NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = T.S.Kosmas Found 53 matches. 2021KO42 Phys.Rev. C 104, 064618 (2021) T.S.Kosmas, V.K.B.Kota, D.K.Papoulias, R.Sahu Coherent elastic neutrino-nucleus scattering (CE ν NS) event rates for Ge, Zn, and Si detector materials NUCLEAR REACTIONS 70,73,76Ge, 64,70Zn, 28Si(ν, ν), (ν, X), E=1.3, 2.3, 4.5, 9.5, 52.8 MeV; calculated squares of proton and neutron form factors, differential and integrated event rates as function of the nuclear recoil energy with π-DAR neutrinos, reactor neutrinos and geoneutrinos. Deformed shell model (DSM), based on realistic nuclear forces, with application to coherent elastic neutrino-nucleus scattering (CEνNS) experiments: CONUS, νGEN, TEXONO, COHERENT, RICOCHET, MINER, NUCLEUS, CONNIE, Coherent Captain-Mills (CCM), European Spallation Source (ESS), vIOLETA, SBC. Relevance to unravelling still remaining uncertainties for the CEνNS process within and beyond the standard model.
doi: 10.1103/PhysRevC.104.064618
2020SA37 Phys.Rev. C 102, 035501 (2020) R.Sahu, D.K.Papoulias, V.K.B.Kota, T.S.Kosmas Elastic and inelastic scattering of neutrinos and weakly interacting massive particles on nuclei NUCLEAR STRUCTURE 127I, 133Cs, 133Xe; calculated levels, J, π, magnetic moments using deformed shell model (DSM), based on Hartree-Fock (HF) intrinsic states with angular momentum projection and band mixing, and compared with experimental data in the ENSDF database. NUCLEAR REACTIONS 23Na, 40Ar, 73Ge, 127I, 133Cs, 133Xe(ν, ν), (ν, ν'), E=reactor and solar neutrinos; calculated static spin matrix elements, normalized spin structure functions and squared proton and neutron nuclear form factors for the ground states, nuclear structure coefficients as functions of the mass of the weakly interacting massive particles (WIMP), event rates due to elastic WIMP-nucleus scattering, differential and integrated event rates as a function of the nuclear recoil energy; deduced expected neutrino-nucleus and WIMP-nucleus events at prominent rare-event detectors, calculated in the framework of the deformed shell model.
doi: 10.1103/PhysRevC.102.035501
2015GI04 Phys.Rev. C 92, 014606 (2015) Detailed description of exclusive muon capture rates using realistic two-body forces NUCLEAR REACTIONS 28Si(μ-, ν)28Al, 32S(μ-, ν)32P, 48Ti(μ-, ν)48Sc, 56Fe(μ-, ν)56Mn, 66Zn(μ-, ν)66Cu, 90Zr(μ-, ν)90Y, E*=0-30 MeV; calculated partial muon capture rates of different multipole transitions, total muon capture rates. Proton-neutron quasiparticle random-phase approximation (pn-QRPA) with Bonn C-D one-boson exchange potential as realistic nuclear force. Comparison with available experimental data. Relevance to muon capture experiments at Paul Scherrer Institute (PSI), Fermilab, Japan Proton Accelerator Research Complex, and RCNP. NUCLEAR STRUCTURE 56Mn, 90Y; calculated levels, J, π using pn-QRPA. Comparison with experimental data.
doi: 10.1103/PhysRevC.92.014606
2012TS05 Phys.Rev. C 86, 044618 (2012) Nuclear responses of 64, 66Zn isotopes to supernova neutrinos NUCLEAR REACTIONS 64,66Zn(ν, ν'), E=10-30, 50 MeV; calculated differential σ(E) as function of excitation energy of the nucleus, flux-averaged cross sections, folded differential and cumulative cross sections using several realistic SN neutrino models. Quasiparticle random-phase approximation using realistic two-body forces. Nuclear responses to energy spectra of supernova (SN) neutrinos.
doi: 10.1103/PhysRevC.86.044618
2012YD01 Nucl.Phys. A896, 1 (2012) E.Ydrefors, K.G.Balasi, T.S.Kosmas, J.Suhonen Detailed study of the neutral-current neutrino-nucleus scattering off the stable Mo isotopes NUCLEAR REACTIONS 92,94,95,96,97,98,100Mo(ν, ν'), E≈0-130 MeV; calculated, analyzed σ, interference contributions to σ, σ(E*) using QRPA and MQPM (microscopic quasiparticle-phonon model) for Mo as ν detector.
