NSR Query Results
Output year order : Descending NSR database version of May 9, 2024. Search: Author = A.Friedman Found 85 matches. 2008KA27 Phys.Rev. C 78, 014301 (2008) K.Katori, I.Ahmad, A.M.Friedman Two-quasineutron states in 24898Cf and 25098Cf and the neutron-neutron residual interactions NUCLEAR REACTIONS 249Cf(d, p), (d, t), E=11, 12, 13, 14 MeV; measured charged particle energies, σ(θ). 248,250Cf; deduced levels, J, π, bands, configurations. Comparison with model calculations.
doi: 10.1103/PhysRevC.78.014301
1998WH01 Phys.Rev. C57, 1112 (1998) D.H.White, R.W.Hoff, H.G.Borner, K.Schreckenbach, F.Hoyler, G.Colvin, I.Ahmad, A.M.Friedman, J.R.Erskine Nuclear Structure of 241Pu from Neutron-Capture, (d, p)-, and (d, t)-Reaction Measurements NUCLEAR REACTIONS 240Pu(n, γ), E=thermal; measured Eγ, Iγ, E(ce), I(ce). 240Pu(d, p), 242Pu(d, t), E=12 MeV; measured σ(E(p), θ), σ(E(t), θ). 241Pu deduced levels, J, π, band structure, configurations. RADIOACTIVITY 245Cm(α); measured Eγ, Iγ. 241Pu deduced levels, J, π.
doi: 10.1103/PhysRevC.57.1112
1990AH02 Phys.Lett. 251B, 338 (1990) I.Ahmad, R.R.Chasman, A.M.Friedman, S.W.Yates Neutron Single Particle States Above the N = 152 Subshell NUCLEAR REACTIONS 250Cf(d, p), E=12 MeV; measured proton spectra. 251Cf deduced levels, rotational bands, Nilsson assignments.
doi: 10.1016/0370-2693(90)90716-J
1988DE24 Appl.Radiat.Isot. 39, 709 (1988) Production of 75Br via the 78Kr(d, nα)75Br Reaction NUCLEAR REACTIONS, ICPND 78Kr(d, nα), E=21.5 MeV; measured residual production yield.
doi: 10.1016/0883-2889(88)90062-7
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
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
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
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
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
1982FR18 J.Labelled Compd.Radiopharm. 19, 1427 (1982) A.M.Friedman, O.J.DeJesus, P.Harper, C.Armstrong Preparation of 75Br by the 78Kr(p, α)75Br Reaction NUCLEAR REACTIONS, ICPND 78Kr(p, α), E=12-15 MeV; measured residual production σ(E). Activation technique.
1980AH01 Phys.Rev. C21, 874 (1980) I.Ahmad, A.M.Friedman, S.W.Yates Vibrational States in 250Cf Excited by the (d, d') Reaction NUCLEAR REACTIONS 250Cf(d, d'), E=15 MeV; measured σ(Ed, θ). 250Cf deduced levels, J, π, B(λ). Mass separated target.
doi: 10.1103/PhysRevC.21.874
1979AH03 Phys.Rev. C20, 290 (1979) I.Ahmad, S.W.Yates, R.K.Sjoblom, A.M.Friedman Proton States in 247Bk Excited by 246Cm(α, t) Reactions and 247Cf (Electron Capture) and 251Es (α) Decays RADIOACTIVITY 247Cf [from (α, 3n), E=40 MeV]; measured Eγ, Iγ, I(ce). 251Es [from 249Cf(α, 2n), E=40 MeV]; measured Eα, Iα. 251Es levels deduced hf. Mass separation. 247Bk deduced levels, ICC, multipolarity, log ft. NUCLEAR REACTIONS 246Cm(α, t), E=28.0, 29.0 MeV; measured σ(Et, θ). 247Bk deduced levels, J, π, Nilsson assignment, (2J+1)S.
doi: 10.1103/PhysRevC.20.290
1979IO01 Nucl.Phys. A313, 283 (1979) V.A.Ionescu, J.Kern, R.F.Casten, W.R.Kane, I.Ahmad, J.Erskine, A.M.Friedman, K.Katori Nuclear Levels in 238Np NUCLEAR REACTIONS 237Np(n, γ), E=17-650, 2600-5500 keV; measured Eγ, Iγ; deduced Q. 237Np(d, p), E=12 MeV; measured σ(Ep). 238Np deduced levels, K, J, π. Nilsson configurations.
