NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = E.L.Tomusiak Found 56 matches. 2011EF01 Phys.Rev. C 83, 057001 (2011) V.D.Efros, W.Leidemann, G.Orlandini, E.L.Tomusiak Frame dependence of 3He transverse (e, e') response functions at intermediate momentum transfers NUCLEAR REACTIONS 3H(e, e'), E at 500-700 MeV/c; analyzed frame dependence of transverse response function using two-fragment model. relativistic effects, realistic NN- and NNN-forces.
doi: 10.1103/PhysRevC.83.057001
2011LE02 Few-Body Systems 49, 71 (2011) W.Leidemann, Vi.D.Efros, G.Orlandini, E.L.Tomusiak Inclusive Electron Scattering Response Functions of 3He
doi: 10.1007/s00601-010-0114-8
2011YU02 Few-Body Systems 50, 375 (2011) L.Yuan, V.D.Efros, W.Leidemann, E.L.Tomusiak 3He Transverse Electron Scattering Response Function with Δ Degrees of Freedom
doi: 10.1007/s00601-010-0152-2
2010EF01 Phys.Rev. C 81, 034001 (2010) V.D.Efros, W.Leidemann, G.Orlandini, E.L.Tomusiak Improved transverse (e, e') response function of 3He at intermediate momentum transfers NUCLEAR REACTIONS 3He(e, e'), E at 400-700 MeV/c; calculated transverse response functions using one-photon exchange approximation and AV18 NN potential and the UIX 3NF as the nuclear force in active nucleon Breit (ANB) frame. Comparison with experimental data.
doi: 10.1103/PhysRevC.81.034001
2010YU08 Phys.Rev. C 82, 054003 (2010) L.Yuan, V.D.Efros, W.Leidemann, E.L.Tomusiak Transverse electron scattering response function of 3He with Δ-isobar degrees of freedom NUCLEAR REACTIONS 3He(e, e'), E at 850, 862, 927 MeV/c; calculated transverse inclusive response function using the Lorentz integral transform method. Comparisons with experimental data.
doi: 10.1103/PhysRevC.82.054003
2008DE15 Phys.Rev. C 77, 044007 (2008) S.Della Monaca, V.D.Efros, A.Khugaev, W.Leidemann, G.Orlandini, E.L.Tomusiak, L.P.Yuan Transverse electron scattering response function of 3He NUCLEAR REACTIONS 3He(e, e), E=250-500 MeV/c; calculated transverse response function, meson exchange currents.
doi: 10.1103/PhysRevC.77.044007
2006BA42 Few-Body Systems 39, 1 (2006) N.Barnea, W.Leidemann, G.Orlandini, V.D.Efros, E.L.Tomusiak On the Accuracy of Hyperspherical Harmonics Approaches to Photonuclear Reactions
doi: 10.1007/s00601-006-0152-4
2006EF01 Bull.Rus.Acad.Sci.Phys. 70, 308 (2006) V.D.Efros, W.Leidemann, G.Orlandini, E.L.Tomusiak Allowance for relativistic effects in (e, e') response functions NUCLEAR REACTIONS 3He(e, e'), E ≈ 50-400 MeV; analyzed response functions, relativistic effects. Various approaches discussed.
2005AR02 Eur.Phys.J. A 23, 147 (2005) H.Arenhovel, W.Leidemann, E.L.Tomusiak General survey of polarization observables in deuteron electrodisintegration NUCLEAR REACTIONS 2H(polarized e, e'p), E not given; calculated polarization observables.
doi: 10.1140/epja/i2004-10061-5
2005EF02 Phys.Rev. C 72, 011002 (2005) V.D.Efros, W.Leidemann, G.Orlandini, E.L.Tomusiak Improved (e, e') response functions at intermediate momentum transfers: The 3He case NUCLEAR REACTIONS 3He(e, e'), E ≈ 50-350 MeV; calculated response functions vs momentum transfer. Frame dependence, realistic NN and NNN forces. Comparison with data.
doi: 10.1103/PhysRevC.72.011002
2004EF01 Phys.Rev. C 69, 044001 (2004) V.D.Efros, W.Leidemann, G.Orlandini, E.L.Tomusiak Longitudinal electron scattering response functions of 3H and 3He NUCLEAR STRUCTURE 3H, 3He; calculated binding energies, radii, electron scattering longitudinal response functions, three-nucleon force effects.
