NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = M.G.Kozlov Found 13 matches. 2023BL03 Phys. Rev. Res. 5, 013191 (2023) J.W.Blanchard, D.Budker, D.DeMille, M.G.Kozlov, L.V.Skripnikov Using parity-nonconserving spin-spin coupling to measure the Tl nuclear anapole moment in a TlF molecular beam NUCLEAR MOMENTS Tl; analyzed available data; deduced new experiment in search of for a Time Reversal-invariance conserving but Parity-nonconserving (PNC) effect induced by the anapole moment of the Tl nucleus, via a vector coupling of the two nuclear spins in TlF.
doi: 10.1103/PhysRevResearch.5.013191
2023DE06 Phys.Rev. C 107, 024307 (2023) Yu.A.Demidov, M.G.Kozlov, A.E.Barzakh, V.A.Yerokhin Bohr-Weisskopf effect in the potassium isotopes ATOMIC PHYSICS K; calculated hyperfine structure constants taking into account the Bohr-Weisskopf and Breit-Rosenthal effects. Dirac-Hartree-Fock, Dirac-Hartree-Fock plus second order many-body perturbation theory (MBPT), and Dirac-Hartree-Fock plus linearized single double coupled-clusters methods. Comparison to experimental results obtained for 39K. NUCLEAR MOMENTS 38,44,46,47,48,49,51K; analyzed experimental data on hyperfine structure constants; deduced nuclear magnetic moments with taking into account corrections caused by relative hyperfine anomaly.
doi: 10.1103/PhysRevC.107.024307
2021PO12 Phys.Rev.Lett. 127, 253001 (2021) S.G.Porsev, M.S.Safronova, M.G.Kozlov Precision Calculation of Hyperfine Constants for Extracting Nuclear Moments of 229Th NUCLEAR MOMENTS 229Th; calculated the energies and magnetic dipole and electric quadrupole hyperfine structure constants for the low-lying states; deduced the nuclear magnetic dipole and electric quadrupole moments, impact of Bohr-Weisskopf effect on the finite nuclear magnetization. Framework of such a relativistic coupled-cluster single double triple method.
doi: 10.1103/PhysRevLett.127.253001
2020BA17 Phys.Rev. C 101, 034308 (2020) A.E.Barzakh, D.Atanasov, A.N.Andreyev, M.Al Monthery, N.A.Althubiti, B.Andel, S.Antalic, K.Blaum, T.E.Cocolios, J.G.Cubiss, P.Van Duppen, T.Day Goodacre, A.de Roubin, Yu.A.Demidov, G.J.Farooq-Smith, D.V.Fedorov, V.N.Fedosseev, D.A.Fink, L.P.Gaffney, L.Ghys, R.D.Harding, D.T.Joss, F.Herfurth, M.Huyse, N.Imai, M.G.Kozlov, S.Kreim, D.Lunney, K.M.Lynch, V.Manea, B.A.Marsh, Y.Martinez Palenzuela, P.L.Molkanov, D.Neidherr, R.D.Page, M.Rosenbusch, R.E.Rossel, S.Rothe, L.Schweikhard, M.D.Seliverstov, S.Sels, C.Van Beveren, E.Verstraelen, A.Welker, F.Wienholtz, R.N.Wolf, K.Zuber Hyperfine anomaly in gold and magnetic moments of Iπ = 11/2- gold isomers NUCLEAR MOMENTS 177m,191m,193m,195mAu; measured hyperfine structure spectra (hfs), hyperfine splitting, differential hyperfine anomaly, magnetic dipole moments using in-source laser resonance-ionization spectroscopy (RILIS) at CERN-ISOLDE. Mass separated Au beams were produced in U(p, X), E=1.4 GeV reaction, and delivered to either the ISOLTRAP Multi-Reflection Time-of-Flight Mass Spectrometer (MR-ToF MS) or the Windmill (WM) decay station. Comparison to the previously measured magnetic moments. 185,186,187,189,189m,191,193,194Au; re-evaluated previously measured magnetic dipole moments by properly accounting for the hyperfine anomaly.