doi: 10.1016/0375-9474(79)90501-3
1978AH02 Phys.Rev. C17, 2163 (1978) I.Ahmad, R.K.Sjoblom, A.M.Friedman, S.W.Yates Proton States in the Z = 99 Nucleus 251Es Excited by 251Fm Electron Capture Decay and 250Cf(α, t) Reaction RADIOACTIVITY 251Fm [from 249Cf(α, 2n)]; measured Eγ, Iγ, I(ce), γγ-coin; deduced α-branching, EC branching, log ft. 251Es deduced levels, ICC, λ, K, J, π. Mass separated activity. NUCLEAR REACTIONS 250Cf(α, t), E=28 MeV; measured σ(Et). 251Es deduced levels. Mass separated 250Cf.
doi: 10.1103/PhysRevC.17.2163
1978GR10 Nucl.Phys. A303, 265 (1978) H.C.Griffin, I.Ahmad, A.M.Friedman, L.E.Glendenin Nuclear Spectroscopic Studies of the 23.7 h 248Bk RADIOACTIVITY 248Bk [from 248Cm(d, 2n), 247Bk(n, γ)]; measured T1/2, Eγ, Iγ, L X-ray-L X-ray, Kα-L X-ray, Kβ-L X-ray, βγ-, β-L X-ray coin; deduced log ft, Qβ-, Q(ϵ), decay branching. 248Cm, 248Cf deduced levels, γ-multipolarity, J, π. Mass separated 248Bk.
doi: 10.1016/0375-9474(78)90357-3
1977AH01 Phys.Rev.Lett. 39, 12 (1977) I.Ahmad, A.M.Friedman, R.R.Chasman, S.W.Yates Proton Orbital 1/2- [521] and the Stability of Superheavy Elements NUCLEAR REACTIONS 250Cf, 246Cm(α, t), E=28 MeV; measured σ(Et). 251Es, 247Bk deduced levels, K, J, π.
doi: 10.1103/PhysRevLett.39.12
1977CH27 Rev.Mod.Phys. 49, 833 (1977) R.R.Chasman, I.Ahmad, A.M.Friedman, J.R.Erskine Survey of Single-Particle States in the Mass Region A > 228 NUCLEAR STRUCTURE 229,231,233Th, 233,235,237,239U, 237,239,241,243,245Pu, 243,245,247,249Cm, 247,249,251,253Cf, 251Fm, 231,233Pa, 235,237,239Np, 239,241,243,245Am, 247,249Bk; analyzed structure data; deduced level character, K, J, π.
doi: 10.1103/RevModPhys.49.833
1976CA25 Phys.Rev. C14, 912 (1976) R.F.Casten, W.R.Kane, J.R.Erskine, A.M.Friedman, D.S.Gale States in 243Pu from the (n, γ), (d, p), and (d, t) Reactions NUCLEAR REACTIONS 242Pu(n, γ), E=2.96 eV; measured Eγ, Iγ, γγ-coin, γγ(t). 242Pu(d, p), (d, t), E=12 MeV; measured σ(θ); deduced Q. 243Pu deduced levels, K, J, π, λ, L, transition rates, Nilsson assignments. Enriched targets.
doi: 10.1103/PhysRevC.14.912
1976HO01 Phys.Rev.Lett. 36, 183 (1976) R.J.Holt, J.P.Schiffer, J.Specht, L.M.Bollinger, G.E.Thomas, S.M.Fried, J.J.Hines, A.M.Friedman Search for Stable, Abnormal (Collapsed) Nuclei in Nature NUCLEAR REACTIONS Rn(n, γ), E=thermal; measured high energy γ rays; deduced Rn nuclei with abnormally-high-density states.
doi: 10.1103/PhysRevLett.36.183
1976VA11 Phys.Rev. C13, 1893 (1976) R.Vandenbosch, M.P.Webb, T.D.Thomas, S.W.Yates, A.M.Friedman Elastic Scattering of 84Kr by 208Pb NUCLEAR REACTIONS 208Pb(84Kr, 84Kr), E=494, 510, 718 MeV; measured σ(θ). Fresnel, parametrized phase shift, optical model analyses.
doi: 10.1103/PhysRevC.13.1893
1976YA02 Phys.Rev.Lett. 36, 1125 (1976) S.W.Yates, I.Ahmad, A.M.Friedman, K.Katori, C.Castaneda, T.E.Ward Configuration Mixing of Two-Quasiparticle States in 250Cf RADIOACTIVITY 250Es; measured Eγ, Iγ. 250Cf deduced levels, K, J, π. NUCLEAR REACTIONS 249Cf(d, p), E=12 MeV; 249Bk(α, t), E=28 MeV; measured σ. 250Cf deduced levels, J, π, K.
