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NSR database version of April 27, 2024.

Search: Author = E.Matthias

Found 45 matches.

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1993GU07      Phys.Rev. A47, 4725 (1993)

J.Gudde, A.Klinkmuller, P.J.West, E.Matthias

Second-Order Magnetic Contributions to the Hyperfine Splitting of the 5snd 1D2 States in 87Sr

NUCLEAR MOMENTS 87Sr; measured hfs; deduced hyperfine interaction parameters.

doi: 10.1103/PhysRevA.47.4725
Citations: PlumX Metrics


1982RI03      Z.Phys. A306, 11 (1982)

H.Rinneberg, J.Neukammer, E.Matthias

Isotope Shifts of Perturbed 6sns 1S0 and 3S1 Rydberg States of Odd Barium Isotopes

NUCLEAR MOMENTS 135,137,138Ba; measured optical isotope shifts.

doi: 10.1007/BF01413401
Citations: PlumX Metrics


1981BE42      Z.Phys. A301, 93 (1981)

R.Beigang, E.Matthias, A.Timmermann

Odd-Even Staggering of Isotope Shifts in the 5 sns 1S0 Rydberg Series of Strontium

NUCLEAR MOMENTS 84,86,87,88Sr; measured isotope shift; deduced odd-even staggering effect. High resolution two-photon spectroscopy.

doi: 10.1007/BF01412470
Citations: PlumX Metrics


1981GE06      Hyperfine Interactions 9, 175 (1981)

H.Gerhardt, F.Jeschonnek, W.Makat, E.Matthias, H.Rinneberg, F.Schneider, A.Timmermann, R.Wenz, P.J.West

Nuclear Charge Radii and Nuclear Moments of Kr and Xe Isotopes by High Resolution Laser Spectroscopy

NUCLEAR MOMENTS 78,80,82,84,86Kr, 124,126,128,130,132,134,136Xe; measured optical isotope shift; deduced nuclear charge radius mass dependence. 85,83Kr, 129,131Xe; measured hfs; deduced coupling constants. 85,83Kr deduced quadrupole moment, μ ratios. High resolution laser spectroscopy, Doppler free measurement.

doi: 10.1007/BF01020915
Citations: PlumX Metrics


1981WE15      Z.Phys. A303, 87 (1981)

R.Wenz, A.Timmermann, E.Matthias

Subshell Effect in Mean Square Charge Radii of Stable Even Cadmium Isotopes

NUCLEAR MOMENTS 106,108,110,112,114,116Cd; measured optical isotope shifts; deduced rms charge radii, subshell effects. Doppler-free saturation spectroscopy.

doi: 10.1007/BF01420264
Citations: PlumX Metrics


1980WE04      Z.Phys. A295, 303 (1980)

R.Wenz, E.Matthias, H.Rinneberg, F.Schneider

Further Evidence for a Linear Relationship between Changes in Nuclear Charge Radii and Binding Energy Per Nucleon

NUCLEAR MOMENTS 126,128,130,132,134,136,138Ba, 124,126,128,130,132,134,136Xe; analyzed isotope shift data; deduced linear variation of charge radii with binding energy per nucleon.

doi: 10.1007/BF01412212
Citations: PlumX Metrics


1979GE06      Z.Phys. A292, 7 (1979)

H.Gerhardt, E.Matthias, H.Rinneberg, F.Schneider, A.Timmermann, R.Wenz, P.J.West

Changes in Nuclear Mean Square Charge Radii of Stable Krypton Isotopes

ATOMIC PHYSICS 78,80,82,84,86Kr; measured isotope shift; deduced changes in mean-square charge radii. Optical transitions, polarization laser spectroscopy.

doi: 10.1007/BF01434624
Citations: PlumX Metrics


1978GE15      Z.Phys. A288, 327 (1978)

H.Gerhardt, E.Matthias, F.Schneider, A.Timmermann

Isotope Shifts and Hyperfine Structure of the 6s-7p Transitions in the Cesium Isotopes 133, 135, and 137

NUCLEAR STRUCTURE 133,135,137Cs; measured hfs; deduced isotope shift. Laser spectrometer.

doi: 10.1007/BF01417714
Citations: PlumX Metrics


1978WE18      Z.Phys. A288, 369 (1978)

P.J.West, E.Matthias

Frequency Modulation of the 6.2 keV Mossbauer States of 181Ta

NUCLEAR REACTIONS 181Ta(γ, γ), E=6.2 keV; measured frequency modulated Mossbauer spectra. 181Ta levels deduced g-factor ratio.

doi: 10.1007/BF01417720
Citations: PlumX Metrics


1977GE05      Phys.Lett. 61A, 377 (1977)

H.Gerhardt, R.Wenz, E.Matthias

Isotope Shifts of the 557 nm Transition in Even Krypton Isotopes

NUCLEAR MOMENTS 78,80,82,84,86Kr; measured isotope shift.

doi: 10.1016/0375-9601(77)90338-3
Citations: PlumX Metrics


1976BO28      Z.Phys. A278, 133 (1976)

R.Bohm, R.Keitel, W.Klinger, W.Witthuhn, W.L.Randolph, E.Matthias

The Magnetic Moment of the First 2+ State in 22Ne

NUCLEAR REACTIONS 4He(19F, 22Ne), E=41.2 MeV; measured recoil 22Ne, γ(t). 22Ne level deduced g.


