Empirical/CSD: the Leggett–Garg two-time survival probability as a Kähler typicality volume #
Category: 3-Local (CSD-ontic layer).
The CSD twin of [Empirical/QM/LeggettGarg.lean]. The Leggett–Garg two-time correlation
⟨Q(0)Q(Δ)⟩ = cos(2Δ) is built (with intermediate collapse) from the qubit survival probability
P(0→0) = cos²Δ = |⟨0, e^{-iΔσ_x}|0⟩⟩|². Here that Born weight is realised as a Fubini–Study
typicality volume on the ontic Σ = ℂℙ¹: for the precessed state |Δ⟩ = cos Δ|0⟩ − i sin Δ|1⟩,
μ_FS { [φ] : Φ₀([φ]) ≤ Φ₀([|Δ⟩]) } = cos²Δ,
with volume = Born computed via the Duistermaat–Heckman theorem fs_moment_pushforward_uniform
(carving-free, busch_effect_gleason-free). So the LG transition statistics are ontic typicality
volumes, not a Born postulate.
References #
Empirical/QM/LeggettGarg.lean (lgCorr_eq); LF4/MomentUniform.lean
(fs_born_volume_ratio_qubit_uncond); Empirical/CSD/MalusVolume.lean (the same volume-frequency
pattern for the Malus law).
The precessed qubit state |Δ⟩ = e^{-iΔσ_x}|0⟩ = cos Δ|0⟩ − i sin Δ|1⟩.
Equations
Instances For
The Leggett–Garg survival probability cos²Δ is a Fubini–Study typicality volume. The
P(0→0) = cos²Δ transition weight of the two-time correlation equals the FS volume of the
moment-sublevel region cut by the precessed state [|Δ⟩] on the ontic ℂℙ¹ — Born as Kähler
volume, via Duistermaat–Heckman.