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Search: Author = H.W.Barz

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2006SC06      Phys.Rev.Lett. 96, 072301 (2006)

W.Scheinast, I.Bottcher, M.Debowski, F.Dohrmann, A.Forster, E.Grosse, P.Koczon, B.Kohlmeyer, F.Laue, M.Menzel, L.Naumann, E.Schwab, P.Senger, Y.Shin, H.Strobele, C.Sturm, G.Surowka, F.Uhlig, A.Wagner, W.Walus, B.Kampfer, H.W.Barz, and the KaoS Collaboration

In-Medium Effects on Phase Space Distributions of Antikaons Measured in Proton-Nucleus Collisions

NUCLEAR REACTIONS C, Au(p, K+X), (p, K-X), E=1.6, 2.5, 3.5 GeV; measured charged kaon production σ(E, θ), σ; deduced medium effects. Comparison with transport model calculations.

doi: 10.1103/PhysRevLett.96.072301
Citations: PlumX Metrics

2005BA55      Phys.Rev. C 71, 065207 (2005)

H.W.Barz, M.Zetenyi

Angular distribution and azimuthal asymmetry for pentaquark production in proton-proton collisions

NUCLEAR REACTIONS 1H(polarized p, X), E ≈ threshold; calculated pentaquark production σ(θ), azimuthal asymmetry, spin correlation parameters.

doi: 10.1103/PhysRevC.71.065207
Citations: PlumX Metrics

2005KO16      J.Phys.(London) G31, S741 (2005)

E.E.Kolomeitsev, C.Hartnack, H.W.Barz, M.Bleicher, E.Bratkovskaya, W.Cassing, L.W.Chen, P.Danielewicz, C.Fuchs, T.Gaitanos, C.M.Ko, A.Larionov, M.Reiter, Gy.Wolf, J.Aichelin

Transport theories for heavy-ion collisions in the 1 A GeV regime

NUCLEAR REACTIONS 197Au(197Au, X), E=0.96, 1.48 GeV/nucleon; Ni(Ni, X), E=1.93 GeV/nucleon; calculated proton, pion, and kaon multiplicities, transverse momentum and rapidity distributions. Several simulation programs compared.

doi: 10.1088/0954-3899/31/6/015
Citations: PlumX Metrics

2005ZE01      Nucl.Phys. A749, 174c (2005)

M.Zetenyi, H.W.Barz

Medium effects on φ meson production in near threshold proton-nucleus collisions

NUCLEAR REACTIONS C, Cu, Te, Au(p, X), E=2.5 GeV; calculated φ meson production σ, nuclear medium effects.

doi: 10.1016/j.nuclphysa.2004.12.028
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2004BA08      Phys.Rev. C 69, 024605 (2004)

H.W.Barz, M.Zetenyi

φ meson production in near-threshold proton-nucleus collisions

NUCLEAR REACTIONS C, Cu, Te, Au(p, X), E ≈ threshold; calculated φ meson production σ; deduced medium effects.

doi: 10.1103/PhysRevC.69.024605
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2003BA92      Phys.Rev. C 68, 041901 (2003)

H.W.Barz, L.Naumann

Contribution of the nucleon-hyperon reaction channels to K- production in proton-nucleus collisions

NUCLEAR REACTIONS C, Au(p, K+X), (p, K-X), E=2.5, 3.5 GeV; calculated kaon production σ(E, θ); deduced role of nucleon-hyperon channels. Transport model, comparisons with data.

doi: 10.1103/PhysRevC.68.041901
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2002BA49      Nucl.Phys. A705, 223 (2002)

H.W.Barz, M.Zetenyi, Gy.Wolf, B.Kampfer

Subthreshold φ Meson Production in Heavy-Ion Collisions

NUCLEAR REACTIONS Ni(Ni, X), E=1.93 GeV/nucleon; Ru(Ru, X), E=1.69 GeV/nucleon; calculated φ meson production σ, momentum distributions. Comparison with data.

doi: 10.1016/S0375-9474(02)00593-6
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2002ZE06      J.Phys.(London) G28, 2133 (2002)

M.Zetenyi, H.W.Barz, Gy.Wolf, B.Kampfer

Subthreshold φ Meson Production in Heavy-Ion Collisions

NUCLEAR REACTIONS Ni(Ni, X), E=1.93 GeV/nucleon; Ru(Ru, X), E=1.69 GeV/nucleon; calculated φ meson yields. Transport model, comparison with data.

