NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = S.Kamerdzhiev Found 81 matches. 2022KA54 Phys.Atomic Nuclei 85, 425 (2022) Characteristics of Pygmy and Giant Resonances within a Microscopic Model for Taking into Account Complex Configurations: Formalism
doi: 10.1134/S1063778822050052
2022SH13 Phys.Atomic Nuclei 85, 42 (2022) M.I.Shitov, D.A.Voitenkov, S.P.Kamerdzhiev, S.V.Tolokonnikov Self-Consistent Calculations of Probabilities for Transitions between 3-1 and 2+1 One-Phonon States in Tin Isotopes NUCLEAR STRUCTURE 118,120,122,124Sn; calculated probabilities for transitions between low-lying one-phonon states in nuclei where there is pairing, B(E1). Self-consistent approach based on the DF3-a Fayans energy density functional.
doi: 10.1134/S1063778822010124
2021KA49 Phys.Atomic Nuclei 84, 649 (2021) Microscopic Model to Take into Account Complex Configurations for Pygmy and Giant Resonances
doi: 10.1134/S1063778821050082
2020KA57 Eur.Phys.J. A 56, 265 (2020) Microscopic theory of pygmy- and giant resonances: accounting for complex 1p1h(X)phonon configurations
doi: 10.1140/epja/s10050-020-00224-7
2018KA45 JETP Lett. 108, 155 (2018) S.P.Kamerdzhiev, D.A.Voitenkov, E.E.Saperstein, S.V.Tolokonnikov Self-Consistent Calculations of the Quadrupole Moments of the Lowest 3- States in Sn and Pb Isotopes NUCLEAR STRUCTURE 100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132Sn, 190,192,194,196,198,200,202,204,206,208,210,212Pb; calculated energies and B(E3). Comparison with available data.
doi: 10.1134/S0021364018150079
2018LA07 Phys.Rev. C 97, 054329 (2018) A.C.Larsen, J.E.Midtbo, M.Guttormsen, T.Renstrom, S.N.Liddick, A.Spyrou, S.Karampagia, B.A.Brown, O.Achakovskiy, S.Kamerdzhiev, D.L.Bleuel, A.Couture, L.Crespo Campo, B.P.Crider, A.C.Dombos, R.Lewis, S.Mosby, F.Naqvi, G.Perdikakis, C.J.Prokop, S.J.Quinn, S.Siem Enhanced low-energy γ-decay strength of 70Ni and its robustness within the shell model RADIOACTIVITY 70Co(β-)[from 9Be(86Kr, X), E=140 MeV/nucleon followed by fragment separation using A1900 fragment separator at NSCL-MSU]; measured Eγ, Iγ, summed γ energies, β-γ-coin using double-sided silicon strip detector (DSSD) for electrons placed in the center of the Summing NaI (SuN) total absorption spectrometer for γ radiation. 70Ni; deduced nuclear level density (NLD) and γ-strength function (γSF) using β-Oslo method. Comparison with previous experimental results, and with HFB+c calculations. NUCLEAR STRUCTURE 70Ni; calculated levels, J, π, B(E2), level densities, γSF, summed γSF, and M1 γ strengths for A=56-76 Ni isotopes. Quasiparticle time-blocking approximation and large-scale shell-model calculations with CA48MH1G and JUN45 interactions. Comparison with experimental results.
doi: 10.1103/PhysRevC.97.054329
2017KA54 JETP Lett. 106, 139 (2017) S.P.Kamerdzhiev, D.A.Voitenkov, E.E.Saperstein, S.V.Tolokonnikov, M.I.Shitov Self-consistent description of EL transitions between one-phonon states in magic nuclei NUCLEAR STRUCTURE 132Sn, 208Pb; calculated energy levels, J, π, B(E2) using quantum theory of many-body systems.
doi: 10.1134/S0021364017150085
2017SA24 J.Phys.(London) G44, 065104 (2017) E.E.Saperstein, S.Kamerdzhiev, D.S.Krepish, S.V.Tolokonnikov, D.Voitenkov The first self-consistent calculation of quadrupole moments of odd semi-magic nuclei accounting for phonon-induced corrections NUCLEAR MOMENTS 111,113,115,117,119,121,123,125,127In, 115,117,119,121,123Sb; calculated quadrupole moments. Comparison with experimental data.
doi: 10.1088/1361-6471/aa65f5
2016AC03 JETP Lett. 104, 374 (2016) O.I.Achakovskiy, S.P.Kamerdzhiev, V.I.Tselyaev Radiative strength function and the pygmy dipole resonance in 208Pb and 70Ni NUCLEAR REACTIONS 208Pb, 70Ni(γ, X), (3He, 3He'), E<10 MeV; analyzed available data; 208Pb, 70Ni. deduced the pygmy-resonance parameters and the E1 strength function.
