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NSR database version of April 11, 2024.

Search: Author = W.Stoffl

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2021HO14      Phys.Rev. C 104, 024610 (2021)

C.J.Horsfield, M.S.Rubery, J.M.Mack, H.W.Herrmann, Y.Kim, C.S.Young, S.E.Caldwell, S.C.Evans, T.S.Sedillo, A.M.McEvoy, N.M.Hoffman, M.A.Huff, J.R.Langenbrunner, G.M.Hale, D.C.Wilson, W.Stoeffl, J.A.Church, E.M.Grafil, E.K.Miller, V.Y.Glebov

First spectral measurement of deuterium-tritium fusion γ rays in inertial fusion experiments

NUCLEAR REACTIONS 3H(d, γ)5He*, E not given; measured fusion Eγ, Iγ from deuterium-tritium (DT) inertial confinement fusion (ICF) implosions with Omega laser, branching ratio of γ rays from transitions to an intermediate excited state and the ground state using R-matrix analysis.

doi: 10.1103/PhysRevC.104.024610
Citations: PlumX Metrics


2021MC05      Phys.Rev. C 103, 064607 (2021)

A.M.McEvoy, H.W.Herrmann, Y.Kim, T.S.Sedillo, H.Geppert-Kleinrath, C.R.Brune, T.N.Massey, A.V.Voinov, C.E.Parker, M.S.Rubery, W.Stoeffl

13C(n, 2nγ)12C γ-ray production in the 14-16 MeV incident neutron energy range

NUCLEAR REACTIONS 12,13C(n, 2nγ), (n, n'γ), E=14.4 to 15.8 MeV; measured Eγ, Iγ using Gas Cherenkov Detector (GCD) and enriched targets at the Omega Laser Facility and at the Ohio University Edwards Accelerator Laboratory; deduced σ(E), and compared with MCNP6.1 predictions. Relevance to feasibility of using 13C-based plastic ablators with embedded 12C layers for 'dark mix' diagnosis of inertial confinement fusion (ICF) implosions.

doi: 10.1103/PhysRevC.103.064607
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14710.


2016CA32      J.Radioanal.Nucl.Chem. 309, 899 (2016)

W.S.Cassata, C.A.Velsko, W.Stoeffl, D.R.Jedlovec, A.B.Golod, D.A.Shaughnessy, C.B.Yeamans, E.R.Edwards, D.H.G.Schneider

Determination of gaseous fission product yields from 14 MeV neutron induced fission of 238U at the National Ignition Facility

NUCLEAR REACTIONS 238U(n, F)133Xe/135Xe/137Xe/138Xe/139Xe, E=14 MeV; measured reaction products; deduced fission yields. Comparison with ENDF, JEFF-3.1 evaluated data.

doi: 10.1007/s10967-015-4662-8
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14434.


2013SA36      Phys.Rev.Lett. 111, 052501 (2013)

D.B.Sayre, C.R.Brune, J.A.Caggiano, V.Y.Glebov, R.Hatarik, A.D.Bacher, D.L.Bleuel, D.T.Casey, C.J.Cerjan, M.J.Eckart, R.J.Fortner, J.A.Frenje, S.Friedrich, M.Gatu-Johnson, G.P.Grim, C.Hagmann, J.P.Knauer, J.L.Kline, D.P.McNabb, J.M.McNaney, J.M.Mintz, M.J.Moran, A.Nikroo, T.Phillips, J.E.Pino, B.A.Remington, D.P.Rowley, D.H.Schneider, V.A.Smalyuk, W.Stoeffl, R.E.Tipton, S.V.Weber, C.B.Yeamans

Measurement of the T+T Neutron Spectrum Using the National Ignition Facility

NUCLEAR REACTIONS 3H(t, 2n), E(cm)=16 keV; measured reaction products, En, In; deduced neutron energy spectra σ(E). R-matrix model, National Ignition Facility (NIF).

doi: 10.1103/PhysRevLett.111.052501
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2051.


