NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = F.Cannata Found 67 matches. 2012DA01 Nucl.Phys. A875, 139 (2012) M.D'Agostino, M.Bruno, F.Gulminelli, L.Morelli, G.Baiocco, L.Bardelli, S.Barlini, F.Cannata, G.Casini, E.Geraci, F.Gramegna, V.L.Kravchuk, T.Marchi, A.Moroni, A.Ordine, Ad.R.Raduta Towards an understanding of staggering effects in dissipative binary collisions NUCLEAR REACTIONS 58,64Ni(32S, X), E-14.5 MeV/nucleon; measured reaction fragments using GARFILED detector array and ring counter; deduced yield, charge distribution, reaction mechanisms, even-odd effects, correlation functions; calculated yields using GEMINI code.
doi: 10.1016/j.nuclphysa.2011.11.011
2011DA11 Nucl.Phys. A861, 47 (2011) M.D'Agostino, M.Bruno, F.Gulminelli, L.Morelli, G.Baiocco, L.Bardelli, S.Barlini, F.Cannata, G.Casini, E.Geraci, F.Gramegna, V.L.Kravchuk, T.Marchi, A.Moroni, A.Ordine, Ad.R.Raduta Reaction mechanisms and staggering in S+Ni collisions NUCLEAR REACTIONS 58,64Ni(32S, X), E=463 MeV; measured Z(particle), A(particle), E(particle), I(particle, θ); deduced yields, even-odd effects, flow; calculated yields, even-odd effects, fragment relative velocity using GEMINI code with different assumptions on reaction mechanism and de-excitation chain.
doi: 10.1016/j.nuclphysa.2011.06.017
2008BR10 Nucl.Phys. A807, 48 (2008) M.Bruno, F.Gulminelli, F.Cannata, M.D'Agostino, F.Gramegna, G.Vannini Signals of bimodality in the fragmentation of Au quasi-projectiles NUCLEAR REACTIONS Au(Au, X), E=35 MeV/nucleon; measured projectile-like fission fragments kinetic energy and charge distributions; deduced fission mechanism features.
doi: 10.1016/j.nuclphysa.2008.03.019
2007CA02 Ann.Phys.(New York) 322, 397 (2007) F.Cannata, J.-P.Dedonder, A.Ventura Scattering in PT-symmetric quantum mechanics
doi: 10.1016/j.aop.2006.05.011
2007GE11 Eur.Phys.J. Special Topics 150, 21 (2007) E.Geraci, U.Abbondanno, L.Bardelli, S.Barlini, M.Bini, M.Bruno, F.Cannata, G.Casini, M.Chiari, M.D'Agostino, J.De Sanctis, A.Giussani, F.Gramegna, V.L.Kravchuk, A.L.Lanchais, P.Marini, A.Moroni, A.Nannini, A.Olmi, A.Ordine, G.Pasquali, S.Piantelli, G.Poggi, G.Vannini, for the NUCL-EX Collaboration Isotope analysis in central heavy ion collisions at intermediate energies NUCLEAR REACTIONS 58,64Ni(32S, X), E=14.5 MeV/nucleon; 58,64Ni(112Sn, X), E=35.0 MeV/nucleon; measured reaction product mass and charge distributions. Deduced isotopic ratios as a function of neutron number of fragments.
doi: 10.1140/epjst/e2007-00255-y
2005CA27 Phys.Rev. C 71, 064320 (2005) R.Capote, A.Ventura, F.Cannata, J.M.Quesada Level densities of transitional Sm nuclei NUCLEAR STRUCTURE 148,149,150,152Sm; calculated level densities, resonance spacing. Interacting boson model, comparison with data.
doi: 10.1103/PhysRevC.71.064320
2005DA10 Nucl.Phys. A749, 55c (2005) M.D'Agostino, M.Bruno, F.Gulminelli, F.Cannata, Ph.Chomaz, G.Casini, E.Geraci, F.Gramegna, A.Moroni, G.Vannini Nuclear liquid-gas phase transition: experimental signals NUCLEAR REACTIONS C, Cu, Au(197Au, X), E=25, 35 MeV/nucleon; analyzed fragments yields, charge distributions; 58Ni(32S, X), E=15.5 MeV/nucleon; analyzed charged fragment correlation functions; deduced liquid-gas phase transition features.
