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Search: Author = J.D.Bronson

Found 35 matches.

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1987NA01      Phys.Rev. C35, 149 (1987)

M.N.Namboodiri, R.K.Choudhury, L.Adler, J.D.Bronson, D.Fabris, U.Garg, P.L.Gonthier, K.Hagel, D.R.Haenni, Y.W.Lui, Z.Majka, G.Mouchaty, T.Murakami, J.B.Natowitz, G.Nebbia, R.P.Schmitt, S.Simon, J.P.Sullivan, D.H.Youngblood

Linear Momentum and Angular Momentum Transfer in the Reactions of 16O with 154Sm

NUCLEAR REACTIONS 154Sm(16O, X), E=180, 310 MeV; measured (ejectile)γ-, (residue)γ-coin, σ(fragment θ, E), < Eγ > vs fragment for X=6,7Li, 7,9,10Be, 10,11B, 11,12,13,14C, 13,14,15N, 15,16,17O; deduced angular, linear momentum transfer correlation.

doi: 10.1103/PhysRevC.35.149
Citations: PlumX Metrics

1986GR10      Phys.Rev. C34, 322 (1986)

P.Grabmayr, G.J.Wagner, K.T.Knopfle, H.Riedesel, P.Bogucki, J.D.Bronson, Y.W.Lui, U.Garg, D.H.Youngblood

Direct Contributions to the Decay of Isoscalar Giant Resonances in 58Ni

NUCLEAR REACTIONS 58Ni(α, 2α), (α, pα), E=129 MeV; measured σ(θ1, θ2, Eα), αα(θ), αp(θ); deduced reaction mechanism. 58Ni deduced isoscalar giant resonance decay mechanism.

doi: 10.1103/PhysRevC.34.322
Citations: PlumX Metrics

1985LU04      Phys.Rev. C31, 1643 (1985)

Y.-W.Lui, J.D.Bronson, D.H.Youngblood, Y.Toba, U.Garg

Giant Quadrupole and Monopole Resonances in 28Si

NUCLEAR REACTIONS 28Si(α, α'), E=129 MeV; measured σ(Eα, θα), σ(θ). 28Si levels deduced isoscalar, electromagnetic transition rates, EWSR.

doi: 10.1103/PhysRevC.31.1643
Citations: PlumX Metrics

1984GA02      Phys.Rev. C29, 93 (1984)

U.Garg, P.Bogucki, J.D.Bronson, Y.-W.Lui, D.H.Youngblood

Giant Monopole Resonance in Transitional and Deformed Nuclei

NUCLEAR REACTIONS 144,148Sm, 142,146,150Nd(α, α'), E=129 MeV; measured σ(Eα'), σ(θ). 142,146Nd deduced giant resonances, Γ, L. 148Sm deduced giant resonances, L, multipole mixing, Γ. 150Nd deduced giant resonance, monopole splitting, Γ, L.

doi: 10.1103/PhysRevC.29.93
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1984LU06      Phys.Rev. C30, 51 (1984)

Y.-W.Lui, P.Bogucki, J.D.Bronson, D.H.Youngblood, U.Garg

Giant Resonances in 112Sn

NUCLEAR REACTIONS 112Sn(α, α'), E=129.1 MeV; measured σ(θ); deduced nuclear incompressibility parameters. 112Sn deduced isoscalar GQR, giant monopole resonances.

doi: 10.1103/PhysRevC.30.51
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1982GA16      Phys.Rev. C25, 3204 (1982)

U.Garg, P.Bogucki, J.D.Bronson, Y.-W.Lui, C.M.Rozsa, D.H.Youngblood

Comment on the Evidence for a Monopole Resonance at Approximately 20 MeV in 58Ni

NUCLEAR REACTIONS 58Ni(α, α'), E=129 MeV; measured σ(θ), σ(Eα'). 58Ni deduced giant resonances, L, possible monopole. DWBA analysis.

