NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = M.Paris Found 37 matches. 2024DE04 Phys.Rev.Lett. 132, 062702 (2024) R.J.deBoer, M.Febbraro, D.W.Bardayan, C.Boomershine, K.Brandenburg, C.Brune, S.Coil, M.Couder, J.Derkin, S.Dede, R.Fang, A.Fritsch, A.Gula, Gy.Gyurky, B.Hackett, G.Hamad, Y.Jones-Alberty, R.Kelmar, K.Manukyan, M.Matney, J.McDonaugh, Z.Meisel, S.Moylan, J.Nattress, D.Odell, P.O'Malley, M.W.Paris, D.Robertson, Shahina, N.Singh, K.Smith, M.S.Smith, E.Stech, W.Tan, M.Wiescher Measurement of the 13C(α, n0)16O Differential Cross Section from 0.8 to 6.5 MeV NUCLEAR REACTIONS 13C(α, n), E=0.8-6.5 MeV; measured reaction products, En, IN; deduced σ(θ), σ, S-factor. Comparison with available data, R-matrix results from ENDF/B-VIII.0 library. The Oak Ridge National Laboratory Deuterated Spectroscopic Array (ODeSA), 5 MV Stable ion Accelerator for Nuclear Astrophysics, the University of Notre Dame Nuclear Science Laboratory.
doi: 10.1103/PhysRevLett.132.062702
2024LE02 Phys.Rev. C 109, 014601 (2024) H.Y.Lee, S.A.Kuvin, L.Zavorka, S.Mosby, B.DiGiovine, G.Hale, M.Paris, D.Votaw, M.White Differential cross sections of the 16O(n, α) reaction at neutron energies from 3.8 to 15 MeV
doi: 10.1103/PhysRevC.109.014601
2024ME02 Phys.Rev. C 109, 034003 (2024) K.D.Meaney, M.W.Paris, G.M.Hale, Y.Kim, J.Kuczek, A.C.Hayes Deuterium-tritium fusion γ-ray spectrum at MeV energies with application to reaction-in-flight inertial confinement fusion measurements
doi: 10.1103/PhysRevC.109.034003
2023KE08 Phys.Rev. C 108, 014603 (2023) K.J.Kelly, M.Devlin, J.M.O'Donnell, E.A.Bennett, M.Paris, P.A.Copp Measurement of the cross section of the Q = 4.4398 MeV 12C(n, n'γ) reaction from threshold to 16.5 MeV using γ and correlated n-γ detection NUCLEAR REACTIONS 12C(n, n'γ), E=4.5-16.5 MeV; measured Eγ, Iγ, En, Iν, nγ-coin; deduced σ(E). Comparison to other experimental data and evaluated values from ENDF/B-VIII.0. Correlated Gamma-Neutron Array for Scattering (CoGNAC) consisting of 54-element EJ-309 liquid scintillator array at Weapons Neutron Research (WNR) facility (LANSCE, LANL).
doi: 10.1103/PhysRevC.108.014603
2023NE10 Eur.Phys.J. N 9, 35 (2023) D.Neudecker, A.M.Lewis, E.F.Matthews, J.Vanhoy, R.C.Haight, D.L.Smith, P.Talou, S.Croft, A.D.Carlson, B.Pierson, A.Wallner, A.Al-Adili, L.Bernstein, R.Capote, M.Devlin, M.Drosg, D.L.Duke, S.Finch, M.W.Herman, K.J.Kelly, A.Koning, A.E.Lovell, P.Marini, K.Montoya, G.P.A.Nobre, M.Paris, B.Pritychenko, H.Sjostrand, L.Snyder, V.Sobes, A.Solders, J.Taieb Templates of Expected Measurement Uncertainties: a CSEWG Effort NUCLEAR REACTIONS 235U(n, F), E<20 MeV; analyzed available data; deduced nubar mean values and uncertainties.
doi: 10.1051/epjn/2023014
2021DU11 Phys.Rev. C 103, 064608 (2021) P.Ducru, B.Forget, V.Sobes, G.Hale, M.Paris Shadow poles in the alternative parametrization of R matrix theory NUCLEAR REACTIONS 134Xe(n, X), E=2186.0, 6315.0 eV p-wave resonances; analyzed neutron resonance parameters by R-matrix theory and using generalized Reich-Moore formalism to convert the Reich-Moore parameters into real R-matrix parameters; deduced existence of shadow poles in the alternative parametrization of R-matrix theory, being considered as an alternative to the traditional Wigner-Eisenbud resonance parameters to document nuclear cross-section values in the nuclear data libraries such as ENDF/B-VIII.0. Discussed how the nuclear reaction community could convert present nuclear data libraries featuring both Wigner-Eisenbud parameters and Reich-Moore parameters to alternative parameters. See also follow-up 2021Du12 article by the same authors about Scattering matrix pole expansions in R-matrix theory, and a related article 2021Du13 about windowed multipole representation in R-matrix cross sections.
