NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = M.J.Ramsey-Musolf Found 45 matches. 2023HA12 Phys.Rev. C 107, 035504 (2023) W.C.Haxton, E.Rule, K.McElvain, M.J.Ramsey-Musolf Nuclear-level effective theory of μ → e conversion: Formalism and applications NUCLEAR REACTIONS 12C, 16O, 19F, 23Na, 27Al, 28Si, 32S, 40Ca, 48Ti, 56Fe, 63,65Cu, 184W, 197Au, 208Pb(μ-, e-), at momentum transfer q=96.54-105.12 MeV; calculated μ to e conversion rates, with derivation of bounds on the coefficients of the charged lepton flavor violation decay (CLFV) operators, and full evaluation of the associated nuclear response functions, and accurate treatment of electron and muon Coulomb effects using advanced shell-model methods. Discussed matching of the nonrelativistic effective theory (NRET) onto higher level effective field theories, and relation of μ to e conversion to μ to e+γ, and μ to 3e. Comparison with results from MEG, MEG II, Mu3e and SINDRUM experiments. Relevance to future μ to e conversion searches at Fermilab (Mu2e) and J-PARC (COMET, DeeMe) experimental facilities to improve and to advance limits to higher orders on charged lepton flavor violation (CLFV) decays of light pseudoscalars via μ to e conversion in Nuclei.
doi: 10.1103/PhysRevC.107.035504
2022CI02 Phys.Rev. C 105, 055504 (2022) V.Cirigliano, K.Fuyuto, M.J.Ramsey-Musolf, E.Rule Next-to-leading order scalar contributions to μ → e conversion NUCLEAR REACTIONS 27Al, 48Ti, 197Au, 208Pb(μ-, e-), at nuclear Fermi momentum=238-265 MeV; calculated μ to e conversion rates, dimensionless overlap integrals, LO, NLO, and two-nucleon contributions using standard model effective field theory (SM-EFT), including next-to-leading order (NLO) terms in one- and two-nucleon interactions in chiral effective theory; discussed implications for testing Higgs-mediated charged lepton flavor violation (CLFV) in future experimental searches at Fermilab and J-PARC facilities.
doi: 10.1103/PhysRevC.105.055504
2018BA24 Phys.Rev. C 98, 015208 (2018) A.Bartolotta, M.J.Ramsey-Musolf Coherent μ-e conversion at next-to-leading order NUCLEAR REACTIONS 27Al(μ-, e-), E not given; analyzed coherent muon to electron conversion versus muon capture at next-to-leading order (NLO); deduced expressions for branching ratio in terms of Wilson coefficients associated with possible physics beyond the standard model, and model-independent parameters for scalar- and vector-mediated muon to electron conversion, and parameters for neutron density distribution. Relevance to SINDRUM II Collaboration experimental results, and next generation experiments, Mu2e and COMET.
doi: 10.1103/PhysRevC.98.015208
2013EN01 Prog.Part.Nucl.Phys. 71, 21 (2013) J.Engel, M.J.Ramsey-Musolf, U.van Kolck Electric dipole moments of nucleons, nuclei, and atoms: The Standard Model and beyond
doi: 10.1016/j.ppnp.2013.03.003
2013GL02 Phys.Rev. C 88, 025202 (2013) M.J.Glatzmaier, S.Mantry, M.J.Ramsey-Musolf Higher twist in electroproduction: Flavor nonsinglet QCD evolution
doi: 10.1103/PhysRevC.88.025202
2013PI02 Phys.Rev. C 87, 015205 (2013) M.Pitschmann, C.-Y.Seng, M.J.Ramsey-Musolf, C.D.Roberts, Se.M.Schmidt, D.J.Wilson Electric dipole moment of the ρ meson
doi: 10.1103/PhysRevC.87.015205
2013SE11 Phys.Rev. C 88, 015202 (2013) Parity-violating deep-inelastic electron-deuteron scattering: Higher twist and parton angular momentum
doi: 10.1103/PhysRevC.88.015202
2011AD03 Rev.Mod.Phys. 83, 195 (2011) E.G.Adelberger, A.Garcia, R.G.H.Robertson, K.A.Snover, A.B.Balantekin, K.Heeger, M.J.Ramsey-Musolf, A.B.Balantekin, K.Heeger, M.J.Ramsey-Musolf, D.Bemmerer, A.Junghans, D.Bemmerer, A.Junghans, C.A.Bertulani, K.-W.Chen, H.Costantini, P.Prati, M.Couder, E.Uberseder, M.Wiescher, R.Cyburt, B.Davids, S.J.Freedman, M.Gai, D.Gazit, L.Gialanella, G.Imbriani, U.Greife, M.Hass, W.C.Haxton, T.Itahashi, K.Kubodera, K.Langanke, D.Leitner, M.Leitner, P.Vetter, L.Winslow, L.E.Marcucci, T.Motobayashi, A.Mukhamedzhanov, R.E.Tribble, F.M.Nunes, T.-S.Park, R.Schiavilla, E.C.Simpson, C.Spitaleri, F.Strieder, H.-P.Trautvetter, K.Suemmerer, S.Typel Solar fusion cross sections. II. The pp chain and CNO cycles NUCLEAR REACTIONS 2H(p, γ), 3He(3He, 2p), (α, γ), (p, e), 7Be, 12C, 14N, 15N, 17O(p, γ), 15N, 16,17,18O(p, α), E<3 MeV; analyzed and evaluated experimental data; deduced recommended values and uncertainties.
