NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = J.R.Calarco Found 54 matches. 2010CR03 Phys.Rev. C 82, 045211 (2010) C.Crawford, T.Akdogan, R.Alarcon, W.Bertozzi, E.Booth, T.Botto, J.R.Calarco, B.Clasie, A.DeGrush, T.W.Donnelly, K.Dow, M.Farkhondeh, R.Fatemi, O.Filoti, W.Franklin, H.Gao, E.Geis, S.Gilad, D.Hasell, P.Karpius, M.Kohl, H.Kolster, T.Lee, E.Lomon, A.Maschinot, J.Matthews, K.McIlhany, N.Meitanis, R.Milner, J.Rapaport, R.Redwine, J.Seely, A.Shinozaki, A.Sindile, S.Sirca, E.Six, T.Smith, B.Tonguc, C.Tschalaer, E.Tsentalovich, W.Turchinetz, Y.Xiao, W.Xu, C.Zhang, Z.Zhou, V.Ziskin, T.Zwart Role of mesons in the electromagnetic form factors of the nucleon
doi: 10.1103/PhysRevC.82.045211
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
2006GU08 Phys.Rev. C 73, 035501 (2006) V.Gudkov, G.L.Greene, J.R.Calarco General classification and analysis of neutron β-decay experiments RADIOACTIVITY 1n(β-); analyzed angular correlations, radiative and recoil corrections, sensitivity to new physics.
doi: 10.1103/PhysRevC.73.035501
2005WI18 J.Res.Natl.Inst.Stand.Technol. 110, 389 (2005) W.S.Wilburn, J.D.Bowman, G.S.Mitchell, J.M.O'Donnell, S.I.Penttila, P.-N.Seo, J.R.Calarco, F.W.Hersmann, T.E.Chupp, T.V.Cianciolo, K.P.Rykaczewski, G.R.Young, R.T.De Souza, W.M.Snow, D.Desai, G.L.Greene, R.K.Grzywacz, E.Frlez, D.Pocanic, T.R.Gentile, V.Gudkov, G.L.Jones Measurement of Neutron Decay Parameters-The abBA Experiment
doi: 10.6028/jres.110.058
1999MO02 Phys.Rev. C59, 221 (1999) J.H.Morrison, H.Baghaei, W.Bertozzi, S.Gilad, J.Glickman, C.E.Hyde-Wright, N.Kalantar-Nayestanaki, R.W.Lourie, S.Penn, P.E.Ulmer, L.B.Weinstein, B.H.Cottman, L.Ghedira, E.J.Winhold, J.R.Calarco, J.Wise, P.Boberg, C.C.Chang, D.Zhang, K.Aniol, M.B.Epstein, D.J.Margaziotis, J.M.Finn, C.Perdrisat, V.Punjabi Quasielastic 12C(e, e'p) Reaction at High Momentum Transfer NUCLEAR REACTIONS 12C(e, e'p), E=696, 796 MeV; measured σ(θ(p), θ(e), E) vs missing energy; deduced relative importance of single- and multi-nucleon knockout, dependence on energy transfer.
doi: 10.1103/PhysRevC.59.221
1995DE23 Phys.Rev. C52, 61 (1995) D.J.DeAngelis, J.R.Calarco, J.E.Wise, H.J.Emrich, R.Neuhausen, H.Weyand Multipole Strength in 12C from the (e, e'α) Reaction for Momentum Transfers up to 0.61 fm -1 NUCLEAR REACTIONS 12C(e, e'p), (e, e'α), E=124.1, 183.4 MeV; measured σ(θ(e'), θ(α)), σ(θ(e'), θ(p)) vs energy transfer. 12C deduced B(E2), EWSR strength.
doi: 10.1103/PhysRevC.52.61
1995KE03 Phys.Lett. 344B, 79 (1995) L.J.H.M.Kester, W.H.A.Hesselink, N.Kalantar-Nayestanaki, J.H.Mitchell, A.Pellegrino, E.Jans, J.Konijn, J.J.M.Steijger, J.L.Visschers, A.Zondervan, J.R.Calarco, D.DeAngelis, F.W.Hersman, W.Kim, Th.S.Bauer, M.W.Kelder, Z.Papandreou, J.Ryckebusch, C.Ciofi degli Atti, S.Simula Two-Nucleon Knock-Out Investigated with the Semi-Exclusive 12C(e, e'p) Reaction NUCLEAR REACTIONS 12C(e, e'p), E=475 MeV; measured σ(E(e'), θ(e'), θp) vs missing energy; deduced virtual photon coupling to pion exchange currents, Δ-excitation roles.
