NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = P.Martin Found 92 matches. 2010LA20 J.Phys.:Conf.Ser. 202, 012032 (2010) M.G.Lang, R.Diehl, W.Wang, P.Martin, R.Voss, K.Kretschmer Observations of cosmic nuclear gamma-ray lines
doi: 10.1088/1742-6596/202/1/012032
2006RE07 Astrophys.J. 647, L41 (2006) M.Renaud, J.Vink, A.Decourchelle, F.Lebrun, P.R.den Hartog, R.Terrier, C.Couvreur, J.Knodlseder, P.Martin, N.Prantzos, A.M.Bykov, H.Bloemen The signature of 44Ti in Cassiopeia a revealed by IBIS/ISGRI on INTEGRAL
doi: 10.1086/507300
2000FE09 Phys.Rev. D62, 013001 (2000) A.Ferrari, J.Collot, M.-L.Andrieux, B.Belhorma, P.de Saintignon, J.-Y.Hostachy, Ph.Martin, M.Wielers Sensitivity Study for New Gauge Bosons and Right-Handed Majorana Neutrinos in pp Collisions at √ s = 14 TeV NUCLEAR REACTIONS 1H(p, X), E(cm)=14 TeV; calculated gauge bosons production σ; deduced discovery potential. Left-right asymmetric model.
doi: 10.1103/PhysRevD.62.013001
1995MA82 Appl.Radiat.Isot. 46, 1065 (1995) P.Martin, G.J.Hancock, S.Paulka, R.A.Akber Determination of 227Ac by α-Particle Spectrometry RADIOACTIVITY 227Ac(α), (β-); measured α-spectra including those of daughter nuclei. Application to environmental samples concentration determination.
doi: 10.1016/0969-8043(95)00222-Y
1995SU24 Hyperfine Interactions 96, 23 (1995) D.Surono, F.-J.Hambsch, P.W.Martin Residence Sites of Fluorine in Crystalline Silicon and Highly Oriented Pyrolytic Graphite NUCLEAR REACTIONS 19F(p, p'), E=2.02 MeV; measured γ(θ, H, t); deduced electric field gradient at F impurity sites in crystalline Si, highly oriented pyrolytic graphite. Model comparison.
doi: 10.1007/BF02066269
1993BE19 Nucl.Phys. A555, 455 (1993) C.Berat, M.Buenerd, J.Y.Hostachy, P.Martin, J.Barrette, B.Berthier, B.Fernandez, A.Miczaika, A.Villari, H.G.Bohlen, S.Kubono, E.Stiliaris, W.von Oertzen Electric Isovector Nuclear Response from 13C Induced Charge-Exchange Reactions NUCLEAR REACTIONS 12C, 40Ca, 58,60Ni, 90Zr, 120Sn, 208Pb(13C, 13N), E=50 MeV/nucleon; measured σ(θ). 12B, 40K, 58,60Co, 90Y, 120In, 208Tl deduced GDR IAS. Microscopic DWBA.
doi: 10.1016/0375-9474(93)90296-A
1993MA66 Hyperfine Interactions 77, 315 (1993) P.W.Martin, D.Surono, F.-J.Hambsch, H.Postma, P.Rietveld TDPAC Measurements with Highly Oriented Pyrolytic Graphite Using the 19F(p, p')19F(*) and 19F(α, n)22Na(*) Reactions NUCLEAR REACTIONS 19F(p, p'), E ≈ resonance; 19F(α, n), E=3.42 MeV; measured γ(θ, H, t); deduced quadrupole interactions for 19F, 22Na levels, highly oriented pyrolytic host material.
doi: 10.1007/BF02320321
1992HU10 Appl.Radiat.Isot. 43, 1393 (1992) J.L.Hutter, T.J.Ruth, P.W.Martin Production of 77Br for TDPAC Studies RADIOACTIVITY 77Br(EC), (β+) [from 78Se(p, X), E=29 MeV]; measured Eγ, Iγ, γγ-coin, γγ(t); deduced suitability as probe for γγ(θ, H, t).
doi: 10.1016/0883-2889(92)90014-6
1992ME02 Phys.Rev. C45, 1189 (1992) A.Menchaca-Rocha, E.Garcia-Solis, E.Belmont-Moreno, M.E.Brandan, M.Buenerd, J.Chauvin, P.DeSaintignon, G.Duhamel, D.Lebrun, P.Martin, G.Perrin, J.Y.Hostachy Low-Energy Intermediate Mass Fragments in the 16O + 12C Reaction at 38 MeV/Nucleon NUCLEAR REACTIONS 12C(16O, X), E=708 MeV; measured σ(fragment θ, E) for X=6Li, 12C, σ(θ) for Z=3-9; deduced reaction residues yield mechanism. Cascade model.
doi: 10.1103/PhysRevC.45.1189
1990BR25 Nucl.Phys. A519, 631 (1990) M.Braeunig, W.von Oertzen, H.G.Bohlen, A.Miczaika, E.Stiliaris, M.Buenerd, C.Berat, J.Chauvin, D.Lebrun, J.Y.Hostachy, Ph.Martin, W.Mittig, J.Barrette, B.Berthier, B.Fernandez Proton Stripping Induced by 13C at 50 MeV/Nucleon on 12C, 40Ca and 58Ni NUCLEAR REACTIONS 12C, 40Ca, 58Ni(13C, 12B), E=50 MeV/nucleon; measured σ(θ). 13N, 41Sc, 59Cu levels deduced configurations, spectroscopic factors.
doi: 10.1016/0375-9474(90)90450-Z
1989BE50 Phys.Lett. 218, 299 (1989) C.Berat, M.Buenerd, J.Chauvin, J.Y.Hostachy, D.Lebrun, P.Martin, J.Barrette, B.Berthier, B.Fernandez, A.Miczaika, W.Mittig, E.Stiliaris, W.von Oertzen, H.Lenske, H.H.Wolter Heavy Ion Charge Exchange Reactions to Probe the Giant Electric Isovector Modes in Nuclei NUCLEAR REACTIONS 12C, 40Ca, 58Ni(13C, 13N), E=50 MeV/nucleon; measured angle integrated spectra, σ(θ). 12B, 40K, 58Co deduced GDR analog.