doi: 10.1103/PhysRevC.103.064608
2021DU12 Phys.Rev. C 103, 064609 (2021) P.Ducru, B.Forget, V.Sobes, G.Hale, M.Paris Scattering matrix pole expansions for complex wave numbers in R-matrix theory NUCLEAR REACTIONS 134Xe(n, X), E=2186.0, 6315.0 eV p-wave resonances; analyzed radioactive state parameters and the R-matrix parameters to yield an identical Kapur-Peierls operator, and exact reconstruction of the scattering matrix of the nuclear interactions, scattering matrix poles are the Siegert-Humblet radioactive poles; discussed subthreshold cross sections through analytic continuation; conclude with the need for the R-matrix community to come to consensus and agreement to set the analytic continuation as the standard way of computing R-matrix operator, in particular, the shift and penetration functions, in performing nuclear reaction data evaluations for the evaluated libraries such as ENSDF, JEFF, BRONDE, JENDL, CENDL, and TENDEL. See also preceding 2021Du11 article by the same authors about shadow poles in the alternative parametrization in R-matrix theory, and a related article 2021Du13 about windowed multipole representation in R-matrix cross sections.
doi: 10.1103/PhysRevC.103.064609
2018BR03 Phys.Rev. C 97, 024603 (2018) C.R.Brune, G.M.Hale, M.W.Paris Monotonic properties of the shift and penetration factors
doi: 10.1103/PhysRevC.97.024603
2018BR05 Nucl.Data Sheets 148, 1 (2018) D.A.Brown, M.B.Chadwick, R.Capote, A.C.Kahler, A.Trkov, M.W.Herman, A.A.Sonzogni, Y.Danon, A.D.Carlson, M.Dunn, D.L.Smith, G.M.Hale, G.Arbanas, R.Arcilla, C.R.Bates, B.Beck, B.Becker, F.Brown, R.J.Casperson, J.Conlin, D.E.Cullen, M.-A.Descalle, R.Firestone, T.Gaines, K.H.Guber, A.I.Hawari, J.Holmes, T.D.Johnson, T.Kawano, B.C.Kiedrowski, A.J.Koning, S.Kopecky, L.Leal, J.P.Lestone, C.Lubitz, J.I.Marquez Damian, C.M.Mattoon, E.A.McCutchan, S.Mughabghab, P.Navratil, D.Neudecker, G.P.A.Nobre, G.Noguere, M.Paris, M.T.Pigni, A.J.Plompen, B.Pritychenko, V.G.Pronyaev, D.Roubtsov, D.Rochman, P.Romano, P.Schillebeeckx, S.Simakov, M.Sin, I.Sirakov, B.Sleaford, V.Sobes, E.S.Soukhovitskii, I.Stetcu, P.Talou, I.Thompson, S.van der Marck, L.Welser-Sherrill, D.Wiarda, M.White, J.L.Wormald, R.Q.Wright, M.Zerkle, G.Zerovnik, Y.Zhu ENDF/B-VIII.0: The 8 th Major Release of the Nuclear Reaction Data Library with CIELO-project Cross Sections, New Standards and Thermal Scattering Data COMPILATION Z=1-118; compiled, analyzed decay data, Maxwellian averaged neutron capture σ, neutron-induced fission σ. NUCLEAR REACTIONS 1,2H, 3He, 6,7Li, 9Be, 10,11B, 12,13C, 14,15N, 16,17,18O, 19F, 20,21,22Ne, 22,23Na, 24,25,26Mg, 26,27Al, 28,29,30,31,32Si, 31P, 32,33,34,35,36S, 35,36,37Cl, 36,37,38,39,40,41Ar, 39,40,41K, 40,41,42,43,44,45,46,47,48Ca, 45Sc, 46,47,48,49,50Ti, 49,50,51V, 50,51,52,53,54Cr, 54,55Mn, 54,55,56,57,58Fe, 58,59Co, 58,59,60,61,62,63,64Ni, 63,64,65Cu, 64,65,66,67,68,69,70Zn, 69,70,71Ga, 70,71,72,73,74,75,76Ge, 73,74,75As, 74,75,76,77,78,79,80,81,82Se, 79,80,81Br, 78,79,80,81,82,83,84,85,86Kr, 85,86,87Rb, 84,85,86,87,88,89,90Sr, 89,90,91Y, 90,91,92,93,94,95,96Zr, 93,94,95Nb, 