NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = M.Ericson Found 70 matches. 2022MA36 Phys.Rev. C 106, 015503 (2022) M.Martini, M.Ericson, G.Chanfray Investigation of the MicroBooNE neutrino cross sections on argon NUCLEAR REACTIONS 40Ar(ν, X), E<1.2 GeV; analyzed data on σ(E) from MicroBooNE experiment; calculated charged current inclusive flux-integrated single differential σ(E). Random phase approximation (RPA) on top of a local Fermi gas calculation.
doi: 10.1103/PhysRevC.106.015503
2021CH35 Phys.Rev. C 104, 015203 (2021) γ production in neutrino interactions with nuclei NUCLEAR REACTIONS 12C(ν, γ), (ν, γπ), E<0.5 GeV; calculated σ(E) for single γ emission, and for γ-pion production σ(E) with and without the inclusion of the 2p-2h contribution in the pion self-energy using meson exchange effects. Relevance to observation of low-energy excess of electron-like events in tMiniBooNE experiment.
doi: 10.1103/PhysRevC.104.015203
2018NI15 Phys.Rev. C 98, 054603 (2018) A.Nikolakopoulos, M.Martini, M.Ericson, N.Van Dessel, R.Gonzalez-Jimenez, N.Jachowicz Mean-field approach to reconstructed neutrino energy distributions in accelerator-based experiments
doi: 10.1103/PhysRevC.98.054603
2016MA45 Phys.Rev. C 94, 015501 (2016) M.Martini, N.Jachowicz, M.Ericson, V.Pandey, T.Van Cuyck, N.Van Dessel Electron-neutrino scattering off nuclei from two different theoretical perspectives NUCLEAR REACTIONS 12C(ν, X), E=150-750 MeV electron and muon neutrinos; calculated charged-current (CC) double differential cross section, momentum transfer versus the transferred energy, Coulomb-longitudinal and transverse contributions to cross sections, ratio of νe over νμ differential cross sections. Continuum random phase approximation (CRPA), and RPA-based calculations. Comparison with experimental data from T2K collaboration.
doi: 10.1103/PhysRevC.94.015501
2015ER01 Phys.Rev. C 91, 035501 (2015) Neutrino versus antineutrino cross sections and CP violation
doi: 10.1103/PhysRevC.91.035501
2014MA67 Phys.Rev. C 90, 025501 (2014) Inclusive and pion production neutrino-nucleus cross sections NUCLEAR REACTIONS 12C(ν, ν'), E<1.2 GeV; analyzed experimental inclusive and pion production double-differential cross section data from T2K collaboration and MiniBooNE experiments on 12C and CH2 targets, using a model based on the nuclear response functions, where the quasielastic response is treated in the random phase approximation (RPA). Discussed need for inclusion of the two-pion channel.
doi: 10.1103/PhysRevC.90.025501
2013MA49 Phys.Rev. C 87, 065501 (2013) Quasielastic and multinucleon excitations in antineutrino-nucleus interactions NUCLEAR REACTIONS 12C(ν-bar, X), E=0.2-2.0 GeV; analyzed quasielastic double differential σ(θ, E) for muonic antineutrino-nucleus collisions from MiniBooNE experiment using the random phase approximation (RPA).
doi: 10.1103/PhysRevC.87.065501
2011CH04 Phys.Rev. C 83, 015204 (2011) Scalar fields in nuclear matter: The roles of spontaneous chiral symmetry breaking and nucleon structure
doi: 10.1103/PhysRevC.83.015204
2011MA68 Phys.Rev. C 84, 055502 (2011) M.Martini, M.Ericson, G.Chanfray Neutrino quasielastic interaction and nuclear dynamics NUCLEAR REACTIONS 12C(ν, ν), E=0.2-2 GeV; analyzed quasielastic double differential σ(θ) data from MiniBooNE experiment; compared with RPA calculations.
doi: 10.1103/PhysRevC.84.055502
2010AL11 Phys.Rev. C 81, 041602 (2010) M.Alvioli, O.Benhar, M.Ericson, M.Strikman Proton decay and nuclear dynamics NUCLEAR STRUCTURE 16O; calculated proton spectral function with the Skyrme force, proton decay. Comparison with other model calculations.