doi: 10.1103/PhysRevC.69.044001
2003RE19 Eur.Phys.J. A 17, 589 (2003) C.Reiss, W.Leidemann, G.Orlandini, E.L.Tomusiak Application of the Lorentz-transform technique to meson photoproduction NUCLEAR REACTIONS 2H(γ, π+), E=0-30 MeV; calculated σ, response functions. Lorentz integral transform technique, comparison with data.
doi: 10.1140/epja/i2003-10027-1
2002AR15 Eur.Phys.J. A 14, 491 (2002) H.Arenhovel, W.Leidemann, E.L.Tomusiak General multipole expansion of polarization observables in deuteron electrodisintegration NUCLEAR REACTIONS 2H(polarized e, e'p), E not given; calculated polarization observables, related features. General multipole expansion.
doi: 10.1140/epja/i2001-10207-y
2002GO24 Nucl.Phys. A707, 365 (2002) J.Golak, R.Skibinski, W.Glockle, H.Kamada, A.Nogga, H.Witala, V.D.Efros, W.Leidemann, G.Orlandini, E.L.Tomusiak Benchmark Calculation of the Three-Nucleon Photodisintegration NUCLEAR REACTIONS 3H, 3He(γ, X), E < 140 MeV; calculated photoabsorption and photodisintegration σ. Fadeev equations and Lorentz integral transform method. Comparison with data.
doi: 10.1016/S0375-9474(02)00989-2
2001EF01 Nucl.Phys. A684, 457c (2001) V.D.Efros, W.Leidemann, G.Orlandini, E.L.Tomusiak Photodisintegration of Three-Body Nuclei with Realistic Interactions and Effects of 3N Forces NUCLEAR REACTIONS 3H, 3He(γ, X), E=0-30 MeV; calculated total photoabsorption σ; deduced 3N force contribution. Comparisons with data.
doi: 10.1016/S0375-9474(01)00503-6
2001EF03 Nucl.Phys. A689, 421c (2001) V.D.Efros, W.Leidemann, G.Orlandini, E.L.Tomusiak Photodisintegration of Trinucleons with Realistic Interactions and Effects of NNN Forces NUCLEAR REACTIONS 3H, 3He(γ, X), E=5-140 MeV; calculated total photoabsorption σ, three-nucleon force effects.
doi: 10.1016/S0375-9474(01)00869-7
2000AR11 Few-Body Systems 28, 147 (2000) H.Arenhovel, W.Leidemann, E.L.Tomusiak Complete Sets of Polarization Observables in Electromagnetic Deuteron Breakup NUCLEAR REACTIONS 2H(e, e'p), (γ, p), E not given; analyzed polarization observables; deduced complete sets.
2000EF03 Phys.Lett. 484B, 223 (2000) V.D.Efros, W.Leidemann, G.Orlandini, E.L.Tomusiak Photodisintegration of Three-Body Nuclei with Realistic 2N and 3N Forces NUCLEAR REACTIONS 3H, 3He(γ, X), E=5-140 MeV; calculated total photoabsorption σ; deduced three-nucleon force contributions. Several models compared. Comparison with data.
doi: 10.1016/S0370-2693(00)00656-0
1999LE41 Fizika(Zagreb) B8, 135 (1999) W.Leidemann, V.D.Efros, G.Orlandini, E.L.Tomusiak Electromagnetic Few-Body Response Functions with the Lorentz Integral Transform NUCLEAR REACTIONS 3He(γ, X), E<140 MeV; 4He(γ, X), E<35 MeV; calculated photoabsorption σ. 4He(e, e'), E not given; calculated longitudinal response function. Lorentz integral transform method. Comparison with data.
1998AR17 Nucl.Phys. A641, 517 (1998) H.Arenhovel, W.Leidemann, E.L.Tomusiak On Complete Sets of Polarization Observables NUCLEAR REACTIONS 2H(e, e'n), (e, e'p), E not given; deduced complete set of polarization observables.
doi: 10.1016/S0375-9474(98)00487-4
1996AR18 Few-Body Systems 20, 47 (1996) H.Arenhovel, W.Leidemann, E.L.Tomusiak Reply to the Comment General Formulae for Polarization Observables in Deuteron Electrodistintegration and Linear Relations
1995AR17 Phys.Rev. C52, 1232 (1995) H.Arenhovel, W.Leidemann, E.L.Tomusiak Nucleon Polarization in Exclusive Deuteron Electrodisintegration with Polarized Electrons and a Polarized Target NUCLEAR REACTIONS 2H(polarized e, X), E not given; calculated structure function for one-, two-nucleon polarization observables. Polarized target.