doi: 10.1103/PhysRevLett.36.1125
1975ER01 Phys.Rev. C11, 561 (1975) J.R.Erskine, G.Kyle, R.R.Chasman, A.M.Friedman Study of 249Bk, 241Am, and 231Pa with Proton Transfer Reactions NUCLEAR REACTIONS 248Cm(3He, d), 248Cm, 240Pu, 230Th(α, t), E=29 MeV; measured σ(Ed), σ(Et). 249Bk, 241Am, 231Pa deduced levels, J, S, β.
doi: 10.1103/PhysRevC.11.561
1975YA03 Phys.Rev. C11, 599 (1975) S.W.Yates, I.Ahmad, A.M.Friedman, F.J.Lynch, R.E.Holland Lifetimes of the 1/2+[631] → 5/2+[622] E2 Transitions in Some Actinide Nuclei RADIOACTIVITY 243,245Bk; measured Eγ, E(ce), γce(t), K X-ray-ce(t). 243,245Cm levels deduced T1/2, B(E2). NUCLEAR REACTIONS 238U(d, pγ), E=12 MeV; 242Pu(d, pγ), (d, tγ), E=16 MeV; measured γ(t). 239U, 241,243Pu levels deduced T1/2, B(E2).
doi: 10.1103/PhysRevC.11.599
1975YA11 Phys.Rev. C12, 442 (1975) S.W.Yates, R.R.Chasman, A.M.Friedman, I.Ahmad, K.Katori Particle-Phonon Interactions in 248Cf and 249Cf NUCLEAR REACTIONS 249Cf(d, d'), E=15 MeV; measured σ(Ed', θ). 249Cf(d, t), E=12 MeV; measured σ(Et, θ). 248,249Cf deduced levels, K, J, π.
doi: 10.1103/PhysRevC.12.442
1975YA13 Phys.Rev. C12, 795 (1975) S.W.Yates, A.M.Friedman, L.Ahmad Octupole States in 246Cm and 248Cm Populated by Inelastic Deuteron Scattering NUCLEAR REACTIONS 246,248Cm(d, d'), E=15 MeV; measured σ(Ed', θ). 246,248Cm(α, α'), E=29 MeV; measured σ(Eα', θ). 246,248Cm deduced levels, K, J, π, B(E3). Enriched targets.
doi: 10.1103/PhysRevC.12.795
1974FR01 Phys.Rev. C9, 760 (1974) A.M.Friedman, K.Katori, D.Albright, J.P.Schiffer Further Studies of Pairing Excitations in Actinide Nuclei: 233U, 237Pu, 235Np, 241Am, 224Ra, and 238Pu NUCLEAR REACTIONS 226Ra, 235U, 237Np, 239Pu, 243Am, 240Pu(p, t); measured σ(θ). 224Ra, 233U, 235Np, 237,238Pu, 241Am deduced levels, excitations, cross sections of pairing excited states.
doi: 10.1103/PhysRevC.9.760
1974PO08 Phys.Rev. C10, 803 (1974) F.T.Porter, I.Ahmad, M.S.Freedman, J.Milsted, A.M.Friedman Proton States, Anomalous Conversion, and K-Auger Spectra in 241Am from 241Cm (Electron Capture) and 245Bk (α) Decays RADIOACTIVITY 241Cm; measured E(ce), I(ce), Eγ, Iγ, T1/2, Xγ-coin, γγ-coin, deduced ICC, Qec, α-branching ratios, EC-branching ratios, log ft. 241Am, 237Pu; measured K, L Auger transitions, fluorescent yield, omegak. 245Bk; measured Eα, Iα, deduced α-branching ratios, hindrance factors. 241Am deduced levels, T1/2, J, π, γ-multipolarity, anomality.
doi: 10.1103/PhysRevC.10.803
1974YA04 Phys.Rev. C9, 1857 (1974) S.W.Yates, F.J.Lynch, R.E.Holland, I.Ahmad, A.M.Friedman Decay of the 22-μs Isomeric State of 38K NUCLEAR REACTIONS 24Mg(16O, pnγ), E=32-56 MeV; measured Eγ, Iγ, γ(t); 35Cl(α, nγ), E=10-16 MeV; measured σ(E, Eγ). 38K deduced levels, T1/2, J, π.
doi: 10.1103/PhysRevC.9.1857
1973FI17 Amer.Chem.Soc., 166th Nat.Mtg., NUCL-36 (1973) C.Fink, A.M.Friedman, L.Greenwood, K.Katori, G.Morrison, B.Zeidman A Study of Elastic and Inelastic Scattering of Lithium Ions from Spherical and Deformed Rare Earth Nuclei NUCLEAR REACTIONS 142,144,148,150Nd(6Li, 6Li), (6Li, 6Li'), (7Li, 7Li), (7Li, 7Li'), E=32 MeV; measured σ(θ), σ(E(6Li), θ), σ(E(7Li), θ). 142,144,148,150Nd levels deduced deformation.
