NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = N.Carlin Found 90 matches. 2019GU32 Eur.Phys.J. A 55, 211 (2019) G.L.Guardo, C.Spitaleri, L.Lamia, R.Spartá, N.Carlin, S.Cherubini, G.Gimenez Del Santo, I.Indelicato, M.La Cognata, D.Lattuada, S.Messina, M.Munhoz, S.S.Perrotta, R.G.Pizzone, G.G.Rapisarda, S.Romano, M.L.Sergi, F.A.Souza, A.Szanto de Toledo, S.Tudisco, A.Tumino The 10B(n, α)7Li cross sections at ultra-low energy through the Trojan Horse Method applied to the 2H(10B, α7Li)1H
doi: 10.1140/epja/i2019-12914-0
2017SP04 Phys.Rev. C 95, 035801 (2017) C.Spitaleri, S.M.R.Puglia, M.La Cognata, L.Lamia, S.Cherubini, A.Cvetinovic, G.D'Agata, M.Gulino, G.L.Guardo, I.Indelicato, R.G.Pizzone, G.G.Rapisarda, S.Romano, M.L.Sergi, R.Sparta, S.Tudisco, A.Tumino, M.Gimenez Del Santo, N.Carlin, M.G.Munhoz, F.A.Souza, A.Szanto de Toledo, A.Mukhamedzhanov, C.Broggini, A.Caciolli, R.Depalo, R.Menegazzo, V.Rigato, I.Lombardo, D.Dell'Aquila Measurement of the 10B(p, α0)7Be cross section from 5 keV to 1.5 MeV in a single experiment using the Trojan horse method NUCLEAR REACTIONS 2H(10B, α7Be), E=27 MeV; measured α and 7Be spectra using ΔE-E method at Pelletron-Linac laboratory of DFN-Sao Paulo; deduced Q-value spectrum, energy scatter plots, momentum distribution, astrophysical S(E) factors, Trojan horse method (THM) astrophysical factor, R-matrix fit of THM data 11C; deduced levels, resonances, center-of-mass energies, J, π, Γp, Γα0, Γα1.
doi: 10.1103/PhysRevC.95.035801
2014SP03 Phys.Rev. C 90, 035801 (2014) C.Spitaleri, L.Lamia, S.M.R.Puglia, S.Romano, M.La Cognata, V.Crucilla, R.G.Pizzone, G.G.Rapisarda, M.L.Sergi, M.Gimenez Del Santo, N.Carlin, M.G.Munhoz, F.A.Souza, A.Szanto de Toledo, A.Tumino, B.Irgaziev, A.Mukhamedzhanov, G.Tabacaru, V.Burjan, V.Kroha, Z.Hons, J.Mrazek, S.-H.Zhou, C.Li, Q.Wen, Y.Wakabayashi, H.Yamaguchi, E.Somorjai Measurement of the 10 keV resonance in the 10B(p, α0)7Be reaction via the Trojan Horse method NUCLEAR REACTIONS 2H(10B, α7Be), E=24.5 MeV; measured particle spectra by ΔE-E method using ionization chambers and position-sensitive detectors at LNS-Catania accelerator facility; analyzed data by Trojan Horse method (THM); deduced Eα-Be and Eα-n two-dimensional plots, experimental momentum distribution and its comparison with DWBA and PWIA calculations, THM bare nucleus astrophysical S(E) factors using R-matrix formalism for 5-100 keV resonances in 11C, dominated by 10-keV resonance corresponding to 8699-keV, 5/2+ level in 11C. 11C; deduced widths of three resonances.
doi: 10.1103/PhysRevC.90.035801
2013IZ01 Phys.Rev. C 88, 065808 (2013) R.Izsak, A.Horvath, A.Kiss, Z.Seres, A.Galonsky, C.A.Bertulani, Zs.Fulop, T.Baumann, D.Bazin, K.Ieki, C.Bordeanu, N.Carlin, M.Csanad, F.Deak, P.DeYoung, N.Frank, T.Fukuchi, A.Gade, D.Galaviz, C.R.Hoffman, W.A.Peters, H.Schelin, M.Thoennessen, G.I.Veres Determining the 7Li(n, γ) cross section via Coulomb dissociation of 8Li NUCLEAR REACTIONS C, Pb(8Li, n), [8Li secondary beam from 9Be(18O, X), E=120 MeV/nucleon primary reaction], E=69.5 MeV/nucleon; 8Li(γ, n)7Li, [γ from 8Li beam impinging on C and Pb targets], E(8Li)=69.5 MeV/nucleon; measured TOF, position and angle of 8Li particles, neutron spectra from Coulomb dissociation of 8Li, E(n), I(n) using MONA neutron detector array at NSCL-MSU cyclotron facility; reconstructed neutron 7Li energy spectra and momentum vectors; deduced σ(E) for 7Li(n, γ)8Li reaction. Surrogate method. Comparison of σ with previous experimental results, and with low-energy effective field theory calculations.
doi: 10.1103/PhysRevC.88.065808
2012LA01 J.Phys.(London) G39, 015106 (2012) L.Lamia, C.Spitaleri, V.Burjan, N.Carlin, S.Cherubini, V.Crucilla, M.G.Munhoz, M.G.Del Santo, M.Gulino, Z.Hons, G.G.Kiss, V.Kroha, S.Kubono, M.La Cognata, C.Li, J.Mrazek, A.Mukhamedzhanov, R.G.Pizzone, S.M.R.Puglia, Q.Wen, G.G.Rapisarda, C.Rolfs, S.Romano, M.L.Sergi, E.Somorjai, F.A.Souza, A.Szanto de Toledo, G.Tabacaru, A.Tumino, Y.Wakabayashi, H.Yamaguchi, S.-H.Zhou New measurement of the 11B(p, α0)8Be bare-nucleus S(E) factor via the Trojan horse method NUCLEAR REACTIONS 2H(11B, α), E=27 MeV; measured reaction products, Eα, Iα. 8Be; deduced σ(θ), S-factors.
doi: 10.1088/0954-3899/39/1/015106
2011BE19 Int.J.Mod.Phys. E20, 943 (2011) C.Beck, N.Rowley, P.Papka, S.Courtin, M.Rousseau, F.A.Souza, N.Carlin, F.Liguori Neto, M.M.De Moura, M.G.Del Santo, A.A.I.Suade, M.G.Munhoz, E.M.Szanto, A.Szanto de Toledo, N.Keeley, A.Diaz-Torres, K.Hagino Cluster model for reactions induced by weakly bound and/or exotic halo nuclei with medium-mass targets
doi: 10.1142/S0218301311019027
2011OL01 Nucl.Phys. A856, 46 (2011) R.A.N.Oliveira, N.Carlin, R.Liguori Neto, M.M.de Moura, M.G.Munhoz, M.G.del Santo, F.A.Souza, E.M.Szanto, A.Szanto de Toledo, A.A.P.Suaide Study of 9Be+ 12C elastic scattering at energies near the Coulomb barrier NUCLEAR REACTIONS 12C(9Be, 9Be), (9Be, X), E=13.0, 14.5, 17.3, 19.0, 21.0 MeV; measured E(particle), I(particle, θ); deduced σ(θ), deformation parameters; calculated σ(θ), M(Eλ) using FRESCO optical model code with Sao Paulo parameters and including also cluster transfer.
doi: 10.1016/j.nuclphysa.2011.02.005
2010BE22 Nucl.Phys. A834, 440c (2010) C.Beck, N.Rowley, P.Papka, S.Courtin, M.Rousseau, F.A.Souza, N.Carlin, R.Liguori Neto, M.M.de Moura, M.G.Del Santo, A.A.P.Suaide, M.G.Munhoz, E.M.Szanto, A.Szanto de Toledo, N.Keeley, A.Diaz-Torres, K.Hagino Reaction mechanisms for weakly-bound, stable nuclei and unstable, halo nuclei on medium-mass targets NUCLEAR REACTIONS 59Co(6Li, X), E=10-40 MeV; calculated evaporation residue σ, σ(θ). 58Ni(7Be, 7Be), E=15.09, 17.13, 18.53, 19.93, 21.43 MeV; calculated σ(θ). Discussed interplay of different processes and systematics of reaction mechanism. Comparison with data.
