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A theory of mesoscopic fluctuations in disordered thin superconducting filmsin a parallel magnetic field is developed. At zero temperature, thesuperconducting state undergoes a phase transition into a state characterizedby superfluid densities of random signs, instead of a spin polarized disorderedFermi liquid phase. Consequently, the ground state belongs to the sameuniversality class as the 2D XY spin glass. As the magnetic field increasesfurther, mesoscopic pairing states are nucleated in an otherwise homogeneousspin polarized disordered Fermi liquid. The statistics of these pairing statesis universal depending on the sheet conductance of the 2D film.Comment: Latex, 39 pages, 2 figures included; to appear in Int. J. Mod. Phys.

A NOVEL SUPERCONDUCTING GLASS STATE IN DISORDERED THIN FILMS IN CLOGSTON LIMIT