doi: 10.1134/S0021364016180053
2016KA64 Phys.Atomic Nuclei 79, 567 (2016) S.P.Kamerdzhiev, O.I.Achakovskiy, A.V.Avdeenkov, S.Goriely On microscopic theory of radiative nuclear reaction characteristics NUCLEAR REACTIONS 72Ni(γ, x), E=5-14 MeV; calculated photoabsorption σ. 115,119Sn(n, γ)(n, γ), E=0.007-10 MeV;121Sn, 208Pb(n, γ), E=0.001-10 MeV; calculated σ. 67Ni, 117,119Sn(n, γ), E≈50, 560 keV; calculated γ multiplicity, σ(Εγ). Different approaches and data and some results taken from publications. NUCLEAR STRUCTURE 58,68,72Ni; calculated pygmy dipole resonance energy, fraction of EWSR. 132Sn, 208Pb; calculated E1 photon strength function. 58,60,62,68,72Ni;110,112,116,118,120,122,124,132,136Sn, 208Pb; calculated γ radiative width Γγ for s-wave neutrons. Different approaches and data and some results taken from publications.
doi: 10.1134/S106377881604013X
2015AC01 Phys.Rev. C 91, 034620 (2015) O.Achakovskiy, A.Avdeenkov, S.Goriely, S.Kamerdzhiev, S.Krewald Impact of phonon coupling on the photon strength function NUCLEAR STRUCTURE 110,112,116,118,120,122,124,132,136Sn, 58,62,68,72Ni; calculated E1 strength function, average radiative width. QRPA, quasiparticle time blocking approximation. Comparison with experimental data. NUCLEAR REACTIONS 115,119Sn(n, γ), E=0.007-10 MeV; calculated σ(E).QRPA, Quasiparticle time blocking approximation. Comparison with experimental data.
doi: 10.1103/PhysRevC.91.034620
2014AC01 Eur.Phys.J. A 50, 6 (2014) O.I.Achakovskiy, S.P.Kamerdzhiev, E.E.Saperstein, S.V.Tolokonnikov Magnetic moments of odd-odd spherical nuclei NUCLEAR STRUCTURE 14,15,16N, 15,17O, 16,17,18,19F, 38,39,40K, 39,41Ca, 40,42Sc, 40,41,42Sc, 54,55,56,57,58,59,60,61Co, 55,56,57,58,59,61Ni, 56,57,58Cu, 87Kr, 89,91Zr, 89Y, 87,90,91Nb, 91,93Mo, 93,94Tc, 95Ru, 105,107,109,111,131,132In, 107,111,113,115,123,125,127,132,133Sn, 113,115,117,123,125,126,127,128,129,132,133,134Sb, 135,137Xe, 136,137,138Cs, 137,139Ba, 138,139,140La, 139,141Ce, 143Nd, 141,142Pr, 143,145,147Sm, 144,145,146Eu, 147Gd, 191,193,195,197,199,201,203,205,206,208Tl, 193,195,197,199,201,203,205,207,209,211Pb, 201,202,203,204,205,206,207,208,209,210,211,212Bi, 211Rn, 213Ra, 212,213Fr; calculated ground state and excited state μ. Compared with other calculations and available data. 58Co, 106,110In, 124Sb, 194,196,198,200,202,204Tl; calculated ground state μ obtained by mixing of two configurations. Compared to data. 55,56,57,59,60Co, 57,61Ni; calculated μ. Compared with published shell model calculations. Self-consistent TFFS (Theory of Finite Fermi Systems).
doi: 10.1140/epja/i2014-14006-1
2014SA54 Phys.Atomic Nuclei 77, 1033 (2014) E.E.Saperstein, O.I.Achakovskiy, S.P.Kamerdzhiev, S.Krewald, J.Speth, S.V.Tolokonnikov Phonon coupling effects in magnetic moments of magic and semimagic nuclei NUCLEAR STRUCTURE 188,190,192,194,196,198,200,202,204,206,207,208,209Pb, 187,189,191,193,195,197,199,201,203,205,207Tl, 209Bi, 100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134Sn, 105,107,109,111,113,115,117,119,121,123,125,127In, 115,117,119,121,123,125,127,129,131,133Sb; calculated energy levels, J, π, magnetic moments, B(E2). Comparison with experimental data.
doi: 10.1134/S1063778814080122
2013SA42 Europhys.Lett. 103, 42001 (2013) E.E.Saperstein, S.Kamerdzhiev, S.Krewald, J.Speth, S.V.Tolokonnikov A model for phonon coupling contributions to electromagnetic moments of odd spherical nuclei NUCLEAR STRUCTURE 187,188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211Tl, 99,100,101,102,103,104,105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131In, 101,102,103,104,105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133Sb; calculated magnetic moments. Theory of Finite Fermi Systems (TFFS), comparison with experimental data.
doi: 10.1209/0295-5075/103/42001
2012TO07 Eur.Phys.J. A 48, 70 (2012) S.V.Tolokonnikov, S.Kamerdzhiev, S.Krewald, E.E.Saperstein, D.Voitenkov Quadrupole moments of spherical semi-magic nuclei within the self-consistent Theory of Finite Fermi Systems NUCLEAR MOMENTS 39,41Ca, 85,87Kr, 87,89Sr, 89,91Zr, 101,103,105,107,109,111,113,115,117,119,121,123,125,127,129,131Sn, 135,137Xe, 137,139Ba, 141,143Nd, 143,145Sm, 147Gd, 197,199,201,205,211Pb, 39K, 41Sc, 87Rb, 105,107,109,111,113,115,117,119,121,123,125,127In, 115,119,121,123Sb, 137Cs, 139La, 141Pr, 145Eu, 205Tl, 203,205,207,209,213Bi; calculated quadrupole moments using self-consistent Finite Fermi Systems with two different functionals. Compared with data.