doi: 10.1016/j.nuclphysa.2010.01.059
2010LA11 Nucl.Phys. A834, 655c (2010) L.Lamia, S.M.R.Puglia, C.Spitaleri, S.Romano, M.G.Del Santo, N.Carlin, M.G.Munhoz, S.Cherubini, G.G.Kiss, V.Kroha, S.Kubono, M.La Cognata, C.-B.Li, R.G.Pizzone, Q.-G.Wen, M.L.Sergi, A.Szanto de Toledo, Y.Wakabayashi, H.Yamaguchi, S.-H.Zhou Indirect study of 11B(p, α0)8Be and 10B(p, α)7Be reactions at astrophysical energies by means of the Trojan Horse Method: recent results NUCLEAR REACTIONS 2H(11B, α8Be), E=27 MeV; 2H(10B, α7Be), E=24.4 MeV; measured Eα, Iα(θ), E(particle), I(particle). 11B(p, α), E(cm)=0-0.6 MeV; 10B(p, α), E(cm)=0-0.15 MeV; deduced S-factor using Trojan Horse Method.
doi: 10.1016/j.nuclphysa.2010.01.115
2010PI09 Nucl.Phys. A834, 673c (2010) R.G.Pizzone, C.Spitaleri, S.Cherubini, M.La Cognata, L.Lamia, S.Romano, M.L.Sergi, A.Tumino, C.Li, Q.Wen, S.Zhou, V.Burjan, V.Kroha, J.Mrazek, N.Carlin, M.G.del Santo, A.Szanto de Toledo, S.Kubono, T.Wakabayashi, H.Yamaguchi, C.Rolfs Trojan Horse Method: a useful tool for electron screening effect investigation NUCLEAR REACTIONS 2H(3He, p), 6Li(p, α), 6Li(d, α), 7Li(p, α), 9Be(p, α), E not given; calculated electron screening effect with Trojan Horse Method.
doi: 10.1016/j.nuclphysa.2010.01.121
2010SO14 Eur.Phys.J. A 44, 181 (2010) F.A.Souza, N.Carlin, C.Beck, N.Keeley, A.Diaz-Torres, R.Liguori Neto, C.Siqueira-Mello, M.M.de Moura, M.G.Munhoz, R.A.N.Oliveira, M.G.Del Santo, A.A.P.Suaide, E.M.Szanto, A.Szanto de Toledo Projectile breakup dynamics for 6Li + 59Co: Kinematical analysis of α - d coincidences NUCLEAR REACTIONS 59Co(6Li, X), E=29.6 MeV; measured p-spectra, d-spectra, α-spectra, αd-coin; deduced σ, σ(θ), breakup reaction mechanism features. Comparison with CDCC model.
doi: 10.1140/epja/i2010-10940-0
2010SO16 Nucl.Phys. A834, 420c (2010) F.A.Souza, N.Carlin, C.Beck, N.Keeley, A.Diaz-Torres, R.Liguori Neto, C.Siqueira-Mello, M.M.de Moura, M.G.Munhoz, R.A.N.Oliveira, M.G.Del Santo, A.A.P.Suaide, E.M.Szanto, A.Szanto de Toledo 6Li direct breakup lifetimes NUCLEAR REACTIONS 59Co(6Li, dα), E=29.6 MeV; measured Eα, Iα(θ), Ed, Id(θ), dα-coin; deduced σ(θ), direct breakup T1/2; calculated T1/2. Discussed breakup reaction mechanism features.
doi: 10.1016/j.nuclphysa.2010.01.054
2009SO04 Nucl.Phys. A821, 36 (2009) F.A.Souza, C.Beck, N.Carlin, N.Keeley, R.Liguori Neto, M.M.de Moura, M.G.Munhoz, M.G.Del Santo, A.A.P.Suaide, E.M.Szanto, A.Szanto de Toledo Reaction mechanisms in the 6Li + 59Co system NUCLEAR REACTIONS 59Co(6Li, X), E=17.4, 21.5, 25.5, 29.6 MeV; measured p-spectra, d-spectra, α-spectra, αd-coin; deduced total α and deuteron production σ and reaction mechanism features using different reaction models.
doi: 10.1016/j.nuclphysa.2009.02.009
2008LA18 Nuovo Cim. B 31, 423 (2008) L.Lamia, C.Spitaleri, N.Carlin, S.Cherubini, M.G.Del Santo, M.Gulino, M.La Cognata, M.G.Munhoz, R.G.Pizzone, S.M.R.Puglia, G.G.Rapisarda, S.Romano, M.L.Sergi, A.Szanto de Toledo, S.Tudisco, A.Tumino Indirect study of (p, α) and (n, α) reactions induced on boron isotopes NUCLEAR REACTIONS 2H(11B, nα), (10B, pα), E=27 MeV; measured Eα, Iα, fragment spectra, cross sections. 11B(p, α), 10B(n, α); deduced S-factors.
doi: 10.1393/ncc/i2009-10303-2
2008RO05 J.Phys.(London) G35, 014008 (2008) S.Romano, C.Spitaleri, S.Cherubini, V.Crucilla, M.Gulino, M.La Cognata, L.Lamia, R.G.Pizzone, S.M.R.Puglia, G.G.Rapisarda, M.L.Sergi, S.Tudisco, A.Tumino, R.E.Tribble, V.Z.Goldberg, A.M.Mukhamedzhanov, G.Tabacaru, L.Trache, V.Kroha, V.Burjan, Z.Hons, J.Mrazek, E.Somorjai, Z.Elekes, Z.Fulop, G.Gyurky, G.Kiss, A.Szanto de Toledo, N.Carlin, M.M.De Moura, M.G.Del Santo, M.G.Munhoz, R.Liguori Neto, F.A.Souza, A.A.P.Suaide, E.Szanto The Trojan horse method in nuclear astrophysics: recent results NUCLEAR REACTIONS 7Li(p, α)α, E(cm)=0-7 MeV; 10B(p, α)7Be, E(cm)=0-400 keV; p(p, p)p, E ≈ 0-0.6 MeV; analyzed cross section, S-factors.Trojan Horse Method.
doi: 10.1088/0954-3899/35/1/014008
2007LA25 Nucl.Phys. A787, 309c (2007) L.Lamia, S.Romano, N.Carlin, S.Cherubini, V.Crucilla, M.M.De Moura, M.G.Del Santo, M.G.Munhoz, M.Gulino, R.Liguori Neto, M.La Cognata, F.Mudo, R.G.Pizzone, S.M.R.Puglia, M.L.Sergi, F.A.Souza, C.Spitaleri, A.A.P.Suaide, E.Szanto, A.Szanto de Toledo, S.Tudisco, A.Tumino Boron depletion: indirect measurement of the 10B(p, α)7Be S(E)-factor NUCLEAR REACTIONS 2H(10B, nα), E=27 MeV; measured Eα, Iα, σ; deduced astrophysical S-factor. Trojan horse method, three-body process.
doi: 10.1016/j.nuclphysa.2006.12.049
2007SO09 Phys.Rev. C 75, 044601 (2007), Erratum Phys.Rev. C 76, 029901 (2007) F.A.Souza, L.A.S.Leal, N.Carlin, M.G.Munhoz, R.Liguori Neto, M.M.de Moura, A.A.P.Suaide, E.M.Szanto, A.Szanto de Toledo, J.Takahashi Effect of breakup on elastic scattering for the 6, 7Li + 59Co systems NUCLEAR REACTIONS 59Co(6Li, 6Li), (7Li, 7Li), E=12-30 MeV; measured elastic σ(θ); deduced breakup threshold anomaly. NUCLEAR STRUCTURE 208Pb; calculated binding energy, neutron and proton radii, sensitivity to coupling corrections. Relativistic mean field theory.
doi: 10.1103/PhysRevC.75.044601
2007WE01 Nucl.Phys. A781, 342 (2007); Erratum Nucl.Phys. A794, 231 (2007) J.C.Werner, L.A.S.Leal, M.G.Munhoz, N.Carlin, L.C.Chamon, N.Added, J.A.P.Brage, R.Liguori Neto, M.M.Coimbra, M.M.de Moura, F.A.Souza, A.A.P.Suaide, E.M.Szanto, A.Szanto de Toledo, J.Takahashi Structure effects in the elastic scattering for the 16O + 46, 50Ti systems NUCLEAR REACTIONS 46,50Ti(16O, 16O), E=30-70 MeV; measured elastic σ(θ); deduced model parameters, threshold anomaly. Unexpected structure effects not observed.
