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Search: Author = J.Lichtenstadt

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2017YA13      Phys.Lett. B 769, 21 (2017)

I.Yaron, D.Izraeli, P.Achenbach, H.Arenhovel, J.Bericic, R.Bohm, D.Bosnar, E.O.Cohen, L.Debenjak, M.O.Distler, A.Esser, I.Friscic, R.Gilman, I.Korover, J.Lichtenstadt, H.Merkel, D.G.Middleton, M.Mihovilovic, U.Muller, E.Piasetzky, J.Pochodzalla, G.Ron, B.S.Schlimme, M.Schoth, F.Schulz, C.Sfienti, S.Sirca, S.Strauch, M.Thiel, A.Tyukin, A.Webe

Polarization-transfer measurement to a large-virtuality bound proton in the deuteron

NUCLEAR REACTIONS 2H(polarized E, E'polarized p), E=600, 630 MeV; measured reaction products; deduced helicity dependent polarization components. Comparison with theoretical calculations.

doi: 10.1016/j.physletb.2017.01.034
Citations: PlumX Metrics


2013RO06      Phys.Rev. C 87, 028202 (2013)

G.Ron, W.Cosyn, E.Piasetzky, J.Ryckebusch, J.Lichtenstadt

Nuclear density dependence of in-medium polarization

NUCLEAR REACTIONS 12C(polarized e, e'p)11B, E at <250 MeV/c; calculated effective densities for protons removed from the s- and p-shells, expected in-medium modification effects. Chiral quark soliton (CQS), and quark meson coupling (QMC) models. Proposed measurement of polarization transfer components for proton knockout from s- or p-shell.

doi: 10.1103/PhysRevC.87.028202
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2001ZH20      Phys.Rev.Lett. 87, 081801 (2001)

H.Zhu, A.Ahmidouch, H.Anklin, H.Arenhovel, C.Armstrong, C.Bernet, W.Boeglin, H.Breuer, P.Brindza, D.Brown, S.Bultmann, R.Carlini, N.Chant, A.Cowley, D.Crabb, S.Danagoulian, D.B.Day, T.Eden, R.Ent, Y.Farah, R.Fatemi, K.Garrow, C.Harris, M.Hauger, A.Honegger, J.Jourdan, M.Kaufmann, M.Khandaker, G.Kubon, J.Lichtenstadt, R.Lindgren, R.Lourie, A.Lung, D.Mack, S.Malik, P.Markowitz, K.McFarlane, P.McKee, D.McNulty, G.Milanovich, J.Mitchell, H.Mkrtchyan, M.Muhlbauer, T.Petitjean, Y.Prok, D.Rohe, E.Rollinde, O.A.Rondon, P.Roos, R.Sawafta, I.Sick, C.Smith, T.Southern, M.Steinacher, S.Stepanyan, V.Tadevosyan, R.Tieulent, A.Tobias, W.Vulcan, G.Warren, H.Wohrle, S.Wood, C.Yan, M.Zeier, J.Zhao, B.Zihlmann

Measurement of the Electric Form Factor of the Neutron Through d(pol)(e(pol), e'n)p at Q2 = 0.5 (GeV/c)2

NUCLEAR REACTIONS 2H(polarized e, e'n), E=2.725 GeV; measured electron and neutron spectra, angular distributions, asymmetries. 1n deduced electric form factor. Solid polarized target.

doi: 10.1103/PhysRevLett.87.081801
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1999DE02      Eur.Phys.J. C 6, 121 (1999)

A.De Roeck, A.Deshpande, V.W.Hughes, J.Lichtenstadt, G.Radel

A Study of the Polarized Structure Function g1p(x, Q2) and the Polarized Gluon Distribution Δg(x, Q2) at HERA

NUCLEAR REACTIONS 1H(polarized e, e'), E=high; calculated spin-dependent asymmetries; deduced implications for polarized structure function, gluon distribution measurements. Polarized target.

doi: 10.1007/s100520050325
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1998ST17      Phys.Rev. D58, 032003 (1998)

L.M.Stuart, P.E.Bosted, L.Andivahis, A.Lung, J.Alster, R.G.Arnold, C.C.Chang, F.S.Dietrich, W.R.Dodge, R.Gearhart, J.Gomez, K.A.Griffioen, R.S.Hicks, C.E.Hyde-Wright, C.Keppel, S.E.Kuhn, J.Lichtenstadt, R.A.Miskimen, G.A.Peterson, G.G.Petratos, S.E.Rock, S.H.Rokni, W.K.Sakumoto, M.Spengos, K.Swartz, Z.Szalata, L.H.Tao

Measurements of the Δ(1232) Transition Form Factor and the Ratio σnp from Inelastic Electron-Proton and Electron-Deuteron Scattering

NUCLEAR REACTIONS 1,2H(e, e'), E=9.8 GeV; measured σ(E', θ); deduced transition form factors, Δ production σ(n)/σ(p).

doi: 10.1103/PhysRevD.58.032003
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1994AN23      Phys.Lett. 336B, 313 (1994)

H.Anklin, E.E.W.Bruins, D.Day, D.Fritschi, B.Groft, F.C.P.Joosse, J.Jourdan, J.Lichtenstadt, M.Loppacher, G.Masson, J.Mitchell, I.Sick, H.J.J.van Veen

Precision Measurement of the Neutron Magnetic Form Factor

NUCLEAR REACTIONS 2H(e, e'n), (e, e'p), E=457.7, 450.9 MeV; measured σ(θ) ratio. 1n deduced magnetic form factor. High precision detector efficiency from 1H(n, p) reaction.

doi: 10.1016/0370-2693(94)90538-X
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1994AN34      Phys.Rev. D50, 5491 (1994)

L.Andivahis, P.E.Bosted, A.Lung, L.M.Stuart, J.Alster, R.G.Arnold, C.C.Chang, F.S.Dietrich, W.Dodge, R.Gearhart, J.Gomez, K.A.Griffioen, R.S.Hicks, C.E.Hyde-Wright, C.Keppel, S.E.Kuhn, J.Lichtenstadt, R.A.Miskimen, G.A.Peterson, G.G.Petratos, S.E.Rock, S.Rokni, W.K.Sakumoto, M.Spengos, K.Swartz, Z.Szalata, L.H.Tao

