NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = G.A.Miller Found 188 matches. Showing 1 to 100. [Next]2023MI14 Phys.Rev. C 108, L031002 (2023) Entanglement maximization in low-energy neutron-proton scattering
doi: 10.1103/PhysRevC.108.L031002
2023MI16 Phys.Rev. C 108, L041601 (2023) Entanglement of elastic and inelastic scattering
doi: 10.1103/PhysRevC.108.L041601
2022CO14 Phys.Rev. C 106, L062501 (2022) Nucleon-nucleon short-ranged correlations, β-decay, and the unitarity of the CKM matrix RADIOACTIVITY 46V(β+); calculated isospin-breaking correction. Investigate the influence of nucleon-nucleon short-ranged correlations on isospin corrections.
doi: 10.1103/PhysRevC.106.L062501
2022CR05 Phys.Rev. C 106, 065502 (2022) Charge-symmetry-breaking effects on neutron β decay in nonrelativistic quark models RADIOACTIVITY 1NN(β-); calculated matrix element, changes to matrix element caused by charge-symmetry-breaking (CSB) effects. Nonrelativistic quark model. Pointed that inclusion of CSB effect reduces matrix element by factor 4.
doi: 10.1103/PhysRevC.106.065502
2022KI22 Phys.Rev. C 106, 055202 (2022) Light-front holography model of the EMC effect NUCLEAR STRUCTURE 2,3H, 3,4He, 9Be, 12C, 27Al, 56Fe, 63Cu, 197Au, 208Pb; calculated EMC effects in comparison to experimental data, effective charges of a proton and neutron with positive and negative chiralities. Two-component model of the EMC (named after the European Muon Collaboration) effect based on light-front holographic QCD (LFHQCD). Comparison to experimental data.
doi: 10.1103/PhysRevC.106.055202
2021CA18 Phys.Rev. C 104, L012201 (2021) Color transparency and the proton form factor: Evidence for the Feynman mechanism
doi: 10.1103/PhysRevC.104.L012201
2021SE13 Phys. Rev. Res. 3, 023240 (2021) E.P.Segarra, J.R.Pybus, F.Hauenstein, D.W.Higinbotham, G.A.Miller, E.Piasetzky, A.Schmidt, M.Strikman, L.B.Weinstein, O.Hen Short-range correlations and the nuclear EMC effect in deuterium and helium-3 NUCLEAR STRUCTURE 2H, 3He; calculated modification of the partonic structure of nucleons bound in atomic nuclei also known as the EMC effect using a convolution formalism that allows isolating the impact of high-momentum nucleons in short-ranged correlated (SRC) pairs.
doi: 10.1103/PhysRevResearch.3.023240
2021ZH03 Phys.Lett. B 813, 136061 (2021) Can a protophobic vector boson explain the ATOMKI anomaly? NUCLEAR REACTIONS 7Li(p, X)8Be, E<1.5 MeV; analyzed available data; deduced an isospin relation between photon and χ couplings to nucleons, relations between protophobic χ-production σ and those for measured photon production.
doi: 10.1016/j.physletb.2020.136061
2020DU04 Phys.Rev. C 101, 035202 (2020) W.Du, Y.Li, X.Zhao, G.A.Miller, J.P.Vary Basis light-front quantization for a chiral nucleon-pion Lagrangian
doi: 10.1103/PhysRevC.101.035202
2020MI11 Phys.Rev. C 102, 022201 (2020) Frame-independent spatial coordinate Zε: Implications for light-front wave functions, deep inelastic scattering, light-front holography, and lattice QCD calculations
doi: 10.1103/PhysRevC.102.022201
2020MI17 Phys.Rev. C 102, 055206 (2020) Discovery versus precision in nuclear physics: A tale of three scales
doi: 10.1103/PhysRevC.102.055206
2019AL25 Phys.Rev. C 100, 035205 (2019) Chiral light-front perturbation theory and the flavor dependence of the light-quark nucleon sea
doi: 10.1103/PhysRevC.100.035205
2019MI04 Phys.Rev. C 99, 035202 (2019) Defining the proton radius: A unified treatment NUCLEAR STRUCTURE 1H; analyzed hydrogen spectroscopy, lepton-proton scattering measurements, and diverse modern parton distributions to understand the meaning of proton radius; defined proton radius and its charge radius from calculations based on perturbation theory, light-front dynamics, and a new relativistic moment expansion (RME) method. Relevance to upcoming PRAD experiment, and Muon-Scattering Experiment (MUSE).
