NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = S.Gales Found 103 matches. Showing 1 to 100. [Next]2020ZY01 Phys.Rev. C 101, 042802 (2020) A.B.Zylstra, H.W.Herrmann, Y.H.Kim, A.McEvoy, J.A.Frenje, M.Gatu-Johnson, R.D.Petrasso, V.Yu.Glebov, C.Forrest, J.Delettrez, S.Gales, M.Rubery 2H(p, γ)3He cross section measurement using high-energy-density plasmas NUCLEAR REACTIONS 2H(p, γ)3He, E=16.35 keV; measured En, In, Eγ, Iγ, using neutron time-of-flight suite and gas Cherenkov detectors for γ radiation at the OMEGA inertial confinement fusion facility at Livermore; deduced S factor for the reaction. Comparison with previous results from accelerator based experiments, evaluations and with model predictions. Relevance to nuclear energy in protostars and brown dwarfs, and to big-bang nucleosynthesis.
doi: 10.1103/PhysRevC.101.042802
2015FI10 Eur.Phys.J. A 51, 185 (2015) D.Filipescu, A.Anzalone, D.L.Balabanski, S.S.Belyshev, F.Camera, M.La Cognata, P.Constantin, L.Csige, P.V.Cuong, M.Cwiok, V.Derya, W.Dominik, M.Gai, S.Gales, I.Gheorghe, B.S.Ishkhanov, A.Krasznahorkay, A.A.Kuznetsov, C.Mazzocchi, V.N.Orlin, N.Pietralla, M.Sin, C.Spitaleri, K.A.Stopani, O.Tesileanu, C.A.Ur, I.Ursu, H.Utsunomiya, V.V.Varlamov, H.R.Weller, N.V.Zamfir, A.Zilges Perspectives for photonuclear research at the Extreme Light Infrastructure - Nuclear Physics (ELI-NP) facility
doi: 10.1140/epja/i2015-15185-9
2015UR02 Acta Phys.Pol. B46, 743 (2015) C.A.Ur, D.Balabanski, G.Cata-Danil, S.Gales, I.Morjan, O.Tesileanu, D.Ursescu, I.Ursu, N.V.Zamfir New Frontiers in Nuclear Physics Research at ELI-NP
doi: 10.5506/APhysPolB.46.743
2014BA17 Acta Phys.Pol. B45, 483 (2014) D.L.Balabanski, G.Cata-Danil, D.Filipescu, S.Gales, O.Tesileanu, C.A.Ur, I.Ursu, N.V.Zamfir The Extreme Light Infrastructure Nuclear Physics Facility: Towards Experiments with Brilliant γ-Ray Beams
doi: 10.5506/APhysPolB.45.483
2010GA23 Nucl.Phys. A834, 717c (2010) SPIRAL2 at GANIL: Next Generation of ISOL Facility for Intense Secondary Radioactive Ion Beams
doi: 10.1016/j.nuclphysa.2010.01.130
2008ZE01 Phys.Rev. C 77, 024307 (2008) R.G.T.Zegers, E.F.Brown, H.Akimune, Sam M.Austin, A.M.van den Berg, B.A.Brown, D.A.Chamulak, Y.Fujita, M.Fujiwara, S.Gales, M.N.Harakeh, H.Hashimoto, R.Hayami, G.W.Hitt, M.Itoh, T.Kawabata, K.Kawase, M.Kinoshita, K.Nakanishi, S.Nakayama, S.Okumura, Y.Shimbara, M.Uchida, H.Ueno, T.Yamagata, M.Yosoi Gamow-Teller strength for the analog transitions to the first T = 1/2, Jπ = 3/2- states in 13C and 13N and the implications for type Ia supernovae NUCLEAR REACTIONS 13C(3He, t), E=420 MeV; measured charged particles, σ(θ); deduced B(GT), levels, J, π. 13C(p, n); deduced electron capture rates in stellar environments as a function of temperature.
doi: 10.1103/PhysRevC.77.024307
2007IB01 Nucl.Phys. A787, 110c (2007) F.Ibrahim, D.Verney, M.Lebois, B.Roussiere, S.Essabaa, S.Franchoo, S.Gales, D.Guillemaud-Mueller, C.Lau, F.Le Blanc, J.F.Le Du, M.C.Mhamed, A.C.Mueller, J.Sauvage, and the ALTO Collaboration The ALTO facility at IPN Orsay and study of neutron rich nuclei in the vicinity of 78Ni NUCLEAR REACTIONS 238U(γ, F)78Zn/132Sn, E not given; measured fission fragment yields. ALTO facility. 238U(n, F)81Zn/83Ga, E not given; measured Eγ, Iγ, Eβ, Iβ, γγ-coin. 81Ga, 83Ge deduced levels, J, π. Online mass separator.
doi: 10.1016/j.nuclphysa.2006.12.021
2007ME25 Nucl.Instrum.Methods Phys.Res. B264, 221 (2007) R.Meharchand, H.Akimune, A.M.van den Berg, Y.Fujita, M.Fujiwara, S.Gales, M.N.Harakeh, H.Hashimoto, R.Hayami, G.W.Hitt, M.Itoh, T.Kawabata, K.Kawase, M.Kinoshita, K.Nakanishi, S.Nakayama, S.Okumura, Y.Shimbara, M.Uchida, T.Yamagata, M.Yosoi, R.G.T.Zegers Atomic charge-exchange between semi-relativistic (ν/c = 0.49) helium ions and targets from carbon to lead NUCLEAR REACTIONS C, Mg, Ni, Zr, Sn, Pb(3He, 3He), E=420 MeV; measured singly to doubly charged yield ratios. Compared results to model calculations.
doi: 10.1016/j.nimb.2007.08.078
2007VE08 Phys.Rev. C 76, 054312 (2007) D.Verney, F.Ibrahim, C.Bourgeois, S.Essabaa, S.Gales, L.Gaudefroy, D.Guillemaud-Mueller, F.Hammache, C.Lau, F.Le Blanc, A.C.Mueller, O.Perru, F.Pougheon, B.Roussiere, J.Sauvage, O.Sorlin, for the PARRNe Collaboration Low-energy states of 8131Ga50 Proton structure of the nuclei close to 78Ni RADIOACTIVITY 81Zn, 81Ga, 81Ge, 81As (β-) [from U(d, F), E=26 MeV]; 81Zn, 81Ga (β-n); measured Eγ, Iγ, γγ-, βγ-coin, half-lives. 81Ga; deduced levels, J, π, configurations. 81Ga, 83As; calculated levels, J, π, configurations. 80Zn, 81Ga, 82Ge, 83As, 84Se, 85Br, 86Kr, 87Rb; systematics.
doi: 10.1103/PhysRevC.76.054312
2007ZE06 Phys.Rev.Lett. 99, 202501 (2007) R.G.Zegers, T.Adachi, H.Akimune, S.M.Austin, A.M.van den Berg, B.A.Brown, Y.Fujita, M.Fujiwara, S.Gales, C.J.Guess, M.N.Harakeh, H.Hashimoto, K.Hatanaka, R.Hayami, G.W.Hitt, M.E.Howard, M.Itoh, T.Kawabata, K.Kawase, M.Kinoshita, M.Matsubara, K.Nakanishi, S.Nakayama, S.Okumura, T.Ohta, Y.Sakemi, Y.Shimbara, Y.Shimizu, C.Scholl, C.Simenel, Y.Tameshige, A.Tamii, M.Uchida, T.Yamagata, M.Yosoi Extraction of Weak Transition Strengths via the (3He, t) Reaction at 420 MeV NUCLEAR REACTIONS 12,13C, 18O, 26Mg, 58Ni, 60Ni, 90Zr, 118Sn, 208Pb(3He, t), E=420 MeV; measured triton spectra and cross sections. Deduced B(GT).
doi: 10.1103/PhysRevLett.99.202501
2006GU02 Phys.Rev. C 73, 014616 (2006) J.Guillot, S.Gales, D.Beaumel, S.Fortier, E.Rich, N.Van Giai, G.Colo, A.M.van den Berg, S.Brandenburg, B.Davids, M.N.Harakeh, M.Hunyadi, M.de Huu, S.Y.van der Werf, H.J.Wortche, C.Baumer, D.Frekers, E.-W.Grewe, P.Haefner, B.C.Junk, M.Fujiwara The (t, 3He) reaction at 43 MeV/nucleon on 48Ca and 58Ni: Results and microscopic interpretation NUCLEAR REACTIONS 12C, 48Ca, 58Ni(t, 3He), E=43 MeV/nucleon; measured excitation energy spectra, σ(E, θ). 48K, 58Co deduced giant resonance features.