Measurements of the Electric and Magnetic Form Factors of the Proton from Q2 = 1.75 to 8.83 (GeV/c)2

NUCLEAR REACTIONS 1H(e, e), E ≈ 9.8 GeV; measured σ(θ). 1H deduced electric, magnetic form factors. Model comparison.

doi: 10.1103/PhysRevD.50.5491
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1993AN04      Nucl.Phys. A553, 713c (1993)

L.Andivahis, P.Bosted, A.Lung, L.Stuart, J.Alster, R.Arnold, C.Chang, F.Dietrich, W.Dodge, R.Gearhart, J.Gomez, K.Griffioen, R.Hicks, C.Hyde-Wright, C.Keppel, S.Kuhn, J.Lichtenstadt, R.Miskimen, G.Peterson, G.Petratos, S.Rock, S.Rokni, W.Sakumoto, M.Spengos, K.Swartz, Z.Szalata, L.Tao

Measurements of the Nucleon Form Factors at Large Momentum Transfers

NUCLEAR REACTIONS 2,1H(e, e), E=1.5-9.8 GeV; measured σ(θ, E). 1H, 1n deduced form factors.

doi: 10.1016/0375-9474(93)90686-R
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1993FR05      Phys.Rev. C47, 1599 (1993)

M.Frodyma, R.G.Arnold, D.Benton, P.E.Bosted, L.Clogher, G.Dechambrier, A.T.Katramatou, J.Lambert, A.Lung, G.G.Petratos, A.Rahbar, S.E.Rock, Z.M.Szalata, B.Debebe, R.S.Hicks, A.Hotta, G.A.Peterson, R.A.Gearhart, J.Alster, J.Lichtenstadt, F.Dietrich, K.van Bibber

Measurements of Transverse Electron Scattering from the Deuteron in the Threshold Region at High Momentum Transfers

NUCLEAR REACTIONS 2H(e, e'X), E=0.734-1.279 GeV; measured σ(θ, E(np)); deduced inelastic structure function ratio. Model comparison.

doi: 10.1103/PhysRevC.47.1599
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1992BO34      Phys.Rev. C46, 2505 (1992)

P.E.Bosted, A.Lung, L.Andivahis, L.M.Stuart, J.Alster, R.G.Arnold, C.C.Chang, F.S.Dietrich, W.Dodge, R.Gearhart, J.Gomez, K.A.Griffioen, R.S.Hicks, C.E.Hyde-Wright, C.Keppel, S.E.Kuhn, J.Lichtenstadt, R.A.Miskimen, G.A.Peterson, G.G.Petratos, S.E.Rock, S.Rokni, W.K.Sakumoto, M.Spengos, K.Swartz, Z.Szalata, L.H.Tao

Measurements of (ν)W2 and R = σ(L)/σ(T) from Inelastic Electron-Aluminum Scattering Near x = 1

NUCLEAR REACTIONS 27Al(e, e'X), E=1.5-5.5 GeV; measured inclusive σ per nucleon, ratio to 2H; deduced σ(L)/σ(T) vs Q2.

doi: 10.1103/PhysRevC.46.2505
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1991BO21      Nucl.Phys. A527, 339c (1991)

P.E.Bosted, L.Clogher, A.Lung, L.Stuart, J.Alster, R.G.Arnold, C.C.Chang, F.Dietrich, W.R.Dodge, R.Gearhart, J.Gomez, K.Griffioen, R.Hicks, C.Hyde-Wright, C.Keppel, S.Kuhn, J.Lichtenstadt, R.Miskimen, G.G.Petratos, G.A.Peterson, S.E.Rock, S.H.Rokni, W.K.Sakumoto, K.Swartz, Z.N.Szalata, L.H.Tao

New Measurements of the Electric and Magnetic Elastic Form Factors of the Proton and Neutron at High Momentum Transfers

NUCLEAR REACTIONS 1H(e, e'), E=1.4-10 GeV; measured electron spectra. 1H deduced magnetic form factor.

doi: 10.1016/0375-9474(91)90123-N
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1991JO09      Nucl.Phys. A527, 340c (1991)

F.C.P.Joosse, Th.S.Bauer, J.F.J.van den Brand, D.Day, E.Jans, J.Jourdan, J.Lichtenstadt, G.Masson, J.Mitchell, I.Sick, P.K.A.de Witt Huberts

A Determination of the Magnetic Form Factor of the Neutron

NUCLEAR REACTIONS 2H(e, e'n), (e, e'p), E not given; measured σ(ratio). 1n deduced magnetic form factor.

doi: 10.1016/0375-9474(91)90123-N
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1991RA08      Phys.Rev.Lett. 66, 1279 (1991)

A.Rahav, J.Alster, D.Ashery, J.Lichtenstadt, I.Navon, E.Piasetzky, P.Amaudruz, M.Botje, W.Burger, C.H.Q.Ingram, R.A.Schumacher, U.Sennhauser, S.A.Wood

Measurement of the 12C(π, 2π) Reactions and Possible Evidence of a Double-Δ Excitation

NUCLEAR REACTIONS 12C(π-, π-π+), (π-, 2π-), E=292 MeV; measured pion spectra, σ(θ); deduced double-Δ excitation evidence.

doi: 10.1103/PhysRevLett.66.1279
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1990AR09      Phys.Rev. C42, R1 (1990)

R.G.Arnold, D.Benton, P.E.Bosted, L.Clogher, G.deChambrier, A.T.Katramatou, J.Lambert, A.Lung, G.G.Petratos, A.Rahbar, S.E.Rock, Z.M.Szalata, B.Debebe, M.B.Frodyma, R.S.Hicks, A.Hotta, G.A.Peterson, R.A.Gearhart, J.Alster, J.Lichtenstadt, F.Dietrich, K.van Bibber

Transverse Electrodisintegration of the Deuteron in the Threshold Region at High Q2

NUCLEAR REACTIONS 2H(e, np), E=0.73-1.3 GeV; measured σ(θ) vs E(np), θ=180°; deduced non-nucleonic degrees of freedom role.

