NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = P.Sauer Found 121 matches. Showing 1 to 100. [Next]2021LA03 Phys.Rev. C 103, 034311 (2021) G.Laskaris, W.Ji, X.Yan, J.Zhou, W.R.Zimmerman, M.W.Ahmed, T.Averett, A.Deltuva, A.C.Fonseca, H.Gao, J.Golak, A.Kafkarkou, H.J.Karwowski, B.Lalremruata, J.Manfredi, J.M.Mueller, P.U.Sauer, R.Skibinski, A.P.Smith, M.B.Tsang, H.R.Weller, H.Witala, Y.K.Wu, Z.W.Zhao First measurement of the asymmetry and the Gerasimov-Drell-Hearn integrand from the 3He((pol)(γ(pol), p)2H reaction at an incident photon energy of 29 MeV NUCLEAR REACTIONS 3He(polarized γ, p)2H, E=29 MeV; measured Ep, Ip, p(θ), time-of-flight, spin-dependent asymmetry and total σ using a circularly polarized, monoenergetic γ-ray beam and a longitudinally polarized 3He target, and an array of depleted silicon surface barrier detectors at the High Intensity γ-ray Source (HIγS) facility at TUNL; deduced contribution from the two-body photo-disintegration to the 3He Gerasimov-Drell-Hearn (GDH) integrands, and compared with the state-of-the art three-nucleon system calculations.
doi: 10.1103/PhysRevC.103.034311
2015DE08 Phys.Rev. C 91, 034002 (2015) Three-nucleon system: Irreducible and reducible contributions of the three-nucleon force NUCLEAR REACTIONS 2H(n, n), E=10, 13 MeV; analyzed neutron analyzing power Ay; 2H(p, p), E=135, 250 MeV; analyzed differential σ(θ) and deuteron vector analyzing power, deuteron-to-proton spin-transfer coefficient, proton analyzing powers Ax and Ay for proton-deuteron breakup using CD Bonn, CD Bonn+Δ, CD Bonn+Δ+U1, CD Bonn+Δ+U2, and CD Bonn+Δ+U3 calculations. Three-nucleon force effects on the bound-state energies.
doi: 10.1103/PhysRevC.91.034002
2015LA22 Phys.Lett. B 750, 547 (2015) G.Laskaris, X.Yan, J.M.Mueller, W.R.Zimmerman, W.Xiong, M.W.Ahmed, T.Averett, P.-H.Chu, A.Deltuva, C.Flower, A.C.Fonseca, H.Gao, J.Golak, J.N.Heideman, H.J.Karwowski, M.Meziane, P.U.Sauer, R.Skibinski, I.I.Strakovsky, H.R.Weller, H.Witala, Y.K.Wu Measurement of the doubly-polarized 3He(pol)(γ(pol), n)pp reaction at 16.5 MeV and its implications for the GDH sum rule NUCLEAR REACTIONS 3He(polarized γ, n), E=12.8, 14.7 MeV; measured reaction products, Eγ, Iγ, En, In; deduced σ(θ, E), σ, contribution from the three-body channel to the Gerasimov-Drell-Hearn (GDH) integrand. Comparison with available data, Monte Carlo simulations using GEANT4.
doi: 10.1016/j.physletb.2015.09.065
2014LA04 Phys.Rev. C 89, 024002 (2014) G.Laskaris, Q.Ye, B.Lalremruata, Q.J.Ye, M.W.Ahmed, T.Averett, A.Deltuva, D.Dutta, A.C.Fonseca, H.Gao, J.Golak, M.Huang, H.J.Karwowski, J.M.Mueller, L.S.Myers, C.Peng, B.A.Perdue, X.Qian, P.U.Sauer, R.Skibinski, S.Stave, J.R.Tompkins, H.R.Weller, H.Witala, Y.K.Wu, Y.Zhang, W.Zheng Spin-dependent cross sections from the three-body photodisintegration of 3He at incident energies of 12.8 and 14.7 MeV NUCLEAR REACTIONS 3He(polarized γ, n), E=12.8, 14.7 MeV; measured time-of-flight spectra, γ spectra, and neutron spectra from three-body breakup of 3He using 16 liquid scintillator detectors, spin-dependent double-differential σ(E, θ) at HiγS-TUNL facility. Monoenergetic circularly polarized γ beam, and longitudinally polarized 3He target. Comparison with previous experimental results, and with theoretical calculations.
doi: 10.1103/PhysRevC.89.024002
2014SA50 Int.J.Mod.Phys. E23, 1430015 (2014) Three-nucleon forces
doi: 10.1142/S021830131430015X
2013LA14 Phys.Rev.Lett. 110, 202501 (2013) G.Laskaris, Q.Ye, B.Lalremruata, Q.J.Ye, M.W.Ahmed, T.Averett, A.Deltuva, D.Dutta, A.C.Fonseca, H.Gao, J.Golak, M.Huang, H.J.Karwowski, J.M.Mueller, L.S.Myers, C.Peng, B.A.Perdue, X.Qian, P.U.Sauer, R.Skibinski, S.Stave, J.R.Tompkins, H.R.Weller, H.Witala, Y.K.Wu, Y.Zhang, W.Zheng First Measurements of Spin-Dependent Double-Differential Cross Sections and the Gerasimov-Drell-Hearn Integrand from 3He(pol) (γ(pol), n)pp at Incident Photon Energies of 12.8 and 14.7 MeV NUCLEAR REACTIONS 3He(polarized γ, n), E=12.8, 14.7 MeV; measured reaction products, En, In; deduced σ, σ(θ, E) and their uncertainties, contributions from the three-body photodisintegration to the 3He Gerasimov-Drell-Hearn integrand. Comparison with available data.
doi: 10.1103/PhysRevLett.110.202501
2011DE04 Few-Body Systems 49, 27 (2011) A.Deltuva, A.C.Fonseca, P.U.Sauer Few-Nucleon Calculations With Δ Degrees of Freedom NUCLEAR STRUCTURE 3H, 3,4He; calculated binding energies. Realistic coupled channel potential CD Bonn + Δ. NUCLEAR REACTIONS 2H(p, p), E=135, 250 MeV;3He(p, p), E=5.54 MeV; calculated σ(θ). Realistic coupled channel potential CD Bonn + Δ.
doi: 10.1007/s00601-010-0110-z
2010DE03 Phys.Rev. C 81, 019802 (2010) A.Deltuva, A.C.Fonseca, P.U.Sauer Comment on "Exact three-dimensional wave function and the on-shell t matrix for the sharply cut-off Coulomb potential: Failure of the standard renormalization factor"
doi: 10.1103/PhysRevC.81.019802
2009DE48 Phys.Rev. C 80, 064004 (2009) A.Deltuva, A.C.Fonseca, P.U.Sauer Relativistic corrections of one-nucleon current in low-energy three-nucleon photonuclear reactions NUCLEAR REACTIONS 1H(d, γ), E=10, 17.5, 29, 45 MeV; 2H(p, γ), E=5, 100 MeV; calculated analyzing powers and σ(θ) for radiative captures as functions of d-3He and p-γ scattering angles. 3He(γ, X), E=11.4, 15.2, 20.6 MeV; calculated linear photon asymmetry, analyzing powers, parallel-antiparallel spin asymmetry, and differential cross sections of two- and three-body photodisintegration of 3He as functions of p-γ scattering angle and nucleon energy. Realistic hadronic dynamics calculations including the Coulomb force. Comparison with experimental data.
