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NSR database version of April 11, 2024.

Search: Author = H.E.Mahnke

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2014MA30      Acta Phys.Pol. B45, 571 (2014)


Nuclear Physics Methods in Cultural Heritage Research - Accelerators for Art

doi: 10.5506/APhysPolB.45.571
Citations: PlumX Metrics

1996ME14      Hyperfine Interactions 97/98, 229 (1996)

H.Metzner, C.Dzionk, S.Hessler, H.-E.Mahnke, I.Luck, R.Scheer, H.J.Lewerenz, M.Gossla, Th.Hahn

Nuclear Probes in the Materials Science of Solar Cells

RADIOACTIVITY 111In(EC); measured γγ(θ, H); deduced solar cells related features.

doi: 10.1007/BF02150179
Citations: PlumX Metrics

1995MA50      Nucl.Phys. A588, 221c (1995)


Radioactive Nuclei in Material Science Research

doi: 10.1016/0375-9474(95)00143-O
Citations: PlumX Metrics

1993SC37      Hyperfine Interactions 80, 1093 (1993)

D.Schumann, H.-E.Mahnke, B.Spellmeyer, G.Sulzer, H.Waldmann, W.-D.Zeitz

PAD Investigation of 19F in Fullerites

NUCLEAR REACTIONS 12C(12C, pα), E=43 MeV; measured γ(θ, H); deduced 19F quadrupole interaction features in Fullerites.

doi: 10.1007/BF00567469
Citations: PlumX Metrics

1992AL17      Z.Phys. A344, 1 (1992)

D.Alber, A.Berger, H.H.Bertschat, H.Grawe, H.Haas, H.Kluge, A.Kuhnert, H.E.Mahnke, K.H.Maier, R.Schubart, B.Spellmeyer, X.Sun, L.Wood

Nuclear Structure Study of the Neutron Deficient Cadmium Isotopes 100,101,102Cd

NUCLEAR REACTIONS 46,47Ti, 50Cr(58Ni, X), E=230, 945 MeV; measured pγ-, ppγ-, nγ-, nnγ-, nγγ-coin, nγγ(t); deduced evidence for 100,101Cd. 70Ge(36Ar, 2n2p), (36Ar, 4n2p), E=135 MeV; measured γ(θ, H, t). 100,101,102Cd deduced isomers g, J, π, T1/2, B(λ), γ-multipolarity, quadrupole moment. Shell model comparison.

doi: 10.1007/BF01291011
Citations: PlumX Metrics

1990MU03      Phys.Rev. B41, 8624 (1990)

W.Muller, H.H.Bertschat, K.Biedermann, R.Kowallik, E.Lahmer-Naim, H.-E.Mahnke, S.Seeger, W.-D.Zeitz, S.Fiechter, H.Tributsch

Perturbed-Angular-Distribution Measurements of the Chemical Shift of Iron in the Disulfides FeS2(Pyrite) and RuS2(laurite)

NUCLEAR REACTIONS 45Sc(12C, 2np), E=42 MeV; measured γ(θ, H, t); deduced chemical shift vs temperture.

doi: 10.1103/PhysRevB.41.8624
Citations: PlumX Metrics

1989SP04      Phys.Rev.Lett. 63, 1463 (1989)

G.D.Sprouse, J.Das, T.Lauritsen, J.Schecker, A.Berger, J.Billowes, C.H.Holbrow, H.-E.Mahnke, S.L.Rolston

Laser Spectroscopy of Light Yb Isotopes On-Line in a Cooled Gas Cell

RADIOACTIVITY 166,158Yb [from 154,144Sm(18O, X), E=101, 108 MeV]; 157,156Yb [from 144Sm(16O, X), E=101, 117 MeV]; 154,152Yb [from 96Ru(60Ni, X), (58Ni, X), E=250, 241 MeV]; measured isotope shifts; deduced rms charge radius changes shell structure dependence.

doi: 10.1103/PhysRevLett.63.1463
Citations: PlumX Metrics

1987BE35      Hyperfine Interactions 34, 547 (1987)

