NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = S.Hoblit Found 41 matches. 2015BR02 J.Phys.(London) G42, 034020 (2015) D.A.Brown, M.Herman, S.Hoblit, E.A.McCutchan, G.P.A.Nobre, B.Pritychenko, A.A.Sonzogni Uncertainty quantification in the Nuclear Data Program NUCLEAR REACTIONS 96Mo, 100Ru, 104Pd, 110Cd, 116Sn, 122,123,124Te, 128,130Xe, 134,136Ba, 142Nd, 148,150Sm, 154Gd, 160Dy, 176Hf, 198Hg, 204Pb(n, γ), E=30 keV; calculated Maxwellian-averaged σ and their uncertainties. ENDF/B-VII.1 evaluated library covariances, s-process.
doi: 10.1088/0954-3899/42/3/034020
2015NO01 Phys.Rev. C 91, 024618 (2015) G.P.A.Nobre, A.Palumbo, M.Herman, D.Brown, S.Hoblit, F.S.Dietrich Derivation of an optical potential for statically deformed rare-earth nuclei from a global spherical potential NUCLEAR REACTIONS 165Ho, 182,184,186W(n, X), E=0.003-200 MeV; calculated total σ(E). 158,160Gd(n, n), (n, n'), E=2.5, 4.1 MeV; Gd(n, n), E=0.334-0.919 MeV; Gd(n, n'), E=4.51-8.41 MeV; 165Ho(n, n), E=0.350, 0.60, 0.79, 0.93 MeV; 165Ho(n, n'), E=1.20, 4.51, 9.99, 11 MeV; 182,184W(n, n), (n, n')E=1.5-6.0 MeV; calculated σ(θ, E). Coupled-channel calculations with optical potential for statically deformed rare-earth nuclei using rotational excited states of the g.s. band. Comparison with experimental data.
doi: 10.1103/PhysRevC.91.024618
2014NO04 Nucl.Data Sheets 118, 224 (2014) G.P.A.Nobre, M.Herman, S.Hoblit, A.Palumbo, R.Capote, A.Trkov Fitting Prompt Fission Neutron Spectra Using Kalman Filter Integrated with Empire Code NUCLEAR REACTIONS 235U(n, F), E=thermal; calculated prompt fission neutron spectra using Los Alamos and Kornilov models incorporated in EMPIRE code; deduced parameters. Compared with data and one model to the other.
doi: 10.1016/j.nds.2014.04.041
2014NO06 Nucl.Data Sheets 118, 266 (2014) G.P.A.Nobre, A.Palumbo, D.Brown, M.Herman, S.Hoblit, F.S.Dietrich Towards a Coupled-channel Optical Potential for Rare-earth Nuclei NUCLEAR REACTIONS 152Sm, 156Gd, 162,166Dy, 180Hf(n, x), E=0.002-20 MeV;184W(n, x), E=0.05-20 MeV; calculated total σ. 184W(n, γ), E=0.003-40 MeV; calculated σ. 184W(n, n), E=1.5-6.0 MeV;184W(n, n'), E=1.5-3.5 MeV;calculated σ(θ) using optical model, coupled channels with quadrupole- and hexadecupole deformed potential and other corrections. Compared to EXFOR data.