92,93,94,95,96,97,98,99,100Mo, 98,99Tc, 96,97,98,99,100,101,102,103,104,105,106Ru, 103,104,105Rh, 102,103,104,105,106,107,108,109,110Pd, 107,108,109,110,111,112,113,114,115,116,117,118Ag, 106,107,108,109,110,111,112,113,114,115,116Cd, 113,114,115In, 112,113,114,115,116,117,118,119,120,121,122,123,124,125,126Sn, 121,122,123,124,125,126Sb, 120,121,122,123,124,125,126,127,128,129,130,121,132Te, 127,128,129,130,131,132,133,134,135I, 123,124,125,126,127,128,129,130,131,132,133,134,135,136Xe, 133,134,135,136,137Cs, 130,131,132,133,134,135,136,137,138,139,140Ba, 138,139,140La, 136,137,138,139,140,141,142,143,144Ce, 141,142,143Pr, 142,143,144,145,146,147,148,149,150Nd, 143,144,145,146,147,148,149,151Pm, 144,145,146,147,148,149,150,151,152,153,154Sm, 151,152,153,154,155,156,157Eu, 152,153,154,155,156,157,158,159,160Gd, 158,159,160,161Tb, 154,155,156,157,158,159,160,161,162,163,164Dy, 165,166Ho, 162,163,164,165,166,167,168,170,170Er, 168,169,170,171Tm, 168,169,170,171,172,173,174,175,176Yb, 175,176Lu, 174,175,176,177,178,179,180,181,182Hf, 180,181,182Ta, 180,181,182,183,184,185,186W, 185,186,187Re, 184,185,186,187,188,189,190,191,192Os, 191,192,193Ir, 190,191,192,193,194,195,196,197,198Pt, 197Au, 196,197,198,199,200,201,202,203,204Hg, 203,204,205Tl, 204,205,206,207,208,209,210Pb, 209,210Bi, 208,209,210Po, 223,224,225,226Ra, 225,226,227Ac, 227,228,229,230,231,232,233,234Th, 229,230,231,232,233Pa, 230,231,232,233,234,235,236,237,238,239,240,241U, 234,235,236,237,238,239Np, 236,237,238,239,240,241,242,243,244,245,246Pu, 240,241,242,243,244Am, 240,241,242,243,244,245,246,247,248,249,250Cm, 245,246,247,248,249,250Bk, 246,247,248,249,250,251,252,253,254Cf, 251,252,253,254,255Es, 255Fm(n, γ), E=30 keV; calculated Maxwellian-averaged σ using ENDF/B-VIII.0 evaluated neutron library. Comparison with ENDF/B-VII.1 and KADONIS values. NUCLEAR REACTIONS 227,228,229,230,231,232,233,234Th, 229,230,231,232,233Pa, 230,231,232,233,234,235,236,237,238,239,240,241U, 234,235,236,237,238,239Np, 236,237,238,239,240,241,242,243,244,245,246Pu, 240,241,242,243,244Am, 240,241,242,243,244,245,246,247,248,249,250Cm, 245,246,247,248,249,250Bk, 246,247,248,249,250,251,252,253,254Cf, 251,252,253,254,255Es, 255Fm(n, γ), (n, F), E=thermal; calculated thermal σ. Comparison with ENDF/B-VII.1, JENDL-4.0u+ and Atlas of Neutron Resonances values.
doi: 10.1016/j.nds.2018.02.001
2018CA07 Nucl.Data Sheets 148, 143 (2018), Erratum Nucl.Data Sheets 163, 280 (2020) A.D.Carlson, V.G.Pronyaev, R.Capote, G.M.Hale, Z.-P.Chen, I.Duran, F.-J.Hambsch, S.Kunieda, W.Mannhart, B.Marcinkevicius, R.O.Nelson, D.Neudecker, G.Noguere, M.Paris, S.P.Simakov, P.Schillebeeckx, D.L.Smith, X.Tao, A.Trkov, A.Wallner, W.Wang Evaluation of the Neutron Data Standards NUCLEAR REACTIONS H, C(n, n), 6Li(n, t), 10B(n, αγ), 197Au(n, γ), 235,238U, 239Pu(n, F), 238U(n, γ), E<20 MeV; analyzed available data; deduced σ and Maxwellian spectrum averaged cross section for the 197Au(n, γ) σ at 30 keV, covariance matrices of the uncertainties. RADIOACTIVITY 252Cf(SF); analyzed available data; deduced spontaneous fission neutron spectrum.
