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NSR database version of April 11, 2024.

Search: Author = A.M.Bernstein

Found 91 matches.

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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
Citations: PlumX Metrics


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
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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
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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
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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
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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
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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
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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
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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
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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
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2003BE44      Eur.Phys.J. A 17, 349 (2003)

A.M.Bernstein

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
Citations: PlumX Metrics


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
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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
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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
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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
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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
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1998BE78      Phys.Lett. 442B, 20 (1998)

A.M.Bernstein

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
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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
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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
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1997BE47      Nucl.Phys. A623, 178c (1997)

A.M.Bernstein

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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1972BE22      Ann.Phys.(New York) 69, 19 (1972)

A.M.Bernstein

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
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1972BE24      Phys.Lett. 39B, 583 (1972)

A.M.Bernstein, W.A.Seidler

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
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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
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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
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1971BE20      Phys.Lett. 34B, 569 (1971)

A.M.Bernstein, W.A.Seidler

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
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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
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1970GI10      Nucl.Phys. A154, 417 (1970)

R.O.Ginaven, A.M.Bernstein

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
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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
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1969BE22      Phys.Letters 29B, 335 (1969)

A.M.Bernstein

A Comparison of Electromagnetic and Isoscalar Transition Rates in Nuclei

doi: 10.1016/0370-2693(69)90376-1
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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
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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
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1969SM02      Nucl.Phys. A125, 339(1969)

S.M.Smith, A.M.Bernstein

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
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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
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1968MA30      Nucl.Phys. A117, 241 (1968)

E.J.Martens, A.M.Bernstein

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
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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
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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
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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
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1967LI13      Phys.Rev. 163, 1170 (1967)

E.P.Lippincott, A.M.Bernstein

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
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1967MA10      Phys.Letters 24B, 669 (1967)

E.J.Martens, A.M.Bernstein

Fractionization of the Octupole Strength in 90Zr

NUCLEAR STRUCTURE 90Zr; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0370-2693(67)90376-0
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1966BE19      Phys.Rev.Letters 17, 321 (1966)

A.M.Bernstein, E.P.Lippincott

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
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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
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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
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1961AM02      Phys.Rev. 123, 1793 (1961)

O.Ames, A.M.Bernstein, M.H.Brennan, D.R.Hamilton

Magnetic Moments of 69-min Ag104 and 27-min Ag104m

NUCLEAR STRUCTURE 104Ag; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.123.1793
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1961PO09      Phys.Rev.Letters 7, 173 (1961)

M.Posner, J.L.Snider, A.M.Bernstein, D.R.Hamilton

Magnetic Moment of N13

NUCLEAR MOMENTS 13N; measured resonance transitions and frequencies; deduced nuclear magnetic moment. Comparison with available data.

doi: 10.1103/PhysRevLett.7.173
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1961SN01      Bull.Am.Phys.Soc. 6, No.3, 224, A1 (1961)

J.L.Snider, M.Posner, A.M.Bernstein, D.R.Hamilton

Nuclear Spins of N13 and C11

NUCLEAR STRUCTURE 13N, 11C; measured not abstracted; deduced nuclear properties.


1960AM01      Bull.Am.Phys.Soc. 5, No.1, 20, F2 (1960)

O.Ames, M.H.Brennan, A.M.Bernstein, D.R.Hamilton

Hyperfine Structure Separations of 70-min Ag104 and 27-min Ag104m

NUCLEAR STRUCTURE 104Ag; measured not abstracted; deduced nuclear properties.


1960AM02      Phys.Rev. 118, 1599 (1960)

O.Ames, A.M.Bernstein, M.H.Brennan, R.A.Haberstroh, D.R.Hamilton

Spins and Decay Modes of Certain Neutron-Deficient Silver Isotopes

NUCLEAR STRUCTURE 104Ag, 103Ag, 102Ag; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.118.1599
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1960BE03      Bull.Am.Phys.Soc. 5, No.1, 20, F1 (1960)

A.M.Bernstein, O.Ames, M.H.Brennan, R.A.Haberstroh, D.R.Hamilton

Ground and First Excited States of Ag104

NUCLEAR STRUCTURE 104Ag; measured not abstracted; deduced nuclear properties.


1960BR03      Bull.Am.Phys.Soc. 5, No.1, 20, F3 (1960)

M.H.Brennan, A.M.Bernstein

Spins and Moments of Odd-Odd Nuclei


1960BR39      Phys.Rev. 120, 927 (1960)

M.H.Brennan, A.M.Bernstein

jj Coupling Model in Odd-Odd Nuclei

doi: 10.1103/PhysRev.120.927
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