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NSR database version of April 11, 2024.

Search: Author = G.Feldman

Found 57 matches.

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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0259.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0232.


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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG0037.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0195.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG0045.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0177.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0149.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


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
Citations: PlumX Metrics


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0638.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0191.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0060.


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
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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
Citations: PlumX Metrics


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0750.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0190.


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
Citations: PlumX Metrics


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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0523.


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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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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