NSR Query Results

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NSR database version of May 21, 2024.

Search: Author = M.Paris

Found 37 matches.

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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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2015HA02      Nucl.Data Sheets 123, 165 (2015)

G.M.Hale, M.W.Paris

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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2010PA28      Phys.Rev. C 82, 035202 (2010)

M.W.Paris, R.L.Workman

Toward a unified description of hadro- and photoproduction: S-wave π- and η-photoproduction amplitudes

doi: 10.1103/PhysRevC.82.035202
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2009PA08      Phys.Rev. C 79, 025208 (2009)


Dynamical coupled channels calculation of pion and omega meson production

doi: 10.1103/PhysRevC.79.025208
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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
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2005CA10      Eur.Phys.J. A 24, Supplement 1, 123 (2005)

J.Carlson, M.Paris

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
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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
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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
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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
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2003PA25      Phys.Rev. C 68, 025201 (2003)


Electromagnetic response of confined Dirac particles

doi: 10.1103/PhysRevC.68.025201
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2003PA28      Eur.Phys.J. A 17, 401 (2003)


Spacelike and timelike response of confined relativistic particles

doi: 10.1140/epja/i2002-10204-8
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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
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2002PA12      Phys.Rev. C65, 035203 (2002)

M.W.Paris, V.R.Pandharipande

Final State Interaction Contribution to the Response of Confined Relativistic Particles

doi: 10.1103/PhysRevC.65.035203
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2000PA42      Phys.Rev. C62, 015201 (2000)

M.W.Paris, V.R.Pandharipande

Quantum Monte Carlo Calculations of Six-Quark States

doi: 10.1103/PhysRevC.62.015201
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Note: The following list of authors and aliases matches the search parameter M.Paris: , M.W.PARIS