We consider the following question: given A ∈ SL ( 2 , R ) , which potentials q for the second order Sturm–Liouville problem have A as its Floquet multiplier? More precisely, define the monodromy map μ taking a potential q ∈ L 2 ( [ 0 , 2 π ] ) to μ ( q ) = Φ ˜ ( 2 π ) , the lift to the universal cover G = SL ( 2 , R ) ˜ of SL ( 2 , R ) of the fundamental matrix map Φ : [ 0 , 2 π ] → SL ( 2 , R ) , Φ ( 0 ) = I , Φ ′ ( t ) = ( 0 1 q ( t ) 0 ) Φ ( t ) . Let H be the real infinite-dimensional separable Hilbert space: we present an explicit diffeomorphism Ψ : G 0 × H → H 0 ( [ 0 , 2 π ] ) 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 , 2 π ] ) be the set of potentials q for which the equation − u ″ + q u = 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 .
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