NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = H.S.Caplan Found 45 matches. 1996FI01 Phys.Rev. C53, 1278 (1996) K.G.Fissum, H.S.Caplan, E.L.Hallin, D.M.Skopik, J.M.Vogt, M.Frodyma, D.P.Rosenzweig, D.W.Storm, G.V.O'Rielly, K.R.Garrow Inclusive Positive Pion Photoproduction NUCLEAR REACTIONS C, Ca, Sn, Pb(γ, π+X), E=184-213 MeV; measured inclusive pion production σ(E, θ), σ(θ), σ; deduced final state interactions role, pion absorption related features. Fermi gas model.
doi: 10.1103/PhysRevC.53.1278
1995IG01 Phys.Rev. C52, 755 (1995) R.Igarashi, J.C.Bergstrom, H.S.Caplan, K.G.E.Doss, E.L.Hallin, D.M.Skopik, D.Delli Carpini, E.C.Booth, E.K.McIntyre, J.P.Miller, M.A.Lucas, B.E.MacGibbon, A.M.Nathan, D.Wells Photon Scattering from 12C and 4He Nuclei Near the Δ(1232) Resonance NUCLEAR REACTIONS 12C(γ, γ), (γ, γ'), E=158.8-290.2 MeV bremsstrahlung; 4He(γ, γ), E=158.8 bremsstrahlung; measured σ(θ). Model comparison.
doi: 10.1103/PhysRevC.52.755
1994CH43 Nucl.Phys. A577, 213c (1994) H.Choi, K.Min, T.Kobayashi, P.F.Yergin, L.Y.Murphy, J.Shaw, H.Tsubota, K.Shoda, H.T.Chung, J.C.Kim, J.M.Vogt, E.M.Hallin, H.S.Caplan, J.C.Bergstrom, D.M.Skopik Positive Photopion Production from 12,13C using Tagged Photons NUCLEAR REACTIONS 13,12C(γ, π+), E=192 MeV; measured σ(θ). 12,13B deduced ΔS=1, ΔT=1 transition features.
doi: 10.1016/0375-9474(94)90858-3
1994RE04 Phys.Rev. C49, 1263 (1994) G.A.Retzlaff, H.S.Caplan, E.L.Hallin, D.M.Skopik, D.Beck, K.I.Blomqvist, G.Dodson, K.Dow, M.Farkhondeh, J.Flanz, S.Kowalski, W.W.Sapp, C.P.Sargent, D.Tieger, W.Turchinetz, C.F.Williamson, W.Dodge, X.K.Maruyama, J.W.Lightbody, Jr., R.Goloskie, J.McCarthy, T.S.Ueng, R.R.Whitney, B.Quinn, S.Dytman, K.Von Reden, R.Schiavilla, J.A.Tjon Threshold Electrodisintegration in the A = 3 System NUCLEAR REACTIONS 3He, 3H(e, e'X), E not given; measured double differential σ; deduced, analyzed longitudinal, transverse response functions. Models comparison.
doi: 10.1103/PhysRevC.49.1263
1993HA31 Phys.Rev. C48, 1497 (1993) E.L.Hallin, D.Amendt, J.C.Bergstrom, H.S.Caplan, R.Igarashi, D.M.Skopik, E.C.Booth, D.Delli Carpini, J.P.Miller, F.J.Federspiel, B.E.MacGibbon, A.M.Nathan Compton Scattering from the Proton NUCLEAR REACTIONS 1H(γ, γ), E=136-289 MeV bremsstrahlung; measured σ(θ), Compton scattering. 1H deduced electric, magnetic polarizabilities.
doi: 10.1103/PhysRevC.48.1497
1992CA30 Nucl.Instrum.Methods Phys.Res. A321, 109 (1992) E.B.Cairns, J.Cameron, C.Choi, H.W.Fielding, P.W.Green, L.G.Greeniaus, E.D.Hackett, L.Holm, N.R.Kolb, E.Korkmaz, P.P.Langill, W.J.McDonald, D.Mack, W.C.Olsen, B.A.Peterson, N.L.Rodning, J.Soukup, J.Zhu, D.Hutcheon, H.S.Caplan, R.E.Pywell, D.M.Skopik, J.M.Vogt, I.J.van Heerden The Saskatchewan-Alberta Large Acceptance Detector for Photonuclear Physics NUCLEAR REACTIONS 1H(p, p), E=220 MeV; measured σ(θ). 4π large acceptance detector.
doi: 10.1016/0168-9002(92)90380-M
1990CA24 Ann.Phys.(Paris) 15, 95 (1990) EROS: The machine and the physics NUCLEAR REACTIONS 2H(γ, 2p), E ≈ 300 MeV; measured reduced σ vs neutron momentum.