doi: 10.1016/j.nuclphysa.2006.11.034
2006HO14 Eur.Phys.J. A 27, Supplement 1, 217 (2006) A.Horvath, K.Ieki, A.Kiss, A.Galonsky, M.Thoennessen, T.Baumann, D.Bazin, C.A.Bertulani, C.Bordeanu, N.Carlin, M.Csanad, F.Deak, P.DeYoung, N.Frank, T.Fukuchi, Zs.Fulop, A.Gade, D.Galaviz, C.Hoffman, R.Izsak, W.A.Peters, H.Schelin, A.Schiller, R.Sugo, Z.Seres, G.I.Veres Can the neutron-capture cross sections be measured with Coulomb dissociation? NUCLEAR REACTIONS C, Pb(8Li, n7Li), E=41 MeV/nucleon; measured particle spectra, angular distributions; deduced nuclear and Coulomb contributions.
doi: 10.1140/epja/i2006-08-033-6
2006PE26 Phys.Rev. C 74, 034608 (2006) D.Pereira, E.S.Rossi, Jr., G.P.A.Nobre, L.C.Chamon, C.P.Silva, L.R.Gasques, M.A.G.Alvarez, R.V.Ribas, J.R.B.Oliveira, N.H.Medina, M.N.Rao, E.W.Cybulska, W.A.Seale, N.Carlin, P.R.S.Gomes, J.Lubian, R.M.Anjos 18O+110Pd: Measurements and realistic coupled-channel analysis in a transitional region NUCLEAR REACTIONS 110Pd(18O, 18O'), (18O, 16O), (18O, 14C), E=40-58 MeV; measured Eγ, Iγ, (particle)γ-coin; deduced excitation functions. Coupled-channels analysis.
doi: 10.1103/PhysRevC.74.034608
2005SO14 Braz.J.Phys. 35, 888 (2005) F.A.Souza, R.Liguori Neto, M.M.de Moura, M.G.Munhoz, A.A.P.Suaide, E.M.Szanto, J.Takahashi, A.Szanto de Toledo, N.Carlin Direct Measurement of the Breakup Process NUCLEAR REACTIONS 12C(6Li, dα), E=26 MeV; 59Co(6Li, dα), E=30 MeV; measured particle spectra, σ(θ(α), θ(d)), three-body final state correlations; deduced reaction mechanism features.
doi: 10.1590/S0103-97332005000500046
2004DA23 Phys.Rev. C 70, 024606 (2004) M.Dasgupta, P.R.S.Gomes, D.J.Hinde, S.B.Moraes, R.M.Anjos, A.C.Berriman, R.D.Butt, N.Carlin, J.Lubian, C.R.Morton, J.O.Newton, A.Szanto de Toledo Effect of breakup on the fusion of 6Li, 7Li, and 9Be with heavy nuclei NUCLEAR REACTIONS 209Bi(6Li, X)213Rn/212Rn/211Rn/210Rn/213At/212At/211At/212Po/211Po/210Po, E=26-48 MeV; 209Bi(7Li, X)214Rn/213Rn/212Rn/211Rn/213At/212At/211At/212Po/211Po/210Po/211Bi, E=26-52 MeV; 208Pb(9Be, X)215Rn/214Rn/213Rn/212Rn/212Po/211Po/210Po, E=36-51 MeV; measured fission, complete and incomplete fusion σ; deduced barrier distributions, breakup effects, other reaction mechanism features.
doi: 10.1103/PhysRevC.70.024606
2004SO23 Prog.Theor.Phys.(Kyoto), Suppl. 154, 101 (2004) F.A.Souza, N.Carlin, P.Miranda, M.M.de Moura, M.G.Munhoz, A.A.P.Suaide, E.M.Szanto, J.Takahashi, A.Szanto de Toledo Study of the Influence of Projectile Breakup on the Fusion Cross Section of 6, 7Li + 12C, 59Co NUCLEAR REACTIONS 59Co(6Li, X), (7Li, X), E=12-30 MeV; measured fusion excitation functions; 12C(6Li, dα), (7Li, tα), E ≈ 30 MeV; measured particle spectra, angular correlations; deduced breakup contribution to fusion, related reaction mechanism features.
doi: 10.1143/PTPS.154.101
2004SO36 Braz.J.Phys. 34, 907 (2004) F.A.Souza, A.Szanto de Toledo, M.G.Munhoz, J.Takahashi, N.Carlin, A.A.P.Suaide, M.M.de Moura, e.M.Szanto Study of the Effect of the Breakup on the Fusion Cross Section of the Systems 6, 7Li+59Co NUCLEAR REACTIONS 59Co(6Li, X), (7Li, X), E=12-26 MeV; measured fusion σ; deduced breakup effects. 59Co(6Li, dα), E=26 MeV; measured Eα, Ed, dα-coin.
doi: 10.1590/S0103-97332004000500054
2004SU02 Phys.Lett. B 579, 271 (2004) A.A.P.Suaide, M.M.de Moura, N.Adde, N.N.Ajitanand, N.Carlin, M.G.Munhoz, F.A.Souza, E.M.Szanto, J.Takahashi, A.Szanto de Toledo Dynamics of light heavy-ion reactions in the framework of their time scales NUCLEAR REACTIONS 10B(16O, X), E(cm)=24 MeV; 12C(16O, X), E(cm)=27.4 MeV; measured particle spectra, correlations; deduced sequential particle emission time scale. 10B(16O, X), E(cm)=17-25 MeV; 12C(19F, X), E(cm)=22-24 MeV; measured excitation functions; deduced compound nucleus lifetime features.
doi: 10.1016/j.physletb.2003.11.012
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
2003CA39 Phys.Rev. C 68, 054614 (2003) W.H.Z.Cardenas, L.F.Canto, N.Carlin, R.Donangelo, M.S.Hussein Interplay of static and dynamic effects in 6He + 238U fusion NUCLEAR REACTIONS 238U(α, X), (6He, X), E(cm)=15-35 MeV; calculated fusion σ, role of neutron halo and breakup channel effects.
doi: 10.1103/PhysRevC.68.054614
2003HO22 Nucl.Phys. A719, 9c (2003) A.Horvath, A.Galonsky, N.Carlin, F.Deak, T.Gomi, V.Guimaraes, Y.Higurashi, K.Hiroshi, K.Ieki, Y.Iwata, A.Kiss, J.Kolata, T.Rauscher, H.Schelin, J.von Schwarzenberg, Z.Seres, S.Takeuchi, S.Typel, R.Warner, J.Weiner Measurements of astrophysical neutron capture cross sections via the inverse reaction NUCLEAR REACTIONS C, Al, Cu, Sn, Pb(15C, nX), E=35 MeV/nucleon; C, Al, Cu, Sn, Pb(9Li, nX), E=40 MeV/nucleon; measured neutron spectra, (fragment)(neutron)-coin, dissociation yields. 8Li, 14C(n, γ), E=low; deduced astrophysical reaction rates.
doi: 10.1016/S0375-9474(03)00951-5
2003KO07 Phys.Rev. C 67, 015806 (2003) H.Kobayashi, K.Ieki, A.Horvath, A.Galonsky, N.Carlin, F.Deak, T.Gomi, V.Guimaraes, Y.Higurashi, Y.Iwata, A.Kiss, J.J.Kolata, T.Rauscher, H.Schelin, Z.Seres, R.Warner Astrophysical reaction rate for the 8Li(n, γ)9Li reaction NUCLEAR REACTIONS Pb(9Li, n8Li), E=39.7 MeV/nucleon; measured neutron and lithium spectra. 8Li(n, γ), E not given; deduced σ, astrophysical reaction rate upper limits. Comparison with previous results.
doi: 10.1103/PhysRevC.67.015806
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
2003SZ14 Braz.J.Phys. 33, 320 (2003) A.Szanto de Toledo, M.G.Munhoz, J.Takahashi, F.A.Souza, E.E.Alonso, N.Carlin, R.Liguori Neto, M.M.Moura, A.A.Suaide, E.M.Szanto Is the Inhibition/Enhancement of Fusion Due to Breakup Still a Puzzle? NUCLEAR REACTIONS 59Co(6Li, X), (7Li, X), E(cm) ≈ 10-26 MeV; analyzed fusion σ, breakup channel contributions.
