NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = R.Lindgren Found 94 matches. 2021SU25 Nat.Phys. 17, 687 (2021), Erratum Nat.Phys. 18, 473 (2022) V.Sulkosky, C.Peng, J.Chen, A.Deur, S.Abrahamyan, K.A.Aniol, D.S.Armstrong, T.Averett, S.L.Bailey, A.Beck, P.Bertin, F.Butaru, W.Boeglin, A.Camsonne, G.D.Cates, C.-C.Chang, S.Choi, E.Chudakov, L.Coman, J.C.Cornejo, B.Craver, F.Cusanno, R.De Leo, C.W.de Jager, J.D.Denton, S.Dhamija, R.Feuerbach, J.M.Finn, S.Frullani, K.Fuoti, H.Gao, F.Garibaldi, O.Gayou, R.Gilman, A.Glamazdin, C.Glashausser, J.Gomez, J.-O.Hansen, D.Hayes, F.W.Hersman, D.W.Higinbotham, T.Holmstrom, T.B.Humensky, C.E.Hyde, H.Ibrahim, M.Iodice, X.Jiang, L.J.Kaufman, A.Kelleher, K.E.Keister, W.Kim, A.Kolarkar, N.Kolb, W.Korsch, K.Kramer, G.Kumbartzki, L.Lagamba, V.Laine, G.Laveissiere, J.J.Lerose, D.Lhuillier, R.Lindgren, N.Liyanage, H.-J.Lu, B.Ma, D.J.Margaziotis, P.Markowitz, K.R.McCormick, M.Meziane, Z.-E.Meziani, R.Michaels, B.Moffit, P.Monaghan, S.Nanda, J.Niedziela, M.Niskin, R.Pandolfi, K.D.Paschke, M.Potokar, A.Puckett, V.A.Punjabi, Y.Qiang, R.D.Ransome, B.Reitz, R.Roche, A.Saha, A.Shabetai, S.Sirca, J.T.Singh, K.Slifer, R.Snyder, P.Solvignon, R.Stringer, R.Subedi, W.A.Tobias, N.Ton, P.E.Ulmer, G.M.Urciuoli, A.Vacheret, E.Voutier, K.Wang, L.Wan, B.Wojtsekhowski, S.Woo, H.Yao, J.Yuan, X.Zhan, X.Zheng, L.Zhu Measurement of the generalized spin polarizabilities of the neutron in the low-Q2 region NUCLEAR REACTIONS 3He(polarized e-, e-), E=1.1-4.4 GeV; measured reaction products, Eβ, Iβ. 1NN; deduced transverse-transverse and longitudinal-transverse interference σ, generalized neutron spin polarizabilities. Comparison with chiral effective field theory calculations.
doi: 10.1038/s41567-021-01245-9
2014KA30 Phys.Rev.Lett. 113, 022502 (2014) J.Katich, X.Qian, Y.X.Zhao, K.Allada, K.Aniol, J.R.M.Annand, T.Averett, F.Benmokhtar, W.Bertozzi, P.C.Bradshaw, P.Bosted, A.Camsonne, M.Canan, G.D.Cates, C.Chen, J.-P.Chen, W.Chen, K.Chirapatpimol, E.Chudakov, E.Cisbani, J.C.Cornejo, F.Cusanno, M.M.Dalton, W.Deconinck, C.W.de Jager, R.De Leo, X.Deng, A.Deur, H.Ding, P.A.M.Dolph, C.Dutta, D.Dutta, L.El Fassi, S.Frullani, H.Gao, F.Garibaldi, D.Gaskell, S.Gilad, R.Gilman, O.Glamazdin, S.Golge, L.Guo, D.Hamilton, O.Hansen, D.W.Higinbotham, T.Holmstrom, J.Huang, M.Huang, H.F.Ibrahim, M.Iodice, X.Jiang, G.Jin, M.K.Jones, A.Kelleher, W.Kim, A.Kolarkar, W.Korsch, J.J.LeRose, X.Li, Y.Li, R.Lindgren, N.Liyanage, E.Long, H.-J.Lu, D.J.Margaziotis, P.Markowitz, S.Marrone, D.McNulty, Z.-E.Meziani, R.Michaels, B.Moffit, C.Munoz Camacho, S.Nanda, A.Narayan, V.Nelyubin, B.Norum, Y.Oh, M.Osipenko, D.Parno, J.C.Peng, S.K.Phillips, M.Posik, A.J.R.Puckett, Y.Qiang, A.Rakhman, R.D.Ransome, S.Riordan, A.Saha, B.Sawatzky, E.Schulte, A.Shahinyan, M.H.Shabestari, S.Sirca, S.Stepanyan, R.Subedi, V.Sulkosky, L.-G.Tang, A.Tobias, G.M.Urciuoli, I.Vilardi, K.Wang, Y.Wang, B.Wojtsekhowski, X.Yan, H.Yao, Y.Ye, Z.Ye, L.Yuan, X.Zhan, Y.Zhang, Y.-W.Zhang, B.Zhao, X.Zheng, L.Zhu, X.Zhu, X.Zong Measurement of the Target-Normal Single-Spin Asymmetry in Deep-Inelastic Scattering from the Reaction 3He ↑ (e, e')X
doi: 10.1103/PhysRevLett.113.022502
2014MO25 J.Phys.(London) G41, 105109 (2014) P.Monaghan, R.Shneor, R.Subedi, B.D.Anderson, K.Aniol, J.Annand, J.Arrington, H.B.Benaoum, F.Benmokhtar, P.Bertin, W.Bertozzi, W.Boeglin, J.P.Chen, S.Choi, E.Chudakov, C.Ciofi degli Atti, E.Cisbani, W.Cosyn, B.Craver, C.W.de Jager, R.J.Feuerbach, E.Folts, S.Frullani, F.Garibaldi, O.Gayou, S.Gilad, R.Gilman, O.Glamazdin, J.Gomez, O.Hansen, D.W.Higinbotham, T.Holmstrom, H.Ibrahim, R.Igarashi, E.Jans, X.Jiang, L.Kaufman, A.Kelleher, A.Kolarkar, E.Kuchina, G.Kumbartzki, J.J.LeRose, R.Lindgren, N.Liyanage, D.J.Margaziotis, P.Markowitz, S.Marrone, M.Mazouz, D.Meekins, R.Michaels, B.Moffit, H.Morita, S.Nanda, C.F.Perdrisat, E.Piasetzky, M.Potokar, V.Punjabi, Y.Qiang, J.Reinhold, B.Reitz, G.Ron, G.Rosner, J.Ryckebusch, A.Saha, B.Sawatzky, J.Segal, A.Shahinyan, S.Sirca, K.Slifer, P.Solvignon, V.Sulkosky, N.Thompson, P.E.Ulmer, G.M.Urciuoli, E.Voutier, K.Wang, J.W.Watson, L.B.Weinstein, B.Wojtsekhowski, S.Wood, H.Yao, X.Zheng, L.Zhu Measurement of the 12C(e, e'p)11B two-body breakup reaction at high missing momentum NUCLEAR REACTIONS 12C(E, E'P), E200-400 MeV; measured reaction products, Ep, Ip; deduced σ(θ, E). Comparison with WS+Glauber calculations.
