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Metadata
slug: cotfas-2026-uncertainty-condition-conjecture
bibkey: cotfas2026dvgs
doi: 10.48550/arXiv.2610.05623
url: https://arxiv.org/abs/2610.05623v1
triage: theorem
motivation_gids:
  - D5/S3/Quantum/CotfasDVGS.result

The uncertainty condition suffices for the mixed discrete Gaussian

Problem

Nicolae Cotfas, Frame-dependent coherence of Gaussian quantum states, arXiv:2610.05623v1, asks after Eq. (22): “As concern ρ̃_σ, we do not know if (11) is sufficient in order to have ρ̃_σ ≥ 0. Based on our numerical investigations, we conjecture that this is true.”

Preregistration #18946 fixes the source formulas and quantifiers. The source note gives the locators and verbatim statements. The settlement is Proved by D5.S3.Quantum.CotfasDVGS.result.

Statement echo

Source clauseLean counterpartFidelity
Eq. (10), continuous Wigner GaussianW, real inverse covariance and determinantLiteral formula
Odd dimension Natural with in claimSame range
Functions on ; addition modulo Integer Finset.Icc subtype; ZMod.valMinAbsCentered modular representative
Eq. (18), displaced parityparity, coefficient in row , column Same phase and selected column
Eq. (22), signed double lattice sumwSum, tsum over Real division in both coordinates; scalar normalization separated
Eq. (21), weighted finite parity sumunnormalizedBoth sums use the centered indices
is a normalizing constantrhoTilde, inverse complex trace times unnormalizedThe proof establishes a nonzero trace
Positive Planck parameter, Universal quantifier
Real symmetric positive-definite covarianceReal two-by-two Matrix.PosDefSymmetry follows from this predicate
Eq. (11), The literal complex matrix in claimNo certificate replaces the condition
Conjectured positivityresult: claim, including positive semidefinitenessExact family
Density normalizationTrace equals one in claimConsequence of the source normalization; strengthens positivity

The public surface comprises W, parity, wSum, unnormalized, rhoTilde, claim and result. All other authored declarations are private and have consumers inside this settlement. The centered index type and density conjunction occur literally in the claim; the proof uses existing covariance and density predicates.

Motivation

A trace-normalized mixed discrete-variable Gaussian can serve as a quantum state when it is positive semidefinite. The theorem supplies that density-operator premise for the exact family in Eqs. (21)–(22), including the determinant-one boundary. It establishes no separate result about coherence quantities or other conclusions of the paper.

Gap

The source states the sufficiency question explicitly. The literature screen recorded in #18946 covers arXiv:2610.05623v1, the predecessor arXiv:2204.07042v4, INSPIRE citing-work abstracts, indexed MathDB searches and the formal-conjectures snapshot named there. It found no settlement in that scope. Direct MathDB access returned HTTP 403; Feng–Luo, International Journal of Theoretical Physics 63, 40 (2024), has a subscription-only main text in which an equivalent result has not been excluded. Literature completeness is ASSUMED-UNVERIFIED.

Route

Write , and . The consumed covariance result GaussianThermometryJointMeasurementRefutation.physical_data gives from the uncertainty condition. rhoTilde_scaling reduces the Planck parameter to .

The private kernel_identity identifies the unnormalized matrix with twice the integer periodization of

The private half_lattice_poisson applies Mathlib’s Complex.tsum_exp_neg_quadratic. The reindexing and Gaussian summability arguments justify the exact signed Wigner construction. kernel_factorization writes , where . The consumed FiniteGaussianSchoenberg.gram_gaussian_posSemidef and the Schur product give finite kernel positivity; closedness gives periodized positivity.

The private kernel_residual_posSemidef subtracts a rank-one kernel while preserving positivity. theta_nonzero proves upper-half-plane theta nonvanishing by duplication and an eventual small-tail bound. It yields strongWave_zero_sum_ne_zero, and hence periodized_kernel_zero_diagonal_pos. A positive diagonal entry excludes zero trace. normalization_isDensity uses GHZMeasureBiseparableBound.IsDensity to complete the density conjunction.