doi: 10.1140/epja/i2012-12070-1
2012VO03 Phys.Rev. C 85, 054319 (2012) D.Voitenkov, S.Kamerdzhiev, S.Krewald, E.E.Saperstein, S.V.Tolokonnikov Self-consistent calculations of quadrupole moments of the first 2+ states in Sn and Pb isotopes NUCLEAR MOMENTS 100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134Sn, 190,192,194,196,198,200,202,204,206,208Pb; calculated static quadrupole moments of first 2+ states. Ground state correlations. Dependence of quadrupole moment on neutron access. Self-consistent calculations based on quasiparticle random-phase approximation (QRPA) and energy density functionals. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.054319
2011AV04 Phys.Rev. C 83, 064316 (2011) A.Avdeenkov, S.Goriely, S.Kamerdzhiev, S.Krewald Self-consistent calculations of the strength function and radiative neutron capture cross section for stable and unstable tin isotopes NUCLEAR STRUCTURE 100,110,112,114,120,124,132,136,142,150,156,166,176Sn; calculated E1 strength functions, integral characteristics of GDR versus A, giant-dipole and pygmy-dipole resonances (GDR, PDR), neutron and proton transitional densities using self-consistent microscopic theory as well as standard quasiparticle random phase approximation (QRPA, QTBA). Comparison with experimental data. Discussed properties of GDR and PDR. NUCLEAR REACTIONS 123,131,149Sn(n, γ), E=0.001-10 MeV; calculated neutron capture cross sections obtained with E1 strength functions calculated within the QRPA, QTBA, and Kopecky-Uhl approaches.
doi: 10.1103/PhysRevC.83.064316
2011AV09 J.Korean Phys.Soc. 59, 967s (2011) A.Avdeenkov, S.Goriely, S.Kamerdzhiev Impact of the Phonon Coupling on the Dipole Strength and Radiative Neutron Capture NUCLEAR REACTIONS 124,132,150Sn(γ, X), E=4-30 MeV;123,131,149Sn(n, γ), E=1.E-3-10 MeV; calculated σ; deduced γ-ray strength functions. Self-consistent extended theory of finite Fermi systems (DTBA) with and without phonon coupling, TALYS code. Comparison with (Q)RPA and Kopecky-Uhl.
doi: 10.3938/jkps.59.967
2011IS01 Phys.Rev. C 83, 034304 (2011) J.Isaak, D.Savran, M.Fritzsche, D.Galaviz, T.Hartmann, S.Kamerdzhiev, J.H.Kelley, E.Kwan, N.Pietralla, C.Romig, G.Rusev, K.Sonnabend, A.P.Tonchev, W.Tornow, A.Zilges Investigation of low-lying electric dipole strength in the semimagic nucleus 44Ca NUCLEAR REACTIONS 44Ca(polarized γ, γ'), E = 6-10, 9.9 MeV; measured Eγ, Iγ, γ(θ), integrated cross sections, and polarization asymmetry at DHIPS facility using S-DALINAC accelerator, and at HIγS facility. 44Ca; deduced levels, J, π, photon branching ratios, widths, B(E1) and B(M1) transition strengths. Comparisons with dipole strengths in 40,48Ca and with microscopic calculations within the extended theory of finite Fermi systems. Dependence of total E1 strength on neutron number.
doi: 10.1103/PhysRevC.83.034304
2011TO13 Phys.Rev. C 84, 064324 (2011) S.V.Tolokonnikov, S.Kamerdzhiev, D.Voitenkov, S.Krewald, E.E.Saperstein Effects of density dependence of the effective pairing interaction on the first 2+ excitations and quadrupole moments of odd nuclei NUCLEAR STRUCTURE 182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214Pb, 102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134Sn; calculated level energies, B(E2) of first 2+ states, diagonal matrix elements of effective proton quadrupole field. 200Pb, 118Sn; calculated proton and neutron transition densities. 204Pb, 116Sn; calculated static proton and neutron effective fields. 105,107,109,111,113,115,117,119,121,123,125,127In, 109,111,113,115,117,119,121, 123,125Sn, 115,117,119,121,123Sb, 205Tl, 191,193,195,197,199,201,203,205,209Pb, 203,205,209Bi; calculated quadrupole moments. Self-consistent theory of finite Fermi systems based on energy density functionals. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.064324
2010AV04 Phys.Atomic Nuclei 73, 1119 (2010) A.V.Avdeenkov, S.Goriely, S.P.Kamerdzhiev Impact of the phonon coupling on the radiative neutron capture NUCLEAR REACTIONS 123,149Sn(n, γ), E<10 MeV; 124,150Sn(γ, X), E<28 MeV; calculated σ; deduced phonon contribution to pigmy-dipole resonance and radiative neutron capture σ. Extended theory of Finite fermi Systems (ETFFS).
doi: 10.1134/S1063778810070057
2009AV04 Phys.Atomic Nuclei 72, 1332 (2009); Yad.Fiz. 72, 1385 (2009) A.V.Avdeenkov, S.P.Kamerdzhiev Pygmy dipole resonance in nuclei NUCLEAR REACTIONS 124Sn(α, αγ), E = 0-30 MeV; calculated photoabsorption σ, isoscalar and isovector strength functions, energies and B(E1) for pygmy and dipole resonances.
