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NSR database version of May 2, 2024.

Search: Author = B.A.Tulupov

Found 23 matches.

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2023GO08      Phys.Rev. C 108, 014328 (2023)

M.L.Gorelik, S.Shlomo, B.A.Tulupov, M.H.Urin

Semimicroscopic description of isoscalar giant multipole resonances in medium-mass closed-shell nuclei

NUCLEAR STRUCTURE 48Ca, 90Zr, 132Sn, 208Pb; calculated isoscalar giant multipole resonances (up to L=3, including L=0 and 2 overtones) parameters, relative energy-weighted strength functions for isoscalar giant monopole, dipole, quadrupole, and octupole resonances (ISGMR, ISGDR, ISGQR and ISGOR), projected transition densities for isoscalar giant multipole resonances, partial branching ratio of direct one-nucleon decay. Particle-hole dispersive optical model (PHDOM). Comparison to experimental data.

doi: 10.1103/PhysRevC.108.014328
Citations: PlumX Metrics


2021GO08      Phys.Rev. C 103, 034302 (2021)

M.L.Gorelik, S.Shlomo, B.A.Tulupov, M.H.Urin

Properties of isoscalar giant multipole resonances in medium-heavy closed-shell nuclei: A semimicroscopic description

NUCLEAR STRUCTURE 208Pb; calculated relative energy-weighted strength functions for isoscalar giant monopole, dipole, quadrupole, and octupole resonances (ISGMR, ISGDR, ISGQR and ISGOR), parameters, projected transition densities for isoscalar giant multipole resonances (ISGMPR) and compared with experimental data, isoscalar collective low-energy 3- and 2+ states, B(E2), B(E3), strength distribution, transition density, and partial and total probabilities of direct one nucleon decay, branching ratios for direct one-proton decay of the ISGDR. Particle-hole dispersive optical model (PHDOM).

doi: 10.1103/PhysRevC.103.034302
Citations: PlumX Metrics


2020GO08      Phys.Atomic Nuclei 83, 125 (2020)

M.L.Gorelik, B.A.Tulupov, M.H.Urin

Semimicroscopic Description of Isoscalar Giant Multipole Resonances in the 208Pb Nucleus

doi: 10.1134/S1063778820020118
Citations: PlumX Metrics


2019TU10      Physics of Part.and Nuclei 50, 550 (2019)

B.A.Tulupov, M.H.Urin

Direct + Semidirect E1 Photoneutron Reactions: Semimicroscopic Description

doi: 10.1134/s106377961905023X
Citations: PlumX Metrics


2018GO03      Nucl.Phys. A970, 353 (2018)

M.L.Gorelik, S.Shlomo, B.A.Tulupov, M.H.Urin

On unitarity of the particle-hole dispersive optical model

NUCLEAR STRUCTURE 208Pb; calculated energy weighted relative isoscalar giant monopole resonance strength functions, energy-averaged radial component of ISM (IsoScalar Monopole) double transition density at different energies, partial and total branching ratios for direct neutron decay of ISGMR using initial and unitary versions of PHDOM (Particle-Hole Dispersive Optical Model). Branching ratios compared with data.

doi: 10.1016/j.nuclphysa.2017.12.006
Citations: PlumX Metrics


2017DZ02      Physics of Part.and Nuclei 48, 139 (2017)

L.Z.Dzhilavyan, A.M.Lapik, V.G.Nedorezov, B.A.Tulupov

Separation of contributions of isovector E2 and E1 giant resonances in direct and inverse reactions with real and virtual photons

COMPILATION 208Pb; compiled data on E2 isovector electric quadrupole resonance and giant E1 (dipole) one; deduced recommended parameters for E2.

doi: 10.1134/S106377961701004X
Citations: PlumX Metrics


2016GO19      Nucl.Phys. A955, 116 (2016)

M.L.Gorelik, S.Shlomo, B.A.Tulupov, M.H.Urin

Investigation of the energy-averaged double transition density of isoscalar monopole excitations in medium-heavy mass spherical nuclei

NUCLEAR STRUCTURE 208Pb; calculated energy-weighted γ isoscalar giant monopole resonance strength function, transition density, double transition density vs radius for E*=13.8, 23, 33, 38 MeV using CRPA (Continuum RPA) and particle-hole dispersive optical model.

doi: 10.1016/j.nuclphysa.2016.06.004
Citations: PlumX Metrics


2015GO15      Phys.Atomic Nuclei 78, 551 (2015); Yad.Fiz. 78, 595 (2015)

