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NSR database version of May 2, 2024.

Search: Author = J.Gindler

Found 59 matches.

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1994AH03      Nucl.Phys. A576, 246 (1994)

I.Ahmad, J.E.Gindler, M.P.Carpenter, D.J.Henderson, E.F.Moore, R.V.F.Janssens, I.G.Bearden, C.C.Foster

Level Structure of the Odd-Odd Nucleus 22489Ac

RADIOACTIVITY 228Pa(α) [from 232Th(p, 5n)]; measured Eα, Iα, Eγ, Iγ, I(ce), αγ-, αγγ-, α(ce)-coin. 224Ac deduced levels, J, π, ICC, γ-multipolarity.

doi: 10.1016/0375-9474(94)90259-3
Citations: PlumX Metrics


1994HE10      Nucl.Phys. A571, 427 (1994)

R.Hentzschel, H.R.Faust, H.O.Denschlag, B.D.Wilkins, J.Gindler

Mass, Charge and Energy Distributions in the Very Asymmetric Fission of 249Cf Induced by Thermal Neutrons

NUCLEAR REACTIONS 249Cf(n, F), E=thermal; measured fission product yields (A=69-87) at various kinetic energies of the fission fragments; deduced nuclear charge, kinetic energy distributions, odd-even factors.

doi: 10.1016/0375-9474(94)90220-8
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22296.


1989DJ01      Nucl.Phys. A496, 346 (1989)

M.Djebara, M.Asghar, J.P.Bocquet, R.Brissot, J.Crancon, Ch.Ristori, E.Aker, D.Engelhardt, J.Gindler, B.D.Wilkins, U.Quade, K.Rudolph

Mass and Nuclear-Charge Yields for 249Cf(n(th), F) at Different Fission-Product Kinetic Energies

NUCLEAR REACTIONS 249Cf(n, F), E=thermal; measured light fission product mass, nuclear-charge distributions vs kinetic energies; deduced fractional independent yields, odd-even effects, mean kinetic energies of masses, elements and isotones.

doi: 10.1016/0375-9474(89)90179-6
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22116.


1987AH05      Nucl.Phys. A472, 285 (1987)

I.Ahmad, J.E.Gindler, A.M.Friedman, R.R.Chasman, T.Ishii

Level Structure of 225Ac

RADIOACTIVITY 229Pa(α) [from 229Th(d, 2n), 230Th(d, 3n)]; measured Eγ, Iγ, I(ce), αγ-, γγ-coin. 225Ra(β-) [from 229Th α-decay]; measured Eγ, Iγ. 225Ac deduced levels, J, π.

doi: 10.1016/0375-9474(87)90211-9
Citations: PlumX Metrics


1986AK04      Radiat.Eff. 93, 1 (1986)

E.Aker, D.Engelhardt, R.Brissot, P.Brissot, P.Geltenbort, F.Gonnenwein, A.Oed, J.Gindler, B.Wilkins

Mass and Energy Distribution of Fission Fragments in 249Cf(n(th), f)

NUCLEAR REACTIONS 249Cf(n, F), E=thermal; measured fission fragment mass, energy distribution; deduced relative mass yields.

doi: 10.1080/00337578608207415
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset21967.


1985BA29      Phys.Rev. C32, 195 (1985); Erratum Phys.Rev. C33, 385 (1986)

B.B.Back, R.R.Betts, J.E.Gindler, B.D.Wilkins, S.Saini, M.B.Tsang, C.K.Gelbke, W.G.Lynch, M.A.McMahan, P.A.Baisden

Angular Distributions in Heavy-Ion-Induced Fission

NUCLEAR REACTIONS, ICPND 208Pb, 232Th, 238U, 248Cm(16O, F), E=85-148 MeV; 208Pb(19F, F), E=110-190 MeV; 208Pb(24Mg, F), E=140-210 MeV; 208Pb(28Si, F), E=160-260 MeV; 197Au(32S, F), E=185-255 MeV; 208Pb(32S, F), E=180-266 MeV; measured total fission σ(E), σ(θ) vs E. Standard fission theory analysis.