1973FR01 Phys.Rev.Lett. 30, 102 (1973) Population of 0+ Excited States in 238Pu and 240Pu by Single-Neutron Transfer Reactions NUCLEAR REACTIONS 239Pu(d, p), (d, t), E=12 MeV; measured σ(Ep), σ(Et), Q. 238,240Pu deduced levels, J.
doi: 10.1103/PhysRevLett.30.102
1973KA38 Phys.Rev. C8, 2336 (1973) K.Katori, A.M.Friedman, J.R.Erskine Two-Neutron Quasiparticle States Observed in 236U with the (d, p) Reaction NUCLEAR REACTIONS 235U(d, p), E=12-16 MeV; measured σ(Ep, θ). 236U deduced levels, J, π.
doi: 10.1103/PhysRevC.8.2336
1972BR46 Phys.Rev. C6, 1374 (1972) T.H.Braid, R.R.Chasman, J.R.Erskine, A.M.Friedman Reaction-Spectroscopy Studies of the Actinide Elements. III. Levels in 241Pu and 243Pu NUCLEAR REACTIONS 242Pu(d, p), E=12 MeV; 240Pu(d, p), E=12 MeV; 242Pu(d, t), E=12 MeV; 241Pu(d, d'), E=12 MeV; measured Q, σ(Ep), σ(Et), σ(Ed'). 240Pu(n, γ), E=thermal; measured Eγ, Iγ. 241Pu, 243Pu deduced levels, J, Nilsson assignments.
doi: 10.1103/PhysRevC.6.1374
1972FR14 Phys.Rev. C6, 2219 (1972) A.M.Friedman, R.H.Siemssen, J.G.Cuninghame Measurements of Nuclear Radii by Heavy-Ion Scattering NUCLEAR REACTIONS 144,146Nd, 152,154Sm, 208Pb, 209Bi(12C, 12C), E=118 MeV; 144,146,148Nd, 152,154Sm, 206,208Pb(16O, 16O), E=130 MeV; measured σ(θ); deduced phase shift parameters.
doi: 10.1103/PhysRevC.6.2219
1972MA15 Phys.Rev. C5, 1380 (1972) J.V.Maher, J.R.Erskine, A.M.Friedman, R.H.Siemssen, J.P.Schiffer Population of 0+ States in Actinide and A ≈ 190 Nuclides by the (p, t) Reaction NUCLEAR REACTIONS 230,232Th, 234,236,238U, 242,244Pu, 248Cm, 182,184,186W, 196Pt(p, t), E=17 MeV; measured σ(Et, θ), Q. 228,230Th, 232,234,236U, 246Cm, 240,242Pu, 180,182,184W, 194Pt deduced levels.
doi: 10.1103/PhysRevC.5.1380
1971BR27 Phys.Rev. C4, 247 (1971) T.H.Braid, R.R.Chasman, J.R.Erskine, A.M.Friedman (d, p) and (d, t) Studies of the Actinide Elements. II. 243Cm, 245Cm, 247Cm, and 249Cm NUCLEAR REACTIONS 244,246,248Cm(d, p), (d, t), E=12, 16 MeV; measured σ(Ep), σ(Et). 243,245,247,249Cm deduced levels, J, Nilsson assignments, deformation parameters.
doi: 10.1103/PhysRevC.4.247
1971FI01 Nucl.Phys. A160, 460 (1971) P.R.Fields, I.Ahmad, A.M.Friedman, J.Lerner, D.N.Metta Alpha Decay of 247Cm RADIOACTIVITY 247Cm[from 246Cm(n, γ)]; measured T1/2, Eα, Iα, Eγ, Iγ, αγ-coin; deduced hindrance factors. 243Pu deduced levels, ICC, γ-multipolarity.J, π. Mass-separated 247Cm.
