Confidence uncertainty: position and momentum can be jointly determined with a guaranteed probability
Pith reviewed 2026-05-08 17:57 UTC · model grok-4.3
The pith
Position and momentum can be jointly localized to arbitrarily small regions with probability at least 50 percent when their target probabilities sum to one or less.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
We define the confidence uncertainty Δ^c x(θ_x) as the smallest Lebesgue measure of any measurable set whose probability content is at least θ_x, and the interval version Δ^I x(θ_x) as the shortest single interval with the same property. For θ_x + θ_p ≤ 1 we prove that both quantities can be made arbitrarily small simultaneously, so the product has infimum zero over all states. For θ_x + θ_p > 1 we obtain the lower bound Δ^c x Δ^c p ≥ 2πℏ (√(θ_x θ_p) − √((1−θ_x)(1−θ_p)) )² by combining Lenard’s projection inequality with the Donoho–Stark operator-norm bound, together with the sharp implicit Landau–Pollak bound for the interval version that involves the largest prolate-spheroidal eigenvalue.
What carries the argument
Confidence uncertainty, defined as the minimal Lebesgue measure of a set (or single interval) that contains probability at least θ.
Load-bearing premise
That the minimal Lebesgue measure of a high-probability set is the right way to quantify how well position and momentum can be jointly determined.
What would settle it
A concrete calculation or measurement showing that, for θ_x = θ_p = 0.5, the product of minimal position and momentum support sizes remains bounded below by a positive number for every quantum state.
Figures
read the original abstract
Heisenberg's uncertainty principle states that the position and momentum of a particle cannot be sharply determined simultaneously. Standard-deviation and entropic formulations capture the spread of the probability distribution but say little about the probability itself contained in a small region. We introduce the "confidence uncertainty" $\Delta^{c}x(\theta_x)$ as the minimal Lebesgue measure of the support set in which the particle is found with probability at least $\theta_x$, and the companion "interval confidence uncertainty" $\Delta^{I}x(\theta_x)$ which restricts the support to a single interval. We prove two complementary uncertainty inequalities. (i) For $\theta_x+\theta_p\le 1$ both confidence uncertainties can be made arbitrarily small simultaneously, so that no nontrivial product bound holds; in particular, position and momentum can be jointly localised with probability at least~$50\%$. (ii) For $\theta_x+\theta_p>1$ a lower bound holds: combining Lenard's projection inequality with the Donoho--Stark operator-norm bound we obtain $\Delta^{c}x\,\Delta^{c}p\geq 2\pi\hbar\bigl(\sqrt{\theta_x\theta_p}-\sqrt{(1-\theta_x)(1-\theta_p)}\bigr)^{\!2}$, and for the interval version we obtain the sharp implicit Landau--Pollak bound $\Delta^{I}x\,\Delta^{I}p\geq 4\hbar\,\lambda_{0}^{-1}\!\bigl((\sqrt{\theta_x\theta_p}-\sqrt{(1-\theta_x)(1-\theta_p)})^{2}\bigr)$, where $\lambda_{0}(c)$ is the largest prolate-spheroidal eigenvalue. We support the analytical bounds with numerical evaluation of $\lambda_{0}(c)$, provide closed-form small-$c$ and large-$c$ asymptotics, compute the optimal Slepian-superposition states that saturate the interval bound, and compare the resulting product against the variance Heisenberg--Kennard, the Bia\l{}ynicki-Birula--Mycielski entropic, and the Donoho--Stark concentration bounds.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript introduces confidence uncertainty Δ^c x(θ_x) as the minimal Lebesgue measure of a set containing probability at least θ_x, and the interval-restricted version Δ^I x(θ_x). It proves two complementary results: for θ_x + θ_p ≤ 1 both can be made arbitrarily small simultaneously (no nontrivial product bound, allowing joint localization with probability ≥50%), while for θ_x + θ_p >1 it derives product lower bounds by combining Lenard's projection inequality with the Donoho-Stark operator-norm bound, yielding Δ^c x Δ^c p ≥ 2πℏ (√(θ_x θ_p) - √((1-θ_x)(1-θ_p)))^2, and a sharp implicit Landau-Pollak bound for the interval case involving the largest prolate-spheroidal eigenvalue λ_0(c). The analytical results are supported by numerical evaluation of λ_0(c), small-c and large-c asymptotics, explicit Slepian-superposition states that saturate the interval bound, and comparisons to the variance Heisenberg-Kennard, entropic Bia lynicki-Birula-Mycielski, and Donoho-Stark bounds.
Significance. If the results hold, the work offers a probability-centric reformulation of joint localization that complements spread-based and entropic uncertainty principles. The demonstration that Δ^c x and Δ^c p (and interval versions) can be simultaneously small for θ_x + θ_p ≤1 is a clear, falsifiable statement with direct implications for quantum mechanics interpretations and applications requiring guaranteed localization probabilities. Credit is given for the parameter-free derivations obtained by direct combination of three external inequalities (Lenard, Donoho-Stark, Landau-Pollak) without internal circularity, the explicit construction of saturating states, closed-form asymptotics, and the numerical evaluation of λ_0(c) with comparisons that situate the new measures relative to existing bounds.
minor comments (2)
- [Abstract] Abstract: the mention of 'numerical evaluation of λ_0(c) and comparison plots' would be strengthened by a brief note on whether error bars or full reproducibility data are provided in the main text or supplement.
- [Introduction] §1 (Introduction): the choice of Lebesgue measure for support size is presented as natural, but a short explicit comparison to alternative quantifiers (e.g., other norms or entropic supports) would address potential reader questions about the definition's uniqueness.
