Where the overwhelming majority comes from: nearness to a pointer ray #
Category: 7-SigmaLayer (the record layer — Paper C A7). BACKLOG #105(a), out of #103.
MacrostateStability.lean (#103) proved the majority half of what makes
#102's record string macroscopic, but conditionally: ★★ measure_robustBasin_ge_one_sub needs
1 − ε ≤ c.rate p i, and #103 recorded why the hypothesis cannot be dropped — globalBasin_prob
makes a cell's measure exactly its Born weight, so no cell is overwhelming unless the weights are.
"Overwhelmingly many microstates share the record" is therefore a statement about the preparation
and the apparatus, not about the coordinate.
This file supplies the hypothesis for the canonical apparatus, and gives it a geometric reading.
What is proved #
offPointer i ψ— the component of a preparation orthogonal to thei-th pointer ray, with ★norm_offPointer_sq:‖offPointer i ψ‖² = ‖ψ‖² − ‖ψ i‖², so the defect is the missing Born weight;- ★
momentMap_mk_eq_coord_sq— for a unit preparation the canonical context's rate is the squared coordinate, and hence ★★one_sub_le_momentMap_of_near_pointer: a preparation within√εof the pointer ray has rate at least1 − εthere. This is the concentration hypothesis, read as a distance; - ★★★
measure_robustBasin_ge_of_near_pointerand the distance form ★★★measure_robustBasin_ge_of_dist_le— near a pointer ray the record macrostate is both overwhelming and robust: the cell of outcomei, restricted to the microstates robust to a record write of sizeδ, carries all butε + δof the epistemic measure. This is #105's statement for the canonical apparatus, obtained by feeding the geometry into #103; - ★★
measure_globalBasin_ge_of_near_pointer— the same without the robustness margin, and ★★★measure_map_recordMacro_ge_of_near_pointer— the macroscopic law of #102's record string puts all butεof its mass on one string, which is the form "almost every microstate records the same outcome" takes in the macroscopic law; - ★
offPointer_singleand ★★measure_robustBasin_ge_of_pointer— non-vacuity: at the pointer state itself the defect is zero and the robust cell carries1 − δ, so the hypothesis is satisfiable and the bound is not empty.
Honest scope #
⚠️ Nothing here drives the base to a pointer ray. The concentration is a property of where the preparation sits, supplied as a hypothesis with a geometric meaning; no dynamics is shown to produce it, and that — a decoherence or pointer-selection model whose rate field concentrates — is BACKLOG #106 and is the hard half of #105. Reading any statement below as "decoherence gives the macrostate" would be exactly the overclaim this file is written to avoid.
⚠️ It is still not fs_chebyshev_concentration.
Thermo/CanonicalTypicality.lean concentrates a base
statistic over the projective space with a polynomial rate; this file is about one preparation's
weight vector at one base point. The two are different statements about different objects and no
theorem joins them.
⚠️ Only the canonical pointer basis. momentContext is the standard-basis context, so "pointer
ray" means a coordinate ray of EuclideanSpace ℂ (Fin N). A general apparatus enters by transporting
the base point with the corresponding unitary, and that transport is not constructed here: no
ContextField built from an arbitrary orthonormal basis appears in the corpus, so nothing below is
stated for one.
⚠️ A near-pointer preparation is a special preparation. For a generic superposition no cell is
overwhelming, and that is correct physics rather than a gap: the bound degrades exactly as the Born
weights spread, and measure_robustBasin_ge_of_dist_le is vacuous once r² + δ ≥ 1. The content is
the rate at which macroscopicity is bought with nearness to the pointer, not a claim that record
macrostates are generically overwhelming.
⚠️ One context. The statements are about a single context's basin, not about a record string of
several contexts; #103's measure_robustBasin_ge_one_sub is per-context and so is everything here.
Nothing is claimed about a joint cell of two contexts, where #102's contextuality warning applies.
References: records-to-spacetime-scoping.md ST-3;
future-work.md; MacrostateStability.lean (#103),
RecordMacrostate.lean (#102), GlobalBasin.lean, LF4/MomentMap.lean;
specs/BACKLOG.md #105, #106, #103, #102.
The defect from a pointer ray #
The component of a preparation orthogonal to the i-th pointer ray. Its norm measures how
far the preparation is from being a definite pointer state for the canonical apparatus.
Equations
- CSD.RecordLayer.offPointer i ψ = ψ - ψ.ofLp i • EuclideanSpace.single i 1
Instances For
★ The defect is exactly the missing Born weight. Parseval in coordinates: removing the
pointer component removes ‖ψ i‖² from the squared norm and nothing else.
Nearness to a pointer ray is the concentration hypothesis #
★★ A preparation within √ε of the pointer ray has rate at least 1 − ε there. This is the
concentration hypothesis of #103, with a geometric reading: the weight that is missing from the
pointer outcome is exactly the squared distance to its ray.
The macrostate near a pointer ray #
★★★ Near a pointer ray the record macrostate is overwhelming and robust. The cell of outcome
i, cut down to the microstates robust to a record write of size δ, carries all but ε + δ of the
epistemic measure — where ε bounds the squared distance from the preparation to the pointer ray.
This is #105's statement for the canonical apparatus: the two halves of "macroscopic" — many
microstates, and stable ones — hold together, with the geometry of the preparation as the only
input.
★★★ The same, read as a distance. A preparation within r of the pointer ray gives a robust
macrostate cell of measure at least 1 − r² − δ. ⚠️ Vacuous once r² + δ ≥ 1: macroscopicity is
bought with nearness to the pointer, at this rate and no better.
★★ Without the robustness margin: the basin of the pointer outcome carries all but ε.
★★★ The macroscopic law puts all but ε of its mass on one record string. #102's
recordMacro for the one-context family, read at a near-pointer preparation: almost every microstate
records the same outcome, in the macroscopic law rather than microscopically.
★★ Non-vacuity: at the pointer state the robust cell carries 1 − δ. The hypothesis of the
theorems above is satisfiable with ε = 0, so the bounds are not empty.