doi: 10.1016/0370-2693(89)91585-2
1989LE12 Phys.Lett. 223B, 139 (1989) D.Lebrun, J.Chauvin, D.Rebreyend, G.Perrin, P.De Saintignon, P.Martin, M.Buenerd, C.Le Brun, J.F.Lecolley, Y.Cassagnou, J.Julien, R.Legrain Heavy Ion Collision Geometry at 93 MeV/u from π-/π+ Measurement NUCLEAR REACTIONS 232Th, 197Au, Ag, 58Ni, 27Al, 12C, 7Li(16O, X)π+/π-, E=93 MeV/nucleon; measured σ(θπ) vs pion momentum, (π-/π+) yield ratio; deduced pion production mechanism.
doi: 10.1016/0370-2693(89)90229-3
1988BU21 Phys.Rev. C38, 2514 (1988) M.Buenerd, K.Bouhelal, Ph.Martin, J.Chauvin, D.Lebrun, G.Perrin, P.de Saintignon, G.Duhamel Quadrupole Transitions at Very Small Momentum Transfer in Nuclei NUCLEAR REACTIONS 58Ni, 92Mo, 120,124Sn, 140Ce, 208Pb(3He, 3He'), E=108.5 MeV; measured σ(θ). 58Ni, 92Mo, 120,124Sn, 140Ce, 208Pb deduced giant resonances excitation, deformation parameters, B(λ).
doi: 10.1103/PhysRevC.38.2514
1988DU17 Phys.Rev. C38, 2509 (1988) G.Duhamel, M.Buenerd, P.de Saintignon, J.Chauvin, D.Lebrun, Ph.Martin, G.Perrin Inelastic Alpha Scattering to the Giant Quadrupole and Monopole Resonances of 58Ni, 92Mo, and 120Sn at 152 MeV NUCLEAR REACTIONS 58Ni, 92Mo, 120Sn(α, α'), E=152 MeV; measured σ(θ). 58Ni, 92Mo, 120Sn deduced giant resonances, Γ, L, sum rule fraction.
doi: 10.1103/PhysRevC.38.2509
1988HO18 Nucl.Phys. A490, 441 (1988) J.Y.Hostachy, M.Buenerd, J.Chauvin, D.Lebrun, Ph.Martin, J.C.Lugol, L.Papineau, P.Roussel, N.Alamanos, J.Arvieux, C.Cerruti Elastic and Inelastic Scattering of 12C Ions at Intermediate Energies NUCLEAR REACTIONS 12C, 208Pb(12C, 12C), (12C, 12C'), E=1449, 2400 MeV; measured elastic, inelastic σ(θ); deduced optical-model parameters, transparency functions, reaction σ, sensitive region and energy dependence of the nuclear potentials. Near-side/far-side decomposition of the angular distributions. Glauber theory, including Fermi motion, Pauli blocking, finite size effects.
doi: 10.1016/0375-9474(88)90514-3
1988VO08 Nucl.Phys. A487, 195 (1988) W.von Oertzen, E.Adamides, M.Buenerd, J.Chauvin, D.Lebrun, J.Y.Hostachy, G.Duhamel, Ph.Martin, G.Perrin, P.de Saintignon Proton Transfer Induced by 13C at 30 MeV/u NUCLEAR REACTIONS 12C, 27Al, 58Ni, 90Zr(13C, 12B), (13C, 14N), E=30 MeV/nucleon; measured σ(θ). 11B, 89Y, 57Co, 91Nb, 59Cu levels deduced spectroscopic factors. DWBA analysis.
doi: 10.1016/0375-9474(88)90136-4
1987AD07 Nucl.Phys. A475, 598 (1987) E.Adamides, H.G.Bohlen, W.von Oertzen, M.Buenerd, J.Chauvin, D.Lebrun, J.Y.Hostachy, Ph.Martin, G.Perrin, P.de Saintignon Three-Body Continuum in (13C, 13N) and (13C, 14N) Reactions NUCLEAR REACTIONS 12C, 27Al, 58Ni, 90Zr(13C, 13N), (13C, 14N), E=390 MeV; measured σ(θ); deduced reaction mecanism. Three-body continuum treatment. Enriched targets. Magnetic spectrometer.
doi: 10.1016/0375-9474(87)90081-9
1987HO03 Phys.Lett. 184B, 139 (1987) J.Y.Hostachy, M.Buenerd, J.Chauvin, D.Lebrun, Ph.Martin, B.Bonin, G.Bruce, J.C.Lugol, L.Papineau, P.Roussel, J.Arvieux, C.Cerruti Elastic Scattering of 12C on 12C at E/A = 120 MeV/u and 200 MeV/u NUCLEAR REACTIONS 12C(12C, 12C), E=120, 200 MeV/nucleon; measured σ(θ); deduced surface transparency onset. Magnetic spectrometer. Optical model analyses.
doi: 10.1016/0370-2693(87)90557-0
1987KA34 Hyperfine Interactions 35, 895 (1987) B.Kastelein, A.den Ouden, H.Postma, H.C.Meijer, P.W.Martin, J.G.Hooley Electric Quadrupole Nuclear Orientation of 182Ta as Graphite Intercalation Compound TaCl(5) RADIOACTIVITY 182Ta(β-); measured γ(θ), oriented nuclei; deduced electric field gradient in TaCl.
doi: 10.1007/BF02394518
1987MA18 Nucl.Phys. A466, 119 (1987) Optical Model Analysis of 14 to 40 MeV Neutron Elastic Scattering from 27Al, 28Si and 32S NUCLEAR REACTIONS 27Al, 28Si, 32S(n, n), (polarized n, n), E=14-40 MeV; analyzed σ(θ), A(θ); deduced model parameters. Optical model.