Falsifier

A covariance satisfying the literal uncertainty condition whose exact infinite-sum matrix has a negative quadratic form or zero trace would contradict the statement. Replacing the signed lattice sum, reversing the parity coefficient convention, or asserting convergence from a finite truncation would change the problem. The Lean result uses the exact formulas and infinite sums.

Evidence

The mathematical source is CotfasDVGS.lean, with its Blueprint. The settling GID is D5/S3/Quantum/CotfasDVGS.result; its admission basis is open-problem-resolution (#18946; Proved), generality is I, and utility is none. No fixed-parameter numerical certificate is part of the module. The axiom closure of every public declaration is contained in {propext, Classical.choice, Quot.sound}.

The escape audit for D5.S3.Quantum.CotfasDVGS.result is unfinished: #19812. A faithful dependent-family registration lacks a compiled source-reconstruction equivalence bridge, intervention and dependence proofs, and current binding evidence. No Reg mirror or declared_validated registration is delivered.

Declaration classification

The classification expands same-delivery helpers and stops at pinned upstream and existing frozen owners. theta_nonzero supplies the nonvanishing argument on the live path through strongWave_zero_sum_ne_zero and periodized_kernel_zero_diagonal_pos to result. Dependency identities and direct consumers are extracted from compiled proof terms and the scoped Lean report.

