NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = M.J.Savage Found 63 matches. 2023HE17 Eur.Phys.J. A 59, 231 (2023) S.M.Hengstenberg, C.E.P.Robin, M.J.Savage Multi-body entanglement and information rearrangement in nuclear many-body systems: a study of the Lipkin-Meshkov-Glick model
doi: 10.1140/epja/s10050-023-01145-x
2023IL03 Phys.Rev. C 108, 064306 (2023) M.Illa, C.E.P.Robin, M.J.Savage Quantum simulations of SO(5) many-fermion systems using qudits
doi: 10.1103/PhysRevC.108.064306
2023RO10 Phys.Rev. C 108, 024313 (2023) Quantum simulations in effective model spaces: Hamiltonian-learning variational quantum eigensolver using digital quantum computers and application to the Lipkin-Meshkov-Glick model
doi: 10.1103/PhysRevC.108.024313
2022TE06 Few-Body Systems 63, 67 (2022) I.Tews, Z.Davoudi, A.Ekstrom, J.D.Holt, K.Becker, R.Briceno, D.J.Dean, W.Detmold, C.Drischler, T.Duguet, E.Epelbaum, A.Gasparyan, J.Gegelia, J.R.Green, H.W.Griesshammer, A.D.Hanlon, M.Heinz, H.Hergert, M.Hoferichter, M.Illa, D.Kekejian, A.Kievsky, S.Konig, H.Krebs, K.D.Launey, D.Lee, P.Navratil, A.Nicholson, A.Parreno, D.R.Phillips, M.Ploszajczak, X.-L.Ren, T.R.Richardson, C.Robin, G.H.Sargsyan, M.J.Savage, M.R.Schindler, P.E.Shanahan, R.P.Springer, A.Tichai, U.van Kolck, M.L.Wagman, A.Walker-Loud, C.-J.Yang, X.Zhang Nuclear Forces for Precision Nuclear Physics: A Collection of Perspectives
doi: 10.1007/s00601-022-01749-x
2021RO10 Phys.Rev. C 103, 034325 (2021) Entanglement rearrangement in self-consistent nuclear structure calculations NUCLEAR STRUCTURE 4,6He; calculated ground-state energy, single-orbital entanglement entropy, neutron-neutron and proton-neutron mutual information (MI) of the harmonic oscillator (HO), Hartree-Fock (HF), natural (NAT) and variational natural (VNAT) bases single-neutron states. Investigated measures of entanglement, entanglement entropy, mutual information, and negativity in 4,6He in a selection of bases and a chiral interaction.
doi: 10.1103/PhysRevC.103.034325
2019JO07 Eur.Phys.J. A 55, 199 (2019) B.Joo, C.Jung, N.H.Christ, W.Detmold, R.G.Edwards, M.Savage, P.Shanahan Status and future perspectives for lattice gauge theory calculations to the exascale and beyond
doi: 10.1140/epja/i2019-12919-7
2017CA06 Prog.Part.Nucl.Phys. 94, 68 (2017) J.Carlson, M.P.Carpenter, R.Casten, C.Elster, P.Fallon, A.Gade, C.Gross, G.Hagen, A.C.Hayes, D.W.Higinbotham, C.R.Howell, C.J.Horowitz, K.L.Jones, F.G.Kondev, S.Lapi, A.Macchiavelli, E.A.McCutchan, J.Natowitz, W.Nazarewicz, T.Papenbrock, S.Reddy, M.J.Savage, G.Savard, B.M.Sherrill, L.G.Sobotka, M.A.Stoyer, M.B.Tsang, K.Vetter, I.Wiedenhoever, A.H.Wuosmaa, S.Yennello White paper on nuclear astrophysics and low-energy nuclear physics, Part 2: Low-energy nuclear physics
doi: 10.1016/j.ppnp.2016.11.002
2017SA42 Phys.Rev.Lett. 119, 062002 (2017) M.J.Savage, P.E.Shanahan, B.C.Tiburzi, M.L.Wagman, F.Winter, S.R.Beane, E.Chang, Z.Davoudi, W.Detmold, K.Orginos, for the NPLQCD Collaboration Proton-Proton Fusion and Tritium β Decay from Lattice Quantum Chromodynamics NUCLEAR REACTIONS 1H(p, X)2H, E not given; calculated fusion σ using the lattice quantum chromodynamics. RADIOACTIVITY 3H(β-); calculated Gamow-Teller nuclear matrix elements using the lattice quantum chromodynamics.