doi: 10.1016/0375-9474(87)90348-4
1987WE07 Phys.Rev. C36, 585 (1987) H.Weigmann, P.W.Martin, R.Kohler, I.van Parijs, F.Poortmans, J.A.Wartena Structure of Unbound States in 29Si from Neutron Resonance Spectroscopy of 28Si + n NUCLEAR REACTIONS 28Si(n, n), (n, γ), E=30-4640 keV; measured total, capture σ(E). 29Si deduced resonances, J, π, (gΓn), (gΓnΓγ/Γ), level density, neutron strength functions, B(λ). Natural target. R-matrix analyses.
doi: 10.1103/PhysRevC.36.585
1986BR25 Phys.Rev. C34, 1484 (1986) M.E.Brandan, A.Menchaca-Rocha, M.Buenerd, J.Chauvin, P.DeSaintignon, G.Duhamel, D.Lebrun, P.Martin, G.Perrin, J.Y.Hostachy Elastic and Inelastic 16O + 12C Scattering at 38 MeV/Nucleon NUCLEAR REACTIONS 12C(16O, 16O), (16O, 16O'), E=608 MeV; measured σ(θ); deduced reaction σ. Magnetic spectrometer. Optical model, DWBA analyses.
doi: 10.1103/PhysRevC.34.1484
1986BU03 Phys.Lett. 167B, 379 (1986) M.Buenerd, J.Chauvin, G.Duhamel, J.Y.Hostachy, D.Lebrun, P.Martin, P.O.Pellegrin, G.Perrin, P.De Saintignon Search for High Excitation Energy Structures in the 20Ne + 208Pb System at E/A = 30 MeV NUCLEAR REACTIONS 208Pb(20Ne, 20Ne), (20Ne, 20Ne'), E=600 MeV; measured σ(E(20Ne)), σ(θ). 208Pb deduced giant resonance excitation. DWBA analysis.
doi: 10.1016/0370-2693(86)91284-0
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.
1986MA38 Phys.Rev. C34, 384 (1986) Analyzing Power of 27Al(n(pol), n(pol)0) at 14 and 17 MeV and the Isospin Dependence of the Optical Model Potential NUCLEAR REACTIONS 27Al(polarized n, n), E=14, 17, 11 MeV; measured σ(θ), analyzing power vs θ; deduced model parameters, isospin dependence, σ. 27Al(polarized p, p), E=19, 23 MeV; analyzed σ(θ), analyzing power vs θ.
doi: 10.1103/PhysRevC.34.384
1986MC04 Phys.Rev.Lett. 56, 2156 (1986) P.L.McGaughey, K.D.Bol, M.R.Clover, R.M.DeVries, N.J.DiGiacomo, J.S.Kapustinsky, W.E.Sondheim, G.R.Smith, J.W.Sunier, Y.Yariv, M.Buenerd, J.Chauvin, D.Lebrun, P.Martin, J.C.Dousse Dynamics of Low-Energy Antiproton Annihilation in Nuclei as Inferred from Inclusive Proton and Pion Measurements NUCLEAR REACTIONS 12C, 89Y, 238U(p-bar, π+X), (p-bar, pX), E at 608 MeV/c; measured annihilation production σ for π+, p. Intranuclear cascade models.
doi: 10.1103/PhysRevLett.56.2156
1986VO02 Z.Phys. A323, 373 (1986) W.von Oertzen, M.Buenerd, J.Chauvin, D.Lebrun, J.Y.Hostachy, Ph.Martin, G.Perrin, P.De Saintignon Charge Exchange Reactions (13C, 13N) and (13C, 13B) on 12C NUCLEAR REACTIONS 12C(13C, 13N), (13C, 13B), E=30 MeV/nucleon; measured σ(E(13N)), σ(E(13B)). 12B, 12N deduced GDR excitation.
1985GA01 Phys.Rev. C31, 94 (1985) S.Gales, C.P.Massolo, S.Fortier, J.P.Schapira, P.Martin, V.Comparat Proton Stripping to Outer Subshells and the Damping of Single-Particle States: 116Sn, 144Sm, and 208Pb(α, t) reactions at 80 MeV NUCLEAR REACTIONS 116Sn, 144Sm, 208Pb(α, t), E=80 MeV; measured σ(Et, θt). 117Sb, 145Eu, 209Bi deduced levels, L, J, π, S, IAS. DWBA analysis. Magnetic spectrometer, enriched targets.
doi: 10.1103/PhysRevC.31.94
1985SM09 Hyperfine Interactions 23, 375 (1985) F.A.Smith, P.W.Martin, A.Shukri Perturbed Angular Correlation Measurements on the 40.9 keV Level of 62Cu. A Preliminary Study of 2Zn-Insulin RADIOACTIVITY 62Zn(β+), (EC) [from 60Ni(α, 2n), E=24 MeV]; measured γγ(θ, H, t). 62Cu deduced quadrupole moment estimate.
doi: 10.1007/BF02058953
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-/π+) ratio.
doi: 10.1016/0375-9474(84)90038-1
1984BL09 J.Phys.(Paris), Colloq.C4, 201 (1984); See 1984Bl23 Y.Blumenfeld, Ph.Chomaz, N.Frascaria, J.P.Garron, J.C.Jacmart, J.C.Roynette, W.Bohne, W.Von Oertzen, M.Buenerd, A.Gamp, D.Lebrun, Ph.Martin High Excitation Energy Structures in Heavy Ion Collisions on a 208Pb Target
1984BL23 J.Phys.(Paris), Colloq.C-4, 201 (1984) Y.Blumenfeld, Ph.Chomaz, N.Frascaria, J.P.Garron, J.C.Jacmart, J.C.Roynette, W.Bohne, W.von Oertzen, M.Buenerd, A.Gamp, D.Lebrun, Ph.Martin High Excitation Energy Structures in Heavy Ion Collisions on a 208Pb Target NUCLEAR REACTIONS 208Pb(36Ar, X), E=11 MeV/nucleon; 208Pb(20Ne, X), E=30 MeV/nucleon; measured fragment σ(θ), σ(EX, θX). Tof spectrometer.
