NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = L.Meyer-Schutzmeister Found 65 matches. 1982HA36 Phys.Rev. C26, 456 (1982) G.Hardie, S.A.Gronemeyer, L.Meyer-Schutzmeister, A.J.Elwyn γ Decay of States in 47Cr NUCLEAR REACTIONS 46Ti(3He, 2n), E=22 MeV; 40Ca(12C, nα), E=38 MeV; measured γγ-coin, γγ(t). 47Cr deduced levels, J, π, Coulomb displacement energy.
doi: 10.1103/PhysRevC.26.456
1980GR04 Phys.Rev. C21, 1290 (1980) S.A.Gronemeyer, L.Meyer-Schutzmeister, A.J.Elwyn, G.Hardie Gamma-Ray Studies in 45V NUCLEAR REACTIONS 40Ca(7Li, 2n), E=14, 15, 16 MeV; 40Ca(6Li, n), E=10, 13.5 MeV; measured Eγ, Iγ, γ(t), nγ-, γγ-coin, γγ(t), T1/2. 45V deduced levels, γ-branching, J, π, T1/2.
doi: 10.1103/PhysRevC.21.1290
1980RA15 Phys.Rev. C22, 2409 (1980) K.Raghunathan, L.L.Rutledge, R.E.Segel, L.Meyer-Schutzmeister Alpha Particle Capture Through the Giant Electric Resonances in 90Zr NUCLEAR REACTIONS 86Sr(α, γ), E=9-12.5 MeV; measured Eγ, σ(E, θ); deduced reaction mechanism. 86Sr level deduced σ(γ, α). 90Zr deduced giant E1, E2 contributions.
doi: 10.1103/PhysRevC.22.2409
1979EL10 Phys.Rev. C20, 1984 (1979) A.J.Elwyn, R.E.Holland, C.N.Davids, L.Meyer-Schutzmeister, F.P.Mooring, W.Ray, Jr. Cross Sections for the 6Li(p, 3He)4He Reaction at Energies between 0.1 And 3.0 MeV NUCLEAR REACTIONS 6Li(p, 3He), E=0.14-3 MeV; measured σ(E, θ); calculated reaction rate parameter, astrophysical S factor. Enriched target.
doi: 10.1103/PhysRevC.20.1984
1979HO04 Phys.Rev. C19, 592 (1979) R.E.Holland, A.J.Elwyn, C.N.Davids, F.J.Lynch, L.Meyer-Schutzmeister, J.E.Monahan, F.P.Mooring, W.Ray, Jr. Absolute Cross Sections for Three-Body Breakup Reactions 6Li(d, n 3He)4He and 6Li(d, p 3He)4He NUCLEAR REACTIONS 6Li(d, pt), E=0.1-0.8 MeV; 6Li(d, n3He), E=0.2-0.8 MeV; measured σ(Ed, Ep, θ), σ(Ed, En, θ), total σ. Comparison with direct breakup, sequential decay.
doi: 10.1103/PhysRevC.19.592
1978JA19 Phys.Rev. C18, 2656 (1978) H.E.Jackson, S.B.Kaufman, D.G.Kovar, L.Meyer-Schutzmeister, K.E.Rehm, J.P.Schiffer, S.L.Tabor, S.E.Vigdor, T.P.Wangler, L.L.Rutledge, Jr., R.E.Segel, R.L.Burman, P.A.M.Gram, R.P.Redwine, M.A.Yates-Williams Gamma-Ray Study of Pion-Induced Reactions on the Nickel Isotopes NUCLEAR REACTIONS 58,60,62,64Ni(π+, Xγ), E=100, 160, 220 MeV; measured prompt, β-delayed γ-spectra. 57,58,59,60,61,62,64Ni, 57,59,60,61Co, 54,55,56,58Fe, 53,55Mn, 50,51,52Cr, 49,51V, 45,46,47,48Ti, 42,44Ca deduced production σ, systematics. Enriched targets.
doi: 10.1103/PhysRevC.18.2656
1978ME02 Phys.Rev. C17, 56 (1978) L.Meyer-Schutzmeister, R.E.Segel, K.Raghunathan, P.T.Debevec, W.R.Wharton, L.L.Rutledge, T.R.Ophel Giant Electric Resonances in 58Ni Studied by Alpha Particle Capture NUCLEAR REACTIONS 54Fe(α, γ), E=7.6-12.8 MeV; measured σ(E, Eγ). 58Ni giant resonances deduced E1, E2 strength.
