  We study the two-dimensional spin-charge separated Ginzburg-Landau theory
containing U(1) gauge interactions as a semi-phenomenological model describing
fluctuating condensates in high temperature superconductivity. Transforming the
original GL action, we abstract the effective action of Cooper pair.
Especially, we clarify how Cooper pair correlation evolves in the normal state
from the point of view of spin-charge separation. Furthermore, we point out how
Cooper pair couples to gauge field in a gauge-invariant way, stressing the
insensitivity of Cooper pair to infrared gauge field fluctuation.
