe, 64, 68Zn and 56, 58, 60, 68Ni NUCLEAR STRUCTURE 44Ca, 54Fe, 64,68Zn, 56,58,60,68Ni; calculated centroid energies for isoscalar and isovector giant dipole, quadrupole, octupole resonances within the spherical Hartree-Fock (HF)-based random phase approximation (RPA) theory with 33 distinct Skyrme-like effective nucleon-nucleon interactions.
doi: 10.1016/j.nuclphysa.2021.122159
2021GO08 Phys.Rev. C 103, 034302 (2021) M.L.Gorelik, S.Shlomo, B.A.Tulupov, M.H.Urin Properties of isoscalar giant multipole resonances in medium-heavy closed-shell nuclei: A semimicroscopic description NUCLEAR STRUCTURE 208Pb; calculated relative energy-weighted strength functions for isoscalar giant monopole, dipole, quadrupole, and octupole resonances (ISGMR, ISGDR, ISGQR and ISGOR), parameters, projected transition densities for isoscalar giant multipole resonances (ISGMPR) and compared with experimental data, isoscalar collective low-energy 3- and 2+ states, B(E2), B(E3), strength distribution, transition density, and partial and total probabilities of direct one nucleon decay, branching ratios for direct one-proton decay of the ISGDR. Particle-hole dispersive optical model (PHDOM).
doi: 10.1103/PhysRevC.103.034302
2021MA67 Phys.Rev. C 104, 044319 (2021) A.G.Magner, A.I.Sanzhur, S.N.Fedotkin, A.I.Levon, S.Shlomo Semiclassical shell-structure micro-macroscopic approach for the level density NUCLEAR STRUCTURE 144,148Sm, 166Ho, 208Pb, 230Th; calculated level densities for low-energy states with different approximations, maximal mean errors in the statistical distribution of states; derived statistical level density as function of the entropy within the micro-macroscopic approximation (MMA) using the mixed micro- and grand-canonical ensembles beyond the standard saddle point method of the Fermi gas model, using mean-field semiclassical periodic-orbit theory. Comparison with experimental densities.
doi: 10.1103/PhysRevC.104.044319
2021MA79 Int.J.Mod.Phys. E30, 2150092 (2021) A.G.Magner, A.I.Sanzhur, S.N.Fedotkin, A.I.Levon, S.Shlomo Shell-structure and asymmetry effects in level densities NUCLEAR STRUCTURE 176,178,180,182,184,186,188,190,192,194,196,198,200Pt; analyzed available data; deduced level densities within the semiclassical extended Thomas-Fermi and periodic-orbit theory beyond the Fermi-gas saddle-point method.
doi: 10.1142/S0218301321500920
2020SH24 Phys.Atomic Nuclei 83, 599 (2020) Isoscalar and Isovector Giant Resonances in Closed Shells Nuclei and Bulk Properties of Nuclear Matter NUCLEAR STRUCTURE 40,48Ca, 68Ni, 90Zr, 116Sn, 144Sm, 208Pb; calculated centroid energies, isoscalar and isovector giant resonances of multipolarities L=0-3 using the fully self-consistent spherical Hartree-Fock (HF)-based random-phase approximation (RPA) theory.
doi: 10.1134/S1063778820040183
2019BO16 Nucl.Phys. A992, 121612 (2019) G.Bonasera, S.Shlomo, D.H.Youngblood, Y.-W.Lui, Krishichayan, J.Button Isoscalar and isovector giant resonances in 92, 94, 96, 98, 100Mo and 90, 92, 94Zr NUCLEAR STRUCTURE 92,94,96,98,100Mo, 90,92,94Zr; calculated response function S(E), centroid energies ECEN of the isoscalar and isovector giant resonances of multipolarity, centroid energy vs nuclear matter incompressibility using spherical Hartree-Fock based RPA with Skyrme-type nucleon-nucleon interaction, difference between the centroid energies vs asymmetrycoefficient for each isotope I=(N-Z)/A, ECEN vs m*/m; compared with data; deduced nuclear matter properties, ECEN for ISGMR, for ISGDR, ISGOR, ISGQR, IVGMR, IVGDR, IVGQR.
doi: 10.1016/j.nuclphysa.2019.121612
2019BU26 Phys.Rev. C 100, 064318 (2019) J.Button, Y.-W.Lui, D.H.Youngblood, X.Chen, G.Bonasera, S.Shlomo Isoscalar E0, E1, and E2 strength in 54Fe and 64, 68Zn NUCLEAR REACTIONS 54Fe, 64,68Zn(α, α'), E=240 MeV; measured Eα, Iα, σ(θ) at the Texas A and M K500 superconducting cyclotron. 54Fe, 64,68Zn; deduced centroid energies, EWSR, widths, strengths and moments of isoscalar E0(ISGMR), E1(ISGDR) and E2(ISGQR) giant resonances using single-folding DWBA calculations with optical model potentials. Comparison with the predictions from HF-RPA calculations using the KDE0v1 Skyrme interaction. Systematics of centroids for E0, E1 and E2 isoscalar giant resonances for 40,44,48Ca, 45,48Ti, 54,56Fe, 56,58,60,68Ni, 64,68Zn.
doi: 10.1103/PhysRevC.100.064318
2018BO22 Phys.Rev. C 98, 054316 (2018) G.Bonasera, M.R.Anders, S.Shlomo Giant resonances in 40, 48Ca, 68Ni, 90Zr, 116Sn, 144Sm, and 208Pb NUCLEAR STRUCTURE 40,48Ca, 68Ni, 90Zr, 116Sn, 144Sm, 208Pb; calculated centroid energies of isoscalar and isovector giant monopole (GMR), giant dipole (GDR), giant quadrupole (GQR), and giant octupole (GOR) resonances using Hartree-Fock based RPA with 33 Skyrme-type effective nucleon-nucleon interactions. Comparison with available experimental data.
