Up to now, the value of the dynamic critical exponent z is still an open qu
estion. We have studied this exponent in the intermediate (XY) critical reg
ime in zero field for a set of high quality Bi2Sr2CaCu2O8+delta single crys
tals both by previously obtained critical exponents of the de critical cond
uctivity fluctuations [1] and in terms of Fisher-Fisher-Huse (FFH) dynamic
scaling [2]. In this regime (i.e. the absence of Coulomb interactions), one
would expect model-E dynamics (z = 1.5) to apply with the conserved charge
-density conjugate to the phase fluctuations. However, we find the dynamic
critical exponent to be z = 2, which is in agreement with the suggestion of
FFH that due to the plasma fluctuation, fully relaxational dynamics, model
A (z = 2), should be appropriate.