Nonlinear Classical Fields

Abstract

We regard a classical field as a medium and so the additional parameter, the velocity of a field,appears. If the one regard as a potential of same field then the self-energies of the fields became finite. Electromagnetic, mechanical, pionic, and somewhat gluonic fields are regarding

Inserted "Different fouvector fields"

References in corpus (2)

• Relativistic, QED, and finite nuclear mass corrections for low-lying states of Li and Be${}^{+}$
• Three-dimensional angular momentum projected relativistic point-coupling approach for the low-lying excited states in ${}^{24}$Mg