NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = J.Randrup Found 146 matches. Showing 1 to 100. [Next]2023GI01 Phys.Rev. C 107, 014612 (2023) N.P.Giha, S.Marin, J.A.Baker, I.E.Hernandez, K.J.Kelly, M.Devlin, J.M.O'Donnell, R.Vogt, J.Randrup, P.Talou, I.Stetcu, A.E.Lovell, O.Litaize, O.Serot, A.Chebboubi, C.-Y.Wu, S.D.Clarke, S.A.Pozzi Correlations between energy and γ-ray emission in 239Pu(n, f) NUCLEAR REACTIONS 239Pu(n, f), E=2-40 MeV; measured fragments, En, In, Eγ, Iγ, (fragments)γ-coin, (fragment)n-coin, nγ-coin; deduced γ spectrum, γ multiplicity, linear relation between incident neutron energy and γ multiplicity. Comparison to fission model calculations done with CGMF, FIFRELIN and FREYA codes. Multiplicity results are compared to ENDF/B-VIII.0 data and to experimental data on 238U(n, F), 239Pu(d, F), 233Pu(d, F), 240Pu(d, F) reactions. Broad-spectrum neutron beam produced via spallation reaction of an 800 MeV proton beam on W target (Los Alamos Neutron Science Center). Chi-Nu liquid scintillator array, a hemispherical array of 54 EJ-309 (n- and γ- measurement) surrounding multifoil parallel-plate avalanche counter (PPAC) serving as target and contain ing 239Pu (fragment measurement).
doi: 10.1103/PhysRevC.107.014612
2023GJ01 Phys.Rev. C 108, 064602 (2023) D.Gjestvang, J.N.Wilson, A.Al-Adili, S.Siem, Z.Gao, J.Randrup, D.Thisse, M.Lebois, N.Jovancevic, R.Canavan, M.Rudigier, D.Etasse, R.-B.Gerst, E.Adamska, P.Adsley, A.Algora, C.Belvedere, J.Benito, G.Benzoni, A.Blazhev, A.Boso, S.Bottoni, M.Bunce, R.Chakma, N.Cieplicka-Orynczak, S.Courtin, M.L.Cortes, P.Davies, C.Delafosse, M.Fallot, B.Fornal, L.Fraile, A.Gottardo, V.Guadilla, G.Hafner, K.Hauschild, M.Heine, C.Henrich, I.Homm, F.Ibrahim, L.W.Iskra, P.Ivanov, S.Jazrawi, A.Korgul, P.Koseoglou, T.Kroll, T.Kurtukian-Nieto, S.Leoni, J.Ljungvall, A.Lopez-Martens, R.Lozeva, I.Matea, K.Miernik, J.Nemer, S.Oberstedt, W.Paulsen, M.Piersa-Silkowska, Y.Popovitch, C.Porzio, L.Qi, P.H.Regan, K.Rezynkina, V.Sanchez-Tembleque, C.Schmitt, P.-A.Soderstrom, C.Surder, G.Tocabens, V.Vedia, D.Verney, N.Warr, B.Wasilewska, J.Wiederhold, M.Yavahchova, S.Ziliani Examination of how properties of a fissioning system impact isomeric yield ratios of the fragments
doi: 10.1103/PhysRevC.108.064602
2022MA26 Phys.Rev. C 105, 054609 (2022) S.Marin, E.P.Sansevero, M.S.Okar, I.E.Hernandez, R.Vogt, J.Randrup, S.D.Clarke, V.A.Protopopescu, S.A.Pozzi Directional dependence of the event-by-event neutron-γ multiplicity correlations in 252Cf(sf) RADIOACTIVITY 252Cf(SF); analyzed Eg and En data collected at the Chi-Nu array at the Los Alamos Neutron Science Center with considering the angle between the emitted particles in addition to their individual energies; deduced nγ-correlations, enhancement of γ-emission around 0.7 and 1.2 MeV, directional alignment for Eγ below 0.7 MeV, correlation between fragment excitation energies and angular momentum. Comparison with model calculations.
doi: 10.1103/PhysRevC.105.054609
2022RA19 Phys.Rev. C 106, 014609 (2022) Probing fission fragment angular momenta by photon measurements RADIOACTIVITY 252Cf(SF); calculated relaxation times for wriggling, bending and twisting as function of neck radius, angular distribution of the collective E2 photons from fission fragments, average angular distribution coefficients, distribution of the opening angle between pairs of E2 photons emitted from even-even product partners. Discussed how certain photon measurements may helpin investigations the of the various rotational modes in fission. Simulations with fission event generator FREYA.
doi: 10.1103/PhysRevC.106.014609
2022RA26 Phys.Rev. C 106, L051601 (2022) Coupled fission fragment angular momenta RADIOACTIVITY 252Cf(SF); calculated fission fragments spin opening angle, spin-spin opening angle distribution. Direct microcanonical and normalmodes sampling procedures. Comparing with calculations made with FREYA code and results obtained in the framework of antisymmetrized molecular dynamics. NUCLEAR REACTIONS 235U(n, F), E=thermal; distribution of the fragment spin opening angle. 2D sampling of the three angular momenta, using moments of inertia corresponding either to touching or to scission.
doi: 10.1103/PhysRevC.106.L051601
2021AL03 Phys.Rev. C 103, 014609 (2021) M.Albertsson, B.G.Carlsson, T.Dossing, P.Moller, J.Randrup, S.Aberg Correlation studies of fission-fragment neutron multiplicities NUCLEAR REACTIONS 235U(n, F), E=0, 5.55 MeV; calculated total fragment kinetic energy (TKE) and distribution of TKE versus heavy-fragment mass number, number of scission events in log scale versus fission fragment mass number and total kinetic energy (TKE), probability distribution for the heavy-fragment share of intrinsic energy, average of the light and heavy-fragment intrinsic energies, average fragment distortion energies and deformations at scission versus TKE, average multiplicity of neutrons evaporated from the light or heavy fragment as function of TKE. Nuclear shape evolution from the ground-state shape to scission obtained from METROPOLIS walk method on the five-dimensional potential-energy surfaces, calculated with the macroscopic-microscopic method for the three-quadratic-surface (3QS) parametrization.