doi: 10.1103/PhysRevC.42.R1
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1990BO18      Phys.Rev. C42, 38 (1990)

P.E.Bosted, A.T.Katramatou, R.G.Arnold, D.Benton, L.Clogher, G.DeChambrier, J.Lambert, A.Lung, G.G.Petratos, A.Rahbar, S.E.Rock, Z.M.Szalata, B.Debebe, M.Frodyma, R.S.Hicks, A.Hotta, G.A.Peterson, R.A.Gearhart, J.Alster, J.Lichtenstadt, F.Dietrich, K.van Bibber

Measurements of the Deuteron and Proton Magnetic Form Factors at Large Momentum Transfers

NUCLEAR REACTIONS 2H(e, e'), E=0.5-1.3 GeV; measured ed-, ep-coin, form factors. 2H deduced magnetic structure function.

doi: 10.1103/PhysRevC.42.38
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1990LI21      Phys.Lett. 244B, 173 (1990)

J.Lichtenstadt, J.Alster, M.A.Moinester, J.Dubach, R.S.Hicks, G.A.Peterson, S.Kowalski

Multi-Nucleon Degrees of Freedom in Inelastic Form Factors of 7Li

NUCLEAR REACTIONS 7Li(e, e'), E=80-680 MeV; measured electromagnetic form factors; deduced multi-nucleon degrees of freedom role.

doi: 10.1016/0370-2693(90)90050-G
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1989LI09      Phys.Lett. 219B, 394 (1989)

J.Lichtenstadt, J.Alster, M.A.Moinester, J.Dubach, R.S.Hicks, G.A.Peterson, S.Kowalski

High Momentum Transfer Longitudinal and Transverse Form Factors of the 7Li Ground-State Doublet

NUCLEAR REACTIONS 7,6Li(e, e), (e, e'), E=80-680 MeV; measured longitudinal, transverse form factors.

doi: 10.1016/0370-2693(89)91083-6
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1989PL05      Phys.Rev. C40, 1861 (1989)

M.A.Plum, R.A.Lindgren, J.Dubach, R.S.Hicks, R.L.Huffman, B.Parker, G.A.Peterson, J.Alster, J.Lichtenstadt, M.A.Moinester, H.Baer

180° Electron Scattering from 14C

NUCLEAR REACTIONS 14C(e, e'), E=82-269 MeV; measured σ(E(e'), θ); deduced 14C, 14B Coulomb energy difference. 14C levels deduced structure coefficients, form factors, IAS.

doi: 10.1103/PhysRevC.40.1861
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1988AR14      Phys.Rev.Lett. 61, 806 (1988)

R.G.Arnold, D.Benton, P.Bosted, L.Clogher, G.DeChambrier, A.T.Katramatou, J.Lambert, A.Lung, G.G.Petratos, A.Rahbar, S.E.Rock, Z.M.Szalata, B.Debebe, M.Frodyma, R.S.Hicks, A.Hotta, G.A.Peterson, R.A.Gearhart, J.Alster, J.Lichtenstadt, F.Dietrich, K.van Bibber

Measurements of Transverse Quasielastic Electron Scattering from the Deuteron at High Momentum Transfers

NUCLEAR REACTIONS 2H(e, e'), E=0.843-1.281 GeV; measured σ(θ, E(e')); deduced scaling function.

doi: 10.1103/PhysRevLett.61.806
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1988AS04      Phys.Lett. 215B, 41 (1988)

D.Ashery, J.Lichtenstadt, E.Piasetzky, C.L.Morris, J.D.Zumbro, R.Gilman, M.W.Rawool, S.Mordechai, B.Boyer, A.Fuentes, K.Johnson, J.W.McDonald, M.J.Smithson, A.Williams, S.H.Yoo, C.F.Moore

A Search for πNN Bound Systems

NUCLEAR REACTIONS 2H(π+, π-), (π-, π+), E=260 MeV; measured possible (πNN) system mass; deduced σ upper limit.

doi: 10.1016/0370-2693(88)91066-0
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1988BR06      Phys.Rev. C37, 1345 (1988)

G.Bruge, D.Garreta, P.Birien, H.Catz, A.Chaumeaux, S.Janouin, D.Legrand, M.C.Lemaire, B.Mayer, J.Pain, F.Perrot, E.Aslanides, O.Bing, D.M.Drake, J.C.Peng, M.Berrada, J.P.Bocquet, E.Monnand, J.Mougey, P.Perrin, J.Lichtenstadt, A.I.Yavin

Elastic Scattering of 179.3 MeV Antiprotons by Deuterium

NUCLEAR REACTIONS 2H(p-bar, p-bar), E=179.3 MeV; measured σ(θ).

doi: 10.1103/PhysRevC.37.1345
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1987AR09      Phys.Rev.Lett. 58, 1723 (1987)

R.G.Arnold, D.Benton, P.Bosted, L.Clogher, G.DeChambrier, A.T.Katramatou, J.Lambert, A.Lung, G.G.Petratos, A.Rahbar, S.E.Rock, Z.M.Szalata, R.A.Gearhart, B.Debebe, M.Frodyma, R.S.Hicks, A.Hotta, G.A.Peterson, J.Alster, J.Lichtenstadt, F.Dietrich, K.van Bibber

Deuteron Magnetic Form Factor Measurements of High Momentum Transfer

NUCLEAR REACTIONS 2H(e, e), E at 0.41-0.54 GeV/c; measured σ(θ). 2H deduced structure function, magnetic form factor. Liquid deuterium, multi-wire proportional chambers.

doi: 10.1103/PhysRevLett.58.1723
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1987AS06      Nucl.Phys. A470, 445 (1987)

E.Aslanides, D.M.Drake, J.C.Peng, D.Garreta, P.Birien, G.Bruge, H.Catz, A.Chaumeaux, S.Janouin, D.Legrand, M.-C.Lemaire, B.Mayer, J.Pain, F.Perrot, M.Berrada, J.P.Bocquet, E.Monnand, J.Mougey, P.Perrin, O.Bing, J.Lichtenstadt, A.I.Yavin

Search for p-bar-Nucleus States using the (p-bar, p) Knock-Out Reaction at 600 MeV/c