doi: 10.1103/PhysRevC.99.035202
2019MI19 Phys.Rev. C 100, 044608 (2019) Coherent-nuclear pion photoproduction and neutron radii NUCLEAR REACTIONS 208Pb(γ, π0), E=180-190 MeV; calculated σ(E) by including the effects of final-state pion-nucleus charge-exchange reactions on the cross sections; analyzed experimental data in 2014Ta14, and deduced a revised value or the neutron skin.
doi: 10.1103/PhysRevC.100.044608
2018MI05 Nucl.Phys. A975, 73 (2018) Luneburg-lens-like structural Pauli attractive core of the nuclear force at short distances
doi: 10.1016/j.nuclphysa.2018.04.007
2017HO08 Phys.Rev. C 95, 035205 (2017) T.J.Hobbs, M.Alberg, G.A.Miller Euclidean bridge to the relativistic constituent quark model
doi: 10.1103/PhysRevC.95.035205
2017ME14 Phys.Rev. C 96, 065207 (2017); Phys.Rev. C 99, 039901 (2019) N.A.Mecholsky, J.Meija-Ott, M.Carmignotto, T.Horn, G.A.Miller, I.L.Pegg Kaon transverse charge density from space- and timelike data
doi: 10.1103/PhysRevC.96.065207
2016HO07 Phys.Rev. C 93, 052801 (2016) T.J.Hobbs, M.Alberg, G.A.Miller Role of nucleon strangeness in supernova explosions
doi: 10.1103/PhysRevC.93.052801
2016HO10 Phys.Rev. C 93, 064603 (2016) J.W.Holt, N.Kaiser, G.A.Miller Microscopic optical potential for exotic isotopes from chiral effective field theory
doi: 10.1103/PhysRevC.93.064603
2016MI10 Phys.Rev. C 93, 045202 (2016) G.A.Miller, M.D.Sievert, R.Venugopalan Probing short-range nucleon-nucleon interactions with an electron-ion collider
doi: 10.1103/PhysRevC.93.045202
2016TE07 Phys.Rev. C 94, 014002 (2016) Meaning of the nuclear wave function NUCLEAR STRUCTURE 2H; calculated four different versions of deuteron wave functions (light-front-spectator, light-front, light-front with scaling, and nonrelativistic), cross sections. Exactly calculable, covariant models of a bound-state wave-state wave function. Relevance to structure of the deuteron in experiments using deuteron target.
doi: 10.1103/PhysRevC.94.014002
2015HE29 Phys.Rev. C 92, 045205 (2015) O.Hen, L.B.Weinstein, E.Piasetzky, G.A.Miller, M.M.Sargsian, Y.Sagi Correlated fermions in nuclei and ultracold atomic gases NUCLEAR REACTIONS 2H(e, e'p), Q2=1.5-3.0 (GeV/c)2; calculated high-momentum tail of the deuteron momentum distribution; deduced short-range correlated different-fermion np pairs, momentum distribution of nucleons in nuclei dominated by spin-triplet pn pairs. Comparison with experimental data. 12C, 56Fe, 197Au(e, e'), Q2>1.5 (GeV/c)2; deduced scaling coefficient from inclusive cross sections. 6Li, 40K; analyzed scattering length and Fermi momentum from measurements of ultracold two-spin-state atomic systems at finite temperature.