moduledeclarationproof_shapeescape_witnessconsumersdirect frozen dependencies
D5/S3/Quantum/CotfasDVGSD5.S3.Quantum.CotfasDVGS.result (sha256:76e6c7d115fcc90748ee7baeb5a85a1ba9c04094d72192d23281e83188ec404c)contentD5.S3.Quantum.CotfasDVGS.theta_nonzerosettlementD5/S3/Estimation/GaussianThermometryJointMeasurementRefutation + D5.S3.Estimation.GaussianThermometryJointMeasurementRefutation.IsGaussianMeasurementCov + sha256:410391e348afb0d9876bdf2548ca1782f14191e2ac259dd3c3d81d1876de06a4
D5/S3/Estimation/GaussianThermometryJointMeasurementRefutation + D5.S3.Estimation.GaussianThermometryJointMeasurementRefutation.physical_data + sha256:5cca2636075e308d2c7601cbf4eec201deeff36ae84f87cba8d1efbc1a1c4ec9
D5/S3/Estimation/GaussianThermometryJointMeasurementRefutation + D5.S3.Estimation.GaussianThermometryJointMeasurementRefutation.thermalCov._proof_1 + sha256:83f1ceeb429672fc69ed7b05221717bed36bfc3d20bfbfaf29d42aff28260770
D5/S3/Quantum/Entanglement/GHZMeasureBiseparableBound + D5.S3.Quantum.Entanglement.GHZMeasureBiseparableBound.IsDensity + sha256:fc9bb0824d5818ff419f72f26095faecc04e62ab59bf26f4f2bcefbb2d380448
D5/S3/Weil/Probability/FiniteGaussianSchoenberg + D5.S3.Weil.Probability.FiniteGaussianSchoenberg.gram_gaussian_posSemidef + sha256:e83ee5619019d4fc81d7390a8b36152737f3dda0b497486e0e5fc9c97d9a1c91
helper (full Lean name)proof_shapeescape_witnessdirect consumers
D5.S3.Quantum.CotfasDVGS.Wbind-onlynoneD5.S3.Quantum.CotfasDVGS.W_coordinates, D5.S3.Quantum.CotfasDVGS.W_gaussian_bound, D5.S3.Quantum.CotfasDVGS.W_nonnegative, D5.S3.Quantum.CotfasDVGS.W_scaling, D5.S3.Quantum.CotfasDVGS.entry_half_lattice, D5.S3.Quantum.CotfasDVGS.kernel_fourier_slice, D5.S3.Quantum.CotfasDVGS.kernel_identity, D5.S3.Quantum.CotfasDVGS.signed_W_lattice_summable, D5.S3.Quantum.CotfasDVGS.wSum, D5.S3.Quantum.CotfasDVGS.wSum_scaling
D5.S3.Quantum.CotfasDVGS.paritybind-onlynoneD5.S3.Quantum.CotfasDVGS.unnormalized, D5.S3.Quantum.CotfasDVGS.unnormalized_entry_midpoint, D5.S3.Quantum.CotfasDVGS.unnormalized_scaling
D5.S3.Quantum.CotfasDVGS.wSumbind-onlynoneD5.S3.Quantum.CotfasDVGS.entry_half_lattice, D5.S3.Quantum.CotfasDVGS.unnormalized, D5.S3.Quantum.CotfasDVGS.unnormalized_entry_midpoint, D5.S3.Quantum.CotfasDVGS.unnormalized_scaling, D5.S3.Quantum.CotfasDVGS.wSum_scaling
D5.S3.Quantum.CotfasDVGS.unnormalizedbind-onlynoneD5.S3.Quantum.CotfasDVGS.entry_half_lattice, D5.S3.Quantum.CotfasDVGS.kernel_identity, D5.S3.Quantum.CotfasDVGS.result, D5.S3.Quantum.CotfasDVGS.rhoTilde, D5.S3.Quantum.CotfasDVGS.rhoTilde_scaling, D5.S3.Quantum.CotfasDVGS.unnormalized_entry_midpoint, D5.S3.Quantum.CotfasDVGS.unnormalized_scaling
D5.S3.Quantum.CotfasDVGS.rhoTildebind-onlynoneD5.S3.Quantum.CotfasDVGS.claim, D5.S3.Quantum.CotfasDVGS.result, D5.S3.Quantum.CotfasDVGS.rhoTilde_scaling
D5.S3.Quantum.CotfasDVGS.claimbind-onlynoneD5.S3.Quantum.CotfasDVGS.result
D5.S3.Quantum.CotfasDVGS.W_scalingbind-onlynoneD5.S3.Quantum.CotfasDVGS.wSum_scaling
D5.S3.Quantum.CotfasDVGS.wSum_scalingbind-onlynoneD5.S3.Quantum.CotfasDVGS.unnormalized_scaling
D5.S3.Quantum.CotfasDVGS.unnormalized_scalingbind-onlynoneD5.S3.Quantum.CotfasDVGS.rhoTilde_scaling
D5.S3.Quantum.CotfasDVGS.rhoTilde_scalingbind-onlynoneD5.S3.Quantum.CotfasDVGS.result
D5.S3.Quantum.CotfasDVGS.uncertainty_det_boundbind-onlynoneD5.S3.Quantum.CotfasDVGS.result
D5.S3.Quantum.CotfasDVGS.normalization_isDensitybind-onlynoneD5.S3.Quantum.CotfasDVGS.result
