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NSR database version of May 24, 2024.

Search: Author = J.J.Kent

Found 22 matches.

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1977KE01      Nucl.Phys. A275, 313 (1977)

J.J.Kent, R.C.Ritter, G.F.Neal

Study of Energy Levels of 92Nb Observed in the 92Zr(p, n) Reaction

NUCLEAR REACTIONS 92Zr(p, n), E=4.25-5.30 MeV; measured σ(E;En). 92Nb deduced levels, J, π. Enriched target.

doi: 10.1016/0375-9474(77)90455-9
Citations: PlumX Metrics


1975KE12      Nucl.Phys. A255, 296 (1975)

J.J.Kent, S.L.Blatt

Energy Levels of 92Nb and 94Tc from 92Zr, 94Mo(p, nγ)92Nb, 94Tc

NUCLEAR REACTIONS 92Zr(p, nγ), E=3.40-5.10 MeV; measured σ(E;Eγ); deduced Q. 92Zr(p, nγ), E=4.90 MeV; measured γγ-coin. 92Nb deduced levels. 94Mo(p, nγ), E=5.80 MeV; measured γγ-coin. 94Tc deduced levels. Enriched targets.

doi: 10.1016/0375-9474(75)90681-8
Citations: PlumX Metrics


1973CH39      Nucl.Instrum.Methods 109, 327 (1973)

C.N.Chang, J.J.Kent, J.F.Morgan, S.L.Blatt

Total Cross Section Measurements by X-Ray Detection of Electron-Capture Residual Activity

NUCLEAR REACTIONS 48Ti(α, n), E=5-11 MeV; measured σ(E).

doi: 10.1016/0029-554X(73)90282-6
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0951.


1973KE01      Phys.Rev. C7, 388 (1973)

J.J.Kent, W.R.Coker, C.F.Moore

Inelastic Proton Scattering from 96Mo Through Isobaric Analog Resonances

NUCLEAR REACTIONS 96Mo(p, p'), (p, p), E=5.2-8.0 MeV; measured σ(θ). 96Mo level deduced J, π. 97Tc deduced IAR, level-width, J, π, S.

doi: 10.1103/PhysRevC.7.388
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1973MO27      Phys.Rev. C8, 2397 (1973)

J.F.Morgan, R.G.Seyler, J.J.Kent

Comparison of Sub-Coulomb Stripping and Analog Resonance Results Near Mass 90

NUCLEAR REACTIONS 89Y, 92Mo(d, p), E=4 MeV; measured σ(Ep, θ). 90Y, 91,93Zr, 93Mo levels deduced λ(lj), S.

doi: 10.1103/PhysRevC.8.2397
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1973NO05      Phys.Rev.Lett. 31, 769 (1973)

G.A.Norton, H.J.Hausman, J.J.Kent, J.F.Morgan, R.G.Seyler

Comparison of Sub-Coulomb Stripping and Analog-Resonance Results Near Closed Shells

NUCLEAR REACTIONS 90,92Zr, 92Mo, 138Ba, 140Ce, 142Nd, 144Sm, 208Pb(d, p); calculated σ(θ). 91,93Zr, 93Mo, 139Ba, 141Ce, 143Nd, 145Sm, 209Pb levels calculated S.

doi: 10.1103/PhysRevLett.31.769
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1972KE24      Nucl.Phys. A197, 177 (1972)

J.J.Kent, J.F.Morgan, R.G.Seyler

Comparison of Sub-Coulomb Stripping and Analog Resonance Results in 93Zr

NUCLEAR REACTIONS 92Zr(d, p), E=4 MeV; measured σ(Ep, θ). 93Zr deduced reduced normalizations, . Enriched target.

doi: 10.1016/0375-9474(72)90754-3
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1972KE32      Z.Phys. 256, 199 (1972)

J.J.Kent, W.R.Coker, C.E.Watson

Absence of Proton Weak Coupling States in 93Nb

NUCLEAR REACTIONS 93Nb(p, p)(p, n), (p, p'), E=5.8-7.6 MeV; measured σ(E). 94Mo deduced IAR, level-width. 93Nb deduced levels.

doi: 10.1007/BF01392093
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1972MO43      Phys.Rev. C6, 2126 (1972)

J.F.Morgan, N.L.Gearhart, H.J.Hausman, J.J.Kent, G.A.Norton, J.W.D.Sinclair

50Ti(p, p'γ) Angular-Correlation Study at Isobaric Analog Resonances

NUCLEAR REACTIONS 50Ti(p, p'γ), E=3-5 MeV; measured σ(E, Ep', θ), p'γ(θ). 51V deduced levels, J, π.

doi: 10.1103/PhysRevC.6.2126
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1971ST27      Phys.Rev. C4, 1684 (1971)

W.S.Steiner, H.J.Hausman, J.J.Kent, J.R.Duray, N.L.Gearhart, J.W.D.Sinclair

Spectroscopy of Some Low-Lying States in 69Zn

NUCLEAR REACTIONS 68Zn(p, p), (p, p'γ), E=3.9-6.1 MeV; measured σ(E;θ), σ(E;Ep', θ, θ(p'γ)), p'γγ-triple correlation. 69Ga deduced isobaric analog resonances, level-width, S, L.