doi: 10.1016/j.nuclphysa.2004.12.008
2004DA12 Nucl.Phys. A734, 512 (2004) M.D'Agostino, M.Bruno, F.Gulminelli, R.Bougault, F.Cannata, Ph.Chomaz, F.Gramegna, N.Le Neindre, A.Moroni, G.Vannini Experimental Signals of Phase Transition NUCLEAR REACTIONS C, Cu, Au(197Au, X), E=25, 35 MeV/nucleon; analyzed fragments angular and charge distributions, related data; deduced thermodynamic features.
doi: 10.1016/j.nuclphysa.2004.01.094
2003DA20 Nucl.Phys. A724, 455 (2003) M.D'Agostino, M.Bruno, F.Gulminelli, R.Bougault, F.Cannata, Ph.Chomaz, F.Gramegna, I.Iori, N.Le Neindre, G.V.Margagliotti, A.Moroni, G.Vannini, J.P.Wieleczko Critical-like behaviours in central and peripheral collisions: a comparative analysis NUCLEAR REACTIONS C, Cu(197Au, X), E=25 MeV/nucleon; Cu, Au(197Au, X), E=35 MeV/nucleon; analyzed fragment charge distributions, correlations; deduced parameters, phase transition features.
doi: 10.1016/S0375-9474(03)01541-0
2002DA05 Nucl.Phys. A699, 795 (2002) M.D'Agostino, R.Bougault, F.Gulminelli, M.Bruno, F.Cannata, Ph.Chomaz, F.Gramegna, I.Iori, N.Le Neindre, G.V.Margagliotti, A.Moroni, G.Vannini On the Reliability of Negative Heat Capacity Measurements NUCLEAR REACTIONS Sn(Xe, X), E=32-50 MeV/nucleon; analyzed heat capacity, kinetic energy fluctuation, other thermodynamic quantities; deduced phase transition.
doi: 10.1016/S0375-9474(01)01287-8
2000DA02 Phys.Lett. 473B, 219 (2000) M.D'Agostino, F.Gulminelli, Ph.Chomaz, M.Bruno, F.Cannata, R.Bougault, F.Gramegna, I.Iori, N.Le Neindre, G.V.Margagliotti, A.Moroni, G.Vannini Negative Heat Capacity in the Critical Region of Nuclear Fragmentation: An experimental evidence of the liquid-gas phase transition NUCLEAR REACTIONS 197Au(197Au, X), E=35 MeV/nucleon; measured light, intermediate fragments charge and angular distributions; deduced negative heat capacity, liquid-gas phase transition.
doi: 10.1016/S0370-2693(99)01486-0
1997CA33 Z.Phys. A358, 275 (1997) F.Cannata, J.-P.Dedonder, M.P.Locher Meson Production and Bose-Einstein Pion Correlations in High Energy Collisions
doi: 10.1007/s002180050327
1996AM01 Z.Phys. A354, 209 (1996) R.D.Amado, F.Cannata, J.-P.Dedonder, M.P.Locher, Y.Lu, V.E.Markushin On the Relationship of the Scaled Phase Space and Skyrme-Coherent State Treatments of Proton Antiproton Annihilation at Rest NUCLEAR REACTIONS 1H(p-bar, X), E at rest; analyzed pion multiplicities, single pion spectra following (p-bar)p annihilation; deduced scaled phase space, Skyrme-coherent state treatments relationship.