doi: 10.1134/S1063778809080080
2009TS03 Phys.Rev. C 79, 034309 (2009) V.Tselyaev, J.Speth, S.Krewald, E.Litvinova, S.Kamerdzhiev, N.Lyutorovich, A.Avdeenkov, F.Grummer Description of the giant monopole resonance in the even-A 112-124Sn isotopes within a microscopic model including quasiparticle-phonon coupling NUCLEAR STRUCTURE 90Zr, 110,112,114,116,118,120,122,124,132Sn, 144Sm, 208Pb; calculated strength distribution, mean energies and widths of isoscalar giant-monopole resonances (ISGMR) using two microscopic models: quasiparticle random phase approximation (QRPA) and quasiparticle time blocking approximation (QTBA) with self-consistence scheme based on Hartree-Fock+Bardeen-Cooper-Schrieffer (HF+BCS) approximation and Skyrme energy functional. Comparison with experimental data.
doi: 10.1103/PhysRevC.79.034309
2008KA40 Eur.Phys.J. A 37, 333 (2008) Interaction of the single-particle and collective degrees of freedom in non-magic nuclei: The role of phonon tadpole terms
doi: 10.1140/epja/i2008-10628-0
2008LY03 Eur.Phys.J. A 37, 381 (2008) N.Lyutorovich, J.Speth, A.Avdeenkov, F.Grummer, S.Kamerdzhiev, S.Krewald, V.I.Tselyaev Self-consistent calculations within the Green's function method including particle-phonon coupling and the single-particle continuum NUCLEAR STRUCTURE 132Sn, 208Pb; calculated levels, J, π, B(E1), GDR, photoabsorption σ, isoscalar/isovector quadrupole strength distributions using a quasiparticle time blocking approximation. Comparison with RPA and data.
doi: 10.1140/epja/i2008-10638-x
2007TE05 Phys.Lett. B 647, 104 (2007) G.Tertychny, V.Tselyaev, S.Kamerdzhiev, F.Grummer, S.Krewald, J.Speth, A.Avdeenkov, E.Litvinova Microscopic description of the low lying and high lying electric dipole strength in stable Ca isotopes NUCLEAR STRUCTURE 40,44,48Ca; calculated B(E1), electric dipole strength distribution, GDR. Extended theory of finite Fermi systems.
doi: 10.1016/j.physletb.2007.01.069
2007TE08 Nucl.Phys. A788, 159c (2007) G.Tertychny, V.Tselyaev, S.Kamerdzhiev, F.Grummer, S.Krewald, J.Speth, E.Litvinova, A.Avdeenkov Pygmy dipole resonance in stable Ca isotopes NUCLEAR STRUCTURE 40,44,48Ca; calculated B(E1), electric dipole strength distribution, transition densities. Extended theory of finite Fermi systems using RPA. Comparison with data.
doi: 10.1016/j.nuclphysa.2007.01.077
2006KA17 Phys.Atomic Nuclei 69, 418 (2006); Yad.Fiz. 69, 442 (2006) Photonuclear Data and Modern Physics of Giant Resonances NUCLEAR STRUCTURE 40,44,48Ca, 50Ti, 52Cr, 54Fe, 90Zr, 104,120,132Sn, 140Ce, 206,208Pb; calculated resonance properties, strength distributions, photoabsorption σ.
doi: 10.1134/S1063778806030057
2006KA34 Phys.Atomic Nuclei 69, 1110 (2006) Extended Theory of Finite Fermi Systems for Magic and Nonmagic Nuclei NUCLEAR REACTIONS 208Pb(e, e'), E=50 MeV; 208Pb(p, p'), E=200 MeV; analyzed particle spectra, isoscalar E2 strength function. 40Ca(α, α'), E=240 MeV; calculated Eα, σ(θ=1.08°). Extended theory of finite Fermi systems, comparisons with data. NUCLEAR STRUCTURE 40,44,48Ca, 104,120,132Sn; calculated pygmy resonance energies. RPA, extended theory of finite Fermi systems, comparisons with data.
doi: 10.1134/S1063778806070039
2004HA51 Phys.Rev.Lett. 93, 192501 (2004) T.Hartmann, M.Babilon, S.Kamerdzhiev, E.Litvinova, D.Savran, S.Volz, A.Zilges Microscopic Nature of the Pygmy Dipole Resonance: The Stable Ca Isotopes NUCLEAR REACTIONS 44Ca(γ, γ'), E=9.9 MeV bremsstrahlung; measured Eγ, Iγ. 44Ca deduced electric dipole strength distribution, pygmy dipole resonance features. NUCLEAR STRUCTURE 40,44,48Ca; analyzed B(E1), summed strength; deduced quasiparticle-phonon coupling contributions to pygmy dipole resonance. Microscopic model.
doi: 10.1103/PhysRevLett.93.192501
2004KA06 Yad.Fiz. 67, 180 (2004); Phys.Atomic Nuclei 67, 183 (2004); Erratum Yad.Fiz. 67, 1632 (2004); Phys.Atomic Nuclei 67, 1610 (2004) S.P.Kamerdzhiev, E.V.Litvinova Green's Function Method in the Problem of Complex Configurations in Fermi Systems with pairing NUCLEAR STRUCTURE 104,120,132Sn; calculated dipole photoabsorption σ, isovector dipole resonance energies, widths; deduced pairing contributions. Green's function method.
