NSR Query Results
Output year order : Descending NSR database version of March 18, 2024. Search: Author = V.Rodin Found 52 matches. 2013IG01 Phys.Atomic Nuclei 76, 429 (2013); Yad.Fiz. 76, 468 (2013) S.Yu.Igashov, V.A.Rodin, M.H.Urin Configuration Splitting of the Gamow-Teller Resonance in Antimony Isotopes: Is This a Real or a Virtual Effect? NUCLEAR STRUCTURE 116,118,120Sb; calculated Gamow-Teller strength functions; deduced The structural effect of splitting of the main maximum of the Gamow-Teller resonance. Comparison with available data.
doi: 10.1134/S1063778813030083
2013RO34 Phys.Rev. C 88, 064318 (2013) Relation between isospin-symmetry-breaking correction to superallowed β decay and the energy of the charge-exchange giant monopole resonance RADIOACTIVITY 10C, 38K, 66As, 70Br(EC), (β+); calculated quantities related to isovector monopole resonance (IVMR) strength distributions, nuclear isospin-symmetry breaking correction δC for superallowed β decays through a new representation based on a single parameter. Isospin-consistent continuum random phase approximation approach. Comparison of values of δC obtained with other methods.
doi: 10.1103/PhysRevC.88.064318
2013SI08 Phys.Rev. C 87, 045501 (2013) F.Simkovic, V.Rodin, A.Faessler, P.Vogel 0νββ and 2νββ nuclear matrix elements, quasiparticle random-phase approximation, and isospin symmetry restoration RADIOACTIVITY 48Ca, 76Ga, 82Se, 96Zr, 100Mo, 110Pd, 116Cd, 124Sn, 128,130Te, 134,136Xe(2β-); calculated parameters of pairing interaction, 0νββ and 2νββ matrix elements. Quasiparticle random-phase approximation (QRPA) calculations with Argonne, and CD-Bonn interactions. Proton-neutron interaction separated into isovector (T=1) and isoscalar (T=0) parts.
doi: 10.1103/PhysRevC.87.045501
2012FA02 Phys.Rev. C 85, 035503 (2012) D.-L.Fang, K.Blaum, S.Eliseev, A.Faessler, M.I.Krivoruchenko, V.Rodin, F.Simkovic Evaluation of the resonance enhancement effect in neutrinoless double-electron capture in 152Gd, 164Er, and 180W atoms RADIOACTIVITY 152Gd, 164Er, 180W(2EC); calculated matrix elements and half-lives for neutrinoless double-electron capture. Deformed quasiparticle random-phase approximation using the realistic charge-dependent Bonn (CD-Bonn) nucleon-nucleon interaction. Comparison of half-life with that for neutrinoless 2β decay of 76Ge.
doi: 10.1103/PhysRevC.85.035503
2012FA15 J.Phys.(London) G39, 124006 (2012) A.Faessler, V.Rodin, F.Simkovic Nuclear matrix elements for neutrinoless double-beta decay and double-electron capture RADIOACTIVITY 76Ge, 82Se, 96Zr, 100Mo, 116Cd, 128,130Te, 136Xe(2β-); calculated averaged neutrinoless nuclear matrix elements, T1/2. QRPA, RQRPA methods.
doi: 10.1088/0954-3899/39/12/124006
2012RO44 J.Phys.:Conf.Ser. 375, 042025 (2012) Status of calculations of the nuclear matrix elements for double beta decay RADIOACTIVITY 48Ca, 76Ge, 82Se, 94,96Zr, 98,100Mo, 104Ru, 110Pd, 116Cd, 124Sn, 128,130Te, 136Xe, 150Nd, 154Sm, 160Gd(2β-); calculated neutrinoless double beta decay transition matrix elements. QRPA approach, projected Hartree-Fock-Bogoliubov method, Interacting Boson Model (IBM-2), comparison with available data.
