NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = A.Parreno Found 44 matches. 2022TE06 Few-Body Systems 63, 67 (2022) I.Tews, Z.Davoudi, A.Ekstrom, J.D.Holt, K.Becker, R.Briceno, D.J.Dean, W.Detmold, C.Drischler, T.Duguet, E.Epelbaum, A.Gasparyan, J.Gegelia, J.R.Green, H.W.Griesshammer, A.D.Hanlon, M.Heinz, H.Hergert, M.Hoferichter, M.Illa, D.Kekejian, A.Kievsky, S.Konig, H.Krebs, K.D.Launey, D.Lee, P.Navratil, A.Nicholson, A.Parreno, D.R.Phillips, M.Ploszajczak, X.-L.Ren, T.R.Richardson, C.Robin, G.H.Sargsyan, M.J.Savage, M.R.Schindler, P.E.Shanahan, R.P.Springer, A.Tichai, U.van Kolck, M.L.Wagman, A.Walker-Loud, C.-J.Yang, X.Zhang Nuclear Forces for Precision Nuclear Physics: A Collection of Perspectives
doi: 10.1007/s00601-022-01749-x
2018MA53 Phys.Rev. C 98, 025208 (2018) Effects of ΛΛ-ΞN mixing in the decay of S= - 2 hypernuclei NUCLEAR STRUCTURE 6He; calculated nonmesonic weak decay of the doubly strange (ΛΛ) hypernucleus, individual and combined meson-exchange contributions to the nonmesonic decay rate using a model that considers the exchange of pseudoscalar and vector mesons.
doi: 10.1103/PhysRevC.98.025208
2016DE04 Phys.Rev.Lett. 116, 112301 (2016) W.Detmold, K.Orginos, A.Parreno, M.J.Savage, B.C.Tiburzi, S.R.Beane, E.Chang, for the NPLQCD Collaboration Unitary Limit of Two-Nucleon Interactions in Strong Magnetic Fields
doi: 10.1103/PhysRevLett.116.112301
2016PE12 Nucl.Phys. A954, 213 (2016) A.Perez-Obiol, D.R.Entem, B.Julia-Diaz, A.Parreno Next-to-leading order effective field theory ΛN → NN potential in coordinate space
doi: 10.1016/j.nuclphysa.2016.04.039
2013BE28 Phys.Rev. C 88, 024003 (2013) S.R.Beane, E.Chang, S.D.Cohen, W.Detmold, P.Junnarkar, H.W.Lin, T.C.Luu, K.Orginos, A.Parreno, M.J.Savage, A.Walker-Loud, for the NPLQCD Collaboration Nucleon-nucleon scattering parameters in the limit of SU(3) flavor symmetry
doi: 10.1103/PhysRevC.88.024003
2013PE05 Phys.Rev. C 87, 044614 (2013) A.Perez-Obiol, D.R.Entem, B.Julia-Diaz, A.Parreno One-loop contributions in the effective field theory for the ΛN → NN transition
doi: 10.1103/PhysRevC.87.044614
2013PE17 Nucl.Phys. A914, 199c (2013) A.Perez-Obiol, D.R.Entem, B.Julia-Diaz, A.Parreno Higher order contributions to the weak ΛN → NN interaction in effective field theory
doi: 10.1016/j.nuclphysa.2013.12.122
2012BA06 Phys.Rev. C 85, 024321 (2012) E.Bauer, G.Garbarino, A.Parreno, A.Ramos Microscopic approach to the proton asymmetry in the nonmesonic weak decay of Λ hypernuclei NUCLEAR STRUCTURE 12C; calculated intrinsic asymmetry parameter, nonmesonic decay widths for polarized hypernucleus. Microscopic diagrammatic nuclear matter formalism. Comparison with experimental data from KEK.
doi: 10.1103/PhysRevC.85.024321
2012PA10 Nucl.Phys. A881, 14 (2012) Binding two baryons in Lattice QCD
doi: 10.1016/j.nuclphysa.2012.02.001
2011PE19 Phys.Rev. C 84, 024606 (2011) A.Perez-Obiol, A.Parreno, B.Julia-Diaz Constraints on effective field theory parameters for the ΛN → N N transition
doi: 10.1103/PhysRevC.84.024606
2010BA13 Nucl.Phys. A836, 199 (2010) E.Bauer, G.Garbarino, A.Parreno, A.Ramos Single and double coincidence nucleon spectra in the weak decay of Λ-hypernuclei NUCLEAR STRUCTURE 12C; calculated hypernucleus non-mesonic weak decay widths and associated decay observables using a nuclear matter model with local density approximation. Comparison with data.