M.L.Gorelik, Sh.Shlomo, B.A.Tulupov, M.H.Urin

Properties of high-energy isoscalar monopole excitations in medium-heavy mass spherical nuclei

NUCLEAR STRUCTURE 208Pb; calculated isoscalar giant monopole resonance strength functions, particle-hole-type isoscalar monopole excitations using FM-DWBA using the Hartree-Fock ground state density and the transition densities obtained from the Hartree-Fock-based random-phase-approximation (RPA).

doi: 10.1134/S1063778815050075
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2014TU06      Phys.Rev. C 90, 034613 (2014)

B.A.Tulupov, M.H.Urin

Description of the simplest photonuclear reactions within the particle-hole dispersive optical model

NUCLEAR REACTIONS 89Y, 140Ce, 208Pb(γ, n), E=10-26 MeV; calculated total and partial photoabsorption σ(E) for isovector giant dipole and quadrupole resonances (IVGDR and IVGQR), partial branching ratios for direct neutron decay. 89Y, 140Ce, 208Pb(n, γ), E=4-16 MeV; calculated partial differential σ(E), anisotropy parameters. Particle-hole dispersive optical model approach. Comparison with experimental results.

doi: 10.1103/PhysRevC.90.034613
Citations: PlumX Metrics


2012TU06      Phys.Atomic Nuclei 75, 1041 (2012); Yad.Fiz. 75, 1105 (2012)

B.A.Tulupov, M.H.Urin

Simplest photonuclear reactions accompanied by the excitation of isovector giant dipole and quadrupole resonances: Semimicroscopic description

NUCLEAR REACTIONS 208,209Pb, 140Ce, 89Y(n, γ), E<18 MeV; calculated σ(θ), asymmetry, partial probabilities and strength functions for direct IVGDR decay. Comparison with available data.

doi: 10.1134/S106377881209013X
Citations: PlumX Metrics


2009TU02      Phys.Atomic Nuclei 72, 737 (2009); Yad.Fiz. 72, 780 (2009)

B.A.Tulupov, M.H.Urin

Fragmentation energy shift of giant nuclear resonances

doi: 10.1134/S106377880904019X
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2009VE01      Phys.Atomic Nuclei 72, 387 (2009); Yad.Fiz. 72, 420 (2009)

S.S.Verbitsky, A.M.Lapic, B.S.Ratner, A.V.Rusakov, M.A.Tikanov, B.A.Tulupov, A.N.Tzelebrovsky

Investigation of giant-dipole-resonance decay in the (γ, n) reactions on 52Cr and 51V nuclei

NUCLEAR REACTIONS 51V(γ, n), E=25.5 MeV; 52Cr(γ, n), E=18.5, 21.0, 23.0 MeV; measured neutron emission spectra, cross sections.

doi: 10.1134/S1063778809030016
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0770.


2006GO14      Phys.Atomic Nuclei 69, 598 (2006); Yad.Fiz. 69, 622 (2006)

M.L.Gorelik, B.A.Tulupov, M.H.Urin

Asymmetry of the Angular Distributions of Products of Photoneutron Direct-Semidirect Reactions in the Region of an Isovector Giant Quadrupole Resonance

NUCLEAR STRUCTURE 208Pb; calculated isovector GQR strength functions, photoabsorption σ.

NUCLEAR REACTIONS 208Pb(γ, n), E ≈ 20-30 MeV; calculated σ(θ), asymmetry. Semimicroscopic approach.

doi: 10.1134/S1063778806040065
Citations: PlumX Metrics


2003GO37      Bull.Rus.Acad.Sci.Phys. 67, 808 (2003)

M.L.Gorelik, B.A.Tulupov, M.H.Urin

Asymmetry of angular distribution of neutrons from (γn) reaction in energy range of isovector electric quadrupole resonance

NUCLEAR REACTIONS 208Pb(γ, n), E=20-30 MeV; calculated angular distribution asymmetry, resonance contributions. Semimicroscopic approach, comparison with data.


1992MU11      Z.Phys. A341, 383 (1992)

S.E.Muraviev, B.A.Tulupov, M.G.Urin

One-Quasiparticle Strength Functions in Medium-Heavy Spherical Nuclei

NUCLEAR STRUCTURE 109Pd, 113,111,115,119Sn, 121,123,129Te, 143Sm, 145Eu, 117Sb; calculated quasiparticle strength function, parameters vs E, widths, spectroscopic factors. 89Zr, 207Pb, 209Bi; calculated quasiparticle strength function, parameters vs E. Generalized coupled-channels approach.


