  Light constituent quark masses and the corresponding dynamical quark masses
are determined by data, the quark-level linear sigma model, and infrared QCD.
This allows to define effective nonstrange and strange current quark masses,
which reproduce the experimental pion and kaon masses very accurately, by
simple additivity. In contrast, the usual nonstrange and strange current quarks
employed by the Particle Data Group and Chiral Perturbation Theory do not allow
a straightforward quantitative explanation of the pion and kaon masses.