doi: 10.1103/PhysRevC.92.045205
2015HO03 Phys.Rev. C 91, 035205 (2015) T.J.Hobbs, M.Alberg, G.A.Miller Constraining nucleon strangeness
doi: 10.1103/PhysRevC.91.035205
2015LI37 Phys.Rev. C 92, 035209 (2015) Polarized lepton-nucleon elastic scattering and a search for a light scalar boson
doi: 10.1103/PhysRevC.92.035209
2015MI11 Phys.Rev. C 91, 055204 (2015) Nonperturbative lepton-sea fermions in the nucleon and the proton radius puzzle
doi: 10.1103/PhysRevC.91.055204
2015MI12 Phys.Rev. C 91, 055503 (2015) Charge symmetry breaking in electromagnetic nucleon form factors in elastic parity-violating electron-nucleus scattering
doi: 10.1103/PhysRevC.91.055503
2014BU10 Phys.Rev. C 90, 024606 (2014) Corrections to the eikonal approximation for nuclear scattering at medium energies NUCLEAR REACTIONS 40Ca(p, p), E=10-100 MeV; calculated total σ(E), and σ(θ) for 40 MeV. Calculated total σ and corrections to the eikonal approximation for scattering of 40 MeV/nucleon 11Be halo nucleus from targets with A=8-220, and comparison with available experimental data. Coulomb breakup of 11Be. Relevance to analysis and accurate modeling of low energy nucleus-nucleus scattering data produced at FRIB.
doi: 10.1103/PhysRevC.90.024606
2014CA26 Phys.Rev. C 90, 025211 (2014) M.Carmignotto, T.Horn, G.A.Miller Pion transverse charge density and the edge of hadrons
doi: 10.1103/PhysRevC.90.025211
2014MI07 Phys.Rev. C 89, 045203 (2014) Pionic and hidden-color, six-quark contributions to the deuteron b1 structure function
doi: 10.1103/PhysRevC.89.045203
2014WA24 Phys.Rev. C 89, 065206 (2014); Erratum Phys.Rev. C 91, 019903 (2015) Charge symmetry breaking and parity violating electron-proton scattering
doi: 10.1103/PhysRevC.89.065206
2013HE18 Int.J.Mod.Phys. E22, 1330017 (2013) O.Hen, D.W.Higinbotham, G.A.Miller, E.Piasetzky, L.B.Weinstein The EMC effect and high momentum nucleons in nuclei
doi: 10.1142/S0218301313300178
2013HO13 Phys.Rev. C 88, 015204 (2013) Incoherent J/ψ electroproduction from the deuteron at energies available at Jefferson Laboratory and the elastic J/ψ-nucleon scattering amplitude
doi: 10.1103/PhysRevC.88.015204
2013HO14 Phys.Rev. C 88, 024614 (2013) J.W.Holt, N.Kaiser, G.A.Miller, W.Weise Microscopic optical potential from chiral nuclear forces
doi: 10.1103/PhysRevC.88.024614
2013HO18 Phys.Rev. C 88, 035202 (2013) Color transparency in the reaction γ* A → p+p+(A-1)*
doi: 10.1103/PhysRevC.88.035202
2013WI08 Phys.Rev. C 88, 044333 (2013) R.B.Wiringa, S.Pastore, S.C.Pieper, G.A.Miller Charge-symmetry breaking forces and isospin mixing in 8Be NUCLEAR STRUCTURE 8Be; calculated levels, J, π, isospin-mixing (IM) matrix elements, isovector energy differences of mirror nuclei 8Be and 8Li; evaluated charge-symmetry breaking (CSB) components of the AV18 potential, contribution from one-photon, one-pion, one-ρ, and ρ-ω mixing. Green's function Monte Carlo (GFMC) calculations with realistic Argonne ν18 (AV18) two-nucleon and Illinois-7 three-nucleon potentials. Comparison with experimental data.