doi: 10.1103/PhysRevC.17.56
1978ME09 Phys.Rev. C17, 1299 (1978) L.Meyer-Schutzmeister, A.J.Elwyn, K.E.Rehm, G.Hardie Lifetime and γ Decay of the Isomeric 19/2- State in 43Ti NUCLEAR REACTIONS 40Ca(α, nγ), E=20 MeV; measured Eγ, Iγ, nγ(t), γγ(t). 43Ti deduced levels, T1/2, B(E2).
doi: 10.1103/PhysRevC.17.1299
1978ME15 Phys.Rev. C18, 1148 (1978) L.Meyer-Schutzmeister, A.J.Elwyn, S.A.Gronemeyer, G.Hardie, R.E.Holland, K.E.Rehm Positive-Parity States in 43Ti NUCLEAR REACTIONS 40Ca(α, nγ), E=20 MeV; measured Eγ, Iγ, γ(t), nγ(t), γγ(t). 43Ti deduced levels, J, π, T1/2, B(E2).
doi: 10.1103/PhysRevC.18.1148
1977EL09 Phys.Rev. C16, 1744 (1977) A.J.Elwyn, R.E.Holland, C.N.Davids, L.Meyer-Schutzmeister, J.E.Monahan, F.P.Mooring, W.Ray, Jr. Absolute Cross Sections for Deuteron-Induced Reactions on 6Li at Energies below 1 MeV NUCLEAR REACTIONS 6Li(d, p), (d, α), E=0.1-1.0 MeV; 6Li(d, n), E=0.2-0.9 MeV; measured σ(E, θ). Enriched target.
doi: 10.1103/PhysRevC.16.1744
1977JA10 Phys.Rev. C16, 730 (1977) H.E.Jackson, S.B.Kaufman, L.Meyer-Schutzmeister, J.P.Schiffer, S.L.Tabor, S.E.Vigdor, J.N.Worthington, L.L.Rutledge, Jr., R.E.Segal, R.L.Burman, P.A.M.Gram, R.P.Redwine, M.A.Yates Energetic Charged Particle Yields Induced by Pions on Complex Nuclei NUCLEAR REACTIONS 27Al, 62Ni, 181Ta(π+, p), (π+, d), (π-, p), (π-, d), E=100, 220 MeV; measured σ for Ep=50-200 MeV, Ed=80-200 MeV.
doi: 10.1103/PhysRevC.16.730
1976HA14 Phys.Rev. C13, 1874 (1976) G.Hardie, L.Meyer-Schutzmeister, D.Gloeckner, T.H.Braid 45Sc(α, d)47Ti Reaction NUCLEAR REACTIONS 45Sc(α, d), E=25 MeV; measured σ(θ). 47Ti deduced levels, J, π. Shell model, DWBA analyses.
doi: 10.1103/PhysRevC.13.1874
1976ME15 Phys.Rev. C14, 109 (1976) L.Meyer-Schutzmeister, G.Hardie, T.Sjoreen Gamma Decay of High-Spin States in 47Ti NUCLEAR REACTIONS 45Sc(α, npγ), E=23 MeV; measured σ(Eγ), γγ-coin, DSA. 47Ti deduced levels, J, π, T1/2, λ. Shell model calculations.
doi: 10.1103/PhysRevC.14.109
1976SE04 Phys.Rev. C13, 1566 (1976) R.E.Segel, L.R.Greenwood, P.Debevec, H.E.Jackson, D.G.Kovar, L.Meyer-Schutzmeister, J.E.Monahan, F.J.D.Serduke, T.P.Wangler, W.R.Wharton, B.Zeidman Prompt Gamma Rays from Nuclear Reactions Induced by 380-MeV π- NUCLEAR REACTIONS S, Ar, Ca, V, 60Ni, As(π-, X), E=380 MeV; measured σ.
