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NSR database version of April 25, 2024.

Search: Author = J.P.Bondorf

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2006CA07      Nucl.Phys. A764, 15 (2006)

L.Carlen, P.Golubev, B.Jakobsson, V.Avdeichikov, C.Ekstrom, C.-J.Friden, A.Kolozhvari, L.Westerberg, A.Siwek, K.Aleklett, H.Persson, C.Rouki, A.S.Botvina, J.P.Bondorf, I.A.Pshenichnov, I.N.Mishustin

Dynamical and statistical fragment emission properties in 200 A MeV 20Ne + 40Ar collisions

NUCLEAR REACTIONS 40Ar(20Ne, X), E=200 MeV/nucleon; measured fragments charge and angular distributions, isotopic yields and ratios; deduced reaction mechanism features. Cascade plus statistical multifragmentation model.

doi: 10.1016/j.nuclphysa.2005.09.009
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2004SC28      Phys.Rev. C 70, 014902 (2004)

C.Scheidenberger, I.A.Pshenichnov, K.Summerer, A.Ventura, J.P.Bondorf, A.S.Botvina, I.N.Mishustin, D.Boutin, S.Datz, H.Geissel, P.Grafstrom, H.Knudsen, H.F.Krause, B.Lommel, S.P.Moller, G.Munzenberg, R.H.Schuch, E.Uggerhoj, U.Uggerhoj, C.R.Vane, Z.Z.Vilakazi, H.Weick

Charge-changing interactions of ultrarelativistic Pb nuclei

NUCLEAR REACTIONS H, C, Al, Cu, Sn, Au(208Pb, X), E=158 GeV/nucleon; measured charge-changing σ; deduced reaction mechanism features. Abrasion-ablation model and relativistic electromagnetic dissociation model analysis.

doi: 10.1103/PhysRevC.70.014902
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0810.


2002BO02      Phys.Rev. C65, 017601 (2002)

J.P.Bondorf, H.Feldmeier, I.N.Mishustin, G.Neergaard

Equilibration and Freeze-Out in an Exploding System

doi: 10.1103/PhysRevC.65.017601
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2002SC01      Phys.Rev.Lett. 88, 042301 (2002)

C.Scheidenberger, I.A.Pshenichnov, T.Aumann, S.Datz, K.Summerer, J.P.Bondorf, D.Boutin, H.Geissel, P.Grafstrom, H.Knudsen, H.F.Krause, B.Lommel, S.P.Moller, G.Munzenberg, R.H.Schuch, E.Uggerhoj, U.Uggerhoj, C.R.Vane, A.Ventura, Z.Z.Vilakazi, H.Weick

Electromagnetically Induced Nuclear-Charge Pickup Observed in Ultrarelativistic Pb Collisions

NUCLEAR REACTIONS H, C, 27Al, Cu, Sn, 197Au, Pb(208Pb, X), E=158 GeV/nucleon; measured charge-pickup σ; deduced role of electromagnetic processes. Comparison with previous results.

doi: 10.1103/PhysRevLett.88.042301
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2001PS01      Phys.Rev. C64, 024903 (2001)

I.A.Pshenichnov, J.P.Bondorf, I.N.Mishustin, A.Ventura, S.Masetti

Mutual Heavy Ion Dissociation in Peripheral Collisions at Ultrarelativistic Energies

NUCLEAR REACTIONS 197Au(197Au, nX), Pb(Pb, nX), E=high; calculated mutual dissociation σ, Coulomb and nuclear contributions. Comparisons with data.

doi: 10.1103/PhysRevC.64.024903
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2000CH40      Eur.Phys.J. A 8, 537 (2000)

K.A.Chikin, V.L.Korotkikh, A.P.Kryukov, L.I.Sarycheva, I.A.Pshenichnov, J.P.Bondorf, I.N.Mishustin

Inclusive Meson Production in Peripheral Collisions of Ultrarelativistic Heavy Ions

NUCLEAR REACTIONS U(U, X), Pb(Pb, X), E=high; calculated single meson production σ following of γγ fusion. Contributions to experimental results from other processes studied. Weizsacker-Williams photons.

doi: 10.1007/s100500070076
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2000PO02      Phys.Lett. 473B, 193 (2000)

A.Polleri, R.Mattiello, I.N.Mishustin, J.P.Bondorf

The Transverse Structure of the Baryon Source in Relativistic Heavy Ion Collisions

NUCLEAR REACTIONS Pb(Pb, X), E=high; analyzed proton, deuteron transverse momentum spectra; deduced source transverse flow, related features. Coalescence model.

doi: 10.1016/S0370-2693(99)01230-7
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1999BO54      Phys.Lett. 470B, 13 (1999)

J.Borg, I.N.Mishustin, J.P.Bondorf

Nuclear Liquid-Gas Phase Transition within the Lattice Gas Model

doi: 10.1016/S0370-2693(99)01231-9
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1999BR41      Phys.Rev. C60, 044905 (1999)

L.V.Bravina, I.N.Mishustin, J.P.Bondorf, A.Faessler, E.E.Zabrodin

Microscopic Study of Freeze-Out in Relativistic Heavy-Ion Collisions at 160A GeV/c Energy

