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arXiv:2608.00751 · International Journal of Theoretical Physics

Generalized Marginals of tie -Wigner Distribution nand Lagrangian Tomography

Maurice de Gosson

math-phmath.FAmath.SGquant-phSubmitted Aug 1, 2026• Announced Aug 4, 2026• 0 citations
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Abstract

We develop a symplectic formulation of the Lagrangian Radon transform based on the transitive action of the symplectic group on the Lagrangian Grassmannian. This geometric framework naturally extends the classical notion of the marginals of the Wigner transform, viewed as elementary tomograms, to arbitrary Lagrangian subspaces. The resulting generalized tomography provides a unified treatment of position and momentum measurements related by symplectic rotations. As applications, we revisit the Pauli reconstruction problem and establish reconstruction formulas for density operators from generalized Lagrangian tomograms.

AI Summary

The paper studies continuous-variable quantum-state reconstruction from integrals of Wigner distributions over affine Lagrangian subspaces. It formulates these tomograms using the compact symplectic subgroup $U(n)=\operatorname{Sp}(n)\cap O(2n)$ and its metaplectic representation, relating the geometry of integration planes to transformed position measurements. For a Lagrangian plane $\ell=\{(x,p):Ax+Bp=0\}$ represented by a symplectic rotation $U$, it derives $R_\ell W\psi(x,p)=|\widehat U\psi(Ax+Bp)|^2$. The argument uses symplectic covariance of the Wigner transform and its usual marginal identities; independence from the orthonormal parametrization of the plane is also established. An extension incorporating matrix rescalings is introduced, followed by a proposed inversion formula integrating over the tomographic coordinate and matrix parameters $A,B$. For centered pure Gaussian states, the paper discusses the ambiguity remaining after position and momentum measurements. In one mode, the undetermined covariance has two possible values, $\sigma_{xp}=\pm\sqrt{\sigma_{xx}\sigma_{pp}-\hbar^2/4}$. It then gives a reconstruction construction based on Bloch–Messiah diagonalization: a tomogram in a diagonalizing frame determines the squeezing eigenvalues. The stated limitation is that this frame must already be known, making the construction primarily theoretical rather than practical. Finally, the formalism is extended to mixed states through spectral decompositions and cross-Wigner distributions. Using the orthonormal-basis property of appropriately normalized cross-Wigner functions, the paper expresses tomograms in terms of density-operator coefficients and outlines coefficient-based reconstruction. No experimental data or numerical reconstruction study is presented.

Little sign of AI-generated textOverclaimsUnclear noveltyUnclear writingPossible error

Central claim may not hold: The general inversion proposition uses an undefined vector-valued phase and an invalid matrix Fourier–delta identity, while integrating beyond the domain on which its transform was defined. The proposed left normalization by Λ⁻¹ does not generally produce a symplectic rotation, so the extended transform's required metaplectic operator need not exist. The claim that two transverse Lagrangian tomograms determine a Gaussian is contradicted by distinct one-dimensional chirped Gaussians with identical position and momentum densities. The density-operator section reverses the Weyl-symbol/Wigner normalization in equation (symba), contradicting its kernel convention and trace formula. The final proposition incorrectly asserts that trace-class operators have absolutely summable matrix entries in arbitrary orthonormal bases, invalidating its stated convergence justification.

Written by gpt-6.1-sol from the paper's full text. Automated: it can be wrong.