NUCLEAR REACTIONS 1,2H, 6Li, 12C, 63Cu, 208Pb, 209Bi(p-bar, p), E=180 MeV; measured σ(Ep, θ=0°); deduced temperatures, proton production σ, mass dependence, effective proton number, quasifree σ(θ=0°).

doi: 10.1016/0375-9474(87)90580-X
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1987HY01      Phys.Rev. C35, 880 (1987)

C.E.Hyde-Wright, W.Bertozzi, T.N.Buti, J.M.Finn, F.W.Hersman, M.V.Hynes, M.A.Kovash, J.J.Kelly, S.Kowalski, J.Lichtenstadt, R.W.Lourie, B.E.Norum, B.Pugh, C.P.Sargent, B.L.Berman, F.Petrovich, J.A.Carr

Electroexcitation of 4- States in 16O

NUCLEAR REACTIONS 16O(e, e'), E=230 MeV; measured σ(E(e'), θ(e')), transverse form factors. 16O deduced levels, J, π, T, spectroscopic amplitudes.

doi: 10.1103/PhysRevC.35.880
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1986AL22      Phys.Rev. C34, 1757 (1986)

A.Altman, D.Ashery, E.Piasetzky, J.Lichtenstadt, A.I.Yavin, W.Bertl, L.Felawka, H.K.Walter, R.J.Powers, R.G.Winter, J.v.d.Pluym

(π±, 2N) Reactions at 165 and 245 MeV

NUCLEAR REACTIONS 12C, Fe, 209Bi, 16,18O(π+, 2p), (π-, 2p), (π+, np), (π-, np), E=165, 245 MeV; measured σ(θ1, θ2); deduced quasideuteron parameters. Natural, enriched targets, ΔE-E telescopes.

doi: 10.1103/PhysRevC.34.1757
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1986BR04      Phys.Lett. 169B, 14 (1986)

G.Bruge, A.Chaumeaux, P.Birien, D.M.Drake, D.Garreta, S.Janouin, D.Legrand, M.C.Lemaire, B.Mayer, J.Pain, M.Berrada, J.P.Bocquet, E.Monnand, J.Mougey, P.Perrin, E.Aslanides, O.Bing, J.Lichtenstadt, A.I.Yavin, J.C.Peng

Comparative Study of the Elastic Scattering of 178.4 MeV Antiprotons by the 16O and 18O Isotopes

NUCLEAR REACTIONS 16,18O(p-bar, p-bar), E=178.4 MeV; measured σ(θ); deduced optical model parameters, neutron excess role.

doi: 10.1016/0370-2693(86)90676-3
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1986ER09      Phys.Rev. C34, 1822 (1986)

A.Erell, J.Alster, J.Lichtenstadt, M.A.Moinester, J.D.Bowman, M.D.Cooper, F.Irom, H.S.Matis, E.Piasetzky, U.Sennhauser

Measurements on Isovector Giant Resonances in Pion Charge Exchange

NUCLEAR REACTIONS 40Ca, 60Ni, 90Zr, 120Sn, 140Ce, 208Pb(π+, π0), (π-, π0), E=165 MeV; measured σ(θ(π), E(π)). 40Ca, 60Ni, 90Zr, 120Sn, 140Ce, 208Pb deduced isovector giant resonances, excitation σ, Γ. DWIA calculations.

doi: 10.1103/PhysRevC.34.1822
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1986FR10      Nucl.Phys. A455, 573 (1986)

E.Friedman, J.Lichtenstadt

The Information Content of Antiproton-Nucleus Scattering Data

NUCLEAR REACTIONS 12C, 16,18O, 40Ca(p-bar, p-bar), E=180 MeV; 40Ca(p-bar, p-bar), E=40 MeV; analyzed data; deduced folding model parameters.

doi: 10.1016/0375-9474(86)90451-3
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1986HE09      Phys.Rev. C33, 1905 (1986)

F.W.Hersman, W.Bertozzi, T.N.Buti, J.M.Finn, C.E.Hyde-Wright, M.V.Hynes, J.Kelly, M.A.Kovash, S.Kowalski, J.Lichtenstadt, R.Lourie, B.Murdock, B.Pugh, F.N.Rad, C.P.Sargent, J.B.Bellicard

Inelastic Electron Scattering from Collective Levels of 154Gd

NUCLEAR REACTIONS 154Gd(e, e), (e, e'), E=78-380 MeV; measured σ(E(e')), σ(θ). 154Gd levels deduced B(λ), transition charge density. Hartree-Fock wave functions, rotational, vibrational models.

doi: 10.1103/PhysRevC.33.1905
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1986IR02      Phys.Rev. C34, 2231 (1986)

F.Irom, J.D.Bowman, G.O.Bolme, E.Piasetzky, U.Sennhauser, J.Alster, J.Lichtenstadt, M.Moinester, J.N.Knudson, S.H.Rokni, E.R.Siciliano

Excitation of Isovector Giant Resonances in Pion Single-Charge Exchange at 120, 165, and 230 MeV

NUCLEAR REACTIONS 40Ca, 60Ni, 120Sn(π+, π0), (π-, π0), E=120, 230 MeV; measured σ(θ(π), E(π)). 40Ca, 60Ni, 120Sn deduced monopole, dipole resonance excitation energies, widths, maximum σ. Scintillator activation technique, π0 spectrometer. DWIA calculations.

doi: 10.1103/PhysRevC.34.2231
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1986JA04      Nucl.Phys. A451, 541 (1986)

S.Janouin, M.-C.Lemaire, D.Garreta, P.Birien, G.Bruge, D.M.Drake, D.Legrand, B.Mayer, J.Pain, J.C.Peng, M.Berrada, J.P.Bocquet, E.Monnand, J.Mougey, P.Perrin, E.Aslanides, O.Bing, J.Lichtenstadt, A.I.Yavin

Optical-Model Analysis of Antiproton-Nucleus Elastic Scattering at 50 and 180 MeV

NUCLEAR REACTIONS 12C, 40Ca, 208Pb(p-bar, p-bar), E ≈ 50, 180 MeV; 16,18O(p-bar, p-bar), E=178.4 MeV; analyzed σ(θ); deduced reaction σ, potential parameters.

