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Emergent Hadron Mass in Strong Dynamics
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π + photoproduction on the proton for photon energies from 0.725 to 2.875 GeV
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Transition form factors and helicity amplitudes for electroexcitation of negative and positive parity nucleon resonances in a light-front quark model
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An isobar model for η photo- and electroproduction on the nucleon
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Poincaré-covariant analysis of heavy-quark baryons
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June 2018 |
Quark propagator with two flavors of O ( a ) -improved Wilson fermions
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Gauge Sector Dynamics in QCD
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Quark model calculations of transition form factors at high photon virtualities
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January 2020 |
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Model analysis of the ep → e ' p π + π − electroproduction reaction on the proton
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Electroexcitation of Nucleon Resonances in a Light-Front Relativistic Quark Model
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Ward–Green–Takahashi identities and the axial-vector vertex
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π - and K -meson Bethe-Salpeter amplitudes
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On some ambiguities in the method of effective charges
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July 1989 |
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Nucleon elastic form factors at accessible large spacelike momenta
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Gluon and ghost propagators in the Landau gauge: Deriving lattice results from Schwinger-Dyson equations
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Multipole amplitudes of pion photoproduction on nucleons up to 2 GeV using dispersion relations and the unitary isobar model
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January 2003 |
Electroexcitation of nucleon resonances from CLAS data on single pion electroproduction
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November 2009 |
Extracting meson-baryon contributions to the electroexcitation of the N ( 1675 ) 5 2 − nucleon resonance
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July 2015 |
New results from the studies of the N ( 1440 ) 1 / 2 + , N ( 1520 ) 3 / 2 − , and Δ ( 1620 ) 1 / 2 − resonances in exclusive e p → e ′ p ′ π + π − electroproduction with the CLAS detector
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Dyson-Schwinger equations and their application to hadronic physics
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January 1994 |
Gauge Invariance and Mass
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January 1962 |
Hadron Wave Functions from Lattice QCD
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Electroproduction of the N * ( 1535 ) nucleon resonance in QCD
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July 2015 |
Resonant contributions to inclusive nucleon structure functions from exclusive meson electroproduction data
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August 2021 |
Completing the Picture of the Roper Resonance
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Pion and kaon structure at the electron-ion collider
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October 2019 |
Nucleon-to-Roper electromagnetic transition form factors at large Q 2
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February 2019 |
Dynamical diquarks in the $${\varvec{\gamma ^{(*)} p\rightarrow N(1535)\frac{1}{2}^-}}$$ transition
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September 2021 |
Dynamical mass generation in continuum quantum chromodynamics
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September 1982 |
New Insight in the Q 2 Dependence of Proton Generalized Polarizabilities
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Two Pion Photo- and Electroproduction with CLAS
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January 2020 |
Elastic and Transition Form Factors of the Δ(1232)
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December 2013 |
CLAS $$\varvec{N^*}$$ N ∗ Excitation Results from Pion and Kaon Electroproduction
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May 2018 |
Transition form factors: γ * + p → Δ ( 1232 ) , Δ ( 1600 )
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August 2019 |
Photo- and electroproduction of eta mesons
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September 1995 |
Imaging Dynamical Chiral-Symmetry Breaking: Pion Wave Function on the Light Front
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March 2013 |
Nucleon resonances in Compton scattering
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November 2018 |
Emergence of Hadron Mass and Structure
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Empirical Consequences of Emergent Mass
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September 2020 |
Unitary isobar model --MAID2007
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October 2007 |
Effective charge from lattice QCD *
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August 2020 |
The CLAS12 Spectrometer at Jefferson Laboratory
- Burkert, V. D.; Elouadrhiri, L.; Adhikari, K. P.