doi: 10.1103/PhysRevC.101.034308
2019VI04 Phys.Rev. C 100, 034318 (2019) A.V.Viatkina, D.Antypas, M.G.Kozlov, D.Budker, V.V.Flambaum Dependence of atomic parity-violation effects on neutron skins and new physics ATOMIC PHYSICS 85,87Rb, 131,134,135,136,137Cs, 130,132,133,134,135,136,137,138Ba, 144,145,146,147,148,149,150,151,152,153,154Sm, 156,158,161,162,163,164Dy, 168,170,171,172,173,174,176Yb, 203,204,205Tl, 202,204,205,206,207,208Pb, 207,208,209,210,211,212,213,220,221,222,223,224,225,226,227,228Fr, 208,209,210,211,212,213,214,220,221,222,223,224,225,226,227,228,229,230,232Ra; calculated mean values of the coefficients as functions of the radius parameter for different elements, assuming Fermi distribution of nuclear density; evaluated relevant coefficients from for the nuclear factor of the Parity-nonconserving (PNC) amplitude in low energy atomic experiments. Relevance to Yb experiment in Mainz and the Fr experiment at TRIUMF.
doi: 10.1103/PhysRevC.100.034318
2018SA48 Phys.Rev.Lett. 121, 213001 (2018) M.S.Safronova, S.G.Porsev, M.G.Kozlov, J.Thielking, M.V.Okhapkin, P.Glowacki, D.M.Meier, E.Peik Nuclear Charge Radii of 229Th from Isotope and Isomer Shifts NUCLEAR MOMENTS 229Th, 232Th; measured frequencies; deduced hyperfine structure, isotopic shift, r.m.s. radii, mean-square radius change between 229Th and its low-lying isomer 229mTh. Comparison with theoretical calculations.
doi: 10.1103/PhysRevLett.121.213001
2009SA52 Nucl.Phys. A827, 411c (2009) M.S.Safronova, R.Pal, D.Jiang, M.G.Kozlov, W.R.Johnson, U.I.Safronova New directions in atomic PNC
doi: 10.1016/j.nuclphysa.2009.05.088
2002DZ01 Phys.Rev. A66, 012111 (2002) V.A.Dzuba, V.V.Flambaum, J.S.M.Ginges, M.G.Kozlov Electric Dipole Moments of Hg, Xe, Rn, Ra, Pu, and TIF Induced by the Nuclear Schiff Moment and Limits on Time-Reversal Violating Interactions ATOMIC PHYSICS 199Hg, 129Xe, 223Rn, 225Ra, 239Pu; calculated atomic electric dipole moments induced by nuclear Schiff moments. Role of parity and time-reversal violating interactions discussed. NUCLEAR MOMENTS 199Hg, 129Xe, 223Rn, 225Ra, 239Pu; calculated atomic electric dipole moments induced by nuclear Schiff moments. Role of parity and time-reversal violating interactions discussed.
doi: 10.1103/PhysRevA.66.012111
2002KO42 Pisma Zh.Eksp.Teor.Fiz. 75, 651 (2002); JETP Lett. 75, 534 (2002) Manifestation of the Nuclear Anapole Moment in the Thallium M1 Transitions ATOMIC PHYSICS 205Tl; analyzed transition amplitudes, hfs; deduced nuclear anapole moment. NUCLEAR MOMENTS 205Tl; analyzed transition amplitudes, hfs; deduced nuclear anapole moment.
doi: 10.1134/1.1500715
2001PO28 Phys.Rev. A64, 064101 (2001) Calculation of the Nuclear Spin-Dependent Parity-Nonconserving Amplitude for the (7s, F = 4) → (7s, F = 5) Transition in Fr ATOMIC PHYSICS 211Fr; calculated nuclear spin-dependent transition amplitude.
doi: 10.1103/PhysRevA.64.064101
1999KO08 Eur.Phys.J. D 5, 59 (1999) Polarizabilities and Hyperfine Structure Constants of the Low-Lying Levels of Barium NUCLEAR MOMENTS Ba; calculated hfs, polarizabilities. Configuration interaction method.
doi: 10.1007/s100530050229
1998DZ02 Zh.Eksp.Teor.Fiz. 114, 1636 (1998); J.Exper.Theo.Phys. 87, 885 (1998) V.A.Dzuba, V.V.Flambaum, M.G.Kozlov, S.G.Porsev Using Effective Operators in Calculating the Hyperfine Structure of Atoms NUCLEAR MOMENTS 205Tl; calculated hfs. Multielectron atoms, effective Hamiltonian for valence electrons.
doi: 10.1134/1.558736
1995PO21 Pisma Zh.Eksp.Teor.Fiz. 61, 449 (1995); JETP Lett. 61, 459 (1995) S.G.Porsev, Yu.G.Rakhlina, M.G.Kozlov Parity Violation in Atomic Ytterbium NUCLEAR STRUCTURE 168,170,171,172,173,174,176Yb; calculated weak nuclear charge. ATOMIC PHYSICS Yb; calculated P-odd impurity amplitude; deduced stronger parity-nonconservation effects than in Cs, Tl.
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