doi: 10.1088/0954-3899/41/10/105109
2012FO06 Phys.Rev.Lett. 108, 092502 (2012) N.Fomin, J.Arrington, R.Asaturyan, F.Benmokhtar, W.Boeglin, P.Bosted, A.Bruell, M.H.S.Bukhari, M.E.Christy, E.Chudakov, B.Clasie, S.H.Connell, M.M.Dalton, A.Daniel, D.B.Day, D.Dutta, R.Ent, L.El Fassi, H.Fenker, B.W.Filippone, K.Garrow, D.Gaskell, C.Hill, R.J.Holt, T.Horn, M.K.Jones, J.Jourdan, N.Kalantarians, C.E.Keppel, D.Kiselev, M.Kotulla, R.Lindgren, A.F.Lung, S.Malace, P.Markowitz, P.McKee, D.G.Meekins, H.Mkrtchyan, T.Navasardyan, G.Niculescu, A.K.Opper, C.Perdrisat, D.H.Potterveld, V.Punjabi, X.Qian, P.E.Reimer, J.Roche, V.M.Rodriguez, O.Rondon, E.Schulte, J.Seely, E.Segbefia, K.Slifer, G.R.Smith, P.Solvignon, V.Tadevosyan S.Tajima, L.Tang, G.Testa, R.Trojer, V.Tvaskis, W.F.Vulcan, C.Wasko, F.R.Wesselmann, S.A.Wood, J.Wright, X.Zheng New Measurements of High-Momentum Nucleons and Short-Range Structures in Nuclei
doi: 10.1103/PhysRevLett.108.092502
2010FO09 Phys.Rev.Lett. 105, 212502 (2010) N.Fomin, J.Arrington, D.B.Day, D.Gaskell, A.Daniel, J.Seely, R.Asaturyan, F.Benmokhtar, W.Boeglin, B.Boillat, P.Bosted, A.Bruell, M.H.S.Bukhari, M.E.Christy, E.Chudakov, B.Clasie, S.H.Connell, M.M.Dalton, D.Dutta, R.Ent, L.El Fassi, H.Fenker, B.W.Filippone, K.Garrow, C.Hill, R.J.Holt, T.Horn, M.K.Jones, J.Jourdan, N.Kalantarians, C.E.Keppel, D.Kiselev, M.Kotulla, R.Lindgren, A.F.Lung, S.Malace, P.Markowitz, P.McKee, D.G.Meekins, T.Miyoshi, H.Mkrtchyan, T.Navasardyan, G.Niculescu, Y.Okayasu, A.K.Opper, C.Perdrisat, D.H.Potterveld, V.Punjabi, X.Qian, P.E.Reimer, J.Roche, V.M.Rodriguez, O.Rondon, E.Schulte, E.Segbefia, K.Slifer, G.R.Smith, P.Solvignon, V.Tadevosyan, S.Tajima, L.Tang, G.Testa, R.Trojer, V.Tvaskis, W.F.Vulcan, C.Wasko, F.R.Wesselmann, S.A.Wood, J.Wright, X.Zheng Scaling of the F2 Structure Function in Nuclei and Quark Distributions at χ > 1
doi: 10.1103/PhysRevLett.105.212502
2007SO06 Phys.Rev. C 75, 034611 (2007) D.S.Sorenson, J.L.Ullmann, A.Ling, B.K.Park, R.C.Haight, N.S.P.King, R.A.Lindgren, H.Baghaei, E.J.Stephenson, F.P.Brady, J.L.Romero, J.Rapaport, B.L.Clausen, C.Wuest, F.Sammarruca Limitations of the distorted-wave impulse approximation in describing the energy dependence of the 10B(n, p)10Be(g.s.) reaction NUCLEAR REACTIONS 10B(n, p), E=70240 MeV; measured σ(E, θ). Comparison with zero- and finite-range DWIA predictions.
doi: 10.1103/PhysRevC.75.034611
2005BE43 Phys.Rev. C 71, 064607 (2005) A.C.Betker, S.Chang, E.J.Stephenson, A.D.Bacher, S.M.Bowyer, W.A.Franklin, J.Liu, C.Olmer, D.L.Prout, S.P.Wells, S.W.Wissink, C.Yu, R.A.Lindgren, H.Baghaei, V.Gladyshev, J.A.Carr, S.K.Yoon, F.Petrovich, B.L.Clausen, J.Lisantti Reaction mechanism for natural parity (p, p') transitions in 10B NUCLEAR REACTIONS 10B(polarized p, p), (polarized p, p'), E=197 MeV; measured σ(E, θ), analyzing power, polarization transfer coefficients. Comparison with model predictions.
doi: 10.1103/PhysRevC.71.064607
2004RO35 Phys.Rev.Lett. 93, 182501 (2004) D.Rohe, C.S.Armstrong, R.Asaturyan, O.K.Baker, S.Bueltmann, C.Carasco, D.Day, R.Ent, H.C.Fenker, K.Garrow, A.Gasparian, P.Gueye, M.Hauger, A.Honegger, J.Jourdan, C.E.Keppel, G.Kubon, R.Lindgren, A.Lung, D.J.Mack, J.H.Mitchell, H.Mkrtchyan, D.Mocelj, K.Normand, T.Petitjean, O.Rondon, E.Segbefia, I.Sick, S.Stepanyan, L.Tang, F.Tiefenbacher, W.F.Vulcan, G.Warren, S.A.Wood, L.Yuan, M.Zeier, H.Zhu, B.Zihlmann, and the E97-006 Collaboration Correlated Strength in the Nuclear Spectral Function NUCLEAR REACTIONS 12C(e, e'p), E=3.3 GeV; measured Ep, electron spectra; deduced spectral function, correlated strength.
doi: 10.1103/PhysRevLett.93.182501
2002SC41 Phys.Rev. C66, 042201 (2002) E.C.Schulte, A.Afanasev, M.Amarian, K.Aniol, S.Becher, K.Benslama, L.Bimbot, P.Bosted, E.Brash, J.Calarco, Z.Chai, C.Chang, T.Chang, J.P.Chen, S.Choi, E.Chudakov, S.Churchwell, D.Crovelli, S.Dieterich, S.Dumalski, D.Dutta, M.Epstein, K.Fissum, B.Fox, S.Frullani, H.Gao, J.Gao, F.Garibaldi, O.Gayou, R.Gilman, A.Glamazdin, C.Glashausser, J.Gomez, V.Gorbenko, J.-O.Hansen, R.J.Holt, J.Hovdebo, G.M.Huber, C.W.de Jager, X.Jiang, C.Jones, M.K.Jones, J.Kelly, E.Kinney, E.Kooijman, G.Kumbartzki, M.Kuss, J.LeRose, M.Liang, R.Lindgren, N.Liyanage, S.Malov, D.Margaziotis, P.Markowitz, K.McCormick, D.Meekins, Z.-E.Meziani, R.Michaels, J.Mitchell, L.Morand, C.Perdrisat, R.Pomatsalyuk, V.Punjabi, A.Radyushkin, R.Ransome, R.Roche, M.Rvachev, A.Saha, A.Sarty, D.Simon, S.Strauch, R.Suleiman, L.Todor, P.Ulmer, G.M.Urciuoli, K.Wijesooriya, B.Wojtsekhowski, F.Xiong, W.Xu High energy angular distribution measurements of the exclusive deuteron photodisintegration reaction NUCLEAR REACTIONS 2H(γ, p), E=1.6, 1.9, 2.4 GeV; measured σ(θ), forward-backward asymmetry. Comparison with model predictions.
doi: 10.1103/PhysRevC.66.042201
2002UL01 Phys.Rev.Lett. 89, 062301 (2002) P.E.Ulmer, K.A.Aniol, H.Arenhovel, J.-P.Chen, E.Chudakov, D.Crovelli, J.M.Finn, K.G.Fissum, O.Gayou, J.Gomez, J.-O.Hansen, C.W.de Jager, S.Jeschonnek, M.K.Jones, M.Kuss, J.J.LeRose, M.Liang, R.A.Lindgren, S.Malov, D.Meekins, R.Michaels, J.Mitchell, C.F.Perdrisat, V.Punjabi, R.Roche, F.Sabatie, A.Saha, R.Suleiman, L.Todor, B.B.Wojtsekhowski 2H(e, e'p)n Reaction at High Recoil Momenta NUCLEAR REACTIONS 2H(e, e'p), E=3.110 GeV; measured Ep, σ vs recoil momentum. Comparison with model predictions.
doi: 10.1103/PhysRevLett.89.062301
2001AR12 Phys.Rev. C64, 014602 (2001) J.Arrington, C.S.Armstrong, T.Averett, O.K.Baker, L.de Bever, C.W.Bochna, W.Boeglin, B.Bray, R.D.Carlini, G.Collins, C.Cothran, D.Crabb, D.Day, J.A.Dunne, D.Dutta, R.Ent, B.W.Filippone, A.Honegger, E.W.Hughes, J.Jensen, J.Jourdan, C.E.Keppel, D.M.Koltenuk, R.Lindgren, A.Lung, D.J.Mack, J.McCarthy, R.D.McKeown, D.Meekins, J.H.Mitchell, H.G.Mkrtchyan, G.Niculescu, I.Niculescu, T.Petitjean, O.Rondon, I.Sick, C.Smith, B.Terburg, W.F.Vulcan, S.A.Wood, C.Yan, J.Zhao, B.Zihlmann x and ξ Scaling of the Nuclear Structure Function at Large x NUCLEAR REACTIONS 2H, C, Fe, 197Au(e, e'X), E=4.045 GeV; measured σ(E, θ), structure functions; deduced scaling features.