doi: 10.1016/j.nds.2014.04.054
2014PA47 Nucl.Data Sheets 118, 596 (2014) G.Palmiotti, M.Salvatores, G.Aliberti, M.Herman, S.D.Hoblit, R.D.McKnight, P.Oblozinsky, P.Talou, G.M.Hale, H.Hiruta, T.Kawano, C.M.Mattoon, G.P.A.Nobre, A.Palumbo, M.Pigni, M.E.Rising, W.-S.Yang, A.C.Kahler Combined Use of Integral Experiments and Covariance Data
doi: 10.1016/j.nds.2014.04.145
2013SA39 Nucl.Phys. A914, 538c (2013) Hyperon photoproduction from polarized H and D towards a complete N* experiment
doi: 10.1016/j.nuclphysa.2013.01.009
2011CH57 Nucl.Data Sheets 112, 2887 (2011) M.B.Chadwick, M.Herman, P.Oblozinsky, M.E.Dunn, Y.Danon, A.C.Kahler, D.L.Smith, B.Pritychenko, G.Arbanas, R.Arcilla, R.Brewer, D.A.Brown, R.Capote, A.D.Carlson, Y.S.Cho, H.Derrien, K.Guber, G.M.Hale, S.Hoblit, S.Holloway, T.D.Johnson, T.Kawano, B.C.Kiedrowski, H.Kim, S.Kunieda, N.M.Larson, L.Leal, J.P.Lestone, R.C.Little, E.A.McCutchan, R.E.MacFarlane, M.MacInnes, C.M.Mattoon, R.D.McKnight, S.F.Mughabghab, G.P.A.Nobre, G.Palmiotti, A.Palumbo, M.T.Pigni, V.G.Pronyaev, R.O.Sayer, A.A.Sonzogni, N.C.Summers, P.Talou, I.J.Thompson, A.Trkov, R.L.Vogt, S.C.van der Marck, A.Wallner, M.C.White, D.Wiarda, P.G.Young ENDF/B-VII.1 Nuclear Data for Science and Technology: Cross Sections, Covariances, Fission Product Yields and Decay Data COMPILATION Z=1-118; compiled, analyzed decay data, Maxwellian averaged neutron capture σ, neutron-induced fission σ. NUCLEAR REACTIONS 1,2H, 3He, 6,7Li, 7,9Be, 10,11B, C, 14,15N, 16,17O, 19F, 22,23Na, 24,25,26Mg, 27Al, 28,29,30Si, 31P, 32,33,34,36S, 35,37Cl, 36,38,40Ar, 39,40,41K, 40,42,43,44,46,48Ca, 45Sc, 46,47,48,49,50Ti, 50,51V, 50,52,53,54Cr, 55Mn, 54,56,57,58Fe, 58,59Co, 58,59,60,61,62,64Ni, 63,65Cu, 65,66,67,68,70Zn, 69,71Ga, 70,72,73,74,76Ge, 74,75As, 74,76,77,78,79,80,82Se, 79,81Br, 78,80,82,83,84,85,86Kr, 85,86,87Rb, 84,86,87,88,89,90Sr, 89,90,91Y, 90,91,92,93,94,95,96Zr, 93,94,95Nb, 92,94,95,96,97,98,99,100Mo, 99Tc, 96,98,99,100,101,102,103,104,105,106Ru, 103,105Rh, 102,104,105,106,107,108,110Pd, 107,109,110,111Ag, 106,108,110,111,112,113,114,115,116Cd, 113,115In, 112,113,114,115,116,117,118,119,120,122,123,124,125,126Sn, 121,123,124,125,126Sb, 120,122,123,124,125,126,127,128,129,130,132Te, 127,129,130,131,135I, 123,124,126,128,129,130,131,132,133,134,135,136Xe, 133,134,135,136,137Cs, 130,132,133,134,135,136,137,138,140Ba, 138,139,140La, 136,138,139,140,141,142,143,144Ce, 141,142,143Pr, 142,143,144,145,146,147,148,150Nd, 147,148,149,151Pm, 144,147,148,149,150,151,152,153,154Sm, 151,152,153,154,155,156,157Eu, 152,153,154,155,156,157,158,160Gd, 159,160Tb, 156,158,160,161,162,163,164Dy, 165,166Ho, 162,164,166,167,168,170Er, 168,169,170Tm, 175,176Lu, 174,176,177,178,179,180Hf, 180,181,182Ta, 180,182,183,184,186W, 185,187Re, 191,193Ir, 197Au, 196,198,199,200,201,202,204Hg, 203,205Tl, 204,206,207,208Pb, 209Bi, 223,224,225,226Ra, 225,226,227Ac, 227,228,229,230,231,232,233,234Th, 229,230,231,232,233Pa, 230,231,232,233,234,235,236,237,238,239,240,241U, 234,235,236,237,238,239Np, 236,237,238,239,240,241,242,243,244,246Pu, 