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NSR database version of April 11, 2024.

Search: Author = G.A.Miller

Found 188 matches.

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2023MI14      Phys.Rev. C 108, L031002 (2023)


Entanglement maximization in low-energy neutron-proton scattering

doi: 10.1103/PhysRevC.108.L031002
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2023MI16      Phys.Rev. C 108, L041601 (2023)


Entanglement of elastic and inelastic scattering

doi: 10.1103/PhysRevC.108.L041601
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2022CO14      Phys.Rev. C 106, L062501 (2022)

L.Condren, G.A.Miller

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
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2022CR05      Phys.Rev. C 106, 065502 (2022)

J.W.Crawford, G.A.Miller

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
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2022KI22      Phys.Rev. C 106, 055202 (2022)

D.N.Kim, G.A.Miller

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
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2021CA18      Phys.Rev. C 104, L012201 (2021)

O.Caplow-Munro, G.A.Miller

Color transparency and the proton form factor: Evidence for the Feynman mechanism

doi: 10.1103/PhysRevC.104.L012201
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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
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2021ZH03      Phys.Lett. B 813, 136061 (2021)

X.Zhang, G.A.Miller

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
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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
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2020MI11      Phys.Rev. C 102, 022201 (2020)

G.A.Miller, S.J.Brodsky

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
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2020MI17      Phys.Rev. C 102, 055206 (2020)


Discovery versus precision in nuclear physics: A tale of three scales

doi: 10.1103/PhysRevC.102.055206
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2019AL25      Phys.Rev. C 100, 035205 (2019)

M.Alberg, G.A.Miller

Chiral light-front perturbation theory and the flavor dependence of the light-quark nucleon sea

doi: 10.1103/PhysRevC.100.035205
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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
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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
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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
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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
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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
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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
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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
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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
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2016TE07      Phys.Rev. C 94, 014002 (2016)

J.D.Terry, G.A.Miller

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
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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
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2015HO03      Phys.Rev. C 91, 035205 (2015)

T.J.Hobbs, M.Alberg, G.A.Miller

Constraining nucleon strangeness

doi: 10.1103/PhysRevC.91.035205
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2015LI37      Phys.Rev. C 92, 035209 (2015)

Y.-S.Liu, G.A.Miller

Polarized lepton-nucleon elastic scattering and a search for a light scalar boson

doi: 10.1103/PhysRevC.92.035209
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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
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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
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2014BU10      Phys.Rev. C 90, 024606 (2014)

M.Buuck, G.A.Miller

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
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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
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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
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2014WA24      Phys.Rev. C 89, 065206 (2014); Erratum Phys.Rev. C 91, 019903 (2015)

M.Wagman, G.A.Miller

Charge symmetry breaking and parity violating electron-proton scattering

doi: 10.1103/PhysRevC.89.065206
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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
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2013HO13      Phys.Rev. C 88, 015204 (2013)

G.T.Howell, G.A.Miller

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
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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
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2013HO18      Phys.Rev. C 88, 035202 (2013)

G.T.Howell, G.A.Miller

Color transparency in the reaction γ* A → p+p+(A-1)*

doi: 10.1103/PhysRevC.88.035202
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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
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2012CL01      Phys.Rev. C 86, 015208 (2012)

I.C.Cloet, G.A.Miller

Nucleon form factors and spin content in a quark-diquark model with a pion cloud

doi: 10.1103/PhysRevC.86.015208
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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
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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
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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
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2011BO18      Phys.Rev. C 83, 064003 (2011)

D.R.Bolton, G.A.Miller

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
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2011CL01      Phys.Rev. C 83, 012201 (2011)

I.C.Cloet, G.A.Miller

Third Zemach moment of the proton

doi: 10.1103/PhysRevC.83.012201
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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
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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
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2010BO03      Phys.Rev. C 81, 014001 (2010)

D.R.Bolton, G.A.Miller

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
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2010BO14      Phys.Rev. C 82, 024001 (2010)

D.R.Bolton, G.A.Miller

Impulse approximation in the np → dπ0 reaction reexamined

doi: 10.1103/PhysRevC.82.024001
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2010MI06      Phys.Rev. C 81, 035201 (2010)

G.A.Miller, B.C.Tiburzi

Relation between equal-time and light-front wave functions

doi: 10.1103/PhysRevC.81.035201
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2010MI17      Phys.Rev. C 82, 025205 (2010)

G.A.Miller, M.Strikman

Color transparency at energies available at the CERN COMPASS experiment

doi: 10.1103/PhysRevC.82.025205
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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
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2009LU06      Phys.Rev. C 79, 024902 (2009)

M.Luzum, G.A.Miller

Elliptic flow from final state interactions in the distorted-wave emission-function model

doi: 10.1103/PhysRevC.79.024902
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2009MI13      Phys.Rev. C 79, 055204 (2009)


Singular charge density at the center of the pion?

doi: 10.1103/PhysRevC.79.055204
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2009MI19      Phys.Rev. C 80, 045210 (2009)


Electromagnetic form factors and charge densities from hadrons to nuclei

doi: 10.1103/PhysRevC.80.045210
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2009MI24      Phys.Rev. C 80, 064319 (2009)

