LF6-D (QM side, general d): Ψ_d violates the CGLMP inequality for every d ≥ 2 #
Category: 3-Local (the general-d-intrinsic Bell violation for Ψ_d, the QM-side
payoff of the CGLMP infrastructure Mathlib/Probability/CGLMP.lean, extending the
d = 3 qutrit violation CGLMPQutrit.cglmp_maxEntangled_qutrit_gt_two to ALL d ≥ 2).
What is proved (general d, no dimension restriction) #
Under the standard CGLMP phase-basis measurements on Ψ_d = maxEntangled d (Alice offsets
α₁ = 0, α₂ = 1/2; Bob offsets β₁ = -1/4, β₂ = 1/4), the joint outcome-difference Born
probabilities pQM x y c = P(A_x − B_y = c) are computed from the Hilbert space for
arbitrary d:
pQM_closed:pQM x y c = 1 / (2 d² sin²(π(c.val + δ_xy)/d)), the standard maximally-entangled CGLMP closed form, DERIVED via thed-th-roots-of-unity Dirichlet / Fejér kerneldirichlet_kernel(‖∑_{j<d} e^{ijφ}‖² = sin²(dφ/2)/sin²(φ/2)), the quarter-integer numeratorsin²(π(m+δ)) = 1/2(sin_sq_pi_delta), and the diagonal contraction withΨ_d(inner_outcome_collapse,hconj_term). No value asserted.cglmpBracket_closed: the CGLMP bracket at indexkin closed form(2/d²)(csc²(π(k+1/4)/d) − csc²(π(k+3/4)/d))(bracketClosed); hencecglmp_maxEntangled_qudit_closedgives the full general-dCGLMP value as∑_{k<⌊d/2⌋} (1 − 2k/(d−1)) · bracketClosed d k.cglmp_maxEntangled_qudit_gt_two (hd : 2 ≤ d): the general-dviolationcglmp d pQM > 2. This is a genuine analytic inequality on thed-dependent trig sum, proved for EVERYd ≥ 2: every bracket term is nonnegative (bracketClosed_nonneg, viasinmonotonicity on(0, π/2]) and every coefficient is nonnegative (coeff_nonneg), so the sum dominates itsk = 0term (Finset.single_le_sum), and thek = 0term alone exceeds2(bracket_zero_gt_two) viasin x ≤ xon theπ/(4d)arm and Jordan's inequalitysin x ≥ 2x/π(jordan_sin, fromstrictConcaveOn_sin_Icc) on the3π/(4d)arm, giving the uniform boundbracketClosed d 0 ≥ 32/π² − 8/9 > 2(π < 3.15). No monotonicity indneeded; the singlek = 0term suffices for alld.no_lhv_realises_maxEntangled_cglmp_d (hd : 2 ≤ d): the general-dBell force. No local-hidden-variable model reproducingΨ_d's CGLMP statisticspQMexists: it would havecglmpLHV = cglmp d pQM > 2, contradictingcglmp_lhv_bound(I_d ≤ 2). Together with the general-dLHV bound this closes the statistical non-locality axis at FULL dimensional generality (matching theGHZ_ndeterministic axis).
Honest scope #
- Genuine computation from
Ψ_d's actual Born probabilities:bornPairis a squared inner product withmaxEntangled d, the outcome vectors are unit CGLMP phase-basis vectors, andpQMis the genuine outcome-difference marginal. The closed form is derived, not asserted. - The
> 2bound is a REAL analytic proof valid for everyd ≥ 2(notdecideover a finite dimension range, not axiomatised). It uses only thek = 0bracket term plus nonnegativity of the tail; the CGLMP value increases towards≈ 2.9696asd → ∞, but only the uniform lower bound32/π² − 8/9 ≈ 2.35is needed. - Foundational-triple-only (no
busch_effect_gleason; the roots-of-unity sums, the trig inequalities, and the finite LHV optimisation are all Gleason-free).
Reference: Collins, Gisin, Linden, Massar, Popescu, Phys. Rev. Lett. 88, 040404
(2002). specs/lf6-plan.md (LF6-D).
The joint offset δ_{xy} = α_x - β_y, the only combination of the two settings the
correlation depends on.
Equations
Instances For
Interface lemmas (CONVENTIONS §9.1, F2): the values the case splits below keep
re-deriving, stated once. Deliberately not @[simp] — existing proofs unfold by name and
must not change behaviour.