doi: 10.1088/0954-3899/28/7/384
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2001BA21      Nucl.Phys. A683, 594 (2001)

H.W.Barz, B.Kampfer

The Role of Three-Body Collisions in φ Meson Production Processes Near Threshold

NUCLEAR REACTIONS 1H, 12C(p, X), E=1.5-2.6 GeV; calculated φ meson production σ; deduced in-medium effects, role of three-body processes. One-boson exchange model.

doi: 10.1016/S0375-9474(00)00446-2
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1999BA28      Phys.Rev. C59, 2214 (1999)


Combined Effects of Nuclear Coulomb Field, Radial Flow, and Opaqueness on Two-Pion Correlations

doi: 10.1103/PhysRevC.59.2214
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1999WO10      Prog.Part.Nucl.Phys. 42, 157 (1999)

G.Wolf, H.W.Barz, B.Kampfer

Thermal Particle Production at SIS ?

doi: 10.1016/S0146-6410(99)00069-1
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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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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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1996BA06      Phys.Rev. C53, R553 (1996)

H.W.Barz, B.Kampfer, Gy.Wolf, W.Bauer

Analysis of Hard Two-Photon Correlations Measured in Heavy-Ion Reactions at Intermediate Energies

NUCLEAR REACTIONS 27Al(36Ar, X), E=95 MeV/nucleon; Ni(86Kr, X), E=60 MeV/nucleon; 197Au(181Ta, X), E=39.5 MeV/nucleon; analyzed hard γγ(θ) data. BUU transport model.

doi: 10.1103/PhysRevC.53.R553
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1996BA21      Phys.Rev. C53, 2536 (1996)


Effects of Nuclear Coulomb Field on Two-Meson Correlation

NUCLEAR STRUCTURE Z=160; calculated two pion, two kaon correlations; deduced Coulomb field role.

doi: 10.1103/PhysRevC.53.2536
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1995HE13      Nucl.Phys. A588, 918 (1995); Erratum Nucl.Phys. A591, 755 (1995)

B.Heide, H.W.Barz

Collective Effects and Multifragmentation in Heavy-Ion Collisions at Intermediate Energies within a Hybrid Model

NUCLEAR REACTIONS 197Au(197Au, X), E=150, 250 MeV/nucleon; calculated multi-fragment flow energy, angular momenta vs impact parameter, charge, velocity distributions. Hybrid model, collective effects.

doi: 10.1016/0375-9474(95)00131-J
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1994HE32      Phys.Lett. 337B, 53 (1994)

B.Heide, H.W.Barz

Effects of Flow on Intermediate Mass Fragments in Central Gold on Gold Collisions

NUCLEAR REACTIONS 197Au(197Au, X), E=150 MeV/nucleon; analyzed fragment velocity distributions, correlation functions, charge, energy spectra; deduced flow effects. Central collisions, Boltzmann-Uehling-Uhlenbeck approach.

doi: 10.1016/0370-2693(94)91442-7
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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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1992HU06      Phys.Rev. C46, R1577 (1992)

J.Hubele, P.Kreutz, V.Lindenstruth, J.C.Adloff, M.Begemann-Blaich, P.Bouissou, G.Imme, I.Iori, G.J.Kunde, S.Leray, Z.Liu, U.Lynen, R.J.Meijer, U.Milkau, A.Moroni, W.F.J.Muller, C.Ngo, C.A.Ogilvie, J.Pochodzalla, G.Raciti, G.Rudolf, H.Sann, A.Schuttauf, W.Seidel, L.Stuttge, W.Trautmann, A.Tucholski, R.Heck, A.R.DeAngelis, D.H.E.Gross, H.R.Jaqaman, H.W.Barz, H.Schulz, W.A.Friedman, R.J.Charity

Statistical Fragmentation of Au Projectiles at E/A = 600 MeV

NUCLEAR REACTIONS C, 27Al, Cu, Pb(197Au, X), E=600 MeV/nucleon; measured intermediate mass fragments mean multiplicity.

doi: 10.1103/PhysRevC.46.R1577
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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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1991BA47      Phys.Lett. 267B, 317 (1991)

H.W.Barz, D.A.Cebra, H.Schulz, G.D.Westfall

Event Shape Analysis of the Reaction 40Ar + 51V within a Prompt Multifragmentation Scenario