NUCLEAR REACTIONS S(S, X), Pb(Pb, X), E at 160 GeV/c/nucleon; calculated particle spectra, emission time, space distributions; deduced freeze-out features. Microscopic quark-gluon string model.

doi: 10.1103/PhysRevC.60.044905
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1999DA11      Nucl.Phys. A650, 329 (1999)

M.D'Agostino, A.S.Botvina, M.Bruno, A.Bonasera, J.P.Bondorf, R.Bougault, P.Desesquelles, E.Geraci, F.Gulminelli, I.Iori, N.Le Neindre, G.V.Margagliotti, I.N.Mishustin, A.Moroni, A.Pagano, G.Vannini

Thermodynamical Features of Multifragmentation in Peripheral Au + Au Collisions at 35 A MeV

NUCLEAR REACTIONS 197Au(197Au, X), E=35 MeV/nucleon; measured light, intermediate fragments energy, charge, multiplicity distributions, two-particle correlations; deduced quasi-projectile equilibration. Event-by-event thermometer proposed.

doi: 10.1016/S0375-9474(99)00097-4
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1999FO08      Phys.Rev. C60, 024601 (1999)

A.Fokin, L.Carlen, R.Ghetti, B.Jakobsson, J.Martensson, Yu.Murin, A.Oskarsson, C.Ekstrom, G.Ericsson, J.Romanski, E.J.van Veldhuizen, L.Westerberg, K.Nybo, T.F.Thorsteinsen, S.Amirelmi, M.Guttormsen, G.Lovhoiden, V.Bellini, F.Palazzolo, M.L.Sperduto, J.P.Bondorf, I.Mishustin, V.Avdeychikov, O.V.Lozhkin, W.A.Friedman, K.K.Gudima, and the CHIC Collaboration

d/p and t/p Ratios in Nucleon-Nucleus and Heavy Ion Reactions: Can entropy be determined ?

NUCLEAR REACTIONS Kr(p, X), E=150-500 MeV; Kr(16O, X), E=22-300 MeV/nucleon; Ar(20Ne, X), E=50-400 MeV/nucleon; measured light charged particles relative yields; deduced emission source density, thermodynamic features. Statistical model calculations.

doi: 10.1103/PhysRevC.60.024601
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1999PO29      Nucl.Phys. A661, 452c (1999)

A.Polleri, R.Mattiello, I.N.Mishustin, J.P.Bondorf

Reconstruction of the Proton Source in Relativistic Heavy Ion Collisions

doi: 10.1016/S0375-9474(99)85063-5
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1999PS01      Phys.Rev. C60, 044901 (1999)

I.A.Pshenichnov, I.N.Mishustin, J.P.Bondorf, A.S.Botvina, A.S.Iljinov

Particle Emission following Coulomb Excitation in Ultrarelativistic Heavy-Ion Collisions

NUCLEAR REACTIONS 197Au(197Au, X), 208Pb(208Pb, X), E=high; calculated fragment, nucleon, pion emission σ, rapidity and transverse momentum distributions following electromagnetic dissociation.

doi: 10.1103/PhysRevC.60.044901
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1998BA29      Phys.Rev. C57, 2536 (1998)

H.W.Barz, J.P.Bondorf, J.J.Gaardhoje, H.Heiselberg

Coulomb Effects on Particle Spectra in Relativistic Nuclear Collisions

NUCLEAR REACTIONS 197Au(197Au, X), Pb(Pb, X), S(S, X), E=high; calculated π-+ ratios; deduced Coulomb effects. Comparison with data.

doi: 10.1103/PhysRevC.57.2536
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1998BO16      Phys.Rev. C58, R27 (1998)

J.P.Bondorf, A.S.Botvina, I.N.Mishustin

Isotopic and Microcanonical Temperatures in Nuclear Multifragmentation

NUCLEAR REACTIONS 197Au(197Au, X), E=35 MeV/nucleon; analyzed data; deduced isotopic, thermodynamic temperatures. Statistical multifragmentation model.

doi: 10.1103/PhysRevC.58.R27
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1998PO05      Phys.Lett. 419B, 19 (1998)

A.Polleri, J.P.Bondorf, I.N.Mishustin

Effects of Collective Expansion on Light Cluster Spectra in Relativistic Heavy Ion Collisions

doi: 10.1016/S0370-2693(97)01455-X
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1998PS01      Phys.Rev. C57, 1920 (1998)

I.A.Pshenichnov, I.N.Mishustin, J.P.Bondorf, A.S.Botvina, A.S.Iljinov

Nuclear Multifragmentation Induced by Electromagnetic Fields of Ultrarelativistic Heavy Ions

NUCLEAR REACTIONS Ag(28Si, X), (16O, X), (32S, X), 208Pb(208Pb, X), E=high; calculated fragment charge distributions, electromagnetic dissociation process σ; deduced contribution to total σ. Other reactions discussed. Comparisons with data.

doi: 10.1103/PhysRevC.57.1920
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1997BA55      Phys.Rev. C56, 1553 (1997)

H.W.Barz, J.P.Bondorf, J.J.Gaardhoje, H.Heiselberg

Freeze-Out Time in Ultrarelativistic Heavy Ion Collisions from Coulomb Effects in Transverse Pion Spectra