doi: 10.1103/PhysRevC.103.014609
2021AL31 Phys.Rev. C 104, 064616 (2021) M.Albertsson, B.G.Carlsson, T.Dossing, P.Moller, J.Randrup, S.Aberg Super-short fission mode in fermium isotopes RADIOACTIVITY 256,258,260,262Fm(SF); calculated potential energy along the paths for the standard and the super-short fission modes, as function of quadrupole moment. 260Fm(SF); calculated contour plots of the number of fission in the A-TKE plane based on 105 spontaneous or thermal fission events. 254,256,258,260,262,264,266,268Fm(SF); calculated contour plot of fraction of fissions via the super-short mode, with typical scission shapes for the two modes. 254,256,258,260Fm(SF); calculated primary fragment mass yields for spontaneous and thermal fission, total kinetic-energy (TKE) distributions. 254,256,258,260,262,264,266,268Fm, 259,260Md(SF); calculated TKE and average total neutron multiplicity versus the neutron number of the initial nucleus. Metropolis method for the super-short fission mode to simulate the strongly damped fission dynamics driven by shape- and energy-dependent level densities, and analyzing scission configurations. Comparison with experimental data.
doi: 10.1103/PhysRevC.104.064616
2021GJ01 Phys.Rev. C 103, 034609 (2021) D.Gjestvang, S.Siem, F.Zeiser, J.Randrup, R.Vogt, J.N.Wilson, F.Bello-Garrote, L.A.Bernstein, D.L.Bleuel, M.Guttormsen, A.Gorgen, A.C.Larsen, K.L.Malatji, E.F.Matthews, A.Oberstedt, S.Oberstedt, T.Tornyi, G.M.Tveten, A.S.Voyles Excitation energy dependence of prompt fission γ-ray emission from 241Pu NUCLEAR REACTIONS 240Pu(d, pF)241Pu*, E=13.5 MeV; measured outgoing protons using SiRi, a silicon ΔE-E detector, fission fragments using NIFF, consisting of four parallel plate avalanche counters (PPACs), prompt fission γ rays (PFG), (particle)γ-coin using Oslo Scintillator Array (OSCAR) of 30 LaBr3:Ce scintillators for γ radiation at the Oslo Cyclotron Laboratory; deduced average total PFG multiplicity per fission, average total PFG energy released per fission, and the average PFG energy in the excitation range of 5.75-8.25 MeV. Comparison with simulations using the fission model FREYA, with previous experimental results, and evaluation in ENDF/B-VIII.0.
doi: 10.1103/PhysRevC.103.034609
2021MA51 Phys.Rev. C 104, L021601 (2021) P.Marevic, N.Schunck, J.Randrup, R.Vogt Angular momentum of fission fragments from microscopic theory NUCLEAR REACTIONS 239Pu(n, F), E=thermal; calculated angular-momentum distributions of 24 fission fragments over a wide range of fragment masses, and total average photon multiplicities. 239Pu(n, F)128Sn/132Sn/138Xe/130Sn/150Ce/110Ru/90Kr, E=thermal; calculated angular-momentum distributions of primary fission fragments, with binding energy calculated as a function of the quadrupole deformation parameter β2 using the HFB model; deduced dependency of nuclear shell structure and deformation on the angular momentum of the fragments. Calculations used fission model FREYA, and a starting set of 1545 scission configurations.
doi: 10.1103/PhysRevC.104.L021601
2021MA54 Phys.Rev. C 104, 024602 (2021) S.Marin, M.S.Okar, E.P.Sansevero, I.E.Hernandez, C.A.Ballard, R.Vogt, J.Randrup, P.Talou, A.E.Lovell, I.Stetcu, O.Serot, O.Litaize, A.Chebboubi, S.D.Clarke, V.A.Protopopescu, S.A.Pozzi Structure in the event-by-event energy-dependent neutron-γ multiplicity correlations in 252Cf(sf) RADIOACTIVITY 252Cf(SF); analyzed Eγ and E(n) data collected at the Chi-Nu array at the Los Alamos Neutron Science Center with the application of the normalized differential multiplicity covariances; deduced neutron-γ correlations, evidence for enhancements in neutron-γ correlations around Eγ=0.7 and 1.2 MeV. Comparison with model calculations. Relevance to disagreement in the literature about correlations between neutron-γ competition and fragment properties.
doi: 10.1103/PhysRevC.104.024602
2021RA14 Phys.Rev.Lett. 127, 062502 (2021) Generation of Fragment Angular Momentum in Fission NUCLEAR REACTIONS 235,238U, 239Pu(n, F), E not given; calculated fission fragments distribution. Comparison with available data. The fission model FREYA. RADIOACTIVITY 252CF(SF); calculated fission fragments distribution. Comparison with available data. The fission model FREYA.
doi: 10.1103/PhysRevLett.127.062502
2021ST06 Nucl.Phys. A1005, 121867 (2021) J.Steinheimer, L.-G.Pang, K.Zhou, V.Koch, J.Randrup, H.Stoecker A machine learning study on spinodal clumping in heavy ion collisions
doi: 10.1016/j.nuclphysa.2020.121867
2021VO02 Phys.Rev. C 103, 014610 (2021) Angular momentum effects in fission NUCLEAR REACTIONS 235U(n, F), E=0.1, 20 MeV; calculated distribution of the opening angle between the spins of the two primary fission fragments, angular distribution of the evaporated neutrons relative to the spin direction of the emitting fragment, mean number of photons emitted as a function of the sum of spins of two primary fragments, contour plot of the velocity distribution of evaporated neutrons, distribution of neutron-neutron opening angle in the plane transverse to the direction of the light product nucleus. 235U(n, F), E>0, <1, >2 MeV; calculated laboratory angular distribution of the evaporated neutrons relative to the direction of the light primary fragment, with and without a rotational boost. 235U(n, F), E>2, <2 MeV; calculated two-neutron angular correlations. 235,235mU(n, F), E=thermal; calculated neutron multiplicity as a function of TKE. Calculations used fission simulation model FREYA, a Monte Carlo approach.