doi: 10.1103/PhysRevC.98.054316
2018GO03 Nucl.Phys. A970, 353 (2018) M.L.Gorelik, S.Shlomo, B.A.Tulupov, M.H.Urin On unitarity of the particle-hole dispersive optical model NUCLEAR STRUCTURE 208Pb; calculated energy weighted relative isoscalar giant monopole resonance strength functions, energy-averaged radial component of ISM (IsoScalar Monopole) double transition density at different energies, partial and total branching ratios for direct neutron decay of ISGMR using initial and unitary versions of PHDOM (Particle-Hole Dispersive Optical Model). Branching ratios compared with data.
doi: 10.1016/j.nuclphysa.2017.12.006
2018KO18 Phys.Rev. C 97, 064302 (2018) V.M.Kolomietz, A.I.Sanzhur, S.Shlomo Self-consistent mean-field approach to the statistical level density in spherical nuclei NUCLEAR STRUCTURE 40,48Ca, 90Zr, 120Sn, 208Pb; calculated proton and neutron particle density parameters, statistical level density parameters. 208Pb; calculated neutron single-particle level density, number of neutron states, nuclear mean field and reduced nuclear mean field, neutron momentum-dependent and frequency-dependent effective mass, temperature dependence of S(n), and temperature dependence of neutron excitation energy. 160Gd; calculated temperature dependence of inverse statistical level density parameter. Self-consistent mean-field approach within the extended Thomas-Fermi approximation with Skryme forces SkM* and KDE0v1.
doi: 10.1103/PhysRevC.97.064302
2017BU16 Phys.Rev. C 96, 054330 (2017) J.Button, Y.-W.Lui, D.H.Youngblood, X.Chen, G.Bonasera, S.Shlomo Isoscalar E0, E1, and E2 strength in 44Ca NUCLEAR REACTIONS 44Ca(α, α'), E=240 MeV; measured Eα, Iα, angular distributions using multipole-dipole-multipole (MDM) spectrometer at Texas A and M K500 superconducting cyclotron. 40Ca; deduced isoscalar giant monopole and quadrupole resonances (ISGMR and ISGQR), widths, E0, E1 and E2 strengths, energy-weighted sum rule (EWSR). Strength distributions compared with the predictions of Hartree-Fock based random phase approximation calculations with the KDE0v1 Skyrme-type interaction.
doi: 10.1103/PhysRevC.96.054330
2017KO19 Phys.Rev. C 95, 054305 (2017) V.M.Kolomietz, S.V.Lukyanov, A.I.Sanzhur, S.Shlomo Equation of state and radii of finite nuclei in the presence of a diffuse surface layer NUCLEAR STRUCTURE 208Pb; calculated equation of state and partial pressure. A=10-220; calculated equimolar nuclear radius versus A. A=20-32, Z=11; calculated rms radius of the proton distribution versus A. A=20-32, Z=11; A=111-125, Z=50; A=204-210, Z=82; calculated isovector shift of nuclear rms radius versus A. Comparison with experimental data. Gibbs-Tolman-Rowlinson-Widom (GTW) approach for nuclear surfaces and nuclear radii.
doi: 10.1103/PhysRevC.95.054305
2017KO21 Phys.Rev. C 95, 054613 (2017) Bulk and isospin instabilities in hot nuclear matter NUCLEAR STRUCTURE 208Pb; calculated dependence of isoscalar instability growth rate on the multipolarity of the particle density fluctuations for temperatures of 0.5, 4, 6, and 8 MeV, instabilities in a hot asymmetric nuclear matter with bulk density distortions, using equation of state of the extended Thomas-Fermi approximation, and KDE0v1 interaction.
doi: 10.1103/PhysRevC.95.054613
2017SH55 Bull.Rus.Acad.Sci.Phys. 81, 1230 (2017) A novel method for determining the single particle potential directly from the measured single particle density: Application to the charge density difference between the isotones 206Pb-205Tl
doi: 10.3103/S1062873817100227
2016BU19 Phys.Rev. C 94, 034315 (2016) J.Button, Y.-W.Lui, D.H.Youngblood, X.Chen, G.Bonasera, S.Shlomo Isoscalar E0, E1, E2, and E3 strength in 94Mo NUCLEAR REACTIONS 94Mo(α, α'), E=240 MeV; measured Eα, Iα, σ(θ) at Texas A and M K500 cyclotron facility; deduced moments, widths, E0, E1, E2 and E3 strength distributions, EWSR for isoscalar giant resonances. Comparison with spherical Hartree-Fock RPA calculations using KDE0v1 Skyrme-type interaction.
doi: 10.1103/PhysRevC.94.034315
2016GO19 Nucl.Phys. A955, 116 (2016) M.L.Gorelik, S.Shlomo, B.A.Tulupov, M.H.Urin Investigation of the energy-averaged double transition density of isoscalar monopole excitations in medium-heavy mass spherical nuclei NUCLEAR STRUCTURE 208Pb; calculated energy-weighted γ isoscalar giant monopole resonance strength function, transition density, double transition density vs radius for E*=13.8, 23, 33, 38 MeV using CRPA (Continuum RPA) and particle-hole dispersive optical model.
doi: 10.1016/j.nuclphysa.2016.06.004
2015AN12 Phys.Rev. C 92, 034318 (2015) Short-range correlations and the 3s1/2 wave function in 206Pb NUCLEAR REACTIONS 205Tl, 206Pb(e, e), E not given; calculated charge distributions, potentials by fits to experimental data, charge densities of a proton, possible effects of short-range correlations on the shell-model wave function of a proton in the 3s1/2 orbit.
doi: 10.1103/PhysRevC.92.034318
2015GO15 Phys.Atomic Nuclei 78, 551 (2015); Yad.Fiz. 78, 595 (2015) M.L.Gorelik, Sh.Shlomo, B.A.Tulupov, M.H.Urin Properties of high-energy isoscalar monopole excitations in medium-heavy mass spherical nuclei NUCLEAR STRUCTURE 208Pb; calculated isoscalar giant monopole resonance strength functions, particle-hole-type isoscalar monopole excitations using FM-DWBA using the Hartree-Fock ground state density and the transition densities obtained from the Hartree-Fock-based random-phase-approximation (RPA).