1987AS09 Nucl.Instrum.Methods Phys.Res. A259, 480 (1987) J.Asai, J.C.Bergstrom, H.S.Caplan, D.M.Skopik Kinematics for Chicane-Beam Electron Coincidence Experiments NUCLEAR REACTIONS 2H(e, e'p), E=400-700 MeV; 3He(e, e'π+), E=150-330 MeV; 12C(e, e'p), E ≤ 900 MeV; 40Ca(e, e'p), E ≤ 350 MeV; calculated azimuthal angle vs incident electron energy. Vertical chicane beam-method.
doi: 10.1016/0168-9002(87)90830-8
1984BE46 Phys.Rev. C30, 1403 (1984) D.H.Beck, S.B.Kowalski, M.E.Schulze, W.E.Turchinetz, J.W.Lightbody, Jr., X.K.Maruyama, W.J.Stapor, H.S.Caplan, G.A.Retzlaff, D.M.Skopik, R.Goloskie Tritium Form Factors at Low q NUCLEAR REACTIONS 3H(e, e), E=100 MeV; measured charge, magnetic form factors, σ(θ); deduced charge and magnetic radii. 3He, 3H deduced binding energy difference Coulomb contribution.
doi: 10.1103/PhysRevC.30.1403
1982LE26 Phys.Rev. C26, 2554 (1982) J.LeRose, K.Min, D.Rowley, B.O.Sapp, P.Stoler, P.-K.Teng, E.J.Winhold, P.F.Yergin, A.M.Bernstein, K.I.Blomqvist, H.S.Caplan, S.A.Dytman, G.Franklin, M.Pauli, K.Shoda, M.Yamazaki π+ Photoproduction from 13C NUCLEAR REACTIONS 13C(γ, π+), E=18, 29, 42 MeV bremsstrahlung; measured σ(θ). DWIA analysis.
doi: 10.1103/PhysRevC.26.2554
1982RO04 Phys.Rev. C25, 2652 (1982) D.Rowley, J.LeRose, K.Min, B.O.Sapp, P.Stoler, E.J.Winhold, P.F.Yergin, A.M.Bernstein, K.I.Blomqvist, H.S.Caplan, S.A.Dytman, G.Franklin, M.Pauli Charged Pion Photoproduction from 10B NUCLEAR REACTIONS 10B(γ, π+), (γ, π-), E=17, 19, 42 MeV; measured σ(θ). 10Be, 10C level deduced σ(ratio). DWIA analysis.
doi: 10.1103/PhysRevC.25.2652
1982SE11 Can.J.Phys. 60, 1257 (1982) R.M.Sealock, H.S.Caplan, B.W.Zulkoskey, A.Szyjewicz, E.L.Tomusiak Electroproduction of Low Energy π+ from 3He NUCLEAR REACTIONS 1H, 3He(e, π+), E=200 MeV; measured σ(θ, E(π)). Three-channel calculation.
doi: 10.1139/p82-172
1982ZU03 Phys.Rev. C26, 1610 (1982) B.W.Zulkoskey, R.M.Sealock, H.S.Caplan, J.C.Bergstrom Electroproduction of π+ from 10B and Its Relation to Electron Scattering NUCLEAR REACTIONS 10B(e, e'π+), E=158.5-165 MeV; measured σ(θ(π), E(π)); deduced photoproduction σ(θ(π)). 10Be level deduced M1 form factor convective term.
doi: 10.1103/PhysRevC.26.1610
1981SE05 Phys.Rev. C23, 1293 (1981) R.M.Sealock, H.S.Caplan, G.J.Lolos, W.C.Haxton Low Energy Angular Distributions for the 12C(e, π+e') Reaction NUCLEAR REACTIONS 12C(e, π+e'), E=200 MeV; measured σ(E(π), θ). DWBA calculations.