1988MU07      Yad.Fiz. 47, 62 (1988)

S.E.Muravyev, B.A.Tulupov, M.G.Urin

Generalized Coupled-Channels Method and Single-Quasiparticle Strength Functions

NUCLEAR STRUCTURE 109Pd, 111,113,115,119Sn, 121,123,129Te, 89Zr, 207Pb, 209Bi, 143Sm, 145Eu; calculated quasiparticle strength function. Generalized coupled-channels model.


1986MA05      Phys.Lett. 167B, 255 (1986)

B.B.Matveev, B.A.Tulupov, S.E.Muraviev, M.G.Urin

On the Damping of Deep-Lying Hole States in Spherical Nuclei

NUCLEAR STRUCTURE 115,119Sn, 123,129Te; calculated g9/2 neutron-hole state strength function; deduced damping effects. Pheonomenological optical model, one quasiparticle states, noncollective many particle configuration coupling.

doi: 10.1016/0370-2693(86)90340-0
Citations: PlumX Metrics


1985MA63      Izv.Akad.Nauk SSSR, Ser.Fiz. 49, 2241 (1985); Bull.Acad.Sci.USSR, Phys.Ser. 49, No.11, 149 (1985)

B.B.Matveev, S.E.Muravev, B.A.Tulupov, M.G.Urin

On the Relaxation of Subbarrier Single Proton States in Spherical Nuclei

NUCLEAR STRUCTURE 145Eu; calculated subbarrier single proton configuration relaxation strength function.


1984MA58      Izv.Akad.Nauk SSSR, Ser.Fiz. 48, 2051 (1984)

B.B.Matveev, S.E.Muravev, B.A.Tulupov, M.G.Urin

Relaxation of Deep Hole States in Spherical Nuclei

NUCLEAR STRUCTURE 115,119Sn, 123,129Te; calculated 1g9/2 neutron hole state strength functions.


1976GU15      Nucl.Phys. A273, 326 (1976)

G.M.Gurevich, L.E.Lazareva, V.M.Mazur, G.V.Solodukhov, B.A.Tulupov

Giant Resonance in the Total Photoabsorption Cross Section of Z ≈ 90 Nuclei

NUCLEAR REACTIONS 232Th, 235,238U, 239Pu(γ, X), E=7-25 MeV; measured total σ(E); deduced integrated σ, Lorentz line parameter. 232Th, 235,238U, 239Pu deduced average β, quadrupole moment, giant resonance structure. 232Th, 234,235,238U, 238,239,240Pu(γ, X), E=8-20 MeV; calculated σ(E). Dynamic collective model. Enriched, natural targets.

doi: 10.1016/0375-9474(76)90594-7
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0090.


1975GO16      Izv.Akad.Nauk SSSR, Ser.Fiz. 39, 134 (1975); Bull.Acad.Sci.USSR, Phys.Ser. 39, No.1, 116 (1975)

A.M.Goryachev, G.N.Zalesnyi, B.A.Tulupov

Cross Sections of Photoneutron Reactions on 64,66,68Zn, 70,72,74,76Ge, 76,78,80,82Se Nuclei

NUCLEAR REACTIONS 64,66,68Zn, 70,72,74,76Ge, 76,78,80,82Se(γ, n), E < 25 MeV; measured σ.

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0815.


1973GO21      Yad.Fiz. 17, 463 (1973); Sov.J.Nucl.Phys. 17, 236 (1974)

A.M.Goryachev, G.N.Zalesnyi, S.F.Semenko, B.A.Tulupov

Giant Dipole Resonance in Nuclei of the Transitional Region Around A ≈ 190

NUCLEAR REACTIONS 184,186W, 190Os, 185,187Re(γ, n), E=7-20 MeV; measured σ(E).

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0645.


1969DO10      Yadern.Fiz. 9, 675 (1969); Soviet J.Nucl.Phys. 9, 391 (1969)

B.S.Dolbilkin, A.I.Isakov, V.I.Korin, L.E.Lazareva, N.V.Linkova, B.A.Tulupov

Gamma-Ray Absorption by Iron Nuclei in the Giant Resonance Region

NUCLEAR REACTIONS 56Fe(γ, X), E =10-26.5 MeV; measured σ(E).

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0540.


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