NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = A.Bernstein Found 110 matches. Showing 1 to 100. [Next]2023BE19 Phys.Rev. C 108, 045503 (2023) E.P.Bernard, E.Mizrachi, J.Kingston, J.Xu, S.V.Pereverzev, T.Pershing, R.Smith, C.G.Prior, N.S.Bowden, A.Bernstein, C.R.Hall, E.Pantic, M.Tripathi, D.N.McKinsey, P.S.Barbeau Thermodynamic stability of xenon-doped liquid argon detectors
doi: 10.1103/PhysRevC.108.045503
2022HO01 J.Phys.(London) G49, 010502 (2022) C.R.Howell, M.W.Ahmed, A.Afanasev, D.Alesini, J.R.M.Annand, A.Aprahamian, D.L.Balabanski, S.V.Benson, A.Bernstein, C.R.Brune, J.Byrd, B.E.Carlsten, A.E.Champagne, S.Chattopadhyay, D.Davis, E.J.Downie, J.M.Durham, G.Feldman, H.Gao, C.G.R.Geddes, H.W.Griesshammer, R.Hajima, H.Hao, D.Hornidge, J.Isaak, R.V.F.Janssens, D.P.Kendellen, M.Kovash, P.P.Martel, U.-G.Meissner, R.Miskimen, B.Pasquini, D.R.Phillips, N.Pietralla, D.Savran, M.R.Schindler, M.H.Sikora, W.M.Snow, R.P.Springer, C.Sun, C.Tang, B.Tiburzi, A.P.Tonchev, W.Tornow, C.A.Ur, D.Wang, H.R.Weller, V.Werner, Y.K.Wu, J.Yan, Z.Zhao, A.Zilges, F.Z.Zomer International workshop on next generation gamma-ray source
doi: 10.1088/1361-6471/ac2827
2021AK04 Phys.Rev. C 104, 065501 (2021) D.S.Akerib, A.K.Al Musalhi, S.K.Alsum, C.S.Amarasinghe, A.Ames, T.J.Anderson, N.Angelides, H.M.Araujo, J.E.Armstrong, M.Arthurs, X.Bai, J.Balajthy, S.Balashov, J.Bang, J.W.Bargemann, D.Bauer, A.Baxter, P.Beltrame, E.P.Bernard, A.Bernstein, A.Bhatti, A.Biekert, T.P.Biesiadzinski, H.J.Birch, G.M.Blockinger, E.Bodnia, B.Boxer, C.A.J.Brew, P.Bras, S.Burdin, J.K.Busenitz, M.Buuck, R.Cabrita, M.C.Carmona-Benitez, M.Cascella, C.Chan, N.I.Chott, A.Cole, M.V.Converse, A.Cottle, G.Cox, O.Creaner, J.E.Cutter, C.E.Dahl, L.de Viveiros, J.E.Y.Dobson, E.Druszkiewicz, S.R.Eriksen, A.Fan, S.Fayer, N.M.Fearon, S.Fiorucci, H.Flaecher, E.D.Fraser, T.Fruth, R.J.Gaitskell, J.Genovesi, C.Ghag, E.Gibson, S.Gokhale, M.G.D.van der Grinten, C.B.Gwilliam, C.R.Hall, S.J.Haselschwardt, S.A.Hertel, M.Horn, D.Q.Huang, M.C.I.gnarra, O.Jahangir, R.S.James, W.Ji, J.Johnson, A.C.Kaboth, A.C.Kamaha, K.Kamdin, K.Kazkaz, D.Khaitan, A.Khazov, I.Khurana, D.Kodroff, L.Korley, E.V.Korolkova, H.Kraus, S.Kravitz, L.Kreczko, B.Krikler, V.A.Kudryavtsev, E.A.Leason, J.Lee, D.S.Leonard, K.T.Lesko, C.Levy, J.Liao, J.Lin, A.Lindote, R.Linehan, W.H.Lippincott, X.Liu, M.I.Lopes, E.Lopez Asamar, B.Lopez Paredes, W.Lorenzon, S.Luitz, P.A.Majewski, A.Manalaysay, L.Manenti, R.L.Mannino, N.Marangou, M.E.McCarthy, D.N.McKinsey, J.McLaughlin, E.H.Miller, E.Mizrachi, A.Monte, M.E.Monzani, J.A.Morad, J.D.Morales Mendoza, E.Morrison, B.J.Mount, A.St.J.Murphy, D.Naim, A.Naylor, C.Nedlik, H.N.Nelson, F.Neves, J.A.Nikoleyczik, A.Nilima, I.Olcina, K.C.Oliver-Mallory, S.Pal, K.J.Palladino, J.Palmer, S.Patton, N.Parveen, E.K.Pease, B.Penning, G.Pereira, A.Piepke, Y.Qie, J.Reichenbacher, C.A.Rhyne, A.Richards, Q.Riffard, G.R.C.Rischbieter, R.Rosero, P.Rossiter, D.Santone, A.B.M.R.Sazzad, R.W.Schnee, P.R.Scovell, S.Shaw, T.A.Shutt, J.J.Silk, C.Silva, R.Smith, M.Solmaz, V.N.Solovov, P.Sorensen, J.Soria, I.Stancu, A.Stevens, K.Stifter, B.Suerfu, T.J.Sumner, N.Swanson, M.Szydagis, W.C.Taylor, R.Taylor, D.J.Temples, P.A.Terman, D.R.Tiedt, M.Timalsina, W.H.To, D.R.Tovey, M.Tripathi, D.R.Tronstad, W.Turner, U.Utku, A.Vaitkus, B.Wang, J.J.Wang, W.Wang, J.R.Watson, R.C.Webb, R.G.White, T.J.Whitis, M.Williams, F.L.H.Wolfs, D.Woodward, C.J.Wright, X.Xiang, J.Xu, M.Yeh, P.Zarzhitsky Projected sensitivity of the LUX-ZEPLIN experiment to the two-neutrino and neutrinoless double β decays of 134Xe RADIOACTIVITY 134Xe(2β-); measured recoiling nuclei and electrons, decay energy spectra using LUX-ZEPLIN (LZ) detector of liquid xenon (LXe), with scintillation and electro-luminescence light detected using 494 photomultipliers at Sanford Underground Research Facility (SURF) in South Dakota; deduced lower limits of T1/2 values for 2νββ and 0νββ decay modes.
doi: 10.1103/PhysRevC.104.065501
2020BE06 Rev.Mod.Phys. 92, 011003 (2020) A.Bernstein, N.Bowden, B.L.Goldblum, P.Huber, I.Jovanovic, J.Mattingly Colloquium: Neutrino detectors as tools for nuclear security NUCLEAR REACTIONS 235,238U, 239,241Pu(n, F), E thermal; analyzed available data on fission fragments, Iβ, Eβ; deduced antineutrino fluxes.
doi: 10.1103/RevModPhys.92.011003
2020SU19 Phys.Rev. C 102, 034616 (2020) F.Sutanto, O.A.Akindele, M.Askins, M.Bergevin, A.Bernstein, N.S.Bowden, S.Dazeley, P.Jaffke, I.Jovanovic, S.Quillin, C.Roecker, S.D.Rountree Measurement of muon-induced high-energy neutrons from rock in an underground Gd-doped water detector
doi: 10.1103/PhysRevC.102.034616
2016LA10 Phys.Rev. C 93, 045808 (2016) D.Lattuada, M.Barbarino, A.Bonasera, W.Bang, H.J.Quevedo, M.Warren, F.Consoli, R.De Angelis, P.Andreoli, S.Kimura, G.Dyer, A.C.Bernstein, K.Hagel, M.Barbui, K.Schmidt, E.Gaul, M.E.Donovan, J.B.Natowitz, T.Ditmire Model-independent determination of the astrophysical S factor in laser-induced fusion plasmas NUCLEAR REACTIONS 2H(d, n)3He, 3He(d, p)4He, E(cm)=5-500 keV; measured deuterium ion energy density distribution from time-of-flight, neutron yields from d+d fusion, angular distribution of neutrons, yield of 14.7-MeV protons using various scintillation detectors; deduced model-independent astrophysical factor S(E). Laser-induced fusion plasmas using Texas Petawatt Laser (TPW). Comparison with previous experimental data. Relevance to primordial abundances in Big Bang nucleosynthesis (BBN) models, and plasma physics.
