NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = G.Feldman Found 57 matches. 2022HO01 J.Phys.(London) G49, 010502 (2022) C.R.Howell, M.W.Ahmed, A.Afanasev, D.Alesini, J.R.M.Annand, A.Aprahamian, D.L.Balabanski, S.V.Benson, A.Bernstein, C.R.Brune, J.Byrd, B.E.Carlsten, A.E.Champagne, S.Chattopadhyay, D.Davis, E.J.Downie, J.M.Durham, G.Feldman, H.Gao, C.G.R.Geddes, H.W.Griesshammer, R.Hajima, H.Hao, D.Hornidge, J.Isaak, R.V.F.Janssens, D.P.Kendellen, M.Kovash, P.P.Martel, U.-G.Meissner, R.Miskimen, B.Pasquini, D.R.Phillips, N.Pietralla, D.Savran, M.R.Schindler, M.H.Sikora, W.M.Snow, R.P.Springer, C.Sun, C.Tang, B.Tiburzi, A.P.Tonchev, W.Tornow, C.A.Ur, D.Wang, H.R.Weller, V.Werner, Y.K.Wu, J.Yan, Z.Zhao, A.Zilges, F.Z.Zomer International workshop on next generation gamma-ray source
doi: 10.1088/1361-6471/ac2827
2022LI18 Phys.Rev.Lett. 128, 132502 (2022) X.Li, M.W.Ahmed, A.Banu, C.Bartram, B.Crowe, E.J.Downie, M.Emamian, G.Feldman, H.Gao, D.Godagama, H.W.Griesshammer, C.R.Howell, H.J.Karwowski, D.P.Kendellen, M.A.Kovash, K.K.H.Leung, D.M.Markoff, J.A.McGovern, S.Mikhailov, R.E.Pywell, M.H.Sikora, J.A.Silano, R.S.Sosa, M.C.Spraker, G.Swift, P.Wallace, H.R.Weller, C.S.Whisnant, Y.K.Wu, Z.W.Zhao Proton Compton Scattering from Linearly Polarized Gamma Rays NUCLEAR REACTIONS 1H(polarized γ, γ'), E=83.4 MeV; measured reaction products, Eγ, Iγ; deduced σ(θ), electromagnetic dipole polarizabilities of the proton. The High Intensity Gamma-Ray Source facility at the Triangle Universities Nuclear Laboratory.
doi: 10.1103/PhysRevLett.128.132502
2020LI10 Phys.Rev. C 101, 034618 (2020) X.Li, M.W.Ahmed, A.Banu, C.Bartram, B.Crowe, E.J.Downie, M.Emamian, G.Feldman, H.Gao, D.Godagama, H.W.Griesshammer, C.R.Howell, H.J.Karwowski, D.P.Kendellen, M.A.Kovash, K.K.H.Leung, D.Markoff, S.Mikhailov, R.E.Pywell, M.H.Sikora, J.A.Silano, R.S.Sosa, M.C.Spraker, G.Swift, P.Wallace, H.R.Weller, C.S.Whisnant, Y.K.Wu, Z.W.Zhao Compton scattering from 4He at the TUNL HIγS facility NUCLEAR REACTIONS 4He(polarized γ, γ), E=81.3 MeV, 100% circularly and linearly polarized γ-ray beam via Compton backscattering from HiγS at TUNL; measured Compton scattered photons at different angles, time-of-flight spectra using an array of large NaI(Tl) detectors; deduced differential σ(θ). Comparison with previous experimental data from Lund at Eγ=87 MeV.
doi: 10.1103/PhysRevC.101.034618
2020ST04 Phys.Rev. C 101, 035207 (2020) B.Strandberg, K.G.Fissum, J.R.M.Annand, W.J.Briscoe, J.Brudvik, F.Cividini, L.Clark, E.J.Downie, K.England, G.Feldman, D.I.Glazier, K.Hamilton, K.Hansen, L.Isaksson, R.Al Jebali, M.A.Kovash, A.E.Kudryavtsev, V.Lensky, S.Lipschutz, M.Lundin, M.Meshkian, D.G.Middleton, L.S.Myers, D.O'Donnell, G.V.O'Rielly, B.Oussena, M.F.Preston, B.Schroder, B.Seitz, I.I.Strakovsky, M.Taragin, V.E.Tarasov, for the PIONS at MAX-lab Collaboration Near-threshold π- photoproduction on the deuteron NUCLEAR REACTIONS 2H(γ, π-), E=147.0, 149.7, 152.3, 154.9, 157.6, 159.8 MeV; measured Eγ, Iγ, total σ(E) using three large NaI(Tl) detectors for γ detection of radiative π- capture in target at the Tagged-Photon Facility of the MAX IV Laboratory in Sweden; deduced probability of π- capture inside the LD2 target. Comparison with theoretical predictions.
