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NSR database version of July 31, 2015.

Search: Author = Z.Mate

Found 43 matches.

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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
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1290.


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
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD4162.


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.


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
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD4162.


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
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD4162.


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
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0375.


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


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
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0375.


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
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0525.


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
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0461.


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.


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
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0325.


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
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0590.


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)

I.Mahunka, Z.Mate, F.Tarkanyi

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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