doi: 10.1103/PhysRevC.80.064004
2008BO32 Phys.Rev. C 78, 054001 (2008) W.U.Boeglin, H.Arenhovel, K.I.Blomqvist, R.Bohm, M.Distler, R.Edelhoff, I.Ewald, R.Florizone, J.Friedrich, R.Geiges, M.Kahrau, M.Korn, H.Kramer, K.W.Krygier, V.Kunde, A.Liesenfeld, K.Merle, R.Neuhausen, E.A.J.M.Offermann, Th.Pospischil, A.W.Richter, G.Rosner, P.Sauer, S.Schardt, A.Serdarevic, A.Wagner, Th.Walcher, S.Wolf, J.Jourdan, I.Sick, M.Kuss, M.Potokar, A.Rokavec, B.Vodenik, S.Sirca fLT response function of 2H(e, e'p)n at Q2=0.33 GeV/c)2 NUCLEAR REACTIONS 2H(e, e'p), E=855.11 MeV; measured σ, missing momentum, kinematic variables; deduced interference response function. Comparison with Coupled Channels Calculations.
doi: 10.1103/PhysRevC.78.054001
2008DE02 Phys.Lett. B 660, 471 (2008) A.Deltuva, A.C.Fonseca, P.U.Sauer Four-nucleon system with Δ-isobar excitation NUCLEAR STRUCTURE 3H, 3,4He; calculated binding energies using a coupled channel potential. NUCLEAR REACTIONS 3H(n, n), E=0-6 MeV; analyzed σ. 3He(p, p), E=5.54 MeV; 3H(p, n), E=6 MeV; 2H(d, d), (d, p), (d, n), E=3 MeV; analyzed σ(θ), analyzing powers. Two-baryon coupled-channel potential with the higher order 3N and 4N forces.
doi: 10.1016/j.physletb.2007.12.058
2008KI21 Few-Body Systems 44, 11 (2008) St.Kistryn, E.Stephan, N.Kalantar-Nayestanaki, A.Biegun, K.Bodek, I.Ciepal, A.Deltuva, E.Epelbaum, A.C.Fonseca, W.Glockle, J.Golak, H.Kamada, M.Kis, B.Klos, A.Kozela, A.Nogga, M.Mahjour-Shafiei, A.Micherdzinska, P.U.Sauer, R.Skibinski, R.Sworst, H.Witala, J.Zejma, W.Zipper Studies of the three-nucleon system dynamics: Cross sections of the deuteron-proton breakup at 130 MeV NUCLEAR REACTIONS 1H(polarized d, 2p), E=130 MeV; measured particle spectra, break-up cross sections.
doi: 10.1007/s00601-008-0245-3
2007DE38 Nucl.Phys. A790, 52c (2007) A.Deltuva, A.C.Fonseca, P.U.Sauer Treatment of the Coulomb interaction in three-nucleon reactions NUCLEAR REACTIONS 2H(p, p), E=3 MeV; calculated σ(θ), analyzing powers. 2H(p, np), E=13 MeV; calculated σ(E, θ). Perturbative approach for screened Coulomb interaction.
doi: 10.1016/j.nuclphysa.2007.03.031
2007DE40 Nucl.Phys. A790, 344c (2007) A.Deltuva, A.C.Fonseca, P.U.Sauer Study of the Coulomb effect in the photodisintegration of 3He NUCLEAR REACTIONS 3He(γ, X), E≈7-17 MeV; calculated total σ. 3He(γ, np), E=55, 85 MeV; calculated σ(θ). 3He(γ, n), (γ, p)E=15 MeV; calculated σ(E, θ), photon asymmetry. Screening and renormalization approach for inclusion of Coulomb interaction.
doi: 10.1016/j.nuclphysa.2007.03.062
2007MA46 Phys.Rev. C 76, 014004 (2007) Y.Maeda, H.Sakai, K.Fujita, M.B.Greenfield, K.Hatanaka, M.Hatano, J.Kamiya, T.Kawabata, H.Kuboki, H.Okamura, J.Rapaport, T.Saito, Y.Sakemi, M.Sasano, K.Sekiguchi, Y.Shimizu, K.Suda, Y.Tameshige, A.Tamii, T.Wakasa, K.Yako, J.Blomgren, P.Mermod, A.Ohrn, M.Osterlund, H.Witala, A.Deltuva, A.C.Fonseca, P.U.Sauer, W.Glockle, J.Golak, H.Kamada, A.Nogga, R.Skibinski Differential cross section and analyzing power measurements for (n-pol, d) elastic scattering at 248 MeV NUCLEAR REACTIONS 2H(n, n), E=248 MeV; measured En, σ and vector analyzing power.
doi: 10.1103/PhysRevC.76.014004
2007ST29 Phys.Rev. C 76, 057001 (2007) E.Stephan, St.Kistryn, R.Sworst, A.Biegun, K.Bodek, I.Ciepal, A.Deltuva, E.Epelbaum, A.Fonseca, W.Glockle, J.Golak, N.Kalantar-Nayestanaki, H.Kamada, M.Kis, A.Kozela, M.Mahjour-Shafiei, A.Micherdzinska, A.Nogga, P.U.Sauer, R.Skibinski, H.Witala, J.Zejma, W.Zipper Vector and tensor analyzing powers of elastic deuteron-proton scattering at 130 MeV deuteron beam energy NUCLEAR REACTIONS 1H(polarized d, d), E=130 MeV; measured cross sections, angular distributions, vector and tensor analyzing powers.
doi: 10.1103/PhysRevC.76.057001
2006BI03 Acta Phys.Pol. B37, 213 (2006) A.Biegun, E.Stephan, St.Kistryn, K.Bodek, I.Ciepal, A.Deltuva, E.Epelbaum, W.Gloeckle, J.Golak, N.Kalantar-Nayestanaki, H.Kamada, M.Kis, B.Klos, A.Kozela, J.Kuros-Zolnierczuk, M.Mahjour-Shafiei, U.-G.Meissner, A.Micherdzinska, A.Nogga, P.U.Sauer, R.Skibinski, R.Sworst, H.Witala, J.Zejma, W.Zipper Three-nucleon force effects in the analyzing powers of the d(pol)p breakup at 130 MeV NUCLEAR REACTIONS 1H(polarized d, 2p), E=130 MeV; measured analyzing powers; deduced no three-nucleon force effects.
2006DE26 Phys.Rev. C 73, 057001 (2006) A.Deltuva, A.C.Fonseca, P.U.Sauer New calculation schemes for proton-deuteron scattering including the Coulomb interaction NUCLEAR REACTIONS 2H(p, p), E=3 MeV; calculated analyzing powers. 2H(p, np), E=130 MeV; calculated σ(E, θ), analyzing power. Perturbative approach for screened Coulomb interaction.
doi: 10.1103/PhysRevC.73.057001
2006KI13 Phys.Lett. B 641, 23 (2006) St.Kistryn, E.Stephan, B.Klos, A.Biegun, K.Bodek, I.Ciepal, A.Deltuva, A.C.Fonseca, N.Kalantar-Nayestanaki, M.Kis, A.Kozela, M.Mahjour-Shafiei, A.Micherdzinska, P.U.Sauer, R.Sworst, J.Zejma, W.Zipper Evidence of the Coulomb-force effects in the cross-sections of the deuteron-proton breakup at 130 MeV NUCLEAR REACTIONS 1H(polarized d, 2p), E=130 MeV; measured σ(θ); deduced Coulomb effects. Comparison with coupled-channel model.
doi: 10.1016/j.physletb.2006.08.013
2006LE23 Phys.Rev. C 73, 064001 (2006) J.Ley, C.Duweke, R.Emmerich, A.Imig, H.Paetz gen.Schieck, J.Golak, H.Witala, E.Epelbaum, A.Deltuva, A.C.Fonseca, W.Glockle, U.-G.Meissner, A.Nogga, P.U.Sauer Cross sections and tensor analyzing powers Ayy of the reaction 1H(d(pol), pp)n in "symmetric constant relative energy" geometries at Ed = 19 MeV NUCLEAR REACTIONS 1H(polarized d, 2p), E=19 MeV; measured σ(E, θ), tensor analyzing powers Ayy for four geometries. Comparisons with Faddeev calculations using phenomenological NN potentials with and without three-body forces, effect of Delta and Coulomb interaction, chiral forces.
