NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = H.W.Barz Found 54 matches. 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
2005BA55 Phys.Rev. C 71, 065207 (2005) 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
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
2005ZE01 Nucl.Phys. A749, 174c (2005) 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
2004BA08 Phys.Rev. C 69, 024605 (2004) 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
2003BA92 Phys.Rev. C 68, 041901 (2003) 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
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
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
2001BA21 Nucl.Phys. A683, 594 (2001) 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
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
1999WO10 Prog.Part.Nucl.Phys. 42, 157 (1999) Thermal Particle Production at SIS ?
doi: 10.1016/S0146-6410(99)00069-1
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-/π+ ratios; deduced Coulomb effects. Comparison with data.
doi: 10.1103/PhysRevC.57.2536
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
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
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
1995HE13 Nucl.Phys. A588, 918 (1995); Erratum Nucl.Phys. A591, 755 (1995) 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
1994HE32 Phys.Lett. 337B, 53 (1994) 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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
1984BA42 Phys.Lett. 143B, 55 (1984) 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
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
1982BA17 Czech.J.Phys. B32, 335 (1982) 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
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
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
1979HO17 Nucl.Phys. A330, 109 (1979) 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
1978BA52 Nucl.Phys. A307, 285 (1978) 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
1978RO05 Nucl.Phys. A297, 237 (1978) 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
1977BA02 Nucl.Phys. A275, 111 (1977) 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
1977HO32 Nukleonika 22, 1175 (1977) 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) 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) 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
1971BA95 Phys.Lett. 37B, 4 (1971) 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
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
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
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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