NSR Query Results

Output year order : Descending
Format : Normal

NSR database version of May 23, 2024.

Search: Author = J.Rizek

Found 12 matches.

Back to query form

1999DR13      J.Phys.(London) G25, 1839 (1999)

O.Dragoun, A.Spalek, M.Rysavy, A.Kovalik, E.A.Yakushev, V.Brabec, A.F.Novgorodov, N.Dragounova, J.Rizek

Search for an Admixture of Heavy Neutrinos in the β-Decay of 241Pu

RADIOACTIVITY 241Pu(β-); measured β spectrum; deduced heavy neutrino admixture upper limits.

doi: 10.1088/0954-3899/25/9/307
Citations: PlumX Metrics

1998RY06      Prog.Part.Nucl.Phys. 40, 335 (1998)

M.Rysavy, V.Brabec, O.Dragoun, N.Dragounova, A.Spalek, J.Rizek, A.Kovalik, A.F.Novgorodov

Measurements of 241Pu β-Spectrum in Search for Admixture of Massive Neutrinos

RADIOACTIVITY 241Pu(β-); measured β spectra; deduced massive neutrino admixture upper limit.

doi: 10.1016/S0146-6410(98)00043-X
Citations: PlumX Metrics

1987GM03      Czech.J.Phys. B37, 1107 (1987)

M.Gmitro, T.D.Kaipov, J.Kvasil, J.Rizek

Continuity Equation Constraint in the Transverse Quadrupole Electric-Type Form Factors

NUCLEAR REACTIONS 12C(e, e'), E not given; calculated form factors. Continuity equation constraint.

doi: 10.1007/BF01597028
Citations: PlumX Metrics

1981ER04      Czech.J.Phys. B31, 482 (1981)

R.A.Eramzhyan, L.Majling, J.Rizek

The Role of Deep Shell Nucleons in the Formation of Giant Dipole Resonance

NUCLEAR REACTIONS 32S(μ-, n), E at rest; calculated σ(En); deduced role of deep shell nucleons in GDR excitation, decay.

doi: 10.1007/BF01596414
Citations: PlumX Metrics

1981ER05      J.Phys.(London) G7, L231 (1981); Corrigendum J.Phys.(London) G8, 595 (1982)

R.A.Eramzhyan, M.Gmitro, S.S.Kamalov, G.V.Micelmacher, J.Rizek

A Method to Determine the Muon-Neutrino Mass

NUCLEAR REACTIONS 16O(μ-, γ), E at rest; calculated relative γ-yield, branching ratio; 12C, 31P(μ-, γ), E at rest; calculated branching ratio; deduced neutrino mass upper limit. Radiative capture, impulse approximation.

doi: 10.1088/0305-4616/7/10/004
Citations: PlumX Metrics

1978ER05      Czech.J.Phys. B28, 1081 (1978)

R.A.Eramzhyan, L.Majling, J.Rizek, R.A.Sakaev

Radiative Pion Capture by 32S

NUCLEAR REACTIONS 32S(π-, γ), E=at rest; calculated transition rates, yield of hard-γ. Shell model with excitation up to 3 oscillator quanta.

doi: 10.1007/BF01602795
Citations: PlumX Metrics

1975ER06      Nucl.Phys. A247, 411 (1975)

R.A.Eramzhyan, L.Majling, J.Rizek

The Proton Channel in Muon Capture by 32S

NUCLEAR REACTIONS 32S(μ-, n); calculated neutron spectra. 31P, 31Si, 31S deduced branching ratios.

doi: 10.1016/0375-9474(75)90132-3
Citations: PlumX Metrics

1973BE16      Nucl.Phys. A204, 357 (1973)

Y.I.Bely, R.A.Eramzhyan, L.Majling, J.Rizek, V.A.Vartanyan

The Neutron Channel in Muon Capture by 15N and 32S

NUCLEAR REACTIONS 15N, 32S(π-, n); 15C, 32P resonances calculated σ(En).

doi: 10.1016/0375-9474(73)90278-9
Citations: PlumX Metrics

1972BE17      Phys.Lett. 39B, 335 (1972)

Y.I.Bely, N.P.Yudin, L.Majling, J.Rizek

What Can Be Learned from de-Excitation Experiments (Question)

NUCLEAR REACTIONS 32S(γ, nγ'), (γ, pγ'), calculated 31P population probability. 31P calculated photoproduction probabilities, branching ratios.

doi: 10.1016/0370-2693(72)90131-1
Citations: PlumX Metrics

1971BE39      Nucl.Phys. A170, 141 (1971)

Y.I.Bely, N.M.Kabachnik, V.G.Neudatchin, N.P.Yudin, L.Majling, J.Rizek

The Electroexcitation of 32S in the Region of the Dipole Resonance

NUCLEAR REACTIONS 32S(e, e'), E=150, 200 MeV; calculated C1+E1, M2 form factors in giant resonance region.

doi: 10.1016/0375-9474(71)90688-9
Citations: PlumX Metrics

1970PL04      Z.Phys. 237, 180 (1970)

Z.Plajner, V.Brabec, L.Maly, J.Rizek, M.Vejs

Excited Levels in the Decay 185Os → 185Re

RADIOACTIVITY 185Os; measured Eγ, Iγ, I(ce), γγ-coin; deduced log.ft. 185Re deduced levels, ICC, γ-multipolarity, J, π. Ge(Li) detector, double-focusing β-spectrometer.

doi: 10.1007/BF01404476
Citations: PlumX Metrics

1970RI18      Czech.J.Phys. 20B, 666 (1970)

J.Rizek, P.Vogel

The 2+ and 3- Collective States in the Sn and Zr Isotopes Using Schematic Forces

NUCLEAR STRUCTURE 92,94,96Zr, 114,116,118,120,122,124Sn; calculated levels, B(EL). Schematic forces, random phase approximation.

Back to query form