doi: 10.1103/PhysRevC.32.195
Citations: PlumX Metrics


1985IS03      Nucl.Phys. A444, 237 (1985)

T.Ishii, I.Ahmad, J.E.Gindler, A.M.Friedman, R.R.Chasman, S.B.Kaufman

Measurement of Rates of Fast E1 Transitions in Ac-Ra Nuclei

RADIOACTIVITY 225Ra(β-); 229Th, 231Pa(α); measured γγ(t), αγ(t). 225Ra levels deduced T1/2, quadrupole moment, B(λ), α-branching ratio. 225,227Ac deduced T1/2, B(λ).

doi: 10.1016/0375-9474(85)90348-3
Citations: PlumX Metrics


1985KU24      Phys.Rev. C32, 2036 (1985)

W.Kutschera, I.Ahmad, S.G.Armato III, A.M.Friedman, J.E.Gindler, W.Henning, T.Ishii, M.Paul, K.E.Rehm

Spontaneous 14C Emission from 223Ra

RADIOACTIVITY 223Ra(14C), (α) [from 227Th decay]; measured 14C(SF-decay), (14C)/α branching ratio. Enge split-pole magnetic spectrograph.

doi: 10.1103/PhysRevC.32.2036
Citations: PlumX Metrics


1984AH01      Phys.Rev.Lett. 52, 503 (1984)

I.Ahmad, R.R.Chasman, J.E.Gindler, A.M.Friedman

Enhanced E1 Transition Rates and Octupole Deformation in 225Ac

RADIOACTIVITY 229Pa(α); 225Ra(β-); measured I(K X-ray), Iγ, ratio. 225Ra level deduced J, π. 225Ac levels deduced J, π, γ-branching, γ-multipolarity, enhanced B(E1), parity doublet rotational band characteristics.

doi: 10.1103/PhysRevLett.52.503
Citations: PlumX Metrics


1984BA01      Phys.Rev.Lett. 52, 397 (1984)

B.B.Back, R.R.Betts, K.Cassidy, B.G.Glagola, J.E.Gindler, L.E.Glendenin, B.D.Wilkins

Fission Anisotropies and Sequential Fission: A Response

NUCLEAR REACTIONS 208Pb, 238U(16O, X), E=80-180 MeV; calculated fission σ(E); deduced sharp cut-off model validity.

doi: 10.1103/PhysRevLett.52.397
Citations: PlumX Metrics


1984WI13      Phys.Rev. C30, 1228 (1984)

B.D.Wilkins, B.B.Back, J.E.Gindler, B.G.Glagola, K.Kwiatkowski, S.H.Zhou, V.E.Viola, Jr.

Mass and Kinetic Energy Distributions in Near-Barrier Fission of 182W

NUCLEAR REACTIONS, ICPND 178Hf(α, F), E=49.2 MeV; measured fission fragment yields, total kinetic energy release vs fragment mass; deduced no shell effects. 182W deduced fission characteristics.

doi: 10.1103/PhysRevC.30.1228
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2498.


1983AH02      Phys.Rev. C27, 2239 (1983)

I.Ahmad, J.Hines, J.E.Gindler

Electron Capture Decay of 237Pu, 235Np and 236Np

RADIOACTIVITY 237Pu(EC), (α) [from 235U(α, 2n), E=31 MeV]; 235Np(EC), (α) [from 235U(d, 2n), E=18 MeV]; 236Np(EC), (β-) [from 238U(d, 4n), E=21 MeV]; measured Eγ, Iγ, I(ce), I X-ray; deduced log ft(EC), log ft(β-). 237Np, 236U, 236Pu deduced levels, J, π, γ-multipolarity. Cooled Si(Li) electron spectrometer, mass separated 237Pu.

