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NSR database version of April 11, 2024.

Search: Author = G.Schatz

Found 61 matches.

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1999AN44      J.Phys.(London) G25, 2161 (1999)

T.Antoni, W.D.Apel, K.Bekk, K.Bernlohr, E.Bollmann, K.Daumiller, P.Doll, J.Engler, F.Fessler, H.J.Gils, R.Glasstetter, R.Haeusler, W.Hafemann, A.Haungs, D.Heck, J.R.Horandel, T.Holst, K.-H.Kampert, H.O.Klages, J.Knapp, H.J.Mathes, H.J.Mayer, J.Milke, D.Muhlenberg, J.Oehlschlager, H.Rebel, M.Risse, M.Roth, G.Schatz, H.Schieler, F.K.Schmidt, T.Thouw, H.Ulrich, J.Unger, J.H.Weber, J.Wentz, T.Wiegert, D.Wochele, J.Kempa, T.Wibig, J.Zabierowski, F.Badea, H.Bozdog, I.M.Brancis, M.Petcu, B.Vulpescu, A.Chilingarian, A.Vardanyan

Test of High-Energy Interaction Models using the Hadronic Core of EAS


1997RU08      Phys.Rev.Lett. 79, 3054 (1997)

B.-U.Runge, M.Dippel, G.Fillebock, K.Jacobs, U.Kohl, G.Schatz

Induced Magnetic Hyperfine Field at Ag Sites Near an Fe(100)/Ag(100) Interface

RADIOACTIVITY 111In(EC); measured γγ(θ, H); deduced induced magnetic hyperfine field at Ag sites near Fe(100)/Ag(100) interface.

doi: 10.1103/PhysRevLett.79.3054
Citations: PlumX Metrics


1996LO11      Hyperfine Interactions 97/98, 203 (1996)

J.Lohmuller, H.H.Bertschat, H.Granzer, H.Haas, G.Schatz, W.-D.Zeitz, and the ISOLDE Collaboration

PAC Investigation of 77Br → 77Se on Silicon Surfaces

RADIOACTIVITY 77Br(EC), (β+) [from 77Rb-decay chain]; measured γγ(θ, H); deduced quadrupole interaction, electric field gradients at (5/2)- level in 77Se.


1993KR25      Hyperfine Interactions 78, 261 (1993)

G.Krausch, R.Fink, K.Jacobs, U.Kohl, J.Lohmuller, B.Luckscheiter, R.Platzer, B.-U.Runge, U.Wohrmann, G.Schatz

Surface and Interface Studies with Perturbed Angular Correlations

RADIOACTIVITY 111In(EC); compiled, reviewed γγ(θ, H) data; deduced 111In/111Cd field gradient distribution relative width on different substitutional step sites.

doi: 10.1007/BF00568148
Citations: PlumX Metrics


1991KL02      Phys.Rev. C44, 2801 (1991)

N.Klay, F.Kappeler, H.Beer, G.Schatz, H.Borner, F.Hoyler, S.J.Robinson, K.Schreckenbach, B.Krusche, U.Mayerhofer, G.Hlawatsch, H.Lindner, T.von Egidy, W.Andrejtscheff, P.Petkov

Nuclear Structure of 176Lu and Its Astrophysical Consequences. I. Level Scheme of 176Lu

NUCLEAR REACTIONS 175Lu(n, γ), (n, e-), E=thermal; measured Eγ, Iγ, I(ce), γγ-coin. 175Lu(d, p), Ed=20.118 MeV; measured proton spectra. 176Lu deduced levels, J, π, T1/2, isomer, neutron separation energy.

doi: 10.1103/PhysRevC.44.2801
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22267.