1975MA02      Nucl.Phys. A237, 182 (1975)

E.Matthias, E.Recknagel, O.Hashimoto, S.Nagamiya, K.Nakai, T.Yamazaki, Y.Yamazaki

The g-Factor Measurement for the 8+ Isomeric State of 86Sr Produced in Kr Gas

NUCLEAR REACTIONS Kr(α, 2n), E=22 MeV; measured αγ(θ, H, t). 86mSr deduced g. Stroboscopic method, natural Kr gas target.

doi: 10.1016/0375-9474(75)90471-6
Citations: PlumX Metrics


1975RA36      Hyperfine Interactions 1, 145 (1975)

W.L.Randolph, J.Asher, J.W.Koen, P.Rowe, E.Matthias

A Measurement of the Ground State Hyperfine Splitting for Li-Like Fluorine Ions by Nuclear Quantum Beats

NUCLEAR REACTIONS 19F(α, α'), E=12.75, 15.6 MeV; measured γγ(θ, H, t). 19F deduced hyperfine splitting.

doi: 10.1007/BF01022448
Citations: PlumX Metrics


1971BR03      Phys.Lett. 34B, 54 (1971)

N.Brauer, B.Focke, B.Lehmann, E.Matthias, D.Riegel

In-Beam Nuclear Magnetic Resonance of the 159 μs Level in 115Sn

NUCLEAR REACTIONS 115In(p, nγ), E=5.9 MeV; measured pγ(θ, H, t). 115Sn level deduced μ.

doi: 10.1016/0370-2693(71)90505-3
Citations: PlumX Metrics


1971BR50      Phys.Lett. 37B, 186 (1971)

N.Brauer, B.Focke, B.Lehmann, E.Matthias, K.Nishiyama, D.Riegel

Time-Differential Observation of NMR by Perturbed Angular Correlation

NUCLEAR REACTIONS 78Se(p, n), E=6.9 MeV; measured pγ(θ, H, t), NMR in SeTl.

doi: 10.1016/0370-2693(71)90047-5
Citations: PlumX Metrics


1968MA56      Proc.Intern.Conf.Hyperfine Struct.Nucl.Radiations, Asilomar, Pacific Grove, Calif. (1967), North-Holland Publ.Co., Amsterdam (1968)

E.Matthias, D.A.Shirley


1968SA07      Phys.Rev.Letters 21, 961 (1968)

C.Sauer, E.Matthias, R.L.Mossbauer

Recoilless Resonance Absorption and Hyperfine Structure of the 6.2-keV State in 181Ta

NUCLEAR REACTIONS 181Ta(γ, γ), E=6.2 keV; measured Mossbauer effect. 181Ta level deduced μ, isomer shift.

doi: 10.1103/PhysRevLett.21.961
Citations: PlumX Metrics


1968TR11      Proc.Intern.Conf.Hyperfine Struct.Nucl.Radiations, Asilomar, Pacific Grove, Calif. (1967), E.Matthias, D.A.Shirley, Eds., North-Holland Publ.Co., Amsterdam, p.145 (1968)

W.J.Treytl, E.Matthias

g-Factor of the 243-keV Level in 86Y

RADIOACTIVITY 86Zr; measured γγ(θ, H, t). 86Y levels deduced g, T1/2.


1968YA08      Phys.Rev. 175, 1476 (1968)

T.Yamazaki, E.Matthias

g-Factor Measurement of a Three-Particle Isomeric State of 209Po Following Pulsed Generation in (α, xn) Reactions

NUCLEAR STRUCTURE 209Po; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.175.1476
Citations: PlumX Metrics


1967NE02      Nucl.Phys. A95, 357 (1967)

