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NSR database version of May 24, 2024.

Search: Author = E.Lomon

Found 16 matches.

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2010CR03      Phys.Rev. C 82, 045211 (2010)

C.Crawford, T.Akdogan, R.Alarcon, W.Bertozzi, E.Booth, T.Botto, J.R.Calarco, B.Clasie, A.DeGrush, T.W.Donnelly, K.Dow, M.Farkhondeh, R.Fatemi, O.Filoti, W.Franklin, H.Gao, E.Geis, S.Gilad, D.Hasell, P.Karpius, M.Kohl, H.Kolster, T.Lee, E.Lomon, A.Maschinot, J.Matthews, K.McIlhany, N.Meitanis, R.Milner, J.Rapaport, R.Redwine, J.Seely, A.Shinozaki, A.Sindile, S.Sirca, E.Six, T.Smith, B.Tonguc, C.Tschalaer, E.Tsentalovich, W.Turchinetz, Y.Xiao, W.Xu, C.Zhang, Z.Zhou, V.Ziskin, T.Zwart

Role of mesons in the electromagnetic form factors of the nucleon

doi: 10.1103/PhysRevC.82.045211
Citations: PlumX Metrics


2002LO16      Phys.Rev. C66, 045501 (2002)

E.L.Lomon

Effect of recent Rp and Rn measurements on extended Gari-Krumpelmann model fits to nucleon electromagnetic form factors

NUCLEAR STRUCTURE 1n, 1H; analyzed electromagnetic form factors.

doi: 10.1103/PhysRevC.66.045501
Citations: PlumX Metrics


2001LO21      Phys.Rev. C64, 035204 (2001)

E.L.Lomon

Extended Gari-Krumpelmann Model Fits to Nucleon Electromagnetic Form Factors

NUCLEAR STRUCTURE 1n, 1H; analyzed electromagnetic form factor data; deduced parameters. Extended Gari-Krumpelmann model, other models compared.

doi: 10.1103/PhysRevC.64.035204
Citations: PlumX Metrics


1994BA09      Phys.Lett. 320B, 206 (1994)

J.Ball, P.A.Chamouard, M.Combet, J.M.Fontaine, R.Kunne, J.M.Lagniel, J.L.Lemaire, G.Milleret, J.L.Sans, J.Bystricky, F.Lehar, A.de Lesquen, M.de Mali, Ph.Demierre, R.Hess, Z.F.Janout, E.L.Lomon, D.Rapin, B.Vuaridel, L.S.Barabash, Z.Janout, V.A.Kalinnikov, Yu.M.Kazarinov, B.A.Khachaturov, V.N.Matafonov, I.L.Pisarev, A.A.Popov, Yu.A.Usov, M.Beddo, D.Grosnick, T.Kasprzyk, D.Lopiano, H.Spinka, A.Boutefnouchet, V.Ghazikhanian, C.A.Whitten

Observation of a Narrow Structure in the pp Elastic Scattering Observable A(oonn) at T(kin) = 2.11 GeV

NUCLEAR REACTIONS 1H(polarized p, p), E=1.96-2.23 GeV; measured spin correlation parameter vs θ. Polarized target. Model comparison.

doi: 10.1016/0370-2693(94)90847-8
Citations: PlumX Metrics


1991KL01      Phys.Rev. C43, 1575 (1991)

W.M.Kloet, E.L.Lomon

Correlation Between the Elastic NN Phase and the Inelastic Analyzing Power

NUCLEAR REACTIONS 1H(polarized p, pπ+), E=0.8 GeV; calculated σ, analyzing power vs proton momentum; deduced 3F3 nucleon-nucleon phase parameter role.

doi: 10.1103/PhysRevC.43.1575
Citations: PlumX Metrics


1989BL07      Phys.Rev. C40, 1541 (1989)

P.G.Blunden, W.R.Greenberg, E.L.Lomon

New Comparisons of the Coupled-Channel Model with Elastic Deuteron Form Factors

NUCLEAR STRUCTURE 2H; calculated electric, magnetic structure function. Coupled-channels model.

doi: 10.1103/PhysRevC.40.1541
Citations: PlumX Metrics


1987GO16      Phys.Rev. D35, 2142 (1987)