doi: 10.1590/s0103-97332003000200031
2002DA23 Phys.Rev. C66, 041602 (2002) M.Dasgupta, D.J.Hinde, K.Hagino, S.B.Moraes, P.R.S.Gomes, R.M.Anjos, R.D.Butt, A.C.Berriman, N.Carlin, C.R.Morton, J.O.Newton, A.Szanto de Toledo Fusion and breakup in the reactions of 6Li and 7Li nuclei with 209Bi NUCLEAR REACTIONS 209Bi(6Li, X), (7Li, X), E(cm)=25-50 MeV; measured fusion, incomplete fusion, and fission excitation functions; deduced reaction mechanism features. Classical trajectory model.
doi: 10.1103/PhysRevC.66.041602
2002SU17 Phys.Rev. C66, 014607 (2002) A.A.P.Suaide, N.Added, N.Aissaoui, E.E.Alonso, W.H.Z.Cardenas, R.J.Fujii, M.M.de Moura, M.G.Munhoz, F.A.Souza, E.M.Szanto, A.Szanto de Toledo, N.Carlin, M.Papa Time Scales for Binary Processes from Light Heavy-Ion Reactions NUCLEAR REACTIONS 10B(16O, 16O), E=44-65 MeV; measured σ(θ). 10B(16O, 12C), E=44-65 MeV; 12C(19F, 12C), (19F, 15N), E=57-64 MeV; measured binary decay excitation functions, widths, σ(θ); deduced time scales, other reaction mechanism features.
doi: 10.1103/PhysRevC.66.014607
2001DE50 Nucl.Phys. A696, 64 (2001) M.M.de Moura, A.A.P.Suaide, N.Added, E.E.Alonso, W.H.Z.Cardenas, R.J.Fujii, M.G.Munhoz, F.A.Souza, E.M.Szanto, A.Szanto de Toledo, J.Takahashi, N.Carlin, N.N.Ajitanand Light Heavy-Ion Reactions: Time scales and emission order of light products NUCLEAR REACTIONS 10B(16O, X), E=62.5 MeV; 12C(16O, X), E=64.0 MeV; measured fragments charge distributions, angular correlations, emission time scales, velocities. Comparison with three-body trajectory Monte Carlo simulation.
doi: 10.1016/S0375-9474(01)01126-5
2000SZ06 Nucl.Phys. A679, 175 (2000) A.Szanto de Toledo, N.Added, W.H.Z.Cardenas, N.Carlin, M.M.de Moura, M.G.Munhoz, A.A.P.Suaide, E.M.Szanto, J.Takahashi Fusion Hindrance in Light Nuclear Systems: Binding energy and/or surface diffuseness effect ? NUCLEAR STRUCTURE Z=3-13; analyzed fusion barrier features; deduced fusion inhibition factor for light systems.
doi: 10.1016/S0375-9474(00)00346-8
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
1999CA50 Phys.Rev. C60, 067602 (1999) R.Cabezas, E.M.Szanto, N.Carlin, N.Added, A.A.P.Suaide, M.M.de Moura, M.Munhoz, R.Liguori Neto, J.Takahashi, R.M.dos Anjos, W.H.Z.Cardenas, A.Szanto de Toledo ' Elastic Fission ' of Very Light Nuclear Systems NUCLEAR REACTIONS 10,11B(9Be, X), (16O, X), (17O, X), (18O, X), 11B(10B, X), 12C(11B, X), (19F, X), E(cm) ≈ 19-56 MeV; measured elastic fission yields; deduced geometrical effects, other reaction mechanism features. Other data analyzed.
doi: 10.1103/PhysRevC.60.067602
1999DA07 Phys.Rev.Lett. 82, 1395 (1999) M.Dasgupta, D.J.Hinde, R.D.Butt, R.M.Anjos, A.C.Berriman, N.Carlin, P.R.S.Gomes, C.R.Morton, J.O.Newton, A.Szanto de Toledo, K.Hagino Fusion Versus Breakup: Observation of large fusion suppression for 9Be + 208Pb NUCLEAR REACTIONS 208Pb(9Be, X), E=35-51 MeV; measured complete, incomplete fusion σ; deduced projectile breakup effects.
doi: 10.1103/PhysRevLett.82.1395
1999PH01 Phys.Rev. C60, 054617 (1999) L.Phair, L.Beaulieu, L.G.Moretto, G.J.Wozniak, D.R.Bowman, N.Carlin, L.Celano, N.Colonna, J.D.Dinius, A.Ferrero, C.K.Gelbke, T.Glasmacher, F.Gramegna, D.O.Handzy, W.C.Hsi, M.J.Huang, I.Iori, Y.D.Kim, M.A.Lisa, W.G.Lynch, G.V.Margagliotti, P.F.Mastinu, P.M.Milazzo, C.P.Montoya, A.Moroni, G.F.Peaslee, R.Rui, C.Schwarz, M.B.Tsang, K.Tso, G.Vannini, F.Zhu Statistical Interpretation of the Correlation between Intermediate Mass Fragment Multiplicity and Transverse Energy NUCLEAR REACTIONS 197Au(129Xe, X), E=30, 40, 50, 60 MeV/nucleon; measured light charged particles, intermediate mass fragments yields, multiplicities, transverse energies. Comparison with statistical model predictions.
doi: 10.1103/PhysRevC.60.054617
1999SZ03 Pramana 53, 483 (1999) A.Szanto de Toledo, N.Carlin, N.Added, E.M.Szanto, M.G.Munhoz, J.Takahashi, A.Suaide, M.M.de Moura Fusion-Fission of Light Nuclear Systems
1998SH04 Phys.Rev. C57, 1508 (1998) W.Q.Shen, M.B.Tsang, N.Carlin, R.J.Charity, J.Feng, C.K.Gelbke, W.C.Hsi, M.J.Huang, G.J.Kunde, M.-C.Lemaire, M.A.Lisa, W.G.Lynch, U.Lynen, Y.G.Ma, G.F.Peaslee, L.Phair, J.Pochodzalla, H.Sann, C.Schwarz, L.G.Sobotka, R.T.de Souza, S.R.Souza, W.Trautmann, C.Williams Disappearance of Rotational Flow and Reaction Plane Dispersions in Kr + Au Collisions NUCLEAR REACTIONS 197Au(84Kr, X), E=35, 55, 70, 100 MeV/nucleon; measured light charged particle σ(θ), dd(θ), tt(θ), αα(θ); deduced rotational flow energy dependence. 4π phoswich detector array.
doi: 10.1103/PhysRevC.57.1508
1998ZE06 Phys.Rev. C58, 3445 (1998) A.Zerwekh, R.Liguori Neto, N.Added, J.C.Acquadro, N.Carlin, M.Frizzarini, F.Malandrino, J.Lubian, R.Cabezas, P.R.S.Gomes, R.M.Anjos, G.M.Santos, A.M.M.Maciel, C.Muri, S.B.Moraes, G.Ramirez, C.Tenreiro Elastic Scattering of 27Al + 27Al at Near Barrier Energies NUCLEAR REACTIONS 27Al(27Al, 27Al), (27Al, 27Al'), E=50-70 MeV; measured σ(θ), integrated σ; deduced optical model parameters.
doi: 10.1103/PhysRevC.58.3445
1997LI15 Phys.Rev. C56, 250 (1997) I.Licot, N.Added, N.Carlin, G.M.Crawley, S.Danczyk, J.Finck, D.Hirata, H.Laurent, D.J.Morrissey, M.M.de Moura, H.R.Schelin, J.Stasko, M.Steiner, A.A.P.Suaide, A.Szanto de Toledo, E.M.Szanto, M.Thoennessen, J.A.Winger Reaction Cross Sections and Radii for f-p Shell Exotic Neutron-Rich Nuclei NUCLEAR REACTIONS, ICPND Si(41Ar, X), (42Ar, X), (43Ar, X), (44Ar, X), (45Ar, X), (46Ar, X), (44K, X), (45K, X), (46K, X), (47K, X), (48K, X), (49K, X), (46Ca, X), (47Ca, X), (48Ca, X), (49Ca, X), (50Ca, X), (51Ca, X), (49Sc, X), (50Sc, X), (51Sc, X), (52Sc, X), (53Sc, X), E=52-69 MeV/nucleon; measured reaction σ. 41,42,43,44,45,46Ar, 44,45,46,47,48,49K, 46,47,48,49,50,51Ca, 49,50,51,52,53Sc deduced strong absorption radii, neutron separation energies. Comparison to Glauber model, RMF theory.