doi: 10.1103/PhysRevC.13.1566
1975JA13 Phys.Rev.Lett. 35, 641 (1975) H.E.Jackson, D.G.Kovar, L.Meyer-Schutzmeister, R.E.Segel, J.P.Schiffer, S.Vigdor, T.P.Wangler, R.L.Burman, D.M.Drake, P.A.M.Gram, R.P.Redwine, V.G.Lind, E.N.Hatch, O.H.Otteson, R.E.McAdams, B.C.Cook, R.B.Clark Systematics of Pion and Proton Interactions with Ni Nuclides NUCLEAR REACTIONS 58,60Ni(π+, X), (π-, X), E=220 MeV; 58,60Ni(p, X), E=200 MeV; 58Ni(π+, X), E=100 MeV; measured σ(fragment) from γ-spectra.
doi: 10.1103/PhysRevLett.35.641
1975JA15 Phys.Rev.Lett. 35, 1170 (1975) H.E.Jackson, D.G.Kovar, L.Meyer-Schutzmeister, S.E.Vigdor, T.P.Wangler, R.E.Segel, J.P.Schiffer, R.L.Burman, P.A.M.Gram, D.M.Drake, V.G.Lind, E.N.Hatch, O.H.Otteson, R.E.McAdams, B.C.Cook, R.B.Clark Absolute Cross Sections for Production of Prompt Nuclear γ Rays by Fast Pions NUCLEAR REACTIONS 27Al(π+, X), E=100 MeV; 51V, 40Ca(π-, X), E=220 MeV; 60Ni(π-, X), (π+, X), E=380 MeV; measured σ(Eγ).
doi: 10.1103/PhysRevLett.35.1170
1975MA13 Phys.Rev.C11, 1141 (1975) J.C.Manthuruthil, C.P.Poirier, L.Meyer-Schutzmeister 48Ti(3He, t)48V Reaction NUCLEAR REACTIONS 48Ti(3He, t), E=25 MeV; measured σ(Et, θ). 48V deduced levels, L, J, π.
doi: 10.1103/PhysRevC.11.1141
1974HA55 Phys.Rev. C10, 1829 (1974) G.Hardie, D.Gloeckner, L.Meyer-Schutzmeister, T.H.Braid Systematics of the (3He, p) Reaction on Some f-Shell Nuclei NUCLEAR REACTIONS 43Ca, 45Sc, 46,48,50Ti(3He, p), E=17 MeV; measured σ(Ep, θ). 45Sc deduced levels, L, J, π.
doi: 10.1103/PhysRevC.10.1829
1974MA08 Phys.Rev. C9, 1440 (1974) J.V.Maher, L.Meyer-Schutzmeister, E.L.Sprenkel-Segel, D.von Ehrenstein, R.J.Nemanich, G.C.Kiang, J.F.Tonn, R.E.Segel Radiative Proton Capture Study of the Giant Dipole Resonance in 55,57Co NUCLEAR REACTIONS 54Fe(p, γ), E=4.7-16.8 MeV; 56Fe(p, γ), E=4.7-17.4 MeV; measured σ(E, θ). 55,57Co deduced resonance.
doi: 10.1103/PhysRevC.9.1440
1973HA27 Phys.Rev. C7, 2466 (1973) G.Hardie, T.H.Braid, L.Meyer-Schutzmeister, J.W.Smith Study of 58Co with the (3He, p) and (3He, pγ) Reactions on 56Fe NUCLEAR REACTIONS 56Fe(3He, pγ), E=13 MeV; measured σ(Ep, θ), pγ-coin, Eγ, Iγ. 58Co deduced levels, J, π, L.
doi: 10.1103/PhysRevC.7.2466
1973JA15 Phys.Rev.Lett. 31, 1353 (1973) H.E.Jackson, L.Meyer-Schutzmeister, T.P.Wangler, R.P.Redwine, R.E.Segel, J.Tonn, J.P.Schiffer Interaction of Fast Negative Pions with 60Ni NUCLEAR REACTIONS 28Si, 60Ni(π-, Xγ), E=500 MeV; measured Eγ, Iγ.
doi: 10.1103/PhysRevLett.31.1353
1973ME04 Nucl.Phys. A199, 593 (1973) L.Meyer-Schutzmeister, J.W.Smith, G.Hardie, H.Siefken, K.T.Knopfle, M.Rogge, C.Mayer-Boricke Study of 47Ti with the 45Sc(3He, p)47Ti and 45Sc(3He, pγ)47Ti Reactions NUCLEAR REACTIONS 45Sc(3He, pγ), E=17 MeV; measured σ(θ), pγ-coin. 47Ti deduced levels, J, π, S, IAS, antianalog states.