doi: 10.1103/PhysRevC.25.3204
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1981LU05      Phys.Rev. C24, 884 (1981)

Y.-W.Lui, J.D.Bronson, C.M.Rozsa, D.H.Youngblood, P.Bogucki, U.Garg

Giant Resonances in 40Ca

NUCLEAR REACTIONS 40Ca(α, α'), E=98.5, 116.8, 129.4 MeV; measured σ(Eα, θ). 40Ca deduced giant resonances, L, EWSR, Γ, J, π. DWBA analysis.

doi: 10.1103/PhysRevC.24.884
Citations: PlumX Metrics

1981YO04      Phys.Rev. C23, 1997 (1981)

D.H.Youngblood, P.Bogucki, J.D.Bronson, U.Garg, Y.-W.Lui, C.M.Rozsa

Systematics of the Giant Monopole Resonance from Inelastic Alpha Scattering

NUCLEAR REACTIONS 12C, 27Al, 40Ca, 48Ti, 58Ni, 64,66Zn, 90Zr, 116,118,120,124Sn, 144,154Sm, 208Pb(α, α'), E=99, 117, 129 MeV; measured σ(θ, Eα); deduced nuclear incompressibility vs mass. 27Al, 40Ca, 48Ti, 58Ni deduced GQR, Γ. 64,66Zn, 90Zr, 116,118,120,124Sn, 144,154Sm, 208Pb deduced GQR, giant monopole resonances, Γ, EWSR.

doi: 10.1103/PhysRevC.23.1997
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1980GA15      Phys.Lett. 93B, 39 (1980)

U.Garg, P.Bogucki, J.D.Bronson, Y.-W.Lui, K.Nagatani, E.Takada, N.Takahashi, T.Tamaya, D.H.Youngblood

Excitation of Giant Resonances in 208Pb Using Inelastic 14N Scattering

NUCLEAR REACTIONS 208Pb(14N, 14N'), E=266 MeV; measured σ(θ, E(14N')). 208Pb deduced GQR, Γ.

doi: 10.1016/0370-2693(80)90090-8
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1980GA21      Phys.Rev.Lett. 45, 1670 (1980)

U.Garg, P.Bogucki, J.D.Bronson, Y.-W.Lui, C.M.Rozsa, D.H.Youngblood

Splitting of the Giant Monopole Resonance with Deformation in Sm Nuclei

NUCLEAR REACTIONS 144,154Sm(α, α'), E=96, 129 MeV; measured σ(θ, Eα). 144,154Sm deduced GQR, giant monopole resonances, Γ, EWSR strengths. 154Sm deduced giant monopole resonance fragmentation. Schematic model.

doi: 10.1103/PhysRevLett.45.1670
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1980LU06      Phys.Lett. 93B, 31 (1980)

Y.-W.Lui, P.Bogucki, J.D.Bronson, U.Garg, C.M.Rozsa, D.H.Youngblood

Observation of the Giant Monopole Resonance in 64,66Zn

NUCLEAR REACTIONS 64,66Zn(α, α), E=129 MeV; measured σ(θ). 64,66Zn, 90Zr, 115In, 116,118,120,124Sn, 144,148Sm, 197Au, 208Pb deduced surface, symmetry term contributions to nuclear compressibility. 64,66Zn deduced T=0 giant monopole resonance, energy-weighted sum rule.

doi: 10.1016/0370-2693(80)90088-X
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1980RO08      Phys.Rev. C21, 1252 (1980)

C.M.Rozsa, D.H.Youngblood, J.D.Bronson, Y.-W.Lui, U.Garg

Isoscalar Breathing Mode State in 90Zr and 116Sn

NUCLEAR REACTIONS 90Zr, 116Sn(α, α'), E=96, 129 MeV; measured σ(θ). 90Zr, 116Sn deduced T=0, giant monopole resonance, GQR, Γ, energy-weighted sum rule, β, nuclear incompressibility. DWBA, liquid drop models.