A.Berger, H.H.Bertschat, H.-E.Mahnke, B.Spellmeyer, W.Shen

Knight Shift of sp-Elements in Bismuth

RADIOACTIVITY 194Pb, 112Sb, 202Bi, 210At, 211Rn; measured γ(θ, H, t); deduced Knight shift in Bi host.

doi: 10.1007/BF02072774
Citations: PlumX Metrics

1987HA27      Hyperfine Interactions 34, 543 (1987)

H.Haas, H.-E.Mahnke, W.G.Shen, Ch.Stenzel

The Knight Shift of Francium in Cesium

NUCLEAR REACTIONS 198Pt(19F, 5n), E=96 MeV; measured γ(θ, H, t). 212Fr deduced isomer Knight shift in Cs.

doi: 10.1007/BF02072773
Citations: PlumX Metrics

1987MA65      Hyperfine Interactions 34, 47 (1987)


In-Beam Measurements of Nuclear Moments

COMPILATION 202Bi, 200,204,206,208,210Po, 209,210,211At, 211,212,208,210Rn; compiled isomeric proton state quadrupole moments.

doi: 10.1007/BF02072678
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1987NA17      Hyperfine Interactions 34, 231 (1987)

E.Naim, C.Broude, E.Dafni, M.Hass, M.H.Rafailovich, H.-E.Mahnke, G.Schatz

Temperature Dependence of the Electric Field Gradient of Hg in Bi

NUCLEAR REACTIONS 164Dy(28Si, 4n), E=136 MeV; measured γ(θ, H, t); deduced 188mHg electric field gradient vs temperature in Bi.

doi: 10.1007/BF02072710
Citations: PlumX Metrics

1986BE40      Phys.Lett. 182B, 11 (1986)

A.Berger, H.Grawe, H.-E.Mahnke, E.Dafni, M.Hass, E.Naim, M.H.Rafailovich

Extreme Sensitivity of Quadrupole Moments of Rn Isomers for Small Deformations

NUCLEAR REACTIONS 209Bi(6Li, 5n), E=60 MeV; 194Pt(18O, 4n), E not given; measured Eγ, Iγ, γ(θ, H, t). 208,210,211Rn deduced isomer quadrupole moment. Other data input.

doi: 10.1016/0370-2693(86)91069-5
Citations: PlumX Metrics

1985BE23      Z.Phys. A321, 403 (1985)

A.Berger, H.-E.Mahnke, H.Grawe, W.Semmler, R.Sielemann

Quadrupole Moments of Neutron Isomers in Sm Isotopes

NUCLEAR REACTIONS 127I(19F, 4n), E=85 MeV; 124Te(20Ne, 4n), E=96 MeV; measured Iγ(θ), oriented nuclei; deduced quadrupole interaction of Sm in Gd. 140,142Sm deduced isomer quadrupole moments, deformation characteristics.

doi: 10.1007/BF01411971
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1985DA13      Nucl.Phys. A441, 501 (1985)

E.Dafni, M.Hass, E.Naim, M.H.Rafailovich, A.Berger, H.Grawe, H.-E.Mahnke

Electric Quadrupole Interaction of 212Rn Isomers in Bi

NUCLEAR REACTIONS 198Pt(18O, 4n), E=77, 84 MeV; 209Bi(6Li, 3n), E=45 MeV; measured I(γ)(θ, t), oriented nuclei. 212Rn deduced quadrupole coupling constants. Pulsed beams, Ge(Li) detectors, Bi single-crystal host.

doi: 10.1016/0375-9474(85)90159-9
Citations: PlumX Metrics

1985DA14      Phys.Rev.Lett. 55, 1269 (1985)

E.Dafni, M.Hass, E.Naim, M.H.Rafailovich, A.Berger, H.Grawe, H.-E.Mahnke

Electric Quadrupole Moment of the 211Rn (63/2)- Isomer: Absence of core deformation at very high spins

NUCLEAR REACTIONS 198Pt(18O, 5n), E=94 MeV; measured γ(θ, H, t). 211Rn deduced high-spin isomer electric quadrupole moment. Single crystal Bi host.