doi: 10.1134/S1063778815050075
2015KR08 Phys.Rev. C 92, 044323 (2015) Krishichayan, Y.-W.Lui, J.Button, D.H.Youngblood, G.Bonasera, S.Shlomo Isoscalar giant resonances in 90, 92, 94Zr NUCLEAR REACTIONS 90,92,94Zr(α, α'), E=240 MeV; measured inelastic α spectra, σ(θ) distributions using multipole-dipole-multipole (MDM) spectrometer at Texas A and M. 90,92,94Zr; deduced E0 (ISGMR), E1 (ISGDR), E2 (ISGQR) and E3 (ISGOR) isoscalar giant resonances, centroid energies, FWHM, widths, strengths EWSR. Comparison with previous experimental studies. DWBA calculations using density-dependent single-folding model. Systematics of centroid energies, widths and strengths for A=90-100, even-even Mo and Zr isotopes. Comparison of strength distributions with Hartree-Fock based RPA calculations using KDE0v1 Skyrme type interaction.
doi: 10.1103/PhysRevC.92.044323
2015YO04 Phys.Rev. C 92, 014318 (2015) D.H.Youngblood, Y.-W.Lui, Krishichayan, J.Button, G.Bonasera, S.Shlomo Isoscalar E0, E1, E2, and E3 strength in 92, 96, 98, 100Mo NUCLEAR REACTIONS 92,96,98,100Mo(α, α'), E=240 MeV; measured Eα, Iα, angular distributions using multipole-dipole-multipole (MDM) spectrometer and a focal plane detector at Texas A and M K500 superconducting cyclotron facility. DWBA analysis of σ(θ) data. 92,96,98,100Mo; deduced isoscalar giant resonances and E0, E1, E2, and E3 transition strengths and EWSR. Comparison with spherical Hartree-Fock-RPA calculations using KDE0v1 Skyrme-type interaction.
doi: 10.1103/PhysRevC.92.014318
2014AU01 Phys.Rev. C 89, 014335 (2014) N.Auerbach, Ch.Stoyanov, M.R.Anders, S.Shlomo Isoscalar and isovector dipole strength distributions in nuclei and the Schiff moment NUCLEAR STRUCTURE 40,48Ca, 56,78Ni, 90,104Zr, 144Sm, 208Pb; calculated strength distribution S(E), S(E)/E, centroid energies, inverse energy moments of isoscalar and isovector dipole resonances (ISD and IVD). Influence dipole strength distribution on nuclear Schiff moment. Self-consistent HF-based RPA calculations using 18 different Skyrme-type effective interactions.
doi: 10.1103/PhysRevC.89.014335
2013AN05 Phys.Rev. C 87, 024303 (2013) M.R.Anders, S.Shlomo, T.Sil, D.H.Youngblood, Y.-W.Lui, Krishichayan Giant resonances in 40Ca and 48Ca NUCLEAR STRUCTURE 40,48Ca; calculated strength functions S(E), centroid energies of isoscalar and isovector (monopole, dipole, quadrupole, and octupole) giant resonances. Self-consistent Hartree-Fock-based random phase approximation calculations with 18 Skyrme-type nucleon-nucleon effective interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.87.024303
2013RO21 Phys.Rev. C 88, 024609 (2013) G.Ropke, S.Shlomo, A.Bonasera, J.B.Natowitz, S.J.Yennello, A.B.McIntosh, J.Mabiala, L.Qin, S.Kowalski, K.Hagel, M.Barbui, K.Schmidt, G.Giuliani, H.Zheng, S.Wuenschel Density determinations in heavy ion collisions
doi: 10.1103/PhysRevC.88.024609
2013YO07 Phys.Rev. C 88, 021301 (2013) D.H.Youngblood, Y.-W.Lui, Krishichayan, J.Button, M.R.Anders, M.L.Gorelik, M.H.Urin, S.Shlomo Unexpected characteristics of the isoscalar monopole resonance in the A ≈ 90 region: Implications for nuclear incompressibility NUCLEAR REACTIONS 90,92,94Zr, 92,96,98,100Mo(α, α'), E=240 MeV; measured α spectra, σ at low angles using Texas A-M cyclotron facility; deduced energies, centroids, widths, E0-EWSR for isoscalar giant monopole resonances (ISGMR), nuclear incompressibility. Comparison with HF-RPA calculations.
doi: 10.1103/PhysRevC.88.021301
2012HA04 Phys.Rev.Lett. 108, 062702 (2012) K.Hagel, R.Wada, L.Qin, J.B.Natowitz, S.Shlomo, A.Bonasera, G.Ropke, S.Typel, Z.Chen, M.Huang, J.Wang, H.Zheng, S.Kowalski, C.Bottosso, M.Barbui, M.R.D.Rodrigues, K.Schmidt, D.Fabris, M.Lunardon, S.Moretto, G.Nebbia, S.Pesente, V.Rizzi, G.Viesti, M.Cinausero, G.Prete, T.Keutgen, Y.El Masri, Z.Majka Experimental Determination of In-Medium Cluster Binding Energies and Mott Points in Nuclear Matter NUCLEAR REACTIONS 112,124Sn(40Ar, X), (64Zn, X), E=47 MeV/nucleon; measured reaction products, Eα, Iα. 2,3H, 3,4He; deduced temperature and density dependence, binding energies, Pauli blocking effects in a quantum statistical approach.
doi: 10.1103/PhysRevLett.108.062702
2012QI06 Phys.Rev.Lett. 108, 172701 (2012) L.Qin, K.Hagel, R.Wada, J.B.Natowitz, S.Shlomo, A.Bonasera, G.Ropke, S.Typel, Z.Chen, M.Huang, J.Wang, H.Zheng, S.Kowalski, M.Barbui, M.R.D.Rodrigues, K.Schmidt, D.Fabris, M.Lunardon, S.Moretto, G.Nebbia, S.Pesente, V.Rizzi, G.Viesti, M.Cinausero, G.Prete, T.Keutgen, Y.El Masri, Z.Majka, Y.G.Ma Laboratory Tests of Low Density Astrophysical Nuclear Equations of State NUCLEAR REACTIONS 112,124Sn(40Ar, X), (64Zn, X)2H/3H/3He/4He, E=47 MeV/nucleon; measured reaction products, Eα, Iα; deduced yields, equilibrium constants for α particle production. Astrophysical equation of state calculations.