doi: 10.1103/PhysRevC.21.1252
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1979BR02      Nucl.Phys. A313, 157 (1979)

D.R.Brown, J.M.Moss, C.M.Rozsa, D.H.Youngblood, J.D.Bronson

Proton Pickup by α-Particles to Unbound States

NUCLEAR REACTIONS 40Ca, 90Zr, 208Pb(α, αp), E=96.8 MeV; measured σ(Eα, θα, Ep, θp); deduced σ for proton pickup to unbound states.

doi: 10.1016/0375-9474(79)90573-6
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1978MO10      Phys.Rev. C18, 741 (1978)

J.M.Moss, D.R.Brown, D.H.Youngblood, C.M.Rozsa, J.D.Bronson

Inelastic Alpha Scattering Studies of the Low-Energy Octupole Resonance

NUCLEAR REACTIONS 40Ca, 66Zn, 75As, 89Y, 90Zr, 92,100Mo, Ag, 116,118,124Sn, 142Nd, 144,148,154Sm, 197Au, 208Pb(α, α'), E=96, 115 MeV; measured σ(θ). 40Ca, 66Zn, 75As, 89Y, 90Zr, 92,100Mo, 107Ag, 116,118,124Sn, 142Nd, 144,148,154Sm, 197Au, 208Pb deduced transition strengths, L, β.

doi: 10.1103/PhysRevC.18.741
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1977YO01      Phys.Rev. C15, 246 (1977)

D.H.Youngblood, A.D.Bacher, D.R.Brown, J.D.Bronson, J.M.Moss, C.M.Rozsa

Particle Decay from the Giant Resonance Region of 40Ca

NUCLEAR REACTIONS 40Ca(α, αp), (α, 2α), E=115 MeV; measured σ(θ), αp(θ) in kinematically complete experiments. 40Ca deduced resonances, branching.

doi: 10.1103/PhysRevC.15.246
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1977YO03      Phys.Rev. C15, 1644 (1977)

D.H.Youngblood, C.M.Rozsa, J.M.Moss, D.R.Brown, J.D.Bronson

Giant Quadrupole Resonance in 24Mg, 27Al, and 28Si

NUCLEAR REACTIONS 24Mg, 27Al, 28Si(α, α'), E=126 MeV; measured σ(θ). 24Mg, 27Al, 28Si deduced giant resonances, L, sum rule fraction.

doi: 10.1103/PhysRevC.15.1644
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1977YO05      Phys.Rev.Lett. 39, 1188 (1977)

D.H.Youngblood, C.M.Rozsa, J.M.Moss, D.R.Brown, J.D.Bronson

Isoscalar Breathing-Mode State in 144Sm and 208Pb

NUCLEAR REACTIONS 144Sm, 208Pb(α, α'), E=96 MeV; measured σ(Eα', θ). 144Sm, 208Pb deduced giant resonances, Γ, L, J, π, β.

doi: 10.1103/PhysRevLett.39.1188
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1976MO21      Phys.Rev.Lett. 37, 816 (1976)

J.M.Moss, D.H.Youngblood, C.M.Rozsa, D.R.Brown, J.D.Bronson

Observation of a Low-Energy Octupole Resonance in Medium-Mass Nuclei

NUCLEAR REACTIONS 90Zr, 118Sn, 142Nd, 144,148,154Sm(α, α'), E ≈ 105 MeV; measured σ(Eα', θ). 90Zr, 118Sn, 142Nd, 144,148,154Sm deduced giant resonance structure, J, π, L.

doi: 10.1103/PhysRevLett.37.816
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1976YO02      Phys.Rev. C13, 994 (1976)