NUCLEAR REACTIONS 51V(40Ar, X), E=35-85 MeV/nucleon; analyzed data; deduced multifragmentation mechanism. Statistical fragmentation followed by sequential decay.

doi: 10.1016/0370-2693(91)90938-M
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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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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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1987BA48      Phys.Lett. 194B, 459 (1987)

H.W.Barz, J.Bondorf, R.Donangelo, J.A.Lopez, H.Schulz

Ternary versus Binary Fragmentation Processes

NUCLEAR REACTIONS 100Mo(100Mo, X), E=12, 14.7, 18.8 MeV/nucleon; calculated ternary to binary fragmentation process ratio. Statistical multifragmentation model.

doi: 10.1016/0370-2693(87)90216-4
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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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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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1984BA42      Phys.Lett. 143B, 55 (1984)

H.W.Barz, H.Iwe

Calculation of Kaon Production in Heavy Ion Collisions within the Cascade Model

NUCLEAR REACTIONS Na, F(20Ne, K+), E=2.1 GeV; calculated kaon production σ. Nonanalog Monte Carlo technique.

doi: 10.1016/0370-2693(84)90803-7
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1983BA22      Z.Phys. A311, 311 (1983)

H.W.Barz, T.S.Biro, B.Lukacs, J.Zimanyi

Energy Dependence of the Production of Pions, Kaons and Antikaons Calculated in the Hadrochemical Model

NUCLEAR REACTIONS Na, F(Ne, K0), (Ne, π), E=1-2 GeV/nucleon; calculated production σ(E). Hadrochemical model.

doi: 10.1007/BF01415686
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1982BA17      Czech.J.Phys. B32, 335 (1982)

H.W.Barz, R.Wunsch

The Description of Hypernuclei in the Continuum Shell-Model

NUCLEAR REACTIONS 12C(K-, π-), E at 800 MeV/c; 16O(K-, π-), E at 715 MeV/c; calculated σ(θ). Continuum shell model.

doi: 10.1007/BF01602082
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1980BA11      J.Phys.(London) G6, L77 (1980)

V.V.Balashov, H.W.Barz, H.U.Jager

On the Nuclear Isovector Quadrupole Moment

NUCLEAR REACTIONS 11B(p, n), E=1 GeV; calculated σ(θ); deduced sensitivity to T=1 component of nuclear quadrupole component. Single elastic collision approximation.

doi: 10.1088/0305-4616/6/4/004
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1979BA60      Nucl.Phys. A330, 273 (1979)


Description of Continuum States of Deformed Nuclei within the Strong-Coupling Model

NUCLEAR REACTIONS 9Be(γ, n), E=4-36 MeV; calculated σ. 9Be(e, e'), E=resonance; calculated longitudinal form factor. Continuum treatment, 1p-1h excitation, adiabatic approximation.

doi: 10.1016/0375-9474(79)90054-X
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1979HO17      Nucl.Phys. A330, 109 (1979)

J.Hohn, H.W.Barz, I.Rotter

Continuum Shell-Model Investigation of the Photoexcited Giant Dipole Resonance in the Non-Magic Nucleus 13C

NUCLEAR REACTIONS 13C(γ, n), E=10-35 MeV; 12C(γ, p), E=20-35 MeV; calculated σ(E). Continuum shell model, 3 particle-2 hole configurations.

doi: 10.1016/0375-9474(79)90540-2
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1978BA52      Nucl.Phys. A307, 285 (1978)

H.W.Barz, I.Rotter, J.Hohn

Continuum Shell-Model Calculation of an Excited-State GDR Observed in the Reaction 15N(p, γ2)

NUCLEAR REACTIONS 15N(p, γ), E=10-24 MeV; calculated σ(E) for an excited-state GDR.

doi: 10.1016/0375-9474(78)90618-8
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1978RO05      Nucl.Phys. A297, 237 (1978)

I.Rotter, H.W.Barz, J.Hohn

Threshold Effects in Nuclear Reactions and the Line Shape of Resonances

NUCLEAR REACTIONS 15N(n, n), 16O(γ, n), (γ, p); calculated σ(θ), threshold effects.

doi: 10.1016/0375-9474(78)90274-9
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1977BA02      Nucl.Phys. A275, 111 (1977)

H.W.Barz, I.Rotter, J.Hohn

Coupled Channels Calculations in the Continuum Shell Model with Complicated Configurations

NUCLEAR REACTIONS 15N(p, n), E=3.75-7.5 MeV; calculated σ. 16O calculated resonances.

doi: 10.1016/0375-9474(77)90279-2
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1977HO32      Nukleonika 22, 1175 (1977)

J.Hohn, H.W.Barz, I.Rotter

On the Role of Complicated Configurations in Giant Resonances of Light Nuclei Investigated in the Frame of the Continuum Shell Model

NUCLEAR REACTIONS 13C(γ, np), E=10-35 MeV; calculated σ(E). 15N(p, γ), E=12-20 MeV; calculated σ(E, θ). Continuum shell model, GDR excitation.

