NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = Z.Mate Found 43 matches. 2015OR03 Nucl.Phys. A940, 194 (2015) A.Ornelas, G.G.Kiss, P.Mohr, D.Galaviz, Zs.Fulop, Gy.Gyurky, Z.Mate, T.Rauscher, E.Somorjai, K.Sonnabend, A.Zilges The 106Cd(α, α)106Cd elastic scattering in a wide energy range for γ process studies NUCLEAR REACTIONS 106Cd(α, α), E=16.1, 17.7, 19.6 MeV; measured Eα, Iα(θ). 106Cd(α, α), E(cm)=15.6-26.0 MeV; calculated σ(θ) using ATOMKI-V1 optical potential; deduced optical model parameters from fit to available data. Potentials compared with those obtained by others using different potentials. 106Cd(α, n), (α, p), (α, γ), E(cm)=7-13 MeV; calculated S-factor using different potentials. Compared with data.
doi: 10.1016/j.nuclphysa.2015.04.008
2012OR03 J.Phys.:Conf.Ser. 337, 012030 (2012) A.Ornelas, D.Galaviz, Zs.Fulop, Gy.Gyurky, G.Kiss, Z.Mate, P.Mohr, T.Rauscher, E.Somorjai, K.Sonnabend, A.Zilges Investigation of α-nuclear potential families from elastic scattering experiments NUCLEAR REACTIONS 106Cd(α, γ), E(cm)=7-12 MeV;106Cd(α, n), E(cm)=10-12 MeV; calculated S-factor using various sets of optical model parameters. 106Cd(α, α), E=16.1-18.8 MeV; calculated σ(θ) using various sets of optical model parameters. Compared with published data of the same group.
doi: 10.1088/1742-6596/337/1/012030
2006KI11 Eur.Phys.J. A 27, Supplement 1, 197 (2006) G.G.Kiss, Zs.Fulop, Gy.Gyurky, Z.Mate, E.Somorjai, D.Galaviz, A.Kretschmer, K.Sonnabend, A.Zilges Study of the 106Cd(α, α)106Cd scattering at energies relevant to the p-process NUCLEAR REACTIONS 106Cd(α, α), E(cm)=15.5, 17, 19 MeV; measured σ(θ); deduced optical model parameters. 106Cd(α, γ), E(cm)=5-11 MeV; calculated astrophysical S-factors.
doi: 10.1140/epja/i2006-08-030-9
2005CS01 Phys.Lett. B 615, 175 (2005) M.Csatlos, A.Krasznahorkay, P.G.Thirolf, D.Habs, Y.Eisermann, T.Faestermann, G.Graw, J.Gulyas, M.N.Harakeh, R.Hertenberger, M.Hunyadi, H.J.Maier, Z.Mate, O.Schaile, H.-F.Wirth Resonant tunneling through the triple-humped fission barrier of 236U NUCLEAR REACTIONS 235U(d, pF), E=9.73 MeV; measured Ep, prompt fission probability vs excitation energy. 236U deduced hyperdeformed rotational bands, fission barrier features, resonant tunneling.
doi: 10.1016/j.physletb.2005.04.042
2005GA21 Phys.Rev. C 71, 065802 (2005) D.Galaviz, Zs.Fulop, Gy.Gyurky, Z.Mate, P.Mohr, T.Rauscher, E.Somorjai, A.Zilges Elastic α scattering on 112Sn and 124Sn at astrophysically relevant energies NUCLEAR REACTIONS 112Sn(α, α), E=14.4, 19.5 MeV; 124Sn(α, α), E=19.5 MeV; measured elastic σ(θ); deduced optical potential parameters. 112Sn(α, γ), E(cm)=7-11 MeV; calculated astrophysical S-factors, reaction rates.