doi: 10.1016/0375-9474(71)90089-3
1970BE44 Inorg.Nucl.Chem.Lett. 6, 747 (1970); ORNL-4581, p.36 (1970) C.E.Bemis, Jr., R.J.Silva, J.E.Bigelow, A.M.Friedman Search for a Long-Lived Spontaneous Fission Isomer of 241Pu NUCLEAR REACTIONS 240Pu(n, γ), E=thermal, > 1 MeV; 242Pu(n, 2n), E > 6.2 MeV; 238U(α, n), E=40 MeV; measured σ. 241Pu deduced no 0.3-yr SF-isomer.
doi: 10.1016/0020-1650(70)80091-5
1970BR01 Phys.Rev. C1, 275 (1970) T.H.Braid, R.R.Chasman, J.R.Erskine, A.M.Friedman (d, p) and (d, t) Reaction Studies of the Actinide Elements. I. U235 NUCLEAR REACTIONS 234U(d, p), 236U(d, t), E=12 MeV; measured σ(Ep), σ(Et), Q. 235U deduced levels, S, rotational band assignments.
doi: 10.1103/PhysRevC.1.275
1970MA29 Phys.Rev.Lett. 25, 302 (1970) J.V.Maher, J.R.Erskine, A.M.Friedman, J.P.Schiffer, R.H.Siemssen Unexpected Strong Pair Correlations in Excited 0+ States of Actinide Nuclei NUCLEAR REACTIONS 230Th, 234,236,238U, 242,244Pu(p, t), E=17 MeV; measured σ(Et, θ). 228Th, 232,234,236U, 240,242Pu deduced levels, J, π.
doi: 10.1103/PhysRevLett.25.302
1969FR01 Nucl.Phys. A127, 33 (1969) A.M.Friedman, I.Ahmad, J.Milsted, D.W.Engelkemeir Energy Levels of 243Am RADIOACTIVITY 243Pu [from 242Pu (n, γ)]; measured Eγ, Iγ, I(ce), γγ-, γce-coin, βγ-delay. 247Bk [from 244Cm(α, p)]; measured Eα, Iα. 243Am deduced levels, J, π, T1/2. Mass-separated 243Pu.
doi: 10.1016/0375-9474(69)90764-7
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
1968AH01 Nucl.Phys. A119, 27 (1968) I.Ahmad, A.M.Friedman, J.P.Unik Energy Levels of 237U RADIOACTIVITY 241Pu; measured Eα, Iα, Eγ, Iγ, γγ-, γα- αγ-coin, αγ-delay, α/β ratio. 237U deduced levels, J, π, T1/2.
doi: 10.1016/0375-9474(68)90803-8
1968FR09 Priv.Comm. (June 1968) A.M.Friedman, J.R.Erskine, R.R.Chapman NUCLEAR STRUCTURE 249Cm, 247Cm, 245Cm, 243Cm; measured not abstracted; deduced nuclear properties.
1967AH02 Phys.Rev. 164, 1537 (1967) I.Ahmad, A.M.Friedman, R.F.Barnes, R.K.Sjoblom, J.Milsted, P.R.Fields Decay of Fm253 NUCLEAR STRUCTURE 253Fm; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.164.1537
1967ER02 Proc.Intern.Conf.Atomic Masses, 3rd, Winnipeg, Canada, R.C.Barber, Ed., Univ.Manitoba Press, p.622 (1967) J.R.Erskine, A.M.Friedman, T.H.Braid, R.R.Chasman Nuclear Q-Value Measurements on a Series of Actinide Nuclei NUCLEAR REACTIONS 230,232Th, 234,236,238U, 240,242Pu, 244,246,248Cm(d, p), E = 12 MeV; 230,232Th, 234,236,238U, 242Pu, 244,246,248Cm(d, t), E = 12 MeV; measured Q.
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
1967FI10 Arkiv Fysik 36, 471 (1967) R.W.Fink, T.H.Braid, A.W.Friedman Delayed Protons Following He3 Reactions with Oxygen, Silicon, and Sulfur Targets
1967FR09 Priv.Comm. (August 1967) A.M.Friedman, J.R.Erskine, R.R.Chapman NUCLEAR STRUCTURE 247Cm, 245Cm; measured not abstracted; deduced nuclear properties.
1966FI07 Nature 212, 131 (1966) P.R.Fields, A.M.Friedman, J.Milsted, J.Lerner, C.M.Stevens, D.Metta Decay Properties of Plutonium-244 and Comments on its Existence in Nature NUCLEAR STRUCTURE 244Pu; measured not abstracted; deduced nuclear properties.
doi: 10.1038/212131a0
1966FR03 Phys.Letters 21, 179 (1966) Alpha Decay of 245Cm NUCLEAR STRUCTURE 245Cm; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(66)90306-4
1966FR04 Priv.Comm. (July 1966) NUCLEAR STRUCTURE 245Cm, 243Cm, 241Pu, 239U, 247Cm, 237U, 235U, 235Th, 233U, 231Th, 229Th; measured not abstracted; deduced nuclear properties.
