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NSR database version of April 27, 2024.

Search: Author = C.De Conti

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2018FO01      J.Phys.(London) G45, 015101 (2018)

C.E.Fontoura, F.Krmpotic, A.P.Galeao, C.De Conti, G.Krein

Nonmesonic weak decay of charmed hypernuclei

NUCLEAR STRUCTURE ¹²N; calculated nonmesonic weak decay of charmed hypernuclei using a relativistic formalism.

doi: 10.1088/1361-6471/aa982a
Citations: PlumX Metrics

2016FO04      J.Phys.(London) G43, 055102 (2016)

C.E.Fontoura, F.Krmpotic, A.P.Galeao, C.De Conti, G.Krein

Relativistic model for the nonmesonic weak decay of single-lambda hypernuclei

RADIOACTIVITY ¹²C(2n), (n), (p); calculated diagrams, hypernuclei resonance widths, nonmesonic decay rates. Comparison with available data.

doi: 10.1088/0954-3899/43/5/055102
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2014KR15      Int.J.Mod.Phys. E23, 1450089 (2014)

F.Krmpotic, C.De Conti

Nonmesonic weak decay dynamics from proton spectra of Λ-hypernuclei

NUCLEAR STRUCTURE ⁵He, ⁷Li, ⁹Be, ¹¹B, ^12,13C, ¹⁵N, ¹⁶O; analyzed available hypernuclei data; deduced resonance widths. Independent particle shell model (IPSM) and one-meson-exchange (OME) potential framework.

doi: 10.1142/S021830131450089X
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2010BE17      Phys.Rev. C 81, 064603 (2010)

C.A.Bertulani, C.De Conti

Pauli blocking and medium effects in nucleon knockout reactions

NUCLEAR REACTIONS ⁹Be(¹¹Be, ¹⁰Be), (¹⁵C, ¹⁴C), (³⁴Ar, ³³Ar), E=10-500 MeV/nucleon; calculated σ and transverse and longitudinal momentum distribution for one-nucleon knockout reactions. Free nucleon-nucleon cross sections obtained using eikonal approximation compared with geometrical treatment of Pauli blocking and with Dirac-Brueckner methods.

doi: 10.1103/PhysRevC.81.064603
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2003BA20      Braz.J.Phys. 33, 297 (2003)

E.F.Batista, B.V.Carlson, C.De Conti, T.Frederico

Polarization Effects in Relativistic Nuclear Pairing

doi: 10.1590/s0103-97332003000200026
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2003BA73      Nucl.Phys. A726, 267 (2003)

C.Barbero, C.De Conti, A.P.Galeao, F.Krmpotic

Kinematical and nonlocality effects on the nonmesonic weak hypernuclear decay

NUCLEAR STRUCTURE ⁵He, ¹²C; calculated nonmesonic hypernuclear decay rates, kinematical and nonlocal effects.

doi: 10.1016/S0375-9474(03)01620-8
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2003BB20      Braz.J.Phys. 33, 297 (2003)

E.F.Batista, B.V.Carlson, C.De Conti, T.Frederico

Polarization Effects in Relativistic Nuclear Pairing

doi: 10.1590/S0103-97332003000200026
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2003CH85      Braz.J.Phys. 33, 238 (2003)

L.C.Chamon, B.V.Carlson, L.R.Gasques, D.Pereira, C.De Conti, M.A.G.Alvarez, M.S.Hussein, M.A.Candido Ribeiro, E.S.Rossi, Jr., C.P.Silva

Nonlocal Description of the Nuclear Interaction

doi: 10.1590/s0103-97332003000200012
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2002AL01      Phys.Rev. C65, 014602 (2002)

M.A.G.Alvarez, E.S.Rossi, Jr., C.P.Silva, L.R.Gasques, L.C.Chamon, D.Pereira, M.N.Rao, B.V.Carlson, C.De Conti, R.M.Anjos, P.R.S.Gomes, J.Lubian, S.Kailas, A.Chatterjee, P.Singh