doi: 10.1103/PhysRevC.71.065802
2005GY03 Nucl.Phys. A758, 517c (2005) Gy.Gyurky, Zs.Fulop, G.Kiss, Z.Mate, E.Somorjai, J.Gorres, A.Palumbo, M.Wiescher, D.Galaviz, A.Kretschmer, K.Sonnabend, A.Zilges, T.Rauscher A comprehensive study of the 106Cd(α, γ)110Sn reaction at energies relevant to the p-process NUCLEAR REACTIONS 106Cd(α, γ), E=8-12.5 MeV; measured Eγ, Iγ, σ. 106Cd(α, α), E ≈ 15, 17, 19 MeV; measured σ(θ). Astrophysical implications discussed, comparison with model predictions.
doi: 10.1016/j.nuclphysa.2005.05.094
2004KR02 Nucl.Phys. A731, 224 (2004) A.Krasznahorkay, H.Akimune, A.M.van den Berg, N.Blasi, S.Brandenburg, M.Csatlos, M.Fujiwara, J.Gulyas, M.N.Harakeh, M.Hunyadi, M.de Huu, Z.Mate, D.Sohler, S.Y.van der Werf, H.J.Wortche, L.Zolnai Neutron-skin thickness in neutron rich isotopes NUCLEAR REACTIONS 208Pb(α, α'), E=196 MeV; measured Eγ, Iγ, αγ-coin; deduced GDR excitation. 112,114,116,118,120,122,124Sn(3He, t), E=177 MeV; measured triton spectra, σ(E, θ); deduced spin-dipole resonance excitation. 112,114,116,118,120,122,124Sn, 208Pb deduced neutron skin thickness, related features. Comparison with previous results.
doi: 10.1016/j.nuclphysa.2003.11.034
2003CS03 Nucl.Phys. A719, 304c (2003) M.Csatlos, A.Krasznahorkay, D.Sohler, A.M.van den Berg, N.Blasi, J.Gulyas, M.N.Harakeh, M.Hunyadi, M.A.de Huu, Z.Mate, S.Y.van der Werf, H.J.Wortche, L.Zolnai Measurement of neutron-skin thickness in 208Pb by excitation of the GDR via inelastic α-scattering NUCLEAR REACTIONS 208Pb(α, α'), E=196 MeV; measured Eα, Eγ, αγ-coin, GDR production σ. 208Pb deduced proton and neutron radii, neutron skin thickness.
doi: 10.1016/S0375-9474(03)00937-0
2003CS04 Acta Phys.Pol. B34, 2119 (2003) M.Csatlos, Z.Gacsi, J.Gulyas, A.Krasznahorkay, A.Krasznahorkay, Jr., Z.Mate, J.Timar, M.Heil, F.Kaeppeler, R.Reifarth, M.Fayez-Hassan Effects of the third minimum on the fission characteristics in the actinide region NUCLEAR REACTIONS 232Th(n, F), E=1.5-1.75 MeV; measured fission fragment kinetic energy and mass distributions; deduced possible hyperdeformed states. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23576. 2003GA30 Nucl.Phys. A718, 578c (2003) D.Galaviz, M.Babilon, Zs.Fulop, Gy.Gyurky, R.Hillier, Z.Mate, P.Mohr, T.Rauscher, E.Somorjai, A.Zilges, L.Zolnai α-nucleus Potentials and Photon-induced Nucleosynthesis NUCLEAR REACTIONS 112Sn(α, α), E(cm) ≈ 14 MeV; measured σ(θ); deduced optical potential parameters.
doi: 10.1016/S0375-9474(03)00858-3
2003GA33 Nucl.Phys. A719, 111c (2003) D.Galaviz, M.Babilon, Zs.Fulop, Gy.Gyurky, Z.Mate, R.Hillier, P.Mohr, T.Rauscher, E.Somorjai, A.Zilges, L.Zolnai Determination of α-nucleus potentials by α-elastic scattering and its implications for the γ-process NUCLEAR REACTIONS 112,124Sn(α, α), E(cm) ≈ 19 MeV; measured σ(θ); deduced potential parameters. Astrophysical implications discussed.