doi: 10.1103/PhysRevC.103.014610
2020AL01 Eur.Phys.J. A 56, 46 (2020) M.Albertsson, B.G.Carlsson, T.Dossing, P.Moller, J.Randrup, S.Aberg Calculated fission-fragment mass yields and average total kinetic energies of heavy and superheavy nuclei
doi: 10.1140/epja/s10050-020-00036-9
2020BE28 J.Phys.(London) G47, 113002 (2020) M.Bender, R.Bernard, G.Bertsch, S.Chiba, J.Dobaczewski, N.Dubray, S.A.Giuliani, K.Hagino, D.Lacroix, Z.Li, P.Magierski, J.Maruhn, W.Nazarewicz, J.Pei, S.Peru, N.Pillet, J.Randrup, D.Regnier, P.G.Reinhard, L.M.Robledo, W.Ryssens, J.Sadhukhan, G.Scamps, N.Schunck, C.Simenel, J.Skalski, I.Stetcu, P.Stevenson, S.Umar, M.Verriere, D.Vretenar, M.Warda, S.Aberg Future of nuclear fission theory
doi: 10.1088/1361-6471/abab4f
2020MU06 Phys.Rev. C 101, 054607 (2020) M.R.Mumpower, P.Jaffke, M.Verriere, J.Randrup Primary fission fragment mass yields across the chart of nuclides NUCLEAR REACTIONS 226Th, 235U, 259Md, 276No(n, F)227Th/236U/260Md/277No, T=0.5-1.5 MeV; 229Th, 237Np, 239Pu, 245Cm, 255,257Fm(n, F)230Th/238Np/240Pu/246Cm/256Fm/258Fm, E*=5.8-6.8 MeV; 205At, 208Rn, 209Fr, 211Ra, 216Ac, 222Th, 230Pa, 233U(n, F)206At/209Rn/210Fr/212Ra/217Ac/223Th/231Pa/234U, E*=11 MeV; calculated mass yield distributions. 236U, 240Pu, 234Cm; calculated projected potential energy surfaces. Z=80-130, A=171-330: calculated mass yield distributions for 3800 nuclei listed as tabular text files in the supplementary material. Finite-Range Liquid-Drop Model (FRLDM). Comparison with experimental data.
doi: 10.1103/PhysRevC.101.054607
2019RA13 Phys.Rev. C 99, 054619 (2019) Sensitivity of neutron observables to the model input in simulations of 252Cf(sf) RADIOACTIVITY 252Cf(SF); analyzed mass distribution, total kinetic energy (TKE), width of the total kinetic energy distribution of fission fragments; calculated neutron multiplicity distribution, neutron multiplicity covariance matrix elements, factorial moments of the neutron multiplicity distribution, neutron spectra, angular distribution of two neutrons, neutron energy-energy correlation, anticorrelation between average total kinetic energy and average neutron multiplicity using the FREYA code. Comparison with experimental data. COMPILATION 252Cf; compiled experimental data for spontaneous fission of 252Cf for mass-dependent fragment yields, the mass-dependent average total fragment kinetic energy (TKE), and the associated TKE dispersion σ(TKE, A) based on entries in the EXFOR database from 1963 to 2014.
doi: 10.1103/PhysRevC.99.054619
2019SC12 Phys.Rev. C 100, 014605 (2019) P.F.Schuster, M.J.Marcath, S.Marin, S.D.Clarke, M.Devlin, R.C.Haight, R.Vogt, P.Talou, I.Stetcu, T.Kawano, J.Randrup, S.A.Pozzi High resolution measurement of tagged two-neutron energy and angle correlations in 252Cf (sf) RADIOACTIVITY 252Cf(SF); measured prompt neutron time of flight, angular distribution of neutrons, nn-coin, prompt neutron emission anisotropy, correlations in angle and energy between prompt neutrons emitted in spontaneous fission using fission chamber and the Chi-Nu liquid scintillator detector array at LANSCE-LANL facility. Comparison with simulations produced by the fission event generators CGMF, FREYA, and MCNPX-POLIMI IPOL(1)=1.
doi: 10.1103/PhysRevC.100.014605
2018MA25 Phys.Rev. C 97, 044622 (2018) M.J.Marcath, R.C.Haight, R.Vogt, M.Devlin, P.Talou, I.Stetcu, J.Randrup, P.F.Schuster, S.D.Clarke, S.A.Pozzi Measured and simulated 252Cf(sf) prompt neutron-photon competition RADIOACTIVITY 252Cf(SF); measured Eγ, Iγ, E(n), I(n), nγ-coin, time of flight distributions for neutrons and photons, event-by-event neutron-photon correlation using Chi-Nu liquid scintillator array of 45 liquid organic scintillation detectors and a fission chamber at LANL; deduced neutron and photon multiplicities. Comparison with MCPNX-PoliMi simulation with CGMF and FREYA models.
doi: 10.1103/PhysRevC.97.044622
2018TA05 Eur.Phys.J. A 54, 9 (2018) P.Talou, R.Vogt, J.Randrup, M.E.Rising, S.A.Pozzi, J.Verbeke, M.T.Andrews, S.D.Clarke, P.Jaffke, M.Jandel, T.Kawano, M.J.Marcath, K.Meierbachtol, L.Nakae, G.Rusev, A.Sood, I.Stetcu, C.Walker Correlated prompt fission data in transport simulations COMPILATION 235U, 239Pu(n, F), E=thermal;252Cf(SF); compiled average prompt fission neutron multiplicity vs fragment mass, prompt fission neutron σ(En), γ-decay energy spectrum σ(Eγ), γ multiplicity, n-n angular correlation. Calculated σ, yields using FREYA and CGMF codes. Compared with data.
doi: 10.1140/epja/i2018-12455-0
2017CL01 Phys.Rev. C 95, 064612 (2017) S.D.Clarke, B.M.Wieger, A.Enqvist, R.Vogt, J.Randrup, R.C.Haight, H.Y.Lee, B.A.Perdue, E.Kwan, C.Y.Wu, R.A.Henderson, S.A.Pozzi Measurement of the energy and multiplicity distributions of neutrons from the photofission of 235U NUCLEAR REACTIONS 235U(γ, F), E<800 MeV white photon source; measured E(n), I(n), neutron time-of-flight spectrum, prompt fission neutron spectrum, neutron multiplicity distribution, average energy of correlated photofission neutron pairs as function of the angle between detectors at the WNR-15L beam line at LANSCE-LANL. Comparison with simulations using FREYA and MCNPX-POLIMI codes.
doi: 10.1103/PhysRevC.95.064612
2017VO13 Phys.Rev. C 96, 064620 (2017) Improved modeling of photon observables with the event-by-event fission model FREYA RADIOACTIVITY 252Cf(SF); calculated photon spectrum, average total photon energy, average photon multiplicity, and energy per photon as a function of fragment mass, total photon energy and the photon multiplicity as functions of total fragment kinetic energy with and without the GDR and RIPL-3, mean total photon energy, mean photon multiplicity and energy per photon as functions of fragment mass number, average fragment angular momentum as function of fragment mass, total photon energy, and photon multiplicity as functions of total fragment kinetic energy TKE, photon multiplicity distributions. Calculations using FREYA (Fission Reaction Event Yield Algorithm) code. Comparison with experimental data. NUCLEAR REACTIONS 233,235U, 239Pu(n, F), E=thermal; calculated total photon energy and photon multiplicity, energy per photon as function of fragment mass, total photon energy as a function of total fragment kinetic energy (TKE), photon energy spectrum. Calculations using FREYA (Fission Reaction Event Yield Algorithm) code. Comparison with experimental data.