doi: 10.1103/PhysRevC.93.045808
2013BA43 Phys.Rev.Lett. 111, 082502 (2013) M.Barbui, W.Bang, A.Bonasera, K.Hagel, K.Schmidt, J.B.Natowitz, R.Burch, G.Giuliani, M.Barbarino, H.Zheng, G.Dyer, H.J.Quevedo, E.Gaul, A.C.Bernstein, M.Donovan, S.Kimura, M.Mazzocco, F.Consoli, R.De Angelis, P.Andreoli, T.Ditmire Measurement of the Plasma Astrophysical S Factor for the 3He(d, p)4He Reaction in Exploding Molecular Clusters NUCLEAR REACTIONS 3He(d, p), E(cm)<300 keV; measured reaction products, TOF, Ep, Ip; deduced S-factors, σ, first measurement in the keV energy range. Comparison with available data.
doi: 10.1103/PhysRevLett.111.082502
2013SP05 Eur.Phys.J. A 49, 136 (2013) N.Sparveris, S.Stave, P.Achenbach, C.Ayerbe Gayoso, D.Baumann, J.Bernauer, A.M.Bernstein, R.Bohm, D.Bosnar, T.Botto, A.Christopoulou, D.Dale, M.Ding, M.O.Distler, L.Doria, J.Friedrich, A.Karabarbounis, M.Makek, H.Merkel, U.Muller, I.Nakagawa, R.Neuhausen, L.Nungesser, C.N.Papanicolas, A.Piegsa, J.Pochodzalla, M.Potokar, M.Seimetz, S.Sirca, S.Stiliaris, Th.Walcher, M.Weis Measurements of the γ*p → Δ reaction at low Q2 NUCLEAR REACTIONS 1H(polarized e, e'p)π0, E(cm)=1205-1240 MeV; measured Ep, Ip(θ); deduced three unpolarized σ. Compared with published calculations.
doi: 10.1140/epja/i2013-13136-2
2011BO21 Phys.Rev. C 84, 035206 (2011) P.Bourgeois, Y.Sato, J.Shaw, R.Alarcon, A.M.Bernstein, W.Bertozzi, T.Botto, J.Calarco, F.Casagrande, M.O.Distler, K.Dow, M.Farkondeh, S.Georgakopoulos, S.Gilad, R.Hicks, M.Holtrop, A.Hotta, X.Jiang, A.Karabarbounis, J.Kirkpatrick, S.Kowalski, R.Milner, R.Miskimen, I.Nakagawa, C.N.Papanicolas, A.J.Sarty, S.Sirca, E.Six, N.F.Sparveris, S.Stave, E.Stiliaris, T.Tamae, G.Tsentalovich, C.Tschalaer, W.Turchinetz, Z.-L.Zhou, T.Zwart Measurements of the generalized electric and magnetic polarizabilities of the proton at low Q2 using the virtual Compton scattering reaction
doi: 10.1103/PhysRevC.84.035206
2011KI19 Phys.Rev. C 84, 028201 (2011) J.M.Kirkpatrick, N.F.Sparveris, I.Nakagawa, A.M.Bernstein, R.Alarcon, W.Bertozzi, T.Botto, P.Bourgeois, J.Calarco, F.Casagrande, M.O.Distler, K.Dow, M.Farkhondeh, S.Georgakopoulos, S.Gilad, R.Hicks, A.Holtrop, A.Hotta, X.Jiang, A.Karabarbounis, S.Kowalski, R.Milner, R.Miskimen, C.N.Papanicolas, A.J.Sarty, Y.Sato, S.Sirca, J.Shaw, E.Six, S.Stave, E.Stiliaris, T.Tamae, G.Tsentalovich, C.Tschalaer, W.Turchinetz, Z.-L.Zhou, T.Zwart Measurement of the partial cross sections σTT , σLT, and (σT + ϵσL) of the 1H(e, e'π+)n reaction in the Δ(1232) resonance NUCLEAR REACTIONS 1H(e, e'π+) at Q2=0.127 GeV/c2; measured electron spectra using OHIPS spectrometer at MIT-Bates facility; deduced differential cross sections for Δ(1232) resonance. Comparison with predictions of MAID, DMT, Sato-Lee, and chiral EFT models.
doi: 10.1103/PhysRevC.84.028201
2009FE07 Phys.Rev. C 80, 065201 (2009) C.Fernandez-Ramirez, A.M.Bernstein, T.W.Donnelly Unexpected impact of D waves in low-energy neutral pion photoproduction from the proton and the extraction of multipoles NUCLEAR REACTIONS 1H(γ, π), E=145-167 MeV; calculated differential σ, σ(θ) using heavy baryon chiral perturbation theory (HBCHPT). Comparison with experimental data.
doi: 10.1103/PhysRevC.80.065201
2009WA04 Phys.Rev.Lett. 102, 122501 (2009) X.Wang, R.V.F.Janssens, M.P.Carpenter, S.Zhu, I.Wiedenhover, U.Garg, S.Frauendorf, T.Nakatsukasa, I.Ahmad, A.Bernstein, E.Diffenderfer, S.J.Freeman, J.P.Greene, T.L.Khoo, F.G.Kondev, A.Larabee, T.Lauritsen, C.J.Lister, B.Meredith, D.Seweryniak, C.Teal, P.Wilson Structure of 240Pu: Evidence for Octupole Phonon Condensation? NUCLEAR REACTIONS 240Pu(208Pb, 208Pb'), E=1300 MeV; measured Eγ, Iγ, γγ-coin. 240Pu; deduced levels, J, π.
doi: 10.1103/PhysRevLett.102.122501
2008SP05 Phys.Rev. C 78, 018201 (2008) N.F.Sparveris, P.Achenbach, C.Ayerbe Gayoso, D.Baumann, J.Bernauer, A.M.Bernstein, R.Bohm, D.Bosnar, T.Botto, A.Christopoulou, D.Dale, M.Ding, M.O.Distler, L.Doria, J.Friedrich, A.Karabarbounis, M.Makek, H.Merkel, U.Muller, I.Nakagawa, R.Neuhausen, L.Nungesser, C.N.Papanicolas, B.Pasquini, A.Piegsa, J.Pochodzalla, M.Potokar, M.Seimetz, S.Sirca, S.Stave, S.Stiliaris, Th.Walcher, M.Weis Virtual Compton scattering measurements in the γ* N → Δ transition NUCLEAR REACTIONS 1H(e, e'p), E=855 MeV; measured virtual Compton scattering σ, missing mass spectra; deduced magnetic dipole amplitude.
doi: 10.1103/PhysRevC.78.018201
2008ST16 Phys.Rev. C 78, 025209 (2008) S.Stave, N.Sparveris, M.O.Distler, I.Nakagawa, P.Achenbach, C.Ayerbe Gayoso, D.Baumann, J.Bernauer, A.M.Bernstein, R.Bohm, D.Bosnar, T.Botto, A.Christopoulou, D.Dale, M.Ding, L.Doria, J.Friedrich, A.Karabarbounis, M.Makek, H.Merkel, U.Muller, R.Neuhausen, L.Nungesser, C.N.Papanicolas, A.Piegsa, J.Pochodzalla, M.Potokar, M.Seimetz, S.Sirca, S.Stiliaris, Th.Walcher, M.Weis, for the A1 Collaboration Measurements of the γ*p → Δ reaction at low Q2: Probing the mesonic contribution NUCLEAR REACTIONS p(polarized e, e'p)π, E=705, 795, 855 MeV; measured σ, σ(θ).Comparison with model calculations.