doi: 10.1016/S0375-9474(03)00977-1
2003KR23 Acta Phys.Hung.N.S. 18, 323 (2003) A.Krasznahorkay, M.Csatlos, L.Csige, Y.Eisermann, T.Faestermann, Z.Gacsi, G.Graw, J.Gulyas, D.Habs, M.N.Harakeh, M.Heil, R.Hertenberger, F.Kappeler, A.Krasznahorkay, Jr., M.J.Maier, Z.Mate, R.Reifarth, P.G.Thirolf, J.Timar, H.F.Wirth Hyperdeformation and Clustering in the Actinide Region NUCLEAR REACTIONS 235U(d, pF), E=9.75 MeV; measured Ep, fission fragment spectra. 236U deduced hyperdeformed states, α-decay features. 232Th(n, F), E ≈ 1.6 MeV; measured fission fragments mass distributions, kinetic energy; deduced cluster effects.
doi: 10.1556/APH.18.2003.2-4.34
2003TH14 Acta Phys.Hung.N.S. 18, 317 (2003) P.G.Thirolf, D.Gassmann, D.Habs, M.Hunyadi, A.Krasznahorkay, E.Mergel, H.Hubel, D.Pansegrau, D.Schwalm, M.J.Chromik, M.Csatlos, J.Domscheit, Y.Eisermann, T.Faestermann, G.Graw, A.Gorgen, J.Gulyas, K.Hauschild, R.Hertenberger, T.Hartlein, F.Kock, A.Lopez-Martens, Z.Mate, H.J.Maier, A.Metz, S.Neumann, A.Neusser, P.Reiter, G.Schonwasser, H.Scheit Detailed Spectroscopy of Superdeformed Actinide Nuclei NUCLEAR REACTIONS 238U(α, 2nF), E=25 MeV; analyzed Eγ, Iγ, (fission fragment)γ-coin. 239Pu(d, pF), E=12.5 MeV; analyzed Ep, (fission fragment)p-coin. 240Pu deduced level structure in superdeformed second minimum.
doi: 10.1556/APH.18.2003.2-4.33
2001FU19 Phys.Rev. C64, 065805 (2001) Zs.Fulop, Gy.Gyurky, Z.Mate, E.Somorjai, L.Zolnai, D.Galaviz, M.Babilon, P.Mohr, A.Zilges, T.Rauscher, H.Oberhummer, G.Staudt 92Mo(α, α)92Mo Scattering, the 92Mo-α Optical Potential, and the 96Ru(γ, α)92Mo Reaction Rate at Astrophysically Relevant Energies NUCLEAR REACTIONS 92Mo(α, α), E(cm) ≈ 13, 16, 19 MeV; measured σ(θ); deduced optical model parameters. 96Ru(γ, α), E not given; calculated astrophysical reaction rates.
doi: 10.1103/PhysRevC.64.065805
2001HU05 Acta Phys.Pol. B32, 699 (2001) M.Hunyadi, D.Gassmann, A.Krasznahorkay, D.Habs, M.Csatlos, Y.Eisermann, T.Faestermann, G.Graw, J.Gulyas, R.Hertenberger, H.J.Maier, Z.Mate, A.Metz, P.Thirolf, M.Chromik, S.Y.van der Werf Superdeformed Rotational Bands in 240Pu NUCLEAR REACTIONS 239Pu(d, pF), E=12.5 MeV; measured proton spectra, (fission fragment)(proton)-coin. 240Pu deduced fission resonance features, superdeformed band.
2001HU12 Phys.Lett. 505B, 27 (2001) M.Hunyadi, D.Gassmann, A.Krasznahorkay, D.Habs, P.G.Thirolf, M.Csatlos, Y.Eisermann, T.Faestermann, G.Graw, J.Gulyas, R.Hertenberger, H.J.Maier, Z.Mate, A.Metz, M.J.Chromik Excited Superdeformed Kπ = 0+ Rotational Bands in β-vibrational Fission Resonances of 240Pu NUCLEAR REACTIONS 239Pu(d, pF), E=12.5 MeV; measured fission fragment and proton spectra, (proton)(fragment)-coin. 240Pu deduced β-vibrational fission resonance features, excited superdeformed bands J, π, energy.