doi: 10.1103/PhysRevC.64.014602
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
2000HI06 Phys.Rev. C61, 054609 (2000) K.Hicks, V.Gladyshev, H.Baghaei, A.Caracappa, A.Cichocki, R.Deininger, R.Finlay, T.Gresko, S.Hoblit, M.Khandaker, O.Kistner, F.X.Li, R.Lindgren, M.Lucas, L.Miceli, B.Norum, J.Rapaport, A.Sandorfi, R.Sealock, L.C.Smith, C.Thorn, S.Thornton, C.S.Whisnant, D.Willits, L.E.Wright The 16O(γ(pol), π-p) Reaction at Eγ ≈ 300 MeV NUCLEAR REACTIONS 16O(polarized γ, π-p), E=290-325 MeV; measured σ(E, θ1, θ2), spin asymmetries. Comparison with DWIA results.
doi: 10.1103/PhysRevC.61.054609
1999AN43 Phys.Lett. 463B, 339 (1999) P.L.Anthony, R.G.Arnold, T.Averett, H.R.Band, M.C.Berisso, H.Borel, P.E.Bosted, S.L.Bultmann, M.Buenerd, T.Chupp, S.Churchwell, G.R.Court, D.Crabb, D.Day, P.Decowski, P.DePietro, R.Erbacher, R.Erickson, A.Feltham, H.Fonvieille, E.Frlez, R.Gearhart, V.Ghazikhanian, J.Gomez, K.A.Griffioen, C.Harris, M.A.Houlden, E.W.Hughes, C.E.Hyde-Wright, G.Igo, S.Incerti, J.Jensen, J.R.Johnson, P.M.King, Yu.G.Kolomensky, S.E.Kuhn, R.Lindgren, R.M.Lombard-Nelsen, J.Marroncle, J.McCarthy, P.McKee, W.Meyer, G.Mitchell, J.Mitchell, M.Olson, S.Penttila, G.Peterson, G.G.Petratos, R.Pitthan, D.Pocanic, R.Prepost, C.Prescott, L.M.Qin, B.A.Raue, D.Reyna, L.S.Rochester, S.Rock, O.A.Rondon-Aramayo, F.Sabatie, I.Sick, T.Smith, L.Sorrell, F.Staley, S.St.Lorant, L.M.Stuart, Z.Szalata, Y.Terrien, A.Tobias, L.Todor, T.Toole, S.Trentalange, D.Walz, R.C.Welsh, F.R.Wesselmann, T.R.Wright, C.C.Young, M.Zeier, H.Zhu, B.Zihlmann Measurement of the Deuteron Spin Structure Function g1d(x) for 1 (GeV/c)2 < Q2 < 40 (GeV/c)2 NUCLEAR REACTIONS 2H, 6Li(polarized e, e'X), E=48.3 GeV; measured electrons σ(θ), longitudinal asymmetries. 2H deduced spin structure function.
doi: 10.1016/S0370-2693(99)00940-5
1999AR07 Phys.Rev.Lett. 82, 2056 (1999) J.Arrington, C.S.Armstrong, T.Averett, O.K.Baker, L.de Bever, C.W.Bochna, W.Boeglin, B.Bray, R.D.Carlini, G.Collins, C.Cothran, D.Crabb, D.Day, J.A.Dunne, D.Dutta, R.Ent, B.W.Filippone, A.Honegger, E.W.Hughes, J.Jensen, J.Jourdan, C.E.Keppel, D.M.Koltenuk, R.Lindgren, A.Lung, D.J.Mack, J.McCarthy, R.D.McKeown, D.Meekins, J.H.Mitchell, H.G.Mkrtchyan, G.Niculescu, I.Niculescu, T.Petitjean, O.Rondon, I.Sick, C.Smith, B.Terburg, W.F.Vulcan, S.A.Wood, C.Yan, J.Zhao, B.Zihlmann Inclusive Electron-Nucleus Scattering at Large Momentum Transfer NUCLEAR REACTIONS C, Fe, 197Au(e, e'X), E=4.045 GeV; measured σ(E, θ); deduced scaling functions.
doi: 10.1103/PhysRevLett.82.2056
1997CL01 Phys.Rev. C55, 625 (1997) B.L.Clausen, T.W.Johnson, R.A.Lindgren, K.Cromer, R.J.Peterson, A.D.Bacher, H.Ward, A.L.Williams Pion Scattering to 6- Stretched States in 32S NUCLEAR REACTIONS 32S(π+, π+), (π-, π-'), E=162 MeV; measured spectra, σ(θ). 32S levels deduced spectroscopic factors, isoscalar, isovector magnetic structure coefficients.
doi: 10.1103/PhysRevC.55.625
1997HI01 Phys.Rev. C55, R12 (1997) K.Hicks, H.Baghaei, A.Caracappa, A.Cichocki, G.Davenport, R.Finlay, V.Gladyshev, T.Gresko, S.Hoblit, M.Khandaker, O.Kistner, F.X.Lee, R.Lindgren, M.Lucas, L.Miceli, B.Norum, J.Rapaport, A.Sandorfi, R.Sealock, L.C.Smith, C.Thorn, S.Thornton, C.S.Whisnant, L.E.Wright Spin Asymmetries from 16O(γ(pol), pπ-) Near Δ Resonance Energies NUCLEAR REACTIONS 16O(polarized γ, pπ-), E=293 MeV; measured spin asymmetry vs θp, θ(π); deduced Δ-nucleus potential, δ lifetime dependences.
doi: 10.1103/PhysRevC.55.R12
1997OF01 Phys.Rev. C55, 1295 (1997) B.G.Ofenloch, R.A.Giannelli, B.G.Ritchie, J.M.O'Donnell, J.N.Knudson, C.L.Morris, C.M.Kormanyos, A.Saunders, J.Z.Williams, R.A.Lindgren, B.L.Clausen Pion-Nucleus Spin-Flip Strength at Low and Resonance Energies NUCLEAR REACTIONS 10B(π+, π+'), E=65 MeV; measured σ(θ). 10B deduced isovector spin-flip strength parameter, B(λ). Other data analyzed.
doi: 10.1103/PhysRevC.55.1295
1997WE01 Phys.Rev. C55, 2773 (1997) J.Wesseling, C.W.de Jager, L.Lapikas, H.de Vries, L.W.Fagg, M.N.Harakeh, N.Kalantar-Nayestanaki, R.A.Lindgren, E.Moya De Guerra, P.Sarriguren 2s1/2 Occupancies in 30Si, 31P, and 32S NUCLEAR REACTIONS 30Si, 31P, 32S(e, e'), E=454.3 MeV; measured form factors; deduced charge distribution, level occupancies. Hartree-Fock calculation.
doi: 10.1103/PhysRevC.55.2773
1996AB02 Phys.Rev.Lett. 76, 587 (1996) K.Abe, T.Akagi, P.L.Anthony, R.Antonov, R.G.Arnold, T.Averett, H.R.Band, J.M.Bauer, H.Borel, P.E.Bosted, V.Breton, J.Button-Shafer, J.P.Chen, T.E.Chupp, J.Clendenin, C.Comptour, K.P.Coulter, G.Court, D.Crabb, M.Daoudi, D.Day, F.S.Dietrich, J.Dunne, H.Dutz, R.Erbacher, J.Fellbaum, A.Feltham, H.Fonvieille, E.Frlez, D.Garvey, R.Gearhart, J.Gomez, P.Grenier, K.A.Griffioen, S.Hoibraten, E.W.Hughes, C.Hyde-Wright, J.R.Johnson, D.Kawall, A.Klein, S.E.Kuhn, M.Kuriki, R.Lindgren, T.J.Liu, R.M.Lombard-Nelsen, J.Marroncle, T.Maruyama, X.K.Maruyama, J.McCarthy, W.Meyer, Z.-E.Meziani, R.Minehart, J.Mitchell, J.Morgenstern, G.G.Petratos, R.Pitthan, D.Pocanic, C.Prescott, R.Prepost, P.Raines, B.Raue, D.Reyna, A.Rijllart, Y.Roblin, L.S.Rochester, S.E.Rock, O.A.Rondon, I.Sick, L.C.Smith, T.B.Smith, M.Spengos, F.Staley, P.Steiner, S.St.Lorant, L.M.Stuart, F.Suekane, Z.M.Szalata, H.Tang, Y.Terrien, T.Usher, D.Walz, J.L.White, K.Witte, C.C.Young, B.Youngman, H.Yuta, G.Zapalac, B.Zihlmann, D.Zimmermann, and the E143 Collaboration Measurements of the Proton and Deuteron Spin Structure Function g2 and Asymmetry A2 NUCLEAR STRUCTURE 1,2H; analyzed data; deduced spin structure function, asymmetry data. Polarized ammonia targets, (polarized e, e') reaction. NUCLEAR REACTIONS 1,2H(polarized e, e'), E=29.1 GeV; measured spin asymmetries. 1,2H deduced spin structure functions. Polarized ammonia targets.