doi: 10.1016/0375-9474(86)90291-5
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1986LE13      Nucl.Phys. A456, 557 (1986)

M.-C.Lemaire, P.Birien, G.Bruge, D.M.Drake, D.Garreta, S.Janouin, D.Legrand, B.Mayer, J.Pain, J.C.Peng, M.Berrada, J.P.Bocquet, E.Monnand, J.Mougey, P.Perrin, E.L.Aslanides, O.Bing, J.Lichtenstadt, A.I.Yavin

Inelastic Scattering of Antiprotons from 12C and 18O at 50 and 180 MeV

NUCLEAR REACTIONS 18O, 12C(p-bar, p-bar), (p-bar, p-bar'), E=46.7, 179.7, 178.4 MeV; measured σ(θ); deduced potential parameters. 12C deduced quadrupole deformation parameters, deformation lengths, B(λ), δ. 18O deduced quadrupole, hexadecapole deformation lengths.

doi: 10.1016/0375-9474(86)90075-8
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1986LI01      Phys.Rev. C33, 655 (1986)

J.Lichtenstadt, D.Ashery, S.A.Wood, E.Piasetzky, P.A.M.Gram, D.W.MacArthur, R.S.Bhalerao, L.C.Liu, G.A.Rebka, Jr., D.Roberts

Pion-Induced Pion Production on the Deuteron

NUCLEAR REACTIONS 2H(π+, π+π-p), (π-, π-π+n), E=256, 331, 450 MeV; measured σ(θ(π+)), σ(θ(π), E(π)); deduced pion induced pion production mechanism.

doi: 10.1103/PhysRevC.33.655
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1985BA09      Nucl.Phys. A436, 621 (1985)

C.J.Batty, E.Friedman, J.Lichtenstadt

Combined Analysis of Antiprotonic Atoms and Antiproton Elastic Scattering Data

ATOMIC PHYSICS 12C, 16O, S, 89Y; analyzed antiprotonic atom data; deduced transition shifts, widths.

NUCLEAR REACTIONS 12C(p-bar, p-bar), E=47 MeV; analyzed σ(θ); deduced antiprotonic atom potential parameters. Antiprotonic atom data input.

doi: 10.1016/0375-9474(85)90551-2
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1985GA02      Phys.Lett. 150B, 95 (1985)

D.Garreta, P.Birien, G.Bruge, A.Chaumeaux, D.M.Drake, S.Janouin, D.Legrand, M.C.Lemaire, B.Mayer, J.Pain, J.C.Peng, M.Berrada, J.P.Bocquet, E.Monnand, J.Mougey, P.Perrin, E.Aslanides, O.Bing, J.Lichtenstadt, A.I.Yavin

Search for Antiproton-Nucleus States with (p-bar, p) Reactions

NUCLEAR REACTIONS 12C, 63Cu, 209Bi(p-bar, pX), E=180 MeV; measured inclusive σ(θ, Ep); deduced no (p-bar)-nucleus states. Intranuclear cascade model.

doi: 10.1016/0370-2693(85)90146-7
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1985LI16      Phys.Rev. C32, 1096 (1985)

J.Lichtenstadt, A.I.Yavin, S.Janouin, P.Birien, G.Bruge, A.Chaumeaux, D.Drake, D.Garreta, D.Legrand, M.C.Lemaire, B.Mayer, J.Pain, J.C.Peng, M.Berrada, J.P.Bocquet, E.Monnand, J.Mougey, P.Perrin, E.Aslanides, O.Bing

Black Body Description of Antiproton-Nucleus Scattering

NUCLEAR REACTIONS 12C, 16,18O, 40Ca(p-bar, p-bar), E=180 MeV; 12C, 40Ca(p-bar, p-bar), E=47 MeV; analyzed σ(θ). 12C, 16,18O, 40Ca deduced black disk radii, diffuseness parameters. Fuzzy black disk model.

doi: 10.1103/PhysRevC.32.1096
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1984AL20      Phys.Lett. 144B, 337 (1984)

A.Altman, D.Ashery, E.Piasetzky, J.Lichtenstadt, A.I.Yavin, W.Bertl, L.Felawka, H.K.Walter, R.J.Powers, R.G.Winter, J.v.d.Pluym

Isotopic Effects in the (π±, 2N) Reactions on 16O and 18O

NUCLEAR REACTIONS 16,18O(π+, 2p), (π+, np), (π-, np), E=165 MeV; measured σ(θ1, θ2), ratio; deduced reaction mechanism.

doi: 10.1016/0370-2693(84)91273-5
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1984BA39      Phys.Lett. 142B, 241 (1984)

C.J.Batty, E.Friedman, J.Lichtenstadt

Optical Potentials for Low Energy Antiproton-Nucleus Interactions

ATOMIC PHYSICS C, O, S, Y; analyzed antiprotonic atom data; deduced model independent potentials. Optical model.

NUCLEAR REACTIONS 12C(p-bar, p-bar), E=47 MeV; analyzed data; deduced model independent potentials. Optical model.

doi: 10.1016/0370-2693(84)91190-0
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1984BO27      J.Phys.(Paris), Colloq.C4, 351 (1984); See 1984Bo51

J.D.Bowman, H.W.Baer, M.D.Cooper, N.S.P.King, H.S.Matis, E.Piasetzky, U.Sennhauser, J.Alster, A.Erell, J.Lichtenstadt, M.A.Moinester, F.Irom, Q.Ingram

A Dependence of the Excitation Energy, Width, and Cross Section of the Isovector Monopole Resonance


1984BO51      J.Phys.(Paris), Colloq.C-4, 351 (1984)

J.D.Bowman, H.W.Baer, M.D.Cooper, N.S.P.King, H.S.Matis, E.Piasetzky, U.Sennhauser, J.Alster, A.Erell, J.Lichtenstadt, M.A.Moinester, F.Irom, Q.Ingram

A Dependence of the Excitation Energy, Width, and Cross Section of the Isovector Monopole Resonance

NUCLEAR REACTIONS 40Ca, 60Ni, 90Zr, 120Sn, 140Ce, 208Pb(π-, π0), E=165 MeV; measured σ(E(π0), θ(π0)), σ(θ(π0)). 40Ca, 60Ni, 90Zr(π+, π0), E not given; measured not abstracted. 40Ca, 60Ni, 90Zr deduced GDR, isovector monopole resonance. RPA, DWIA analyses.