doi: 10.1103/PhysRevC.101.035207
2018ST10 Phys.Rev. C 98, 012201 (2018) B.Strandberg, J.R.M.Annand, W.Briscoe, J.Brudvik, F.Cividini, L.Clark, E.J.Downie, K.England, G.Feldman, K.G.Fissum, D.I.Glazier, K.Hamilton, K.Hansen, L.Isaksson, R.Al Jebali, M.A.Kovash, S.Lipschutz, M.Lundin, M.Meshkian, D.G.Middleton, L.S.Myers, D.O'Donnell, G.O'Rielly, B.Oussena, M.F.Preston, B.Schroder, B.Seitz, I.Strakovsky, M.Taragin, for the COMPTON @ MAX-LAB Collaboration Compton scattering from the deuteron above pion-production threshold NUCLEAR REACTIONS 2H(γ, γ'), E=143.2, 148.4, 153.2, 158.5 MeV bremsstrahlung photons produce by electron beam of about 190 MeV at the MAX-IV Laboratory in Lund; measured Eγ, γ(θ), γγ-coin, and differential σ(θ) of Compton scattered photons above the pion-production threshold using Compton and Two-Photon Spectrometer (CATS) at MAX IV Laboratory.
doi: 10.1103/PhysRevC.98.012201
2017SI26 Phys.Rev. C 96, 055209 (2017) M.H.Sikora, M.W.Ahmed, A.Banu, C.Bartram, B.Crowe, E.J.Downie, G.Feldman, H.Gao, H.W.Griesshammer, H.Hao, C.R.Howell, H.J.Karwowski, D.P.Kendellen, M.A.Kovash, X.Li, D.M.Markoff, S.Mikhailov, V.Popov, R.E.Pywell, J.A.Silano, M.C.Spraker, P.Wallace, H.R.Weller, C.S.Whisnant, Y.K.Wu, W.Xiong, X.Yan, Z.W.Zhao Compton scattering from 4He at 61 MeV NUCLEAR REACTIONS 4He(γ, γ'), E=61 MeV; measured Eγ, Iγ, Compton scattering differential σ(θ) using NaI(Tl) detectors and liquid 4He target at HIγS facility at TUNL. Data interpreted using phenomenological model sensitive to the dipole isoscalar electromagnetic polarizabilities of the nucleon. Comparison with previous experimental data. Benchmarks for future calculations from effective field theories and lattice quantum chromodynamics.
doi: 10.1103/PhysRevC.96.055209
2015MY04 Phys.Rev. C 92, 025203 (2015) L.S.Myers, J.R.M.Annand, J.Brudvik, G.Feldman, K.G.Fissum, H.W.Griesshammer, K.Hansen, S.S.Henshaw, L.Isaksson, R.Jebali, M.A.Kovash, M.Lundin, D.G.Middleton, A.M.Nathan, B.Schroder, S.C.Stave Compton scattering from the deuteron below pion-production threshold
doi: 10.1103/PhysRevC.92.025203
2014CA24 Nucl.Data Sheets 120, 163 (2014) C.L.Cahill, G.Feldman, W.J.Briscoe The Science of Nuclear Materials: A Modular, Laboratory-based Curriculum
doi: 10.1016/j.nds.2014.07.035
2014MY01 Phys.Rev. C 89, 035202 (2014) L.S.Myers, K.Shoniyozov, M.F.Preston, M.D.Anderson, J.R.M.Annand, M.Boselli, W.J.Briscoe, J.Brudvik, J.I.Capone, G.Feldman, K.G.Fissum, K.Hansen, S.S.Henshaw, L.Isaksson, R.Jebali, M.A.Kovash, K.Lewis, M.Lundin, I.J.D.MacGregor, D.G.Middleton, D.E.Mittelberger, M.Murray, A.M.Nathan, S.Nutbeam, G.V.O'Rielly, B.Schroder, B.Seitz, S.C.Stave, H.R.Weller, for the COMPTON @ MAX-lab Collaboration Compton scattering from 12C using tagged photons in the energy range 65-115 MeV NUCLEAR REACTIONS 12C(γ, γ), E=65-115 MeV; measured photon spectra, σ(E, θ) at Tagged-Photon Facility of the MAX IV-Lund Laboratory; deduced bound-nucleon polarizabilities. GEANT4 lineshape analysis of Compton-scattered photon spectrum. Phenomenological model. Comparison with previous experimental results.
doi: 10.1103/PhysRevC.89.035202
2014MY04 Phys.Rev. C 90, 027603 (2014) L.S.Myers, M.W.Ahmed, G.Feldman, A.Kafkarkou, D.P.Kendellen, I.Mazumdar, J.M.Mueller, M.H.Sikora, H.R.Weller, W.R.Zimmerman Compton scattering from 6Li at 86 MeV NUCLEAR REACTIONS 6Li, 16O(polarized γ, γ), E=86 MeV; measured Eγ, Iγ, σ(θ) at HIγS facility at TUNL; deduced E1, E2, QD resonance parameters. GEANT4 simulations. Discussed nuclear polarizability. Comparison with earlier experimental results for 16O target.
