Nuclear Science References (NSR)

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NSR database version of April 27, 2024.

Search: Author = J.Bronson

Found 36 matches.

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
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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
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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
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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
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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, ^{116,118,120,124}Sn, ^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, ^{116,118,120,124}Sn, ^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, ^{116,118,120,124}Sn, ^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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1973NA09 Phys.Rev.Lett. 31, 250 (1973)

K.Nagatani, D.H.Youngblood, R.Kenefick, J.Bronson

(¹⁰B, ⁷Li) and (¹⁰B, ⁷Be) Analog Reactions on ¹²C

NUCLEAR REACTIONS ¹²C(¹⁰B, ⁷Li), (¹⁰B, ⁷Be), E=100 MeV; measured σ(E(⁷Li), θ), σ(E(⁷Be), θ). ¹⁵O, ¹⁵N deduced levels.

doi: 10.1103/PhysRevLett.31.250
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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 ^{198,200,202,204}Hg(¹⁶O, ¹⁶O'γ), E = 40 MeV; measured γγ(θ, H). ^{198,200,202,204}Hg 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.