NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = V.V.Flambaum Found 78 matches. 2023AL03 Phys.Rev. A 107, 032805 (2023) S.O.Allehabi, V.A.Dzuba, V.V.Flambaum Calculation of the hyperfine structure of Dy, Ho, Cf, and Es ATOMIC PHYSICS Dy, Ho, Cf, Es; calculated the magnetic dipole HFS constants A and electric quadrupole HFS constant B for the sake of interpretation of the measurements in terms of nuclear magnetic moment μ and electric quadrupole moment Q using the configuration interaction (CI) method for open shells with a large number of valence electrons.
doi: 10.1103/PhysRevA.107.032805
2023DA04 Phys.Rev. C 107, 035502 (2023) F.Dalton, V.V.Flambaum, A.J.Mansour Enhanced Schiff and magnetic quadrupole moments in deformed nuclei and their connection to the search for axion dark matter NUCLEAR STRUCTURE 153Eu, 153Sm, 155Gd, 161,163Dy, 165Er, 221,223Fr, 223Rn, 225,227Ac, 225Ra, 229Th, 229Pa, 233,235U, 237Np, 239Pu; calculated collective Schiff moments for octupole deformed nuclei which contain a low lying energy doublet to the ground state with identical spin and opposing parity, energy shift in solids induced by nuclear Schiff moment and magnetic quadrupole moment. Discussed candidate crystals, which could be used for axion dark matter search, which may exhibit an enhanced energy shift due to the nuclear Schiff moment octupole mechanism.
doi: 10.1103/PhysRevC.107.035502
2023WE04 Phys.Rev. C 107, 034313 (2023) F.Weber, T.E.Albrecht-Schonzart, S.O.Allehabi, S.Berndt, M.Block, H.Dorrer, C.E.Dullmann, V.A.Dzuba, J.G.Ezold, V.V.Flambaum, V.Gadelshin, S.Goriely, A.Harvey, R.Heinke, S.Hilaire, M.Kaja, T.Kieck, N.Kneip, U.Koster, J.Lantis, C.Mokry, D.Munzberg, S.Nothhelfer, S.Oberstedt, S.Peru, S.Raeder, J.Runke, V.Sonnenschein, M.Stemmler, D.Studer, P.Thorle-Pospiech, H.Tomita, N.Trautmann, S.Van Cleve, J.Warbinek, K.Wendt Nuclear moments and isotope shifts of the actinide isotopes 249-253Cf probed by laser spectroscopy NUCLEAR MOMENTS 249,250,251,252,253Cf; measured hyperfine spectra; deduced energy positions of three atomic ground-state transitions, isotope shifts. 249,251,253Cf; deduced nuclear magnetic dipole moments, hyperfine parameters. 249,253Cf; deduced spectroscopic quadrupole moments. Comparison with previous experimental data. Laser resonance ionisation high-resolution spectroscopy. Comparison to theoretical estimations. RISIKO mass separator at Johannes Gutenberg University Mainz.
doi: 10.1103/PhysRevC.107.034313
2022FA04 Phys.Rev. C 105, L051303 (2022) P.Fadeev, J.C.Berengut, V.V.Flambaum Effects of variation of the fine structure constant α and quark mass mq in Mossbauer nuclear transitions NUCLEAR STRUCTURE 57Fe, 67Zn, 83Kr, 99Ru, 119Sn, 121Sb, 125Te, 127,129I, 149Sm, 151,153Eu, 155,157Gd, 161Dy, 181Ta, 197Au, 229Th, 235U, 243Am; analyzed nuclear structure data, information on change of rms charge radius and intrinsic quadrupole moment between ground and excited states; deduced sensitivity of nuclear (Mossbauer) transitions to variation of fine structure constant and quark mass. Discussed the possibility of studies 8-eV in 229Th and 76-eV in 235U transition by means of laser spectroscopy.
doi: 10.1103/PhysRevC.105.L051303
2022FI01 Phys.Rev.Lett. 128, 073001 (2022) N.L.Figueroa, J.C.Berengut, V.A.Dzuba, V.V.Flambaum, D.Budker, D.Antypas Precision Determination of Isotope Shifts in Ytterbium and Implications for New Physics ATOMIC PHYSICS 168,170,172,174,176Yb; measured frequencies; deduced isotope shifts for the five spinless Yb isotopes, nonlinearity in the joint King-plot analysis due to the deformation of the Yb nuclei. Doppler-free two-photon spectroscopy.