doi: 10.1016/j.nds.2018.02.002
2018CH12 Nucl.Data Sheets 148, 189 (2018) M.B.Chadwick, R.Capote, A.Trkov, M.W.Herman, D.A.Brown, G.M.Hale, A.C.Kahler, P.Talou, A.J.Plompen, P.Schillebeeckx, M.T.Pigni, L.Leal, Y.Danon, A.D.Carlson, P.Romain, B.Morillon, E.Bauge, F.-J.Hambsch, S.Kopecky, G.Giorginis, T.Kawano, J.Lestone, D.Neudecker, M.Rising, M.Paris, G.P.A.Nobre, R.Arcilla, O.Cabellos, I.Hill, E.Dupont, A.J.Koning, D.Cano-Ott, E.Mendoza, J.Balibrea, C.Paradela, I.Duran, J.Qian, Z.Ge, T.Liu, L.Hanlin, X.Ruan, W.Haicheng, M.Sin, G.Noguere, D.Bernard, R.Jacqmin, O.Bouland, C.De Saint Jean, V.G.Pronyaev, A.V.Ignatyuk, K.Yokoyama, M.Ishikawa, T.Fukahori, N.Iwamoto, O.Iwamoto, S.Kunieda, C.R.Lubitz, M.Salvatores, G.Palmiotti, I.Kodeli, B.Kiedrowski, D.Roubtsov, I.Thompson, S.Quaglioni, H.I.Kim, Y.O.Lee, U.Fischer, S.Simakov, M.Dunn, K.Guber, J.I.Marquez Damian, F.Cantargi, I.Sirakov, N.Otuka, A.Daskalakis, B.J.McDermott, S.C.van der Marck CIELO Collaboration Summary Results: International Evaluations of Neutron Reactions on Uranium, Plutonium, Iron, Oxygen and Hydrogen NUCLEAR REACTIONS 1H, 16O, 56Fe, 235,238U, 239Pu(n, X), E<20 MeV; analyzed available data; calculated σ, σ(θ), σ(θ, E).
doi: 10.1016/j.nds.2018.02.003
2018GA21 Phys.Rev.Lett. 121, 042501 (2018) M.Gatu-Johnson, C.J.Forrest, D.B.Sayre, A.Bacher, J.-L.Bourgade, C.R.Brune, J.A.Caggiano, D.T.Casey, J.A.Frenje, V.Yu.Glebov, G.M.Hale, R.Hatarik, H.W.Herrmann, R.Janezic, Y.H.Kim, J.P.Knauer, O.Landoas, D.P.McNabb, M.W.Paris, R.D.Petrasso, J.E.Pino, S.Quaglioni, B.Rosse, J.Sanchez, T.C.Sangster, H.Sio, W.Shmayda, C.Stoeckl, I.Thompson, A.B.Zylstra Experimental Evidence of a Variant Neutron Spectrum from the T(t, 2n)α Reaction at Center-of-Mass Energies in the Range of 16-50 KeV NUCLEAR REACTIONS 3H(t, 2n), E(cm)=16-50 keV; measured reaction products, En, In; deduced neutron spectra inferred from R-matrix analysis of the measured NTOF-spectra.
doi: 10.1103/PhysRevLett.121.042501
2017ZY01 Phys.Rev.Lett. 119, 222701 (2017) A.B.Zylstra, J.A.Frenje, M.Gatu-Johnson, G.M.Hale, C.R.Brune, A.Bacher, D.T.Casey, C.K.Li, D.McNabb, M.Paris, R.D.Petrasso, T.C.Sangster, D.B.Sayre, F.H.Seguin Proton Spectra from 3He+T and 3He+3He Fusion at Low Center-of-Mass Energy, with Potential Implications for Solar Fusion Cross Sections NUCLEAR REACTIONS 3He(3He, X), E(cm)=165 keV; 3He(t, X), E=86 keV; measured reaction products, Ep, Ip; deduced yields. Comparison with R-matrix calculations.