NUCLEAR REACTIONS Pb(Pb, X), E=158 GeV/nucleon; analyzed pion, kaon production yield ratios vs transverse mass; deduced model parameter sensitivity, Coulomb effects role, freeze-out time. S, Pb(S, X), E=200 GeV/nucleon; analyzed pion production yields ratio. Hanbury-Brown-Twiss analysis.

doi: 10.1103/PhysRevC.56.1553
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1997BO33      Nucl.Phys. A624, 706 (1997)

J.P.Bondorf, O.Friedrichsen, D.Idier, I.N.Mishustin

A Molecular Dynamics Model for Nuclear Clusterization

NUCLEAR STRUCTURE 4He, 12C, 16O, 32S, 64Ge, 131Xe, 197Au; calculated average density vs radius. 16O, 197Au; calculated average densities in momentum, coordinate space. 197Au; calculated nucleon momentum distribution. Nuclear molecular dynamics model.

NUCLEAR REACTIONS 197Au(197Au, X), E=150 MeV/nucleon; calculated collision rate vs time; 131Xe(131Xe, X), E=180 MeV/nucleon; calculated cluster spreading width vs time; 64Ge(64Ge, X), E=150 MeV/nucleon; calculated neutron, intermediate mass fragment spectra, collision rate, temperature, density vs time; 64Ge(64Ge, X), E=75, 150, 300 MeV/nucleon; calculated intermediate mass fragment excitation vs time; deduced cluster formation dynamics related features. Nuclear molecular dynamics model.

doi: 10.1016/S0375-9474(97)00382-5
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1996DE27      Nucl.Phys. A604, 183 (1996)

P.Desesquelles, J.P.Bondorf, I.N.Mishustin, A.S.Botvina

Global Protocol for Comparison of Simulated Data with Experimental Data

doi: 10.1016/0375-9474(96)00126-1
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1995BO29      Phys.Lett. 359B, 261 (1995)

J.P.Bondorf, D.Idier, I.N.Mishustin

Self-Organization in Expanding Nuclear Matter

NUCLEAR STRUCTURE 131Xe; calculated average nucleon density time evolution, two-body collision rate, breaking time vs inward flow velocity. 64Ge; calculated intermediate mass fragment vs inward flow velocity. Molecular dynamics model.

NUCLEAR REACTIONS Ge(Ge, X), E=150 MeV/nucleon; calculated nucleon trajectories for cluster, its environment. Molecular dynamics model.

doi: 10.1016/0370-2693(95)01104-X
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1995BR23      Nucl.Phys. A594, 425 (1995)

L.V.Bravina, I.N.Mishustin, J.P.Bondorf

Phase-Space Distribution of Hadrons at Freeze-Out

NUCLEAR REACTIONS S(S, X), 197Au(197Au, X), E at 11.6 GeV/c/nucleon; analyzed final state hadrons momentum, space distributions correlation; deduced particle emission related features. Microscopic quark-gluon string model.

doi: 10.1016/0375-9474(95)00365-8
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1995BR29      Phys.Lett. 354B, 196 (1995)

L.V.Bravina, I.N.Mishustin, N.S.Amelin, J.P.Bondorf, L.P.Csernai

Freeze-Out in Relativistic Heavy Ion Collisions at AGS Energies

NUCLEAR REACTIONS S(S, X), 197Au(197Au, X), E at 11.6 GeV/c/nucleon; analyzed collision dynamics, pion emission mechanism; deduced freeze out characteristics. Quark gluon string model.

doi: 10.1016/0370-2693(95)00680-J
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1995SC11      Nucl.Phys. A584, 704 (1995)

F.Schussler, H.Nifenecker, B.Jakobsson, V.Kopljar, K.Soderstrom, S.Leray, C.Ngo, S.Souza, J.P.Bondorf, K.Sneppen

Fragment Emission Pattern in Central and Semi-Central Heavy-Ion Collisions

NUCLEAR REACTIONS Ag, Br(C, X), (O, X), (Ar, X), (Kr, X), E=50-220 MeV/nucleon; measured momentum vectors for all charged fragments. Emulsions, central collisions.

doi: 10.1016/0375-9474(94)00771-E
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1994BO32      Phys.Rev.Lett. 73, 628 (1994)

J.P.Bondorf, A.S.Botvina, I.N.Mishustin, S.R.Souza

Formation and Breakup of Extra-Large Composite System in Central Au + Au Collisions

NUCLEAR REACTIONS 197Au(197Au, X), E=100 MeV/nucleon; analyzed multi-fragmentation data; deduced composite system formation, breakup mechanisms.

doi: 10.1103/PhysRevLett.73.628
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1994SO08      Phys.Rev. C50, 257 (1994)

S.R.Souza, F.Schussler, R.Donangelo, K.Sneppen, J.P.Bondorf, R.Elmer, B.Jakobsson, S.Leray, C.Ngo, H.Nifenecker

Angular Patterns from Fragments Produced in Central Heavy-Ion Collisions

NUCLEAR REACTIONS Ag, Br(16O, X), E=210 MeV/nucleon; Ag, Br(36Ar, X), E=65 MeV/nucleon; Ag, Br(84Kr, X), E=95 MeV/nucleon; analyzed fragment σ(θ), multipolarity coefficients; deduced multi-fragmenting system shape features. Molecular dynamical approach.