1991KL03      Phys.Rev. C44, 2839 (1991)

N.Klay, F.Kappeler, H.Beer, G.Schatz

Nuclear Structure of 176Lu and Its Astrophysical Consequences. II. 176Lu, a Thermometer for Stellar Helium Burning

RADIOACTIVITY 176Lu; calculated temperature dependence of half-life under stellar conditions; deduced s-process temperature.

doi: 10.1103/PhysRevC.44.2839
Citations: PlumX Metrics


1987KL05      Hyperfine Interactions 34, 577 (1987)

T.Klas, J.Voigt, W.Keppner, R.Platzer, R.Wesche, G.Schatz

Electric Field Gradient at 111In on Cu(100) Surfaces and Its Utilization for Indium Surface Diffusion

RADIOACTIVITY 111In(EC); measured γγ(θ, H, t); deduced electric field gradient at 111In on Cu(100).

doi: 10.1007/BF02072778
Citations: PlumX Metrics


1987ME22      Hyperfine Interactions 38, 723 (1987)

G.Meisel, K.Bekk, H.Rebel, G.Schatz

Atomic Beam, Optogalvanic and Stored Ion Spectroscopy for Radioactive Isotopes

NUCLEAR MOMENTS 204,206,208,207Pb; measured hfs, isotope shifts. Laser induced resonance absorption.

NUCLEAR STRUCTURE 241,242m,243Am; measured optical isotope shifts. Laser induced resonances absorption.

doi: 10.1007/BF02394871
Citations: PlumX Metrics


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


1986AN06      Nucl.Phys. A451, 471 (1986)

M.Anselment, W.Faubel, S.Goring, A.Hanser, G.Meisel, H.Rebel, G.Schatz

The Odd-Even Staggering of the Nuclear Charge Radii of Pb Isotopes

RADIOACTIVITY 196,197,197m,211,214Pb; measured hfs, isotope shift; deduced hyperfine constants. 196,197,197m,198,199,200,201,202,202m,203,204,205,206,207,208,209,210,211,212,214Pb deduced nuclear charge radii, nuclear, odd-even staggering parameters, μ, quadrupole moment. Laser spectroscopic techniques, other data input.

doi: 10.1016/0375-9474(86)90071-0
Citations: PlumX Metrics


1986AN24      Phys.Rev. C34, 1052 (1986)

M.Anselment, K.Bekk, A.Hanser, H.Hoeffgen, G.Meisel, S.Goring, H.Rebel, G.Schatz

Charge Radii and Moments of Tin Nuclei by Laser Spectroscopy

NUCLEAR MOMENTS 112,114,115,116,117,118,119,120,122,124Sn; measured isotope shift, hfs; deduced rms charge radius, μ, electric quadrupole moments. Laser spectroscopy.

RADIOACTIVITY 117m,110,111,113,121,121m,123,125Sn; measured isotope shift, hfs; deduced rms charge radius differences, magnetic dipole, electric quadrupole moments. Laser spectroscopy.

doi: 10.1103/PhysRevC.34.1052
Citations: PlumX Metrics


1985RA28      Phys.Lett. 163B, 327 (1985)

M.H.Rafailovich, S.Vajda, E.Dafni, G.Schatz, S.Rolston, S.Y.Zhu, G.D.Sprouse

A g-Factor Measurement of the 239Am Fission Isomer

NUCLEAR REACTIONS 237Np(α, 2n), E=tandem; measured γ(θ, H, t). 239Am deduced fission isomer g.

doi: 10.1016/0370-2693(85)90290-4
Citations: PlumX Metrics


1984DR09      Phys.Lett. 149B, 311 (1984)

G.D.Dracoulis, T.Lonnroth, S.Vajda, O.C.Kistner, M.H.Rafailovich, E.Dafni, G.Schatz

Quadrupole Moments of the 12+ Isomers in 188Hg and 190Hg

NUCLEAR REACTIONS 164Dy(28Si, 4n), E=136 MeV; 175Lu(19F, 4n), E=91 MeV; measured γ(θ, H, t) vs temperature. 188,190Hg deduced isomer quadrupole moment, configuration.

doi: 10.1016/0370-2693(84)90413-1
Citations: PlumX Metrics


1983DA01      Nucl.Phys. A394, 245 (1983)

E.Dafni, M.H.Rafailovich, T.Marshall, G.Schatz, G.D.Sprouse

Electric Quadrupole Moments of High Spin Isomers in 209Po and 210Po

NUCLEAR REACTIONS 207,208Pb(α, xn), E=24, 35 MeV; measured γγ(θ, H, t). 209,210Po levels deduced quadrupole moment. Isomer recoil implantation in Sn.

