NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = K.Freitag Found 47 matches. 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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
1973HE13 Z.Phys. 260, 57 (1973) 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
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
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
1968HA37 Radiochim.Acta 9, 51 (1968) Das Nuklid 198Bi RADIOACTIVITY 198Bi; measured T1/2, Eγ, I(ce).
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