2012KI10      Phys.Rev. C 85, 061601 (2012)

Y.Kim, J.M.Mack, H.W.Herrmann, C.S.Young, G.M.Hale, S.Caldwell, N.M.Hoffman, S.C.Evans, T.J.Sedillo, A.McEvoy, J.Langenbrunner, H.H.Hsu, M.A.Huff, S.Batha, C.J.Horsfield, M.S.Rubery, W.J.Garbett, W.Stoeffl, E.Grafil, L.Bernstein, J.A.Church, D.B.Sayre, M.J.Rosenberg, C.Waugh, H.G.Rinderknecht, M.G.Johnson, A.B.Zylstra, J.A.Frenje, D.T.Casey, R.D.Petrasso, E.K.Miller, V.Yu.Glebov, C.Stoeckl, T.C.Sangster

Determination of the deuterium-tritium branching ratio based on inertial confinement fusion implosions

NUCLEAR REACTIONS 3H(d, γ)5He, 3H(d, n)4He, E(cm)=14-24 keV; measured absolute neutron and γ-ray yields in inertial confinement fusion (ICF) conditions; deduced branching ratio of γ-to-neutron in d+t reaction. Measurement of γ-to-proton branching ratio in 3He(d, γ)5Li and 3He(d, p)4He reactions used for cross calibration. Comparison with previous studies.

doi: 10.1103/PhysRevC.85.061601
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1937.


1997SC21      Phys.Rev. C56, 1320 (1997)

M.Schramm, K.H.Maier, M.Rejmund, L.D.Wood, N.Roy, A.Kuhnert, A.Aprahamian, J.Becker, M.Brinkman, D.J.Decman, E.A.Henry, R.Hoff, D.Manatt, L.G.Mann, R.A.Meyer, W.Stoeffl, G.L.Struble, T.-F.Wang

Study of Excited States in 208Pb by Particle-γ Coincidences with the 207Pb(d, p)208Pb and 209Bi(t, α)208Pb Reactions

NUCLEAR REACTIONS 207Pb(d, p), E=10 MeV; 209Bi(t, α), E=11.5 MeV; measured Eγ, Iγ, pγ-, αγ-coin. 208Pb deduced levels, J, π, spectroscopic factors, configurations.

doi: 10.1103/PhysRevC.56.1320
Citations: PlumX Metrics


1995ST26      Phys.Rev.Lett. 75, 3237 (1995)

W.Stoeffl, D.J.Decman

Anomalous Structure in the Beta Decay of Gaseous Molecular Tritium

RADIOACTIVITY 3H; measured β end point energy spectra; deduced anomalous structure, ν-mass implications. Gaseous molecular tritium.

doi: 10.1103/PhysRevLett.75.3237
Citations: PlumX Metrics


1991BE03      Nucl.Phys. A522, 483 (1991)

J.A.Becker, A.Berger, J.Blomqvist, D.J.Decman, R.Estep, E.Henry, K.H.Maier, L.G.Mann, R.A.Meyer, N.A.F.M.Poppelier, N.Roy, W.Stoffl, G.L.Struble, L.D.Wood

Quadrupole Moments of Low-Energy Isomers in 210Po

NUCLEAR REACTIONS 209Bi(t, 2n), E=13.5-17 MeV; measured Iγ(θ, t); deduced quadrupole interaction frequencies. 210Po levels deduced quadrupole moments. Shell model, effective charges.

doi: 10.1016/0375-9474(91)90077-J
Citations: PlumX Metrics


1989ES01      Phys.Rev. C39, 76 (1989)

R.Estep, R.K.Sheline, D.J.Decman, E.A.Henry, L.G.Mann, R.A.Meyer, W.Stoffl, L.E.Ussery, J.Kantele

Levels in 112Pd and 102Mo

NUCLEAR REACTIONS 110Pd, 100Mo(t, pγ), E=16 MeV; measured pγ-, pγγ-coin. 102Mo, 112Pd deduced levels, J, π, band structure.

doi: 10.1103/PhysRevC.39.76
Citations: PlumX Metrics


1989MA12      Z.Phys. A332, 263 (1989)

K.H.Maier, A.Aprahamian, J.A.Becker, D.J.Decman, E.A.Henry, R.G.Lanier, L.G.Mann, R.A.Meyer, K.Sale, N.Roy, W.Stoffl, G.L.Struble, J.Blomqvist

Decay of the (21/2)- Isomer in 211Bi and Structure of the νg9/22πh9/2 Levels

NUCLEAR REACTIONS 209Bi(t, p), E=11.5-17 MeV; measured E(γ), I(γ), γγ-, p(ce)-coin, γ(ce)(t), σ(Eγ). 211Bi deduced isomer decay, ICC ratios, γ-multipolarity, level J, π, configuration, (γ+e-) branching ratios.