doi: 10.1016/0375-9474(73)90600-3
1973SM02 Phys.Rev. C7, 1099 (1973) J.W.Smith, L.Meyer-Schutzmeister, T.H.Braid, P.P.Singh, G.Hardie Study of the 50V Nucleus with the (3He, d), (3He, p), and (3He, pγ) Reactions NUCLEAR REACTIONS 48Ti(3He, pγ), E=13 MeV; measured σ(Ep, Eγ), pγ-coin. 50V deduced levels, transitions. 48Ti(3He, pγ), 49Ti(3He, d), 51V(3He, α), E=22 MeV; measured σ(Ep, θ), σ(Ed, θ), σ(Eα, θ). Deduced L, S. 50V deduced levels, J, π.
doi: 10.1103/PhysRevC.7.1099
1973SM12 Phys.Rev. C8, 2232 (1973) J.W.Smith, L.Meyer-Schutzmeister, G.Hardie, P.P.Singh Study of 1+ States in 48V NUCLEAR REACTIONS 46Ti(3He, pγ), E=17 MeV; measured σ(Ep, θ), pγ-coin. 48V deduced levels, J, π.
doi: 10.1103/PhysRevC.8.2232
1972GR25 Phys.Rev. C6, 805 (1972) K.O.Groeneveld, L.Meyer-Schutzmeister, A.Richter, U.Strohbusch Backward-Angle Elastic Scattering of 16O on 40Ca and 48Ca NUCLEAR REACTIONS 40,48Ca(16O, 16O), E=25-45 MeV; measured σ(E;θ); deduced optical model parameters.
doi: 10.1103/PhysRevC.6.805
1972HA27 Phys.Rev. C5, 1600 (1972) G.Hardie, T.H.Braid, L.Meyer-Schutzmeister, J.W.Smith Study of 57Co with the 56Fe(3He, d) and 56Fe(3He, dγ) Reactions NUCLEAR REACTIONS 56Fe(3He, d), (3He, dγ), E=22 MeV; measured σ(Ed, θ(d), Eγ). 57Co deduced levels, J, π, L(p).
doi: 10.1103/PhysRevC.5.1600
1971KN04 Phys.Rev. C4, 818 (1971) K.T.Knopfle, M.Rogge, C.Mayer-Boricke, D.S.Gemmell, L.Meyer-Schutzmeister, H.Ohnuma, N.G.Puttaswamy 31P(3He, pγ)33S and 39K(3He, pγ)41Ca Reactions and the γ Decay of Analog States in 33S and 41Ca NUCLEAR REACTIONS 31P, 39K(3He, pγ), E=12, 13 MeV; measured σ(Ep, Eγ, θ(p)). 33S, 41Ca deduced levels, J, π, isobaric analogs, γ-branching.
doi: 10.1103/PhysRevC.4.818
1971ME08 Phys.Rev.Lett. 27, 869 (1971) L.Meyer-Schutzmeister, D.S.Gemmell Angular Distributions for T(np)=1 and T(np)=0 Transfers in (3He, p) Reactions NUCLEAR REACTIONS 27Al, 31P, 39K(3He, p), E not given; analyzed σ(θ); deduced L(np), T(np) transitions.
doi: 10.1103/PhysRevLett.27.869
1971VO04 Phys.Rev.Lett. 27, 107 (1971) D.von Ehrenstein, L.Meyer-Schutzmeister, J.E.Monahan, A.Richter, J.C.Stoltzfus Isospin Nonconservation in the Reaction 12C(d, α2)10B(1.74, T = 1) NUCLEAR REACTIONS 12C(d, α), E = 14-17 MeV; measured σ(Eα, θ); deduced non-compound-nucleus contribution.
doi: 10.1103/PhysRevLett.27.107
1970OH03 Nucl.Phys. A149, 141 (1970) H.Ohnuma, F.T.Kuchnir, D.S.Gemmell, R.E.Holland, L.Meyer-Schutzmeister, N.G.Puttaswamy Study of the Excited States in 30Si by Means of the 30Si(α, α'γ)30Si Reaction NUCLEAR REACTIONS 30Si(α, α'γ), E=13, 16 MeV; measured σ(Eα', Eγ, θ). 30Si levels deduced J, π. Enriched target.
