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Search: Author = H.Caplan

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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0589.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0552.


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
Citations: PlumX Metrics


1992MI11      Nucl.Phys. A546, 199c (1992)

J.P.Miller, E.J.Austin, J.Bergstrom, E.C.Booth, H.Caplan, D.Delli Carpini, G.Dodson, M.Doss, K.P.Gall, E.Hallin, R.Igarashi, M.A.Lucas, E.K.McIntyre, A.M.Nathan, C.Rangacharyulu, D.Skopik, D.Warner, D.P.Wells, D.A.Whitehouse

Nuclear Compton Scattering from Pion Threshold to the Delta

NUCLEAR REACTIONS 4He(γ, γ), E=148, 280, 187 MeV; 1H(γ, γ), E not given; analyzed σ(θ), Compton scattering. Different models.

doi: 10.1016/0375-9474(92)90511-H
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1991DE02      Phys.Rev. C43, 1525 (1991)

D.Delli Carpini, E.C.Booth, J.P.Miller, R.Igarashi, J.Bergstrom, H.Caplan, M.Doss, E.Hallin, C.Rangacharyulu, D.Skopik, M.A.Lucas, A.M.Nathan, D.P.Wells

Coherent Photon Scattering Cross Sections for Helium Near the Delta Resonance

NUCLEAR REACTIONS 4He(γ, γ), E=187-280 MeV bremsstrahlung; measured σ(θ). Isobar-hole model.

doi: 10.1103/PhysRevC.43.1525
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1991DE19      Nucl.Phys. A527, 341c (1991)

D.Delli Carpini, E.C.Booth, J.P.Miller, D.Amendt, J.Bergstrom, H.Caplan, M.Doss, E.Hallin, R.Igarashi, D.Skopik, F.J.Federspiel, B.MacGibbon, A.Nathan

Compton Scattering on the Proton Near the Δ Resonance

NUCLEAR REACTIONS 1H(γ, γ), E=145-280 MeV; measured σ(θ).

doi: 10.1016/0375-9474(91)90123-N
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1990CA24      Ann.Phys.(Paris) 15, 95 (1990)

H.S.Caplan

EROS: The machine and the physics

NUCLEAR REACTIONS 2H(γ, 2p), E ≈ 300 MeV; measured reduced σ vs neutron momentum.


1988DO13      Phys.Rev.Lett. 61, 1706 (1988)

K.Dow, S.Dytman, D.Beck, A.Bernstein, I.Blomqvist, H.Caplan, D.Day, M.Deady, P.Demos, W.Dodge, G.Dodson, M.Farkhondeh, J.Flanz, K.Giovanetti, R.Goloskie, E.Hallin, E.Knill, S.Kowalski, J.Lightbody, R.Lindgren, X.Maruyama, J.McCarthy, B.Quinn, G.Retzlaff, W.Sapp, C.Sargent, D.Skopik, I.The, D.Tieger, W.Turchinetz, T.Ueng, N.Videla, K.von Reden, R.Whitney, C.Williamson

Longitudinal Response Functions and Sum Rules for Quasielastic Electron Scattering from 3H and 3He

NUCLEAR REACTIONS 3H, 3He(e, e'X), E not given; measured longitudinal response function; deduced sum rules.

doi: 10.1103/PhysRevLett.61.1706
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1987BE30      Phys.Rev.Lett. 59, 1537 (1987)

D.Beck, A.Bernstein, I.Blomqvist, H.Caplan, D.Day, P.Demos, W.Dodge, G.Dodson, K.Dow, S.Dytman, M.Farkhondeh, J.Flanz, K.Giovanetti, R.Goloskie, E.Hallin, E.Knill, S.Kowalski, J.Lightbody, R.Lindgren, X.Maruyama, J.McCarthy, B.Quinn, G.Retzlaff, W.Sapp, C.Sargent, D.Skopik, I.The, D.Tieger, W.Turchinetz, T.Ueng, N.Videla, K.von Reden, R.Whitney, C.Williamson

Isoscalar and Isovector Form Factors of 3H and 3He for Q below 2.9 fm-1 from Electron-Scattering Measurements

NUCLEAR REACTIONS 3H, 3He(e, e), E not given; measured σ(θ). 3H, 3He deduced charge, magnetic form factors.

doi: 10.1103/PhysRevLett.59.1537
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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
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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
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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
Citations: PlumX Metrics


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
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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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
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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
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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
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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
Citations: PlumX Metrics


1975KI08      Phys.Lett. 56B, 442 (1975)

J.C.Kim, H.S.Caplan, I.P.Auer

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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1969HU05      Nucl.Phys. A127, 417 (1969)

R.M.Hutcheon, H.S.Caplan

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
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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
Citations: PlumX Metrics


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
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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
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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
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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
Citations: PlumX Metrics


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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Note: The following list of authors and aliases matches the search parameter H.Caplan: , H.S.CAPLAN