240,241,242,243,244Am, 240,241,242,243,244,245,246,247,248,249,250Cm, 245,246,247,249,250Bk, 246,248,249,250,251,252,253,254Cf, 251,252,253,254,255Es, 255Fm(n, γ), E=30 keV; calculated Maxwellian-averaged σ using ENDF/B-VII.1 evaluated neutron library. Comparison with ENDF/B-VII.0 and KADONIS values. NUCLEAR REACTIONS 227,228,229,230,231,232,233,234Th, 229,230,231,232,233Pa, 230,231,232,233,234,235,236,237,238,239,240,241U, 234,235,236,237,238,239Np, 236,237,238,239,240,241,242,243,244,246Pu, 240,241,242,243,244Am, 240,241,242,243,244,245,246,247,248,249,250Cm, 245,246,247,249,250Bk, 246,248,249,250,251,252,253,254Cf, 251,252,253,254,255Es, 255Fm(n, γ), (n, F), E=thermal; calculated thermal σ. Comparison with ENDF/B-VII.0, JENDL-4.0 and Atlas of Neutron Resonances values.
doi: 10.1016/j.nds.2011.11.002
2011HO19 Nucl.Data Sheets 112, 3075 (2011) S.Hoblit, Y.-S.Cho, M.Herman, C.M.Mattoon, S.F.Mughabghab, P.Oblozinsky, M.T.Pigni, A.A.Sonzogni Neutron Cross Section Covariances for Structural Materials and Fission Products
doi: 10.1016/j.nds.2011.11.006
2003BE57 Phys.Rev. C 68, 054607 (2003) V.Bellini, M.Capogni, A.Caracappa, L.Casano, A.D'Angelo, F.Ghio, B.Girolami, S.Hoblit, L.Hu, M.Khandaker, O.C.Kistner, L.Miceli, D.Moricciani, A.M.Sandorfi, C.Schaerf, C.E.Thorn Polarized Compton scattering from 4He in the Δ region NUCLEAR REACTIONS 4He(polarized γ, γ'), E=206-310 MeV; measured σ(θ), polarization asymmetries; deduced dipole and quadrupole contributions, related reaction mechanism features.
doi: 10.1103/PhysRevC.68.054607
2001BL09 Phys.Rev. C64, 025203 (2001) G.Blanpied, M.Blecher, A.Caracappa, R.Deininger, C.Djalali, G.Giordano, K.Hicks, S.Hoblit, M.Khandaker, O.C.Kistner, A.Kuczewski, F.Lincoln, M.Lowry, M.Lucas, G.Matone, L.Miceli, B.M.Preedom, D.Rebreyend, A.M.Sandorfi, C.Schaerf, R.M.Sealock, H.Stroher, C.E.Thorn, S.T.Thornton, J.Tonnison, C.S.Whisnant, H.Zhang, X.Zhao, and the LEGS Collaboration N → Δ Transition and Proton Polarizabilities from Measurements of p(γ(pol), γ), p(γ(pol), π0), and p(γ(pol), π+) NUCLEAR REACTIONS 1H(polarized γ, γ), (polarized γ, π0), (polarized γ, π+), E=213-333 MeV; measured σ, σ(E, θ), asymmetries; deduced Δ resonance excitation mixing ratio, helicity amplitudes, quadrupole moment. 1H deduced spin polarizabilities, Baldin sum rule. Multipole analysis, comparison with previous data.
doi: 10.1103/PhysRevC.64.025203
2000BL02 Phys.Rev. C61, 024604 (2000) G.Blanpied, M.Blecher, A.Caracappa, C.Djalali, M.-A.Duval, G.Giordano, K.Hicks, S.Hoblit, M.Khandaker, O.C.Kistner, G.Matone, L.Miceli, W.K.Mize, C.Molinari, B.M.Preedom, A.M.Sandorfi, C.Schaerf, R.M.Sealock, D.Rebreyend, C.E.Thorn, S.T.Thornton, K.Vaziri, C.S.Whisnant, X.Zhao, and the LEGS Collaboration Measurement of 2H(γ(pol), p)n with Linearly Polarized Photons in the Δ Resonance Region NUCLEAR REACTIONS 2H(polarized γ, p), E=110-315 MeV; measured proton spectra, polarization dependent and independent σ(θ), integrated σ, beam asymmetry; deduced Δ resonance role. Coupled-channels calculations, comparisons with previous results.