doi: 10.1016/0375-9474(70)90384-2
1970RI14 Phys.Rev. C2, 1361 (1970) A.Richter, L.Meyer-Schutzmeister, J.C.Stoltzfus, D.von Ehrenstein Isospin Nonconservation in the 28Si(d, α1)26Al0. 23, T=1 Reaction NUCLEAR REACTIONS 28Si(d, α), E=12-17 MeV; measured θ(E;Eα, θ(α));deduced reaction mechanism.
doi: 10.1103/PhysRevC.2.1361
1969HA40 Nucl.Phys. A134, 673 (1969) G.Hardie, R.E.Holland, L.Meyer-Schutzmeister, F.T.Kuchnir, H.Ohnuma Energy Levels in 33P NUCLEAR REACTIONS 30Si(α, pγ), E = 16.5 MeV; measured σ(Ep, θ), σ(Ep, Eγ, θ(pγ)). 33P deduced levels, J, π, γ-branching. Enriched target.
doi: 10.1016/0375-9474(69)90030-X
1969ME19 Phys.Rev. 187, 1210 (1969) L.Meyer-Schutzmeister, D.S.Gemmell, R.E.Holland, F.T.Kuchnir, H.Ohnuma, N.G.Puttaswamy Study of the Al27(He3, p)Si29 and Al27(He3, pγ)Si29 Reactions NUCLEAR REACTIONS 27Al(3He, pγ), E=12 MeV; measured σ(Ep, Eγ, θ(p)). 29Si deduced levels, J, π, L, isobaric analog, anti-analog state.
doi: 10.1103/PhysRev.187.1210
1968BE25 Nucl.Phys. A116, 682(1968) R.C.Bearse, L.Meyer-Schutzmeister, R.E.Segel The 23Na(p, γ)24Mg Reaction and the Giant Dipole Resonance in 24Mg NUCLEAR REACTIONS 23Na(p, γ), E=4-12.4 MeV; measured σ(E;Eγ, θ).
doi: 10.1016/0375-9474(68)90399-0
1968ME04 Nucl.Phys. A108, 180(1968) L.Meyer-Schutzmeister, Z.Vager, R.E.Segel, P.P.Singh The Giant Dipole Resonance Excited by α-Capture NUCLEAR REACTIONS 24Mg(α, γ), E = 5.3-14.5 MeV; 26Mg(α, γ), E = 4-13.5 MeV; 28Si(α, γ), E = 7-12 MeV; measured σ(E; Eγ, θ). 28Si, 30Si, 32S levels deduced J, π properties of giant dipole resonance. Enriched 24,26Mg targets. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0255. 1967SC08 Phys.Rev. 155, 1191 (1967) J.J.Schwartz, W.P.Alford, T.H.Braid, L.Meyer-Schutzmeister Level Structure and Decay Scheme of Sc43 NUCLEAR STRUCTURE 43Sc; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.155.1191
1967SE02 Nucl.Phys. A93, 31(1967) R.E.Segel, Z.Vager, L.Meyer-Schutzmeister, P.P.Singh, R.G.Allas Radiative Capture by 19F: The Giant Dipole Resonances in 20Ne NUCLEAR REACTIONS 19F(p, γ), E = 2.88-12.80 MeV; measured σ(E; Eγ, θ); deduced correlation functions. 20Ne compound-nucleus deduced J, π.
doi: 10.1016/0375-9474(67)90169-8
1966ME09 Phys.Rev. 147, 743 (1966) L.Meyer-Schutzmeister, D.Von Ehrenstein, R.G.Allas Isospin Selection Rule in the C12(d, α)B10 Reaction NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.147.743
1966VO01 Nucl.Phys. 79, 625(1966) D.Von Ehrenstein, L.Meyer-Schutzmeister, R.G.Allas Study of the 39K(p, α)36Ar Reaction NUCLEAR REACTIONS 39K(p, α), E = 10.0-13.0 MeV; measured σ(E, Eα, θ). 36Ar levels deduced, J, statistical properties. Enriched target.