doi: 10.1134/1.1644022
2004KA11 Phys.Rep. 393, 1 (2004) S.Kamerdzhiev, J.Speth, G.Tertychny Extended theory of finite Fermi systems: collective vibrations in closed shell nuclei
doi: 10.1016/j.physrep.2003.11.001
2003LI11 Yad.Fiz. 66, 584 (2003); Phys.Atomic Nuclei 66, 558 (2003) E.V.Litvinova, S.P.Kamerdzhiev, V.I.Tselyaev Temperature Generalization of the Quasiparticle Random-Phase Approximation with Allowance for a Continuum NUCLEAR STRUCTURE 104,120Sn; calculated dipole photoabsorption σ vs excitation energy, resonance features. Continuum quasiparticle RPA.
doi: 10.1134/1.1563722
2002KA57 Phys.Rev. C66, 044304 (2002) Excitations of the unstable nuclei 48Ni and 49Ni NUCLEAR STRUCTURE 48,49Ni, 48Ca, 49Sc; calculated strength functions, resonance features. Continuum RPA and odd RPA.
doi: 10.1103/PhysRevC.66.044304
2001KA06 Phys.Rev. C63, 034304 (2001) S.P.Kamerdzhiev, R.J.Liotta, V.I.Tselyaev Random Phase Approximation for Odd Nuclei and Its Application to the Description of the Electric Dipole Modes in 17O NUCLEAR STRUCTURE 16,17O; calculated E1 resonance photoabsorption σ. Generalization of RPA for odd nuclei.
doi: 10.1103/PhysRevC.63.034304
2001KA33 Yad.Fiz. 64, No 4, 686 (2001); Phys.Atomic Nuclei 64, 627 (2001) S.P.Kamerdzhiev, E.V.Litvinova Some Problems in the Generalized Theory of Finite Fermi Systems
doi: 10.1134/1.1368221
2001KA62 Eur.Phys.J. A 12, 285 (2001) S.Kamerdzhiev, E.Litvinova, D.Zawischa Quasiparticle-Phonon Interaction in Non-Magic Nuclei
doi: 10.1007/s100500170006
2000KA22 Eur.Phys.J. A 7, 483 (2000) S.Kamerdzhiev, J.Speth, G.Tertychny Microscopic Analysis of the Breathing Mode in 40Ca and 58Ni NUCLEAR REACTIONS 40Ca, 58Ni(α, α'), E=240 MeV; analyzed isoscalar monopole resonance transition densities. Microscopic model.
doi: 10.1007/s100500050421
1999AV02 Yad.Fiz. 62, No 4, 610 (1999); Phys.Atomic Nuclei 62, 563 (1999) A.V.Avdeenkov, S.P.Kamerdzhiev Description of Excitations in Odd Nonmagic Nuclei by Green's Function Method NUCLEAR STRUCTURE 119,121Sn; calculated single-particle strength distributions, neutron states spectrocopic factors. Single-particle Green's function method.
1999AV03 Pisma Zh.Eksp.Teor.Fiz. 69, 669 (1999); JETP Lett. 69, 715 (1999) A.V.Avdeenkov, S.P.Kamerdzhiev On the Mechanisms of Superfluidity in Atomic Nuclei
doi: 10.1134/1.568080
1999AV05 Phys.Lett. 459B, 423 (1999) A.V.Avdeenkov, S.P.Kamerdzhiev The Role of Ground State Correlations in the Single-Particle Strength of Odd Nuclei with Pairing NUCLEAR STRUCTURE 119,121Sn; calculated single-particle levels, spectroscopic factors; deduced role of ground-state correlations, quasiparticle-phonon interactions. Comparisons with data.
doi: 10.1016/S0370-2693(99)00719-4
1998KA29 Phys.Rev. C58, 172 (1998) S.Kamerdzhiev, R.J.Liotta, E.Litvinova, V.Tselyaev Continuum Quasiparticle Random-Phase Approximation Description of Isovector E1 Giant Resonances NUCLEAR STRUCTURE 100,104,120,132Sn; calculated E1 photoabsorption σ; deduced continuum effect on giant resonances. Continuum RPA, forced consistency procedure.
doi: 10.1103/PhysRevC.58.172
1998KA44 Acta Phys.Pol. B29, 2231 (1998) S.Kamerdzhiev, J.Speth, G.Tertychny Effects of the Quasiparticle-Phonon Interaction in Magic and Non-Magic Nuclei NUCLEAR REACTIONS 40Ca, 58Ni(α, α'), E=240 MeV; analyzed E0 resonance strength distributions; deduced quasiparticle-phonon interaction role.
1998TS15 Bull.Rus.Acad.Sci.Phys. 62, 880 (1998) V.I.Tselyaev, S.P.Kamerdzhiev, R.Liotta, E.V.Litvinova Calculation of E1 Resonance by the ' QRPA + Continuum ' Model NUCLEAR STRUCTURE 104,120Sn; calculated isovector E1 resonance strength distribution; deduced role of single-particle continuum. QRPA plus continuum model.