1984BU22 Nucl.Phys. A424, 313 (1984) M.Buenerd, A.Lounis, J.Chauvin, D.Lebrun, P.Martin, G.Duhamel, J.C.Gondrand, P.De Saintignon Elastic and Inelastic Scattering of Carbon Ions at Intermediate Energies NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E=360, 1016 MeV; 208Pb(13C, 13C), (13C, 13C'), E=390 MeV; measured σ(θ); deduced optical model parameters, transparency functions, reaction σ, inelastic σ(E).
doi: 10.1016/0375-9474(84)90186-6
1984CH18 Z.Phys. A318, 41 (1984) Ph.Chomaz, N.Frascaria, Y.Blumenfeld, J.P.Garron, J.C.Jacmart, J.C.Roynette, W.Bohne, A.Gamp, W.Von Oertzen, M.Buenerd, D.Lebrun, Ph.Martin High Excitation Energy Structures in 208Pb NUCLEAR REACTIONS 208Pb(36Ar, 36Ar'), E=11 MeV/nucleon; 208Pb(20Ne, 20Ne'), E=30 MeV/nucleon; measured σ(θ), σ(θ, E(36Ar')), σ(θ, E(20Ne')); deduced reaction mechanism. 208Pb deduced high excitation structures, excitation process, Γ. DWBA analysis.
doi: 10.1007/BF02117213
1983ME22 Phys.Lett. 131B, 31 (1983) A.Menchaca-Rocha, M.E.Brandan, M.Buenerd, J.Chauvin, D.Lebrun, P.Martin, P.de Saintignon, J.C.Gondrand, I.Dorion, A.Lounis Measurement of Reactions Induced by 30 MeV/A 12C NUCLEAR REACTIONS 12C, 58Ni(12C, α), (12C, 9Be), (12C, X), 197Au(12C, X), E=30 MeV/nucleon; measured σ(θ, Eα), σ(θ, E(9Be)), σ(fragment θ) for X=10C, 10B, 7Be, 6,7Li. Coalescence model analysis.
doi: 10.1016/0370-2693(83)91085-7
1983WA01 Phys.Rev. C27, 98 (1983) E.Warde, G.J.Costa, D.Magnac, R.Seltz, C.Gerardin, M.Buenerd, Ph.Martin, W.Saathoff, C.A.Wiedner Band Structure in 180Ta Studied with Transfer Reactions NUCLEAR REACTIONS 181Ta(p, d), E=19 MeV; 179Hf(3He, d), E=36 MeV; 179Hf(α, t), E=62.2 MeV; measured σ(θ). 180Ta deduced levels, J, π, isomer state neutron separation energies, characteristics, rotational bands, bandhead configurations. DWBA, Nilsson model analyses.
doi: 10.1103/PhysRevC.27.98
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
1982GA12 Phys.Rev.Lett. 48, 1593 (1982) G.Gales, C.P.Massolo, S.Fortier, E.Gerlic, J.Guillot, E.Hourani, J.M.Maison, J.P.Schapira, B.Zwieglinski, P.Martin, V.Comparat High-Lying Proton Strengths Observed in Stripping Reactions NUCLEAR REACTIONS 144Sm(α, t), E=80 MeV; 144Sm(3He, d), E=240 MeV; measured σ(θ), σ(Et), σ(Ed). 145Eu deduced broad structures, Γ, L, J, π, C2S, h9/2, i13/2 proton strength distribution. Zero-range DWBA analysis.
doi: 10.1103/PhysRevLett.48.1593
1981BU08 Phys.Lett. 102B, 242 (1981) M.Buenerd, J.Pinston, J.Cole, C.Guet, D.Lebrun, J.M.Loiseaux, P.Martin, E.Monnand, J.Mougey, H.Nifenecker, R.Ost, P.Perrin, Ch.Ristori, P.de Saintignon, F.Schussler, L.Carlen, H.A.Gustafsson, B.Jakobsson, T.Johansson, G.Jonsson, J.Krumlinde, I.Otterlund, H.Ryde, B.Schroder, G.Tibell, J.B.Bondorf, O.B.Nielsen Elastic and Inelastic Scattering of 1.03 GeV 12C Projectiles NUCLEAR REACTIONS 12C, Ca, 89Y, 208Pb(12C, 12C), (12C, 12C'), E=86 MeV/nucleon; measured σ(θ); deduced optical model parameters. 40Ca deduced evidence for GQR. Natural Ca target. Optical model, DWBA analyses.
doi: 10.1016/0370-2693(81)90867-4
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
1980BU16 Phys.Rev.Lett. 45, 1667 (1980) M.Buenerd, D.Lebrun, Ph.Martin, P.de Saintignon, C.Perrin Evidence for Deformation Effect on the Giant Monopole Resonance NUCLEAR REACTIONS 140Ce, 144,150,152Sm, 159Tb, 165Ho, 169Tm, 181Ta, 197Au, 208Pb, 232Th(3He, 3He'), E=108.5 MeV; measured σ(E(3He), θ). 140Ce, 144,150,152Sm, 159Tb, 165Ho, 169Tm, 181Ta, 197Au, 208Pb, 232Th deduced giant monopole resonance, Γ, EWSR strengths, coupling to giant quadrupole vibrations.
doi: 10.1103/PhysRevLett.45.1667
1980LE25 Phys.Lett. B97, 358 (1980) D.Lebrun, M.Buenerd, P.Martin, P.de Saintignon, G.Perrin Is there a Giant Monopole Resonance in Light Nuclei < Question > NUCLEAR REACTIONS 12C, 27Al, 40Ca, 56Fe, 58,60Ni(3He, 3He'), E=108.5 MeV; measured σ(E(3He), θ). 40Ca deduced weak giant monopole resonance. 12C, 27Al, 56Fe, 58,60Ni deduced monopole resonance, Γ, EWSR. DWBA analysis.
