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NSR database version of May 3, 2024.

Search: Author = F.Sterba

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2003KR11      Czech.J.Phys. 53, 483 (2003)

M.Krticka, J.Liptak, J.Materna, F.Sterba, J.Sterbova, J.Vrzal, M.Wintrova

Properties of some bound states of the 56Fe nucleus excited by the 55Mn(p, γ)56Fe reaction

NUCLEAR REACTIONS 55Mn(p, γ), E=1.3-1.8 MeV; measured Eγ, Iγ, DSA. 56Fe deduced levels, J, π, T1/2, branching ratios, level density and resonance decay features.

doi: 10.1023/A:1024653525657
Citations: PlumX Metrics


2000MA82      Czech.J.Phys. 50, 1097 (2000)

J.Materna, J.Liptak, F.Sterba, J.Sterbova, J.Vrzal

Properties of Some Resonances of the 55Mn(p, γ)56Fe Reaction in the Ep = (1.3-1.8) MeV Region

NUCLEAR REACTIONS 55Mn(p, γ), E=1.3-1.8 MeV; measured Eγ, Iγ. 56Fe deduced resonances J, π, decay branching, IAR features.

doi: 10.1023/A:1022848400062
Citations: PlumX Metrics


1992MA23      Czech.J.Phys. B42, 499 (1992)

X.T.Mai, J.Liptak, F.Sterba, P.Cejnar, J.Sterbova

Angular Distributions of γ-Rays from Four Resonances of the 55Mn(p, γ)56Fe Reaction

NUCLEAR REACTIONS 55Mn(p, γ), E(cm)=1.32-1.649 MeV; measured γ(θ). 56Fe deduced resonances, J, π, δ.


1989NO02      Czech.J.Phys. B39, 494 (1989)

D.Nosek, J.Kvasil, F.Sterba, P.Holan

Properties of the Lowest States in the Odd-Odd 160Tm and 162Tm Nuclei

NUCLEAR STRUCTURE 160,162Tm; calculated levels, B(λ). Two-quasiparticle plus rotor model.

doi: 10.1007/BF01597715
Citations: PlumX Metrics


1988ST03      Czech.J.Phys. B38, 150 (1988)

F.Sterba, J.Liptak, Nguyen An Ninh, J.Sterbova

Some Properties of 1805 keV Resonance in p + 55Mn Interaction

NUCLEAR REACTIONS, ICPND 55Mn(p, p'γ), (p, nγ), (p, γ), E=1.3-2 MeV; measured γ yields, σ(E). 56Fe deduced resonance, possible J, π.


1988ST14      Czech.J.Phys. B38, 741 (1988)

F.Sterba, J.Liptak, Nguyen An Ninh, J.Sterbova, J.Stary

Excitation Functions for Some Output Channels following the p + 55Mn Interaction at E(p) = 1.3-2.0 MeV

NUCLEAR REACTIONS, ICPND 55Mn(p, p'), (p, nγ), (p, γ), E=1.3-2 MeV; measured σ(E), γ yields. 56Fe deduced resonances, J, π.


1981ST09      Czech.J.Phys. B31, 578 (1981)

F.Sterba

The Inelastic Scattering of Deuterons on the Odd Deformed Nuclei Near the Coulomb Barrier

NUCLEAR REACTIONS 155,157Gd, 167Er(d, d'), E=12.1 MeV; 233,235U(d, d'), E=13.1 MeV; analyzed σ(θ). DWBA calculations.


1980ST29      Czech.J.Phys. 30, 747 (1980)

F.Sterba, J.Kvasil, P.Holan

The ΔN = 2 Mixing of the 1/2+[660], 1/2+[400] and 3/2+[651], 3/2+[402] Nilsson States in 161Dy and 163Dy

NUCLEAR STRUCTURE 161,163Dy; calculated levels, K=(1/2)+, (3/2)+ rotational bands. Coriolis, ΔN=2 interactions.

NUCLEAR REACTIONS 162,160Dy(d, p), 164,162Dy(d, t), E=12.1 MeV; calculated σ(Ep), σ(Et). DWBA theory, ΔN=2 rotational band mixing spectroscopic amplitudes.


1980ST31      Czech.J.Phys. B30, 1175 (1980)

F.Sterba, J.Kvasil, P.Holan

The Structure of the States in the 161Dy and 163Dy Isotopes Excited by the One-Neutron Transfer Reactions

NUCLEAR REACTIONS 162Dy(d, t), (d, p), E=12.1 MeV; analyzed data. 161,163Dy deduced levels, configurations, rotational bands. DWBA analysis, pairing, multipole-multipole, Coriolis, ΔN=2 interactions.


1979ST26      Czech.J.Phys. 29, 1215 (1979)

F.Sterba, P.Holan, J.Kvasil, M.Horakova, R.K.Sheline

The Study of the 188Re Nucleus by the 189Os(t, α)188Re Reaction at Et = 15.1 MeV

NUCLEAR REACTIONS 189Os(t, α), E=15.1 MeV; measured σ(Et, θ). 188Re deduced levels, band structure, Nilsson assignment. DWBA, Coriolis coupling calculation.


1978KV01      Czech.J.Phys. B28, 291 (1978)

J.Kvasil, F.Sterba, P.Holan

Influence of Coriolis Coupling on Inelastic Scattering of Deuterons

NUCLEAR STRUCTURE 155,157Gd, 167Er; calculated B(E2). Nilsson potential with hexadecapole deformation, Coriolis coupling.

doi: 10.1007/BF01597217
Citations: PlumX Metrics


1978ST11      Czech.J.Phys. B28, 31 (1978)

F.Sterba, J.Sterbova, J.Kvasil

The Study of the 233U and 235U by the Inelastic Scattering of 13.1 MeV Deuterons

NUCLEAR REACTIONS 233,235U(d, d'), E=13.1 MeV; measured σ(Ed'). 233,235U deduced levels, B(E2).