doi: 10.1103/PhysRevC.78.025209
2008WE11 Eur.Phys.J. A 38, 27 (2008) M.Weis, P.Bartsch, D.Baumann, J.Bermuth, A.M.Bernstein, K.Bohinc, R.Bohm, M.Ding, M.O.Distler, I.Ewald, J.M.Friedrich, J.Friedrich, M.Kahrau, M.Kohl, K.W.Krygier, A.Liesenfeld, H.Merkel, P.Merle, U.Muller, R.Neuhausen, M.M.Pavan, Th.Pospischil, M.Potokar, G.Rosner, H.Schmieden, M.Seimetz, S.Sirca, A.Wagner, Th.Walcher, for The A1 Collaboration Separated cross-sections in π0 electroproduction at threshold at Q2 = 0.05 GeV2/c2 NUCLEAR REACTIONS 1H(e, e'p), E=854.49 MeV; measured neutral pion production σ(θ), missing mass spectra. 1H(polarized e, e'p), E=854.49 MeV; measured beam helicity asymmetry. Comparison with model calculations.
doi: 10.1140/epja/i2008-10644-6
2007SP06 Phys.Lett. B 651, 102 (2007) N.F.Sparveris, P.Achenbach, C.Ayerbe Gayoso, D.Baumann, J.Bernauer, A.M.Bernstein, R.Bohm, D.Bosnar, T.Botto, A.Christopoulou, D.Dale, M.Ding, M.O.Distler, L.Doria, J.Friedrich, A.Karabarbounis, M.Makek, H.Merkel, U.Muller, I.Nakagawa, R.Neuhausen, L.Nungesser, C.N.Papanicolas, A.Piegsa, J.Pochodzalla, M.Potokar, M.Seimetz, S.Sirca, S.Stave, S.Stiliaris, Th.Walcher, M.Weis Determination of quadrupole strengths in the γ*p → Δ(1232) transition at Q2 = 0.20 (GeV/c)2
doi: 10.1016/j.physletb.2007.04.056
2006BO29 Phys.Rev.Lett. 97, 212001 (2006) P.Bourgeois, Y.Sato, J.Shaw, R.Alarcon, A.M.Bernstein, W.Bertozzi, T.Botto, J.Calarco, F.Casagrande, M.O.Distler, K.Dow, M.Farkhondeh, S.Georgakopoulos, S.Gilad, R.Hicks, M.Holtrop, A.Hotta, X.Jiang, A.Karabarbounis, J.Kirkpatrick, S.Kowalski, R.Milner, R.Miskimen, I.Nakagawa, C.N.Papanicolas, A.J.Sarty, S.Sirca, E.Six, N.F.Sparveris, S.Stave, E.Stiliaris, T.Tamae, G.Tsentalovich, C.Tschalaer, W.Turchinetz, Z.-L.Zhou, T.Zwart Measurements of the Generalized Electric and Magnetic Polarizabilities of the Proton at Low Q2 Using the Virtual-Compton-Scattering Reaction NUCLEAR REACTIONS 1H(e, e'), E=570-670 MeV; measured σ(E, θ), response functions. 1H deduced polarizability radii. Virtual Compton scattering.
doi: 10.1103/PhysRevLett.97.212001
2005SP01 Phys.Rev.Lett. 94, 022003 (2005) N.F.Sparveris, R.Alarcon, A.M.Bernstein, W.Bertozzi, T.Botto, P.Bourgeois, J.Calarco, F.Casagrande, M.O.Distler, K.Dow, M.Farkhondeh, S.Georgakopoulos, S.Gilad, R.Hicks, M.Holtrop, A.Hotta, X.Jiang, A.Karabarbounis, J.Kirkpatrick, S.Kowalski, R.Milner, R.Miskimen, I.Nakagawa, C.N.Papanicolas, A.J.Sarty, Y.Sato, S.Sirca, J.Shaw, E.Six, S.Stave, E.Stiliaris, T.Tamae, G.Tsentalovich, C.Tschalaer, W.Turchinetz, Z.-L.Zhou, T.Zwart Investigation of the Conjectured Nucleon Deformation at Low Momentum Transfer NUCLEAR REACTIONS 1H(e, e'π0), E=950 MeV; measured Ep, σ(θ). 1H deduced quadrupole to dipole amplitude ratios.
doi: 10.1103/PhysRevLett.94.022003
2003BE44 Eur.Phys.J. A 17, 349 (2003) Deviation of the nucleon shape form spherical symmetry: Experimental status NUCLEAR REACTIONS 1H(e, e'X), E=high; analyzed σ, asymmetry. 1H deduced deformation.
doi: 10.1140/epja/i2002-10176-7
2003SP01 Phys.Rev. C 67, 058201 (2003) N.F.Sparveris, R.Alarcon, D.Barkhuff, A.Bernstein, W.Bertozzi, J.Calarco, F.Casagrande, J.Chen, J.Comfort, M.O.Distler, G.Dodson, S.Dolfini, A.Dooley, K.Dow, M.Farkhondeh, S.Gilad, R.Hicks, M.Holtrop, A.Hotta, X.Jiang, N.Kaloskamis, A.Karabarbounis, S.Kowalski, C.Kunz, D.Margaziotis, C.Mertz, R.Milner, R.Miskimen, I.Nakagawa, C.N.Papanicolas, M.M.Pavan, G.Peterson, A.Ramirez, D.Rowntree, A.J.Sarty, J.Shaw, E.Six, S.Soong, E.Stiliaris, D.Tieger, C.Tschalaer, W.Turchinetz, C.Vellidis, G.A.Warren, A.Young, J.Zhao, Z.-L.Zhou, T.Zwart Measurement of the RLT response function for π0 electroproduction at Q2=0.070 (GeV/c)2 in the N → Δ transition NUCLEAR REACTIONS 1H(e, e'π0), E=0.82 GeV; measured response functions. Out-of-plane detection technique.
doi: 10.1103/PhysRevC.67.058201
2001EW01 Phys.Lett. 499B, 238 (2001) I.Ewald, P.Bartsch, D.Baumann, J.Bermuth, A.M.Bernstein, K.Bohinc, R.Bohm, N.Clawiter, S.Derber, M.Ding, M.O.Distler, J.Friedrich, J.M.Friedrich, M.Kahrau, M.Kohl, A.Kozlov, K.W.Krygier, A.Liesenfeld, H.Merkel, P.Merle, U.Muller, R.Neuhausen, M.Pavan, Th.Pospischil, M.Potokar, D.Rohe, G.Rosner, H.Schmieden, S.Sirca, A.Wagner, Th.Walcher, M.Weis Coherent π0 Threshold Production from the Deuteron at Q2 = 0.1 GeV2/c2 NUCLEAR REACTIONS 2H(e, e'π0), E=345, 435, 720 MeV; measured missing mass distributions, σ(θ), σ; deduced partial wave contributions. Comparison with Chiral Perturbation theory.
doi: 10.1016/S0370-2693(00)01396-4
2001ME08 Phys.Rev.Lett. 86, 2963 (2001) C.Mertz, C.E.Vellidis, R.Alarcon, D.H.Barkhuff, A.M.Bernstein, W.Bertozzi, V.Burkert, J.Chen, J.R.Comfort, G.Dodson, S.Dolfini, K.Dow, M.Farkhondeh, J.M.Finn, S.Gilad, R.W.Gothe, X.Jiang, K.Joo, N.I.Kaloskamis, A.Karabarbounis, J.J.Kelly, S.Kowalski, C.Kunz, R.W.Lourie, J.I.McIntyre, B.D.Milbrath, R.Miskimen, J.H.Mitchell, C.N.Papanicolas, C.F.Perdrisat, A.J.Sarty, J.Shaw, S.-B.Soong, D.Tieger, C.Tschalaer, W.Turchinetz, P.E.Ulmer, S.Van Verst, G.A.Warren, L.B.Weinstein, S.Williamson, R.J.Woo, A.Young Search for Quadrupole Strength in the Electroexcitation of the Δ+(1232) NUCLEAR REACTIONS 1H(e, e'π0), E=719, 799 MeV; measured recoil protons σ(φ), longitudinal-transverse asymmetry and response; deduced quadrupole strength in Δ resonance excitation.
