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NSR database version of April 11, 2024.

Search: Author = K.Freitag

Found 47 matches.

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1999SC17      Phys.Rev.Lett. 82, 4787 (1999)

P.Schuurmans, J.Camps, P.De Moor, K.Freitag, P.Herzog, M.Huyse, R.Paulsen, N.Severijns, A.Van Geert, P.Van Duppen, B.Will, and the NICOLE and ISOLDE Collaborations

Angular Distributions of α Particles Emitted by Deformed Oriented Nuclei

RADIOACTIVITY 221Fr(α) [from 221Rn decay following Th(p, X)]; 227,229Pa(α) [from 232Th(p, xn)]; measured Eα, Iα(θ) from oriented nuclei; deduced anisotropy, deformation effects. Mass-separated sources.

doi: 10.1103/PhysRevLett.82.4787
Citations: PlumX Metrics

1999SE07      Phys.Rev. B59, 13948 (1999)

G.Seewald, E.Hagn, E.Zech, K.Freitag, P.Herzog

Nuclear Magnetic Resonance of 82Br in hcp Co

RADIOACTIVITY 82Br(β-) [from 81Br(n, γ)]; measured Iγ(θ), NMR on oriented nuclei; deduced hyperfine fields in hcp Co, spin-lattice relaxation.

doi: 10.1103/PhysRevB.59.13948
Citations: PlumX Metrics

1998SE09      Phys.Rev.Lett. 80, 5289 (1998)

G.Seewald, E.Hagn, E.Zech, K.Freitag, P.Herzog, D.Forkel-Wirth, and the ISOLDE Collaboration

Drastic Increase of the Nuclear Deformation in Bromine between A = 79 and 77

RADIOACTIVITY 77Br(EC); 82Br(β-); measured Iγ(H, θ), electric quadrupole interaction frequencies in hcp Co; deduced quadrupole moments, deformation. Modulated adiabatic passage on oriented nuclei. Systematics for bromine isotopes discussed.

doi: 10.1103/PhysRevLett.80.5289
Citations: PlumX Metrics

1998WE13      Eur.Phys.J. A 3, 25 (1998)

T.Weber, J.de Boer, K.Freitag, J.Groger, C.Gunther, P.Herzog, V.G.Soloviev, A.V.Sushkov, N.Yu.Shirikova

Nuclear Levels in 228Th Populated in the Decay of 228Pa (II)

RADIOACTIVITY 228Pa(EC); measured Eγ, Iγ, γγ-coin. 228Th deduced levels, J, π, δ, B(E2), rotational bands.

NUCLEAR STRUCTURE 228Th; calculated levels J, π, transition strengths. Quasiparticle-phonon model.

doi: 10.1007/s100500050146
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.

1997MU08      Phys.Rev. C55, 2267 (1997)

U.Muller, P.Sevenich, K.Freitag, C.Gunther, P.Herzog, G.D.Jones, C.Kliem, J.Manns, T.Weber, B.Will, and the ISOLDE Collaboration

Level Structure of 227Th Investigated in the α Decay of 231U

RADIOACTIVITY 231U(α) [from 232Th(α, 5n), E=53 MeV]; measured Eα, Iα, Eγ, Iγ. 227Ac(β-); 227Th(α) [from 227Ac(β-decay)]; 223Ra(α) [from 227Th(α-decay)]; measured αγ-coin, I(ce), Eα, Iα, oriented nuclei. 227Th deduced levels, J, π, γ-multipolarity, α hindrance factors, reduced transition rates, octupole deformation.

doi: 10.1103/PhysRevC.55.2267
Citations: PlumX Metrics

1997RE25      Phys.Rev. B55, 14200 (1997)

M.Renteria, F.G.Requejo, A.G.Bibiloni, A.F.Pasquevich, J.Shitu, K.Freitag

Perturbed-Angular-Correlation Study of the Electric-Field Gradient in 181Hf-Doped and Inplanted Indium Sesquioxide