doi: 10.1016/j.nuclphysa.2012.10.001
2011BA36 Nucl.Phys. A868-869, 82 (2011) K.G.Balasi, E.Ydrefors, T.S.Kosmas Theoretical study of neutrino scattering off the stable even Mo isotopes at low and intermediate energies
doi: 10.1016/j.nuclphysa.2011.08.003
2011TS04 Phys.Rev. C 83, 054612 (2011) Low-energy neutral-current neutrino scattering on 128, 130Te isotopes NUCLEAR REACTIONS 128,130Te(ν, ν'), E<100 MeV; calculated differential cross sections as function of excitation energy, total σ(E). Quasiparticle random phase approximation (QRPA) with realistic two-nucleon forces. Comparison with experimental data.Relevance to double-beta decay experiments.
doi: 10.1103/PhysRevC.83.054612
2011TS09 Phys.Rev. C 84, 064620 (2011) Analyzing astrophysical neutrino signals using realistic nuclear structure calculations and the convolution procedure NUCLEAR REACTIONS 128,130Te(ν, ν'), E<70 MeV; calculated convoluted single and double-differential cross sections, convoluted total cross section, synthetic β-beam spectral distributions. Quasiparticle random-phase approximation, Fermi-Dirac and power-law distributions. Relevance to supernova neutrino spectra. RADIOACTIVITY 6He(β-); calculated boosted β-beam antineutrino spectrum generated by accelerating β-radioactive ions of 6He.
doi: 10.1103/PhysRevC.84.064620
2011YD01 Nucl.Phys. A866, 67 (2011), Erratum Nucl.Phys. A878, 1 (2012) E.Ydrefors, K.G.Balasi, T.S.Kosmas, J.Suhonen The response of 95, 97Mo to supernova neutrinos NUCLEAR REACTIONS 95,97Mo(ν, ν'), (ν-bar, ν-bar'), E=0-120 MeV; calculated neutral-current coherent, incoherent σ using wavefunctions from MQPM (Microscopic Quasiparticle-Phonon Model).
doi: 10.1016/j.nuclphysa.2011.07.007
2010DI11 Phys.Scr. 82, 065201 (2010) P.C.Divari, V.C.Chasioti, T.S.Kosmas Neutral current neutrino-98Mo reaction cross sections at low and intermediate energies NUCLEAR REACTIONS 98Mo(ν, ν'), E < 70 MeV; calculated flux-averaged total σ for neutral current scattering, σ(θ, E). QRPA, two-parameter Fermi-Dirac distribution for the supernova neutrino energy spectrum.
doi: 10.1088/0031-8949/82/06/065201
2010KA41 J.Phys.:Conf.Ser. 202, 012029 (2010) G.I.Karathanou, V.Tsikoudi, T.S.Kosmas Simulated analysis of low-flux solar neutrinos and their terrestrial detection NUCLEAR REACTIONS 28Si(ν, ν), (ν, ν'), E=0.0000642-0.075 MeV; measured reaction products; deduced σ, dσ using published formfactors.
doi: 10.1088/1742-6596/202/1/012029
2009CH57 Nucl.Phys. A829, 234 (2009) A unified formalism for the basic nuclear matrix elements in semi-leptonic processes NUCLEAR REACTIONS 98Mo(ν, ν'), E=0-100 MeV; calculated σ, σ(θ) using QRPA for dominant multipole states.
doi: 10.1016/j.nuclphysa.2009.08.009
2007CH38 Prog.Part.Nucl.Phys. 59, 481 (2007) V.Ch.Chasioti, T.S.Kosmas, P.C.Divari Inelastic neutrino-nucleus reaction cross sections at low neutrino-energies NUCLEAR REACTIONS 40Ar(ν, ν'), E< 100 MeV; 56Fe(ν, ν'), E=10-100 MeV; calculated energy and angular dependence of σ and integrated inelastic neutrino-nucleus cross sections.
doi: 10.1016/j.ppnp.2007.01.003
2006DE31 Nucl.Phys. B752, 80 (2006) F.Deppisch, T.S.Kosmas, J.W.F.Valle Enhanced μ- - e- conversion in nuclei in the inverse seesaw model NUCLEAR REACTIONS 27Al, 48Ti, 197Au(μ-, e-), E not given; analyzed μ- → e- conversion data; deduced parameters. 12C, 27Al, 32S, 40Ca, 48Ti, 63Cu, 90Zr, 112Cd, 197Au, 208Pb, 238U(μ-, e-), E not given; analyzed conversion rates, branching ratios, related features. Inverse seesaw model of neutrino masses.