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Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, Vol. 959
https://doi.org/10.1016/j.nima.2020.163419
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Discretization effects on renormalized gauge-field Green’s functions, scale setting, and the gluon mass
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December 2018 |
Quasi-Particles and Gauge Invariance in the Theory of Superconductivity
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February 1960 |
Strong Running Coupling from the Gauge Sector of Domain Wall Lattice QCD with Physical Quark Masses
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April 2019 |
Measurements of the γ*p → Δ reaction at low Q2
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October 2013 |
Nucleon and Roper electromagnetic elastic and transition form factors
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February 2012 |
Isobar channels in the production of π+π− pairs on a proton by virtual photons
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The Physics of the B Factories
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Ghost dynamics in the soft gluon limit
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September 2021 |
Lattice three-gluon vertex in extended kinematics: Planar degeneracy
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March 2023 |
Nucleon Resonance Structure Studies via Exclusive KY Electroproduction
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June 2016 |
A schematic model of baryons and mesons
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February 1964 |
The pion: an enigma within the Standard Model
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The decay constants fD and f D s $$ {f}_{D_s} $$ in the continuum limit of Nf = 2 + 1 domain wall lattice QCD
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December 2017 |
Emergence of mass in the gauge sector of QCD*
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November 2022 |
Revealing the structure of light pseudoscalar mesons at the electron–ion collider
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May 2021 |
Perspective on the Origin of Hadron Masses
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December 2016 |
Pion mass and decay constant
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Selected Science Opportunities for the EicC
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Amplitude reconstruction from complete electroproduction experiments and truncated partial-wave expansions
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August 2017 |
Beam-recoil transferred polarization in K+Y electroproduction in the nucleon resonance region with CLAS12
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Structure of the neutral pion and its electromagnetic transition form factor
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April 2016 |
Extracting the σ -term from low-energy pion-nucleon scattering
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December 2017 |
Measurements of e p → e ′ π + π − p ′ cross sections with CLAS at 1.40 GeV < W < 2.0 GeV and 2.0 GeV 2 < Q 2 < 5.0 GeV 2
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August 2017 |
Electromagnetic excitation of nucleon resonances
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September 2011 |
Electromagnetic $${\varvec{N}}^{\varvec{*}}$$ N ∗ Transition Form Factors in the ANL-Osaka Dynamical Coupled-Channels Approach
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March 2018 |
Field theories with « Superconductor » solutions
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On mass and matter
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Masses of Ground- and Excited-State Hadrons
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Insights into the emergence of mass from studies of pion and kaon structure
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September 2021 |
FLAG Review 2019: Flavour Lattice Averaging Group (FLAG)
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February 2020 |
Experimental Determination of the QCD Effective Charge αg1(Q)
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May 2022 |
An experimental program with high duty-cycle polarized and unpolarized positron beams at Jefferson Lab
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August 2021 |
The Nucleon Resonance Structure from the π+π−p Electroproduction Reaction off Protons
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May 2019 |
Studies of Nucleon Resonance Structure in Exclusive Meson Electroproduction
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June 2013 |
Jülich-Bonn-Washington model for pion electroproduction multipoles
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June 2021 |
Resonance Electroproduction and the Origin of Mass
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January 2020 |
Strong QCD Insights from Excited Nucleon Structure Studies with CLAS and CLAS12
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August 2020 |
Science Requirements and Detector Concepts for the Electron-Ion Collider
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October 2022 |
Pseudoscalar meson radial excitations
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Photo- and Electrocouplings of Nucleon Resonances
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July 2022 |
QCD at finite temperature and chemical potential from Dyson–Schwinger equations
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March 2019 |
Domain wall QCD with physical quark masses
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April 2016 |
Diquark correlations in hadron physics: Origin, impact and evidence
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January 2021 |
Pion Electromagnetic Form Factor at Spacelike Momenta
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October 2013 |
Nucleon and $${\Delta}$$ Δ Elastic and Transition Form Factors
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October 2014 |
Measurements of e p → e ′ π + n at 1.6 < W < 2.0 GeV and extraction of nucleon resonance electrocouplings at CLAS
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April 2015 |
Reflections upon the emergence of hadronic mass
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December 2020 |
Virtual Compton scattering measurements in the nucleon resonance region
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October 2019 |
Exploring smoking-gun signals of the Schwinger mechanism in QCD
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January 2022 |
Coupled-channels analysis of pion and η electroproduction within the Jülich-Bonn-Washington model
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July 2022 |
Sigma Terms of Light-Quark Hadrons
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January 2006 |
N $$^*$$ ∗ Experiments and Their Impact on Strong QCD Physics
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April 2018 |
Electroexcitation of nucleon resonances at Q 2 = 0 . 65 ( GeV / c ) 2 from a combined analysis of single- and double-pion electroproduction data
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October 2005 |