doi: 10.1016/0375-9474(83)90171-9
Citations: PlumX Metrics


1983DA29      Hyperfine Interactions 15/16, 101 (1983)

E.Dafni, F.D.Davidovsky, A.Gelberg, M.Haas, E.Naim, G.Schatz

Electric Quadrupole Interaction of Ce Isomers in Tin

NUCLEAR REACTIONS 122,124Sn(16O, 4n), 124Sn(18O, 4n), E=76 MeV; measured γ(θ, H, t) in Sn. 138,136,134Ce deduced isomer quadrupole moments, ratios, electric field gradient temperature dependence in Sn.

doi: 10.1007/BF02159726
Citations: PlumX Metrics


1983KE13      Hyperfine Interactions 15/16, 203 (1983)

W.Keppner, W.Korner, G.Schatz

Isotopic Mass Effect of the Electric Field Gradient in Noncubic Metals

RADIOACTIVITY 111In(EC); measured γγ(θ, H, t); deduced 111Cd electric field gradient in Cd isotopes.

doi: 10.1007/BF02159738
Citations: PlumX Metrics


1983KE16      Hyperfine Interactions 15/16, 853 (1983)

W.Keppner, W.Korner, G.Schatz

Structural Phase Transition in Cadmium Titanate Observed by Electric Quadrupole Interaction

RADIOACTIVITY 111In(EC); measured γγ(θ, H); deduced quadrupole interactions at 111Cd vs T in CdTiO3.

doi: 10.1007/BF02147381
Citations: PlumX Metrics


1983KL12      Hyperfine Interactions 15/16, 433 (1983)

T.Klas, P.Heubes, G.Schatz

Electric Field Gradients in Dilute Aluminium Alloys

RADIOACTIVITY 111In(EC); measured γγ(θ, H, t); deduced electric field gradients in PdAl alloys.

doi: 10.1007/BF02159784
Citations: PlumX Metrics


1983RA36      Hyperfine Interactions 15/16, 43 (1983)

M.H.Rafailovich, E.Dafni, G.Schatz, S.Y.Zhu, K.Dybdal, S.Vajda, C.Alonso-Arias, S.Rolston, G.D.Sprouse

g-Factor Measurements of Fission Isomers

RADIOACTIVITY 239mAm, 237Pu(SF) [from 235U, 237Np(α, 2n), E=25 MeV]; measured fission fragment anisotropy, isomer T1/2, g.

NUCLEAR REACTIONS 235U, 237Np(α, 2n), E=25 MeV; measured γ(θ, H, t). 239Am, 237Pu deduced fission isomer g, T1/2.

doi: 10.1007/BF02159713
Citations: PlumX Metrics


1983TH03      J.Phys.(London) G9, 443 (1983)

R.C.Thompson, M.Anselment, K.Bekk, S.Goring, A.Hanser, G.Meisel, H.Rebel, G.Schatz, B.A.Brown

High-Resolution Measurements of Isotope Shifts and Hyperfine Structure in Stable and Radioactive Lead Isotopes

RADIOACTIVITY 210Pb; 212Pb [from 232Th decay]; 205Pb [from 204Pb(n, γ)]; 209Pb [from 208Pb(d, p)]; 198,199,200,202Pb [from Hg(α, xn), E=104 MeV]; 201,202m,203Pb [from Tl(d, xn), E=38, 48 MeV]; measured hfs, isotope shifts. 201,202m,205,209Pb deduced μ, quadrupole moment, rms charge radii. 199Pb level deduced J, π, μ, quadrupole moment, rms charge radius. 198,210,212Pb deduced rms charge radius. Droplet model, Skyrme interactions.