doi: 10.1016/j.nuclphysb.2006.06.032
2006DI05 Nucl.Phys. A767, 259 (2006) P.C.Divari, J.D.Vergados, T.S.Kosmas Transition matrix elements for the exotic double-charge exchange μ- → e+ conversion in 27Al NUCLEAR REACTIONS 27Al(μ-, e+), E not given; calculated transition matrix elements for neutrinoless conversion; deduced reaction mechanism features.
doi: 10.1016/j.nuclphysa.2005.12.003
2006KO20 Czech.J.Phys. 56, 467 (2006) M.Kortelainen, J.Suhonen, J.Toivanen, T.S.Kosmas Theoretical LSP detection rates for dark-matter detectors NUCLEAR STRUCTURE 23Na, 71Ga, 73Ge, 127I; calculated static spin matrix elements, detection rates for lightest supersymmetric particle. Shell model.
doi: 10.1007/s10582-006-0110-x
2006MO05 Int.J.Mod.Phys. E15, 659 (2006) Ch.C.Moustakidis, T.S.Kosmas, F.Simkovic, A.Faessler The effects of deformation and pairing correlations on nuclear charge form factor NUCLEAR STRUCTURE 24,26Mg, 28Si, 32S; calculated charge form factors, quadrupole moments, deformation, pairing correlations.
doi: 10.1142/S0218301306004570
2006PA13 Phys.Rev. C 73, 035502 (2006) P.Papakonstantinou, T.S.Kosmas, J.Wambach, A.Faessler Continuum random-phase approximation study of the incoherent μ- - e- conversion rate and its spurious 1- admixture NUCLEAR REACTIONS 208Pb(μ-, e-), E at rest; calculated transition strength distribution, incoherent rate; deduced spurious contribution from 1- state. Continuum RPA.
doi: 10.1103/PhysRevC.73.035502
2006PA22 Czech.J.Phys. 56, 481 (2006) P.Papakonstantinou, J.Wambach, O.Civitarese, T.S.Kosmas The role of the continuum and the spurious 1- transitions in incoherent μ--e- conversion rate calculations NUCLEAR REACTIONS 40Ca, 208Pb(μ-, e), E at rest; calculated conversion rates, strength distributions. Self-consistent continuum RPA, Skyrme interactions.
doi: 10.1007/s10582-006-0112-8
2005LI34 Phys.Rev. C 72, 025803 (2005) Screened thermonuclear reactions and predictive stellar evolution of detached double-lined eclipsing binaries
doi: 10.1103/PhysRevC.72.025803
2004HO15 Phys.Lett. B 584, 31 (2004) E.Holmlund, M.Kortelainen, T.S.Kosmas, J.Suhonen, J.Toivanen Microscopic calculation of the LSP detection rates for the 71Ga, 73Ge and 127I dark-matter detectors NUCLEAR STRUCTURE 71Ga, 73Ge, 127I; calculated levels, J, π, μ, supersymmetric particle scattering cross sections. Implications for dark matter search discussed.
doi: 10.1016/j.physletb.2004.01.045
2004HO16 Yad.Fiz. 67, 1220 (2004); Phys.Atomic Nuclei 67, 1198 (2004) E.Holmlund, M.Kortelainen, T.S.Kosmas, J.Suhonen, J.Toivanen Theoretical LSP Detection Rates for 71Ga, 73Ge, and 127I Dark-Matter Detectors NUCLEAR STRUCTURE 71Ga, 73Ge, 127I; calculated interaction rates with light supersymmetric particles. Microscopic quasiparticle-phonon model.
doi: 10.1134/1.1772459
2003KO69 Phys.Rev. C 68, 054315 (2003) T.S.Kosmas, A.Faessler, R.Sahu Transition matrix elements for μ-e conversion in 72Ge using the deformed Hartree-Fock method NUCLEAR STRUCTURE 72Ge; calculated levels, J, π. Deformed Hartree-Fock method. NUCLEAR REACTIONS 72Ge(μ-, e-), E not given; calculated transition matrix elements. Deformed Hartree-Fock method.