doi: 10.1103/PhysRevC.61.024604
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
2000HO14 Prog.Part.Nucl.Phys. 44, 149 (2000) Scattering of Real Photons and the Structure of Baryons NUCLEAR REACTIONS 1H(γ, γ'), (polarized γ, γ'), E=230, 287, 323 MeV; analyzed σ(θ), related data; deduced proton spin polarizability parameters.
doi: 10.1016/S0146-6410(00)00067-3
1999BE05 Nucl.Phys. A646, 55 (1999) V.Bellini, M.Capogni, A.Caracappa, L.Casano, A.D'Angelo, F.Ghio, B.Girolami, S.Hoblit, L.Hu, M.Khandaker, O.C.Kistner, L.Miceli, D.Moricciani, A.M.Sandorfi, C.Schaerf, M.L.Sperduto, C.E.Thorn Coherent π0 Photo-Production on 4He at Intermediate Energies with Polarized Photons NUCLEAR REACTIONS 4He(polarized γ, π0), E=206-322 MeV; measured unpolarized pions σ(θ), photon beam asymmetry. Test of Δ-hole model. Tagged photon beam.
doi: 10.1016/S0375-9474(98)00628-9
1998TO09 Phys.Rev.Lett. 80, 4382 (1998) J.Tonnison, A.M.Sandorfi, S.Hoblit, A.M.Nathan First Extraction of a Spin Polarizability of the Proton NUCLEAR REACTIONS 1H(γ, X), E=33-309 MeV; analyzed data; deduced proton backward spin polarizability. Dispersion analysis.
doi: 10.1103/PhysRevLett.80.4382
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
1996BL03 Phys.Rev.Lett. 76, 1023 (1996) G.Blanpied, M.Blecher, A.Caracappa, C.Djalali, G.Giordano, K.Hicks, S.Hoblit, M.Khandaker, O.C.Kistner, G.Matone, L.Miceli, C.Molinari, B.Preedom, D.Rebreyend, A.M.Sandorfi, C.Schaerf, R.M.Sealock, H.Stroher, C.E.Thorn, S.T.Thornton, C.S.Whisnant, H.Zhang, X.Zhao, and the LEGS Collaboration Polarized Compton Scattering from the Proton NUCLEAR REACTIONS 1H(polarized γ, γ), E=213-333 MeV; measured σ(θ), asymmetry vs E, Compton scattering; deduced resolution of earlier data problems. Model analysis.
doi: 10.1103/PhysRevLett.76.1023
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
1995BL13 Phys.Rev. C52, R455 (1995) G.Blanpied, M.Blecher, A.Caracappa, C.Djalali, M.-A.Duval, G.Giordano, K.Hicks, S.Hoblit, M.Khandaker, O.C.Kistner, G.Matone, L.Miceli, W.K.Mize, B.M.Preedom, D.Rebreyend, A.M.Sandorfi, C.Schaerf, R.M.Sealock, C.E.Thorn, S.T.Thornton, K.Vaziri, C.S.Whisnant, X.Zhao, P.Wilhelm, H.Arenhovel, and the LEGS Collaboration New Measurements of 2H(polarized γ, p)n and Spin Problems in Coupled NΔ/NN Interactions NUCLEAR REACTIONS, ICPND 2H(polarized γ, p), E=113-315 MeV; measured σ(θ) vs E, σ(E). Tagged beam. NΔ/NN coupled-channel analysis.
