NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = S.Sanders Found 64 matches. 2013SA19 Nucl.Phys. A904-905, 98c (2013) S.J.Sanders, for the CMS Collaboration Overview of results on flow and correlations from the CMS collaboration
doi: 10.1016/j.nuclphysa.2013.01.050
2009SA43 Nucl.Phys. A830, 179c (2009) S.J.Sanders, and the BRAHMS Collaboration Forward-rapidity azimuthal and radial flow of identified particles for √ sNN = 200 GeV Au+Au collisions
doi: 10.1016/j.nuclphysa.2009.09.018
2007SA64 J.Phys.(London) G34, S1083 (2007) S.J.Sanders, for the BRAHMS Collaboration Rapidity and pt dependence of identified-particle elliptic flow at RHIC
doi: 10.1088/0954-3899/34/8/S161
2005AR18 Nucl.Phys. A757, 1 (2005) I.Arsene, I.G.Bearden, D.Beavis, C.Besliu, B.Budick, H.Boggild, C.Chasman, C.H.Christensen, P.Christiansen, J.Cibor, R.Debbe, E.Enger, J.J.Gaardhoje, M.Germinario, O.Hansen, A.Holm, A.K.Holme, K.Hagel, H.Ito, E.Jakobsen, A.Jipa, F.Jundt, J.I.Jordre, C.E.Jorgensen, R.Karabowicz, E.J.Kim, T.Kozik, T.M.Larsen, J.H.Lee, Y.K.Lee, S.Lindahl, G.Lovhoiden, Z.Majka, A.Makeev, M.Mikelsen, M.J.Murray, J.Natowitz, B.Neumann, B.S.Nielsen, D.Ouerdane, R.Planeta, F.Rami, C.Ristea, O.Ristea, D.Rohrich, B.H.Samset, D.Sandberg, S.J.Sanders, R.A.Scheetz, P.Staszel, T.S.Tveter, F.Videbaek, R.Wada, Z.Yin, I.S.Zgura Quark-gluon plasma and color glass condensate at RHIC? The perspective from the BRAHMS experiment NUCLEAR REACTIONS 197Au(197Au, X), E(cm)=130, 200 GeV/nucleon; analyzed data; deduced possible quark-gluon plasma formation.
doi: 10.1016/j.nuclphysa.2005.02.130
2004SZ01 Nucl.Phys. A734, 311 (2004) A.Szanto de Toledo, F.A.Souza, C.Beck, S.J.Sanders, M.G.Munhoz, J.Takahashi, N.Carlin, A.A.P.Suaide, M.de Moura, E.M.Szanto Fusion and breakup in reactions involving weakly bound nuclei NUCLEAR REACTIONS 59Co(6Li, X), (7Li, X), E(cm) ≈ 10-25 MeV; analyzed fusion σ. 59Co(6Li, X), E=26 MeV; analyzed deuteron and alpha spectra, correlations.
doi: 10.1016/j.nuclphysa.2004.01.055
2003BE34 Phys.Rev. C 67, 054602 (2003) C.Beck, F.A.Souza, N.Rowley, S.J.Sanders, N.Aissaoui, E.E.Alonso, P.Bednarczyk, N.Carlin, S.Courtin, A.Diaz-Torres, A.Dummer, F.Haas, A.Hachem, K.Hagino, F.Hoellinger, R.V.F.Janssens, N.Kintz, R.Liguori Neto, E.Martin, M.M.Moura, M.G.Munhoz, P.Papka, M.Rousseau, A.Sanchez i Zafra, O.Stezowski, A.A.Suaide, E.M.Szanto, A.Szanto de Toledo, S.Szilner, J.Takahashi Near-barrier fusion of weakly bound 6Li and 7Li nuclei with 59Co NUCLEAR REACTIONS 59Co(6Li, xnypzα), (7Li, xnypzα), E(cm) ≈ 10-25 MeV; measured fusion, evaporation residue σ; deduced reaction mechanism features.
doi: 10.1103/PhysRevC.67.054602
2003BE75 Acta Phys.Hung.N.S. 18, 297 (2003) C.Beck, M.Rousseau, P.Papka, A.Sanchez i Zafra, C.Bhattacharya, V.Rauch, P.Bednarczyk, S.Courtin, O.Dorvaux, F.Haas, A.Nourreddine, I.Piqueras, J.Robin, L.El Bakali, C.Enaux, E.Galmar, S.Szilner, O.Stezowski, A.Prevost, S.Thummerer, W.von Oertzen, A.Hachem, E.Martin, A.Fahli, A.Morsad, A.Szanto de Toledo, S.J.Sanders Search for Cluster Emission and Extremely Deformed Shapes Using Charged-Particle Spectroscopy NUCLEAR REACTIONS 12C, 28Si(28Si, X), E=180 MeV; 12C(27Al, X), E=150 MeV; 12C(31P, X), E=112 MeV; 12C(32S, X), E=140 MeV; measured Eα, Ep, angular correlations between light charged particles and evaporation residues; deduced highly deformed configurations, cluster emission features. Other reactions discussed.
doi: 10.1556/APH.18.2003.2-4.30
2003SO19 Nucl.Phys. A718, 544c (2003) F.A.Souza, A.Szanto de Toledo, N.Carlin, R.Liguori Neto, A.A.Suaide, M.M.Moura, E.M.Szanto, M.G.Munhoz, J.Takahashi, C.Beck, S.J.Sanders Fusion of weakly bound light nuclei NUCLEAR REACTIONS 59Co(6Li, X), (7Li, X), E=11-26 MeV; measured fusion σ.
