NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = L.Majling Found 32 matches. 2010MA56 Physics of Part.and Nuclei 41, 1111 (2010) Delayed clusters accompanying nonmesonic weak decay of the Λ-hypernuclei: a clue to nonleptonic processes NUCLEAR STRUCTURE 4H, 4He, 7,8He, 7,8,9,10Li, 7,8,9,10,11Be, 8,9,10,11B, 10,11C; calculated clusters for one- and two-nucleon decay of hypernuclei.
doi: 10.1134/S1063779610070294
2008AV07 Phys.Atomic Nuclei 71, 2101 (2008); Yad.Fiz. 71, 2137 (2008) A.V.Averyanov, S.A.Avramenko, V.D.Aksinenko, M.Kh.Anikina, S.N.Bazylev, V.P.Balandin, Yu.A.Batusov, Yu.A.Belikov, Yu.T.Borzunov, O.V.Borodina, A.I.Golokhvastov, L.B.Golovanov, C.Granja, A.B.Ivanov, Yu.L.Ivanov, A.Yu.Isupov, Z.Kohout, A.M.Korotkova, A.G.Litvinenko, J.Lukstins, A.I.Malakhov, L.Majling, O.Majlingova, P.K.Manyakov, V.T.Matyushin, I.I.Migulina, G.P.Nikolaevsky, O.B.Okhrimenko, A.N.Parfenov, N.G.Parfenova, V.F.Peresedov, S.N.Plyashkevich, S.Pospisil, P.A.Rukoyatkin, I.S.Saitov, R.A.Salmin, V.M.Slepnev, I.V.Slepnev, M.Solar, B.Sopko, V.Sopko, E.A.Strokovsky, V.V.Tereshchenko, A.A.Feshchenko, T.Horazdovsky, D.Chren, Yu.A.Chencov, I.P.Yudin Studying of hypernuclei with nuclotron beams
doi: 10.1134/S1063778808120119
2007MA74 Phys.Atomic Nuclei 70, 1611 (2007) What can we learn about baryon-baryon interaction from hypernuclei 6ΛH and 8ΛH? NUCLEAR STRUCTURE 4,6,8H; calculated level energies, J, π for Λ hypernuclei.
doi: 10.1134/S1063778807090190
2006MA38 Phys.Atomic Nuclei 69, 810 (2006); Yad.Fiz. 69, 838 (2006) L.Majling, V.A.Kuzmin, T.V.Tetereva Alpha Particles Accompanying the Weak Decay of 10ΛBe and 10ΛB Hypernuclei NUCLEAR STRUCTURE 10Be, 10B; analyzed hypernucleus α-decay widths, dependence on ΛN interaction, related features.
doi: 10.1134/S1063778806050048
2005BA86 Fiz.Elem.Chastits At.Yadra 36, 319 (2005); Physics of Part.and Nuclei 36, 169 (2005) Yu.A.Batusov, J.Lukstins, L.Majling, A.N.Parfenov "Alpha Decays" of 10ΛBe and 10ΛB Hypernuclei on a Nuclotron: A Clue to Some Puzzles In Nonleptonic Processes NUCLEAR STRUCTURE 10Be, 10B; calculated branching fractions for hypernucleus α-decay, nuclear structure effects.
2005MA46 Nucl.Phys. A754, 184c (2005) L.Majling, Yu.A.Batusov, J.Lukstins, A.N.Parfenov "Alpha-decays" of 10ΛBe and 10ΛB hypernuclei NUCLEAR STRUCTURE 10Be, 10B; analyzed hypernucleus decay widths.
doi: 10.1016/j.nuclphysa.2005.02.074
2004MA89 Yad.Fiz. 67, 1832 (2004); Phys.Atomic Nuclei 67, 1804 (2004) L.Majling, V.A.Kuzmin, T.V.Tetereva "Alpha Decays" of 10ΛBe and 10ΛB Hypernuclei: Phenomenological Analysis and Role of Nuclear Structure NUCLEAR STRUCTURE 10Be, 10B; calculated hypernucleus decay widths, nuclear structure effects.
