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NSR database version of May 22, 2024.

Search: Author = M.Ericson

Found 70 matches.

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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
Citations: PlumX Metrics

2021CH35      Phys.Rev. C 104, 015203 (2021)

G.Chanfray, M.Ericson

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2015ER01      Phys.Rev. C 91, 035501 (2015)

M.Ericson, M.Martini

Neutrino versus antineutrino cross sections and CP violation

doi: 10.1103/PhysRevC.91.035501
Citations: PlumX Metrics

2014MA67      Phys.Rev. C 90, 025501 (2014)

M.Martini, M.Ericson

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
Citations: PlumX Metrics

2013MA49      Phys.Rev. C 87, 065501 (2013)

M.Martini, M.Ericson

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
Citations: PlumX Metrics

2011CH04      Phys.Rev. C 83, 015204 (2011)

G.Chanfray, M.Ericson

Scalar fields in nuclear matter: The roles of spontaneous chiral symmetry breaking and nucleon structure

doi: 10.1103/PhysRevC.83.015204
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
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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
Citations: PlumX Metrics

2007CH06      Phys.Rev. C 75, 015206 (2007)

G.Chanfray, M.Ericson

QCD susceptibilities and nuclear matter saturation in a chiral theory: Inclusion of pion loops

doi: 10.1103/PhysRevC.75.015206
Citations: PlumX Metrics

2007ER06      Eur.Phys.J. A 34, 215 (2007)

M.Ericson, G.Chanfray

Constraints on nuclear-matter properties from QCD susceptibilities

doi: 10.1140/epja/i2007-10498-x
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2005CH46      Eur.Phys.J. A 25, 151 (2005)

G.Chanfray, M.Ericson

QCD susceptibilities and nuclear-matter saturation in a relativistic chiral theory

doi: 10.1140/epja/i2005-10074-6
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2003CH09      Eur.Phys.J. A 16, 291 (2003)

G.Chanfray, M.Ericson

Fluctuations of the quark densities in nuclei

doi: 10.1140/epja/i2002-10078-8
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2003ER01      Phys.Rev. C 67, 022201 (2003)

M.Ericson, S.Kumano

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
Citations: PlumX Metrics

2003ER05      Eur.Phys.J. A 18, 463 (2003)

M.Ericson, G.Chanfray

Scalar and pseudoscalar QCD susceptibilities in nuclei

doi: 10.1140/epja/i2002-10260-0
Citations: PlumX Metrics

2003ER06      Prog.Theor.Phys.(Kyoto), Suppl. 149, 121 (2003)

M.Ericson, G.Chanfray

Scalar and Pseudoscalar Susceptibilities in Nuclei

doi: 10.1143/PTPS.149.121
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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
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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
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2001ER03      Nucl.Phys. A690, 110c (2001)


Role of Mesons in Chiral Symmetry Restoration and Associated Signals

doi: 10.1016/S0375-9474(01)00935-6
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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
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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
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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
Citations: PlumX Metrics

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
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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
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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
Citations: PlumX Metrics

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
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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1994DE08      Phys.Rev. C49, R1763 (1994)

J.Delorme, M.Ericson

s-Wave Pion-Nucleus Interaction and Weak Coupling Constants

doi: 10.1103/PhysRevC.49.R1763
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1994ER05      Phys.Lett. 328B, 259 (1994)

M.Ericson, T.Ericson, P.Vogel

High Energy Gamow-Teller Strength in Double Beta Decay

doi: 10.1016/0370-2693(94)91476-1
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
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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
Citations: PlumX Metrics

1989ER03      Nucl.Phys. A495, 602 (1989)

M.Ericson, J.D.Vergados

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
Citations: PlumX Metrics

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
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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
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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1987ER02      Phys.Lett. 188B, 11 (1987)

M.Ericson, M.Rosa-Clot

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
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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
Citations: PlumX Metrics

1986ER04      Z.Phys. A324, 373 (1986)

M.Ericson, M.Rosa-Clot

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
Citations: PlumX Metrics

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
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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1975ER03      Nucl.Phys. A241, 487 (1975)

M.Ericson, M.Krell

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
Citations: PlumX Metrics

1972ER02      Phys.Lett. 38B, 359 (1972)

M.Ericson, M.Krell

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
Citations: PlumX Metrics

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Note: The following list of authors and aliases matches the search parameter M.Ericson: , M.N.ERICSON