RADIOACTIVITY 181Hf(β-); measured γγ(θ); deduced 181Ta hyperfine parameters, electric field gradients in In2O3, amorphism dependence.

doi: 10.1103/PhysRevB.55.14200
Citations: PlumX Metrics

1997WE05      Z.Phys. A358, 281 (1997)

T.Weber, J.deBoer, K.Freitag, J.Groger, C.Gunther, J.Manns, U.Muller

Variety of Vibrational Excitations in 228Th

RADIOACTIVITY 228Pa(EC); measured γγ-coin. 228Th deduced levels, J, π, K, band structure, moments of inertia.

doi: 10.1007/s002180050330
Citations: PlumX Metrics

1996GU08      Phys.Rev. C54, 679 (1996)

C.Gunther, S.Boehmsdorff, K.Freitag, J.Manns, U.Muller

Is There Experimental Evidence for an Interpretation of the Lowest K = 0 Collective Excitation of Deformed Nuclei as a Phonon Excitation of the γ Band ( Question )

NUCLEAR STRUCTURE N = 90-114; analyzed Er, Dy, Gd, Sm, Os, W, Hf, Yb isotopes levels, B(λ) data. 168Er; analyzed B(λ). 160Dy, 160Ho; calculated Eγ, Iγ; deduced (β)-vibrations interpretation related features.

doi: 10.1103/PhysRevC.54.679
Citations: PlumX Metrics

1995BA42      Z.Phys. A352, 47 (1995)

H.Baltzer, K.Freitag, C.Gunther, P.Herzog, J.Manns, U.Muller, R.Paulsen, P.Sevenich, T.Weber, B.Will

Nuclear Levels in 228Th Populated in the Decay of 228Pa

RADIOACTIVITY 228Pa(EC) [from 232Th(p, 5n), E=40 MeV]; measured Eγ, Iγ, (eγ)-coin, I(ce). 228Th deduced levels, J, π, K, band structure, Iγ, δ, B(λ) ratios, γ multipolarity. Low temperature source orientation.

doi: 10.1007/BF01292760
Citations: PlumX Metrics

1995GR25      Nucl.Instrum.Methods Phys.Res. B101, 422 (1995)

U.Grabowy, H.Busch, A.Gohla, K.-H.Speidel, S.Kremeyer, G.Jakob, K.Freitag, J.Gerber, W.Assmann

Preparation and Analysis of Targets with Implanted Thick Ar Layers for In-Beam γ-Spectroscopy

NUCLEAR REACTIONS 40Ar(62Ni, 62Ni'), E=150 MeV; measured Eγ, Iγ following target Coulomb excitation; deduced Ar content of target. Implantation of 40Ar ions in thick Fe layers.

doi: 10.1016/0168-583X(95)00558-7
Citations: PlumX Metrics

1994AC02      Z.Phys. A350, 13 (1994)

B.Ackermann, H.Baltzer, K.Freitag, C.Gunther, P.Herzog, J.Manns, U.Muller, R.Paulsen, P.Sevenich, T.Weber, B.Will, J.de Boer, G.Graw, A.I.Levon, M.Loewe, A.Losch, E.Muller-Zanotti

Experimental Investigation of Vibrational Excitations in 230Th

RADIOACTIVITY 230Pa(β+), (EC), (β-) [from 232Th(p, 3n), E not given]; measured Eγ, Iγ, I(ce). 230Th levels deduced Iγ, γ-multipolarity.

NUCLEAR REACTIONS 230Th(d, np), E=23 MeV; measured (ce)(ce)-, γ(ce)-coin. 232Th(p, t), E=22 MeV; measured σ(θ). 230Th deduced levels, J, π, K, γ-multipolarity, B(λ), high-spin band structure.

doi: 10.1007/BF01285047
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0942.