doi: 10.1016/S0375-9474(03)00838-8
2003SZ04 Nucl.Phys. A722, 248c (2003) A.Szanto de Toledo, E.E.Alonso, N.Carlin, R.Liguori Neto, M.M.Moura, M.G.Munhoz, A.A.Suaide, F.A.Souza, E.M.Szanto, J.Takahashi, C.Beck, M.Rousseau, P.Bednarczyk, S.Courtin, F.Hass, O.Stezowski, S.Szilner, S.J.Sanders Fusion of light weakly bound nuclei NUCLEAR REACTIONS 59Co(6Li, X), (7Li, X), E=11-26 MeV; measured fusion σ; deduced reaction mechanism features.
doi: 10.1016/S0375-9474(03)01373-3
2002BH01 Phys.Rev. C65, 014611 (2002) C.Bhattacharya, M.Rousseau, C.Beck, V.Rauch, R.M.Freeman, D.Mahboub, R.Nouicer, P.Papka, O.Stezowski, A.Hachem, E.Martin, A.K.Dummer, S.J.Sanders, A.Szanto De Toledo Deformation Effects in 56Ni Nuclei Produced in 28Si + 28Si at 112 MeV NUCLEAR REACTIONS 28Si(28Si, X), E=112 MeV; measured Eα, Ep, light charged particles σ(θ), angular correlations; deduced deformation effects. 30Si(30Si, X), E=120 MeV; analyzed Eα, related data. Statistical model analysis.
doi: 10.1103/PhysRevC.65.014611
2002RO35 Phys.Rev. C66, 034612 (2002) M.Rousseau, C.Beck, C.Bhattacharya, V.Rauch, O.Dorvaux, K.Eddahbi, C.Enaux, R.M.Freeman, F.Haas, D.Mahboub, R.Nouicer, P.Papka, O.Stezowski, S.Szilner, A.Hachem, E.Martin, S.J.Sanders, A.K.Dummer, A.Szanto de Toledo Highly Deformed 40Ca Configurations in 28Si + 12C NUCLEAR REACTIONS 12C(28Si, X), E=112, 180 MeV; measured Ep, Eα, σ(θ), energy and angular correlations between light and heavy fragments. 40Ca deduced highly deformed configurations. Statistical model analysis.
doi: 10.1103/PhysRevC.66.034612
2002SA69 Acta Phys.Hung.N.S. 15, 315 (2002) S.J.Sanders, for the BRAHMS Collaboration Charged Particle Multiplicities at BRAHMS NUCLEAR REACTIONS 197Au(197Au, X), E(cm)=130 GeV/nucleon; measured charged particle pseudorapidity densities.
doi: 10.1556/APH.15.2002.3-4.14
2001BE01 Phys.Rev. C63, 014607 (2001) C.Beck, R.Nouicer, D.Disdier, G.Duchene, G.de France, R.M.Freeman, F.Haas, A.Hachem, D.Mahboub, V.Rauch, M.Rousseau, S.J.Sanders, A.Szanto de Toledo Molecular Resonance and Highly Deformed Fission Fragments in 28Si + 28Si NUCLEAR REACTIONS 28Si(28Si, X), E=111.6 MeV; measured Eγ, Iγ, excitation energy spectra, angular distributions, (fragment)(fragment)-, (fragment)γ-coin. 56Ni deduced quasimolecular resonance features. 28Si, 24Mg, 32S deduced transition intensities. Eurogam II array.
doi: 10.1103/PhysRevC.63.014607
2001BH07 Pramana 57, 203 (2001) C.Bhattacharya, M.Rousseau, C.Beck, V.Rauch, R.M.Freeman, R.Nouicer, F.Haas, O.Dorvaux, K.Eddahbi, P.Papka, O.Stezowski, S.Szilner, D.Mahboub, A.Szanto de Toledo, A.Hachem, E.Martin, S.J.Sanders Deformation Effects in the 28Si + 12C and 28Si + 28Si Reactions NUCLEAR REACTIONS 12C, 28Si(28Si, X), E=112, 180 MeV; measured Eα, light charged particle and heavy fragment spectra; deduced di-nuclear system features, deformation effects. Statistical model calculations. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6120. 2001CL05 Phys.Rev.Lett. 87, 172503 (2001) S.T.Clark, G.Hackman, R.V.F.Janssens, R.M.Clark, P.Fallon, S.N.Floor, G.J.Lane, A.O.Macchiavelli, J.Norris, S.J.Sanders, C.E.Svensson Empirical Investigation of Extreme Single-Particle Behavior of Nuclear Quadrupole Moments in Highly Collective A ∼ 150 Superdeformed Bands NUCLEAR REACTIONS 122Sn(29Si, 5n), E=155 MeV; measured Eγ, Iγ, γγ-coin, DSA. 146Gd deduced superdeformed bands quadrupole moments. Gammasphere array. NUCLEAR STRUCTURE 142Sm, 143Eu, 144,148,149,150Gd, 149,151Tb, 151,152Dy; analyzed superdeformed bands quadrupole moments; deduced parameters. 146Gd; calculated superdeformed bands quadrupole moments. Empirical formula based on additivity of single-particle orbital quadrupole moments.