doi: 10.1103/PhysRevC.73.014616
2006PE20 Eur.Phys.J. A 28, 307 (2006) O.Perru, D.Verney, F.Ibrahim, O.Bajeat, C.Bourgeois, F.Clapier, E.Cottereau, C.Donzaud, S.Du, M.Ducourtieux, S.Essabaa, S.Gales, D.Guillemaud-Mueller, O.Hubert, C.Lau, H.Lefort, F.Le Blanc, A.C.Mueller, J.Obert, N.Pauwels, J.C.Potier, F.Pougheon, J.Proust, B.Roussiere, J.Sauvage, O.Sorlin Study of the N = 50 major shell effect toward 78Ni at PARRNe: Evidence of a weak-coupling structure in 8332Ge51 RADIOACTIVITY 83Ga(β-); 84Ga(β-n) [from 238U(n, F), E=fast]; measured Eγ, Iγ, Eβ, Iβ, γγ-coin, βγ-coin. 83Ge deduced levels, J, π, transitions. Isotope separator.
doi: 10.1140/epja/i2005-10285-9
2006ZE01 Phys.Rev. C 74, 024309 (2006) R.G.T.Zegers, H.Akimune, S.M.Austin, D.Bazin, A.M.van den Berg, G.P.A.Berg, B.A.Brown, J.Brown, A.L.Cole, I.Daito, Y.Fujita, M.Fujiwara, S.Gales, M.N.Harakeh, H.Hashimoto, R.Hayami, G.W.Hitt, M.E.Howard, M.Itoh, J.Janecke, T.Kawabata, K.Kawase, M.Kinoshita, T.Nakamura, K.Nakanishi, S.Nakayama, S.Okumura, W.A.Richter, D.A.Roberts, B.M.Sherrill, Y.Shimbara, M.Steiner, M.Uchida, H.Ueno, T.Yamagata, M.Yosoi The (t, 3He) and (3He, t) reactions as probes of Gamow-Teller strength NUCLEAR REACTIONS 26Mg(t, 3He), E=115 MeV/nucleon; 26Mg(3He, t), E=140 MeV/nucleon; measured σ(E, θ); deduced Gamow-Teller transition strengths. Comparison with model predictions.
doi: 10.1103/PhysRevC.74.024309
2005GU11 Nucl.Phys. A752, 349c (2005) J.Guillot, C.Baumer, D.Beaumel, A.M.van den Berg, S.Brandenburg, G.Colo, B.Davids, S.Fortier, D.Frekers, E.-W.Grewe, M.Fujiwara, S.Gales, P.Haefner, M.N.Harakeh, M.Hunyadi, M.de Huu, B.C.Junk, E.Rich, N.Van Giai, S.Y.van der Werf, H.J.Wortche Investigation of Isovector Excitations via the (t, 3He) reaction at Et=43 MeV/u on 58Ni and 48Ca targets: microscopic interpretation NUCLEAR REACTIONS 48Ca, 58Ni(t, 3He), E=130 MeV; analyzed particle spectra, σ(θ); deduced resonance features.
doi: 10.1016/j.nuclphysa.2005.02.044
2004GU02 Nucl.Phys. A731, 106 (2004) J.Guillot, D.Beaumel, A.M.van den Berg, S.Brandenburg, B.Davids, S.Fortier, M.Fujiwara, S.Gales, M.N.Harakeh, M.Hunyadi, M.de Huu, H.J.Wortche Investigation of IVGRs via the 58Ni(t, 3He)58Co reaction NUCLEAR REACTIONS 58Ni(t, 3He), E=130 MeV; measured particle spectra, σ(θ); deduced monopole resonance strength distribution. Comparison with RPA predictions.
doi: 10.1016/j.nuclphysa.2003.11.022
2004VE14 Braz.J.Phys. 34, 979 (2004) D.Verney, F.Ibrahim, O.Perru, O.Bajeat, C.Bourgeois, F.Clapier, E.Cottereau, C.Donzaud, S.Du, M.Ducourtieux, S.Essabaa, S.Gales, L.Gaudefroy, D.Guillemaud-Mueller, F.Hammache, F.Hosni, C.Lau, H.Lefort, F.Le Blanc, A.C.Mueller, N.Pauwels, J.C.Potier, F.Pougheon, J.Proust, B.Roussiere, J.Sauvage, O.Sorlin Study of the N=50 Shell Closure Close to 78Ni RADIOACTIVITY 83Ga, 81Zn(β-) [from U(d, X)]; measured Eγ, Iγ, γγ-, βγ-coin, T1/2. 81Ga, 83As deduced levels.
doi: 10.1590/S0103-97332004000500075
2004ZE02 Nucl.Phys. A731, 121 (2004) R.G.T.Zegers, H.Abend, H.Akimune, A.M.van den Berg, H.Fujimura, H.Fujita, Y.Fujita, M.Fujiwara, S.Gales, K.Hara, M.N.Harakeh, T.Ishikawa, T.Kawabata, K.Kawase, T.Mibe, K.Nakanishi, S.Nakayama, H.Toyokawa, M.Uchida, T.Yamagata, K.Yamasaki, M.Yosoi Excitation and decay of the isovector spin-flip giant monopole resonance via the 208Pb(3He, tp) reaction at 410 MeV NUCLEAR REACTIONS 208Pb(3He, t), (3He, tp), E=410 MeV; measured particle spectra, σ(E, θ). 208Bi deduced giant monopole resonance energy, width, decay features.
doi: 10.1016/j.nuclphysa.2003.11.024
2003GA40 Nucl.Phys. A722, 148c (2003) Towards the next generation of Radioactive Ion Beam Facilities
doi: 10.1016/S0375-9474(03)01351-4
2003PE18 Yad.Fiz. 66, 1467 (2003); Phys.Atomic Nuclei 66, 1421 (2003) O.Perru, F.Ibrahim, O.Bajeat, C.Bourgeois, F.Clapier, E.Cottereau, C.Donzaud, M.Ducourtieux, S.Gales, D.Guillemaud-Mueller, C.Lau, H.Lefort, F.Le Blanc, A.C.Mueller, J.Obert, N.Pauwels, J.C.Potier, F.Pougheon, J.Proust, B.Roussiere, J.Sauvage, O.Sorlin, D.Verney Decay of Neutron-Rich Ga Isotopes near N = 50 at PARRNe RADIOACTIVITY 83,84Ga(β-), (β-n) [from 238U(n, F)]; measured Eγ, Iγ, γγ-, βγ-coin, T1/2. 82,83,84Ge deduced transitions. Mass-separated sources.
doi: 10.1134/1.1601744
2003ZE03 Phys.Rev.Lett. 90, 202501 (2003) R.G.T.Zegers, H.Abend, H.Akimune, A.M.van den Berg, H.Fujimura, H.Fujita, Y.Fujita, M.Fujiwara, S.Gales, K.Hara, M.N.Harakeh, T.Ishikawa, T.Kawabata, K.Kawase, T.Mibe, K.Nakanishi, S.Nakayama, H.Toyokawa, M.Uchida, T.Yamagata, K.Yamasaki, M.Yosoi Excitation and Decay of the Isovector Giant Monopole Resonances via the 208Pb(3He, tp)Reaction at 410 MeV NUCLEAR REACTIONS 208Pb(3He, t), E=410 MeV; measured σ(E, θ). 208Bi deduced isovector spin-flip giant monopole resonance energy, proton decay branching ratio. 207Pb deduced strong feeding of deep neutron-hole states.