doi: 10.1016/0029-5582(66)90268-9
1965AL06 Nucl.Phys. 61, 289 (1965) R.G.Allas, L.Meyer-Schutzmeister, D.Von Ehrenstein Energy Levels of Ar36 and Ar38 NUCLEAR REACTIONS 39K(p, α), E=10.4 MeV; 41K(p, α), Ep=9.0, 10.5 MeV; measured σ(Eα). 36,38Ar deduced levels. Enriched targets.
doi: 10.1016/0029-5582(65)90902-8
1965BR38 Bull.Am.Phys.Soc. 10, No.4, 480, EA11 (1965) T.H.Braid, L.Meyer-Schutzmeister (He3, α) Reactions on Medium-Weight Nuclei NUCLEAR REACTIONS 50Ti, 51V, 52Cr, 54,56Fe(3He, α), E = 12-14 MeV; measured σ(Eα, θ). 50V, 53,55Fe deduced levels, L(n), isobaric analog. Magnetic spectrograph.
1965ME01 Bull.Am.Phys.Soc. 10, No.1, 10, AC13 (1965) L.Meyer-Schutzmeister, R.E.Segel Search for a 4.97-MeV Doublet in Ne20 NUCLEAR STRUCTURE 20Ne; measured not abstracted; deduced nuclear properties.
1965ME10 Nucl.Phys. 71, 343(1965) L.Meyer-Schutzmeister, R.E.Segel Search for a Second State in Ne20 Near 4.97 MeV NUCLEAR REACTIONS 23Na(p, α)20Ne, E = 10, 12 MeV; measured σ(Eα). 20Ne deduced levels.
doi: 10.1016/0029-5582(65)90721-2
1965SI11 Nucl.Phys. 65, 577(1965) P.P.Singh, R.E.Segel, L.Meyer-Schutzmeister, S.S.Hanna, R.G.Allas Giant Resonances and Fine Structure in Si28 from the Al27(p, γ)Si28 Reaction NUCLEAR REACTIONS 27Al(p, γ), E=4-12.5 MeV; measured σ(E; Eγ, θ). 28Si deduced mean level width. Natural target.
doi: 10.1016/0029-5582(65)90326-3
1964AL03 Bull. Am. Phys. Soc. 9, No. 1, 79, HC12 (1964) R.G.Allas, L.Meyer-Schutzmeister, D.von Ehrenstein States in Ar36 with Excitation Energies below 7 MeV NUCLEAR STRUCTURE 36Ar; measured not abstracted; deduced nuclear properties.
1964AL10 Bull. Am. Phys. Soc. 9, No. 5, 553, N6 (1964) R.G.Allas, L.Meyer-Schutzmeister, D.von Ehrenstein States in 38A with Excitation Energies below 6.3 MeV NUCLEAR STRUCTURE 38Ar; measured not abstracted; deduced nuclear properties.
1964AL20 Nucl. Phys. 58, 122 (1964) R.G.Allas, S.S.Hanna, L.Meyer-Schutzmeister, R.E.Segel Radiative Capture of Protons by B11 and the Giant Dipole Resonance in C12 NUCLEAR REACTIONS 11B(p, γ), Ep=4-14 MeV; measured σ(E, θ), Eγ. Enriched target.
doi: 10.1016/0029-5582(64)90527-9
1964ME10 Rev.Mod.Phys. 36, 392 (1964) L.Meyer-Schutzmeister, S.S.Hanna, J.Heberle, J.Diaz, R.W.Reno Internal Magnetic Field in Gadolinium NUCLEAR STRUCTURE 155Eu; measured not abstracted; deduced nuclear properties.
1964ME12 Bull.Am.Phys.Soc. 9, No.6, 666, Y9 (1964) L.Meyer-Schutzmeister, R.E.Segel, Z.Vager Studies of Mg24(α, γ)Si28 NUCLEAR STRUCTURE 28Si; measured not abstracted; deduced nuclear properties.
1964SE10 Bull.Am.Phys.Soc. 9, No.6, 665, Y2 (1964) R.E.Segel, L.Meyer-Schutzmeister, P.P.Singh, Z.Vager F19(p, γ)Ne20 Giant Resonances NUCLEAR STRUCTURE 19F, 20Ne; measured not abstracted; deduced nuclear properties.
