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We derive the linearized Ginzburg-Landau (GL) equation for an ultra-thin superconducting film with curvature in a magnetic field. By introducing a novel transverse order parameter that varies slowly along the film, and applying the superconducting/vacuum boundary condition, we decouple the linearized GL equation into a transverse part and a surface part that includes the superconducting geometric potential (GP). The nucleation of the superconducting state in curved thin superconducting films can be equivalently described by the surface part equation. In the equivalent GL free energy of a curved superconducting film, the superconducting GP enables the film to remain in the superconducting state even when the superconducting parameter $ α$ turns positive by further reducing the quadratic term of the order parameter. Furthermore, we numerically investigate the phase transition of a rectangle thin superconducting film bent around a cylindrical surface. Our numerical results show that the superconducting GP enhances the superconductivity of the curved film by weakening the effect of the magnetic field, and the increase of the critical temperature, in units of the bulk critical temperature, is equal to the product of the negative superconducting GP and the square of the zero-temperature coherence length, which agrees with our theoretical predictions.