doi: 10.1103/PhysRevC.90.027603
2014MY06 Phys.Rev.Lett. 113, 262506 (2014) L.S.Myers, J.R.M.Annand, J.Brudvik, G.Feldman, K.G.Fissum, H.W.Griesshammer, K.Hansen, S.S.Henshaw, L.Isaksson, R.Jebali, M.A.Kovash, M.Lundin, J.A.McGovern, D.G.Middleton, A.M.Nathan, D.R.Phillips, B.Schroder, S.C.Stave, for the COMPTON @ MAX-lab Collaboration Measurement of Compton Scattering from the Deuteron and an Improved Extraction of the Neutron Electromagnetic Polarizabilities NUCLEAR REACTIONS 2H(γ, γ), (γ, E), E=65-115 MeV; measured reaction products, Eγ, Iγ; deduced the isoscalar polarizabilities and reduced the statistical uncertainty on these quantities. Comparison with available data.
doi: 10.1103/PhysRevLett.113.262506
2013WE01 Acta Phys.Pol. B44, 587 (2013) H.R.Weller, M.W.Ahmed, J.M.Mueller, L.S.Myers, W.R.Zimmerman, G.Feldman, M.H.Sikora Precise Determination of the Isovector Giant Quadrupole Resonance in Nuclei NUCLEAR REACTIONS 89Y, 209Bi(γ, γ'), E<36 MeV; measured reaction products, Eγ, Iγ; deduced polarization ratios, IVGQR parameters, Isovector E2 energy weighted sum rule, width, resonance parameters. 124Sn, 142Nd(γ, γ'), E not given; calculated yields.
doi: 10.5506/APhysPolB.44.587
2012MY05 Phys.Rev. C 86, 044614 (2012) L.S.Myers, M.W.Ahmed, G.Feldman, S.S.Henshaw, M.A.Kovash, J.M.Mueller, H.R.Weller Compton scattering from 6Li at 60 MeV NUCLEAR REACTIONS 6Li, 16O(polarized γ, γ), E=60 MeV; measured Compton scattered γ spectra, angular distributions using High Intensity Gamma-Ray Source (HIγS) at TUNL facility; deduced Compton scattering σ(θ).
doi: 10.1103/PhysRevC.86.044614
2011HE18 Phys.Rev.Lett. 107, 222501 (2011) S.S.Henshaw, M.W.Ahmed, G.Feldman, A.M.Nathan, H.R.Weller New Method for Precise Determination of the Isovector Giant Quadrupole Resonances in Nuclei NUCLEAR REACTIONS 209Bi(γ, γ), E=15-26 MeV; measured reaction products, Eγ, Iγ; deduced parameters of isovector giant quadrupole resonance (IVGQR).
doi: 10.1103/PhysRevLett.107.222501
2009KA29 Phys.Rev. C 80, 044001 (2009) M.Karlsson, J.-O.Adler, L.E.M.Andersson, V.Avdeichikov, B.L.Berman, M.J.Boland, W.J.Briscoe, J.Brudvik, J.R.Calarco, G.Feldman, K.G.Fissum, K.Hansen, D.Hornidge, L.Isaksson, N.R.Kolb, A.A.Kotov, P.Lilja, M.Lundin, B.Nilsson, D.Nilsson, G.V.O'Rielly, G.E.Petrov, B.Schroder, I.I.Strakovsky, L.A.Vaishnene Measurement of the differential cross section for the two-body photodisintegration of 3He at ΦLAB = 90 degrees using tagged photons in the energy range 14-31 MeV NUCLEAR REACTIONS 3He(γ, d)(γ, p), E=14-31 MeV; measured proton and deuteron spectra, and differential cross sections as a function of Eγ using tagged-photon facility at MAX-lab. The two-body photodisintegration of 3He investigated. Comparison with previous measurements and theoretical calculations using Faddeev technique.
doi: 10.1103/PhysRevC.80.044001
2005PS01 Eur.Phys.J. A 24, 69 (2005) I.A.Pshenichnov, B.L.Berman, W.J.Briscoe, C.Cetina, G.Feldman, P.Heimberg, A.S.Iljinov, I.I.Strakovsky Intranuclear-Cascade model calculation of photofission probabilities for actinide nuclei NUCLEAR REACTIONS Pb, 232Th, 233,235,238U, 237Np(γ, F), E=0.068-3.77 GeV; calculated photofission probabilities, absolute σ. Intranuclear-cascade model, comparisons with data.
doi: 10.1140/epja/i2004-10130-9
2004DE09 Eur.Phys.J. A 19, Supplement 1, 275 (2004) C.de Jager, B.Wojtsekhowski, D.Tedeschi, B.Vlahovic, D.Abbott, J.Asai, G.Feldman, T.Hotta, M.Khadaker, H.Kohri, T.Matsumara, T.Mibe, T.Nakano, V.Nelyubin, G.Orielly, A.Rudge, P.Weilhammer, M.Wood, T.Yorita, R.Zegers A pair polarimeter for linearly polarized high energy photons
doi: 10.1140/epjad/s2004-03-045-5
2004FR30 Phys.Rev. C 70, 044317 (2004) C.Fransen, N.Pietralla, A.P.Tonchev, M.W.Ahmed, J.Chen, G.Feldman, U.Kneissl, J.Li, V.N.Litvinenko, B.Perdue, I.V.Pinayev, H.H.Pitz, R.Prior, K.Sabourov, M.Spraker, W.Tornow, H.R.Weller, V.Werner, Y.K.Wu, S.W.Yates Parity assignments to strong dipole excitations of 92Zr and 96Mo NUCLEAR REACTIONS 92Zr(polarized γ, γ'), E=3.47, 3.64 MeV; 96Mo(γ, γ'), E=2.80, 3.30, 3.43, 3.60, 3.90 MeV; measured Eγ, Iγ, azimuthal asymmetry. 92Zr, 96Mo levels deduced π.