doi: 10.1103/PhysRevLett.119.222701
2015BR07 Phys.Rev. C 92, 014003 (2015) C.R.Brune, J.A.Caggiano, D.B.Sayre, A.D.Bacher, G.M.Hale, M.W.Paris R-matrix description of particle energy spectra produced by low-energy 3H + 3H reactions NUCLEAR REACTIONS 3H(t, 2n)4He, E(cm)=16, 57 keV; 3He(3He, 2p)4He, E(cm)=165 keV; calculated neutron, proton and α-particle energy distributions for different reaction channels, fits to experimental neutron time-of-flight spectra, proton and α spectra. Phenomenological R-matrix analysis for the three-body final states. 5He; deduced fits to the 3/2- ground and 1/2- first excited states.
doi: 10.1103/PhysRevC.92.014003
2015HA02 Nucl.Data Sheets 123, 165 (2015) Data Covariances from R-Matrix Analyses of Light Nuclei NUCLEAR REACTIONS 4He(n, n), 3H(d, d), (d, n), (d, γ), E<28 MeV; 12C(n, n), (n, n'), E<6.45 MeV; calculated σ covariances. R-matrix analysis code EDA.
doi: 10.1016/j.nds.2014.12.029
2015KU03 Nucl.Data Sheets 123, 159 (2015) S.Kunieda, T.Kawano, M.Paris, G.M.Hale, K.Shibata, T.Fukahori Covariance of Neutron Cross Sections for 16O through R-matrix Analysis NUCLEAR REACTIONS 16O(n, X), E<5 MeV; calculated σ and covariances. R-matrix analysis, comparison with available data.
doi: 10.1016/j.nds.2014.12.028
2014HA03 Phys.Rev. C 89, 014623 (2014) G.M.Hale, L.S.Brown, M.W.Paris Effective field theory as a limit of R-matrix theory for light nuclear reactions NUCLEAR REACTIONS 3H(d, n)4He, E(cm)<0.10 MeV; analyzed astrophysical S(E) factor by single level four-parameter R-matrix fit. Corresponds to nonrelativistic effective quantum field theory description in companion (2014Br02) article for d+t fusion reaction.
doi: 10.1103/PhysRevC.89.014623
2014KU13 Nucl.Data Sheets 118, 250 (2014) S.Kunieda, T.Kawano, M.Paris, G.Hale, K.Shibata, T.Fukahori R-matrix Analysis for n +16O Cross-sections up to En=6.0 MeV with Covariances NUCLEAR REACTIONS 16O(n, α), E=0.5-4.7 MeV;13C(α, n), E=0.7-4.7 MeV; calculated σ using multi-channel R-matrix with care for covariances; deduced resonances. Compared to ENDF/B-VII.1 and Harisopulos data.
doi: 10.1016/j.nds.2014.04.050
2014PA34 Nucl.Data Sheets 120, 184 (2014) M.Paris, G.Hale, A.Hayes-Sterbenz, G.Jungman R-matrix Analysis of Reactions in the 9B Compound System NUCLEAR REACTIONS 6Li(3He, 3He), (3He, p), (3He, d), (3He, γ), 2H(7Be, X)9B, E<6 MeV; analyzed available data.; deduced σ, σ(θ), resonance widths. Two-body unitary R-matrix method using the code EDA.
doi: 10.1016/j.nds.2014.07.041
2012CH32 Phys.Rev. C 86, 015206 (2012) W.Chen, H.Gao, W.J.Briscoe, D.Dutta, A.E.Kudryavtsev, M.Mirazita, M.W.Paris, P.Rossi, S.Stepanyan, I.I.Strakovsky, V.E.Tarasov, R.L.Workman Amplitude analysis of γn → π-p data above 1 GeV
doi: 10.1103/PhysRevC.86.015206
2012WO02 Phys.Rev. C 85, 025201 (2012) R.L.Workman, W.J.Briscoe, M.W.Paris, I.I.Strakovsky Updated SAID analysis of pion photoproduction data
doi: 10.1103/PhysRevC.85.025201
2012WO05 Phys.Rev. C 86, 015202 (2012) R.L.Workman, M.W.Paris, W.J.Briscoe, I.I.Strakovsky Unified Chew-Mandelstam SAID analysis of pion photoproduction data
doi: 10.1103/PhysRevC.86.015202
2012WO06 Phys.Rev. C 86, 035202 (2012) R.L.Workman, R.A.Arndt, W.J.Briscoe, M.W.Paris, I.I.Strakovsky Parameterization dependence of T-matrix poles and eigenphases from a fit to πN elastic scattering data
doi: 10.1103/PhysRevC.86.035202
2011LA16 J.Korean Phys.Soc. 59, 995s (2011) A.B.Laptev, R.C.Haight, R.A.Arndt, W.J.Briscoe, M.W.Paris, I.I.Strakovsky, R.L.Workman The Recent Absolute Total np and pp Cross Section Determinations: Quality of Data Description and Prediction of Experimental Observables NUCLEAR REACTIONS 1H(p, p), E=0-3000 MeV;1H(n, n), E=0-1300 MeV; calculated, analyzed np and pp SAID facility scattering σ; evaluated σ using partial-wave analysis.