doi: 10.1103/PhysRevLett.55.1269
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1985ST16      Z.Phys. A322, 83 (1985)

C.Stenzel, H.Grawe, H.Haas, H.-E.Mahnke, K.H.Maier

E2 Moments and g-Factors in Neutron Deficient Lead Isotopes

NUCLEAR REACTIONS 158,160Gd(36Ar, 4n), E=175 MeV; 156Gd(40Ar, 4n), E=185 MeV; measured Eγ, Iγ(t). 182W(16O, 4n), E=85 MeV; measured γ(θ, H, t). 190,192Pb deduced isomer T1/2, B(E2), quadrupole moment. 194Pb deduced isomer T1/2, quadrupole moment, g, B(E2). 196,198Hg(α, xn), E=60 MeV; analyzed data. 195,196,197,198,199,200Pb levels deduced g, T1/2, configuration. Two-quasiparticle Tamm-Dancoff calculation, surface delta interaction.

doi: 10.1007/BF01412020
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1984AL01      Nucl.Phys. A413, 353 (1984)

D.Alber, H.Grawe, H.Haas, H.-E.Mahnke, W.Semmler, W.-D.Zeitz

Recoil Distance Lifetime Measurements in 125Xe

NUCLEAR REACTIONS 116Cd(12C, 3n), E=47 MeV; measured γγ(t), Doppler shift recoil. 125Xe deduced levels, T1/2, (Γ(γ)+Γ(e)), B(E2). Ge(Li), NaI(Tl) detectors, plunger.

doi: 10.1016/0375-9474(84)90379-8
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1984BE68      Phys.Lett. 101A, 507 (1984)

H.H.Bertschat, H.-E.Mahnke, E.Dafni, F.D.Davidovsky, M.Hass

Local Magnetic Susceptibility in α-Cerium

NUCLEAR REACTIONS 122Sn(16O, 4n), E not given; measured γ(θ, H, t); deduced local magnetic susceptibility in α-Cerium.

doi: 10.1016/0375-9601(84)90430-4
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1984MA10      Phys.Lett. 134B, 153 (1984)

H.-E.Mahnke, O.Hausser, H.Grawe, H.Kluge, W.Semmler

Spin Rotation of 162Yb in Unresolved High-Spin States

NUCLEAR REACTIONS 80Se(86Kr, 4n), E=362 MeV; measured γγ-coin, γ(θ, H), recoil. 162Yb deduced high-spin state spin rotation, average g, quadrupole moment. Sectored NaI sum spectrometer.

doi: 10.1016/0370-2693(84)90660-9
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1983AL21      Z.Phys. A314, 17 (1983)

D.Alber, H.H.Bertschat, H.Grawe, H.Haas, H.-E.Mahnke, M.Menningen, W.Semmler, R.Sielemann, W.-D.Zeitz

The g-Factor and the Electric Quadrupole Moment of the 7/2+ Isomer in 125Xe

RADIOACTIVITY 125Xe(EC), (β+) [from 116Cd(12C, 3n), E=52, 57 MeV]; measured γ(θ, H, t), γγ(t), recoil; deduced electric quadrupole interaction, electric field gradient for Xe in Cd. 125Xe deduced isomer T1/2, quadrupole moment, g, level T1/2, γ-branching, B(E2).

doi: 10.1007/BF01411824
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1983MA08      Phys.Lett. 122B, 27 (1983)

H.-E.Mahnke, W.Semmler, H.Grawe, H.Haas, R.Sielemann

Quadrupole Moments of High-Spin Isomers in Astatine Isotopes

NUCLEAR REACTIONS 209Bi(α, 4n), (α, 3n), (α, 2n), E=45, 60 MeV; measured γ(θ, H, t). 211,210,209At deduced high-spin isomer T1/2, quadrupole moment, nuclear quadrupole interaction, configuration effects.

doi: 10.1016/0370-2693(83)91161-9
Citations: PlumX Metrics

1983MA79      Hyperfine Interactions 15/16, 223 (1983)