doi: 10.1103/PhysRevLett.108.172701
2012SH27 J.Phys.:Conf.Ser. 337, 012014 (2012) Equation of State of Symmetric And Asymmetric Nuclear Matter At Various Densities And Temperatures NUCLEAR STRUCTURE 90Zr, 116Sn, 144Sm, 208Pb; calculated isoscalar giant magnetic resonance centroid energy using self-consistent RPA with different interactions. Compared to data.
doi: 10.1088/1742-6596/337/1/012014
2012WA20 Phys.Rev. C 85, 064618 (2012) R.Wada, K.Hagel, L.Qin, J.B.Natowitz, Y.G.Ma, G.Ropke, S.Shlomo, A.Bonasera, S.Typel, Z.Chen, M.Huang, J.Wang, H.Zheng, S.Kowalski, C.Bottosso, M.Barbui, M.R.D.Rodrigues, K.Schmidt, D.Fabris, M.Lunardon, S.Moretto, G.Nebbia, S.Pesente, V.Rizzi, G.Viesti, M.Cinausero, G.Prete, T.Keutgen, Y.El Masri, Z.Majka Nuclear matter symmetry energy at 0.03 ≤ ρ/ρ0 NUCLEAR REACTIONS 112,124Sn(40Ar, X), (64Zn, X), E=47 MeV/nucleon; measured charged particle and neutron spectra and multiplicity; deduced coalescence parameters and model volumes as a function of surface velocity, nuclear temperature, density, isoscaling parameter, symmetry free energy and symmetry entropy versus density. NIMROD multidetector at Texas A
doi: 10.1103/PhysRevC.85.064618
2011LU07 Phys.Rev. C 83, 044327 (2011) Y.-W.Lui, D.H.Youngblood, S.Shlomo, X.Chen, Y.Tokimoto, Krishichayan, M.Anders, J.Button Isoscalar giant resonances in 48Ca NUCLEAR REACTIONS 48Ca(α, α'), E=240 MeV; measured Eα, Iα, cross sections, σ(θ) for isoscalar giant resonances. 48Ca; deduced B(E2), B(E3), E0, E1, E2 E3+E4 energy-weighted sum rules (EWSR), isoscalar strength distributions, giant resonances, centroid energies. Comparison with mean-field-based random-phase approximation.
doi: 10.1103/PhysRevC.83.044327
2011NA20 Int.J.Mod.Phys. E20, 987 (2011) J.B.Natowitz, K.Hagel, R.Wada, L.Qin, Z.Chen, P.Sahu, G.Ropke, S.Kowalski, C.Bottosso, S.Shlomo, M.Barbui, D.Fabris, M.Lunardon, S.Moretto, G.Nebbia, S.Pesente, V.Rizzi, G.Viesti, M.Cinausero, G.Prete, T.Keutgen, Y.El Masri, Z.Majka Clustered low density nuclear matter in near Fermi energy collisions
doi: 10.1142/S0218301311019118
2010NA07 Phys.Rev.Lett. 104, 202501 (2010) J.B.Natowitz, G.Ropke, S.Typel, D.Blaschke, A.Bonasera, K.Hagel, T.Klahn, S.Kowalski, L.Qin, S.Shlomo, R.Wada, H.H.Wolter Symmetry Energy of Dilute Warm Nuclear Matter NUCLEAR REACTIONS 92Mo, 197Au(64Zn, X), E=35 MeV/nucleon; analyzed heavy-ion collision data; deduced free neutron and proton yields, temperatures, densities, symmetry energy. Quantum-statistical model of nuclear matter.
doi: 10.1103/PhysRevLett.104.202501
2010QI06 Nucl.Phys. A834, 521c (2010) L.Qin, J.B.Natowitz, G.Roepke, K.Hagel, R.Wada, Z.Chen, M.Huang, S.Kowalski, C.Bottosso, S.Shlomo, M.Barbui, A.Bonasera, M.Rodrigues, D.Fabris, M.Lunardon, S.Moretto, G.Nebbia, S.Pesente, V.Rizzi, G.Viesti, M.Cinausero, G.Prete, T.Keutgen, Y.El Masri, Z.Majka Laboratory Studies of low density matter
doi: 10.1016/j.nuclphysa.2010.01.081
2010SH18 Phys.Atomic Nuclei 73, 1390 (2010) Modern energy density functional for nuclei and the nuclear matter equation of state
doi: 10.1134/S1063778810080120
2010SH33 Iader.Fiz.Enerh. 11, 347 (2010); Nuc.phys.atom.energ. 11, 347 (2010) Freeze-out properties of hot nuclear matter created in heavy ion collisions NUCLEAR REACTIONS 58Ni(40Ca, X), (40Ar, X), 58Fe(40Ca, X), (40Ar, X), E=33 MeV/nucleon; analyzed data; deduced temperature, baryon density.
2009AU02 Phys.Rev.Lett. 103, 172501 (2009) η/s Ratio in Finite Nuclei
doi: 10.1103/PhysRevLett.103.172501
2009SH12 Phys.Rev. C 79, 034604 (2009) S.Shlomo, G.Ropke, J.B.Natowitz, L.Qin, K.Hagel, R.Wada, A.Bonasera Effect of medium dependent binding energies on inferring the temperatures and freeze-out density of disassembling hot nuclear matter from cluster yields
doi: 10.1103/PhysRevC.79.034604
2008SH27 Iader.Fiz.Enerh. 9 no.3, 7 (2008); Nuc.phys.atom.energ. 9, no.3, 7 (2008) Mean-field approximation for finite nuclei and nuclear matter NUCLEAR STRUCTURE 90Zr, 116Sn, 144Sm, 208Pb; calculated isoscalar monopole resonance. 16,24O, 34Si, 40,48Ca, 48,56,68,78Ni, 88Sr, 90Zr, 100,132Sn, 208Pb;calculated binding energies, charge rms radii. Self-consistent Hartree-Fock based random phase approximation. Comparison with experimental data.