1997AV07 Bull.Rus.Acad.Sci.Phys. 61, 1656 (1997) A.V.Avdeenkov, S.P.Kamerdzhiev Effect of Quasiparticle-Phonon Interaction on Single-Particle Filling Numbers for Nonmagic Nuclei NUCLEAR STRUCTURE 86Kr, 120Sn, 208Pb; calculated single-particle occupancies; deduced quasiparticle-phonon interaction contribution. Green's function method.
1997KA17 Phys.Rev. C55, 2101 (1997) S.Kamerdzhiev, J.Lisantti, P.von Neumann-Cosel, A.Richter, G.Tertychny, J.Wambach Fine Structure of the Giant Isoscalar Quadrupole Resonance in 208Pb Observed in High-Resolution (e, e') and (p, p') Experiments NUCLEAR REACTIONS 208Pb(p, p'), E=200 MeV; measured proton spectra. 208Pb(e, e'), E=50 MeV; analyzed electron spectra. 208Pb deduced giant isoscalar quadrupole resonance fine structure. RPA modes coupled to surface vibration.
doi: 10.1103/PhysRevC.55.2101
1997KA20 Yad.Fiz. 60, No 3, 572 (1997); Phys.Atomic Nuclei 60, 497 (1997) Equations for Single-Particle Green's Functions in Nonmagic Nuclei
1997KA50 Bull.Rus.Acad.Sci.Phys. 61, 122 (1997) Microscopic Theory of Giant Resonances (A Review) NUCLEAR STRUCTURE 40,48Ca, 208Pb, 100,132Sn, 56,78Ni, 16O; compiled, reviewed giant multipole resonance calculations; deduced models improvement related features.
1997KA57 Nucl.Phys. A624, 328 (1997) S.Kamerdzhiev, J.Speth, G.Tertychny Microscopic Description of the E0, E2 and E1 Giant Resonances in 40Ca, 48Ca and 56Ni NUCLEAR STRUCTURE 40,48Ca, 56Ni; calculated E0, E1, E2 giant resonances, strength functions, E1 transition densities; deduced ground-state correlations role. Continuum RPA, particle-hole-phonon coupling.
doi: 10.1016/S0375-9474(97)00315-1
1997KA80 Fiz.Elem.Chastits At.Yadra 28, 333 (1997); Phys.Part.Nucl. 28, 134 (1997) S.P.Kamerdzhiev, G.Ya.Tertychnyi, V.I.Tselyaev The Method of Time-Ordered Graph Decoupling and Its Application to the Description of Giant Resonances in Magic Nuclei NUCLEAR STRUCTURE 40,48Ca, 56Ni, 208Pb; calculated giant resonance E, Γ, photoabsorption σ. Time-ordered graph decoupling method.
1996AV07 Bull.Rus.Acad.Sci.Phys. 60, 1716 (1996) A.V.Avdeenkov, S.P.Kamerdzhiev On Application of the Optical Potential Theory to Calculation of Nucleon-Nucleus Cross Sections NUCLEAR REACTIONS 120Sn, 208Pb(n, γ)E=0-4 MeV; calculated optical potentials, s-wave absorption σ. Green function potential, particle+phonon states.
1996KA09 Nucl.Phys. A599, 373c (1996) Distribution of Giant Resonance Strength in Stable and Unstable Nuclei NUCLEAR REACTIONS 208Pb(γ, X), E ≤ 40 MeV; compiled, reviewed calculations of giant resonance photoabsorption σ(E). 208Pb(γ, n), E ≤ 22 MeV; calculated σ(E). Microscopic theory. NUCLEAR STRUCTURE 48,40Ca, 56,78Ni, 100,132Sn, 208Pb; compiled, reviewed calculations of B(M1).
doi: 10.1016/0375-9474(96)00080-2
1996KA53 Bull.Rus.Acad.Sci.Phys. 60, 702 (1996) S.P.Kamerdzhiev, E.V.Litvinova Simple Model of Dynamic Correlation Effects in a Nuclear Ground State NUCLEAR STRUCTURE 40Ca, 16O; calculated levels, B(λ). Microscopic two-level model, ground state correlation effects.
1995KA35 Phys.Rev.Lett. 74, 3943 (1995) S.Kamerdzhiev, J.Speth, G.Tertychny Splitting of the Isoscalar E2 Giant Resonance and Evidence of Low-Lying E0 Strength in 40Ca NUCLEAR STRUCTURE 40Ca; calculated E2, E0 giant resonances EWSR depletion, E2 transition strength function.
doi: 10.1103/PhysRevLett.74.3943
1994KA04 Phys.Lett. 321B, 6 (1994) S.Kamerdzhiev, O.Rosso, G.Tertychnyi, W.Unkelbach On the Nature of Low-Lying 1+ Levels in Spherical Open-Shell Nuclei NUCLEAR STRUCTURE 96Zr; calculated levels, B(λ); deduced ground state correlations role. RPA, quasipaticle RPA, 1p1h coupling to phonon ground state correlations.
doi: 10.1016/0370-2693(94)90319-0
1994KA10 Nucl.Phys. A569, 313c (1994) S.Kamerdzhiev, G.Tertychnyi, J.Speth Theoretical Description of Giant Resonances in Stable and Unstable Magic Nuclei NUCLEAR REACTIONS 208Pb(γ, X), E ≤ 35 MeV; calculated photoabsorption σ(E). Microscopic approach, Green function method, RPA with complex configuration. NUCLEAR STRUCTURE 40Ca, 56,78Ni, 100,132Sn, 208Pb; calculated diverse giant resonance excitation functions, B(λ). Microscopic approach, Green function method, RPA with complex configuration.