doi: 10.1016/S0370-2693(01)00341-0
2001KR05 Acta Phys.Pol. B32, 657 (2001) A.Krasznahorkay, D.Habs, M.Hunyadi, D.Gassmann, M.Csatlos, Y.Eisermann, T.Faestermann, G.Graw, J.Gulyas, R.Hertenberger, H.J.Maier, Z.Mate, A.Metz, J.Ott, P.Thirolf, S.Y.van der Werf Superdeformation, Hyperdeformation and Clustering in the Actinide Region NUCLEAR REACTIONS 238U(α, 2n), E=25 MeV; measured Eγ, Iγ, E(ce), I(ce), delayed fission. 240Pu deduced levels, J, π built on fission isomer. 239Pu(d, pF), E=12.5 MeV; 233,235U(d, pF), E not given; measured proton spectra, (fission fragment)(proton)-coin. 240Pu, 234,236U deduced fission isomer deformation features.
2001KR17 Acta Phys.Hung.N.S. 13, 111 (2001) A.Krasznahorkay, D.Habs, M.Hunyadi, D.Gassmann, M.Csatlos, Y.Eisermann, T.Faestermann, G.Graw, J.Gulyas, R.Hertenberger, H.J.Maier, Z.Mate, A.Metz, J.Ott, P.G.Thirolf, S.Y.van der Werf Hyperdeformation and Clusterization in the Actinide Region NUCLEAR REACTIONS 233,235U(d, pF), E=9.7, 12.5 MeV; measured proton spectra, fission fragment spectra, mass distributions. 234,236U deduced fission probabilities, hyperdeformation.
doi: 10.1556/APH.13.2001.1-3.12
2001MO20 Nucl.Phys. A688, 424c (2001) P.Mohr, M.Babilon, D.Galaviz, A.Zilges, Zs.Fulop, Gy.Gyurky, Z.Mate, E.Somorjai, L.Zolnai, H.Oberhummer α-Nucleus Potentials at Astrophysically Relevant Energies NUCLEAR REACTIONS 92Mo(α, α), E=14-20 MeV; measured σ(θ); deduced optical model parameters. Comparison with neighboring nuclei.
doi: 10.1016/S0375-9474(01)00744-8
2001TH16 Acta Phys.Hung.N.S. 13, 93 (2001) P.G.Thirolf, D.Gassmann, D.Habs, M.J.Chromik, Y.Eisermann, G.Graw, R.Hertenberger, H.J.Maier, A.Metz, P.Reiter, T.Faestermann, A.Krasznahorkay, M.Hunyadi, M.Csatlos, J.Gulyas, Z.Mate, D.Pansegrau, H.Scheit, D.Schwalm, E.Mergel, H.Hubel, A.Gorgen Detailed Spectroscopy in the Superdeformed Second Minimum of 240Pu NUCLEAR REACTIONS 238U(α, 2n), E=25 MeV; measured Eγ, Iγ, E(ce), I(ce), (fragment)γ-coin following delayed fission. 240Pu deduced superdeformed levels, J, π, ICC.
doi: 10.1556/APH.13.2001.1-3.11
1999HU12 Acta Phys.Pol. B30, 1263 (1999) M.Hunyadi, A.Krasznahorkay, M.Csatlos, Y.Eisermann, T.Faestermann, D.Gassmann, G.Graw, J.Gulyas, D.Habs, R.Hertenberger, H.J.Maier, A.Metz, Z.Mate, J.Ott, P.Thirolf Multi-Phonon Superdeformed States in 240Pu NUCLEAR REACTIONS 239Pu(d, pF), E=12.5 MeV; measured proton spectra, p-(Fission fragment)-coin. 240Pu deduced multiphonon superdeformed band.