doi: 10.1007/s002180050033
1995AM01 Phys.Rev. C51, 1587 (1995) R.D.Amado, F.Cannata, J.-P.Dedonder, M.P.Locher, Y.Lu Isospin Recoupling and Bose-Einstein Pion Correlations in (N-bar)N Annihilations
doi: 10.1103/PhysRevC.51.1587
1994AM03 Phys.Rev.Lett. 72, 970 (1994) R.D.Amado, F.Cannata, J.-P.Dedonder, M.P.Locher, B.Shao Coherent Pion Radiation from Nucleon-Antinucleon Annihilation
doi: 10.1103/PhysRevLett.72.970
1994AM05 Phys.Rev. C50, 640 (1994) R.D.Amado, F.Cannata, J.-P.Dedonder, M.P.Locher, B.Shao Coherent State Formulation of Pion Radiation from Nucleon-Antinucleon Annihilation
doi: 10.1103/PhysRevC.50.640
1994AM11 Phys.Lett. 339B, 201 (1994) R.D.Amado, F.Cannata, J.-P.Dedonder, M.P.Locher, Y.Lu Bose-Einstein Pion Correlations in (N-bar)N Annihilations
doi: 10.1016/0370-2693(94)91155-X
1994AM16 Int.J.Mod.Phys. E3, 171 (1994) R.D.Amado, R.Bijker, F.Cannata, J.P.Dedonder, N.R.Walet Quartets of Superdeformed Bands and Supersymmetry Breaking NUCLEAR STRUCTURE 152Dy, 151Tb, 150,146,147,148Gd, 192,193,194Hg; analyzed superdeformed bands, associated properties; deduced supersymmetry breaking related features.
doi: 10.1142/S0218301394000061
1994CA14 Phys.Rev. C49, 2798 (1994) F.Cannata, D.E.Kharzeev, F.Piccinini Collective Effects in the Nuclear Interactions of Charmonium at Low Energy
doi: 10.1103/PhysRevC.49.2798
1994DO17 Nuovo Cim. 107A, 661 (1994) P.Doleschall, M.Bruno, F.Cannata, M.D'Agostino About the Present Status of α-d Faddeev Calculations Including the Coulomb Interaction Above the Break-Up Threshold
doi: 10.1007/BF02768799
1993CA32 Nuovo Cim. 106A, 989 (1993) G-Parity Tests in (n-bar)p Annihilation NUCLEAR REACTIONS 1H(n-bar, X), E not given; calculated asymmetry vs multi-pionic channel effective mass distributions; deduced G-parity violation test possibility for annihilation in flight.
doi: 10.1007/BF02786667
1991AM03 Phys.Rev.Lett. 67, 2777 (1991) R.D.Amado, R.Bijker, F.Cannata, J.P.Dedonder Supersymmetric Quantum Mechanics and Superdeformed Nuclei NUCLEAR STRUCTURE A=146-198; deduced supersymmetry role in superdeformation.
doi: 10.1103/PhysRevLett.67.2777
1991BR02 Phys.Rev. C43, 201 (1991) M.Bruno, F.Cannata, M.D'Agostino, M.L.Fiandri, M.Herman, H.M.Hofmann Isospin Breaking Effects in the Reaction 4He(d, 3He)3H at Low Energies NUCLEAR REACTIONS 4He(d, 3He), E=23-25 MeV; measured σ(θ); deduced σ asymmetry, S-matrix elements. Resonating group model predictions comparison.
doi: 10.1103/PhysRevC.43.201
1991KU09 Yad.Fiz. 53, 942 (1991); Sov.J.Nucl.Phys. 53, 582 (1991) Yu.A.Kuperin, D.M.Latypov, S.P.Merkurev, M.Bruno, F.Cannata dα Scattering in a Three-Body Model NUCLEAR REACTIONS 2H(α, α), E ≤ 20 MeV; calculated σ(θ), phase shifts vs E, σ(θp, θα) following breakup. Three-body model.
1990AM07 Phys.Rev. C41, 1289 (1990) R.D.Amado, F.Cannata, J.P.Dedonder Supersymmetric Quantum Mechanics, the Pauli Principle, and Nucleon-Alpha Scattering
doi: 10.1103/PhysRevC.41.1289
1990BR09 Phys.Rev. C41, 2435 (1990) M.Bruno, F.Cannata, M.D'Agostino, M.L.Fiandri, M.Herman, H.M.Hofmann Isospin Breaking in the Analyzing Power of 3H(3He, 2H)4He and the Inverse Reaction NUCLEAR REACTIONS 3H(polarized 3He, d), E=18 MeV; calculated analyzing power; deduced isospin symmetry violation matrix element. Resonating group model.