doi: 10.1103/PhysRevC.81.041602
2010MA19 Phys.Rev. C 81, 045502 (2010) M.Martini, M.Ericson, G.Chanfray, J.Marteau Neutrino and antineutrino quasielastic interactions with nuclei NUCLEAR REACTIONS 12C(ν, X), (ν-bar, X), E=0.05-1.2 GeV; calculated quasielastic σ and differential σ versus energy transfer using framework of the nuclear response functions treated in the random phase approximation (RPA). Comparison with experimental data.
doi: 10.1103/PhysRevC.81.045502
2009MA69 Phys.Rev. C 80, 065501 (2009) M.Martini, M.Ericson, G.Chanfray, J.Marteau Unified approach for nucleon knock-out and coherent and incoherent pion production in neutrino interactions with nuclei NUCLEAR REACTIONS 12C(ν, π), E<1.5 GeV; calculated σ and differential σ using theory of nuclear response in random phase approximation. Comparison with experimental data.
doi: 10.1103/PhysRevC.80.065501
2007CH06 Phys.Rev. C 75, 015206 (2007) QCD susceptibilities and nuclear matter saturation in a chiral theory: Inclusion of pion loops
doi: 10.1103/PhysRevC.75.015206
2007ER06 Eur.Phys.J. A 34, 215 (2007) Constraints on nuclear-matter properties from QCD susceptibilities
doi: 10.1140/epja/i2007-10498-x
2006CH15 Eur.Phys.J. A 27, 191 (2006) G.Chanfray, D.Davesne, M.Ericson, M.Martini Two-pion production processes, chiral symmetry and NN interaction in the medium
doi: 10.1140/epja/i2005-10245-5
2005CH46 Eur.Phys.J. A 25, 151 (2005) QCD susceptibilities and nuclear-matter saturation in a relativistic chiral theory
doi: 10.1140/epja/i2005-10074-6
2003CH09 Eur.Phys.J. A 16, 291 (2003) Fluctuations of the quark densities in nuclei
doi: 10.1140/epja/i2002-10078-8
2003CH28 Phys.Lett. B 563, 61 (2003) G.Chanfray, M.Ericson, M.Oertel In-medium modification of the isovector pion-nucleon amplitude
doi: 10.1016/S0370-2693(03)00596-3
2003CH50 Phys.Rev. C 68, 035209 (2003) G.Chanfray, M.Ericson, P.A.M.Guichon Scalar susceptibility and chiral symmetry restoration in nuclei
doi: 10.1103/PhysRevC.68.035209
2003ER01 Phys.Rev. C 67, 022201 (2003) Nuclear modification of transverse-longitudinal structure function ratio NUCLEAR STRUCTURE 1H, 14N; calculated structure functions, transverse-longitudinal admixture, nuclear effects.
doi: 10.1103/PhysRevC.67.022201
2003ER05 Eur.Phys.J. A 18, 463 (2003) Scalar and pseudoscalar QCD susceptibilities in nuclei
doi: 10.1140/epja/i2002-10260-0
2003ER06 Prog.Theor.Phys.(Kyoto), Suppl. 149, 121 (2003) Scalar and Pseudoscalar Susceptibilities in Nuclei
doi: 10.1143/PTPS.149.121
2001CH27 Phys.Rev. C63, 055202 (2001) G.Chanfray, M.Ericson, P.A.M.Guichon Chiral Symmetry and Quantum Hadrodynamics
doi: 10.1103/PhysRevC.63.055202
2001DE03 Nucl.Phys. A680, 250c (2001) J.Delorme, M.Ericson, P.A.M.Guichon, A.W.Thomas Mass Reduction as Signal of Chiral Symmetry Restoration
doi: 10.1016/S0375-9474(00)00422-X
2001ER03 Nucl.Phys. A690, 110c (2001) Role of Mesons in Chiral Symmetry Restoration and Associated Signals
doi: 10.1016/S0375-9474(01)00935-6
2000BA40 Phys.Rev. C61, 055202 (2000) J.-L.Ballot, M.Ericson, M.R.Robilotta Quark Condensate in the Deuteron NUCLEAR STRUCTURE 2H; analyzed many-body effects quark condensate in the deuteron. Feynman-Hellmann theorem.