doi: 10.1103/PhysRevC.52.R455
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
1992BL12 Phys.Rev.Lett. 69, 1880 (1992) G.Blanpied, M.Blecher, A.Caracappa, C.Djalali, M.-A.Duval, G.Giordano, S.Hoblit, M.Khandaker, O.C.Kistner, G.Matone, L.Miceli, W.K.Mize, B.M.Preedom, A.M.Sandorfi, C.Schaerf, R.M.Sealock, C.E.Thorn, S.T.Thornton, K.Vaziri, C.S.Whisnant, X.Zhao, M.A.Moinester, and the LEGS Collaboration p(γ(pol), π0) Reaction and the E2 Excitation of the Δ NUCLEAR REACTIONS 1H(polarized γ, π0), E=243, 314 MeV; measured σ(θ); deduced E2 δ excitation.
doi: 10.1103/PhysRevLett.69.1880
1991BL11 Phys.Rev.Lett. 67, 1206 (1991) G.S.Blanpied, M.Blecher, A.Caracappa, C.Djalali, M.-A.Duval, G.Giordano, S.Hoblit, O.C.Kistner, G.Matone, L.Miceli, W.K.Mize, B.M.Preedom, A.M.Sandorfi, C.Schaerf, R.M.Sealock, C.E.Thorn, S.T.Thornton, K.Vaziri, C.S.Whisnant, and the LEGS Collaboration Beam-Polarization Observables in D(γ(pol), p)n and the Nuclear Tensor Force NUCLEAR REACTIONS 2H(polarized γ, p), E=191-222 MeV; measured σ(θ), asymmetry, polarization difference vs θ; deduced short-range tensor interaction role.
doi: 10.1103/PhysRevLett.67.1206
1991HO14 Nucl.Phys. A527, 358c (1991) S.Hoblit, G.Blanpied, M.Blecher, A.Caracappa, C.Djalali, M.-A.Duval, G.Giordano, O.C.Kistner, G.Matone, W.K.Mize, L.Miceli, B.M.Preedom, A.M.Sandorfi, C.Schaerf, R.M.Sealock, C.E.Thorn, S.T.Thornton, K.Vaziri, C.S.Whisnant Photon-Beam Polarization Asymmetries in d(γ(pol), p)n NUCLEAR REACTIONS 2H(polarized γ, p), E not given; measured polarization asymmetry; deduced meson exchange, Δ-isobar currents role.
doi: 10.1016/0375-9474(91)90125-P
1991HO19 Phys.Rev. C44, 2372 (1991) Photon-Decay Modes of the Giant Dipole Resonance in Even-A Nd Isotopes NUCLEAR REACTIONS 142,146,148,150Nd(γ, γ), (γ, γ'), E < 20 MeV; measured Eγ, Iγ, σ(E). 142,146,148,150Nd deduced coupling of GDR to surface modes, dipole transition strength distribution.
doi: 10.1103/PhysRevC.44.2372
1990BL17 J.Phys.(Paris), Colloq.C-6, 483 (1990) G.Blanpied, M.Blecher, A.Caracappa, C.Djalali, M.A.Duval, G.Giordano, S.Hoblit, O.K.Kistner, G.Matone, L.Miceli, W.K.Mize, B.M.Preedom, A.M.Sandorfi, C.Schaerf, R.M.Sealock, C.E.Thorn, S.T.Thornton, C.S.Whisnant, D.Babusci, L.Casano, S.d'Angelo, B.Girolami, P.Picozza Physics with Polarized Photons NUCLEAR REACTIONS 2H(polarized γ, p), E=206 MeV; measured longitudinal, transverse σ(θ) difference. Preliminary results, other data discussed. Model comparison.