doi: 10.1103/PhysRevLett.86.2963
2001SC51 Phys.Rev.Lett. 87, 232501 (2001) A.Schmidt, P.Achenbach, J.Ahrens, H.J.Arends, R.Beck, A.M.Bernstein, V.Hejny, M.Kotulla, B.Krusche, V.Kuhr, R.Leukel, I.J.D.McGregor, J.C.McGeorge, V.Metag, V.M.Olmos de Leon, F.Rambo, U.Siodlaczek, H.Stroher, Th.Walcher, J.Weiss, F.Wissmann, M.Wolf Test of Low-Energy Theorems for 1H(γ(pol), π0)1H in the Threshold Region NUCLEAR REACTIONS 1H(polarized γ, π0), E=144-168 MeV; measured σ, σ(θ), photon asymmetry; deduced partial wave amplitudes. Tagged-photon beam.
doi: 10.1103/PhysRevLett.87.232501
1999DO30 Phys.Rev. C60, 064622 (1999) S.M.Dolfini, R.O.Alarcon, H.Arenhovel, R.Beck, A.M.Bernstein, W.Bertozzi, W.Boeglin, S.Boffi, J.R.Comfort, D.Dale, G.Dodson, K.Dow, M.B.Epstein, M.Farkhondeh, S.Gilad, J.Gorgen, M.Holtrop, D.Jordan, W.Kim, S.Kowalski, R.Laszewski, J.Mandeville, D.J.Margaziotis, D.Martinez, T.McIlvain, R.Miskimen, C.Papanicolas, M.Radici, D.Tieger, W.Turchinetz, C.E.Vellidis, L.Weinstein, S.Williamson Out-of-Plane Measurements of the Fifth Response Function of the Exclusive Electronuclear Response NUCLEAR REACTIONS 2H, 12C(polarized e, e'p), E=560 MeV; measured coincidence yields, σ(θ), beam asymmetry; deduced unpolarized σ, fifth response function f'(LT). Magnetic spectrometers, out-of-plane measurements. DWIA calculations.
doi: 10.1103/PhysRevC.60.064622
1999ME27 Nucl.Phys. (Supplement) A654, 527c (1999) C.Mertz, A.M.Bernstein, M.O.Distler, N.I.Kaloskamis, R.W.Lourie, C.N.Papanicolas, C.E.Vellidis, G.A.Warren, and the OOPS and FPP Collaborations Recent Measurements of γ*N → Δ Response Functions at Bates NUCLEAR REACTIONS 1H(polarized e, e'π+), (polarized e, e'π0), E not given; measured σ(θ), asymmetry.
doi: 10.1016/S0375-9474(00)88493-6
1998BE78 Phys.Lett. 442B, 20 (1998) Light Quark Mass Difference and Isospin Breaking in Electromagnetic Pion Production NUCLEAR REACTIONS 1H(γ, π0), E=145-170 MeV; calculated matrix elements; deduced unitary cusp, dynamical isospin breaking effect. Comparison with data. Chiral perturbation theory.
doi: 10.1016/S0370-2693(98)01257-X
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
1997BE08 Phys.Rev. C55, 1509 (1997) A.M.Bernstein, E.Shuster, R.Beck, M.Fuchs, B.Krusche, H.Merkel, H.Stroher Observation of a Unitary Cusp in the Threshold γp → π0p Reaction NUCLEAR REACTIONS 1H(γ, π0), E=threshold-270 MeV; analyzed σ(E), σ(θ); deduced s-, p-wave multipoles, unitary cusp. Tagged photon beam. Minimal model assumptions.
doi: 10.1103/PhysRevC.55.1509
1997BE47 Nucl.Phys. A623, 178c (1997) Measurements of Pion Properties and Production Amplitudes: Probing confinement scale QCD NUCLEAR REACTIONS 1H(γ, π0), E=155.85 MeV; compiled, reviewed σ(θ), other data, real, virtual photons; deduced confinement scale QCD related features.
doi: 10.1016/S0375-9474(97)00437-5
1996FU04 Phys.Lett. 368B, 20 (1996) M.Fuchs, J.Ahrens, G.Anton, R.Averbeck, R.Beck, A.M.Bernstein, A.R.Gabler, F.Harter, P.D.Harty, S.Hlavac, B.Krusche, I.J.D.MacGregor, V.Metag, R.Novotny, R.O.Owens, J.Peise, M.Robig-Landau, A.Schubert, R.S.Simon, H.Stroher, V.Tries Neutral Pion Photoproduction from the Proton Near Threshold NUCLEAR REACTIONS 1H(γ, π0), E=140-270 MeV; measured σ(θ), σ(E); deduced s-, p-wave multipoles vs E. Tagged photon beam. Low energy theorem, chiral perturbation theory analyses.
doi: 10.1016/0370-2693(95)01488-8
1995DO14 Phys.Rev. C51, 3479 (1995) S.Dolfini, R.Alarcon, H.Arenhovel, R.Beck, A.Bernstein, W.Bertozzi, W.Boeglin, L.Cardman, J.Comfort, D.Dale, G.Dodson, K.Dow, M.Epstein, M.Farkhondeh, S.Gilad, J.Gorgen, M.Holtrop, D.Jordan, W.Kim, S.Kowalski, R.Laszewski, J.Mandeville, D.Margaziotis, D.Martinez, T.McIlvain, R.Miskimen, C.Papanicolas, D.Tieger, W.Turchinetz, L.Weinstein, S.Williamson Out-of-Plane Quasielastic Scattering from Deuterium using Polarized Electrons NUCLEAR REACTIONS 2H(polarized e, e'p), E=560 MeV; measured helicity independent coincidence σ(E, θ(e)) vs missing momentum, electron helicity asymmetry, A(e); deduced imaginary part of the longitudinal-transverse interference structure function f'(LT).
doi: 10.1103/PhysRevC.51.3479
1994MA26 Phys.Rev.Lett. 72, 3325 (1994) J.Mandeville, R.Alarcon, R.Beck, A.Bernstein, W.Bertozzi, W.Boeglin, S.Boffi, L.Cardman, J.Comfort, D.Dale, G.Dodson, S.Dolfini, K.Dow, M.Epstein, S.Gilad, J.Gorgen, M.Holtrop, D.Jordan, W.Kim, S.Kowalski, R.Laszewski, D.Margaziotis, D.Martinez, T.McIlvain, R.Miskimen, C.Papanicolas, M.Radici, D.Tieger, W.Turchinetz, L.Weinstein, S.Williamson First Measurement of the Imaginary Part of the Transverse-Longitudinal Nuclear Response NUCLEAR REACTIONS 12C(polarized e, e'p), E=560 MeV; measured asymmetry, differential σ, fifth structure function; deduced direct knockout, rescattering amplitudes interference.
doi: 10.1103/PhysRevLett.72.3325
1993BE06 Phys.Rev. C47, 1274 (1993) A.M.Bernstein, S.Nozawa, M.A.Moinester Quadrupole Amplitude in the γN → Δ Δ → γN Transition NUCLEAR REACTIONS 1H(γ, π+), (γ, π0), E=340 MeV; calculated σ(θ), double polarization observables; deduced E2/M1 ratio extraction constraints.
doi: 10.1103/PhysRevC.47.1274
1992CH02 Phys.Rev. C45, 915 (1992) T.E.Chupp, R.A.Loveman, A.K.Thompson, A.M.Bernstein, D.R.Tieger Tests of a High Density Polarized 3He Target for Electron Scattering
doi: 10.1103/PhysRevC.45.915
1992TH03 Phys.Rev.Lett. 68, 2901 (1992); Erratum Phys.Rev.Lett. 69, 391 (1992) A.K.Thompson, A.M.Bernstein, T.E.Chupp, D.J.De Angelis, G.E.Dodge, G.Dodson, K.A.Dow, M.Farkhondeh, W.Fong, J.Y.Kim, R.A.Loveman, J.M.Richardson, H.Schmieden, D.R.Tieger, T.C.Yates, M.E.Wagshul, J.D.Zumbro Quasielastic Scattering of Polarized Electrons from Polarized 3He and Measurement of the Neutron's Form Factors NUCLEAR REACTIONS 3He(polarized e, e'), E=578 MeV; measured quasielastic scattering asymmetry; deduced 1n electric form factor implications. Polarized target.
doi: 10.1103/PhysRevLett.68.2901
1991BE14 Phys.Rev. C43, 2742 (1991) C.Bennhold, L.Tiator, A.M.Bernstein, S.S.Kamalov 0+ - 0+ Transition in Charged Photopion Reactions NUCLEAR REACTIONS 14C(γ, π-), E=200 MeV; calculated σ(θ); deduced non-spin-flip term role in 0+ → 0+ transition.