doi: 10.1103/PhysRevLett.119.062002
2017SH23 Phys.Rev.Lett. 119, 062003 (2017) P.E.Shanahan, B.C.Tiburzi, M.L.Wagman, F.Winter, E.Chang, Z.Davoudi, W.Detmold, K.Orginos, M.J.Savage, for the NPLQCD Collaboration Isotensor Axial Polarizability and Lattice QCD Input for Nuclear Double-β Decay Phenomenology
doi: 10.1103/PhysRevLett.119.062003
2017TI08 Phys.Rev. D 96, 054505 (2017) B.C.Tiburzi, M.L.Wagman, F.Winter, E.Chang, Z.Davoudi, W.Detmold, K.Orginos, M.J.Savage, P.E.Shanahan, for the NPLQCD Collaboration Double-β decay matrix elements from lattice quantum chromodynamics
doi: 10.1103/PhysRevD.96.054505
2016DE04 Phys.Rev.Lett. 116, 112301 (2016) W.Detmold, K.Orginos, A.Parreno, M.J.Savage, B.C.Tiburzi, S.R.Beane, E.Chang, for the NPLQCD Collaboration Unitary Limit of Two-Nucleon Interactions in Strong Magnetic Fields
doi: 10.1103/PhysRevLett.116.112301
2014BE38 Eur.Phys.J. A 50, 148 (2014) S.R.Beane, Z.Davoudi, M.J.Savage Constraints on the universe as a numerical simulation
doi: 10.1140/epja/i2014-14148-0
2013BE28 Phys.Rev. C 88, 024003 (2013) S.R.Beane, E.Chang, S.D.Cohen, W.Detmold, P.Junnarkar, H.W.Lin, T.C.Luu, K.Orginos, A.Parreno, M.J.Savage, A.Walker-Loud, for the NPLQCD Collaboration Nucleon-nucleon scattering parameters in the limit of SU(3) flavor symmetry
doi: 10.1103/PhysRevC.88.024003
2010LU10 Phys.Rev. C 82, 034003 (2010) T.Luu, M.J.Savage, A.Schwenk, J.P.Vary Nucleon-nucleon scattering in a harmonic potential
doi: 10.1103/PhysRevC.82.034003
2007BE10 Nucl.Phys. B768, 38 (2007) S.R.Beane, K.Orginos, M.J.Savage, and the NPLQCD Collaboration Strong-isospin violation in the neutron-proton mass difference from fully-dynamical lattice QCD and PQQCD NUCLEAR STRUCTURE 1n, 1H; calculated neutron-proton mass difference, strong-isospin violating component.
doi: 10.1016/j.nuclphysb.2006.12.023
2007BE52 Nucl.Phys. A794, 62 (2007) S.R.Beane, P.F.Bedaque, T.C.Luu, K.Orginos, E.Pallante, A.Parreno, M.J.Savage, and the NPLQCD Collaboration Hyperon-nucleon scattering from fully-dynamical lattice QCD
doi: 10.1016/j.nuclphysa.2007.07.006
2006BE25 Phys.Rev.Lett. 97, 012001 (2006) S.R.Beane, P.F.Bedaque, K.Orginos, M.J.Savage Nucleon-Nucleon Scattering from Fully Dynamical Lattice QCD
doi: 10.1103/PhysRevLett.97.012001
2005BE02 Nucl.Phys. A747, 55 (2005) S.R.Beane, P.F.Bedaque, A.Parreno, M.J.Savage A framework for exploring the interactions and decays of hyperons with lattice QCD
doi: 10.1016/j.nuclphysa.2004.09.081
2005BE58 Nucl.Phys. A761, 259 (2005) DVCS-dissociation of the deuteron and the EMC effect NUCLEAR REACTIONS 2H(γ, n), E not given; calculated amplitudes for deeply-virtual Compton scattering. Pionless effective field theory, EMC effect.