doi: 10.1103/PhysRevLett.87.172503
2001SA09 J.Phys.(London) G27, 671 (2001) S.J.Sanders, for the BRAHMS Collaboration Strangeness at BRAHMS
doi: 10.1088/0954-3899/27/3/352
1999AI02 Phys.Rev. C60, 034614 (1999) N.Aissaoui, N.Added, N.Carlin, G.M.Crawley, S.Danczyk, J.Finck, M.M.de Moura, D.Hirata, D.J.Morrissey, S.J.Sanders, J.Stasko, M.Steiner, A.A.P.Suaide, E.M.Szanto, A.Szanto de Toledo, M.Thoennessen, J.A.Winger Strong Absorption Radii from Reaction Cross Section Measurements for Neutron-Rich Nuclei NUCLEAR REACTIONS Si(30Al, X), (31Al, X), (32Al, X), (33Al, X), (32Si, X), (33Si, X), (34Si, X), (35Si, X), (36Si, X), (34P, X), (35P, X), (36P, X), (37P, X), (38P, X), (39P, X), (36S, X), (37S, X), (38S, X), (39S, X), (40S, X), (41S, X), (39Cl, X), (40Cl, X), (41Cl, X), (42Cl, X), (43Cl, X), (44Cl, X), (41Ar, X), (42Ar, X), (43Ar, X), (44Ar, X), (45Ar, X), (46Ar, X), (44K, X), (45K, X), (46K, X), (47K, X), (48K, X), (46Ca, X), (47Ca, X), (48Ca, X), (49Ca, X), (50Ca, X), (49Sc, X), (50Sc, X), (51Sc, X), (52Sc, X), (53Ti, X), (54Ti, X), E ≈ 38-80 MeV/nucleon; measured mean energy-integrated reaction σ. 30,31,32,33Al, 32,33,34,35,36Si, 34,35,36,37,38,39P, 36,37,38,39,40,41S, 39,40,41,42,43,44Cl, 41,42,43,44,45,46Ar, 44,45,46,47,48K, 46,47,48,49,50Ca, 49,50,51,52Sc, 53,54Ti deduced strong absorption radii. Secondary beams from 55Mn fragmentation.
doi: 10.1103/PhysRevC.60.034614
1999BH08 Nucl.Phys. (Supplement) A654, 841c (1999) C.Bhattacharya, M.Rousseau, C.Beck, V.Rauch, R.Nouicer, R.M.Freeman, O.Stezowski, D.Mahboub, S.Belhabib, A.Hachem, E.Martin, A.Dummer, S.J.Sanders, A.Szanto de Toledo Role of Deformation in the Decay of 56Ni and 40Ca Di-Nuclei NUCLEAR REACTIONS 12C, 28Si(28Si, αX), E=112.6 MeV; measured Eα, Iα(θ); deduced deformation effects. Statistical model analysis, spin-dependent level density.
doi: 10.1016/S0375-9474(00)88558-9
1999NO06 Phys.Rev. C60, 041303 (1999) R.Nouicer, C.Beck, R.M.Freeman, F.Haas, N.Aissaoui, T.Bellot, G.de France, D.Disdier, G.Duchene, A.Elanique, A.Hachem, F.Hoellinger, D.Mahboub, V.Rauch, S.J.Sanders, A.Dummer, F.W.Prosser, A.Szanto de Toledo, Sl.Cavallaro, E.Uegaki, Y.Abe Vanishing Spin Alignment: Experimental indication of a triaxial 28Si + 28Si Nuclear Molecule NUCLEAR REACTIONS 28Si(28Si, 28Si), (28Si, 28Si'), E=111.6 MeV; measured (fragment)γ-, (fragment)(fragment)-coin, σ(E, θ); deduced fragment spin correlations, molecular configuration.
doi: 10.1103/PhysRevC.60.041303
1999SA45 Phys.Rep. 311, 487 (1999) S.J.Sanders, A.Szanto de Toledo, C.Beck Binary Decay of Light Nuclear Systems
doi: 10.1016/S0370-1573(98)00092-1
1998CA02 Phys.Rev. C57, 731 (1998) Sl.Cavallaro, E.De Filippo, G.Lanzano, A.Pagano, M.L.Sperduto, R.Dayras, R.Legrain, E.Pollacco, C.Beck, B.Djerroud, R.M.Freeman, F.Haas, A.Hachem, B.Heusch, D.Mahboub, A.Morsad, R.Nouicer, S.J.Sanders Fusion and Binary-Decay Mechanisms in the 35Cl + 24Mg System at E/A ≈ 8 MeV NUCLEAR REACTIONS 24Mg(35Cl, X), E=282 MeV; measured fragments σ(E, Z, θ), fusion, binary mechanism σ; deduced partially-damped binary product decay times, reaction mechanism.
doi: 10.1103/PhysRevC.57.731
1997SA20 Phys.Rev. C55, 2541 (1997) S.J.Sanders, A.K.Dummer, K.A.Farrar, F.W.Prosser, B.Fornal, R.V.F.Janssens, M.P.Carpenter, T.L.Khoo, C.Beck, D.Mahboub, F.Haas, Sl.Cavallaro, M.Sferrazza, R.Mayer, D.Nisius, G.de Angelis Quasielastic Transfer in the 136Xe + 64Ni Reaction NUCLEAR REACTIONS 64Ni(136Xe, X), E=549 MeV; measured Eγ, Iγ, (particle)γ-coin, Iγ(θ); deduced single, multi-nucleon transfer probabilities.
doi: 10.1103/PhysRevC.55.2541
1997SZ02 Phys.Rev. C56, 558 (1997) A.Szanto de Toledo, S.J.Sanders, C.Beck Statistical Description of Strongly Damped Binary Yields from the 28Si + 16O Reaction NUCLEAR REACTIONS 28Si(14N, X), 28Si(12C, X), 24Mg(12C, X), 24Mg(16O, X), 28Si, (16O, X), E not given; calculated number of reaction channels vs grazing angular momentum. 28Si(16O, X), E(cm)=39.1, 50.1 MeV; analyzed σ(E), fragment charge distributions; deduced energy-dependent orbiting component. Statistical model.