doi: 10.1103/PhysRevC.27.2239
Citations: PlumX Metrics


1983BA07      Phys.Rev.Lett. 50, 818 (1983)

B.B.Back, R.R.Betts, K.Cassidy, B.G.Glagola, J.E.Gindler, L.E.Glendenin, B.D.Wilkins

Experimental Signatures of Quasifission Reactions

NUCLEAR REACTIONS 238U(16O, F), E=90, 110, 130, 148 MeV; 208Pb(32S, F), E=185, 198, 205, 219, 225 MeV; measured fission fragment σ(θ), absolute total fission σ; deduced quasifission mechanism, rigid to effective moment of inertia ratio. Optical, extra push model analyses.

doi: 10.1103/PhysRevLett.50.818
Citations: PlumX Metrics


1983GI05      Phys.Rev. C27, 2058 (1983)

J.E.Gindler, L.E.Glendenin, D.J.Henderson, J.W.Meadows

Mass Distributions in Monoenergetic-Neutron-Induced Fission of 239Pu

NUCLEAR REACTIONS 239Pu(n, F)87Kr/88Kr/91Sr/92Sr/93Y/97Zr/99Mo/103Ru/105Ru/109Pd/111Ag/112Pd/115Cd/121Sn/125Sn/127Sb/129Sb/132Te/134Te/133I/134I/135I/135Xe/140Ba/142La/143Ce, E=0.17-7.9 MeV; measured fission fragment yield vs mass, σ(fission) vs E. Activation technique.

doi: 10.1103/PhysRevC.27.2058
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12817.


1982AH08      Phys.Rev.Lett. 49, 1758 (1982)

I.Ahmad, J.E.Gindler, R.R.Betts, R.R.Chasman, A.M.Friedman

Possible Ground-State Octupole Deformation in 229Pa

RADIOACTIVITY 229Pa(EC), 229U(EC) [from mass separation]; measured I(ce), Eγ, Iγ, γγ-, γ(X-ray)-, (ce)(X-ray)-coin. 229Pa deduced levels, J, π, K, γ-multipolarity, ground state doublet splitting, Nilsson assignment.

NUCLEAR REACTIONS 231Pa(p, t), E=16.5 MeV; measured σ(Et). 229Pa deduced levels, J, π, possible octupole deformation, Nilsson assignment, K.

doi: 10.1103/PhysRevLett.49.1758
Citations: PlumX Metrics


1981GI02      J.Inorg.Nucl.Chem. 43, 895 (1981)

J.E.Gindler, D.J.Henderson, L.E.Glendenin

Spontaneous Fission Yields for 246Cm

RADIOACTIVITY, Fission 246Cm(SF); measured Eγ, Iγ; deduced cumulative yields for 95,97Zr, 99Mo, 103,105Ru, 111,112Ag, 131,133,135I, 132Te, 140Ba, 141,143,144Ce, 142La, 147Nd.

doi: 10.1016/0022-1902(81)80145-5
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset10986.


1981GI05      J.Inorg.Nucl.Chem. 43, 1433 (1981)

J.E.Gindler, L.E.Glendenin, D.J.Henderson

Mass Distribution for Thermal-Neutron-Induced Fission of 229Th

NUCLEAR REACTIONS, Fission 229Th(n, F), E=thermal; measured yields for 77,78As, 83Se, 85m,87,88Kr, 84Br, 91,92Sr, 93,94Y, 95,97Zr, 99Mo, 103,105Ru, 109,112Pd, 115Cd, 111Ag, 121,125Sn, 127,129Sb, 132,134Te, 131,133,135I, 140Ba, 141,143,144Ce, 142La, 147,149Nd. Activation technique.

doi: 10.1016/0022-1902(81)80313-2
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset10966.