doi: 10.1103/PhysRevC.50.257
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1993BA11      Phys.Rev. C47, R1838 (1993)

W.Bauer, J.P.Bondorf, R.Donangelo, R.Elmer, B.Jakobsson, H.Schulz, F.Schussler, K.Sneppen

Large Radial Flow in Nucleus-Nucleus Collisions

NUCLEAR REACTIONS Ag, Br(94Kr, X), E=70-120 MeV/nucleon; measured fragment transverse kinetic energy vs fragment charge; deduced excited matter explosive breakup. Other reactions discussed.

doi: 10.1103/PhysRevC.47.R1838
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1993BO22      Phys.Rev. C48, 459 (1993)

J.P.Bondorf, C.H.Dasso, R.Donangelo, G.Pollarolo, H.Schulz, K.Sneppen

Deep Inelastic Collision followed by Disassembly in the Reaction 136Xe + 209Bi at E(lab)/A = 28.2 MeV

NUCLEAR REACTIONS 209Bi(136Xe, X), E=28.2 MeV/nucleon; calculated neutron, charged particle multiplicities. Highly dissipative process, independent colliding nuclei decay.

doi: 10.1103/PhysRevC.48.459
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1992BA26      Phys.Rev. C45, R2541 (1992)

H.W.Barz, J.P.Bondorf, R.Donangelo, I.N.Mishustin, H.Schulz, K.Sneppen

Fluctuations and Intermittency in Multifragmentation Processes

NUCLEAR STRUCTURE Z=79; calculated multiplicity distribution, factorial moments vs resolution; deduced intermittency causes. Cold, Copenhagen statistical multi-fragmentation models.

doi: 10.1103/PhysRevC.45.R2541
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1992BA32      Phys.Rev. C46, R42 (1992)

H.W.Barz, J.P.Bondorf, C.H.Dasso, R.Donangelo, G.Pollarolo, H.Schulz, K.Sneppen

Mechanism for Nuclear Disassembly of the Ar + Th and Pb + Au Systems at Intermediate Energies

NUCLEAR REACTIONS 232Th(40Ar, xn), E=27-77 MeV/nucleon; 197Au(208Pb, xn), E=29 MeV/nucleon; analyzed neutron multiplicity data; deduced collision process binary character.

doi: 10.1103/PhysRevC.46.R42
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1992BA51      Nucl.Phys. A548, 427 (1992)

H.W.Barz, J.P.Bondorf, R.Donangelo, F.S.Hansen, B.Jakobsson, L.Karlsson, H.Nifenecker, R.Elmer, H.Schulz, F.Schussler, K.Sneppen, K.Soderstrom

Analysis of Central Events in the Reaction of 16O and 36Ar with Emulsion at 210 and 65 MeV per Nucleon

NUCLEAR REACTIONS Ag, Br(16O, X), E ≈ 210 MeV/nucleon; Ag, Br(36Ar, X), E ≈ 65 MeV/nucleon; measured fragment charge, emission angle; deduced fragmentation mechanism features. Additional momentum flow tensor analysis.

doi: 10.1016/0375-9474(92)90693-E
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1992BA69      Nucl.Phys. A545, 213c (1992)

H.W.Barz, J.P.Bondorf, A.S.Botwina, R.Donangelo, I.N.Mishustin, H.Schulz, K.Sneppen

Gating in Fragmentation Processes ( Question )

NUCLEAR REACTIONS 232Th(40Ar, X), E=44, 77 MeV/nucleon; calculated neutron multiplicity distributions. Equilibrium approach to fragmentation, ergodicity assumption.

NUCLEAR STRUCTURE A=272; Z=108; calculated fission fragment multiplicity distribution. Equilibrium approach to fragmentation, ergodicity assumption.

doi: 10.1016/0375-9474(92)90460-2
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1992BO17      Phys.Rev. C46, 374 (1992)

J.P.Bondorf, C.H.Dasso, G.Massari, G.Pollarolo

Probing Time Scales in Projectile Fragmentation Processes at Intermediate Energies

NUCLEAR REACTIONS 197Au(16O, X), E=32.5 MeV/nucleon; calculated outgoing particle velocity distribution contours; deduced projectile breakup time scales. Target Coulomb field distorting effects.

doi: 10.1103/PhysRevC.46.374
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1991BA41      Nucl.Phys. A531, 453 (1991)

H.W.Barz, J.P.Bondorf, R.Donangelo, R.Elmer, F.S.Hansen, B.Jakobsson, L.Karlsson, H.Nifenecker, H.Schulz, F.Schussler, K.Sneppen, K.Soderstrom

Flow Effects in Intermediate-Energy Nuclear Collisions

NUCLEAR REACTIONS Ag, Br(36Ar, X), E ≈ 50-80 MeV/nucleon; Ag, Br(16O, X), E ≈ 200-220 MeV/nucleon; analyzed fragment average kinetic energy vs charge; deduced reaction mechanism features, per nucleon flow energy. Statistical multi-fragmentation model.