1989RO04      Phys.Lett. 221B, 6 (1989)

N.Roy, K.H.Maier, A.Aprahamian, J.A.Becker, D.J.Decman, E.A.Henry, L.G.Mann, R.A.Meyer, W.Stoeffl, G.L.Struble

Electromagnetic Decay of 10+ States and Yrast Isomers in 208Pb

NUCLEAR REACTIONS 209Bi(t, α), E=11.5 MeV; measured αγ-coin. 208Pb levels deduced decay features, γ-branching ratios, configurations.

doi: 10.1016/0370-2693(89)90181-0
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1988MA32      Phys.Rev. C38, 74 (1988)

L.G.Mann, K.H.Maier, A.Aprahamian, J.A.Becker, D.J.Decman, E.A.Henry, R.A.Meyer, N.Roy, W.Stoffl, G.L.Struble

Levels of the Four Lowest Two-Particle Configurations in 210Po Studied by In-Beam γ-Ray and Conversion-Electron Spectroscopy with the 209Bi(t, 2n) Reaction

NUCLEAR REACTIONS, ICPND 209Bi(t, 2n), E=11.5-17 MeV; measured Eγ, Iγ, I(ce), γγ(t), γ production σ. 210Po deduced levels J, π, γ-branching, ICC, γ-multipolarity, configurations. Shell model.

doi: 10.1103/PhysRevC.38.74
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1987ES01      Phys.Rev. C35, 1485 (1987)

R.J.Estep, R.K.Sheline, D.J.Decman, E.A.Henry, L.G.Mann, R.A.Meyer, W.Stoffl, L.E.Ussery, J.Kantele

Measurement of E0 Transitions in Neutron-Rich Nuclei near A = 100

NUCLEAR REACTIONS 98,100Mo, 104Ru, 106,108,110Pd(t, p), E=16 MeV; measured γp-, (ce)p-coin. 100,102Mo, 106Ru, 108,110,112Pd deduced levels, T1/2, E0 transitions, E0/E2 branching ratios.

doi: 10.1103/PhysRevC.35.1485
Citations: PlumX Metrics


1986SC25      J.Phys.(London) G12, 411 (1986)

H.H.Schmidt, W.Stoffl, T.von Egidy, P.Hungerford, H.J.Scheerer, K.Schreckenbach, H.G.Borner, D.D.Warner, R.E.Chrien, R.C.Greenwood, C.W.Reich

The Level Structure of 155Gd from (n, γ), (d, p) and (d, t) Studies

NUCLEAR REACTIONS 154Gd(n, γ), E ≤ 24 keV; 154Gd(d, p), 156Gd(d, t), E=14, 20 MeV; measured Eγ, Iγ, I(ce), σ(Ep), σ(Et). 155Gd levels deduced J, π, γ-branching, ICC, γ-multipolarity, neutron binding energy, rotational band structure, configuration.

doi: 10.1088/0305-4616/12/5/008
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1986YA06      Z.Phys. A324, 417 (1986)

S.W.Yates, R.Julin, P.Kleinheinz, B.Rubio, L.G.Mann, E.A.Henry, W.Stoffl, D.J.Decman, J.Blomqvist

Particle-Hole Multiplets in 146Gd from In-Beam Studies of Non-Yrast Levels

NUCLEAR REACTIONS, ICPND 144Sm(α, 2n), E=23-28 MeV; measured σ(E), Eγ, Iγ, γ(θ), I(ce), γγ-coin. 146Gd deduced levels, γ-multipolarity, ICC, γ-branching, J, π. Ge(Li) detectors, coincidence measurements.