doi: 10.1103/PhysRevC.70.044317
2004PE24 Phys.Rev. C 70, 064305 (2004) B.A.Perdue, M.W.Ahmed, A.P.Tonchev, H.R.Weller, G.Feldman, V.N.Litvinenko, I.V.Pinayev, B.E.Norum, R.M.Prior, M.C.Spraker, B.D.Sawatzky Compton scattering of polarized γ rays by 16O for Eγ = 25-40 MeV NUCLEAR REACTIONS 16O(polarized γ, γ'), E=25-40 MeV; measured polarization asymmetries; deduced resonance features.
doi: 10.1103/PhysRevC.70.064305
2002CE04 Phys.Rev. C65, 044622 (2002) C.Cetina, P.Heimberg, B.L.Berman, W.J.Briscoe, G.Feldman, L.Y.Murphy, H.Crannell, A.Longhi, D.I.Sober, J.C.Sanabria, G.Ya.Kezerashvili Photofission of Heavy Nuclei from 0.2 to 3.8 GeV NUCLEAR REACTIONS Pb, 232Th, 233,235,238U, 237Np(γ, F), E=0.17-3.84 GeV; measured fission σ; deduced reaction mechanism features. Tagged photon beam.
doi: 10.1103/PhysRevC.65.044622
2001WA24 Phys.Rev. C64, 014603 (2001) B.J.Warkentin, D.L.Hornidge, R.Igarashi, J.C.Bergstrom, E.L.Hallin, N.R.Kolb, R.E.Pywell, D.M.Skopik, J.M.Vogt, G.Feldman Nuclear Compton Scattering from 12C and Bound-Nucleon Polarizabilities NUCLEAR REACTIONS 12C(γ, γ), (γ, γ'), E=84-105 MeV; measured Eγ, Iγ, σ(θ); deduced approximate bound nucleon polarizabilities. Tagged photon beam.
doi: 10.1103/PhysRevC.64.014603
2000CE02 Phys.Rev.Lett. 84, 5740 (2000) C.Cetina, B.L.Berman, W.J.Briscoe, P.L.Cole, G.Feldman, P.Heimberg, L.Y.Murphy, S.A.Philips, J.C.Sanabria, H.Crannell, A.Longhi, D.I.Sober, G.Ya.Kezerashvili Photofission of Heavy Nuclei at Energies Up to 4 GeV NUCLEAR REACTIONS Pb, 232Th, 233,235,238U, 237Np(γ, F), E=0.17-3.84 GeV; measured photofission σ. Tagged photons, simultaneous measurement.
doi: 10.1103/PhysRevLett.84.5740
2000HO02 Phys.Rev.Lett. 84, 2334 (2000) D.L.Hornidge, B.J.Warkentin, R.Igarashi, J.C.Bergstrom, E.L.Hallin, N.R.Kolb, R.E.Pywell, D.M.Skopik, J.M.Vogt, G.Feldman Elastic Compton Scattering from the Deuteron and Nucleon Polarizabilities NUCLEAR REACTIONS 2H(γ, γ), E=84-105 MeV; measured Eγ, Iγ, σ(θ). 1n, 1H deduced polarizabilities. Tagged photons, large-volume NaI spectrometer.
doi: 10.1103/PhysRevLett.84.2334
2000KO36 Phys.Rev.Lett. 85, 1388 (2000) N.R.Kolb, A.W.Rauf, R.Igarashi, D.L.Hornidge, R.E.Pywell, B.J.Warkentin, E.Korkmaz, G.Feldman, G.V.O'Rielly Quasifree Compton Scattering from the Deuteron and Nucleon Polarizabilities NUCLEAR REACTIONS 2H(γ, nγ), E=236-260 MeV bremsstrahlung; measured Eγ, Iγ, σ(θ). 1H, 1n deduced polarizabilities in deuteron bound state.
doi: 10.1103/PhysRevLett.85.1388
2000RI10 Phys.Rev. C61, 064612 (2000) B.J.Rice, R.S.Canon, E.A.Wulf, H.R.Weller, K.Keeter, N.R.Kolb, C.Mueller, R.E.Pywell, G.A.Retzlaff, D.M.Skopik, G.Feldman Two-Deuteron Photodisintegration of 4He at Eγ = 150-250 MeV NUCLEAR REACTIONS 4He(γ, d), E=150-250 MeV; measured deuteron spectra, σ(θ), σ, dd-coin; deduced reaction mechanism features. Transition matrix element analysis, direct capture calculation.