1966FR11 Radiochim.Acta 5, 192 (1966) A.M.Friedman, J.Milsted, D.Metta, D.Henderson, J.Lerner, A.L.Harkness, D.J.Rokop Alpha Decay Half Lives of 148Gd, 150Gd, and 146Sm NUCLEAR STRUCTURE 146Sm, 150Gd, 148Gd; measured not abstracted; deduced nuclear properties.
1966HO01 Phys.Rev. 148, 1192 (1966); See keynumber 1966RG01 R.W.Hoff, C.P.Bailey, G.W.Barton, G.H.Coleman, M.S.Coops, J.E.Evans, B.A.Hannon, W.N.Hayes, R.A.Heckman, E.K.Hulet, R.W.Lougheed, R.J.Morrow, R.S.Newbury, B.J.Qualheim, R.Quong, E.H.Stearns, H.D.Wilson, J.P.Balagna, J.W.Barnes, G.A.Cowan, W.R.Daniels, B.J.Dropesky, G.P.Ford, J.S.Gilmore, S.B.Helmick, D.C.Hoffman, J.D.Knight, G.W.Knobeloch, C.J.Orth, T.T.Shull, H.L.Smith, W.G.Warren, K.Wolfsberg, F.Asaro, J.Burnett, B.B.Cunningham, S.M.Fried, J.T.Haley, A.Ghiorso, J.Green, R.Latimer, F.T.McCarthy, H.V.Michel, M.C.Michel, D.F.Mosier, T.C.Parsons, I.Perlman, J.E.Rees, J.C.Wallmann, R.F.Barnes, L.J.Basile, H.Diamond, P.R.Fields, A.M.Friedman, E.P.Horowitz, J.K.Lerner, D.N.Metta, J.Milsted, R.K.Sjoblom, C.M.Stevens Nuclear Decay Properties of Heavy Nuclides Produced in Thermonuclear Explosions - Par and Barbel Events RADIOACTIVITY 251,252,253,254Cf, 255Es, 257,258Fm(α), 250Cm(SF), 251Bk, 252Cm(β-) [from U(n, F), U(n, X), E ∼ 2 MeV]; measured decay products, Eα, Iα; deduced α-particles energies, α-decay branchings, T1/2. Two low-yield thermonuclear explosions, the Par and Barbel events, chemical separation of products. NUCLEAR REACTIONS Cm(n, X)249Cf/250Cf/252Cf/252Cf/253Cf/254Cf/253Es/254Es/255Es, E thermal; measured reaction products, Eα, Iα, Eβ, Iβ; deduced isotopic abundances. Cm irradions, reactor.
doi: 10.1103/PhysRev.148.1192
1965BR03 Bull.Am.Phys.Soc. 10, No.1, 120, KC13 (1965) T.H.Braid, A.M.Friedman, R.W.Fink Delayed Proton Emission from Isotopes of Neon, Sulfur, and Argon NUCLEAR STRUCTURE 17Ne, 28S; measured not abstracted; deduced nuclear properties.
1965BR22 Phys.Letters 18, 149 (1965) T.H.Braid, R.R.Chasman, J.R.Erskine, A.M.Friedman Energy Level Structure of 231Th, 235U, 237U, 241Pu and 243Pu as Observed at High Resolution with (d, p) Reactions NUCLEAR STRUCTURE 237U, 235U, 231Th, 241Pu, 243Pu; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(65)90695-5
1965ER01 Bull.Am.Phys.Soc. 10, No.1, 40, CD13 (1965) J.R.Erskine, A.M.Friedman, T.H.Braid Energy Level Structure of U237 as Observed with the U236(d, p)U237 Reaction NUCLEAR STRUCTURE 237U; measured not abstracted; deduced nuclear properties.
1965FR11 Bull.Am.Phys.Soc. 10, No.4, 540, KA13 (1965) A.M.Friedman, J.R.Erskine, T.H.Braid Measurement of the Quadrupole Moments and Deformations of Th230, U234, U236, Pu240, and Pu242 by Inelastic Scattering of Deuterons NUCLEAR STRUCTURE 240Pu, 242Pu, 234U, 236U, 230Th; measured not abstracted; deduced nuclear properties.