doi: 10.1103/PhysRevC.56.558
1996BA17 Phys.Rev. C53, 1734 (1996) B.B.Back, P.B.Fernandez, B.G.Glagola, D.Henderson, S.Kaufman, J.G.Keller, S.J.Sanders, F.Videbaek, T.F.Wang, B.D.Wilkins Entrance-Channel Effects in Quasifission Reactions NUCLEAR REACTIONS 182W(32S, X), (32S, 32S), E=166-260 MeV; 166Er(48Ti, X), (48Ti, 48Ti), E=220-298 MeV; 154Sm(60Ni, X), (60Ni, 60Ni), E=269-421 MeV; measured σ(θ), deep-inelastic, fission like σ(θ) vs fragment mass; deduced complete fusion contribution to fission like σ, entrance channel dependence.
doi: 10.1103/PhysRevC.53.1734
1996BE17 Phys.Rev. C54, 227 (1996) C.Beck, D.Mahboub, R.Nouicer, T.Matsuse, B.Djerroud, R.M.Freeman, F.Haas, A.Hachem, A.Morsad, M.Youlal, S.J.Sanders, R.Dayras, J.P.Wieleczko, E.Berthoumieux, R.Legrain, E.Pollacco, Sl.Cavallaro, E.De Filippo, G.Lanzano, A.Pagano, M.L.Sperduto 35Cl + 12C Asymmetrical Fission Excitation Functions NUCLEAR REACTIONS 12C(35Cl, F), E=150-280 MeV; measured σ(E, θ), fission (fragment)(fragment) correlations, missing charge distributions; deduced charge deficit systematics, fusion-fission σ(E). Extended Hauser-Feshbach method, transition-state formalism.
doi: 10.1103/PhysRevC.54.227
1996FA14 Phys.Rev. C54, 1249 (1996) K.A.Farrar, S.J.Sanders, A.K.Dummer, A.T.Hasan, F.W.Prosser, B.B.Back, I.G.Bearden, R.R.Betts, M.P.Carpenter, B.Crowell, M.Freer, D.J.Henderson, R.V.F.Janssens, T.L.Khoo, T.Lauritsen, Y.Liang, D.Nisius, A.H.Wuosmaa, C.Beck, R.M.Freeman, Sl.Cavallaro, A.Szanto de Toledo Fission Decay of 48Cr at E(*)(CN) ≈ 60 MeV NUCLEAR REACTIONS 12C(36Ar, X), 28Si(20Ne, X), 24Mg(24Mg, X), E(cm)=47, 45.5, 44.4 MeV; measured Eγ, Iγ, (particle)(particle)γ-coin; deduced σ(A) for fission, evaporation residues. 48Ca deduced spin distribution, fission decay features.
doi: 10.1103/PhysRevC.54.1249
1995CA06 Nucl.Phys. A583, 161c (1995) Sl.Cavallaro, C.Beck, E.Berthoumieux, R.Dayras, E.De Filippo, G.Di Natale, B.Djerroud, R.M.Freeman, A.Hachem, F.Haas, B.Heusch, G.Lanzano, R.Legrain, D.Mahboub, A.Morsad, A.Pagano, E.Pollacco, S.J.Sanders, M.L.Sperduto Origin and Decay-Properties of Binary Fragments Produced in the 35Cl + 24Mg Reaction at E/A ≈ 8 MeV/A NUCLEAR REACTIONS 24Mg(35Cl, X), E=260, 282.4 MeV; measured σ(fragment θ, E), (fragment)(fragment)(θ); deduced binary fragment origin, decay mechanisms.
doi: 10.1016/0375-9474(94)00725-3
1995MO39 Nucl.Instrum.Methods Phys.Res. B99, 308 (1995) E.F.Moore, W.Henning, R.V.F.Janssens, T.L.Khoo, S.J.Sanders, I.Ahmad, H.Amro, D.Blumenthal, M.P.Carpenter, B.Crowell, M.W.Drigert, D.Gassmann, R.G.Henry, T.Lauritsen, C.J.Lister, D.Nisius Search for the Two-Phonon Octupole Vibrational State in 208Pb NUCLEAR REACTIONS 208Pb, 209Bi, 58,64Ni, 160Gd(208Pb, 208Pb'), E=1305 MeV; measured γγ-coin, Eγ, Iγ following projectile excitation. 208Pb deduced no evidence for two-phonon octupole vibrational state.
doi: 10.1016/0168-583X(94)00687-3
1994AN05 Phys.Rev. C49, 2018 (1994) R.M.Anjos, N.Added, N.Carlin, L.Fante, Jr., M.C.S.Figueira, R.Matheus, E.M.Szanto, C.Tenreiro, A.Szanto de Toledo, S.J.Sanders Competing Reaction Mechanisms for the 16,17,18O + 10,11B and 19F + 9Be Systems NUCLEAR REACTIONS 10,11B(16O, 16O), (17O, 17O), (18O, 18O), E=42-63 MeV; measured σ(θ); deduced optical model parameters. 10,11B(16O, X), (17O, X), (18O, X), E=22-64 MeV; 9Be(19F, X), E=56 MeV; measured fusion, quasielastic, strong damped reaction yields; deduced reaction systematics.