doi: 10.1103/PhysRevC.61.055202
2000CH26 Eur.Phys.J. A 8, 283 (2000) G.Chanfray, D.Davesne, J.Delorme, M.Ericson, J.Marteau Pion Scalar Density and Chiral Symmetry Restoration at Finite Temperature and Density
doi: 10.1007/s100500070111
2000DE06 Phys.Rev. C61, 025202 (2000) J.Delorme, M.Ericson, P.A.M.Guichon, A.W.Thomas Correlator Mixing and Mass Reduction as Signals of Chiral Symmetry Restoration
doi: 10.1103/PhysRevC.61.025202
2000ER03 Nucl.Phys. A663-664, 369c (2000) M.Ericson, G.Chanfray, J.Delorme, M.Rosa-Clot Manifestations of Chiral Symmetry Restoration in Photon Reactions
doi: 10.1016/S0375-9474(99)00619-3
2000MA26 Nucl.Phys. A663-664, 783c (2000) J.Marteau, J.Delorme, M.Ericson Nuclear Correlation Effects in Neutrino-Oxygen Interactions and the Atmospheric Neutrino Anomaly NUCLEAR REACTIONS 16O(ν, X), E=1 GeV; calculated σ(E, θ); deduced contributions. Implications for atmospheric neutrino interactions discussed.
doi: 10.1016/S0375-9474(99)00743-5
2000MA59 Nucl.Instrum.Methods Phys.Res. A451, 76 (2000) J.Marteau, J.Delorme, M.Ericson Nuclear Effects in Neutrino-Nucleus Interactions NUCLEAR REACTIONS 16O(ν, X), E=0.1-5 GeV; calculated σ; deduced nuclear contributions. Implications for detection of atmospheric events discussed.
doi: 10.1016/S0168-9002(00)00375-2
1999BE73 Nucl.Phys. A661, 661c (1999) M.J.Bennett, M.Bobrek, J.G.Boissevain, C.L.Britton, J.Chang, R.Conway, R.Cunningham, M.S.Emery, M.N.Ericson, S.-Y.Fung, S.Hahn, H.W.van Hecke, D.Jaffe, J.H.Kang, S.Y.Kim, Y.G.Kim, L.J.Marek, J.A.Moore, J.H.Park, G.Richardson, S.S.Ryu, B.R.Schlei, T.Shiina, J.Simon-Gillo, G.Smith, C.Y.Soon, J.P.Sullivan, Y.Takahashi, G.Xu The PHENIX Multiplicity and Vertex Detector
doi: 10.1016/S0375-9474(99)85112-4
1999CH16 Phys.Lett. 455B, 39 (1999) G.Chanfray, J.Delorme, M.Ericson, M.Rosa-Clot Pion Number and Correlator Mixing
doi: 10.1016/S0370-2693(99)00473-6
1999ER03 Nucl.Phys. (Supplement) A654, 483c (1999) M.Ericson, G.Chanfray, J.Delorme Manifestation of Chiral Symmetry Restoration in a Dense Medium
doi: 10.1016/S0375-9474(00)88483-3
1998AL13 Nucl.Phys. A634, 233 (1998) W.M.Alberico, G.Chanfray, J.Delorme, M.Ericson, A.Molinari The Semi-Classical Approach to the Exclusive Electron Scattering
doi: 10.1016/S0375-9474(98)00160-2
1998CH23 Nucl.Phys. A637, 421 (1998) G.Chanfray, J.Delorme, M.Ericson Chiral Symmetry Restoration and Parity Mixing
doi: 10.1016/S0375-9474(98)00237-1
1998ER04 Acta Phys.Pol. B29, 2349 (1998) Chiral Symmetry Restoration and Parity Mixing
1996CH40 Phys.Lett. 388B, 673 (1996) G.Chanfray, M.Ericson, J.Wambach The Quark Condensate at Finite Temperature
doi: 10.1016/S0370-2693(96)01209-9
1996DE26 Nucl.Phys. A603, 239 (1996) J.Delorme, G.Chanfray, M.Ericson Chiral Lagrangians and Quark Condensate in Nuclei
doi: 10.1016/0375-9474(96)80001-8
1996SZ01 Nucl.Phys. A596, 397 (1996) A.Szczurek, M.Ericson, H.Holtmann, J.Speth Testing the Meson Cloud in the Nucleon in Drell-Yan Processes NUCLEAR REACTIONS 1n, 1H(p, p), E not given; calculated dilepton production K-factors vs x(F). Meson cloud model.