1990HE03 Nucl.Phys. A506, 223 (1990) R.D.Heil, B.Kasten, W.Scharfe, P.A.Butler, H.Friedrichs, S.D.Hoblit, U.Kneissl, S.Lindenstruth, M.Ludwig, G.Muller, H.H.Pitz, K.W.Rose, M.Schumacher, U.Seemann, J.Simpson, P.von Brentano, Th.Weber, C.Wesselborg, A.Zilges Parity Assignments in Nuclear Resonance Fluorescence Experiments Using Compton Polarimeters NUCLEAR REACTIONS 142,150Nd, 232Th(γ, γ'), E=4.1 MeV bremsstrahlung; measured Eγ, Iγ, asymmetry, linear polarization. 142,150Nd, 232Th deduced levels, J, π, Γ0, (Γ0)2/Γ0.
doi: 10.1016/0375-9474(90)90384-X
1990PI04 Nucl.Phys. A509, 587 (1990); Errata Nucl.Phys. A514, 749 (1990) H.H.Pitz, R.D.Heil, U.Kneissl, S.Lindenstruth, U.Seemann, R.Stock, C.Wesselborg, A.Zilges, P.von Brentano, S.D.Hoblit, A.M.Nathan Low-Energy Photon Scattering Off 142, 146, 148, 150Nd: An investigation in the mass region of a nuclear shape transition NUCLEAR REACTIONS 142,146,148,150Nd(γ, γ'), E=4.1 MeV bremsstrahlung; measured Eγ, Iγ, γ(θ). 142,146,148,150Nd deduced levels, J, π, Γ0, B(λ). Enriched targets.
doi: 10.1016/0375-9474(90)90092-Z
1990WI15 Phys.Rev. C42, 2148 (1990) W.Wilke, U.Kneissl, Th.Weber, H.Stroher, L.S.Cardman, P.T.Debevec, S.D.Hoblit, R.T.Jones, A.M.Nathan Photofission of 238U with Monochromatic Gamma Rays in the Energy Range 11-16 MeV NUCLEAR REACTIONS 238U(γ, F), E=11-16 MeV; measured fission fragment σ(θ), fragment mass distributions; deduced anisotropy, fragment mass asymmetry relationship.
doi: 10.1103/PhysRevC.42.2148
1989AL01 Phys.Rev. C39, 324 (1989) R.Alarcon, A.M.Nathan, S.F.LeBrun, S.D.Hoblit Photon Scattering in the Giant Resonance Region of 24Mg, 28Si, and 32S NUCLEAR REACTIONS 24Mg, 28Si, 32S(γ, γ'), E=17-28 MeV; measured σ(θ) vs E. 24Mg, 28Si, 32S deduced GDR properties.
doi: 10.1103/PhysRevC.39.324
1989KA16 Phys.Rev.Lett. 63, 609 (1989); Erratum Phys.Rev.Lett. 63, 2695 (1989) B.Kasten, R.D.Heil, P.v.Brentano, P.A.Butler, S.D.Hoblit, U.Kneissl, S.Lindenstruth, G.Muller, H.H.Pitz, K.W.Rose, W.Scharfe, M.Schumacher, U.Seemann, Th.Weber, C.Wesselborg, A.Zilges Evidence for a Cluster of Collective 1+ States in 150Nd Near 3 MeV NUCLEAR REACTIONS 150Nd(γ, γ'), E=2.8-3.1 MeV bremsstrahlung; measured Eγ, Iγ, γ linear polarization, asymmetry. 150Nd deduced levels, J, π, B(λ), (Γ02/Γ). Compton polarimeters.
doi: 10.1103/PhysRevLett.63.609
1988DA20 Phys.Lett. 214B, 329 (1988) D.S.Dale, A.M.Nathan, F.J.Federspiel, S.D.Hoblit, J.Hughes, D.Wells Elastic Photon Scattering 209Bi: Meson exchange contributions to the dipole sum and the orbital g factor NUCLEAR REACTIONS 209Bi(γ, γ), E=12-18 MeV; measured σ(θ). 209Bi deduced ehancement to sum rule near GDR.
doi: 10.1016/0370-2693(88)91372-X
1988LA23 Phys.Rev.Lett. 61, 1710 (1988) R.M.Laszewski, R.Alarcon, D.S.Dale, S.D.Hoblit Distribution of M1 Transitions in 208Pb NUCLEAR REACTIONS 208Pb(polarized γ, γ'), E=5.8-7.6 MeV; measured σ(Eγ, E), asymmetry. 208Pb deduced B(M1) distribution. Linearly polarized tagged photon beam.