doi: 10.1016/j.nuclphysa.2005.07.018
2004BE07 Phys.Lett. B 585, 106 (2004) S.R.Beane, P.F.Bedaque, A.Parreno, M.J.Savage Two nucleons on a lattice
doi: 10.1016/j.physletb.2004.02.007
2004CH14 Nucl.Phys. A735, 441 (2004) Soft pion emission in DVCS
doi: 10.1016/j.nuclphysa.2004.02.005
2004DE42 Phys.Lett. B 599, 32 (2004) Nucleon properties at finite volume: the ε'-regime
doi: 10.1016/j.physletb.2004.08.029
2004DE44 Nucl.Phys. A743, 170 (2004) Electroweak matrix elements in the two-nucleon sector from lattice QCD
doi: 10.1016/j.nuclphysa.2004.07.007
2003AR17 Nucl.Phys. A726, 339 (2003) D.Arndt, S.R.Beane, M.J.Savage The ΛQΛQ potential
doi: 10.1016/j.nuclphysa.2003.07.007
2003BE01 Nucl.Phys. A713, 148 (2003) Variation of fundamental couplings and nuclear forces NUCLEAR STRUCTURE 2n, 2H; calculated binding energies, dependence on quark mass.
doi: 10.1016/S0375-9474(02)01268-X
2003BE15 Nucl.Phys. A717, 91 (2003) The quark-mass dependence of two-nucleon systems NUCLEAR STRUCTURE A=2; calculated scattering lengths vs pion mass.
doi: 10.1016/S0375-9474(02)01586-5
2003BE16 Nucl.Phys. A717, 104 (2003) Pions in the pionless effective field theory
doi: 10.1016/S0375-9474(03)00594-3
2003BE19 Phys.Rev. D 67, 054502 (2003) Partially quenched nucleon-nucleon scattering
doi: 10.1103/PhysRevD.67.054502
2003BE63 Phys.Rev. C 68, 065802 (2003) P.F.Bedaque, G.Rupak, M.J.Savage Goldstone bosons in the 3P2 superfluid phase of neutron matter and neutrino emission
doi: 10.1103/PhysRevC.68.065802
2003BE64 Phys.Rev. D 68, 114502 (2003) Nucleon properties at finite lattice spacing in chiral perturbation theory NUCLEAR STRUCTURE 1n, 1H; calculated masses, μ, matrix elements. Chiral perturbation theory, finite lattice spacing.
doi: 10.1103/PhysRevD.68.114502
2003SA42 Nucl.Phys. A721, 94c (2003) Effective Field Theory for Nuclear Physics
doi: 10.1016/S0375-9474(03)01021-2
2002AR01 Nucl.Phys. A697, 429 (2002) Chiral Corrections to Matrix Elements of Twist-2 Operators
doi: 10.1016/S0375-9474(01)01223-4
2002BE22 Nucl.Phys. A700, 377 (2002) S.R.Beane, P.F.Bedaque, M.J.Savage, U.van Kolck Towards a Perturbative Theory of Nuclear Forces
doi: 10.1016/S0375-9474(01)01324-0
2002BE34 Phys.Lett. 535B, 177 (2002) Nucleon-Nucleon Interactions on the Lattice
doi: 10.1016/S0370-2693(02)01762-8
2002BE68 Nucl.Phys. A709, 319 (2002) Nucleons in Two-Flavor Partially-Quenched Chiral Perturbation Theory NUCLEAR STRUCTURE 1n, 1H; calculated mass, μ, axial vector currents. Partially-quenched chiral perturbation theory.
doi: 10.1016/S0375-9474(02)01086-2
2002CH42 Nucl.Phys. A707, 452 (2002) Matrix Elements of Twist-2 Operators in Quenched Chiral Perturbation Theory
doi: 10.1016/S0375-9474(02)00994-6
2002SA15 Nucl.Phys. A700, 359 (2002) The Magnetic Moments of the Octet Baryons in Quenched Chiral Perturbation Theory
doi: 10.1016/S0375-9474(01)01315-X
2001BE25 Nucl.Phys. A688, 931 (2001) S.R.Beane, P.F.Bedaque, M.J.Savage Renormalization Group Improved Gap Equation for Color Superconductors
doi: 10.1016/S0375-9474(00)00595-9
2001BE62 Nucl.Phys. A694, 511 (2001) Rearranging Pionless Effective Field Theory NUCLEAR REACTIONS 1H(n, γ), E not given; calculated σ. 2H(γ, γ), E=49 MeV; calculated σ(θ). Pionless effective field theory, operator redundancy, dibaryon fields. NUCLEAR STRUCTURE 2H; calculated electric form factor. Pionless effective field theory, operator redundancy, dibaryon fields.