1981GI06      J.Inorg.Nucl.Chem. 43, 1743 (1981)

J.E.Gindler, L.E.Glendenin, D.J.Henderson

Mass Distributions for the Fission of 250Cf

NUCLEAR REACTIONS, Fission 249Cf(n, F), E=thermal; measured yields for 85m,88Kr, 91,92Sr, 93,94Y, 95,97Zr, 99Mo, 103,105Ru, 109,112Pd, 111Ag, 115,115m,117Cd, 121,123,125Sn, 127,129Sb, 131,133,134,135I, 132,134Te, 135Xe, 136,137Cs, 139,140Ba, 141,143,144Ce, 142La, 147,149Nd, 151Pm, 153,155,156Sm, 157Eu; deduced mass distribution characteristics. Activation technique.

RADIOACTIVITY, Fission 250Cf(SF); measured yields for 101,104Tc, 105Ru, 107Rh, 133I, 139Ba, 142La; deduced heavy, light fragment mean mass.

doi: 10.1016/0022-1902(81)80376-4
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12710.


1981GI18      J.Inorg.Nucl.Chem. 43, 445 (1981)

J.E.Gindler, L.E.Glendenin, E.L.Krapp, S.J.Fernandez, K.F.Flynn, D.J.Henderson

Mass distribution in thermal-neutron-induced fission of long-lived 236Np

NUCLEAR REACTIONS 236Np(n, F)84Br/85Kr/87Kr/88Kr/91Sr/92Sr/93Y/95Zr/97Zr/99Mo/103Ru/104Tc/105Ru/104Tc/105Ru/109Pd/111Ag/112Pd/115Cd/121Sn/125Sn/127Sb, E thermal; measured fission products, Eγ, Iγ; deduced fission yields.

doi: 10.1016/0022-1902(81)80481-2
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset10967.


1981GI19      Trans.Amer.Nucl.Soc. 39, 877 (1981)

J.E.Gindler, L.E.Glendenin, D.J.Henderson, J.W.Meadows

Neutron-Induced Fission Yields of 235U from 0.17 to 8.1 MeV

NUCLEAR REACTIONS 235U(n, F)84Br/85Kr/87Kr/88Kr/89Rb/91Sr/92Sr/93Y/94Y/95Zr/97Zr/99Mo/103Ru/105Ru/109Pd/111Ag/112Pd/115Cd/121Sn/125Sn/127Sb/129Sb/131I/132Te/133I/134Te/134I/135Xe/138Xe/139Ba/140Ba/141Ce/142La/143Ce/144Ce/147Nd/149Pm/151Pm, E=0.17-8.1 MeV; measured fission products, Eγ, Iγ, Eβ, Iβ; deduced yields.

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12729.


1981GL04      Phys.Rev. C24, 2600 (1981)

L.E.Glendenin, J.E.Gindler, D.J.Henderson, J.W.Meadows

Mass Distributions for Monoenergetic-Neutron-Induced Fission of 235U

NUCLEAR REACTIONS, Fission 235U(n, F), E=0.17, 0.55, 1, 2, 4, 5.5, 6.3, 7.1, 8.1 MeV; measured yields vs E for 84Br, 85m,87,88Kr, 89Rb, 91,92Sr, 93,94Y, 95,97Zr, 99Mo, 103,105Ru, 109,112Pd, 111Ag, 115Cd, 121,125Sn, 127,129Sb, 131,133,134,135I, 135,138Xe, 139,140Ba, 141,143,144Ce, 142La, 141,143,144Ce, 147Nd, 149,151Pm; deduced second-chance fission characteristics. Activation techniques.

doi: 10.1103/PhysRevC.24.2600
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12729.