doi: 10.1103/PhysRevLett.61.1710
1987AL16 Phys.Rev. C36, 954 (1987) R.Alarcon, R.M.Laszewski, A.M.Nathan, S.D.Hoblit Photon Scattering from 90Zr below Neutron Emission Threshold NUCLEAR REACTIONS 90Zr(γ, γ), (γ, γ'), E=8.1-10.5 MeV; measured elastic, inelastic σ(E); deduced total σ(E). 90Zr deduced B(E1), GDR dominance.
doi: 10.1103/PhysRevC.36.954
1987BI15 Phys.Rev. C36, 1293 (1987) Y.Birenbaum, R.Alarcon, S.D.Hoblit, R.M.Laszewski, A.M.Nathan Photon Scattering on 238U and the Interpretation of Near-Threshold Photofission Resonances NUCLEAR REACTIONS 238U(γ, γ), E=4.8-6.4 MeV; measured σ(E, θ=135°); deduced total σ(E). 238U deduced fission transmission factors.
doi: 10.1103/PhysRevC.36.1293
1987LA19 Phys.Rev.Lett. 59, 431 (1987) R.M.Laszewski, R.Alarcon, S.D.Hoblit Giant M1 Resonance in 90Zr NUCLEAR REACTIONS 90Zr(polarized γ, γ), E=8.1-10.5 MeV; measured σ(E), γ asymmetry vs E. 90Zr deduced giant M1 transition strength distribution.
doi: 10.1103/PhysRevLett.59.431
1987LE12 Phys.Rev. C35, 2005 (1987) S.F.LeBrun, A.M.Nathan, S.D.Hoblit Photon Scattering in the Giant Dipole Resonance Region of 16O NUCLEAR REACTIONS 16O(γ, γ), E=21.7-27.5 MeV; measured σ(θγ) vs Eγ; deduced photoabsorption σ(E). 16O deduced GDR components, Γ. Water target, NaI detector.
doi: 10.1103/PhysRevC.35.2005
1986LA31 Phys.Rev. C34, 2013 (1986) R.M.Laszewski, P.Rullhusen, S.D.Hoblit, S.F.LeBrun Giant M1 Resonance in 140Ce NUCLEAR REACTIONS 140Ce(polarized γ, γ), E=6.7-8.7 MeV; measured σ, γ asymmetry. 140Ce deduced M1 transition strength, giant resonance. NaI detector.
doi: 10.1103/PhysRevC.34.2013
1986NA13 Phys.Rev. C34, 480 (1986) A.M.Nathan, P.L.Cole, P.T.Debevec, S.D.Hoblit, S.F.LeBrun, D.H.Wright Photon Scattering from 206Pb NUCLEAR REACTIONS 206Pb(γ, γ'), E=12-30 MeV; measured σ(θ) vs E. 206Pb deduced GDR properties. Tagged photons.
doi: 10.1103/PhysRevC.34.480
1985LA02 Phys.Rev.Lett. 54, 530 (1985) R.M.Laszewski, P.Rullhusen, S.D.Hoblit, S.F.LeBrun Giant M1 Resonance in Pb NUCLEAR REACTIONS 206Pb(polarized γ, γ), E=6.7-8.1 MeV; measured σ(E), asymmetry vs Eγ. 206Pb deduced B(M1) distribution strength.
doi: 10.1103/PhysRevLett.54.530
1985LA07 Nucl.Instrum.Methods 228, 334 (1985) R.M.Laszewski, P.Rullhusen, S.D.Hoblit, S.F.Lebrun Enhanced Linear Polarization for Tagged Photon Beams NUCLEAR REACTIONS 24Mg(polarized γ, γ), E=10.7 MeV; 28Si(polarized γ, γ), E=11.4 MeV; measured asymmetry ratio. Tagged linearly polarized beam.
doi: 10.1016/0168-9002(85)90278-5
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