1999KR16 Phys.Lett. 461B, 15 (1999) A.Krasznahorkay, D.Habs, M.Hunyadi, D.Gassmann, M.Csatlos, Y.Eisermann, T.Faestermann, G.Graw, J.Gulyas, R.Hertenberger, H.J.Maier, Z.Mate, A.Metz, J.Ott, P.Thirolf, S.Y.van der Werf On the Excitation Energy of the Ground State in the Third Minimum of 234U NUCLEAR REACTIONS 233U(d, pF), E=12.5 MeV; measured proton spectra, (fission fragment)(proton)-coin. 234U deduced fission probability vs excitation energy, rotational bands, hyperdeformation, third minimum ground state energy, level density. Comparison with Fermi-gas formula.
doi: 10.1016/S0370-2693(99)00826-6
1999KR18 Acta Phys.Pol. B30, 1467 (1999) A.Krasznahorkay, M.Hunyadi, M.Csatlos, Y.Eisermann, T.Faestermann, D.Gassmann, G.Graw, J.Gulyas, D.Habs, R.Hertenberger, H.J.Maier, A.Metz, Z.Mate, J.Ott, P.Thirolf Hyperdeformed Rotational Bands in 234U NUCLEAR REACTIONS 233U(d, pF), E=12.5 MeV; measured proton spectrum, p(fission fragment)-coin. 234U deduced hyperdeformed band.
1998BR29 Acta Phys.Hung.N.S. 7, 355 (1998) M.Brenner, E.Indola, K.-M.Kallman, T.Lonnroth, P.Manngard, M.Halldorsdottir, Th.Karlsson, Z.Mate, L.Zolnai, V.Z.Goldberg, G.V.Rogatchev, M.V.Rojkov, I.N.Serikov, W.Trzaska, R.Wolski Energy-Spin Relations of Mid-sd-Shell Nuclear States - A Cluster Effect NUCLEAR REACTIONS 28Si(α, α), (α, α'), E=12.4-17.1 MeV; measured σ(E, θ); deduced resonances, Fourier amplitudes. 32S(α, α), E=13.2-15.4 MeV; measured σ(E, θ). 32S deduced alpha cluster states.
1998KR02 Phys.Rev.Lett. 80, 2073 (1998) A.Krasznahorkay, M.Hunyadi, M.N.Harakeh, M.Csatlos, T.Faestermann, A.Gollwitzer, G.Graw, J.Gulyas, D.Habs, R.Hertenberger, H.J.Maier, Z.Mate, D.Rudolph, P.Thirolf, J.Timar, B.D.Valnion Experimental Evidence for Hyperdeformed States in U Isotopes NUCLEAR REACTIONS 235U(d, pF), E=9.73, 13.0 MeV; measured p-spectra, (fission fragment)p-coin, fission fragment σ(θ). 236U deduced resonances, fission probability vs excitation energy, evidence for hyperdeformation. Results for other U isotopes discussed.
doi: 10.1103/PhysRevLett.80.2073
1998KR19 Acta Phys.Hung.N.S. 7, 35 (1998) A.Krasznahorkay, M.Hunyadi, M.Csatlos, A.Balanda, A.Gollwitzer, G.Graw, J.Gulyas, D.Habs, R.Hertenberger, Z.Mate, H.J.Maier, D.Rudolph, P.Thirolf, J.Timar, B.D.Valnion Hyperdeformed States in the Third Minimum of the Fission Potential NUCLEAR REACTIONS 235U(d, pF), E=9.7, 13 MeV; measured proton spectra, fission fragments angular distributions, (proton)(fragment)-coin. 234,236U deduced rotational bands, possible hyperdeformed states. Third minimum of fission potential.
1997CS04 Acta Phys.Pol. B28, 37 (1997) M.Csatlos, A.Krasznahorkay, M.Hunyadi, J.Gulyas, Z.Mate, J.Molnar, J.Timar, L.Vegh Properties of 236U at the Third-Minimum Deformation NUCLEAR REACTIONS 235U(d, pF), E=9.73 MeV; measured Ep, Ip, (fragment)p-coin. 236U deduced fission probability vs excitation energy, resonance E, Γ, evidence for hyperdeformed potential well.