doi: 10.1103/PhysRevC.88.044333
2012CL01 Phys.Rev. C 86, 015208 (2012) Nucleon form factors and spin content in a quark-diquark model with a pion cloud
doi: 10.1103/PhysRevC.86.015208
2012DU14 Eur.Phys.J. A 48, 187 (2012) Jo.Dudek, R.Ent, R.Essig, K.S.Kumar, C.Meyer, R.D.McKeown, Z.E.Meziani, G.A.Miller, M.Pennington, D.Richards, L.Weinstein, G.Young, S.Brown Physics opportunities with the 12 GeV upgrade at Jefferson Lab
doi: 10.1140/epja/i2012-12187-1
2012MI25 Phys.Rev. C 86, 065201 (2012) G.A.Miller, A.W.Thomas, J.D.Carroll Nuclear quasielastic electron scattering limits nucleon off-mass shell properties
doi: 10.1103/PhysRevC.86.065201
2012WA18 Phys.Rev.Lett. 108, 232301 (2012) A.Walker-Loud, C.E.Carlson, G.A.Miller Electromagnetic Self-Energy Contribution to Mp-Mn and the Isovector Nucleon Magnetic Polarizability
doi: 10.1103/PhysRevLett.108.232301
2011BO18 Phys.Rev. C 83, 064003 (2011) Impulse approximation in nuclear pion production reactions: Absence of a one-body operator NUCLEAR REACTIONS 1H(n, d)π0, E not given; calculated impulse amplitude of pion production, threshold cross section. Impulse approximation with relativistic formalism. Two-body distorted-wave operator. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.064003
2011CL01 Phys.Rev. C 83, 012201 (2011) Third Zemach moment of the proton
doi: 10.1103/PhysRevC.83.012201
2011MI14 Phys.Rev. C 84, 045205 (2011) G.A.Miller, M.Strikman, C.Weiss Realizing vector meson dominance with transverse charge densities
doi: 10.1103/PhysRevC.84.045205
2011VE02 Phys.Rev. C 83, 015203 (2011) S.Venkat, J.Arrington, G.A.Miller, X.Zhan Realistic transverse images of the proton charge and magnetization densities
doi: 10.1103/PhysRevC.83.015203
2010BO03 Phys.Rev. C 81, 014001 (2010) Charge symmetry breaking in the np → dπ0 reaction NUCLEAR REACTIONS n(p, π0)d, E not given; calculated σ, angular distribution asymmetries, and analyzing powers using heavy baryon chiral perturbation theory. Comparison with experimental data.
doi: 10.1103/PhysRevC.81.014001
2010BO14 Phys.Rev. C 82, 024001 (2010) Impulse approximation in the np → dπ0 reaction reexamined
doi: 10.1103/PhysRevC.82.024001
2010MI06 Phys.Rev. C 81, 035201 (2010) Relation between equal-time and light-front wave functions
doi: 10.1103/PhysRevC.81.035201
2010MI17 Phys.Rev. C 82, 025205 (2010) Color transparency at energies available at the CERN COMPASS experiment
doi: 10.1103/PhysRevC.82.025205
2009FO06 Phys.Rev. C 80, 027001 (2009) A.C.Fonseca, R.Machleidt, G.A.Miller Nucleon-nucleon charge symmetry breaking and the dd → απ0 reaction
doi: 10.1103/PhysRevC.80.027001
2009LU06 Phys.Rev. C 79, 024902 (2009) Elliptic flow from final state interactions in the distorted-wave emission-function model
doi: 10.1103/PhysRevC.79.024902
2009MI13 Phys.Rev. C 79, 055204 (2009) Singular charge density at the center of the pion?