doi: 10.1134/1.1811182
2003MA38 Czech.J.Phys. 53, 667 (2003) L.Majling, J.Lukstins, A.N.Parfenov, D.Chren, M.Solar, B.Sopko Relativistic hypernuclei: old problems and new prospects NUCLEAR STRUCTURE 10Be, 10B; calculated hypernucleus nonmesonic decay widths, dependence on weak interaction model. Proposed experiment using relativistic hypernuclei discussed.
doi: 10.1023/A:1025311529699
2001MA66 Yad.Fiz. 64, No 6, 1228 (2001); Phys.Atomic Nuclei 64, 1152 (2001) Spectroscopy of the Λ Hypernuclei: New problems and prospects NUCLEAR STRUCTURE 3,4H, 4,5He, 9Be, 11B, 12C, 16O, 28Si, Fe, 209Bi, 238U; analyzed hypernucleus decay features.
doi: 10.1134/1.1383633
2001MA81 Nucl.Phys. A691, 185c (2001) Non-Mesonic Weak Decay of the Λ10Be and Λ10B Hypernuclei NUCLEAR STRUCTURE 10Be, 10B; calculated hypernucleus partial and total decay widths.
doi: 10.1016/S0375-9474(01)01027-2
1998MA56 Nucl.Phys. A639, 125c (1998) Baryonic Decays of p-Shell Hypernuclei NUCLEAR STRUCTURE 10B; calculated Λ hypernucleus levels, baryonic decay modes branching ratios.
doi: 10.1016/S0375-9474(98)00261-9
1997MA79 Fiz.Elem.Chastits At.Yadra 28, 253 (1997); Phys.Part.Nucl. 28, 101 (1997) L.Majling, V.N.Fetisov, R.A.Eramzhyan Decay Properties of 1p-Shell Hypernuclei: II. Baryon decays
1995MA20 Nucl.Phys. A585, 211c (1995) Production of (Lambda)-Hypernuclei with a Large Neutron Excess and a Neutron Halo NUCLEAR STRUCTURE A=3-9; analyzed hypernuclei binding energies data; deduced extrapolations.
doi: 10.1016/0375-9474(94)00567-7
1994MA68 Prog.Theor.Phys.(Kyoto), Suppl. 117, 55 (1994) Hypernuclear γ Spectroscopy - Progress, Problems and Unexplored Possibilities - NUCLEAR STRUCTURE A=4; A=7; A=9; compiled, reviewed hypernuclear γ-transitions. A=13; analyzed possible γ-transitions in hypernuclei. NUCLEAR REACTIONS 13C(K-, π-), E at 0.8 GeV/c; analyzed possible γ-transitions in hypernuclei.
doi: 10.1143/PTPS.117.55
1993MA63 Bull.Rus.Acad.Sci.Phys. 57, 1661 (1993) A Review of Hypernuclear Spectroscopy: Problems, progress, prospects
1992MA49 Czech.J.Phys. B42, 1197 (1992) L.Majling, R.A.Eramzhyan, V.N.Fetisov Baryonic Decay and 1p-Shell Hypernuclear Spectroscopy NUCLEAR REACTIONS 13C, 14,15N, 6,7Li, 9Be, 12C(K-, π-), E not given; 12,13C(K-, π-), E at 550 MeV/c; analyzed data; deduced 12C hypernucleus proton decay features. Translationally invariant shell model.
doi: 10.1007/BF01591401
1992MA57 Nucl.Phys. A547, 73c (1992) L.Majling, V.N.Fetisov, R.A.Eramzhyan Strong Decays and (Lambda)N Interaction in p-Shell Hypernuclei NUCLEAR STRUCTURE A=10; analyzed hypernucleus data; deduced (lambda)N-interaction, hypernuclear resonance decay properties.