doi: 10.1103/PhysRevLett.76.587
1995AB02 Phys.Rev.Lett. 74, 346 (1995) K.Abe, T.Akagi, P.L.Anthony, R.Antonov, R.G.Arnold, T.Averett, H.R.Band, J.M.Bauer, H.Borel, P.E.Bosted, V.Breton, J.Button-Shafer, J.P.Chen, T.E.Chupp, J.Clendenin, C.Comptour, K.P.Coulter, G.Court, D.Crabb, M.Daoudi, D.Day, F.S.Dietrich, J.Dunne, H.Dutz, R.Erbacher, J.Fellbaum, A.Feltham, H.Fonvieille, E.Frlez, D.Garvey, R.Gearhart, J.Gomez, P.Grenier, K.A.Griffioen, S.Hoibraten, E.W.Hughes, C.Hyde-Wright, J.R.Johnson, D.Kawall, A.Klein, S.E.Kuhn, M.Kuriki, R.Lindgren, T.J.Liu, R.M.Lombard-Nelsen, J.Marroncle, T.Maruyama, X.K.Maruyama, J.McCarthy, W.Meyer, Z.-E.Meziani, R.Minehart, J.Mitchell, J.Morgenstern, G.G.Petratos, R.Pitthan, D.Pocanic, C.Prescott, R.Prepost, P.Raines, B.Raue, D.Reyna, A.Rijllart, Y.Roblin, L.S.Rochester, S.E.Rock, O.A.Rondon, I.Sick, L.C.Smith, T.B.Smith, M.Spengos, F.Staley, P.Steiner, S.St.Lorant, L.M.Stuart, F.Suekane, Z.M.Szalata, H.Tang, Y.Terrien, T.Usher, D.Walz, J.L.White, K.Witte, C.C.Young, B.Youngman, H.Yuta, G.Zapalac, B.Zihlmann, D.Zimmermann, and the E143 Collaboration Precision Measurement of the Proton Spin Structure Function g1(p) NUCLEAR REACTIONS 1H(polarized e, e'), E=9.7-29.1 GeV; measured asymmetry. 1H deduced spin structure function g1(p). Polarized 15NH3 target.
doi: 10.1103/PhysRevLett.74.346
1995AD01 Phys.Rev. C51, 17 (1995) G.S.Adams, H.Baghaei, A.Caracappa, W.Clayton, A.D'Angelo, S.Hoblit, M.Khandaker, O.C.Kistner, T.Kobayashi, R.Lindgren, L.Miceli, C.Ruth, A.M.Sandorfi, C.Schaerf, R.M.Sealock, L.C.Smith, P.Stoler, D.J.Tedeschi, C.E.Thorn, S.T.Thornton, K.Vaziri, C.S.Whisnant, E.J.Winhold Measurement of γ(pol)d → pnπ0 at Large Nucleon Momenta NUCLEAR REACTIONS 2H(polarized γ, nπ0), E=290 MeV; measured σ(θn, θp) vs neutron momentum; deduced beam asymmetries. Cascade Monte Carlo calculation.
doi: 10.1103/PhysRevC.51.17
1995SE02 Phys.Rev. C51, 1926 (1995) R.M.Sellers, D.M.Manley, M.M.Niboh, D.S.Weerasundara, R.A.Lindgren, B.L.Clausen, M.Farkhondeh, B.E.Norum, B.L.Berman Inelastic Electron Scattering from 18O at Backward Angles NUCLEAR REACTIONS 18O(e, e'), E=140.3-275.2 MeV; measured electron spectra, form factors. 18O levels deduced reduced transition probabilities, J, π, T.
doi: 10.1103/PhysRevC.51.1926
1994GA18 Phys.Rev. C50, 289 (1994) L.A.C.Garcia, B.D.Anderson, D.M.Manley, A.R.Baldwin, R.Pourang, E.Steinfelds, J.W.Watson, R.A.Lindgren, B.L.Clausen, A.D.Bacher, C.C.Foster Identification of 4- States in the 14C(p, n)14N Reaction at 135 MeV NUCLEAR REACTIONS 14C(p, n), E=135 MeV; measured neutron spectra, σ(E(n), θ=135°), σ(θ) vs momentum. 14N deduced levels, J, π, T, isovector transition strengths.
doi: 10.1103/PhysRevC.50.289
1994PE08 Phys.Rev. C49, 3000 (1994) M.Petraitis, J.P.Connelly, H.Crannell, L.W.Fagg, J.T.O'Brien, D.I.Sober, J.R.Deininger, S.E.Williamson, R.Lindgren, S.Raman Low-Multipolarity Magnetic Transitions in 30Si, 32S, and 34S Studied by 180° Electron Scattering NUCLEAR REACTIONS 30Si, 32,34S(e, e'), E=28.4-63.4 MeV; measured spectra, σ. 32,34S, 30Si deduced M1, M2 transition strength fragmentation features.
doi: 10.1103/PhysRevC.49.3000
1994RU04 Phys.Rev.Lett. 72, 617 (1994) C.Ruth, G.S.Adams, H.Baghaei, A.Caracappa, W.B.Clayton, A.D'Angelo, M.-A.Duval, G.Giordano, S.Hoblit, O.C.Kistner, J.M.Laget, R.Lindgren, G.Matone, L.Miceli, W.K.Mize, M.A.Moinester, A.M.Sandorfi, C.Schaerf, R.M.Sealock, L.C.Smith, P.Stoler, D.J.Tedeschi, P.K.Teng, C.E.Thorn, S.T.Thornton, K.Vaziri, C.S.Whisnant, E.J.Winhold First Measurement of the Reaction 3He(γ(pol), p)X with Polarized Photons NUCLEAR REACTIONS 3He(polarized γ, p), E=195-304 MeV; measured σ(θ), photon asymmetry vs proton momentum; deduced three-nucleon absorption evidence. Linear beam polarization.
doi: 10.1103/PhysRevLett.72.617
1994TE07 Phys.Rev.Lett. 73, 408 (1994) D.J.Tedeschi, G.S.Adams, G.Audit, H.Baghaei, A.Caracappa, W.B.Clayton, A.D'Angelo, M.A.Duval, G.Giordano, S.Hoblit, O.C.Kistner, J.M.Laget, R.Lindgren, G.Matone, L.Miceli, W.K.Mize, M.Moinester, C.Ruth, A.Sandorfi, C.Schaerf, R.M.Sealock, L.C.Smith, P.Stoler, P.K.Teng, C.E.Thorn, S.T.Thornton, K.Vaziri, C.S.Whisnant, E.J.Winhold Exclusive Photodisintegration of 3He with Polarized Photons NUCLEAR REACTIONS 3He(polarized γ, np), (polarized γ, 2p), E=235-305 MeV; measured σ(θ1, θ2, p1), asymmetry; deduced reaction mechanism.
doi: 10.1103/PhysRevLett.73.408
1993WA06 Phys.Rev. C47, 2123 (1993) L.Wang, X.Yang, J.Rapaport, C.D.Goodman, C.C.Foster, Y.Wang, R.A.Lindgren, E.Sugarbaker, D.Marchlenski, S.de Lucia, B.Luther, L.Rybarcyk, T.N.Taddeucci, B.K.Park 10B(p, n)10C Reaction at 186 MeV NUCLEAR REACTIONS 10B(p, n), (polarized p, n), E=186 MeV; measured σ(θn, En), analyzing power, polarization, polarization transfer. 10C deduced resonances, J, π, possible IAS character.
doi: 10.1103/PhysRevC.47.2123
1992BA76 Phys.Rev.Lett. 69, 2054 (1992) H.Baghaei, R.A.Lindgren, P.Slocum, E.J.Stephenson, A.D.Bacher, S.Chang, J.Lisantti, J.Liu, C.Olmer, S.Wells, S.W.Wissink, B.L.Clausen, J.A.Carr, S.K.Yoon, F.Petrovich Spin Transverse-Longitudinal Composition of the Isovector Effective NN Interaction from 10B(p(pol), p(pol)') at 200 MeV NUCLEAR REACTIONS 10B(polarized p, p), E=200 MeV; measured σ(θ), analyzing power, induced polarization, polarization transfer coefficients vs θ; deduced large transverse to longitudinal spin-dependent interaction ratio.