Precise Nuclear Matter Densities from Heavy-Ion Collisions

NUCLEAR REACTIONS ¹⁶O(¹⁶O, ¹⁶O), E=1120 MeV; ⁹²Mo(¹⁶O, ¹⁶O), E=49 MeV; ^58,60,62,64Ni, ⁸⁸Sr, ^90,92Zr, ¹²⁰Sn, ¹³⁸Ba, ²⁰⁸Pb(¹⁶O, ¹⁶O), E not given; ^58,60Ni(¹⁸O, ¹⁸O), E not given; analyzed σ. ^16,18O deduced matter density distributions, related features. ¹⁶O, ⁵⁸Ni(e, e), E not given; calculated σ vs momentum transfer.

doi: 10.1103/PhysRevC.65.014602
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2002CH39      Phys.Rev. C66, 014610 (2002)

L.C.Chamon, B.V.Carlson, L.R.Gasques, D.Pereira, C.De Conti, M.A.G.Alvarez, M.S.Hussein, M.A.Candido Ribeiro, E.S.Rossi, Jr., C.P.Silva

Toward a Global Description of the Nucleus-Nucleus Interaction

NUCLEAR STRUCTURE Z=1-82; analyzed charge distribution data, radii. ¹⁶O, ⁵⁶Fe, ¹²⁰Sn, ²⁰⁸Pb; calculated nucleon density distributions.

NUCLEAR REACTIONS ⁵⁸Ni(¹⁶O, X), E not given; ⁵⁸Ni(α, X), E=139 MeV; calculated folding potential; deduced parameters. Other reaction data analyzed.

doi: 10.1103/PhysRevC.66.014610
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2002GA16      Phys.Rev. C65, 044314 (2002)

L.R.Gasques, L.C.Chamon, C.P.Silva, D.Pereira, M.A.G.Alvarez, E.S.Rossi, Jr., V.P.Likhachev, B.V.Carlson, C.De Conti

Determination of the ¹²C Nuclear Density Through Heavy-Ion Elastic Scattering Experiments

NUCLEAR REACTIONS ⁵⁸Ni(¹²C, ¹²C), E=26-28.5 MeV; ²⁰⁸Pb(¹²C, ¹²C), E=54.5-57 MeV; measured σ(θ); deduced potential features. ¹²C deduced nucleon density distribution. Comparisons with other reactions and with model predictions.

doi: 10.1103/PhysRevC.65.044314
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1634.

2002RO29      Nucl.Phys. A707, 325 (2002)

E.S.Rossi, Jr., D.Pereira, L.C.Chamon, C.P.Silva, M.A.G.Alvarez, L.R.Gasques, J.Lubian, B.V.Carlson, C.De Conti

Effect of the ¹⁸O Nuclear Density on the Nuclear Potentials of the ¹⁸O + ^{58, 60}Ni Systems

NUCLEAR REACTIONS ^58,60Ni(¹⁸O, ¹⁸O'), (¹⁸O, ¹⁷O), (¹⁸O, ¹⁶O), E=34-38 MeV; measured quasielastic, inelastic, transfer σ, σ(θ); deduced nuclear potential features. ¹⁸O deduced neutron density distribution. Comparison with previous results, model predictions.

doi: 10.1016/S0375-9474(02)01009-6
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0180.

2000DE52      Phys.Lett. 494B, 46 (2000)

C.De Conti, A.P.Galeao, F.Krmpotic

Rho-Nucleon Tensor Coupling and Charge-Exchange Resonances

NUCLEAR STRUCTURE ²⁰⁸Pb; calculated Gamow-Teller strength distribution, role of rho-nucleon tensor coupling, related features. Self-consistent RPA.

doi: 10.1016/S0370-2693(00)01192-8
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1998DE51      Phys.Lett. 444B, 14 (1998)

C.De Conti, A.P.Galeao, F.Krmpotic

Relativistic RPA for Isobaric Analogue and Gamow-Teller Resonances in Closed Shell Nuclei

NUCLEAR STRUCTURE ⁴⁸Ca, ⁹⁰Zr, ²⁰⁸Pb; calculated IAS, Gamow-Teller resonances energy, strength. Self-consistent relativistic RPA.

doi: 10.1016/S0370-2693(98)01373-2
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