doi: 10.1016/0370-2693(94)01583-X
1995KE06 Phys.Rev.Lett. 74, 1712 (1995) L.J.H.M.Kester, W.H.A.Hesselink, N.Kalantar-Nayestanaki, J.H.Mitchell, A.Pellegrino, E.Jans, J.Konijn, J.J.M.Steijger, J.L.Visschers, A.Zondervan, J.R.Calarco, D.DeAngelis, F.W.Hersman, W.Kim, Th.S.Bauer, M.W.Kelder, Z.Papandreou, C.Giusti, F.D.Pacati Short-Range Nucleon-Nucleon Correlations Investigated with the Reaction 12C(e, e'pp) NUCLEAR REACTIONS 12C(e, e'2p), E=475 MeV; measured σ(E(e'), (θp)1, (θp)2, θ(e'), (Ep1), (Ep2)); deduced short range nucleon-nucleon correlations role in two-nucleon knockout.
doi: 10.1103/PhysRevLett.74.1712
1995ZO01 Nucl.Phys. A587, 697 (1995) A.Zondervan, L.J.de Bever, E.Jans, J.Konijn, M.Kruijer, J.J.M.Steijger, J.L.Visschers, P.J.Countryman, W.H.A.Hesselink, N.Kalantar-Nayestanaki, L.J.H.M.Kester, J.H.Mitchell, A.Pellegrino, J.R.Calarco, F.W.Hersman, M.Leuschner, T.P.Smith, Th.S.Bauer, M.W.Kelder, C.Giusti, F.D.Pacati, J.Ryckebusch, M.Vanderhaeghen The 12C(e, e'p) and 12C(e, e'pp) Reactions in the Δ-Resonance Region NUCLEAR REACTIONS 12C(e, e'p), (e, e'2p), E ≈ Δ resonance; measured six-fold, ninefold differential σ; deduced reaction mechanism. Model comparison.
doi: 10.1016/0375-9474(95)00044-2
1994CA08 Nucl.Phys. A569, 363c (1994) Putting the Giant Resonance Under the Electron Microscope NUCLEAR REACTIONS 12C(e, e'p), E=86 MeV; analyzed (e'p)(θ) data; deduced giant resonances study implications.
doi: 10.1016/0375-9474(94)90127-9
1994LE02 Phys.Rev. C49, 955 (1994) M.Leuschner, J.R.Calarco, F.W.Hersman, E.Jans, G.J.Kramer, L.Lapikas, G.van der Steenhoven, P.K.A.de Witt Huberts, H.P.Blok, N.Kalantar-Nayestanaki, J.Friedrich Quasielastic Proton Knockout from 16O NUCLEAR REACTIONS 16O(e, e'p), E=304-521 MeV; measured missing mass spectra, quasielastic σ; deduced proton spectral function, momentum distributions. 15N levels deduced spectroscopic factors.
doi: 10.1103/PhysRevC.49.955
1993DE10 Phys.Rev.Lett. 70, 2872 (1993) D.De Angelis, J.R.Calarco, J.E.Wise, H.J.Emrich, R.Neuhausen, H.Weyand Isoscalar E2 Strength in 12C from the (e, e'α) Reaction NUCLEAR REACTIONS 12C(e, e'α), E=124.1-183.4 MeV; measured σ(θ(e), θ(α)) vs energy transfer. 12C deduced GQR associated EWSR, B(E2).
doi: 10.1103/PhysRevLett.70.2872
1993KE02 Nucl.Phys. A553, 709c (1993) L.J.H.M.Kester, Th.S.Bauer, J.R.Calarco, P.C.Countryman, W.H.A.Hesselink, F.W.Hersman, E.Jans, N.Kalantar-Nayestanaki, M.W.Kelder, W.Kim, J.Konijn, M.Kruijer, J.M.Mitchell, Z.Papandreou, A.Pellegrino, J.J.M.Steijger, J.L.Visschers, A.Zondervan The Reactions 12C(e, e'pp) and 12C(e, e'p) in the Dip Region NUCLEAR REACTIONS 12C(e, e'p), (e, e'2p), E=470 MeV; measured missing energy spectrum, pp-correlations; deduced clear pp-correlation evidence.