doi: 10.1103/PhysRevLett.69.2054
1992WE08 Nucl.Phys. A547, 519 (1992) J.Wesseling, C.W.de Jager, L.Lapikas, H.de Vries, M.N.Harakeh, N.Kalantar-Nayestanaki, L.W.Fagg, R.A.Lindgren, D.Van Neck Electron-Induced Proton Knock-Out from 30Si, 31P and 32S NUCLEAR REACTIONS 30Si, 31P, 32S(e, e'p), E=330, 454 MeV; measured excitation spectra at given central missing momentum. 30Si, 31P, 32S deduced rms radii, momentum distributions, l=0, 1, 2 transitions spectral functions, integrated knockout spectroscopic strength. Shell model, quasiparticle phonon model calculations.
doi: 10.1016/0375-9474(92)90036-J
1991LI35 Phys.Rev. C44, 2413 (1991) R.A.Lindgren, B.L.Clausen, G.S.Blanpied, J.Hernandez, C.S.Mishra, W.K.Mize, C.S.Whisnant, B.G.Ritchie, C.L.Morris, S.J.Seestrom-Morris, C.F.Moore, P.A.Seidl, B.H.Wildenthal, R.Gilman, J.A.Carr Pion Scattering to 6- Stretched States in 24Mg and 26Mg NUCLEAR REACTIONS 26,24Mg(π+, π+'), (π-, π-'), E=116-180 MeV; measured pion spectra, σ(θ). 26,24Mg levels deduced stretched configuration isoscalar, isovector strength.
doi: 10.1103/PhysRevC.44.2413
1990BL04 Phys.Rev. C41, 1625 (1990) G.S.Blanpied, J.Hernandez, C.S.Mishra, W.K.Mize, C.S.Whisnant, B.G.Ritchie, C.L.Morris, S.J.Seestrom-Morris, C.F.Moore, P.A.Seidl, R.A.Lindgren, B.H.Wildenthal, R.Gilman Pion Elastic and Inelastic Scattering from 24Mg and 26Mg NUCLEAR REACTIONS 26,24Mg(π+, π+'), (π-, π-'), E=150, 180 MeV; measured σ(θ), σ(E(π)). 26,24Mg levels deduced deformation parameters, neutron, proton matrix elements.
doi: 10.1103/PhysRevC.41.1625
1990CL02 Phys.Rev. C41, 2246 (1990) B.L.Clausen, J.T.Brack, M.R.Braunstein, J.J.Kraushaar, R.A.Loveman, R.J.Peterson, R.A.Ristinen, R.A.Lindgren, M.A.Plum Analysis of Pion Scattering to Stretched States in 60Ni and Other Nuclei using Woods-Saxon Wave Functions NUCLEAR REACTIONS 60Ni(π+, π+'), (π-, π-'), E=162 MeV; measured σ(θ). 14C, 28Si, 54Fe, 60Ni deduced stretched state parameters. Other data input.
doi: 10.1103/PhysRevC.41.2246
1990CL03 Phys.Rev.Lett. 65, 547 (1990) B.L.Clausen, R.A.Lindgren, M.Farkhondeh, L.W.Fagg, D.I.Sober, C.W.de Jager, H.de Vries, N.Kalantar-Nayestanaki, B.L.Berman, K.S.Dhuga, J.A.Carr, F.Petrovich, P.E.Burt Electroexcitation of 6- States in 32S NUCLEAR REACTIONS 32S(e, e'), E=207 MeV; measured σ(E(e')), form factors; deduced spectator nucleons role. 32S levels deduced extreme single particle model strengths. Stretched state transitions.
doi: 10.1103/PhysRevLett.65.547
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
1989SE01 Phys.Rev. C39, 749 (1989) R.E.Segel, A.Amusa, D.F.Geesaman, R.D.Lawson, B.Zeidman, C.Olmer, A.D.Bacher, G.T.Emery, C.W.Glover, H.Nann, W.P.Jones, S.Y.van der Werf, R.A.Lindgren Fragmentation of High-Spin Particle-Hole States in 26Mg NUCLEAR REACTIONS 26Mg(polarized p, p'), E=135 MeV; measured σ(θ), A(θ). 26Mg deduced levels, J, π. 28Si deduced levels, J, π, isoscalar, isovector excitation amplitudes. Other data input.
doi: 10.1103/PhysRevC.39.749
1988CL03 Phys.Rev. C38, 589 (1988) B.L.Clausen, R.J.Peterson, R.A.Lindgren Electron Scattering Form Factors of Stretched Transitions Using Woods-Saxon Wave Functions NUCLEAR REACTIONS 12,14C, 16O, 24,26Mg, 28Si, 48Ca, 54Fe, 58,60Ni, 90Zr, 208Pb(e, e'), E not given; calculated form factors; deduced single particle sum rule strength fractions.
doi: 10.1103/PhysRevC.38.589
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
1988HI02 Phys.Rev.Lett. 60, 905 (1988) R.S.Hicks, J.Button-Shafer, B.Debebe, J.Dubach, A.Hotta, R.L.Huffman, R.A.Lindgren, G.A.Peterson, R.P.Singhal, C.W.de Jager Determination of Single-Nucleon Wave Functions by Transverse Electron Scattering NUCLEAR REACTIONS 10,11B(e, e), 10B(e, e'), E=203-416 MeV; measured form factors. 10B deduced 1p3/2 wave function radial shape.
doi: 10.1103/PhysRevLett.60.905
1988SO07 Phys.Rev. C38, 654 (1988) D.I.Sober, L.W.Fagg, B.Zeidman, R.D.Lawson, D.F.Geesaman, G.C.Morrison, O.Karban, X.K.Maruyama, H.de Vries, E.A.J.M.Offermann, C.W.de Jager, R.A.Lindgren, J.F.A.van Hienen Electroexcitation of 8- States in 52Cr NUCLEAR REACTIONS 52Cr(e, e'), E=170-260 MeV; measured σ(E(e')), θ=115°, 154°. 52Cr deduced B(M8), total T=2, T=3 strengths, sums for M8 transitions. Shell model.
doi: 10.1103/PhysRevC.38.654
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
1987HI09 Phys.Rev. C36, 485 (1987) R.S.Hicks, R.L.Huffman, R.A.Lindgren, G.A.Peterson, M.A.Plum, J.Button-Shafer Electroexcitation of Discrete Levels in 12C and High Momentum Transfers NUCLEAR REACTIONS 12,13C(e, e'), E=80-485 MeV; measured σ(E(e'), θ). 13,12C levels deduced transverse excitation form factors. Enriched 13C target. Shell model.
doi: 10.1103/PhysRevC.36.485
1987LI30 Can.J.Phys. 65, 666 (1987) R.A.Lindgren, M.Leuschner, B.L.Clausen, R.J.Peterson, M.A.Plum, F.Petrovich Isovector Excitation of 1(h-bar x Omega) Stretched States in Nuclei: Effects of meson exchange currents, unbound wave functions, and knockout exchange amplitudes on the extraction of particle-hole strengths NUCLEAR REACTIONS 14C, 26Mg, 28Si, 54Fe, 60Ni(e, e'), E ≈ 136-205 MeV; analyzed σ(E(e'), θ(e')). 14C, 26Mg, 28Si, 54Fe, 60Ni deduced form factors, particle-hole strengths, amplitudes, B(λ). Meson exchange currents.
doi: 10.1139/p87-095
1987PE03 Phys.Rev. C35, 495 (1987) R.J.Peterson, B.L.Clausen, J.J.Kraushaar, R.A.Lindgren, M.A.Plum, W.W.Jacobs, H.Nann Proton Stripping to 8- Stretched States in 60Ni NUCLEAR REACTIONS 59Co(α, t), E=80.9 MeV; measured σ(θ). 60Ni deduced levels, J, π, T, spectroscopic factors. Magnetic spectrometer. DWBA analyses.
doi: 10.1103/PhysRevC.35.495
1986HI06 Phys.Rev. C34, 1161 (1986) R.S.Hicks, R.A.Lindgren, M.A.Plum, G.A.Peterson, H.Crannell, D.I.Sober, H.A.Thiessen, D.J.Millener M4 Excitations in 13C NUCLEAR REACTIONS 13C(e, e'), E=78-338 MeV; measured σ(E, θ). 13C levels deduced from factors, isoscalar, isovector transition amplitudes. Shell model.