doi: 10.1103/PhysRevLett.128.073001
2022FL01 Phys.Rev. C 105, 015501 (2022) Parity and time-reversal invariance violation in neutron-nucleus scattering NUCLEAR REACTIONS 232Th(n, n), E=8-392 eV; analyzed neutron resonances for parity violating (PV) effect and the parity and time reversal invariance violating (PTRIV) effects using statistical theory based on the properties of chaotic eigenstates; deduced P-odd asymmetries. 153Eu, 155,157Gd, 159Tb, 161,163Dy, 233U, 237Np; discussed static or dynamical octupole ground state deformations from observed rotational spectra for target nuclei suitable for neutron scattering experiments.
doi: 10.1103/PhysRevC.105.015501
2022FL05 Phys.Rev. C 105, 065503 (2022) Enhanced magnetic quadrupole moments in nuclei with octupole deformation and their CP-violating effects in molecules NUCLEAR MOMENTS 153Eu, 161Dy, 221,223Fr, 223Ra, 223Rn, 225,227Ac, 229Th, 229Pa, 233,235U, 237Np; calculated CP violating magnetic quadrupole moments (MQM) in octupole-deformed nuclei, and energy shifts produced due to MQM interaction with the electron magnetic field of the molecules: EuO, EuN+, RaF, AcO, AcN+, AcF+, ThO, and ThF+ using relativistic many-body methods.
doi: 10.1103/PhysRevC.105.065503
2021FL03 Phys.Rev. C 103, 054603 (2021) Resonance photoproduction of pionic atoms at the proposed Gamma Factory NUCLEAR REACTIONS 7Li, 11B, 12C, 14N(γ, π-), E AP 140 MeV; calculated resonant cross-section for bound π- production in 1s state at the Gamma Factory. 40Ca, 90Zr(γ, π-), E=high; analyzed and fitted experimental data for total widths. Z=9-92; calculated resonant cross sections for producing ns pionic states, partial Γγ for 1s pionic states, Γγ/Γ(total) of ns pionic states for final nuclei of Z=9-92.
doi: 10.1103/PhysRevC.103.054603
2020AL10 Phys.Rev. C 102, 024326 (2020) S.O.Allehabi, V.A.Dzuba, V.V.Flambaum, A.V.Afanasjev, S.E.Agbemava Using isotope shift for testing nuclear theory: The case of nobelium isotopes NUCLEAR STRUCTURE 252,254No; calculated nuclear charge distributions, rms charge radii for five nuclear models using covariant density functional theory (CDFT) with state-of-the-art covariant energy density functionals, isotope shifts and field isotope shifts for four electric dipole atomic transitions using CI+MBPT method. Comparison with experimental data. 254No, 286No; calculated difference in charge radii, isotope shifts between 254No and hypothetical 286No in different nuclear models for four electric dipole transitions from the ground state.
doi: 10.1103/PhysRevC.102.024326
2020FA08 Phys.Rev. A 102, 052833 (2020) P.Fadeev, J.C.Berengut, V.V.Flambaum Sensitivity of 229Th nuclear clock transition to variation of the fine-structure constant RADIOACTIVITY 229Th(IT); analyzed available data; deduced the quadrupole moment sensitivity, frequency shift, fine-structure constant impact, possible effect of the octupole deformation.
doi: 10.1103/PhysRevA.102.052833
2020FL01 Phys.Rev. C 101, 015502 (2020) Enhanced nuclear Schiff moment in stable and metastable nuclei NUCLEAR STRUCTURE 153Eu, 227Ac, 235U, 237Np; analyzed octupole deformations in stable and nuclei with long half-lives; deduced estimates of the enhanced Schiff moments, atomic electric dipole moments (EDMs), and T, P-odd interaction constants in molecules containing these nuclei. Discussed possible experiments to test CP-violation theories predicting T, P-violating nuclear forces, and search for axions. 152Sm, 153Eu, 226Ra, 227Ac, 234,235,236U, 237Np; plotted experimental energy levels of positive and negative parities as function of J(J+1) rotational bands.
doi: 10.1103/PhysRevC.101.015502
2020LA03 Phys.Rev. A 101, 012514 (2020) B.G.C.Lackenby, V.A.Dzuba, V.V.Flambaum Calculation of atomic properties of superheavy elements Z = 110-112 and their ions ATOMIC PHYSICS Ds, Rg, Cn; calculated spectra, electric dipole transition rates, and isotope shifts of the superheavy elements and their ions using a recently developed, efficient version of the ab initio configuration-interaction combined with perturbation theory to treat distant effects.