doi: 10.1103/PhysRevC.79.055204
2009MI19 Phys.Rev. C 80, 045210 (2009) Electromagnetic form factors and charge densities from hadrons to nuclei
doi: 10.1103/PhysRevC.80.045210
2009MI24 Phys.Rev. C 80, 064319 (2009) Isospin-symmetry-breaking corrections to superallowed Fermi β decay: Radial excitations
doi: 10.1103/PhysRevC.80.064319
2009RI07 Phys.Rev. C 80, 015201 (2009) Connecting the Breit frame to the infinite momentum light front frame: How GE turns into F1
doi: 10.1103/PhysRevC.80.015201
2009RI09 Phys.Rev. C 80, 025206 (2009) Neutron charge density from simple pion cloud models
doi: 10.1103/PhysRevC.80.025206
2008FR07 Phys.Rev. C 78, 015208 (2008) L.Frankfurt, G.A.Miller, M.Strikman Color transparency in semi-inclusive electroproduction of ρ mesons NUCLEAR REACTIONS 12C, 56Fe(e, e'); calculated color transparency.
doi: 10.1103/PhysRevC.78.015208
2008LU13 Phys.Rev. C 78, 054905 (2008) M.Luzum, J.G.Cramer, G.A.Miller Understanding the optical potential in Hanbury-Brown-Twiss interferometry
doi: 10.1103/PhysRevC.78.054905
2008MI21 Phys.Rev. C 78, 032201 (2008) Neutron negative central charge density: An inclusive-exclusive connection
doi: 10.1103/PhysRevC.78.032201
2008MI22 Phys.Rev. C 78, 035501 (2008) Isospin-symmetry-breaking corrections to superallowed Fermi β decay: Formalism and schematic models
doi: 10.1103/PhysRevC.78.035501
2007CL04 Phys.Rev.Lett. 99, 242502 (2007) B.Clasie, X.Qian, J.Arrington, R.Asaturyan, F.Benmokhtar, W.Boeglin, P.Bosted, A.Bruell, M.E.Christy, E.Chudakov, W.Cosyn, M.M.Dalton, A.Daniel, D.Day, D.Dutta, L.El Fassi, R.Ent, H.C.Fenker, J.Ferrer, N.Fomin, H.Gao, K.Garrow, D.Gaskell, C.Gray, T.Horn, G.M.Huber, M.K.Jones, N.Kalantarians, C.E.Keppel, K.Kramer, A.Larson, Y.Li, Y.Liang, A.F.Lung, S.Malace, P.Markowitz, A.Matsumura, D.G.Meekins, T.Mertens, G.A.Miller, T.Miyoshi, H.Mkrtchyan, R.Monson, T.Navasardyan, G.Niculescu, I.Niculescu, Y.Okayasu, A.K.Opper, C.Perdrisat, V.Punjabi, A.W.Rauf, V.M.Rodriquez, D.Rohe, J.Ryckebusch, J.Seely, E.Segbefia, G.R.Smith, M.Strikman, M.Sumihama, V.Tadevosyan, L.Tang, V.Tvaskis, A.Villano, W.F.Vulcan, F.R.Wesselmann, S.A.Wood, L.Yuan, X.C.Zheng Measurement of Nuclear Transparency for the A(e, e'π+) Reaction NUCLEAR REACTIONS 2H, 12C, 27Al, 63Cu, 197Au(e, e'π+), E=4.021-5.767 GeV; measured electron and pion energies. Deduced nuclear transparency.
doi: 10.1103/PhysRevLett.99.242502
2007KV03 Phys.Rev. C 76, 025203 (2007) Subtleties of Lorentz invariance and shapes of the nucleon
doi: 10.1103/PhysRevC.76.025203
2007LA17 Phys.Rev. C 75, 055204 (2007) Initial-state Coulomb interaction in the dd → απ0 reaction NUCLEAR REACTIONS 2H(d, π0), E=228.5, 231.8 MeV; calculated momenta, and cross sections by including the effects of initial state Coulomb interactions.