D.H.Youngblood, J.M.Moss, C.M.Rozsa, J.D.Bronson, A.D.Bacher, D.R.Brown

Giant Resonances Observed in the Scattering of 96- and 115-MeV Alpha Particles

NUCLEAR REACTIONS 14N, 16O, 20Ne, 27Al, 28Si, 32S, 36,40Ar, 40Ca, 48Ti, 56Fe, 58,60Ni, 59Co, 66Zn, 90Zr, 94,96,100Mo, 141Pr, 142Nd, 144,148,154Sm, 159Tb, 174Yb, 208Pb(α, α'), E=96, 115 MeV; measured σ(Eα', θ). 32S, 36,40Ar, 40Ca, 48Ti, 56Fe, 58,60Ni, 59Co, 66Zn, 90Zr, 94,96,100Mo, 141Pr, 142Nd, 144,148,154Sm, 159Tb, 174Yb, 208Pb deduced resonances, Γ, β, L. 32S, 36,40Ar, 40Ca, 58Ni, 90Zr, 148Sm, 208Pb deduced B(λ).

doi: 10.1103/PhysRevC.13.994
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1975KI12      Phys.Rev.Lett. 35, 552 (1975)

T.Kishimoto, J.M.Moss, D.H.Youngblood, J.D.Bronson, C.M.Rozsa, D.R.Brown, A.D.Bacher

Giant Quadrupole Resonance in Deformed Nuclei

NUCLEAR REACTIONS 144,148,154Sm(α, α'), E=115 MeV; measured σ(Eα', θ). 144,148,154Sm GQR deduced Γ.

doi: 10.1103/PhysRevLett.35.552
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1975MO04      Phys.Rev.Lett. 34, 748 (1975)

J.M.Moss, C.M.Rozsa, D.H.Youngblood, J.D.Bronson, A.D.Bacher

Isoscalar Giant Resonance in Light Nuclei (A ≤ 40)

NUCLEAR REACTIONS 40Ca, 36,40Ar, 32S, 28Si, 27Al, 20Ne, 16O(α, α), E=96.6 MeV; measured σ(θ). 32S, 36,40Ar, 40Ca giant resonances deduced level-width, S.

doi: 10.1103/PhysRevLett.34.748
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1975NA15      Phys.Rev. C12, 1575 (1975)

K.G.Nair, H.Voit, C.W.Towsley, M.Hamm, J.D.Bronson, K.Nagatani

Transfer Reactions with Heavy Ions on Light Nuclei

NUCLEAR REACTIONS 12C, 16O(14N, 13N), (14N, 13C), 16O(14N, 15N), E=155 MeV; 12C, 14N, 16O(10B, 11C), (10B, 11B), 14N, 16O(10B, 9Be), E=155 MeV; measured σ(θ). 11,13C, 17F, 15,17O, 13,15N levels deduced S.

doi: 10.1103/PhysRevC.12.1575
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetR0019.

1974MO22      Phys.Lett. 53B, 51 (1974)

J.M.Moss, C.M.Rozsa, J.D.Bronson, D.H.Youngblood

Systematics of Giant Resonances from Inelastic Alpha-Particle Scattering

NUCLEAR REACTIONS 27Al, 40Ca, 90Zr, Pb, 24Mg(α, α'), E=96, 115 MeV; measured σ(Eα'). 40Ca, 90Zr, 208Pb deduced resonance.

doi: 10.1016/0370-2693(74)90341-4
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1973RO25      Phys.Rev. C8, 961 (1973)

J.G.Rogers, M.Jain, J.D.Bronson

Measurement of the 2H(p, 2p)n Reaction Over a Large Volume of Phase Space

NUCLEAR REACTIONS 2H(p, 2p), E=39.5 MeV; measured σ(Ep, θ), pp-coin.

doi: 10.1103/PhysRevC.8.961
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1972MC11      Phys.Rev. C5, 1796 (1972)

J.A.McIntyre, P.H.Beatty, J.D.Bronson, R.J.Hastings, J.G.Rogers, M.S.Shaw

Investigation of Proton-Proton Quasifree Scattering in the Reaction 2H(p, 2p)n

NUCLEAR REACTIONS 2H(p, 2p), E=39.5 MeV; measured σ(E(p1), θ(p1), phi(p1), E(p2), θ(p2), phi(p2)).