doi: 10.1103/PhysRevC.52.1232
1995TO08 Phys.Rev. C52, 1963 (1995) E.L.Tomusiak, W.Leidemann, H.M.Hofmann Photon Polarization in the 4He(γ, d(pol))2H Reaction NUCLEAR REACTIONS 4He(polarized γ, d), E=50 MeV; calculated σ(θ), photon asymmetry, polarization observables vs θ.
doi: 10.1103/PhysRevC.52.1963
1994LE16 Phys.Rev. C50, 630 (1994) W.Leidemann, G.Orlandini, M.Traini, E.L.Tomusiak Two-Body Correlations from (e, e'd) Reactions: 4He(e, e'd)2H as a Test Case NUCLEAR REACTIONS 4He(e, e'd), E not given; calculated structure functions; deduced short-range, tensor correlations role.
doi: 10.1103/PhysRevC.50.630
1994RA39 Few-Body Systems 17, 71 (1994) A.S.Raskin, E.L.Tomusiak, J.L.Friar Gauge-Invariant Nuclear Pion-Photoproduction Amplitude with Binding-Induced Contributions
doi: 10.1007/BF01074446
1993AR19 Few-Body Systems 15, 109 (1993) H.Arenhovel, W.Leidemann, E.L.Tomusiak General Formulae for Polarization Observables in Deuteron Electrodisintegration and Linear Relations
1992AR13 Phys.Rev. C46, 455 (1992) H.Arenhovel, W.Leidemann, E.L.Tomusiak Exclusive Deuteron Electrodisintegration with Polarized Electrons and a Polarized Target NUCLEAR REACTIONS 2H(polarized e, X), E not given; calculated various structure functions, exclusive breakup. Nonrelativistic framework, polarized target.
doi: 10.1103/PhysRevC.46.455
1992LE05 Phys.Lett. 279B, 212 (1992) W.Leidemann, G.Orlandini, M.Traini, E.L.Tomusiak Final State Effects in the 4He(e, e'D)D Reaction NUCLEAR REACTIONS 4He(e, e'd), E not given; calculated σ(θ(e'), E(e'), θd) vs four-momentum transfer. Plane wave approximation, final state effects, correlated, harmonic oscillator basis wave functions for 4He.
doi: 10.1016/0370-2693(92)90381-D
1991LE01 Phys.Rev. C43, 1022 (1991) W.Leidemann, E.L.Tomusiak, H.Arenhovel Inclusive Deuteron Electrodisintegration with Polarized Electrons and a Polarized Target NUCLEAR REACTIONS 2H(polarized e, np), E not given; calculated inclusive disintegration form factors. Polarized target.
doi: 10.1103/PhysRevC.43.1022
1990BH04 Phys.Rev. C42, 1867 (1990) R.K.Bhaduri, W.Leidemann, G.Orlandini, E.L.Tomusiak rms Radius of the Deuteron NUCLEAR STRUCTURE 2H; calculated rms radius; deduced linear relationship to triplet scattering length.
doi: 10.1103/PhysRevC.42.1867
1988AR16 Z.Phys. A331, 123 (1988); Erratum Z.Phys. A334, 363 (1989) H.Arenhovel, W.Leidemann, E.L.Tomusiak The Role of the Neutron Electric Form Factor in d(e, e'N)N Including Polarization Observables NUCLEAR REACTIONS 2H(e, e'p), E not given; calculated proton P(θ), vector asymmetry vs E(np); deduced 1n electric form factor role.
1988FR11 Phys.Rev. C37, 2852 (1988) J.L.Friar, B.F.Gibson, G.L.Payne, E.L.Tomusiak, M.Kimura Trinucleon Magnetic Moments: 34-Channel results NUCLEAR STRUCTURE 3H, 3He; calculated μ. Configuration space Faddeev wave functions, one-body, meson exchange currents.
doi: 10.1103/PhysRevC.37.2852
1988TO06 Phys.Lett. 206B, 187 (1988) Model Independent Determination of G(En) from the d(pol)(e(pol), e'n)p Reaction NUCLEAR REACTIONS 2H(polarized e, e'n), E not given; calculated np-asymmetry; deduced neutron electric form factor. Polarized target.
doi: 10.1016/0370-2693(88)91489-X
1986BH05 Phys.Lett. 173B, 369 (1986) R.K.Bhaduri, M.V.N.Murthy, E.L.Tomusiak Six-Quark Bag, Exchange Currents and Trinucleon Magnetic Moments NUCLEAR STRUCTURE 3H, 3He; calculated μ. Six quark bag, exchange currents.
