Measurements of the zero-field resistive transition of Bi2Sr2CaCu2O8 s
ingle crystals suggest that a bulk zero-resistance state develops thro
ugh a sequential process characterized by two transition temperatures.
The upper transition corresponds to Josephson coupling of parallel Cu
O bilayers, and the lower transition to the conventional Kosterlitz-Th
ouless dissociation of bound vortex excitations. Measurements using a
''flux transformer'' electrode geometry indicate a pronounced peak in
the secondary voltage, which is suppressed by an external magnetic fie
ld.