1984ER03      Phys.Rev.Lett. 52, 2134 (1984)

A.Erell, J.Alster, J.Lichtenstadt, M.A.Moinester, J.D.Bowman, M.D.Cooper, F.Irom, H.S.Matis, E.Piasetzky, U.Sennhauser, Q.Ingram

Properties of the Isovector Monopole and Other Giant Resonances in Pion Charge Exchange

NUCLEAR REACTIONS 40Ca, 60Ni, 90Zr, 120Sn, 140Ce, 208Pb(π+, π0), (π-, π0), E=165 MeV; measured σ(θ, E(π)). 40K, 40Sc, 60Co, 60Cu, 90Nb, 90Y, 120In, 120Sb, 140La, 140Pr, 208Bi, 208Tl deduced GDR, fragmentation, isovector monopole resonance. DWIA analysis, RPA wave functions.

doi: 10.1103/PhysRevLett.52.2134
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1984GA04      Phys.Lett. 135B, 266 (1984)

D.Garreta, P.Birien, G.Bruge, A.Chaumeaux, D.M.Drake, S.Janouin, D.Legrand, M.C.Mallet-Lemaire, B.Mayer, J.Pain, J.C.Peng, M.Berrada, J.P.Bocquet, E.Monnand, J.Mougey, P.Perrin, E.Aslanides, O.Bing, A.Erell, J.Lichtenstadt, A.I.Yavin

Scattering of Antiprotons from Carbon at 46.8 MeV

NUCLEAR REACTIONS 12C(p-bar, p-bar), (p-bar, p-bar'), E=46.8 MeV; calculated σ(E(p-bar)), σ(θ); deduced (p-bar)-carbon optical potential parameter limits.

doi: 10.1016/0370-2693(84)90388-5
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1984GA32      Phys.Lett. 149B, 64 (1984)

D.Garreta, P.Birien, G.Bruge, A.Chaumeaux, D.M.Drake, S.Janouin, D.Legrand, M.C.Lemaire, B.Mayer, J.Pain, J.C.Peng, M.Berrada, J.P.Bocquet, E.Monnand, J.Mougey, P.Perrin, E.Aslanides, O.Bing, J.Lichtenstadt, A.I.Yavin

Elastic Scattering of Antiprotons from Carbon, Calcium, and Lead at 180 MeV

NUCLEAR REACTIONS 12C, 40Ca, 208Pb(p-bar, p-bar), E=180 MeV; measured σ(θ); deduced potential parameters. Optical model analysis.

doi: 10.1016/0370-2693(84)91552-1
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1984HE02      Phys.Rev. C29, 97 (1984)

J.Heisenberg, J.Dawson, T.Milliman, O.Schwentker, J.Lichtenstadt, C.N.Papanicolas, J.Wise, J.S.McCarthy, N.Hintz, H.P.Blok

Excitation of Positive-Parity States in Electron Scattering from 90Zr

NUCLEAR REACTIONS 90Zr(e, e'), E=70-368 MeV; measured σ(θ), σ(E(e')); deduced g9/2 proton orbit radius. 90Zr levels deduced charge distribution, transition charge densities, M7 transition current density. DWBA analysis.

doi: 10.1103/PhysRevC.29.97
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1984MO03      Phys.Rev.Lett. 52, 1203 (1984)

M.A.Moinester, D.R.Gill, J.Vincent, D.Ashery, S.Levenson, J.Alster, A.Altman, J.Lichtenstadt, E.Piasetzky, K.A.Aniol, R.R.Johnson, H.W.Roser, R.Tacik, W.Gyles, B.Barnett, R.J.Sobie, H.P.Gubler

Isospin Dependence of Pion Absorption on Nucleon Pairs at T(π) = 65 MeV

NUCLEAR REACTIONS 3He(π+, 2p), (π-, np), E=65 MeV; measured pp-, pn-coin, σ(θp1, Ep2), σ(θn, Ep); deduced σ(reaction) ratio, isospin dependence.

doi: 10.1103/PhysRevLett.52.1203
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1984PA02      Phys.Rev.Lett. 52, 247 (1984)

C.N.Papanicolas, J.Heisenberg, J.Lichtenstadt, J.S.McCarthy, D.Goutte, J.M.Cavedon, B.Frois, M.Huet, P.Leconte, Phan Xuan Ho, S.Platchkov, I.Sick

Effective Charge of Neutron Quasiparticle Pairs in 206Pb and 204Pb

NUCLEAR REACTIONS 204,206,208Pb(e, e'), E=52-502 MeV; measured σ. 204,206,208Pb levels deduced transition charge densities, B(λ).

doi: 10.1103/PhysRevLett.52.247
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1984PI08      Phys.Rev.Lett. 53, 540 (1984)

E.Piasetzky, P.A.M.Gram, D.W.MacArthur, G.A.Rebka, Jr., C.A.Bordner, S.Hoibraten, E.R.Kinney, J.L.Matthews, S.A.Wood, D.Ashery, J.Lichtenstadt

Pion-Induced Pion Production on the Deuteron

NUCLEAR REACTIONS 2H(π-, π-π+n), E=256, 331 MeV; 2H(π+, π+π-p), E=256 MeV; measured double-pion production σ vs E(π), θ(π); deduced quasifree production on nucleon, (pion)(two-nucleon) bound system production upper limits.

doi: 10.1103/PhysRevLett.53.540
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1984PL02      Phys.Lett. 137B, 15 (1984)

M.A.Plum, R.A.Lindgren, J.Dubach, R.S.Hicks, R.L.Huffman, B.Parker, G.A.Peterson, J.Alster, J.Lichtenstadt, M.A.Moinester, H.Baer

