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NSR database version of May 24, 2024.

Search: Author = J.Bergstrom

Found 51 matches.

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2008BA24      Phys.Rev. C 77, 064601 (2008)

M.G.Barnett, R.Igarashi, R.E.Pywell, J.C.Bergstrom

Near threshold (γ, π0) reactions for 4He and 12C

NUCLEAR REACTIONS 4He(γ, π0), E=141-159 MeV; measured σ, angular distributions; deduced reduced isovector amplitudes. 12C(γ, π0); analyzed σ, deduced reduced isovector amplitudes.

doi: 10.1103/PhysRevC.77.064601
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0138.


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.


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.


1999BE14      Phys.Rev. C59, 2588 (1999)

J.C.Bergstrom, R.Igarashi, J.M.Vogt

Measurement of the 6Li(γ, π0) Reaction Near Threshold

NUCLEAR REACTIONS 6Li(γ, π0), E ≈ threshold; measured σ, σ(E, θ); deduced partial wave amplitudes.

doi: 10.1103/PhysRevC.59.2588
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
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1998BE22      Phys.Rev. C57, 3203 (1998)

J.C.Bergstrom, R.Igarashi, J.M.Vogt, N.Kolb, R.E.Pywell, D.M.Skopik, E.Korkmaz

Measurement of the 2H(γ, π0) Reaction Near Threshold

NUCLEAR REACTIONS 2H(γ, π0), E ≈ threshold; measured σ(E), σ(E, θ); deduced nuclear S-wave, P-wave amplitudes.

doi: 10.1103/PhysRevC.57.3203
Citations: PlumX Metrics


1998BE67      Phys.Rev. C58, 2574 (1998)

J.C.Bergstrom

Measurement of the 1H(γ, π0) Cross Section Near Threshold. III. Angular Coefficients

NUCLEAR REACTIONS 1H(γ, π0), E=144.7-169.3 MeV; measured σ(θ); deduced angular distribution coefficients.

doi: 10.1103/PhysRevC.58.2574
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1997BE13      Phys.Rev. C55, 2016 (1997)

J.C.Bergstrom, R.Igarashi, J.M.Vogt

Measurement of the 1H(γ, π0) Cross Section Near Threshold. II. Pion Angular Distributions

NUCLEAR REACTIONS 1H(γ, π0), E=144.7-169.3 MeV; analyzed data; deduced S-, P-wave amplitude characteristics.

doi: 10.1103/PhysRevC.55.2016
Citations: PlumX Metrics


1997BE22      Phys.Rev. C55, 2923 (1997)

J.C.Bergstrom, R.Igarashi, J.M.Vogt

Measurement of the 12C(γ, π0) Reaction Near Threshold

NUCLEAR REACTIONS 12C(γ, π0), E=110.8-160.8 MeV; measured σ(E), σ(E, θ); deduced isovector P-wave amplitude, inelastic γ, π0 transition to the 4.43 MeV (2+) state.

doi: 10.1103/PhysRevC.55.2923
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1996BE08      Phys.Rev. C53, R1052 (1996)

J.C.Bergstrom, J.M.Vogt, R.Igarashi, K.J.Keeter, E.L.Hallin, G.A.Retzlaff, D.M.Skopik, E.C.Booth

Measurement of the 1H(γ, π0) Cross Section Near Threshold

NUCLEAR REACTIONS 1H(γ, π0), E=144.7-169.3 MeV; measured σ(E), σ(E, θ); deduced S-wave amplitudes. Low energy theorem, heavy baryon chiral perturbation theory.

doi: 10.1103/PhysRevC.53.R1052
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1995BE39      Phys.Rev. C52, 1986 (1995)

J.C.Bergstrom

Comparing the p-Wave Multipoles for π0 Photoproduction with Low-Energy Predictions

NUCLEAR REACTIONS 1H(γ, π0), E=threshold; analyzed calculated p-wave π0 photoproduction amplitudes. Heavy-baryon chiral perturbation theory based new low-energy theorems.

doi: 10.1103/PhysRevC.52.1986
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0589.


1995SH20      Phys.Rev. C52, 199 (1995)

J.Shaw, H.Choi, T.Kobayashi, P.Stoler, T.Gresko, K.Keeter, J.H.Mitchell, B.Norum, T.P.Welch, H.T.Chung, J.C.Kim, H.B.van den Brink, W.H.A.Hesselink, J.C.Bergstrom, E.L.Hallin, H.S.Kaplan, D.M.Skopik, J.M.Vogt

Negative Pion Photoproduction from 15N in the Region of the Δ Resonance

NUCLEAR REACTIONS 15N(γ, π-), E=220 MeV; measured σ(θ). Models comparison.

doi: 10.1103/PhysRevC.52.199
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1995VO17      Nucl.Instrum.Methods Phys.Res. A366, 100 (1995)

J.M.Vogt, J.C.Bergstrom, R.Igarashi, K.J.Keeter

Igloo: A neutral pion spectrometer for low energy photoproduction studies

NUCLEAR REACTIONS 12C(γ, π0), E ≈ 130-165 MeV; measured total σ(E), pion yields. Lead glass Cherenkov counters used in π0 spectrometer.