G.A.Miller, A.Schwenk

Isospin-symmetry-breaking corrections to superallowed Fermi β decay: Radial excitations

doi: 10.1103/PhysRevC.80.064319
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2009RI07      Phys.Rev. C 80, 015201 (2009)

J.A.Rinehimer, G.A.Miller

Connecting the Breit frame to the infinite momentum light front frame: How GE turns into F1

doi: 10.1103/PhysRevC.80.015201
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2009RI09      Phys.Rev. C 80, 025206 (2009)

J.A.Rinehimer, G.A.Miller

Neutron charge density from simple pion cloud models

doi: 10.1103/PhysRevC.80.025206
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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
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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
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2008MI21      Phys.Rev. C 78, 032201 (2008)

G.A.Miller, J.Arrington

Neutron negative central charge density: An inclusive-exclusive connection

doi: 10.1103/PhysRevC.78.032201
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2008MI22      Phys.Rev. C 78, 035501 (2008)

G.A.Miller, A.Schwenk

Isospin-symmetry-breaking corrections to superallowed Fermi β decay: Formalism and schematic models

doi: 10.1103/PhysRevC.78.035501
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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
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2007KV03      Phys.Rev. C 76, 025203 (2007)

A.Kvinikhidze, G.A.Miller

Subtleties of Lorentz invariance and shapes of the nucleon

doi: 10.1103/PhysRevC.76.025203
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2007LA17      Phys.Rev. C 75, 055204 (2007)

T.A.Lahde, G.A.Miller

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
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2007MI03      J.Phys.(London) G34, 703 (2007)

G.A.Miller, J.G.Cramer

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
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2007MI04      Nucl.Phys. A782, 251c (2007)

G.A.Miller, J.G.Cramer

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
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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
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2007MI26      Phys.Rev. C 76, 024001 (2007)

G.A.Miller, A.Schwenk

Resonant relativistic corrections and the Ay problem

doi: 10.1103/PhysRevC.76.024001
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2007MI29      Phys.Rev.Lett. 99, 112001 (2007)


Charge Densities of the Neutron and Proton

doi: 10.1103/PhysRevLett.99.112001
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2007MI43      Phys.Rev. C 76, 065209 (2007)


Densities, parton distributions, and measuring the nonspherical shape of the nucleon

doi: 10.1103/PhysRevC.76.065209
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2006CR05      Nucl.Phys. A774, 857 (2006)

J.G.Cramer, G.A.Miller

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
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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
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2006KV03      Phys.Rev. C 73, 065203 (2006)

A.Kvinikhidze, G.A.Miller

Shapes of the nucleon

NUCLEAR STRUCTURE A=1; calculated spin-dependent density operators, deformations.

doi: 10.1103/PhysRevC.73.065203
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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
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2006MI26      Nucl.Phys. B(Proc.Supp.) S161, 185 (2006)


Light front calculations of nucleon form factors

doi: 10.1016/j.nuclphysbps.2006.08.016
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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
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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
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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
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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
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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
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2005SM06      Phys.Rev. C 72, 022203 (2005)

J.R.Smith, G.A.Miller

Polarized quark distributions in nuclear matter

doi: 10.1103/PhysRevC.72.022203
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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
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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
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2004MI22      Phys.Rev. C 69, 044004 (2004)

G.A.Miller, M.Strikman

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2004MI39      Phys.Rev. C 70, 022202 (2004)


Even parity Θ pentaquark and stable antistrange nuclear matter

doi: 10.1103/PhysRevC.70.022202
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2004SM11      Phys.Rev. C 70, 065205 (2004)

J.R.Smith, G.A.Miller

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2003SM08      Phys.Rev.Lett. 91, 212301 (2003)

J.R.Smith, G.A.Miller

Chiral Solitons in Nuclei: Saturation, EMC Effect, and Drell-Yan Experiments

doi: 10.1103/PhysRevLett.91.212301
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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
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2002CO16      Phys.Rev. C65, 067001 (2002)

J.R.Cooke, G.A.Miller

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
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2002CO22      Phys.Rev. C66, 034002 (2002)

J.R.Cooke, G.A.Miller

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
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2002MI02      Phys.Rev. C65, 015211 (2002)

G.A.Miller, J.R.Smith

Return of the EMC Effect

doi: 10.1103/PhysRevC.65.015211
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2002MI13      Nucl.Phys. A699, 247c (2002)


Light Front Nuclear Theory

doi: 10.1016/S0375-9474(01)01500-7
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2002MI24      Phys.Rev. C65, 065205 (2002)

G.A.Miller, M.R.Frank

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
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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
Citations: PlumX Metrics

2002MI52      Nucl.Phys. B(Proc.Supp.) S112, 223 (2002)


Fermi Gas Model

doi: 10.1016/S0920-5632(02)01786-3
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2002SM06      Phys.Rev. C65, 055206 (2002); Erratum Phys.Rev. C66, 049903 (2002)

J.R.Smith, G.A.Miller

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
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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.

doi: 10.1103/PhysRevC.64.055204
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2001HA17      Phys.Rev. C63, 044002 (2001)

C.Hanhart, G.A.Miller, F.Myhrer, T.Sato, U.van Kolck

Toy Model for Pion Production in Nucleon-Nucleon Collisions

doi: 10.1103/PhysRevC.63.044002
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