doi: 10.1103/PhysRevC.4.1684
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1970CO29      Phys.Rev. C2, 2023 (1970)

W.R.Coker, J.J.Kent

Charge-Exchange Threshold Effect in 93Nb(d, p)94Nb

NUCLEAR REACTIONS 93Nb(d, p), E=5-10 MeV; measured σ(E); deduced charge-exchange threshold effect.

doi: 10.1103/PhysRevC.2.2023
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1970KE02      Phys.Rev. C1, 336 (1970)

J.J.Kent, K.P.Lieb, C.F.Moore

Isobaric Analog Resonances in 92Zr(p, p')

NUCLEAR REACTIONS 92Zr(p, p), (p, p'), E=6-10 MeV; measured σ(E;Ep', θ). 93Nb deduced isobaric analog resonances, J, level-width, S, L(p).

doi: 10.1103/PhysRevC.1.336
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1970KE03      Phys.Rev. C1, 346 (1970)

J.J.Kent, C.F.Moore, C.E.Watson

Nuclear-Structure Study of 98Mo from (p, p') on Analog Resonances

NUCLEAR REACTIONS 98Mo(p, p), (p, p'), E=6-8 MeV; measured σ(E;Ep', θ). 99Tc deduced isobaric analog resonances, L(p), J, level-width, S.

doi: 10.1103/PhysRevC.1.346
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1970LI09      Phys.Lett. 32B, 273 (1970)

K.P.Lieb, J.J.Kent, T.Hausmann, C.E.Watson

Weak-Coupling States in Odd Zr Isotopes

NUCLEAR REACTIONS 94Zr(p, p), (p, p'), E=6.0-8.6 MeV; measured σ(E). 95Nb deduced isobaric analog resonances. 91,93,95Zr deduced weak-coupling states, S.

doi: 10.1016/0370-2693(70)90526-5
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1970LI22      Phys.Rev. C2, 1822 (1970)

K.-P.Lieb, J.J.Kent, T.Hausmann, C.E.Watson

Proton Decay of Isobaric Analog Resonances in 95Nb

NUCLEAR REACTIONS 94Zr(p, p), (p, p'), E=6.0-8.5 MeV; measured σ(E;θ). 95Nb deduced resonances, J, π, level-width, isobaric analogs. 95Zr deduced levels, J, π, S.

doi: 10.1103/PhysRevC.2.1822
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1970MO15      Nucl.Instrum.Methods 79, 353 (1970)

C.F.Moore, J.G.Kulleck, W.R.Coker, R.G.Clarkson, J.J.Kent, W.J.Courtney

Detection of Internal Conversion Electrons in Charged Particle Spectra

NUCLEAR REACTIONS 90Zr(p, p'), E=7.34 MeV; Zr(p, X), E=9.4 MeV; 89Y(p, n), (p, p'), E not given; 72Ge(p, n), E=5.2-5.9 MeV; measured E(ce), σ(E). Detector - Si(Li).

doi: 10.1016/0029-554X(70)90164-3
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1969LI11      Phys.Rev. 182, 1341 (1969)

K.P.Lieb, T.Hausmann, J.J.Kent

92Mo(p, p'γ) Reaction via Isobaric Analog Resonances

NUCLEAR REACTIONS 92Mo(p, p'γ), E=5.5-8.2 MeV; measured σ(E;Eγ, θ(γ)). 93Tc deduced resonances, level-width, S. 92Mo deduced levels.

doi: 10.1103/PhysRev.182.1341
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1968LI10      Z.Physik 217, 213 (1968)

K.P.Lieb, T.Hausmann, J.J.Kent, C.F.Moore

The Decay of the 11.80 MeV Isobaric Analog Resonance in 93Tc to Negative Parity States in 92Mo

NUCLEAR REACTIONS 92Mo(p, p'γ), E=7.96 MeV; measured σ(Eγ, θ). 93Tc deduced isobaric analog resonances, level-width, S.

doi: 10.1007/BF01394098
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1968LI11      Phys.Rev. 175, 1482 (1968)

K.P.Lieb, J.J.Kent, C.F.Moore

Isobaric-Analog Study of 90Zr

NUCLEAR STRUCTURE 91Nb, 90Zr; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.175.1482
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1967MO06      Phys.Rev.Letters 18, 345 (1967)

C.F.Moore, S.A.A.Zaidi, J.J.Kent

Single-Particle States Built on the Second 0+ State in 90Zr

NUCLEAR STRUCTURE 91Nb; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.18.345
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1966MO15      Phys.Rev.Letters 17, 926 (1966)

C.F.Moore, C.E.Watson, S.A.A.Zaidi, J.J.Kent, J.G.Kulleck

Experimental Observation of the Coupling of the Analogous Channels in a (d, p) and (d, n) Reaction

NUCLEAR STRUCTURE 91Nb, 91Zr; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.17.926
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1966MO29      Univ.Texas Accelerator Lab.Annual Rept., p.16 (1966); ORO-2972-25 (1966)

C.F.Moore, C.E.Watson, S.A.A.Zaidi, J.J.Kent, J.G.Kulleck

Experimental Observation of the Coupling of the (d, p) and (d, n) Reaction Channels

NUCLEAR STRUCTURE 91Zr, 91Nb; measured not abstracted; deduced nuclear properties.


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