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NSR database version of April 11, 2024.

Search: Author = L.Meyer-Schutzmeister

Found 65 matches.

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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0012.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0034.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2748.


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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1530.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2743.


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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1896.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2149.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF1152.


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
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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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0200.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1485.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0344.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0268.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1958ME77      Bull.Am.Phys.Soc. 3, No.3, 188, K10 (1958)

L.Meyer-Schutzmeister, S.S.Hanna

Resonanct Absorption of Gamma Rays in B11


1957ME27      Phys.Rev. 108, 1506 (1957)

L.Meyer-Schutzmeister, S.S.Hanna

Energy Levels in B10 in the Reaction Li6(α, γ)B10

doi: 10.1103/PhysRev.108.1506
Citations: PlumX Metrics


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