Isoscalar and Isovector M4 Spin Transitions in 14C

NUCLEAR REACTIONS 14C(e, e'), E=100-300 MeV; measured σ(E(e')), transverse form factor. 14C levels deduced M4 spin transition density isoscalar, isovector amplitudes, σ(π+)/σ(π-). Pion data input.

doi: 10.1016/0370-2693(84)91096-7
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1983AL07      Phys.Rev.Lett. 50, 1187 (1983)

A.Altman, E.Piasetzky, J.Lichtenstadt, A.I.Yavin, D.Ashery, R.J.Powers, W.Bertl, L.Felawka, H.K.Walter, R.G.Winter, J.v.d.Pluym

Observation of a Quasideuteron Component in the Reaction 12C(π+, 2p)

NUCLEAR REACTIONS 12C(π+, 2p), E=165, 245 MeV; measured σ(θ1, θ2), σ(θ1, θ2, E2); deduced quasideuteron component, σ, reaction mechanism.

doi: 10.1103/PhysRevLett.50.1187
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1983HE21      Phys.Lett. 132B, 47 (1983)

F.W.Hersman, W.Bertozzi, T.N.Buti, J.M.Finn, C.Hyde-Wright, M.V.Hynes, J.Kelly, M.A.Kovash, S.Kowalski, J.Lichtenstadt, R.Lourie, B.Murdock, B.Pugh, F.N.Rad, C.P.Sargent, J.B.Bellicard

A Test of the Interacting Boson Approximation using Electron Scattering

NUCLEAR REACTIONS 154Gd(e, e'), E not given; measured σ(θ). 154Gd levels deduced electric quadrupole transition charge density linear dependence. Interacting boson approximation.

doi: 10.1016/0370-2693(83)90219-8
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1983LI07      Phys.Lett. 121B, 377 (1983)

J.Lichtenstadt, J.Alster, M.A.Moinester, J.Dubach, R.S.Hicks, G.A.Peterson, S.Kowalski

The Low Lying Levels of 7Li Studied by Electron Scattering

NUCLEAR REACTIONS 7Li(e, e), (e, e'), E=80-300 MeV; measured M1, M3, E2 form factors. Shell model interpretation.

doi: 10.1016/0370-2693(83)91181-4
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1983SC01      Phys.Rev.Lett. 50, 15 (1983)

O.Schwentker, J.Dawson, J.Robb, J.Heisenberg, J.Lichtenstadt, C.N.Papanicolas, J.Wise, J.S.McCarthy, L.T.van der Bijl, H.P.Blok

E2 Transition Densities and Proton Shell Structure in 88Sr, 89Y, and 90Zr

NUCLEAR REACTIONS 88Sr, 89Y, 90Zr(e, e'), E not given; measured σ(θ). 89Y, 90Zr levels deduced E2 transition charge densities. 88Sr levels deduced spectroscopic amplitudes, E2 transition charge densities. Fourier-Bessel expansion, RPA, broken pair calculations.

doi: 10.1103/PhysRevLett.50.15
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1982HE03      Phys.Rev. C25, 2292 (1982)

J.Heisenberg, J.Lichtenstadt, C.N.Papanicolas, J.S.McCarthy

Excitation of Low Lying Natural Parity Levels in 208Pb by Inelastic Electron Scattering

NUCLEAR REACTIONS 208Pb(e, e'), E=50-335 MeV; measured σ(E(e'), θ). 208Pb levels deduced transition charge, current densities. DWBA analysis.

doi: 10.1103/PhysRevC.25.2292
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1982PA05      Phys.Lett. 108B, 279 (1982)

C.N.Papanicolas, J.Heisenberg, J.Lichtenstadt, J.S.McCarthy, D.Goutte, J.M.Cavedon, B.Frois, M.Huet, P.Leconte, Phan Xuan Ho, S.Platchkov, I.Sick

Transition Charge Densities for the Lowest E5 Transitions in 208Pb

NUCLEAR REACTIONS 208Pb(e, e'), E not given; measured σ(θ) vs momentum transfer. 208Pb levels deduced transition charge densities.

doi: 10.1016/0370-2693(82)91192-3
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1982PI04      Phys.Lett. 114B, 414 (1982)

E.Piasetzky, A.Altman, J.Lichtenstadt, A.I.Yavin, D.Ashery, W.Bertl, L.Felawka, H.K.Walter, F.W.Schleputz, R.J.Powers, R.G.Winter, J.v.d.Pluym

Observation of the (π-, π-n) and (π+, π+p) Reactions at 165 MeV

NUCLEAR REACTIONS C, Fe, Bi(π-, π-n), (π+, π+p), E=165 MeV; measured σ(θπ, θn), σ(θπ, θp); deduced σ(quasifree) ratio.

doi: 10.1016/0370-2693(82)90082-X
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1982PI06      Phys.Rev. C26, 2702 (1982)

E.Piasetzky, A.Altman, J.Lichtenstadt, A.I.Yavin, D.Ashery, W.Bertl, L.Felawka, H.K.Walter, F.W.Schleputz, R.J.Powers, R.G.Winter, J.v.d.Pluym

Pion-Induced Nucleon Knockout Reactions on 16O and 18O

NUCLEAR REACTIONS 16,18O(π+, π+p), (π-, π-p), (π-, π-n), E=165 MeV; measured π+p-, π-p-, π-n-coin; deduced absorption, scattering channel coupling. Scintillator detector array, H216O, H218O targets.

doi: 10.1103/PhysRevC.26.2702
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1982SC08      Phys.Lett. 112B, 40 (1982)

O.Schwentker, J.Dawson, S.McCaffrey, J.Robb, J.Heisenberg, J.Lichtenstadt, C.N.Papanicolas, J.Wise, J.S.McCarthy, N.Hintz, H.P.Blok

Measurement of the Effective E5 Single-Particle Transition Densities in 89Y and 90Zr

NUCLEAR REACTIONS 89Y, 90Zr(e, e'), E not given; measured σ(θ) vs momentum transfer. 89Y, 90Zr level deduced effective E5 transition charge, current densities, configuration.

doi: 10.1016/0370-2693(82)90901-7
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1981PA04      Phys.Lett. 99B, 96 (1981)