doi: 10.1088/1742-6596/375/1/042025
2012SA23 Phys.Rev. C 85, 061301 (2012) M.Sasano, H.Sakai, K.Yako, T.Wakasa, M.Dozono, V.Rodin, A.Faessler, K.Fujita, M.B.Greenfield, K.Hatanaka, K.Itoh, T.Kawabata, H.Kuboki, Y.Maeda, K.Miki, K.Muto, S.Noji, H.Okamura, Y.Sakemi, K.Sekiguchi, Y.Shimizu, Y.Sasamoto, Y.Tameshige, A.Tamii, T.Uesaka Gamow-Teller transition strengths in the intermediate nucleus of the 116Cd double-β decay by the 116Cd(p, n)116In and 116Sn(n, p)116In reactions at 300 MeV NUCLEAR REACTIONS 116Cd(p, n), E=295 MeV; 116Sn(n, p), E=293 MeV; measured E(n), I(n) using n-TOF method, E(p), I(p), double-differential σ, σ(θ); deduced B(GT) strengths for transitions to 1+ states in 116In in β- and β+ channels. Comparison with QRPA predictions including IVSM component. Relevance to nuclear matrix element of the 116Cd ββ decay.
doi: 10.1103/PhysRevC.85.061301
2011FA02 Phys.Rev. C 83, 034320 (2011) D.Fang, A.Faessler, V.Rodin, F.Simkovic Neutrinoless double-β decay of deformed nuclei within quasiparticle random-phase approximation with a realistic interaction RADIOACTIVITY 76Ge, 150Nd, 160Gd(2β-); calculated nuclear matrix elements for neutrinoless double β decay using quasiparticle random-phase approximation with realistic residual interaction. Analyzed short-range correlations and the quenching of the axial vector coupling constant. 150Nd; probe of the Majorana neutrino mass.
doi: 10.1103/PhysRevC.83.034320
2011GU14 Phys.Rev. C 83, 064318 (2011) C.J.Guess, T.Adachi, H.Akimune, A.Algora, S.M.Austin, D.Bazin, B.A.Brown, C.Caesar, J.M.Deaven, H.Ejiri, E.Estevez, D.Fang, A.Faessler, D.Frekers, H.Fujita, Y.Fujita, M.Fujiwara, G.F.Grinyer, M.N.Harakeh, K.Hatanaka, C.Herlitzius, K.Hirota, G.W.Hitt, D.Ishikawa, H.Matsubara, R.Meharchand, F.Molina, H.Okamura, H.J.Ong, G.Perdikakis, V.Rodin, B.Rubio, Y.Shimbara, G.Susoy, T.Suzuki, A.Tamii, J.H.Thies, C.Tur, N.Verhanovitz, M.Yosoi, J.Yurkon, R.G.T.Zegers, J.Zenihiro The 150Nd(3He, t) and 150Sm(t, 3He) reactions with applications to ββ decay of 150Nd NUCLEAR REACTIONS 150Nd(3He, t), E=140 MeV/nucleon; 150Sm(t, 3He), E=115 MeV/nucleon; measured triton and 3He spectra, excitation energy spectra, differential cross sections, σ(θ) 150Pm; deduced B(GT) strengths; isovector spin-flip giant monopole resonance (IVSGMR). Grand Raiden Spectrometer for (3He, t) and S-800 spectrometer for (t, 3He). Comparison with Quasi-Particle Random Phase Approximation (QRPA) calculations. Application to double β decay of 150Nd. RADIOACTIVITY 150Nd(2β-); calculated matrix elements for 0νββ and 2νββ decay modes using QRPA calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.064318
2011IG01 Phys.Rev. C 83, 044301 (2011) S.Yu.Igashov, V.Rodin, A.Faessler, M.H.Urin Gamow-Teller strength distributions for ββ-decaying nuclei within continuum quasiparticle random-phase approximation RADIOACTIVITY 76Ge, 100Mo, 116Cd, 130Te(2β-); calculated Gamow-Teller amplitudes and strength distributions, matrix elements for 2νββ decay mode. Continuum quasiparticle random-phase approximation (QRPA). Comparison with experimental data.