1980GL05      Phys.Rev. C22, 152 (1980)

L.E.Glendenin, J.E.Gindler, I.Ahmad, D.J.Henderson, J.W.Meadows

Mass Distributions in Monoenergetic-Neutron-Induced Fission of 232Th

NUCLEAR REACTIONS 232Th(n, F), E=2, 3, 4, 5.9, 6.4, 6.9, 7.6, 8 MeV; measured Eγ, Iγ, Iβ; deduced production σ for 77,78Se, 84Br, 85,87,88Kr, 88,89Rb, 91,92,93Sr, 91,93,94Y, 97Zr, 97Nb, 99Mo, 99,101Tc, 103,105Ru, 109,112Pd, 111Ag, 115Cd, 121Sn, 127,129Sb, 131,133,135I, 132,134Te, 135,138Xe, 138Cs, 139,140,141Ba, 140,142La, 141,143,146Ce, 147,149Nd.

doi: 10.1103/PhysRevC.22.152
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset10920.


1979GI04      Phys.Rev. C19, 1806 (1979)

J.Gindler

Dependence of Neutron Yield on Fragment Mass for Several Low-Energy Fissioning Systems

RADIOACTIVITY, Fission 252,254Cf (SF), 256Fm (SF); measured nothing; deduced neutron yield, fragment mass, energy distributions. Iterative method.

NUCLEAR REACTIONS 245Cm, 254Es(n, F), E=thermal; measured nothing; deduced neutron yield, fragment mass, energy distributions. Iterative method.

doi: 10.1103/PhysRevC.19.1806
Citations: PlumX Metrics


1979GI06      Nucl.Sci.Eng. 70, 101 (1979)

J.E.Gindler, L.E.Glendenin, J.W.Meadows, Jr., K.F.Flynn

Fission Yields for Fast-Neutron Fission of Uranium-238

NUCLEAR REACTIONS 238U(n, F), E=1.5-7.7 MeV; measured nothing; calculated fission yields in 238U exposed to watt neutron spectrum. Results compared with available compilations for fast fission yields.

doi: 10.13182/NSE79-A18933
Citations: PlumX Metrics


1978NA01      Phys.Rev. C17, 163 (1978)

S.Nagy, K.F.Flynn, J.E.Gindler, J.W.Meadows, L.E.Glendenin

Mass Distributions in Monoenergetic-Neutron-Induced Fission of 238U

NUCLEAR REACTIONS 238U(n, F), E=1.5, 2.0, 3.9, 5.5, 6.9, 7.7 MeV; measured mass yields.

doi: 10.1103/PhysRevC.17.163
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset10798.


1977FL07      J.Inorg.Nucl.Chem. 39, 759 (1977)

K.F.Flynn, J.E.Gindler, L.E.Glendenin

Mass Distributions for the Spontaneous Fission of 248Cm and 250Cf

RADIOACTIVITY, Fission 248Cm(SF), 250Cf(SF); measured mass distribution fission yield.

doi: 10.1016/0022-1902(77)80149-8
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset10979.


1977GI11      Inorg.Nucl.Chem.Lett. 13, 95 (1977)

J.E.Gindler, L.E.Glendenin

The Half-Lives of 109Pd and 112Pd

RADIOACTIVITY 109,112Pd; measured T1/2.

doi: 10.1016/0020-1650(77)80061-5
Citations: PlumX Metrics


1977GI15      Phys.Rev. C16, 1483 (1977)

J.E.Gindler, K.F.Flynn, L.E.Glendenin, R.K.Sjoblom

Distribution of Mass, Kinetic Energy, and Neutron Yield in the Spontaneous Fission of 254Fm

RADIOACTIVITY, Fission 254Fm(SF); measured radiochemical mass yields, fragment energy; deduced neutron yields, σ(A, E(fragment)).

doi: 10.1103/PhysRevC.16.1483
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset10642.


1976FL03      J.Inorg.Nucl.Chem. 38, 661 (1976)

K.F.Flynn, J.E.Gindler, L.E.Glendenin, R.K.Sjoblom

Mass Distributions for the Spontaneous Fission of 253Es and the Thermal-Neutron-Induced Fission of 254Es

RADIOACTIVITY, Fission 253Es(SF); measured mass yield.

