NSR Query Results
Output year order : Descending NSR database version of May 1, 2024. Search: Author = E.P.Horwitz Found 9 matches. 1982AH01 Nucl.Phys. A373, 434 (1982) Alpha Decay of 257100Fm RADIOACTIVITY 257Fm [from neutron irradiation of 244Cm in HFIR reactor]; measured Eα, Iα, I(ce), Eγ, Iγ; deduced hindrance factors. 253Cf deduced levels, γ-multipolarity, J, π.
doi: 10.1016/0375-9474(82)90543-7
1975WO02 J.Inorg.Nucl.Chem. 37, 21 (1975) K.L.Wolf, J.P.Unik, E.P.Horwitz, C.A.A.Bloomquist, D.Henderson, R.Sjoblom Production of Actinide Elements Using Secondary Reactions Induced by 19 GeV Electrons NUCLEAR REACTIONS U(e, X), E=19 GeV; measured yields of secondary reactions.
doi: 10.1016/0022-1902(75)80117-5
1972FL04 Phys.Rev. C5, 1725 (1972) K.F.Flynn, E.P.Horwitz, C.A.A.Bloomquist, R.F.Barnes, R.K.Sjoblom, P.R.Fields, L.E.Glendenin Distribution of Mass in the Spontaneous Fission of 256Fm RADIOACTIVITY, Fission 256Fm(SF); measured T1/2, mass distribution, fission yield.
doi: 10.1103/PhysRevC.5.1725
1972UN01 Nucl.Phys. A191, 233 (1972) J.P.Unik, E.P.Horwitz, K.L.Wolf, I.Ahmad, S.Fried, D.Cohen, P.R.Fields, C.A.A.Bloomquist, D.J.Henderson Production of Actinides and the Search for Super-Heavy Elements Using Secondary Reactions Induced by GeV Protons NUCLEAR REACTIONS W(p, X), E=28 GeV; 238U(p, X), E=12, 28 GeV; measured yields, cross sections, actinides, upper limits for transactinides.
doi: 10.1016/0375-9474(72)90513-1
1970AH01 Nucl.Phys. A140, 141 (1970) I.Ahmad, R.K.Sjoblom, R.F.Barnes, E.P.Horwitz, P.R.Fields Nuclear Decay Properties of Light Einsteinium Isotopes RADIOACTIVITY 248,249,250,251Es[from 249Bk(3He, xn), (α, xn)]; measured T1/2, Eα, Eγ, Iγ, γγ-coin, I(ce). 249,251Es; measured α/K X-ray ratios. 249,251Es deduced J, π. 249,251Cf deduced levels, J, π. 250Cf transitions deduced γ-multipolarity.
doi: 10.1016/0375-9474(70)90890-0
1970FI12 Nucl.Phys. A154, 407 (1970) P.R.Fields, I.Ahmad, R.F.Barnes, R.K.Sjoblom, E.P.Horwitz Nuclear Properties of 254Md, 255Md, 256Md, 257Md and 258Md RADIOACTIVITY 254,255,256,257,258Md[from 253,254,255Es(α, xn)]; measured T1/2, Eα, Iα, αγ-coin, α/(α+EC) ratio; deduced hindrance factors. 254mMd; measured T1/2.
doi: 10.1016/0375-9474(70)90166-1
1969MI08 J.Inorg.Nucl.Chem. 31, 1561 (1969) J.Milsted, E.P.Horwitz, A.M.Friedman, D.N.Metta Decay Properties of Berkelium-249 and Californium-249 RADIOACTIVITY 249Bk; measured Eα, Iα; deduced α/β-branching ratio, T1/2 (SF). 249Cf; measured Eα; deduced T1/2 (α), T1/2 (SF).
doi: 10.1016/0022-1902(69)80370-2
1968FI03 J.Inorg.Nucl.Chem. 30, 1345 (1968) P.R.Fields, I.Ahmad, R.K.Sjoblom, R.F.Barnes, E.P.Horwitz Nuclear Properties of 246Am and 247Am RADIOACTIVITY 247Am; measured T1/2, Eγ. 246Am; measured T1/2, Eγ, Iγ. 246Cm deduced levels.
doi: 10.1016/0022-1902(68)80272-6
1967FI03 Nucl.Phys. A96, 440 (1967) P.R.Fields, H.Diamond, A.M.Friedman, J.Milsted, J.L.Lerner, R.F.Barnes, R.K.Sjoblom, D.N.Metta, E.P.Horwitz Some New Properties of 254Es and 255Es RADIOACTIVITY 254,255Es[from Es(n, γ)]; measured T1/2, Eγ, Eα, Iα, αγ-coin, SF. 254Fm[from 254Es]; measured T1/2. 250Bk, 254Es deduced levels, J, π. 253Es(n, γ), reactor n-spectrum; measured σ.
doi: 10.1016/0375-9474(67)90725-7
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