1993AC02      Nucl.Phys. A559, 61 (1993)

B.Ackermann, H.Baltzer, C.Ensel, K.Freitag, V.Grafen, C.Gunther, P.Herzog, J.Manns, M.Marten-Tolle, U.Muller, J.Prinz, I.Romanski, R.Tolle, J.deBoer, N.Gollwitzer, H.J.Maier

Collective E1 Transitions in Even-A Ra, Th, and U Nuclei

NUCLEAR REACTIONS 226Ra(α, xn), 230,232Th(α, 4n), E=28, 42, 55 MeV; 226Ra, 230,232Th(d, np), E=23, 28 MeV; measured Eγ, Iγ, I(ce), (e-)γ-coin. 226Ra, 224,226,228,230,232Th, 230,232U deduced levels, B(λ) ratios, intrinsic electric dipole moments. Other data input.

RADIOACTIVITY 228Pa(EC), (α); 230Pa(EC), (α), (β-) [from 232Th(p, xn)]; measured Iγ, I(ce). 226Ra, 224,226,228,230,232Th, 230,232U deduced levels, B(E1)/B(E2) ratios, intrinsic electric dipole moments. Other data input.

doi: 10.1016/0375-9474(93)90180-6
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Data from this article have been entered in the XUNDL database. For more information, click here.

1993LO10      Hyperfine Interactions 77, 103 (1993)

E.Lohmann, K.Freitag, Th.Schaefer, R.Vianden

The Magnetic Hyperfine Field at Cu in Fe, Co and Ni and the Magnetic Moment of the 41 keV, 2+ State of 62Cu

RADIOACTIVITY 62Zn(β+), (EC); measured γγ(θ, H); deduced magnetic hyperfine field at Cu in Fe, Co, Ni. 62Cu level deduced g.

doi: 10.1007/BF02320304
Citations: PlumX Metrics

1993SP01      Nucl.Phys. A552, 140 (1993)

K.-H.Speidel, H.Busch, S.Kremeyer, U.Knopp, J.Cub, M.Bussas, W.Karle, K.Freitag, U.Grabowy, J.Gerber

Measurements of Magnetic Moments of 134,136Xe(2+1) and the Mean Life of the 136Xe(2+1) State

NUCLEAR REACTIONS 132,134Xe(32S, 32S'), E=100 MeV; measured γ(θ, H) in polarized Fe, (particle) γ-coin, Coulomb excitation. 134,136Xe level deduced g, T1/2. Implanted Xe targets.

doi: 10.1016/0375-9474(93)90336-V
Citations: PlumX Metrics

1993VE02      Phys.Rev. B47, 490 (1993)

J.A.Vercesi, A.G.Bibiloni, C.P.Massolo, M.S.Moreno, A.F.Pasquevich, K.Freitag

Hyperfine Characterization of 181Ta in In2O3

RADIOACTIVITY 181Hf(β-); measured γγ(θ, H); deduced hyperfine interaction at 181Ta in In2O3.

doi: 10.1103/PhysRevB.47.490
Citations: PlumX Metrics

1989HE05      Z.Phys. A332, 247 (1989)

P.Herzog, U.Dammrich, K.Freitag, C.-D.Herrmann, K.Schlosser

The Magnetic Moments of (νg9/2)-Levels in Odd Zn Isotopes

RADIOACTIVITY 69m,71mZn; measured NMR, oriented nuclei; deduced μ.

1989HE07      Nucl.Phys. A493, 83 (1989)

C.-D.Herrmann, B.Prillwitz, U.Dammrich, K.Freitag, P.Herzog, D.Mayer, K.Schlosser, I.Ragnarsson

Magnetic Dipole Moments of the Ground State of 228,230Pa

RADIOACTIVITY 228,230Pa [from 232Th(p, 5n), (p, 3n), mass separation]; measured I(γ)(θ, T) in Fe; deduced μ. Low temperature nuclear orientation.

doi: 10.1016/0375-9474(89)90533-2
Citations: PlumX Metrics

1988BR36      Phys.Rev. B38, 11019 (1988)