doi: 10.1103/PhysRevC.41.2435
1990BR14 Phys.Rev. C42, 448 (1990) M.Bruno, F.Cannata, M.D'Agostino, M.L.Fiandri 4Li(g.s.) Formation in the 3He + p + n Reaction NUCLEAR REACTIONS 3He(d, p3He), E=23 MeV; measured σ(θ1, θ2, E). 4Li deduced ground state width. PWIA, Breit-Wigner analysis.
doi: 10.1103/PhysRevC.42.448
1990CA09 Phys.Rev. C41, 1637 (1990) F.Cannata, J.P.Dedonder, W.R.Gibbs Optical Potentials for Charged-Hadron-Nucleus Scattering: Role of Coulomb excitations NUCLEAR REACTIONS 40Ca(π+, π+), (π-, π-), E=50-180 MeV; calculated σ(θ); deduced Coulomb shift role.
doi: 10.1103/PhysRevC.41.1637
1990CL01 Nucl.Phys. A508, 261c (1990) M.Clajus, P.M.Egun, W.Gruebler, P.Hautle, W.Kretschmer, A.Rauscher, W.Schuster, R.Weidmann, M.Haller, M.Bruno, F.Cannata, M.D'Agostino, I.Slaus, P.A.Schmelzbach, B.Vuaridel, F.Sperisen, H.Witala, Th.Cornelius, W.Glockle Investigation of (ϵ1) and the 3P(J) Phase Shifts in the n-p System by the Measurement of Polarization Transfer Coefficients in p-d Elastic Scattering NUCLEAR REACTIONS 2H(polarized p, p), E=22.7 MeV; measured T22(θ), polarization transfer coefficient. Faddeev calculation.
doi: 10.1016/0375-9474(90)90482-2
1990CL05 Phys.Lett. 245B, 333 (1990) M.Clajus, P.M.Egun, W.Gruebler, P.Hautle, I.Slaus, B.Vuaridel, F.Sperisen, W.Kretschmer, A.Rauscher, W.Schuster, R.Weidmann, M.Haller, M.Bruno, F.Cannata, M.D'Agostino, H.Witala, Th.Cornelius, W.Glockle, P.A.Schmelzbach Investigation of the Nucleon-Nucleon Tensor Force in the Three-Nucleon System NUCLEAR REACTIONS 2H(polarized p, p), E=22.7 MeV; measured polarization transfer coefficient, analyzed other data; deduced sensitivity to tensor force.
doi: 10.1016/0370-2693(90)90654-O
1990FI06 Yad.Fiz. 51, 1551 (1990); Sov.J.Nucl.Phys. 51, 978 (1990) G.F.Filippov, V.S.Vasilevsky, M.Bruno, F.Cannata, M.D'Agostino, F.Ortolani Collective Excitations of 4He in d + d, n + 3He, and p + 3H Scattering NUCLEAR STRUCTURE 4He; calculated levels, collective, cluster degrees of freedom, scattering phenomena. NUCLEAR REACTIONS 3H(p, p), 3He(n, n), 2H(d, d), E ≤ 20 MeV; calculated phase shift vs E.
1990GR20 J.Phys.(Paris), Colloq.C-6, 451 (1990) W.Gruebler, M.Clajus, P.M.Egun, P.Hautle, A.Weber, P.A.Schmelzbach, I.Slaus, B.Vuaridel, F.Sperisen, W.Kretschmer, A.Rauscher, R.Weidmann, R.O.Karschnick, Th.Walter, M.Bruno, F.Cannata, M.d'Agostino Polarization Transfer in Elastic p-d Scattering at E(p) = 22.7 MeV NUCLEAR REACTIONS 2H(polarized p, p), E=22.7 MeV; measured polarization transfer coefficient vs θ. Faddeev calculations.