D5.S3.Quantum.CotfasDVGS.kernelbind-onlynoneD5.S3.Quantum.CotfasDVGS.finite_periodization_posSemidef, D5.S3.Quantum.CotfasDVGS.kernel_factorization, D5.S3.Quantum.CotfasDVGS.kernel_fourier_slice, D5.S3.Quantum.CotfasDVGS.kernel_identity, D5.S3.Quantum.CotfasDVGS.kernel_lattice_summable, D5.S3.Quantum.CotfasDVGS.kernel_norm_bound, D5.S3.Quantum.CotfasDVGS.kernel_posSemidef, D5.S3.Quantum.CotfasDVGS.kernel_residual_posSemidef, D5.S3.Quantum.CotfasDVGS.periodization_posSemidef, D5.S3.Quantum.CotfasDVGS.periodized_kernel_zero_diagonal_pos, D5.S3.Quantum.CotfasDVGS.result
D5.S3.Quantum.CotfasDVGS.wavebind-onlynoneD5.S3.Quantum.CotfasDVGS.kernel_factorization, D5.S3.Quantum.CotfasDVGS.kernel_posSemidef, D5.S3.Quantum.CotfasDVGS.kernel_residual_posSemidef, D5.S3.Quantum.CotfasDVGS.strongWave_factorization
D5.S3.Quantum.CotfasDVGS.kernel_factorizationbind-onlynoneD5.S3.Quantum.CotfasDVGS.kernel_posSemidef, D5.S3.Quantum.CotfasDVGS.kernel_residual_posSemidef
D5.S3.Quantum.CotfasDVGS.lambda_nonnegativebind-onlynoneD5.S3.Quantum.CotfasDVGS.kernel_posSemidef, D5.S3.Quantum.CotfasDVGS.kernel_residual_posSemidef
D5.S3.Quantum.CotfasDVGS.finite_gaussian_posSemidefbind-onlynoneD5.S3.Quantum.CotfasDVGS.finite_gaussian_residual_posSemidef, D5.S3.Quantum.CotfasDVGS.kernel_posSemidef
D5.S3.Quantum.CotfasDVGS.kernel_posSemidefbind-onlynoneD5.S3.Quantum.CotfasDVGS.finite_periodization_posSemidef
D5.S3.Quantum.CotfasDVGS.sum_subtype_pairbind-onlynoneD5.S3.Quantum.CotfasDVGS.finite_periodization_posSemidef, D5.S3.Quantum.CotfasDVGS.lattice_sum_nonnegative
D5.S3.Quantum.CotfasDVGS.finite_periodization_posSemidefbind-onlynoneD5.S3.Quantum.CotfasDVGS.periodization_posSemidef
D5.S3.Quantum.CotfasDVGS.periodization_posSemidefbind-onlynoneD5.S3.Quantum.CotfasDVGS.result
D5.S3.Quantum.CotfasDVGS.gaussian_shifted_summablebind-onlynoneD5.S3.Quantum.CotfasDVGS.kernel_lattice_summable, D5.S3.Quantum.CotfasDVGS.signed_W_lattice_summable, D5.S3.Quantum.CotfasDVGS.strongWave_summable
D5.S3.Quantum.CotfasDVGS.kernel_norm_boundbind-onlynoneD5.S3.Quantum.CotfasDVGS.kernel_lattice_summable
D5.S3.Quantum.CotfasDVGS.kernel_lattice_summablebind-onlynoneD5.S3.Quantum.CotfasDVGS.kernel_identity, D5.S3.Quantum.CotfasDVGS.periodized_kernel_zero_diagonal_pos, D5.S3.Quantum.CotfasDVGS.result
D5.S3.Quantum.CotfasDVGS.centered_eq_of_dvdbind-onlynoneD5.S3.Quantum.CotfasDVGS.halfLatticeMap_injective, D5.S3.Quantum.CotfasDVGS.midpoint_unique
D5.S3.Quantum.CotfasDVGS.halfLatticeMapbind-onlynoneD5.S3.Quantum.CotfasDVGS.halfLatticeEquiv, D5.S3.Quantum.CotfasDVGS.halfLatticeMap_injective, D5.S3.Quantum.CotfasDVGS.halfLatticeMap_surjective, D5.S3.Quantum.CotfasDVGS.midpoint_exists
D5.S3.Quantum.CotfasDVGS.halfLatticeMap_injectivebind-onlynoneD5.S3.Quantum.CotfasDVGS.halfLatticeEquiv
D5.S3.Quantum.CotfasDVGS.valMinAbs_sub_dvdbind-onlynoneD5.S3.Quantum.CotfasDVGS.halfLatticeMap_surjective, D5.S3.Quantum.CotfasDVGS.midpoint_unique
D5.S3.Quantum.CotfasDVGS.halfLatticeMap_surjectivebind-onlynoneD5.S3.Quantum.CotfasDVGS.halfLatticeEquiv, D5.S3.Quantum.CotfasDVGS.midpoint_exists
D5.S3.Quantum.CotfasDVGS.halfLatticeEquivbind-onlynoneD5.S3.Quantum.CotfasDVGS.entry_half_lattice
D5.S3.Quantum.CotfasDVGS.inverse_quadratic_coordinatesbind-onlynoneD5.S3.Quantum.CotfasDVGS.W_coordinates, D5.S3.Quantum.CotfasDVGS.inverse_quadratic_lower_bound
D5.S3.Quantum.CotfasDVGS.W_coordinatesbind-onlynoneD5.S3.Quantum.CotfasDVGS.kernel_fourier_slice
D5.S3.Quantum.CotfasDVGS.inverse_quadratic_lower_boundbind-onlynoneD5.S3.Quantum.CotfasDVGS.W_gaussian_bound
D5.S3.Quantum.CotfasDVGS.half_lattice_poissonbind-onlynoneD5.S3.Quantum.CotfasDVGS.kernel_fourier_slice
D5.S3.Quantum.CotfasDVGS.theta_series_summablebind-onlynoneD5.S3.Quantum.CotfasDVGS.theta_duplication