doi: 10.1103/PhysRevC.96.064620
2017WA08 Phys.Rev. C 95, 024618 (2017) D.E.Ward, B.G.Carlsson, T.Dossing, P.Moller, J.Randrup, S.AAberg Nuclear shape evolution based on microscopic level densities NUCLEAR REACTIONS 226Th, 234,236U, 240Pu(γ, F), (n, F), E(n)=thermal; calculated yield of fragments as function of proton number and angular momentum and excitation energy using parameter-free microscopic level densities obtained with the Metropolis-walk method. Comparison with experimental data. NUCLEAR STRUCTURE 236U; calculated microscopic level density as a function of angular momentum and excitation energy, potential-energy curves and mass asymmetry versus elongation using Metropolis walk, combinatorial method.
doi: 10.1103/PhysRevC.95.024618
2016BL07 Eur.Phys.J. A 52, 267 (2016) D.Blaschke, J.Aichelin, E.Bratkovskaya, V.Friese, M.Gazdzicki, J.Randrup, O.Rogachevsky, O.Teryaev, V.Toneev Topical issue on Exploring Strongly Interacting Matter at High Densities - NICA White Paper
doi: 10.1140/epja/i2016-16267-x
2016RA32 Eur.Phys.J. A 52, 218 (2016) Exploring high-density baryonic matter: Maximum freeze-out density
doi: 10.1140/epja/i2016-16218-7
2016ST23 Eur.Phys.J. A 52, 239 (2016) Spinodal amplification and baryon number fluctuations in nuclear collisions at NICA
doi: 10.1140/epja/i2016-16239-2
2016WA03 Phys.Rev. C 93, 014606 (2016) T.Wang, G.Li, L.Zhu, Q.Meng, L.Wang, H.Han, W.Zhang, H.Xia, L.Hou, R.Vogt, J.Randrup Correlations of neutron multiplicity and γ-ray multiplicity with fragment mass and total kinetic energy in spontaneous fission of 252Cf RADIOACTIVITY 252Cf(SF); measured E(n), I(n), Eγ, Iγ; deduced total kinetic energy (TKE), neutron and γ-ray multiplicities, correlations of neutron and γ-ray multiplicities, ratio of average γ-ray yield to the average neutron multiplicity as function of fragment mass, γ-ray multiplicity as a function of the total fragment kinetic energy TKE.
doi: 10.1103/PhysRevC.93.014606
2015MO07 Phys.Rev. C 91, 044316 (2015) Calculated fission-fragment yield systematics in the region 74≤Z≤94 and 90≤N≤150 RADIOACTIVITY Z=74-94, N=90-150(SF); 186,190,196W, 195,201Au, 171,176,180,198,202Hg, 199,201,203Tl, 206,210Po, 195,201,207Bi, 209,213At(SF), [compound nuclei in the excitation range of 11-38 MeV]; calculated fission-fragment mass yields for 987 nuclides; reference database for theoretical fission-fragment mass yields. Benchmarked Brownian shape-motion method with random walks on the previously calculated five-dimensional potential-energy surfaces. Comparison with available data.
doi: 10.1103/PhysRevC.91.044316
2015VE02 Comput.Phys.Commun. 191, 178 (2015) J.M.Verbeke, J.Randrup, R.Vogt Fission Reaction Event Yield Algorithm, FREYA - For event-by-event simulation of fission
doi: 10.1016/j.cpc.2015.02.002
2014GH09 Phys.Rev. C 90, 041301 (2014) L.Ghys, A.N.Andreyev, M.Huyse, P.Van Duppen, S.Sels, B.Andel, S.Antalic, A.Barzakh, L.Capponi, T.E.Cocolios, X.Derkx, H.De Witte, J.Elseviers, D.V.Fedorov, V.N.Fedosseev, F.P.Hessberger, Z.Kalaninova, U.Koster, J.F.W.Lane, V.Liberati, K.M.Lynch, B.A.Marsh, S.Mitsuoka, P.Moller, Y.Nagame, K.Nishio, S.Ota, D.Pauwels, R.D.Page, L.Popescu, D.Radulov, M.M.Rajabali, J.Randrup, E.Rapisarda, S.Rothe, K.Sandhu, M.D.Seliverstov, A.M.Sjodin, V.L.Truesdale, C.Van Beveren, P.Van den Bergh, Y.Wakabayashi, M.Warda Evolution of fission-fragment mass distributions in the neutron-deficient lead region RADIOACTIVITY 194,196At, 200,202Fr(β+F)[from U(p, X), E=1.4 GeV at CERN-ISOLDE using HRS and GPS separators]; measured mass and energy distributions of coincident fission fragments after β-delayed fission, ratio of α to β-delayed-fission decays, total kinetic energy. 196At, 200Fr; deduced β-delayed fission decay probabilities, new region of multimodal fission in the neutron-deficient lead region. 196Po; Calculated potential energy surface contour. Comparison with Finite-range liquid-drop (FRLDM) and Hartree-Fock-Bogoliubov (HFB) model calculations. Comparison with experimental results for β-delayed fission of 180Tl.
doi: 10.1103/PhysRevC.90.041301
2014MO17 Phys.Rev. C 90, 014601 (2014) P.Moller, J.Randrup, A.Iwamoto, T.Ichikawa Fission-fragment charge yields: Variation of odd-even staggering with element number, energy, and charge asymmetry NUCLEAR REACTIONS 234U, 240Pu(n, F), E=thermal; 222,226,228Th, 234U(γ, F), E=11 MeV; analyzed magnitude of the odd-even staggering for fission-fragment charge-yield distributions; deduced total energies, potential energies, and excitation energies from saddle to scission at different locations in the five-dimensional deformation space; correlation of odd-even staggering with excitation energy.
doi: 10.1103/PhysRevC.90.014601
2014MU01 Phys.Rev. C 89, 034615 (2014) J.M.Mueller, M.W.Ahmed, R.H.France, M.S.Johnson, H.J.Karwowski, L.S.Myers, J.Randrup, M.H.Sikora, M.C.Spraker, S.Stave, J.R.Tompkins, R.Vogt, H.R.Weller, C.S.Whisnant, W.R.Zimmerman Prompt neutron polarization asymmetries in photofission of 232Th, 233, 235, 238U, 237Np, and 239, 240Pu NUCLEAR REACTIONS 232Th, 233,235,238U, 237Np, 239,240Pu(polarized γ, F), E=5.3-7.6 MeV; measured E(n), I(n), time-of flight spectrum, angular distribution, and polarization asymmetry of prompt neutrons generated by fission, θ(fragment) at HIγS-TUNL facility; deduced angular distribution coefficients b and c, and compared with predicted values from FREYA computer code of event-by-event Monte Carlo prompt neutron+γ-ray emission calculation. Discussed differences in polarization asymmetries between the even-even actinides and odd-A actinides.
