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NSR database version of April 27, 2024.

Search: Author = C.M.Rozsa

Found 19 matches.

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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
Citations: PlumX Metrics

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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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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1975BR05      Phys.Rev. C11, 1042 (1975)

B.J.Brunner, R.G.Arns, S.E.Caldwell, C.M.Rozsa, J.W.Smith, S.W.Sprague

Low-Energy Levels and Gamma Transitions in ⁵⁸Co

NUCLEAR REACTIONS ⁵⁵Mn(α, nγ), E=9.5 MeV; measured Eγ, DSA. ⁵⁸Fe(p, nγ), E=3.3-4.73 MeV; measured σ(E, Eγ, θ). ⁵⁸Co levels deduced T_1/2, J, γ-mixing.

doi: 10.1103/PhysRevC.11.1042
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1975CA36      Phys.Rev. C12, 2084 (1975)

S.E.Caldwell, L.A.Alexander, R.G.Arns, B.J.Brunner, M.A.Kovash, C.M.Rozsa, J.W.Smith

Lifetimes of Some Low-Lying Levels of ⁵⁵Co

NUCLEAR REACTIONS ⁵⁴Fe(³He, dγ), E=11 MeV; measured Eγ, DSA, dγ-coin. ⁵⁵Co deduced levels, T_1/2, γ-branching.

doi: 10.1103/PhysRevC.12.2084
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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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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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1971SP12      Phys.Rev. C4, 2074 (1971)

S.W.Sprague, R.G.Arns, B.J.Brunner, S.E.Caldwell, C.M.Rozsa

Lifetimes of Some Low-Lying Levels of ⁵²Cr

NUCLEAR REACTIONS ⁵¹V(³He, d), E=11 MeV; measured Doppler-shift attenuation. ⁵²Cr levels deduced T_1/2. Ge(Li) detector.

doi: 10.1103/PhysRevC.4.2074
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Note: The following list of authors and aliases matches the search parameter C.M.Rozsa: , C.M.ROZSA