D5.S3.Quantum.CotfasDVGS.exp_pi_intbind-onlynoneD5.S3.Quantum.CotfasDVGS.phase_half_lattice, D5.S3.Quantum.CotfasDVGS.theta_term_shift
D5.S3.Quantum.CotfasDVGS.neg_one_int_squarebind-onlynoneD5.S3.Quantum.CotfasDVGS.theta_term_shift
D5.S3.Quantum.CotfasDVGS.theta_term_shiftbind-onlynoneD5.S3.Quantum.CotfasDVGS.theta_duplication
D5.S3.Quantum.CotfasDVGS.parityLatticeMapbind-onlynoneD5.S3.Quantum.CotfasDVGS.parityLatticeMap_injective, D5.S3.Quantum.CotfasDVGS.theta_duplication
D5.S3.Quantum.CotfasDVGS.parityLatticeMap_injectivebind-onlynoneD5.S3.Quantum.CotfasDVGS.theta_duplication
D5.S3.Quantum.CotfasDVGS.theta_duplicationbind-onlynoneD5.S3.Quantum.CotfasDVGS.theta_nonzero
D5.S3.Quantum.CotfasDVGS.theta_nonzero_smallbind-onlynoneD5.S3.Quantum.CotfasDVGS.theta_nonzero
D5.S3.Quantum.CotfasDVGS.theta_nonzerocontentD5.S3.Quantum.CotfasDVGS.theta_nonzeroD5.S3.Quantum.CotfasDVGS.strongWave_zero_sum_ne_zero
D5.S3.Quantum.CotfasDVGS.W_nonnegativebind-onlynoneD5.S3.Quantum.CotfasDVGS.signed_W_lattice_summable
D5.S3.Quantum.CotfasDVGS.W_gaussian_boundbind-onlynoneD5.S3.Quantum.CotfasDVGS.signed_W_lattice_summable
D5.S3.Quantum.CotfasDVGS.signed_W_lattice_summablebind-onlynoneD5.S3.Quantum.CotfasDVGS.entry_half_lattice
D5.S3.Quantum.CotfasDVGS.midpoint_existsbind-onlynoneD5.S3.Quantum.CotfasDVGS.kernel_identity
D5.S3.Quantum.CotfasDVGS.parity_supportbind-onlynoneD5.S3.Quantum.CotfasDVGS.unnormalized_entry_midpoint
D5.S3.Quantum.CotfasDVGS.midpoint_uniquebind-onlynoneD5.S3.Quantum.CotfasDVGS.unnormalized_entry_midpoint
D5.S3.Quantum.CotfasDVGS.gaussian_fourier_termbind-onlynoneD5.S3.Quantum.CotfasDVGS.kernel_fourier_slice
D5.S3.Quantum.CotfasDVGS.kernel_fourier_slicebind-onlynoneD5.S3.Quantum.CotfasDVGS.kernel_identity
D5.S3.Quantum.CotfasDVGS.finite_gaussian_residual_posSemidefbind-onlynoneD5.S3.Quantum.CotfasDVGS.kernel_residual_posSemidef
D5.S3.Quantum.CotfasDVGS.strongWavebind-onlynoneD5.S3.Quantum.CotfasDVGS.kernel_residual_posSemidef, D5.S3.Quantum.CotfasDVGS.periodized_kernel_zero_diagonal_pos, D5.S3.Quantum.CotfasDVGS.strongWave_factorization, D5.S3.Quantum.CotfasDVGS.strongWave_norm, D5.S3.Quantum.CotfasDVGS.strongWave_summable, D5.S3.Quantum.CotfasDVGS.strongWave_zero_sum_ne_zero
D5.S3.Quantum.CotfasDVGS.strongWave_factorizationbind-onlynoneD5.S3.Quantum.CotfasDVGS.kernel_residual_posSemidef
D5.S3.Quantum.CotfasDVGS.kernel_residual_posSemidefbind-onlynoneD5.S3.Quantum.CotfasDVGS.periodized_kernel_zero_diagonal_pos
D5.S3.Quantum.CotfasDVGS.strongWave_normbind-onlynoneD5.S3.Quantum.CotfasDVGS.strongWave_summable
D5.S3.Quantum.CotfasDVGS.strongWave_summablebind-onlynoneD5.S3.Quantum.CotfasDVGS.periodized_kernel_zero_diagonal_pos
D5.S3.Quantum.CotfasDVGS.strongWave_zero_sum_ne_zerocontentD5.S3.Quantum.CotfasDVGS.theta_nonzeroD5.S3.Quantum.CotfasDVGS.periodized_kernel_zero_diagonal_pos
D5.S3.Quantum.CotfasDVGS.lattice_sum_nonnegativebind-onlynoneD5.S3.Quantum.CotfasDVGS.periodized_kernel_zero_diagonal_pos
D5.S3.Quantum.CotfasDVGS.periodized_kernel_zero_diagonal_poscontentD5.S3.Quantum.CotfasDVGS.theta_nonzeroD5.S3.Quantum.CotfasDVGS.result
D5.S3.Quantum.CotfasDVGS.kernelLatticeEquivbind-onlynoneD5.S3.Quantum.CotfasDVGS.kernel_identity
D5.S3.Quantum.CotfasDVGS.phase_half_latticebind-onlynoneD5.S3.Quantum.CotfasDVGS.entry_half_lattice
D5.S3.Quantum.CotfasDVGS.unnormalized_entry_midpointbind-onlynoneD5.S3.Quantum.CotfasDVGS.entry_half_lattice
D5.S3.Quantum.CotfasDVGS.entry_half_latticebind-onlynoneD5.S3.Quantum.CotfasDVGS.kernel_identity
D5.S3.Quantum.CotfasDVGS.kernel_identitybind-onlynoneD5.S3.Quantum.CotfasDVGS.result