doi: 10.1016/0375-9474(92)90711-R
1991FE06 Z.Phys. A339, 399 (1991) V.N.Fetisov, L.Majling, J.Zofka, R.A.Eramzhyan Effective Lambda N-Interaction and Spectroscopy of Low-Lying States of 1p-Shell Hypernuclei NUCLEAR STRUCTURE A=7-16; analyzed hypernuclei data; deduced model parameters. Shell model, effective Lambda-nucleon potential.
doi: 10.1007/BF01560643
1991MA55 Czech.J.Phys. B41, 1083 (1991) L.Majling, J.Zofka, R.A.Eramzhyan, V.N.Fetisov On the Configurational Splitting of Strangeness Analog State NUCLEAR STRUCTURE A=10; calculated hypernuclear levels, γ-decay; deduced s-1s(lambda) configuration decay features.
doi: 10.1007/BF01598983
1991ZO01 Fiz.Elem.Chastits At.Yadra 22, 1292 (1991); Sov.J.Part.Nucl. 22, 628 (1991) J.Zofka, L.Majling, V.N.Fetisov, R.A.Eramzhyan Decay Properties of 1p-Shell Hypernuclei. I. Excited Bound States NUCLEAR STRUCTURE A=7-16; calculated hypernuclear spectra, decay characteristics. Shell model.
1990MA69 Z.Phys. A337, 337 (1990) L.Majling, J.Zofka, V.N.Fetisov, P.N.Lebedev, R.A.Eramzhyan A Note on the Origin of Secondary Hypernuclear γ-Quanta from 10B(Lambda)
1987MA08 Phys.Lett. 183B, 263 (1987) L.Majling, J.Zofka, V.N.Fetisov, R.A.Eramzhyan On the Spectroscopy of the 13C(Lambda) Hypernucleus ATOMIC PHYSICS, Mesic-Atoms 13C(K-, π-), E not given; calculated hypernuclear levels, baryonic, γ-decays, excitation, daughter spectra. Many-body bound shell model.
doi: 10.1016/0370-2693(87)90960-9
1983FE07 Z.Phys. A314, 239 (1983) V.N.Fetisov, L.Majling, J.Zofka, R.A.Eramzhyan Excitation and Structure of Hypernuclear Resonances in (K+, π-), (K+, π0)-Reactions on 1p-Shell Nuclei NUCLEAR REACTIONS 7,6Li, 10,11B, 9Be, 12,13C, 16O, 14,15N(K-, π-), E not given; analyzed data; deduced Lambda-hyperon nuclear subsystem coupling, 1p-, 1s-state single particle energies. Shell model.
doi: 10.1007/BF01879883
1983MA63 Phys.Lett. 130B, 235 (1983) L.Majling, J.Zofka, V.N.Fetisov, R.A.Eramzhyan On Nucleon Decays of Hypernuclear Resonances - Population of Bound Hypernuclear Levels NUCLEAR REACTIONS 14C, 14N(K-, π-), (K-, π0), E=0-25 MeV; calculated hypernuclear resonance production, nucleon decay characteristics.
doi: 10.1016/0370-2693(83)91132-2
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
1980MA21 Phys.Lett. 92B, 256 (1980) L.Majling, M.Sotona, J.Zofka, V.N.Fetisov, R.A.Eramzhyan Supermultiplet Structure and Decay Properties of Hypernuclear 1+ Resonances in 6Li NUCLEAR REACTIONS 6Li(K-, π-), E at 790 MeV/c; calculated σ(E(λ particle), E); deduced λ particle resonance decay properties.
doi: 10.1016/0370-2693(80)90258-0
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
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
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
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
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
1966IS02 Phys.Letters 22, 301 (1966) B.S.Ishkhanov, I.M.Kapitonov, L.Majling Specific Features of the Photodisintegration of Nuclei in the 1f-2p shell NUCLEAR STRUCTURE 58Ni; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(66)90624-X
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