doi: 10.1103/PhysRevC.43.2742
1990FR14 Phys.Rev. C42, 2310 (1990) J.L.Friar, B.F.Gibson, G.L.Payne, A.M.Bernstein, T.E.Chupp Neutron Polarization in Polarized 3He Targets NUCLEAR STRUCTURE 3He; calculated neutron, proton density matrix parameter; deduced neutron polarization to be 87% of 3He target polarization.
doi: 10.1103/PhysRevC.42.2310
1990GH01 Phys.Rev. C41, 653 (1990) L.Ghedira, D.Myers, B.H.Cottman, K.Sankhavaram, M.D.Seneviratne, P.Stoler, E.J.Winhold, M.Yamazaki, P.F.Yergin, J.H.J.Distelbrink, K.Rohrich, Ch.Schmitt, V.H.Walther, A.M.Bernstein, K.I.Blomqvist, J.A.Nelson 14N(γ, π+)14C(g.s.) at Photon Energies of 230, 260, and 320 MeV NUCLEAR REACTIONS 14N(γ, π+), E=230, 260 MeV; measured σ(θ); deduced Δ effects. Delta-hole model analysis.
doi: 10.1103/PhysRevC.41.653
1990VO01 Phys.Rev. C41, 1084 (1990) K.F.von Reden, C.Alcorn, S.A.Dytman, B.Lowry, B.P.Quinn, D.H.Beck, A.M.Bernstein, K.I.Blomqvist, G.Dodson, K.A.Dow, J.Flanz, G.Retzlaff, C.P.Sargent, W.Turchinetz, M.Farkhondeh, J.S.McCarthy, T.S.Ueng, R.R.Whitney Quasielastic Electron Scattering and Coulomb Sum Rule in 4He NUCLEAR REACTIONS 4He(e, e'), E=365-725 MeV; measured σ(θ, E(e')); deduced longitudinal, transverse response functions. 4He deduced Coulomb sum rule.
doi: 10.1103/PhysRevC.41.1084
1988DO13 Phys.Rev.Lett. 61, 1706 (1988) K.Dow, S.Dytman, D.Beck, A.Bernstein, I.Blomqvist, H.Caplan, D.Day, M.Deady, P.Demos, W.Dodge, G.Dodson, M.Farkhondeh, J.Flanz, K.Giovanetti, R.Goloskie, E.Hallin, E.Knill, S.Kowalski, J.Lightbody, R.Lindgren, X.Maruyama, J.McCarthy, B.Quinn, G.Retzlaff, W.Sapp, C.Sargent, D.Skopik, I.The, D.Tieger, W.Turchinetz, T.Ueng, N.Videla, K.von Reden, R.Whitney, C.Williamson Longitudinal Response Functions and Sum Rules for Quasielastic Electron Scattering from 3H and 3He NUCLEAR REACTIONS 3H, 3He(e, e'X), E not given; measured longitudinal response function; deduced sum rules.
doi: 10.1103/PhysRevLett.61.1706
1988DY01 Phys.Rev. C38, 800 (1988) S.A.Dytman, A.M.Bernstein, K.I.Blomqvist, T.J.Pavel, B.P.Quinn, R.Altemus, J.S.McCarthy, G.H.Mechtel, T.S.Ueng, R.R.Whitney Inclusive Electron Scattering from 2H, 3He, and 4He NUCLEAR REACTIONS 3,2H, 4He(e, e'), E=174-597 MeV; measured σ(θ(e'), E(e')); deduced longitudinal, transverse response functions.
doi: 10.1103/PhysRevC.38.800
1988MI07 Phys.Rev. C37, 1600 (1988) R.A.Miskimen, A.M.Bernstein, G.Bernhardt, C.F.Williamson, B.A.Brown, R.Alarcon Transition Densities in 30Si Studied by Electron Scattering and Coupled-Channel Calculations of 650 MeV Proton Scattering NUCLEAR REACTIONS 30Si(p, p'), E=650 MeV; 30Si(e, e'), E not given; analyzed data. 30Si deduced transition densities.
doi: 10.1103/PhysRevC.37.1600
1988QU04 Phys.Rev. C37, 1609 (1988) B.P.Quinn, A.M.Bernstein, K.I.Blomqvist, S.A.Dytman, T.J.Pavel, R.M.Altemus, J.S.McCarthy, G.Mechtel, R.R.Whitney, T.S.Ueng, H.Arenhovel, W.Leidemann, J.M.Laget Measurements of Total and Separated Response Functions of the Deuteron through the Quasielastic Peak Region for q ≈ 300-500 MeV/c NUCLEAR REACTIONS 2H(e, e'), E ≈ 300-440 MeV; measured σ(θ(e'), E(e')); deduced longitudinal, transverse response functions.
doi: 10.1103/PhysRevC.37.1609
1987BE30 Phys.Rev.Lett. 59, 1537 (1987) D.Beck, A.Bernstein, I.Blomqvist, H.Caplan, D.Day, P.Demos, W.Dodge, G.Dodson, K.Dow, S.Dytman, M.Farkhondeh, J.Flanz, K.Giovanetti, R.Goloskie, E.Hallin, E.Knill, S.Kowalski, J.Lightbody, R.Lindgren, X.Maruyama, J.McCarthy, B.Quinn, G.Retzlaff, W.Sapp, C.Sargent, D.Skopik, I.The, D.Tieger, W.Turchinetz, T.Ueng, N.Videla, K.von Reden, R.Whitney, C.Williamson Isoscalar and Isovector Form Factors of 3H and 3He for Q below 2.9 fm-1 from Electron-Scattering Measurements NUCLEAR REACTIONS 3H, 3He(e, e), E not given; measured σ(θ). 3H, 3He deduced charge, magnetic form factors.
doi: 10.1103/PhysRevLett.59.1537
1987OC01 Phys.Rev. C35, 1063 (1987) J.S.O'Connell, W.R.Dodge, J.W.Lightbody, Jr., X.K.Maruyama, J.-O.Adler, K.Hansen, B.Schroder, A.M.Bernstein, K.I.Blomqvist, B.H.Cottman, J.J.Comuzzi, R.A.Miskimen, B.P.Quinn, J.H.Koch, N.Ohtsuka Electromagnetic Excitation of the Delta Resonance in Nuclei NUCLEAR REACTIONS 1H, 4He, 9Be, 12C, 16O(e, e'X), E=537, 730 MeV; measured inclusive σ(E(e'), θ(e')); deduced quasifree peak positions, widths, average separation energies. Dispersion matched energy loss spectrometer. Model calculations.
doi: 10.1103/PhysRevC.35.1063
1987YA02 Phys.Rev. C35, 355 (1987) M.Yamazaki, P.K.Teng, B.H.Cottman, L.Ghedira, K.Min, P.Stoler, E.J.Winhold, P.F.Yergin, A.M.Bernstein, K.I.Blomqvist, J.H.J.Distelbrink, J.A.Nelson, S.A.Dytman 16O(γ, π+)16N Reaction at 320 MeV Photon Energy NUCLEAR REACTIONS 16O(γ, π+), E=320 MeV; measured σ(θ), σ(θ, pion momentum). Medium energy pion spectrometer. DWIA calculations.
doi: 10.1103/PhysRevC.35.355
1986TE01 Phys.Lett. 177B, 25 (1986) P.K.Teng, B.H.Cottman, L.Ghedira, K.Min, P.Stoler, E.J.Winhold, M.Yamazaki, P.F.Yergin, A.M.Bernstein, K.I.Blomqvist, J.H.J.Distelbrink, J.A.Nelson, K.Rohrich, Ch.Schmitt, L.Tiator, V.H.Walther, S.A.Dytman, L.E.Wright Angular Distribution Measurement of 14N(γ, π+)14C(gs) at E(γ) = 320 MeV NUCLEAR REACTIONS 14N(γ, π+), E=320 MeV; measured σ(θ). DWIA, momentum space.