H.-E.Mahnke, W.Semmler

Probe Atom Dependence of the Electric Field Gradient in Bismuth

NUCLEAR REACTIONS 181Ta(16O, 5n), E=100 MeV; measured γ(θ, H, t); deduced Tl electric field gradient in Bi. 192Tl deduced isomer quadrupole moment.

doi: 10.1007/BF02159743
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1983RA07      Phys.Rev.Lett. 50, 1001 (1983)

M.H.Rafailovich, E.Dafni, H.-E.Mahnke, G.D.Sprouse

Observation of a Positive Hyperfine Field for Dilute Fe Impurities in Ca

NUCLEAR REACTIONS 45Sc(12C, 2np), E=39 MeV; measured γ(θ, H, t) vs temperature; deduced magnetic hyperfine field for Fe in Ca metal, unquenched orbital local moment.

doi: 10.1103/PhysRevLett.50.1001
Citations: PlumX Metrics

1983SE04      Z.Phys. A309, 349 (1983)

W.Semmler, H.-E.Mahnke, H.Grawe, R.Sielemann

Quadrupole Moment of the (19/2)- Isomer in 115Sb

NUCLEAR REACTIONS 100Mo(19F, 4n), E=76 MeV; measured γ(θ, H, t); deduced quadrupole coupling constant for Sb in Bi. 115Sb deduced isomer quadrupole moment. Enriched target, recoil implantation in heated Bi single crystal.

doi: 10.1007/BF01413838
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1983SE21      Hyperfine Interactions 15/16, 219 (1983)

W.Semmler, H.Haas, H.-E.Mahnke, R.Sielemann

Antimony in Cadmium - An Extreme Case of Probe Atom Dependent EFG

NUCLEAR REACTIONS 103Rh(12C, 3n), E=60 MeV; measured γ(θ, H, t); deduced Sb field gradient in Cd. Recoil ion implantation.

doi: 10.1007/BF02159742
Citations: PlumX Metrics

1983ST15      Nucl.Phys. A411, 248 (1983)

Ch.Stenzel, H.Grawe, H.Haas, H.-E.Mahnke, K.H.Maier

Magnetic Moments of (νi13/2)(-n) Isomers in Neutron-Deficient Lead Isotopes

NUCLEAR REACTIONS 156Gd(40Ar, 4n), E=185 MeV; 196,198,204Hg(α, xn), E=45, 60 MeV; measured Iγ(θ, H, t). 192,196,198,200,205,206Pb level deduced g, T1/2. Ge(Li) detectors, enriched liquid metallic Hg targets.

doi: 10.1016/0375-9474(83)90391-3
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1983ST16      Hyperfine Interactions 15/16, 97 (1983)

Ch.Stenzel, H.Grawe, H.Haas, H.-E.Mahnke, K.H.Maier

Magnetic Moment of the 12+-Isomer in 192Pb

NUCLEAR REACTIONS 156Gd(40Ar, 4n), E=185 MeV; measured γ(θ, H, t). 192Pb deduced isomer T1/2, μ.

doi: 10.1007/BF02159725
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1982HA22      Nucl.Phys. A379, 287 (1982)

O.Hausser, H.E.Mahnke, T.K.Alexander, H.R.Andrews, J.F.Sharpey-Schafer, M.L.Swanson, D.Ward, P.Taras, J.Keinonen

Quadrupole Moments of Yrast Isomers in 144, 147, 148Gd

NUCLEAR REACTIONS 120,124Sn(28Si, xn), E=108-144 MeV; measured Iγ(θ, H, t) vs T. 144,147,148Gd levels deduced quadrupole moment, tentative J, deformation. Pulsed beam, Ge(Li) detectors, recoil implantation into Gd.

doi: 10.1016/0375-9474(82)90394-3
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1982MA29      Phys.Rev. C26, 493 (1982)

H.-E.Mahnke, E.Dafni, M.H.Rafailovich, G.D.Sprouse, E.Vapirev

Quadrupole Moment of the 8- Isomer in 112Sb

NUCLEAR REACTIONS 103Rh(12C, 3n), E=50 MeV; measured Iγ(θ, t, H). 112Sb deduced isomer level quadrupole moment. Pulsed beam, recoil implantation in Sb, Sn single crystal, polycrystalline In foil.