1989AR04 Phys.Rev. C40, 55 (1989) N.Arena, Seb.Cavallaro, G.Fazio, G.Giardina, A.Italiano, M.Herman, M.Bruno, F.Cannata, M.D'Agostino, M.Lombardi Three-Body Effects in the 7Li(d, ααn) Reaction NUCLEAR REACTIONS 7Li(d, 2α), E=6.8 MeV; measured σ(θ1, θ2) vs arc length; deduced three body effects. 5He deduced (3/2)+ level width. Enriched target.
doi: 10.1103/PhysRevC.40.55
1989BR23 Nucl.Phys. A501, 462 (1989) M.Bruno, F.Cannata, M.D'Agostino, M.L.Fiandri, M.Herman, H.M.Hofmann, B.Vuaridel, W.Gruebler, V.Konig, P.A.Schmelzbach, K.Elsener Barshay-Temmer Test for the 4He(d(pol), 3He)3H Reaction NUCLEAR REACTIONS 4He(d, 3He), E(cm)=14-33 MeV; measured σ(θ, E), iT11(θ, E); deduced asymmetries with respect to θ(cm)=90°, isospin violation magnitude. Resonating group calculations.
doi: 10.1016/0375-9474(89)90141-3
1989BR26 Few-Body Systems 6, 175 (1989) M.Bruno, F.Cannata, M.D'Agostino, M.L.Fiandri, M.Lombardi Final-State Interactions and Quasi-Free Mechanism in the 3He(d, 3Hp)p Reaction NUCLEAR REACTIONS 3He(d, pt), E=23.083; measured absolute σ(θ1, θ2) vs arc length; deduced quasifree mechanism, final state interaction roles.
doi: 10.1007/BF01229462
1989CL06 Helv.Phys.Acta 62, 926 (1989) M.Clajus, P.M.Egun, W.Gruebler, P.Hautle, A.Weber, P.A.Schmelzbach, I.Slaus, B.Vuaridel, F.Sperisen, W.Kretschmer, A.Rauscher, R.Weidmann, M.Haller, R.O.Karschnick, M.Bruno, F.Cannata, M.D'Agostino Polarization Transfer in the Reaction 2H(p(pol), p(pol))2H at Ep = 22.7 MeV NUCLEAR REACTIONS 2H(polarized p, p), E=22.7 MeV; measured polarization transfer vs θ. Model analysis.
1989VU01 Nucl.Phys. A499, 429 (1989) B.Vuaridel, W.Gruebler, V.Konig, K.Elsener, P.A.Schmelzbach, M.Bittcher, D.Singy, I.Borbely, M.Bruno, F.Cannata, M.D'Agostino New Constraints on D-State Contributions to the Trinucleon Wave Functions NUCLEAR REACTIONS 4He(polarized d, 3He), E=32.21-49.7 MeV; measured σ(θ, E), analyzing power vs θ. 3H, 3He deduced ratios of the D- to S-state asymptotic normalization.
doi: 10.1016/0375-9474(89)90538-1
1988BR18 Phys.Rev. C38, 521 (1988) M.Bruno, F.Cannata, M.D'Agostino, M.L.Fiandri, M.Herman, H.F.Hofmann, B.Vuaridel, V.Konig, W.Gruebler, P.A.Schmelzbach, K.Elsener, M.Bittcher, D.Singy Role of Tensor Forces in the 4He(d(pol), 3He)3H Reaction NUCLEAR REACTIONS 4He(polarized d, 3He), E(cm)=23 MeV; calculated σ(θ), analyzing power vs θ; deduced S-matrix elements, observables tensor force dependences.
doi: 10.1103/PhysRevC.38.521
1988BR27 J.Phys.(London) G14, L235 (1988) M.Bruno, F.Cannata, M.D'Agostino, M.L.Fiandri, M.Frisoni, M.Lombardi 3He-Induced d(*) Production NUCLEAR REACTIONS 3He(d, p3He), E=23.083 MeV; measured σ(θ1, θ2) vs arc length; deduced singlet d production σ.