doi: 10.1016/0375-9474(91)90621-C
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1991WE05      Phys.Scr. 43, 240 (1991)

M.Westenius, M.Berg, H.-A.Gustafsson, B.Jakobsson, A.Kristiansson, A.Oskarsson, H.Ryde, S.Kox, F.Merchez, F.Schussler, J.P.Bondorf, O.-B.Nielsen, E.Andersen, G.Lovhoiden, T.F.Thorsteinsen, M.Maurel

Effects of Momentum Conservation on Light Particle Correlations in Intermediate Energy 12C Induced Heavy Ion Reactions

NUCLEAR REACTIONS C, 27Al, Cu(12C, X), E=35 MeV/nucleon; measured light charged particle-coin; deduced momentum conservation role.

doi: 10.1088/0031-8949/43/3/004
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1990BA26      Phys.Lett. 244B, 161 (1990)

H.W.Barz, J.P.Bondorf, K.Sneppen, H.Schulz

Velocity Correlations in the Multifragmentation Scenario

NUCLEAR REACTIONS Ag(16O, X), E=84 MeV/nucleon; calculated fragment relative velocity distribution function; deduced correlation data need. Primordial hot fragment evaporation.

doi: 10.1016/0370-2693(90)90047-A
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1990JA03      Nucl.Phys. A509, 195 (1990)

B.Jakobsson, G.Jonsson, L.Karlsson, V.Kopljar, B.Noren, K.Soderstrom, F.Schussler, E.Monnand, H.Nifenecker, G.Fai, J.P.Bondorf, K.Sneppen

On the Observation of a Transition from Fusion to Multifragmentation in High Multiplicity 16O Induced Reactions

NUCLEAR REACTIONS Br, Ag(16O, X), E=94 MeV/nucleon; measured high multiplicity collision charge distribution; deduced charge distribution moments.

doi: 10.1016/0375-9474(90)90381-U
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1990WE04      Nucl.Phys. A509, 630 (1990)

M.Westenius, M.Berg, H.-A.Gustafsson, B.Jakobsson, A.Kristiansson, A.Oskarsson, H.Ryde, S.Kox, F.Merchez, F.Schussler, J.P.Bondorf, O.-B.Nielsen, E.Andersen, G.Lovhoiden, T.F.Thorsteinsen, M.Maurel

Light-Particle Emission and Projectile Breakup in 35A MeV 12C Induced Collisions

NUCLEAR REACTIONS C, 27Al, Cu, 197Au(12C, X), E=35 MeV/nucleon; measured (particle)(particle)-coin, light charged particle inclusive spectra; deduced source velocities.

doi: 10.1016/0375-9474(90)90095-4
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1989BA09      Phys.Rev. C39, 1176 (1989)

H.W.Barz, H.Schulz, J.P.Bondorf, R.Donangelo, K.Sneppen

Multiplicity Distributions for the Reaction 40Ar on 27Al Calculated in the Statistical Multifragmentation Model

NUCLEAR REACTIONS 27Al(40Ar, X), E=25, 65 MeV/nucleon; calculated intermediate mass fragment production σ vs multiplicity. Statistical multifragmentation model.

doi: 10.1103/PhysRevC.39.1176
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1988BA28      Phys.Rev. C37, 2910 (1988)

H.W.Barz, J.P.Bondorf, J.A.Lopez, H.Schulz

Emission Temperature and Source Radii Inferred from Two-Particle Correlation Measurements in Nuclear Collisions

NUCLEAR REACTIONS 197Au(40Ar, X), E=60 MeV/nucleon; calculated fragment yield vs mass distribution. Kr(p, 12C), E not given; calculated σ(E(12C)). Statistical multi-fragmentation model.

doi: 10.1103/PhysRevC.37.2910
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1988BA53      Phys.Lett. 211B, 10 (1988)

H.W.Barz, H.Schulz, J.P.Bondorf, J.Lopez, K.Sneppen

On Isotopic Yield Ratios of Complex Fragments from Heavy Ion Induced Reactions

NUCLEAR STRUCTURE 58,64Ni, 108Ag, 197Au; calculated complex fragment isotope yield ratio. Statistical model.

doi: 10.1016/0370-2693(88)90797-6
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1987BA02      Nucl.Phys. A462, 742 (1987)

H.W.Barz, J.P.Bondorf, H.Schulz

Energy Spectra of Fragments Calculated with the Model of the Statistical Multifragmentation of Nuclei

NUCLEAR REACTIONS Kr, Xe(p, X), E=80-350 GeV; calculated σ(fragment E) for X=12C, 16O. Statistical multi-fragmentation model.

doi: 10.1016/0375-9474(87)90574-4
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1987BA03      Phys.Lett. 184B, 125 (1987)

H.W.Barz, J.P.Bondorf, H.Schulz

On the Limiting Excitation Energy of Nuclei

NUCLEAR STRUCTURE A=100; calculated entropy, temperature, multiplicity. Multi-fragmentation model.

doi: 10.1016/0370-2693(87)90554-5
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1987BA31      Phys.Lett. 191B, 232 (1987)