doi: 10.1016/j.nuclphysa.2010.01.246
2010PA34 Nucl.Phys. A835, 184c (2010) A.Parreno, and the NPLQCD Collaboration YN and YY interactions from lattice QCD simulations
doi: 10.1016/j.nuclphysa.2010.01.192
2008CH11 Nucl.Phys. A804, 162 (2008) C.Chumillas, G.Garbarino, A.Parreno, A.Ramos A theoretical overview of hypernuclear weak decay NUCLEAR STRUCTURE 5He, 12C; calculated non-mesonic weak decay widths and asymmetry parameters in hypernuclei. Comparison with data.
doi: 10.1016/j.nuclphysa.2008.01.021
2007BE52 Nucl.Phys. A794, 62 (2007) S.R.Beane, P.F.Bedaque, T.C.Luu, K.Orginos, E.Pallante, A.Parreno, M.J.Savage, and the NPLQCD Collaboration Hyperon-nucleon scattering from fully-dynamical lattice QCD
doi: 10.1016/j.nuclphysa.2007.07.006
2007CH67 Nucl.Phys. A791, 329 (2007) C.Chumillas, A.Parreno, A.Ramos The Δ N → N N transition in finite nuclei
doi: 10.1016/j.nuclphysa.2007.04.022
2007CH78 Phys.Lett. B 657, 180 (2007) C.Chumillas, G.Garbarino, A.Parreno, A.Ramos Two-pion-exchange in the non-mesonic weak decay of Λ-hypernuclei NUCLEAR STRUCTURE 5He, 11B, 12C; calculated non-mesonic weak decay parameters in hypernuclei including final state interactions. Comparison with data.
doi: 10.1016/j.physletb.2007.08.094
2005AL08 Phys.Rev.Lett. 94, 082501 (2005) W.M.Alberico, G.Garbarino, A.Parreno, A.Ramos Asymmetries in the Nonmesonic Weak Decay of Polarized Λ Hypernuclei NUCLEAR STRUCTURE 5He, 11B, 12C; calculated proton angular distributions, related parameters for nonmesonic weak decay of polarized hypernuclei; deduced final state interaction effects.
doi: 10.1103/PhysRevLett.94.082501
2005BE02 Nucl.Phys. A747, 55 (2005) S.R.Beane, P.F.Bedaque, A.Parreno, M.J.Savage A framework for exploring the interactions and decays of hyperons with lattice QCD
doi: 10.1016/j.nuclphysa.2004.09.081
2005GA24 Nucl.Phys. A754, 137c (2005) G.Garbarino, A.Parreno, A.Ramos Non-mesonic weak decay of Λ-hypernuclei: a new determination of the Γn/Γp ratio NUCLEAR STRUCTURE 5He, 12C; analyzed hypernucleus decay rates, related observables.
doi: 10.1016/j.nuclphysa.2004.12.071
2005PA38 Nucl.Phys. A754, 127c (2005) A.Parreno, C.Bennhold, B.R.Holstein An EFT for the weak ΛN interaction NUCLEAR STRUCTURE 5He, 11B, 12C; analyzed hypernucleus decay rates, related features; deduced parameters. Effective field theory framework.
doi: 10.1016/j.nuclphysa.2005.01.008
2004BE07 Phys.Lett. B 585, 106 (2004) S.R.Beane, P.F.Bedaque, A.Parreno, M.J.Savage Two nucleons on a lattice
doi: 10.1016/j.physletb.2004.02.007
2004GA26 Phys.Rev. C 69, 054603 (2004) G.Garbarino, A.Parreno, A.Ramos Towards a solution of the Γn/Γp puzzle in the nonmesonic weak decay of Λ hypernuclei NUCLEAR STRUCTURE 5He, 12C; calculated En, Ep, coincidence observables for hypernucleus nonmesonic decay; deduced dependence on neutron- and proton-induced hyperon decay rates.
doi: 10.1103/PhysRevC.69.054603
2004PA39 Phys.Rev. C 70, 051601 (2004) A.Parreno, C.Bennhold, B.R.Holstein ΛN → NN weak interaction in effective-field theory NUCLEAR STRUCTURE 5He, 11B, 12C; calculated hypernucleus weak decay rates, related observables.
