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NSR database version of May 3, 2024.

Search: Author = S.R.Beane

Found 35 matches.

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2022BE18      Nucl.Phys. A1024, 122478 (2022)

S.R.Beane, R.C.Farrell

UV/IR symmetries of the S-matrix and RG flow

doi: 10.1016/j.nuclphysa.2022.122478
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2009BE25      Phys.Rev. C 80, 011001 (2009)

S.R.Beane, D.B.Kaplan, A.Vuorinen

Perturbative nuclear physics

doi: 10.1103/PhysRevC.80.011001
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2005BE08      Nucl.Phys. A747, 311 (2005)

S.R.Beane, M.Malheiro, J.A.McGovern, D.R.Phillips, U.van Kolck

Compton scattering on the proton, neutron, and deuteron in chiral perturbation theory to O(Q4)

NUCLEAR REACTIONS 1n, 1,2H(γ, γ'), E ≈ 40-200 MeV; calculated σ(θ). Chiral perturbation theory, comparison with data.

doi: 10.1016/j.nuclphysa.2004.09.068
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2004BE24      Nucl.Phys. A737, 16 (2004)

S.R.Beane

Nuclear Physics from QCD

doi: 10.1016/j.nuclphysa.2004.03.045
Citations: PlumX Metrics

2004BE38      Phys.Rev. D 70, 034507 (2004)

S.R.Beane

Nucleon masses and magnetic moments in a finite volume

NUCLEAR STRUCTURE 1n, 1H; calculated finite-size corrections to mass, μ.

doi: 10.1103/PhysRevD.70.034507
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2003BE19      Phys.Rev. D 67, 054502 (2003)

S.R.Beane, M.J.Savage

Partially quenched nucleon-nucleon scattering

doi: 10.1103/PhysRevD.67.054502
Citations: PlumX Metrics

2003BE35      Nucl.Phys. A720, 399 (2003)

S.R.Beane, V.Bernard, E.Epelbaum, Ulf-G.Meissner, D.R.Phillips

The S-wave pion-nucleon scattering lengths from pionic atoms using effective field theory

ATOMIC PHYSICS, Mesic-atoms 1,2H(π-, X), E at rest; analyzed pionic atoms decay data; deduced pion-nucleon scattering lengths.

doi: 10.1016/S0375-9474(03)01008-X
Citations: PlumX Metrics

2003BE40      Phys.Lett. B 567, 200 (2003); Erratum Phy.Lett. B 607, 320 (2005)

S.R.Beane, M.Malheiro, J.A.McGovern, D.R.Phillips, U.van Kolck

Nucleon polarizabilities from low-energy Compton scattering

NUCLEAR REACTIONS 1,2H(γ, γ), E ≈ 40-200 MeV; analyzed σ(θ). 1n, 1H deduced polarizabilities.

doi: 10.1016/j.physletb.2003.06.040
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1999BE42      Nucl.Phys. A656, 367 (1999)

S.R.Beane, M.Malheiro, D.R.Phillips, U.van Kolck

Compton Scattering on the Deuteron in Baryon Chiral Perturbation Theory

NUCLEAR REACTIONS 2H(γ, γ'), E=49, 69, 95 MeV; calculated Compton scattering σ(θ). Baryon chiral perturbation theory, comparisons with data.

doi: 10.1016/S0375-9474(99)00312-7
Citations: PlumX Metrics

1998BE02      Phys.Rev. C57, 424 (1998)

S.R.Beane, V.Bernard, T.-S.H.Lee, U.-G.Meissner

Isoscalar S-Wave π-N Scattering Length a+ from π-Deuteron Scattering

NUCLEAR REACTIONS 2H(π, X), E not given; calculated scattering length; deduced πN scattering length related features.

doi: 10.1103/PhysRevC.57.424
Citations: PlumX Metrics

1998BE17      Nucl.Phys. A632, 445 (1998)

S.R.Beane, T.D.Cohen, D.R.Phillips

The Potential of Effective Field Theory in NN Scattering

doi: 10.1016/S0375-9474(98)00007-4
Citations: PlumX Metrics

1998BE83      Acta Phys.Pol. B29, 3161 (1998)

S.R.Beane

Status of Effective Field Theory of NN Scattering

1998PH01      Nucl.Phys. A631, 447c (1998)

D.R.Phillips, S.R.Beane, T.D.Cohen

Regularization and Renormalization in Effective Theories of the Nucleon-Nucleon Interaction

doi: 10.1016/S0375-9474(98)00045-1
Citations: PlumX Metrics

1997BE19      Nucl.Phys. A618, 381 (1997)

S.R.Beane, V.Bernard, T.-S.H.Lee, Ulf.-G.Meissner, U.van Kolck

Neutral Pion Photoproduction on Deuterium in Baryon Chiral Perturbation Theory to Order q4

NUCLEAR REACTIONS 2H(γ, X), E ≈ threshold; calculated π0 production σ related features; deduced sensitivity to γn → π0n amplitude. Baryon chiral perturbation theory to order q4.

doi: 10.1016/S0375-9474(97)00133-4
Citations: PlumX Metrics

1995BE53      Phys.Rev. C52, 2914 (1995)

S.R.Beane, C.Y.Lee, U.van Kolck

Neutral Pion Photoproduction on Nuclei in Baryon Chiral Perturbation Theory

doi: 10.1103/PhysRevC.52.2914
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