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NSR database version of April 11, 2024.

Search: Author = E.L.Tomusiak

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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1988TO06      Phys.Lett. 206B, 187 (1988)

E.L.Tomusiak, H.Arenhovel

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1980DR05      Can.J.Phys. 58, 768 (1980)

E.T.Dressler, E.L.Tomusiak

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0227.


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
Citations: PlumX Metrics


1977AS07      Can.J.Phys. 55, 2066 (1977); Erratum Can.J.Phys. 56, 1526 (1978)

J.Asai, E.L.Tomusiak

Electroproduction of Low Energy π+ from 3He

NUCLEAR REACTIONS 3He(e, π+), (e, t), E ≈ 230 MeV; calculated σ.

doi: 10.1139/p77-250
Citations: PlumX Metrics


1977FA09      Phys.Rev. C16, 2117 (1977)

K.K.Fang, E.L.Tomusiak

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
Citations: PlumX Metrics


1977TO20      Phys.Lett. 72B, 1 (1977)

E.L.Tomusiak, E.T.Dressler

Pion Electroproduction from 6Li

NUCLEAR REACTIONS 6Li(γ, π+); calculated σ(E(6He)).

doi: 10.1016/0370-2693(77)90047-8
Citations: PlumX Metrics


1976BE22      Nucl.Phys. A262, 196 (1976)

J.C.Bergstrom, E.L.Tomusiak

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1971DU06      Phys.Lett. 35B, 554 (1971)

S.Dutta, E.L.Tomusiak

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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