NUCLEAR MOMENTS 204,206,207Pb; measured hfs, isotope shifts; deduced rms charge radii. Droplet model, Skyrme interactions.

doi: 10.1088/0305-4616/9/4/010
Citations: PlumX Metrics


1982AN15      Phys.Rev. C26, 2194 (1982)

A.Andl, K.Bekk, S.Goring, A.Hanser, G.Nowicki, H.Rebel, G.Schatz, R.C.Thompson

Isotope Shifts and Hyperfine Structure of the 4s2 1S0-4s4p 1P1 Transition in Calcium Isotopes

NUCLEAR MOMENTS 40,42,43,44,46,48Ca, 41,45,47Ca [from 40,44,46Ca(n, γ), E=thermal]; measured hfs, isotope shifts. 41,45,47Ca deduced hyperfine constants, rms charge radii differences, μ. 43Ca deduced hyperfine constants, rms charge radii differences. 40,42,44,46,48Ca deduced rms charge radii differences. Laser spectroscopy, resonance fluorescence technique.

doi: 10.1103/PhysRevC.26.2194
Citations: PlumX Metrics


1982DA17      Nucl.Phys. A383, 421 (1982)

E.Dafni, C.Broude, F.D.Davidovsky, M.Hass, G.Schatz

Magnetic Moments of Isomeric Bandheads in Transitional Nuclei: 119I and 192Tl

NUCLEAR REACTIONS 109Ag(13C, 3n), E=52 MeV; 181Ta(16O, 5n), E=100 MeV; measured Iγ(θ, t). 119I level deduced g, T1/2. 192Tl level deduced g, quadrupole moment, T1/2.

doi: 10.1016/0375-9474(82)90085-9
Citations: PlumX Metrics


1982RA04      Phys.Rev.Lett. 48, 982 (1982); Erattum Phys.Rev.Lett. 49, 244 (1982)

M.H.Rafailovich, E.Dafni, G.Schatz, S.Y.Zhu, K.Dybdal, S.Vajda, C.Alonso-Arias, G.D.Sprouse

Measurement of the g Factor of the 237Pu Short-Lived Fission Isomer

NUCLEAR REACTIONS 235U(α, 2n), E=25.2 MeV; measured γ(θ, H, T). 237Pu deduced fission isomer g, Nilsson configuration.

doi: 10.1103/PhysRevLett.48.982
Citations: PlumX Metrics


1982SC27      Z.Phys. B49, 23 (1982)

G.Schatz, E.Dafni, H.H.Bertschat, C.Broude, F.D.Davidovsky, M.Hass

Electric Quadrupole Interaction of 192Tl(8-) Nuclei in Hexagonal Tl and in Tetragonal In Metals

RADIOACTIVITY 192Tl(EC), (β+) [from 181Tl(16O, 5n), E=100 MeV]; measured γ(θ, H, t); deduced isomer electric quadrupole interaction, quadrupole moment. Recoil implantation, noncubic hosts.

doi: 10.1007/BF01312965
Citations: PlumX Metrics


1981KE10      Hyperfine Interactions 9, 293 (1981)

W.Keppner, W.Korner, P.Heubes, G.Schatz

Temperature Dependence of the Electric Field Gradient at 111Cd in Ga- and Bi-Metal

RADIOACTIVITY 111In; measured γγ(θ, T) in Ga, Bi; deduced 111Cd electric field gradient temperature dependence.

doi: 10.1007/BF01020934
Citations: PlumX Metrics


1979BE25      Z.Phys. A291, 219 (1979)

K.Bekk, A.Andl, S.Goring, A.Hanser, G.Nowicki, H.Rebel, G.Schatz

Laserspectroscopic Studies of Collective Properties of Neutron Deficient Ba Nuclei

NUCLEAR MOMENTS 126,129m,129,135mBa; measured optical isotope shift, hfs. 126,129m,129,135mBa deduced differences of rms charge radii, μ, quadrupole moment. Laser spectroscopy. Quasiparticle-plus-triaxial rotor, droplet model.

doi: 10.1007/BF01409187
Citations: PlumX Metrics


1979HE14      Hyperfine Interactions 7, 93 (1979)

P.Heubes, W.Keppner, G.Schatz

Quadrupole Interaction at 111Cd Nuclei in Single-Crystalline Thallium

RADIOACTIVITY 111In; measured γγ(θ, H, t) in Tl. 111Cd deduced temperature dependence of quadrupole interaction.

doi: 10.1007/BF01021495
Citations: PlumX Metrics


1979SH03      Phys.Rev. C19, 1324 (1979)