doi: 10.1103/PhysRevC.89.034615
2014RA09 Phys.Rev. C 89, 044601 (2014) Refined treatment of angular momentum in the event-by-event fission model freya RADIOACTIVITY 252Cf(SF); calculated angular correlation of evaporated neutrons, angular distribution of neutrons relative to the direction of the angular momentum of the emitted nucleus, photon multiplicity distribution using refined event-by-event fission model FREYA code. Treatment of angular momenta in FREYA. Comparison with experimental data. NUCLEAR REACTIONS 239Pu(n, F), E=thermal; calculated distribution of the angle between the post-evaporation fragment angular momentum and that of the of the initial compound nucleus using improved FREYA code.
doi: 10.1103/PhysRevC.89.044601
2014ST07 Phys.Rev. C 89, 034901 (2014) J.Steinheimer, J.Randrup, V.Koch Non-equilibrium phase transition in relativistic nuclear collisions: Importance of the equation of state
doi: 10.1103/PhysRevC.89.034901
2014TA16 Nucl.Data Sheets 118, 227 (2014) P.Talou, T.Kawano, I.Stetcu, R.Vogt, J.Randrup Monte Carlo Predictions of Prompt Fission Neutrons and Photons: a Code Comparison RADIOACTIVITY 252Cf(SF); calculated neutron, γ average kinetic energy, neutron multiplicity, γ multiplicity from different fission fragments. Compared with
doi: 10.1016/j.nds.2014.04.043
2014VO04 Nucl.Data Sheets 118, 220 (2014) Event-by-event Modeling of Prompt Neutrons and Photons from Neutron-induced and Spontaneous Fission with FREYA NUCLEAR REACTIONS 235U, 239Pu(n, F), E not given (probably low); calculated neutron, γ average kinetic energy, neutron multiplicity, γ multiplicity from fission fragments. Compared with other calculations and data. RADIOACTIVITY 252Cf(SF); calculated neutron, γ average kinetic energy, neutron multiplicity, γ multiplicity from fission fragments. Compared with other calculations and data.
doi: 10.1016/j.nds.2014.04.041
2014VO14 Phys.Rev. C 90, 064623 (2014) Neutron angular correlations in spontaneous and neutron-induced fission NUCLEAR REACTIONS 235U(n, F), E>0.425 keV; calculated nn(θ, E(n)) between two neutrons emitted in fission using event-by-event models of fission, FREYA. Comparison with experimental data, including that for thermal-neutron induced fission. RADIOACTIVITY 252Cf(SF); calculated nn(θ) between two neutrons emitted as a function of the opening angle, neutron multiplicity distribution using event-by-event models of fission, FREYA. Comparison with experimental data.
doi: 10.1103/PhysRevC.90.064623
2013RA34 Phys.Rev. C 88, 064606 (2013) Energy dependence of fission-fragment mass distributions from strongly damped shape evolution NUCLEAR REACTIONS Pb(205At, X), E*=19.41 MeV; Pb(206At, X), E*=20.63 MeV; Pb(204Rn, X), E*=16.10 MeV; Pb(205Rn, X), E*=17.20 MeV; Pb(206Rn, X), E*=18.20 MeV; Pb(207Rn, X), E*=19.14 MeV; Pb(208Rn, X), E*=19.93 MeV; Pb(209Rn, X), E*=20.75 MeV; Pb(206Fr, X), E*=15.98 MeV; Pb(207Fr, X), E*=16.84 MeV; Pb(208Fr, X), E*=17.71 MeV; Pb(209Fr, X), E*=18.60 MeV; Pb(210Fr, X), E*=19.40 MeV; Pb(211Fr, X), E*=20.02 MeV; Pb(212Fr, X), E*=20.72 MeV; Pb(217Fr, X), E*=16.74 MeV; Pb(218Fr, X), E*=16.40 MeV; Pb(209Ra, X), E*=16.54 MeV; Pb(210Ra, X), E*=17.26 MeV; Pb(211Ra, X), E*=18.00 MeV; Pb(212Ra, X), E*=18.40 MeV; Pb(213Ra, X), E*=19.11 MeV; Pb(214Ra, X), E*=18.94 MeV; Pb(215Ra, X), E*=17.93 MeV; Pb(216Ra, X), E*=17.01 MeV; Pb(217Ra, X), E*=15.80 MeV; Pb(218Ra, X), E*=15.25 MeV; Pb(219Ra, X), E*=14.81 MeV; Pb(212Ac, X), E*=16.66 MeV; Pb(213Ac, X), E*=17.00 MeV; Pb(214Ac, X), E*=17.52 MeV; Pb(215Ac, X), E*=17.36 MeV; Pb(216Ac, X), E*=16.19 MeV; Pb(217Ac, X), E*=15.08 MeV; Pb(218Ac, X), E*=14.40 MeV; Pb(219Ac, X), E*=14.03 MeV; Pb(220Ac, X), E*=13.71 MeV; Pb(221Ac, X), E*=13.34 MeV; Pb(222Ac, X), E*=13.13 MeV; Pb(223Ac, X), E*=12.69 MeV; Pb(224Ac, X), E*=12.50 MeV; Pb(225Ac, X), E*=12.05 MeV; Pb(226Ac, X), E*=11.71 MeV; Pb(217Th, X), E*=15.02 MeV; Pb(218Th, X), E*=13.99 MeV; Pb(219Th, X), E*=13.17 MeV; Pb(220Th, X), E*=12.45 MeV; Pb(221Th, X), E*=12.27 MeV; Pb(222Th, X), E*=11.99 MeV; Pb(223Th, X), E*=12.20 MeV; Pb(224Th, X), E*=11.85 MeV; Pb(225Th, X), E*=11.59 MeV; Pb(226Th, X), E*=11.20 MeV; Pb(227Th, X), (228Th, X), (229Th, X), (224Pa, X), (225Pa, X), (226Pa, X), (227Pa, X), (228Pa, X), (229Pa, X), (230Pa, X), (231Pa, X), (232Pa, X), (230U, X), (231U, X), (232U, X), (233U, X), (234U, X), E*=11.0 MeV, [secondary At, Rn, Fr, Ra, Ac, Th, Pa, U beams from 9Be(238U, X), E=1 GeV/nucleon primary fragmentation reaction, fission by γ rays produced in incident secondary beams on a Pb target via the GDR]; calculated relative fission fragment charge yield distributions as function of nuclear excitation energy by Metropolis method. Comparison and benchmarking with experimental data from GSI. Shell-plus-pairing correction term. Damped Brownian shape evolution.