doi: 10.1103/PhysRevC.49.2018
1994FA18 Nucl.Instrum.Methods Phys.Res. A346, 177 (1994) K.A.Farrar, A.T.Hasan, F.W.Prosser, S.J.Sanders, D.J.Henderson A Large-Acceptance Bragg Curve Spectrometer with a Longitudinal Electric Field and a Segmented Anode NUCLEAR REACTIONS 197Au(36Ar, 36Ar), E=188 MeV; measured energy spectra. Large angle Bragg curve spectrometer.
doi: 10.1016/0168-9002(94)90702-1
1994HA03 Phys.Rev. C49, 1031 (1994) A.T.Hasan, S.J.Sanders, K.A.Farrar, F.W.Prosser, B.B.Back, R.R.Betts, M.Freer, D.J.Henderson, R.V.F.Janssens, A.H.Wuosmaa, A.Szanto de Toledo Heavy-Ion Resonance and Statistical Fission Competition in the 24Mg + 24Mg System at E(c.m.) = 44.4 MeV NUCLEAR REACTIONS 24Mg(24Mg, F), (24Mg, X), E(cm)=44.4 MeV; measured fission fragment, evaporation residue σ(θ). 48Cr deduced fission characteristics.
doi: 10.1103/PhysRevC.49.1031
1994SA04 Phys.Rev. C49, 1016 (1994) S.J.Sanders, A.Hasan, F.W.Prosser, B.B.Back, R.R.Betts, M.P.Carpenter, D.J.Henderson, R.V.F.Janssens, T.L.Khoo, E.F.Moore, P.R.Wilt, F.L.H.Wolfs, A.H.Wuosmaa, K.B.Beard, Ph.Benet Selective Population of States in Fission Fragments from the 32S + 24Mg Reaction NUCLEAR REACTIONS 24Mg(32S, F), E=120.9, 129 MeV; 24Mg(32S, 24Mg), E(cm)=51, 54.5 MeV; measured fission, reaction (particle)(particle)γ-, particle(γ)-, (particle)(particle)-coin; deduced selective population of 28Si states in 56Ni fission. Statistical model.
doi: 10.1103/PhysRevC.49.1016
1993AN08 Nucl.Phys. A555, 621 (1993) R.M.Anjos, C.Tenreiro, A.Szanto de Toledo, S.J.Sanders Fusion-Fission Rather Than Orbiting in 18O + 10,11B Reactions NUCLEAR REACTIONS 10,11B(18O, X), E=47 MeV; measured σ(θ), σ(fragment Z) for fusion, strongly damped binary processes.
doi: 10.1016/0375-9474(93)90491-F
1993AN15 Phys.Rev. C48, R2154 (1993) R.M.Anjos, N.Added, N.Carlin, L.Fante, Jr., M.C.S.Figueira, R.Matheus, H.R.Schelin, E.M.Szanto, C.Tenreiro, A.Szanto de Toledo, S.J.Sanders Fission Decay of Very Light Nuclear Systems NUCLEAR REACTIONS 10,11B(16O, X), (17O, X), (18O, X), 9Be(19F, X), E < 5 MeV/nucleon; measured σ(fragment θ); deduced fusion followed by fission evidence.
doi: 10.1103/PhysRevC.48.R2154
1993BE15 Phys.Rev. C47, 2093 (1993) C.Beck, B.Djerroud, F.Haas, R.M.Freeman, A.Hachem, B.Heusch, A.Morsad, M.Vuillet-A-Cilles, S.J.Sanders Asymmetric Fission of 47V Induced by the 23Na + 24Mg Reaction NUCLEAR REACTIONS 24Mg(23Na, X), (23Na, F), E=89.1 MeV; measured fragment total kinetic energy, σ vs charge. 47V deduced no entrance channel effects in fission. Other reactions data analyzed.
doi: 10.1103/PhysRevC.47.2093
1993SM04 Phys.Rev. C47, 2740 (1993) M.S.Smith, P.V.Magnus, K.I.Hahn, R.M.Curley, P.D.Parker, T.F.Wang, K.E.Rehm, P.B.Fernandez, S.J.Sanders, A.Garcia, E.G.Adelberger Gamma Width of 14O(*)(5.17 MeV) and the Stellar 13N(p, γ)14O Reaction Rate NUCLEAR REACTIONS 14N(p, n), E(cm)=11.67 MeV; measured σ(θ). 1H(14N, 14O), E=175 MeV; measured 14O momentum spectra; deduced 13N(p, γ)14O stellar reaction rate. 14O level deduced Γγ/Γ.
doi: 10.1103/PhysRevC.47.2740
1991EV02 Nucl.Phys. A526, 365 (1991) P.M.Evans, A.E.Smith, C.N.Pass, L.Stuttge, B.B.Back, R.R.Betts, B.K.Dichter, D.J.Henderson, S.J.Sanders, F.Videbaek, B.D.Wilkins Dissipative Reaction Mechanisms in Medium-Mass Nuclear Collisions NUCLEAR REACTIONS 40Ca(40Ca, X), E=197, 231 MeV; measured fragment mass, charge distributions, σ(θ), strongly damped σ. Finite-range liquid drop model calculations, fast fission, asymmetric fission interpretations.
doi: 10.1016/0375-9474(91)90291-D
1991FU03 J.Phys.(London) G17, 555 (1991) B.R.Fulton, S.J.Bennett, M.Freer, J.T.Murgatroyd, S.C.Allcock, W.D.M.Rae, A.E.Smith, R.R.Betts, B.B.Back, S.Sanders, F.Videbaek Search for Large Cluster Breakup of 40Ca NUCLEAR REACTIONS 12C(40Ca, 12CX), E=300 MeV; measured total energy spectra following projectile breakup. 12C(24Mg, 212C), E not given; analyzed total energy spectra following projectile breakup; deduced no large cluster 40Ca breakup evidence.