doi: 10.1103/PhysRevC.70.051601
2003GA24 Phys.Rev.Lett. 91, 112501 (2003) G.Garbarino, A.Parreno, A.Ramos Nucleon-Nucleon Coincidence Spectra in the Nonmesonic Weak Decay of Λ Hypernuclei and the Γn/Γp Puzzle NUCLEAR STRUCTURE 5He, 12C; calculated nucleon-nucleon coincidence spectra for nonmesonic weak decay of hypernuclei, ratio of neutron to proton decay widths, final state interaction effects.
doi: 10.1103/PhysRevLett.91.112501
2003PA47 Nucl.Phys. A721, 967c (2003) A.Parreno, A.Ramos, G.Garbarino, C.Bennhold Λ- and ΛΛ-hypernuclear decay predictions in a OME model. NUCLEAR STRUCTURE 5,6He, 12C; calculated hypernucleus decay widths. Meson-exchange model, comparison with data.
doi: 10.1016/S0375-9474(03)01261-2
2002PA02 Phys.Rev. C65, 015204 (2002) Final-State Interactions in Hypernuclear Decay
doi: 10.1103/PhysRevC.65.015204
2002PA03 Phys.Rev. C65, 015205 (2002) A.Parreno, A.Ramos, C.Bennhold Novel Weak Decays in Doubly Strange Systems NUCLEAR STRUCTURE 6He; calculated ΛΛ hypernucleus partial weak decay rates.
doi: 10.1103/PhysRevC.65.015205
2001HA18 Phys.Rev. C63, 044318 (2001) Role of Deformation in the Nonmesonic Decay of Light Hypernuclei NUCLEAR STRUCTURE 9Be; calculated hypernucleus nonmesonic decay rate, asymmetry parameter; deduced deformation effects.
doi: 10.1103/PhysRevC.63.044318
2001PA19 Nucl.Phys. A684, 389c (2001) Chiral Unitary Approach to the Low Energy πN Scattering NUCLEAR REACTIONS 1H(π-, X), E ≈ 700-1800 MeV; analyzed data; deduced coupling constants. Chiral unitary approach.
doi: 10.1016/S0375-9474(01)00404-3
2000NA29 Nucl.Phys. A678, 187 (2000) J.C.Nacher, A.Parreno, E.Oset, A.Ramos, A.Hosaka, M.Oka Chiral Unitary Approach to the πN*N*, νN*N* Couplings for the N*(1535) Resonance
doi: 10.1016/S0375-9474(00)00311-0
2000OS03 Nucl.Phys. A663-664, 497c (2000) E.Oset, A.Hosaka, J.C.Nacher, M.Oka, J.A.Oller, A.Parreno, J.R.Pelaez, A.Ramos, H.Toki SU(3) Chiral Approach to Meson and Baryon Dynamics
doi: 10.1016/S0375-9474(99)00640-5
2000OS04 Nucl.Phys. A670, 111c (2000) E.Oset, J.A.Oller, J.R.Pelaez, A.Ramos, H.C.Chiang, F.Guerrero, S.Hirenzaki, T.S.H.Lee, E.Marco, J.C.Nacher, Y.Okumura, A.Parreno, H.Toki, M.Vicente-Vacas Recent Progress on the Chiral Unitary Approach to Meson Meson and Meson Baryon Interactions NUCLEAR REACTIONS 1H(γ, K+X), E=1.7 GeV; calculated pion, hyperon production σ. Unitary approach.
doi: 10.1016/S0375-9474(00)00080-4
2000PA29 Nucl.Phys. A670, 257c (2000) A.Parreno, C.Bennhold, A.Ramos Decay of Hypernuclei NUCLEAR STRUCTURE 12C; calculated hypernucleus decay observables.
doi: 10.1016/S0375-9474(00)00108-1
2000PA65 Acta Phys.Hung.N.S. 11, 397 (2000) A.Parreno, C.Bennhold, A.Ramos, M.Zarei Decay of Single- and Double-Λ Hypernuclei NUCLEAR STRUCTURE 5He, 11B, 12C; calculated hypernuclei non-mesonic and baryonic decay widths and branching ratios. Comparison with data.
