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NSR database version of April 11, 2024.

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD4340.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD4136.


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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD4169.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
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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.

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
Citations: PlumX Metrics

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
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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
Citations: PlumX Metrics


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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