doi: 10.1088/0954-3899/17/4/014
1991SA28 Phys.Rev. C44, 2676 (1991) Fusion-Fission in Nuclear Systems with 40 ≤ A(CN) ≤ 80 NUCLEAR REACTIONS, ICPND 28Si(12C, X), (12C, F), E(cm)=34.5 MeV; 24Mg(16O, X), (16O, F), E(cm)=31.8 MeV; 28Si(14N, X), (14N, F), E(cm)=40 MeV; 35Cl(12C, X), (12C, F), E(cm)=51.1 MeV; 23Na(24Mg, X), (24Mg, F), E(cm)=45.5 MeV; 24Mg(32S, X), (32S, F), E(cm)=51.6, 60.5 MeV; 40Ca(40Ca, X), (40Ca, F), E(cm)=98.5, 115.5 MeV; 50Cr(28Si, X), (28Si, F), E(cm)=96.2 MeV; calculated fusion, fission, evaporation residue, 8Be production σ; deduced fission mechanism. Fusion followed by fission. Diffuse surface, finite-range model. NUCLEAR STRUCTURE A=40-80; calculated spin-, mass assymmetry-dependent saddle point energies. Diffuse surface, finite-range model.
doi: 10.1103/PhysRevC.44.2676
1990SA14 Phys.Rev. C41, R1901 (1990) S.J.Sanders, B.B.Back, R.V.F.Janssens, D.G.Kovar, D.Habs, D.Henderson, T.-L.Khoo, H.Korner, G.-E.Rathke, T.F.Wang, F.L.H.Wolfs, K.B.Beard Additional Evidence for Fusion-Fission in 32S + 24Mg Reactions: Division of excitation energy and spin in the fission fragments NUCLEAR REACTIONS 24Mg(32S, 12C), E=140 MeV; measured γ(12C)-coin, E(γ); deduced reaction mechanism, scission temperature.
doi: 10.1103/PhysRevC.41.R1901
1989BE17 Phys.Rev. C39, 2202 (1989) C.Beck, D.G.Kovar, S.J.Sanders, B.D.Wilkins, D.J.Henderson, R.V.F.Janssens, W.C.Ma, M.F.Vineyard, T.F.Wang, C.F.Maguire, F.W.Prosser, G.Rosner Fusion of 16O + 40Ca at E(lab)(16O) = 13.4 MeV/Nucleon NUCLEAR REACTIONS 40Ca(16O, X), E=13.4 MeV/nucleon; measured evaporation residue σ(θ), fusion-fission fragment σ(θ); deduced fusion σ(E) limits.
doi: 10.1103/PhysRevC.39.2202
1989EV02 Phys.Lett. 229B, 25 (1989) P.M.Evans, A.E.Smith, C.N.Pass, L.Stuttge, R.R.Betts, S.J.Sanders, B.B.Back, B.K.Dichter, D.J.Henderson, F.Videbaek, B.D.Wilkins Damped Reactions in Medium Mass Nuclei NUCLEAR REACTIONS 40Ca(40Ca, X), E=197, 231 MeV; 50Cr(28Si, X), E=150 MeV; measured σ(fragment θ) vs mass, charge; deduced reaction mechanism.
doi: 10.1016/0370-2693(89)90148-2
1989SA39 Phys.Rev. C40, 2091 (1989) S.J.Sanders, D.G.Kovar, B.B.Back, C.Beck, D.J.Henderson, R.V.F.Janssens, T.F.Wang, B.D.Wilkins Binary Decay of 56Ni Formed in the 32S + 24Mg Reaction NUCLEAR REACTIONS 24Mg(32S, X), E=120.4, 141.2 MeV; measured σ(fragment mass, E, θ); deduced fusion-fission σ. Binary decay, coincidence geometry.
doi: 10.1103/PhysRevC.40.2091
1989WO01 Phys.Rev. C39, 865 (1989) F.L.H.Wolfs, R.V.F.Janssens, R.Holzmann, T.L.Khoo, W.C.Ma, S.J.Sanders 64Ni + 92Zr Fission Yields at Energies Close to the Coulomb Barrier NUCLEAR REACTIONS 92Zr(64Ni, F), (64Ni, 64Ni), E=240-300 MeV; measured σ(θ), fission fragment σ(θ); deduced fission, evaporation residue σ(E). 156Er deduced spin distribution diffuseness.
doi: 10.1103/PhysRevC.39.865
1988SA05 Phys.Rev. C37, 1318 (1988) S.J.Sanders, B.B.Back, R.R.Betts, D.Henderson, R.V.F.Janssens, K.E.Rehm, F.Videbaek 48Ti + 104Ru Single-Nucleon Transfer at the Barrier NUCLEAR REACTIONS 104Ru(48Ti, 49Ti), E=161.8 MeV; measured σ(θ); deduced transfer probability vs closest approach reduced distance. DWBA analysis.
doi: 10.1103/PhysRevC.37.1318
1987DI02 Phys.Rev. C35, 1304 (1987) B.K.Dichter, P.D.Parker, S.J.Sanders, R.R.Betts, S.Saini Search for Shape Isomers in 56Ni NUCLEAR REACTIONS 40Ca(16O, 28Si), E=74.925-77.25 MeV; measured σ(θ), Q, σ(E). 56Ni deduced resonances, Γ. Other data input.