doi: 10.1103/RevModPhys.83.195
2011GO21 Phys.Rev. C 84, 015502 (2011) M.Gorchtein, C.J.Horowitz, M.J.Ramsey-Musolf Model dependence of the γ Z dispersion correction to the parity-violating asymmetry in elastic ep scattering NUCLEAR REACTIONS 1H(polarized e, e), E=2.2375-5.498 GeV; calculated total photoabsorption cross section, differential cross section for inclusive electroproduction; deduced theory uncertainty at the kinematics of the Q-Weak experiment. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.015502
2010MA65 Phys.Rev. C 82, 065205 (2010) S.Mantry, M.J.Ramsey-Musolf, G.F.Sacco Examination of higher-order twist contributions in parity-violating deep-inelastic electron-deuteron scattering
doi: 10.1103/PhysRevC.82.065205
2008RA14 Nucl.Phys. A805, 137c (2008) Nuclear Science and the New Standard Model
doi: 10.1016/j.nuclphysa.2008.02.234
2007LI54 Phys.Rev. C 76, 035503 (2007) C.-P.Liu, M.J.Ramsey-Musolf, W.C.Haxton, R.G.E.Timmermans, A.E.L.Dieperink Atomic electric dipole moments: The Schiff theorem and its corrections
doi: 10.1103/PhysRevC.76.035503
2007RA25 Eur.Phys.J. A 32, 379 (2007) Future directions in parity violation From quarks to the cosmos
doi: 10.1140/epja/i2006-10413-1
2006RA33 Ann.Rev.Nucl.Part.Sci. 56, 1 (2006) Hadronic Parity Violation: A New View Through the Looking Glass
doi: 10.1146/annurev.nucl.54.070103.181255
2005ER02 Prog.Part.Nucl.Phys. 54, 351 (2005) Low energy tests of the weak interaction
doi: 10.1016/j.ppnp.2004.08.001
2005RA05 Eur.Phys.J. A 24, Supplement 2, 197 (2005) Parity-violation with electrons: Theoretical perspectives
doi: 10.1140/epjad/s2005-04-049-3
2005ZH05 Nucl.Phys. A748, 435 (2005) S.-L.Zhu, C.M.Maekawa, B.R.Holstein, M.J.Ramsey-Musolf, U.van Kolck Nuclear parity violation in effective field theory
doi: 10.1016/j.nuclphysa.2004.10.032
2004CI07 Phys.Rev.Lett. 93, 231802 (2004) V.Cirigliano, A.Kurylov, M.J.Ramsey-Musolf, P.Vogel Neutrinoless Double Beta Decay and Lepton Flavor Violation
doi: 10.1103/PhysRevLett.93.231802
2004DI19 Phys.Rev. C 70, 054003 (2004) L.Diaconescu, M.J.Ramsey-Musolf Vector analyzing power in elastic electron-proton scattering NUCLEAR REACTIONS 1H(polarized e, e), E=0-1 GeV; calculated vector analyzing power. Effective field theory.
doi: 10.1103/PhysRevC.70.054003
2004SP01 Phys.Lett. B 583, 79 (2004) D.T.Spayde, D.H.Beck, R.Hasty, T.Averett, D.Barkhuff, G.Dodson, K.Dow, M.Farkhondeh, W.Franklin, E.Tsentalovich, B.Yang, T.Zwart, E.J.Beise, H.Breuer, R.Tieulent, R.Carr, S.Covrig, B.W.Filippone, T.M.Ito, R.D.McKeown, W.Korsch, S.Kowalski, B.Mueller, M.L.Pitt, M.J.Ramsey-Musolf, J.Ritter, S.P.Wells The strange quark contribution to the proton's magnetic moment NUCLEAR REACTIONS 1H(polarized e, e'), E=200 MeV; analyzed polarization observables, related data. 1H deduced strange quark contribution to μ.