doi: 10.1103/PhysRevC.73.064001
2005DE17 Phys.Rev. C 71, 054005 (2005) A.Deltuva, A.C.Fonseca, P.U.Sauer Momentum-space treatment of the Coulomb interaction in three-nucleon reactions with two protons NUCLEAR REACTIONS 2H(p, p), E=3, 9, 10, 135 MeV; 2H(p, γ), E=3, 150 MeV; 1H(d, γ), E=17.5 MeV; calculated σ(θ), analyzing powers. 3He(e, e'p), E=66-530 MeV; calculated σ(E, θ).
doi: 10.1103/PhysRevC.71.054005
2005DE21 Phys.Rev. C 71, 064003 (2005) A.Deltuva, A.C.Fonseca, A.Kievsky, S.Rosati, P.U.Sauer, M.Viviani Benchmark calculation for proton-deuteron elastic scattering observables including the Coulomb interaction NUCLEAR REACTIONS 2H(p, p), E=3-65 MeV; calculated σ(θ), proton and deuteron analyzing powers, tensor analyzing powers, spin transfer coefficients.
doi: 10.1103/PhysRevC.71.064003
2005DE39 Phys.Rev.Lett. 95, 092301 (2005) A.Deltuva, A.C.Fonseca, P.U.Sauer Calculation of Proton-Deuteron Breakup Reactions including the Coulomb Interaction between the Two Protons NUCLEAR REACTIONS 2H(p, np), E=13, 65, 130 MeV; calculated σ(E, θ), Ay(θ), Coulomb interaction effects.
doi: 10.1103/PhysRevLett.95.092301
2005DE56 Phys.Rev. C 72, 054004 (2005); Erratum Phys.Rev. C 72, 059903 (2005) A.Deltuva, A.C.Fonseca, P.U.Sauer Momentum-space description of three-nucleon breakup reactions including the Coulomb interaction NUCLEAR REACTIONS 2H(p, np), E=10-130 MeV; 3He(γ, np), E ≈ 15-85 MeV; calculated σ(E, θ), analyzing powers, response functions. Screening and renormalization approach for inclusion of Coulomb interaction.
doi: 10.1103/PhysRevC.72.054004
2005ER03 Phys.Rev. C 71, 064004 (2005) K.Ermisch, H.R.Amir-Ahmadi, A.M.van den Berg, R.Castelijns, B.Davids, A.Deltuva, E.Epelbaum, W.Glockle, J.Golak, M.N.Harakeh, M.Hunyadi, M.A.de Huu, N.Kalantar-Nayestanaki, H.Kamada, M.Kis, M.Mahjour-Shafiei, A.Nogga, P.U.Sauer, R.Skibinski, H.Witala, H.J.Wortche Systematic investigation of three-nucleon force effects in elastic scattering of polarized protons from deuterons at intermediate energies NUCLEAR REACTIONS 2H(polarized p, p), E=108, 120, 135, 150, 170, 190 MeV; measured σ(θ) and vector analyzing power; deduced three-nucleon forces contribution and necessity of inclusion. Comparisons with model predictions.
doi: 10.1103/PhysRevC.71.064004
2005KI19 Phys.Rev. C 72, 044006 (2005) St.Kistryn, E.Stephan, A.Biegun, K.Bodek, A.Deltuva, E.Epelbaum, K.Ermisch, W.Glockle, J.Golak, N.Kalantar-Nayestanaki, H.Kamada, M.Kis, B.Klos, A.Kozela, J.Kuros-Zolnierczuk, M.Mahjour-Shafiei, U.-G.Meissner, A.Micherdzinska, A.Nogga, P.U.Sauer, R.Skibinski, R.Sworst, H.Witala, J.Zejma, W.Zipper Systematic study of three-nucleon force effects in the cross section of the deuteron-proton breakup at 130 MeV NUCLEAR REACTIONS 2H(p, 2p), E=130 MeV; measured Ep, pp-coin, σ(θ1, θ2); deduced three-nucleon force effects.
doi: 10.1103/PhysRevC.72.044006
2005ME09 Phys.Lett. B 617, 18 (2005) A.A.Mehmandoost-Khajeh-Dad, H.R.Amir-Ahmadi, J.C.S.Bacelar, A.M.van den Berg, R.Castelijns, A.Deltuva, E.D.van Garderen, W.Glockle, J.Golak, N.Kalantar-Nayestanaki, H.Kamada, M.Kis, R.Koohi-Fayegh-Dehkordi, H.Lohner, M.Mahjour-Shafiei, H.Mardanpour, J.G.Messchendorp, A.Nogga, P.Sauer, S.V.Shende, R.Skibinski, H.Witala, H.J.Wortche Spin observables in deuteron-proton radiative capture at intermediate energies NUCLEAR REACTIONS 1H(polarized d, γ), E=55, 66.5, 90 MeV/nucleon; measured Eγ, (particle)γ-coin, vector and tensor analyzing powers. Comparison with model predictions.
doi: 10.1016/j.physletb.2005.04.071
2004DE11 Phys.Rev. C 69, 034004 (2004) A.Deltuva, L.P.Yuan, J.Adam, Jr., A.C.Fonseca, P.U.Sauer Trinucleon photonuclear reactions with Δ-isobar excitation: Processes below pion-production threshold NUCLEAR REACTIONS 2H(p, γ), E=100, 150 MeV; calculated σ(θ), analyzing powers. 1H(d, γ), E=20, 95 MeV; calculated σ(θ). 3H(γ, np), E=5-30 MeV; calculated photodisintegration σ. 3He(γ, np), E=85-140 MeV; calculated σ(θ). Charge-dependent potential, role of isobar excitation discussed. Comparisons with data.
doi: 10.1103/PhysRevC.69.034004
2004DE43 Phys.Rev. C 70, 034004 (2004) A.Deltuva, L.P.Yuan, J.Adam, Jr., P.U.Sauer Three-body electrodisintegration of the three-nucleon bound state with Δ-isobar excitation: Processes below pion-production threshold NUCLEAR REACTIONS 3H, 3He(e, e), E not given; calculated electromagnetic form factors. 3He(e, e'2p), E=390, 563.7 MeV; calculated σ(E, θ). 3H, 3He(e, e'X), E=high; calculated longitudinal and transverse response. Δ-isobar excitation effects discussed. NUCLEAR MOMENTS 3H, 3He; calculated μ. Comparison with data.
doi: 10.1103/PhysRevC.70.034004
2004FR16 Nucl.Phys. A737, 260 (2004) T.Frederico, J.H.O.Sales, B.V.Carlson, P.U.Sauer Light-front time picture of few-body systems
doi: 10.1016/j.nuclphysa.2004.03.087
2003CH05 Phys.Rev. C 67, 014002 (2003) K.Chmielewski, A.Deltuva, A.C.Fonseca, S.Nemoto, P.U.Sauer Breakup in nucleon-deuteron scattering with Δ-isobar excitation NUCLEAR REACTIONS 2H(p, np), E=13, 65 MeV; 1H(d, np), E=52 MeV; calculated σ(E, θ), analyzing powers. Coupled-channel two-baryon potential, Δ-isobar excitation, comparisons with data.
doi: 10.1103/PhysRevC.67.014002
2003DE07 Phys.Rev. C 67, 034001 (2003) A.Deltuva, K.Chmielewski, P.U.Sauer Nucleon-deuteron scattering with Δ-isobar excitation: Chebyshev expansion of two-baryon transition matrix NUCLEAR REACTIONS 2H(n, n), (n, np), (p, p), (p, np), E=10, 65, 135 MeV; calculated elastic and breakup σ(θ), analyzing powers. Solution of Faddeev equations by Chebyshev expansion of two-baryon transition matrix. Comparison with data.
doi: 10.1103/PhysRevC.67.034001
2003DE16 Phys.Rev. C 67, 054004 (2003) A.Deltuva, K.Chmielewski, P.U.Sauer Nucleon-deuteron scattering with Δ-isobar excitation: Perturbation theory NUCLEAR REACTIONS 2H(n, n), (p, p)(n, np), (p, np), E=13-190 MeV; calculated σ(E, θ), Ay(θ), Δ-isobar excitation contribution. Perturbative approach, comparisons with data.