doi: 10.1016/0375-9474(93)90685-Q
1993WE01 Phys.Rev. C47, 225 (1993) L.B.Weinstein, J.Morrison, A.Perry, H.Baghaei, W.Bertozzi, W.U.Boeglin, J.M.Finn, J.Glickman, C.E.Hyde-Wright, N.Kalantar-Nayestanaki, R.W.Lourie, J.A.Nelson, S.Penn, W.W.Sapp, C.P.Sargent, P.E.Ulmer, B.H.Cottman, L.Ghedira, E.J.Winhold, J.R.Calarco, J.Wise, P.Boberg, C.C.Chang, N.S.Chant, P.G.Roos, D.Chang, K.Aniol, M.B.Epstein, D.J.Margaziotis, C.Perdrisat, V.Punjabi, R.Whitney N(*) Electroproduction and Propagation in Nuclei NUCLEAR REACTIONS 12C(γ, π-X), E=virtual bremsstrahlung; measured σ vs missing energy with p-emission; deduced N(*)-nucleus interaction features.
doi: 10.1103/PhysRevC.47.225
1993WI08 Phys.Rev. C47, 2539 (1993) J.E.Wise, J.R.Calarco, J.P.Connelly, S.A.Fayans, F.W.Hersman, J.H.Heisenberg, R.S.Hicks, W.Kim, T.E.Milliman, R.A.Miskimen, G.A.Peterson, A.P.Platonov, E.E.Saperstein, R.P.Singhal Ground-State Magnetization Density of 89Y NUCLEAR REACTIONS 89Y(e, e), E=71-262 MeV; measured σ(θ), θ=180°. 89Y deduced ground state M1 form factor. Fourier-Bessel analysis.
doi: 10.1103/PhysRevC.47.2539
1992FR05 Phys.Rev.Lett. 68, 1667 (1992) J.P.Fritsch, H.J.Emrich, A.Grasmuck, R.Neuhausen, S.Schardt, N.Zimmermann, J.R.Calarco, M.Potokar Isoscalar E2 Strength in 16O from the (e, e'α) Reaction NUCLEAR REACTIONS 16O(e, e'α), E=124.1, 183.4 MeV; measured σ(θ(e), θα). 16O deduced isoscalar electric quadrupole strength distribution.
doi: 10.1103/PhysRevLett.68.1667
1992HO08 Phys.Rev. C46, 499 (1992) D.J.Horen, C.L.Morris, S.J.Seestrom, F.W.Hersman, J.R.Calarco, M.Holtrop, M.Leuschner, M.Rawool-Sullivan, R.W.Garnett, S.J.Greene, M.A.Plum, J.D.Zumbro Isospin Character of the Transition to the 0.803-MeV State in 206Pb from π± Scattering at 180 MeV NUCLEAR REACTIONS 206Pb(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=180 MeV; measured missing mass spectra, σ(θ). 206Pb deduced neutron, proton matrix elements ratio for quadrupole, octupole transitions. Deformed optical model, DWIA analyses.
doi: 10.1103/PhysRevC.46.499
1992KI10 Phys.Rev. C45, 2290 (1992) W.Kim, B.L.Miller, J.R.Calarco, L.S.Cardman, J.P.Connelly, S.A.Fayans, B.Frois, D.Goutte, J.H.Heisenberg, F.W.Hersman, V.Meot, T.E.Milliman, P.Mueller, C.N.Papanicolas, A.P.Platonov, V.Yu.Ponomarev, J.E.Wise Interplay between Single-Particle and Collective Degrees of Freedom in the Excitation of the Low-Lying States in 140Ce NUCLEAR REACTIONS 140Ce(e, e'), E=190 MeV; measured σ(E(e')), θ=45°. 140Ce levels deduced form factors, transition charge densities, B(λ), configurations. Quasiparticle-phonon model, self-consistent finite Fermi system theory.