doi: 10.1016/S0375-9474(01)01088-0
2001SA10 Nucl.Phys. A686, 413 (2001) The Anapole Form Factor of the Deuteron NUCLEAR STRUCTURE 2H; calculated anapole form factor at leading order in effective field theory expansion.
doi: 10.1016/S0375-9474(00)00568-6
2001SA65 Nucl.Phys. A695, 365 (2001) Parity Violation in Low-Energy np → dγ and the Deuteron Anapole Moment NUCLEAR REACTIONS 1H(polarized n, γ), E=low; calculated asymmetry, relation to deuteron anapole moment.
doi: 10.1016/S0375-9474(01)01105-8
2000BE33 Phys.Rev. C62, 018501 (2000) Parity Violation in γp(pol) Compton Scattering NUCLEAR REACTIONS 1H(γ, γ'), E=100 MeV; calculated asymmetry, parity violating amplitude. Polarized target. Chiral perturbation theory.
doi: 10.1103/PhysRevC.62.018501
2000PH01 Phys.Lett. 473B, 209 (2000) D.R.Phillips, G.Rupak, M.J.Savage Improving the Convergence of NN Effective Field Theory NUCLEAR STRUCTURE 2H; calculated radius, quadrupole moment. Low-energy effective field theory.
doi: 10.1016/S0370-2693(99)01496-3
1999CH21 Nucl.Phys. A653, 386 (1999) J.-W.Chen, G.Rupak, M.J.Savage Nucleon-Nucleon Effective Field Theory without Pions NUCLEAR REACTIONS 1H(n, γ), E=low; calculated σ, effective range parameters. Effective field theory without pions. NUCLEAR STRUCTURE 2H; calculated form factors. Effective field theory without pions.
doi: 10.1016/S0375-9474(99)00298-5
1999CH31 Phys.Lett. 464B, 1 (1999) Isoscalar M1 and E2 Amplitudes in np → dγ NUCLEAR REACTIONS 1H(n, γ), E=low; calculated isoscaler M1 and E2 amplitudes. NUCLEAR STRUCTURE 2H; calculated quadrupole form factor.
doi: 10.1016/S0370-2693(99)01007-2
1999CH38 Phys.Rev. C60, 065205 (1999) np → dγ for Big-Bang Nucleosynthesis NUCLEAR REACTIONS 1H(n, γ), E(cm) < 1 MeV; 2H(γ, n), E=2.6-9.0 MeV; calculated σ. Pionless nucleon-nucleon effective field theory.
doi: 10.1103/PhysRevC.60.065205
1999KA01 Phys.Rev. C59, 617 (1999) D.B.Kaplan, M.J.Savage, M.B.Wise Perturbative Calculation of the Electromagnetic Form Factors of the Deuteron NUCLEAR REACTIONS 2H(e, e), E not given; calculated σ(q2), form factors. NUCLEAR STRUCTURE 2H; calculated charge radius, electromagnetic moments.
doi: 10.1103/PhysRevC.59.617
1999KA11 Phys.Lett. 449B, 1 (1999) D.B.Kaplan, M.J.Savage, R.P.Springer, M.B.Wise An Effective Theory Calculation of the Parity Violating Asymmetry in n(pol) + p → d + γ NUCLEAR REACTIONS 1H(polarized n, γ), E not given; calculated parity violating asymmetry.
doi: 10.1016/S0370-2693(99)00032-5
1999SA12 Phys.Rev. C59, 2293 (1999) Pionic Matrix Elements in Neutrinoless Double-β Decay
doi: 10.1103/PhysRevC.59.2293
1999SA23 Nucl.Phys. A652, 273 (1999) M.J.Savage, K.A.Scaldeferri, M.B.Wise n + p → d + γ in Effective Field Theory NUCLEAR REACTIONS 1H(n, γ), E=low; calculated σ; deduced contributions. Effective field theory.
