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NSR database version of April 11, 2024.

Search: Author = H.Schulz

Found 45 matches.

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1994DO13      Phys.Rev. C49, 3182 (1994)

R.Donangelo, A.Romanelli, H.Schulz, A.C.Sicardi-Schifino

Dynamical Effects in the Growth of Density Instabilities

doi: 10.1103/PhysRevC.49.3182
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1994SE14      Phys.Lett. 338B, 111 (1994)

A.D.Sedrakian, D.Blaschke, G.Ropke, H.Schulz

Nuclear In-Medium Effects on the Thermal Conductivity and Viscosity of Neutron Star Matter

NUCLEAR REACTIONS 1n(n, n), E not given; calculated σ vs E(rel) in nuclear medium; deduced neutron star matter viscosity, thermal conductivity in-medium effects dependence.

doi: 10.1016/0370-2693(94)91352-8
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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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1993CA34      Phys.Lett. 318B, 415 (1993)

L.F.Canto, R.Donangelo, A.Romanelli, H.Schulz

A Coupled-Channels Study of 11Li Coulomb Dissociation

NUCLEAR REACTIONS Pb(11Li, X), E=28 MeV/nucleon; analyzed projectile breakup data; deduced continuum-continuum coupling role. Coupled-channels approach, semi-classical approximation, breakup into 9Li+2n.

doi: 10.1016/0370-2693(93)91533-S
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1993IE01      Phys.Rev.Lett. 70, 730 (1993)

K.Ieki, D.Sackett, A.Galonsky, C.A.Bertulani, J.J.Kruse, W.G.Lynch, D.J.Morrissey, N.A.Orr, H.Schulz, B.M.Sherrill, A.Sustich, J.A.Winger, F.Deak, A.Horvath, A.Kiss, Z.Seres, J.J.Kolata, R.E.Warner, D.L.Humphrey

Coulomb Dissociation of 11Li

NUCLEAR REACTIONS Pb(11Li, X), E=28 MeV/nucleon; measured nn-correlation following projectile dissociation; deduced dissociation mechanism.

doi: 10.1103/PhysRevLett.70.730
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1993SA21      Phys.Rev. C48, 118 (1993)

D.Sackett, K.Ieki, A.Galonsky, C.A.Bertulani, H.Esbensen, J.J.Kruse, W.G.Lynch, D.J.Morrissey, N.A.Orr, B.M.Sherrill, H.Schulz, A.Sustich, J.A.Winger, F.Deak, A.Horvath, A.Kiss, Z.Seres, J.J.Kolata, R.E.Warner, D.L.Humphrey

Electromagnetic Excitation of 11Li

NUCLEAR REACTIONS Pb(11Li, X), E=28 MeV/nucleon; measured 9Li(n)-, γ(9Li)-coin following 11Li Coulomb dissociation; deduced dissociation σ, photonuclear σ(E1), breakup mechanism.

doi: 10.1103/PhysRevC.48.118
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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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1992PH02      Phys.Lett. 291B, 7 (1992)

L.Phair, M.A.Lisa, D.R.Bowman, C.K.Gelbke, W.G.Gong, Y.D.Kim, W.G.Lynch, G.F.Peaslee, H.Schulz, R.T.de Souza, M.B.Tsang, F.Zhu

Fluctuations in Multifragment Decays

NUCLEAR REACTIONS 197Au(36Ar, X), E=35-110 MeV/nucleon; analyzed charged particle distributions; deduced inconsistency with intermittency signals assumption.

doi: 10.1016/0370-2693(92)90111-G
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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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1990RO12      Fiz.Elem.Chastits At.Yadra 21, 364 (1990); Sov.J.Part.Nucl 21, 153 (1990)

G.Ropke, H.Schulz, K.K.Gudima, V.D.Toneev

Dynamical Approaches to Heavy-Ion Collisions at Intermediate Energies

NUCLEAR REACTIONS 40Ca(40Ca, X), E=50-400 MeV/nucleon; calculated nucleon density evolution. Various dynamical methods.