P.Gonzalez, P.LaFrance, E.L.Lomon

Correlation of pp Data with Predictions of Improved Six-Quark Structure Models

NUCLEAR REACTIONS 1H(polarized p, p), E=1.8-2.8 GeV/c; calculated total σ, spin-spin correlation parameters. Coupled-channels model, cloudy bag model dynamics, polarized target.

doi: 10.1103/PhysRevD.35.2142
Citations: PlumX Metrics


1987SI19      Phys.Rev. C36, 2479 (1987)

W.P.Sitarski, P.G.Blunden, E.L.Lomon

Deuteron Properties of the Coupled Nucleon and Isobar Channels Model

NUCLEAR STRUCTURE 2H; calculated magnetic, elastic monopole, quadrupole form factors. Coupled nucleon, isobar channels models.

doi: 10.1103/PhysRevC.36.2479
Citations: PlumX Metrics


1985LO09      Nucl.Phys. A434, 139c (1985)

E.L.Lomon

R-Matrix Prediction of QCD Structure in Hadrons and the Experimental Determination of QCD Properties

NUCLEAR REACTIONS 1H(polarized p, π+), E=1-2.3 GeV; calculated recoil nucleus analyzing power vs θ; deduced 3S1, 1S0 resonant structure. R-matrix formalism.

doi: 10.1016/0375-9474(85)90497-X
Citations: PlumX Metrics


1977LO08      Phys.Lett. 68B, 419 (1977)

E.L.Lomon

Dependence of Forward Deuteron Photodisintegration on the D State

NUCLEAR REACTIONS 2H(γ, p), E < 130 MeV; calculated dependence of forward σ on D-state.

doi: 10.1016/0370-2693(77)90457-9
Citations: PlumX Metrics


1976PR11      Phys.Lett. 65B, 31 (1976)

B.M.Preedom, C.W.Darden, R.D.Edge, T.Marks, M.J.Saltmarsh, K.Gabathuler, E.E.Gross, C.A.Ludemann, P.Y.Bertin, M.Blecher, K.Gotow, J.Alster, R.L.Burman, J.P.Perroud, R.P.Redwine, B.Goplen, W.R.Gibbs, E.L.Lomon

The Deuteron D-State and the π+ + d → p + p Reaction

NUCLEAR REACTIONS 2H(π+, 2p), E=40, 50, 60 MeV; measured σ(θ); deduced deuteron d-state probability.

doi: 10.1016/0370-2693(76)90527-X
Citations: PlumX Metrics


1974GO07      Phys.Rev.Lett. 32, 1012 (1974)

B.Goplen, W.R.Gibbs, E.L.Lomon

Off-Shell Effects in Pion-Deuteron Absorption

NUCLEAR REACTIONS 2H(π+, 2p); calculated σ.

doi: 10.1103/PhysRevLett.32.1012
Citations: PlumX Metrics


1974LO05      Phys.Rev. C9, 1329 (1974)

E.Lomon, R.Wilson

Neutron-Proton Scattering at a Few MeV

NUCLEAR REACTIONS 1H(n, n), E approx 10 MeV; calculated σ(θ), P(θ), σ, correlated experiments.

doi: 10.1103/PhysRevC.9.1329
Citations: PlumX Metrics


1973SH11      Phys.Rev. C8, 53 (1973)

J.Shao, E.L.Lomon

Jastrow-Type Brueckner-Hartree-Fock Calculation for Finite Nuclei

NUCLEAR STRUCTURE 16O, 40,48Ca; calculated matrix elements, Hartree-Fock, Bethe-Goldstone wave functions, binding energies.

doi: 10.1103/PhysRevC.8.53
Citations: PlumX Metrics


1972SH20      Phys.Rev. C6, 758 (1972)

J.Shao, W.H.Bassichis, E.L.Lomon

Suitability of the Feshbach-Lomon Potential for Hartree-Fock Calculations in Finite Nuclei

NUCLEAR STRUCTURE 4He, 40,48Ca; calculated binding energies, rms radii. Hartree-Fock method, Feshbach-Lomon potential.

doi: 10.1103/PhysRevC.6.758
Citations: PlumX Metrics


1960ST15      Nuovo Cimento 15, 150 (1960)

R.C.Stabler, E.L.Lomon

Proton-Proton Scattering Phase Shifts at 150 MeV

doi: 10.1007/BF02860339
Citations: PlumX Metrics


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Note: The following list of authors and aliases matches the search parameter E.Lomon: , E.L.LOMON