H.W.Barz, J.P.Bondorf, R.Donangelo, H.Schulz, K.Sneppen

Isotope Distribution in Nuclear Multifragmentation

NUCLEAR REACTIONS Kr(p, X), E=3.7, 6.5, 8 MeV/nucleon; calculated isotope distribution for mass ≤ 35. Statistical multi-fragmentation model.

doi: 10.1016/0370-2693(87)90245-0
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1987BA73      Europhys.Lett. 4, 997 (1987)

H.W.Barz, J.P.Bondorf, C.Guet, J.Lopez, H.Schulz

Subthreshold Pion Production and Statistical Multifragmentation in Nucleus-Nucleus Collisions

NUCLEAR REACTIONS 40Ca(40Ar, π0), E=44 MeV/nucleon; calculated σ(E(π0)). Multifragmentation model.

doi: 10.1209/0295-5075/4/9/008
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1987BO50      Nucl.Phys. A475, 663 (1987)

A.S.Botvina, A.S.Iljinov, I.N.Mishustin, J.P.Bondorf, R.Donangelo, K.Sneppen

Statistical Simulation of the Break-Up of Highly Excited Nuclei

NUCLEAR REACTIONS, MECPD Ag(3He, X), E ≈ 50-200 MeV; calculated σ(θ) for X=Li, C, N, O, Na.

doi: 10.1016/0375-9474(87)90232-6
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1986AN13      Phys.Lett. 174B, 18 (1986)

L.N.Andronenko, A.A.Kotov, L.A.Vaishnene, W.Neubert, H.W.Barz, J.P.Bondorf, R.Donangelo, H.Schulz

Mass Yield Distributions for 1 GeV Proton-Induced Nuclear Reactions on Ni and Ag

NUCLEAR REACTIONS Ni, Ag(p, X), E=1 GeV; calculated inclusive fragment σ vs mass.

doi: 10.1016/0370-2693(86)91120-2
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1986BA70      Nucl.Phys. A460, 714 (1986)

H.W.Barz, J.P.Bondorf, H.Schulz, L.N.Andronenko, A.A.Kotov, L.A.Vaishnene, W.Neubert

Onset of Multifragmentation Dominance at 1 GeV Proton-Induced Nuclear Reaction for Target Nuclei with A ≤ 160

RADIOACTIVITY 252Cf(SF); measured fission (fragment)(fragment)(θ); deduced longitudinal momentum transfer, multifragmentation dominance.

NUCLEAR REACTIONS Ag, Sm, U(p, F), E=1 GeV; measured fission (fragment)(fragment)(θ); deduced longitudinal momentum transfer, multifragmentation dominance.

doi: 10.1016/0375-9474(86)90533-6
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1986CA30      Phys.Scr. 34, 475 (1986)

L.Carlen, H.-A.Gustafsson, B.Jakobsson, A.Kristiansson, A.Oskarsson, H.Ryde, M.Westenius, J.P.Bondorf, O.-B.Nielsen, G.Lovhoiden, T.-F.Thorsteinsen, C.Guet, H.Nifenecker, D.Heuer, F.Schussler, M.Buenerd, P.Martin, J.Julien

Heavy Ion Collisions at Intermediate Energies

NUCLEAR REACTIONS 12C, 40Ca, 89Y, 208Pb(12C, 12C), E=1.032 GeV; compiled, analyzed σ(θ); Be, C, Ag(12C, X), E=86, 1050 MeV/nucleon; compiled, analyzed fragment σ; 12C(12C, 7Be), (12C, π+), (12C, 10B), Ag(12C, 7Be), 197Au(12C, X), E=75-86 MeV/nucleon; compiled double differential σ; C, Al, Au(C, 2p), E not given; compiled, analyzed pp-coin, σ ratio.


1985HE20      Phys.Lett. 161B, 269 (1985)

D.Heuer, R.Bertholet, C.Guet, M.Maurel, H.Nifenecker, Ch.Ristori, F.Schussler, J.P.Bondorf, O.B.Nielsen

Light Particles and Projectile-Like Fragments from the 40Ar + 12C Reaction at 44 MeV/Nucleon

NUCLEAR REACTIONS Ag, 12C(40Ar, X), E=1760 MeV; 12C(40Ar, X), E=8520 MeV; mesured production σ vs fragment Z. 12C, Ag(40Ar, 29Si), E=1760 MeV; measured σ(θ, E(29Si)); deduced reaction mechanism.

doi: 10.1016/0370-2693(85)90759-2
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1985KR03      Phys.Lett. 155B, 31 (1985)

P.Kristiansson, L.Carlen, H.-A.Gustafsson, B.Jakobsson, A.Oskarsson, H.Ryde, J.P.Bondorf, O.-B.Nielsen, G.Lovhoiden, T.-F.Thorsteinsen, D.Heuer, H.Nifenecker

Large-Angle Light Particle Correlations in 12C Induced Reactions at 85A MeV

NUCLEAR REACTIONS 197Au, 12C(12C, 2pX), (12C, 2dX), E=85 MeV/nucleon; measured (particle)(particle)-correlation ratio, difference vs θ; deduced structure, reaction mechanism.

doi: 10.1016/0370-2693(85)91027-5
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1985KR21      Nucl.Phys. A447, 577c (1985)