doi: 10.1103/PhysRevC.75.055204
2007MI03 J.Phys.(London) G34, 703 (2007) Polishing the lens: I.Pionic final state interactions and HBT correlations: distorted wave emission-function (DWEF) formalism and examples
doi: 10.1088/0954-3899/34/4/009
2007MI04 Nucl.Phys. A782, 251c (2007) Quantum dynamics, the RHIC HBT puzzle, and the chiral phase transition NUCLEAR REACTIONS 197Au(197Au, X), E(cm)=200 GeV/nucleon; analyzed pion correlations.
doi: 10.1016/j.nuclphysa.2006.10.011
2007MI09 Eur.Phys.J. A 31, 578 (2007) Implications of the nuclear EMC effect COMPILATION 1n, 1H; compiled muon scattering data from nucleon and discussed implications of the EMC effect.
doi: 10.1140/epja/i2006-10258-6
2007MI26 Phys.Rev. C 76, 024001 (2007) Resonant relativistic corrections and the Ay problem
doi: 10.1103/PhysRevC.76.024001
2007MI29 Phys.Rev.Lett. 99, 112001 (2007) Charge Densities of the Neutron and Proton
doi: 10.1103/PhysRevLett.99.112001
2007MI43 Phys.Rev. C 76, 065209 (2007) Densities, parton distributions, and measuring the nonspherical shape of the nucleon
doi: 10.1103/PhysRevC.76.065209
2006CR05 Nucl.Phys. A774, 857 (2006) The RHIC HBT puzzle, chiral symmetry restoration, and pion opacity NUCLEAR REACTIONS Au(Au, X), E(cm)=200 GeV/nucleon; calculated HBT radii, pion transverse momentum spectrum. Relativistic quantum wave-mechanical optical model with distorted wave emission function. Comparison with data.
doi: 10.1016/j.nuclphysa.2006.06.151
2006DE06 Phys.Rev. C 73, 015204 (2006) W.Detmold, G.A.Miller, J.R.Smith Role of the nuclear vector potential in deep inelastic scattering
doi: 10.1103/PhysRevC.73.015204
2006KV03 Phys.Rev. C 73, 065203 (2006) Shapes of the nucleon NUCLEAR STRUCTURE A=1; calculated spin-dependent density operators, deformations.
doi: 10.1103/PhysRevC.73.065203
2006LA14 Phys.Rev. C 74, 018201 (2006) A.Larson, G.A.Miller, M.Strikman Pionic color transparency NUCLEAR REACTIONS 12C, 64Cu, 197Au(e, e'X), E not given; calculated transparency vs momentum transfer for pion production. Semiclassical approximation.
doi: 10.1103/PhysRevC.74.018201
2006MI26 Nucl.Phys. B(Proc.Supp.) S161, 185 (2006) Light front calculations of nucleon form factors
doi: 10.1016/j.nuclphysbps.2006.08.016
2006MI33 Ann.Rev.Nucl.Part.Sci. 56, 253 (2006) G.A.Miller, A.K.Opper, E.J.Stephenson Charge Symmetry Breaking and QCD
doi: 10.1146/annurev.nucl.56.080805.140446
2006NO08 Phys.Lett. B 639, 465 (2006) A.Nogga, A.C.Fonseca, A.Gardestig, C.Hanhart, C.J.Horowitz, G.A.Miller, J.A.Niskanen, U.van Kolck Realistic few-body physics in the dd → απ0 NUCLEAR REACTIONS 2H(d, π0), E=293 MeV; calculated σ, related matrix elements. Effective field theory with four-body theory.
doi: 10.1016/j.physletb.2006.04.058
2005CR01 Phys.Rev.Lett. 94, 102302 (2005); Erratum Phys.Rev.Lett. 95, 139901 (2005) J.G.Cramer, G.A.Miller, J.M.S.Wu, J.-H.Yoon Quantum Opacity, the RHIC Hanbury Brown-Twiss Puzzle, and the Chiral Phase Transition
doi: 10.1103/PhysRevLett.94.102302
2005MA33 Phys.Rev. C 71, 055204 (2005) H.H.Matevosyan, G.A.Miller, A.W.Thomas Comparison of nucleon form factors from lattice QCD against the light front cloudy bag model and extrapolation to the physical mass regime
doi: 10.1103/PhysRevC.71.055204
2005MB08 Phys.Rev. C 72, 065204 (2005) H.H.Matevosyan, A.W.Thomas, G.A.Miller Study of lattice QCD form factors using the extended Gari-Krumpelmann model NUCLEAR STRUCTURE 1H; calculated electromagnetic form factors, quark mass dependence. Vector meson dominance model.