doi: 10.1103/PhysRevA.101.012514
2019AN01 Nat.Phys. 15, 120 (2019) D.Antypas, A.Fabricant, J.E.Stalnaker, K.Tsigutkin, V.V.Flambaum, D.Budker Isotopic variation of parity violation in atomic ytterbium ATOMIC PHYSICS Yb; measured transition frequencies; deduced isotopic variation of parity violation.
doi: 10.1038/s41567-018-0312-8
2019FA07 Phys.Rev. C 100, 015504 (2019) Time-reversal invariance violation in neutron-nucleus scattering
doi: 10.1103/PhysRevC.100.015504
2019FL04 Phys.Rev. C 99, 035501 (2019) Enhanced nuclear Schiff moment and time-reversal violation in 229Th containing molecules NUCLEAR STRUCTURE 229Th; calculated collective Schiff moment in 229ThO molecules; discussed measurements of time-reversal- and parity- and charge conjugation and parity violating electric dipole moments. Comparison with other theoretical predictions.
doi: 10.1103/PhysRevC.99.035501
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
2018GE05 Phys.Rev. A 98, 022508 (2018) A.J.Geddes, L.V.Skripnikov, A.Borschevsky, J.C.Berengut, V.V.Flambaum, T.P.Rakitzis Enhanced nuclear-spin-dependent parity-violation effects using the 199HgH molecule ATOMIC PHYSICS 199Hg; analyzed available data; deduced a proposal for low-energy optical rotation experiment to extract the anapole moment and shed light on the underlying theory of hadronic parity violation.
doi: 10.1103/PhysRevA.98.022508
2018HA34 Phys.Rev. A 98, 032510 (2018) Y.Hao, M.ILias, E.Eliav, P.Schwerdtfeger, V.V.Flambaum, A.Borschevsky Nuclear anapole moment interaction in BaF from relativistic coupled-cluster theory ATOMIC PHYSICS Ba, F; calculated of the P-odd interaction coefficient describing the nuclear anapole moment effect on the molecular electronic structure.
doi: 10.1103/PhysRevA.98.032510
2018LA08 J.Phys.(London) G45, 075105 (2018) Weak quadrupole moments NUCLEAR MOMENTS 9Be, 21Ne, 27Al, 131Xe, 133Cs, 151,153Eu, 163Dy, 167Er, 173Yb, 177,179Hf, 181Ta, 201Hg, 229Th; calculated quadrupole distributions of neutrons, Lorentz invariance violating energy shifts, weak quadrupole moments.
doi: 10.1088/1361-6471/aac65d
2018LA11 Phys.Rev. A 98, 022518 (2018) B.G.C.Lackenby, V.A.Dzuba, V.V.Flambaum Calculation of atomic spectra and transition amplitudes for the superheavy element Db (Z=105) ATOMIC PHYSICS Db, Ta; calculated atomic spectra and other properties of superheavy element dubnium, energy levels for low-lying states of Db and Db II, electric dipole transition amplitudes between the ground state and low-lying states of opposite parity, isotope shift for these transitions, and the ionization potential of Db. Method combining configuration interaction with perturbation theory.
doi: 10.1103/PhysRevA.98.022518
2018LA13 Phys.Rev. A 98, 042512 (2018) B.G.C.Lackenby, V.A.Dzuba, V.V.Flambaum Atomic structure calculations of superheavy noble element oganesson (Z=118) ATOMIC PHYSICS Rn, Og; calculated spectrum of E1 transitions, transition rates, radial electron density. Comparison with available data.
doi: 10.1103/physreva.98.042512
2018RA11 Phys.Rev.Lett. 120, 232503 (2018) S.Raeder, D.Ackermann, H.Backe, R.Beerwerth, J.C.Berengut, M.Block, A.Borschevsky, B.Cheal, P.Chhetri, Ch.E.Dullmann, V.A.Dzuba, E.Eliav, J.Even, R.Ferrer, V.V.Flambaum, S.Fritzsche, F.Giacoppo, S.Gotz, F.P.Hessberger, M.Huyse, U.Kaldor, O.Kaleja, J.Khuyagbaatar, P.Kunz, M.Laatiaoui, F.Lautenschlager, W.Lauth, A.K.Mistry, E.Minaya Ramirez, W.Nazarewicz, S.G.Porsev, M.S.Safronova, U.I.Safronova, B.Schuetrumpf, P.Van Duppen, T.Walther, C.Wraith, A.Yakushev Probing Sizes and Shapes of Nobelium Isotopes by Laser Spectroscopy NUCLEAR MOMENTS 252,253,254No; measured excitation spectra, hyperfine structure components; deduced nuclear magnetic and quadrupole moments, charge radii. Comparison with the state-of-the-art nuclear density functional calculations.