doi: 10.1103/PhysRevLett.90.202501
2002IB01 Eur.Phys.J. A 15, 357 (2002) F.Ibrahim, J.Obert, O.Bajeat, J.M.Buhour, D.Carminati, F.Clapier, C.Donzaud, M.Ducourtieux, J.M.Dufour, S.Essabaa, S.Gales, D.Guillemaud-Mueller, F.Hosni, O.Hubert, A.Joinet, U.Koster, C.Lau, H.Lefort, G.Le Scornet, J.Lettry, A.C.Mueller, M.Mirea, N.Pauwels, O.Perru, J.C.Potier, J.Proust, F.Pougheon, H.Ravn, L.Rinolfi, G.Rossat, H.Safa, M.G.Saint Laurent, M.Santana-Leitner, O.Sorlin, D.Verney Photofission for the production of radioactive beams: Experimental data from an on-line measurement NUCLEAR REACTIONS 238U(γ, F)89Kr/90Kr/91Kr/92Kr/137Xe/138Xe/139Xe/140Xe, E=50 MeV bremsstrahlung; measured photofission yields. Application to radioactive beam facilities discussed.
doi: 10.1140/epja/i2001-10222-0
2001WI05 Nucl.Phys. A683, 48 (2001) J.S.Winfield, S.Fortier, W.N.Catford, S.Pita, N.A.Orr, J.Van de Wiele, Y.Blumenfeld, R.Chapman, S.P.G.Chappell, N.M.Clarke, N.Curtis, M.Freer, S.Gales, H.Langevin-Joliot, H.Laurent, I.Lhenry, J.M.Maison, P.Roussel-Chomaz, M.Shawcross, K.Spohr, T.Suomijarvi, A.de Vismes Single-Neutron Transfer from 11Begs via the (p, d) Reaction with a Radioactive Beam NUCLEAR REACTIONS 1H(11Be, 10Be), E=35.3 MeV/nucleon; 1H(15N, 14N), E=38.9 MeV/nucleon; measured σ(θ). 11Be levels deduced spectroscopic factors, configurations. Vibrational coupling model, radioactive beam.
doi: 10.1016/S0375-9474(00)00463-2
2000YO09 Phys.Rev. C62, 044604 (2000) G.H.Yoo, G.M.Crawley, J.H.Kelley, N.A.Orr, J.C.Stasko, J.S.Winfield, S.Gales, S.Fortier, H.Laurent, T.Suomijarvi, J.E.Finck Proton Decay following the Transfer Reaction (7Li, 6He) on 40Ca and 90Zr NUCLEAR REACTIONS 40Ca, 90Zr(7Li, 6He), E=50 MeV/nucleon; measured E(6He), proton spectra and angular distribution following residual nucleus decay, (helium)p-coin; deduced reaction mechanism features. Comparison with model predictions.
doi: 10.1103/PhysRevC.62.044604
1999FO09 Phys.Lett. 461B, 22 (1999) S.Fortier, S.Pita, J.S.Winfield, W.N.Catford, N.A.Orr, J.Van de Wiele, Y.Blumenfeld, R.Chapman, S.P.G.Chappell, N.M.Clarke, N.Curtis, M.Freer, S.Gales, K.L.Jones, H.Langevin-Joliot, H.Laurent, I.Lhenry, J.M.Maison, P.Roussel-Chomaz, M.Shawcross, M.Smith, K.Spohr, T.Suomijarvi, A.de Vismes Core Excitation in 11Begs via the p(11Be, 10Be)d Reaction NUCLEAR REACTIONS 1H(11Be, 10Be), E=35.3 MeV/nucleon; measured particle spectra, (particle)d-coin, σ(E, θ). 11Be deduced core excitation, vibrational coupling. DWBA analysis. Secondary beam from 15N fragmentation.
doi: 10.1016/S0370-2693(99)00825-4
1999GA38 Nucl.Phys. A654, 19c (1999) Nuclear Physics Today
doi: 10.1016/S0375-9474(99)00245-6
1999WI04 J.Phys.(London) G25, 755 (1999) J.S.Winfield, S.Fortier, W.N.Catford, S.Pita, N.A.Orr, Y.Blumenfeld, R.Chapman, S.P.G.Chappell, N.M.Clarke, N.Curtis, M.Freer, S.Gales, K.L.Jones, H.Langevin-Joliot, H.Laurent, I.Lhenry, J.-M.Maison, P.Roussel-Chomaz, M.Shawcross, M.Smith, K.Spohr, T.Suomijarvi, A.de Vismes Structure of 11Be from the (d, p) Reaction in Inverse Kinematics NUCLEAR REACTIONS 1H(11Be, 10Be), E=35 MeV/nucleon; measured d, Be spectra, yield vs excitation energy. 11Be deduced halo features.
doi: 10.1088/0954-3899/25/4/029
1996BE16 Nucl.Phys. A599, 265c (1996) D.Beaumel, S.Fortier, S.Gales, J.Guillot, H.Langevin-Joliot, H.Laurent, J.M.Maison, J.Vernotte, J.Bordewijk, S.Brandenburg, A.Krasznahorkay, G.M.Crawley, C.P.Massolo, M.Renteria, A.Khendriche Decay Properties of High-Lying Single-Particles Modes NUCLEAR REACTIONS 64Ni, 90Zr, 120Sn, 208Pb(α, n3He), E=120 MeV; measured neutron spectra, nn(θ). 91Zr, 209Pb deduced resonances, J, π, neutron decay features.
doi: 10.1016/0375-9474(96)00068-1
1996LH02 Phys.Rev. C54, 593 (1996) I.Lhenry, T.Suomijarvi, Y.Blumenfeld, Ph.Chomaz, N.Frascaria, J.P.Garron, J.C.Roynette, J.A.Scarpaci, D.Beaumel, S.Fortier, S.Gales, H.Laurent, A.Gillibert, G.M.Crawley, J.Finck, G.Yoo, J.Barreto One-Nucleon Transfer Reactions to Continuum States Induced by Heavy Ion Projectiles NUCLEAR REACTIONS 207Pb, 209Bi, 59Co(20Ne, 19Ne), (20Ne, 21Na), (20Ne, 19F), E=48 MeV/nucleon; 207Pb, 209Bi, 63Cu(36Ar, 35Ar), (36Ar, 37K), E=42 MeV/nucleon; measured σ(E, θ); deduced structure, particle-hole states, collective strength. RPA, DWBA calculations, Bonaccorso-Brink single-particle transfer model.
doi: 10.1103/PhysRevC.54.593
1996WI05 Phys.Rev. C54, 125 (1996) J.S.Winfield, D.Beaumel, S.Gales, H.Laurent, I.Lhenry, J.M.Maison, G.M.Crawley, S.Danczyk, S.E.Hirzebruch, J.C.Stasko, T.Suomijarvi The (7Li, 7Beγ) Reaction and Isovector Spin Strength in 40Ca NUCLEAR REACTIONS 12C, 40Ca(7Li, 7Be), E=70 MeV/nucleon; measured (particle)γ-coin. 40Ca deduced continuum isovector spin strength. Spectrometer, CsI detectors.
doi: 10.1103/PhysRevC.54.125
1995FO19 Phys.Rev. C52, 2401 (1995) S.Fortier, D.Beaumel, S.Gales, J.Guillot, H.Langevin-Joliot, H.Laurent, J.M.Maison, J.Bordewijk, S.Brandenburg, A.Krasznahorkay, G.M.Crawley, C.P.Massolo, M.Renteria, A.Khendriche Damping of Unbound Single-Particle Modes NUCLEAR REACTIONS 64Ni, 90Zr, 120Sn(α, 3He), E=120 MeV; measured 3He-spectra, neutron spectra following residual decay, n(3He)-coin. 91Zr, 121Sn, 65Ni deduced non-statistical neutron branching ratios. Statistical analysis.
doi: 10.1103/PhysRevC.52.2401
1995HO10 Nucl.Phys. A588, 729 (1995) M.A.Hofstee, S.Y.van der Werf, A.M.van den Berg, N.Blasi, J.A.Bordewijk, W.T.A.Borghols, R.De Leo, G.T.Emery, S.Fortier, S.Gales, M.N.Harakeh, P.den Heijer, C.W.de Jager, H.Langevin-Joliot, S.Micheletti, M.Morlet, M.Pignanelli, J.M.Schippers, H.de Vries, A.Willis, A.van der Woude Localized 1(h-bar x Omega) Particle-Hole Strength in Nuclei NUCLEAR REACTIONS 90Zr, 116Sn, 196Pt, 208Pb(p, p'), E=201 MeV; 116Sn(polarized p, p'), E=133.8 MeV; 90Zr, 116Sn, 196Pt(α, α'), E=120 MeV; measured σ(θ). 116Sn, 196Pt(e, e'), E=278, 333 MeV; measured form factors. 90Zr, 116Sn, 196Pt, 208Pb deduced 0, 1(h-bar x omega) strength distribution. DWBA calculation, effective NN-force.