doi: 10.1016/j.physletb.2004.01.002
2003KU06 Phys.Rev. C 67, 035502 (2003) A.Kurylov, M.J.Ramsey-Musolf, P.Vogel Radiative corrections to low-energy neutrino reactions NUCLEAR REACTIONS 2H(ν, ep), (ν-bar, e+n), E=low; 1H(p, e+ν), E ≈ 0.93 MeV; calculated radiative corrections to σ.
doi: 10.1103/PhysRevC.67.035502
2003KU18 Nucl.Phys. B667, 321 (2003) A.Kurylov, M.J.Ramsey-Musolf, S.Su Supersymmetric effects in deep inelastic neutrino-nucleus scattering
doi: 10.1016/S0550-3213(03)00528-5
2003LI10 Phys.Rev. C 67, 035501 (2003) C.-P.Liu, G.Prezeau, M.J.Ramsey-Musolf Hadronic parity violation and inelastic electron-deuteron scattering NUCLEAR REACTIONS 2H(e, e'), E=120, 194 MeV; calculated σ, σ(θ), parity-violating asymmetry, hadronic contributions.
doi: 10.1103/PhysRevC.67.035501
2002HA21 Phys.Rev. C65, 045502 (2002) W.C.Haxton, C.-P.Liu, M.J.Ramsey-Musolf Nuclear Anapole Moments NUCLEAR STRUCTURE 131In, 131,133Sn, 133Sb, 133Cs, 205,207Tl, 207,209Pb, 209Bi; calculated anapole moments; analyzed data; deduced constraints on parity-nonconserving coupling constants. Meson-exchange approach.
doi: 10.1103/PhysRevC.65.045502
2002KU19 Phys.Rev. C65, 055501 (2002) A.Kurylov, M.J.Ramsey-Musolf, P.Vogel Radiative Corrections in Neutrino-Deuterium Disintegration NUCLEAR REACTIONS 2H(ν, pe), (ν, nν), E=2-16 MeV; calculated radiative corrections.
doi: 10.1103/PhysRevC.65.055501
2001HA33 Phys.Rev.Lett. 86, 5247 (2001) W.C.Haxton, C.-P.Liu, M.J.Ramsey-Musolf Anapole Moment and Other Constraints on the Strangeness Conserving Hadronic Weak Interaction NUCLEAR STRUCTURE 133Cs, 205Tl; calculated nuclear polarization contributions to anapole moments; deduced constraints on parity-nonconserving meson couplings.
doi: 10.1103/PhysRevLett.86.5247
2001ZH03 Phys.Rev. D63, 033006 (2001) S.-L.Zhu, S.J.Puglia, B.R.Holstein, M.J.Ramsey-Musolf Chiral Symmetry and the Parity-Violating NNπ Yukawa Coupling
doi: 10.1103/PhysRevD.63.033006
2001ZH24 Phys.Rev. C64, 035502 (2001) S.L.Zhu, S.Puglia, B.R.Holstein, M.J.Ramsey-Musolf Subleading Corrections to Parity-Violating Pion Photoproduction
doi: 10.1103/PhysRevC.64.035502
2000RA21 Phys.Rev. D62, 056009 (2000) Nuclear β Decay, Atomic Parity Violation, and New Physics
doi: 10.1103/PhysRevD.62.056009
2000ZH25 Phys.Rev. D62, 033008 (2000) S.-H.Zhu, S.J.Puglia, B.R.Holstein, M.J.Ramsey-Musolf Nucleon Anapole Moment and Parity-Violating ep Scattering NUCLEAR REACTIONS 1H(e, X), E not given; calculated axial vector radiative corrections, role of parity violating effects.