doi: 10.1016/0375-9474(95)00401-7
1995DE39 Phys.Rev. C52, 2222 (1995) J.Delorme, M.Ericson, T.Ericson, P.Vogel Pion and Neutron Production by Cosmic-Ray Muons Underground NUCLEAR REACTIONS C(γ, X), E ≤ 100 GeV; calculated photoabsorption, π+ photoproduction σ(E), primary neutron production yields, other aspects. Equivalent photon method.
doi: 10.1103/PhysRevC.52.2222
1994DE08 Phys.Rev. C49, R1763 (1994) s-Wave Pion-Nucleus Interaction and Weak Coupling Constants
doi: 10.1103/PhysRevC.49.R1763
1994ER04 Phys.Rev. C49, R2293 (1994) Possible Way Out of the (p, n) Puzzle NUCLEAR REACTIONS 40Ca(p, n), E not given; calculated longitudinal, transverse response function vs energy transfer; deduced NN-interaction pion-exchange part medium renormalization implications. Comparison of different models.
doi: 10.1103/PhysRevC.49.R2293
1994ER05 Phys.Lett. 328B, 259 (1994) High Energy Gamow-Teller Strength in Double Beta Decay
doi: 10.1016/0370-2693(94)91476-1
1994ER07 Nucl.Phys. A577, 147c (1994) The s-Wave π-Nucleus Interaction and the (p, n) Puzzle NUCLEAR REACTIONS Ca(p, n), E not given; compiled, reviewed longitudinal response data, analyses; deduced π-nucleus s-wave interaction, (p, n) data connection.
doi: 10.1016/0375-9474(94)90848-6
1993LA07 Nucl.Phys. A555, 237 (1993) I.Laktineh, W.M.Alberico, J.Delorme, M.Ericson Coherent Photoproduction of Neutral Pions in Nuclei as a Detector of Nuclear Pionic Modes NUCLEAR REACTIONS 16O(π+, π+), (π-, π-), E=303 MeV; calculated averaged σ(θ). 16O(π+, π+), (π-, π-), E ≈ 160-500 MeV; 12C(π+, π+), (π-, π-), E ≈ 200-500 MeV; calculated averaged σ(E). 4He, 12C, 16O(γ, π0); calculated σ(E). 12C(γ, π0), E=235 MeV; calculated σ(θ). Coherent production.
doi: 10.1016/0375-9474(93)90321-N
1989AL28 Phys.Lett. 233B, 37 (1989) W.M.Alberico, M.Ericson, A.Molinari, Z.-X.Wang The Δ in the Nuclear Quasi-Elastic Peak NUCLEAR STRUCTURE 40Ca, 12C; calculated transverse response function. Quasielastic peak region, Δ degree of freedom.
doi: 10.1016/0370-2693(89)90611-4
1989ER03 Nucl.Phys. A495, 602 (1989) The Effects of Pion-Exchange Corrections on the 2ν ββ Decay Nuclear Matrix Elements RADIOACTIVITY 48Ca(2β); calculated two-neutrino accompanied β-decay matrix element. Pion exchange corrections.
doi: 10.1016/0375-9474(89)90362-X
1988AL20 Phys.Rev. C38, 109 (1988) W.M.Alberico, A.De Pace, M.Ericson, M.B.Johnson, A.Molinari Spin-Isospin Nuclear Responses with Hadronic Probes NUCLEAR REACTIONS 40Ca(3He, t), E not given; calculated σ(θt, Et). RPA spin-isospin nuclear responses.
doi: 10.1103/PhysRevC.38.109
1988ER05 Z.Phys. A331, 369 (1988) M.Ericson, W.Leidemann, G.Orlandini Proton-Neutron Correlations and the Longitudinal Nuclear Response NUCLEAR STRUCTURE 12C, 40Ca; calculated longitudinal response function; deduced p-n correlations role.
