Alberto Levrero
Istituto Nazionale di Fisica Nucleare
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Featured researches published by Alberto Levrero.
Reviews in Mathematical Physics | 1998
Paolo Aniello; Gianni Cassinelli; Ernesto De Vito; Alberto Levrero
We consider a semidirect product G=A×′H, with A abelian, and its unitary representations of the form where x0 is in the dual group of A, G0 is the stability group of x0 and m is an irreducible unitary representation of G0∩H. We give a new selfcontained proof of the following result: the induced representation is square-integrable if and only if the orbit G[x0] has nonzero Haar measure and m is square-integrable. Moreover we give an explicit form for the formal degree of .
Journal of Mathematical Physics | 2000
Gianni Cassinelli; Giacomo Mauro D’Ariano; E. De Vito; Alberto Levrero
The paper is devoted to the mathematical foundation of quantum tomography using the theory of square-integrable representations of unimodular Lie groups.
Foundations of Physics | 2000
Gianni Cassinelli; E. De Vito; Pekka Lahti; Alberto Levrero
Using a recent result of Busch and Gudder, we reconsider a theorem of Ludwig which allows one to identify a class of effect automorphisms as the symmetry transformations in quantum mechanics.
Journal of Mathematical Physics | 1998
Paolo Aniello; Gianni Cassinelli; Ernesto De Vito; Alberto Levrero
We consider a semidirect product G=Rn×′H and its unitary representations U of the form IndG0G(p0m) where Ind is the unitary induction, p0 is in the dual group of Rn, G0 is the stability group of p0, and m is a unitary representation of G0∩H. We give sufficient conditions such that U defines a wavelet transform and a discrete frame.
Journal of Fourier Analysis and Applications | 2001
Paolo Aniello; Gianni Cassinelli; Ernesto De Vito; Alberto Levrero
For groups which are the semidirect product of some vector group with a unimodular group we prove that the existence of a discrete frame obtained from an at-most countable set of vectors through the action of a given unitary representation implies that the representation in use has to be square-integrable.
Journal of Mathematical Physics | 2000
Gianni Cassinelli; Ernesto De Vito; Pekka Lahti; Alberto Levrero
We give necessary and sufficient conditions for the set of Neumark projections of a countable set of phase space observables to constitute a resolution of the identity, and we give a criteria for a phase space observable to be informationally complete. The results will be applied to the phase space observables arising from an irreducible representation of the Heisenberg group.
Reviews in Mathematical Physics | 1998
Gianni Cassinelli; Ernesto De Vito; Pekka Lahti; Alberto Levrero
The homomorphisms of a connected Lie group G into the symmetry group of a quantum system are classified in terms of unitary representations of a simply connected Lie group associated with G. Moreover, an explicit description of the T-multipliers of G is obtained in terms of the ℝ-multipliers of the universal covering G* of G and the characters of G*. As an application, the Poincare group and the Galilei group, both in 3+1 and 2+1 dimensions, are considered.
Journal of Mathematical Physics | 1999
Paolo Aniello; Gianni Cassinelli; Ernesto De Vito; Alberto Levrero
Let (P,V) be an irreducible imprimitivity system for a group H based on a dual group  of an Abelian group A and acting on a Hilbert space H. Given ψ∈H, we find necessary and sufficient conditions in order that the set of vectors {∫Â〈â,a〉¯Vh−1 dP(â)ψ : a∈A, h∈H} be a frame in H. Moreover, we apply these results to some examples that are considered in the literature in the context of square-integrability modulo a coset space.
Journal of Mathematical Physics | 2000
Gianni Cassinelli; E. De Vito; Alberto Levrero
We give a definition of square-integrability for imprimitivity systems and we prove that the square-integrable ones share most of the properties of square-integrable representations of groups.
Journal of Mathematical Physics | 1997
Gianni Cassinelli; E. De Vito; Alberto Levrero
We show that the cyclic adiabatic evolution of a quantum system is completely integrable as a classical Hamiltonian system. In this context the Berry phases arise naturally as cohomology of the invariant tori.