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The mass rigidity of a stationary random measure M on Rᵈ or Zᵈ (called number rigidity for a point process) entails that for a bounded set A the knowledge of M on Ac determines M (A) ; the k-order rigidity for an integer k means we can recover the moments of the restriction of M on A^c up to order k. We show that the k-rigidity properties of a random stationary measure M can be characterised by the integrability properties around 0 of s, the continuous part of the spectral measure, by exploiting a connection with Schwartz' Paley-Wiener theorem for analytic functions of exponential type. If 1/s is not integrable in zero, M is mass rigid, and similarly if s has a zero of order 2k in 0, then M is k-rigid. In the continuous setting, these local conditions are also necessary if s has finitely many zeros, or is isotropic, or is at the opposite separable. This explains why no model seems to exhibit rigidity in dimension d 3, and allows to efficiently recover many recent rigidity results about point processes. In the discrete setting, these results hold provided \#A > 2k. For a continuous Determinantal point process with reduced kernel, k-rigidity is equivalent to (1-²) ^-1 having a zero of order 2k in 0, which answers questions on completeness and number rigidity. We also explore the consequences of these statements in the less tractable realm of Riesz gases.
Raphaël Lachièze-Rey (Fri,) studied this question.