doi: 10.1016/0370-2693(86)90007-9
1985BE41 Phys.Rev. C32, 1208 (1985) A.M.Bernstein, B.H.Cottman, P.Dick, C.N.Papanicolas Predictions of Elastic Alpha Particle Scattering from the Theoretical Nuclear Densities NUCLEAR REACTIONS 40Ca(α, α), E=42, 79, 104, 142 MeV; 44,42Ca(α, α), E=42, 104 MeV; 48Ca(α, α), E=42, 79, 104 MeV; calculated σ(θ). Double-folding model, Hartree-Fock densities.
doi: 10.1103/PhysRevC.32.1208
1985BR20 Phys.Lett. 164B, 217 (1985) V.R.Brown, A.M.Bernstein, V.A.Madsen The Reversal Effect for Neutron and Proton Multipole Matrix Elements in Higher 2+ Transitions NUCLEAR STRUCTURE 118Sn, 54Fe, 90Zr, 208Pb; calculated 2+ multipole neutron, proton matrix elements; deduced spin-orbit intruder role. RPA.
doi: 10.1016/0370-2693(85)90312-0
1985CO15 Phys.Rev.Lett. 55, 684 (1985) B.H.Cottman, K.Min, P.Stoler, P.K.Teng, E.J.Winhold, M.Yamazaki, P.F.Yergin, A.M.Bernstein, K.I.Blomqvist, J.H.J.Distelbrink, J.A.Nelson, K.Rohrich, C.Schmitt, L.Tiator, V.H.Walther, G.Audit, S.A.Dytman, L.E.Wright Measurement of 14N(γ, π+)14C(g.s.) at 200 MeV: A test of the distorted-wave impulse approximation for charged-pion photoproduction below the Δ(1232) resonance NUCLEAR REACTIONS 14N(γ, π+), E=200 MeV bremsstrahlung; measured σ(θ, E(π)) vs pion momentum, σ(θ) vs momentum transfer; deduced structure effects. DWIA, one-body pion photoproduction operator.
doi: 10.1103/PhysRevLett.55.684
1984FR12 Phys.Rev. C30, 1632 (1984) G.B.Franklin, A.M.Bernstein, K.I.Blomqvist, S.A.Dytman, N.Paras, M.Pauli, J.LeRose, K.Min, D.Rowley, B.O.Sapp, P.Stoler, E.J.Winhold, P.F.Yergin Electroproduction of Low Energy Pions from Deuterium NUCLEAR REACTIONS 2H(e, π+), (e, π-), E=185-235 MeV; measured electroproduction pion yields, σ(θ(π), E(π)), ratio. DWIA analysis.
doi: 10.1103/PhysRevC.30.1632
1984OC01 Phys.Rev.Lett. 53, 1627 (1984) J.S.O'Connell, W.R.Dodge, J.W.Lightbody, Jr., X.K.Maruyama, J.-O.Adler, K.Hansen, B.Schroder, A.M.Bernstein, K.I.Blomqvist, B.H.Cottman, J.J.Comuzzi, R.A.Miskimen, B.P.Quinn Electron Scattering in the Excitation Region of the Delta Resonance on Nuclei with A = 1 to 16 NUCLEAR REACTIONS 1H, 4He, 9Be, 12C, 16O(e, e'), E=730 MeV; measured σ vs energy loss; deduced (σ/A) in the quasifree, isobar resonance regions.
doi: 10.1103/PhysRevLett.53.1627
1983MA17 Phys.Lett. 123B, 13 (1983) V.A.Madsen, T.Suzuki, A.M.Bernstein, V.R.Brown Neutron and Proton Multipole Matrix Elements in 48Ca and 208Pb NUCLEAR STRUCTURE 48Ca, 208Pb; calculated neutron, proton multipole matrix element ratios. RPA.
doi: 10.1016/0370-2693(83)90947-4
1983MI25 Phys.Lett. 131B, 26 (1983) R.A.Miskimen, A.M.Bernstein, B.Quinn, S.A.Wood, M.V.Hynes, G.S.Blanpied, B.G.Ritchie, V.R.Brown DWIA Predictions of (p, p') Data using Electromagnetically Constrained Densities NUCLEAR REACTIONS 28,30Si, 34S, 40,42Ca(polarized p, p'), E=650 MeV; measured σ(θ). 24,26Mg(polarized p, p'), E=800 MeV; analyzed σ(θ). DWIA, proton, neutron transition densities, electromagnetic constraints.
doi: 10.1016/0370-2693(83)91084-5
1983SH01 Phys.Rev. C27, 443 (1983) K.Shoda, M.Yamazaki, M.Torikoshi, H.Tsubota, K.Min, E.J.Winhold, A.M.Bernstein Pion Angular Distribution in 13C(γ, π+)13B(g.s.) NUCLEAR REACTIONS 13C(γ, π+), E=194 MeV bremsstrahlung; measured σ(θ). Comparison with DWIA calculations.
doi: 10.1103/PhysRevC.27.443
1982BE32 Phys.Rev.Lett. 49, 451 (1982) A.M.Bernstein, R.A.Miskimen, B.Quinn, S.A.Wood, M.V.Hynes, G.S.Blanpied, B.G.Ritchie, V.R.Brown Determination of Relative Signs of Neutron and Proton Transition Matrix Elements: Strong cancellation observed for the 34S(O+ → 22+) transition NUCLEAR REACTIONS 34S, 42Ca(polarized p, p'), E=650 MeV; 30Si(polarized p, p'), E=650, 800 MeV; measured σ(θ). 26Mg, 30Si, 42Ca, 34S deduced neutron, proton transition matrix element relative sign.
doi: 10.1103/PhysRevLett.49.451
1982BR24 Phys.Rev. C26, 2247 (1982) B.A.Brown, B.H.Wildenthal, W.Chung, S.E.Massen, M.Bernas, A.M.Bernstein, R.Miskimen, V.R.Brown, V.A.Madsen Isovector E2 Matrix Elements from Electromagnetic Transitions in the s-d shell: Experiment and shell-model calculations. NUCLEAR STRUCTURE A=17-39; calculated B(E2) for isovector transitions; deduced isovector effective charge. Shell model.
doi: 10.1103/PhysRevC.26.2247
1982LE06 Phys.Rev. C25, 1702 (1982) J.J.LeRose, K.Min, D.Rowley, B.O.Sapp, P.Stoler, E.J.Winhold, P.F.Yergin, A.M.Bernstein, K.I.Blomqvist, S.Dytman, G.Franklin, M.Pauli Anomalously Low Cross Section in 13C(γ, π-)13N(g.s.) NUCLEAR REACTIONS 13C(γ, π-), E=17, 29, 42 MeV; measured σ(E(π), θ=90°). DWIA calculations.
doi: 10.1103/PhysRevC.25.1702
1982LE26 Phys.Rev. C26, 2554 (1982) J.LeRose, K.Min, D.Rowley, B.O.Sapp, P.Stoler, P.-K.Teng, E.J.Winhold, P.F.Yergin, A.M.Bernstein, K.I.Blomqvist, H.S.Caplan, S.A.Dytman, G.Franklin, M.Pauli, K.Shoda, M.Yamazaki π+ Photoproduction from 13C NUCLEAR REACTIONS 13C(γ, π+), E=18, 29, 42 MeV bremsstrahlung; measured σ(θ). DWIA analysis.
doi: 10.1103/PhysRevC.26.2554
1982PA08 Phys.Rev. C25, 1296 (1982) C.N.Papanicolas, W.Q.Sumner, J.S.Blair, A.M.Bernstein Variation of the Matter Densities of Nuclei from 40Ca to 68Zn NUCLEAR REACTIONS 40,42,44,48Ca, 46,48,50Ti, 52Cr, 54,56Fe, 58,60,62,64Ni, 63,65Cu, 64,66,68Zn(α, α), E=42 MeV; analyzed σ(θ). 40,42,44,48Ca, 46,48,50Ti, 52Cr, 54,56Fe, 58,60,62,64Ni, 63,65Cu, 64,66,68Zn deduced rms radii. Microscopic optical model.