doi: 10.1103/PhysRevC.83.044301
2011RO29 Phys.Rev. C 84, 014322 (2011) Origin of a sensitive dependence of calculated ββ-decay amplitudes on the particle-particle residual interaction RADIOACTIVITY 76Ge, 100Mo, 130Te(2β-); calculated Gamow-Teller (GT) and Fermi matrix elements M2ν for 2νββ decay, and the monopole transition contributions to the total matrix elements M0null of neutrinoless ββ decay. Quasiparticle random-phase approximation (QRPA and RQRPA) approach.
doi: 10.1103/PhysRevC.84.014322
2011RO33 Nucl.Phys. B(Proc.Supp.) S217, 35 (2011) Assessing the possibility to measure nuclear matrix elements of neutrinoless double beta decay in charge-exchange reactions
doi: 10.1016/j.nuclphysbps.2011.04.060
2010ES06 J.Phys.(London) G37, 125108 (2010) A.Escuderos, A.Faessler, V.Rodin, F.Simkovic Contributions of different neutron pairs in different approaches for neutrinoless double-beta decay RADIOACTIVITY 48Ca, 76Ge, 82Se, 94,96Zr, 98,100Mo, 104Ru, 110Pd, 116Cd, 124Sn, 128,130Te, 136Xe, 150Nd, 154Sm(2β-); calculated the neutrinoless 2β-decay matrix elements. QRPA, shell, HFB, IBM models.
doi: 10.1088/0954-3899/37/12/125108
2010FA03 Phys.Rev. C 81, 037303 (2010) D.Fang, A.Faessler, V.Rodin, M.Saleh Yousef, F.Simkovic Running sums for 2νββ-decay matrix elements within the quasiparticle random-phase approximation with account for deformation RADIOACTIVITY 76Ge, 150Nd(2β-); calculated matrix elements (running sums) for 2-neutrino double β decay using deformation and p-p strength parameters in quasiparticle random-phase approximation (QRPA) approach.
doi: 10.1103/PhysRevC.81.037303
2010FA17 Phys.Rev. C 82, 051301 (2010) D.-L.Fang, A.Faessler, V.Rodin, F.Simkovic Neutrinoless double-β decay of 150Nd accounting for deformation NUCLEAR STRUCTURE 150Nd(2β-); calculated neutrinoless double-beta decay matrix elements while accounting for β2 deformation parameter. Microscopic calculation with quasiparticle random phase approximation (QRPA) approach and realistic residual interaction. Relevance for SNO+ collaboration and the best sensitivity for the Majorana neutrino mass measurement.
doi: 10.1103/PhysRevC.82.051301
2010RO07 Prog.Part.Nucl.Phys. 64, 238 (2010) Can the nuclear matrix elements of neutrinoless double beta decay be measured?
doi: 10.1016/j.ppnp.2009.12.019
2009RO22 Phys.Rev. C 80, 041302 (2009) Can one measure nuclear matrix elements of neutrinoless double β decay?
doi: 10.1103/PhysRevC.80.041302
2009SA04 Phys.Rev. C 79, 014314 (2009) M.Saleh Yousef, V.Rodin, A.Faessler, F.Simkovic Two-neutrino double β decay of deformed nuclei within the quasiparticle random-phase approximation with a realistic interaction RADIOACTIVITY 76Ge(2β-), 150Nd(2β-); calculated excitation energies, Gamow-Teller strength distributions. Quasiparticle random phase approximation.
doi: 10.1103/PhysRevC.79.014314
2009SI11 Phys.Rev. C 79, 055501 (2009) F.Simkovic, A.Faessler, H.Muther, V.Rodin, M.Stauf 0ν ΒΒ-decay nuclear matrix elements with self-consistent short-range correlations RADIOACTIVITY 76Ge, 82Se, 96Zr, 100Mo, 116Cd, 128Te, 130Te, 136Xe(2β-); calculated nucleon wave function, ratio of neutrino potentials and nuclear matrix elements for neutrinoless double beta decay using renormalized quasiparticle random phase approximation (RQRPA) and standard QRPA methods.
