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Search: Author = F.Cannata

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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
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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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


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
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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
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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
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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
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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
Citations: PlumX Metrics


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
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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
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1993CA32      Nuovo Cim. 106A, 989 (1993)

F.Cannata, D.E.Kharzeev

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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1566.


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
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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
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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
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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
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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
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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
Citations: PlumX Metrics


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
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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
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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
Citations: PlumX Metrics


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
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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
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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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2172.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0074.


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
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1986BO44      Europhys.Lett. 2, 941 (1986)

S.Boffi, F.Cannata, M.Radici

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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1195.


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
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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
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1981WE10      Phys.Rev. C24, 349 (1981)

C.Werntz, F.Cannata

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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1191.


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
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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
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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
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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
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1977CA13      Nuovo Cim. 38A, 1 (1977)

F.Cannata, M.Savoia

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)

A.Nagl, F.Cannata, H.Uberall

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
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1974CA04      Phys.Rev. C9, 782 (1974)

F.Cannata, C.Werntz

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
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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
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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
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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
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1974MU13      Phys.Lett. 51B, 225 (1974)

N.C.Mukhopadhyay, F.Cannata

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
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1973BE38      Phys.Lett. 45B, 445 (1973)

J.Bernabeu, F.Cannata

Configuration Mixing and Total Muon Capture Rates

NUCLEAR REACTIONS 12C(μ, X); calculated capture rate.

doi: 10.1016/0370-2693(73)90639-4
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1973BE51      Nucl.Phys. A215, 411 (1973)

J.Bernabeu, F.Cannata

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
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1973CA25      Lett.Nuovo Cim. 8, 466 (1973)

F.Cannata, J.Ros

Spin-Dependent Effects in Giant-Resonance Excitation of Doubly-Closed-Shell Nuclei

NUCLEAR REACTIONS 16O(γ, π); calculated σ.

doi: 10.1007/BF02824496
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1972CA08      Phys.Rev. C5, 1189 (1972)

F.Cannata, R.Leonard

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
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1971CA28      Nucl.Phys. A173, 665 (1971)

F.Cannata, R.Leonardi

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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