doi: 10.1016/0370-2693(86)90396-5
1985TO21 Phys.Rev. C32, 2075 (1985) E.L.Tomusiak, M.Kimura, J.L.Friar, B.F.Gibson, G.L.Payne, J.Dubach Trinucleon Magnetic Moments NUCLEAR STRUCTURE 3H, 3He; calculated μ, magnetic form factors; deduced dominant charge exchange effects. Various potential models, configuration space Faddeev equations.
doi: 10.1103/PhysRevC.32.2075
1983FR05 Phys.Rev. C27, 1364 (1983) J.L.Friar, S.Fallieros, E.L.Tomusiak, D.Skopik, E.G.Fuller Electric Polarizability of the Deuteron NUCLEAR STRUCTURE 2H; analyzed photoabsorption data; deduced electric polarizability. Dispersion relation, Compton scattering effects.
doi: 10.1103/PhysRevC.27.1364
1982SE11 Can.J.Phys. 60, 1257 (1982) R.M.Sealock, H.S.Caplan, B.W.Zulkoskey, A.Szyjewicz, E.L.Tomusiak Electroproduction of Low Energy π+ from 3He NUCLEAR REACTIONS 1H, 3He(e, π+), E=200 MeV; measured σ(θ, E(π)). Three-channel calculation.
doi: 10.1139/p82-172
1981AS05 J.Phys.(London) G7, 131 (1981) J.Asai, E.L.Tomusiak, E.T.Dressler Electropion Production in the Three-Nucleon System NUCLEAR REACTIONS 3He(e, π+), 3H(e, π-), E=170, 200, 229.7 MeV; calculated σ(θ(π+), E(π+)), σ(θ(π-)), E(π-).
doi: 10.1088/0305-4616/7/2/005
1981FR15 Phys.Rev. C24, 665 (1981) J.L.Friar, B.F.Gibson, E.L.Tomusiak, G.L.Payne Configuration Space Faddeev Calculations. IV. Trinucleon Charge Density NUCLEAR STRUCTURE 3He, 3H; calculated charge densities. Faddeev calculations, several potential models.
doi: 10.1103/PhysRevC.24.665
1981TO13 Phys.Rev. C24, 2351 (1981) E.L.Tomusiak, J.L.Friar, B.F.Gibson, J.Dubach. G.L.Payne Threshold 3He(γ, π+)3H NUCLEAR REACTIONS 3He(γ, π+), E=threshold; calculated σ. Impulse approximation, realistic wave functions.
doi: 10.1103/PhysRevC.24.2351
1980DR05 Can.J.Phys. 58, 768 (1980) A Study of the 3He(γ, π+)3H Cross Section Near Threshold NUCLEAR REACTIONS 3He(γ, π+), E=1-5 MeV; calculated total σ. Pion, fermion momenta, isobar resonance contributions.
doi: 10.1139/p80-106
1979SK05 Phys.Rev. C20, 2025 (1979) D.M.Skopik, J.Asai, E.L.Tomusiak, J.J.Murphy II Experiment and Theory for the Reactions 7Li(γ, t)4He for E < 50 MeV NUCLEAR REACTIONS 7Li(γ, t), Eγ=threshold to 50 MeV; measured σ(E;Eα, θα), σ(E;Et, θt); calculated 3H-α cluster model cross section.
doi: 10.1103/PhysRevC.20.2025
1978SK01 Phys.Rev. C18, 2219 (1978) D.M.Skopik, E.L.Tomusiak, J.Asai, J.J.Murphy, II Electropion Production in 3He Determined by Measuring the Triton Recoil Cross Section NUCLEAR REACTIONS 3He(e, eπ+t), E ≈ 200 MeV; measured σ(Et, θ).
doi: 10.1103/PhysRevC.18.2219
1977AS07 Can.J.Phys. 55, 2066 (1977); Erratum Can.J.Phys. 56, 1526 (1978) Electroproduction of Low Energy π+ from 3He NUCLEAR REACTIONS 3He(e, π+), (e, t), E ≈ 230 MeV; calculated σ.
doi: 10.1139/p77-250
1977FA09 Phys.Rev. C16, 2117 (1977) Three-Body Model of 6Li Using Hyperspherical Harmonics NUCLEAR STRUCTURE Li; calculated charge form factor, M1 transition form factor. Hyperspherical technique, αpn model.
