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Search: Author = T.T.Bardin

Found 22 matches.

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1977BA23      Phys.Rev. C15, 1933 (1977)

T.T.Bardin, J.A.Becker, D.Kohler, B.A.Watson

Search for the Reaction t + t → α + d + e- + ν-bar

NUCLEAR REACTIONS 3H(t, d), E=1.4 MeV; measured production σ. Implications for solar neutrino rate.

doi: 10.1103/PhysRevC.15.1933
Citations: PlumX Metrics

1976BA45      Phys.Rev. C14, 1782 (1976)

T.T.Bardin, J.G.Pronko, R.E.McDonald, A.R.Poletti, J.B.McGrory

Gamma-Ray Spectroscopy of Low-Lying States in 56Cr

NUCLEAR REACTIONS 54Cr(t, pγ), E=2.9 MeV; measured Eγ, Iγ, pγ-coin, γ(t), pγ(θ). 56Cr deduced levels, γ-branching, J, π, T1/2, δ. Shell model analysis.

doi: 10.1103/PhysRevC.14.1782
Citations: PlumX Metrics

1976PR01      Phys.Rev. C13, 608 (1976)

J.G.Pronko, T.T.Bardin, J.A.Becker

Gamma-Ray Spectroscopy Studies of the Lower Excited States of 53V

NUCLEAR REACTIONS 51V(t, pγ), E=2.9 MeV; measured pγ(t), DSA, Eγ. 53V deduced levels, J, π, T1/2, δ, γ-branching.

doi: 10.1103/PhysRevC.13.608
Citations: PlumX Metrics

1975WA20      Phys.Rev.Lett. 35, 1333 (1975)

B.A.Watson, T.T.Bardin, J.A.Becker, T.R.Fisher

Two-Photon Decay of the 6.05-MeV State of 16O

NUCLEAR REACTIONS 19F(p, αγ), E=1.89 MeV; measured αγ-, γγ-coin. 16O level deduced two-photon decay, branching.

doi: 10.1103/PhysRevLett.35.1333
Citations: PlumX Metrics

1974BA05      Phys.Rev. C9, 790 (1974)

T.T.Bardin, J.A.Becker, T.R.Fisher

Statistical-Model Analysis of Gamma-Ray Angular Distributions Following the 48Ti(p, p')48Ti Reaction at E = 5.0 MeV

NUCLEAR REACTIONS 48Ti(p, p'), E=5.0 MeV; measured σ(Eγ, θ). 48Ti deduced γ-mixing.

doi: 10.1103/PhysRevC.9.790
Citations: PlumX Metrics

1974BE28      Phys.Rev. C10, 99 (1974)

J.A.Becker, T.T.Bardin, T.R.Fisher, B.A.Watson, E.K.Warburton

Lifetime Limits for the 46Ca 2+1 (1.35-MeV) and 0+2 (2.42-MeV) States

NUCLEAR REACTIONS 44Ca(t, pγ); measured pγcoin, DSA. 46Ca levels deduced T1/2.

doi: 10.1103/PhysRevC.10.99
Citations: PlumX Metrics

1974FI01      Phys.Rev. C9, 598 (1974)

T.R.Fisher, T.T.Bardin, J.A.Becker, B.A.Watson

Nuclear Lifetimes in 42Ar

NUCLEAR REACTIONS 40Ar(t, pγ), Et=2.8 MeV; measured σ(Ep, Eγ, θ(γ)). Doppler shift attenuation. 42Ar deduced levels, Iγ, T1/2. Solid Ar target.

doi: 10.1103/PhysRevC.9.598
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1974PR04      Phys.Rev. C9, 1430 (1974); Erratum Phys.Rev. C10, 1249 (1974)

J.G.Pronko, T.T.Bardin, J.A.Becker, T.R.Fisher, R.E.McDonald, A.R.Poletti

Gamma-Ray Spectroscopy Studies of 52Ti

NUCLEAR REACTIONS 50Ti(t, pγ), E=2.9 MeV; measured Eγ, Iγ, DSA, γγ(θ). 52Ti levels deduced J, π, T1/2, γ-mixing.

doi: 10.1103/PhysRevC.9.1430
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1974PR11      Phys.Rev. C10, 1345 (1974)

J.G.Pronko, T.T.Bardin, J.A.Becker, R.E.McDonald, A.R.Poletti

γ-Ray Deexcitation of 50Ti States in the Region of 4-MeV Excitation

NUCLEAR REACTIONS 48Ti(t, pγ), E=2.9 MeV; measured pγ-coin, pγ(θ), Eγ, Iγ, DSA. 50Ti deduced levels, T1/2, γ-branching ratios, J, π, γ-mixing.

doi: 10.1103/PhysRevC.10.1345
Citations: PlumX Metrics

1973BA02      Phys.Rev. C7, 190 (1973)

T.T.Bardin, J.A.Becker, T.R.Fisher

Level Structure of 48Ti for E(x) < 3.5 MeV

RADIOACTIVITY 48V; measured Eγ, Iγ. 48Ti deduced levels, J, π, γ-branching.