doi: 10.1088/0305-4616/14/11/002
1988VU01 Nucl.Phys. A484, 34 (1988) B.Vuaridel, W.Gruebler, V.Konig, K.Elsener, P.A.Schmelzbach, J.Ulbricht, Ch.Forstner, M.Bittcher, D.Singy, M.Bruno, F.Cannata, M.D'Agostino, I.Borbely Experimental Investigation of Charge Symmetry Breaking Effects in the Reaction 4He(d(pol), 3He)3H between E(d) = 32 and 50 MeV NUCLEAR REACTIONS 4He(polarized d, 3He), E=32.1-49.7 MeV; measured σ(θ), σ(E), vector, tensor analyzing powers vs θ; deduced charge symmetry breaking effects.
doi: 10.1016/0375-9474(88)90139-X
1987BO54 Nuovo Cim. 98A, 291 (1987) S.Boffi, C.Giusti, F.D.Pacati, F.Cannata Missing Strength in (e, e'p) Reactions and Nonlocality in Final-State Interactions NUCLEAR REACTIONS 12C, 16O, 40Ca, 51V, 90Zr(e, e'p), E not given; calculated occupation number damping factor.
1987BR07 Phys.Rev. C35, 1563 (1987) M.Bruno, F.Cannata, M.D'Agostino, M.L.Fiandri, M.Frisoni, H.Oswald, P.Niessen, J.Schulte-Uebbing, H.Paetz gen.Schieck, P.Doleschall, M.Lombardi Coulomb Effects in the Alpha-Induced Deuteron Breakup NUCLEAR REACTIONS 2H(α, pα), E=11.3 MeV; 4He(d, pα), E=6-7 MeV; measured σ(θα, θp) versus arc length; deduced sensitivity to Coulomb effects. Kinematically complete experiment. Three-body Faddeev calculation comparison.
doi: 10.1103/PhysRevC.35.1563
1986BO44 Europhys.Lett. 2, 941 (1986) Phenomenology of (γ, π0) Reaction on Nuclei NUCLEAR REACTIONS 40Ca(γ, π0), E=180 MeV; 40Ca(π-, π-), E=44.5 MeV; calculated σ(θ). DWBA.
doi: 10.1209/0295-5075/2/12/009
1985DO03 Phys.Lett. 152B, 1 (1985) P.Doleschall, Gy.Bencze, M.Bruno, F.Cannata, M.D'Agostino An Approximate Treatment of Coulomb Effects in a Three-Body Model of the d(α, αp)n Breakup Reaction NUCLEAR REACTIONS 2H(α, αp), E ≈ breakup threshold; calculated σ(θ1, θ2) vs arc length. Three-body model, Coulomb effects.
doi: 10.1016/0370-2693(85)91127-X
1983BR23 Nucl.Phys. A407, 29 (1983) M.Bruno, F.Cannata, M.D'Agostino, B.Jenny, W.Gruebler, V.Konig, P.A.Schmelzbach, P.Doleschall Kinematically Complete Measurement of Cross Sections and Vector and Tensor Analyzing Powers of 4He(d(pol), pα)n at E(d)(pol) = 10 MeV NUCLEAR REACTIONS 4He(polarized d, pα), E=10.045 MeV; measured σ(θ(α), θ(p)), iT11(θ(α), θ(p)), T20(θ(α), θ(p)), T21(θ(α), θ(p)), T22(θ(α), (p)) versus arclength. Kinematically complete experiment, vector, tensor polarized beam, gaseous target. Comparison with three-body microscopic calculations.
doi: 10.1016/0375-9474(83)90306-8
1982BO16 Nucl.Phys. A379, 509 (1982) S.Boffi, F.Cannata, F.Capuzzi, C.Giusti, F.D.Pacati Orthogonality and the Perey Factor in Knockout Reactions Induced by Electromagnetic Probes NUCLEAR REACTIONS 16O(γ, p), E=80 MeV; calculated σ(θ). Knockout reactions, channel orthogonality, optical potentials.
doi: 10.1016/0375-9474(82)90011-2
1982BR09 Nuovo Cim. 68A, 35 (1982) M.Bruno, F.Cannata, M.D'Agostino, C.Maroni, I.Massa, M.Lombardi Experimental Study on Low-Energy 2H(α, α)2H Elastic Scattering NUCLEAR REACTIONS, ICPND 2H(α, α), E=6-14 MeV; measured σ(Ed), αd-coin, σ(E), σ(θ), reaction σ. 6Li resonances deduced Γ, α, proton, neutron reduced widths. Faddeev formalism, multi-channel, multi-level R-matrix analyses.