doi: 10.1016/0168-9002(95)00557-9
Citations: PlumX Metrics


1994BE31      Phys.Rev. C50, 2979 (1994)

J.C.Bergstrom

Photopion p-Wave Multipoles Near Threshold from 12C(γ, π0) and 1H(γ, π0)

NUCLEAR REACTIONS 12C(γ, π0), E ≈ 140-200 MeV; calculated σ(E). 12C(π+, π+), E=30-80 MeV; calculated σ(θ); 12C(e, e), E not given; calculated single matter form factor; deduced nucleon isovector-multipole combination near π0-threshold.

doi: 10.1103/PhysRevC.50.2979
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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
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1993BE42      Phys.Rev. C48, 1508 (1993)

J.C.Bergstrom, E.L.Hallin

Unitarity Cusp in Proton Compton Scattering

NUCLEAR REACTIONS 1H(γ, γ), E=100-300 MeV; calculated σ(θ), Compton scattering; deduced Wigner cusp evidence.

doi: 10.1103/PhysRevC.48.1508
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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.


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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1992WE11      Phys.Rev.Lett. 69, 2761 (1992)

T.P.Welch, P.H.Karen, J.H.Mitchell, B.E.Norum, H.P.Blok, H.B.van den Brink, C.W.de Jager, E.Jans, L.Lapikas, H.de Vries, J.Wesseling, J.Bergstrom, M.Deady

Electroproduction of π0 on the Proton Near Threshold

NUCLEAR REACTIONS 1H(e, e'π0), E=350, 500 MeV; measured σ(θ(e), E(e)), invariant energy; deduced longitudinal, transverse contributions.

doi: 10.1103/PhysRevLett.69.2761
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1991BE23      Phys.Rev. C44, 1768 (1991)

J.C.Bergstrom

p(γ, π0) Cross Section and the Low Energy Theorem

NUCLEAR REACTIONS 1H(γ, π0), E ≈ 144-160 MeV; analyzed σ(E), σ(θ) data; deduced low-energy theorem breakdown features.

doi: 10.1103/PhysRevC.44.1768
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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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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
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1984BE13      Phys.Rev. C29, 1168 (1984)

J.C.Bergstrom, R.Neuhausen, G.Lahm

Electroexcitation of Levels in 14N between 12 and 21 MeV

NUCLEAR REACTIONS 14N(e, e'), E=112-300 MeV; measured σ(E(e'), θ) vs E. 14N levels deduced form factors, transition strengths, configuration. Comparison with pion scattering.

doi: 10.1103/PhysRevC.29.1168
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1984HU07      Phys.Lett. 139B, 249 (1984)

R.L.Huffman, R.S.Hicks, J.Dubach, B.Parker, M.A.Plum, G.Lahm, R.Neuhausen, J.C.Bergstrom

Comparison of Isoscalar and Isovector (e, e') M1 Form Factors at High Momentum Transfer

NUCLEAR REACTIONS 14N(e, e), (e, e'), E not given; measured M1 form factors. 14N deduced isoscalar, isovector transition differences. Shell model comparison.

doi: 10.1016/0370-2693(84)91073-6
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1983DE53      Nucl.Phys. A411, 337 (1983)

U.Deutschmann, G.Lahm, R.Neuhausen, J.C.Bergstrom

Electron Scattering Studies of Magnetic Isovector Transitions in 12C at High Momentum Transfer

NUCLEAR REACTIONS 12C(e, e'), E=80-330 MeV; measured σ(E, E(e'), θ). 12C deduced levels, Γ, form factors, transition current density, Γ(γ0).

doi: 10.1016/0375-9474(83)90534-1
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1982BE11      Phys.Rev. C25, 1156 (1982)

J.C.Bergstrom, S.B.Kowalski, R.Neuhausen

Elastic Magnetic Form Factor of 6Li

NUCLEAR REACTIONS 6Li(e, e'), E=80-300 MeV; measured σ(E, E(e'), θ). 6Li deduced M1 form factor, ground state current density. Cluster model, exchange currents.

doi: 10.1103/PhysRevC.25.1156
Citations: PlumX Metrics


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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1980BE20      Phys.Rev. C21, 2496 (1980)

J.C.Bergstrom

Electroexcitation of 6Li with Application to the Reactions 6Li(π-, γ)1s 6He(0+, 2+)

NUCLEAR REACTIONS 6Li(e, e'), E=76-141 MeV; measured σ(E, Ee', θ). 6Li levels deduced form factors, wave functions. 6He levels deduced radiative pion capture rate.

doi: 10.1103/PhysRevC.21.2496
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1980BE28      Nucl.Phys. A341, 13 (1980)

J.C.Bergstrom

Inelastic Electron Scattering from 6Li Near the t-τ Threshold

NUCLEAR REACTIONS 6Li(e, e'), E=102, 123 MeV; measured σ(E;Ee', θ). 6Li deduced form factor. Cluster model.