1985MA26      Nucl.Phys. A439, 299 (1985)

H.E.Martz, R.G.Lanier, G.L.Struble, L.G.Mann, R.K.Sheline, W.Stoffl

The 152,154Eu(t, α) Reactions: Studies of the (11/2)[505] bands in 151Sm and 153Sm

NUCLEAR REACTIONS, ICPND 152,154Eu(t, α), E=16 MeV; measured Q, σ(θ), σ(Eα); deduced σ(E). 151,153Sm deduced levels, J, π. Nilsson configurations, anomalous intensities, neutron orbitals β2.

doi: 10.1016/0375-9474(85)90433-6
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1270.


1985MA48      Phys.Rev. C32, 1416 (1985)

K.H.Maier, W.Stoffl, R.K.Sheline, J.A.Becker, D.J.Decman, E.A.Henry, L.G.Mann, G.L.Struble, L.E.Ussery, J.A.Cizewski, B.H.Erkkila

Electromagnetic Transitions in 205Hg

NUCLEAR REACTIONS 204Hg(t, d), E=14.2, 16 MeV; measured Eγ, Iγ, γ(θ), γγ(t). 205Hg deduced levels J, π, γ transition T1/2.

doi: 10.1103/PhysRevC.32.1416
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1984BE14      Phys.Rev. C29, 1268 (1984)

J.A.Becker, R.G.Lanier, L.G.Mann, G.L.Struble, K.H.Maier, L.E.Ussery, W.Stoffl, T.W.Nail, R.K.Sheline, J.A.Cizewski, B.H.Erkkila, J.Blomqvist

3291-keV J(π) = (25/2)+ Level in 205Tl

NUCLEAR REACTIONS 204Hg(t, 2n), E=10.8-16.5 MeV; measured Eγ, Iγ, γγ-coin, γ(t). 205Tl deduced levels, J, π, isomer decay, yrast sequence.

doi: 10.1103/PhysRevC.29.1268
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1984CL01      Phys.Rev. C29, 657 (1984)

P.F.Cloessner, W.Stoffl, R.K.Sheline, R.G.Lanier

Low-Lying States in 96Nb from the (t, α) Reaction

NUCLEAR REACTIONS 97Mo(t, α), E=17 MeV; measured σ(θ), σ(Eα). 96Nb deduced levels, J, π, configuration. Enriched target. DWBA analysis.

doi: 10.1103/PhysRevC.29.657
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1441.


1984DE17      Nucl.Instrum.Methods 219, 523 (1984)

D.J.Decman, E.A.Henry, J.Kantele, L.G.Mann, W.Stoffl, R.J.Estep, L.E.Ussery

Electron Spectroscopy in Coincidence with Protons from the (t, p) Reaction

NUCLEAR REACTIONS 98Mo, 204Pb(t, p), E=16 MeV; measured σ(Ep), (ce)p-coin. 98Mo(t, p), (t, t'), (t, 2n), 100Mo(t, p), (t, 2n), E=16 MeV; measured I(ce), (ce)p-coin. Electron spectrometer in coincidence with thin annular Si(Au) proton detector.

doi: 10.1016/0167-5087(84)90225-4
Citations: PlumX Metrics


1984KA10      Phys.Rev. C29, 1693 (1984)

J.Kantele, W.Stoffl, L.E.Ussery, D.J.Decman, E.A.Henry, R.J.Estep, R.W.Hoff, L.G.Mann

Reinvestigation of the Gamma Branch from the 238U Shape Isomer

NUCLEAR REACTIONS, ICPND 238U(d, np), E=18.1 MeV; measured Eγ, Iγ; deduced (isomeric/ground state) σ. 238U deduced shape isomer SF, conversion decay characteristics, levels.

RADIOACTIVITY 238mU(SF), (IT) [from 238U(d, np), E=18.1 MeV]; measured Eγ, Iγ; deduced isomer decay process relative probabilities.

doi: 10.1103/PhysRevC.29.1693
Citations: PlumX Metrics


1984KA17      ATOMKI Kozlem. 26, 59 (1984)

J.Kantele, W.Stoffl, L.E.Ussery, D.J.Decman, E.A.Henry, R.J.Estep, R.W.Hoff, L.G.Mann

Gamma Branch from the 238U Shape Isomer

NUCLEAR REACTIONS, ICPND 238U(d, np), E=18 MeV; measured γ spectra; deduced 238mU production σ. 238U deduced isomer decay characteristics, transitions. In-beam spectroscopy.