doi: 10.1103/PhysRevC.26.493
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1982ZE05      Z.Phys. A308, 227 (1982)

W.-D.Zeitz, D.Alber, H.Grawe, H.Haas, R.Keitel, H.-E.Mahnke, W.Semmler, R.Sielemann

Electromagnetic Transition Strengths and Nuclear Moments in 123Xe

NUCLEAR REACTIONS 114Cd(12C, 3n), (13C, 4n), E=50-62 MeV; measured γγ-coin, recoil, γ(θ, H, t); deduced quadrupole coupling constant for Xe in Cd. 123Xe deduced levels, J, π, isomer T1/2, g, γ-branching, γ-multipolarity, δ(E2/M1), B(λ), μ, quadrupole moment. Triaxial rotor-particle model.

doi: 10.1007/BF01418284
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1981DA06      Phys.Rev. C23, 1612 (1981)

E.Dafni, H.E.Mahnke, J.W.Noe, M.H.Rafailovich, G.D.Sprouse

E2 Moments of the 43Sc(19/2-) and the 43Ti(19/2-) States and the 40Ca Core Deformation

NUCLEAR REACTIONS 27Al(19F, 2np), E=45.5 MeV; 40Ca(α, p), (α, n), E=21 MeV; measured γγ(θ, t) in Ti. 43Sc, 43Ti levels deduced B(E2), static quadrupole moment, isomer T1/2, quadrupole coupling constant.

doi: 10.1103/PhysRevC.23.1612
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1980HA02      Phys.Rev.Lett. 44, 132 (1980)

O.Hausser, H.-E.Mahnke, J.F.Sharpey-Schafer, M.L.Swanson, P.Taras, D.Ward, H.R.Andrews, T.K.Alexander

Quadrupole Moment of a High-Spin Yrast Trap in 147Gd

NUCLEAR REACTIONS 124Sn(28Si, 5nγ), E=144 MeV; measured γ(θ, t), oriented nuclei, quadrupole interactions. 147Gd levels deduced quadrupole moments, quasiparticle configuration, β. Pulsed beam.

doi: 10.1103/PhysRevLett.44.132
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1980HA52      Hyperfine Interactions 8, 271 (1980)

O.Hausser, D.Ward, T.K.Alexander, H.R.Andrews, W.J.L.Buyers, H.-E.Mahnke, J.F.Sharpey-Schafer, P.Skensved, M.L.Swanson, P.Taras

The Electric Field Gradient for Gd in Gadolinium Metal

NUCLEAR REACTIONS 120Sn(28Si, 4n), E=130 MeV; measured γ(θ, H), recoil in Gd host. 144Gd deduced temperature dependence of electric field gradient in Gd above Curie point. 156,158,160Gd(α, α'), E=6 MeV; measured Coulomb excitation, Iγ; deduced electric field gradient for Gd in Gd.

1979MA37      Phys.Lett. 88B, 48 (1979)

H.-E.Mahnke, T.K.Alexander, H.R.Andrews, O.Hausser, P.Taras, D.Ward, E.Dafni, G.D.Sprouse

Quadrupole Moments of the 12+ States in 206Pb and 200Pb

NUCLEAR REACTIONS 204,198Hg(α, 2n), E=33 MeV; measured γ(θ, H, t). 206,200Pb levels deduced quadrupole moments, T1/2, B(E2).

doi: 10.1016/0370-2693(79)90110-2
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1978DE29      Phys.Rev. C18, 2061 (1978)

M.S.Dewey, H.-E.Mahnke, P.Chowdhury, U.Garg, T.P.Sjoreen, D.B.Fossan

Magnetic Moment Measurement of the 129Cs 11/2- Isomer in a CsI Cubic Environment

NUCLEAR REACTIONS 127I(α, 2nγ), E=22 MeV; measured spin rotation in γ(θ, H, t). 129Cs level deduced g. Pulsed beam, CsI target, TDPAD technique.

