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NSR database version of March 18, 2024.

Search: Author = V.Rodin

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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
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2013RO34      Phys.Rev. C 88, 064318 (2013)

V.Rodin

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
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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
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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
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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
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2012RO44      J.Phys.:Conf.Ser. 375, 042025 (2012)

V.Rodin

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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23169.


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2347. Data from this article have been entered in the XUNDL database. For more information, click here.


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
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2011RO29      Phys.Rev. C 84, 014322 (2011)

V.Rodin, A.Faessler

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 M 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
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2011RO33      Nucl.Phys. B(Proc.Supp.) S217, 35 (2011)

V.Rodin, A.Faessler

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
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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
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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
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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
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2010RO07      Prog.Part.Nucl.Phys. 64, 238 (2010)

V.Rodin

Can the nuclear matrix elements of neutrinoless double beta decay be measured?

doi: 10.1016/j.ppnp.2009.12.019
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2009RO22      Phys.Rev. C 80, 041302 (2009)

V.Rodin, A.Faessler

Can one measure nuclear matrix elements of neutrinoless double β decay?

doi: 10.1103/PhysRevC.80.041302
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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
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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
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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
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2008RO04      Phys.Rev. C 77, 025502 (2008)

V.Rodin, A.Faessler

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
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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
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2007AM07      Phys.Rev. C 76, 014604 (2007)

K.Amos, A.Faessler, V.Rodin

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
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2007RO15      Prog.Part.Nucl.Phys. 59, 268 (2007)

V.Rodin

Neutron skin and giant resonances in nuclei

doi: 10.1016/j.ppnp.2007.01.023
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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
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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
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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
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2006RO14      Prog.Part.Nucl.Phys. 57, 226 (2006)

V.Rodin, A.Faessler

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
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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
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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
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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
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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
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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
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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
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2003RO24      Yad.Fiz. 66, 2178 (2003); Phys.Atomic Nuclei 66, 2128 (2003)

V.A.Rodin, M.H.Urin

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
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2003RO26      Bull.Rus.Acad.Sci.Phys. 67, 1777 (2003)

V.A.Rodin, M.H.Urin

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)

V.A.Rodin, A.E.L.Dieperink

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
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2002RO41      Phys.Rev. C 66, 051303 (2002)

V.Rodin, A.Faessler

Fully renormalized quasiparticle random-phase approximation fulfills Ikeda sum rule exactly

doi: 10.1103/PhysRevC.66.051303
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2002RO42      Phys.Rev. C 66, 064608 (2002)

V.A.Rodin, M.H.Urin

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
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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
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2001RO12      Nucl.Phys. A687, 276c (2001)

V.A.Rodin, M.H.Urin

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
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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
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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
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2000RO12      Phys.Lett. 480B, 45 (2000)

V.A.Rodin, M.H.Urin

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
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2000RO26      Fiz.Elem.Chastits At.Yadra 31, 976 (2000); Phys.Part.Nucl. 31, 490 (2000)

V.A.Rodin, M.G.Urin

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)

V.A.Rodin, M.H.Urin

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
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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
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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)

V.A.Rodin, M.G.Urin

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)

V.A.Rodin, M.H.Urin

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
Citations: PlumX Metrics


1995RO29      Bull.Rus.Acad.Sci.Phys. 59, 724 (1995)

V.A.Rodin, M.G.Urin

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)

V.A.Rodin, M.G.Urin

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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