NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = E.Lomon Found 16 matches. 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
2002LO16 Phys.Rev. C66, 045501 (2002) 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
2001LO21 Phys.Rev. C64, 035204 (2001) 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
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
1991KL01 Phys.Rev. C43, 1575 (1991) 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
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
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
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
1985LO09 Nucl.Phys. A434, 139c (1985) 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
1977LO08 Phys.Lett. 68B, 419 (1977) 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
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
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
1974LO05 Phys.Rev. C9, 1329 (1974) 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
1973SH11 Phys.Rev. C8, 53 (1973) 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
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
1960ST15 Nuovo Cimento 15, 150 (1960) Proton-Proton Scattering Phase Shifts at 150 MeV
doi: 10.1007/BF02860339
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