doi: 10.1103/PhysRevC.67.054004
2003DE19 Phys.Rev. C 68, 024005 (2003) A.Deltuva, R.Machleidt, P.U.Sauer Realistic two-baryon potential coupling two-nucleon and nucleon-Δ-isobar states: Fit and applications to three-nucleon system NUCLEAR STRUCTURE 3H, 3He; calculated binding energies, Δ-isobar effect, nucleon and Δ momentum distributions. NUCLEAR REACTIONS 2H(n, n), (p, p), E=108-190 MeV; 2H(n, np), (p, np), E=65 MeV; calculated σ(θ), analyzing powers. Two-baryon coupled-channels potential.
doi: 10.1103/PhysRevC.68.024005
2003DE43 Mod.Phys.Lett. A 18, 426 (2003) A.Deltuva, K.Chmielewski, P.U.Sauer Nucleon-deuteron scattering with Δ-isobar excitation: new technical developments NUCLEAR REACTIONS 2H(p, p), E=120-170 MeV; calculated σ(θ), analyzing powers, role of Δ-isobar excitation. Two-dimensional Chebyshev expansion of the two-baryon transition matrix.
doi: 10.1142/S0217732303010624
2003YU10 Mod.Phys.Lett. A 18, 244 (2003) L.P.Yuan, K.Chmielewski, A.Deltuva, M.Oelsner, P.U.Sauer, J.Adam, Jr. Two-body electro disintegration of the trinucleon bound state NUCLEAR REACTIONS 3He(e, e'p), E=390, 2400 MeV; calculated σ(E, θ), asymmetry.
doi: 10.1142/S0217732303010296
2002YU02 Few-Body Systems 32, 83 (2002) L.P.Yuan, K.Chmielewski, M.Oelsner, P.U.Sauer, A.C.Fonseca, J.Adam, Jr. Trinucleon Photo-Reactions with Δ-Isobar Excitation: Radiative nucleon-deuteron capture and two-body photo-disintegration of the three-nucleon bound state NUCLEAR REACTIONS 1H(d, γ), E ≈ 0-100 MeV; calculated σ(θ), polarization observables. 3H, 3He(γ, X), E ≈ 5-40 MeV; calculated photo-disintegration σ, σ(θ). Effects of Δ-isobar excitation discussed.
doi: 10.1007/s00601-002-0109-1
2002YU05 Phys.Rev. C 66, 054004 (2002) L.P.Yuan, K.Chmielewski, M.Oelsner, P.U.Sauer, J.Adam Two-body electrodisintegration of the three-nucleon bound state with Δ-isobar excitation NUCLEAR REACTIONS 3He(e, e'p), (polarized e, e'p), E=360-2400 MeV; calculated σ(θ), σ(E), asymmetries; deduced role of Δ-isobar excitation. Comparisons with data.
doi: 10.1103/PhysRevC.66.054004
2001SA13 Nucl.Phys. A684, 531c (2001) P.U.Sauer, K.Chmielewski, S.Nemoto, S.Oryu Three-Nucleon Force Mediated by Δ-Isobar Excitation: Application to Nucleon-Deuteron Scattering NUCLEAR REACTIONS 2H(n, n), (p, p), E=2-135 MeV; calculated σ(θ), polarization observables; deduced role of Δ-isobar excitation. Comparison with data.
doi: 10.1016/S0375-9474(01)00375-X
2001SA23 Phys.Rev. C63, 064003 (2001) J.H.O.Sales, T.Frederico, B.V.Carlson, P.U.Sauer Renormalization of the Ladder Light-Front Bethe-Salpeter Equation in the Yukawa Model
doi: 10.1103/PhysRevC.63.064003
2001SA32 Nucl.Phys. A689, 341c (2001) P.U.Sauer, K.Chmielewski, S.Nemoto, S.Oryu Nucleon-Deuteron Scattering with Δ-Isobar Excitation NUCLEAR REACTIONS 2H(p, p), (n, n), E=135 MeV; calculated Ay(θ), other spin observables. 2H(p, np), (n, np), E=65 MeV; calculated σ(θ), Ay(θ). Comparisons with data.
doi: 10.1016/S0375-9474(01)00850-8
2001YU06 Nucl.Phys. A689, 433c (2001) L.P.Yuan, K.Chmielewski, M.Oelsner, P.U.Sauer, A.C.Fonseca, J.Adam, Jr. Description of Electromagnetic Processes in the Three-Nucleon System with Δ-Isobar Excitation NUCLEAR REACTIONS 1H(d, γ), E=19.8 MeV; calculated σ(θ), analyzing power. 3He(e, e'p), E=367, 390 MeV; calculated σ(θ). Comparisons with data.
doi: 10.1016/S0375-9474(01)00872-7
2000FR07 Nucl.Phys. A663-664, 389c (2000) J.M.Friedrich, P.Bartsch, D.Baumann, J.Berthot, P.Y.Bertin, V.Breton, W.U.Boeglin, R.Bohm, N.d'Hose, T.Caprano, S.Derber, N.Degrande, M.Ding, M.O.Distler, J.E.Ducret, R.Edelhoff, I.Ewald, H.Fonvieille, J.Friedrich, R.Geiges, Th.Gousset, P.A.M.Guichon, H.Holvoet, Ch.Hyde-Wright, P.Jennewein, M.Kahrau, S.Kerhoas, M.Korn, H.Kramer, K.W.Krygier, V.Kunde, B.Lannoy, D.Lhuillier, A.Liesenfeld, C.Marchand, D.Marchand, J.Martino, H.Merkel, K.Merle, P.Merle, G.De Meyer, J.Mougey, R.Neuhausen, E.Offermann, Th.Pospischil, G.Quemener, O.Ravel, Y.Roblin, J.Roche, D.Rohe, G.Rosner, D.Ryckbosch, P.Sauer, H.Schmieden, S.Schardt, G.Tamas, M.Tytgat, M.Vanderhaeghen, L.Van Hoorebeke, R.Van de Vyver, J.Van de Wiele, P.Vernin, A.Wagner, Th.Walcher The First Dedicated Virtual Compton Scattering Experiment at MAMI NUCLEAR REACTIONS 1H(e, e'γ), E not given; measured ep-coin, σ(E, θ(e), θ(p)); deduced structure function.
doi: 10.1016/S0375-9474(99)00624-7
2000SA13 Phys.Rev. C61, 044003 (2000) J.H.O.Sales, T.Frederico, B.V.Carlson, P.U.Sauer Light-Front Bethe-Salpeter Equation
doi: 10.1103/PhysRevC.61.044003
1999DE45 Nucl.Phys. A660, 219 (1999) J.P.B.C.de Melo, T.Frederico, H.W.L.Naus, P.U.Sauer Convariance of Light-Front Models: Pair current
doi: 10.1016/S0375-9474(99)00371-1
1999LI41 Phys.Lett. 468B, 20 (1999) A.Liesenfeld, A.W.Richter, S.Sirca, K.I.Blomqvist, W.U.Boeglin, K.Bohinc, R.Bohm, M.Distler, D.Drechsel, R.Edelhoff, I.Ewald, J.Friedrich, J.M.Friedrich, R.Geiges, M.Kahrau, M.Korn, K.W.Krygier, V.Kunde, H.Merkel, K.Merle, U.Muller, R.Neuhausen, T.Pospischil, M.Potokar, A.Rokavec, G.Rosner, P.Sauer, S.Schardt, H.Schmieden, L.Tiator, B.Vodenik, A.Wagner, Th.Walcher, S.Wolf A Measurement of the Axial Form Factor of the Nucleon by the p(e, e'π+)n Reaction at W = 1125 MeV NUCLEAR REACTIONS 1H(e, e'π+), E=405-855 MeV; measured longitudinal, transverse σ(θ); deduced axial mass parameter. Effective Lagrangian model.