P.Kristiansson, J.P.Bondorf, L.Carlen, H.-A.Gustafsson, B.Jakobsson, A.Kristiansson, G.Lovhoiden, H.Nifenecker, O.-B.Nielsen, A.Oskarsson, H.Ryde, T.-F.Thorsteinsen, M.Westenius

Large-Angle Correlations Observed in Intermediate Energy Heavy Ion Collisions

NUCLEAR REACTIONS 12C, 27Al, 64Cu, 197Au(12C, 2p), (12C, 2d), (12C, 2t), (12C, 2α), E=85 MeV/nucleon; measured (particle)(particle)(θ), large angle; deduced reaction mechanism.

doi: 10.1016/0375-9474(86)90633-0
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1985NI05      Nucl.Phys. A442, 478 (1985)

H.Nifenecker, J.P.Bondorf

Nuclear Electromagnetic Bremsstrahlung: A new tool for studying heavy-ion reactions

NUCLEAR REACTIONS 238U(12C, γ), E=84 MeV/nucleon; 197Au(85Kr, γ), E=2550, 850 MeV; 197Au(20Ne, γ), E=140, 200, 600 MeV; calculated electromagnetic bremsstrahlung σ(Eγ, θ). Classical theory.

doi: 10.1016/S0375-9474(85)80028-2
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1984BE35      Nucl.Phys. A423, 511 (1984)

V.Bernard, J.Girard, J.Julien, R.Legrain, J.Poitou, A.Oskarsson, L.Carlen, H.-A.Gustafsson, B.Jakobsson, P.Kristiansson, B.Noren, I.Otterlund, H.Ryde, T.Johansson, G.Tibell, R.Bertholet, C.Guet, M.Maurel, H.Nifenecker, P.Perrin, F.Schussler, M.Buenerd, D.Lebrun, P.Martin, G.Lovhoiden, J.P.Bondorf, O.-B.Nielsen, A.Palmeri

Production of Charged Pions in Intermediate-Energy Heavy-Ion Collisions

NUCLEAR REACTIONS 7Li, 12C, 208Pb(12C, π+), E=60, 75, 85 MeV/nucleon; measured production σ(θ), σ(θ, E(π)); deduced (π-+) ratio.

doi: 10.1016/0375-9474(84)90038-1
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1984BO40      Nucl.Phys. A430, 445 (1984)

J.P.Bondorf, M.N.De, G.Fai, A.O.T.Karvinen

Spectator Recoil in Intermediate-Energy Heavy Ion Collisions

NUCLEAR REACTIONS 108Ag(40Ca, X), (12C, X), E=86 MeV/nucleon; 108Ag(20Ne, X), E=170 MeV/nucleon; calculated fragment recoil momentum vs spectator mass.

doi: 10.1016/0375-9474(84)90048-4
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1982BU17      Phys.Rev. C26, 1299 (1982)

M.Buenerd, P.Martin, R.Bertholet, C.Guet, M.Maurel, J.Mougey, H.Nifenecker, J.Pinston, P.Perrin, F.Schussler, J.Julien, J.P.Bondorf, L.Carlen, H.A.Gustafsson, B.Jakobsson, T.Johansson, P.Kristiansson, O.B.Nielsen, A.Oskarsson, I.Otterlund, H.Ryde, B.Schroder, G.Tibell

Observation of Rainbow Scattering in the 12C + 12C System at E(cm) = 508 MeV

NUCLEAR REACTIONS 12C(12C, 12C), E=1.016 GeV; measured σ(θ); deduced optical model parameters, σ(reaction), nuclear rainbow effect.

doi: 10.1103/PhysRevC.26.1299
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1319.


1982PR04      Nucl.Phys. A385, 483 (1982)

M.Prakash, S.Shlomo, B.S.Nilsson, J.P.Bondorf, F.E.Serr

Matter, Momentum and Energy Flow in Heavy-Ion Collisions

NUCLEAR REACTIONS 16O(16O, X), E=80, 320, 640 MeV; 40Ca(40Ca, X), E=800 MeV; calculated matter, momentum, energy flow. TDHF, Wigner distribution function.

doi: 10.1016/0375-9474(82)90099-9
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1981MO20      Phys.Lett. 105B, 25 (1981)

J.Mougey, R.Ost, M.Buenerd, A.J.Cole, C.Guet, D.Lebrun, J.M.Loiseaux, P.Martin, M.Maurel, E.Monnand, H.Nifenecker, P.Perrin, J.Pinston, C.Ristori, P.de Saintignon, F.Schussler, L.Carlen, B.Jakobsson, A.Oskarsson, I.Otterlund, B.Schroder, H.A.Gustafsson, T.Johansson, H.Ryde, J.P.Bondorf, O.B.Nielsen, G.Tibell

Projectile Fragments from 86 MeV/Nucleon 12C Induced Reactions

NUCLEAR REACTIONS 12C, Ag, Au(12C, X), E=86 MeV/nucleon; measured σ(fragment E, θ); deduced production σ for 6,7,8,9Li, 7,9,10Be, 8,10,11B, 9,10,11C, 12B. Fragmentation model.

doi: 10.1016/0370-2693(81)90032-0
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1981PR07      Phys.Rev.Lett. 47, 898 (1981)

