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NSR database version of April 11, 2024.

Search: Author = S.J.Sanders

Found 63 matches.

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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0520.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
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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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0407.


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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0407.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0407.


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1190.


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
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1991SA28      Phys.Rev. C44, 2676 (1991)

S.J.Sanders

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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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