doi: 10.1103/PhysRevC.56.250
1997TA01 Phys.Rev.Lett. 78, 30 (1997) J.Takahashi, M.Munhoz, E.M.Szanto, N.Carlin, N.Added, A.A.P.Suaide, M.M.de Moura, R.Liguori Neto, A.Szanto de Toledo, L.F.Canto Is Fusion Inhibited for Weakly Bound Nuclei ( Question ) NUCLEAR REACTIONS 12C, 9Be(6Li, X), (7Li, X), E=6-33 MeV; measured evaporation residue spectra; deduced fusion probability vs E, effective separation energy.
doi: 10.1103/PhysRevLett.78.30
1997TS02 Phys.Rev. C55, R557 (1997) M.B.Tsang, C.Williams, M.J.Huang, W.G.Lynch, L.Phair, D.R.Bowman, J.Dinius, C.K.Gelbke, D.O.Handzy, W.C.Hsi, G.J.Kunde, M.A.Lisa, G.F.Peaslee, A.Botvina, M.-C.Lemaire, S.R.Souza, G.Van Buren, R.J.Charity, L.G.Sobotka, C.Schwarz, U.Lynen, J.Pochodzalla, H.Sann, W.Trautmann, D.Fox, R.T.de Souza, N.Carlin Fragment Multiplicity Dependent Charge Distributions in Heavy Ion Collisions NUCLEAR REACTIONS 197Au(84Kr, X), E=35-400 MeV/nucleon; measured intermediate mass fragment element distributions dependence on the multiplicity of detected fragments.
doi: 10.1103/PhysRevC.55.R557
1997WI06 Phys.Rev. C55, R2132 (1997); Comment Phys.Rev. C59, 550 (1999) C.Williams, W.G.Lynch, C.Schwarz, M.B.Tsang, W.C.Hsi, M.J.Huang, D.R.Bowman, J.Dinius, C.K.Gelbke, D.O.Handzy, G.J.Kunde, M.A.Lisa, G.F.Peaslee, L.Phair, A.Botvina, M.-C.Lemaire, S.R.Souza, G.Van Buren, R.J.Charity, L.G.Sobotka, U.Lynen, J.Pochodzalla, H.Sann, W.Trautmann, D.Fox, R.T.de Souza, N.Carlin Fragment Distributions for Highly Charged Systems NUCLEAR REACTIONS 197Au(Kr, X), E=35, 55, 70, 100, 200, 400 MeV/nucleon; measured fragment charge distributions, mean transverse energy < E(t) >, rotational energy; deduced radial expansion velocities. Statistical model.
doi: 10.1103/PhysRevC.55.R2132
1996HU10 Phys.Rev.Lett. 77, 3739 (1996) M.J.Huang, R.C.Lemmon, F.Daffin, W.G.Lynch, C.Schwarz, M.B.Tsang, C.Williams, P.Danielewicz, K.Haglin, W.Bauer, N.Carlin, R.J.Charity, R.T.de Souza, C.K.Gelbke, W.C.Hsi, G.J.Kunde, M.-C.Lemaire, M.A.Lisa, U.Lynen, G.F.Peaslee, J.Pochodzalla, H.Sann, L.G.Sobotka, S.R.Souza, W.Trautmann Mass Dependence of Directed Collective FLow NUCLEAR REACTIONS 197Au(84Kr, X), E=200 MeV/nucleon; measured fragment collective sidewards flow per nucleon mass dependence; deduced momentum dependent nuclear mean field evidence. BUU model.
doi: 10.1103/PhysRevLett.77.3739
1996MO02 Phys.Rev.Lett. 76, 372 (1996) L.G.Moretto, L.Phair, R.Ghetti, K.Tso, N.Colonna, W.Skulski, G.J.Wozniak, D.R.Bowman, N.Carlin, M.Chartier, C.K.Gelbke, W.G.Gong, W.C.Hsi, Y.D.Kim, M.A.Lisa, W.G.Lynch, G.F.Peaslee, C.Schwarz, R.T.de Souza, M.B.Tsang, F.Zhu Phase Coexistence in Multifragmentation ( Question ) NUCLEAR REACTIONS 197Au(36Ar, X), E=110 MeV/nucleon; analyzed charge distributions data; deduced multi-fragmentation phase coexistence related features.
doi: 10.1103/PhysRevLett.76.372
1996MO18 Phys.Rev.Lett. 77, 2634 (1996) L.G.Moretto, Th.Rubehn, L.Phair, N.Colonna, G.J.Wozniak, D.R.Bowman, G.F.Peaslee, N.Carlin, R.T.de Souza, C.K.Gelbke, W.G.Gong, Y.D.Kim, M.A.Lisa, W.G.Lynch, C.Williams Charge Correlations and Dynamical Instabilities in the Multifragment Emission Process NUCLEAR REACTIONS Cu(Xe, X), E at 50 MeV/nucleon; measured multi-fragmentation associated higher order charge correlations; deduced no evidence for preferred breakup into equal-sized fragments.
doi: 10.1103/PhysRevLett.77.2634
1996PH03 Phys.Rev.Lett. 77, 822 (1996) L.Phair, L.G.Moretto, G.J.Wozniak, R.T.de Souza, D.R.Bowman, N.Carlin, C.K.Gelbke, W.G.Gong, Y.D.Kim, M.A.Lisa, W.G.Lynch, G.F.Peaslee, M.B.Tsang, F.Zhu Reducibility and Thermal and Mass Scaling in Angular Correlations from Multifragmentation Reactions NUCLEAR REACTIONS 197Au(36Ar, X), E=50 MeV/nucleon; analyzed light charged particle azimuthal correlations data; deduced reducibility, thermal, mass scaling related features.
doi: 10.1103/PhysRevLett.77.822
1995MO09 Phys.Rev.Lett. 74, 1530 (1995) L.G.Moretto, L.Phair, K.Tso, K.Jing, G.J.Wozniak, R.T.de Souza, D.R.Bowman, N.Carlin, C.K.Gelbke, W.G.Gong, Y.D.Kim, M.A.Lisa, W.G.Lynch, G.F.Peaslee, M.B.Tsang, F.Zhu Are Multifragment Emission Probabilities Reducible to an Elementary Binary Emission Probability NUCLEAR REACTIONS 197Au(36Ar, X), E=80, 110 MeV/nucleon; measured intermediate mass fragment distribution multiplicity; deduced emission probability characteristics, consequences.
doi: 10.1103/PhysRevLett.74.1530
1995MU04 Nucl.Phys. A587, 367 (1995) J.T.Murgatroyd, S.J.Bennett, N.M.Clarke, B.R.Fulton, G.J.Gyapong, C.D.Jones, D.L.Watson, T.M.Cormier, H.Dejbakhsh, A.Szanto de Toledo, N.Carlin Termination of the 12C-12C Cluster States Revealed in the 12C)(20Ne, 12C12C)8Be Breakup Reaction NUCLEAR REACTIONS 12C(20Ne, 212C), E=300 MeV; measued (12C)(12C)-coin. 24Mg deduced energies of breakup states.
doi: 10.1016/0375-9474(95)00003-J
1995PH03 Phys.Rev.Lett. 75, 213 (1995) L.Phair, K.Tso, R.Ghetti, G.J.Wozniak, L.G.Moretto, R.T.de Souza, D.R.Bowman, N.Carlin, C.K.Gelbke, W.G.Gong, Y.D.Kim, M.A.Lisa, W.G.Lynch, G.F.Peaslee, M.B.Tsang, F.Zhu Reducibility and Thermal Scaling of Charge Distributions in Multifragmentation NUCLEAR REACTIONS 197Au(36Ar, X), E=110 MeV/nucleon; calculated multi-fragmentation charge distribution; deduced reducibility, thermal scaling.