doi: 10.1103/PhysRevC.79.055501
2008IG02 Phys.Atomic Nuclei 71, 1267 (2008) S.Yu.Igashov, V.A.Rodin, M.H.Urin, A.Faessler Gamow-Teller strength distributions for ββ-decaying nuclei within continuum QRPA NUCLEAR STRUCTURE 116Cd(2β-); 130Te(2β-); calculated Gamow-Teller strength distributions; QRPA model.
doi: 10.1134/S1063778808070211
2008RO04 Phys.Rev. C 77, 025502 (2008) Description of double β decay within the continuum quasiparticle random-phase approximation RADIOACTIVITY 76Ge, 100Mo, 130Te (2β-); calculated matrix elements using cQPRA model. 2νββ and 0νββ decay.
doi: 10.1103/PhysRevC.77.025502
2008SI14 Phys.Rev. C 77, 045503 (2008) F.Simkovic, A.Faessler, V.Rodin, P.Vogel, J.Engel Anatomy of the 0νββ nuclear matrix elements RADIOACTIVITY 76Ge, 82Se, 96Zr, 100Mo, 116Cd, 128,130Te, 136Xe (2β-); calculated angular momenta, half-lives, neutrinoless double β decay matrix elements. Quasiparticle random phase approximation.
doi: 10.1103/PhysRevC.77.045503
2007AM07 Phys.Rev. C 76, 014604 (2007) Charge-exchange reaction cross sections and the Gamow-Teller strength for double β decay NUCLEAR REACTIONS 76Ge(p, n)76As, 76Se(n, p)76As, E=200 MeV; calculated σ(θ) and total cross sections.
doi: 10.1103/PhysRevC.76.014604
2007RO15 Prog.Part.Nucl.Phys. 59, 268 (2007) Neutron skin and giant resonances in nuclei
doi: 10.1016/j.ppnp.2007.01.023
2007SA31 Prog.Part.Nucl.Phys. 59, 494 (2007) M.Saleh Yousef, V.Rodin, A.Faessler Solution of the BCS equations for deformed nuclei using realistic pairing interaction NUCLEAR STRUCTURE 150Nd, 150Sm; calculated proton and neutron pairing strengths as a function of the deformation parameter using BCS formalism.
doi: 10.1016/j.ppnp.2007.01.015
2007VA01 Phys.Rev. C 75, 014311 (2007) H.K.T.van der Molen, H.Akimune, A.M.van den Berg, I.Daito, H.Fujimura, Y.Fujita, M.Fujiwara, M.N.Harakeh, M.Hunyadi, F.Ihara, T.Inomata, K.Ishibashi, J.Janecke, N.Kalantar-Nayestanaki, H.Laurent, I.Lhenry, T.W.O'Donnell, V.A.Rodin, A.Tamii, H.Toyokawa, M.H.Urin, H.Yoshida, M.Yosoi Damping mechanisms of high-lying single-particle states in 91Nb NUCLEAR REACTIONS 90Zr(α, t), (α, pt), E=180 MeV; measured triton and proton spectra, pt-coin. 91Nb deduced excited states energies, proton emission features. Optical-model coupled-channels analysis.
doi: 10.1103/PhysRevC.75.014311
2006RO04 Nucl.Phys. A766, 107 (2006); Erratum Nucl.Phys. A793, 213 (2007) V.A.Rodin, A.Faessler, F.Simkovic, P.Vogel Assessment of uncertainties in QRPA 0νββ-decay nuclear matrix elements NUCLEAR STRUCTURE 76Ge, 82Se, 96Zr, 100Mo, 116Cd, 128,130Te, 136Xe, 150Nd; calculated 0ν-accompanied 2β-decay matrix elements. Quasiparticle RPA and renormalized quasiparticle RPA.
doi: 10.1016/j.nuclphysa.2005.12.004
2006RO14 Prog.Part.Nucl.Phys. 57, 226 (2006) First application of the continuum-QRPA to the description of the double beta decay RADIOACTIVITY 130Te(2β-); calculated 0νββ- and 2νββ-decay amplitudes. Quasiparticle RPA.
