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Eigenvalues and Eigenvectors for a Hermitian Gaussian Operator: Role of the Schrödinger-Robertson Uncertainty Relation

Robert F. Snider

Published Nov 7, 2022• 0 citations
Publisher
DOI
10.37247/paam3ed.3.23.11

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Eigenvalues and eigenvectors for a hermitian gaussian operator: Role of the Schrödinger-Robertson uncertainty relation

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The eigenvalues and eigenvectors of a normalized gaussian operator do not seem to have been previously considered. I solve this problem for 1-dimensional translational systems. I also address the question as to whether a gaussian operator is a density operator. To answer that question, it is first necessary to be sure what conditions must be satisfied, so a short review of density operators is given. Since position and momentum do not commute in quantum mechanics, it is useful to start with the consequences of the noncommutation, which is generally the Schrödinger-Robertson uncertainty relation, which is also briefly reviewed. It is found that the question of whether a gaussian operator is a density operator is directly tied to this uncertainty relation. Since the Wigner function is the phase space representation of a translational density operator, it is natural to consider the gaussian phase space function associated with a gaussian operator and to compare the phase space and operator properties. Throughout such discussions, the independent parameters in these functions are the first and second moments of position and momentum. The application of this formalism to the free translation and spreading of a gaussian packet is given and shows the formal similarity between classical and quantum behavior, whereas the literature standardly only considers the pure state case (equivalent to a single wavefunction).

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The historical development of uncertainty relation, begining with first Heisenberg's thoughts of uncertainty principle is summed up in this thesis. After proving validity of Schwarz inequality general uncertainty relation for two hermitian operators is obtained, and from this general version the validity of Heisenberg uncertainty relation is than proved. The most important part of this work is the obtention of two new uncertainty relations, which are stronger then Heisenberg or Robertson-Schrödinger uncertainty relation, and their specific form for two examples - a free particle in a state discribed by the gaussian wave packet and the linear harmonic oscillator with a wave function in the shape of gaussian packet.

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The Robertson--Schrödinger Uncertainty Remainder as a Dirichlet--Neumann-Type Compatibility Deficit

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This preprint introduces an exact Hilbert-space decomposition of the Robertson--Schrödinger uncertainty relation into a canonical quantum minimum, a covariance contribution, and a non-negative orthogonal remainder. The remainder, denoted R_DN[ψ], is interpreted as a Dirichlet--Neumann-type compatibility deficit between the position and momentum fluctuation vectors. The work does not introduce a new uncertainty principle. Rather, it gives a geometric interpretation of the Robertson--Schrödinger saturation condition: the deficit vanishes precisely when the momentum fluctuation vector is a complex scalar multiple of the position fluctuation vector. This characterizes Robertson--Schrödinger-saturating Gaussian states, possibly with a quadratic phase. The approach is motivated by the Hamilton--Jacobi relation between coordinate-type and momentum-type boundary data. Examples involving an uncorrelated Gaussian state, a quadratic-phase Gaussian state, and a Fock state illustrate the role of the deficit.

•May 11, 2026•0 citations
The eigenvalues and eigenvectors of a normalized gaussian operator do not seem to have been previously considered. I solve this problem for 1-dimensional translational systems. I also address the question as to whether a gaussian operator is a density operator. To answer that question, it is first necessary to be sure what conditions must be satisfied, so a short review of density operators is given. Since position and momentum do not commute in quantum mechanics, it is useful to start with the consequences of the noncommutation, which is generally the Schrödinger-Robertson uncertainty relation, which is also briefly reviewed. It is found that the question of whether a gaussian operator is a density operator is directly tied to this uncertainty relation. Since the Wigner function is the phase space representation of a translational density operator, it is natural to consider the gaussian phase space function associated with a gaussian operator and to compare the phase space and operator properties. Throughout such discussions, the independent parameters in these functions are the first and second moments of position and momentum. The application of this formalism to the free translation and spreading of a gaussian packet is given and shows the formal similarity between classical and quantum behavior, whereas the literature standardly only considers the pure state case (equivalent to a single wavefunction).
The historical development of uncertainty relation, begining with first Heisenberg's thoughts of uncertainty principle is summed up in this thesis. After proving validity of Schwarz inequality general uncertainty relation for two hermitian operators is obtained, and from this general version the validity of Heisenberg uncertainty relation is than proved. The most important part of this work is the obtention of two new uncertainty relations, which are stronger then Heisenberg or Robertson-Schrödinger uncertainty relation, and their specific form for two examples - a free particle in a state discribed by the gaussian wave packet and the linear harmonic oscillator with a wave function in the shape of gaussian packet.
This preprint introduces an exact Hilbert-space decomposition of the Robertson--Schrödinger uncertainty relation into a canonical quantum minimum, a covariance contribution, and a non-negative orthogonal remainder. The remainder, denoted R_DN[ψ], is interpreted as a Dirichlet--Neumann-type compatibility deficit between the position and momentum fluctuation vectors. The work does not introduce a new uncertainty principle. Rather, it gives a geometric interpretation of the Robertson--Schrödinger saturation condition: the deficit vanishes precisely when the momentum fluctuation vector is a complex scalar multiple of the position fluctuation vector. This characterizes Robertson--Schrödinger-saturating Gaussian states, possibly with a quadratic phase. The approach is motivated by the Hamilton--Jacobi relation between coordinate-type and momentum-type boundary data. Examples involving an uncorrelated Gaussian state, a quadratic-phase Gaussian state, and a Fock state illustrate the role of the deficit.