doi: 10.1103/PhysRevLett.120.232503
2017FL01 Phys.Rev.Lett. 118, 142501 (2017) Effects of the Lorentz Invariance Violation on Coulomb Interactions in Nuclei and Atoms
doi: 10.1103/PhysRevLett.118.142501
2017FL04 Phys.Rev. A 96, 012516 (2017) V.V.Flambaum, V.A.Dzuba, C.Harabati Effect of nuclear quadrupole moments on parity nonconservation in atoms ATOMIC PHYSICS Yb, Fr, Ra; calculated quadrupole moment which leads to tensor contribution to the parity nonconserving interaction between nuclei and electrons. Comparison with available data.
doi: 10.1103/PhysRevA.96.012516
2016FL02 Phys.Rev.Lett. 117, 072501 (2016) Enhancing the Effect of Lorentz Invariance and Einstein's Equivalence Principle Violation in Nuclei and Atoms NUCLEAR STRUCTURE 133Cs, 85,87Rb, 131Xe, 201Hg, 21Ne; calculated quadrupole moments, possible Local Lorentz invariance violating (LLIV) and Einstein equivalence principle violating (EEPV) effects.
doi: 10.1103/PhysRevLett.117.072501
2012BE32 J.Phys.:Conf.Ser. 337, 012043 (2012) J.C.Berengut, V.V.Flambaum, V.F.Dmitriev Quark-mass variation effect on big bang nucleosynthesis NUCLEAR REACTIONS 3H(d, n), E not given;3He(d, p), E not given; analyzed resonance influence on σ within big bang nucleosynthesis. 3He(α, γ), E not given; calculated 7Be and via β-capture 7Li abundances vs light quark mass.
doi: 10.1088/1742-6596/337/1/012043
2012FL03 Phys.Rev. C 85, 068502 (2012) Screening and finite-size corrections to the octupole and Schiff moments NUCLEAR STRUCTURE 199Hg, 205Tl; calculated nuclear octupole moment including the electron screening correction, and Z2α2 correction to the Schiff moments due to finite nuclear size. Relevance to test of CP-violation theories.
doi: 10.1103/PhysRevC.85.068502
2011FL04 J.Phys.(London) G38, 055105 (2011) V.V.Flambaum, G.McManus, S.G.Porsev Bound state of a heavy charged massive particle and a nucleus
doi: 10.1088/0954-3899/38/5/055105
2010ON01 Phys.Rev. C 82, 014320 (2010) A.Ong, J.C.Berengut, V.V.Flambaum Effect of spin-orbit nuclear charge density corrections due to the anomalous magnetic moment on halonuclei NUCLEAR STRUCTURE 6,8He, 6,7,8,9,11Li, 7Be; calculated spin-orbit contribution to nucleon charge density of halo nuclei; deduced charge radii. Comparison with experimental data, and with theoretical calculations using no-core shell model (NCSM) and Greens function Monte Carlo (GFMC) method.
doi: 10.1103/PhysRevC.82.014320
2010PO09 Phys.Rev.Lett. 105, 182501 (2010) S.G.Porsev, V.V.Flambaum, E.Peik, Chr.Tamm Excitation of the Isomeric 229mTh Nuclear State via an Electronic Bridge Process in 229Th+ RADIOACTIVITY 229Th(IT); calculated isomeric transition, energy levels, excitation probability; deduced two-photon bridge process.
doi: 10.1103/PhysRevLett.105.182501
2009BE53 Phys.Rev.Lett. 102, 210801 (2009) J.C.Berengut, V.A.Dzuba, V.V.Flambaum, S.G.Porsev Proposed Experimental Method to Determine α Sensitivity of Splitting between Ground and 7.6 eV Isomeric States in 229Th RADIOACTIVITY 229Th(IT); calculated energies, field shift constants, isotope shifts, electric-quadrupole hyperfine-structure parameters.
doi: 10.1103/physrevlett.102.210801
2009BR02 Phys.Rev. C 79, 035501 (2009) B.A.Brown, A.Derevianko, V.V.Flambaum Calculations of the neutron skin and its effect in atomic parity violation NUCLEAR STRUCTURE 129,131,133,135,137Cs, 130,132,134,136,138Ba, 144,146,148,150,152,154Sm, 156,158,160,162,164Dy, 168,170,172,174,176Yb, 203,205Tl, 204,206,208Pb, 209Bi, 209,211,213,215,217,219,221Fr, 210,212,214,216,218,220,222Ra; calculated neutron skins and proton distribution rms radii using Skyrme and relativistic Hartree formulations with Skxs(20) functionals. Atomic parity nonconservation.
