We consider the following question: given A ∈ SL(2, R), which potentials q for the second order SturmLiouville problem have A as its Floquet multiplier? More precisely, define the monodromy map μ taking a potential q ∈ L 2 ([0, 2π ]) to μ(q) = Φ(2π), the lift to the universal cover G = SL(2, R) of SL(2, R) of the fundamental matrix map Φ : [0, 2π ] → SL(2, R),Let H be the real infinite-dimensional separable Hilbert space: we present an explicit diffeomorphism Ψ : G 0 × H → H 0 ([0, 2π ]) such that the composition μ • Ψ is the projection on the first coordinate, where G 0 is an explicitly given open subset of G diffeomorphic to R 3 . The key ingredient is the correspondence between potentials q and the image in the plane of the first row of Φ, parametrized by polar coordinates, which we call the Kepler transform. As an application among others, let C 1 ⊂ L 2 ([0, 2π ]) be the set of potentials q for which the equation −u + qu = 0 admits a nonzero periodic solution: C 1 is diffeomorphic to the disjoint union of a hyperplane and Cartesian products of the usual cone in R 3 with H.