doi: 10.1103/PhysRevLett.75.213
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
1994FO11 Phys.Rev. C50, 2424 (1994) D.Fox, R.T.de Souza, T.Glasmacher, L.Phair, D.R.Bowman, N.Carlin, C.K.Gelbke, W.G.Gong, Y.D.Kim, M.A.Lisa, W.G.Lynch, G.F.Peaslee, M.B.Tsang, F.Zhu Time Scale for Multifragmentation in Intermediate Energy Heavy-Ion Reactions NUCLEAR REACTIONS 197Au(36Ar, X), E=35-110 MeV/nucleon; measured (fragment)(fragment) correlation vs Z1, Z2, σ(fragment E, θ), other aspects; deduced multi-fragmentation time scale features. Microcanonical model.
doi: 10.1103/PhysRevC.50.2424
1994LI19 Phys.Rev. C49, 2788 (1994) M.A.Lisa, W.G.Gong, C.K.Gelbke, N.Carlin, R.T.de Souza, Y.D.Kim, W.G.Lynch, T.Murakami, G.Poggi, M.B.Tsang, H.M.Xu, K.Kwiatkowski, V.E.Viola, Jr., S.J.Yennello Proton Evaporation Time Scales from Longitudinal and Transverse Two-Proton Correlation Functions NUCLEAR REACTIONS 27Al(129Xe, X), E=31 MeV/nucleon; analyzed pp-correlations data; deduced evidence for emission from long-lived composite system.
doi: 10.1103/PhysRevC.49.2788
1994MO34 Phys.Rev.Lett. 73, 3070 (1994) C.P.Montoya, W.G.Lynch, D.R.Bowman, G.F.Peaslee, N.Carlin, R.T.de Souza, C.K.Gelbke, W.G.Gong, Y.D.Kim, M.A.Lisa, L.Phair, M.B.Tsang, J.B.Webster, C.Williams, N.Colonna, K.Hanold, M.A.McMahan, G.J.Wozniak, L.G.Moretto Fragmentation of Necklike Structures NUCLEAR REACTIONS Cu(129Xe, X), E=49.8 MeV/nucleon; measured intermediate mass fragment yield vs velocity; deduced necklike structure role in emission.
doi: 10.1103/PhysRevLett.73.3070
1994PE06 Phys.Rev. C49, R2271 (1994) G.F.Peaslee, M.B.Tsang, C.Schwarz, M.J.Huang, W.S.Huang, W.C.Hsi, C.Williams, W.Bauer, D.R.Bowman, M.Chartier, J.Dinius, C.K.Gelbke, T.Glasmacher, D.O.Handzy, M.A.Lisa, W.G.Lynch, C.M.Mader, L.Phair, M.-C.Lemaire, S.R.Souza, G.Van Buren, R.J.Charity, L.G.Sobotka, G.J.Kunde, U.Lynen, J.Pochodzalla, H.Sann, W.Trautmann, D.Fox, R.T.de Souza, G.Peilert, W.A.Friedman, N.Carlin Energy Dependence of Multifragmentation in 84Kr + 197Au Collisions NUCLEAR REACTIONS 197Au(84Kr, X), E=35, 55, 70, 100, 200, 400 MeV/nucleon; measured intermediate mass fragment, total charged particle multiplicities; deduced multi-fragmentation energy dependence. QMD model.
doi: 10.1103/PhysRevC.49.R2271
1994SC15 Phys.Rev. C49, 3316 (1994) C.Schwarz, W.G.Gong, N.Carlin, C.K.Gelbke, Y.D.Kim, W.G.Lynch, T.Murakami, G.Poggi, R.T.de Souza, M.B.Tsang, H.M.Xu, K.Kwiatkowski, V.E.Viola, S.J.Yennello Anomalous Populations of Particle-Unbound States in 10B NUCLEAR REACTIONS 27Al, 197Au(14N, X), E=75 MeV/nucleon; 122Sn, 27Al(129Xe, X), E=31 MeV/nucleon; measured B fragments inclusive yields, (9Be)(p)-correlation functions. 10B deduced particle unstable states relative populations. Statistical calculations.
doi: 10.1103/PhysRevC.49.3316
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
1993BA10 Nucl.Phys. A553, 749c (1993) W.Bauer, D.R.Bowman, N.Carlin, N.Colonna, R.T.de Souza, C.K.Gelbke, W.G.Gong, K.Hanold, Y.D.Kim, M.A.Lisa, W.G.Lynch, M.A.McMahan, L.G.Moretto, G.F.Peaslee, L.Phair, M.B.Tsang, C.Williams, G.J.Wozniak, F.Zhu Multifragment Emission in 36Ar + 197Au and 129Xe + 197Au Collisions NUCLEAR REACTIONS 197Au(129Xe, X), E=50 MeV/nucleon; 197Au(36Ar, X), E=50-110 MeV/nucleon; measured intermediate mass fragments number, charged particle multiplicity. Model analysis.
doi: 10.1016/0375-9474(93)90692-Q
1993BO16 Phys.Rev.Lett. 70, 3534 (1993) D.R.Bowman, G.F.Peaslee, N.Carlin, R.T.de Souza, C.K.Gelbke, W.G.Gong, Y.D.Kim, M.A.Lisa, W.G.Lynch, L.Phair, M.B.Tsang, C.Williams, N.Colonna, K.Hanold, M.A.McMahan, G.J.Wozniak, L.G.Moretto Sources and Emission Time Scales in E/A = 50 MeV 129Xe + (nat)Cu Reactions NUCLEAR REACTIONS Cu(129Xe, X), E=50 MeV/nucleon; measured (fragment)(fragment)(θ), velocity distributions; deduced source features, emission times.
doi: 10.1103/PhysRevLett.70.3534
1993FA05 Nucl.Phys. A552, 82 (1993) L.Fante, Jr., N.Added, R.M.Anjos, N.Carlin, M.M.Coimbra, M.C.S.Figueira, R.Matheus, E.M.Szanto, A.Szanto de Toledo Fusion and Peripheral Processes in the 9Be + 10,11B Reactions NUCLEAR REACTIONS 10,11B(9Be, X), E=10-40 MeV; measured σ(fragment θ, E), σ(fragment A, Z) for fusion, quasi-elastic, elastic scattering; deduced critical grazing angular momentum, binary processes role. Statistical model calculations.
doi: 10.1016/0375-9474(93)90332-R
1993FI07 Nucl.Phys. A561, 453 (1993) M.C.S.Figueira, E.M.Szanto, R.M.Anjos, N.Added, N.Carlin, L.Fante, Jr., R.Matheus, A.Szanto de Toledo Complete Fusion of 9Be + 29Si NUCLEAR REACTIONS 29Si(9Be, X), (9Be, 9Be), E=17-40 MeV; measured σ(θ, E) for fusion, elastic scattering; deduced critical, grazing angular momentum. Statistical model calculations.
doi: 10.1016/0375-9474(93)90021-O
1993FO01 Phys.Rev. C47, R421 (1993); Erratum Phys.Rev. C48, 3135 (1993) D.Fox, R.T.de Souza, L.Phair, D.R.Bowman, N.Carlin, C.K.Gelbke, W.G.Gong, Y.D.Kim, M.A.Lisa, W.G.Lynch, G.F.Peaslee, M.B.Tsang, F.Zhu Extraction of the Multifragmentation Time Scale in Intermediate Energy Heavy-Ion Reactions NUCLEAR REACTIONS 197Au(36Ar, X), E=50-110 MeV/nucleon; measured charged particle multiplicity, intermediate mass fragment correlation; deduced multi-fragmentation time scale.
doi: 10.1103/PhysRevC.47.R421
1993GO01 Phys.Rev. C47, R429 (1993) W.G.Gong, P.Danielewicz, C.K.Gelbke, N.Carlin, R.T.de Souza, Y.D.Kim, W.G.Lynch, T.Murakami, G.Poggi, M.B.Tsang, H.M.Xu, S.Pratt, K.Kwiatkowski, V.E.Viola, Jr., S.J.Yennello, J.C.Shillcock Two-Deuteron Correlation Functions in 14N + 27Al Collisions at E/A = 75 MeV NUCLEAR REACTIONS 27Al(14N, X), E=75 MeV/nucleon; measured dd-, pp-correlation functions; deduced ejectile time span differences. Microscopic transport model.