NUCLEAR REACTIONS 254Es(n, F), E=thermal; measured mass yield.

doi: 10.1016/0022-1902(76)80333-8
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13340.


1976GI14      Inorg.Nucl.Chem.Lett. 12, 931 (1976)

J.E.Gindler

The Half-Lives of 83Rb and 84Rb

RADIOACTIVITY 83,84Rb; measured T1/2.

doi: 10.1016/0020-1650(76)80011-6
Citations: PlumX Metrics


1975FL04      J.Inorg.Nucl.Chem. 37, 881 (1975)

K.F.Flynn, J.E.Gindler, L.E.Glendenin

The Mass Distribution for Spontaneous Fission of 252Cf

RADIOACTIVITY, Fission 252Cf(SF); measured fission yields for 35 mass chains.

doi: 10.1016/0022-1902(75)80666-X
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13459.


1975FL06      Phys.Rev. C11, 1676 (1975)

K.F.Flynn, J.E.Gindler, R.K.Sjoblom, L.E.Glendenin

Mass Distributions for Thermal-Neutron-Induced Fission of 255Fm and 251Cf

NUCLEAR REACTIONS 251Cf, 255Fm(n, F), E=0.025 eV; measured radiochemical mass yields, σ.

doi: 10.1103/PhysRevC.11.1676
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset10516.


1975FL09      Phys.Rev. C12, 1478 (1975)

K.F.Flynn, J.E.Gindler, L.E.Glendenin

Distribution of Mass in Thermal-Neutron-Induced Fission of 257Fm

NUCLEAR REACTIONS 257Fm(n, F), E=0.025 eV; measured radiochemical mass yields.

doi: 10.1103/PhysRevC.12.1478
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13458.


1975FL10      Trans.Amer.Nucl.Soc. 22, 677 (1975)

K.F.Flynn, S.Nagy, L.E.Glendenin, J.E.Gindler, J.W.Meadows

Monoenergetic Neutron Fission of 238U

NUCLEAR REACTIONS 238U(n, F)83Br/85Kr/87Kr/88Kr/89Rb/89Sr/91Y/92Sr/93Y/94Y/95Zr/97Zr/99Mo/101Mo/103Ru/105Ru/106Ru/107Rh/109Pd/111Ag/112Pd/115Cd/121Sn/125Sn/131I/132Te/133I/135I/138Xe/139Ba/140Ba/141Ce/142La/143Ce/144Ce/146Ce/147Nd/149Nd/149Pm/151Pm/153Sm/156Eu, E=2, 8 MeV; measured reaction products, Eγ, Iγ; deduced fission product yields.

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset10798.


1974GE06      J.Phys.(Paris) 35, 483 (1974)

S.Gerstenkorn, P.Luc, J.Verges, D.W.Engelkemeir, J.E.Gindler, F.S.Tomkins

Structures Hyperfines du Spectre d'Etincelle, Moment Magnetique et Quadrupolaire de l'Isotope 229 du Thorium

NUCLEAR MOMENTS 229Th; measured μ, quadrupole moment. Optical spectroscopy.

doi: 10.1051/jphys:01974003506048300
Citations: PlumX Metrics


1973GI06      J.Inorg.Nucl.Chem. 35, 2617 (1973)

J.E.Gindler, K.F.Flynn, L.E.Glendenin

The Half-Life of 132Cs

RADIOACTIVITY 132Cs; measured T1/2.

doi: 10.1016/0022-1902(73)80490-7
Citations: PlumX Metrics


1972EN06      J.Inorg.Nucl.Chem. 34, 1799 (1972)

D.W.Engelkemeir, J.E.Gindler

The Negatron Half-Life of the Long-Lived 236Np Isomer

RADIOACTIVITY 236mNp; measured T1/2.

doi: 10.1016/0022-1902(72)80525-6
Citations: PlumX Metrics


1970AU01      J.Inorg.Nucl.Chem. 32, 731 (1970)

D.C.Aumann, J.E.Gindler

The Ratio of 111Pd Isomers Formed in Charged-Particle and Photon-Induced Fission of Several Heavy Nuclides

NUCLEAR REACTIONS, Fission 230,232Th, 236U(α, F), E=24-45 MeV; 232Th, 233,234,235,236,238U(γ, F), E < 17 MeV; measured 110Ag activity. 111Pd deduced isomeric σ ratio.

doi: 10.1016/0022-1902(70)80055-0
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0086.