doi: 10.1016/S0375-9474(99)00146-3
1998CH46 Nucl.Phys. A644, 221 (1998) J.-W.Chen, H.W.Griesshammer, M.J.Savage, R.P.Springer The Polarizability of the Deuteron NUCLEAR STRUCTURE 2H; calculated scalar, tensor polarizabilities. Effective field theory calculations.
doi: 10.1016/S0375-9474(98)00580-6
1998CH47 Nucl.Phys. A644, 245 (1998) J.-W.Chen, H.W.Griesshammer, M.J.Savage, R.P.Springer γ-Deuteron Compton Scattering in Effective Field Theory NUCLEAR REACTIONS 2H(γ, γ'), E=49, 69 MeV; calculated Compton scattering σ(θ). Effective field theory expansion.
doi: 10.1016/S0375-9474(98)00591-0
1998KA25 Phys.Lett. 424B, 390 (1998) D.B.Kaplan, M.J.Savage, M.B.Wise A New Expansion for Nucleon-Nucleon Interactions
doi: 10.1016/S0370-2693(98)00210-X
1998KA62 Nucl.Phys. B534, 329 (1998) D.B.Kaplan, M.J.Savage, M.B.Wise Two-Nucleon Systems from Effective Field Theory
doi: 10.1016/S0550-3213(98)00440-4
1998SA05 Phys.Rev. C57, 1478 (1998) Weak ΛΛK0 Interaction
doi: 10.1103/PhysRevC.57.1478
1998SA43 Nucl.Phys. A639, 325c (1998) NNK and ΛΛK Amplitudes in Chiral Perturbation Theory
doi: 10.1016/S0375-9474(98)00290-5
1998SA59 Nucl.Phys. A644, 235 (1998); Erratum Nucl.Phys. 657, 457 (1999) Parity Violation in Effective Field Theory and the Deuteron Anapole Moment NUCLEAR STRUCTURE 2H; calculated anapole moment. Effective field theory, hadronic parity violation.
doi: 10.1016/S0375-9474(98)00592-2
1997SA19 Phys.Rev. C55, 2185 (1997) ΔΔ Intermediate state in 1S0 NN Scattering from Effective Field Theory
doi: 10.1103/PhysRevC.55.2185
1996KA04 Phys.Lett. 365B, 244 (1996) The Spin-Flavor Dependence of Nuclear Forces from Large-N QCD NUCLEAR STRUCTURE 18F, 18Ne, 18O; analyzed level data. 18F, 18Ne; analyzed β+-decay; deduced SU(4) symmetry related features. Chiral perturbation theory, large-N limit QCD.
doi: 10.1016/0370-2693(95)01277-X
1996KA56 Nucl.Phys. B478, 629 (1996) D.B.Kaplan, M.J.Savage, M.B.Wise Nucleon-Nucleon Scattering from Effective Field Theory
doi: 10.1016/S0550-3213(96)00357-4
1996SA02 Phys.Rev. C53, 441 (1996); Erratum Phys.Rev. C54, 2786 (1996) Kaon-Nucleon Couplings for Weak Decays of Hypernuclei
doi: 10.1103/PhysRevC.53.441
1988WI12 Nucl.Instrum.Methods Phys.Res. A267, 242 (1988) M.Wiescher, J.Gorres, K.L.Kratz, B.Leist, K.H.Chang, B.W.Filippone, L.W.Mitchell, M.J.Savage, R.B.Vogelaar The Fabrication and Properties of a 22Na Target NUCLEAR REACTIONS 23Na(p, γ), E ≈ 310-340 keV; 19F(p, α), E ≈ 600-900 keV; measured thick target yield. 30Si(p, γ), E=620 keV; measured Eγ, Iγ. 24Mg(d, α), E not given; measured Eγ, Iγ; deduced 22Na target feasibility.
doi: 10.1016/0168-9002(88)90471-8
1985LE17 Nucl.Phys. A443, 210 (1985) P.M.Lewis, A.R.Poletti, M.J.Savage, C.L.Woods The Mean Life of the Second 0+ State in 42Ca NUCLEAR REACTIONS 42Ca(p, p'γ), E=5 MeV; measured pγ-coin. 42Ca level deduced T1/2, B(E2). Enriched target, direct electronic timing.
doi: 10.1016/0375-9474(85)90260-X
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