doi: 10.1016/j.ppnp.2006.01.007
2006RO25 Czech.J.Phys. 56, 495 (2006) V.Rodin, A.Faessler, F.Simkovic, P.Vogel Uncertainties in the 0νββ-decay nuclear matrix elements RADIOACTIVITY 48Ca, 76Ge, 82Se, 96Zr, 100Mo, 116Cd, 128,130Te, 136Xe(2β-); analyzed 0νββ-decay matrix elements, uncertainties. Quasiparticle RPA, renormalized quasiparticle RPA.
doi: 10.1007/s10582-006-0113-7
2005RO01 Nucl.Phys. A747, 297 (2005) V.A.Rodin, M.H.Urin, A.Faessler Sensitive behavior of 2νββ-decay amplitude within QRPA and broken SU(4) symmetry in nuclei NUCLEAR STRUCTURE 76Ge, 100Mo, 130Te; calculated 2ν2β-decay amplitudes. Quasiparticle RPA, broken SU(4) symmetry.
doi: 10.1016/j.nuclphysa.2004.10.010
2004KU16 J.Phys.(London) G30, 1253 (2004) A.A.Kuliev, A.Faessler, M.Guner, V.Rodin Fully renormalized quasi-particle random phase approximation, spurious states and ground state correlations NUCLEAR STRUCTURE 150Nd, 154Sm, 168Er; calculated 1+ states energies, configurations. Renormalized quasiparticle RPA.
doi: 10.1088/0954-3899/30/9/023
2003DI12 Phys.Rev. C 68, 064307 (2003) A.E.L.Dieperink, Y.Dewulf, D.Van Neck, M.Waroquier, V.Rodin Nuclear symmetry energy and the neutron skin in neutron-rich nuclei
doi: 10.1103/PhysRevC.68.064307
2003PA53 Phys.Rev. C 68, 064310 (2003); Erratum Phys.Rev. C 75, 059902 (2007) L.Pacearescu, V.Rodin, F.Simkovic, A.Faessler Two-neutrino double β decay within fully renormalized quasiparticle random-phase approximation: Effect of the restoration of the Ikeda sum rule NUCLEAR STRUCTURE 76Ge, 82Se, 100Mo, 116Cd, 128Te, 130Xe; calculated matrix elements for 2ν-accompanied 2β-decay, effect of sum rule. Fully renormalized quasiparticle RPA.
doi: 10.1103/PhysRevC.68.064310
2003RO18 Phys.Rev. C 68, 044302 (2003) V.A.Rodin, A.Faessler, F.Simkovic, P.Vogel Uncertainty in one 0νββ decay nuclear matrix elements NUCLEAR STRUCTURE 76Ge, 100Mo, 130Te, 136Xe; calculated 0ν-accompanied 2β-decay matrix elements. Renormalized quasiparticle RPA.
doi: 10.1103/PhysRevC.68.044302
2003RO24 Yad.Fiz. 66, 2178 (2003); Phys.Atomic Nuclei 66, 2128 (2003) On the Fermi and Gamow-Teller Strength Distributions in Medium-Heavy Mass Nuclei NUCLEAR STRUCTURE 90Zr, 112,114,116,118,120,122,124Sn, 208Pb; calculated Fermi and Gamow-Teller strength distributions. Self-consistent continuum RPA approach.
doi: 10.1134/1.1634320
2003RO26 Bull.Rus.Acad.Sci.Phys. 67, 1777 (2003) Semimicroscopic description of photonuclear reactions with excitation of giant dipole resonance in medium-heavy nuclei NUCLEAR REACTIONS 89Y, 140Ce, 208Pb(γ, X), E=8-24 MeV; calculated photoabsorption σ, GDR excitation. 89Y, 140Ce, 208Pb(n, γ), E=4-20 MeV; calculated σ(E, θ), GDR excitation. Semimicroscopic approach, comparison with data. NUCLEAR STRUCTURE 48Ca, 208Pb; calculated partial branching ratios for direct neutron decay of GDR. Semimicroscopic approach, comparison with data.
