We analyze the smoothness of the ground state energy of a one-parameter Hamiltonian by studying the differential geometry of the numerical range and continuity of the maximum-entropy inference. The domain of the inference map is the numerical range, a convex compact set in the plane. We show that its boundary, viewed as a manifold, has the same order of differentiability as the ground state energy. We prove that discontinuities of the inference map correspond to C1-smooth crossings of the ground state energy with a higher energy level. Discontinuities may appear only at C1-smooth points of the boundary of the numerical range. Discontinuities exist at all C2-smooth non-analytic boundary points and are essentially stronger than at analytic points or at points which are merely C1-smooth (non-exposed points).
REFERENCES
The notion of lower semi-continuity of a set-valued function goes back to Kuratowski and Bouligand, see Sec. 6.1 of Ref. 10.
That fA is open at |x⟩ means that fA maps neighborhoods of |x⟩ in to neighborhoods of fA(|x⟩) in W.
The idea of viewing non-exposed points as exposed points of facets is a special case of the conception of poonem.27
The relative interior of a subset M of is the interior of M with respect to the topology of the affine hull of M.
What we call reverse Gauss map xW is known as reverse spherical image map.69
For k ≥ 1, a Ck- submanifold M of is a subset such that for each point p of M there is a (real) Ck-diffeomorphism g : U → V from an open neighborhood U of p in to an open neighborhood V of 0 in such that g(M ∩ U) lies in the x1-axis of . The subset M is an analytic submanifold of , if g can be chosen to be an analytic diffeomorphism.
The notation un-regn(K) indicates that every regular normal vector u ∈ regn(K) which lies in un-regn(K) is the unique inner unit normal vector at xK(u), because xK(u) is a smooth point.