doi: 10.1103/PhysRevD.62.033008
1999HA53 Phys.Rev. C60, 045204 (1999); Erratum Phys.Rev. C62, 049902 (2000) H.-W.Hammer, M.J.Ramsey-Musolf K(K-bar) Continuum and Isoscalar Nucleon Form Factors
doi: 10.1103/PhysRevC.60.045204
1999HA54 Phys.Rev. C60, 045205 (1999); Erratum Phys.Rev. C62, 049903 (2000) H.-W.Hammer, M.J.Ramsey-Musolf Spectral Content of Isoscalar Nucleon Form Factors
doi: 10.1103/PhysRevC.60.045205
1999RA17 Phys.Rev. C60, 015501 (1999) Low-Energy Parity-Violation and New Physics
doi: 10.1103/PhysRevC.60.015501
1998BA70 Nucl.Phys. A640, 259 (1998) L.L.Barz, H.Forkel, H.-W.Hammer, F.S.Navarra, M.Nielsen, M.J.Ramsey-Musolf K* Mesons and Nucleon Strangeness
doi: 10.1016/S0375-9474(98)00438-2
1998HA04 Phys.Lett. 416B, 5 (1998) H.-W.Hammer, M.J.Ramsey-Musolf Nucleon Vector Strangeness Form Factors: Multi-pion continuum and the OZI rule
doi: 10.1016/S0370-2693(97)01322-1
1998IT04 Phys.Rev. C58, 2595 (1998) Strange Mesonic Transition Form Factor in the Chiral Constituent Quark Model
doi: 10.1103/PhysRevC.58.2595
1998MU10 Nucl.Phys. A633, 481 (1998) N.C.Mukhopadhyay, M.J.Ramsey-Musolf, S.J.Pollock, J.Liu, H.-W.Hammer Parity-Violating Excitation of the Δ(1232): Hadron structure and new physics
doi: 10.1016/S0375-9474(98)00147-X
1997RA13 Phys.Rev. C55, 3066 (1997) Chiral Symmetry and the Nucleon's Vector Strangeness Form Factors NUCLEAR STRUCTURE 1n; calculated strangeness vector current form factors; deduced utility of chiral symmetry approach. Several models compared.
doi: 10.1103/PhysRevC.55.3066
1996BA59 Phys.Rev. C54, 1954 (1996) M.B.Barbaro, A.De Pace, T.W.Donnelly, A.Molinari, M.J.Musolf Probing Nucleon Strangeness with Neutrinos: Nuclear model dependences
doi: 10.1103/PhysRevC.54.1954
1996GO03 Phys.Rev. C53, 399 (1996) Strange Mesonic Transition Form Factor
doi: 10.1103/PhysRevC.53.399
1994MU11 Phys.Rev. C50, 2173 (1994) M.J.Musolf, R.Schiavilla, T.W.Donnelly Many-Body Currents and the Strange-Quark Content of 4He NUCLEAR REACTIONS 4He(polarized e, e), E not given; calculated parity violating asymmetry; deduced meson exchange currents, strange quark content roles. Monte Carlo techniques, variational approach.
doi: 10.1103/PhysRevC.50.2173
1993MU18 Phys.Lett. 318B, 263 (1993) Meson-Exchange Currents and the Strangeness Radius of 4He NUCLEAR STRUCTURE 4He; calculated meson exchange current contribution to the strangeness radius ρ(s); deduced ρ(s) extraction (from 4He(e, e) parity violating asymmetry) implications.
doi: 10.1016/0370-2693(93)90125-2
1992DO05 Nucl.Phys. A541, 525 (1992) T.W.Donnelly, M.J.Musolf, W.M.Alberico, M.B.Barbaro, A.De Pace, A.Molinari Parity-Violating Quasielastic Electron Scattering NUCLEAR REACTIONS 12C(e, e'X), E not given; calculated response functions, asymmetry. Parity-violating quasielastic electron scattering, relativistic Fermi gas model.
doi: 10.1016/0375-9474(92)90220-E
1992MU14 Nucl.Phys. A546, 509 (1992) The Interpretation of Parity-Violating Electron-Scattering Experiments NUCLEAR REACTIONS 1H(polarized e, e), E=250-1000 MeV; calculated total asymmetry vs θ, longitudinal, axial parity violating responses contribution. Other reactions considered.
doi: 10.1016/0375-9474(92)90545-U
1989HA22 Phys.Rev.Lett. 63, 949 (1989) W.C.Haxton, E.M.Henley, M.J.Musolf Nucleon and Nuclear Anapole Moments NUCLEAR STRUCTURE 19F, 133Cs; calculated one-body, polarization, exchange-current contribution to the anapole matrix element. Shell model.
doi: 10.1103/PhysRevLett.63.949
Back to query form Note: The following list of authors and aliases matches the search parameter M.J.Ramsey-Musolf: M.J.MUSOLF, M.J.RAMSEY-MUSOLF |