doi: 10.1103/PhysRevC.23.1293
1979AN08 Nucl.Phys. A322, 237 (1979) E.J.Ansaldo, J.C.Bergstrom, R.Yen, H.S.Caplan Inelastic Electron Scattering from 10B NUCLEAR REACTIONS 10B(e, e'), E=67-194 MeV; measured σ(E;Ee', θ). 10B deduced form factors, reduced widths, multipolarities, (π-, γ) rates. Helm model. Enriched targets.
doi: 10.1016/0375-9474(79)90424-X
1979BO19 Phys.Rev. C20, 879 (1979) D.I.Bonbright, A.M.McDonald, W.T.H.van Oers, J.W.Watson, H.S.Caplan, J.M.Cameron, J.G.Rogers, J.Soukup, W.M.Kloet, C.Stolk, J.A.Tjon Noncoplanar 2H(p, 2p)n Reaction NUCLEAR REACTIONS 2H(p, 2p), E=23.0, 39.5 MeV; measured two types of constant-relative-energy loci. Faddeev calculations, Reid soft-core potentials.
doi: 10.1103/PhysRevC.20.879
1978KI01 Nucl.Phys. A297, 301 (1978) J.C.Kim, R.S.Hicks, R.Yen, I.P.Auer, H.S.Caplan, J.C.Bergstrom Electron Scattering from 17O NUCLEAR REACTIONS 17O(e, e), (e, e'), E=62.5-125 MeV; measured σ(E, θ). 17O deduced form factors, B(λ), rms charge radius. Gas target.
doi: 10.1016/0375-9474(78)90278-6
1977AN25 Can.J.Phys. 55, 2129 (1977) E.J.Ansaldo, J.C.Bergstrom, H.S.Caplan, R.Yen Electroexcitation of 15N Levels from 9.7 to 14.7 MeV NUCLEAR REACTIONS 15N(e, e'), E=60-194 MeV; measured σ(E). 15N transitions deduced form factors.
doi: 10.1139/p77-256
1977HI02 Nucl.Phys. A278, 261 (1977) R.S.Hicks, I.P.Auer, J.C.Bergstrom, H.S.Caplan Electroexcitation of Giant Resonances in 181Ta NUCLEAR REACTIONS 181Ta(e, e'), E=79-120 MeV; measured σ(E, Ee', θ). 181Ta deduced giant multipole resonance parameters, B(EL).
doi: 10.1016/0375-9474(77)90239-1
1977NO06 Nucl.Phys. A289, 275 (1977) B.E.Norum, J.C.Bergstrom, H.S.Caplan Electroexcitation of the Giant Resonance of 17O NUCLEAR REACTIONS 17O(e, e'), E=65-168 MeV; measured σ(E;Ee', θ). 17O giant resonance deduced form factors. Comparison with particle-hole model.
doi: 10.1016/0375-9474(77)90033-1
1975KI08 Phys.Lett. 56B, 442 (1975) Widths of the 6.32 and 9.16 MeV Levels in 15N NUCLEAR REACTIONS 15N(e, e'); measured σ(Ee')/σ. 15N levels deduced γ-width, γ-mixing.
doi: 10.1016/0370-2693(75)90407-4
1975KI09 Nucl.Phys. A246, 282 (1975) J.C.Kim, H.S.Caplan, J.C.Bergstrom Low Lying Octupole Excitations in 15N NUCLEAR REACTIONS 15N(e, e'), E=84-122 MeV; measured σ(E, Ee', θ). 15N levels deduced form factors, deduced B(E3) values. 15N gas target.
doi: 10.1016/0375-9474(75)90646-6
1975KI15 Phys.Lett. 57B, 341 (1975) J.C.Kim, R.Yen, I.P.Auer, H.S.Caplan Low-Lying Octupole Excitations in 17O NUCLEAR REACTIONS 17O(e, e'), E=84-122 MeV; measured charge σ. 17O levels deduced B(E3).
doi: 10.1016/0370-2693(75)90466-9
1975KL10 Nucl.Phys. A255, 435 (1975) F.J.Kline, I.P.Auer, J.C.Bergstrom, H.S.Caplan Electron Scattering from 70Ge and 72Ge NUCLEAR REACTIONS 70,72Ge(e, e'), E=84-120 MeV; measured σ(E, Ee', θ). 70,72Ge deduced levels, J, π, B(E2), B(E3), ground-state charge density, form factors. Enriched 70,72Ge targets.
doi: 10.1016/0375-9474(75)90691-0
1974NA25 Rev.Brasil.Fisica 4, 241 (1974) I.C.Nascimento, C.F.Wong, H.S.Caplan Electromagnetic Form Factors for the 14.39 and 17.50 MeV Levels of 9Be NUCLEAR REACTIONS 9Be(e, e'), E=95.8, 104.7 MeV; measured σ. 9Be levels deduced form factors.