doi: 10.1103/PhysRevC.45.2290
1991KI13 Phys.Rev. C44, 2400 (1991) W.Kim, J.R.Calarco, J.P.Connelly, J.H.Heisenberg, F.W.Hersman, T.E.Milliman, J.E.WIse, B.L.Miller, C.N.Papanicolas, V.Yu.Ponomarev, E.E.Saperstein, A.P.Platonov Properties of Low-Lying States in 142Ce via High Resolution Electron Scattering NUCLEAR REACTIONS 142Ce(e, e'), E=100-370 MeV; measured reaction products, Eβ, Iβ; deduced σ(E(e'), θ=45°), form factors, B(E2). 142Ce levels deduced charge densities. Quasiparticle-phonon approach, finite Fermi system.
doi: 10.1103/PhysRevC.44.2400
1991PO06 Nucl.Phys. A527, 372c (1991) M.Potokar, J.R.Calarco, J.E.Wise, N.Zimmermann, H.Weyand, H.J.Emrich, J.P.Fritsch, A.Grasmuck, R.Neuhausen, S.Schardt Separation of the Longitudinal and Transverse Amplitudes for the Giant Dipole Resonances of 12C and 16O from Measurement of the (e, e'p0) Angular Correlations NUCLEAR REACTIONS 12C, 16O(e, e'p), E not given; measured σ(θ(e'), θ(p)) vs energy transfer. 12C, 16O deduced GDR amplitudes features.
doi: 10.1016/0375-9474(91)90126-Q
1991WE10 Nucl.Phys. A527, 348c (1991) L.B.Weinstein, H.Baghaei, W.Bertozzi, J.M.Finn, J.Glickman, C.E.Hyde-Wright, N.Kalantar-Nayestanaki, R.W.Lourie, J.A.Nelson, W.W.Sapp, C.P.Sargent, P.E.Ulmer, B.H.Cottman, L.Ghedira, E.J.Winhold, J.R.Calarco, J.Wise, P.Boberg, C.C.Chang, D.Zhang, D.Zhang, K.Aniol, M.B.Epstein, D.J.Margaziotis, C.Perdrisat, V.Punjabi Non-Single-Particle Interactions at Quasi-Elastic Kinematics NUCLEAR REACTIONS 12C(e, e'p), E=460 MeV; measured σ(θp, θ(e')) vs missing energy; deduced deeply bound deuteron knockout. Compiled, reviewed other data.
doi: 10.1016/0375-9474(91)90124-O
1990CO05 Phys.Rev. C41, 1039 (1990) P.J.Countryman, K.A.Griffioen, K.Van Bibber, M.R.Yearian, J.R.Calarco Direct Measurement of the Branching Ratio Γn/Γf of 238U in Inelastic Alpha Scattering in the Giant Resonance Region NUCLEAR REACTIONS 238U(α, α'F), E=120 MeV; measured σ(fragment θα, E, En) following fission. 238U deduced Γn/Γ(F) near giant resonances, B(λ), sum rule exhaustion.
doi: 10.1103/PhysRevC.41.1039
1990HA09 Phys.Rev. C41, 1619 (1990) K.Hansen, J.-O.Adler, K.I.Blomqvist, D.Nilsson, A.Sandell, B.Schroder, W.R.Dodge, J.W.Lightbody, Jr., J.S.O'Connell, J.R.Calarco, J.P.Connelly, F.W.Hersman, W.Kim, M.Leuschner Electrofission in the Quasifree and Delta Regions NUCLEAR REACTIONS 233,238U(e, e'F), E=720-830 MeV; measured σ(E, θ), fission probability; deduced mean nuclear excitation energy. Parallel plate avalanche detector.
doi: 10.1103/PhysRevC.41.1619
1990WE06 Phys.Rev.Lett. 64, 1646 (1990) L.B.Weinstein, H.Baghaei, W.Bertozzi, J.M.Finn, J.Glickman, C.E.Hyde-Wright, N.Kalantar-Nayestanaki, R.W.Lourie, J.A.Nelson, W.W.Sapp, C.P.Sargent, P.E.Ulmer, B.H.Cottman, L.Ghedira, E.J.Winhold, J.R.Calarco, J.Wise, P.Boberg, C.C.Chang, D.Zhang, K.Aniol, M.B.Epstein, D.J.Margaziotis, C.Perdrisat, V.Punjabi Quasielastic Reaction Mechanism Studied Using the Reaction 12C(e, e'p) NUCLEAR REACTIONS 12C(e, e'p), E not given; measured missing energy spectra; deduced subshell spectroscopic factors.