doi: 10.1103/PhysRevC.79.035501
2009FL01 Phys.Rev. C 79, 034302 (2009) Enhanced effect of quark mass variation in 229Th and limits from Oklo data NUCLEAR STRUCTURE 229Th, 150Sm; calculated enhancement of effects of variation of quark mass and strong interaction parameter on the 7.6-eV transition from the first excited state in 229Th and on the 0.1 eV resonance in 150Sm from extrapolations of calculations for light nuclei. 2,3H, 3,4,5,6,7He, 6,7Li, 7,8,9Be; calculated variations of nuclear binding energies, spin-orbit intervals, nuclear radius, shifts of nuclear resonances and weakly-bound energy levels. Comparisons with data from Oklo natural reactor and estimates from Walecka model.
doi: 10.1103/PhysRevC.79.034302
2008DZ03 Europhys.Lett. 84, 22001 (2008) The effect of atomic electrons on nuclear fission
doi: 10.1209/0295-5075/84/22001
2007AU07 Phys.Atomic Nuclei 70, 1654 (2007) N.Auerbach, V.F.Dmitriev, V.V.Flambaum, A.Lisetskiy, R.A.Senkov, V.G.Zelevinsky Is it possible to enhance the nuclear Schiff moment by nuclear collective modes? NUCLEAR MOMENTS 217,219,221Ra, 217,219,221Rn; calculated the nuclear Schiff moment using the QRPA formalism.
doi: 10.1134/S106377880709027X
2007FL02 Phys.Rev. C 76, 054002 (2007) Dependence of nuclear binding on hadronic mass variation NUCLEAR STRUCTURE 2,3H, 3,4,5He, 6,7Li, 7,8Be; calculated ground-state energies, multi-nucleon energies using various Hamiltonians.
doi: 10.1103/PhysRevC.76.054002
2007FL03 Phys.Rev. C 76, 065206 (2007) Influence of meson widths on Yukawa-like potentials and lattice correlation functions
doi: 10.1103/PhysRevC.76.065206
2006AU02 Phys.Rev. C 74, 025502 (2006) N.Auerbach, V.F.Dmitriev, V.V.Flambaum, A.Lisetskiy, R.A.Sen'kov, V.G.Zelevinsky Nuclear Schiff moment in nuclei with soft octupole and quadrupole vibrations NUCLEAR STRUCTURE 217,219,221Ra; calculated Schiff moments, role of soft collective quadrupole and octupole vibrations. Quasiparticle RPA. NUCLEAR MOMENTS 217,219,221Ra; calculated Schiff moments, role of soft collective quadrupole and octupole vibrations. Quasiparticle RPA.
doi: 10.1103/PhysRevC.74.025502
2006FL01 Europhys.Lett. 74, 813 (2006) Possible evidence for "dark radiation" from Big Bang Nucleosynthesis data
doi: 10.1209/epl/i2006-10031-y
2006FL02 Phys.Rev. C 73, 055501 (2006) Dependence of nuclear magnetic moments on quark masses and limits on temporal variation of fundamental constants from atomic clock experiments NUCLEAR MOMENTS 1,2H, 3He, 87Rb, 111Cd, 129Xe, 133Cs, 171Yb, 199Hg; calculated μ, sensitivity to variation in quark masses and fine structure constant.
doi: 10.1103/PhysRevC.73.055501
2006FL03 Phys.Rev.Lett. 97, 092502 (2006) Enhanced Effect of Temporal Variation of the Fine Structure Constant and the Strong Interaction in 229Th NUCLEAR STRUCTURE 229Th; calculated transition frequency, sensitivity to temporal variation of fundamental constants.
doi: 10.1103/PhysRevLett.97.092502
2005DM02 Phys.Rev. C 71, 068501 (2005) Relativistic corrections to the nuclear Schiff moment NUCLEAR MOMENTS 199Hg, 205Tl; calculated Schiff moments, relativistic corrections.
doi: 10.1103/PhysRevC.71.068501
2005FL01 J.Phys.(London) G31, 355 (2005) Quantum tunnelling of a complex system: effects of a finite size and intrinsic structure
doi: 10.1088/0954-3899/31/5/006
2004KU21 Phys.Rev. C 70, 047601 (2004); Erratum Phys.Rev. C 71, 029901 (2005) M.Yu.Kuchiev, B.L.Altshuler, V.V.Flambaum Exponential enhancement of nuclear reactions in a condensed matter environment NUCLEAR REACTIONS 1H(t, X), (7Li, X), E=low; calculated enhancement of σ in condensed matter environment.