doi: 10.1103/PhysRevC.68.054315
2003PA01 Nucl.Phys. A713, 81 (2003) P.Papakonstantinou, E.Mavrommatis, T.S.Kosmas The two-body momentum distribution in finite nuclei NUCLEAR STRUCTURE 4He, 16O; calculated two-body momentum distributions. Analytical expression, independent-particle shell model.
doi: 10.1016/S0375-9474(02)01295-2
2002CH26 Czech.J.Phys. 52, 467 (2002) Closed Expressions for the Nuclear Moments in Semi-Leptonic Processes
doi: 10.1023/A:1015349008360
2002DI14 Nucl.Phys. A703, 409 (2002) P.C.Divari, J.D.Vergados, T.S.Kosmas, L.D.Skouras The Exotic Double-Charge Exchange μ- → e+ Conversion in Nuclei NUCLEAR REACTIONS 27Al(μ-, e+), E not given; calculated transition matrix elements for neutrinoless conversion; deduced reaction mechanism features.
doi: 10.1016/S0375-9474(01)01533-0
2002KO30 Prog.Part.Nucl.Phys. 48, 307 (2002) Current Nuclear Physics Issues in Studying the Neutrinoless (μ-, e-) Conversion in Nuclei NUCLEAR REACTIONS 72Ge(μ-, e-), E not given; calculated photonic and nonphotonic conversion matrix elements, deformation effects.
doi: 10.1016/S0146-6410(02)00139-4
2002KO55 J.Phys.(London) G28, 2907 (2002) On the muon-nucleus integrals entering the neutrinoless μ-→ e-conversion rates NUCLEAR REACTIONS 16O, 19F, 24Mg, 28Si, 36Ar, 48Ti, 56Fe, 64Zn, 98Mo, 112Cd, 124Sn, 139La, 156Gd, 181Ta, 186W, 208Pb, 209Bi, 238U(μ-, e-), E at rest; calculated neutrinoless conversion rate, related features.
doi: 10.1088/0954-3899/28/12/302
2001DI21 Part. and Nucl., Lett. 104, 53 (2001) P.C.Divari, J.D.Vergados, T.S.Kosmas, L.D.Skouras Exotic Muon-to-Positron Conversion in Nuclei: Partial transition sum evaluation by using shell model NUCLEAR REACTIONS 27Al(μ-, e+), E not given; calculated matrix elements, strength distribution, total rate. Intermediate neutrino mixing model.
2001KO08 Nucl.Phys. A683, 443 (2001) Exotic μ- → e- Conversion in Nuclei: Energy moments of the transition strength and average energy of the outgoing e- NUCLEAR REACTIONS 48Ti, 60Ni, 72Ge, 112Cd, 162Yb, 208Pb(μ-, e), E not given; calculated transition strengths, average energy of outgoing electron. Renormalized quasiparticle RPA, comparison with closure approximation.
doi: 10.1016/S0375-9474(00)00471-1
2001KO32 Czech.J.Phys. 51, 459 (2001) T.S.Kosmas, T.Siiskonen, J.Suhonen Upper Limits for Lepton-Flavor Violation from the Exotic μ- → e- Conversion NUCLEAR REACTIONS 27Al, 48Ti, 208Pb(μ-, e-), E not given; calculated muon-electron conversion matrix elements, branching ratio limits.
doi: 10.1023/A:1017552016301
2001KO40 Phys.Lett. 511B, 203 (2001) T.S.Kosmas, S.Kovalenko, I.Schmidt Nuclear μ--e- Conversion in Strange Quark Sea NUCLEAR STRUCTURE 27Al, 48Ti, 197Au; calculated muon-to-electron conversion matrix elements. Effective Lagrangian approach.
doi: 10.1016/S0370-2693(01)00657-8
2000DI12 Phys.Rev. C61, 054612 (2000) P.C.Divari, T.S.Kosmas, J.D.Vergados, L.D.Skouras Shell Model Calculations for Light Supersymmetric Particle Scattering Off Light Nuclei NUCLEAR STRUCTURE 19F, 23Na, 29Si; calculated wave functions, matrix elements, form factors for elastic scattering of light supersymmetric particles. Shell model. Application to cold dark matter search discussed.
doi: 10.1103/PhysRevC.61.054612
2000FA18 Nucl.Phys. B587, 25 (2000) A.Faessler, T.S.Kosmas, S.Kovalenko, J.D.Vergados Exotic μ--e- Conversion in Nuclei and R-Parity Violating Supersymmetry NUCLEAR STRUCTURE 27Al, 48Ti, 208Pb; calculated μ--e- conversion transition matrix elements; deduced limits on R-parity violating parameters. Minimal supersymmetric standard model.