doi: 10.1016/0370-2693(80)90619-X
1979BU08 Phys.Lett. 84B, 305 (1979) M.Buenerd, C.Bonhomme, D.Lebrun, P.Martin, J.Chauin, G.Duhamel, G.Perrin, P.de Saintignon Inelastic Scattering of 108.5 MeV 3He Particles at Very Small Momentum Transfer to the Giant Monopole Resonance of 90Zr and 208Pb NUCLEAR REACTIONS 90Zr, 208Pb(3He, 3He'), E=105 MeV; measured σ(θ). 90Zr, 208Pb deduced giant M1 resonance. DWBA analysis.
doi: 10.1016/0370-2693(79)90045-5
1979GA13 Nucl.Phys. A327, 349 (1979) Y.R.Gaillard, P.Martin, G.Perrin, P.Desaintignon, M.Buenerd, J.M.Loiseaux, J.L.Escudie, A.Tarrats, H.V.Geramb Excitation Function of Giant Resonances as Doorway States in the 12C(P, P)12C Reaction between 19 and 23 MeV NUCLEAR REACTIONS 12C(p, p), E=19.15-23.34 MeV; measured σ(E, θ)A(E, θ). 13N deduced giant resonance strength distribution. Optical model, coupled channel, anti-symmetrized distorted-wave approximation.
doi: 10.1016/0375-9474(79)90264-1
1979MA06 Nucl.Phys. A315, 291 (1979) P.Martin, Y.Gaillard, P.de Saintignon, G.Perrin, J.Chauvin, G.Duhamel, J.M.Loiseaux Excitation of Low-Lying Levels and Giant Resonances in 90Zr via 57.5 MeV Polarized Proton Inelastic Scattering NUCLEAR REACTIONS 90Zr(polarized p, p'), E=57.5 MeV; measured σ(E(X), θ), Ay(E(X), θ), E=0-27 MeV. 90Zr deduced excitation of bound states, giant resonances. Collective, microscopic-model distorted-wave analysis. Enriched target.
doi: 10.1016/0375-9474(79)90612-2
1979MO12 Phys.Rev. C20, 1593 (1979) A.Moalem, Y.Gaillard, A.M.Bemolle, M.Buenerd, J.Chauvin, G.Duhamel, D.Lebrun, P.Martin, G.Perrin, P.de Saintignon Isotopic Dependence of the Giant Quadrupole Resonance in the Stable Even-Mass Molybdenum Nuclei NUCLEAR REACTIONS 100,98,96,94,92Mo(3He, 3He'), E=110 MeV; measured σ(E, θ). 100,98,96,94,92Mo deduced E, Γ, strength of GQR.
doi: 10.1103/PhysRevC.20.1593
1978BU10 Phys.Rev.Lett. 40, 1482 (1978) M.Buenerd, D.Lebrun, J.Chauvin, Y.Gaillard, J.M.Loiseaux, P.Martin, G.Perrin, P.de Saintignon Heavy-Ion Inelastic Scattering to Giant Resonances NUCLEAR REACTIONS 90Zr, 208Pb(12C, 12C'), E=120 MeV; 40Ca, 90Zr, 197Au, 208Pb, 209Bi(14N, 14N'), E=161 MeV; measured spectra. 40Ca, 90Zr, 197Au, 208Pb, 209Bi deduced giant resonances.
doi: 10.1103/PhysRevLett.40.1482
1978DO01 Phys.Rev. C17, 131 (1978) H.Doubre, J.C.Roynette, E.Plagnol, J.M.Loiseaux, P.Martin, P.deSaintignon Experimental Study of the 20Ne + 12C System. NUCLEAR REACTIONS 12C(20Ne, 20Ne), (20Ne, 20Ne'), (20Ne, 16O), E=45-93 MeV; measured σ(E;θ). Optical model, coupled-channel analysis.
doi: 10.1103/PhysRevC.17.131
1977BU19 Nucl.Phys. A286, 377 (1977) M.Buenerd, P.Martin, P.de Saintignon, J.M.Loiseaux Study of the High-Lying States of 12C by Inelastic Scattering of Hadrons NUCLEAR REACTIONS 12C(p, p'), E=45, 155 MeV; 12C(α, α'), E=60 MeV; measured σ(θ). 12C deduced levels, J, π, L, T, λ, βlr, strengths.
doi: 10.1016/0375-9474(77)90591-7
1977MC01 Can.J.Phys. 55, 456 (1977) P.R.H.McConnell, P.W.Martin, B.G.Turrell Nuclear Orientation of 206Bi in Nickel RADIOACTIVITY 206Bi; measured γ-spectra, γ(θ, t); deduced hyperfine field. 206Pb transitions deduced δ.
doi: 10.1139/p77-064
1977PE09 Phys.Lett. 68B, 55 (1977) G.Perrin, D.Lebrun, J.Chauvin, P.Martin, P.De Saintignon, D.Eppel, H.V.Geramb, H.L.Yadav, V.A.Madsen The Octupole Giant Resonance Strength in 16O NUCLEAR REACTIONS 16O(polarized p, p'), E=42.5, 44.0, 49.3 MeV; measured σ(Ep', θ), A(θ). 16O deduced octupole strength.
doi: 10.1016/0370-2693(77)90033-8
1976BU15 Phys.Rev. C14, 1316 (1976) M.Buenerd, P.Martin, P.de Saintignon, J.M.Loiseaux Experimental Study of Giant Dipole and Quadrupole Resonances in 16O NUCLEAR REACTIONS 16O(p, p'), E=45 MeV; 16O(α, α'), E=60 MeV; measured σ(θ). 16O giant resonance deduced Γ.
doi: 10.1103/PhysRevC.14.1316
1976CH28 Nucl.Phys. A274, 223 (1976) A.Chevarier, N.Chevarier, A.Demeyer, P.Martin, P.de Saintignon Incomplete Fusion Observed in 12C and 16O Induced Reactions Leading to The Same Composite Systems NUCLEAR REACTIONS 51V, 56Fe(16O, X), E=81 MeV; 55Mn, 60Ni(12C, X), E=77 MeV; measured σ(E(fragment charge), θ), Z=2-9.