doi: 10.1103/PhysRevC.70.047601
2003FL03 Phys.Rev. C 68, 035502 (2003) Enhancement of nuclear Schiff moments and time-reversal violation in atoms due to soft nuclear octupole vibrations NUCLEAR MOMENTS 223Rn, 223,225Ra; calculated nuclear Schiff moments, atomic electric dipole moments, role of soft octupole vibrations. NUCLEAR STRUCTURE 223Rn, 223,225Ra; calculated nuclear Schiff moments, atomic electric dipole moments, role of soft octupole vibrations.
doi: 10.1103/PhysRevC.68.035502
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
2002KU03 J.Phys.(London) G28, 47 (2002) M.Yu.Kuchiev, B.L.Altshuler, V.V.Flambaum Low-Energy Nuclear Reactions Boosted by Collisions with Environment (Carambole Collisions) NUCLEAR REACTIONS 2H(d, d), E < 800 eV; calculated σ(θ=135°). 2H(d, p), E < 500 eV; calculated relative fusion probability, environmental effects. Three-elastic-collision mechanism.
doi: 10.1088/0954-3899/28/1/304
2001AL37 J.Phys.(London) G27, 2345 (2001) B.L.Altshuler, V.V.Flambaum, M.Yu.Kuchiev, V.G.Zelevinsky ' Colliding Beam ' Enhancement Mechanism of Deuteron-Deuteron Fusion Reactions in Matter NUCLEAR REACTIONS 2H(d, X), E=low; calculated enhancement mechanism for fusion reactions in matter.
doi: 10.1088/0954-3899/27/11/312
2000BE36 Phys.Rev. C62, 024610 (2000) J.C.Berengut, V.V.Flambaum, G.F.Gribakin Unusual Statistics of Interference Effects in Neutron Scattering from Compound Nuclei
doi: 10.1103/PhysRevC.62.024610
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
1997FL01 Phys.Rev. C56, 1641 (1997) Anapole Moment and Nucleon Weak Interactions ATOMIC PHYSICS 133Cs; analyzed parity nonconserving (PNC) interaction related data; deduced anapole moment constant, p-nucleus PNC potential strength, other aspects.
doi: 10.1103/PhysRevC.56.1641
1997FL02 Phys.Rev. C56, 2820 (1997) V.V.Flambaum, D.W.Murray, S.R.Orton Time Invariance Violating Nuclear Electric Octupole Moments NUCLEAR STRUCTURE 127I, 133Cs, 209Bi, 223Ra, 223Rn, 225Ac, 223Fr, 229Pa; calculated nuclear electric octupole moments, contribution to atomic electric dipole moments. ATOMIC PHYSICS 127I, 133Cs, 209Bi, 223Ra, 223Rn, 225Ac, 223Fr, 229Pa; calculated nuclear electric octupole moments, contribution to atomic electric dipole moments.
doi: 10.1103/PhysRevC.56.2820
1997SP03 Phys.Rev. C56, 1357 (1997) V.Spevak, N.Auerbach, V.V.Flambaum Enhanced T-Odd, P-Odd Electromagnetic Moments in Reflection Asymmetric Nuclei NUCLEAR STRUCTURE 223,225Ra, 223Rn, 221,223Fr, 225Ac, 229Pa; calculated T-odd, P-odd collective electric moments; deduced atomic electric dipole moments enhancement. Reflection asymmetry, two-fluid liquid drop model, particle plus core model.
doi: 10.1103/PhysRevC.56.1357
1996AU06 Phys.Rev.Lett. 76, 4316 (1996) N.Auerbach, V.V.Flambaum, V.Spevak Collective T- and P-Odd Electromagnetic Moments in Nuclei with Octupole Deformations NUCLEAR STRUCTURE 223,225Ra, 223Rn, 229Pa, 199Hg, 129Xe; analyzed collective T-odd, P-odd electromagnetic moments, octupole deformation for nuclei.
doi: 10.1103/PhysRevLett.76.4316
1996DM04 Phys.Rev. C54, 3305 (1996) V.F.Dmitriev, V.B.Telitsin, V.V.Flambaum, V.A.Dzuba Core Contribution to the Nuclear Magnetic Quadrupole Moment NUCLEAR STRUCTURE 133Cs, 131Xe; calculated core contribution to magnetic quadrupole moment.