doi: 10.1103/PhysRevC.47.R429
1993PH01 Nucl.Phys. A564, 453 (1993) L.Phair, D.R.Bowman, N.Carlin, C.K.Gelbke, W.G.Gong, Y.D.Kim, M.A.Lisa, W.G.Lynch, G.F.Peaslee, R.T.de Souza, M.B.Tsang, C.Williams, F.Zhu, N.Colonna, K.Hanold, M.A.McMahan, G.J.Wozniak Azimuthal Correlations as a Test for Centrality in Heavy-Ion Collisions NUCLEAR REACTIONS 197Au(36Ar, X), E=35-110 MeV/nucleon; 197Au(129Xe, X), E=50 MeV/nucleon; measured (particle)(particle)(φ); deduced central collisions selectivity features.
doi: 10.1016/0375-9474(93)90515-Y
1993SC21 Phys.Rev. C48, 676 (1993) C.Schwarz, W.G.Gong, N.Carlin, C.K.Gelbke, Y.D.Kim, W.G.Lynch, T.Murakami, G.Poggi, R.T.de Souza, M.B.Tsang, H.M.Xu, D.E.Fields, K.Kwiatkowski, V.E.Viola, Jr., S.J.Yennello Emission Temperatures from Widely Separated States in 14N- and 129Xe-Induced Reactions NUCLEAR REACTIONS 27Al, 197Au(14N, X), E=75 MeV/nucleon; 27Al, 122Sn(129Xe, X), E=31 MeV/nucleon; measured light charged particle relative momentum correlation functions, inclusive σ(fragment θ, E) for α, 6Li, 7Be; deduced nuclear temperatures of 4He, 5Li, and 8Be.
doi: 10.1103/PhysRevC.48.676
1993TS01 Phys.Rev. C47, 2717 (1993) M.B.Tsang, D.R.Bowman, N.Carlin, P.Danielewicz, C.K.Gelbke, W.G.Gong, Y.D.Kim, W.G.Lynch, L.Phair, R.T.de Souza, F.Zhu Multiplicity Dependence of Azimuthal Distributions for 36Ar + 197Au Collisions at E/A = 35 MeV NUCLEAR REACTIONS 197Au(36Ar, X), E=35 MeV/nucleon; measured charged particle azimuthal multiplicity, anisotropy; deduced scaling. Coalescence model, Boltzmann-Uehling-Uhlenbeck theory.
doi: 10.1103/PhysRevC.47.2717
1992AD02 Nucl.Phys. A540, 328 (1992) N.Added, R.M.Dos Anjos, N.Carlin, L.Fante, Jr., M.C.S.Figueira, R.Matheus, E.M.Szanto, A.Szanto de Toledo, M.S.Hussein, C.A.Bertulani, L.F.Canto Direct Versus Statistical Break-Up Processes in the 16,18O + 27Al, 28Si Reactions at E/A ≤ 4 MeV NUCLEAR REACTIONS 27Al(18O, αX), 27Al, 28Si(16O, αX), E=48-64 MeV; measured Eα, σ(fragment θ, θα) for X=12,14C; deduced breakup, incomplete fusion yields. Direct, statistical models.
doi: 10.1016/0375-9474(92)90207-Z
1992BO29 Phys.Rev. C46, 1834 (1992) D.R.Bowman, C.M.Mader, G.F.Peaslee, W.Bauer, N.Carlin, R.T.de Souza, C.K.Gelbke, W.G.Gong, Y.D.Kim, M.A.Lisa, W.G.Lynch, L.Phair, M.B.Tsang, C.Williams, N.Colonna, K.Hanold, M.A.McMahan, G.J.Wozniak, L.G.Moretto, W.A.Friedman Intermediate Mass Fragment Emission as a Probe of Nuclear Dynamics NUCLEAR REACTIONS 12C, 27Al, 51V, Cu, 89Y, 197Au(129Xe, X), E=50 MeV/nucleon; measured fragment muliplicity, charge distribution; deduced correlation with charged particle multiplicity, target independence. Hybrid model, dynamical emission aspects.
doi: 10.1103/PhysRevC.46.1834
1992KI02 Phys.Rev. C45, 338 (1992) Y.D.Kim, R.T.de Souza, D.R.Bowman, N.Carlin, C.K.Gelbke, W.G.Gong, W.G.Lynch, L.Phair, M.B.Tsang, F.Zhu Intermediate Mass Fragment Emission in 36Ar + 197Au Collisions at E/A = 35 MeV NUCLEAR REACTIONS 197Au(36Ar, X), E=35 MeV/nucleon; measured (fragment)(fragment)(θ), energy spectra, multiplicity distributions; deduced intermediate mass fragments time scales.
doi: 10.1103/PhysRevC.45.338
1992TS01 Phys.Lett. 297B, 243 (1992) M.B.Tsang, P.Danielewicz, D.R.Bowman, N.Carlin, C.K.Gelbke, W.G.Gong, Y.D.Kim, W.G.Lynch, L.Phair, R.T.de Souza, F.Zhu Reaction Dynamics and Deuteron Production NUCLEAR REACTIONS 197Au(36Ar, X), E=35 MeV/nucleon; measured σ(θp, Ep), σ(θd, Ed), azimuthal distributions. Microscopic transport model including deuteron production, Coulomb effects.
doi: 10.1016/0370-2693(92)91256-9
1992WI04 Phys.Rev. C45, 2300 (1992) J.L.Wile, D.E.Fields, K.Kwiatkowski, S.J.Yennello, K.B.Morley, E.Renshaw, V.E.Viola, C.K.Gelbke, W.G.Lynch, N.Carlin, H.M.Xu, W.G.Gong, M.B.Tsang, J.Pochodzalla, R.T.deSouza, D.J.Fields, S.M.Austin Excitation Functions for Complex Fragment Emission in the E/A = 20-100 MeV 14N + (nag)Ag, 197Au Reactions NUCLEAR REACTIONS Ag, 197Au(14N, X), E=20-100 MeV/nucleon; measured σ(fragment θ, E); deduced fragment emission mechanism. Three-source model.
doi: 10.1103/PhysRevC.45.2300
1991BO30 Phys.Rev.Lett. 67, 1527 (1991) D.R.Bowman, G.F.Peaslee, R.T.de Souza, N.Carlin, C.K.Gelbke, W.G.Gong, Y.D.Kim, M.A.Lisa, W.G.Lynch, L.Phair, M.B.Tsang, C.Williams, N.Colonna, K.Hanold, M.A.McMahan, G.J.Wozniak, L.G.Moretto, W.A.Friedman Multifragment Disintegration of the 129Xe + 197Au System at E/A = 50 MeV NUCLEAR REACTIONS 197Au(129Xe, X), E=50 MeV/nucleon; measured charged particle multiplicities. Dynamical, statistical models.
doi: 10.1103/PhysRevLett.67.1527
1991DE33 Phys.Lett. 268B, 6 (1991) R.T.de Souza, L.Phair, D.R.Bowman, N.Carlin, C.K.Gelbke, W.G.Gong, Y.D.Kim, M.A.Lisa, W.G.Lynch, G.F.Peaslee, M.B.Tsang, H.M.Xu, F.Zhu, W.A.Friedman Multifragment Emission in the Reaction 36Ar + 197Au at E/A = 35, 50, 80, and 110 MeV NUCLEAR REACTIONS 197Au(36Ar, X), E=35-110 MeV/nucleon; measured fragment multiplicity distributions, first, second moments. Statistical decay model.
doi: 10.1016/0370-2693(91)90913-B
1991GO05 Phys.Rev. C43, 1804 (1991) W.G.Gong, C.K.Gelbke, W.Bauer, N.Carlin, R.T.de Souza, Y.D.Kim, W.G.Lynch, T.Murakami, G.Poggi, D.P.Sanderson, M.B.Tsang, H.M.Xu, D.E.Fields, K.Kwiatkowski, R.Planeta, V.E.Viola, Jr., S.J.Yennello, S.Pratt Space-Time Evolution of the Reactions 14N + 27Al, 197Au at E/A = 75 MeV and 129Xe + 27Al, 122Sn at E/A = 31 MeV Probed by Two-Proton Intensity Interferometry NUCLEAR REACTIONS 27Al, 197Au(14N, 2p), E=75 MeV/nucleon; 27Al, 122Sn(129Xe, 2p), E=31 MeV/nucleon; measured two-proton correlation function; deduced reaction mechanism.