2002RO27 Phys.Lett. 541B, 71 (2002) Electromagnetic Transitions between Giant Resonances within a Continuum-RPA Approach NUCLEAR STRUCTURE 90Nb, 208Bi; calculated radiative widths and branching ratios for E1 transitions between resonance states. Continuum-RPA approach.
doi: 10.1016/S0370-2693(02)02187-1
2002RO41 Phys.Rev. C 66, 051303 (2002) Fully renormalized quasiparticle random-phase approximation fulfills Ikeda sum rule exactly
doi: 10.1103/PhysRevC.66.051303
2002RO42 Phys.Rev. C 66, 064608 (2002) Semimicroscopical description of the simplest photonuclear reactions accompanied by excitation of the giant dipole resonance in medium-heavy mass nuclei NUCLEAR REACTIONS 89Y, 140Ce, 208Pb(γ, X), E ≈ 8-24 MeV; calculated photoabsorption σ. 89Y, 140Ce, 208Pb(γ, n), E ≈ 8-24 MeV; calculated σ(E, θ=90°). Continuum RPA, effect of GDR excitation discussed. NUCLEAR STRUCTURE 48Ca, 208Pb; analyzed GDR neutron decay branching ratio.
doi: 10.1103/PhysRevC.66.064608
2001KR23 Phys.Rev. C64, 067302 (2001) A.Krasznahorkay, H.Akimune, M.Fujiwara, M.N.Harakeh, J.Janecke, V.A.Rodin, M.H.Urin, M.Yosoi Distribution of the Gamow-Teller Strength in 90Nb and 208Bi NUCLEAR REACTIONS 90Zr, 208Pb(3He, t), E=450 MeV; measured triton spectra. 90Nb, 208Bi deduced Gamow-Teller strength distributions. Continuum RPA calculations.
doi: 10.1103/PhysRevC.64.067302
2001RO12 Nucl.Phys. A687, 276c (2001) Direct-Decay Properties of Charge-Exchange Spin Giant Resonances NUCLEAR STRUCTURE 90Nb, 208Bi; calculated Gamow-Teller, spin-dipole, isovector spin-monopole and isovector monopole giant resonances parameters, strength functions, proton decay properties. Continuum Random Phase Approximations method, comparison with data.
doi: 10.1016/S0375-9474(01)00632-7
2001VA10 Phys.Lett. 502B, 1 (2001) H.K.T.van der Molen, H.Akimune, A.M.van den Berg, I.Daito, H.Fujimura, Y.Fujita, M.Fujiwara, M.N.Harakeh, F.Ihara, T.Inomata, K.Ishibashi, J.Janecke, N.Kalantar-Nayestanaki, H.Laurent, I.Lhenry, T.W.O'Donnell, V.A.Rodin, A.Tamii, H.Toyokawa, M.H.Urin, H.Yoshida, M.Yosoi Structure of 11/2- Analog State in 91Nb Populated by the 90Zr(α, t) Reaction NUCLEAR REACTIONS 90Zr(α, t), E=180 MeV; measured triton spectra, delayed proton spectra following IAS decay. 91Nb level deduced configuration. 91Nb, 91Zr deduced neutron, proton separation energies, spectroscopic factors. Comparison with continuum RPA predictions.
doi: 10.1016/S0370-2693(01)00168-X
2001VA28 Acta Phys.Hung.N.S. 13, 21 (2001) A.M.van den Berg, H.Akimune, I.Daito, H.Fujimura, M.Fujiwara, Y.Fujita, M.N.Harakeh, F.Ihara, T.Inomata, K.Ishibashi, J.Janecke, N.Kalantar-Nayestanaki, H.Laurent, I.Lhenry, H.K.T.van der Molen, T.O'Donnell, V.A.Rodin, A.Tamii, H.Toyokawa, M.H.Urin, H.Yoshida, M.Yosoi Collective and Single-Particle States at High Excitation Energy NUCLEAR REACTIONS 90Zr(α, t), E=180 MeV; measured triton spectra, delayed proton spectra following residual nucleus decay, σ(E, θ). 91Nb deduced level configurations, IAS decay features, damping of single-paritcle states.