doi: 10.1103/PhysRevC.88.064606
2013ST07 Phys.Rev. C 87, 054903 (2013) Spinodal density enhancements in simulations of relativistic nuclear collisions
doi: 10.1103/PhysRevC.87.054903
2013VO04 Phys.Rev. C 87, 044602 (2013) Event-by-event study of photon observables in spontaneous and thermal fission RADIOACTIVITY 252Cf(SF); analyzed prompt photon multiplicity distribution as function of fragment mass and TKE, average neutron multiplicity as a function of fragment TKE, neutron-photon correlations, nn(θ). Event-by-event FREYA fission model by assuming no competition between prompt photon and neutron emissions. NUCLEAR REACTIONS 235U(n, F), E=thermal; analyzed prompt photon multiplicity distribution, neutron-photon correlations. Event-by-event FREYA fission model by assuming no competition between prompt photon and neutron emissions.
doi: 10.1103/PhysRevC.87.044602
2012MO04 Phys.Rev. C 85, 024306 (2012) P.Moller, J.Randrup, A.J.Sierk Calculated fission yields of neutron-deficient mercury isotopes RADIOACTIVITY 180Tl(EC); calculated Gamow-Teller β-strength function, T1/2. Comparison with experimental data. 174,176,178,180,182,184,186,188Hg(SF); calculated fragment mass yields. Method of Brownian shape motion. NUCLEAR STRUCTURE 174,180,188Hg; calculated potential-energy surfaces, energy minima, saddles, major valleys, major ridges. Brownian shape motion (Metropolis) treatment.
doi: 10.1103/PhysRevC.85.024306
2012PI13 Phys.Rev. C 86, 025203 (2012) Surface tension of quark matter in a geometrical approach
doi: 10.1103/PhysRevC.86.025203
2012RA26 Phys.Scr. T150, 014033 (2012) Brownian shape motion: fission fragment mass distributions NUCLEAR REACTIONS 240Pu, 234,236U, 222,224,226,228Th(n, F), E=6-11 MeV; calculated fission fragment yields. Comparison with experimental data.
doi: 10.1088/0031-8949/2012/T150/014033
2012ST16 Phys.Rev.Lett. 109, 212301 (2012) Spinodal Amplification of Density Fluctuations in Fluid-Dynamical Simulations of Relativistic Nuclear Collisions
doi: 10.1103/PhysRevLett.109.212301
2012VO01 Phys.Rev. C 85, 024608 (2012) R.Vogt, J.Randrup, D.A.Brown, M.A.Descalle, W.E.Ormand Event-by-event evaluation of the prompt fission neutron spectrum from 239Pu(n, f) NUCLEAR REACTIONS 239Pu(n, F), E<20 MeV; analyzed chance fission probability, probability for pre-equilibrium neutron emission, fragment mass yields, total and average fragment kinetic energies, neutron multiplicity, prompt neutron spectra, neutron-neutron correlation coefficient contour plots. Event-by-event fission model FREYA with multichance fission and pre-equilibrium neutron emission. Comparison with ENDF-B/VII.0 evaluation.
doi: 10.1103/PhysRevC.85.024608
2011RA02 Phys.Rev.Lett. 106, 132503 (2011) Brownian Shape Motion on Five-Dimensional Potential-Energy Surfaces:Nuclear Fission-Fragment Mass Distributions NUCLEAR REACTIONS 233,235U, 239Pu(n, F), E=thermal; 234U(γ, F), E=11 MeV; 222,224,226,228Th(γ, F), E=11 MeV; calculated distribution of charge fission yields. Comparison with experimental data.
doi: 10.1103/PhysRevLett.106.132503
2011RA06 Int.J.Mod.Phys. E20, 299 (2011) Spinodal phase separation in nuclear collisions
doi: 10.1142/S021830131101765X
2011RA27 Phys.Rev. C 84, 034613 (2011) J.Randrup, P.Moller, A.J.Sierk Fission-fragment mass distributions from strongly damped shape evolution NUCLEAR REACTIONS 239Pu(n, F)240Pu, E=8-14 MeV; 234,236U(n, F)235U/236U, E=8-14 MeV; 234U(γ, F)234U, E=8-14 MeV; 222,224,226,228Th(γ, F)222Th/224Th/226Th/228Th, E=8-14 MeV; calculated fission fragment mass and charge yields, comparison with experimental data. Random walks on a five-dimensional potential energy surface within the framework of the Smoluchowski equation of motion. NUCLEAR STRUCTURE 222,224,226,228Th, 240Pu; calculated fission fragment mass and charge distributions. 222Th; calculated contours of three shapes relevant to fission, and the most probable symmetric fragment division in 111Rh isotope.
doi: 10.1103/PhysRevC.84.034613
2011VO11 Phys.Rev. C 84, 044621 (2011) Event-by-event study of neutron observables in spontaneous and thermal fission RADIOACTIVITY 238U, 240Pu, 244Cm, 252Cf(SF); calculated yields, total fragment kinetic energies, neutron multiplicities, prompt fission neutron spectra, angular correlations between two neutrons. Event-by-event fission model FREYA for fission neutron correlations. Comparison with experimental data. NUCLEAR REACTIONS 235U(n, F), 239Pu(n, F), E=thermal; calculated yields, total fragment kinetic energies, prompt fission neutron spectra, angular correlations between two neutrons. Event-by-event fission model FREYA for fission neutron correlations. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.044621
2011VO12 J.Korean Phys.Soc. 59, 895s (2011) R.Vogt, J.Randrup, J.Pruet, W.Younes Calculation of 239Pu Fission Observables in an Event-by-Event Simulation NUCLEAR REACTIONS 239Pu(n, f), E=0.5-5.5 MeV; calculated prompt σ(En), fragment TKE, average neutron multiplicity, correlation coefficients using FREYA event generator. Comparison to data.
doi: 10.3938/jkps.59.895
2010RA18 Phys.Rev. C 82, 034902 (2010) Spinodal phase separation in relativistic nuclear collisions
doi: 10.1103/PhysRevC.82.034902
2009RA09 Phys.Rev. C 79, 054911 (2009) Phase transition dynamics for baryon-dense matter
doi: 10.1103/PhysRevC.79.054911
2009RA18 Phys.Rev. C 80, 024601 (2009) Calculation of fission observables through event-by-event simulation NUCLEAR REACTIONS 235U, 239Pu(n, X), E=0.53 MeV; calculated kinetic energy and dispersions of neutrons, total energies of fission fragments, multiplicity of neutrons emitted by fission fragments, neutron-neutron angular correlations and neutron-photon correlations using a new computational model, the fission reaction event yield algorithm (FREYA).