1965FR13 Bull.Am.Phys.Soc. 10, No.8, 1099, CD3 (1965); Oral Report Alpha Decay of Cm245 NUCLEAR STRUCTURE 245Cm; measured not abstracted; deduced nuclear properties.
1965ME14 Bull.Am.Phys.Soc. 10, No.8, 1099, CD2 (1965) D.Metta, A.M.Friedman, P.Fields, J.Milsted, J.Lerner, C.Stevens Decay Properties of Pu244 NUCLEAR STRUCTURE 244Pu; measured not abstracted; deduced nuclear properties.
1965MI08 Nucl.Phys. 71, 299 (1965) J.Milsted, A.M.Friedman, C.M.Stevens The Alpha Half-Life of Berkelium-247; A New Long-Lived Isomer of Berkelium-248 RADIOACTIVITY 247Bk [from 244Cm(α, n)247Cf(capture), 244Cm(α, p)]; measured T1/2(α). 248mBk [from 246Cm(α, pn)]; measured lower limit T1/2(α), T1/2(β).
doi: 10.1016/0029-5582(65)90719-4
1963FI08 Phys.Rev. 131, 1249 (1963) P.R.Fields, A.M.Friedman, J.Lerner, D.Metta, R.Sjoblom Possible Existence of Curium in Nature II NUCLEAR STRUCTURE 247Cm; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.131.1249
1963FR02 Phys.Rev. 129, 1752 (1963) A.M.Friedman, J.Milsted, O.Skilbreid Properties of Eu145, Eu146, Eu147, Gd146, and Gd147 NUCLEAR STRUCTURE 147Gd, 146Eu, 146Gd, 147Eu, 145Eu; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.129.1752
1963FR04 Phys.Rev. 131, 772 (1963) Alpha Decay of Cf246 NUCLEAR STRUCTURE 246Cf; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.131.772
1963FR06 Bull.Am.Phys.Soc. 8, No.7, 525, I10 (1963) A.M.Friedman, J.Milsted, A.L.Harkness α Decay Half-Lives of Gd148, Gd150, and Sm146 NUCLEAR STRUCTURE 146Sm, 150Gd, 148Gd; measured not abstracted; deduced nuclear properties.
1963FR15 Phys.Rev. 131, 1203 (1963) A.M.Friedman, J.W.Meadows, A.B.Smith, P.R.Fields, J.Milsted, J.F.Whalen Fission fragment kinetic energies of Cf246, Cf248, and Cf254 RADIOACTIVITY 246,248,254Cf(SF); measured products. Data were imported from EXFOR entry 13654.
doi: 10.1103/PhysRev.131.1203
1962FR01 Bull.Am.Phys.Soc. 7, No.4, 352, XA7 (1962) Properties of Gd146, Gd147, Gd148, Eu145, Eu146, Eu147 NUCLEAR STRUCTURE 148Gd, 147Gd, 146Eu, 146Gd, 145Eu; measured not abstracted; deduced nuclear properties.
1962MI01 Bull.Am.Phys.Soc. 7, No.4, 353, XA14 (1962) α Decay of Bk249 NUCLEAR STRUCTURE 249Bk; measured not abstracted; deduced nuclear properties.
1958CO72 Phys.Rev. 112, 960 (1958) S.Cox, P.Fields, A.Friedman, R.Sjoblom, A.Smith Delayed Neutrons from the Spontaneous Fission of Cf252
doi: 10.1103/PhysRev.112.960
1958SM99 Phys.Rev. 111, 1633 (1958) A.Smith, P.Fields, A.Friedman, R.Sjoblom Thermal-Neutron-Induced Fission of Th229 NUCLEAR REACTIONS 229Th(n, f), E=0.0253 eV; measured products. Data were imported from EXFOR entry 13653.
doi: 10.1103/PhysRev.111.1633
1957FI53 Phys.Rev. 107, 1460 (1957) P.R.Fields, A.M.Friedman, J.Milsted, H.Atterling, W.Forsling, L.W.Holm, B.Astrom Production of the New Element 102 NUCLEAR REACTIONS 244Cm(13C, 4n), (13C, 6n), E=65-100 MeV; measured reaction products, Eα, Iα. 251,253No; deduced α-particle energies, decay curves, T1/2. The 225-cm cyclotron.
doi: 10.1103/physrev.107.1460
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
1956MA32 Phys.Rev. 102, 1097 (1956) L.B.Magnusson, A.M.Friedman, D.Engelkemeir, P.R.Fields, F.Wagner, Jr. Properties of Bk245
doi: 10.1103/PhysRev.102.1097
1956SM97 Phys.Rev. 104, 699 (1956) A.B.Smith, P.R.Fields, A.M.Friedman Prompt Gamma Rays Accompanying the Spontaneous Fission of Cf252 RADIOACTIVITY 252Cf(SF); measured decay products, Eγ, Iγ; deduced prompt photon energy spectra, fission yields.