doi: 10.1103/PhysRevC.61.064612
2000SA09 Phys.Rev. C61, 034604 (2000) J.C.Sanabria, B.L.Berman, C.Cetina, P.L.Cole, G.Feldman, N.R.Kolb, R.E.Pywell, J.M.Vogt, V.G.Nedorezov, A.S.Sudov, Ya.Kezerashvili Photofission of Actinide Nuclei in the Quasideuteron and Lower Part of the Δ Energy Region NUCLEAR REACTIONS 232Th, 233,235,238U, 237Np(γ, F), E=68-264 MeV; measured photofission σ. 232Th, 233,235,238U, 237Np deduced relative fissility. Tagged photons, comparisons with previous results.
doi: 10.1103/PhysRevC.61.034604
1999BE79 Nucl.Phys. (Supplement) A654, 837c (1999) B.L.Berman, C.Cetina, P.L.Cole, W.R.Dodge, G.Feldman, J.C.Sanabria, N.Kolb, R.E.Pywell, J.Vogt, V.Nedorezov, A.Sudov, G.Ya.Kezerashvili Photofission of Actinide and Pre-Actinide Nuclei in the Quasideuteron and Delta Energy Regions NUCLEAR REACTIONS Pb, 197Au(γ, F), E=122-222 MeV; measured fission σ. 232Th, 233,235,238U, 237Np(γ, F), E=64-264 MeV; measured fission σ; deduced relative fissilities. Tagged photon beams.
doi: 10.1016/S0375-9474(00)88557-7
1999KO43 Phys.Rev.Lett. 83, 3609 (1999) E.Korkmaz, N.R.Kolb, D.A.Hutcheon, G.V.O'Rielly, J.C.Bergstrom, G.Feldman, D.Jordan, A.K.Opper, R.E.Pywell, B.Sawatzky, D.M.Skopik Measurement of thr γp → π+n Reaction Near Threshold NUCLEAR REACTIONS 1H(γ, π+), E=152-154 MeV; measured σ(θ), neutron yields; deduced electric dipole amplitude. Comparison with chiral perturbation theory.
doi: 10.1103/PhysRevLett.83.3609
1998QU01 Phys.Rev. C57, 2118 (1998) M.A.Quraan, E.D.Hackett, E.Korkmaz, W.J.McDonald, A.K.Opper, N.L.Rodning, G.Feldman, N.R.Kolb, G.V.O'Rielly, R.E.Pywell, D.M.Skopik Final State Interactions in 2H(γ, ppπ-) Near the Δ(1232) Resonance NUCLEAR REACTIONS 2H(γ, 2pπ-), E=220-280 MeV; measured σ(φ(π)), σ(θ(π)), σ(Eγ), σ(θ(Δ)); deduced final state interactions, Δ-resonance role.
doi: 10.1103/PhysRevC.57.2118
1996BE13 Phys.Rev. C53, 1759 (1996) J.A.Behr, K.A.Snover, C.A.Gossett, G.Feldman, J.H.Gundlach, M.Kicinska-Habior Nonstatistical γ Emission in 3He- and α-Induced Reactions NUCLEAR REACTIONS 61Ni, 95Mo, 119,124Sn, 148,154Sm, 181Ta(α, γ), E=11-28 MeV; C, O, 61,62Ni, 95,96Mo, 120,124Sn, 148Sm, 181Ta(3He, γ), E=11-28 MeV; measured γ-ray production σ(Eγ) at θγ=90°; deduced systematics of nonstatistical γ-ray yields. Statistical model, direct plus semdirect excitation of the giant dipole resonance, including Coulomb, projectile excitation.
doi: 10.1103/PhysRevC.53.1759
1996FE07 Phys.Rev. C54, R2124 (1996) G.Feldman, K.E.Mellendorf, R.A.Eisenstein, F.J.Federspiel, G.Garino, R.Igarashi, N.R.Kolb, M.A.Lucas, B.E.MacGibbon, W.K.Mize, A.M.Nathan, R.E.Pywell, D.P.Wells Compton Scattering, Meson Exchange, and the Polarizabilities of Bound Nucleons NUCLEAR REACTIONS 16O(γ, γ), E=27-108 MeV; measured Eγ, Iγ, σ(θ) vs E; deduced bound-nucleon polarizability, meson-exchange contribution.
doi: 10.1103/PhysRevC.54.R2124
1996HA03 Phys.Rev. C53, R1047 (1996) E.D.Hackett, W.J.McDonald, A.K.Opper, M.A.Quraan, N.L.Rodning, F.M.Rozon, G.Feldman, N.R.Kolb, R.E.Pywell, D.M.Skopik, D.E.Tiller, J.M.Vogt, E.Korkmaz, G.V.O'Rielly Reaction Mechanisms in 12C(γ, pp) Near 200 MeV NUCLEAR REACTIONS 12C(γ, 2pX), E=187-227 MeV; measured inclusive differential σ. Monte Carlo intranuclear cascade calculation.