1970GI02      Nucl.Phys. A145, 337 (1970)

J.Gindler, H.Munzel, J.Buschmann, G.Christaller, F.Michel, G.Rohde

Fragment Angular Distributions in the Fission of Heavy Nuclei by 103 MeV Helium Ions and 51.5 MeV Deuterons

NUCLEAR REACTIONS, Fission 197Au, 209Bi, 233,234,235,238U(α, F), E=103 MeV; 209Bi, 233,234,235,238U(d, F), E=51.5 MeV; measured fission fragment σ(θ), σ(α), F, σ(d), F. Enriched targets.

doi: 10.1016/0375-9474(70)90427-6
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetB0030.


1969AU02      J.Inorg.Nucl.Chem. 31, 1935 (1969)

D.C.Aumann, K.F.Flynn, J.E.Gindler, L.E.Glendenin

Formation of 111Pd isomers in neutron fission of several heavy nuclides

NUCLEAR REACTIONS, Fission 232Th, 233,235,238U(n, F), E= thermal; measured 111Pd isomer yield ratios. 111Rh deduced β-branching.

doi: 10.1016/0022-1902(69)90008-6
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13242.


1968CO28      Phys.Rev. 176, 1421(1968)

R.E.Cote, H.Diamond, J.E.Gindler, H.Shwe

Neutron Resonances of Th230

NUCLEAR REACTIONS 230Th(n, X), E = 0.05-500 eV; measured σ(E). 230Th deduced T1/2. 231Th deduced resonances, level-width.

doi: 10.1103/PhysRev.176.1421
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12280.


1966CO21      WASH-1068, p.17 (1966); and Priv.Comm. (1966)

R.E.Cote, H.Diamond, J.E.Gindler

The Neutron Resonances of Th230

NUCLEAR STRUCTURE 231Th; measured not abstracted; deduced nuclear properties.


1964GI07      Phys.Rev. 136, B1333 (1964)

J.E.Gindler, G.L.Bate, J.R.Huizenga

Fission Fragment Angular Distributions in Charged- Particle-Induced Fission of Ra226

NUCLEAR REACTIONS 226Ra(α, f), 226Ra(d, f), 226Ra(p, f), E=-1.0 eV-43 MeV; measured products; deduced σ(θ), σ, σ(E). Data were imported from EXFOR entry C0714.

doi: 10.1103/PhysRev.136.B1333
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0714.


1963DI05      J.Inorg.Nucl.Chem. 25, 143 (1963)

H.Diamond, J.E.Gindler

Alpha Half-Lives of 216Po, 217At and 218Rn

NUCLEAR STRUCTURE 217At, 218Rn, 216Po; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0022-1902(63)80001-9
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1963GI17      Radiochim.Acta 2, 58 (1963)

J.E.Gindler, D.W.Engelkemeir

Half-Life Determination of 220Rn

NUCLEAR STRUCTURE 220Rn; measured not abstracted; deduced nuclear properties.


1962DI08      TID-16202 (1962); Nucl.Sci.Abstr. 17, 1511, Abstr.11632 (1963)

H.Diamond, J.E.Gindler

Alpha Half-Lives of Po216, At217 and Rn218

NUCLEAR STRUCTURE 218Rn, 217At, 216Po; measured not abstracted; deduced nuclear properties.