doi: 10.1103/PhysRev.104.699
1956SM98 Phys.Rev. 102, 813 (1956) A.B.Smith, A.M.Friedman, P.R.Fields Spontaneous fission kinetics of Cf252 RADIOACTIVITY 252Cf(SF); measured products. Data were imported from EXFOR entry 13655.
doi: 10.1103/PhysRev.102.813
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
1955FI37 J.Inorg.Nuclear Chem. 1, 262 (1955) P.R.Fields, M.H.Studier, A.M.Friedman, H.Diamond, R.Sjoblom, P.D.Sellers Production of Pu245 and Am245 by Neutron Irradiation of Pu244
doi: 10.1016/0022-1902(55)80031-0
1954DI11 Phys.Rev. 94, 1083 (1954) H.Diamond, L.B.Magnusson, J.F.Mech, C.M.Stevens, A.M.Friedman, M.H.Studier, P.R.Fields, J.R.Huizenga Identification of Californium Isotopes 249, 250, 251, and 252 from Pile-Irradiated Plutonium
doi: 10.1103/PhysRev.94.1083
1954FI14 Phys.Rev. 94, 209 (1954) P.R.Fields, M.H.Studier, J.F.Mech, H.Diamond, A.M.Friedman, L.B.Magnusson, J.R.Huizenga Additional Properties of Isotopes of Elements 99 and 100
doi: 10.1103/PhysRev.94.209
1954FR19 Phys.Rev. 95, 1501 (1954) A.M.Friedman, A.L.Harkness, P.R.Fields, M.H.Studier, J.R.Huizenga Alpha Half-Lives of Cm244, Cm245, and Cm246
doi: 10.1103/PhysRev.95.1501
1954MA90 Phys.Rev. 96, 157 (1954) L.B.Magnusson, M.H.Studier, P.R.Fields, C.M.Stevens, J.F.Mech, A.M.Friedman, H.Diamond, J.R.Huizenga Berkelium and Californium Isotopes Produced in Neutron Irradiation of Plutonium
doi: 10.1103/PhysRev.96.1576
1954MA98 Phys.Rev. 96, 1576 (1954) L.B.Magnusson, M.H.Studier, P.R.Fields, C.M.Stevens, J.F.Mech, A.M.Friedman, H.Diamond, J.R.Huizenga Berkelium and californium isotopes produced in neutron irradiation of plutonium NUCLEAR REACTIONS 249Bk(n, γ), 250Cf(n, γ), 251Cf(n, γ), 252Cf(n, γ), E=0.0253 eV; measured products, 250Bk, Eγ, Iγ; deduced σ, σ(E). Data were imported from EXFOR entry 12568.
doi: 10.1103/PhysRev.96.1576
1954ST06 Phys.Rev. 93, 1428 (1954) M.H.Studier, P.R.Fields, H.Diamond, J.F.Mech, A.M.Friedman, P.A.Sellers, G.Pyle, C.M.Stevens, L.B.Magnusson, J.R.Huizenga Elements 99 and 100 from Pile-Irradiated Plutonium
doi: 10.1103/PhysRev.93.1428
1954ST33 Phys.Rev. 94, 974 (1954) C.M.Stevens, M.H.Studier, P.R.Fields, J.F.Mech, P.A.Sellers, A.M.Friedman, H.Diamond, J.R.Huizenga Curium Isotopes 246 and 247 from Pile-Irradiated Plutonium
doi: 10.1103/PhysRev.94.974
1954ST98 Phys.Rev. 93, 1433 (1954) M.H.Studier, P.R.Fields, P.H.Sellers, A.M.Friedman, C.M.Stevens, J.F.Mech, H.Diamond, J.Sedlet, J.R.Huizenga Plutonium-244 from Pile-Irradiated Plutonium NUCLEAR REACTIONS 239,240,241,242,243Pu, 243Am(n, γ), E thermal; measured reaction products. 244Pu; deduced yields, σ. RADIOACTIVITY 244Am(EC), (β-), 243Pu(β-); measured decay products; deduced T1/2.
doi: 10.1103/PhysRev.93.1433
Back to query form Note: The following list of authors and aliases matches the search parameter A.Friedman: , A.M.FRIEDMAN, A.W.FRIEDMAN |