C.N.Papanicolas, J.Heisenberg, J.Lichtenstadt, J.S.McCarthy

High Multipolarity Electroexcitations in 207Pb and 206Pb

NUCLEAR REACTIONS 206,207Pb(e, e'), E not given; measured σ(θ(e')), form factors. 206,207Pb deduced levels, E10 transition strength distribution.

doi: 10.1016/0370-2693(81)90958-8
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1980GO12      Phys.Rev.Lett. 45, 1618 (1980)

D.Goutte, J.B.Bellicard, J.M.Cavedon, B.Frois, M.Huet, P.Leconte, Phan Xuan Ho, S.Platchkov, J.Heisenberg, J.Lichtenstadt, C.N.Papanicolas, I.Sick

Determination of the Charge Density of the Octupole Vibration in 208Pb

NUCLEAR REACTIONS 208Pb(e, e'), E=502 MeV; measured σ(θ). 208Pb level deduced transition charge density.

doi: 10.1103/PhysRevLett.45.1618
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1980HA21      Phys.Lett. 93B, 213 (1980)

I.Hamamoto, J.Lichtenstadt, G.F.Bertsch

Core-Polarization Effects on the Magnetic Transitions in the 208Pb Region

NUCLEAR REACTIONS 208Pb(e, e'), E=50-355 MeV; calculated transverse form factors, magnetization current densities; deduced magnetic transition-strength reduction. Core polarization, DWBA, coupled channels treatment.

doi: 10.1016/0370-2693(80)90497-9
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1980HA45      Phys.Lett. B96, 249 (1980)

I.Hamamoto, J.Lichtenstadt, G.F.Bertsch

Reduction of Magnetic and Tranverse Electric Scattering Amplitudes in 207Pb by Core Polarization

NUCLEAR REACTIONS 207Pb(e, e'), E not given; calculated σ(θ) vs momentum transfer, transverse electric, magnetic form factors; deduced core polarization effects. Particle-hole model, zero-range interaction.

NUCLEAR STRUCTURE 207Pb; calculated transition current densities. Particle-hole model, zero-range interaction.

doi: 10.1016/0370-2693(80)90759-5
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1980LI04      Phys.Rev.Lett. 44, 858 (1980)

J.Lichtenstadt, C.N.Papanicolas, C.P.Sargent, J.Heisenberg, J.S.McCarthy

Investigation of Natural-Parity High-Spin States in 208Pb by (e, e') Reactions

NUCLEAR REACTIONS 208Pb(e, e'), E=70-335 MeV; measured reduced σ(θ). 208Pb deduced high-spin states, parity, configuration. DWBA analysis, Hartree-Fock wave functions.

doi: 10.1103/PhysRevLett.44.858
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1980PA09      Phys.Rev.Lett. 45, 106 (1980)

C.N.Papanicolas, J.Lichtenstadt, C.P.Sargent, J.Heisenberg, J.S.McCarthy

Suppression of the Transverse Scattering Amplitude in 207Pb

NUCLEAR REACTIONS 207Pb(e, e'), E not given; measured longitudinal, transverse form factors, σ(θ). 207Pb levels deduced transverse amplitude quenching.

doi: 10.1103/PhysRevLett.45.106
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1979LI13      Phys.Rev. C20, 497 (1979)

J.Lichtenstadt, J.Heisenberg, C.N.Papanicolas, C.P.Sargent, A.N.Courtemanche, J.S.McCarthy

High-Spin States of Jπ = 12-, 14- in 208Pb Studied by (e, e')

NUCLEAR REACTIONS 208Pb(e, e'), E=50-335 MeV; measured σ(E). 208Pb deduced levels, J, π. DWBA, Hartree-Fock single-particle wave functions.

doi: 10.1103/PhysRevC.20.497
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1979NA10      Nucl.Phys. A329, 127 (1979)

E.Navon, A.Marinov, J.Lichtenstadt, Ch.Drory, R.Benin, A.Knoll, J.Burde, M.Paul

Study of Isobaric Analogue States in 49Sc and Core Excited States in 49Ca

NUCLEAR REACTIONS 48Ca(p, p'), (p, p'), E=5.55-8.4 MeV; measured σ(Ep, θ) σ(Ep', θ). 49Sc deduced resonances L(p), J, π, Γp, Γp', S. Enriched target.

doi: 10.1016/0375-9474(79)90285-9
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1978LI05      Phys.Rev.Lett. 40, 1127 (1978)

J.Lichtenstadt, J.Heisenberg, C.N.Papanicolas, C.P.Sargent, A.N.Courtemanche, J.S.McCarthy

Observation of 12- Magnetic Spin States in 208Pb

NUCLEAR REACTIONS 208Pb(e, e'), E=50-335 MeV; measured σ(E). 208Pb deduced levels, J, π.

doi: 10.1103/PhysRevLett.40.1127
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1978LI27      Nucl.Phys. A311, 61 (1978)

J.Lichtenstadt, A.Marinov, M.Paul, J.Burde, S.Mordechai

Study of the 41K(d, p)42K Reaction

NUCLEAR REACTIONS 41K(d, p), E=10 MeV; measured σ(θ). 42K deduced levels, L, J, π, S. DWBA analysis. Enriched target.

doi: 10.1016/0375-9474(78)90502-X
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1978PA10      Phys.Rev.Lett. 41, 537 (1978)

C.N.Papanicolas, J.Heisenberg, J.Lichtenstadt, A.N.Courtemanche, J.S.McCarthy

Electron Scattering on 207Pb and the Induced Charge of the Neutron

NUCLEAR REACTIONS 207Pb(e, e'), E=50-320 MeV; measured σ(E). 207Pb levels deduced effective charges.

doi: 10.1103/PhysRevLett.41.537
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1977PA24      Nucl.Phys. A289, 94 (1977)

M.Paul, A.Marinov, J.Burde, C.Drory, J.Lichtenstadt, S.Mordechai, E.Navon

Particle-Hole States in 42K Studied by the 44Ca(d, α)43K Reaction

NUCLEAR REACTIONS 44Ca(d, α), E=11 MeV; measured σ(θ). 42K deduced levels, L, J, π. DWBA analysis. Enriched target.

doi: 10.1016/0375-9474(77)90523-1
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