doi: 10.1016/0375-9474(76)90238-4
1976LE16 Nucl.Phys. A265, 291 (1976) D.Lebrun, G.Perrin, P.Martin, P.de Saintignon, J.Arvieux, M.Buenerd, H.V.Geramb, K.A.Amos Evidence of an Isoscalar E3 Giant Resonance in 16O NUCLEAR REACTIONS 16O(polarized p, p'), E=31.7, 33.8, 35.8, 36.8, 39.9 MeV; measured σ(Ep', θ), A(θ). 16O deduced isoscalar resonance, E3 strengths. Distorted wave analyses include giant resonance effects.
doi: 10.1016/0375-9474(76)90355-9
1976PO05 Nucl.Phys. A262, 493 (1976) R.J.Powers, F.Boehm, P.Vogel, A.Zehnder, T.King, A.R.Kunselman, P.Roberson, P.Martin, G.H.Miller, R.E.Welsh, D.A.Jenkins Muonic X-Ray Study of the Charge Distribution of 165Ho ATOMIC PHYSICS 165Ho(μ-, X-ray); measured E(X-ray), I(X-ray). 165Ho deduced quadrupole moment, hexadecapole moment, nuclear charge distribution. NUCLEAR MOMENTS 165Ho; measured muonic X-rays, quadrupole moment, hexadecapole moment, nuclear charge distribution.
doi: 10.1016/0375-9474(76)90511-X
1975DO06 J.Phys.(Paris), Suppl.Lett. 36, L-113 (1975) H.Doubre, E.Plagnol, J.C.Roynette, J.M.Loiseaux, P.Martin, P.de Saintignon How Does the Elastic Scattering of 12C + 20Ne Compare with That of 16O + 16O (Question) NUCLEAR REACTIONS 12C(20Ne, 20Ne), (20Ne, 16O), (20Ne, X), E(cm)=22-28 MeV; measured σ(θ).
doi: 10.1051/jphyslet:01975003605011300
1975PO03 Phys.Rev.Lett. 34, 492 (1975) R.J.Powers, F.Boehm, P.Vogel, A.Zehnder, T.King, A.R.Kunselman, P.Roberson, P.Martin, G.H.Miller, R.E.Welsh, D.A.Jenkins Precise Determination of E2 and E4 Moments in 165Ho from Muonic X Rays NUCLEAR MOMENTS 165Ho; analyzed hfs data; deduced quadrupole moment.
doi: 10.1103/PhysRevLett.34.492
1974BU17 Phys.Rev.Lett. 33, 1233 (1974) M.Buenerd, P.de Saintignon, P.Martin, J.M.Loiseaux Proton Inelastic Scattering to Dipole States of 12C and Isovector Collective Models NUCLEAR REACTIONS 12C(p, p'), E=45, 155 MeV; measured σ(Ep', θ). 12C deduced resonances, L, level-width.
doi: 10.1103/PhysRevLett.33.1233
1974CO34 Nucl.Phys. A233, 73 (1974) S.Cochavi, S.Gilad, M.A.Moinester, J.Alster, M.Buenerd, P.Martin Study of the 91Zr(d, 3He)90Y Reaction NUCLEAR REACTIONS 91Zr(d, 3He), E=28 MeV; measured σ(E(3He), θ). 90Y deduced levels, L(p), C2S, J, π. Enriched target.
doi: 10.1016/0375-9474(74)90241-3
1974GI09 Nucl.Phys. A233, 81 (1974) S.Gilad, S.Cochavi, M.A.Moinester, J.Alster, M.Buenerd, P.Martin Study of the 92,96Zr(d, α)90,94Y Reactions NUCLEAR REACTIONS 92,94,96Zr(d, α), E=28 MeV; measured σ(Eα, θ). 96Zr(d, α), E=28 MeV; measured Q. 90,92,94Y deduced levels, J, π. Enriched targets.
doi: 10.1016/0375-9474(74)90242-5
1974KE18 Aust.J.Phys. 27, 759 (1974) M.J.Kenny, P.W.Martin, L.E.Carlson, J.A.Biggerstaff Gamma Ray Transitions Following keV Neutron Capture in 2s-1d Shell Nuclei NUCLEAR REACTIONS 19F(n, γ), E=27, 44, 49 keV; 27Al(n, γ), E=35 keV; 28Si(n, γ), E=38, 66.7 keV; 29Si(n, γ), E=15, 26 keV; 32S(n, γ), E=30, 43 keV; 40Ar(n, γ), E=15-70 keV; measured Eγ, Iγ. 20F, 29,30Si, 28Al, 33S resonances deduced transitions, γ-width, E1, M1-strength.
doi: 10.1071/PH740759
1974PO12 Nucl.Phys. A230, 413 (1974) R.J.Powers, P.Martin, G.H.Miller, R.E.Welsh, D.A.Jenkins Muonic 197Au: A Test of the Weak-Coupling Model NUCLEAR MOMENTS 197Au; measured quadrupole moment, nuclear charge distribution. Muonic X-rays. ATOMIC PHYSICS, Mesic-Atoms 197Au; measured E(X), I(X); deduced nuclear charge distribution, quadrupole moment, weak-coupling parameters.
doi: 10.1016/0375-9474(74)90147-X
1973CA31 Aust.J.Phys. 26, 459 (1973) L.E.Carlson, M.R.Najam, W.F.Davidson, J.A.Biggerstaff, P.W.Martin The Placement of the 188 keV Transition in 70Ga NUCLEAR REACTIONS 70Zn, 71Ga(p, nγ), E=3 MeV; measured Eγ, γ(t). 70Ga level deduced T1/2.
doi: 10.1071/PH730459
1973DU02 Phys.Rev. C7, 637 (1973) Study of 42K, 42Ca and 46K, 46Ca by Pickup Reactions NUCLEAR REACTIONS 44,48Ca(p, t), 43Ca(p, d), E=40 MeV; 44,48Ca(p, 3He), E=40, 56 MeV; measured σ(θ). 42K, 46K, 42,46Ca deduced levels, J, π, L(n), S.