1999PA15 Phys.Rev. C59, 2122 (1999) A.Parreno, A.Ramos, N.G.Kelkar, C.Bennhold Weak Strangeness Production Reaction pn → pΛ in a One-Boson-Exchange Model NUCLEAR REACTIONS 1n(p, X), E at 900-1200 MeV/c; calculated hyperon production σ, σ(θ); deduced sensitivity to hyperon-nucleon interaction. One-meson exchange model.
doi: 10.1103/PhysRevC.59.2122
1998GO06 Nucl.Phys. A631, 740c (1998) J.Golak, K.Miyagawa, H.Kamada, H.Witala, W.Glockle, A.Parreno, A.Ramos, C.Bennhold The Nonmesonic Weak Decay of Hypertriton NUCLEAR STRUCTURE 3H; calculated hypernucleus nonmesonic decay rate.
doi: 10.1016/S0375-9474(98)00102-X
1998PA29 Nucl.Phys. A639, 333c (1998) A.Parreno, A.Ramos, C.Bennhold, K.Maltman Violation of the ΔI = 1/2 Rule in the Nonmesonic Weak Decay of Λ Hypernuclei NUCLEAR STRUCTURE 12C; calculated hypernucleus weak decay observables; deduced ΔI=3/2 contributions.
doi: 10.1016/S0375-9474(98)00292-9
1998PA30 Phys.Lett. 435B, 1 (1998) A.Parreno, A.Ramos, C.Bennhold, K.Maltman Violation of the ΔI = 1/2 Rule in the Nonmesonic Weak Decay of Hypernuclei NUCLEAR STRUCTURE 12C; calculated hypernucleus decay observables; deduced sensitivity to ΔI=3/2 amplitudes.
doi: 10.1016/S0370-2693(98)00832-6
1998RA23 Nucl.Phys. A639, 307c (1998) A.Ramos, A.Parreno, C.Bennhold, E.Oset, L.L.Salcedo, M.J.Vincente-Vacas Non-Mesonic Weak Decay of Λ Hypernuclei NUCLEAR STRUCTURE 12C, 16O, 20Ne, 40Ca, 56Fe, 89Y, 208Pb; calculated hypernuclei mesonic, one-, two-nucleon induced decay rates. 12C; calculated neutron spectra, proton spectra from hypernucleus decay. 208Pb; calculated proton, neutron multiplicities from hypernucleus decay.
doi: 10.1016/S0375-9474(98)00288-7
1997GO04 Phys.Rev. C55, 2196 (1997); Erratum Phys.Rev. C56, 2892 (1997) J.Golak, K.Miyagawa, H.Kamada, H.Witala, W.Glockle, A.Parreno, A.Ramos, C.Bennhold Nonmesonic Weak Decay of the Hypertriton NUCLEAR STRUCTURE A=3; calculated hypertriton nonmesonic weak decay rate. Three-body Faddeev equations.
doi: 10.1103/PhysRevC.55.2196
1997PA18 Phys.Rev. C56, 339 (1997) A.Parreno, A.Ramos, C.Bennhold Weak Decay of Hypernuclei NUCLEAR STRUCTURE A=5; A=11; A=12; calculated ΛN to NN decay rate of 5He(Λ), 11B(Λ), 12C(Λ) hypernuclei. Shell model, realistic short-range correlations.
doi: 10.1103/PhysRevC.56.339
1995PA12 Nucl.Phys. A585, 373c (1995) Short Range Correlations in the Weak Decay of (Lambda) Hypernuclei NUCLEAR STRUCTURE A=5; calculated (lambda)N → NN decay rate, hypernucleus.
doi: 10.1016/0375-9474(94)00615-T
1995PA18 Phys.Rev. C51, 2477 (1995) Short Range Correlations in the Weak Decay of (Lambda) Hypernuclei NUCLEAR STRUCTURE A=5; A=12; calculated lambda N → NN decay rate of 5He(lambda), 12C(lambda) hypernuclei. Short range correlations, schematic microscopic model.
doi: 10.1103/PhysRevC.51.2477
1995PA36 Phys.Rev. C52, R1768 (1995); Erratum Phys.Rev. C54, 1500 (1996) A.Parreno, A.Ramos, C.Bennhold Role of the ρ Meson in the Nonmesionic Hypernuclear Decay NUCLEAR STRUCTURE A=12; calculated ρ-, π-exchange contribution to (Λ)N-, NN-decay rate in hypernucleus 12C(Λ); deduced ρ-exchange central potential role.
doi: 10.1103/PhysRevC.52.R1768
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