doi: 10.1103/PhysRevC.72.065204
2005SM06 Phys.Rev. C 72, 022203 (2005) Polarized quark distributions in nuclear matter
doi: 10.1103/PhysRevC.72.022203
2004BR01 Phys.Lett. B 578, 69 (2004) S.J.Brodsky, L.Frankfurt, R.Gilman, J.R.Hiller, G.A.Miller, E.Piasetzky, M.Sargsian, M.Strikman Hard photodisintegration of a proton pair in 3He NUCLEAR REACTIONS 3He(γ, 2p), E=high; calculated σ(E, θ). Several models compared.
doi: 10.1016/j.physletb.2003.10.018
2004GA22 Phys.Rev. C 69, 044606 (2004) A.Gardestig, C.J.Horowitz, A.Nogga, A.C.Fonseca, C.Hanhart, G.A.Miller, J.A.Niskanen, U.van Kolck Survey of charge symmetry breaking operators for dd → απ0 NUCLEAR REACTIONS 2H(d, π0), E=228.5, 231.8 MeV; calculated pion production total σ, charge symmetry breaking amplitudes; deduced reaction mechanism features. Effective field theory approach.
doi: 10.1103/PhysRevC.69.044606
2004MI22 Phys.Rev. C 69, 044004 (2004) Relation between the deuteron form factor at high momentum transfer and the high energy neutron-proton scattering amplitude NUCLEAR STRUCTURE 2H; calculated form factor, relationship to neutron-proton scattering amplitude.
doi: 10.1103/PhysRevC.69.044004
2004MI24 Phys.Rev. C 69, 052201 (2004) Handling the handbag diagram in Compton scattering on the proton NUCLEAR REACTIONS 1H(γ, γ'), E ≈ 2-6 GeV; calculated σ(θ), helicity correlation parameters.
doi: 10.1103/PhysRevC.69.052201
2004MI39 Phys.Rev. C 70, 022202 (2004) Even parity Θ pentaquark and stable antistrange nuclear matter
doi: 10.1103/PhysRevC.70.022202
2004SM11 Phys.Rev. C 70, 065205 (2004) Chiral solitons in nuclei: Electromagnetic form factors NUCLEAR STRUCTURE 1H; calculated electromagnetic form factors of bound proton. Chiral quark-soliton model.
doi: 10.1103/PhysRevC.70.065205
2004TI07 Phys.Rev. D 70, 093008 (2004) B.C.Tiburzi, W.Detmold, G.A.Miller Double distributions for the proton NUCLEAR STRUCTURE 1H; calculated generalized parton distributions, form factors.
doi: 10.1103/PhysRevD.70.093008
2003MI08 Phys.Rev. C 67, 042501 (2003) Nuclear spin-isospin correlations, parity violation, and the fπ problem NUCLEAR STRUCTURE 18,19F, 133Cs, 205Tl; analyzed parity-nonconserving coupling constants, spin-isospin correlations, related features.
doi: 10.1103/PhysRevC.67.042501
2003MI16 Phys.Rev. C 68, 022201 (2003) Shapes of the proton NUCLEAR STRUCTURE 1H; analyzed form factor data; calculated spin-dependent quark densities, deformation features.