R.E.Shroy, A.K.Gaigalas, G.Schatz, D.B.Fossan

High-Spin States in Odd-Mass 113-119Sb: ΔJ = 1 Bands on 9/2+ Proton-Hole States

NUCLEAR REACTIONS 110,112,114,116Cd(6Li, 3n), E=24-34 MeV; measured γγ-coin, γ(E, θ, t), γ(θ, H, t), γ-branching. 113,115,117,119Sb deduced levels, γ multipolarities, J, π, T1/2. 115mSb deduced g-factor. Enriched target.

doi: 10.1103/PhysRevC.19.1324
Citations: PlumX Metrics


1978NO09      Phys.Rev. C18, 2369 (1978)

G.Nowicki, K.Bekk, S.Goring, A.Hanser, H.Rebel, G.Schatz

Nuclear Charge Radii and Nuclear Moments of Neutron Deficient Ba Isotopes from High Resolution Laser Spectroscopy

NUCLEAR MOMENTS 128,131,133Ba; measured isotope shift, hfs, J, nuclear charge radii. Laser spectroscopy.

doi: 10.1103/PhysRevC.18.2369
Citations: PlumX Metrics


1977NO04      Phys.Rev.Lett. 39, 332 (1977)

G.Nowicki, K.Bekk, S.Goring, H.Hanser, H.Rebel, G.Schatz

Nuclear Radii and Magnetic Moments of 128,131Ba from High-Resolution Laser Spectroscopy

NUCLEAR MOMENTS 128,131Ba; measured isotope shift, hfs. 128,130,131Ba deduced differences of mean-square charge radii. 131Ba deduced μ. Doppler-free laser spectroscopy.

doi: 10.1103/PhysRevLett.39.332
Citations: PlumX Metrics


1976SJ01      Phys.Rev. C14, 1023 (1976)

T.P.Sjoreen, G.Schatz, S.K.Bhattacherjee, B.A.Brown, D.B.Fossan, P.M.S.Lesser

High-Spin States and Neutron-Hole Influence in 209At

NUCLEAR REACTIONS 206Pb(6Li, 3nγ), E=29-34 MeV; measured σ(Eγ, θ, H, t), γγ-coin. 209At deduced levels, J, π, λ, T1/2, B(E2), g.

doi: 10.1103/PhysRevC.14.1023
Citations: PlumX Metrics


1975CH09      Nucl.Phys. A239, 253 (1975)

J.Christiansen, G.Hempel, H.Ingwersen, W.Klinger, G.Schatz, W.Witthuhn

Investigation of Delayed Fission in 236U

NUCLEAR REACTIONS 235U(d, pF), E=11 MeV; measured prompt, delayed fission. 236mU(SF) deduced T1/2, isomeric to prompt fission ratio. 232Th(d, F), E=11 MeV; measured prompt fission.

doi: 10.1016/0375-9474(75)90449-2
Citations: PlumX Metrics


1975GA11      Phys.Rev.Lett. 35, 555 (1975)

A.K.Gaigalas, R.E.Shroy, G.Schatz, D.B.Fossan

Deformed 9/2+ States and ΔJ = 1 Rotational Bands in 113,115,117,119Sb Nuclei

NUCLEAR REACTIONS 110,112,114,116Cd(6Li, 3nγ), E < 35 MeV; measured σ(Eγ, θ), γγ-coin, γ(t). 113,115,117,119Sb deduced levels, K, J, π.

doi: 10.1103/PhysRevLett.35.555
Citations: PlumX Metrics


1975IN01      Phys.Rev. C11, 243 (1975)

H.Ingwersen, W.Klinger, G.Schatz, W.Witthuhn

Nuclear g Factors of the (21/2)- and the (29/2)+ States in 211At

NUCLEAR REACTIONS 209Bi(α, 2n), E=30, 33 MeV; measured γ(θ, H, t). 211At levels deduced g.

doi: 10.1103/PhysRevC.11.243
Citations: PlumX Metrics


1975KL02      Nucl.Phys. A240, 137 (1975)

H.Klewe-Nebenius, D.Habs, K.Wisshak, H.Faust, G.Nowicki, S.Goring, H.Rebel, G.Schatz, M.Schwall

The Level Scheme of 137Pr; Evidence for Prolate Nuclear Shape

RADIOACTIVITY 137Nd[from 141Pr(α, 7np)]; measured Eγ, Iγ, γγ-coin, E(ce), I(ce); deduced ICC. 137Pr deduced levels, J, π. Mass separated sources.

