aiqbench analysis
This paper derives the Kijowski time-of-arrival POVM by minimizing modifications to the Schrödinger current to eliminate negative probability flows, offering a rigorous physical justification for its unique kernel structure. The analysis demonstrates that enforcing non-negativity on states with single-sign momentum support naturally separates directional contributions while preserving individual momentum components. This work advances fundamental quantum measurement theory without relying on external first-arrival conditions or imposing arbitrary constraints.
Deriving the Kijowski Arrival-Time POVM from the Schr\"odinger Current: Minimal Positivity and Uniqueness
arXiv:2609.08458v1 Announce Type: new Abstract: Quantum backflow refers here to the appearance of a negative Schr\"odinger current for a state whose momentum support is entirely positive. We ask for the smallest modification of the free Schr\"odinger current that makes it nonnegative for every such state, while preserving the current of each individual momentum component. We show that the required minimal modification changes the free-particle momentum kernel according to \[ K_{\rm Sch}(p,p')=\frac{p+p'}{2m} \;\longrightarrow\; K_{\min}(p,p')=\frac{\sqrt{pp'}}{m}. \] The resulting current is positive and normalized and therefore defines an arrival-time POVM. Extending the directional no-backflow requirement to states containing both momentum signs forces the cross-sector kernel to vanish, \[ K_{\min}^{+-}=K_{\min}^{-+}=0, \] so that the full current is the sum of two independent directional contributions. The resulting POVM is exactly the Kijowski time-of-arrival POVM, providing a current-based physical motivation for both its directional kernels and their separation. Within the diagonal-preserving pairwise-minimal construction considered here, the result is unique. The construction itself does not impose a first-arrival condition.
Abstract:Quantum backflow refers here to the appearance of a negative Schrödinger current for a state whose momentum support is entirely positive. We ask for the smallest modification of the free Schrödinger current that makes it nonnegative for every such state, while preserving the current of each individual momentum component. We show that the required minimal modification changes the free-particle momentum kernel according to \[ K_{\rm Sch}(p,p')=\frac{p+p'}{2m} \;\longrightarrow\; K_{\min}(p,p')=\frac{\sqrt{pp'}}{m}. \] The resulting current is positive and normalized and therefore defines an arrival-time POVM. Extending the directional no-backflow requirement to states containing both momentum signs forces the cross-sector kernel to vanish, \[ K_{\min}^{+-}=K_{\min}^{-+}=0, \] so that the full current is the sum of two independent directional contributions. The resulting POVM is exactly the Kijowski time-of-arrival POVM, providing a current-based physical motivation for both its directional kernels and their separation. Within the diagonal-preserving pairwise-minimal construction considered here, the result is unique. The construction itself does not impose a first-arrival condition.
arXiv:2609.08458 [quant-ph]
(or arXiv:2609.08458v1 [quant-ph] for this version)
https://doi.org/10.48550/arXiv.2609.08458 Focus to learn more arXiv-issued DOI via DataCite (pending registration)
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