doi: 10.1103/PhysRevC.68.022201
2003SA06 J.Phys.(London) G29, R1 (2003) M.M.Sargsian, J.Arrington, W.Bertozzi, W.Boeglin, C.E.Carlson, D.B.Day, L.L.Frankfurt, K.Egiyan, R.Ent, S.Gilad, K.Griffioen, D.W.Higinbotham, S.Kuhn, W.Melnitchouk, G.A.Miller, E.Piasetzky, S.Stepanyan, M.I.Strikman, L.B.Weinstein Hadrons in the nuclear medium
doi: 10.1088/0954-3899/29/3/201
2003SM08 Phys.Rev.Lett. 91, 212301 (2003) Chiral Solitons in Nuclei: Saturation, EMC Effect, and Drell-Yan Experiments
doi: 10.1103/PhysRevLett.91.212301
2003ST16 Phys.Rev.Lett. 91, 142302 (2003) E.J.Stephenson, A.D.Bacher, C.E.Allgower, A.Gardestig, C.M.Lavelle, G.A.Miller, H.Nann, J.Olmsted, P.V.Pancella, M.A.Pickar, J.Rapaport, T.Rinckel, A.Smith, H.M.Spinka, U.van Kolck Observation of the Charge Symmetry Breaking d + d → 4He + π0 Reaction Near Threshold NUCLEAR REACTIONS 2H(d, π0), (d, 2γ), E=228.5, 231.8 MeV; measured missing mass spectra, pion production total σ; deduced charge symmetry breaking features.
doi: 10.1103/PhysRevLett.91.142302
2002CO16 Phys.Rev. C65, 067001 (2002) Pion-Only, Chiral Light-Front Model of the Deuteron NUCLEAR STRUCTURE 2H; calculated binding energies; deduced relativity and chiral symmetry effects. Light-front pion-only model.
doi: 10.1103/PhysRevC.65.067001
2002CO22 Phys.Rev. C66, 034002 (2002) Deuteron Binding Energies and Form Factors from Light-Front Hamiltonian Field Theory NUCLEAR STRUCTURE 2H; calculated binding energy, form factors, effects of broken rotational invariance in light-front dynamics.
doi: 10.1103/PhysRevC.66.034002
2002MI02 Phys.Rev. C65, 015211 (2002) Return of the EMC Effect
doi: 10.1103/PhysRevC.65.015211
2002MI13 Nucl.Phys. A699, 247c (2002) Light Front Nuclear Theory
doi: 10.1016/S0375-9474(01)01500-7
2002MI24 Phys.Rev. C65, 065205 (2002) Q2 Independence of QF2/F1, Poincare Invariance, and the Nonconservation of Helicity NUCLEAR STRUCTURE 1H; calculated form factors. Relativistic constituent quark model.
doi: 10.1103/PhysRevC.65.065205
2002MI38 Phys.Rev. C66, 032201 (2002) Light Front Cloudy Bag Model: Nucleon electromagnetic form factors NUCLEAR STRUCTURE 1n, 1H; calculated electromagnetic form factors. Light front cloudy bag model.
doi: 10.1103/PhysRevC.66.032201
2002MI52 Nucl.Phys. B(Proc.Supp.) S112, 223 (2002) Fermi Gas Model
doi: 10.1016/S0920-5632(02)01786-3
2002SM06 Phys.Rev. C65, 055206 (2002); Erratum Phys.Rev. C66, 049903 (2002) Return of the EMC Effect: Finite nuclei NUCLEAR REACTIONS 16O, 40Ca, 208Pb(e, e'X), E not given; calculated structure function ratios. Comparison with data, possible medium modification of nucleon structure discussed.
doi: 10.1103/PhysRevC.65.055206
2001BR37 Phys.Rev. C64, 055204 (2001) S.J.Brodsky, J.R.Hiller, C.-R.Ji, G.A.Miller Perturbative QCD and Factorization of Coherent Pion Photoproduction on the Deuteron NUCLEAR REACTIONS 2H(γ, π0), E < 40 GeV; calculated photoproduction amplitude. Perturbative QCD, factorization of amplitude, comparison with data.
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