A systematic solution of a model for copper oxides reveals a line of transi
tions T = T-p(x.) for x, the doping away from half filling less than a crit
ical value, to a phase with broken time reversal and rotational symmetry. T
he single-particle spectrum in this phase is calculated to have a gap simil
ar to[cos(k(x)a/pi) - cos(k(y)a/pi)](2). The properties in this phase are c
ompared to the properties of the so-called "pseudogap phase" of the copper
oxides.