doi: 10.1016/0375-9474(94)90122-8
1994KA28 Nucl.Phys. A577, 641 (1994) S.Kamerdzhiev, G.Tertychny, J.Speth, J.Wambach The Role of 1p1h (x) Phonon Ground-State Correlations in the Isoscalar E0 Excitations of Magic Nuclei NUCLEAR STRUCTURE 40,48Ca, 208Pb, 56Ni; calculated isoscalar E0 transition strength functions. Extended RPA, continuum effects.
doi: 10.1016/0375-9474(94)90937-7
1993KA11 Nucl.Phys. A555, 90 (1993) S.Kamerdzhiev, J.Speth, G.Tertychnyi, V.Tselyaev Microscopic Description of the Giant Electric-Dipole Resonance in Magic Nuclei NUCLEAR REACTIONS 40,48Ca(γ, X), E=10-32 MeV; 208Pb(γ, X), E ≈ 6-20 MeV; calculated photoabsorption σ(E). 40,48Ca, 208Pb deduced E1 resonances integral characteristics, giant resonances. Extended RPA approach.
doi: 10.1016/0375-9474(93)90315-O
1993KA25 Z.Phys. A346, 253 (1993) S.Kamerdzhiev, J.Speth, G.Tertychnyi, J.Wambach M1 Resonances in Unstable Magic Nuclei NUCLEAR STRUCTURE 48Ca, 208Pb, 56,78Ni, 100,132Sn; calculated M1 transition strength distributions, B(M1). Microscopic approach, RPA configurations, single particle continuum.
doi: 10.1007/BF01292513
1992KA04 Phys.Lett. 275B, 1 (1992) Calculation of the Giant Dipole Resonance in Hot Nonspherical Heavy Nuclei with Realistic Forces NUCLEAR STRUCTURE 160Er; calculated B(E1) strength spectral distribution at different temperatures. Hot nuclei, quasiparticle RPA.
doi: 10.1016/0370-2693(92)90841-Q
1992KA30 Phys.Lett. 287B, 293 (1992) S.Kamerdzhiev, G.Tertychnyi, W.Unkelbach Giant Dipole Resonance in 208Pb within the Approach Including 1p1h (x) Phonon Configurations and Continuum NUCLEAR STRUCTURE 208Pb; calculated E1 giant resonances, Γ, photoabsorption σ(E). RPA, 1p1h plus phonon configurations, continuum. NUCLEAR REACTIONS 208Pb(γ, X), E=6-20 MeV; calculated giant resonances, E1 photoabsorption σ(E). RPA, 1p1h plus phonon configurations, continuum.
doi: 10.1016/0370-2693(92)90985-D
1991KA26 Phys.Lett. 267B, 12 (1991) S.P.Kamerdzhiev, G.Ya.Tertychnyi, V.I.Tselyaev Calculations of E1 Resonances in 40Ca, 48Ca and 208Pb Including 1p1h(x) Phonon Configurations NUCLEAR STRUCTURE 40,48Ca, 208Pb; calculated E1 resonances, Γ, sum rule strength. Microscopic model, (1px1h)+phonon configuration. NUCLEAR REACTIONS 40,48Ca(γ, X), E=8-32 MeV; 208Pb(γ, X), E ≈ 6-20 MeV; calculated absorption σ(E). Microscopic model, (1px1h)+phonon configuration.
doi: 10.1016/0370-2693(91)90515-R
1991KA30 Pisma Zh.Eksp.Teor.Fiz. 53, 393 (1991); JETP Lett.(USSR) 53, 412 (1991) S.P.Kamerdzhiev, G.Ya.Tertychnyi Calculations of the E1 Resonance in 48Ca in the 1P1H + 2P2H + Continuum Approximation NUCLEAR REACTIONS 48Ca(γ, X), E ≈ 12-26 MeV; calculated double photoabsorption σ(E). 48Ca deduced E1 resonance, Γ. Finite Fermi system theory, RPA.
1991KA42 Izv.Akad.Nauk SSSR, Ser.Fiz. 55, 49 (1991); Bull.Acad.Sci.USSR, Phys.Ser. 55, No.1, 45 (1991) Effects from Ground-State 2p2h Correlation on the M1 Resonance in 208Pb NUCLEAR STRUCTURE 208Pb; calculated B(λ), isovector M1 resonance spreading width; deduced 2p-2h ground state correlation role. Microscopic model, 1p-1h coupling to phonon included.
1989KA28 Z.Phys. A334, 19 (1989) A Microscopic Model Taking into Account 2p2h Configurations in Magic Nuclei. Calculations of M1 Excitations NUCLEAR STRUCTURE 16O, 40,42,44,48Ca, 54Fe, 90Zr, 208Pb; calculated B(λ). Green's function formalism, 2p-2h configurations, microscopic model.
1988KA36 Izv.Akad.Nauk SSSR, Ser.Fiz. 52, 874 (1988); Bull.Acad.Sci.USSR, Phys.Ser. 52, No.5, 38 (1988) Calculating M1 Excitations in 42Ca, 44Ca, and 54Fe Incorporating 1p1h (x) Phonon Configurations NUCLEAR STRUCTURE 42,44Ca, 54Fe; calculated levels, B(λ). Phonon coupled to 1p-1h.