doi: 10.1103/PhysRevC.54.3305
1996VO16 Phys.Lett. 385B, 17 (1996) O.K.Vorov, N.Auerbach, V.V.Flambaum Structure of Low-Energy Collective 0--States in Doubly Magic Nuclei and Matrix Elements of the P-Odd and P- and T-Odd Weak Interaction
doi: 10.1016/0370-2693(96)00861-1
1995FL02 Phys.Rev. C51, 1521 (1995) Induced Parity Nonconserving Interaction and Enhancement of Two-Nucleon Parity Nonconserving Forces NUCLEAR STRUCTURE Th, U; calculated induced parity nonconserving interaction matrix elements in this region; deduced strength relative to residual two-nucleon weak interaction.
doi: 10.1103/PhysRevC.51.1521
1995FL04 Phys.Rev. C51, 2914 (1995) Effects of T- and P-Odd Weak Nucleon Interaction in Nuclei: Renormalizations due to residual strong interaction, matrix elements between compound states and their correlations with P-violating matrix elements
doi: 10.1103/PhysRevC.51.2914
1995FL07 Phys.Lett. 350B, 8 (1995) Possible Doublet Mechanism for a Regular Component of Parity Violation in Neutron Scattering NUCLEAR REACTIONS 232Th(polarized n, n), E not given; calculated parity nonconserving asymmetry; deduced possible doublet mechanism role in observed sign correlations.
doi: 10.1016/0370-2693(95)00325-F
1994FL01 Phys.Lett. 320B, 211 (1994) Spin Hedgehog and Collective Magnetic Quadrupole Moments Induced by Parity and Time Invariance Violating Interaction NUCLEAR STRUCTURE 163,161Dy; calculated collective magnetic quadrupole moment. Parity, time invariance violating interaction.
doi: 10.1016/0370-2693(94)90646-7
1994FL02 Phys.Rev. C49, 1827 (1994) Renormalization of the P- and T-Odd Nuclear Potentials by the Strong Interaction and Enhancement of P-Odd Effective Field
doi: 10.1103/PhysRevC.49.1827
1994FL07 Phys.Rev. C50, 3122 (1994) Random-Sign Observables Nonvanishing Upon Averaging: Enhancement of weak perturbations and parity nonconservation in compound nuclei
doi: 10.1103/PhysRevC.50.3122
1993FL02 Phys.Rev.Lett. 70, 4051 (1993) Matrix Elements between Nuclear Compound States and Dynamical Enhancement of the Weak Interaction NUCLEAR STRUCTURE 233Th; calculated intercompound states weak interaction mean squared matrix element; deduced agreement with data.
doi: 10.1103/PhysRevLett.70.4051
1993FL05 Phys.Rev. C48, 1329 (1993) Magnetic Interaction between Relativistic Atomic Electrons and Parity Nonconserving Nuclear Moments NUCLEAR STRUCTURE 133Cs, 209Bi; calculated relativistic electrons, P-odd nuclear current magnetic interaction; deduced finite size corrections magnitude.
doi: 10.1103/PhysRevC.48.1329
1992FL01 Phys.Rev. C45, 437 (1992) Regular Mechanism of Parity and Time Invariance Nonconserving Effects Enhancement in Neutron Capture and Scattering Near p-Wave Compound Resonances NUCLEAR STRUCTURE 239U, 233Th; calculated sign, magnitude of parity nonconserving effects; deduced mechanism of small interaction dynamical enhancements.
doi: 10.1103/PhysRevC.45.437
1989DZ03 Phys.Lett. 142A, 373 (1989) V.A.Dzuba, V.V.Flambaum, A.Ya.Kraftmakher, O.P.Sushkov Summation of the High Orders of Perturbation Theory in the Correlation Correction to the Hyperfine Structure and to the Amplitudes of E1-Transitions in the Caesium Atom NUCLEAR MOMENTS 133Cs; calculated hfs correlation correction. Higher order perturbation theory term summation.
doi: 10.1016/0375-9601(89)90385-X
1987DZ02 Phys.Scr. 36, 69 (1987) V.A.Dzuba, V.V.Flambaum, P.G.Silvestrov, O.P.Sushkov Parity Non-Conservation in Thallium and Caesium NUCLEAR STRUCTURE 205Tl, 133Cs; calculated parity non-conserving electric dipole transition amplitudes. Time-dependent Hartree-Fock method.
doi: 10.1088/0031-8949/36/1/010
1986FL01 Nucl.Phys. A449, 750 (1986) V.V.Flambaum, I.B.Khriplovich, O.P.Sushkov On the P- and T-Nonconserving Nuclear Moments NUCLEAR STRUCTURE 129,131Xe, 199,201Hg, 203,205Tl; calculated electric dipole, magnetic quadrupole, Schiff moments; deduced P-, T-nonconserving nucleon-nucleon interactions.
