Abstract
On a null-plane (light-front), all effects of spontaneous chiral symmetry
breaking are contained in the three Hamiltonians (dynamical Poincaré
generators), while the vacuum state is a chiral invariant. This property is
used to give a general proof of Goldstone's theorem on a null-plane. Focusing
on null-plane QCD with N degenerate flavors of light quarks, the
chiral-symmetry breaking Hamiltonians are obtained, and the role of vacuum
condensates is clarified. In particular, the null-plane Gell-Mann-Oakes-Renner
formula is derived, and a general prescription is given for mapping all
chiral-symmetry breaking QCD condensates to chiral-symmetry conserving
null-plane QCD condensates. The utility of the null-plane description lies in
the operator algebra that mixes the null-plane Hamiltonians and the chiral
symmetry charges. It is demonstrated that in a certain non-trivial limit, the
null-plane operator algebra reduces to the symmetry group SU(2N) of the
constituent quark model.
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