1976BA48      Yad.Fiz. 24, 508 (1976); Sov.J.Nucl.Phys. 24, 264 (1976)

H.W.Barz, I.Birke, H.U.Jager, H.R.Kissener, I.Rotter, J.Hohn

Shell-Model Calculations for the 16O + γ Reaction with and Without Allowance for the Continuous Spectrum

NUCLEAR REACTIONS 16O(γ, n), (γ, p), (γ, X), E ≤ 26 MeV; calculated σ. Shell model.

1976RO16      Yad.Fiz. 24, 513 (1976); Sov.J.Nucl.Phys. 24, 266 (1976)

I.Rotter, H.W.Barz, J.Hohn

On Threshold Effects in Nuclear Reactions

NUCLEAR REACTIONS 15N(n, n'), E ≈ threshold; calculated σ; deduced threshold effects. Shell model.

1975BA26      Nukleonika 20, 413 (1975)

H.W.Barz, I.Rotter

The Calculation of Resonance Parameters in the Continuum Shell Model

NUCLEAR REACTIONS 15N(n, n), E=14.2-15.6 MeV; calculated σ, resonance parameters.

1975RO31      Fiz.Elem.Chastits At.Yadra 6, 435 (1975); Sov.J.Particles Nucl. 6, 175 (1976)

I.Rotter, H.W.Barz, R.Wunsch, J.Hohn

Coupled-Channels Method of Calculations in the Shell Model with Allowance for the Continuous Spectrum

NUCLEAR REACTIONS 15N(n, n), E=13-17 MeV; 15N(p, n), E=7.5-8.5 MeV; 16O(μ-, X); calculated σ.

1973BA74      Nucl.Phys. A217, 141 (1973)

H.W.Barz, V.E.Bunakov, A.M.El-Naiem

Recent Developments in the Theory of Stripping to Unbound States

NUCLEAR REACTIONS 15N, 16O(d, p), calculated σ(θ).

doi: 10.1016/0375-9474(73)90628-3
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1971BA95      Phys.Lett. 37B, 4 (1971)

H.W.Barz, I.Rotter, J.Hohn

Shell-Model Aspects in Coupled Channel Calculations Using Feshbach Projection Technique

NUCLEAR REACTIONS 15N(n, n), E=1-11 MeV; calculated σ(θ). 16N calculated resonances, level-width. Coupled-channel approximation, Feshbach projection method.

doi: 10.1016/0370-2693(71)90553-3
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1969BA19      Nucl.Phys. A126, 577 (1969)

H.W.Barz, K.Hehl, C.Riedel, R.A.Broglia

The Structure of 42Ca and 42Sc Investigated by Two-Nucleon Transfer Reactions

NUCLEAR STRUCTURE 42Ca, 42Sc; calculated levels using coexistence model.

NUCLEAR REACTIONS 40Ca(t, p), 40Ca(3He, p); calculated σ(θ), P(θ).

doi: 10.1016/0375-9474(69)90848-3
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1968BA51      Nucl.Phys. A122, 625(1968)

H.W.Barz, K.Hehl, C.Riedel, R.A.Broglia

An Average Set of Optical Triton Parameters Obtained from the Fit of (t, p) Angular Distributions

NUCLEAR REACTIONS 48Ca, 63Cu, 118Sn, 154Sm, 208Pb, 238U(t, p), E = 12 MeV; calculated σ(θ); deduced optical model parameters.

doi: 10.1016/0375-9474(68)90581-2
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1965BA31      Nucl.Phys. 73, 473 (1965)

H.W.Barz, R.Fulle, D.Netzband, R.Reif, K.Schlott, J.Slotta

The Reaction 10B(d, p0)11B

NUCLEAR REACTIONS 10B(d, p0), E = 13.5 MeV; measured σ(θ). 11B deduced level-width, L, S. Enriched target.

doi: 10.1016/0029-5582(65)90692-9
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