doi: 10.1103/PhysRevLett.64.1646
1990WI13 Phys.Rev. C42, 1077 (1990) J.E.Wise, F.W.Hersman, J.H.Heisenberg, T.E.Milliman, J.P.Connelly, J.R.Calarco, C.N.Papanicolas Single-Particle Excitations in 89Y NUCLEAR REACTIONS 89Y(e, e'), E=370.9, 622.8 MeV; measured σ(θ), form factors. 89Y deduced transition charge, current densities. DWBA analysis, shell model. NUCLEAR STRUCTURE 89Y; calculated levels, transition charge, current densities. Shell model.
doi: 10.1103/PhysRevC.42.1077
1989BA03 Phys.Rev. C39, 177 (1989) H.Baghaei, W.Bertozzi, K.I.Blomqvist, J.M.Finn, J.Flanz, C.E.Hyde-Wright, N.Kalantar-Nayestanaki, R.W.Lourie, J.Nelson, W.W.Sapp, C.P.Sargent, P.Ulmer, L.Weinstein, B.H.Cottman, P.K.Teng, E.J.Winhold, M.Yamazaki, J.R.Calarco, F.W.Hersman, C.Perdrisat, V.Punjabi, M.Epstein, D.J.Margaziotis Electroexcitation of the Δ Resonance in the (e, e'p) Reaction NUCLEAR REACTIONS 12C(e, e'p), E=460, 647; measured σ(E(e'), θp, θ(e')) vs missing energy; deduced reaction mechanism.
doi: 10.1103/PhysRevC.39.177
1989GR01 Phys.Rev.Lett. 62, 689 (1989) K.A.Griffioen, K.Van Bibber, J.R.Calarco Transition Radii and Sum Rules in 238U(e, e'F) NUCLEAR REACTIONS 238U(e, e'F), E not given; calculated, discussed transition radii, sum rules for E1, E2, E3 and E0.
doi: 10.1103/PhysRevLett.62.689
1988KU08 Phys.Rev. C37, 2281 (1988) P.M.Kurjan, J.R.Calarco, G.A.Fisher, S.S.Hanna Giant E1 Resonances in 20Ne Observed with the 19F(p(pol), γ0γ1)20Ne Reactions NUCLEAR REACTIONS, ICPND 19F(polarized p, γ), E=3-10 MeV; measured γ yield, σ(θγ). 20Ne deduced transition γ multipolarity, GDR features.
doi: 10.1103/PhysRevC.37.2281
1987UL03 Phys.Rev.Lett. 59, 2259 (1987) P.E.Ulmer, H.Baghaei, W.Bertozzi, K.I.Blomqvist, J.M.Finn, C.E.Hyde-Wright, N.Kalantar-Nayestanaki, S.Kowalski, R.W.Lourie, J.Nelson, W.W.Sapp, C.P.Sargent, L.Weinstein, B.H.Cottman, P.K.Teng, E.J.Winhold, M.Yamazaki, J.R.Calarco, F.W.Hersman, J.J.Kelly, M.E.Schulze, G.Audit Missing-Energy Dependence of the Separated Response Functions for the Reaction 12C(e, e'p) NUCLEAR REACTIONS 12C(e, e'p), E=288, 443 MeV; measured transverse, longitudinal response functions, spectral function difference vs missing energy; deduced reaction mechanism.
doi: 10.1103/PhysRevLett.59.2259
1986CO10 Radiat.Eff. 92, 295 (1986) P.J.Countryman, K.A.Griffioen, N.Z.Oremland, K.van Bibber, M.R.Yearian, J.R.Calarco, J.G.Woodworth Measurement of the Neutron Spectra from the Decay of the Giant Quadrupole Resonance in 238U NUCLEAR REACTIONS 238U(α, α'F), (α, α'nF), E=120 MeV; measured fission(fragment)α-, n(fragment)(α)-coin, σ(Eα'). 238U deduced GQR neutron decay characteristics.
doi: 10.1080/00337578608208338
1986GR18 Phys.Rev. C34, 1375 (1986) K.A.Griffioen, P.J.Countryman, K.T.Knopfle, K.Van Bibber, M.R.Yearian, J.G.Woodworth, D.Rowley, J.R.Calarco Coincident Electrofission of 238U at q ≈ 0.26, 0.40, and 0.55 fm-1 NUCLEAR REACTIONS 238U(e, e'F), E=80.3, 81.6, 82.5, 118.4, 119.1, 120.7, 159.9, 163.8 MeV; measured σ(θ(e'), fragment θ) vs excitation following fission. 238U levels deduced transition radii, multipole fission probability, Γ, EWSR, strength functions, form factors. Magnetic spectrometer, parallel plate avalanche counter. Quasiparticle random phase approximation.