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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1988DO12      Z.Phys. A331, 107 (1988)

B.S.Dolbilkin, R.L.Kondratiev, V.P.Lisin, Sh.Khan, Th.Kihm, K.T.Knopfle, H.J.Schulz, Chenlin Wen, J.Friedrich

Direct Decay of the Giant Dipole Resonance in 58,60Ni and 64Zn from (e, e'c) Experiments

NUCLEAR REACTIONS 58,60Ni, 64Zn(e, e'p), (e, e'α), E=137.2 MeV; measured e'(particle)-coin spectra. 59,57Co, 63Cu deduced level population strengths.

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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1987GU05      Yad.Fiz. 45, 80 (1987)

K.K.Gudima, G.Ropke, V.D.Toneev, H.Schulz

Entropy of a System Formed in Heavy Ion Collisions

NUCLEAR REACTIONS Ar(Ar, X), Ca(Ca, X), 93Nb(93Nb, X), E=0.4-2 GeV/nucleon; calculated entropy evolution. Cascade model.

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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1985RO10      Phys.Rev. C31, 1556 (1985)

G.Ropke, H.Schulz, L.N.Andronenko, A.A.Kotov, W.Neubert, E.N.Volnin

Depletion of Light Cluster Production in 1 GeV Proton-Nucleus Collisions

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

doi: 10.1103/PhysRevC.31.1556
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1984RO19      Nucl.Phys. A424, 594 (1984)

G.Ropke, M.Schmidt, H.Schulz

Particle Clustering and Mott Transitions in Hot Nuclear Matter at Finite Temperature (III). Heavy Cluster Abundances and Coulomb Interaction

NUCLEAR STRUCTURE A=1-16; calculated cluster abundance vs mass. Debye-Thomas-Fermi approach, Coulomb interaction.

doi: 10.1016/0375-9474(84)90011-3
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1981MU17      Fiz.Elem.Chastits At.Yadra 12, 1001 (1981); Sov.J.Part.Nucl. 12, 403 (1981)

L.Munchow, H.Schulz

Quasiclassical Theory of Rapid Rotation

NUCLEAR STRUCTURE A=40-100; calculated density distribution, shape dependence on spin. Rotating nuclei, quasiclassical theory.

1978EF01      Nucl.Phys. A309, 344 (1978)

V.N.Efimov, H.Schulz

On a Simple Energy-Dependent Boundary Condition Model and the Binding Energy of the Triton

NUCLEAR STRUCTURE 3H; calculated binding energy. Energy-dependent boundary condition model.

doi: 10.1016/0375-9474(78)90486-4
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1976PE13      Yad.Fiz. 24, 313 (1976); Sov.J.Nucl.Phys. 24, 163 (1977)

V.P.Permyakov, H.Schulz

Dynamical Effects in Interactions of Complex Nuclei

NUCLEAR REACTIONS 208Pb, 146Nd, 152Sm(16O, X), 208Pb, 232Th(84Kr, X); calculated Coulomb barrier.

1974BA57      Phys.Scr. 10, 115 (1974)

J.Bang, V.E.Bunakov, F.A.Gareev, R.M.Jamalejev, H.Schulz

On the Possibilities in Calculations of Stripping Form Factors

NUCLEAR REACTIONS 42Ca(p, d); calculated σ(Ed, θ), form factors.

doi: 10.1088/0031-8949/10/3/004
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1974BA65      Yad.Fiz. 20, 346 (1974); Sov.J.Nucl.Phys. 20, 184 (1975)

J.Bang, T.Elin, H.Schulz

Calculation of Form Factors for Two-Nucleon Cluster Transfer

NUCLEAR REACTIONS 12C(t, p); calculated σ(Ep, θ), form factors.