doi: 10.1103/PhysRevC.25.1296
1982RO04 Phys.Rev. C25, 2652 (1982) D.Rowley, J.LeRose, K.Min, B.O.Sapp, P.Stoler, E.J.Winhold, P.F.Yergin, A.M.Bernstein, K.I.Blomqvist, H.S.Caplan, S.A.Dytman, G.Franklin, M.Pauli Charged Pion Photoproduction from 10B NUCLEAR REACTIONS 10B(γ, π+), (γ, π-), E=17, 19, 42 MeV; measured σ(θ). 10Be, 10C level deduced σ(ratio). DWIA analysis.
doi: 10.1103/PhysRevC.25.2652
1982TE01 Phys.Rev. C26, 1313 (1982) P.K.Teng, A.Chaudhury, J.J.LeRose, K.Min, D.Rowley, B.O.Sapp, P.Stoler, E.J.Winhold, P.F.Yergin, A.M.Bernstein, K.I.Blomqvist, G.Franklin, N.Paras, M.Pauli, B.Schoch Reaction 9Be(γ, π+)9Li(g.s.) at θ(π) = 90° NUCLEAR REACTIONS 9Be(γ, π+), E=175, 187, 200 MeV; measured σ(θ=90°). Helm model, DWIA, different multipole admixtures.
doi: 10.1103/PhysRevC.26.1313
1981BE31 Phys.Lett. 103B, 255 (1981) A.M.Bernstein, V.R.Brown, V.A.Madsen Neutron and Proton Transition Matrix Elements and Inelastic Hadron Scattering NUCLEAR STRUCTURE 26Mg, 48Ca, 208Pb; calculated neutron, proton transition matrix element ratio. Inelastic hadron scattering, electromagnetic transition rate input.
doi: 10.1016/0370-2693(81)90219-7
1981BE49 Phys.Lett. 106B, 259 (1981) A.M.Bernstein, V.R.Brown, V.A.Madsen The Variation of βR with Probe in Inelastic Hadron Scattering and the Adequacy of First-Order Calculations NUCLEAR REACTIONS 116Sn, 90Zr, 58Ni(p, p'), E=800 MeV, 1.047 GeV; 116Sn, 90Zr, 58Ni(π, π'), E=162 MeV; 116Sn, 90Zr, 58Ni(α, α'), E=65 MeV; analyzed data; deduced probe dependence of deformation length. Brown-Madsen, schematic models.
doi: 10.1016/0370-2693(81)90530-X
1980BO24 Phys.Rev.Lett. 45, 1544 (1980) P.E.Bosted, K.I.Blomqvist, A.M.Bernstein, S.A.Dytman, R.A.Miskimen Differential Cross Section for 16O(γ, π+)16N and 10B(γ, π+)10Be in the Δ(1236) Region NUCLEAR REACTIONS 10B, 16O(γ, π+), E=80-210 MeV; measured σ(θ). DWIA analysis.
doi: 10.1103/PhysRevLett.45.1544
1980ST15 Phys.Rev. C22, 911 (1980) P.Stoler, E.J.Winhold, F.O'Brien, P.F.Yergin, D.Rowley, K.Min, J.LeRose, A.M.Bernstein, K.I.Blomqvist, G.Franklin, N.Paras, M.Pauli Experimental Test of Virtual Photon Theory for Pion Electroproduction on Light Nuclei NUCLEAR REACTIONS 16O(e, π+), E=180.4 MeV; 9Be(e, π+), E=184.8 MeV; 1H(e, π+), E=230 MeV; measured σ(E(π+), θ) relative to σ(photoproduction). PWBA, virtual photon theory.
doi: 10.1103/PhysRevC.22.911
1979BO23 Phys.Rev.Lett. 43, 1473 (1979) P.E.Bosted, K.I.Blomqvist, A.M.Bernstein Total Cross Section for (γ, π-) Reactions in the Δ Region NUCLEAR REACTIONS 7Li, 12C(γ, π-), E=threshold-360 MeV; measured σ(E).
doi: 10.1103/PhysRevLett.43.1473
1979MI06 Phys.Rev. C19, 1416 (1979) F.L.Milder, E.C.Booth, B.Chasan, A.M.Bernstein, J.Comuzzi, G.Franklin, A.Nagl, H.Uberall Positive-Pion Photoproduction on 12C Near Threshold NUCLEAR REACTIONS 12C(γ, π+), E=bremsstrahlung endpoint to 175 MeV; deduced σ(E); calculated σ(E), DWIA.
doi: 10.1103/PhysRevC.19.1416
1979PA06 Phys.Rev.Lett. 42, 1455 (1979) N.Paras, A.M.Bernstein, K.I.Blomqvist, G.Franklin, M.Pauli, B.Schoch, J.LeRose, K.Min, D.Rowley, P.Stoler, E.J.Winhold, P.F.Yergin Electroproduction of Charged Pions from 12C Leading to Discrete Final Nuclear States NUCLEAR REACTIONS 12C(e, π+), (e, π-), E not given; measured production σ. Virtual photon theory analysis.
doi: 10.1103/PhysRevLett.42.1455
1977BE54 Phys.Lett. 71B, 48 (1977) A.M.Bernstein, V.R.Brown, V.A.Madsen Explanation of the Near Equality of Isoscalar and Electromagnetic Transition Rates in Neutron-Excess Nuclei: Comparison with Data NUCLEAR STRUCTURE 42,44Ca, 58,60,62,64Ni, 116,118,120Sn, 206Pb, 50Ti, 52Cr, 54Fe, 88Sr, 90Zr, 92Mo, 138Ba, 140Ce, 144Sm; calculated ratios of isoscalar, electromagnetic transition rates to lowest 2+ level.
doi: 10.1016/0370-2693(77)90736-5
1977BO03 Phys.Lett. 66B, 236 (1977) E.C.Booth, B.Chasan, A.M.Bernstein, P.Bosted, J.H.Koch Threshold Photoproduction of π+ Mesons in Deuterium NUCLEAR REACTIONS 2H(γ, π+), E=threshold-9 MeV; measured σ(E).
doi: 10.1016/0370-2693(77)90869-3
1976BE39 Phys.Rev.Lett. 37, 819 (1976) A.M.Bernstein, N.Paras, W.Turchinetz, B.Chasan, E.C.Booth Reaction 12C(γ, π-)12N Near the Threshold NUCLEAR REACTIONS 12C(γ, π-), E=120-170 MeV bremsstrahlung; measured σ(E).
doi: 10.1103/PhysRevLett.37.819
1976MI15 Phys.Rev. C14, 807 (1976) K.Min, P.Stoler, S.Trentalange, E.J.Winhold, P.F.Yergin, A.M.Bernstein, W.Turchinetz, K.S.R.Sastry 11B(γ, π-)11C Cross Section Near Threshold NUCLEAR REACTIONS 11B(γ, π-), E=120-170 MeV bremsstrahlung; measured yields by residual activity; deduced σ(E).
doi: 10.1103/PhysRevC.14.807
1972BE22 Ann.Phys.(New York) 69, 19 (1972) A Qualitative Description of the Spectra 17O and 41Ca NUCLEAR STRUCTURE 17O, 41Ca; calculated levels, p-H states. Weak coupling model.
doi: 10.1016/0003-4916(72)90003-6
1972BE24 Phys.Lett. 39B, 583 (1972) The Distribution of Nucleons in the Nuclear Surface from Elastic Alpha-Particle Scattering NUCLEAR REACTIONS 90Zr, 208Pb(α, α), E=104 MeV; measured σ(θ). 90Zr, 208Pb deduced rms radii, density distributions.
doi: 10.1016/0370-2693(72)90002-0
1972FI20 Phys.Lett. 41B, 298 (1972) I.Fischman, C.E.Thorn, A.M.Bernstein, D.Cline Dominance of the Stripping over the Knockout Mechanism in the 40Ca(α, p)43Sc Reaction at 28.5 MeV NUCLEAR REACTIONS 40Ca(α, p), E=28.5 MeV; measured σ(Ep, θ); deduced stripping dominance over knockout. 43Sc deduced levels.
doi: 10.1016/0370-2693(72)90583-7
1972LE35 Phys.Rev. C6, 1254 (1972) G.M.Lerner, J.C.Hiebert, L.L.Rutledge, Jr., A.M.Bernstein Energy Dependence of Elastic α-Particle Scattering: Microscopic model NUCLEAR REACTIONS 40Ca(α, α), E=40-115.4 MeV; analyzed σ(θ); deduced energy dependence of optical model parameters.