doi: 10.1016/S0550-3213(00)00446-6
2000KO08 Nucl.Phys. A665, 183 (2000) The Inclusive μ - e Conversion Process with Renormalized Quasiparticle Random-Phase Approximation NUCLEAR REACTIONS 48Ti, 60Ni, 72Ge, 112Cd, 162Yb, 208Pb(μ-, e-), E not given; calculated coherent and incoherent muon-electron conversion matrix elements. Renormalized quasiparticle RPA.
doi: 10.1016/S0375-9474(99)00688-0
2000PA32 Nucl.Phys. A673, 171 (2000) P.Papakonstantinou, E.Mavrommatis, T.S.Kosmas Generalized Momentum Distribution in Finite Nuclei NUCLEAR STRUCTURE 16O, 40Ca; calculated generalized momentum distributions; deduced finite-size effects.
doi: 10.1016/S0375-9474(00)00135-4
2000PA35 Prog.Part.Nucl.Phys. 44, 87 (2000) P.Papakonstantinou, E.Mavrommatis, T.S.Kosmas Beyond the One-Body Momentum Distribution in Finite Nuclei NUCLEAR STRUCTURE 16O; calculated generalized momentum distribution; deduced finite-size effects.
doi: 10.1016/S0146-6410(00)00061-2
2000SI31 Phys.Rev. C62, 035502 (2000) T.Siiskonen, J.Suhonen, T.S.Kosmas Realistic Nuclear Matrix Elements for the Lepton-Flavor Violating μ- → e- Conversion in 27Al and 48Ti NUCLEAR REACTIONS 27Al, 48Ti(μ-, e), E not given; calculated transition matrix elements; deduced flavor violation constraints.
doi: 10.1103/PhysRevC.62.035502
1999SI20 Phys.Rev. C60, 062501 (1999) T.Siiskonen, J.Suhonen, T.S.Kosmas New Limits for Lepton-Flavor Violation from the μ- → e- Conversion in 27Al NUCLEAR REACTIONS 27Al(μ-, e), E at rest; calculated transition matrix elements; deduced lepton-flavor violation limits. ATOMIC PHYSICS, Mesic-atoms 27Al(μ-, e), E at rest; calculated transition matrix elements; deduced lepton-flavor violation limits.
doi: 10.1103/PhysRevC.60.062501
1998KO41 Yad.Fiz. 61, No 7, 1261 (1998); Phys.Atomic Nuclei 61, 1161 (1998) T.S.Kosmas, J.D.Vergados, A.Faessler Muon-Number-Violating Processes in Nuclei NUCLEAR REACTIONS 48Ti, 60Ni, 72Ge, 112Cd, 162Yb, 208Pb(μ-, e-), E not given; calculated exotic muon-electron conversion matrix elements, rates, mean excitation energies; deduced dominance of coherent mode.
1998SC47 Phys.Lett. 443B, 7 (1998) J.Schwieger, T.S.Kosmas, A.Faessler The Exotic μ- → e- Conversion Rates by Explicit Normalized Quasiparticle RPA Calculations NUCLEAR REACTIONS 48Ti, 60Ni, 72Ge, 112Cd, 162Yb, 208Pb(μ-, e), E at rest; calculated ground-state nucleon-nucleon correlations, normalization factors, transition matrix elements; deduced constraints on flavor violating parameters. Renormalized quasiparticle RPA.
doi: 10.1016/S0370-2693(98)01331-8
1997KO20 J.Phys.(London) G23, 693 (1997) T.S.Kosmas, A.Faessler, J.D.Vergados The New Limits of the Neutrinoless (μ-, e-) Conversion Branching Ratio NUCLEAR REACTIONS 208Pb, 48Ti(μ-, e-), E not given; calculated exotic μ- → e- conversion ratio; deduced new limits on associated elementary particle parameters. Different models.
doi: 10.1088/0954-3899/23/6/008
1997KO26 Phys.Rev. C56, 526 (1997) T.S.Kosmas, A.Faessler, F.Simkovic, J.D.Vergados State-by-State Calculations for All Channels of the Exotic (μ-, e-) Conversion Process NUCLEAR STRUCTURE 48Ti, 60Ni, 72Ge, 112Cd, 162Yb, 208Pb; calculated coherent, total μ- → e- conversion matrix elements; deduceddependence on mass, Z. Quasiparticle RPA.