doi: 10.1103/PhysRevC.34.1375
1986LO03 Phys.Rev.Lett. 56, 2364 (1986); Erratum Phys.Rev.Lett. 57, 653 (1986) R.W.Lourie, H.Baghaei, W.Bertozzi, K.I.Blomqvist, J.M.Finn, C.E.Hyde-Wright, N.Kalantar-Nayestanaki, J.Nelson, S.Kowalski, C.P.Sargent, W.W.Sapp, P.Ulmer, J.Wiggins, B.H.Cottman, P.K.Teng, E.J.Winhold, M.Yamazaki, J.R.Calarco, F.W.Hersman, J.J.Kelly, M.E.Schulze Reaction 12C(e, e'p) in the Dip Region NUCLEAR REACTIONS 12C(e, e'p), E=459 MeV; measured missing energy spectra, e'p-coin; deduced reaction mechanism.
doi: 10.1103/PhysRevLett.56.2364
1985WO03 Phys.Lett. 153B, 226 (1985) J.G.Woodworth, D.Rowley, J.D.T.Arruda-Neto, P.J.Countryman, K.A.Griffioen, D.H.H.Hoffmann, K.T.Knopfle, K.Van Bibber, M.R.Yearian, J.R.Calarco The Inclusive Electrofission of 238U at Incident Energies Between 45 and 120 MeV NUCLEAR REACTIONS 238U(e, e'F), E=47.6-119.1 MeV; measured fission fragment (e')-coin, σ(E).
doi: 10.1016/0370-2693(85)90536-2
1984CA34 Phys.Lett. 146B, 179 (1984) J.R.Calarco, J.Arruda-Neto, K.A.Griffioen, S.S.Hanna, D.H.H.Hoffmann, B.Neyer, R.E.Rand, K.Wienhard, M.R.Yearian Observation of Monopole Strength in the 12C(e, e'p0)11B Reaction NUCLEAR REACTIONS 12C(e, e'p), E=86, 118, 126 MeV; measured σ(E(e'), θ(e'), θp), forward, backward asymmetry. 12C deduced possible monopole resonance, EWSR.
doi: 10.1016/0370-2693(84)91012-8
1984GR26 Phys.Rev.Lett. 53, 2382 (1984); Erratum Phys.Rev.Lett. 54, 852 (1985) K.A.Griffioen, P.J.Countryman, K.T.Knopfle, K.Van Bibber, M.R.Yearian, J.G.Woodworth, D.Rowley, J.R.Calarco Coincidence Electron Scattering (e, e'f) and Multipole Strength Functions in 238U NUCLEAR REACTIONS 238U(e, e'F), E=80.3, 118.4, 163.8 MeV; measured σ(θ(e'), E(e')), fission(fragment)(e)-coin. 238U deduced multipole strength function distributions, EWSR. Model-dependent form factors, least-squares fitting procedure.
doi: 10.1103/PhysRevLett.53.2382
1983CA08 Phys.Rev. C27, 1866 (1983) J.R.Calarco, B.L.Berman, T.W.Donnelly Implications of the Experimental Results on the Photodisintegration of 4He NUCLEAR REACTIONS 4He(γ, p), (γ, n), E=20-50 MeV; calculated σ(E), ratios; deduced nuclear force charge asymmetry. 4He deduced isospin mixing.
doi: 10.1103/PhysRevC.27.1866
1983CA14 Phys.Rev. C28, 483 (1983); Erratum Phys.Rev. C29, 672 (1983) J.R.Calarco, S.S.Hanna, C.C.Chang, E.M.Diener, E.Kuhlmann, G.A.Fisher Absolute Cross Section for the Reaction 3H(p, γ0)4He and a Review of 4He(γ, p0)3H Measurements NUCLEAR REACTIONS 3H(p, γ0), E=8.34, 13.6 MeV; measured σ(θ=90°).
