NSR Query Results
Output year order : Descending NSR database version of May 1, 2024. Search: Author = L.Birstein Found 8 matches. 1989AL06 Nucl.Instrum.Methods Phys.Res. A276, 127 (1989) D.E.Alburger, Y.Akiba, E.Baker, L.Birstein, J.W.Olness, M.J.Tannenbaum Response of a Thin Avalanche Detector to Simultaneous Minimum Ionizing Particles NUCLEAR REACTIONS 19F(p, α), E=2 MeV; measured β+, β- spectra following 16O level decay; deduced detector response. Thin avalanche detector.
doi: 10.1016/0168-9002(89)90624-4
1976BI06 Nucl.Instrum.Methods 133, 279 (1976) The Manufacture of Needle Type Si(Li) Detectors for Bio-Medical Use RADIOACTIVITY 32P; measured Eβ.
doi: 10.1016/0029-554X(76)90620-0
1971BU09 Nucl.Phys. A167, 583 (1971) J.Burde, G.Engler, A.Ginsburg, V.Shitzer, A.A.Jaffe, A.Marinov, L.Birstein Isobaric Analogue Resonances in 127I, 125I and 123I NUCLEAR REACTIONS 126Te, 124Te, 122Te(p, p), (p, p')E=7.54-12.50 MeV;7.30-11.04 MeV;6.70-7.76, 8.51-11.20 MeV; measured σ(Ep, θ), σ(Ep, θ). 127I, 125I, 123I deduced resonances, L, J, π, p-width, S. 126Te deduced levels J, π. Enriched targets.
doi: 10.1016/0375-9474(71)90065-0
1970BU01 Nucl.Phys. A141, 375 (1970) J.Burde, G.Engler, A.Ginsburg, A.A.Jaffe, A.Marinov, L.Birstein Study of Elastic and Inelastic Scattering of Protons from 128Te and 130Te at Isobaric Analogue Resonances NUCLEAR REACTIONS 128Te, 130Te(p, p), (p, p'), (p, p'γ), E=7.66-11.87 MeV, 7.48-12.65 MeV; measured σ(E;θ), σ(E;Ep', Eγ, θ). 129,131I deduced resonances, J, π, L(p), level-width, S. 128,130Te deduced levels, J, π. Enriched targets.
doi: 10.1016/0375-9474(70)90854-7
1968BI01 Phys.Letters 26B, 220 (1968) L.Birstein, R.Chechik, C.Drory, E.Friedman, A.A.Jaffe, A.Wolf The Angular Distribution of Gamma Rays Following (α, n) and (p, n) Reactions NUCLEAR STRUCTURE 63Zn, 68Ga; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(68)90347-X
1968BI03 Nucl.Phys. A113, 193 (1968) L.Birstein, T.Chechik, C.Drory, E.Friedman, A.A.Jaffe, A.Wolf The Angular Distributions of Gamma Rays Following (α, n) and (p, n) Reactions NUCLEAR REACTIONS 59Co, 63Cu, 68Zn(p, nγ), E=3.1-5.2 MeV; 56Fe, 60Ni, 65Cu(α, nγ), E=6.5-9.3 MeV; measured σ(Eγ, θ). 59Ni, 63Zn, 68Ga deduced levels, J. Enriched targets.
doi: 10.1016/0375-9474(68)90893-2
1967BI04 Nucl.Phys. A97, 203 (1967) L.Birstein, C.Drory, A.A.Jaffe, J.Zioni The Reactions 60Ni(p, n)60Cu and 60Ni(α, n)63Zn NUCLEAR REACTIONS 60Ni(p, nγ), E = 7.0-7.8 MeV; 60Ni(α, nγ), E = 8.7-10.1 MeV; measured σ(E;Eγ), γγ-coin; deduced Q. 60Cu, 63Zn deduced levels. Enriched target, Ge(Li) detector.
doi: 10.1016/0375-9474(67)90780-4
1966BI07 Nucl.Phys. 84, 81 (1966) L.Birstein, M.Harchol, A.A.Jaffe, A.Tsukrovitz The Energy Levels of 63Zn NUCLEAR REACTIONS 63Cu(p, n), E=4-9 MeV; measured σ(E), Eγ, Iγ, nγ-coin, Q. 63Zn deduced levels, J, π. Enriched target.
doi: 10.1016/0029-5582(66)90434-2
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