1984MA43      Phys.Rev. C30, 1702 (1984)

K.H.Maier, M.Menningen, L.E.Ussery, T.W.Nail, R.K.Sheline, J.A.Becker, D.J.Decman, R.G.Lanier, L.G.Mann, W.Stoffl, G.L.Struble

Measurement of the Quadrupole Moment of the 5- Level in 206Hg

NUCLEAR REACTIONS 204Hg(t, p), E=16 MeV; measured γ(θ, H, t), Eγ. 206Hg level deduced quadrupole moment, reduced E2 matrix element, effective charge.

doi: 10.1103/PhysRevC.30.1702
Citations: PlumX Metrics


1984ST24      Nucl.Instrum.Methods 227, 77 (1984)

W.Stoffl, E.A.Henry

An Electron Spectrometer with a Superconducting Magnet Transporter for In-Beam Use

NUCLEAR REACTIONS 144Sm(t, 2n), E=16 MeV; measured I(ce). 235U(d, X), E=18 MeV; measured E X-ray, I X-ray. Electron spectrometer with superconducting magnet transporter.


1983BE28      Nucl.Instrum.Methods 211, 379 (1983)

J.A.Becker, J.B.Carlson, R.G.Lanier, K.H.Maier, L.G.Mann, G.L.Struble, T.W.Nail, R.K.Sheline, W.Stoffl, L.E.Ussery, J.A.Cizewski, B.Erkkila

In-Beam Gamma-Ray Studies with Tritons

NUCLEAR REACTIONS 208Pb(t, 2n), E=11-16 MeV; measured Eγ, Iγ, relative γ yield vs E, γγ-coin, I(K X-ray), γ(θ). 204Hg(t, 2n), E=16 MeV; measured Eγ, Iγ.

doi: 10.1016/0167-5087(83)90263-6
Citations: PlumX Metrics


1983DE34      Phys.Rev. C28, 1060 (1983)

D.J.Decman, J.A.Becker, J.B.Carlson, R.G.Lanier, L.G.Mann, G.L.Struble, K.H.Maier, W.Stoffl, R.K.Sheline

Electromagnetic Properties of Isomers in 210Pb

NUCLEAR REACTIONS 208Pb(t, p), E=16 MeV; measured γ(θ, H). 210Pb deduced isomer T1/2, μ, g9/2 neutron orbital effective charge.

doi: 10.1103/PhysRevC.28.1060
Citations: PlumX Metrics


1983KA11      Phys.Rev.Lett. 51, 91 (1983)

J.Kantele, W.Stoffl, L.E.Ussery, D.J.Decman, E.A.Henry, R.W.Hoff, L.G.Mann, G.L.Struble

Observation of an E0 Isomeric Transition from the 238U Shape Isomer

RADIOACTIVITY 238mU [from 238U(d, pn), E=18 MeV]; measured I(ce); deduced shape isomer E0 transition, J, π, T1/2 assignment consistency. Reevaluation of Iγ data, superconducting, solenoid type electron spectrometer.

doi: 10.1103/PhysRevLett.51.91
Citations: PlumX Metrics


1983MA15      Phys.Rev. C27, 1431 (1983)

K.H.Maier, T.Nail, R.K.Sheline, W.Stoffl, J.A.Becker, J.B.Carlson, R.G.Lanier, L.G.Mann, G.L.Struble, J.A.Cizewski, B.H.Erkkila

Structure of 209Bi Deduced from the 208Pb(t, 2nγ) Reaction

NUCLEAR REACTIONS 208Pb(t, 2n), E=11-16 MeV; measured Eγ, Iγ(θ), σ(Eγ), γγ(t), γγ-coin. 209Bi deduced levels, J, π, multiplet structure, γ-multipolarity, γ-branching.

doi: 10.1103/PhysRevC.27.1431
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1982BE38      Phys.Rev. C26, 914 (1982)

J.A.Becker, J.B.Carlson, R.G.Lanier, L.G.Mann, G.L.Struble, K.H.Maier, L.Ussery, W.Stoffl, T.Nail, R.K.Sheline, J.A.Cizewski

2.102-MeV Level in 206Hg and the Spin Gyromagnetic Ratio of the 3-s Proton

NUCLEAR REACTIONS 204Hg(t, p), E=16 MeV; measured γ(θ, H), γ-yields; deduced 3s proton g. 206Hg levels deduced J, π, g, T1/2.