doi: 10.1016/S0370-2693(99)01204-6
1999RO30 Nucl.Phys. (Supplement) A654, 547c (1999) J.Roche, P.Bartsch, J.Berthot, P.Y.Bertin, V.Breton, W.U.Boeglin, R.Bohm, N.d'Hose, T.Caprano, S.Derber, N.Degrande, M.Distler, J.E.Ducret, R.Edelhoff, I.Ewald, H.Fonvieille, J.Friedrich, J.M.Friedrich, R.Geiges, Th.Gousset, P.A.M.Guichon, H.Holvoet, Ch.Hyde-Wright, P.Jennewein, M.Kahrau, S.Kerhoas, M.Korn, H.Kramer, K.W.Krygier, V.Kunde, B.Lannoy, D.Lhuillier, A.Liesenfeld, C.Marchand, D.Marchand, J.Martino, H.Merkel, K.Merle, P.Merle, G.De Meyer, J.Mougey, R.Neuhausen, E.Offermann, Th.Pospischil, G.Quemener, O.Ravel, Y.Roblin, G.Rosner, D.Ryckbosch, P.Sauer, H.Schmieden, S.Schardt, G.Tamas, M.Tytgat, M.Vanderhaeghen, L.Van Hoorebeke, R.Van de Vyver, J.Van de Wiele, P.Vernin, A.Wagner, Th.Walcher, S.Wolf Virtual Compton Scattering Under π0 Threshold at Q2 = 0.33 GeV2. Preliminary Results. NUCLEAR REACTIONS 1H(e, e'γ), E=750-855 MeV; measured ep-coin, photon polarization, σ(θ). Virtual Compton scattering.
doi: 10.1016/S0375-9474(00)88498-5
1998AN13 Phys.Lett. 428B, 248 (1998) H.Anklin, L.J.deBever, K.I.Blomqvist, W.U.Boeglin, R.Bohm, M.Distler, R.Edelhoff, J.Friedrich, D.Fritschi, R.Geiges, J.Gotz, A.Honegger, P.Jennewein, J.Jourdan, M.Kahrau, M.Korn, H.Kramer, K.W.Krygier, G.Kubon, V.Kunde, A.Liesenfeld, G.Masson, K.Merle, R.Neuhausen, E.A.J.M.Offermann, Th.Petitjean, Th.Pospischil, M.Potokar, L.M.Qin, A.W.Richter, A.Rokavec, G.Rosner, P.Sauer, S.Schardt, I.Sick, S.Sirca, Ph.Trueb, M.Tuccillo, B.Vodenik, A.Wagner, Th.Walcher, G.Warren, S.Wolf, J.Zhao, M.Zeier, B.Zihlmann Precise Measurements of the Neutron Magnetic Form Factor NUCLEAR REACTIONS 2H(e, e'p), (e, e'n), E not given; measured σ ratios vs momentum transfer; deduced neutron magnetic form factor G(mn).
doi: 10.1016/S0370-2693(98)00442-0
1998BL06 Phys.Lett. 421B, 71 (1998) K.I.Blomqvist, W.U.Boeglin, R.Bohm, M.Distler, R.Edelhoff, J.Friedrich, R.Geiges, M.K.Jones, M.Kahrau, M.Korn, H.Kramer, K.W.Krygier, V.Kunde, M.Kuss, A.Liesenfeld, K.Merle, C.L.Morris, R.Neuhausen, E.A.J.M.Offermann, Th.Pospischil, M.Potokar, R.D.Ransome, A.W.Richter, B.G.Ritchie, A.Rokavec, G.Rosner, J.Ryckebusch, P.Sauer, S.Schardt, B.Vodenik, A.Wagner, Th.Walcher, S.Wolf, M.K.Yadav Investigation of Short-Range Nucleon-Nucleon Correlations using the Reaction 12C(e, e'pp) in Close to 4π Geometry NUCLEAR REACTIONS 12C(e, e'2p), E=705 MeV; measured nine-fold σ(E, θ), missing momentum spectra; deduced short-range nucleon-nucleon correlations.
doi: 10.1016/S0370-2693(98)00024-0
1998BL07 Phys.Lett. 424B, 33 (1998) K.I.Blomqvist, W.U.Boeglin, R.Bohm, M.Distler, R.Edelhoff, I.Ewald, R.Florizone, J.Friedrich, R.Geiges, J.Jourdan, M.Kahrau, M.Korn, H.Kramer, K.W.Krygier, V.Kunde, M.Kuss, A.Liesenfeld, K.Merle, R.Neuhausen, E.A.J.M.Offermann, Th.Pospischil, M.Potokar, A.W.Richter, A.Rokavec, G.Rosner, P.Sauer, S.Schardt, A.Serdarevic, B.Vodenik, I.Sick, S.Sirca, A.Wagner, Th.Walcher, S.Wolf Large Recoil Momenta in the D(e, e'p)n Reaction NUCLEAR REACTIONS 2H(e, e'p), E=855.11 MeV; measured σ(θ(e), θ(p)) vs missing momentum; deduced possible virtual nucleon excitation role. Model comparisons.
doi: 10.1016/S0370-2693(98)00151-8
1998DE17 Nucl.Phys. A631, 574c (1998) J.P.B.C.de Melo, J.H.O.Sales, T.Frederico, P.U.Sauer Pairs in the Light-Front and Convariance
doi: 10.1016/S0375-9474(98)00070-0
1998DI03 Phys.Rev.Lett. 80, 2294 (1998) M.O.Distler, A.M.Bernstein, K.I.Blomqvist, W.U.Boeglin, R.Bohm, R.Edelhoff, J.Friedrich, R.Geiges, M.Kahrau, M.Korn, H.Kramer, K.W.Krygier, V.Kunde, M.Kuss, A.Liesenfeld, H.Merkel, K.Merle, R.Neuhausen, Th.Pospischil, M.Potokar, A.Rokavec, A.W.Richter, G.Rosner, P.Sauer, St.Schardt, H.Schmieden, S.Sirca, B.Vodenik, A.Wagner, Th.Walcher, St.Wolf Measurement of Separated Structure Functions in the p(e, e'p)π0 Reaction at Threshold and Chiral Perturbation Theory NUCLEAR REACTIONS 1H(e, e'π0), E=435, 555, 855 MeV; measured pion σ(E, θ); deduced structure functions. Comparison with chiral perturbation theory calculations.
doi: 10.1103/PhysRevLett.80.2294
1998NE05 Phys.Rev. C58, 2599 (1998) S.Nemoto, K.Chmielewski, S.Oryu, P.U.Sauer Discrepancy in the Cross Section Minimum of Elastic Nucleon-Deuteron Scattering NUCLEAR REACTIONS 2H(n, n), (p, p), E=2-135 MeV; calculated σ(θ); deduced Δ-isobar excitation contribution. Three-particle scattering equations. Comparison with data.
doi: 10.1103/PhysRevC.58.2599
1998NE07 Few-Body Systems 24, 213 (1998) S.Nemoto, K.Chmielewski, N.W.Schellingerhout, J.Haidenbauer, S.Oryu, P.U.Sauer Nucleon-Deuteron Scattering with Δ-Isobar Excitation, I: Test of separable expansion NUCLEAR REACTIONS 2H(n, X), (p, X), E not given; calculated scattering matrix elements; deduced Δ-isobar role, separable expansion validity. 2H(n, n), E=10, 67 MeV; calculated σ(θ), spin observables. Coupled-channels approach.
doi: 10.1007/s006010050087
1998NE08 Few-Body Systems 24, 241 (1998) S.Nemoto, K.Chmielewski, U.Meyer, J.Haidenbauer, S.Oryu, P.U.Sauer Nucleon-Deuteron Scattering with Δ-Isobar Excitation, II: Elastic scattering NUCLEAR REACTIONS 2H(polarized n, n), (polarized p, p), E=10, 67 MeV; calculated σ(θ), analyzing powers, spin transfer coefficients; deduced Δ-isobar excitation role. Comparison with data.