doi: 10.1007/BF02902733
1982BR17 Nucl.Phys. A386, 269 (1982) M.Bruno, F.Cannata, M.D'Agostino, M.L.Fiandri, M.Frisoni, G.Vannini, M.Lombardi The Low Energy 2H(α, αp)n Reaction NUCLEAR REACTIONS 2H(α, pα), E=9.847-13.991 MeV; measured σ(θα, θp) versus arc length. Kinematically complete experiment, solid target.
doi: 10.1016/0375-9474(82)90113-0
1981BR25 Phys.Rev. C24, 2751 (1981) M.Bruno, F.Cannata, M.D'Agostino, M.L.Fiandri, M.Frisoni, G.Vannini, M.Lombardi, Y.Koike 2H(α, pα)n Reaction near Threshold NUCLEAR REACTIONS 2H(α, pα), E=10.27, 11.3, 13 MeV; measured σ(Ep, θp, θα). Solid target.
doi: 10.1103/PhysRevC.24.2751
1981WE10 Phys.Rev. C24, 349 (1981) Isospin Mixing in the 2H(α, αp)n Reaction NUCLEAR REACTIONS 2H(α, αp), E=12.87, 23.7 MeV; calculated σ(θ) for singlet deuteron production; deduced reaction mechanism, isospin mixing effects. Nucleon-alpha impulse approximation, intermediate coupling shell model.
doi: 10.1103/PhysRevC.24.349
1980BR19 Lett.Nuovo Cim. 27, 265 (1980) M.Bruno, F.Cannata, M.D'Agostino, C.Maroni, M.Lombardi D(α, α)D Cross-Section Measurement NUCLEAR REACTIONS 2H(α, α), E=5.962-13.911 MeV; measured σ(θ, E).
doi: 10.1007/BF02817300
1980BR20 Lett.Nuovo Cim. 29, 1 (1980) M.Bruno, F.Cannata, M.D'Agostino, G.Vannini, F.Bongiovanni, M.Frisoni, M.Lombardi 5He(g.s.) Production in the 2H(α, pα)n Reaction Near Threshold NUCLEAR REACTIONS 2H(α, pα), E=9.847, 12.87 MeV; measured absolute σ(θp, θα, Eα). 5He level deduced Γ. Faddeev calculations, proton spectator model.
doi: 10.1007/BF02745332
1980BR28 Lett.Nuovo Cim. 29, 385 (1980) M.Bruno, F.Cannata, M.D'Agostino, G.Vannini, M.Lombardi, Y.Kioke << Singlet deuteron >> Production in the 2H(α, pα)n Reaction at Low Energies NUCLEAR REACTIONS 2H(α, pα), E=9.847, 12.87 MeV; measured σ(θα, θp, Ep); deduced neutron-proton final state interactions, isospin forbidden singlet deuteron production.
doi: 10.1007/BF02743237
1979BO40 Nuovo Cim. 54A, 165 (1979) G.Bonsignori, F.Cannata, G.Fratamico, M.Savoia Nuclear-Structure Effects in a Microscopic Theory for (α, α') Reactions in Even-Even Tin Isotopes NUCLEAR REACTIONS 116,122Sn(α, α'), E=27 MeV; analyzed σ(θ). Microscopic quasiparticle theory, Woods-Saxon single-particle states.
doi: 10.1007/BF02899786
1979GU01 Phys.Lett. 80B, 203 (1979) C.Guaraldo, A.Maggiora, R.Scrimaglio, F.Balestra, L.Busso, R.Garfagnini, G.Piragino, F.Cannata Elastic Backward Scattering of Positive Pions from 12C at 23, 29 and 35 MeV NUCLEAR REACTIONS 12C(π+, π+), E=23, 29, 35 MeV; measured σ(θ), θ > 161°; comparison with calculations based on Ericson-Ericson-Lorentz-Lorenz effect, models of Landau-Thomas, Stricker, others.
doi: 10.1016/0370-2693(79)90198-9
1977CA13 Nuovo Cim. 38A, 1 (1977) Exotic States in a Tin Isotope NUCLEAR STRUCTURE 116Sn; calculated pion content of ground, low-lying states in a phenomological model based on static approximation for the pion-nucleus interaction.