doi: 10.15407/jnpae
2007KO04 Phys.Rev. C 75, 014601 (2007) S.Kowalski, J.B.Natowitz, S.Shlomo, R.Wada, K.Hagel, J.Wang, T.Materna, Z.Chen, Y.G.Ma, L.Qin, A.S.Botvina, D.Fabris, M.Lunardon, S.Moretto, G.Nebbia, S.Pesente, V.Rizzi, G.Viesti, M.Cinausero, G.Prete, T.Keutgen, Y.El Masri, Z.Majka, A.Ono Experimental determination of the symmetry energy of a low density nuclear gas NUCLEAR REACTIONS 92Mo, 197Au(64Zn, X), E=35 MeV/nucleon; measured light charged particle spectra, multiplicities, yield ratios; deduced temperature- and density-dependent symmetry energy coefficients.
doi: 10.1103/PhysRevC.75.014601
2007KO51 Nucl.Phys. A787, 619c (2007) S.Kowalski, J.B.Natowitz, S.Shlomo, R.Wada, K.Hagel, J.Wang, T.Materna, Z.Chen, Y.G.Ma, L.Qin, A.S.Botvina, D.Fabris, M.Lunardon, S.Moretto, G.Nebbia, S.Pesente, V.Rizzi, G.Viesti, M.Cinausero, G.Prete, T.Keutgen, Y.El Masri, Z.Majka, A.Ono Clustering and Symmetry Energy in a Low Density Nuclear Gas NUCLEAR REACTIONS 92Mo, 197Au(64Zn, X), E=35 MeV/nucleon; analyzed charged-particle and neutron mutliplicities; deduced cluster formation, reaction mechanism features and isoscaling parameters.
doi: 10.1016/j.nuclphysa.2006.12.092
2007SH51 Iader.Fiz.Enerh. 8 no.3, 7 (2007); Nuc.phys.atom.energ. 8, no.3, 7 (2007) The equation of state of symmetric and asymmetric nuclear matter NUCLEAR STRUCTURE 80Zr; calculated isoscalar multipole giant resonances centroid positions. 208Pb; calculated isoscalar multipole strength functions. 90Zr, 116Sn, 144Sm, 208Pb; calculated isoscalar giant monopole and isoscalar giant dipole resonance energies.Self-consistent HF-RPA calculations.
doi: 10.15407/jnpae
2006DE16 Phys.Rev. C 73, 034602 (2006) J.N.De, S.K.Samaddar, S.Shlomo, J.B.Natowitz Continuous phase transition and negative specific heat in finite nuclei NUCLEAR STRUCTURE 40,50Ca, 150Re, 150Nd; calculated thermodynamic quantities, phase transition features. Heated liquid-drop model.
doi: 10.1103/PhysRevC.73.034602
2006KO08 Phys.Rev. C 73, 024312 (2006) V.M.Kolomietz, A.G.Magner, S.Shlomo Splitting of the isovector giant dipole resonance in neutron-rich spherical nuclei NUCLEAR STRUCTURE A=40-240; analyzed GDR energies, splitting mechanisms. Fermi-liquid-drop model.
doi: 10.1103/PhysRevC.73.024312
2006KO48 Phys.Scr. 73, 458 (2006) V.M.Kolomietz, S.V.Radionov, S.Shlomo The influence of memory effects on dispersions of kinetic energy at nuclear fission
doi: 10.1088/0031-8949/73/5/008
2006SH17 Phys.Atomic Nuclei 69, 1132 (2006) S.Shlomo, T.Sil, V.K.Au, O.G.Pochivalov Current Status of Equation of State of Nuclear Matter NUCLEAR STRUCTURE 80Zr, 100,116Sn; calculated isoscalar strength distributions. 90Zr, 116Sn, 144Sm, 208Pb; calculated isoscalar giant monopole resonance energies. Fully self-consistent approach.
doi: 10.1134/S1063778806070064
2006SH21 Eur.Phys.J. A 30, 23 (2006) S.Shlomo, V.M.Kolomietz, G.Colo Deducing the nuclear-matter incompressibility coefficient from data on isoscalar compression modes NUCLEAR STRUCTURE 90Zr, 116Sn, 208Pb; analyzed GMR and GDR features; deduced incompressibility coefficient.
doi: 10.1140/epja/i2006-10100-3
2006SH30 Int.J.Mod.Phys. E15, 1909 (2006) Nuclear matter properties from collective modes in nuclei
doi: 10.1142/S0218301306005423
2006SI10 Phys.Rev. C 73, 034316 (2006) T.Sil, S.Shlomo, B.K.Agrawal, P.-G.Reinhard Effects of self-consistency violation in Hartree-Fock RPA calculations for nuclear giant resonances revisited NUCLEAR STRUCTURE 16O, 40,60Ca, 56Ni, 80,90,110Zr, 100,116Sn, 144Sm, 208Pb; calculated isoscalar and isovector giant resonance energies, consequences of self-consistency violation. 208Pb; calculated giant resonance strength functions.
doi: 10.1103/PhysRevC.73.034316
2005AG10 Phys.Rev. C 72, 014310 (2005) Determination of the parameters of a Skyrme type effective interaction using the simulated annealing approach NUCLEAR STRUCTURE 16,24O, 34Si, 40,48Ca, 48,56,68,78Ni, 88Sr, 90Zr, 100,132Sn, 208Pb; analyzed binding energies, radii, breathing-mode energies, related data; deduced Skyrme parameters. 40Ca, 208Pb; calculated single-particle energies. Simulated annealing approach.
doi: 10.1103/PhysRevC.72.014310
2005AG16 Eur.Phys.J. A 25, Supplement 1, 525 (2005) Breathing mode energy and nuclear matter incompressibility coefficient within relativistic and non-relativistic models NUCLEAR STRUCTURE 16O, 40,48Ca, 90Zr, 116,132Sn, 208Pb; calculated binding energies, radii. 90Zr, 116Sn, 144Sm, 208Pb; calculated breathing mode energies.