Numerical experiment

Experiment directory, commit 04bafcea983207a1fa6056376aa68d57319d2fa1:

  • python3 check.py, run from that directory, exits 0. Script SHA-256: e590d9f1a35641dad4b659163e4b678ad34a5857beb62032952007133fa0181b. It checks 600 covariances with , including determinant-one samples, at and with lattice cutoff 40: zero failures, worst relative minimum eigenvalue . All 36 sampled cases are non-PSD.
  • python3 identity.py, run from that directory, exits 0. Script SHA-256: 9121d2a4c4a9479e0c28235bce7e4b10dabb256302626e7ac6bf3e29ff48647c. The entrywise kernel-identity error is at most for and four covariances.

These are numerical computations on truncated sums, not uniform proofs or a necessity theorem.

Triage

ItemStatusEvidence and scope
SettlementProved, kernel-checkedD5.S3.Quantum.CotfasDVGS.result, exactly the binding conventions and ,
MechanismProved, kernel-checkedPrivate kernel_identity, kernel_factorization, kernel_residual_posSemidef, theta_nonzero and periodized_kernel_zero_diagonal_pos on result’s path
Determinant boundaryProved, kernel-checkedresult uses uniformly; both and are included
NecessityOpenThe 36 sub-bound examples are computed by the pinned check.py above; they do not establish necessity for the discrete matrix
Dimension oneOpen in this deliveryNumerical samples are computed above; the delivered theorem retains and makes no separate claim
Novelty and literature completenessOpen; ASSUMED-UNVERIFIEDClassical Gaussian, Poisson and theta ingredients carry no originality claim; the Feng–Luo main text is not excluded

What the settlement shows

Proved, kernel-checked. The nonnegative uncertainty defect controls the Gaussian Gram factor, while a rank-one residual bound and theta nonvanishing give strict diagonal positivity. This handles and in the same argument. The exact normalized matrix is a density operator throughout the source’s stated family.

Explanation from the factorization. At , and the Gaussian factor is one; thus the displayed kernel is . The parameter entering the exponential damping is ; no equality between alone and a mixing variance is asserted.

Open. Necessity of the uncertainty condition for the discrete matrix, a separate dimension-one theorem, weaker covariance hypotheses, sharpness beyond the source family, and additional coherence results are not settled here. The paper’s uses of these matrices obtain their density-operator premise under the hypotheses of result; no other source theorem is certified by this delivery.

ASSUMED-UNVERIFIED

Literature-search completeness, including the subscription-only Feng–Luo text, remains unverified. No originality of the classical ingredients is claimed. The escape registration remains unfinished under #19812. Finite numerical checks have only the tested scope specified above.