Simulated Author's Rebuttal
We thank the referee for their thorough summary of the manuscript and for recommending acceptance. We appreciate the recognition of the parameter-free derivations, the explicit saturating states, and the comparisons to existing uncertainty principles.
Circularity Check
No significant circularity detected
full rationale
The derivation begins with explicit new definitions of the confidence uncertainties Δ^c x(θ_x) and Δ^I x(θ_x) as minimal measures of sets carrying probability at least θ_x. The two main inequalities are then obtained by direct application of three independent external theorems (Lenard projection inequality, Donoho–Stark operator-norm bound, and Landau–Pollak prolate-spheroidal eigenvalue bound) whose statements contain no reference to the new quantities. For the regime θ_x + θ_p ≤ 1 the lower-bound expression evaluates to a non-positive number, which immediately implies that no nontrivial product bound exists; this is a straightforward algebraic consequence rather than a self-referential step. No self-citations appear as load-bearing premises, no parameters are fitted and then relabeled as predictions, and no ansatz is imported via prior work by the same authors. The entire chain therefore remains self-contained against external benchmarks.
Axiom & Free-Parameter Ledger
axioms (2)
- domain assumption Lebesgue measure on R is the appropriate size for support sets of wave functions
- standard math Lenard's projection inequality, Donoho-Stark operator-norm bound, and Landau-Pollak inequality hold for the relevant operators
invented entities (2)
-
confidence uncertainty Δ^c x(θ_x)
no independent evidence
-
interval confidence uncertainty Δ^I x(θ_x)
no independent evidence
Lean theorems connected to this paper
-
Cost.FunctionalEquation (J = ½(x+x⁻¹)−1)washburn_uniqueness_aczel unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
Δ^c x · Δ^c p ≥ 2πℏ (√(θ_x θ_p) − √((1−θ_x)(1−θ_p)))²
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Reference graph
Works this paper leans on
-
[1]
We compute it on[−1,1] by the same Gauss–Legendre discretisation that supplied λ0(c), and exhibit its position density together with the 5 0.0 0.2 0.4 0.6 0.8 1.0 x 0.0 0.2 0.4 0.6 0.8 1.0p trivial: x + p 1 Tight Landau--Pollak bound on Ix Ip/ 1 2 4 6 8 0.0 2.5 5.0 7.5 10.0 12.5 15.0 17.5 20.0 lower bound on Ix Ip/ FIG. 4. Numerical landscape of the tight...
-
[2]
Heisenberg, Zeitschrift für Physik43, 172 (1927)
W. Heisenberg, Zeitschrift für Physik43, 172 (1927)
work page 1927
-
[3]
E. H. Kennard, Zeitschrift für Physik44, 326 (1927)
work page 1927
-
[4]
H. P. Robertson, Phys. Rev.34, 163 (1929)
work page 1929
-
[5]
E. Schrödinger, Sitzungsber. Preuss. Akad. Wiss., Phys. Math. Kl.19, 296 (1930)
work page 1930
- [6]
-
[7]
H. F. Hofmann and S. Takeuchi, Phys. Rev. A68, 032103 (2003)
work page 2003
- [8]
-
[9]
J.-L. Li, K. Du, and C.-F. Qiao, J. Phys. A47, 085302 (2014)
work page 2014
-
[10]
Y.-M. Park, J. Math. Phys.46, 042109 (2005)
work page 2005
- [11]
- [12]
-
[13]
I. I. Hirschman, Am. J. Math.79, 152 (1957)
work page 1957
- [14]
-
[15]
I. Białynicki-Birula and J. Mycielski, Commun. Math. Phys.44, 129 (1975)
work page 1975
- [16]
- [17]
-
[18]
P. J. Coles, M. Berta, M. Tomamichel, and S. Wehner, Rev. Mod. Phys.89, 015002 (2017)
work page 2017
- [19]
- [20]
-
[21]
A. Rényi, in Proc. Fourth Berkeley Symp. Math. Stat. Prob., Vol. 1 (University of California Press, 1961) pp. 547–561
work page 1961
-
[22]
V.V.DodonovandA.V.Dodonov, Phys.Scr.90, 074049 (2015)
work page 2015
-
[23]
A. E. Rastegin, Ann. Phys.531, 1800466 (2019)
work page 2019
-
[24]
D. T. Pegg, Phys. Rev. A58, 4307 (1998)
work page 1998
- [25]
-
[26]
H. J. Landau and H. O. Pollak, Bell Syst. Tech. J.40, 65 (1961)
work page 1961
-
[27]
H. J. Landau and H. O. Pollak, Bell Syst. Tech. J.41, 1295 (1962)
work page 1962
- [28]
-
[29]
D. L. Donoho and P. B. Stark, SIAM J. Appl. Math.49, 906 (1989)
work page 1989
- [30]
-
[31]
G. B. Folland and A. Sitaram, J. Fourier Anal. Appl.3, 207 (1997)
work page 1997
-
[32]
Nazarov, Algebra i Analiz5, 3 (1993), translation in St
F. Nazarov, Algebra i Analiz5, 3 (1993), translation in St. Petersburg Math. J.5(1994), 663–717
work page 1993
-
[33]
A. Osipov and V. Rokhlin, Appl. Comput. Harmon. Anal.36, 108 (2014). Appendix A: Proof of Theorem 2 LetX, P⊆Rbe measurable sets,|X|<∞,|P|< ∞. WriteP X for the multiplication operatorf(x)7→ 1X(x)f(x)onL 2(R), andQ P =F −11P Ffor the cor- responding spectral projection in momentum, with the Fourier transformFψ(p) = (2πℏ) −1/2R e−ipx/ℏψ(x) dx. The kernel ofP...
work page 2014
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.