Alice's setting offset, x = false branch.
Alice's setting offset, x = true branch.
Bob's setting offset, y = false branch.
Bob's setting offset, y = true branch.
Alice's measurement phase on computational index j for outcome k of setting x:
2π j (k + α_x) / d. The offset α_x is what distinguishes her two settings.
Equations
- CSD.LF6.CGLMPQudit.aAngle d x k j = 2 * Real.pi * ↑↑j * (↑k.val + CSD.LF6.CGLMPQudit.alphaOff x) / ↑d
Instances For
Bob's measurement phase on computational index j for outcome l of setting y:
-2π j (l + β_y) / d. The sign is opposite to Alice's, so a product measurement pairs
their phases by difference.
Equations
Instances For
Alice's measurement vector for outcome k of setting x: the normalised Fourier
vector carrying the phases aAngle.
Equations
- CSD.LF6.CGLMPQudit.aVec d x k = WithLp.toLp 2 fun (j : Fin d) => (↑√↑d)⁻¹ * Complex.exp (↑(CSD.LF6.CGLMPQudit.aAngle d x k j) * Complex.I)
Instances For
Bob's measurement vector for outcome l of setting y: the normalised Fourier vector
carrying the phases bAngle.
Equations
- CSD.LF6.CGLMPQudit.bVec d y l = WithLp.toLp 2 fun (j : Fin d) => (↑√↑d)⁻¹ * Complex.exp (↑(CSD.LF6.CGLMPQudit.bAngle d y l j) * Complex.I)
Instances For
The joint measurement vector for the outcome pair (k, l) at settings (x, y): the
product vector aVec ⊗ bVec on the two-qudit register.
Equations
- CSD.LF6.CGLMPQudit.outcome d x y k l = WithLp.toLp 2 fun (p : Fin d × Fin d) => (CSD.LF6.CGLMPQudit.aVec d x k).ofLp p.1 * (CSD.LF6.CGLMPQudit.bVec d y l).ofLp p.2
Instances For
The Born probability of the outcome pair (k, l) at settings (x, y) on the maximally
entangled state.
Equations
- CSD.LF6.CGLMPQudit.bornPair d x y k l = ‖inner ℂ (CSD.LF6.CGLMPQudit.outcome d x y k l) (CSD.LF6.maxEntangled d)‖ ^ 2
Instances For
The joint phase base -2π (k - l + δ_{xy}) / d: the single angle the pair probability
depends on, so the correlation is a function of the outcome difference k - l alone.
Equations
Instances For
Jordan + reduction infra #
pQM and its closed form #
The quantum correlation P(A - B = c) at settings (x, y): the total Born weight of
all outcome pairs whose difference is c. This is the quantity the CGLMP bracket combines.
Equations
- CSD.LF6.CGLMPQudit.pQM d x y c = ∑ l : ZMod d, CSD.LF6.CGLMPQudit.bornPair d x y (c + l) l
Instances For
The bracket closed form #
The closed form of the k-th CGLMP bracket term on the maximally entangled state: the
difference of two 1/sin² weights a quarter-step either side of k. Summing these with the
CGLMP coefficients gives the qudit Bell value.
Equations
Instances For
Nonnegativity of coefficients and bracket terms #
The k=0 bracket exceeds 2 (the analytic lower bound) #
The general-d CGLMP violation and the Bell force #
The general-d closed-form CGLMP value for Ψ_d. The CGLMP functional on Ψ_d's
Born table is the ⌊d/2⌋-term weighted sum of the Dirichlet-kernel brackets
(2/d²)(csc²(π(k+1/4)/d) − csc²(π(k+3/4)/d)), the standard maximally-entangled CGLMP value.
Derived (cglmpBracket_closed), not asserted.
The general-d CGLMP violation (QM side). For every d ≥ 2, Ψ_d = maxEntangled d
violates the CGLMP inequality: its CGLMP value exceeds the local-hidden-variable bound 2.
A genuine analytic inequality on the d-dependent Dirichlet-kernel trig sum, proved for ALL
d ≥ 2 (the sum dominates its k = 0 term, and that term alone is ≥ 32/π² − 8/9 > 2
uniformly in d). Extends the d = 3 qutrit result
CGLMPQutrit.cglmp_maxEntangled_qutrit_gt_two to full dimensional generality.