doi: 10.1103/PhysRevC.35.1304
1987KE04 Phys.Rev. C36, 1364 (1987) J.G.Keller, B.B.Back, B.G.Glagola, D.Henderson, S.B.Kaufman, S.J.Sanders, R.H.Siemssen, F.Videbaek, B.D.Wilkins, A.Worsham Distribution of Reaction Strength in 32S + 182W Collisions NUCLEAR REACTIONS 182W(32S, 32S), (32S, X), E=166, 177, 222, 260 MeV; measured σ(θ); deduced reaction, deep inelastic, fission σ(E), fission product mass, reaction strength distributions.
doi: 10.1103/PhysRevC.36.1364
1987SA52 Phys.Rev.Lett. 59, 2856 (1987) S.J.Sanders, D.G.Kovar, B.B.Back, C.Beck, B.K.Dichter, D.Henderson, R.V.F.Janssens, J.G.Keller, S.Kaufman, T.-F.Wang, B.Wilkins, F.Videbaek Asymmetric Fission of 56Ni NUCLEAR REACTIONS, ICPND 24Mg(32S, X), E=141.8 MeV; measured mass, velocity spectra, binary reaction σ(A); deduced fission reaction yield characteristics. 56Ni deduced fission mechanism.
doi: 10.1103/PhysRevLett.59.2856
1986SA25 Phys.Rev. C34, 1746 (1986) S.J.Sanders, R.R.Betts, I.Ahmad, K.T.Lesko, S.Saini, B.D.Wilkins, F.Videbaek, B.K.Dichter Fission-Like Yields in 16O + 40,44Ca Reactions NUCLEAR REACTIONS 40,44Ca(16O, X), E=69.3-87.3 MeV; measured σ(E, θ) vs mass, evaporation residue yields; deduced fusion σ(E). Enriched target, tof. Deep-inelastic scattering calculations.
doi: 10.1103/PhysRevC.34.1746
1985SA11 Phys.Rev. C31, 1775 (1985) S.J.Sanders, H.Ernst, W.Henning, C.Jachcinski, D.G.Kovar, J.P.Schiffer, J.Barrette Energy Dependence of the Cross Sections for the 24Mg(16O, 12C)28Si(g.s) Reaction NUCLEAR REACTIONS 24Mg(16O, 12C), E(cm)=36-54 MeV; measured σ(E), σ(θ). 40Ca deduced possible resonances, parameters.
doi: 10.1103/PhysRevC.31.1775
1983PE08 Phys.Rev. C28, 710 (1983) J.F.Petersen, R.J.Ascuitto, D.G.Kovar, W.Henning, S.J.Sanders 12C on 48Ca Transfer Reactions: A test of the effective Q-value model NUCLEAR REACTIONS 48Ca(12C, 11B), (12C, 13C), (12C, 12C), E=45 MeV; measured σ(θ), σ(E(11B)), σ(E(13C)); deduced optical model parameters. DWBA, effective Q model analyses.
doi: 10.1103/PhysRevC.28.710
1982ER08 Phys.Lett. 119B, 307 (1982) H.Ernst, W.Henning, C.N.Davids, W.S.Freeman, T.J.Humanic, M.Paul, S.J.Sanders, F.W.Prosser, Jr., R.A.Racca Prompt Compound Nuclear K X-Rays in Fusion Reactions Induced by a Heavy Projectile NUCLEAR REACTIONS 116,120,124Sn(32S, X), E=130-202 MeV; measured E(X-ray), I(X-ray), (X-ray)(X-ray)-coin, K X-ray production σ, multiplicities; deduced K X-ray yield role in complete fusion.
doi: 10.1016/0370-2693(82)90676-1
1981JA10 Phys.Rev. C24, 2070 (1981) C.M.Jachcinski, D.G.Kovar, R.R.Betts, C.N.Davids, D.F.Geesaman, C.Olmer, M.Paul, S.J.Sanders, J.L.Yntema Fusion of 24Mg + 24Mg NUCLEAR REACTIONS 24Mg(24Mg, X), E(cm)=24.7-66.2 MeV; measured σ(fusion, E). Activation technique.
doi: 10.1103/PhysRevC.24.2070
1981MC02 Nucl.Phys. A358, 411c (1981) R.D.McKeown, J.P.Schiffer, H.E.Jackson, M.Paul, S.J.Sanders, J.R.Specht, E.J.Stephenson, R.P.Redwine, R.E.Segel, J.Arends, J.Eyink, H.Hartmann, A.Hegerath, B.Mecking, G.Noldeke, H.Rost Comparison of Pion and Photon Induced Reactions on Complex nuclei NUCLEAR REACTIONS 12C(π+, p), (π-, p), E=220 MeV; 12C(γ, p), E=343 MeV; analyzed σ(θp, Ep); deduced Δ production mechanism.
doi: 10.1016/0375-9474(81)90354-7
1981MC09 Phys.Rev. C24, 211 (1981) R.D.McKeown, S.J.Sanders, J.P.Schiffer, H.E.Jackson, M.Paul, J.R.Specht, E.J.Stephenson, R.P.Redwine, R.E.Segel Inclusive Reactions of Pions on Nuclei NUCLEAR REACTIONS 4He, 6Li, 9Be, 12C, 27Al, Ni, 181Ta(π+, p), (π-, p), (π+, π+'), (π-, π-'), E=100, 160, 220 MeV; measured σ(θ, Ep), inclusive pion yields.
doi: 10.1103/PhysRevC.24.211
1980MC03 Phys.Rev.Lett. 44, 1033 (1980) R.D.McKeown, S.J.Sanders, J.P.Schiffer, H.E.Jackson, M.Paul, J.R.Specht, E.J.Stephenson, R.P.Redwine, R.E.Segel How Many Nucleons Are Involved in Pion Absorption in Nuclei < Question > NUCLEAR REACTIONS 12C, 27Al, 58Ni, 181Ta(π+, p), (π-, p), E=100, 160, 220 MeV; measured inclusive production σ(θ). 12C, 27Al, 58Ni, 181Ta deduced effective number of participating nucleons.
