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NSR database version of April 11, 2024.

Search: Author = M.J.Savage

Found 63 matches.

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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2023RO10      Phys.Rev. C 108, 024313 (2023)

C.E.P.Robin, M.J.Savage

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
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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
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2021RO10      Phys.Rev. C 103, 034325 (2021)

C.Robin, M.J.Savage, N.Pillet

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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2005BE58      Nucl.Phys. A761, 259 (2005)

S.R.Beane, M.J.Savage

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
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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
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2004CH14      Nucl.Phys. A735, 441 (2004)

J.-W.Chen, M.J.Savage

Soft pion emission in DVCS

doi: 10.1016/j.nuclphysa.2004.02.005
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2004DE42      Phys.Lett. B 599, 32 (2004)

W.Detmold, M.J.Savage

Nucleon properties at finite volume: the ε'-regime

doi: 10.1016/j.physletb.2004.08.029
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2004DE44      Nucl.Phys. A743, 170 (2004)

W.Detmold, M.J.Savage

Electroweak matrix elements in the two-nucleon sector from lattice QCD

doi: 10.1016/j.nuclphysa.2004.07.007
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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
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2003BE01      Nucl.Phys. A713, 148 (2003)

S.R.Beane, M.J.Savage

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
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2003BE15      Nucl.Phys. A717, 91 (2003)

S.R.Beane, M.J.Savage

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
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2003BE16      Nucl.Phys. A717, 104 (2003)

S.R.Beane, M.J.Savage

Pions in the pionless effective field theory

doi: 10.1016/S0375-9474(03)00594-3
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2003BE19      Phys.Rev. D 67, 054502 (2003)

S.R.Beane, M.J.Savage

Partially quenched nucleon-nucleon scattering

doi: 10.1103/PhysRevD.67.054502
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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
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2003BE64      Phys.Rev. D 68, 114502 (2003)

S.R.Beane, M.J.Savage

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
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2003SA42      Nucl.Phys. A721, 94c (2003)


Effective Field Theory for Nuclear Physics

doi: 10.1016/S0375-9474(03)01021-2
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2002AR01      Nucl.Phys. A697, 429 (2002)

D.Arndt, M.J.Savage

Chiral Corrections to Matrix Elements of Twist-2 Operators

doi: 10.1016/S0375-9474(01)01223-4
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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
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2002BE34      Phys.Lett. 535B, 177 (2002)

S.R.Beane, M.J.Savage

Nucleon-Nucleon Interactions on the Lattice

doi: 10.1016/S0370-2693(02)01762-8
Citations: PlumX Metrics

2002BE68      Nucl.Phys. A709, 319 (2002)

S.R.Beane, M.J.Savage

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
Citations: PlumX Metrics

2002CH42      Nucl.Phys. A707, 452 (2002)

J.-W.Chen, M.J.Savage

Matrix Elements of Twist-2 Operators in Quenched Chiral Perturbation Theory

doi: 10.1016/S0375-9474(02)00994-6
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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
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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
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2001BE62      Nucl.Phys. A694, 511 (2001)

S.R.Beane, M.J.Savage

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
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2001SA10      Nucl.Phys. A686, 413 (2001)

M.J.Savage, R.P.Springer

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
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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
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2000BE33      Phys.Rev. C62, 018501 (2000)

P.F.Bedaque, M.J.Savage

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
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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
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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
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1999CH31      Phys.Lett. 464B, 1 (1999)

J.W.Chen, G.Rupak, M.J.Savage

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
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1999CH38      Phys.Rev. C60, 065205 (1999)

J.-W.Chen, M.J.Savage

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
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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
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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
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1999SA12      Phys.Rev. C59, 2293 (1999)


Pionic Matrix Elements in Neutrinoless Double-β Decay

doi: 10.1103/PhysRevC.59.2293
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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
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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
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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
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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
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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
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1998SA05      Phys.Rev. C57, 1478 (1998)

M.J.Savage, R.P.Springer

Weak ΛΛK0 Interaction

doi: 10.1103/PhysRevC.57.1478
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1998SA43      Nucl.Phys. A639, 325c (1998)

M.J.Savage, R.P.Springer

NNK and ΛΛK Amplitudes in Chiral Perturbation Theory

doi: 10.1016/S0375-9474(98)00290-5
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1998SA59      Nucl.Phys. A644, 235 (1998); Erratum Nucl.Phys. 657, 457 (1999)

M.J.Savage, R.P.Springer

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
Citations: PlumX Metrics

1997SA19      Phys.Rev. C55, 2185 (1997)


ΔΔ Intermediate state in 1S0 NN Scattering from Effective Field Theory

doi: 10.1103/PhysRevC.55.2185
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1996KA04      Phys.Lett. 365B, 244 (1996)

D.B.Kaplan, M.J.Savage

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
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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
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1996SA02      Phys.Rev. C53, 441 (1996); Erratum Phys.Rev. C54, 2786 (1996)

M.J.Savage, R.P.Springer

Kaon-Nucleon Couplings for Weak Decays of Hypernuclei

doi: 10.1103/PhysRevC.53.441
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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
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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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Note: The following list of authors and aliases matches the search parameter M.J.Savage: , M.J.SAVAGE