1997MO04 Phys.Rev. C55, 1523 (1997) P.Mohr, T.Rauscher, H.Oberhummer, Z.Mate, Zs.Fulop, E.Somorjai, M.Jaeger, G.Staudt 144Sm-α Optical Potential at Astrophysically Relevant Energies Derived from 144Sm(α, α)144Sm Elastic Scattering NUCLEAR REACTIONS 144Sm(α, α), E=20 MeV; measured σ(θ); deduced optical parameters at astrophysically relevant energy, very limited uncertainities.
doi: 10.1103/PhysRevC.55.1523
1996KR07 Acta Phys.Pol. B27, 139 (1996) A.Krasznahorkay, M.Hunyadi, M.Csatlos, I.Dioszegi, J.Gulyas, Z.Mate Evidence for Hyperdeformed Nuclear Shape in 236U NUCLEAR REACTIONS 235U(d, pF), E=9-73 MeV; measured fission probability vs excitation energy. 236U deduced resonances, possible superdeformed, hyperdeformed bands.
1994BR19 Nucl.Phys. A574, 397 (1994) A.Bredbacka, M.Brenner, K.-M.Kallman, P.Manngard, Z.Mate, S.Szilagyi, L.Zolnai Low-Energy Elastic-Scattering of Alpha Particles from 34S, 50Cr and 62Ni NUCLEAR REACTIONS 34S, 50Cr, 62Ni(α, α), E=12.8, 14.6, 16.3, 18.1 MeV; 34S(α, α), E=20 MeV; measured σ(θ). Enriched target, semiconductor detector. Optical-model analysis.
doi: 10.1016/0375-9474(94)90237-2
1989MA62 Acta Phys.Acad.Sci.Hung. 65, 287 (1989) Z.Mate, S.Szilagyi, L.Zolnai, A.Bredbacka, M.Brenner, K.-M.Kallman, P.Manngard Low Energy Alpha Scattering on 62Ni NUCLEAR REACTIONS 62Ni(α, α), E=12.8-18.1 MeV; measured σ(θ); deduced model parameter energy dependence. Optical model. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0461. 1984CS01 Nucl.Phys. A413, 311 (1984) J.Cseh, E.Koltay, Z.Mate, E.Somorjai, L.Zolnai Levels in 23Na Excited by the 19F(α, α)19F, 19F(α, γ)23Na and 19F(α, p)22Ne Reactions NUCLEAR REACTIONS 19F(α, α), E=1.5-3.7 MeV; measured σ(E, θ). 23Na deduced resonances, J, π, Γ, Γ(α). 19F(α, p), E=1.5-3.7 MeV; measured σ(E). 23Na deduced resonances, Γ. 19F(α, γ), E=1.5-3.7 MeV; measured σ(E), σ(E, E(γ)), σ(E(γ), θ). 23Na deduced resonances, Γ, J, γ-branching, resonance strength.
doi: 10.1016/0375-9474(84)90377-4
1982CS01 Nucl.Phys. A385, 43 (1982) J.Cseh, E.Koltay, Z.Mate, E.Somorjai, L.Zolnai Levels of 28Si from the 24Mg(α, α)24Mg and 24Mg(α, γ)28Si Reactions NUCLEAR REACTIONS 24Mg(α, α), E=2.6-4.9 MeV; measured σ(E, θ). 24Mg(α, γ), E=3.7-5.1 MeV; measured σ(E), σ(Eγ, θ). 28Si deduced resonances, Γ, Γα, J, π, γ-branching, resonance strength, Γγ, δ. Enriched targets. R-matrix analysis.
doi: 10.1016/0375-9474(82)90488-2
1980ZO04 Izv.Akad.Nauk SSSR, Ser.Fiz. 44, 2281 (1980) L.Zolnai, E.Koltai, Z.Mate, I.Chekh, E.Shomoryai Radiation from States of 23Na Excited in the Reactions (α, α), (α, p), (α, γ) NUCLEAR REACTIONS 19F(α, α), (α, p), (α, γ), E=2.35-3.74 MeV; measured σ(E). 23Na deduced resonances, L, J, π, Γα, Γα/Γ. R-matrix analysis. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0925. 1975DA16 ATOMKI Kozlem. 17, 217 (1975) H.U.Dang, T.Fenyes, J.Gulyas, A.Kiss, E.Koltay, Z.Mate A 45Sc atommag szerkezetenek vizsgalata NUCLEAR REACTIONS 45Sc(p, p'γ), E=2, 2.5, 3, 3.5, 4 MeV; measured σ(E, Ep', Eγ). 45Sc deduced levels, γ-branching, J, π.