1986KA29 Yad.Fiz. 43, 1426 (1986) Analysis of the Microscopic Model of taking 2p2h Configurations into Account NUCLEAR STRUCTURE 48Ca, 90Zr, 208Pb; calculated levels, B(M1). Microscopic model.
1986KA48 Yad.Fiz. 44, 606 (1986) Single-Particle Characteristics in Problem taking Account of Complex Configurations NUCLEAR STRUCTURE 208Pb; calculated neutron energy levels. Single particle motion, quasiparticle-phonon interaction.
1985TK01 Yad.Fiz. 42, 832 (1985) The ' 1p1h + Phonon ' Configuration Effect on M1 Excitations in Magic Nuclei NUCLEAR STRUCTURE 40,48Ca, 208Pb, 90Zr; calculated levels, B(λ). Microscopic model.
1984KA08 Izv.Akad.Nauk SSSR, Ser.Fiz. 48, 97 (1984); Bull.Acad.Sci.USSR, Phys.Ser. 48, No.1, 95 (1984) Calculation of M1-Resonance Characteristics in 208Pb and Estimate of 1p1h + 31--Phonon Configurations NUCLEAR STRUCTURE 208Pb; calculated B(M1) distribution. Finite Fermi system, diagrammatic approach.
1984KA18 Phys.Lett. 142B, 225 (1984) M1 Resonance Calculations in Magic Nuclei taking into Account 1p1h + Phonon Configurations NUCLEAR STRUCTURE 40,48Ca, 208Pb, 90Zr; calculated M1 resonance characteristics, strength distribution, B(M1). Microscopic model, Green's function technique.
doi: 10.1016/0370-2693(84)91186-9
1984KA39 Pisma Zh.Eksp.Teor.Fiz. 40, 31 (1984); JETP Lett.(USSR) 40, 756 (1984) Calculated Properties of M1 Excitations in 40Ca and 48Ca NUCLEAR STRUCTURE 40,48Ca; calculated levels, B(M1) strength distribution. Microscopic model.
1977KA20 Acta Phys.Pol. B8, 415 (1977) S.P.Kamerdzhiev, I.N.Borzov, V.N.Tkachev M1 Resonance and Comparative Study of E1, E2 and M1 Resonances in Near-Threshold Region NUCLEAR STRUCTURE 88Sr, 90Zr, 114,116,120,124,126Sn, 140Ce, 202,204,208Pb; calculated M1 resonance characteristics. NUCLEAR REACTIONS 90Zr, 208Pb, 120Sn(γ, γ); calculated E1, E2, M1 resonance contributions to absorption σ.
1976TK01 Yad.Fiz. 24, 715 (1976); Sov.J.Nucl.Phys. 24, 373 (1976) V.N.Tkachev, I.N.Borzov, S.P.Kamerdzhiev M1 Transitions in Spherical Nuclei NUCLEAR STRUCTURE 88Sr, 90Zr, 140Ce, 114,116,120,124,126Sn, 140Ce, 202,204,208Pb; calculated M1 resonances, γ absorption σ, B(λ). 207,209Pb, 209Bi, 207Tl; calculated μ, B(M1).
1975BO10 Yad.Fiz. 21, 31 (1975); Sov.J.Nucl.Phys. 21, 15 (1975) Electric Quadrupole Transitions in 88Sr and 90Zr NUCLEAR STRUCTURE 88Sr, 90Zr; calculated levels, B(E2).
1973KA36 Phys.Lett. 47B, 147 (1973) Electric Quadrupole Transitions in 120Sn and 208Pb NUCLEAR STRUCTURE 120Sn, 208Pb; calculated levels, B(E2).
doi: 10.1016/0370-2693(73)90592-3
1972KA32 Yad.Fiz. 15, 676 (1972); Sov.J.Nucl.Phys. 15, 379 (1972) E1 and E2 Transitions in Medium and Heavy Spherical Nuclei NUCLEAR STRUCTURE 112,120,124Sn, 208Pb; calculated levels, B(E2); analyzed giant resonance structure.
1971KA37 Yad.Fiz. 13, 1335 (1971); Sov.J.Nucl.Phys. 13, 767 (1971) Low-Lying 2+ Levels of Pb208 NUCLEAR STRUCTURE 208Pb; calculated low-lying levels, B(E2).
1970KA24 Yad.Fiz. 11, 537 (1970); Sov.J.Nucl.Phys. 301 (1970) Low-Lying 'Single-Phonon' 0+ Levels in Spherical Nuclei NUCLEAR STRUCTURE 118,120Sn, 140Ce, 142Nd, 202,204Pb; calculated single-phonon o+ levels, B(E0).
1969KA30 Yadern.Fiz. 9, 324 (1969); Soviet J.Nucl.Phys. 9, 190 (1969) Collective Oscillations of Nuclei in the Theory of Finite Fermi Systems NUCLEAR STRUCTURE 124Sn, 204Pb; calculated effective monopole, quadrupole charges.
1967KA21 Yadern.Fiz. 5, 971 (1967); Soviet J.Nucl.Phys. 5, 693 (1967) E2 transition and Effective Quadrupole Charge in Odd Near-Magic Nuclei
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