doi: 10.1103/PhysRevC.28.483
1980CA11 Phys.Lett. 92B, 67 (1980) J.R.Calarco, P.M.Kurjan, G.A.Fisher, S.S.Hanna Intermediate Structure in the Giant E1 Resonance in the 19F(p, γ0)20Ne Reaction NUCLEAR REACTIONS 19F(p, γ), (polarized p, γ), E=3.5-10 MeV; measured σ(E, θ); deduced E1, E2 capture amplitudes, intermediate structure. Doorway resonances model.
doi: 10.1016/0370-2693(80)90305-6
1980SA29 Phys.Rev.Lett. 45, 1615 (1980) A.M.Sandorfi, J.R.Calarco, R.E.Rand, H.A.Schwettman Fission Modes of 24Mg NUCLEAR REACTIONS, Fission 24Mg(e, F), E=26-40 MeV; measured production σ(E) for α, 12C, 16O fragments. 24Mg deduced enhanced asymmetric fission, resonances, statistical giant resonance decay, clustering.
doi: 10.1103/PhysRevLett.45.1615
1979KU10 Phys.Rev. C20, 5 (1979) E.Kuhlmann, J.R.Calarco, V.K.C.Cheng, D.G.Mavis, J.R.Hall, S.S.Hanna E1 and E2 Strength in 32S and 34S Observed in α-Capture Reactions NUCLEAR REACTIONS 28Si(α, γ0), E=5-16 MeV; 30Si(α, γ0), E=4-15 MeV; measured σ(E, Eγ, θγ). 32,34S deduced E1, E2 strengths. Enriched targets.
doi: 10.1103/PhysRevC.20.5
1979PH04 Phys.Rev. C19, 2091 (1979) T.W.Phillips, B.L.Berman, D.D.Faul, J.R.Calarco, J.R.Hall 4He(γ, p)-to-(γ, n) Cross-Section Ratio NUCLEAR REACTIONS 4He(γ, 3He), (γ, t), E=31-51 MeV; measured σ(θ) ratio; deduced σ(γ, p)/σ(γ, n).
doi: 10.1103/PhysRevC.19.2091
1979VE02 Phys.Rev. C19, 1705 (1979) E.Ventura, J.R.Calarco, C.C.Chang, E.M.Diener, D.G.Mavis, S.S.Hanna, G.A.Fisher Structure in the Giant Resonance Region of 16O Observed with the Reaction 13C(3He, γ)16O NUCLEAR REACTIONS 13C(3He, γ), E=3.0-8.5 MeV; measured σ(E(3He), Eγ, θ). 16O deduced resonances, structure in giant resonance region. Enriched 13C target.
doi: 10.1103/PhysRevC.19.1705
1977CA21 Phys.Rev.Lett. 39, 925 (1977) J.R.Calarco, S.W.Wissink, M.Sasao, K.Wienhard, S.S.Hanna Structure in the Giant Dipole Resonance of 16O: Evidence for a Secondary Doorway State from Polarized-Proton Capture NUCLEAR REACTIONS 15N(polarized p, γ); measured σ. 16O deduced doorway state, parameters in GDR region.
doi: 10.1103/PhysRevLett.39.925
1977JA03 Phys.Rev.Lett. 38, 1201 (1977) M.J.Jakobson, G.R.Burleson, J.R.Calarco, M.D.Cooper, D.C.Hagerman, I.Halpern, R.H.Jeppesen, K.F.Johnson, L.D.Knutson, R.E.Marrs, H.O.Meyer, R.P.Redwine Neutron Radii of Calcium Isotopes from Pion Total Cross Section Measurements NUCLEAR REACTIONS 40,44,48Ca(π+, X), (π-, X), E=90-240 MeV; measured total σ(E) differences.
doi: 10.1103/PhysRevLett.38.1201
1976BR28 Phys.Rev. C14, 896 (1976) D.R.Brown, I.Halpern, J.R.Calarco, P.A.Russo, D.L.Hendrie, H.Homeyer Neutron Pickup by Alpha Particles to Unbound States NUCLEAR REACTIONS 12C, Rh, 208Pb, U(α, 5He), E=42, 90 MeV; measured αn-coin, σ.