1973BE19 Phys.Rev. C7, 2228 (1973) J.C.Bergstrom, I.P.Auer, M.Ahmad, F.J.Kline, J.H.Hough, H.S.Caplan, J.L.Groh Electroexcitation of 9Be Levels in the 14- 18-MeV Region NUCLEAR REACTIONS 9Be(e, e'), E=62-122 MeV; measured σ(E;E(e')). 9Be levels deduced form factors, radius, quadrupole moment, level-width.
doi: 10.1103/PhysRevC.7.2228
1973BE49 Nucl.Phys. A213, 609 (1973) J.C.Bergstrom, I.P.Auer, F.J.Kline, H.S.Caplan Electroexcitation of 16O Levels Near 10 MeV Excitation NUCLEAR REACTIONS 16O(e, e'), E=100-126 MeV; measured σ(E;Ee', θ); deduced form factors. 16O deduced β2, β4 deformations, level-width. BeO target.
doi: 10.1016/0375-9474(73)90755-0
1973SI31 Can.J.Phys. 51, 2125 (1973) R.P.Singhal, H.S.Caplan, J.R.Moreira, T.E.Drake Inelastic Electron Scattering from 20,22Ne NUCLEAR REACTIONS 20,22Ne(e, e'), E=102 MeV; measured σ(Ee'), form factors. 20,22Ne levels deduced B(E2).
doi: 10.1139/p73-278
1971GR27 Can.J.Phys. 49, 2073 (1971) J.L.Groh, R.P.Singhal, H.S.Caplan Elastic Scattering of Electrons from Argon-40 NUCLEAR REACTIONS 40Ar(e, e), E=78, 82, 89, 120 MeV; measured σ(E;θ); deduced form factors. 40Ar deduced rms charge radius.
doi: 10.1139/p71-250
1971GR33 Can.J.Phys. 49, 2743 (1971) J.L.Groh, R.P.Singhal, H.S.Caplan, B.S.Dolbilkin Inelastic Electron Scattering from 18O NUCLEAR REACTIONS 18O(e, e'), E=92.5, 105.9 MeV; measured σ(Ee'); deduced form factors. 18O T=1 levels deduced B(EL).
doi: 10.1139/p71-333
1971MO15 Can.J.Phys. 49, 1434 (1971) J.R.Moreira, R.P.Singhal, H.S.Caplan Charge Radii of 20,22Ne Determined from Elastic Electron Scattering NUCLEAR REACTIONS 20,22Ne(e, e), E=140 MeV; measured σ(θ); deduced form factor. 20,22Ne deduced nuclear charge radii.
doi: 10.1139/p71-169
1971SH09 Nucl.Phys. A166, 162 (1971) Y.M.Shin, C.F.Wong, H.S.Caplan Comparison of Photoprotons from 12C and 13C NUCLEAR REACTIONS 12,13C(e, e'p), E=43 MeV; measured σ(Ep, θ(p)). 13C deduced giant resonance structure. Enriched targets.
doi: 10.1016/0375-9474(71)90420-9
1971YA02 Nucl.Phys. A162, 71 (1971) C.S.Yang, E.L.Tomusiak, R.K.Gupta, H.S.Caplan Electron Scattering from 13C NUCLEAR REACTIONS 13C(e, e), (e, e'), E=40-125 MeV; measured σ(E;θ), σ(E;Ee', θ); deduced form factors. 13C deduced levels, level-width, γ-mixing, rms charge radius. Enriched solid, gas targets.
doi: 10.1016/0375-9474(71)90486-6
1970KI02 Can.J.Phys. 48, 83 (1970) J.C.Kim, R.P.Singhal, H.S.Caplan Inelastic Electron Scattering from the 13 MeV Region in Oxygen-16 NUCLEAR REACTIONS 16O(e, e'), E=11.5-13.25 MeV; measured σ(E;Ee'); deduced form factor. 16O deduced levels, level-width, transition radii, reduced matrix elements.