doi: 10.1103/PhysRevC.53.R1047
1996KO45 Phys.Rev. C54, 2175 (1996) N.R.Kolb, G.Feldman, G.V.O'Rielly, R.E.Pywell, D.M.Skopik, E.D.Hackett, M.A.Quraan, N.L.Rodning 3He(γ, pp)n Cross Sections with Tagged Photons Below the Δ Resonance Energy NUCLEAR REACTIONS 3He(γ, 2p), E=161-208 MeV; measured absolute σ(θ(pp), φ(pp)). Tagged photons. Model comparison.
doi: 10.1103/PhysRevC.54.2175
1995MA68 Phys.Rev. C52, 2097 (1995) B.E.MacGibbon, G.Garino, M.A.Lucas, A.M.Nathan, G.Feldman, B.Dolbilkin Measurement of the Electric and Magnetic Polarizabilities of the Proton NUCLEAR REACTIONS 1H(γ, γ), E=70-148 MeV; measured Compton scattering σ(θ) vs E; deduced magnetic polarizabilities α(bar), β(bar). Simultaneous use of tagged, untagged beam over certain energy range.
doi: 10.1103/PhysRevC.52.2097
1994BA02 Phys.Rev. C49, 912 (1994) M.J.Balbes, J.C.Riley, G.Feldman, H.R.Weller, D.R.Tilley Polarized Deuteron Capture by 3He and 3H at and above the Fusion Resonance Region NUCLEAR REACTIONS 3He, 3H(polarized d, γ), E=0.4-8.6 MeV; measured Eγ, Iγ, σ(θ), vector, tensor analyzing power vs θ; deduced transition matrix elements, reaction mechanism. Resonating group model.
doi: 10.1103/PhysRevC.49.912
1994FL04 Phys.Rev.Lett. 72, 3476 (1994); Erratum Phys.Rev.Lett. 73, 1190 (1994) R.E.Florizone, J.Asai, G.Feldman, E.L.Hallin, D.M.Skopik, J.M.Vogt, R.C.Haight, S.M.Sterbenz Simultaneous Measurement of the (γ, p)/(γ, n) Cross-Section Ratio in 4He as a Test of Charge Symmetry NUCLEAR REACTIONS, ICPND 4He(γ, p), (γ, n), E=25-60 MeV bremsstrahlung; measured σ(θ) vs E; deduced angle integrated yields. 4He deduced no significant charge symmetry violation evidence.
doi: 10.1103/PhysRevLett.72.3476
1994GO17 Phys.Rev. C50, 1528 (1994) M.A.Godwin, E.Hayward, G.Feldman, L.H.Kramer, H.R.Weller, W.R.Dodge Isovector Giant Quadrupole Resonance Observed in 89Y(p(pol), γ)90Zr NUCLEAR REACTIONS 89Y(polarized p, γ), E=18.5-28.5 MeV; measured Eγ, Iγ(θ), analyzing power (θ=90°) vs Ep; deduced model parameters. 90Zr deduced giant quadrupole resonances, widths, E2 strength distribution features.
doi: 10.1103/PhysRevC.50.1528
1994KO11 Phys.Rev. C49, 2586 (1994) N.R.Kolb, E.B.Cairns, E.D.Hackett, E.Korkmaz, T.Nakano, A.K.Opper, M.A.Quraan, N.L.Rodning, F.M.Rozon, J.Asai, G.Feldman, E.Hallin, G.V.O'Rielly, R.E.Pywell, D.M.Skopik 3He(γ, pd) Cross Sections with Tagged Photons Below the Δ Resonance NUCLEAR REACTIONS 3He(γ, pd), E=166-213 MeV; measured σ(θ). Tagged photons.
doi: 10.1103/PhysRevC.49.2586
1994WI08 Nucl.Phys. A577, 653 (1994) J.Z.Williams, G.Feldman, H.R.Weller, D.R.Tilley Radiative Capture of Polarized Deuterons by 6Li and the D-State of 8Be NUCLEAR REACTIONS 6Li(polarized d, γ), E=2-14 MeV; measured σ(E) vs θ, vector, tensor analyzing power vs θ, E; deduced transition matrix elements phases. 8Be deduced D-state probability. Direct capture, multi-channel resonating group model.
doi: 10.1016/0375-9474(94)90938-5
1993FE01 Phys.Rev. C47, 1436 (1993) G.Feldman, K.A.Snover, J.A.Behr, C.A.Gossett, J.H.Gundlach, M.Kicinska-Habior Statistical γ Decay of the Giant Dipole Resonance in Highly Excited 46Ti and 52Cr NUCLEAR REACTIONS 27Al(19F, X), E=30-60 MeV; 48Ti(α, X), E=12-28 MeV; measured inclusive γ production σ(E). 46Ti, 52Cr deduced GDR built on excited states, parameters.
doi: 10.1103/PhysRevC.47.1436
1993SA03 Phys.Rev. C47, 459 (1993) A.J.Sarty, K.G.R.Doss, G.Feldman, E.L.Hallin, R.E.Pywell, G.A.Retzlaff, D.M.Skopik, H.R.Weller, W.R.Dodge, J.W.Lightbody, Jr., J.S.O'Connell, C.C.Chang Measurement of the Reaction 3He(γ, pp)n and Its Relation to Three-Body Forces NUCLEAR REACTIONS 3He(γ, 2p), E=90-250 MeV bremsstrahlung; measured σ(θn, θp) vs neutron momentum; deduced two-pion-exchange, three-body absorption mechanisms role.