doi: 10.1103/PhysRevC.34.1161
1986PE01 Phys.Rev. C33, 31 (1986) R.J.Peterson, B.L.Clausen, J.J.Kraushaar, H.Nann, W.W.Jacobs, R.A.Lindgren, M.A.Plum Proton Stripping to 6- Stretched States of 26Al NUCLEAR REACTIONS 24,25Mg(α, t), E=80.9 MeV; measured σ(Et), σ(θ). 26Al deduced levels, J, π, T, spectroscopic factors, stretched transition characteristics.
doi: 10.1103/PhysRevC.33.31
1984BU06 Phys.Rev. C29, 713 (1984) P.E.Burt, L.W.Fagg, H.Crannell, D.I.Sober, W.Stapor, J.T.O'Brien, J.W.Lightbody, X.K.Maruyama, R.A.Lindgren, C.P.Sargent Low Multipolarity Magnetic Transitions in 32S Excited by Electron Scattering NUCLEAR REACTIONS 32S(e, e'), E=34-74 MeV; measured σ(θ). 32S levels deduced transition form factors, multipolarity, B(M1), Γ.
doi: 10.1103/PhysRevC.29.713
1984GE06 Phys.Rev. C30, 952 (1984) D.F.Geesaman, R.D.Lawson, B.Zeidman, G.C.Morrison, A.D.Bacher, C.Olmer, G.R.Burleson, W.B.Cottingame, S.J.Greene, R.L.Boudrie, C.L.Morris, R.A.Lindgren, W.H.Kelly, R.E.Segel, L.W.Swenson Quenching of Isoscalar Spin-Flip Strength in 54Fe NUCLEAR REACTIONS 54Fe(π+, π+'), (π-, π-'), E=162 MeV; measured σ(θ), σ(E(π)). 54Fe levels deduced isoscalar, isovector strengths.
doi: 10.1103/PhysRevC.30.952
1984HI06 Phys.Rev. C30, 1 (1984) R.S.Hicks, J.B.Flanz, R.A.Lindgren, G.A.Peterson, L.W.Fagg, D.J.Millener Magnetic Multipole Excitations in 12C by Inelastic Electron Scattering NUCLEAR REACTIONS 12C(e, e'), E=50.7-338 MeV; measured σ(E(e')), θ=180°, form factors. 12C deduced resonances, J, π, Γ. Shell model comparison.
doi: 10.1103/PhysRevC.30.1
1984LI25 J.Phys.(Paris), Colloq.C-4, 433 (1984) Stretched Excitations as a Means to Study the Spin Modes of the Nucleus with Electromagnetic and Hadronic Probes NUCLEAR REACTIONS 51V, 50Ti, 52Cr, 54Fe(e, e'), (p, p'), E not given; analyzed B(M1) data. 12,13,14C, 14N(e, e'), E=196.5-225 MeV; analyzed σ(Ee', θe'). 12,14C, 14N, 16O, 24,26Mg, 28Si, 48Ca, 54Fe, 58Ni, 90Zr, 208Pb(e, e'), E not given; analyzed σ(Ee', θe'). 12,14C, 14N, 16O, 24,26Mg, 28Si, 48Ca, 54Fe, 58Ni, 90Zr, 208Pb deduced stretched states spectroscopic strength, transverse factors.
1984MI14 Nucl.Phys. A430, 189 (1984) H.Miessen, H.Rothhaas, G.Luhrs, G.A.Peterson, R.S.Hicks, R.A.Lindgren, B.L.Berman, S.Kowalski, C.F.Williamson Elastic Magnetic Electron Scattering from 29Si and 31P NUCLEAR REACTIONS 29Si, 31P(e, e), E=90-280 MeV; measured transverse electric σ(θ) vs E, form factors. 29Si, 31P deduced radial current densities, occupation probabilities, 2s1/2 neutron, proton orbitals. Enriched 29Si, natural 31P targets. Particle-core coupling, shell model interpretations.
doi: 10.1016/0375-9474(84)90200-8
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
1983SI11 Phys.Rev. C28, 513 (1983) R.P.Singhal, J.Dubach, R.S.Hicks, R.A.Lindgren, B.Parker, G.A.Peterson Electron Scattering at 180° from the ' Single-Hole ' States in 15N NUCLEAR REACTIONS 15N(e, e), (e, e'), E=70-327 MeV; measured σ(E, θ). 15N levels deduced form factors. Shell, core polarization models comparison.
doi: 10.1103/PhysRevC.28.513
1982BU05 Phys.Rev. C25, 2805 (1982) P.E.Burt, L.W.Fagg, H.Crannell, D.I.Sober, W.Stapor, J.T.O'Brien, X.K.Maruyama, J.W.Lightbody, R.A.Lindgren Electron Scattering Study of the 10.32 MeV Transition in 40Ca NUCLEAR REACTIONS 40Ca(e, e'), E=31-65 MeV; measured σ(θ), σ(E(e')), form factors. 40Ca transition deduced B(M1), Γ.
doi: 10.1103/PhysRevC.25.2805
1982HI07 Phys.Rev. C26, 339 (1982) R.S.Hicks, J.Dubach, R.A.Lindgren, B.Parker, G.A.Peterson Elastic Magnetic Scattering of Electrons from 13C NUCLEAR REACTIONS 13C(e, e), E=80-338 MeV; measured σ(E, θ). 13C deduced M1 form factor. Shell model.
doi: 10.1103/PhysRevC.26.339
1982HI10 Phys.Rev. C26, 920 (1982) R.S.Hicks, R.L.Huffman, R.A.Lindgren, B.Parker, G.A.Peterson, S.Raman, C.P.Sargent Inelastic Electron Scattering from 208Pb at 180° NUCLEAR REACTIONS 208Pb(e, e'), E=40.5, 50.4, 60.3, 75.2 MeV; measured σ(θ=180°). 208Pb deduced levels, transverse form factors. Enriched target, magnetic spectrometer.
doi: 10.1103/PhysRevC.26.920
1981LI05 Phys.Rev.Lett. 46, 706 (1981) R.A.Lindgren, J.B.Flanz, R.S.Hicks, B.Parker, G.A.Peterson, R.D.Lawson, W.Teeters, C.F.Williamson, S.Kowalski, X.K.Maruyama Comparison of Inelastic Electron Scattering with [g9/2 x (f1/2-3)(J)] (8)- Shell-Model Calculations for the T=1 and T=2, 8-States in 54Fe NUCLEAR REACTIONS 54Fe(e, e'), E=205.1 MeV; measured σ(E(e')), form factors. 54Fe levels deduced J, π, T, γ-multipolarity, B(M8) strength distribution. Shell model calculations.
doi: 10.1103/PhysRevLett.46.706
1981LI19 Phys.Rev.Lett. 47, 1266 (1981) R.A.Lindgren, M.A.Plum, W.J.Gerace, R.S.Hicks, B.Parker, G.A.Peterson, R.Singhal, C.F.Williamson, X.K.Maruyama, F.Petrovich Isospin Splitting of Isovector High-Spin ' Stretched ' Particle-Hole Excitations in Non-Self-Conjugate Nuclei NUCLEAR REACTIONS 60Ni(e, e'), E=205 MeV; measured σ(θ(e), E(e)). 60Ni deduced levels, J, π, T, B(M8), isospin splitting. Lane model parametrization, stretched particle-hole excitations. NUCLEAR STRUCTURE 13C, 15N, 54,56Fe, 58,60Ni; calculated isospin splitting. Lane model parametrization, stretched particle-hole excitation.
doi: 10.1103/PhysRevLett.47.1266
1980JO03 Phys.Rev. C21, 1162 (1980) E.C.Jones, Jr., W.L.Bendel, L.W.Fagg, R.A.Lindgren Magnetic Electron Scattering from Deuterium at Low-Momentum Transfer NUCLEAR REACTIONS 2H(e, e'), E=56.4 MeV; measured σ. 2H deduced magnetic form factor.
doi: 10.1103/PhysRevC.21.1162
1979AN01 Nucl.Phys. A313, 445 (1979) N.Anantaraman, H.E.Gove, R.A.Lindgren, J.Toke, J.P.Trentelman, J.P.Draayer, F.C.Jundt, G.Guillaume Alpha-Particle Strengths from the 16O(6Li, d)20Ne Reaction NUCLEAR REACTIONS 16O(6Li, d), E=20, 32, 38 MeV; measured σ(Ed, θ). 20Ne levels deduced Sα. DWBA analysis. Natural target.