doi: 10.1007/s006010050088
1997BL13 Nucl.Phys. A626, 871 (1997) K.I.Blomqvist, W.U.Boeglin, R.Bohm, M.Distler, R.Edelhoff, J.Friedrich, R.Geiges, M.Kahrau, S.Kamalov, M.Kirchbach, M.Kohl, M.Korn, H.Kramer, K.W.Krygier, V.Kunde, M.Kuss, J.M.Laget, A.Liesenfeld, K.Merle, R.Neuhausen, E.A.J.M.Offermann, Th.Pospischil, M.Potokar, C.Rangacharyulu, A.Richter, A.W.Richter, A.Rokavec, G.Rosner, P.Sauer, St.Schardt, G.Schrieder, T.Suda, L.Tiator, B.Vodenik, A.Wagner, Th.Walcher, St.Wolf Pion Electroproduction in the 3He(e, e'π+)3H Reaction at Intermediate Energies NUCLEAR REACTIONS 3He(e, e'π+), E=555-855 MeV; measured transverse, longitudinal σ(θ(π)); deduced transverse, longitudinal structure functions. Standard Born amplitudes for elementary pion production, three-body Fadeev wave functions.
doi: 10.1016/S0375-9474(97)00463-6
1997SC03 Phys.Rev. C55, 1051 (1997) Polarization Effects in Pion Electroproduction from 3He NUCLEAR REACTIONS 3He(polarized e, e'X), E=0.88 GeV; calculated transverse-longitudinal asymmetry in pion production energy regime vs energy transfer; deduced polarized 3He as substitute for neutron spin targets related features. Polarized target.
doi: 10.1103/PhysRevC.55.1051
1997SC24 Phys.Rev. C56, 2293 (1997) Polarized Deep-Inelastic Lepton Scattering from the Polarized Two- and Three-Nucleon Bound States NUCLEAR REACTIONS 2H, 3He(polarized e, e'), E not given; calculated structure functions. Polarized targets, front form dynamics. NUCLEAR STRUCTURE 3He, 2H, 1n; calculated spin structure function vs x. Front form dynamics.
doi: 10.1103/PhysRevC.56.2293
1996BL02 Z.Phys. A353, 415 (1996) K.I.Blomqvist, W.U.Boeglin, R.Bohm, M.Distler, D.Drechsel, R.Edelhoff, J.Friedrich, R.Geiges, O.Hanstein, M.Kahrau, M.Korn, H.Kramer, K.W.Krygier, V.Kunde, M.Kuss, A.Liesenfeld, K.Merle, R.Neuhausen, E.A.J.M.Offermann, Th.Pospischil, M.Potokar, A.Rokavec, A.W.Richter, G.Rosner, P.Sauer, S.Schardt, H.Schmieden, S.Sirca, L.Tiator, B.Vodenik, A.Wagner, Th.Walcher, S.Wolf Precise Pion Electroproduction in the p(e, e'π+)n Reaction at W = 1125 MeV NUCLEAR REACTIONS 1H(e, e'π+), E(cm)=1125 MeV; measured missing energy spectra, coincidence, longitudinal σ, asymmetry; deduced longitudinal, transverse structure functions, interference term.
doi: 10.1007/BF01285153
1996BL20 Phys.Rev.Lett. 77, 2396 (1996) K.I.Blomqvist, W.U.Boeglin, R.Bohm, M.Distler, R.Edelhoff, J.Friedrich, R.Geiges, M.Kahrau, M.Korn, H.Kramer, K.W.Krygier, V.Kunde, M.Kuss, J.M.Laget, A.Liesenfeld, K.Merle, R.Neuhausen, E.A.J.M.Offermann, Th.Pospischil, M.Potokar, C.Rangacharyulu, A.Rokavec, A.Richter, A.W.Richter, G.Rosner, P.Sauer, St.Schardt, G.Schrieder, T.Suda, B.Vodenik, A.Wagner, Th.Walcher, St.Wolf Forward-Angle 3He(e, e'π±) Coincident Electroproduction and the Search for Δ's in the Ground State of 3He NUCLEAR REACTIONS 3He(e, e'π+), E=555-855 MeV; measured σ(θ(π)) vs missing mass; deduced preformed Δ++ related features.
doi: 10.1103/PhysRevLett.77.2396
1996BU52 Few-Body Systems 21, 149 (1996) A.J.Buchmann, H.Henning, P.U.Sauer Meson and Quark Degrees of Freedom and the Radius of the Deuteron NUCLEAR STRUCTURE 2H; analyzed longitudinal structure function, charge radius; deduced meson exchange contributions.
doi: 10.1007/s006010050045
1996MI11 Phys.Lett. 379B, 67 (1996) R.G.Milner, C.Bloch, J.F.J.van den Brand, H.J.Bulten, D.DeSchepper, T.W.Donnelly, R.Ent, C.D.Goodman, J.-O.Hansen, W.W.Jacobs, C.E.Jones, W.Korsch, L.H.Kramer, K.Lee, M.Leuschner, W.Lorenzon, N.C.R.Makins, D.Marchlenski, H.O.Meyer, M.A.Miller, J.S.Neal, P.V.Pancella, S.F.Pate, W.K.Pitts, B.von Przewoski, T.Rinckel, P.U.Sauer, G.Savopulos, R.-W.Schulze, A.Smith, J.Sowinski, F.Sperisen, E.R.Sugarbaker, M.A.Titko, C.Tschalar, O.Unal, T.P.Welch, Z.-L.Zhou The Spin Dependent Momentum Distributions of the Neutron and Proton in 3He NUCLEAR REACTIONS 3He(polarized p, 2p), (polarized p, np), E=197 MeV; analyzed data. 3He deduced nucleon momentum distribution spin asymmetries. PWIA model, Faddeev calculation.
doi: 10.1016/0370-2693(96)00450-9
1995BL02 Phys.Lett. 344B, 85 (1995) K.I.Blomqvist, W.U.Boeglin, R.Bohm, M.Distler, R.Edelhoff, J.Friedrich, R.Geiges, M.Kahrau, M.Korn, H.Kramer, K.W.Krygier, V.Kunde, M.Kuss, J.Lac, A.Liesenfeld, K.Merle, R.Neuhausen, E.A.J.M.Offermann, Th.Pospischil, M.Potokar, A.W.Richter, A.Rokavec, G.Rosner, P.Sauer, S.Schardt, A.Serdarevic, Th.Veit, B.Vodenik, A.Wagner, Th.Walcher, S.Wolf High-Momentum Components in the 1p Orbitals of 16O NUCLEAR REACTIONS 16O(e, e'p), E=855 MeV; measured σ(E(e'), θ(e'), Ep, θp). 16O deduced proton momentum distribution. Natural target.
doi: 10.1016/0370-2693(94)01540-S
1995BL10 Z.Phys. A351, 353 (1995) K.I.Blomqvist, W.U.Boeglin, R.Bohm, M.Distler, R.Edelhoff, J.Friedrich, R.Geiges, M.Kahrau, M.Korn, H.Kramer, K.W.Krygier, V.Kunde, M.Kuss, J.Lac, A.Liesenfeld, K.Merle, R.Neuhausen, E.A.J.M.Offermann, Th.Pospischil, M.Potokar, A.W.Richter, A.Rokavec, G.Rosner, P.Sauer, S.Schardt, A.Serdarevic, Th.Veit, B.Vodenik, A.Wagner, Th.Walcher, S.Wolf No Evidence for Medium Effects in the 12C(e, e'p)11B(g.s.) Reaction NUCLEAR REACTIONS 12C(e, e'p), E not given; measured distorted momentum distribution vs missing momentum; deduced spectroscopic factor for transition to 11B(g.s). Parallel, anti-parallel kinenmatics.