doi: 10.1103/PhysRevC.80.024601
2009VO08 Phys.Rev. C 80, 044611 (2009) R.Vogt, J.Randrup, J.Pruet, W.Younes Event-by-event study of prompt neutrons from 239Pu(n, f) NUCLEAR REACTIONS 239Pu(n, f), E=0.5-5.5 MeV; analyzed prompt neutron spectra from 0.1 to 10 MeV, fragment kinetic energies and excitation energies for fragment A=80-160, and average neutron multiplicities as a function of fragment mass number using Monte Carlo model FREYA. Comparisons with experimental data and ENDF-B/VII evaluations.
doi: 10.1103/PhysRevC.80.044611
2007AR11 Phys.Rev. C 75, 034902 (2007) I.C.Arsene, L.V.Bravina, W.Cassing, Yu.B.Ivanov, A.Larionov, J.Randrup, V.N.Russkikh, V.D.Toneev, G.Zeeb, D.Zschiesche Dynamical phase trajectories for relativistic nuclear collisions NUCLEAR REACTIONS Au(Au, X), E=5-40 GeV/nucleon; calculated time evolution of net baryon density and energy, related phase trajectories.
doi: 10.1103/PhysRevC.75.034902
2007RA33 J.Phys.(London) G34, S261 (2007) Exploring hot and baryon-dense matter with nucleus-nucleus collisions
doi: 10.1088/0954-3899/34/8/S11
2006KO59 Nucl.Phys. A774, 643 (2006) Strangeness trapping
doi: 10.1016/j.nuclphysa.2006.06.105
2006KO61 Nucl.Phys. A774, 841 (2006) Baryon-strangeness correlations: a diagnostic of strongly interacting matter
doi: 10.1016/j.nuclphysa.2006.06.147
2006ON04 Eur.Phys.J. A 30, 109 (2006) Dynamical models for fragment formation
doi: 10.1140/epja/i2006-10110-1
2006RA23 Phys.Rev. C 74, 047901 (2006) Maximum freeze-out baryon density in nuclear collisions
doi: 10.1103/PhysRevC.74.047901
2005KO36 Phys.Rev.Lett. 95, 182301 (2005) Baryon-Strangeness Correlations: A Diagnostic of Strongly Interacting Matter NUCLEAR REACTIONS 197Au(197Au, X), E(cm)=200 GeV/nucleon; calculated baryon-strangeness correlation coefficient vs rapidity.
doi: 10.1103/PhysRevLett.95.182301
2005KO46 Phys.Rev. C 72, 064903 (2005) Signals of spinodal hadronization: Strangeness trapping
doi: 10.1103/PhysRevC.72.064903
2005RA10 Nucl.Phys. A752, 384c (2005) Phase Transitions from Intermediate to Relativistic Energies
doi: 10.1016/j.nuclphysa.2005.02.093
2004CH02 Phys.Rep. 389, 263 (2004) P.Chomaz, M.Colonna, J.Randrup Nuclear spinodal fragmentation
doi: 10.1016/j.physrep.2003.09.006
2004RA07 Phys.Rev.Lett. 92, 122301 (2004) Spinodal Decomposition during the Hadronization Stage at RHIC?
doi: 10.1103/PhysRevLett.92.122301
2004RA11 Phys.Rev. C 69, 047901 (2004) Thermodynamic consistency of the equation of state of strongly interacting matter
doi: 10.1103/PhysRevC.69.047901
2004SO31 J.Phys.(London) G30, L35 (2004) S.Soff, S.Kesavan, J.Randrup, H.Stocker, N.Xu φ-meson production at RHIC, strong colour fields and intrinsic transverse momenta NUCLEAR REACTIONS 197Au(197Au, X), E(cm)=200 GeV/nucleon; calculated φ-mesons transverse momentum spectra, particle yield ratios, effects of strong colour fields.
doi: 10.1088/0954-3899/30/12/L01
2003RA37 Phys.Rev. C 68, 031903 (2003) Production of the exotic Θ baryon in relativistic nuclear collisions NUCLEAR REACTIONS 197Au(197Au, X), E=high; calculated exotic baryon production σ.
doi: 10.1103/PhysRevC.68.031903
2003RA38 Phys.Rev. C 68, 034909 (2003) Chromodynamic Weibel instabilities in relativistic nuclear collisions
doi: 10.1103/PhysRevC.68.034909
2002RA19 Phys.Rev. C65, 054906 (2002) Charged-Pion Correlations Caused by Chiral Relaxation Dynamics in High-Energy Nuclear Collisions
doi: 10.1103/PhysRevC.65.054906
2002RA52 Acta Phys.Hung.N.S. 16, 169 (2002) Correlated Charged Pions from Chiral Dynamics in High-Energy Nuclear Collisions
doi: 10.1556/APH.16.2002.1-4.19
2001RA02 Nucl.Phys. A681, 100c (2001) Chiral Phase Transition in High-Energy Collisions
doi: 10.1016/S0375-9474(00)00489-9
2001RA19 Phys.Rev. C63, 061901 (2001) Probing Chiral Dynamics by Charged-Pion Correlations
doi: 10.1103/PhysRevC.63.061901
2000BL19 Phys.Rev. C62, 041901 (2000) M.Bleicher, J.Randrup, R.Snellings, X.-N.Wang Enhanced Event-by-Event Fluctuations in Pion Multiplicity as a Signal of Disoriented Chiral Condensates in Relativistic Heavy-Ion Collisions NUCLEAR REACTIONS 197Au(197Au, X), E=high; calculated pion rapidity, multiplicity distributions, factorial moments; deduced signal for disoriented chiral condensate.
doi: 10.1103/PhysRevC.62.041901
2000PE04 Phys.Rev. C61, 024906 (2000) Dynamical Simulation of Disoriented Chiral Condensate Formation in Bjorken Rods
doi: 10.1103/PhysRevC.61.024906
2000RA30 Phys.Rev. C62, 064905 (2000) Quantum Field Treatment of Disoriented-Chiral-Condensate Dynamics
doi: 10.1103/PhysRevC.62.064905
1999HE19 Ann.Phys.(New York) 274, 1 (1999) Spin-Isospin Modes in Heavy-Ion Collisions II. Transport Simulations NUCLEAR REACTIONS 1H(p, nX), E(cm)=2-3 GeV; calculated Δ production σ. 197Au(197Au, X), E=1 GeV/nucleon; 40Ar(p, X), E=500 MeV; calculated Δ production rates, invariant mass spectra, pions production rate, transverse momentum, related in-medium quantities. Transport simulations.