doi: 10.1103/PhysRevC.47.459
1992BA04 Phys.Rev. C45, R487 (1992) M.J.Balbes, G.Feldman, H.R.Weller, D.R.Tilley Polarized d + 3He Capture Into the (3/2)+ Fusion Resonance of 5Li and the Role of the Tensor Force NUCLEAR REACTIONS 3He(polarized d, γ), E=0.8 MeV; measured absolute σ(θ), vector, tensor analyzing power vs θ; deduced tensor force role. 5Li level deduced E1 transition matrix elements. Resonanting group model.
doi: 10.1103/PhysRevC.45.R487
1992KI01 Phys.Rev. C45, 569 (1992) M.Kicinska-Habior, K.A.Snover, J.A.Behr, C.A.Gossett, J.H.Gundlach, G.Feldman Comparison of Giant Dipole Resonance Decay in Stiff 92Mo and Soft 100Mo Excited Nuclei NUCLEAR REACTIONS 76Se(17O, X), E=50, 72.2 MeV; 82Se(18O, X), E=49.1-72.8 MeV; measured σ(Eγ), θ=90°. 92,100Mo deduced GDR built on excited states, decay features.
doi: 10.1103/PhysRevC.45.569
1991BA02 Phys.Rev. C43, 343 (1991) M.J.Balbes, G.Feldman, L.H.Kramer, H.R.Weller, D.R.Tilley Ground-State Widths of 5He and 5Li Determined in the 3H(d, γ)5He and the 3He(d, γ)5Li Reactions NUCLEAR REACTIONS 3H, 3He(d, γ), E=8.6 MeV; measured Eγ, Iγ. 5Li, 5He level deduced Γ, nucleon decay widths.
doi: 10.1103/PhysRevC.43.343
1991FE01 Phys.Rev. C43, 223 (1991) G.Feldman, L.H.Kramer, H.R.Weller, E.Hayward, W.R.Dodge Isovector Giant Quadrupole Resonance Observed in 30Si(p(pol), γ)31P NUCLEAR REACTIONS 30Si(polarized p, γ), E=20-36 MeV; measured σ(θ), analyzing power vs θ. 31P deduced isovector GQR, parameters.
doi: 10.1103/PhysRevC.43.223
1991WI04 Phys.Rev. C43, 1363 (1991) V.Wijekumar, J.Z.Williams, G.Feldman, H.R.Weller, D.R.Tilley Resolution of the Twofold Ambiguity in the E1 Capture Amplitudes for the 13C(p(pol), γ)14N Reaction NUCLEAR REACTIONS 13C(polarized p, γ), E=3-4.2 MeV; measured Eγ, Iγ, σ(θ), analyzing power; deduced E1 capture mechanism.
doi: 10.1103/PhysRevC.43.1363
1991WI19 Phys.Lett. 273B, 216 (1991) J.Z.Williams, G.Feldman, H.R.Weller, D.R.Tilley The 6Li(d(pol), γ)8Be Reaction at E(d) = 9.0 MeV and the D-State of 8Be NUCLEAR REACTIONS 6Li(polarized d, γ), E=90 MeV; measured Eγ, Iγ, σ(θ), vector, tensor analyzing power vs θ. 8Be deduced d+6Li D-state probability.
doi: 10.1016/0370-2693(91)91674-K
1990FE06 Phys.Rev. C42, R1167 (1990) G.Feldman, M.J.Balbes, L.H.Kramer, J.Z.Williams, H.R.Weller, D.R.Tilley 3H(p, γ)4He Reaction and the (γ, p)/(γ, n) Ratio in 4He NUCLEAR REACTIONS, ICPND 3H(p, γ), E=2-15 MeV; measured σ(E, θ=90°); deduced σ(E) for (γ, p), σ(γ, p)/σ(γ, n). 4He deduced no charge symmetry violation evidence.
doi: 10.1103/PhysRevC.42.R1167
1990KI04 Phys.Rev. C41, 2075 (1990) M.Kicinska-Habior, K.A.Snover, J.A.Behr, G.Feldman, C.A.Gossett, J.H.Gundlach Spin Dependence of the Giant-Dipole-Resonance Strength Function in Highly Excited Nuclei in the Mass Region A = 39-45 NUCLEAR REACTIONS, ICPND 27Al(12C, X), E=33.8-62.7 MeV; 27Al(13C, X), E=39.7 MeV; 27Al(15N, X), E=29.2, 44.7 MeV; 27Al(18O, X), E=31.5-72.5 MeV; measured continuum Eγ, Iγ, γ(θ); deduced fusion σ. 39,40K, 42Ca, 45Sc deduced GDR strength function.