NUCLEAR REACTIONS 139La(α, 6nγ), E=70-104 MeV; measured σ(E, Eγ, θ), E(ce), I(ce), γ(t); deduced ICC. 137Pr deduced levels, J, π, T1/2. Natural target. Ge(Li), Si(Li) detectors with magnetic filter.

doi: 10.1016/0375-9474(75)90442-X
Citations: PlumX Metrics


1975SC25      Phys.Lett. 57B, 231 (1975)

G.Schatz, R.Brenn, D.B.Fossan

Stroboscopic Observation of Quadrupole Hyperfine Interactions

NUCLEAR REACTIONS 66Zn(α, n), E=16 MeV; measured γγ(θ, H, t). 69mGe deduced hyperfine frequency.

doi: 10.1016/0370-2693(75)90062-3
Citations: PlumX Metrics


1974HE22      Nucl.Phys. A234, 81 (1974)

P.Heubes, H.Ingwersen, H.G.Johann, W.Klinger, W.Loeffler, G.Schatz

The Magnetic Moment of the 9/2+ State in 85Rb, Mesonic Contributions in the Z = 37 Region and Blocking of Core Polarization in the 1f5/2 Proton Shell

NUCLEAR REACTIONS 85Rb(d, pn), E=11 MeV; measured (θ, H, t). 85Rb deduced g. Natural target.

doi: 10.1016/0375-9474(74)90380-7
Citations: PlumX Metrics


1973HE10      Phys.Rev. C7, 2128 (1973)

P.Heubes, H.Ingwersen, W.Klinger, W.Lampert, W.Loeffler, G.Schatz, W.Witthuhn

Magnetic Moment of the 1.8-μs State in 122Sb

NUCLEAR REACTIONS 122Sn(p, nγ), E=11 MeV; measured γ(θ, H, t). 122Sb level deduced μ, T1/2.

doi: 10.1103/PhysRevC.7.2128
Citations: PlumX Metrics


1972CH34      Rev.Roum.Phys. 17, 751 (1972)

J.Christiansen, P.Heubes, H.Ingwersen, H.G.Johann, W.Klinger, W.Kreische, W.Lampert, W.Loeffler, G.Schatz, W.Witthuhn

Magnetic Moments of Isomeric States in 66Ga, 78Br and 81Br

NUCLEAR MOMENTS 66mGa, 78mBr, 81mBr; measured g.


1972HA08      Nucl.Phys. A182, 1 (1972)

G.Hauser, R.Lohken, G.Nowicki, H.Rebel, G.Schatz, G.Schweimer, J.Specht

(α, τ) and (α, t) Reactions with 104 MeV α-Particles

NUCLEAR REACTIONS 12C, 40Ca(α, 3He0), (α, t0), (α, α0); 27Al(α, t0), (α, t1), (α, α0);E=104 MeV; measured σ(θ); deduced normalization factors. 13C, 13N, 28Si, 41Ca, 41Sc deduced absolute S.

doi: 10.1016/0375-9474(72)90198-4
Citations: PlumX Metrics


1972HA23      Z.Phys. 250, 179 (1972)

D.Habs, H.Klewe-Nebenius, R.Lohken, S.Goring, J.van Klinken, H.Rebel, G.Schatz

Quasirotational Groundstate Bands of Even-Even Nuclei with 50 < N, Z < 82

RADIOACTIVITY 142Eu, 140Eu; measured Eγ, Iγ, I(ce), γγ-coin. 140Eu; measured T1/2. 142Sm deduced levels, J, π.