J.O.Newton, F.S.Stephens, R.M.Diamond, K.Kotajima, E.Matthias

Angular Distributions of Gamma Rays Produced in Reactions with Heavy Ions

NUCLEAR REACTIONS 184W(α, 2nγ), E = 20-34 MeV; 182W, 186W(α, 2nγ), E = 27 MeV; 159Tb, 165Ho, 181Ta(11B, 4nγ), E = 54 MeV, (14N, 5nγ), E = 93 MeV; 159Tb(19F, 4nγ), E = 92 MeV; measured σ(Eγ, θ). 166Yb, 168,172Hf, 174W, 184,186,188Os, 188Pt, 190Hg deduced levels, alignment, J. Enriched, natural targets.

doi: 10.1016/0375-9474(67)90507-6
Citations: PlumX Metrics


1966DI06      Phys.Rev.Lett. 16, 1205 (1966)

R.M.Diamond, E.Matthias, J.O.Newton, F.S.Stephens

Nuclear Alignment in Heavy-Ion Reactions

NUCLEAR REACTIONS 197Au(α, 2nγ), E not given; measured σ(Eγ, θ(γ)). 199Tl deduced levels, J, π.

doi: 10.1103/PhysRevLett.16.1205
Citations: PlumX Metrics


1966MA54      Nucl.Instr.Methods 45, 309 (1966)

E.Matthias, D.A.Shirley

Digital Analysis of Perturbed Angular Correlations

NUCLEAR STRUCTURE 100Rh; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-554X(66)90306-5
Citations: PlumX Metrics


1966MA64      Phys.Rev.Letters 16, 974 (1966)

E.Matthias, D.A.Shirley, M.P.Klein, N.Edelstein

Detection of Nuclear Magnetic Resonance in a 235-nsec Nuclear State by Perturbed Angular Correlations

RADIOACTIVITY 100Pd; measured γγ(θ, H). 100Rh; deduced hyperfine field for Rh in Ni.

doi: 10.1103/PhysRevLett.16.974
Citations: PlumX Metrics


1965FR15      Phys.Letters 15, 163 (1965)

R.B.Frankel, J.Huntzicker, E.Matthias, S.S.Rosenblum, D.A.Shirley, N.J.Stone

Sign Change of Induced Hyperfine Fields in the 5p shell

NUCLEAR STRUCTURE 125Te; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.15.958
Citations: PlumX Metrics


1965KA02      Nucl.Phys. 61, 582(1965)

E.Karlsson, E.Matthias, S.Gustafsson, K.Johansson, A.G.Svensson, S.Ogaza, P.da Rocha Andrade

The Magnetic Moment of the 3/2+ State in Tl203 and the Question of Core Excitations

RADIOACTIVITY 203Pb[from 203Tl(d, 2n)] measured γγ(θ), γγ(θ, H). 203Tl deduced μ 0.279 level. Natural target.

doi: 10.1016/0029-5582(65)90608-5
Citations: PlumX Metrics


1965KA05      Nucl.Phys. 64, 8 (1965); E.Karlsson - Priv.Comm. (April 1972)

E.Karlsson, E.Matthias, A.G.Svensson, K.Johansson

The Magnetic Moment of the 9/2+ Rotational State in Lu175

RADIOACTIVITY 175Yb[from 174Yb(n, γ)]; measured γγ(θ, H), viscosity. 175Lu [14 keV level] deduced g, μ. Enriched target.

doi: 10.1016/0029-5582(65)90839-4
Citations: PlumX Metrics


1965MA11      Phys.Rev.Letters 14, 46 (1965)

E.Matthias, S.S.Rosenblum, D.A.Shirley

Influence of a Randomly Oriented Magnetic Field on Angular Correlations

NUCLEAR STRUCTURE 111In; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.14.46
Citations: PlumX Metrics


1965MA27      Phys.Rev. 139, B532 (1965)

E.Matthias, S.S.Rosenblum, D.A.Shirley

g Factor of the 90-keV Level in Ru99 and the Paramagnetic Correction in Transition Atoms

NUCLEAR STRUCTURE 99Ru, 99Rh; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.139.B532
Citations: PlumX Metrics


1965MA34      Phys.Rev. 140, B264 (1965)

E.Matthias, D.A.Shirley, J.S.Evans, R.A.Naumann

Half-Life and g Factor of the 75-keV Level of Rh100

NUCLEAR STRUCTURE 100Rh, 100Pd; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.140.B264
Citations: PlumX Metrics


1964EA02      Bull.Am.Phys.Soc. 9, No.4, 435, ED8 (1964)

W.Easley, J.Huntzicker, E.Matthias, S.S.Rosenblum, D.A.Shirley

Nuclear Zeeman Effect in 193Ir

NUCLEAR STRUCTURE 193Ir; measured not abstracted; deduced nuclear properties.


1964KA25      Arkiv Fysik 26, 260 (1964)

E.Karlsson, E.Matthias, A.Svensson, K.Johansson, S.Gustavsson, P.Andrade

g-Factors of the First Excited States in Lu175 and Tl203

NUCLEAR STRUCTURE 203Tl, 175Lu; measured not abstracted; deduced nuclear properties.