doi: 10.1103/PhysRevC.56.526
1997SC33 Phys.Rev. C56, 2830 (1997) J.Schwieger, A.Faessler, T.S.Kosmas Detailed Study of the Incoherent μ- → e- Conversion Rate: Elimination of spurious contaminations from the 1- contribution NUCLEAR STRUCTURE 48Ti, 60Ni, 72Ge, 112Cd, 162Yb, 208Pb; calculated incoherent muon-electron conversion matrix elements; deduced importance to lepton flavor violation studies. Quasiparticle RPA.
doi: 10.1103/PhysRevC.56.2830
1996KO03 Phys.Rev. C53, 1409 (1996) Charged Current Neutrino-Nucleus Reaction Cross Sections at Intermediate Energies NUCLEAR REACTIONS 12C, 37Cl, 40Ar, 81Br, 71Ga, 98Mo, 115In, 127I, 205Tl(ν, e-), (ν, μ-), (ν, e+), (ν, μ+), E ≤ 0.5 GeV; calculated σ(E) for these and inclusive, semi-inclusive reactions.
doi: 10.1103/PhysRevC.53.1409
1996KO34 Phys.Rep. 264, 251 (1996) (μ-, e-) Conversion: A symbiosis of particle and nuclear physics NUCLEAR STRUCTURE 48Ti, 60Ni, 72Ge, 112Cd, 162Yb, 208Pb; calculated coherent (μ-, e-) conversion matrix elements. Shell model, RPA approaches comparison.
doi: 10.1016/0370-1573(95)00041-0
1994KO09 Nucl.Phys. A570, 637 (1994) T.S.Kosmas, J.D.Vergados, O.Civitarese, A.Faessler Study of the Muon Number Violating (μ-, e-) Conversion in a Nucleus by using Quasi-Particle RPA NUCLEAR REACTIONS 48Ti(μ-, e-), E at rest; calculated total, coherent conversion rates. Quasiparticle RPA.
doi: 10.1016/0375-9474(94)90077-9
1993CH28 Nucl.Phys. A559, 526 (1993) H.C.Chiang, E.Oset, T.S.Kosmas, A.Faessler, J.D.Vergados Coherent and Incoherent (μ-, e-) Conversion in Nuclei NUCLEAR STRUCTURE A=12-238; calculated coherent, incoherent (μ-, e-) conversion matrix elements, form factors, widths. Flavour lepton number violating theories.
doi: 10.1016/0375-9474(93)90259-Z
1992KO03 Nucl.Phys. A536, 72 (1992) Nuclear Densities with Fractional Occupation Probabilities of the States NUCLEAR STRUCTURE 40Ca; calculated charge density distribution, charge form factor. Z=2-92; calculated mean square radii. Harmonic oscillator shell model, surface orbits fractional occupation probabilities.
doi: 10.1016/0375-9474(92)90246-G
1991AN05 Can.J.Phys. 69, 114 (1991) G.S.Anagnostatos, T.S.Kosmas, E.F.Hefter, C.N.Panos Semiclassical Approximation for the Isotopic Shift of Charge Radii in Ca Isotopes NUCLEAR STRUCTURE 40,41,42,43,44,45,46,47,48Ca; analyzed isotope shift, rms charge, mass radii. Isomorphic shell model.
doi: 10.1139/p91-017
1990KO10 Nucl.Phys. A510, 641 (1990) Study of the Flavour Violating (μ-, e-) Conversion in Nuclei NUCLEAR STRUCTURE A=4-208; calculated total (μ-, e-) conversion rate; deduced coherent conversion rate ratio. Shell model, effective operators.
doi: 10.1016/0375-9474(90)90353-N
1989KO01 Phys.Lett. 217B, 19 (1989) Sum Rules for the Inclusive μ-e Conversion Exotic Reaction NUCLEAR STRUCTURE A=4-208; calculated (μ-, e-) total conversion rate. Sum rules.
doi: 10.1016/0370-2693(89)91508-6
1988KO30 Phys.Lett. 215B, 460 (1988) Nuclear Matrix Elements for the Coherent μ-e Conversion Process NUCLEAR STRUCTURE A ≤ 200; analyzed n, p elastic nuclear form factor systematics; deduced coherent (μ-e) conversion process matrix elements.
doi: 10.1016/0370-2693(88)91341-X
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