We derive Heisenberg uncertainty principles for pairs of Linear Canonical Transforms of a given function, by resorting to the fact that these transforms are just metaplectic operators associated with free symplectic matrices. The results obtained synthesize and generalize previous results found in the literature, because they apply to all signals, in arbitrary dimension and any metaplectic operator (which includes Linear Canonical Transforms as particular cases). Moreover, we also obtain a generalization of the Robertson-Schrödinger uncertainty principle for Linear Canonical Transforms. We also propose a new quadratic phase-space distribution, which represents a signal along two intermediate directions in the time-frequency plane. The marginal distributions are always non-negative and permit a simple interpretation in terms of the Radon transform. We also give a geometric interpretation of this quadratic phase-space representation as a Wigner distribution obtained upon Weyl quantization on a non-standard symplectic vector space. Finally, we derive the multidimensional version of the Hardy uncertainty principle for metaplectic operators and the Paley-Wiener theorem for Linear Canonical Transforms.
The notion of polarity between sets, well-known from convex geometry, is a geometric version of the Fourier transform. We exploit this analogy to propose a new simple definition of quantum indeterminacy, using what we call "hbar-polar quantum pairs", which can be viewed as pairs of position-momentum indeterminacy with minimum spread. The existence of such pairs is guaranteed by the usual uncertainty principle, but is at the same time more general. We use recent advances in symplectic topology to show that this quantum indeterminacy can be measured using a particular symplectic capacity related to action and which reduces to area in the case of one degree of freedom. We show in addition that polar quantum pairs are closely related to Hardy's uncertainty principle about the localization of a function and its Fourier transform.
We propose a geometric formulation of quantum indeterminacy based on polar duality between convex bodies representing position and momentum data. A pair (X,P) of centrally symmetric convex bodies is said to satisfy the indeterminacy condition when the h-polar of X is included in P. We show that this condition naturally arises from the geometry of quantum blobs and is closely related to Hardy's uncertainty principle and the Donoho--Stark inequalities. Using symplectic capacities and John ellipsoids, we associate a canonical covariance ellipsoid with every quantum polar pair and prove that it satisfies the quantum condition. The Robertson--Schrödinger inequalities follow as a consequence. This provides a non-statistical formulation of quantum indeterminacy from which the usual uncertainty relations emerge. which the usual uncertainty relations emerge.
We replace the usual notion of quantum cell from statistical mechanics by that of "quantum blob". A quantum blob is the transform, by a linaer symplectic transformation, of a phase space ball with radius equal to the square root of h-bar. The intersection of a quantum blob with any symplectic plane is an ellipse with area one half of h. This very special property, which is closed related to the principle of the symplectic camel, leads to a symplectic invariant statement of the uncertainty principle. We moreover prove that the average of a phase space Gaussian over a quantum blob is the Wigner transform of a minimum uncertainty Gaussian.
We establish anisotropic uncertainty principles (UPs) for general metaplectic operators acting on
L2(Rd), including degenerate cases associated with symplectic matrices whose
B-block has nontrivial kernel. In this setting, uncertainty phenomena are shown to be intrinsically
directional and confined to an effective phase-space dimension given by
rank(B).
First, we prove sharp Heisenberg-Pauli-Weyl type inequalities involving only the directions
corresponding to
ker(B)⊥, with explicit lower bounds expressed in terms of geometric
quantities associated with the underlying symplectic transformation. We also provide a complete
characterization of all extremizers, which turn out to be partially Gaussian functions with free
behavior along the null directions of
B.
Building on this framework, we extend the Beurling-Hörmander theorem to the metaplectic
setting, obtaining a precise polynomial-Gaussian structure for functions satisfying suitable
exponential integrability conditions involving both
f and its metaplectic transform. Finally,
we prove a Morgan-type (or Gel'fand--Shilov type) uncertainty principle for metaplectic operators,
identifying a sharp threshold separating triviality from density of admissible functions and
showing that this threshold is invariant under metaplectic transformations.
Our results recover the classical Fourier case and free metaplectic transformations as special
instances, and reveal the geometric and anisotropic nature of uncertainty principles in the
presence of symplectic degeneracies.