doi: 10.1103/PhysRevC.41.2075
1988GO05 J.Phys.(London) G14, Supplement S267 (1988) C.A.Gossett, J.A.Behr, G.Feldman, J.H.Gundlach, M.Kicinska-Habior, K.A.Snover Systematic Behaviour of the Giant Dipole Resonance in Highly Excited Nuclei NUCLEAR REACTIONS 154Sm(12C, X), E=61.2 MeV; calculated σ(Eγ, E). 166Er deduced GDR role. NUCLEAR STRUCTURE 108Sn, 140Ce, 156,166Er; calculated photoabsorption σ; deduced GDR role.
doi: 10.1088/0305-4616/14/S/028
1988LA14 Phys.Rev. C38, 565 (1988) J.L.Langenbrunner, G.Feldman, H.R.Weller, D.R.Tilley, B.Wachter, T.Mertelmeier, H.M.Hofmann 2H(d(pol), γ)4He Reaction at E(d) = 1.2 MeV NUCLEAR REACTIONS 2H(polarized d, γ), E=1.2 MeV; measured σ(θ), analyzing power vs θ; deduced γ-multipolarity, relative transition strengths. Microscopic multi-channel resonating group model.
doi: 10.1103/PhysRevC.38.565
1987KI17 Phys.Rev. C36, 612 (1987) M.Kicinska-Habior, K.A.Snover, C.A.Gossett, J.A.Behr, G.Feldman, H.K.Glatzel, J.H.Gundlach, E.F.Garman Statistical Giant Dipole Resonance Decay of Highly Excited States of 63Cu NUCLEAR REACTIONS 59Co(α, γ), E=17.8-28.4 MeV; 57Fe(6Li, X), E=13.9-36 MeV; 51V(12C, X), E=26.3-64.7 MeV; 45Sc(18O, X), E=39.9-75.1 MeV; measured σ(Eγ). 63Cu deduced giant dipole resonance parameters. 62,63Cu, 60,62Ni, 59Co, 56Fe deduced level densities. NaI detector. Statistical model analyses.
doi: 10.1103/PhysRevC.36.612
1986HA30 Phys.Lett. 176B, 297 (1986) M.N.Harakeh, D.H.Dowell, G.Feldman, E.F.Garman, R.Loveman, J.L.Osborne, K.A.Snover Role of Isospin in the Statistical Decay of the Giant Dipole Resonance Built on Excited States NUCLEAR REACTIONS 25Mg(3He, γ), E=11.8 MeV; 12C(16O, γ), E=40.2 MeV; 12C(12C, γ), 12,13C(13C, γ), E=40 MeV; measured σ vs Eγ, γ yields. 28Si, 24,25,26Mg deduced GDR, Γ, EWSR, T-mixing parameters.
doi: 10.1016/0370-2693(86)90167-X
1985GO04 Phys.Rev.Lett. 54, 1486 (1985) C.A.Gossett, K.A.Snover, J.A.Behr, G.Feldman, J.L.Osborne Deformation of Heated Nuclei Observed in the Statistical Decay of the Giant Dipole Resonance NUCLEAR REACTIONS 154,148Sm(12C, X), E=63 MeV; measured Eγ, Iγ, continuum spectra, σ(Eγ). 160,166Er deduced excited state based GDR parameters, splitting, deformation at high temperature.
doi: 10.1103/PhysRevLett.54.1486
1983DO03 Phys.Rev.Lett. 50, 1191 (1983) D.H.Dowell, G.Feldman, K.A.Snover, A.M.Sandorfi, M.T.Collins Excited-State Giant Dipole Resonances in (p, γ): A new probe of single-particle strengths NUCLEAR REACTIONS 27Al(p, γ), E=11-39 MeV; measured Eγ, Iγ, σ(θγ) vs Eγ. 28Si deduced GDR, Γ, configuration.
doi: 10.1103/PhysRevLett.50.1191
1983KU01 Phys.Rev. C27, 948 (1983) E.Kuhlmann, K.A.Snover, G.Feldman, M.Hindi Alpha Capture into the Giant Quadrupole Resonance in 28Si NUCLEAR REACTIONS, ICPND 24Mg(α, γ), E=4.3-14 MeV; measured Eγ, Iγ, σ(E, Eγ, θγ); deduced E1, E2 capture σ. 28Si deduced E1, E2 transition strengths. Enriched target. Hauser-Feshbach formalism, isospin effects.
doi: 10.1103/PhysRevC.27.948
1983SN02 Phys.Rev. C27, 493 (1983) K.A.Snover, G.Feldman, M.M.Hindi, E.Kuhlmann, M.N.Harakeh, M.Sasao, M.Noumachi, Y.Fujita, M.Fujiwara, K.Hosono 27Al(p, γ)28Si and 27Al(3He, d)28Si to the Stretched 11.58 MeV (6-, 0) and 14.36 MeV (6-, 1) Levels NUCLEAR REACTIONS 27Al(p, γ), E ≈ 2876 keV; measured σ(Eγ, E). 28Si resonance deduced Γ, Γp, Γγ, configuration, B(M1). 27Al(3He, d), E=40, 60 MeV; measured σ(θ); deduced optical model parameters. 28Si levels deduced S, configuration. DWBA analysis.
doi: 10.1103/PhysRevC.27.493
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