doi: 10.3938/jkps.59.995
2011WO06 Eur.Phys.J. A 47, 143 (2011) R.L.Workman, M.W.Paris, W.J.Briscoe, L.Tiator, S.Schumann, M.Ostrick, S.S.Kamalov Model dependence of single-energy fits to pion photoproduction data NUCLEAR REACTIONS 1H(γ, π0), E=200-1200 MeV; calculated σ, σ(θ) using MAID with different γ multipolarities. Compared with data.
doi: 10.1140/epja/i2011-11143-y
2010PA28 Phys.Rev. C 82, 035202 (2010) Toward a unified description of hadro- and photoproduction: S-wave π- and η-photoproduction amplitudes
doi: 10.1103/PhysRevC.82.035202
2009PA08 Phys.Rev. C 79, 025208 (2009) Dynamical coupled channels calculation of pion and omega meson production
doi: 10.1103/PhysRevC.79.025208
2009WO02 Phys.Rev. C 79, 038201 (2009) R.L.Workman, R.A.Arndt, M.W.Paris Resonance parameters from K-matrix and T-matrix poles
doi: 10.1103/PhysRevC.79.038201
2005CA10 Eur.Phys.J. A 24, Supplement 1, 123 (2005) Parity violation in few-nucleon systems NUCLEAR REACTIONS 1H(polarized p, p), E=10-350 MeV; 1H(polarized n, n), E(cm)=5-180 MeV; calculated longitudinal asymmetry, parity-violation effects. 1H(n, γ), E=thermal; calculated total σ, parity-violating asymmetry.
doi: 10.1140/epjad/s2005-05-022-x
2005PA14 Phys.Rev. C 71, 022201 (2005) V.R.Pandharipande, M.W.Paris, I.Sick Virtual photon asymmetry for confined, interacting Dirac particles with spin symmetry
doi: 10.1103/PhysRevC.71.022201
2005PA17 Eur.Phys.J. A 24, Supplement 1, 143 (2005) M.W.Paris, V.R.Pandharipande, I.Sick Spin asymmetries for confined Dirac particles
doi: 10.1140/epjad/s2005-05-025-7
2004SC38 Phys.Rev. C 70, 044007 (2004) R.Schiavilla, J.Carlson, M.Paris Parity-violating interaction effects in the np system NUCLEAR REACTIONS 1H(polarized n, n), E=0-180 MeV; 1H(polarized n, γ), E=thermal; 2H(polarized γ, n), E=threshold-20 MeV; 2H(polarized e, e'n), E=70-104 MeV; calculated σ, σ(θ), parity-violating asymmetries.
doi: 10.1103/PhysRevC.70.044007
2003PA25 Phys.Rev. C 68, 025201 (2003) Electromagnetic response of confined Dirac particles
doi: 10.1103/PhysRevC.68.025201
2003PA28 Eur.Phys.J. A 17, 401 (2003) Spacelike and timelike response of confined relativistic particles
doi: 10.1140/epja/i2002-10204-8
2003SC04 Phys.Rev. C 67, 032501 (2003) R.Schiavilla, J.Carlson, M.Paris Parity-violating interactions and currents in the deuteron NUCLEAR REACTIONS 1H(polarized n, γ), E=thermal; calculated radiative capture σ, asymmetry, parity-violation effects. 2H(e, e'p), E=193 MeV; calculated longitudinal asymmetry vs momentum transfer, parity-violation effects.
doi: 10.1103/PhysRevC.67.032501
2002PA12 Phys.Rev. C65, 035203 (2002) Final State Interaction Contribution to the Response of Confined Relativistic Particles
doi: 10.1103/PhysRevC.65.035203
2000PA42 Phys.Rev. C62, 015201 (2000) Quantum Monte Carlo Calculations of Six-Quark States
doi: 10.1103/PhysRevC.62.015201
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