1964MA38      Bull.Am.Phys.Soc. 9, No.7, 741, Y4 (1964)

E.Matthias, S.Rosenblum, D.A.Shirley

g-factor of the 90-keV Level in Ru99 and the Internal Magnetic Field of Ru Dissolved in Ni

NUCLEAR STRUCTURE 99Rh, 99Ru; measured not abstracted; deduced nuclear properties.


1963MA10      Nucl.Phys. 40, 656 (1963)

E.Matthias, L.Bostrom, A.Maciel, M.Salomon, T.Lindqvist

Magnetic Dipole Interaction Studied by the Differential Angular Correlation Method

NUCLEAR STRUCTURE 181Ta, 111Cd; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(63)90310-9
Citations: PlumX Metrics


1963SA19      Nucl.Phys. 46, 377 (1963)

M.Salomon, L.Bostrom, T.Lindqvist, E.Matthias, M.Perez

Measurement of g-Factors of Excited States in Cd111, Pb204

NUCLEAR STRUCTURE 111Cd, 204Pb; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(63)90607-2
Citations: PlumX Metrics


1962KA14      Arkiv Fysik 22, 257 (1962)

E.Karlsson, E.Matthias, S.Ogaza

The Gyromagnetic Ratio of the First Rotational State in Hf178

NUCLEAR STRUCTURE 178Hf; measured not abstracted; deduced nuclear properties.


1962LE17      Ark.Fys. 22, 420 (1962)

C.A.Lerjefors, E.Matthias, E.Karlsson

Determination of the Rotational g-Factors for the First Excited States in Os186,188 and a Preliminary Result for the Magnetic Moment of the 113-keV Level in Hf177

NUCLEAR STRUCTURE 188Ir, 188Os, 188Re, 186Os, 186Re, 177Lu, 177Hf; measured not abstracted; deduced nuclear properties.


1962MA42      Ark.Fys. 22, 139 (1962)

E.Matthias, E.Karlsson, C.A.Lerjefors

Nuclear g-Factor of the 113 keV Rotational State in the Odd A Nucleus Hf177

NUCLEAR STRUCTURE 177Hf; measured not abstracted; deduced nuclear properties.


1962ST24      TID-17089 (Pt. II) (1962)

R.M.Steffen, E.Matthias, W.Schneider

Tables of Directional Correlation Attenuation Coefficients for Combined Magentic Dipole and Randomly Oriented Electric Quadrupole Interactions


1962ST25      TID-17089 (Pt.I) (1962)

R.M.Steffen, E.Matthias, W.Schneider

Tables of Directional Correlation Attenuation Coefficients for Combined Magnetic Dipole and Randomly Oriented Electric Quadrupole Interactions


1961KA09      Nucl.Phys. 25, 385 (1961)

E.Karlsson, C.-A.Lerjefors, E.Matthias

The Gyromagnetic Ratio of the 155 keV-Rotational Level in Os188

NUCLEAR STRUCTURE 188Os, 188Re; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(61)90168-7
Citations: PlumX Metrics


1961LE06      Nuclear Phys. 25, 404 (1961)

C.A.Lerjefors, E.Matthias, E.Karlsson

The Gyromagnetic Ratio of the 137 keV Rotational Level in Os186

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

doi: 10.1016/0029-5582(61)90169-9
Citations: PlumX Metrics


1960BO07      Nuclear Phys. 15, 239 (1960)

E.Bodenstedt, E.Matthias, H.J.Korner, E.Gerdau, F.Frisius, D.Hovestadt

The Nuclear g-Factor of the 111 keV Rotational Level and Other Angular Correlation Measurements on W184

NUCLEAR STRUCTURE 184Re; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(60)90305-9
Citations: PlumX Metrics


1959BO43      Z.Physik 153, 423 (1959)

E.Bodenstedt, E.Matthias, H.J.Korner

Das magnetische Momente des 181 keV-Niveaus von Technetium 99

doi: 10.1007/BF01337609
Citations: PlumX Metrics


1959BO56      Nuclear Phys. 11, 584 (1959)

E.Bodenstedt, H.J.Korner, E.Matthias

Angular Correlation Measurements on Cs133 and the Magnetic Moment of the 81 keV-Level

doi: 10.1016/0029-5582(59)90300-1
Citations: PlumX Metrics


1958BO70      Z.Naturforsch. 13a, 425 (1958)

E.Bodenstedt, E.Matthias, H.J.Korner, R.H.Siemssen

The Gyromagnetic Ratio of the 92 keV Level of Pm147


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