doi: 10.1016/0375-9474(79)90512-8
1979EN01 Phys.Rev. C19, 569 (1979) N.Ensslin, L.W.Fagg, R.A.Lindgren, W.L.Bendel, E.C.Jones, Jr. Inelastic Electron Scattering from 14N at 180° NUCLEAR REACTIONS 14N(e, e'), E=40.6, 50.6, 60.2 MeV; measured σ(E), θ=180°; deduced Γ0, multipolarities.
doi: 10.1103/PhysRevC.19.569
1979FL08 Phys.Rev.Lett. 43, 1922 (1979) J.B.Flanz, R.S.Hicks, R.A.Lindgren, G.A.Peterson, J.Dubach, W.C.Haxton Electron Scattering, Isospin Mixing, and the Structure of the 12.71- and 15.11-MeV Levels in 12C NUCLEAR REACTIONS 12C(e, e'), E not given; measured form factors at θ=180°; deduced charge-dependent isospin-mixing matrix element. 12C levels deduced isospin mixing, structure.
doi: 10.1103/PhysRevLett.43.1922
1979JO02 Phys.Rev. C19, 610 (1979) E.C.Jones, Jr., W.L.Bendel, L.W.Fagg, R.A.Lindgren 180° Electron Scattering from 3He NUCLEAR REACTIONS 3He(e, e'), E=40, 51, 61 MeV; measured σ(E, 180°); deduced magnetic radius.
doi: 10.1103/PhysRevC.19.610
1979LI06 Phys.Rev.Lett. 42, 1524 (1979) R.A.Lindgren, W.J.Gerace, A.D.Bacher, W.G.Love, F.Petrovich Tensor Force and Inelastic Electron and Proton Scattering to Unnatural-Parity States of Stretched Configurations NUCLEAR STRUCTURE 12C, 16O, 24Mg, 28Si, 58Ni, 208Pb; analyzed(e, e'), (p, p') transitions involving unnatural parity states; deduced high-momentum components of tensor term of nucleon-nucleon force.
doi: 10.1103/PhysRevLett.42.1524
1978FL09 Phys.Rev.Lett. 41, 1642 (1978) J.B.Flanz, R.S.Hicks, R.A.Lindgren, G.A.Peterson, A.Hotta, B.Parker, R.C.York Convection Currents and Spin Magnetization in E2 Transitions of 12C NUCLEAR REACTIONS 12C(e, e'); measured square of electromagnetic form factors; 12C 4.439-MeV level deduced contribution of nuclear convection currents. 12C 16.107-MeV level deduced spin magnetization contributions.
doi: 10.1103/PhysRevLett.41.1642
1978LI02 Phys.Rev.Lett. 40, 504 (1978) R.A.Lindgren, C.F.Williamson, S.Kowalski Fragmentation of Isovector M8 Strength in 58Ni NUCLEAR REACTIONS 58Ni(e, e), E=153.6, 167.6, 172.2, 196.3, 221.0, 228.1, 242.6, 263.9 MeV; measured σ(E). 58Ni deduced levels, form factors, M8 strength.
doi: 10.1103/PhysRevLett.40.504
1978LI25 Phys.Rev.Lett. 41, 1705 (1978) R.A.Lindgren, J.B.Franz, W.J.Gerace, R.S.Hicks, A.Hotta, D.Huse, G.A.Peterson, R.C.York, C.F.Williamson, S.Kowalski Isoscalar Character of the Jπ = 6+, E(x) = 5.125 MeV State in 58Ni NUCLEAR REACTIONS 58Ni(e, e'), E=189.6-251.1 MeV; measured σ(E, θ). 58Ni 5.12-MeV level deduced transverse, longitudinal form factors, configuration.
doi: 10.1103/PhysRevLett.41.1705
1977FA02 Phys.Rev. C15, 1181 (1977) L.W.Fagg, R.A.Lindgren, W.L.Bendel, E.C.Jones, Jr. Form Factor for the Electroexcitation of the 5.36 MeV Transition in 6Li NUCLEAR REACTIONS 6Li(e, e'), E=40.5, 50.5 MeV; measured σ. 6Li level deduced form factors.
doi: 10.1103/PhysRevC.15.1181
1977FA05 Phys.Rev. C16, 923 (1977) L.W.Fagg, W.L.Bendel, R.A.Lindgren, E.C.Jones, Jr. Transitions in 27Al Excited by 180° Electron Scattering NUCLEAR REACTIONS 27Al(e, e'), E=37.3, 50.9, 60.5 MeV; measured σ(E). 27Al transitions deduced λ, Γ.
doi: 10.1103/PhysRevC.16.923
1977FU03 Nucl.Phys. A284, 329 (1977) H.W.Fulbright, C.L.Bennett, R.A.Lindgren, R.G.Markham, S.C.McGuire, G.C.Morrison, U.Strohbusch, J.Toke Four-Nucleon Transfer via the (6Li, d) Reaction NUCLEAR REACTIONS 40,42,44,48Ca, 50Ti, 50,52,54Cr, 54,56Fe, 58,60,62Ni, 90Zr(6Li, d), E=28-38 MeV; measured σ(Ed, θ). 44Ti, 54,58,56Fe, 58,60Ni, 62,64,66Zn deduced levels, Sα, L, J, π. DWBA analysis.
doi: 10.1016/0375-9474(77)90127-0
1977ZA02 Phys.Rev.Lett. 38, 750 (1977) H.Zarek, B.O.Pich, T.E.Drake, D.J.Rowe, W.Bertozzi, C.Creswell, A.Hirsch, M.V.Hynes, S.Kowalski, B.Norum, F.N.Rad, C.P.Sargent, C.F.Williamson, R.A.Lindgren Discovery of a 6-, T = 1 Resonance in 24Mg via High-Resolution Inelastic Electron Scattering NUCLEAR REACTIONS 24Mg(e, e'), E=108-260 MeV; measured spectra. 24Mg deduced resonance, J, π, t.
doi: 10.1103/PhysRevLett.38.750
1976BO24 Phys.Rev. C14, 4 (1976) R.N.Boyd, D.Elmore, W.P.Alford, J.P.Draayer, R.A.Lindgren Levels in 28Si via the 26Mg(3He, n) Reaction NUCLEAR REACTIONS 26Mg(3He, n), E=15 MeV; measured σ(En, θ). 28Si levels deduced S. DWBA analysis.
doi: 10.1103/PhysRevC.14.4
1976FA13 Phys.Rev. C14, 1727 (1976) L.W.Fagg, R.A.Lindgren, W.L.Bendel, E.C.Jones, Jr. Transitions Excited in 10B by 180° Electron Scattering NUCLEAR REACTIONS 10B(e, e'), E=40-61 MeV; measured σ(E). 10B levels deduced Γ0, λ.
doi: 10.1103/PhysRevC.14.1727
1976LI23 Phys.Rev. C14, 1789 (1976) R.A.Lindgren, W.L.Bendel, E.C.Jones, Jr., L.W.Fagg, X.K.Maruyama, L.W.Lightbody, Jr., S.P.Fivozinsky Electroexcitation of the T(0) + 1 Giant M1 Resonance in 58,60Ni NUCLEAR REACTIONS 58,60Ni(e, e'), E=40, 50, 60, 75 MeV; measured σ(E). 58,60Ni deduced levels, J, π, T, B(M1).
doi: 10.1103/PhysRevC.14.1789
1975AL05 Nucl.Phys. A243, 269 (1975) W.P.Alford, R.A.Lindgren, D.Elmore, R.N.Boyd Jπ = 0+ States in the (fp) Shell Excited in the (3He, n) Reaction NUCLEAR REACTIONS 46,48,50Ti, 50,52,54Cr, 54,56,58Fe, 58,60,62,64Ni(3He, n), E=15 MeV; measured σ(θ, En). 48,50,52Cr, 52,54,56Fe, 56,58,60Ni, 60,62,64,66Zn levels deduced J, π, L, S. DWBA analysis, model comparison. Enriched targets.
doi: 10.1016/0375-9474(75)90248-1
1975FU02 Phys.Lett. 53B, 449 (1975) H.W.Fulbright, U.Strohbusch, R.G.Markham, R.A.Lindgren, G.C.Morrison, S.C.McGuire, C.L.Bennett (6Li, d) Spectroscopy in the f-p Shell NUCLEAR REACTIONS 40,42,44,48Ca, 50Ti, 52Cr, 54,56Fe, 58,60,62Ni, 90Zr(6Li, d), E=28, 32 MeV; measured σ(Ed, θ). 58Ni levels deduced J.
doi: 10.1016/0370-2693(75)90215-4
1975LI19 Phys.Rev.Lett. 35, 1423 (1975) R.A.Lindgren, W.L.Bendel, L.W.Fagg, E.C.Jones, Jr. Evidence for Giant M2 States in 208Pb NUCLEAR REACTIONS 208Pb(e, e'), E=37.5, 40.5, 50.5, 60.5 MeV; measured σ(E, Ee'). 208Pb resonances deduced J, π.
doi: 10.1103/PhysRevLett.35.1423
1975UB01 Acta Phys.Austr. 41, 341 (1975) H.Uberall, A.Nagl, R.A.Lindgren, L.W.Fagg Giant Multipole Spin Flip Resonances and Spin Flip Sum Rules NUCLEAR REACTIONS 20Ne, 24Mg, 58Ni(e, e'), E=60 MeV; 12C, 24Mg, 58Ni(e, e'), E=100, 200, 300 MeV; calculated σ. 12C, 24Mg, 58Ni calculated E2 spin flip strengths.