doi: 10.1103/PhysRevLett.44.1033
1980MC10 Phys.Rev.Lett. 45, 2015 (1980) R.D.McKeown, J.P.Schiffer, H.E.Jackson, M.Paul, S.J.Sanders, J.R.Specht, E.J.Stephenson, R.P.Redwine, R.E.Segel, J.Arends, J.Eyink, H.Hartmann, A.Hegerath, B.Mecking, G.Noldeke, H.Rost Comparison of Pion- and Photon-Induced Reactions on 12C NUCLEAR REACTIONS 12C(π+, p), (π-, p), E=220 MeV; 12C(γ, p), E=343 MeV; analyzed σ(θp, Ep); deduced possible common reaction mechanism via isobar production.
doi: 10.1103/PhysRevLett.45.2015
1980PA08 Phys.Rev. C21, 1802 (1980) M.Paul, S.J.Sanders, D.F.Geesaman, W.Henning, D.G.Kovar, C.Olmer, J.P.Schiffer, J.Barrette, M.J.LeVine 24Mg(16O, 12C)28Si and 24Mg(16O, 16O)24Mg Reactions at Backward Angles NUCLEAR REACTIONS 24Mg(16O, 12C), (16O, 16O), E=24-40 MeV; measured σ(E, θ). 40Ca deduced resonances, J. DWBA, Legendre polynomial, correlation analyses.
doi: 10.1103/PhysRevC.21.1802
1980SA12 Phys.Rev. C21, 1810 (1980) S.J.Sanders, M.Paul, J.Cseh, D.F.Geesaman, W.Henning, D.G.Kovar, R.Kozub, C.Olmer, J.P.Schiffer Resonant Behavior of the 24Mg(16O, 12C)28Si Reaction NUCLEAR REACTIONS 24Mg(16O, 12C), E(cm)=26.3-32.4 MeV; measured σ(E, θ). 40Ca deduced resonances, J, Γ. Breit-Wigner resonance, direct amplitudes.
doi: 10.1103/PhysRevC.21.1810
1980SA31 Phys.Rev. C22, 1914 (1980) S.J.Sanders, C.Olmer, D.F.Geesaman, W.Henning, D.G.Kovar, M.Paul, J.P.Schiffer Resonant Behavior of the 24Mg(16O, 12C)28Si* (6.4 < Ex < 10 MeV) Reaction NUCLEAR REACTIONS 24Mg(16O, 12C), E(cm)=24-36 MeV; measured σ(E, θ), σ(E(12C)). 40Ca resonances deduced entrance, exit channel partial widths. DWBA analysis.
doi: 10.1103/PhysRevC.22.1914
1979KO20 Phys.Rev. C20, 1305 (1979) D.G.Kovar, D.F.Geesaman, T.H.Braid, Y.Eisen, W.Henning, T.R.Ophel, M.Paul, K.E.Rehm, S.J.Sanders, P.Sperr, J.P.Schiffer, S.L.Tabor, S.Vigdor, B.Zeidman, F.W.Prosser, Jr. Systematics of Carbon- and Oxygen-Induced Fusion on Nuclei with 12 ≤ A ≤ 19 NUCLEAR REACTIONS 12C(12C, X), E(cm)=7.4-31.2 MeV; 12C(13C, X), E(cm)=7.6-24.9 MeV; 12C(14N, X), E(cm)=15.1-24.0 MeV; 12C(15N, X), E(cm)=8.9-26.7 MeV; 12C(16O, X), E(cm)=12.9-27.0 MeV; 12C(18O, X), E(cm)=11.9-28.0 MeV; 12C(19F, X), E(cm)=11.6-27.1 MeV; 16O(16O, X), E(cm)=16.9-36.0 MeV; measured fusion σ(E); deduced fusion barrier parameters.
doi: 10.1103/PhysRevC.20.1305
1979MA26 Phys.Rev. C20, 1340 (1979) L.M.Martz, S.J.Sanders, P.D.Parker, C.B.Dover (6Li, t), (6Li, 3He), and (7Li, t) Reactions into the A = 19 Nuclei NUCLEAR REACTIONS 15N(7Li, t), E=40 MeV; 16O(6Li, t), (6Li, 3He), E=46 MeV; measured σ(θ). 19Ne, 19F deduced levels; calculated triton-cluster states.
doi: 10.1103/PhysRevC.20.1340
1979SA29 Phys.Rev. C20, 1743 (1979) S.J.Sanders, L.M.Martz, P.D.Parker Spectroscopy of High Spin States in 16O and 20Ne Using the (12C, 8Be)(α0) Reaction NUCLEAR REACTIONS 16O, 12C(12C, α8Be), E=78 MeV; measured particle-particle (θ). 16O, 20Ne resonances deduced J, π, Γα0/Γ.
doi: 10.1103/PhysRevC.20.1743
1978PA04 Phys.Rev.Lett. 40, 1310 (1978) M.Paul, S.J.Sanders, J.Cseh, D.F.Geesaman, W.Henning, D.G.Kovar, C.Olmer, J.P.Schiffer Resonant Effects in the Reaction 24Mg(16O, 12C)28Si NUCLEAR REACTIONS 24Mg(16O, 12C), E=47, 52, 57 MeV; measured σ(θ).
doi: 10.1103/PhysRevLett.40.1310
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