doi: 10.1140/epjad/i2005-06-003-7
2005SH01 Rep.Prog.Phys. 68, 1 (2005) Hot nuclei
doi: 10.1088/0034-4885/68/1/R01
2004AG04 Phys.Rev. C 70, 014308 (2004) Consequences of self-consistency violations in Hartree-Fock random-phase approximation calculations of the nuclear breathing mode energy NUCLEAR STRUCTURE 40,60Ca, 56Ni, 80,90,110Zr, 100Sn, 208Pb; calculated giant monopole resonance energies, effect of self-consistency violations. Hartree-Fock RPA.
doi: 10.1103/PhysRevC.70.014308
2004AG06 Phys.Rev. C 70, 057302 (2004) Critical densities for the Skyrme type effective interactions
doi: 10.1103/PhysRevC.70.057302
2004KO04 Phys.Rep. 390, 133 (2004) Nuclear Fermi-liquid drop model
doi: 10.1016/j.physrep.2003.10.013
2004KO10 Phys.Rev. C 69, 024314 (2004) V.M.Kolomietz, S.V.Lukyanov, S.Shlomo Shape fluctuations in a Fermi system with nonlinear dissipativity
doi: 10.1103/PhysRevC.69.024314
2004NA05 Int.J.Mod.Phys. E13, 269 (2004) J.B.Natowitz, K.Hagel, Y.Ma, M.Murray, L.Qin, S.Shlomo, R.Wada, J.Wang Relationships between caloric curves and the critical point of nucleonic matter
doi: 10.1142/S0218301304002041
2004SA29 Phys.Rev. C 69, 064615 (2004) S.K.Samaddar, J.N.De, S.Shlomo Flow effects on multifragmentation in the canonical model NUCLEAR STRUCTURE 109Ag, 197Au; calculated fragment multiplicities, flow effects in multifragmentation of hot nuclei. Analytically solvable canonical model.
doi: 10.1103/PhysRevC.69.064615
2004SH13 Nucl.Phys. A734, 589 (2004) Status of the nuclear matter equation of state as determined from compression modes NUCLEAR STRUCTURE 90Zr, 116Sn, 144Sm, 208Pb; calculated giant monopole resonance energies, incompressibility coefficient. 208Pb; calculated GDR strength distribution. Several models compared with data.
doi: 10.1016/j.nuclphysa.2004.01.108
2004SI01 Phys.Rev. C 69, 014602 (2004) T.Sil, S.K.Samaddar, J.N.De, S.Shlomo Liquid-gas phase transition in infinite and finite nuclear systems NUCLEAR STRUCTURE 50Ca, 150,186Re; calculated thermodynamic quantities, phase transition features. Heated liquid drop model.
doi: 10.1103/PhysRevC.69.014602
2003AG04 Phys.Rev. C 67, 034314 (2003) B.K.Agrawal, S.Shlomo, A.I.Sanzhur Self-consistent Hartree-Fock based random phase approximation and the spurious state mixing NUCLEAR STRUCTURE 80Zr; calculated isoscalar giant resonance strength functions, transition densities, spurious state mixing effects. Self-consistent Hartree-Fock, continuum RPA.
doi: 10.1103/PhysRevC.67.034314
2003AG10 Phys.Rev. C 68, 031304 (2003) Nuclear matter incompressibility coefficient in relativistic and nonrelativistic microscopic models NUCLEAR STRUCTURE 16O, 40,48Ca, 90Zr, 116,132Sn, 208Pb; analyzed binding energies, radii; deduced parameters. 90Zr, 116Sn, 144Sm, 208Pb; analyzed giant monopole resonance parameters; deduced nuclear matter incompressibility coefficient. Comparison of relativistic and nonrelativistic approaches.
doi: 10.1103/PhysRevC.68.031304
2003KO37 Phys.Rev. C 68, 014614 (2003) V.M.Kolomietz, A.I.Sanzhur, S.Shlomo Non-Markovian effects on the dynamics of bubble growth in hot asymmetric nuclear matter
doi: 10.1103/PhysRevC.68.014614
2003SH30 Nucl.Phys. A719, 225c (2003) S.Shlomo, A.I.Sanzhur, B.K.Agrawal Isoscalar giant monopole and dipole resonances and the nuclear matter incompressibility coefficient NUCLEAR REACTIONS 116Sn(α, α'), E=240 MeV; calculated isoscalar GDR strength distribution, excitation σ(E). RPA approach, comparison with data.
doi: 10.1016/S0375-9474(03)00923-0
2003SH34 Nucl.Phys. A722, 98c (2003) Current status of the nuclear matter incompressibility coefficient as deduced from data on compression modes NUCLEAR REACTIONS 116Sn(α, α'), E=240 MeV; analyzed giant resonance excitation σ, energy weighted sum rule, nuclear matter incompressibility coefficient.
doi: 10.1016/S0375-9474(03)01343-5
2003SH39 Phys.Rev. C 68, 064301 (2003) S.Shlomo, V.M.Kolomietz, B.K.Agrawal Isoscalar giant monopole resonance and its overtone in microscopic and macroscopic models NUCLEAR STRUCTURE 90Zr, 116Sn, 144Sm, 208Pb; calculated isoscalar giant monopole resonance centroid energies. 208Pb; calculated giant resonance transition densities.
doi: 10.1103/PhysRevC.68.064301
2002KO08 Yad.Fiz. 65, 68 (2002); Phys.Atomic Nuclei 65, 65 (2002) Surface Instability of a Nuclear Fermi Liquid Drop NUCLEAR STRUCTURE 40,48Ca, 208Pb; calculated stiffness coefficient vs temperature, limiting temperature vs deformation. Liquid drop model.
doi: 10.1134/1.1446555
2002NA22 Phys.Rev. C66, 031601 (2002) J.B.Natowitz, K.Hagel, Y.Ma, M.Murray, L.Qin, S.Shlomo, R.Wada, J.Wang Caloric Curves and Nuclear Expansion NUCLEAR STRUCTURE A=30-240; 90Zr; calculated, analyzed density vs excitation energy. Expanding Fermi gas hypothesis.