doi: 10.1006/aphy.1999.5906
1999HI06 Prog.Theor.Phys.(Kyoto) 102, 89 (1999) Y.Hirata, Y.Nara, A.Ohnishi, T.Harada, J.Randrup Quantum Fluctuation Effects on Hyperfragment Formation from Ξ- Absorption at Rest on 12C NUCLEAR REACTIONS 12C(Ξ-, X), E at rest; calculated hypernucleus fragments mass distributions; deduced quantum fluctuation effects. Microscopic transport model.
doi: 10.1143/PTP.102.89
1999RA23 Acta Phys.Hung.N.S. 9, 289 (1999) Enhanced Pion Production in DCC Dynamics
1999SC16 Phys.Rev. C59, 3329 (1999) J.Schaffner-Bielich, J.Randrup Disoriented Chiral Condensate Dynamics with the SU(3) Linear Sigma Model
doi: 10.1103/PhysRevC.59.3329
1998HE30 Phys.Lett. 439B, 243 (1998) Transport Simulations with π and Δ In-Medium Properties NUCLEAR REACTIONS 197Au(197Au, X), E=1 GeV/nucleon; calculated Δ resonance decay widths, invariant mass, pions transverse momentum spectra; deduced in-medium effects. Transport calculations.
doi: 10.1016/S0370-2693(98)01109-5
1998HI16 Nucl.Phys. A639, 389c (1998) Y.Hirata, Y.Nara, A.Ohnishi, T.Harada, J.Randrup Formation of Twin and Double Λ Hypernuclei from Ξ- Absorption at Rest on 12C NUCLEAR REACTIONS 12C(Ξ-, X), E at rest; calculated hypernucleus production rates.
doi: 10.1016/S0375-9474(98)00302-9
1998KL01 Phys.Rev. C57, 280 (1998) Y.Kluger, V.Koch, J.Randrup, X.-N.Wang Dileptons from Disoriented Chiral Condensates
doi: 10.1103/PhysRevC.57.280
1998KO40 Nucl.Phys. A638, 447c (1998) V.Koch, J.Randrup, X.N.Wang, Y.Kluger Dileptons from Disoriented Chiral Condensates NUCLEAR REACTIONS Pb(Pb, X), E=158 GeV/nucleon; calculated dilepton invariant mass spectra.
doi: 10.1016/S0375-9474(98)00362-5
1998OH02 Nucl.Phys. A630, 223c (1998) A.Ohnishi, J.Randrup, Y.Hirata, N.Otuka, Y.Nara, T.Harada Quantum Fluctuation Effects on Nuclear and Atomic Cluster Formation
doi: 10.1016/S0375-9474(97)00760-4
1998RA06 Nucl.Phys. A630, 468c (1998) DCC Formation and Observation in Nucleus-Nucleus Collisions
doi: 10.1016/S0375-9474(97)00786-0
1998RA20 Nucl.Phys. A638, 439c (1998) Transport Treatment of DCC Dynamics
doi: 10.1016/S0375-9474(98)00354-6
1998RA24 Phys.Lett. 435B, 251 (1998) Transport Simulation of the Linear Sigma Model
doi: 10.1016/S0370-2693(98)00858-2
1997GU11 Phys.Lett. 403B, 191 (1997) A.Guarnera, Ph.Chomaz, M.Colonna, J.Randrup Multifragmentation with Brownian One-Body Dynamics NUCLEAR STRUCTURE 197Au; calculated fragment multiplicity vs time, charge distribution after compression to double density. Brownian one-body dynamics.
doi: 10.1016/S0370-2693(97)00515-7
1997HE12 Phys.Rev. C56, 1187 (1997) Comment on ' Influence of the In-Medium Pion Dispersion Relation in Heavy Ion Collisions '
doi: 10.1103/PhysRevC.56.1187
1997HE19 Phys.Lett. 411B, 1 (1997) Effects of Spin-Isospin Modes in Transport Simulations NUCLEAR REACTIONS 197Au(197Au, X), E=1 GeV/nucleon; calculated pion, Δ multiplicity, decay rates vs time, neutral pion transverse momentum spectra; deduced in-medium properties effects. Transport model.
doi: 10.1016/S0370-2693(97)00965-9
1997OH01 Phys.Lett. 394B, 260 (1997) Quantum Fluctuation Effects on Nuclear Fragment Formation NUCLEAR REACTIONS 197Au(197Au, X), E=100-400 MeV/nucleon; analyzed intermediate mass fragment multiplicity before, after statistical decay. Quantal Langevin model.
doi: 10.1016/S0370-2693(97)00032-4
1997RA11 Nucl.Phys. A616, 531 (1997) Mean-Field Treatment of the Linear σ Model in Dynamical Calculations of DCC Observables
doi: 10.1016/S0375-9474(97)00003-1
1996AY01 Z.Phys. A355, 407 (1996) S.Ayik, Ph.Chomaz, M.Colonna, J.Randrup Analysis of Boltzmann-Langevin Dynamics in Nuclear Matter
doi: 10.1007/s002180050130
1996HE04 Nucl.Phys. A597, 672 (1996) Treatment of Pionic Modes at the Nuclear Surface for Transport Descriptions
doi: 10.1016/0375-9474(95)00433-5
1996RA28 Acta Phys.Pol. B27, 253 (1996) Dynamics of Catastrophic Processes in Nuclear Physics
1996RA39 Phys.Rev.Lett. 77, 1226 (1996) Amplification of Pionic Instabilities in High-Energy Collisions ( Question )
doi: 10.1103/PhysRevLett.77.1226
1995BU04 Nucl.Phys. A581, 356 (1995) G.F.Burgio, Ph.Chomaz, M.Colonna, J.Randrup Simulation of Transport Equations for Unstable Systems: Comparison between lattice and test-particle methods
doi: 10.1016/0375-9474(94)00525-R
1995HE15 Phys.Rev. C52, 427 (1995) Dilepton Production from Pion Annihilation in a Realistic Δ-Hole Model
doi: 10.1103/PhysRevC.52.427
1995HE37 Ann.Phys.(New York) 244, 12 (1995) Spin-Isospin Modes in Heavy-Ion Collisions I: Nuclear Matter at Finite Temperatures NUCLEAR REACTIONS 1H(π, X), E=high; calculated σ for Δ++ production σ vs invariant mass. 1H(p, X), E=high; calculated σ(θ) for Δ++. Microscopic transport simulations.
doi: 10.1006/aphy.1995.1106
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