1975NA16 Phys.Rev. C12, 1586 (1975) Distorted-Wave Approximation and Nuclear Correlations in Pion Reactions NUCLEAR REACTIONS 12C(γ, π-); calculated σ(θ). Distorted pion wave.
doi: 10.1103/PhysRevC.12.1586
1974CA04 Phys.Rev. C9, 782 (1974) Isospin Breaking in the Reactions 3H + 9Be → 6Li + 6He, 6Li* + 6He NUCLEAR REACTIONS 9Be(t, 6He); failure of experimental symmetry around 90° explained by radial functions difference. Implications for muon capture 6He calculated.
doi: 10.1103/PhysRevC.9.782
1974CA21 Can.J.Phys. 52, 1405 (1974) F.Cannata, B.A.Lamers, C.W.Lucas, A.Nagl, H.Uberall, C.Werntz, F.J.Kelly Radiative Pion Capture in Flight and Charged Pion Photoproduction in Nuclei NUCLEAR REACTIONS 12C(γ, π+), E=160, 170, 180 MeV; 12C(π, γ), E=20, 30, 40 MeV; calculated σ(θ).
doi: 10.1139/p74-187
1974CA24 Phys.Rev.Lett. 33, 1316 (1974) F.Cannata, C.W.Lucas, Jr., C.W.Werntz Threshold Photoproduction of Pions on 6Li NUCLEAR REACTIONS 6Li(γ, π+); calculated σ(π+).
doi: 10.1103/PhysRevLett.33.1316
1974CA25 Phys.Rev. C10, 2093 (1974) F.Cannata, C.W.Lucas, Jr., C.Werntz Contributions of Nucleon Momenta to the Pion Optical Potential NUCLEAR REACTIONS 12C(π, π), E=120, 180 MeV; calculated σ(θ).
doi: 10.1103/PhysRevC.10.2093
1974MU13 Phys.Lett. 51B, 225 (1974) The Persistence of Supermultiplet Selection Rules in Nuclear Weak and Electromagnetic Transitions NUCLEAR STRUCTURE 6Li, 9Be, 10,11B, 12,13C, 14N; calculated giant M1 resonances, level-width.
doi: 10.1016/0370-2693(74)90279-2
1973BE38 Phys.Lett. 45B, 445 (1973) Configuration Mixing and Total Muon Capture Rates NUCLEAR REACTIONS 12C(μ, X); calculated capture rate.
doi: 10.1016/0370-2693(73)90639-4
1973BE51 Nucl.Phys. A215, 411 (1973) SU(4) Breaking, Allowed Transitions and Total Muon Capture Rates in Nuclei NUCLEAR REACTIONS 6Li, 12C(μ, ν); calculated muon capture rate.
doi: 10.1016/0375-9474(73)90664-7
1973CA25 Lett.Nuovo Cim. 8, 466 (1973) Spin-Dependent Effects in Giant-Resonance Excitation of Doubly-Closed-Shell Nuclei NUCLEAR REACTIONS 16O(γ, π); calculated σ.
doi: 10.1007/BF02824496
1972CA08 Phys.Rev. C5, 1189 (1972) Forward Neutrino-Induced Reactions on Doubly-Closed-Shell Nuclei NUCLEAR REACTIONS 12C(ν, e), 12C(ν, μ), calculated σ(θ) for giant resonance excitation. Sum-rule techniques.
doi: 10.1103/PhysRevC.5.1189
1971CA28 Nucl.Phys. A173, 665 (1971) Isotensor Dipole Sum Rules in Nuclear Electroexcitation NUCLEAR REACTIONS 12C, 16O, 28Si(e, e'), Q < 100 MeV/c; calculated integrated form factors. Isotensor dipole sum rules.
doi: 10.1016/0375-9474(71)90978-X
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