doi: 10.1103/PhysRevC.7.637
1973HE06 Phys.Lett. 43B, 289 (1973) Symmetry Studies of the Sequential Reaction 7Li(d, αn)4He NUCLEAR REACTIONS 7Li(d, αn)E=1.0; measured αn(θ).
doi: 10.1016/0370-2693(73)90442-5
1973HE26 Nucl.Phys. A212, 78 (1973) Angular Correlation Measurements in the 7Li(d, nα)4He Reaction NUCLEAR REACTIONS 7Li(d, αn), E=1.0 MeV; measured σ(En, Eα, θ(n), θ(α)). Enriched target.
doi: 10.1016/0375-9474(73)90038-9
1973LU01 Phys.Rev. C7, 1678 (1973) G.R.Lucas, Jr., P.Martin, G.H.Miller, R.E.Welsh, D.A.Jenkins, R.J.Powers, A.R.Kunselman Neutron Emission Following Muon Capture in 142Ce, 140Ce, 138Ba, and 120Sn NUCLEAR REACTIONS 120Sn, 138Ba, 140,142Ce(μ-, nγ); measured Eγ, Iγ, 139,140,141,142La, 135,136,137,138Ba, 117,118,119,120In deduced levels, absolute yield per muon capture.
doi: 10.1103/PhysRevC.7.1678
1973MA03 Nucl.Phys. A202, 257 (1973) Excited States of 16O between 13.5 and 15.0 MeV NUCLEAR REACTIONS 12C(α, α0), 12C(α, α'), E=8.5-10.5 MeV; measured σ(Eα;θ). 16O deduced resonances, J, π, level-width. Natural target.
doi: 10.1016/0375-9474(73)90222-4
1973MA36 Can.J.Phys. 51, 2197 (1973) P.W.Martin, R.McFadden, B.L.White Small Angle Elastic Scattering of 4.3 MeV Neutrons from U, Bi, and Pb NUCLEAR REACTIONS Pb, Bi, U(n, n), E=4.3 MeV; measured σ(θ).
doi: 10.1139/p73-286
1973MA45 Phys.Rev. C8, 2453 (1973) P.Martin, G.H.Miller, R.E.Welsh, D.A.Jenkins, R.J.Powers, A.R.Kunselman Nuclear Polarization and Charge Parameters Using the Muonic 2s State ATOMIC PHYSICS 120Sn, 138Ba, 140,142Ce, 206Pb; measured muonic X-rays. Deduced nuclear polarization.
doi: 10.1103/PhysRevC.8.2453
1973MA46 Nucl.Phys. A212, 304 (1973) P.Martin, J.B.Viano, J.M.Loiseaux, Y.Le Chalony (d, 6Li) Reactions on Intermediate Mass Nuclei NUCLEAR REACTIONS 40,42Ca, 56Fe, 58Ni(d, 6Li), E=28 MeV; 56Fe, 114Sn(d, 6Li), E=36 MeV; measured σ(θ); 36,38Ar, 52Cr, 54Fe, 110Cd levels deduced relative S. Enriched targets.
doi: 10.1016/0375-9474(73)90566-6
1973MO03 Nucl.Phys. A202, 473 (1973) M.A.Moinester, G.Finkel, J.Alster, P.Martin Neutron Hole States in 91Mo and 93Mo Studied by the (p, d) Reaction NUCLEAR REACTIONS 92Mo(p, d), 94Mo(p, d), E=40 MeV; measured σ(Ed, θ), Q. 91,93Mo deduced levels, L(n), C2S, J, π, analog states. Enriched targets.
doi: 10.1016/0375-9474(73)90637-4
1973TE05 Phys.Lett. 45B, 235 (1973) Y.Terrien, J.L.Escudie, M.Buenerd, J.M.Loiseaux, P.Martin, J.B.Viano The Role of the Imaginary Part in the Microscopic Description of (p, p') Scattering NUCLEAR REACTIONS 92Mo, 116,120,124Sn(p, p'), E=40 MeV; measured σ(θ).
doi: 10.1016/0370-2693(73)90191-3
1972DA14 Can.J.Phys. 50, 2373 (1972) P.W.Daly, R.L.A.Gorling, P.W.Martin, B.G.Turrell The Magnetic Moment of 59Fe RADIOACTIVITY 59Fe; oriented nuclei; measured Iγ(θ); deduced μ limit.
doi: 10.1139/p72-313
1972MA23 Nucl.Phys. A185, 465 (1972) P.Martin, M.Buenerd, Y.Dupont, M.Chabre Proton-Deuteron Reactions at 40 MeV on the Calcium Isotopes NUCLEAR REACTIONS 40,42,44,48Ca(p, d);E=40 MeV; measured σ(θ). 39,41,43,47Ca deduced levels, J, π, L, S. Enriched targets.
doi: 10.1016/0375-9474(72)90025-5
1972MA53 Nucl.Phys. A194, 491 (1972) A Search for an 8+ Level in 16O with the 12C(α, 8Be)8Be Reaction NUCLEAR REACTIONS 12C(α, 8Be), E=15.0-18.96 MeV; measured σ(Eα;θ). 16O deduced levels. Natural target.
doi: 10.1016/0375-9474(72)90997-9
1972MI11 Phys.Rev. C6, 487 (1972) G.H.Miller, M.Eckhause, P.Martin, R.E.Welsh Yields of Gamma Rays Emitted Following Capture of Negative Muons by 28Si and 24Mg NUCLEAR REACTIONS 24Mg, 28Si(μ-, Xγ), E approx 0; measured σ(Eγ), γ-ray yields.
doi: 10.1103/PhysRevC.6.487
1972MI15 Phys.Lett. 41B, 50 (1972) G.H.Miller, M.Eckhause, F.R.Kane, P.Martin, R.E.Welsh Negative Muon Capture in Carbon Leading to Specific Final States NUCLEAR REACTIONS 12C(μ-, Xγ), E approx 0; measured σ(Eγ); deduced direct capture rate to 12B states.
