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NSR database version of May 24, 2024.

Search: Author = R.C.Carrasco

Found 8 matches.

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1994CA09      Nucl.Phys. A570, 701 (1994)

R.C.Carrasco, M.J.Vicente Vacas, E.Oset

Inclusive (γ, N), (γ, NN) and (γ, Nπ) Reactions in Nuclei at Intermediate Energies

NUCLEAR REACTIONS 16O, 48Ti, 208Pb(γ, p), E=227, 390 MeV; calculated σ(θp, Ep). 16O(γ, pn), (γ, 2p), E=227-390 MeV; calculated two-nucleon emission differential σ vs missing energy. All relevant mechanisms included.

doi: 10.1016/0375-9474(94)90080-9
Citations: PlumX Metrics


1993CA30      Phys.Rev. C48, 2333 (1993)

R.C.Carrasco

Inclusive Eta Photoproduction in Nuclei

NUCLEAR REACTIONS 1H, 1n(γ, X), E=700-900 MeV; 16O, 208Pb(γ, X), E=600-900 MeV; calculated inclusive eta production σ(E). 208Pb, 16O(γ, X), E=800 MeV; calculated σ(θ) vs eta momentum.

doi: 10.1103/PhysRevC.48.2333
Citations: PlumX Metrics


1993CA35      Nucl.Phys. A565, 797 (1993)

R.C.Carrasco, J.Nieves, E.Oset

Coherent (γ, π0) Photoproduction in a Local Approximation to the Delta-Hole Model

NUCLEAR REACTIONS 40Ca, 208Pb, 12C(γ, π0), E ≈ 150-450 MeV; calculated σ(θ) vs E. 12C(γ, π0), E=290 MeV; analyzed σ(θ). Coherent pion photoproduction, Δ-hole model, local approximation.

doi: 10.1016/0375-9474(93)90005-I
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1993NI13      Nucl.Phys. A565, 785 (1993)

J.Nieves, E.Oset, R.C.Carrasco

Deeply Bound Pionic Atoms with Resonant Compton Scattering

NUCLEAR REACTIONS 41Ca(γ, γ), E=142.6-145 MeV; 4He(γ, γ), E=142.6-145, 180 MeV; 17O(γ, γ), E=142.6-145 MeV; calculated σ(θ); deduced deeply bound pionic atoms role.

doi: 10.1016/0375-9474(93)90004-H
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1992CA02      Phys.Rev. C45, 764 (1992)

R.C.Carrasco, E.Oset

Enchancement of the Nuclear Dipole Sum: Microscopic approach

NUCLEAR REACTIONS 208Pb(γ, X), E=100-400 MeV; calculated photonuclear σ(E); deduced dipole sum rule enhancement factor.

doi: 10.1103/PhysRevC.45.764
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1992CA04      Nucl.Phys. A536, 445 (1992)

R.C.Carrasco, E.Oset

Interaction of Real Photons with Nuclei from 100 to 500 MeV

NUCLEAR REACTIONS 12C, 208Pb(γ, X), E ≈ 100-500 MeV; 16O(γ, X), E ≈ 100-400 MeV; calculated σ(E). 1H(γ, π0), E=260, 320 MeV; calculated σ(θ). Real photon interaction with nuclei.

doi: 10.1016/0375-9474(92)90109-W
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1992CA16      Nucl.Phys. A541, 585 (1992)

R.C.Carrasco, E.Oset, L.L.Salcedo

Inclusive (γ, π) Reactions in Nuclei

NUCLEAR REACTIONS 12C, 208Pb(γ, X), E ≈ 100-400 MeV; calculated photonuclear σ(E)/mass. 12C, 208Pb, Cu, Sn(γ, π+X), (γ, π-X), (γ, π0X), E ≈ 200-400 MeV; calculated σ(E). 208Pb(γ, π+), (γ, π-), E ≈ 200-400 MeV; calculated σ(θ). 208Pb(γ, π+), (γ, π-), E=280-390 MeV; calculated σ(θ) vs pion momentum. 12C(γ, π+), E not given; calculated σ(θ, E(π)). Inclusive reactions, microscopic many-body theories, direct indirect photoabsorption separation.

doi: 10.1016/0375-9474(92)90222-6
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1990CH12      Nucl.Phys. A510, 573 (1990); Errata Nucl.Phys. A514, 749 (1990)

H.C.Chiang, E.Oset, R.C.Carrasco, J.Nieves, J.Navarro

Inclusive Radiative Pion Capture in Nuclei

NUCLEAR STRUCTURE A=6-209; calculated radiative pion capture widths. 6,7Li, 9Be, 10,11B, 12,13C, 14N, 16,18O, 19F, 40Ca, 209Bi; calculated radiative pion capture branching ratios. Many-body approach, Pauli blocking, medium polarization.

ATOMIC PHYSICS, Mesic-Atoms A=6-209; calculated radiative pion capture widths. 6,7Li, 9Be, 10,11B, 12,13C, 14N, 16,18O, 19F, 40Ca, 209Bi; calculated radiative pion capture branching ratios. Many-body approach, Pauli blocking, medium polarization.

doi: 10.1016/0375-9474(90)90349-Q
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