W.D.Brewer, P.Roman, M.Bottcher, B.Illerhaus, H.Marshak, K.Freitag, P.Herzog

Nuclear Magnetic Resonance on Oriented Rare-Earth Nuclei in Rare-Earth Hosts: Application to 160Tb

RADIOACTIVITY 160Tb; measured NMR, oriented nuclei, γ(θ) anisotropy in Tb.

doi: 10.1103/PhysRevB.38.11019
Citations: PlumX Metrics

1987DR06      Z.Phys. A326, 279 (1987)

O.Dragoun, V.Brabec, M.Rysavy, A.Spalek, K.Freitag

Some Nuclear and Atomic Properties of 201Hg Determined by Conversion Electron Spectroscopy

RADIOACTIVITY 201Tl(EC); measured ce spectra, I(ce). 201Hg levels deduced ICC ratios, B(M1), δ, natural line widths. Electrostatic spectrometer. Theoretical calculations.

1987HE11      Nucl.Instrum.Methods Phys.Res. B26, 471 (1987)

P.Herzog, U.Dammrich, K.Freitag, B.Prillwitz, J.Prinz, K.Schlosser

Hyperfine Interaction Studies by Nuclear Orientation and NMR/ON On-Line to an Electromagnetic Isotope Separator - Experiences with the System FOLBIS

RADIOACTIVITY 82Br, 233Pa(β-); measured NMR, γ ray anisotropy vs inverse temperature; deduced 82Br hyperfine frequency in Fe, 233Pa effective electric interaction frequency in Zn.

doi: 10.1016/0168-583X(87)90797-X
Citations: PlumX Metrics

1987MA42      Phys.Rev.Lett. 59, 1764 (1987)

H.Marshak, W.D.Brewer, P.Roman, E.Klein, K.Freitag, P.Herzog

Nuclear Double Resonance of Tb: 160Tb oriented at low temperatures

RADIOACTIVITY 160Tb(β-); measured NMR, quadrupole splitting, oriented nuclei. 159,160Tb deduced g factor, quadrupole moment ratios.

doi: 10.1103/PhysRevLett.59.1764
Citations: PlumX Metrics

1986HE10      Z.Phys. B63, 241 (1986)

P.Herzog, U.Dammrich, K.Freitag, C.-D.Herrmann, K.Schlosser, J.C.Soares

Nuclear Magnetic Resonance of 175Hf Oriented in Iron

RADIOACTIVITY 175Hf(EC); measured NMR, oriented nuclei; deduced Hf magnetic hyperfine field in Fe.

doi: 10.1007/BF01309244
Citations: PlumX Metrics

1986RO07      Phys.Rev.Lett. 56, 1976 (1986)

P.Roman, W.D.Brewer, E.Klein, H.Marshak, K.Freitag, P.Herzog

Magnetic Resonance of 160Tb Oriented in a Terbium Single Crystal at Low Temperatures

RADIOACTIVITY 160Tb(β-); measured NMR, oriented nuclei; deduced magnetic resonance, quadrupole interaction frequency. 160Tb deduced quadrupole moment. Source implantation in single ferromagnetic terbium crystal.

doi: 10.1103/PhysRevLett.56.1976
Citations: PlumX Metrics

1985HE12      Hyperfine Interactions 22, 167 (1985)

P.Herzog, U.Dammrich, K.Freitag, C.-D.Herrmann, K.Schlosser

The Magnetic Hyperfine Field of Lutetium in Iron by NMR/ON

RADIOACTIVITY 177Lu(β-); measured NMR, oriented nuclei in Fe; deduced magnetic hyperfine field of Lu in Fe.

doi: 10.1007/BF02063988
Citations: PlumX Metrics

1985HE13      Hyperfine Interactions 22, 173 (1985)

P.Herzog, U.Dammrich, K.Freitag, C.-D.Herrmann, K.Schlosser

NMR/ON of 206Bi Implanted at T < 0.2 K and at Room Temperature into Nickel

RADIOACTIVITY 206Bi(EC) [from 209Bi(d, 5n)206Po(EC-decay)]; measured NMR, oriented nuclei in Ni; deduced BiNi hyperfine field.