doi: 10.1016/0375-9474(95)00057-8
1995LA22 Phys.Rev. C52, 3066 (1995) H.Laurent, J.A.Scarpaci, D.Beaumel, Y.Blumenfeld, S.Fortier, N.Frascaria, S.Gales, J.P.Garron, J.Guillot, I.Lhenry, J.C.Roynette, J.M.Maison, T.Suomijarvi, A.Gillibert, P.Roussel-Chomaz, A.Van der Woude Role of the Breakup Process in the 48Ca(20Ne, 19Ne n) Reaction at 48A MeV NUCLEAR REACTIONS 48Ca(20Ne, n19Ne), E=48 MeV/nucleon; measured E(19Ne), En, σ(En, θ); deduced neutron multiplicity, reaction mechanism. Breakup process model.
doi: 10.1103/PhysRevC.52.3066
1995LH02 Nucl.Phys. A583, 115c (1995) I.Lhenry, D.Beaumel, S.Fortier, S.Gales, H.Laurent, J.M.Maison, F.Azaiez, Y.Blumenfeld, J.Guillot, H.Langevin-Joliot, T.Suomijarvi, S.Brandenburg, G.M.Crawley, J.Finck, J.Stasko A Search for the Isovector Monopole Resonance in 208Pb NUCLEAR REACTIONS 208Pb(13C, 13N), E=60 MeV/nucleon; measured σ(θ), missing energy spectra. 208Tl deduced level, neutron decay features.
doi: 10.1016/0375-9474(94)00643-2
1994BE07 Phys.Rev. C49, 2444 (1994) D.Beaumel, S.Fortier, S.Gales, J.Guillot, H.Langevin-Joliot, H.Laurent, J.M.Maison, J.Vernotte, J.A.Bordewijk, S.Brandenburg, A.Krasznahorkay, G.M.Crawley, C.P.Massolo, M.Renteria Decay Modes of High-Lying Single-Particle States in 209Pb NUCLEAR REACTIONS 208Pb(α, n3He), E=122 MeV; measured E(3He), (3He)n-, γ(3He)-coin, neutron angular correlations. 209Pb deduced direct decay branching ratios, Γ(spreading)/Γ, Γn/Γ for structures at high excitation. Statistical model calculations.
doi: 10.1103/PhysRevC.49.2444
1994GA10 Nucl.Phys. A569, 393c (1994) Statistical and Direct Decay of High-Lying Single-Particle Excitations NUCLEAR REACTIONS 208Pb(α, 3He), E=183 MeV; 90Zr(7Li, 6He), E=30 MeV/nucleon; compiled, reviewed data, analyses. 209Pb, 91Nb deduced resonance decay features.
doi: 10.1016/0375-9474(94)90130-9
1994LA10 Nucl.Phys. A569, 297c (1994) H.Laurent, S.Gales, D.Beaumel, G.M.Crawley, J.E.Finck, S.Fortier, J.M.Maison, C.P.Massolo, D.J.Mercer, J.S.Winfield, G.H.Yoo Spin-Isospin Multipole Excitations by Means of the (6Li, 6He) Reaction at 100 A.MeV NUCLEAR REACTIONS 12,13C, 58Ni, 90Zr, 208Pb(6Li, 6He), E=100 MeV/nucleon; measured σ(θ, E(6He)). 13,12N, 58Cu, 90Nb, 208Bi deduced spin-isospin multipole excitation features.
doi: 10.1016/0375-9474(94)90120-1
1993LA31 Nucl.Instrum.Methods Phys.Res. A326, 517 (1993) H.Laurent, H.Lefort, D.Beaumel, Y.Blumenfeld, S.Fortier, S.Gales, J.Guillot, J.C.Roynette, P.Volkov, S.Brandenburg EDEN: A neutron time-of-flight multidetector for decay studies of giant states NUCLEAR REACTIONS 48Ca(20Ne, X), E=48 MeV/nucleon; measured n+γ spectra. 16O, 12C(α, n3He), E=120 MeV; measured neutron spectra. 16O(α, n3He), E=120 MeV; measured n(3He)(θ). 17O level deduced Γn/Γ. Neutron tof multi-detector.
doi: 10.1016/0168-9002(93)90854-B
1993RO20 Phys.Rev. C48, R2148 (1993) G.Rotbard, G.Berrier-Ronsin, O.Constantinescu, S.Fortier, S.Gales, M.Hussonnois, J.B.Kim, J.M.Maison, L.-H.Rosier, J.Vernotte, Ch.Briancon, R.Kulessa, Yu.Ts.Oganessian, S.A.Karamian Blocking Effect in the 16+ → 16+ (p, t) Transition on the Isomeric 178m2Hf Target NUCLEAR REACTIONS 178Hf(p, t), E=19 MeV; measured σ(θ); deduced aligned quasineutron orbitals blocking effect. 178Hf deduced isomer to isomer, 0+ → 0+ transition σ ratio. Target in isomeric state.
doi: 10.1103/PhysRevC.48.R2148
1993YO01 Phys.Rev. C47, 1200 (1993) G.H.Yoo, G.M.Crawley, N.A.Orr, J.S.Winfield, J.E.Finck, S.Gales, Ph.Chomaz, I.Lhenry, T.Suomijarvi High-Lying Resonances Observed in Heavy-Ion Transfer Reactions NUCLEAR REACTIONS 207,208Pb, 209Bi, 89Y, 90,91Zr(7Li, 6Li), (7Li, 6He), (12C, 13C), (12C, 13N), E=30 MeV/nucleon; measured σ(θ, E); deduced structure.
doi: 10.1103/PhysRevC.47.1200
1991DU01 Phys.Rev. C43, 1116 (1991) G.Duhamel-Chretien, G.Perrin, C.Perrin, V.Comparat, E.Gerlic, S.Gales, C.P.Massolo Neutron Hole States in 89Zr via the (p(pol), d) Reaction at 58 MeV NUCLEAR REACTIONS 90Zr(polarized p, d), E=58 MeV; measured σ(θ), vector analyzing power. 89Zr deduced levels, J, π, spectroscopic factors. DWBA analysis.
doi: 10.1103/PhysRevC.43.1116
1991MA06 Phys.Rev. C43, 1687 (1991) C.P.Massolo, S.Fortier, S.Gales, F.Azaiez, E.Gerlic, J.Guillot, E.Hourani, H.Langevin-Joliot, J.M.Maison, J.P.Schapira, G.M.Crawley Onset of Neutron Single-Particle Strengths in the Tin Isotopic Chain NUCLEAR REACTIONS 124,122,120,118,116,112Sn(α, 3He), E=183 MeV; measured σ(θ) vs excitation energy; deduced model parameters. 113,117,119,121,123,125Sn levels deduced L, C2S, neutron particle response function. Enriched targets. DWBA analysis.
doi: 10.1103/PhysRevC.43.1687
1990FO04 Phys.Rev. C41, 2689 (1990) S.Fortier, S.Gales, S.M.Austin, W.Benenson, G.M.Crawley, C.Djalali, J.S.Winfield, G.Yoo One-Nucleon-Transfer Reactions Induced by 20Ne at 500 and 600 MeV NUCLEAR REACTIONS 90Zr, 208Pb(20Ne, 19Ne), (20Ne, 21Ne), (20Ne, 21Na), E=500, 600 MeV; measured σ(fragment E, θ) vs excitation. 91Zr, 209Pb deduced structure characteristics. DWBA analysis. Enriched targets.
doi: 10.1103/PhysRevC.41.2689
1989FO01 Phys.Rev. C39, 82 (1989) S.Fortier, S.Gales, E.Hourani, J.M.Maison, C.P.Massolo, J.P.Schapira Neutron-Hole Strengths and Core Coupling in 87Sr via the 88Sr(3He, α)87Sr Reaction NUCLEAR REACTIONS 88Sr(3He, α), E=36 MeV; measured σ(E(α)), σ(θ). 87Sr deduced levels, spectroscopic factors, L. DWBA, CRC analyses. Enriched target.
doi: 10.1103/PhysRevC.39.82
1989GE03 Phys.Rev. C39, 2190 (1989) E.Gerlic, J.Guillot, H.Langevin-Joliot, J.Van de Wiele, S.Gales, G.Duhamel, G.Perrin, C.P.Massolo, M.Sakai Stretched High-Spin Two-Neutron-Hole States in 206Pb and 114Sn via the (p, t) Reaction at 168 MeV NUCLEAR REACTIONS 116Sn, 208Pb(p, t), E=168 MeV; measured σ(θ), σ(Et). 114Sn, 206Pb deduced levels, J, π, configuration, two-neutron hole strengths. DWBA analysis.
doi: 10.1103/PhysRevC.39.2190
1989HO19 Z.Phys. A334, 277 (1989) E.Hourani, F.Azaiez, Ph.Dessagne, A.Elayi, S.Fortier, S.Gales, J.M.Maison, P.Massolo, Ch.Miehe, A.Richard Search for Proton Radioactivity in 65As, 69Br and 97Y RADIOACTIVITY 65As [from 40Ca(28Si, 2np)]; 69Br [from 40Ca(32S, 2np)]; 97Y [from 40Ca(40Ca, 2np)]; measured particle spectra, (particle)(particle)-coin spectra; deduced no proton activity evidence.