1962HU14      Nucl.Phys. 34, 439 (1962)

J.R.Huizenga, K.M.Clarke, J.E.Gindler, R.Vandenbosch

Photofission Cross Sections Of Several Nuclei With Mono-Energetic Gamma Rays

NUCLEAR REACTIONS 232Th(γ, f), 233U(γ, f), 234U(γ, f), 235U(γ, f), 236U(γ, f), 238U(γ, f), 237Np(γ, f), E=6.1-7 MeV; measured products; deduced σ, σ(E). Data were imported from EXFOR entry M0505.

doi: 10.1016/0029-5582(62)90231-6
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1961CO16      Bull.Am.Phys.Soc. 6, No.5, 417, C1 (1961)

R.E.Cote, H.Diamond, J.E.Gindler

Total Neutron Cross Section of Th229

NUCLEAR STRUCTURE 229Th; measured not abstracted; deduced nuclear properties.

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12298.


1960EN09      Priv.Comm., quoted by 1964Hy02, p.637, unpublished (1960)

D.Engelkemeir, J.Gindler


1960GI03      Phys.Rev. 119, 1645 (1960)

J.E.Gindler, D.W.Engelkemeir

Alpha Decay of Np235

NUCLEAR STRUCTURE 235Np; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.119.1645
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1960GI04      J.Inorg.Nuclear Chem. 15, 1 (1960)

J.E.Gindler, K.F.Flynn, J.Gray, Jr.

Thermal Neutron Fission Cross-Section of 229Th

NUCLEAR STRUCTURE 229Th; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0022-1902(60)80002-4
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12259.


1959GI54      Phys.Rev. 115, 1271 (1959)

J.E.Gindler, J.Gray, Jr., J.R.Huizenga

Neutron Fission Cross Sections of Pu236 and Pu237

doi: 10.1103/PhysRev.115.1271
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1959GI58      J.Inorg.Nuclear Chem. 12, 8 (1959)

J.E.Gindler, R.K.Sjoblom

Electron-Capture/Negatron-Emission Branching Ratio of 236Np (22 hr)

doi: 10.1016/0022-1902(59)80086-5
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1958GI05      Phys.Rev. 109, 1263 (1958)

J.E.Gindler, J.R.Huizenga, D.W.Engelkemeir

Neptunium Isotopes: 234, 235, 236

doi: 10.1103/PhysRev.109.1263
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1956FR07      Phys.Rev. 102, 585 (1956)

A.M.Friedman, J.E.Gindler, R.F.Barnes, R.Sjoblom, P.R.Fields

Properties of Fm252

doi: 10.1103/PhysRev.102.585
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1956HU28      Bull.Am.Phys.Soc. 1, No.4, 171, E7 (1956)

J.R.Huizenga, D.W.Engelkemeir, M.S.Freedman, F.T.Porter, J.E.Gindler

Radiations of Np234


1955BE99      Proc.Int.Conf.Peaceful Uses Atomic Energy, Geneva (1955), United Nations Publ., Vol.7, p.261 (1956)

W.C.Bentley, H.Diamond, P.R.Fields, A.M.Friedman, J.E.Gindler, D.C.Hess, J.R.Huizenga, M.G.Inghram, A.H.Jaffey, L.B.Magnusson, W.M.Manning, J.F.Mech, G.L.Pyle, R.Sjoblom, C.M.Stevens, M.H.Studier

The Formation of Higher Isotopes and Higher Elements by Reactor Irradiation of Pu239; Some Nuclear Properties of the Heavier Isotopes


1955FI36      Phys.Rev. 100, 172 (1955)

P.R.Fields, J.E.Gindler, A.L.Harkness, M.H.Studier, J.R.Huizenga, A.M.Friedman

Electron Capture Decay of Am244 and the Spontaneous Fission Half-Life Of Pu244

doi: 10.1103/PhysRev.100.172
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1955ST10      Phys.Rev. 97, 88 (1955)

M.H.Studier, J.E.Gindler, C.M.Stevens

Long-Lived Isomer of Np236

doi: 10.1103/PhysRev.97.88
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