doi: 10.1016/0375-9474(80)90358-9
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1980BR17      Nucl.Phys. A344, 475 (1980)

W.J.Briscoe, H.Crannell, J.C.Bergstrom

Elastic Electron Scattering from the Isotopes 35Cl and 37Cl

NUCLEAR REACTIONS 35,37Cl(e, e'), E=116, 194 MeV; measured σ(E, θ). 35,37Cl deduced nuclear charge distributions. Enriched targets.

doi: 10.1016/0375-9474(80)90402-9
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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
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1979BE38      Nucl.Phys. A327, 439 (1979)

J.C.Bergstrom, U.Deutschmann, R.Neuhausen

Electron Scattering from the 3.65 MeV (O+, T = 1) State in 6Li at High Momentum Transfer

NUCLEAR REACTIONS 6Li(e, e'), E=140-330 MeV; measured σ(E;Ee', θ). 6Li levels deduced form factors, transition current density, Γγ.

doi: 10.1016/0375-9474(79)90268-9
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1979BE39      Nucl.Phys. A327, 458 (1979)

J.C.Bergstrom

6Li Electromagnetic Form Factors and Phenomenological Cluster Models

NUCLEAR REACTIONS 6Li(e, e), (e, e'), E not given; calculated longitudinal, transverse form factors. Anti-symmetrized α-d, α-t cluster models.

doi: 10.1016/0375-9474(79)90269-0
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1978AN12      Phys.Rev. C18, 597 (1978)

E.J.Ansaldo, J.C.Bergstrom, R.Yen

Electroexcitation of Giant Resonances in 15N

NUCLEAR REACTIONS 15N(e, e'), E=52-193.5 MeV; measured σ(E, Ee', θ). 15N giant resonances deduced differential form factors, strength distributions. Helm model.

doi: 10.1103/PhysRevC.18.597
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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
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1976BE22      Nucl.Phys. A262, 196 (1976)

J.C.Bergstrom, E.L.Tomusiak

Inelastic Electron Scattering from 6Li Near the α-d Threshold

NUCLEAR REACTIONS 6Li(e, e'), E=0-8 MeV; measured σ(E, θ), θ=99.9°, 140.7°. 6Li levels deduced form factors. Comparison between form factors, α-d cluster model calculations.

doi: 10.1016/0375-9474(76)90613-8
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1975BE12      Phys.Rev. C11, 1514 (1975)

J.C.Bergstrom

Second Born Approximation for Magnetic Multipole Electroexcitation

NUCLEAR REACTIONS C(e, e'), E=45, 120 MeV; Ca(e, e'), E=60 MeV; Ni(e, e'), E=50 MeV; calculated Coulomb correction factors.

doi: 10.1103/PhysRevC.11.1514
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1975BE42      Nucl.Phys. A251, 401 (1975)

J.C.Bergstrom, I.P.Auer, R.S.Hicks

Electroexcitation of the 0+ (3.562 MeV) Level of 6Li and its Application to the Reaction 6Li(γ, π+)6He

NUCLEAR REACTIONS 6Li(e, e'), E=35-125 MeV; measured σ(E;Ee', θ). 6Li level deduced form factor, Γ.

doi: 10.1016/0375-9474(75)90537-0
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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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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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1974BE21      Phys.Rev. C9, 2435 (1974)

J.C.Bergstrom

Magnetic Moment of the Deuteron and Spin-Orbit Potentials

NUCLEAR MOMENTS 2H; calculated μ. Percentage d state deduced.

doi: 10.1103/PhysRevC.9.2435
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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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1973BE50      Nucl.Phys. A215, 232 (1973)

J.C.Bergstrom, I.P.Auer

Form Factors of the 2+ (11.52 MeV) and 0+ (12.05 MeV) Levels of 16O

NUCLEAR REACTIONS 16O(e, e'), E=101-126 MeV; measured σ(E;Ee', θ); deduced form factors. BeO target.

doi: 10.1016/0375-9474(73)90652-0
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1971BE51      Phys.Rev. C4, 1514 (1971)

J.C.Bergstrom, H.Crannell, F.J.Kline, J.T.O'Brien, J.W.Lightbody, Jr., S.P.Fivozinsky

Electroexcitation of the Giant Resonance of 13C

NUCLEAR REACTIONS 12,13C(e, e'), E=55, 77, 81, 106 MeV; measured σ(Ee'). 13C deduced resonances, level-width, giant resonance structure.

doi: 10.1103/PhysRevC.4.1514
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1970BE03      Phys.Rev.Lett. 24, 152 (1970)

J.C.Bergstrom, W.Bertozzi, S.Kowalski, X.K.Maruyama, J.W.Lightbody, Jr., S.P.Fivozinsky, S.Penner

Electroexcitation of the Low-Lying States of O16

NUCLEAR REACTIONS 16O(e, e'), E=51-105 MeV; measured σ(E;E'); deduced inelastic form factors. 16O levels deduced deformation parameters.

doi: 10.1103/PhysRevLett.24.152
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Note: The following list of authors and aliases matches the search parameter J.Bergstrom: , J.C.BERGSTROM