M.Prakash, S.Shlomo, B.S.Nilsson, J.P.Bondorf, F.E.Serr

Microscopic Dynamical Calculation of Nucleon Flow in Heavy-Ion Reactions

NUCLEAR REACTIONS 16O(16O, X), E=80, 320, 640 MeV; calculated nucleon flow; deduced nucleon exchange mechanism. Deep inelastic collisions, microscopic dynamical calculation.

doi: 10.1103/PhysRevLett.47.898
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1980BO01      Nucl.Phys. A333, 285 (1980)

J.P.Bondorf, J.N.De, G.Fai, A.O.T.Karvinen, B.Jakobsson, J.Randrup

Promptly Emitted Particles in Nuclear Collisions

NUCLEAR REACTIONS 158Gd(12C, X), E=152 MeV; 146Nd(16O, X), E=126.5 MeV; 158Gd(α, X), E=45 MeV; 136Xe(45Sc, X), E=1360 MeV; calculated σ(E) for 1, 2 prompt nucleons. Proximity model, coupling of internal nucleon motion to relative nuclear motion.

doi: 10.1016/0375-9474(80)90234-1
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1979BO15      Phys.Lett. 84B, 162 (1979)

J.P.Bondorf, J.N.De, A.O.T.Karvinen, G.Fai, B.Jakobsson

Prompt Emission of Nucleons in Heavy-Ion Collisions

NUCLEAR REACTIONS 146Nd(16O, n), E=126.5 MeV; 158Gd(12C, n), E=152 MeV; calculated σ(E, θn, En); deduced mechanism of production of quasifree prompt emission. Sharp surface model.

doi: 10.1016/0370-2693(79)90273-9
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1979JA11      Phys.Lett. 82B, 35 (1979)

B.Jakobsson, J.P.Bondorf, G.Fai

Production of Pions in Heavy Ion Reactions below 500 MeV/Nucleon

NUCLEAR REACTIONS 16O, 108Ag, 238U(20Ne, π+), (20Ne, π-), E=250 MeV/nucleon; 238U(16O, π+), (16O, π-), E not given; Li, Na, Ba, Pb(12C, π-), (40Ar, π-), E=400 MeV/nucleon; calculated production σ, average multiplicity, absorption probability. Glauber multiple-scattering formalism with independent NN-scattering, two-step isobar model.

doi: 10.1016/0370-2693(79)90419-2
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1976BO41      Phys.Lett. 65B, 217 (1976)

J.P.Bondorf, H.T.Feldmeier, S.Garpman, E.C.Halbert

Classical Microscopic Description of U + U Collisions

NUCLEAR REACTIONS 235U(235U, X); calculated collision parameters.

doi: 10.1016/0370-2693(76)90166-0
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1975BO08      Phys.Rev. C11, 1265 (1975)

J.P.Bondorf, J.R.Huizenga, M.I.Sobel, D.Sperber

Classical Model for Strongly Damped Collisions in Heavy-Ion Reactions

NUCLEAR REACTIONS 209Bi(84Kr, X), E=600 MeV; analyzed reaction.

doi: 10.1103/PhysRevC.11.1265
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1973BO06      Nucl.Phys. A202, 30 (1973)

J.P.Bondorf

Statistical Fluctuations and Compound Elastic Scattering for 12C(12C, 12C)12C and 16O(16O, 16O)16O

NUCLEAR REACTIONS 12C(12C, 12C), 16O(16O, 16O), E=4-16 MeV cms; analyzed σ(E). Compound-nucleus model.

doi: 10.1016/0375-9474(73)90238-8
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1971BA30      Nucl.Phys. A165, 449 (1971)

B.B.Back, J.P.Bondorf, G.A.Otroschenko, J.Pedersen, B.Rasmussen

Fission of U, Np, Pu and Am Isotopes Excited in the (d, p) Reaction

NUCLEAR REACTIONS, Fission 233,235U, 237Np, 238,239,241Pu, 241,243Am(d, pF), E=13.0 MeV; measured σ(Ep, E(fragment)). 234,236U, 238Np, 239,240,242Pu, 242,244Am deduced fission probability, fission barrier heights, transparencies.

doi: 10.1016/0375-9474(71)90461-1
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1968BO16      Phys.Letters 27B, 5 (1968)

J.P.Bondorf, P.Von Brentano, P.Richard

Configurations of the Lowest 4- State in 208Pb

NUCLEAR STRUCTURE 208Pb; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0370-2693(68)90317-1
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1968EJ03      Phys.Lett. 28B, 304 (1968)

H.Ejiri, J.P.Bondorf

The (p, γ) Reaction Through Isobaric Analogue- and Giant Dipole Resonances

NUCLEAR REACTIONS 140Ce(p, γ), E not given; analyzed data. 141Pr deduced IAR, GDR amplitudes ratio, phase difference. Microscopic approach.

doi: 10.1016/0370-2693(68)90117-2
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1966AN04      Phys.Letters 22, 651 (1966)

B.L.Andersen, J.P.Bondorf, B.S.Madsen

Single-Particle Widths in 207Pb (pp) and (pp') for the Isobaric Analogue State of the Ground State of 208Pb

NUCLEAR STRUCTURE 208Bi; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.22.651
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