doi: 10.1103/PhysRevC.18.2061
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1976LE03      Nucl.Phys. A258, 103 (1976)

W.Leitz, H.-E.Mahnke, W.Semmler, R.Sielemann, T.Wichert

The Half-Lives of the First and Second Excited States in 66Ga

NUCLEAR REACTIONS 63Cu(α, nγ), E=12.2 MeV; 66Zn(p, nγ), E=6.6 MeV; measured αγ-delay, pγ-delay, γγ delayed coin. 66Ga excited levels deduced T1/2, g-factor analyzed. Enriched targets. Ge(Li), Si(Li) detectors.

doi: 10.1016/0375-9474(76)90531-5
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1975BA07      Phys.Lett. 50A, 413 (1975)

W.Bartsch, J.Golczewski, W.Leitz, H.-E.Mahnke, W.Semmler, R.Sielemann, T.Wichert

Electric Quadrupole Interaction of Recoil-Implanted Zinc in Cadmium

NUCLEAR REACTIONS 64Ni(α, nγ), E=12.5 MeV; measured Eγ. 67Zn level deduced quadrupole coupling constant.

doi: 10.1016/0375-9601(75)90104-8
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1975MA30      Nucl.Phys. A247, 195 (1975)

H.-E.Mahnke, G.Kaindl, F.Bacon, D.A.Shirley

Nuclear Orientation of 2.3 d 198mAu

RADIOACTIVITY 198mAu [from 198Pt(d, 2n), 196Pt(α, pn)]; measured Iγ(θ, t) in Fe, Ni; deduced μ, δ; enriched targets.

doi: 10.1016/0375-9474(75)90630-2
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1973BA11      Phys.Rev. C7, 1654 (1973)

F.Bacon, G.Kaindl, H.-E.Mahnke, D.A.Shirley

Nuclear Magnetic Resonance of Oriented 196Au, 198Au, and 200m-Au

RADIOACTIVITY 200mAu; measured γ(θ, H, t), NMR. 200mAu deduced J, μ. 200Hg deduced γ-mixing. 196,198Au measured NMR, deduced hyperfine field in Ni, hyperfine anomaly. 197,198Au deduced hyperfine anomaly.

doi: 10.1103/PhysRevC.7.1654
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1973CH19      Z.Phys. 261, 13 (1973)

J.Christiansen, H.E.Mahnke, U.Morfeld, E.Recknagel, D.Riegel, W.Witthuhn

Mossbauer Effect in α-Fe2O3 Following the Reaction 56Fe(d, p)57Fe

NUCLEAR REACTIONS 56Fe(d, pγ), E=5.1 MeV; measured Mossbauer effect. 57Fe deduced quadrupole splitting.

doi: 10.1007/BF01402278
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1973HA09      Phys.Rev.Lett. 30, 656 (1973)

H.Haas, W.Leitz, H.-E.Mahnke, W.Semmler, R.Sielemann, T.Wichert

Quadrupole Interaction of Ge Nuclei in Zn and Ga Following Nuclear Reactions

NUCLEAR REACTIONS Zn, 66Zn(α, nγ), E=13 MeV; Ga(p, nγ), E=6.5 MeV; measured Iγ(θ, t). 67,69,71Ge; deduced quadrupole interaction, quadrupole moment.

doi: 10.1103/PhysRevLett.30.656
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1973KA28      Phys.Rev. C8, 1074 (1973)

G.Kaindl, F.Bacon, H.-E.Mahnke, D.A.Shirley

Nuclear Magnetic Resonance on Oriented 101Rh-m

RADIOACTIVITY 101mRh; measured γ(θ, t), NMR. 101Rh levels deduced J, π, γ-mixing, g.

doi: 10.1103/PhysRevC.8.1074
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1972BA16      Phys.Lett. 38A, 401 (1972)

F.Bacon, H.Haas, G.Kaindl, H.-E.Mahnke

Magnetic Hyperfine Fields at Bismuth in Iron and Nickel

RADIOACTIVITY 204Bi; measured Iγ(θ, H, t), γγ(θ, H, t) in Fe, Ni; deduced magnetic hyperfine fields.