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To appear in IJTP

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We develop a symplectic formulation of the Lagrangian Radon transform based on the transitive action of the symplectic group on the Lagrangian Grassmannian. This geometric framework naturally extends the classical notion of the marginals of the Wigner transform, viewed as elementary tomograms, to arbitrary Lagrangian subspaces. The resulting generalized tomography provides a unified treatment of position and momentum measurements related by symplectic rotations. As applications, we revisit the Pauli reconstruction problem and establish reconstruction formulas for density operators from generalized Lagrangian tomograms.
The paper studies continuous-variable quantum-state reconstruction from integrals of Wigner distributions over affine Lagrangian subspaces. It formulates these tomograms using the compact symplectic subgroup U(n)=Sp⁡(n)∩O(2n)U(n)=\operatorname{Sp}(n)\cap O(2n)U(n)=Sp(n)∩O(2n) and its metaplectic representation, relating the geometry of integration planes to transformed position measurements.
For a Lagrangian plane ℓ={(x,p):Ax+Bp=0}\ell=\{(x,p):Ax+Bp=0\}ℓ={(x,p):Ax+Bp=0} represented by a symplectic rotation UUU, it derives RℓWψ(x,p)=∣U^ψ(Ax+Bp)∣2R_\ell W\psi(x,p)=|\widehat U\psi(Ax+Bp)|^2Rℓ​Wψ(x,p)=∣Uψ(Ax+Bp)∣2. The argument uses symplectic covariance of the Wigner transform and its usual marginal identities; independence from the orthonormal parametrization of the plane is also established. An extension incorporating matrix rescalings is introduced, followed by a proposed inversion formula integrating over the tomographic coordinate and matrix parameters A,BA,BA,B.
For centered pure Gaussian states, the paper discusses the ambiguity remaining after position and momentum measurements. In one mode, the undetermined covariance has two possible values, σxp=±σxxσpp−ℏ2/4\sigma_{xp}=\pm\sqrt{\sigma_{xx}\sigma_{pp}-\hbar^2/4}σxp​=±σxx​σpp​−ℏ2/4​. It then gives a reconstruction construction based on Bloch–Messiah diagonalization: a tomogram in a diagonalizing frame determines the squeezing eigenvalues. The stated limitation is that this frame must already be known, making the construction primarily theoretical rather than practical.
Finally, the formalism is extended to mixed states through spectral decompositions and cross-Wigner distributions. Using the orthonormal-basis property of appropriately normalized cross-Wigner functions, the paper expresses tomograms in terms of density-operator coefficients and outlines coefficient-based reconstruction. No experimental data or numerical reconstruction study is presented.
Quasiprobability measures on a canonical phase space give rise through the action of Weyl's quantization map to operator-valued measures and, in particular, to region operators. Spectral properties, transformations, and general construction methods of such operators are investigated. Geometric trace-increasing maps of density operators are introduced for the construction of region operators associated with one-dimensional domains, as well as with two-dimensional shapes (segments, canonical polygons, lattices, etc.). Operational methods are developed that implement such maps in terms of unitary operations by introducing extensions of the original quantum system with ancillary spaces (qubits). Tomographic methods of reconstruction of the Wigner function based on the radon transform technique are derived by the construction methods for region operators. A Hamiltonian realization of the region operator associated with the radon transform is provided, together with physical interpretations.
We study a generalization of the Wigner function to arbitrary tuples of hermitian operators. We show that for any collection of hermitian operators A1...An , and any quantum state there is a unique joint distribution on R^n, with the property that the marginals of all linear combinations of the operators coincide with their quantum counterpart. In other words, we consider the inverse Radon transform of the exact quantum probability distributions of all linear combinations. We call it the Wigner distribution, because for position and momentum this property defines the standard Wigner function. We discuss the application to finite dimensional systems, establish many basic properties and illustrate these by examples. The properties include the support, the location of singularities, positivity, the behavior under symmetry groups, and informational completeness.
We study a generalization of the Wigner function to arbitrary tuples of Hermitian operators. We show that for any collection of Hermitian operators A1, …, An and any quantum state, there is a unique joint distribution on Rn with the property that the marginals of all linear combinations of the Ak coincide with their quantum counterparts. In other words, we consider the inverse Radon transform of the exact quantum probability distributions of all linear combinations. We call it the Wigner distribution because for position and momentum, this property defines the standard Wigner function. We discuss the application to finite dimensional systems, establish many basic properties, and illustrate these by examples. The properties include the support, the location of singularities, positivity, the behavior under symmetry groups, and informational completeness.
Some non-linear generalizations of classical Radon tomography were recently introduced by M. Asorey et al [Phys. Rev. A 77, 042115 (2008), where the straight lines of the standard Radon map are replaced by quadratic curves (ellipses, hyperbolas, circles) or quadratic surfaces (ellipsoids, hyperboloids, spheres). We consider here the quantum version of this novel non-linear approach and obtain, by systematic use of the Weyl map, a tomographic encoding approach to quantum states. Non-linear quantum tomograms admit a simple formulation within the framework of the star-product quantization scheme and the reconstruction formulae of the density operators are explicitly given in a closed form, with an explicit construction of quantizers and dequantizers. The role of symmetry groups behind the generalized tomographic maps is analyzed in some detail. We also introduce new generalizations of the standard singular dequantizers of the symplectic tomographic schemes, where the Dirac delta-distributions of operator-valued arguments are replaced by smooth window functions, giving rise to the new concept of "thick" quantum tomography. Applications for quantum state measurements of photons and matter waves are discussed.
The two-dimensional Radon transform of the Wigner quasiprobability is introduced in canonical form and the functions playing a role in its inversion are discussed. The transformation properties of this Radon transform with respect to displacement and squeezing of states are studied and it is shown that the latter is equivalent to a symplectic transformation of the variables of the Radon transform with the contragredient matrix to the transformation of the variables in the Wigner quasiprobability. The reconstruction of the density operator from the Radon transform and the direct reconstruction of its Fock-state matrix elements and of its normally ordered moments are discussed. It is found that for finite-order moments the integration over the angle can be reduced to a finite sum over a discrete set of angles. The reconstruction of the Fock-state matrix elements from the normally ordered moments leads to a new representation of the pattern functions by convergent series over even or odd Hermite polynomials which is appropriate for practical calculations. The structure of the pattern functions as first derivatives of the products of normalizable and non-normalizable eigenfunctions to the number operator is considered from the point of view of this new representation.