doi: 10.1007/BF02063989
Citations: PlumX Metrics

1985HE16      Z.Phys. A322, 281 (1985)

P.Herzog, U.Dammrich, K.Freitag, C.-D.Herrmann, K.Schlosser

Ratio of the Electric Quadrupole Moments of 122,124Sb

RADIOACTIVITY 122Sb(β-), (EC), (β+) [from Sb neutron irradiation]; 124Sb(β-) [from Sb neutron irradiation]; measured γ(θ, T), orientation in Sb, Zn; deduced quadrupole interaction frequencies, electric field gradient in Sb, Zn. 122,124Sb level deduced quadrupole moment ratio. Low temperature nuclear orientation.

doi: 10.1007/BF01411892
Citations: PlumX Metrics

1983HE09      Z.Phys. A311, 351 (1983)

P.Herzog, H.Walitzki, K.Freitag, H.Hildebrand, K.Schlosser

Nuclear Orientation and NMR/ON of 205,207Po

RADIOACTIVITY 205,207Po(EC), (β+); measured NMR, γ(θ), oriented nuclei; deduced zero external field resonance frequencies, magnetic hyperfine field of Po in Fe, Ni, electric interaction frequencies in Zn, Be hosts. 205,207Po levels deduced T1/2, quadrupole moment ratio, g. 205,207Bi levels deduced multipole mixing parameters, γ-multipolarity.

doi: 10.1007/BF01415691
Citations: PlumX Metrics

1983HE25      Z.Phys. B54, 31 (1983)

P.Herzog, K.Freitag, C.-D.Herrmann, K.Schlosser

The Electric Field Gradient at the Nuclear Site of 177Lu in Zn and In

RADIOACTIVITY 177Lu(β-) [from Lu metal thermal neutron irradiation]; measured γ(θ), oriented nuclei at low temperature; deduced electric quadrupole interaction frequency, field gradient for 177Lu in Zn, In.

doi: 10.1007/BF01507946
Citations: PlumX Metrics

1983HE26      Z.Phys. A314, 215 (1983)

P.Herzog, K.Freitag, H.Hildebrand, M.Reuschenbach, H.Walitzki

Nuclear Orientation of 198,199Au in Zn and Cd

RADIOACTIVITY 198,199Au(β-) [from 197Au(n, γ), successive inadiation]; measured γ(θ, T), oriented nuclei; deduced quadrupole interaction frequencies. 198,199Au deduced quadrupole moment ratio. Implantation in Zn, Cd crystals.

doi: 10.1007/BF01879880
Citations: PlumX Metrics

1983HE28      Hyperfine Interactions 15/16, 329 (1983)

P.Herzog, K.Freitag, C.Herrmann, K.Schlosser

NMR/ON of 206Bi(Fe) Produced by Decay of Cold Implanted 206Po

RADIOACTIVITY 206Po(EC), (α); measured NMR, γ(θ), oriented nuclei; deduced effective spin relaxation time for 206Bi in Fe. Low temperature source implantation.

doi: 10.1007/BF02159767
Citations: PlumX Metrics

1983RA40      Hyperfine Interactions 15/16, 487 (1983)

J.H.Raudies, H.Appel, G.M.Then, W.-G.Thies, K.Freitag, J.P.F.Sellschop, M.E.Stemmet

TDPAC Studies on 181Hf Implanted into Diamond

RADIOACTIVITY 181Hf(β-); measured γγ(θ, H, t); deduced electric field gradients. Source implantation in cleaved single crystal diamonds.

doi: 10.1007/BF02159797
Citations: PlumX Metrics

1983SC38      Z.Phys. A313, 305 (1983)

P.Schuler, K.Hardt, C.Gunther, K.Freitag, P.Herzog, H.Niederwestberg, H.Reif, E.B.Shera, M.V.Hoehn

Experimental Investigation of Low Lying Excited States in 201Hg

RADIOACTIVITY 201Tl(EC); measured I(ce), γ(ce)(t), γγ(θ). 201Hg deduced levels, T1/2, J, π.