doi: 10.1556/APH.13.2001.1-3.4
2000RO12 Phys.Lett. 480B, 45 (2000) On the Neutron Radiative Capture in the Vicinity of the Giant Dipole Resonance NUCLEAR REACTIONS 208Pb(n, γ), E=5-18 MeV; calculated capture σ, σ(E, θ) near GDR. Semimicroscopical approach, comparisons with data.
doi: 10.1016/S0370-2693(00)00367-1
2000RO26 Fiz.Elem.Chastits At.Yadra 31, 976 (2000); Phys.Part.Nucl. 31, 490 (2000) Description of Radiative and ' Weak ' Strength Functions of Nuclear Compound States within a Semimicroscopic Approach NUCLEAR STRUCTURE 54Cr, 106Pd, 114Cd, 116In, 137,139Ba, 144Nd; calculated electric and magnetic dipole decay strength distributions. Semimicroscopic approach, comparisons with data.
2000RO38 Phys.Rev. C62, 067601 (2000) E1 Transitions between Spin-Dipole and Gamow-Teller Giant Resonances NUCLEAR STRUCTURE 90Zr, 90Nb, 208Pb, 208Bi; calculated branching ratios for E1 transitions between spin-dipole and Gamow-Teller resonances. Extended continuum RPA approach.
doi: 10.1103/PhysRevC.62.067601
1999MO04 Phys.Lett. 447B, 8 (1999) E.A.Moukhai, V.A.Rodin, M.H.Urin Structure and Decay Properties of Spin-Dipole Giant Resonances within a Semimicroscopical Approach NUCLEAR STRUCTURE 208Bi; calculated spin-dipole giant resonance strength distribution, direct proton decay branching ratios. Continuum RPA.
doi: 10.1016/S0370-2693(98)01578-0
1999MO32 Bull.Rus.Acad.Sci.Phys. 63, 88 (1999) E.A.Moukhai, V.A.Rodin, M.H.Urin Semimicroscopic Description of the Structure and Decay Characteristics of Charge-Exchange Spin-Dipole Giant Resonances NUCLEAR STRUCTURE 208Bi, 208Tl; calculated strength functions and total proton width of the spin dipole giant resonance. Random Phase Approximation.
1998RO43 Bull.Rus.Acad.Sci.Phys. 62, 1693 (1998) Photon Strength Functions of Neutron Resonances within Semimicroscopic Approach NUCLEAR STRUCTURE 54Cr, 106Pd, 114Cd, 116In, 144Nd; calculated M1, E1 photon strength functions of neutron resonances. Semimicroscopic approach.
1997RO02 Phys.Rev. C55, 1583 (1997) Evaluation of the Mean Intensity of the P-Odd Mixing of Nuclear Compound States NUCLEAR STRUCTURE 57Fe, 82Br, 110,108Ag, 112,114Cd, 116In, 118Sn, 140La, 233Th, 238U; calculated parity violating interaction rms matrix elements. Unified description of mixing, electromagnetic transition.
doi: 10.1103/PhysRevC.55.1583
1995RO29 Bull.Rus.Acad.Sci.Phys. 59, 724 (1995) Quantitatively Estimated Average Intensity of P-Odd Mixing of Nuclear Compound States NUCLEAR STRUCTURE 57Fe, 82Br, 114,112Cd, 118Sn, 140La, 233Th, 239U; calculated levels Γγ(M1)/(Γγ(E1)), P-odd mixing matrix elements. Phenomenological model.
1994RO22 Bull.Rus.Acad.Sci.Phys. 58, 733 (1994) On Ratio of Intensities of E1 and M1 Transitions between Nuclear Compound States NUCLEAR STRUCTURE 144Nd, 137,139Ba; calculated E1, M1 transition Iγ for compound nuclei. Semi-empirical approach.
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