doi: 10.1139/p70-013
1970SI02 Phys.Rev.Lett. 24, 73 (1970) R.P.Singhal, J.R.Moreira, H.S.Caplan RMS Charge Radii of 16,17,18O by Elastic Electron Scattering NUCLEAR REACTIONS 16,17,18O(e, e), E=94-121 MeV; measured σ(E;θ); deduced elastic form factors. 16,17,18O deduced rms charge radii.
doi: 10.1103/PhysRevLett.24.73
1970WO10 Can.J.Phys. 48, 1917 (1970) C.F.Wong, R.M.Hutcheon, Y.M.Shin, H.S.Caplan Electrodisintegration of Lithium NUCLEAR REACTIONS 6,7Li(e, X), (γ, X), E < 90 MeV; measured σ(E;E(X)).
doi: 10.1139/p70-241
1969HU05 Nucl.Phys. A127, 417 (1969) Inelastic Electron Scattering from 6Li and 7Li NUCLEAR REACTIONS 6Li(e, e'), 7Li(e, e'), E=60-130 MeV; measured relative σ(Ee', θ), deduced form factors. Enriched targets.
doi: 10.1016/0375-9474(69)90582-X
1968DR01 Nucl.Phys. A118, 138 (1968) T.E.Drake, E.L.Tomusiak, H.S.Caplan The Excitation of Strong Transitions in the Giant Resonance of 12C, 16O and 28Si NUCLEAR REACTIONS 12C, 16O, 28Si(e, e') E=140 MeV; measured σ(Ee', θ);deduced form factors. Natural targets.
doi: 10.1016/0375-9474(68)90192-9
1968HU03 Nucl.Phys. A107, 266 (1968) R.M.Hutcheon, T.E.Drake, V.W.Stobie, G.A.Beer, H.S.Caplan Inelastic Electron Scattering from the 3.56 MeV Excited State of 6Li NUCLEAR REACTIONS 6Li(e, e'), E = 60-130 MeV; measured σ(E', θ); deduced form factors. Enriched target.
doi: 10.1016/0375-9474(68)90618-0
1968RI06 Nucl.Phys. A114, 685(1968) G.Ricco, H.S.Caplan, R.M.Hutcheon, R.Malvano Inelastic Electron Scattering from the Giant Resonance in 12C NUCLEAR REACTIONS 12C(e, e'), E=60-100 MeV; measured σ(E, Ee', θ). Natural target.
doi: 10.1016/0375-9474(68)90297-2
1967DR05 Phys.Rev. 163, 947 (1967) T.E.Drake, R.M.Hutcheon, V.W.Stobie, G.A.Beer, H.S.Caplan Inelastic Scattering of Electrons from the 19.08-MeV Level in Oxygen-16 NUCLEAR STRUCTURE 16O; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.163.947
1963GE06 Phys.Canada 19, No.3, 19, Abstr.4.8 (1963) N.W.Gebbie, H.S.Caplan, J.D.Prentice M1-E2 Mixing Ratios of Low-Lying Gamma Rays Transitions in F19 NUCLEAR STRUCTURE 19F; measured not abstracted; deduced nuclear properties.
1963PR01 Phys.Letters 3, 201 (1963) J.D.Prentice, N.W.Gebbie, H.S.Caplan The Spins and Parities of the 1.35 and 1.46 MeV Levels of F19 NUCLEAR STRUCTURE 19F; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(63)90079-9
1963SI04 Phys.Canada 19, No.3, 18, Abstr.4.7 (1963) J.J.Simpson, J.D.Prentice, H.S.Caplan Lifetime of the 2.15 Mev. Level in B10 NUCLEAR STRUCTURE 6Li; measured not abstracted; deduced nuclear properties.
1962PR01 Bull.Am.Phys.Soc. 7, No.1, 72, V7 (1962) J.D.Prentice, N.W.Gebbie, H.S.Caplan, N.R.Steenberg The Spins and Particles of the 1.35-MeV and 1.46-MeV Levels in F19 NUCLEAR STRUCTURE 19F; measured not abstracted; deduced nuclear properties.
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