doi: 10.1103/PhysRevC.5.1796
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1972RO28      Phys.Rev.Lett. 29, 1181 (1972)

J.G.Rogers, D.P.Saylor, J.D.Bronson, M.Jain

Destructive Interference Effects in D(p, 2p)n at E = 39.5 MeV

NUCLEAR REACTIONS 2H(p, 2p), E=39.5 MeV; measured σ(E(p1), E(p2), θ(p2)); deduced destructive interference effects.

doi: 10.1103/PhysRevLett.29.1181
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1968KA27      Proc.Intern.Conf.Hyperfine Struct.Nucl.Radiations, Asilomar, Pacific Grove, Calif. (1967), E.Matthias, D.A.Shirley, Eds., North-Holland Publ.Co., Amsterdam, p.208 (1968)

R.Kalish, L.Grodzins, D.E.Murnick, R.R.Borchers, B.Herskind, J.D.Bronson

Magnetic Moments of the First Excited 2+ States in Even Hg Isotopes

NUCLEAR REACTIONS 198,200,202,204Hg(16O, 16O'γ), E = 40 MeV; measured γγ(θ, H). 198,200,202,204Hg levels deduced g.

1967KA16      Phys.Rev. 161, 1196 (1967); R.R.Borchers - Priv.Comm. (May 1972)

R.Kalish, L.Grodzins, R.R.Borchers, J.D.Bronson, B.Herskind

Magnetic Moments of the First Excited 2+ States in the Even Pt Isotopes

NUCLEAR STRUCTURE 194Pt, 196Pt, 198Pt; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.161.1196
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1967MU22      Phys.Rev. 163, 254 (1967); R.R.Borchers - Priv.Comm. (May 1972)

D.E.Murnick, L.Grodzins, J.D.Bronson, B.Herskind, R.R.Borchers

Effective Magnetic Fields on Samarium-150 in Ferromagnetic Lattices

NUCLEAR STRUCTURE 150Sm; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.163.254
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1966BO19      Phys.Rev.Letters 17, 1099 (1966)

R.R.Borchers, J.D.Bronson, D.E.Murnick, L.Grodzins

Magnetic Moments of 2+ States in Even Te Nuclei

NUCLEAR STRUCTURE 128Te, 126Te, 122Te, 120Te, 124Te; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.17.1099
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1965BR18      Nucl.Phys. 68, 241 (1965)

J.D.Bronson, W.D.Simpson, W.R.Jackson, G.C.Phillips

Three α-Particle Decay of C12

NUCLEAR STRUCTURE 12C, 11B; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(65)90643-7
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1964BR05      Bull. Am. Phys. Soc. 9, No. 4, 406, CA4 (1964)

J.D.Bronson, W.D.Simpson, W.R.Jackson, G.C.Phillips

Reaction-Mechanism Study of 11B(p, 2α)4He

NUCLEAR STRUCTURE 11B; measured not abstracted; deduced nuclear properties.

1963BR03      Bull.Am.Phys.Soc. 8, No.2, 125, U8 (1963)

J.D.Bronson, W.D.Simpson, G.C.Phillips

3-α Decay from Protons on B11

NUCLEAR STRUCTURE 11B; measured not abstracted; deduced nuclear properties.

1963PI04      Nucl.Phys. 48, 75 (1963)

A.E.Pitts, J.D.Bronson, T.A.Belote, G.C.Phillips

Evidence for Sequential Two-Body Decay in the C12(d, p, N)C12 Reaction

NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(63)90144-5
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1962BR09      Bull.Am.Phys.Soc. 7, No.2, 119, J4 (1962)

J.D.Bronson, Jr., E.H.Beckner, G.C.Phillips

The 1.7-MeV Anomaly in Be9

NUCLEAR STRUCTURE 9Be; measured not abstracted; deduced nuclear properties.

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