doi: 10.1016/0370-2693(72)90365-6
1972MI18 Phys.Rev.Lett. 29, 1194 (1972) G.H.Miller, M.Eckhause, F.R.Kane, P.Martin, R.E.Welsh γ-Neutrino Angular Correlations in Muon Capture NUCLEAR REACTIONS 28Si(μ-, νγ), E approx 0; measured νγ(θ).
doi: 10.1103/PhysRevLett.29.1194
1972SC19 Phys.Rev. C5, 1593 (1972) J.P.Schapira, M.Chabre, Y.Dupont, P.Martin Reaction 42Ca(p, t)40Ca at 40 MeV NUCLEAR REACTIONS 42Ca(p, t), E=40 MeV; measured σ(Et, θ). 40Ca deduced levels, J, π.
doi: 10.1103/PhysRevC.5.1593
1971JE04 Nucl.Phys. A175, 73 (1971) D.A.Jenkins, R.J.Powers, P.Martin, G.H.Miller, R.E.Welsh 2s Atomic Level in Muonic 208Pb ATOMIC PHYSICS, Mesic-Atoms 208Pb; measured μ-mesic E(X-ray), I(X-ray). 208Pb deduced nuclear charge parameters, nuclear polarization.
doi: 10.1016/0375-9474(71)90622-1
1971OP01 Nucl.Phys. A173, 609 (1971) T.R.Ophel, Ph.Martin, S.D.Cloud, J.M.Morris Energy Levels of 16O in the Region of Excitation between 13.5 and 15.0 MeV NUCLEAR REACTIONS 12C(α, α0), 12C(α, α'), 12C(α, α'γ), 12C(α, p), Eα=8.5-10.5 MeV; measured σ(Eα;θ), Doppler profiles. 16O deduced levels, J, π, level-width. Natural target.
doi: 10.1016/0375-9474(71)90975-4
1970BL07 Nucl.Phys. B19, 632 (1970) R.Blomquist, M.Eckhause, F.R.Kane, J.R.Kane, P.Martin, G.H.Miller, W.W.Sapp, C.B.Spence, R.E.Welsh Nuclear Gamma Rays in 19F Following Stopping Pions NUCLEAR REACTIONS 19F(π-, Xγ), E approx o; measured Eγ. 19F deduced transitions.
doi: 10.1016/0550-3213(70)90373-1
1970DU01 Phys.Lett. 31B, 68 (1970) Observation of T = 4 States in 46Ca and Level Structure of 46K NUCLEAR REACTIONS 48Ca(p, t), (p, 3He), E=40 MeV; measured σ(Et, θ), σ(E(3He), θ). 46K, 46Ca deduced levels, J, π, isobaric analogs.
doi: 10.1016/0370-2693(70)90044-4
1970JE05 Phys.Lett. 32B, 267 (1970) D.A.Jenkins, R.J.Powers, P.Martin, G.H.Miller, R.E.Welsh, A.R.Kunselman The 2s Atomic Level in Muonic 140Ce ATOMIC PHYSICS, Mesic-Atoms 140Ce; measured μ-mesic X-ray spectra; deduced nuclear charge distribution, polarization.
doi: 10.1016/0370-2693(70)90524-1
1970OP01 Phys.Lett. 32B, 101 (1970) T.R.Ophel, S.D.Cloud, P.Martin, J.M.Morris A 6+ Level in 16O NUCLEAR REACTIONS 12C(α, α), (α, α'), E=8.5-10.5 MeV; measured σ(E;θ). 16O deduced resonance.
doi: 10.1016/0370-2693(70)90597-6
1968MA28 Can.J.Phys. 46, 1657 (1968) Gamma Rays from the Interaction of 14.1-MeV Neutrons NUCLEAR STRUCTURE 25Mg, 24Mg, 26Mg, 27Mg, 56Fe, 55Mn, 32S, 28Si, 29Si, 30Si, 22Ne, 23Ne, 23Na; measured not abstracted; deduced nuclear properties.
doi: 10.1139/p68-495
1968RE10 Can.J.Phys. 46, 2241 (1968) M.A.Reimann, P.W.Martin, E.W.Vogt Effect of the Lifetime of the Intermediate 5Li State in the 6Li(3He, αp)4He Reaction NUCLEAR STRUCTURE 6Li; measured not abstracted; deduced nuclear properties.
doi: 10.1139/p68-575
1968WI08 Nucl.Phys. A114, 377(1968) M.R.Wigan, R.A.Bell, P.J.Martin, O.N.Jarvis, J.P.Scanlon Measurements of the Differential Cross Section and Polarization in Proton-Proton Scattering at About 98 MeV NUCLEAR REACTIONS 1H(p, p), (polarized p, p), E approx 98 MeV; measured σ(θ), polarization P(θ).
doi: 10.1016/0375-9474(68)90361-8
1967JE01 Nucl.Phys. A105, 689(1967) H.Jeremie, P.Martin, A.Calamand Three-Body Break-up in the Reaction 7Li(d, n)αα NUCLEAR REACTIONS 7Li(d, n)αα, E=180 keV; measured σ(Eα, θ nα). Natural target.
doi: 10.1016/0375-9474(67)90545-3
1967RE03 Phys.Rev.Letters 18, 246 (1967) M.A.Reimann, P.W.Martin, E.W.Vogt Structure-Dependent Asymmetry in Sequential Breakup from the Reaction Li6(He3, Pα)He4 NUCLEAR STRUCTURE 6Li; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.18.246
1964ST30 Nucl.Phys. 60, 349 (1964) Gamma Rays From The Interaction Of 14 Mev Neutrons With C12 And Mg24 NUCLEAR REACTIONS 12C(n, n'), 24Mg(n, n'), E=14.1 MeV; measured products, 12C, 24Mg; deduced σ(θ). Data were imported from EXFOR entry 21132.
doi: 10.1016/0029-5582(64)90669-8
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