doi: 10.1103/PhysRevC.6.1254
1971BE20 Phys.Lett. 34B, 569 (1971) An Alpha-Particle Optical Potential from the Nuclear Density Distribution NUCLEAR REACTIONS 16O, 28Si, 40Ca(α, α), E=104 MeV; calculated σ(θ); deduced optical potential from nuclear density distribution.
doi: 10.1016/0370-2693(71)90138-9
1971SM04 Nucl.Phys. A173, 32 (1971) S.M.Smith, P.G.Roos, C.Moazed, A.M.Bernstein Fragmentation of One-Hole State Strengths in the 208Pb(p, d)207Pb Reaction by Hole-Core Coupling States NUCLEAR REACTIONS 208Pb(p, d), E=41 MeV; measured σ(Ed, θ). 207Pb deduced levels, J, π, S. Enriched target.
doi: 10.1016/0375-9474(71)90746-9
1970GI10 Nucl.Phys. A154, 417 (1970) The (α, p) Reaction on 40,42,44,48Ca and 48Ti at 31 MeV NUCLEAR REACTIONS 40,42,44,48Ca(α, p), 48Ti(α, p), E=31 MeV; measured σ(Ep, θ), Q. 43,45,47,51Sc, 51V deduced levels, J, π, L. Enriched targets.
doi: 10.1016/0375-9474(70)90167-3
1970SM06 Priv.Comm. to be Published (1970) S.M.Smith, P.G.Roos, C.Moazed, A.M.Bernstein Deviations from the Simple Shell Model Found in the 208Pb(p, d)207Pb Reaction
1970SM07 Nucl.Phys. A158, 497 (1970) S.M.Smith, P.G.Roos, A.M.Bernstein, C.Moazed Test of the Shell Model for 206Pb by the 208Pb(p, t) Reaction NUCLEAR REACTIONS 208Pb(p, t), E=40 MeV; measured σ(Et, θ). 206Pb deduced levels, L, J, π. Enriched target.
doi: 10.1016/0375-9474(70)90199-5
1969BE22 Phys.Letters 29B, 335 (1969) A Comparison of Electromagnetic and Isoscalar Transition Rates in Nuclei
doi: 10.1016/0370-2693(69)90376-1
1969BE30 Phys.Letters 30B, 20 (1969) A.M.Bernstein, M.Duffy, E.P.Lippincott The Relative Spatial Distributions of Neutrons and Protons in the Surface of 48Ca NUCLEAR REACTIONS 40,48Ca(α, α), E=29, 31 MeV; measured σ(θ). 40,48Ca deduced nuclear charge distributions.
doi: 10.1016/0370-2693(69)90275-5
1969MO18 Nucl.Phys. A139, 1 (1969) C.Moazed, K.Nagatani, A.M.Bernstein A Study of 50Sc via the 48Ca(α, d) Reaction NUCLEAR REACTIONS 48Ca(α, d), E=31 MeV; measured σ(Ed, θ). 50Sc deduced levels, J, π, L, T. Enriched targets.
doi: 10.1016/0375-9474(69)90253-X
1969SM02 Nucl.Phys. A125, 339(1969) The 42,44Ca(p, t)40,42Ca Reactions at 26.5 MeV NUCLEAR REACTIONS 42,44Ca(p, t), 42Ca(p, p), E=26.5 MeV; measured σ(Et, θ), σ(Ep, θ). 40Ca, 42Ca deduced levels, J, π, L. Enriched targets.
doi: 10.1016/0375-9474(69)91078-1
1968BE23 Nucl.Phys. A115, 79 (1968) A.M.Bernstein, E.P.Lippincott, J.T.Sample, C.B.Thorn The 48Ti(α, α') Reaction and Systematics of Octupole States in the Ti Isotopes NUCLEAR REACTIONS 48Ti(α, α'), E = 31; measured σ(Eα', θ). 48Ti deduced levels, J, π. Enriched target.
doi: 10.1016/0375-9474(68)90642-8
1968MA30 Nucl.Phys. A117, 241 (1968) The 90Zr and 92Mo(α, α') Reactions at 31 MeV NUCLEAR REACTIONS 90Zr, 92Mo(α, α'), E=31 MeV; measured σ(Eα', θ). 90Zr, 92Mo deduced levels, J. Enriched targets.
doi: 10.1016/0375-9474(68)90842-7
1968SM05 Nucl.Phys. A113, 303(1968) S.M.Smith, A.M.Bernstein, M.E.Rickey The 42,44Ca(p, d)41,43Ca Reactions at 26.5 MeV NUCLEAR REACTIONS 42Ca(p, d), 44Ca(p, d), E=26.5 MeV; measured σ(Ed, θ). 41Ca, 43Ca deduced levels, J, π, L, T. Enriched targets.
doi: 10.1016/0375-9474(68)90408-9
1968SM06 Phys.Rev. 169, 951 (1968) S.M.Smith, C.Moazed, A.M.Bernstein, P.G.Roos Experimental and Theoretical Investigation of the Pb208(p, t)Pb206 Reaction at 40 MeV NUCLEAR STRUCTURE 206Pb; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.169.951
1967GI09 Phys. Letters 25B, 206 (1967) R.O.Ginaven, A.M.Bernstein, R.M.Drisko, J.B.McGrory The 48Ca(α, p)51Sc Reaction; Experimental Results and Shell Model Calculations NUCLEAR STRUCTURE 51Sc; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(67)90038-X
1967LI13 Phys.Rev. 163, 1170 (1967) Nuclear Structure of Ca40, 42, 44, 48 from Inelastic Alpha-Particle Scattering NUCLEAR STRUCTURE 40Ca, 44Ca, 42Ca, 48Ca; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.163.1170
1967MA10 Phys.Letters 24B, 669 (1967) Fractionization of the Octupole Strength in 90Zr NUCLEAR STRUCTURE 90Zr; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(67)90376-0
1966BE19 Phys.Rev.Letters 17, 321 (1966) Systematics of 3- and 5- States in Ca40,42,44,48 and Ti50 NUCLEAR STRUCTURE 40Ca, 42Ca, 44Ca, 48Ca, 50Ti; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.17.321
1965BA03 Phys.Letters 14, 129 (1965) R.W.Bauer, A.M.Bernstein, G.Heymann, E.P.Lippincott, N.S.Wall Ca40(α, α'): A Test of Particle-Hole Calculations NUCLEAR STRUCTURE 40Ca; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(65)90451-8
1965BE05 Bull.Am.Phys.Soc. 10, No.1, 122, KD10 (1965) Zr90(α, α') Reaction at 30.5 MeV NUCLEAR STRUCTURE 90Zr; measured not abstracted; deduced nuclear properties.
1965GI05 MIT-2098-251, p.64 (1965) R.Ginaven, S.M.Smith, A.Bernstein Ca42,44,48 and Ti48 Targets NUCLEAR REACTIONS 42,44,48Ca, 48Ti(α, p), E not given; measured σ(Ep, θ). 47Sc, 51V deduced levels, J, π, S.
1965LI03 Bull.Am.Phys.Soc. 10, No.1, 122, KD8 (1965) Elastic and Inelastic Scattering of 30.5-MeV α Particles on Ti50 NUCLEAR STRUCTURE 50Ti; measured not abstracted; deduced nuclear properties.
1964BE24 Phys. Rev. 136, B27 (1964) A.M.Bernstein, R.A.Haberstroh, D.R.Hamilton, M.Posner, J.L.Snider Spin and Magnetic Moment of N13 NUCLEAR STRUCTURE 13N; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.136.B27
1963GR07 Bull.Am.Phys.Soc. 8, No.4, 358, N11 (1963) C.R.Gruhn, N.S.Wall, A.Bernstein, N.Baron, J.Need, J.Vincent, E.Boschitz Elastic Scattering of 30- to 40-MeV α-Particles from Ca40 at Large Angles NUCLEAR STRUCTURE 40Ca; measured not abstracted; deduced nuclear properties.
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