NUCLEAR REACTIONS 201Hg(α, α'), E=16 MeV; measured σ(E'α), Coulomb excitation. 201Hg levels deduced B(E2).

1980HE02      Z.Phys. A294, 13 (1980)

P.Herzog, K.Freitag, M.Reuschenbach, H.Walitzki

Nuclear Orientation of 111mCd in Zn and Be and the Quadrupole Moment of the 245 keV State

RADIOACTIVITY 111mCd [from 110Pd(α, 3n), E=40 MeV]; measured γ(θ, t), oriented nuclei; deduced electric field gradient sign in Be. 111Cd level deduced quadrupole moment.

doi: 10.1007/BF01473117
Citations: PlumX Metrics

1980HE05      Nucl.Phys. A337, 261 (1980)

P.Herzog, K.Krien, K.Freitag, M.Reuschenbach, H.Walitzki

Sudden Change of Quadrupole Moment between the First 5/2- States of 197Hg and 199Hg

RADIOACTIVITY 197mHg [from 197Au(d, 2n)]; 199mHg [from 198Pt(α, 3n)]; measured ceγ(θ, H, t). 197Hg level deduced quadrupole moment. 199Hg level deduced quadrupole-interaction frequency.

doi: 10.1016/0375-9474(80)90055-X
Citations: PlumX Metrics

1980KR11      Hyperfine Interactions 7, 401 (1980)

K.Krien, F.Reuschenbach, J.C.Soares, P.Herzog, H.-R.Folle, B.Perscheid, R.Trzcinski, K.Freitag

The Electric Field Gradients for Hg at Different Lattice Sites in Be

RADIOACTIVITY 199Tl [from 197Au(α, xn), E=30 MeV]; measured ceγ(θ, H, t) in Be. 199Hg deduced electric field gradients at different lattice sites in Be.

doi: 10.1007/BF01021523
Citations: PlumX Metrics

1980KR12      Hyperfine Interactions 7, 413 (1980)

K.Krien, F.Reuschenbach, J.C.Soares, R.Vianden, R.Trzcinski, K.Freitag, M.Hage-Ali, P.Siffert

Quadrupole Interaction Studies of Hg in Zn and Lattice Location of Hg And Au in Zn

RADIOACTIVITY 197mHg [from 197Au(d, xn), E=19 MeV]; 199Tl [from 197Au(α, xn), E=30 MeV]; 199Au [from double neutron capture on 197Au]; measured ceγ(θ, H, t), βγ(θ, H, t) in Zn. 197Hg, 199Au deduced quadrupole interaction constant in Zn.

doi: 10.1007/BF01021524
Citations: PlumX Metrics

1977FR10      Z.Phys. A282, 39 (1977)

K.Freitag, K.Krien, J.C.Soares, P.Herzog, W.D.Schneider, E.Bodenstedt

The Penetration Parameter λ of the Anomalous M1-Conversion of the 482 keV Transition in 181Ta

RADIOACTIVITY 181Hf; measured γγ(θ, H, t), γce-coin. 181Ta deduced δ, ICC, penetration parameter of M1 transition.

doi: 10.1007/BF01881004
Citations: PlumX Metrics

1976JA06      Phys.Rev. B13, 59 (1976)

P.K.James, P.Herzog, N.J.Stone, K.Freitag

Combined Lattice-Location-Hyperfine-Interaction Experiments on Hg Implanted in Fe

NUCLEAR MOMENTS 197,203Hg; measured hyperfine anomaly. NMR.

doi: 10.1103/PhysRevB.13.59
Citations: PlumX Metrics

1976KA26      Hyperfine Interactions 1, 485 (1976)