1988DA01 Phys.Rev. C37, 250 (1988) V.M.Datar, S.Fortier, S.Gales, E.Hourani, H.Langevin, J.M.Maison, C.P.Massolo Search for Short Lived Neutral Particle in the 15.1 MeV Isovector Transition of 12C NUCLEAR REACTIONS 12C(p, p'), E=19 MeV; measured e+e--coin; deduced no neutral φ-particle evidence, Γ(φ)/Γγ upper limits.
doi: 10.1103/PhysRevC.37.250
1988GA32 Phys.Rep. 166, 125 (1988) S.Gales, Ch.Stoyanov, A.I.Vdovin Damping of High-Lying Single-Particle Modes in Heavy Nuclei
doi: 10.1016/0370-1573(88)90066-X
1988HO03 Nucl.Instrum.Methods Phys.Res. A264, 357 (1988) E.Hourani, J.Kumpulainen, F.Azaiez, S.Fortier, S.Gales, J.M.Maison, P.Massolo, B.Ramstein, J.P.Schapira Mass Identification in Heavy Ion Collection with the Spectrometer SOLENO NUCLEAR REACTIONS 24Mg(16O, X), E=87.5 MeV; 12C(32S, X), E=121 MeV; 24Mg(32S, X), E=121 MeV; measured σ(fragment E), mass distribution. Mass spectrometer. RADIOACTIVITY 252Cf(SF); measured fission fragment distribution. Mass spectrometer.
doi: 10.1016/0168-9002(88)90924-2
1988LA18 Phys.Rev. C38, 1168 (1988) H.Langevin-Joliot, V.Datar, E.Gerlic, J.Van de Wiele, F.Azaiez, S.Fortier, S.Gales, J.Guillot, J.M.Maison, C.P.Massolo, G.Duhamel, G.Perrin Highest Spin n-p States in Heavy Nuclei via the (α, d) Reaction at 218 MeV NUCLEAR REACTIONS 90Zr, 120Sn, 144Sm, 208Pb(α, d), E=218 MeV; measured σ(θ). 92Nb, 122Sb, 146Eu, 210Bi deduced levels, J, π. DWBA analysis.
doi: 10.1103/PhysRevC.38.1168
1987FO16 Phys.Rev. C36, 1830 (1987) S.Fortier, S.Gales, S.M.Austin, W.Benenson, G.M.Crawley, C.Djalali, J.H.Lee, J.van der Plicht, J.S.Winfield Search for High Excitation Energy Structures in 90Zr and 208Pb, via 20Ne Inelastic Scattering NUCLEAR REACTIONS 90Zr, 208Pb(20Ne, 20Ne'), E=500, 600 MeV; measured σ(E(20Ne')); deduced structure, excitation mechanism.
doi: 10.1103/PhysRevC.36.1830
1986AN29 Phys.Rev.Lett. 57, 2375 (1986) N.Anantaraman, J.S.Winfield, S.M.Austin, A.Galonsky, J.van der Plicht, C.C.Chang, G.Ciangaru, S.Gales (6Li, 6He) Reaction as a Probe of Spin-Transfer Strength NUCLEAR REACTIONS 7Li, 12,14C, 26Mg, 90Zr(6Li, 6He), E=210 MeV; measured σ(E(6He)), σ(θ). 7Be, 12,14N, 26Al, 90Nb levels deduced σ, Gamow-Teller transition strength correlation. Spectrograph, focal plane detector. DWBA calculations.
doi: 10.1103/PhysRevLett.57.2375
1986MA49 Phys.Rev. C34, 1256 (1986) C.P.Massolo, F.Azaiez, S.Gales, S.Fortier, E.Gerlic, J.Guillot, E.Hourani, J.M.Maison Damping of High-Spin Single-Particle Strengths in 209Pb NUCLEAR REACTIONS 208Pb(α, 3He), E=183 MeV; measured σ(θ), σ(E(3He)); deduced model parameters. 209Pb deduced levels, J, π, L, strength functions. Enriched target, magnetic spectrometer. DWBA analysis.
doi: 10.1103/PhysRevC.34.1256
1985AZ03 Nucl.Phys. A444, 373 (1985) F.Azaiez, S.Fortier, S.Gales, E.Hourani, J.M.Maison, J.Kumpulainen, J.P.Schapira The γ-Decay of the 1g9/2 and 2p Inner-Hole States in 111Sn via the 112Sn(3He, αγ) Reaction at 32 MeV NUCLEAR REACTIONS 112Sn(3He, αγ), E=32 MeV; measured σ(Eα, Eγ). 111Sn levels deduced possible J, π, γ-decay of inner hole states, 1g9/2, 2p strength functions. Magnetic spectrometer, Ge(Li) detector, enriched target.
doi: 10.1016/0375-9474(85)90458-0
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
1985HO21 Phys.Lett. 160B, 375 (1985) E.Hourani, M.Hussonnois, L.Stab, L.Brillard, S.Gales, J.P.Schapira Evidence for the Radioactive Decay of 226Ra by 14C Emission RADIOACTIVITY 226Ra(14C), (α); measured (14C) to α-branching ratio. 222Ra(14C); measured 14C spectrum. 241Am(34Si); measured 34Si emission upper limit. Magnetic spectrometer.
doi: 10.1016/0370-2693(85)90004-8
1984FO10 Phys.Rev. C30, 79 (1984) J.L.Foster, Jr., S.E.Darden, M.C.Rozak, J.A.Ross, J.P.Martin, L.Lessard, S.Gales, G.Noury, J.M.Pearson, P.Depommier, M.C.Hermida, M.Ruiz 130Te(p(pol), p1) and 130Te(p, p1(pol)) Reactions on Analog Resonances NUCLEAR REACTIONS 130Te(polarized p, p), (polarized p, p'), E(cm)=10.1-10.7 MeV; measured σ(θ) vs E, analyzing power vs θ, E, polarization vs θ; deduced optical model parameters. 131I deduced IAR, J, π, configuaration. Coupled-channels analysis.
doi: 10.1103/PhysRevC.30.79
1984GA16 J.Phys.(Paris), Colloq.C4, 39 (1984); See 1984Ga37 Investigation of Inner and Outer Subshells via Transfer Reactions
1984GA24 Phys.Lett. 144B, 323 (1984) S.Gales, C.P.Massolo, F.Azaiez, S.Fortier, E.Gerlic, J.Guillot, E.Hourani, J.M.Maison, J.P.Schapira, G.M.Crawley High-Lying Neutron Particle States Observed via the (α, 3He) Reaction at 183 MeV NUCLEAR REACTIONS 116,118,120Sn(α, 3He), E=183 MeV; measured σ(θ, E(3He)), σ(θ). 117,119Sn deduced high lying neutron states. 121Sn deduced high lying neutron states, possible J, π, C2S. DWBA analysis.
doi: 10.1016/0370-2693(84)91270-X
1984GA37 J.Phys.(Paris), Colloq.C-4, 39 (1984) Investigation of Inner and Outer Subshells via Transfer Reactions NUCLEAR REACTIONS 118Sn(3He, α), E=81.7 MeV; 116Sn(3He, α), E=283 MeV; 117,119Sn(p, d), 118,120Sn(p, t), E=42 MeV; 90Zr, 120Sn, 208Pb(α, 3He), E=183 MeV; 90Zr, 120Sn, 144Sm, 208Pb(3He, d), E=240 MeV; analyzed residual energy spectra. 90Zr(polarized p, d), E=90 MeV; analyzed residual energy spectra, analyzing power. 116Sn(p, t), E=130 MeV; analyzed σ(Et, θt). 116Sn, 208Pb(α, 6He), E=218, 220 MeV; measured σ(θ), σ(E(6He), θ(6He)). 208Pb, 144Sm, 116Sn(α, t), E=80 MeV; measured σ(θt, Et). 117Sb, 145Eu, 209Bi deduced level Γ, spectroscopic factors. 208Pb, 120Sn, 90Zr(α, 3He), E=183 MeV; measured σ(E(3He), θ(3He)).