NUCLEAR REACTIONS 144Sm, 142Nd, 141Pr, 136,140Ce, 139La(α, xnypzα), E=45-104 MeV; measured σ(E;Eγ), αγ-delay. 140Sm, 142Sm, 144Gd, 136Nd deduced levels, J, π, quasirotational ground-state band structure.

doi: 10.1007/BF01386948
Citations: PlumX Metrics


1972HE11      Nucl.Phys. A188, 417 (1972)

P.Heubes, H.G.Johann, W.Klinger, W.Kreische, W.Lampert, W.Loeffler, G.Schatz, W.Witthuhn

The Magnetic Moment of the First Excited State in 66Ga

NUCLEAR REACTIONS 66Zn(p, nγ), Ep=10 MeV; measured pγ(θ, H, t). 66Ga deduced T1/2, g. Natural target.

doi: 10.1016/0375-9474(72)90066-8
Citations: PlumX Metrics


1972RE05      Nucl.Phys. A182, 145 (1972)

H.Rebel, G.W.Schweimer, G.Schatz, J.Specht, R.Lohken, G.Hauser, D.Habs, H.Klewe-Nebenius

Quadrupole and Hexadecapole Deformation of 2s-1d Shell Nuclei

NUCLEAR REACTIONS 20Ne, 22Ne, 24Mg, 26Mg, 28Si(α, α), (α, α'), E=104 MeV; measured σ(θ); deduced optical potentials. 20,22Ne, 24,26Mg, 28Si deduced quadrupole, hexadecapole deformation parameters by a coupled-channel analysis. Enriched targets.

doi: 10.1016/0375-9474(72)90207-2
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0215.


1972RE15      Z.Phys. 256, 258 (1972)

H.Rebel, R.Lohken, G.W.Schweimer, G.Schatz, G.Hauser

Elastische und Inelastische Streuung von 104 MeV Alpha-Teilchen an 58,60,62,64Ni

NUCLEAR REACTIONS 58,60,62,64Ni(α, α), (α, α'), E=104 MeV; measured σ(θ); deduced optical model parameters. 58,60,62,64Ni deduced β(L), B(E2), rms radii.

doi: 10.1007/BF01392099
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0255.


1971CH28      Phys.Lett. 35B, 501 (1971); Priv.Comm. (July 1973)

J.Christiansen, H.Ingwersen, H.G.Johann, W.Klinger, W.Kreische, W.Lampert, G.Schatz, W.Witthuhn

The g-Factor of the Isomeric 9/2+ State of 81Br

NUCLEAR REACTIONS 80Se(d, nγ), E=10 MeV; measured dγ(θ, H, t), dγ-delay. 81Br level deduced g, T1/2. Stroboscopic method.

doi: 10.1016/0370-2693(71)90382-0
Citations: PlumX Metrics


1971HA49      Lett.Nuovo Cim. 2, 405 (1971)

G.Hauser, R.Lohken, G.Nowicki, H.Rebel, G.Schatz, W.Schweimer, J.Specht

Experimental Determination of the Normalization Factors for (α, tau) and (α, t) Reactions

NUCLEAR REACTIONS 40Ca(α, 3He), (α, t), E=104 MeV; measured σ(θ); deduced normalization factors.

doi: 10.1007/BF02780421
Citations: PlumX Metrics


1971IN04      Nucl.Phys. A171, 241 (1971)

H.Ingwersen, W.Klinger, W.Kreische, W.Lampert, G.Schatz, W.Witthuhn, E.A.Ivanov

Lifetime and g-Factor of the 181 keV Level in 78Br

NUCLEAR REACTIONS 78Se(p, nγ), Ep=5.5, 10.0 MeV; measured pγ(θ, H, t). 78Br deduced levels, T1/2, g. Natural, enriched targets.

doi: 10.1016/0375-9474(71)90021-2
Citations: PlumX Metrics


1971LO17      Z.Phys. 245, 425 (1971)

R.Lohken, H.Rebel, G.Schatz

A Numerical Method of Analyzing Beta Decay Measurements and its Application to the 1- → 0+ Transitions of 170Tm, 186Re and 210Bi

RADIOACTIVITY 170Tm, 186Re, 210Bi; measured nothing; analyzed available data; deduced nuclear matrix elements.