doi: 10.1103/PhysRevC.66.031601
2002SH12 Phys.Rev. C65, 044310 (2002) Isoscalar Giant Dipole Resonance and Nuclear Matter Incompressibility Coefficient NUCLEAR STRUCTURE 116Sn, 208Pb; calculated isoscalar GDR strength functions. Removal of contributions from spurious state mixing discussed. Hartree-Fock RPA approach.
doi: 10.1103/PhysRevC.65.044310
2002SH45 Acta Phys.Hung.N.S. 16, 303 (2002) Nuclear Equation of State and Compression Modes NUCLEAR STRUCTURE 116Sn, 208Pb; calculated GDR strength functions, equation of state. Self-consistent RPA.
doi: 10.1556/APH.16.2002.1-4.33
2001AG09 Phys.Rev. C64, 024305 (2001) B.K.Agrawal, T.Sil, S.K.Samaddar, J.N.De, S.Shlomo Coulomb Energy Differences in Mirror Nuclei Revisited NUCLEAR STRUCTURE 15,16,17O, 32S, 39,40,41,48Ca, 56Ni, 90Zr, 208Pb; calculated radii. 15,17O, 15N, 17F, 39,41Ca, 39K, 41Sc, 55,57Ni, 55Co, 57Cu; calculated Coulomb displacement energies. Relativistic mean-field model, comparison with other models and data.
doi: 10.1103/PhysRevC.64.024305
2001KO47 Phys.Rev. C64, 024315 (2001) V.M.Kolomietz, A.I.Sanzhur, S.Shlomo, S.A.Firin Equation of State and Phase Transitions in Asymmetric Nuclear Matter
doi: 10.1103/PhysRevC.64.024315
2001KO60 Phys.Rev. C64, 044304 (2001) Sound Modes in Hot Nuclear Matter
doi: 10.1103/PhysRevC.64.044304
2001KO70 Phys.Rev. C64, 054302 (2001) V.M.Kolomietz, S.V.Radionov, S.Shlomo Memory Effects on Descent from the Nuclear Fission Barrier NUCLEAR STRUCTURE 236U; calculated collective variables time evolution for fissioning system, fragment kinetic energies vs relaxation time, role of memory effect in saddle-to-scission time.
doi: 10.1103/PhysRevC.64.054302
2001SH45 Pramana 57, 557 (2001) Compression Modes and the Nuclear Matter Incompressibility Coefficient NUCLEAR STRUCTURE 28Si, 40Ca, 58Ni, 116Sn, 208Pb; calculated monopole strength distributions, resonance and incompressibility features. Hartree-Fock-RPA approach.
doi: 10.1007/s12043-001-0062-4
2000GO38 Phys.Rev. C62, 044301 (2000) M.L.Gorelik, S.Shlomo, M.H.Urin Structure and Direct Nucleon Decay Properties of Isoscalar Giant Monopole and Dipole Resonances NUCLEAR STRUCTURE 90Zr, 116,124Sn, 144Sm, 208Pb; calculated isoscaler giant monopole resonance energies, widths, nucleon escape widths. Continuum RPA, comparisons with data.
doi: 10.1103/PhysRevC.62.044301
2000KO12 Phys.Rev. C61, 034312 (2000) A.Kolomiets, O.Pochivalov, S.Shlomo Microscopic Description of Excitation of Nuclear Isoscalar Giant Resonances by Inelastic Scattering of 240 MeV α Particles NUCLEAR REACTIONS 28Si, 40Ca, 58Ni, 116Sn(α, α), (α, α'), E=240 MeV; analyzed σ(θ). 28Si, 40Ca, 58Ni, 116Sn deduced isoscalar giant monopole, quadrupole resonance features. Folding model DWBA, microscopic RPA.
doi: 10.1103/PhysRevC.61.034312
2000KO29 Phys.Rev. C61, 064302 (2000) Isoscalar Compression Modes within Fluid Dynamic Approach NUCLEAR STRUCTURE A=90-210; calculated isoscalar giant monopole, dipole resonance energies. 208Pb; calculated resnonance energies, widths vs incompressibility, damping parameter. Fluid dynamic approach.
doi: 10.1103/PhysRevC.61.064302
1999KO07 Yad.Fiz. 62, No 1, 91 (1999); Phys.Atomic Nuclei 62, 86 (1999) V.M.Kolomietz, S.V.Lukyanov, V.A.Plujko, S.Shlomo Two-Body Contribution to the Relaxation of Collective Excitations in Cold Finite Fermi Systems
1999KO22 Phys.Rev. C59, 3139 (1999) A.Kolomiets, V.M.Kolomietz, S.Shlomo Giant Monopole Resonance and Nuclear Incompressibility within the Fermi-Liquid Drop Model
doi: 10.1103/PhysRevC.59.3139
1999KO40 Phys.Rev. C60, 044612 (1999) Low Density Instability in a Nuclear Fermi-Liquid Drop NUCLEAR STRUCTURE 40Ca, 208Pb; calculated liquid-drop instability features, dependence on multipolarity of particle density fluctuations.
doi: 10.1103/PhysRevC.60.044612
1999MU06 Phys.Rev. C59, 2040 (1999) S.E.Muraviev, I.Rotter, S.Shlomo, M.H.Urin 4(h-bar)ω Isoscalar Monopole Giant Resonance in 208Pb and Resonance Trapping NUCLEAR STRUCTURE 208Pb; calculated 4(h-bar)ω isoscalar giant monopole resonance strength function; deduced continuum coupling role, resonance trapping effect. Continuum-RPA approach.
doi: 10.1103/PhysRevC.59.2040
1998AB16 Phys.Rev. C57, 2342 (1998) V.I.Abrosimov, O.I.Davidovskaja, V.M.Kolomietz, S.Shlomo Free Surface Response in a Finite Fermi System
doi: 10.1103/PhysRevC.57.2342
1998AG13 Phys.Rev. C58, 3004 (1998) B.K.Agrawal, S.K.Samaddar, J.N.De, S.Shlomo Large-Model-Space Calculation of the Nuclear Level Density Parameter at Finite Temperature NUCLEAR STRUCTURE 40Ca, 56Fe; calculated level density parameter vs temperature; deduced shell effects, continuum corrections, other contributions. Microscopic model.