1984GA38 Phys.Rev.Lett. 53, 759 (1984) S.Gales, E.Hourani, M.Hussonnois, J.P.Schapira, L.Stab, M.Vergnes Exotic Nuclear Decay of 223Ra by Emission of 14C Nuclei RADIOACTIVITY 223Ra(α), (14C); measured relative branching ratio.
doi: 10.1103/PhysRevLett.53.759
1983GA07 Nucl.Phys. A398, 19 (1983) S.Gales, G.M.Crawley, D.Weber, B.Zwieglinski Neutron-Hole Strength Distributions in Heavy Nuclei (II). The 144,148,152Sm(3He, α)143,147,151Sm and the 144,148,150,152,154Sm(p, d)143,147,149,151,153Sm Reactions NUCLEAR REACTIONS 144,148,152Sm(3He, α), E=70 MeV; measured σ(Eα, θ); 144,148,150,152,154Sm(p, d), E=42 MeV; measured σ(Ed, θ). 143,147,149,151,153Sm deduced levels, L, J, π, C2S. Enriched target, magnetic spectrometer. Zero-range, finite-range DWBA calculations, inner-shells analysis. Comparison with the quasiparticle phonon, Nilsson models.
doi: 10.1016/0375-9474(83)90646-2
1983KA18 Phys.Rev. C28, 1065 (1983) J.Kasagi, G.M.Crawley, E.Kashy, J.Duffy, S.Gales, E.Gerlic, D.Friesel Highly Excited Hole Strength Observed in the 90Zr(p(pol), d)89Zr Reaction NUCLEAR REACTIONS 90Zr(polarized p, d), E=90 MeV; measured σ(Ed), σ(θ), analyzing power vs θ. 89Zr deduced levels, J, π, C2S. Finite-range DWBA.
doi: 10.1103/PhysRevC.28.1065
1982CR01 Phys.Lett. 109B, 8 (1982) G.M.Crawley, W.Benenson, G.Bertsch, S.Gales, D.Weber, B.Zwieglinski Pairing Model Predictions for (p, t) Experiments on the Cadmium Isotopes NUCLEAR REACTIONS 110,112,114,116Cd(p, t), E=42 MeV; measured σ(Et). 106Cd(p, t), E=42 MeV; measured σ(Et), Q. 110,112,114,116,106Cd deduced two-particle pickup from deep orbits. 104Cd deduced mass excess. Split-pole spectrograph, position sensitive proportional counter. Pairing model.
doi: 10.1016/0370-2693(82)90450-6
1982GA17 Nucl.Phys. A381, 40 (1982) S.Gales, E.Gerlic, G.Duhamel, G.Perrin, C.Perrin, V.Comparat Spin of Deep-Hole States in 111Sn via the 112Sn(d(pol), t) Reaction NUCLEAR REACTIONS 112Sn(polarized d, t), E=40 MeV; measured σ(Et), σ(θ), A(θ); deduced valence, inner-hole components. 111Sn deduced levels, L, J, π, C2S. Enriched target, polarized beam, magnetic spectrometer. DWBA analysis.
doi: 10.1016/0375-9474(82)90499-7
1982GA18 Nucl.Phys. A381, 173 (1982) S.Gales, G.M.Crawley, D.Weber, B.Zwieglinski Neutron-Hole Strength Distributions in Heavy Nuclei (I): The reactions 124,130Te(3He, α)123,129Te and 122,124,130Te(p, d)121,123,129Te NUCLEAR REACTIONS 124,130Te(3He, α), E=70 MeV; measured σ(Eα, θ). 122,124,130Te(p, d), E=42 MeV; measured σ(θ). 121,123,129Te deduced levels, L, J, π, C2S. Enriched targets, magnetic spectrometer. DWBA, inner-shell analysis.
doi: 10.1016/0375-9474(82)90139-7
1982GE06 Phys.Lett. 117B, 20 (1982) E.Gerlic, J.Guillot, H.Langevin-Joliot, S.Gales, M.Sakai, J.Van de Wiele, G.Duhamel, G.Perrin High Lying Two-Neutron Hole States in 206Pb and 114Sn Observed via the (α, 6He) Reaction at 218 MeV NUCLEAR REACTIONS 208Pb, 116Sn(α, 6He), E=218 MeV; measured σ(E(6He)), σ(θ); deduced reaction mechanism. 114Sn, 206Pb deduced levels, J, π, L, configuration. Zero-range DWBA analysis.
doi: 10.1016/0370-2693(82)90865-6
1982HO17 Nucl.Phys. A391, 432 (1982) E.Hourani, S.Fortier, J.M.Maison, S.Gales, J.P.Schapira Direct Transfer and Two-Step Processes in the 42Ca(α, 3He)43Ca Reaction NUCLEAR REACTIONS 42Ca(α, 3He), E=36 MeV; measured σ(E, θ). 43Ca deduced levels, L, S. DWBA, coupled-channel analyses. Enriched target.
doi: 10.1016/0375-9474(82)90618-2
1982ZW02 Nucl.Phys. A389, 301 (1982) B.Zwieglinski, W.Benenson, G.M.Crawley, S.Gales, D.Weber Study of 11B at High Excitations with the 9Be(3He, p)11B and 9Be(α, d)11B Reactions NUCLEAR REACTIONS 9Be(3He, p), E=38 MeV; 9Be(α, d), E=48 MeV; measured σ(E(p), θ), σ(E(d)). 11B deduced levels, widths, isospin purity, L, normalization factors. DWBA analysis, shell-model form factors. Natural targets.
doi: 10.1016/0375-9474(82)90521-8
1981CR01 Phys.Rev. C23, 589 (1981) G.M.Crawley, W.Benenson, G.Bertsch, S.Gales, D.Weber, B.Zwieglinski Hole States in the Tin Isotopes Observed by the (p, t) Reaction NUCLEAR REACTIONS 112,116,118,120,122,124Sn(p, t), E=42 MeV; measured σ(Et, θ); 117,119Sn(p, d), E=42 MeV; measured σ(Ed). 110,114,116,118,120,122Sn deduced broad resonances, Γ. DWBA analysis. Enriched targets.
doi: 10.1103/PhysRevC.23.589
1981CR02 Phys.Rev. C23, 1818 (1981) G.M.Crawley, J.Kasagi, S.Gales, E.Gerlic, D.Friesel, A.Bacher Spin of Deep Hole States from (p(pol), d) Reactions NUCLEAR REACTIONS 90Zr, 120Sn(polarized p, d), E=90 MeV; measured σ(θ), analyzing power vs θ; deduced optical model parameters. 89Zr, 119Sn levels deduced J, π, C2S.
doi: 10.1103/PhysRevC.23.1818
1981FO09 Nucl.Phys. A370, 189 (1981) S.Fortier, J.M.Maison, P.Picot, S.Gales, E.Hourani, J.P.Schapira Two-Step Processes in the 40Ca(α, 3He)41Ca Reaction NUCLEAR REACTIONS 40Ca(α, 3He), E=36 MeV; measured σ(E(3He), θ). 41Ca deduced levels, L, S. DWBA, coupled-channels analyses. Enriched target.