doi: 10.1103/PhysRevC.43.1804
1991KI12 Phys.Rev.Lett. 67, 14 (1991) Y.D.Kim, R.T.de Souza, D.R.Bowman, N.Carlin, C.K.Gelbke, W.G.Gong, W.G.Lynch, L.Phair, M.B.Tsang, F.Zhu, S.Pratt Time Scale for Emission of Intermediate-Mass Fragments in 36Ar + 197Au Collisions at E/A = 35 MeV NUCLEAR REACTIONS 197Au(36Ar, X), E=35 MeV/nucleon; measured σ(fragment θ, E) for X=Be, B, C, (fragment)(fragment)(θ); deduced intermediate mass fragment emission time scale. Final state Coulomb-interaction models.
doi: 10.1103/PhysRevLett.67.14
1991SO12 Phys.Rev. C44, R2257 (1991); Erratum Phys.Rev. C46, 819 (1992) L.G.Sobotka, L.Gallamore, A.Chbihi, D.G.Sarantites, D.W.Stracener, W.Bauer, D.R.Bowman, N.Carlin, R.T.DeSouza, C.K.Gelbke, W.G.Gong, S.Hannuschke, Y.D.Kim, W.G.Lynch, R.Ronningen, M.B.Tsang, F.Zhu, J.R.Beene, M.L.Halbert, M.Thoennessen Particle Multiplicity Dependence of High-Energy Photon Production in a Heavy-Ion Reaction NUCLEAR REACTIONS 93Nb(40Ar, X), E=65 MeV/nucleon; measured high energy γ- production vs particle multiplicity.
doi: 10.1103/PhysRevC.44.R2257
1991TS01 Phys.Rev. C44, 2065 (1991) M.B.Tsang, R.T.de Souza, Y.D.Kim, D.R.Bowman, N.Carlin, C.K.Gelbke, W.G.Gong, W.G.Lynch, L.Phair, F.Zhu Reaction Plane Determination for 36Ar + 197Au Collisions at E/A = 35 MeV NUCLEAR REACTIONS 197Au(36Ar, X), (36Ar, F), E=35 MeV/nucleon; measured σ(E, θ), σ(E, θ, φ) for residuals, fission fragments, X=p, d, t, α, Li, Be, B, C, N, O; deduced reaction plane uncertainties, azimuthal distribution. Monte Carlo simulation.
doi: 10.1103/PhysRevC.44.2065
1991WI16 Phys.Lett. 264B, 26 (1991) J.L.Wile, D.E.Fields, K.Kwiatkowski, K.B.Morley, E.Renshaw, S.J.Yennello, V.E.Viola, N.Carlin, C.K.Gelbke, W.G.Gong, W.G.Lynch, R.T.de Souza, M.B.Tsang, H.M.Xu Complex Fragment Emission in the E/A = 60-100 MeV 14N + (nat)Ag, 197Au Reactions NUCLEAR REACTIONS Ag, 197Au(14N, X), E=60-100 MeV/nucleon; measured fragment production σ(E) for fragment Z=3-15. Three-source model.
doi: 10.1016/0370-2693(91)90697-O
1990DE46 Nucl.Instrum.Methods Phys.Res. A295, 109 (1990) R.T.De Souza, N.Carlin, Y.D.Kim, J.Ottarson, L.Phair, D.R.Bowman, C.K.Gelbke, W.G.Gong, W.G.Lynch, R.A.Pelak, T.Peterson, G.Poggi, M.B.Tsang, H.M.Xu The MSU Miniball 4π Fragment Detection Array NUCLEAR REACTIONS 197Au(40Ar, X), E=35 MeV/nucleon; measured fragment spectra. Fast-plastic CSI(Tl) phoswich detectors.
doi: 10.1016/0168-9002(90)90429-A
1990GO05 Nucl.Instrum.Methods Phys.Res. A287, 639 (1990) W.G.Gong, N.Carlin, C.K.Gelbke, R.Dayton Quality Tests of CsI(Tl) Scintillators NUCLEAR REACTIONS 12C(α, d), (α, t), (α, α'), E=160 MeV; measured particle spectra. Cylindrical CsI(Tl) detectors.
doi: 10.1016/0168-9002(90)91589-4
1990GO16 Phys.Lett. 246B, 21 (1990) W.G.Gong, C.K.Gelbke, N.Carlin, R.T.de Souza, Y.D.Kim, W.G.Lynch, T.Murakami, G.Poggi, D.Sanderson, M.B.Tsang, H.M.Xu, D.E.Fields, K.Kwiatkowski, R.Planeta, V.E.Viola, Jr., S.J.Yennello, S.Pratt Two-Proton Correlation Functions for Equilibrium and Non-Equilibrium Emission NUCLEAR REACTIONS 122Sn, 197Au, 27Al(129Xe, 2p), E=31 MeV/nucleon; measured 2p-correlation functions; deduced emission process time scale differences.
doi: 10.1016/0370-2693(90)91301-Q
1990GO32 Phys.Rev.Lett. 65, 2114 (1990) W.G.Gong, W.Bauer, C.K.Gelbke, N.Carlin, R.T.de Souza, Y.D.Kim, W.G.Lynch, T.Murakami, G.Poggi, D.P.Sanderson, M.B.Tsang, H.M.Xu, S.Pratt, D.E.Fields, K.Kwiatkowski, R.Planeta, V.E.Viola, Jr., S.J.Yennello Intensity-Interferometric Test of Nuclear Collision Geometries Obtained from the Boltzmann-Uehling-Uhlenbeck Equation NUCLEAR REACTIONS 27Al(14N, X), E=75 MeV/nucleon; measured pp-correlation. Boltzmann-Uehling-Uhlenbeck equation based analysis.
doi: 10.1103/PhysRevLett.65.2114
1990TS02 Phys.Rev. C42, R15 (1990) M.B.Tsang, Y.D.Kim, N.Carlin, Z.Chen, C.K.Gelbke, W.G.Gong, W.G.Lynch, T.Murakami, T.Nayak, R.M.Ronningen, H.M.Xu, F.Zhu, L.G.Sobotka, D.W.Stracener, D.G.Sarantites, Z.Majka, V.Abenante Azimuthal Distributions of Fission Fragments and α Particles Emitted in the Reactions 36Ar + 238U at E/A = 20 and 35 MeV and 14N + 238U at E/A = 50 MeV NUCLEAR REACTIONS 238U(36Ar, F), E=20, 35 MeV/nucleon; 238U(14N, F), E=50 MeV/nucleon; measured fission (fragment)α(θ, φ); deduced in-plane, out of plane anisotropies.
doi: 10.1103/PhysRevC.42.R15
1989KI12 Phys.Rev.Lett. 63, 494 (1989) Y.D.Kim, M.B.Tsang, C.K.Gelbke, W.G.Lynch, N.Carlin, Z.Chen, R.Fox, W.G.Gong, T.Murakami, T.K.Nayak, R.M.Ronningen, H.M.Xu, F.Zhu, W.Bauer, L.G.Sobotka, D.Stracener, D.G.Sarantites, Z.Majka, V.Abenante, H.Griffin Multifragment Emission Observed for the Reaction 36Ar + 238U at E/A = 35 MeV NUCLEAR REACTIONS 238U(36Ar, X), E=35 MeV/nucleon; measured charged particle multiplicities; deduced reaction mechanism.
doi: 10.1103/PhysRevLett.63.494
1989TS01 Phys.Lett. 220B, 492 (1989) M.B.Tsang, Y.D.Kim, N.Carlin, Z.Chen, R.Fox, C.K.Gelbke, W.G.Gong, W.G.Lynch, T.Murakami, T.K.Nayak, R.M.Ronningen, H.M.Xu, F.Zhu, L.Sobotka, D.Stracener, D.G.Sarantites, Z.Majka, V.Abenante, H.Griffin Reaction Filters. Charged-Particle Multiplicity and Linear Momentum Transfer NUCLEAR REACTIONS 238U(36Ar, X), E=35 MeV/nucleon; 238U(14N, X), E=50 MeV/nucleon; measured charged particle multiplicity vs θ(ff). 4π charged particle detector.
doi: 10.1016/0370-2693(89)90774-0
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