1977ST31      Czech.J.Phys. 27B, 531 (1977)

J.Sterbova, F.Sterba

The Octupole States in Odd Uranium Isotopes 233U and 235U

NUCLEAR REACTIONS 233,235U(d, d'), E=13.1 MeV; measured σ(Ed'). 233,235U deduced levels, B(E3), K, J, π.


1976ST20      Czech.J.Phys. 26B, 753 (1976)

F.Sterba, P.Holan, R.K.Sheline

The Study of the 161Tb Nucleus by the 162Dy(t, α)161Tb Reaction

NUCLEAR REACTIONS 162Dy(t, α), E=15 MeV; measured σ(Eα). 161Tb deduced levels, S.


1975HO21      Czech.J.Phys. 25B, 963 (1975)

P.Holan, M.Rozkos, F.Sterba

The Study of the Angular Distributions of Tritons from the Reaction 162Dy(d, t)161Dy at 12.1 MeV

NUCLEAR REACTIONS 162Dy(d, t), E=12.1 MeV; measured σ(Et, θ). 161Dy deduced levels, K, J, π.

doi: 10.1007/BF01597576
Citations: PlumX Metrics


1974HO24      Czech.J.Phys. 24B, 395 (1974)

P.Holan, M.Rozkos, F.Sterba, J.Cejpek

The Study of the Angular Distributions of Protons from the Reaction 162Dy(d, p)163Dy at 12.1 MeV

NUCLEAR REACTIONS 162Dy(d, p), E=12.1 MeV; measured σ(Ep, θ). 163Dy deduced levels, J, π, L, S.

doi: 10.1007/BF01594075
Citations: PlumX Metrics


1973ST07      Czech.J.Phys. 23B, 25 (1973)

F.Sterba, J.Sterbova, M.Rozkos

Angular Distributions of 12 MeV Deuterons Inelastically Scattered by the 162Dy

NUCLEAR REACTIONS 162Dy(d, d'), E=12.1 MeV; measured σ(Ed', θ). 162Dy deduced levels, L, J, π.


1973ST18      Czech.J.Phys. 23B, 601 (1973)

F.Sterba, J.Sterbova, M.Rozkos

Energy Levels of 167Er Populated by the (d, d') Reaction

NUCLEAR REACTIONS 167Er(d, d'), E=12.1 MeV; measured σ(Ed', θ). 167Er deduced levels, J, π, B(E2).


1971ST03      Nucl.Phys. A162, 353 (1971)

F.Sterba, P.O.Tjom, B.Elbek

Energy Levels of 155Gd and 157Gd Populated by the (d, d') Reaction

NUCLEAR REACTIONS 155,157Gd(d, d'), Ed=12.1 MeV; measured σ(Ed', θ). 155,157Gd deduced levels, B(E2), B(E3). Enriched targets.

doi: 10.1016/0375-9474(71)90990-0
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0343.


1970RO27      Czech.J.Phys. 20B, 492 (1970)

M.Rozkos, F.Sterba

Energy Spectra of Neutrons from the Reaction Co59(p, n) at E Approx. 6.05 - 6.3 MeV

NUCLEAR REACTIONS 59Co(p, n), E=6.05-6.3 MeV; measured σ(En); deduced reaction mechanism.

doi: 10.1007/BF01698409
Citations: PlumX Metrics


1970RO28      Czech.J.Phys. 20B, 487 (1970)

M.Rozkos, F.Sterba, I.Wilhelm

Angular Distribution of Protons from the Reaction Co59(n, p)Fe59 for E Approx. 6.3 MeV

NUCLEAR REACTIONS 59Co(n, p), E=6.3 MeV; measured σ(En, θ); deduced reaction mechanism.

doi: 10.1007/BF01698408
Citations: PlumX Metrics


1968ST22      Czech.J.Phys. 18B, 900 (1968)

F.Sterba

The Study of the Ground State Rotational Bands in U 233 and U 235 by the Inelastic Scattering of Deuterons

NUCLEAR STRUCTURE 235U, 233U; measured not abstracted; deduced nuclear properties.


1968ST24      Contrib.Intern.Symp.Nucl.Struct., Dubna, p.60 (1968)

F.Sterba, J.Sterbova

The Inelastic Scattering of Deuterons by the U233 and U235

NUCLEAR REACTIONS 233,235U(d, d'), E=13 MeV; measured σ, σ(Ed'). 233,235U deduced levels, K, γ-multipolarity.


1967PO15      Czech.J.Phys. 17B, 707 (1967)

S.Pospisil, M.Rozkos, F.Sterba, I.Wilhelm

Angular Distributions of Fast Neutrons from the Reaction Co59(p, n) at E = 4.05-5.23 MeV

NUCLEAR REACTIONS 59Co(p, n), E=5.23-4.05 MeV; measured σ(E, En, θ); deduced reaction mechanism.


1965RO12      Czech.J.Phys. 15B, 151 (1965)

M.Rozkos, F.Sterba, J.Sterbova

A Study of the Co59(p, n) Reaction at E = 5.75-6.39 MeV

NUCLEAR STRUCTURE 59Ni; measured not abstracted; deduced nuclear properties.

doi: 10.1007/BF01688860
Citations: PlumX Metrics


1958DR74      Czechoslov.J.Phys. 8, 648 (1958)

L.Drska, I.Chudacek, F.Sterba

Measurement of SOme Neutron Spectra by the Nuclear Emulsion Method

doi: 10.1007/BF01572177
Citations: PlumX Metrics


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