doi: 10.1007/BF01291135
1995HA08 Phys.Rev.Lett. 74, 654 (1995) J.-O.Hansen, M.A.Titko, D.DeSchepper, G.Dodson, T.W.Donnelly, K.Dow, R.Endt, M.Farkhondeh, W.Korsch, L.H.Kramer, K.Lee, N.C.R.Makins, R.G.Milner, D.R.Tieger, T.P.Welch, C.E.Jones, J.Arrington, E.J.Beise, B.Bray, R.W.Carr, B.W.Filippone, H.Gao, A.Lung, R.D.McKeown, B.Mueller, M.L.Pitt, R.-W.Schulze, P.U.Sauer, E.Candell, J.Napolitano, C.Tripp, B.B.Wojtsekhowski, W.Lorenzon Transverse-Longitudinal Asymmetry in the Quasielatic 3He(pol)(e(pol), e') Reaction NUCLEAR REACTIONS 3He(polarized e, e'), E=370 MeV; measured transverse-longitudinal asymmetry. Polarized target. Plane wave impulse approximation analysis.
doi: 10.1103/PhysRevLett.74.654
1995HE16 Phys.Rev. C52, R471 (1995) H.Henning, J.Adam, Jr., P.U.Sauer, A.Stadler Relations between Isoscalar Charge Form Factors of Two- and Three-Nucleon Systems NUCLEAR STRUCTURE 2,3H, 3He; calculated isoscalar charge form factors. One-, two-nucleon correlations of relativistic order.
doi: 10.1103/PhysRevC.52.R471
1995ST12 Phys.Rev. C51, 2896 (1995) A.Stadler, J.Adam, Jr., H.Henning, P.U.Sauer Triton Calculations with π and ρ Exchange Three-Nucleon Forces NUCLEAR STRUCTURE 3H; calculated binding energy; deduced πNN cut-off parameter dependence. Momentum space, Faddeev equations, π-, ρ-exchange three-nucleon forces.
doi: 10.1103/PhysRevC.51.2896
1994VA03 Phys.Rev. C49, 1799 (1994) A.Valcarce, F.Fernandez, H.Garcilazo, M.T.Pena, P.U.Sauer Effects of a Quark-Model-Based Nucleon-Δ Potential on the Two-Nucleon System Above Pion Threshold NUCLEAR REACTIONS 1H(p, X), (p, π+), E=300-900 MeV; 2H(π+, π+), E ≤ 300 MeV; analyzed σ(E). 1H(p, π+), (polarized p, π+), E=578, 800 MeV; 2H(π+, π+), E=140, 256 MeV; analyzed σ(θ), polarization data. Nonrelativistic quark model, nucleon-Δ potential.
doi: 10.1103/PhysRevC.49.1799
1994VE08 Z.Phys. A349, 161 (1994) T.Veit, K.I.Blomqvist, W.U.Boeglin, M.Distler, R.Edelhoff, J.Friedrich, R.Geiges, M.Korn, H.Kramer, K.W.Krygier, V.Kunde, A.Liesenfeld, K.Merle, R.Neuhausen, E.A.J.M.Offermann, Th.Pospischil, A.W.Richter, G.Rosner, P.Sauer, S.Schardt, A.Wagner, Th.Walcher, S.Wolf Model-Independent Separation of Structure Functions Over an Extended Kinematical Region NUCLEAR REACTIONS 12C(e, e'p), E ≈ quasifree region; calculated structure functions, separation. Model independent approach.
doi: 10.1007/BF01291175
1993SC18 Phys.Rev. C48, 38 (1993) Inelastic Electron Scattering from the Three-Nucleon Bound States with Polarization NUCLEAR REACTIONS 3He(polarized e, e'X), E not given; calculated structure function. PWIA, polarized target.
doi: 10.1103/PhysRevC.48.38
1992HE04 Nucl.Phys. A537, 367 (1992) Comment on the Trinucleon Electromagnetic Form Factors NUCLEAR REACTIONS 3H, 3H(e, e), E not given; calculated form factors. Paris, Bonn potentials.
doi: 10.1016/0375-9474(92)90361-M
1992PE03 Phys.Rev. C45, 1487 (1992) M.T.Pena, H.Garcilazo, U.Oelfke, P.U.Sauer Effect of the NΔ Interaction on Observables of the πNN and γNN Systems NUCLEAR REACTIONS 1H(polarized p, π), E=578, 800 MeV; calculated analyzing power, iT11, other polarization observables vs θ. 2H(γ, π0), E=300 MeV; calculated σ(θ), asymmetry, polarization observables vs θ; deduced NΔ-interaction role.
doi: 10.1103/PhysRevC.45.1487
1992SA09 Nucl.Phys. A543, 291c (1992) The Three-Nucleon Force and the Δ-Mechanism for Pion Production and Absorption NUCLEAR STRUCTURE 3H; calculated binding energy. Δ-isobar, pion degrees of freedom in force model. NUCLEAR REACTIONS 1H(p, X), E ≈ 0.2-1 GeV; calculated spin-dependent, spin-independent total σ(E). 1H(polarized p, π+), E=578 MeV; calculated σ(θ), analyzing power vs θ, spin correlation parameter vs θ. 1H(polarized p, π+), E=800 MeV; calculated σ(θ), beam asymmetry vs θ. Δ-isobar, pion degrees of freedom in force model.
doi: 10.1016/0375-9474(92)90425-J
1992ST04 Phys.Rev. C46, 64 (1992) Effect of the Three-Nucleon Force on the Three-Nucleon Ground State: Reducible and irreducible contributions NUCLEAR STRUCTURE 3H; calculated binding energy, D-state probability; deduced three-nucleon force role. Tucson-Melbourne two-pion exchange three-nucleon force, reducible, irreducible contributions.
doi: 10.1103/PhysRevC.46.64
1991AD06 Nucl.Phys. A531, 623 (1991) J.Adam, Jr., Ch.Hajduk, H.Henning, P.U.Sauer, E.Truhlik Weak Meson-Exchange Currents and the Tritium β-Decay RADIOACTIVITY 3H(β-); calculated one-, two-baryon contributions to Gamow-Teller matrix element. Phenomenological, chiral-invariant Lagrangian based meson exchange currents.
doi: 10.1016/0375-9474(91)90744-Q
1991MI17 Phys.Rev. C44, R1725 (1991) Total Cross Section for p + p → p + p + π0 Near Threshold NUCLEAR REACTIONS 1H(p, pπ0), E ≈ threshold; calculated pion production σ vs E.
doi: 10.1103/PhysRevC.44.R1725
1991ST10 Phys.Rev. C44, 2319 (1991) A.Stadler, W.Glockle, P.U.Sauer Faddeev Equations with Three-Nucleon Force in Momentum Space NUCLEAR STRUCTURE 3H; calculated binding energy. Faddeev equations, three-nucleon force.
doi: 10.1103/PhysRevC.44.2319
1990OE02 Nucl.Phys. A518, 593 (1990) U.Oelfke, P.U.Sauer, F.Coester Convolution Models of Deep Inelastic Scattering: The three-nucleon bound states as a test case NUCLEAR STRUCTURE 3He, 3H; calculated structure function ratio, p, n, Δ-isobar distribution function. Convolution models.
doi: 10.1016/0375-9474(90)90181-K
1990PE07 Phys.Rev. C42, 855 (1990) M.T.Pena, H.Henning, P.U.Sauer Effect of the Nucleon-Delta Interaction on Properties of the Three-Nucleon Ground State NUCLEAR STRUCTURE 3He; calculated charge monopole, magnetic dipole form factors; deduced nucleon-Δ interaction role.
doi: 10.1103/PhysRevC.42.855
1989ME10 Nucl.Phys. A499, 637 (1989) H.Meier-Hajduk, U.Oelfke, P.U.Sauer Inclusive Electron Scattering from 3He NUCLEAR REACTIONS 3He(e, e'X), E=3.3-14.7 GeV; calculated σ(θ(e'), E(e')), response functions. Plane wave approximation.
