We project onto the light front the pion’s Poincaré-covariant Bethe-Salpeter wave function obtained using two different approximations to the kernels of quantum chromodynamics’ Dyson-Schwinger equations. At an hadronic scale, both computed results are concave and significantly broader than the asymptotic distribution amplitude, φasyπ(x)=6x(1−x); e.g., the integral of φπ(x)/φasyπ(x) is 1.8 using the simplest kernel and 1.5 with the more sophisticated kernel. Independent of the kernels, the emergent phenomenon of dynamical chiral-symmetry breaking is responsible for hardening the amplitude
The Dyson-Schwinger equation for the quark propagator is handled in the infrared in three ways: (i) ...
AbstractWe investigate the neutral pion photoproduction on the proton near threshold in covariant ch...
The Dyson-Schwinger equation for the quark propagator is handled in the infrared in three ways: (i) ...
We project onto the light front the pion's Poincaré-covariant Bethe-Salpeter wave function obtained ...
Abstract We describe results for the pion distribution amplitude (PDA) at the non-perturbative scale...
A rainbow-ladder truncation of QCD’s Dyson-Schwinger equations is used to calculate ρ- and ϕ-meson v...
Dyson-Schwinger equations furnish a Poincare' covariant approach to hadron physics. They reveal that...
The pseudoscalar projection of the pionʼs Poincaré-covariant Bethe–Salpeter amplitude onto the light...
A rainbow-ladder truncation of QCD's Dyson-Schwinger equations is used to calculate rho- and ph...
Dynamical chiral-symmetry breaking (DCSB) in QCD is investigated in the Schwinger-Dyson (SD) formali...
We investigate the neutral pion photoproduction on the proton near threshold in covariant chiral per...
We compute the kaon's valence-quark (twist-two parton) distribution amplitude (PDA) by projecting it...
The lightest meson, the pion, features two faces -- one is the elementary Goldstone boson of QCD and...
The Dyson-Schwinger equation for the quark propagator is handled in the infrared in three ways: (i) ...
The Dyson-Schwinger equation for the quark propagator is handled in the infrared in three ways: (i) ...
The Dyson-Schwinger equation for the quark propagator is handled in the infrared in three ways: (i) ...
AbstractWe investigate the neutral pion photoproduction on the proton near threshold in covariant ch...
The Dyson-Schwinger equation for the quark propagator is handled in the infrared in three ways: (i) ...
We project onto the light front the pion's Poincaré-covariant Bethe-Salpeter wave function obtained ...
Abstract We describe results for the pion distribution amplitude (PDA) at the non-perturbative scale...
A rainbow-ladder truncation of QCD’s Dyson-Schwinger equations is used to calculate ρ- and ϕ-meson v...
Dyson-Schwinger equations furnish a Poincare' covariant approach to hadron physics. They reveal that...
The pseudoscalar projection of the pionʼs Poincaré-covariant Bethe–Salpeter amplitude onto the light...
A rainbow-ladder truncation of QCD's Dyson-Schwinger equations is used to calculate rho- and ph...
Dynamical chiral-symmetry breaking (DCSB) in QCD is investigated in the Schwinger-Dyson (SD) formali...
We investigate the neutral pion photoproduction on the proton near threshold in covariant chiral per...
We compute the kaon's valence-quark (twist-two parton) distribution amplitude (PDA) by projecting it...
The lightest meson, the pion, features two faces -- one is the elementary Goldstone boson of QCD and...
The Dyson-Schwinger equation for the quark propagator is handled in the infrared in three ways: (i) ...
The Dyson-Schwinger equation for the quark propagator is handled in the infrared in three ways: (i) ...
The Dyson-Schwinger equation for the quark propagator is handled in the infrared in three ways: (i) ...
AbstractWe investigate the neutral pion photoproduction on the proton near threshold in covariant ch...
The Dyson-Schwinger equation for the quark propagator is handled in the infrared in three ways: (i) ...