doi: 10.1103/PhysRevC.14.896
1975KU06 Phys.Rev. C11, 1525 (1975) E.Kuhlmann, E.Ventura, J.R.Calarco, D.G.Mavis, S.S.Hanna E1 and E2 Strength in 24Mg and 26Mg Observed in α-Capture Reactions NUCLEAR REACTIONS 20Ne(α, γ), E=2.5-20 MeV; 22Ne(α, γ), E=4.5-16 MeV; measured σ(E, Eγ, θ(γ)). 24,26Mg deduced E1, E2 strength. Enriched targets.
doi: 10.1103/PhysRevC.11.1525
1974HA01 Phys.Rev.Lett. 32, 114 (1974) S.S.Hanna, H.F.Glavish, R.Avida, J.R.Calarco, E.Kuhlmann, R.LaCanna Evidence for a Giant Quadrupole Resonance in 16O NUCLEAR REACTIONS 15N(polarized p, γ), E=8.69, 12.6, 14.5 MeV; measured σ(E;θ), A(θ). 16O deduced resonances, J, π.
doi: 10.1103/PhysRevLett.32.114
1974SL01 Phys.Rev.Lett. 33, 784 (1974) D.C.Slater, J.R.Hall, J.R.Calarco, B.A.Watson, J.A.Becker Three-Body Breakup Reaction 40Ca(16O, 12Cα) NUCLEAR REACTIONS 40Ca(16O, α12C), E=64 MeV; measured α12C-coin; deduced reaction mechanism.
doi: 10.1103/PhysRevLett.33.784
1974WH01 Phys.Rev. C9, 156 (1974) W.R.Wharton, J.G.Cramer, J.R.Calarco, K.G.Nair Study of the 6Li(6Li, 6Li*(3.56))6Li*(3.56) and the 6Li(6Li, 6He)6Be Reactions NUCLEAR REACTIONS 6Li(6Li, 6Li'), (6Li, 6He), E=28-36 MeV; measured σ(E;θ).
doi: 10.1103/PhysRevC.9.156
1973VE09 Phys.Lett. 46B, 364 (1973) E.Ventura, J.R.Calarco, W.E.Meyerhof, A.M.Young Direct and Resonant Capture Observed in the 3H(3He, γ)6Li Reaction NUCLEAR REACTIONS 3H(3He, γ), E=0-30 MeV; calculated σ(E;θ).
doi: 10.1016/0370-2693(73)90141-X
1973WH02 Phys.Rev.Lett. 31, 54 (1973) W.R.Wharton, J.G.Cramer, D.H.Wilkinson, J.R.Calarco, K.G.Nair Measurement and Microscopic Analysis of the Reactions 6Li(6Li, 6Li*(3.56))6Li*(3.56) and 6Li(6Li, 6He)6Be NUCLEAR REACTIONS 6Li(6Li, 6Li'), 6Li(6Li, 6He), E=28-36 MeV; measured σ(E(6Li); E(6Li'), E(6He), σ(6Li), θ(6He)), DWBA microscopic analysis.
doi: 10.1103/PhysRevLett.31.54
1972HA52 Phys.Lett. 40B, 631 (1972) S.S.Hanna, H.F.Glavish, E.M.Diener, J.R.Calarco, C.C.Chang, R.Avida, R.N.Boyd The Giant Dipole Resonance in 16O Observed with the Polarized Proton Capture Reaction NUCLEAR REACTIONS 15N(polarized p, γ), E=7.4-15 MeV; measured σ(E), analyzing power(E;θ). 16O deduced giant E1 resonance structure.
doi: 10.1016/0370-2693(72)90614-4
1972LI16 Phys.Rev. C5, 1622 (1972) C.Ling, D.Bodansky, J.R.Calarco, J.M.Cameron Neutron-Gamma Competition Following (d, d') Reactions NUCLEAR REACTIONS 25Mg, 57Fe, 61Ni, 91Zr, 119Sn(d, d'n), E=19 MeV; measured σ(Ed', θ(d'), θ(n)), neutron fractional yields; deduced reaction mechanism.
doi: 10.1103/PhysRevC.5.1622
1971BR21 Nucl.Phys. A166, 515 (1971) W.J.Braithwaite, J.R.Calarco, J.M.Cameron, D.W.Storm Energy Dependence of Quasifree Scattering in the 2H(p, pn)p Reaction NUCLEAR REACTIONS 2H(p, pn), E=14, 17, 20, 23 MeV; measured σ(E;Ep, En, θ(p), θ(n)) for quasifree scattering.
doi: 10.1016/0375-9474(71)90903-1
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