1988VO07 Phys.Lett. 212B, 259 (1988) P.Vogel, M.Ericson, J.D.Vergados Sum Rules for Two-Particle Operators and Double Beta Decay RADIOACTIVITY 76Ge, 54Fe(2β); calculated double Gamow-Teller, Fermi operator sum rules, Gamow-Teller transition strength.
doi: 10.1016/0370-2693(88)91313-5
1987AL04 Phys.Lett. 183B, 135 (1987) W.M.Alberico, A.De Pace, M.Ericson, M.B.Johnson, A.Molinari Spin-Isospin Surface Responses NUCLEAR REACTIONS Ca, Pb(p, p'), E=20-100 MeV; calculated spin-isospin longitudinal, transverse responses, free isovector response ratio. RPA calculations.
doi: 10.1016/0370-2693(87)90426-6
1987AL05 Nucl.Phys. A462, 269 (1987) W.M.Alberico, P.Czerski, M.Ericson, A.Molinari Inclusive Charge Longitudinal Response in Finite Nuclei NUCLEAR STRUCTURE 12C, 40Ca, 56Fe; calculated charge dynamic, static longitudinal structure factors. Semi-classical RPA theory.
doi: 10.1016/0375-9474(87)90548-3
1987AL24 Nucl.Phys. A475, 233 (1987) W.M.Alberico, G.Chanfray, M.Ericson, A.Molinari Proton and Neutron Contributions to the Charge Longitudinal Response NUCLEAR STRUCTURE 12C, 40,48Ca; calculated charge longitudinal response function; deduced p, n contributions, differences. RPA.
doi: 10.1016/0375-9474(87)90164-3
1987ER02 Phys.Lett. 188B, 11 (1987) Compton Scattering and Pion Number in Nuclei NUCLEAR STRUCTURE 2H; calculated spin-independent Compton amplitude vs pion excess number per nucleon.
doi: 10.1016/0370-2693(87)90696-4
1986AL13 Phys.Rev. C34, 977 (1986) W.M.Alberico, A.Molinari, A.De Pace, M.Ericson, M.B.Johnson Random Phase Approximation Spin-Isospin Nuclear Response in the Deep Inelastic Region NUCLEAR REACTIONS 40Ca(e, e'), E not given; calculated longitudinal response, transverse dynamic structure factors. RPA.
doi: 10.1103/PhysRevC.34.977
1986ER04 Z.Phys. A324, 373 (1986) The Electromagnetic Polarizability and the Swelling of Nucleons in the Nucleus NUCLEAR STRUCTURE 1H; calculated charge radius, electromagnetic polarizability changes. Nuclear enviornment pion cloud distortion.
1986OR03 Phys.Lett. 179B, 201 (1986) G.Orlandini, M.Traini, M.Ericson Spin-Dependent Isoscalar Response Functions and Interpretation of Polarization-Transfer Measurements NUCLEAR REACTIONS 4He, 16O, 40Ca(p, p'), E not given; calculated isoscalar, isovector spin-isospin response functions; deduced model parameters.
doi: 10.1016/0370-2693(86)90566-6
1985DE10 J.Phys.(London) G11, 343 (1985) J.Delorme, M.Ericson, A.Figureau Lorentz-Lorenz Quenching for the Gamow-Teller Sum Rule NUCLEAR STRUCTURE A ≈ 10-250; calculated Gamow-Teller Lorentz-Lorenz sum rule quenching.
doi: 10.1088/0305-4616/11/3/012
1985ST09 Phys.Lett. 156B, 291 (1985) U.Stroth, R.W.Hasse, P.Schuck, W.M.Alberico, A.Molinari, M.Ericson On the Nuclear Isovector Spin Response in the Quasielastic Peak Region NUCLEAR REACTIONS 208Pb(p, p'), E not given; calculated longitudinal, transverse nuclear response. Nonlocal mean field plus particle-hole interactions. NUCLEAR STRUCTURE 40Ca; calculated structure function. 48Ca, 12C; calculated transverse nuclear response function.