doi: 10.1016/0375-9474(81)90072-5
1981PE02 Nucl.Phys. A356, 61 (1981) G.Perrin, G.Duhamel, C.Perrin, E.Gerlic, S.Gales, V.Comparat Analyzing Powers of Valence and Inner Neutron-Hole States in 115Sn via the 116Sn(d(pol), t) Reaction NUCLEAR REACTIONS 116Sn(polarized d, t), E=40 MeV; measured σ(Et, θ), A(θ). 115Sn deduced valence and inner hole components. 115Sn levels deduced L, J, π, C2S. Enriched target, magnetic spectrometer. DWBA analysis.
doi: 10.1016/0375-9474(81)90118-4
1981ST08 Phys.Rev. C23, 2447 (1981) G.L.Struble, L.G.Mann, R.G.Lanier, W.M.Buckley, J.Kern, G.Crawley, S.Gales, D.Mueller, F.Girshick Influence of Complex States and Deformation on Neutron Pairing Vibrations in the Even Sm Istopes NUCLEAR REACTIONS 144,148,150,152,154Sm(p, t), E=42 MeV; measured σ(Et, θt); deduced level systematics in Sm isotopes. 142Sm deduced levels, J. Enriched targets, Q3D, Enge split-pole spectrographs. DWBA.
doi: 10.1103/PhysRevC.23.2447
1980CR02 Phys.Rev. C22, 316 (1980) G.M.Crawley, S.Gales, D.Weber, B.Zwieglinski, W.Benenson, D.Friesel, A.Bacher, B.M.Spicer Deep Hole States Observed in (p, t) Reactions NUCLEAR REACTIONS 120,122,124Sn(p, t), E=89 MeV; measured σ(Et, θ). 118,120,122Sn deduced levels, Γ. DWBA, enriched targets.
doi: 10.1103/PhysRevC.22.316
1980GA01 Phys.Rev. C21, 98 (1980) S.Gales, Y.El Hage, J.P.Schapira, S.Fortier, H.Laurent, J.M.Maison High-Spin Analog Resonances Near the N = 50 Neutron Shell NUCLEAR REACTIONS 92Mo(3He, d), E=28.5 MeV; 96Zr(3He, d), E=39 MeV; measured σ(Ed, θ). 92Mo(3He, pd), E=30 MeV; 96Zr(3He, pd), E=37.5 MeV; measured σ(Ed, Ep, θp). 93Tc, 97Nb deduced IAS, L, J, π, S, Γp, Γp'. DWBA, Gamow function form factors. Magnetic analysis, enriched targets.
doi: 10.1103/PhysRevC.21.98
1980GE01 Phys.Rev. C21, 124 (1980) E.Gerlic, G.Berrier-Ronsin, G.Duhamel, S.Gales, E.Hourani, H.Langevin-Joliot, M.Vergnes, J.Van de Wiele Neutron-Hole Distributions in 111,115,119Sn as Observed in the (3He, α) Reaction NUCLEAR REACTIONS 112,116,120Sn(3He, α), E=39 MeV; measured σ(Eα, θ). 111,115,119Sn deduced levels, L, J, π, C2S. Two-step, zero-range DWBA, unified model calculations.
doi: 10.1103/PhysRevC.21.124
1980PA07 Phys.Lett. 91B, 41 (1980) R.C.Pardo, S.Gales, R.M.Ronningen, L.H.Harwood Mass of 146Gd and 147Gd and Shell Closure at Z = 64 NUCLEAR REACTIONS 144Sm(12C, 9Be), (12C, 10Be), E=75 MeV; measured σ(E(9Be), θ), σ(E(10Be), θ); deduced proton gap at Z=64. 146,147Gd deduced mass, levels.
doi: 10.1016/0370-2693(80)90658-9
1980ST13 Phys.Lett. 93B, 26 (1980) G.L.Struble, L.G.Mann, R.G.Lanier, W.M.Buckley, J.Kern, G.Crawley, S.Gales, D.Mueller, F.Girshick The Behavior of High-Energy Neutron Pairing Strength in the Samarium Isotopes NUCLEAR REACTIONS 144,148,150,152,154Sm(p, t), E=42 MeV; measured σ(θ, Et). 142Sm deduced structure. 146,148Sm deduced two-neutron transfer strength localization. Shell model. Q3D spectrograph, Enge split-pole spectrometer.
doi: 10.1016/0370-2693(80)90087-8
1979FO09 Nucl.Phys. A321, 137 (1979) Study of the 58Ni(t, α)57Ni Reaction at 25 MeV NUCLEAR REACTIONS 58Ni(3He, α), E=25 MeV; measured σ(θ). 57Ni deduced levels, L, J, π, S, analog states. DWBA, crc analysis. Enriched target.
doi: 10.1016/0375-9474(79)90688-2
1978FO23 Phys.Lett. 78B, 52 (1978) Investigation of High-Spin States in 47Ca Through Double-Step Processes in the 48Ca(τ, α)47Ca Reaction NUCLEAR REACTIONS 48Ca(3He, α), E=25 MeV; measured σ(Eα, θ). 47Ca deduced levels, J, π, L. CCBA analysis.
doi: 10.1016/0370-2693(78)90345-3
1978FO34 Nucl.Phys. A311, 324 (1978) S.Fortier, E.Hourani, M.N.Rao, S.Gales Spectroscopic Study of the N = 27 Nuclei by Means of the (τ, α) Reaction NUCLEAR REACTIONS 48Ca, 48,50Ti, Cr, 54Fe(3He, α), E=25 MeV; measured σ(Eα, θ). 47Ca, 47,49Ti, 49,51,52,53Cr, 53Fe deduced levels, L, J, π, S, analog states. DWBA, coupled-channel analyses. Enriched targets.
doi: 10.1016/0375-9474(78)90518-3
1978GA06 Phys.Rev. C17, 1308 (1978) S.Gales, Y.El Hage, S.Fortier, H.Laurent, J.M.Maison, J.P.Schapira Proton Decay of T > Hole States in Heavy Nuclei by Means of the (3He, αp) Reaction on 96Zr and 144Sm NUCLEAR REACTIONS 96Zr, 144Sm(3He, pα), E=39 MeV; measured σ(Ep, Eα, θ(p)). 95Zr, 143Sm deduced IAS, proton branching. 94Y deduced levels, J, π, Γp, S. Enriched targets.
doi: 10.1103/PhysRevC.17.1308
1978GA09 Phys.Rev.Lett. 41, 292 (1978) S.Gales, G.M.Crawley, D.Weber, B.Zwieglinski Observation of the T > = 45/2 Components of Deep Hole States in 207Pb via the (3He, α) Reaction at 70 MeV NUCLEAR REACTIONS 208Pb(3He, α), E=70 MeV; measured σ(Eα, θ). 207Pb deduced levels, S.
doi: 10.1103/PhysRevLett.41.292
1978GA23 Phys.Rev. C18, 2475 (1978) S.Gales, G.M.Crawley, D.Weber, B.Zwieglinski Inner Hole States in 207Pb via the 208Pb(3He, α)207Pb Reaction at 70 MeV NUCLEAR REACTIONS 208Pb(3He, α), E=70 MeV; measured σ(E, θ). 207Pb deduced levels, L, J, π, C2S, inner shell S. Enriched target, magnetic spectrometer.
doi: 10.1103/PhysRevC.18.2475
1978HE15 Nucl.Phys. A303, 313 (1978) K.Heyde, M.Waroquier, P.Van Isacker, H.Vincx, S.Gales, V.Paar Study of Isobaric Analogue Resonances in f-p Shell Nuclei: A Unified-Model Description NUCLEAR REACTIONS 48Ca, 50Ti, 52Cr, 54Fe, 58Ni(3He, dp); analyzed data. 49Ca, 51Ti, 53Cr, 55Fe, 59Ni deduced levels, S.
doi: 10.1016/0375-9474(78)90361-5
1978SC07 Phys.Rev. C17, 1588 (1978) J.P.Schapira, J.M.Maison, M.N.Rao, S.Fortier, S.Gales, H.Laurent γ Decay and Splitting of the First Analog State in 53Mn, 55Co, and 59Cu NUCLEAR REACTIONS 52Cr, 54Fe, 58Ni(3He, dγ), E=18 MeV; measured σ(Ed, Eγ). 53Mn, 55Co, 59Cu deduced levels, γ-branching, δ. Natural, enriched targets, Ge(Li) detectors.