1971RE09      Phys.Rev.Lett. 26, 1190 (1971)

H.Rebel, G.W.Schweimer, J.Specht, G.Schatz, R.Lohken, D.Habs, G.Hauser, H.Klewe-Nebenius

Hexadecapole Moments of 20Ne and 28Si from Scattering of 104-MeV α Particles

NUCLEAR REACTIONS 20Ne, 28Si(α, α'), E=104 MeV; measured σ(θ). 20Ne, 28Si deduced Q20, deformation parameters β2, β4.

doi: 10.1103/PhysRevLett.26.1190
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0215.


1971SP08      Nucl.Phys. A171, 65 (1971)

J.Specht, G.W.Schweimer, H.Rebel, G.Schatz, R.Lohken, G.Hauser

Evidence for Oblate Shape of 12C from Inelastic α-Particle Scattering

NUCLEAR REACTIONS 12C(α, α'), E=104 MeV; measured σ(Eα', θ). 12C deduced deformation lengths, electrical quadrupole, hexadecapole moments.

doi: 10.1016/0375-9474(71)90363-0
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0216.


1971VA22      Z.Phys. 246, 369 (1971)

J.van Klinken, S.Goring, D.Habs, M.von Hartrott, H.Klewe-Nebenius, R.Lohken, H.Rebel, G.Schatz

139Sm, a New Nuclide of Relevance for the Systematics of the N = 77 Isomers

RADIOACTIVITY 139Sm, 139mSm, 137mNd, 135mCe; measured T1/2, Eγ, Iγ, I(ce). 135Ce, 137Nd, 139Sm deduced levels, ICC, γ-multipolarity.

doi: 10.1007/BF02115801
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1970SP01      Nucl.Phys. A143, 373 (1970)

J.Specht, H.Rebel, G.Schatz, G.W.Schweimer, G.Hauser, R.Lohken

Inelastic Scattering of 104 MeV α-Particles on 12C, 20Ne and 64Ni

NUCLEAR REACTIONS 12C, 20Ne, 64Ni(α, α'), E = 104 MeV; measured σ(Eα', θ); deduced reduced matrix elements. 12C, 20Ne, 64Ni levels deduced deformations, mixing parameters. Enriched targets.

doi: 10.1016/0375-9474(70)90571-3
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0885.


1969HA14      Nucl.Phys. A128, 81 (1969)

G.Hauser, R.Lohken, H.Rebel, G.Schatz, G.W.Schweimer, J.Specht

Elastic Scattering of 104 MeV Alpha Particles

NUCLEAR REACTIONS 6Li, 9Be, 12C, 14N, 16O, 20Ne, 40Ar, 64Ni, 90Zr, 124Sn, 208Pb, 209Bi(α, α), E=104 MeV; measured σ(θ); deduced phase shifts, optical potentials. Enriched targets.

doi: 10.1016/0375-9474(69)90980-4
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0216.


1965LO06      Z.Physik 187, 1 (1965)

R.Lohken, H.Rebel, G.Schatz

Relativmessung der Elektronenpolarisation beim β-Zerfall: Au199 und P32

NUCLEAR STRUCTURE 199Au, 32P; measured not abstracted; deduced nuclear properties.


1964LO11      Z.Physik 181, 396 (1964)

R.Lohken, H.Rebel, G.Schatz

Relativmessung der Elektronenpolarisation beim β-Zerfall: Re186 und P32

NUCLEAR STRUCTURE 186Re; measured not abstracted; deduced nuclear properties.


1964RE06      Z.Physik 180, 392 (1964)

H.Rebel, G.Schatz, W.Buhring

Relativmessung der Elektronenpolarisation beim β-Zerfall: Tl204 und P32

NUCLEAR STRUCTURE 32P, 204Tl; measured not abstracted; deduced nuclear properties.

doi: 10.1007/BF01380524
Citations: PlumX Metrics


1964SC11      Z.Physik 177, 495 (1964)

G.Schatz, H.Rebel, W.Buhring

Relativmessung der Elektronenpolarisation beim β-Zerfall: RaE(Bi210)-P32

NUCLEAR STRUCTURE 210Bi, 32P; measured not abstracted; deduced nuclear properties.

doi: 10.1007/BF01375205
Citations: PlumX Metrics


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