NUCLEAR REACTIONS 48Ti(p, p'), (α, α'), (35Cl, 35Cl'), Ep=6.4, 5.0;Eα=5 MeV;E(Cl)=64 MeV; measured Eγ, Iγ, γγ-coin, DSA. 48Ti deduced levels, J, π, T1/2, level-width, γ-branching.

doi: 10.1103/PhysRevC.7.190
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1973FI03      Phys.Rev. C7, 1878 (1973)

T.R.Fisher, T.T.Bardin, J.A.Becker, L.F.Chase, Jr., D.Kohler, R.E.McDonald, A.R.Poletti, J.G.Pronko

Gamma-Ray Spectroscopy of Low-Lying Levels in 28Mg

NUCLEAR REACTIONS 26Mg(t, pγ), E=2.9 MeV; measured σ(Ep, Eγ), pγ(θ), DSA. 28Mg deduced transitions, levels, T1/2, γ-branching, γ-mixing, J.

doi: 10.1103/PhysRevC.7.1878
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1973PO02      Phys.Rev. C7, 1433 (1973)

A.R.Poletti, T.T.Bardin, J.G.Pronko, R.E.McDonald

Lifetimes in 33P by the Doppler-Shift-Attenuation Method

NUCLEAR REACTIONS 31P(t, pγ), E=2.9 MeV; measured σ(Ep), Eγ, Doppler-shift attenuation; 33P deduced levels, T1/2, J, π.

doi: 10.1103/PhysRevC.7.1433
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1973PO03      Phys.Rev. C7, 1479 (1973)

A.R.Poletti, T.T.Bardin, R.E.McDonald, J.G.Pronko

33P; Angular Correlation Studies of Excited States

NUCLEAR REACTIONS 31P(t, pγ), E=2.9 MeV; measured σ(Ep), pγ(θ), Eγ, Iγ. 33P deduced levels, γ-mixing, J, π.

doi: 10.1103/PhysRevC.7.1479
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1972BA26      Phys.Rev. C5, 1351 (1972)

T.T.Bardin, J.A.Becker, T.R.Fisher

Radiative Decay of the P29 8.38-MeV Level

NUCLEAR REACTIONS 28Si(p, γ), E=5.83 MeV; measured σ(Eγ, θ(γ)). 29P deduced levels, J, π, γ-mixing, γ-branching. Ge(Li) detectors.

doi: 10.1103/PhysRevC.5.1351
Citations: PlumX Metrics

1971BA62      Phys.Rev.Lett. 27, 866 (1971)

T.T.Bardin, J.A.Becker

Comparison of Analogous ΔT = 0 β- and γ-Ray Decays in the Nuclear 2s-1d Shell

NUCLEAR STRUCTURE A=21-35; compared M1, Δt=0 γ-width with level-width calculated from G-T β-decay ft-values.

doi: 10.1103/PhysRevLett.27.866
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1971BA73      Phys.Rev. C4, 1625 (1971)

T.T.Bardin, J.A.Becker, T.R.Fisher, A.D.W.Jones

Levels of Si29 with Excitation Energy below 6.4 MeV

NUCLEAR REACTIONS 26Mg(α, nγ), E=5-8 MeV; measured σ(E;Eγ, θ(γ)), Doppler shift attenuation. 29Si deduced levels, J, π, T1/2, γ-branching, γ-mixing.

doi: 10.1103/PhysRevC.4.1625
Citations: PlumX Metrics

1970BA04      Phys.Rev.Lett. 24, 772 (1970)

T.T.Bardin, J.A.Becker, T.R.Fisher, A.D.W.Jones

Properties of the 5.256-MeV State in Si29: Evidence for a Rotational Band with Kπ=7/2-

NUCLEAR REACTIONS 26Mg(α, nγ), E=6.0, 6.2, 6.4, 6.6 MeV; measured σ(E;Eγ, θ(γ)), Doppler shift attenuation. 29Si level deduced J, π, T1/2, level-width, γ-mixing, quadrupole moment.

doi: 10.1103/PhysRevLett.24.772
Citations: PlumX Metrics

1970BA65      Phys.Rev. C2, 2283 (1970)

T.T.Bardin, J.A.Becker, R.E.McDonald, A.D.W.Jones

Study of the 33Cl(β+)33S Decay

RADIOACTIVITY 33Cl; measured Eγ, Iγ, T1/2; deduced log ft, β-branching. 33S deduced levels. 25Al; measured Eγ, Iγ; deduced β-branching.

doi: 10.1103/PhysRevC.2.2283
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1968GE05      Bull. Am. Phys. Soc. 13, No. 11, 1446, ED1 (1968)

K.N.Geller, D.Eccleshall, T.T.Bardin

(He3, n) Reactions on Fe54 and Ni58

NUCLEAR STRUCTURE 60Zn, 56Ni; measured not abstracted; deduced nuclear properties.

1967BA35      Phys.Rev. 160, 1043 (1967)

T.T.Bardin, R.C.Cohen, S.Devons, D.Hitlin, E.Macagno, J.Rainwater, K.Runge, C.S.Wu, R.C.Barrett

Magnetic Dipole and Electric Quadrupole Hyperfine Effects in Bi209 Muonic X Rays

NUCLEAR STRUCTURE 209Bi; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.160.1043
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1966BA04      Phys.Rev.Letters 16, 718 (1966)

T.T.Bardin, R.C.Barrett, R.C.Cohen, S.Devons, D.Hitlin, E.Macagno, C.Nissim-Sabat, J.Rainwater, K.Runge, C.S.Wu

Isotope Shifts in Muonic X Rays of Sn118,119,120, Nd142,144,146, and W182,184,186

NUCLEAR STRUCTURE, Mesic-Atoms 142Nd, 146Nd, 144Nd, 120Sn, 119Sn, 118Sn, 184W, 182W, 186W; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.16.718
Citations: PlumX Metrics

1966BA40      Nucl.Phys. 88, 169 (1966)

T.T.Bardin, K.Runge, C.S.Wu

The Metastable d3/2 Hole State in 47Sc

RADIOACTIVITY 47Ca [from Oak Ridge]; measured Eγ, Iγ, γγ-coin, γγ-delay. 47Sc deduced level, T1/2.

doi: 10.1016/0029-5582(66)90458-5
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