doi: 10.1103/PhysRevC.17.1588
1977FO06 Nucl.Phys. A288, 82 (1977) S.Fortier, J.M.Maison, S.Gales, H.Laurent, J.P.Schapira Spectroscopic Study of 55Co via the 54Fe(τ, d)55Co and 54Fe(τ, dp)54Fe Reactions NUCLEAR REACTIONS 54Fe(3He, d), E=25 MeV; measured σ(Ed, θ). 54Fe(3He, dp), E=24 MeV; measured σ(Ed), dp(θ, t). 55Co deduced levels, J, π, L, S, IAS, population parameters, Γp, Γp'. 55Fe, 55Co deduced Coulomb energy difference. Enriched target.
doi: 10.1016/0375-9474(77)90082-3
1977GA17 Nucl.Phys. A288, 201 (1977) S.Gales, E.Hourani, S.Fortier, H.Laurent, J.M.Maison, J.P.Schapira Neutron-Hole Strengths and Isobaric Analog States in 95Zr NUCLEAR REACTIONS 91,92,94,96Zr(3He, α), E=39 MeV; measured σ(Eα, θ). 90,91,93,95Zr deduced levels, L, J, π, S. 95Y-95Zr analog pairs deduced Coulomb displacement energies, Γ, L, J, π, S. Enriched target, magnetic spectrometer.
doi: 10.1016/0375-9474(77)90130-0
1977GA18 Nucl.Phys. A288, 221 (1977) S.Gales, E.Hourani, S.Fortier, H.Laurent, J.M.Maison, J.P.Schapira Deeply Bound Hole States and Isobaric Analog States in 89Zr NUCLEAR REACTIONS 90Zr(3He, α), E=39 MeV; measured σ(Eα, θ). 89Zr deduced levels, L, J, π, S. Enriched target, magnetic spectrometer.
doi: 10.1016/0375-9474(77)90131-2
1977LA07 Nucl.Phys. A284, 501 (1977) H.Laurent, C.P.Massolo, J.P.Schapira, S.Fortier, S.Gales, J.M.Maison A Time-Integrated Perturbed Angular Correlation Measurement on the First 2+ of 24Mg, Using Charge State Separation NUCLEAR REACTIONS 24Mg(32S, 32S), E=67 MeV; measured γ(θ) on recoil into vacuum in the 12+, 11+, 10+, 9+ charge states. 24Mg deduced ionic electron configurations. Natural target.
doi: 10.1016/0375-9474(77)90399-2
1976GA04 Nucl.Phys. A259, 189 (1976) S.Gales, S.Fortier, H.Laurent, J.M.Maison, J.P.Schapira Spectroscopic Studies of Unbound Isobaric Analog States in 49V and 51V Via the 48,50Ti(τ, d) and the 48,50Ti(τ, dp) Reactions NUCLEAR REACTIONS 48,50Ti(3He, d), E=25.0 MeV; measured σ(Ed, θ). 48,50Ti(3He, pd), E=25.5 MeV; measured σ(Ed, Ep, θ). 49,51V deduced IAS, L, J, π, S, Γp, proton branching. 49,51V, 49,51Ti analog pairs deduced Coulomb displacement energies. DWBA analysis using Gamov functions as form factors. Enriched, natural targets.
doi: 10.1016/0375-9474(76)90062-2
1976GA15 Nucl.Phys. A265, 213 (1976) S.Gales, S.Fortier, H.Laurent, J.M.Maison, J.P.Schapira Population and Proton Decay of the g9/2 Isobaric Analog State in 53Mn via the 52Cr(τ, dp)52Cr Reaction NUCLEAR REACTIONS 52Cr(3He, pd), E=24 MeV; measured σ(Ed, Ep, θ(p)). 53Mn deduced IAS, J, Γp, S.
doi: 10.1016/0375-9474(76)90350-X
1976GA19 Nucl.Phys. A268, 257 (1976); Erratum Nucl.Phys. A280, 499 (1977) S.Gales, S.Fortier, H.Laurent, J.M.Maison, J.P.Schapira Proton States in 59Cu and Structure of the 59Cu-59Ni Analog Pair NUCLEAR REACTIONS 58Ni(3He, d), E=25 MeV; measured σ(E, θ). 58Ni(3He, pd), E=24 MeV; measured σ(Ed, Ep, θ(p)). 59Cu deduced levels, L, J, π, S, isobaric analog states, population parameters, Γp, Γp'. 59Ni-59Cu isotopes deduced Coulomb energy differences. Enriched target.
doi: 10.1016/0375-9474(76)90462-0
1976GA20 Phys.Rev. C14, 842 (1976) S.Gales, S.Fortier, H.Laurent, J.M.Maison, J.P.Schapira Unbound Isobaric Analog States in 53Mn: The Reactions 52Cr(3He, d)53Mn and 52Cr(3He, dp)52Cr NUCLEAR REACTIONS 52Cr(3He, d), E=25 MeV; measured σ(Ed, θ). 52Cr(3He, pd), E=24 MeV; measured σ(Ed, Ep, θ(p)). 53Mn deduced IAS, L, J, π, S, Γp, proton branching. 53Cr, 53Mn analog pairs deduced Coulomb displacement energies. DWBA analysis using Gamov functions as form factors. Natural targets.
doi: 10.1103/PhysRevC.14.842
1975FO15 Nucl.Phys. A254, 189 (1975) S.Fortier, S.Gales, H.Laurent, J.M.Maison, J.P.Schapira Gamma Decay of Analog States in 41Ca NUCLEAR REACTIONS 42Ca(3He, αγ), E=18 MeV; measured σ(Eα, Eγ, theta(γ)), Doppler shift. 41Ca levels deduced J, δ, γ-branching, T1/2. Enriched target.
doi: 10.1016/0375-9474(75)90591-6
1975GA10 Phys.Lett. 56B, 449 (1975) S.Gales, S.Fortier, H.Laurent, J.M.Maison, J.P.Schapira Angular Correlation Studies of Isobaric Analog States in 49Sc via the 48Ca(τ, dp)48Sc Reaction NUCLEAR REACTIONS 48Ca(3He, pd), E=25.5 MeV; measured dp-coin. 49Sc deduced IAS, L, J, π, S, p-width.
doi: 10.1016/0370-2693(75)90409-8
1974LA14 Nucl.Instrum.Methods 117, 17 (1974) H.Laurent, J.P.Schapira, S.Fortier, S.Gales, J.M.Maison Un Systeme de Detection a 0° du Faisceau, Utilisant un Triplet de Lentilles Quadrupolaires Magnetiques NUCLEAR REACTIONS 42Ca(3He, α), (3He, d), E=15, 18 MeV; measured Eα, Iα, Ed, Id. 41Ca deduced levels, analog resonance.
doi: 10.1016/0029-554X(74)90378-4
1973GA01 Nucl.Phys. A202, 535 (1973) S.Gales, L.Lessard, J.L.Foster, Jr. The 144Nd(d, p) and 144Nd(d, t) Reactions and Isobaric Analog Resonances In 144Nd(p, p0) and 144Nd(p, p') NUCLEAR REACTIONS 144Nd(d, p), (d, t), Ed=12.6 MeV; measured Q, σ(E, θ). 145Nd, 143Nd deduced levels, (J), π, L. 144Nd(p, p0), 144Nd(p, p'), Ep=9.3-12 MeV; measured σ(E). 145Pm deduced isobaric analog resonances level-width, J, π.
doi: 10.1016/0375-9474(73)90641-6
1973MA31 Nucl.Phys. A210, 221 (1973) R.Martin, L.Bimbot, S.Gales, L.Lessard, D.Spalding, W.G.Weitkamp, O.Dietzsch, J.L.Foster, Jr. The 144Sm(p, p') Reaction on Analog Resonances NUCLEAR REACTIONS 144Sm(p, p'), E=9.3-11 MeV; measured σ(E, θ). 144Sm deduced levels, J, π, S.
doi: 10.1016/0375-9474(73)90299-6
1973VE06 Phys.Rev. C8, 178 (1973) J.Vernotte, S.Gales, M.Langevin, J.M.Maison Investigation of the Lowest T = 2 State of 32S in the 31P + p Reactions NUCLEAR REACTIONS 31P(p, γ), (p, p'γ), (p, αγ), E=3.27-3.3 MeV; measured σ(Eγ), σ(E). 32S deduced resonances, T, J, π, γ-branching.
doi: 10.1103/PhysRevC.8.178
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