doi: 10.1016/0370-2693(85)91611-9
1984AL04 Phys.Lett. 136B, 307 (1984) W.M.Alberico, M.Ericson, A.Molinari Unifying Photon and Pion Absorption NUCLEAR REACTIONS 56Fe(e, e'X), E not given; calculated transverse magnetic response function vs excitation. Deep inelastic inclusive reaction, meson exchange, nucleon-nucleon correlation, 2p-2h contribution.
doi: 10.1016/0370-2693(84)92009-4
1984AL27 Phys.Rev. C30, 1776 (1984) W.M.Alberico, M.Ericson, A.Molinari Interpretation of the Polarization Transfer Measurement in the (p, p') Reaction on 208Pb NUCLEAR STRUCTURE 40Ca; calculated transverse magnetic response vs excitation energy. 40,48Ca, 56Fe; calculated transverse sum rule function; deduced inconclusivity of volume spin-isospin response nature derived from 208Pb(p, p') analysis.
doi: 10.1103/PhysRevC.30.1776
1984AL28 Ann.Phys.(New York) 154, 356 (1984) W.M.Alberico, M.Ericson, A.Molinari The Role of Two Particle-Two Hole Excitations in the Spin-Isospin Nuclear Response NUCLEAR REACTIONS 56Fe(e, e'), E at 210-410 MeV/c; calculated transverse magnetic response function vs E(e'). 208Pb(γ, X), E ≈ 25-175 MeV; calculated quasideuteron component photoabsorption σ(E). Microscopic approach, meson exchange currents, nucleon-nucleon interactions.
doi: 10.1016/0003-4916(84)90155-6
1984ER04 J.Phys.(Paris), Colloq.C4, 489 (1984); See 1984Er07 Recent Aspects of the Nuclear Spin Isospin Response Function
1984ER07 J.Phys.(Paris), Colloq.C-4, 489 (1984) Recent Aspects of the Nuclear Spin Isospin Response Function NUCLEAR REACTIONS 56Fe(e, e'), E=370 MeV; calculated transverse response functions. NUCLEAR STRUCTURE 2H, Fe; calculated structure function ratio.
1982AL12 Nucl.Phys. A379, 429 (1982) W.M.Alberico, M.Ericson, A.Molinari Quenching and Hardening in the Transverse Quasi-Elastic Peak NUCLEAR REACTIONS 56Fe(e, e'), E=0.1-14 GeV; 12C(e, e'), E=120-560 MeV; calculated transverse magnetic response function; deduced quenching, hardening effects. RPA, particle-hole, isobar-hole interactions.
doi: 10.1016/0375-9474(82)90007-0
1981ER11 Nucl.Phys. A372, 377 (1981) M.Ericson, P.Guichon, R.D.Viollier Nuclear Axial Polarizability and the α + α Interaction NUCLEAR REACTIONS 4He(α, α), E=25-50 MeV; calculated phase shifts, (L)≥4; deduced nuclear polarization. Two pion exchange, static pion field.
doi: 10.1016/0375-9474(81)90041-5
1980DE04 Phys.Lett. 89B, 327 (1980) J.Delorme, M.Ericson, A.Figureau, N.Giraud Critical Opalescence of the Nuclear Pion Field: A Possible Evidence in the M1 (15.11 MeV) Form Factor of 12C NUCLEAR REACTIONS 12C(e, e'), E not given; calculated nuclear pion field, squared T=1 magnetic form factors. Nuclear polarization, nucleon-, isobar-hole excitations.
doi: 10.1016/0370-2693(80)90135-5
1975ER03 Nucl.Phys. A241, 487 (1975) Difference of Total Cross Sections for π± on 9Be and the π-9Be Effective Coupling Constant NUCLEAR REACTIONS 9Be(π-, X), (π+, X), E < 100 MeV; calculated cross-section difference.
doi: 10.1016/0375-9474(75)90399-1
1972ER02 Phys.Lett. 38B, 359 (1972) Features of the π Nuclear Scattering at Low Energy NUCLEAR REACTIONS 12C(π-, π-), (π+, π+), E < 120 MeV; calculated σ(E), Argand plots. 208Pb(π-, π-), (π+, π+), E not given; calculated Argand plots.
doi: 10.1016/0370-2693(72)90156-6
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