doi: 10.1016/0375-9474(86)90331-3
1985DZ01 Phys.Lett. 154B, 93 (1985) V.A.Dzuba, V.V.Flambaum, P.G.Silvestrov Bounds on Electric Dipole Moments and T-Violating Weak Interactions of the Nucleons NUCLEAR STRUCTURE 129Xe; calculated electric dipole moment; deduced T-odd interaction constant bounds.
doi: 10.1016/0370-2693(85)90564-7
1985DZ04 Phys.Scr. 32, 507 (1985) V.A.Dzuba, V.V.Flambaum, O.P.Sushkov Hyperfine Structures of Ra+ and Nuclear Magnetic Moments of Radium Isotopes NUCLEAR MOMENTS 211,213,221,223,225,227,229Ra; calculated μ. Relativistic Hartree-Fock method, hfs data input. ATOMIC PHYSICS Ra; calculated hfs, fine structure intervals, levels. Relativistic Hartree-Fock method.
doi: 10.1088/0031-8949/32/5/009
1985FL03 Nucl.Phys. A435, 352 (1985) Angular and Polarization Correlations in the (n, γ) Reaction NUCLEAR REACTIONS 35Cl, 81Br, 113Cd, 117Sn, 139La(polarized n, γ), E ≈ resonance; calculated odd-, even-parity correlation parameters.
doi: 10.1016/0375-9474(85)90469-5
1985FL04 Nucl.Phys. A444, 611 (1985) V.V.Flambaum, V.B.Telitsin, O.B.Sushkov Parity Nonconservation in pα Scattering NUCLEAR REACTIONS 4He(polarized p, p), E=15 MeV; analyzed σ(θ), asymmetry parameter vs θ; deduced parity nonconservation effect magnitude.
doi: 10.1016/0375-9474(85)90108-3
1985FL05 Phys.Lett. 162B, 213 (1985) V.V.Flambaum, I.B.Khriplovich, O.P.Sushkov Limit on the Constant of T-Nonconserving Nucleon-Nucleon Interaction NUCLEAR MOMENTS 129,131Xe, 199,201Hg, 203,205Tl; calculated Schiff moments; deduced T-noninvariant nucleon-nucleon interaction constant limit. Electric dipole moment data input.
doi: 10.1016/0370-2693(85)90908-6
1984DZ01 J.Phys.(London) B17, 1953 (1984) V.A.Dzuba, V.V.Flambaum, O.P.Sushkov Relativistic Many-Body Calculations of the Hyperfine-Structure Intervals in Caesium and Francium Atoms NUCLEAR MOMENTS 133Cs; calculated hfs. Relativistic Hartree-Fock theory. RADIOACTIVITY 208,209,210,211,212Fr(α), (β+), (EC); 213Fr(α), (EC); calculated μ;. Relativistic Hartree-Fock theory, hfs data analysis.
doi: 10.1088/0022-3700/17/10/005
1984DZ02 Phys.Lett. 103A, 265 (1984) V.A.Dzuba, V.V.Flambaum, P.G.Silvestrov, O.P.Sushkov Relativistic Many-Body Calculation of Parity-Violating E1-Amplitude for 6S → 7S Transition in Atomic Cesium ATOMIC PHYSICS Cs; calculated parity violating 6S-7S transition E1 amplitude.
doi: 10.1016/0375-9601(84)90122-1
1984FL03 Phys.Lett. 146B, 367 (1984) V.V.Flambaum, I.B.Khriplovich, O.P.Sushkov Nuclear Anapole Moments NUCLEAR STRUCTURE 133Cs, 203,205Tl, 207Pb, 209Bi; calculated parity violating electromagnetic nuclear moment; deduced P-odd electron-nucleus interaction effective coupling constant. Woods-Saxon potential, analytic approach.
doi: 10.1016/0370-2693(84)90140-0
1983DM01 Phys.Lett. 125B, 1 (1983) V.F.Dmitriev, V.V.Flambaum, O.P.Sushkov, V.B.Telitsin The Parity Violating Rotation of the Neutron Spin in Helium NUCLEAR REACTIONS 4He(polarized n, n), E=low; calculated spin rotation angle. Parity violating nucleon-nucleon interaction.
doi: 10.1016/0370-2693(83)91221-2
1981SU11 Yad.Fiz. 33, 59 (1981); Sov.J.Nucl.Phys. 33, 31 (1981) Mechanism for Parity Violation in Fission NUCLEAR REACTIONS, Fission 233,235U, 239Pu(polarized n, F), E=thermal; analyzed light fragment asymmetry, parity violation; deduced magnitude, mechanism for parity violation. Strong deformation, opposite parity rotational state mixing.
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