doi: 10.1016/0375-9601(72)90224-1
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1972BA22      Phys.Rev.Lett. 28, 720 (1972)

F.Bacon, G.Kaindl, H.-E.Mahnke, D.A.Shirley

Nuclear Magnetic Resonance on Oriented Platinum-195m in Iron

NUCLEAR MOMENTS 195mPt; measured J, μ, Iγ(θ, t); deduced γ-mixing. NMR, oriented nuclei.

doi: 10.1103/PhysRevLett.28.720
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1971BA94      Phys.Lett. 37B, 181 (1971)

F.Bacon, G.Kaindl, H.-E.Mahnke, D.A.Shirley

Magnetic Moment of the 12- Isomer of 196Au

NUCLEAR MOMENTS 196mAu; measured μ.

doi: 10.1016/0370-2693(71)90045-1
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1971CH10      Nucl.Phys. A164, 367 (1971)

J.Christiansen, H.-E.Mahnke, E.Recknagel, D.Riegel, W.Witthuhn

Lifetime and g-Factor of the 273 keV Level in 74As

NUCLEAR REACTIONS 74Ge(p, nγ), Ep=3.5-5.2 MeV; measured σ(E;Eγ), γγ-coin, γγ-delay, pγ(θ, H, t). 74As deduced levels, T1/2, g. Enriched target.

doi: 10.1016/0375-9474(71)90220-X
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1970BE23      Phys.Rev.Lett. 25, 102 (1970)

H.Bertschat, J.Christiansen, H.-E.Mahnke, E.Recknagel, G.Schatz, R.Sielemann, W.Witthuhn

Time-Dependent Relaxation of Aligned Nuclei Due to Radiation-Induced Vacancies in Solid Germanium

RADIOACTIVITY 73mAs[from 72Ge(d, n)]; measured Iγ(θ, H); deduced time dependence of nuclear alignment.

doi: 10.1103/PhysRevLett.25.102
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1970BE29      Nucl.Phys. A150, 282 (1970)

H.Bertschat, J.Christiansen, H.-E.Mahnke, E.Recknagel, G.Schatz, R.Sielemann, W.Witthuhn

Stroboscopic and Time-Differential Observation of the Nuclear Larmor Precession on the 20 ms Isomeric State of 71Ge

NUCLEAR REACTIONS 71Ga(p, nγ), E=5.2 MeV; measured γγ(θ, H, t). 71Ge level deduced g. Natural target.

doi: 10.1016/0375-9474(70)90951-6
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1970BE33      Nucl.Phys. A151, 193 (1970)

H.Bertschat, J.Christiansen, H.-E.Mahnke, E.Recknagel, G.Schatz, R.Sielemann, B.Spellmeyer, W.Witthuhn

Magnetic Moment of the 10 μsec Level in 58Co

NUCLEAR REACTIONS 57Fe(d, nγ), E=5.5 MeV; measured dγ(θ, H, t). 58Co level deduced g. Enriched target.

doi: 10.1016/0375-9474(70)90978-4
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1970CH05      Phys.Rev. C1, 613 (1970)

J.Christiansen, H.-E.Mahnke, E.Recknagel, D.Riegel, G.Schatz, G.Weyer, W.Witthuhn

Stroboscopic Observation of Nuclear Larmor Precession

NUCLEAR REACTIONS 69Ga(p, nγ), E=4.4 MeV; measured γγ(θ, H, t); deduced nuclear Larmor precession frequency. 69mGe deduced g.

doi: 10.1103/PhysRevC.1.613
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1968CH17      Phys.Rev.Letters 21, 554(1968)

J.Christiansen, H.-E.Mahnke, E.Recknagel, D.Riegel, G.Weyer, W.Witthuhn

Perturbed Angular Correlation of Nuclei Coherently Excited by Pulsed-Beam Techniques

NUCLEAR REACTIONS 69Ga(p, n), E not given; measured p, γ(θ, H, t). 69Ge level deduced g, μ. Pulsed beam.

doi: 10.1103/PhysRevLett.21.554
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