E.N.Kaufmann, K.Krien, J.C.Soares, K.Freitag

Quadrupole Interaction at Ta and Lattice Location of Hf in Be

RADIOACTIVITY 181Hf; measured γγ(θ, H, t). 181Ta deduced quadrupole interaction in Be.

doi: 10.1007/BF01022478
Citations: PlumX Metrics

1975HU15      Phys.Rev. C12, 2013 (1975)

H.Hubel, K.Freitag, E.Schoeters, R.E.Silverans, L.Vanneste, R.A.Naumann

Magnetic Moment of the Iπ = 25/2- Isomer in 179Hf and Anomalous Orbital Proton g Factor

RADIOACTIVITY 177Lu, 179mHf; measured γ(θ) polarized nuclei, γ(θ, H); deduced g, δ, magnetic hyperfine interaction μH.

doi: 10.1103/PhysRevC.12.2013
Citations: PlumX Metrics

1975KR12      Hyperfine Interactions 1, 217 (1975)

K.Krien, J.C.Soares, K.Freitag, R.Vianden, A.G.Bibiloni

The Electric Quadrupole Interaction of the 134 keV State of 197Hg in the Metal Hosts Cd, Zn, Sn and Ti Studied by e--γ TDPAC Measurements

NUCLEAR MOMENTS 197mHg; measured γce(θ, t); deduced quadrupole coupling constants.

doi: 10.1007/BF01022455
Citations: PlumX Metrics

1975SC16      Z.Phys. A272, 203 (1975)

E.Schoeters, R.E.Silverans, L.Vanneste, K.Freitag, H.Hubel

Magnetic Moment of the Iπ = 23/2- Isomer in 177Lu and Additivity in the Deformed Region

RADIOACTIVITY 177,177mLu; measured γ(θ, H). 177mLu deduced μ. Low temperature nuclear orientation.

doi: 10.1007/BF01408148
Citations: PlumX Metrics

1975SO12      Hyperfine Interactions 1, 45 (1975)

J.C.Soares, K.Krien, K.Freitag

Magnetic Hyperfine Fields at Ta in Co and Fe Hosts Measured by the e--γ Time-Differential Perturbed-Angular-Correlation Method

RADIOACTIVITY 181Hf; measured γce(θ, H, t); deduced hyperfine fields in Co, Fe hosts.

doi: 10.1007/BF01022441
Citations: PlumX Metrics

1973HE13      Z.Phys. 260, 57 (1973)

P.Herzog, K.Krien, K.Freitag

Perturbed αγ-Angular Correlations in the Decay of 228Th

RADIOACTIVITY 224Ra, 228Th; measured αγ(θ, H). 224Ra deduced g. 220Rn, 224Ra deduced hyperfine fields.

doi: 10.1007/BF01398070
Citations: PlumX Metrics

1973KR18      Phys.Rev. B8, 2248 (1973)

K.Krien, A.G.Bibiloni, K.Freitag, J.C.Soares, R.Vianden

Measurements of the Magnetic Hyperfine Fields at Hg in Fe, Co, and Ni Hosts by the e--γ Time-Differential Perturbed-Angular-Correlation Method

RADIOACTIVITY 197m,197Hg; measured Eγ(θ), hfs.

doi: 10.1103/PhysRevB.8.2248
Citations: PlumX Metrics

1973SO09      Phys.Lett. 45A, 465 (1973)

J.C.Soares, K.Krien, A.G.Bibiloni, K.Freitag, R.Vianden

Determination of the Quadrupole Splitting of the First Excited State of 119Sn in β-Tin by the e--γ TDPAC Technique

RADIOACTIVITY 119mSn; measured ceγ(t). 119Sn level deduced quadrupole moment splitting.

doi: 10.1016/0375-9601(73)90710-X
Citations: PlumX Metrics

1968HA37      Radiochim.Acta 9, 51 (1968)

A.Hanser, K.Freitag

Das Nuklid 198Bi

RADIOACTIVITY 198Bi; measured T1/2, Eγ, I(ce).

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