doi: 10.1103/PhysRevC.16.2117
1977TO20 Phys.Lett. 72B, 1 (1977) Pion Electroproduction from 6Li NUCLEAR REACTIONS 6Li(γ, π+); calculated σ(E(6He)).
doi: 10.1016/0370-2693(77)90047-8
1976BE22 Nucl.Phys. A262, 196 (1976) Inelastic Electron Scattering from 6Li Near the α-d Threshold NUCLEAR REACTIONS 6Li(e, e'), E=0-8 MeV; measured σ(E, θ), θ=99.9°, 140.7°. 6Li levels deduced form factors. Comparison between form factors, α-d cluster model calculations.
doi: 10.1016/0375-9474(76)90613-8
1976SK02 Phys.Rev. C14, 789 (1976) D.M.Skopik, E.L.Tomusiak, E.T.Dressler, Y.M.Shin, J.J.Murphy, II Theory and Experiment for the Reaction 6Li(e, d)e', 4He NUCLEAR REACTIONS 6Li(e, e'd), E=23.8 MeV; measured σ(Ed, θ). 6Li(γ, X); measured nothing; deduced σ(Eγ).
doi: 10.1103/PhysRevC.14.789
1975SK02 Phys.Rev. C11, 693 (1975) D.M.Skopik, J.J.Murphy, II, Y.M.Shin, K.F.Chong, E.L.Tomusiak Electrodisintegration of 3He NUCLEAR REACTIONS 3He(e, d), E=43, 70, 103 MeV; measured σ(Ed, θ).
doi: 10.1103/PhysRevC.11.693
1974BR23 Can.J.Phys. 52, 1322 (1974) T.J.Brady, E.L.Tomusiak, J.S.Levinger Deuteron Polarization in e-d Scattering NUCLEAR REACTIONS 2H(e, e); calculated form factors, P.
doi: 10.1139/p74-177
1974CH05 Nucl.Phys. A218, 43 (1974) K.F.Chong, M.C.Phenneger, Y.M.Shin, D.M.Skopik, E.L.Tomusiak Experiment and Theory for the 2H(e, p)e'n Reaction NUCLEAR REACTIONS 2H(e, p), E=30.5, 37.6, 70.0, 106.6 MeV; θ(lab)=27.6°-150°; measured σ(E;Ep, θ).
doi: 10.1016/0375-9474(74)90018-9
1973SH20 Izv.Akad.Nauk SSSR, Ser.Fiz. 37, 1863 (1973); Bull.Acad.Sci.USSR, Phys.Ser. 37, No.9, 60 (1974) Y.M.Shin, D.M.Skopik, E.L.Tomusiak Coincidence Study of the 3He(e, pd)e' Reaction and New Results on the 2H(e, p)ne' Reaction NUCLEAR REACTIONS 3He(e, pd), E=100 MeV; measured σ(Ep, Ed). 2H(e, p), E=38, 106 MeV; measured σ(Ep, θ(p)).
1973SK02 Phys.Lett. 43B, 481 (1973) D.M.Skopik, Y.M.Shin, E.L.Tomusiak, M.C.Phenneger, K.F.Chong Electrodisintegration of the Deuteron NUCLEAR REACTIONS 2H(e, p);E=37.6, 106.6 MeV; measured σ(Ep, θ).
doi: 10.1016/0370-2693(73)90351-1
1971DU06 Phys.Lett. 35B, 554 (1971) Monopole Form Factors and the α-Cluster Model NUCLEAR REACTIONS 12C, 16O(e, e), (e, e'), E not given; calculated elastic, inelastic monopole form factors. α-cluster model.
doi: 10.1016/0370-2693(71)90284-X
1971YA02 Nucl.Phys. A162, 71 (1971) C.S.Yang, E.L.Tomusiak, R.K.Gupta, H.S.Caplan Electron Scattering from 13C NUCLEAR REACTIONS 13C(e, e), (e, e'), E=40-125 MeV; measured σ(E;θ), σ(E;Ee', θ); deduced form factors. 13C deduced levels, level-width, γ-mixing, rms charge radius. Enriched solid, gas targets.
doi: 10.1016/0375-9474(71)90486-6
1968DR01 Nucl.Phys. A118, 138 (1968) T.E.Drake, E.L.Tomusiak, H.S.Caplan The Excitation of Strong Transitions in the Giant Resonance of 12C, 16O and 28Si NUCLEAR REACTIONS 12C, 16O, 28Si(e, e') E=140 MeV; measured σ(Ee', θ);deduced form factors. Natural targets.
doi: 10.1016/0375-9474(68)90192-9
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