doi: 10.1103/PhysRevC.58.3004
1998DE07 Phys.Rev. C57, 1398 (1998) J.N.De, S.Shlomo, S.K.Samaddar Level Density Parameter in a Refined Thomas-Fermi Theory NUCLEAR STRUCTURE 150Sm; calculated level density parameter vs temperature. Thomas-Fermi theory, second-order corrections.
doi: 10.1103/PhysRevC.57.1398
1998DE12 Nucl.Phys. A630, 192c (1998) Liquid-Gas Phase Transition in Finite Nuclei NUCLEAR STRUCTURE 150Sm; calculated caloric curve, specific heat; deduced phase transition. Thomas-Fermi theory.
doi: 10.1016/S0375-9474(97)00756-2
1998KO19 Phys.Rev. C57, R2808 (1998) A.Kolomiets, V.M.Kolomietz, S.Shlomo Shell Effects on Nuclear Incompressibility
doi: 10.1103/PhysRevC.57.R2808
1998KO26 Phys.Rev. C58, 198 (1998) V.M.Kolomietz, S.V.Lukyanov, V.A.Plujko, S.Shlomo Collisional Relaxation of Collective Motion in a Finite Fermi Liquid
doi: 10.1103/PhysRevC.58.198
1998RO21 Phys.Rev. C58, 884 (1998) Magnetic Dipole Moments of Odd-Odd N = Z Nuclei NUCLEAR STRUCTURE 2H, 6Li, 10B, 14N, 18F, 22Na, 26Al, 38K, 46V; calculated ground, low-lying states μ. Core-deuteron cluster model. Comparison with data.
doi: 10.1103/PhysRevC.58.884
1997DE09 Phys.Rev. C55, R1641 (1997) J.N.De, S.Das Gupta, S.Shlomo, S.K.Samaddar Caloric Curve for Finite Nuclei in Thomas-Fermi Theory NUCLEAR STRUCTURE 150Sm; calculated proton density profile vs temperature, volume, temperature vs excitation energy per particle, specific heat per particle vs temperature. 85Kr; calculated temperature vs excitation energy per particle, specific heat per particle vs temperature. Finite temperature Thomas-Fermi theory.
doi: 10.1103/PhysRevC.55.R1641
1997KO03 Phys.Rev. C55, 1376 (1997) A.Kolomiets, V.M.Kolomietz, S.Shlomo Determination of the Temperature of a Disassembling Nucleus from Fragment Yields
doi: 10.1103/PhysRevC.55.1376
1997SA62 Phys.Rev.Lett. 79, 4962 (1997) S.K.Samaddar, J.N.De, S.Shlomo Effect of Flow on the Caloric Curve for Finite Nuclei NUCLEAR STRUCTURE 150Sm; calculated energy, specific heat per nucleon vs temperature, proton rms radius, density; deduced liquid-gas phase transition. Finite temperature Thomas-Fermi theory.
doi: 10.1103/PhysRevLett.79.4962
1997SH15 Phys.Rev. C55, 1972 (1997) S.Shlomo, V.M.Kolomietz, H.Dejbakhsh Single Particle Level Density in a Finite Depth Potential Well
doi: 10.1103/PhysRevC.55.1972
1997SH17 Phys.Rev. C55, R2155 (1997) Effect of Flow on the Freeze-Out Density and Temperature of Disassembling Hot Nuclei
doi: 10.1103/PhysRevC.55.R2155
1997WA01 Phys.Rev. C55, 227 (1997) R.Wada, R.Tezkratt, K.Hagel, F.Haddad, A.Kolomiets, Y.Lou, J.Li, M.Shimooka, S.Shlomo, D.Utley, B.Xiao, N.Mdeiwayeh, J.B.Natowitz, Z.Majka, J.Cibor, T.Kozik, Z.Sosin Excitation Energies and Temperatures of Hot Nuclei Produced in the Reactions of 63Cu + 197Au at 35A MeV NUCLEAR REACTIONS 197Au(63Cu, X), E=35 MeV/nucleon; measured energy, multiplicity of n, p, d, t, 3He, α, intermediate mass fragment (Z ≤ 10) heavy fragments (60 ≤ A ≤ 170)-coin, mass and velocity of heavy fragments; deduced temperatures, excitation energies of primary heavy fragments. Dynamical plus statistical model, QMD model simulations.
doi: 10.1103/PhysRevC.55.227
1996BO05 Phys.Rev. C53, 855 (1996) Ye.A.Bogila, V.M.Kolomietz, A.I.Sanzhur, S.Shlomo Preequilibrium Decay in the Exciton Model for Nuclear Potential with a Finite Depth NUCLEAR STRUCTURE 40Ca; calculated transition, total decay rates for given exciton state, preequilibrium nucleon emission particle spectra. Exciton model, particle-hole level density.
doi: 10.1103/PhysRevC.53.855
1996KI16 Nucl.Phys. A608, 32 (1996) D.Kiderlen, V.M.Kolomietz, S.Shlomo Nuclear Shape Fluctuations in Fermi-Liquid Drop Model
doi: 10.1016/S0375-9474(96)00274-6
1996KO14 Phys.Rev. C54, R472 (1996) A.Kolomiets, E.Ramakrishnan, H.Johnston, F.Gimeno-Nogues, B.Hurst, D.O'Kelly, D.J.Rowland, S.Shlomo, T.White, J.Winger, S.J.Yennello Nuclear Temperature of the Disassembling Source in Central Heavy-Ion Collisions from Isotope Yields NUCLEAR REACTIONS 58Ni, 58Fe(40Ca, X), (40Ar, X), E=33 MeV/nucleon; analyzed isotopic yields for Z=2-6 isotopes; deduced nuclear temperature. Statistical model approach.
doi: 10.1103/PhysRevC.54.R472
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