doi: 10.1016/0375-9474(89)90056-0
1989ME11 Nucl.Phys. A499, 669 (1989) Effects of Final-State Interaction in Inelastic Electron Scattering from the Three-Nucleon System NUCLEAR REACTIONS 3He(e, e'X), E=0.667, 3.26 GeV; calculated σ(θ(e'), E(e')), response function.
doi: 10.1016/0375-9474(89)90057-2
1989SA18 Nucl.Phys. A497, 441c (1989) Electromagnetic Study of the δ-Resonance NUCLEAR REACTIONS 1H(polarized p, π+), E=578 MeV; analyzed σ(θ), polarization observables data. Force model.
doi: 10.1016/0375-9474(89)90486-7
1987PO17 Nucl.Phys. A474, 557 (1987); Erratum Nucl.Phys. A550, 563 (1992) H.Popping, P.U.Sauer, Zhang Xi-Zheng The Two-Nucleon System above Pion Threshold: A force model with Δ-isobar and pion degrees of freedom NUCLEAR REACTIONS 1H(p, X), (p, p), (p, π+), E=200-1000 MeV; calculated σ(E). Force model, isobar, pion degrees of freedom.
doi: 10.1016/0375-9474(87)90595-1
1987SA08 Nucl.Phys. A463, 273c (1987) Electromagnetic Form Factors of the Three-Nucleon Bound States NUCLEAR STRUCTURE 3H, 3He; compiled electromagnetic form factors; deduced rms radii, μ. Force models.
doi: 10.1016/0375-9474(87)90670-1
1987SA13 Nucl.Phys. A465, 686 (1987) Microscopic Nuclear Structure with Sub-Baryonic Degrees of Freedom: Quarks form a dibaryon NUCLEAR STRUCTURE 3He; calculated charge form factor, binding energy. 3H; calculated binding energy; deduced sub-baryonic degrees of freedom role.
doi: 10.1016/0375-9474(87)90561-6
1987ST09 Nucl.Phys. A465, 651 (1987) W.Strueve, Ch.Hajduk, P.U.Sauer, W.Theis 3He and 3H Electromagnetic Form Factors NUCLEAR STRUCTURE 3H, 3He; calculated electromagnetic form factors, μ, rms radii. Single-Δ isobar admixtures.
doi: 10.1016/0375-9474(87)90560-4
1986OE02 Czech.J.Phys. B36, 926 (1986) Are There Loose Quarks in Nuclei ( Question ) NUCLEAR STRUCTURE 2,3H, 3He; calculated structure function ratio. Realistic Faddeev wave function.
doi: 10.1007/BF01797501
1986SA07 Czech.J.Phys. B36, 278 (1986) Microscopic Nuclear Structure with Subnucleonic Degrees of Freedom NUCLEAR STRUCTURE 3H, 3He; calculated charge, magnetic form factors. Force model. NUCLEAR REACTIONS 1H(p, π+), (polarized p, π+), E=578 MeV; 2H(π, π), E=142-292 MeV; calculated σ(θ), vector, tensor analyzing power vs θ. Force model.
doi: 10.1007/BF01597160
1983HA18 Nucl.Phys. A405, 581 (1983) Ch.Hajduk, P.U.Sauer, W.Strueve Properties of the Three-Nucleon Bound States with Virtual Δ-Isobar Excitation NUCLEAR STRUCTURE 3He; calculated point proton distribution, charge, magnetic form factors. 3H; calculated charge, magnetic form factors. Virtual isobar excitation.
doi: 10.1016/0375-9474(83)90519-5
1983HA19 Nucl.Phys. A405, 605 (1983) Ch.Hajduk, P.U.Sauer, Shin Nan Yang Validity of Approximative Treatments of Δ-Isobar Degrees of Freedom NUCLEAR STRUCTURE 3He; calculated ground state wave function, binding energy, magnetic moment corrections, magnetic form factors. Perturbative approach, isobar degrees of freedom.
doi: 10.1016/0375-9474(83)90520-1
1983ME03 Nucl.Phys. A395, 332 (1983) H.Meier-Hajduk, Ch.Hajduk, P.U.Sauer, W.Theis Quasi-Elastic Electron Scattering from 3He NUCLEAR REACTIONS 3He(e, e'X), E=0.5, 3.26-8.61 GeV; calculated inclusive σ(θ, E(e')). Plane wave impulse approximation.
doi: 10.1016/0375-9474(83)90047-7
1983SA28 Nuovo Cim. 76A, 309 (1983) The Three-Nucleon Bound State with Isobaric and Pionic Degrees of Freedom NUCLEAR STRUCTURE 3He; calculated charge, magnetic form factors, point proton distribution. Isobar, pionic degrees of freedom.
doi: 10.1007/BF02833728
1983ST11 Nucl.Phys. A405, 620 (1983) W.Strueve, Ch.Hajduk, P.U.Sauer Exchange-Current Contributions to the 3He Magnetic Properties NUCLEAR STRUCTURE 3He, 3H; calculated μ, magnetic form factor, rms radii. Paris, Reid soft-core potentials, isobar degrees of freedom, momentum space representation, meson exchange effects.
doi: 10.1016/0375-9474(83)90521-3
1982BA41 Nucl.Phys. A386, 460 (1982) H.Baier, W.Bentz, Ch.Hajduk, P.U.Sauer Δ-Isobar Contributions to the Charge Asymmetry of the Three-Nucleon Bound States NUCLEAR STRUCTURE 3H, 3He; calculated binding energy difference; deduced isobar charge symmetry contribution. One photon exchange.
doi: 10.1016/0375-9474(82)90031-8
1982HA20 Czech.J.Phys. B32, 263 (1982) Ch.Hajduk, P.U.Sauer, W.Strueve The Magnetic Form Factor of 3He NUCLEAR STRUCTURE 3He; calculated magnetic form factor. Meson exchange, isobar admixtures.
doi: 10.1007/BF01602064
1982SA03 Czech.J.Phys. B32, 176 (1982) The Three-Nucleon Bound State with Mesonic and Internal Nucleonic Degrees of Freedom NUCLEAR STRUCTURE 3H, 3He; calculated binding energy, electromagnetic form factors.
doi: 10.1007/BF01608044
1981FU09 Prog.Theor.Phys.(Kyoto) 65, 1461 (1981) Effect of the N*(Roper) and Δ Resonances on the 1S0 Nucleon-Nucleon Scattering Phase Shift NUCLEAR REACTIONS 1H(π, π), E < 600 MeV; 1H(p, p), E < 500 MeV; calculated phase shifts. Isobar, Roper resonances, noncovariant model.
doi: 10.1143/PTP.65.1461
1981HA07 Nucl.Phys. A352, 413 (1981) Ch.Hajduk, P.U.Sauer, H.Arenhovel, D.Drechsel, M.M.Giannini On the Contribution of the Δ -Isobar to the Charge Form Factor of 3He NUCLEAR STRUCTURE 3He; calculated charge form factor. Faddeev equations, Δ-isobar.
doi: 10.1016/0375-9474(81)90420-6
1981HA41 Nucl.Phys. A369, 321 (1981) Reliability of Faddeev Calculations in Momentum Space for the Bound Three-Nucleon System NUCLEAR STRUCTURE 3H, 3He; calculated neutron, proton densities, charge form factors. Faddeev equations, Reid, Paris potentials, momentum space.
doi: 10.1016/0375-9474(81)90023-3
1979HA27 Nucl.Phys. A322, 329 (1979) Effect of the Δ(1236) Isobar on the Three-Nucleon Bound States NUCLEAR STRUCTURE 3H, 3He; calculated bound state properties, Δ-isobar. Faddeev equations.
doi: 10.1016/0375-9474(79)90429-9
Back to query form [Next] Note: The following list of authors and aliases matches the search parameter P.Sauer: , P.U.SAUER |