1975FE09 Nucl.Phys. A247, 103 (1975) T.Fenyes, I.Mahunka, Z.Mate, R.V.Jolos, V.Paar Excitation of Light Hg Nuclei in the Decay of Tl NUCLEAR STRUCTURE 188,189,190,191,192,193,194,195,197Tl; analyzed, reviewed experimental data; calculated levels.
doi: 10.1016/0375-9474(75)90280-8
1975VA20 Yad.Fiz. 22, 873 (1975); Sov.J.Nucl.Phys. 22, 455 (1976) T.B.Vandlik, J.Vandlik, N.G.Zaitseva, Z.Mate, I.Mahunka, M.Mahunka, H.Tyrroff, T.Fenyes Decay of the Isotopes 192Tl and 190Tl RADIOACTIVITY 190,192Tl; measured Eγ, Iγ, I(ce), T1/2; deduced log ft, ICC. 190,192Hg deduced levels, J, π, λ.
1974MA14 ATOMKI Kozlem. 16, 133 (1974) EC/β+ Elagazasi Tenyezok a 191,193,195,197Tl Izotopok Bomlasanal RADIOACTIVITY 191,193,195,197Tl; measured Eγ, Iγ, I(X), deduced EC/β+ ratios.
1974VA19 Izv.Akad.Nauk SSSR, Ser.Fiz. 38, 695 (1974); Bull.Acad.Sci.USSR, Phys.Ser. 38, No.4, 26 (1974) J.Vandlik, N.G.Zaitseva, Z.Mate, I.Mahunka, H.Tyrroff, T.Fenyes Investigation of the Decay 191Tl → 191Hg → 191Au RADIOACTIVITY 191Tl, 191Hg; measured T1/2, Eγ, Iγ. 191Au deduced levels, J, π, λ.
1974VA23 Izv.Akad.Nauk SSSR, Ser.Fiz. 38, 689 (1974); Bull.Acad.Sci.USSR, Phys.Ser. 38, No.4, 21 (1974) T.B.Vandlik, J.Vandlik, N.G.Zaitseva, Z.Mate, I.Mahunka, M.Mahunka, H.Tyrroff, T.Fenyes, V.I.Fominykh Decay Scheme of 193Tl RADIOACTIVITY 193Tl [from Pb + 660-MeV p]; measured Eγ, Iγ, I(ce), T1/2, γγ-coin. 193Hg deduced levels, J, π, γ-multipolarity.
1973VA26 Izv.Akad.Nauk SSSR, Ser.Fiz. 37, 1796 (1973); Bull.Acad.Sci.USSR, Phys.Ser. 37, No.9, 9 (1974) T.B.Vandlik, Y.Vandlik, N.G.Zaitseva, I.Mahunka, Z.Mate, H.Tyrroff, T.Fenyes, V.I.Fominykh The Decay Scheme of 197Tl RADIOACTIVITY 197Tl [from Pb(660-MeV p, X), isotope separator]; measured Eγ, Iγ, I(ce), γγ-coin; deduced log ft, Iβ+. 197Hg deduced levels, J, π, ICC, γ-multipolarity.
1972VA12 Pisma Zh.Eksp.Teor.Fiz. 15, 386 (1972); JETP Lett.(USSR) 15, 271 (1972) T.B.Vandlik, Y.Vandlik, N.G.Zaitseva, Z.Mate, I.Mahunka, M.Mahunka, T.Fenyes, H.Tyrroff, M.Jachim The New Isotope Tl189
1970VA27 Izv.Akad.Nauk SSSR, Ser.Fiz. 34, 1656 (1970); Bull.Acad.Sci.USSR, Phys.Ser. 34, 1472 (1971) Y.Vandlik, N.G.Zaitseva, Z.Mate, I.Mahunka, M.Mahunka, T.Fenesh New Isotopes 190Tl and 188Tl RADIOACTIVITY 188,190Tl[from Pb(660-MeV p, X)]; measured T1/2, Eγ, Iγ. 188,190Hg deduced levels, J, π.
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