doi: 10.1103/PhysRevC.26.914
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1982MA05      Phys.Rev.Lett. 48, 466 (1982)

K.H.Maier, J.A.Becker, J.B.Carlson, R.G.Lanier, L.G.Mann, G.L.Struble, T.Nail, R.K.Sheline, W.Stoffl, L.Ussery

g Factor of the Jπ = 25/2+ Isomer in 205Tl and the Anomalous Orbital Magnetism of the Proton

NUCLEAR REACTIONS 204Hg(t, 2n), E=16 MeV; measured γ(θ, H, t); deduced g(πh11/2-1). 205Tl level deduced g. Thick, enriched liquid target.

doi: 10.1103/PhysRevLett.48.466
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1982SC03      Nucl.Phys. A376, 149 (1982)

K.Schreckenbach, A.I.Namenson, W.F.Davidson, T.Von Egidy, H.G.Borner, J.A.Pinston, R.K.Smither, D.D.Warner, R.F.Casten, M.L.Stelts, D.H.White, W.Stoffl

Rotational-Vibrational Band Structure in 155Sm

NUCLEAR REACTIONS 154Sm(n, γ), E=thermal, ≥ 100 eV, 2, 24 keV; measured Eγ, Iγ; 154Sm(n, e), E=thermal; measured I(ce). 155Sm deduced levels, neutron binding energy, transitions, γ-multipolarity, J, π, ICC. Curved crystal, magnetic conversion electron, Ge(Li) pair spectrometers, enriched target. Nilsson model, Coriolis, ΔN=2 couplings.

doi: 10.1016/0375-9474(82)90058-6
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13839.


1981LA02      Phys.Lett. 99B, 23 (1981)

R.G.Lanier, G.L.Struble, L.G.Mann, W.Stoffl, I.C.Oelrich, J.Scheerer, I.D.Proctor, D.W.Heikkinen, R.H.Howell

Evidence for a Strongly Deformed Prolate Shape at N=87 from 154Eu and 152Eu(p, t) Reactions

NUCLEAR REACTIONS 152,154Eu(p, t), E=20 MeV; measured σ(Et, θ). 150Eu deduced prolate structure. 150,152Eu deduced levels, J, π, L, rotational bands, Nilsson assignments, rotational parameter. Q3D spectrograph. DWBA analysis.

doi: 10.1016/0370-2693(81)90796-6
Citations: PlumX Metrics


1978VO05      Z.Phys. A286, 341 (1978)

T.von Egidy, W.Kaiser, W.Mampe, C.Hillenbrand, W.Stoffl, R.G.Lanier, K.Muhlbauer, O.W.B.Schult, H.R.Koch, H.A.Baader, R.L.Mlekodaj, R.K.Sheline, E.B.Shera, J.Ungrin, P.T.Prokofjev, L.I.Simonova, M.K.Balodis, H.Seyfarth, B.Kardon, W.Delang, P.Gottel, D.Breitig, W.R.Kane, R.F.Casten, H.J.Scheerer, P.Glassl, E.Huenges, M.Loffler, H.Rosler, H.K.Vonach

Nuclear Levels in 152Eu

NUCLEAR REACTIONS 151Eu(n, X), E=th; measured Eγ, Iγ, E(ce), I(ce), γγ-coin, γγ(t). 151Eu(d, p), E=12, 14 MeV; 153Eu(d, t), E=12 MeV; 153Eu(p, d), E=18 MeV; measured σ. 152Eu deduced levels, K, J, π, T1/2, B(E2), ICC, Nilsson configurations. Curved crystal spectrometer, Ge(Li), Si(Li) detectors. Enriched targets.

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0321.


1977ST14      Z.Phys. A282, 97 (1977)

W.Stoffl, D.Rabenstein, K.Schreckenbach, T.von Egidy

Levels in 154Eu Populated by Thermal Neutron Capture

NUCLEAR REACTIONS 153Eu(n, γ), E=th; measured Eγ, Iγ, I(ce), γγ-coin, γ(t). 154Eu deduced levels, T1/2, λ, hindrance factors.


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