1974AL14 Phys.Rev. C10, 1013 (1974) W.P.Alford, R.A.Lindgren, D.Elmore, R.N.Boyd Structure of 42Ti from the 40Ca(3He, n)42Ti Reaction NUCLEAR REACTIONS 40Ca(3He, n), E=15 MeV; measured σ(En, θ). 42Ti deduced levels, J, π, L, analogs. DWBA analysis.
doi: 10.1103/PhysRevC.10.1013
1974LI01 Phys.Lett. 48B, 209 (1974) R.A.Lindgren, R.G.Markham, H.W.Fulbright The 6Li-Induced Three-Nucleon Transfer Reaction on 40Ca NUCLEAR REACTIONS 40Ca(6Li, 3He), (6Li, t), E=34.0, 36.0 MeV; measured σ(E(3He), E(3H), θ). 43Sc, 43Ti deduced levels, L, J, π, S.
doi: 10.1016/0370-2693(74)90012-4
1974LI02 Phys.Lett. 49B, 263 (1974) R.A.Lindgren, J.P.Trentelman, N.Anantaraman, H.E.Gove, J.C.Jundt Odd-Parity Levels Excited in 32S and 36Ar via 'Alpha-Particle' Transfer NUCLEAR REACTIONS 28Si, 32S(6Li, d), E=32 MeV; measured σ(Ed). 32S, 36Ar deduced levels, J, π.
doi: 10.1016/0370-2693(74)90429-8
1974MA43 Phys.Rev. C10, 2257 (1974); Erratum Phys.Rev. C17, 856 (1978) X.K.Maruyama, R.A.Lindgren, W.L.Bendel, E.C.Jones, Jr., L.W.Fagg Excitation of M1 and M2 States in 22Ne by 183° Electron Scattering NUCLEAR REACTIONS 22Ne(e, e'), E=37, 50, 60 MeV; measured σ(Ee'). 22Ne levels deduced J, π, B(λ).
doi: 10.1103/PhysRevC.10.2257
1973AL23 Phys.Lett. 46B, 356 (1973) W.P.Alford, R.A.Lindgren, D.Elmore, R.N.Boyd Two-Particle, Two-Hole Jπ = 0+ States in 40Ca NUCLEAR REACTIONS 38Ar(3He, n), E=15 MeV; measured σ(En, θ). 40Ca deduced levels, J, π.
doi: 10.1016/0370-2693(73)90138-X
1973PA14 Phys.Rev. C8, 1557 (1973); Erratum Phys.Rev. C9, 1673 (1974) Y.S.Park, A.Niiler, R.A.Lindgren Spectroscopy of 10B Levels from the 9Be(d, n)10B Reaction NUCLEAR REACTIONS 9Be(d, n), E=7, 12, 15, 16 MeV; measured σ(E;En, θ). 10B deduced levels, J, π, L, S.
doi: 10.1103/PhysRevC.8.1557
1972AL48 Phys.Lett. 42B, 60 (1972) W.P.Alford, R.A.Lindgren, D.Elmore A Comparison of (3He, n) Ground-State Transitions in the (fp) Shell with Predictions of the Pairing Vibrational Model NUCLEAR REACTIONS 46Ti, 54Fe, 58Ni(3He, n), E=15 MeV; measured σ(θ).
doi: 10.1016/0370-2693(72)90716-2
1972LI02 Nucl.Phys. A180, 1 (1972) R.A.Lindgren, R.G.Hirko, J.G.Pronko, A.J.Howard, M.W.Sachs, D.A.Bromley A Study of 23Na NUCLEAR REACTIONS 23Na(α, α'γ), 26Mg(p, αγ), Eα=16.85 MeV, Ep=14.25 MeV; measured αγ(θ), pγ(θ), Iγ. 23Na levels deduced J, branching, multipole mixing ratios. Enriched 26Mg target.
doi: 10.1016/0375-9474(72)90152-2
1972LI24 Phys.Rev.Lett. 29, 798 (1972) R.A.Lindgren, H.H.Gutbrod, H.W.Fulbright, R.G.Markham Odd-Parity Three-Particle, One-Hole Structure in 18F via the Reaction 15N(6Li, t)18F NUCLEAR REACTIONS 15N(6Li, t), E=30 MeV; measured σ(Et, θ). 18F deduced odd-parity, 3p-1h structure.
doi: 10.1103/PhysRevLett.29.798
1972PR06 Nucl.Instrum.Methods 98, 445 (1972) Angular Correlations of Sequential Particle Decay for Aligned Nuclei
doi: 10.1016/0029-554X(72)90226-1
1971HI05 Particles and Nuclei 1, 372 (1971) R.G.Hirko, R.A.Lindgren, A.J.Howard, J.G.Pronko, M.W.Sachs, D.A.Bromley Nuclear Structure Studies on 29Al NUCLEAR REACTIONS 27Al(t, p), E=3.34 MeV; measured σ(Ep, θ). 26Mg(α, pγ), E=13.82, 14 MeV; measured σ(Ep, Eγ, θ(γ), θ(pγ)). 29Al deduced levels, J, π, γ-mixing, γ-branching.
1971LI27 Phys.Lett. 37B, 358 (1971) R.A.Lindgren, F.C.Young, B.Cotton Spins of the Isospin Mixed 5.61 and 5.67 MeV Levels in 18F NUCLEAR REACTIONS 19F(3He, α), E=5-6 MeV; measured σ(E;Eα, θ(αα)). 18F levels deduced J, π.
doi: 10.1016/0370-2693(71)90201-2
1971LI34 Bull.Am.Phys.Soc. 16, No.10, 1177 EB8 (1971) Colinear Particle-Particle Angular Correlations on the Ca40 (p, α) K37 (po) Ar36 Reaction RADIOACTIVITY 37K(p) [from 40Ca(p, α), E=15.75 MeV]; measured Ep, Ip, Eα, Iα; deduced levels, J, angular correlation of p in coincidence with α-particles from 40Ca(p, α), σ(θ).
1971YO05 Nucl.Phys. A176, 289 (1971) F.C.Young, R.A.Lindgren, W.Reichart Spin-Parity Determinations of 10B Levels by 11B(3He, α)10B(α0)6Li Correlations NUCLEAR REACTIONS 11B(3He, α), α + 6Li, E=5.0, 4.55, 2.8 MeV; measured σ(Eα;E(αα), θ(αα)), σ(Eα;E(6Li)θ(6Li)). 10B deduced levels, J, π. Enriched target.
doi: 10.1016/0375-9474(71)90271-5
1970LI08 Phys.Lett. 32B, 103 (1970) R.A.Lindgren, J.G.Pronko, A.J.Howard, D.A.Bromley The Identification of Mirror State Structure in 21Na and 21Ne NUCLEAR REACTIONS 24Mg(p, α); E=17.5 MeV; measured σ(Eα, Ep), αp(θ). 21Na levels deduced J.
doi: 10.1016/0370-2693(70)90598-8
1970PR01 Nucl.Phys. A140, 465 (1970) J.G.Pronko, R.A.Lindgren, D.A.Bromley Structure of 21Na from the 24Mg(p, α)21Na Reaction NUCLEAR REACTIONS 24Mg(p, α), E=17.5 MeV; measured αγ(θ), Iγ, σ(Eα, θ(α)). 21Na levels deduced J, γ-branching, γ-mixing . Enriched target.
doi: 10.1016/0375-9474(70)90337-4
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