1974BA85      Fiz.Elem.Chastits At.Yadra 5, 263 (1974); Sov.J.Particles Nucl. 5, 103 (1974)

J.Bang, V.E.Bunakov, F.A.Gareev, H.Schulz

Configuration Mixing Effects in Single-Nucleon Transfer Reactions

NUCLEAR REACTIONS 42Ca(p, d), E=26.5 MeV; calculated form factors. 176Yb(d, p), E=121 MeV; calculated σ(Ed, θ). 170Er(d, p); calculated σ.

1973GA12      Yad.Fiz. 17, 761 (1973); Sov.J.Nucl.Phys. 17, 397 (1974)

F.A.Gareev, M.Baznat, H.J.Wiebicke, H.Schulz

One-Nucleon Transfer Reactions to Quasi-Intersecting Levels 1/2+ [660] and 1/2+[400], 3/2+ [651] and 3/2+ [402]

NUCLEAR REACTIONS 160Gd, 164Dy(d, t); measured nothing, calculated σ(θ). 159Gd, 163Dy levels deduced β.

1973GA24      Nucl.Phys. A215, 570 (1973)

F.A.Gareev, R.M.Jamalejev, H.Schulz, J.Bang

A Method for Calculation of Stripping Form Factors in CCBA

NUCLEAR REACTIONS 52Cr(d, p), E=7.5 MeV; calculated σ(Ep, θ). 53Cr calculated levels, J, π, L.

doi: 10.1016/0375-9474(73)90489-2
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1972BE19      JINR-E4-6353 (1972)

V.B.Belyaev, H.Schulz

Calculation of the Body-Form Factor for the 3He and 3H Nuclei by Means Of the Modified BKR Potential

NUCLEAR STRUCTURE 3H, 3He; calculated charge form factors; analyzed singlet, triplet N-N interaction contributions.

1972GA06      Nucl.Phys. A182, 625 (1972)

S.I.Gabrakov, A.A.Kuliev, N.I.Pyatov, D.I.Salamov, H.Schulz

Collective 1+ States in Doubly Even Deformed Nuclei

NUCLEAR STRUCTURE 168Er; calculated levels, B(M1). Tamm-dankoff, RPA.

doi: 10.1016/0375-9474(72)90541-6
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1972KU15      Nucl.Phys. A189, 257 (1972)

A.B.Kurepin, H.Schulz, H.J.Wiebicke

Coupled-Channel Analysis of 12 MeV Proton Scattering on 148,154Sm

NUCLEAR REACTIONS 148,154Sm(p, p), (p, p'), E=12 MeV; analyzed σ(θ). 148,154Sm deduced deformation parameters β2, β4. Coupled-channel formalism.

doi: 10.1016/0375-9474(72)90294-1
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1972SC04      Nucl.Phys. A180, 625 (1972)

H.Schulz, H.J.Wiebicke, F.A.Gareev

Deuteron Stripping on Deformed Nuclei

NUCLEAR REACTIONS 24Mg, 176Yb(d, p), E=13.5, 12 MeV; calculated σ(θ). Coupled-channel DWBA.

doi: 10.1016/0375-9474(72)90884-6
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1970SC32      Nucl.Phys. A159, 324 (1970)

H.Schulz, H.J.Wiebicke, R.Fulle, D.Netzband, K.Schlott

A Generalized DWBA Model Applied to the 24Mg(d, p)25Mg Reaction at E = 13.5 MeV

NUCLEAR REACTIONS 24Mg(d, p), E=13.5 MeV; calculated σ(θ). DWBA.

doi: 10.1016/0375-9474(70)90045-X
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1967SC16      Nucl.Phys. A101, 577 (1967)

H.Schulz, H.J.Wiebicke, R.Reif

Single-Particle States in Non-Local Potentials and Direct Nuclear Reactions

doi: 10.1016/0375-9474(67)90653-7
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Note: The following list of authors and aliases matches the search parameter H.Schulz: , H.J.SCHULZ