1964WE02 Phys.Rev. 133, B590 (1964) J.A.Weinman, L.Meyer-Schutzmeister, L.L.Lee, Jr. States in Si28 with 12.7 < e < 13.7 MeV by (α, γ) and (α, α) Reactions on Mg24 NUCLEAR STRUCTURE 28Si; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.133.B590
1963AL01 Bull.Am.Phys.Soc. 8, No.1, 11, BA6 (1963) R.G.Allas, S.S.Hanna, L.L.Lee, Jr., L.Meyer-Schutzmeister, R.E.Segel Reaction B11(p, γ)C12 in the Range 4 < Ep < 10 MeV NUCLEAR STRUCTURE 11B; measured not abstracted; deduced nuclear properties.
1963AL02 Bull.Am.Phys.Soc. 8, No.1, 48, NA7 (1963) R.G.Allas, D.von Ehrenstein, L.Meyer-Schutzmeister, J.A.Weinman K39(p, α)Ar36 Reaction NUCLEAR STRUCTURE 36Ar; measured not abstracted; deduced nuclear properties.
1963AL16 Bull.Am.Phys.Soc. 8, No.7, 538, S7 (1963) R.G.Allas, J.R.Erskine, L.Meyer-Schutzmeister, D.von Ehrenstein Population of the First T=1 State in B10 by the Reaction C12(d, α)B10 NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
1963AL17 Bull.Am.Phys.Soc. 8, No.7, 538, S11 (1963) R.G.Allas, S.S.Hanna, L.Meyer-Schutzmeister, R.E.Segel, P.P.Singh Capture Reactions Al27(p, γ)Si28,28* in the Giant-Dipole Region of Si28* NUCLEAR STRUCTURE 28Si; measured not abstracted; deduced nuclear properties.
1963AL33 ANL-6720, p.24 (1963) R.Allas, M.Grace, S.S.Hanna, L.Meyer-Schutzmeister, R.E.Segel, P.P.Singh (p, γ) Properties of Individual Unbound Levels NUCLEAR STRUCTURE 16O; measured not abstracted; deduced nuclear properties.
1962HE01 Bull.Am.Phys.Soc. 7, No.1, 39, KA8 (1962) C.L.Herzenberg, L.Meyer-Schutzmeister, L.L.Lee, Jr., S.S.Hanna Mossbauer Effect in Gd155 NUCLEAR STRUCTURE 155Gd; measured not abstracted; deduced nuclear properties.
1962WE02 Bull.Am.Phys.Soc. 7, No.1, 72, V10 (1962) J.A.Weinman, L.L.Lee, Jr., L.Meyer-Schutzmeister, S.S.Malik Capture of Alpha Particles by Mg24 NUCLEAR STRUCTURE 28Si; measured not abstracted; deduced nuclear properties.
1962WE15 ANL-6612; Erratum VII (1962) J.A.Weinman, L.Meyer-Schutzmeister, L.L.Lee, Jr. Excited States of Light Nuclei NUCLEAR STRUCTURE 22Ne; measured not abstracted; deduced nuclear properties.
1962WE16 ANL-6603, p.47 (1962) J.A.Weinman, L.Meyer-Schutzmeister, L.L.Lee, Jr. Excited States of Light Nuclei NUCLEAR STRUCTURE 18O, 21Ne; measured not abstracted; deduced nuclear properties.
1960HA33 Phys.Rev. 120, 2211 (1960) S.S.Hanna, L.Meyer-Schutzmeister, R.S.Preston, D.H.Vincent Nuclear Zeeman Effect in Sn119 NUCLEAR STRUCTURE 119Sn; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.120.2211
1959HA11 Phys.Rev. 115, 986 (1959) S.S.Hanna, L.Meyer-Schutzmeister Resonant Absorption by the 9.17-MeV Level in N14
doi: 10.1103/PhysRev.115.986
1959LE36 Phys.Rev.Letters 3, 223 (1959) L.L.Lee, Jr., L.Meyer-Schutzmeister, J.P.Schiffer, D.Vincent Nuclear Resonance Absorption of Gamma Rays at Low Temperatures
doi: 10.1103/PhysRevLett.3.223
1958ME77 Bull.Am.Phys.Soc. 3, No.3, 188, K10 (1958) L.Meyer-Schutzmeister, S.S.Hanna Resonanct Absorption of Gamma Rays in B11
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