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arXiv:1308.4029 · Physical Review A

Geometric formulation of the uncertainty principle

G. M. Bosyk, Tristán M. Osán, Pedro W. Lamberti, M. Portesi

Published Mar 10, 2014• 15 citations
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Abstract

A geometric approach to formulate the uncertainty principle between quantum observables acting on an $N$-dimensional Hilbert space is proposed. We consider the fidelity between a density operator associated with a quantum system and a projector associated with an observable, and interpret it as the probability of obtaining the outcome corresponding to that projector. We make use of fidelity-based metrics such as angle, Bures, and root infidelity to propose a measure of uncertainty. The triangle inequality allows us to derive a family of uncertainty relations. In the case of the angle metric, we recover the Landau-Pollak inequality for pure states and show, in a natural way, how to extend it to the case of mixed states in arbitrary dimension. In addition, we derive and compare alternative uncertainty relations when using other known fidelity-based metrics.

DOI
10.1103/physreva.89.034101

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A geometric approach to formulate the uncertainty principle between quantum observables acting on an NNN-dimensional Hilbert space is proposed. We consider the fidelity between a density operator associated with a quantum system and a projector associated with an observable, and interpret it as the probability of obtaining the outcome corresponding to that projector. We make use of fidelity-based metrics such as angle, Bures, and root infidelity to propose a measure of uncertainty. The triangle inequality allows us to derive a family of uncertainty relations. In the case of the angle metric, we recover the Landau-Pollak inequality for pure states and show, in a natural way, how to extend it to the case of mixed states in arbitrary dimension. In addition, we derive and compare alternative uncertainty relations when using other known fidelity-based metrics.
We provide a twofold extension of Landau-Pollak uncertainty relations for mixed quantum states and for positive operator-valued measures, by recourse to geometric considerations. The generalization is based on metrics between pure states, having the form of a function of the square of the inner product between the states. The triangle inequality satisfied by such metrics plays a crucial role in our derivation. The usual Landau-Pollak inequality is thus a particular case (derived from Wootters metric) of the family of inequalities obtained, and, moreover, we show that it is the most restrictive relation within the family.
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Quantum uncertainty, famously encapsulated by Heisenberg's principle, is a cornerstone of quantum mechanics, traditionally understood through the algebraic non-commutativity of observable operators. This paper proposes a novel framework: the commutator geometry of wavefunctions, aiming to unify diverse manifestations of quantum uncertainty within a single, intrinsic geometric description of the quantum state space. By establishing a direct link between the algebraic structure of commutators and the differential geometry of projective Hilbert space, we demonstrate how the inherent non-commutativity of observables fundamentally sculpts the geometry of quantum states. This approach allows for the derivation of geometric measures of uncertainty that intrinsically capture the limitations on simultaneous measurability. We show how this geometric formulation not only recovers existing uncertainty relations, such as the Robertson-Schroedinger inequality, but also provides a more profound, unified interpretation of quantum uncertainty as a manifestation of curvature and metric properties within the space of wavefunctions. The methodology involves constructing a commutator-induced metric and curvature tensor on the quantum state manifold, revealing how the degree of non-commutativity directly dictates the "fuzziness" or "spread" in observable values. Illustrative examples, including position-momentum and angular momentum, are used to demonstrate the efficacy and intuitive appeal of this geometric perspective. The implications of this unified geometric understanding extend to foundational issues in quantum mechanics, potentially offering new insights into quantum gravity, quantum information theory, and the very nature of quantum reality, where uncertainty is not merely a statistical limitation but an intrinsic geometric feature of the universe.
We propose a framework for the quantum geometry of expectation values over arbitrary sets of operators and establish a link between this geometry and the eigenstates of Hamiltonian families generated by these operators. We show that the boundary of expectation value space corresponds to the ground state, which presents a natural bound that generalizes Heisenberg's uncertainty principle. To demonstrate the versatility of our framework, we present several practical applications, including providing a stronger nonlinear quantum bound that violates the Bell inequality and an explicit construction of the density functional. Our approach provides an alternative time-independent quantum formulation that transforms the linear problem in a high-dimensional Hilbert space into a nonlinear algebro-geometric problem in a low dimension, enabling us to gain new insights into quantum systems.
Geometrical structures of quantum mechanics provide us with new insightful results about the nature of quantum theory. In this work we consider mixed quantum states represented by finite rank density operators. We review our geometrical framework that provide the space of density operators with Riemannian and symplectic structures, and we derive a geometric uncertainty relation for observables acting on mixed quantum states. We also give an example that visualizes the geometric uncertainty relation for spin-12\frac{1}{2}21​ particles.
Uncertainty principle is one of the cornerstones of quantum theory. In the literature, there are two types of uncertainty relations, the operator form concerning the variances of physical observables and the entropy form related to entropic quantities. Both these forms are inequalities involving pairwise observables, and are found to be nontrivial to incorporate multiple observables. In this work we introduce a new form of uncertainty relation which may give out complete trade-off relations for variances of observables in pure and mixed quantum systems. Unlike the prevailing uncertainty relations, which are either quantum state dependent or not directly measurable, our bounds for variances of observables are quantum state independent and immune from the "triviality" problem of having zero expectation values. Furthermore, the new uncertainty relation may provide a geometric explanation for the reason why there are limitations on the simultaneous determination of different observables in N-dimensional Hilbert space.