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Virtual cochains, rational Thom augmentation and bordism for an oriented implicit atlas

Statement

Assume full AC. Let Z be compact Hausdorff with a specified locally orientable implicit atlas of virtual dimension d, satisfying the corrected relative regular-locus, extra-section submersion, relative finite-group freeness and tame-boundary axioms of Pardon implicit atlases and virtual fundamental class package. Then there is an explicitly constructed rational virtual cochain complex, with its canonical natural derived comparison to Čech cochains with virtual orientation coefficients, and a normalized obstruction-space Thom augmentation. They define [Z]vir:Hˇd(Z;oZrel⁡∂Z)⟶Q. For empty boundary use oZ; for an oriented atlas these are the indicated constant rational orientation coefficients. The functional is independent of finite covering subatlas and compatible with the described chart shrinking/refinement maps. It is the ordinary fundamental pairing on an actually regular oriented manifold. The construction applies when the regular thickening manifolds are Hausdorff without a global second-countability assumption.

The construction respects its actual boundary connector: [∂Z]vir(a)=[Z]vir(δa) and i∗[∂Z]vir=0. In particular a compact oriented implicit-atlas bordism of dimension d+1 between Z0,Z1, with a continuous map F to Y, gives equality of the two endpoint pushforward functionals on Hˇd(Y;Q). Covariant pushforward is defined by precomposition with Čech pullback. All finite-isotropy factors are rational, including ∣ΓI∣−1 on the Thom augmentation. This theorem is GIVEN an actual atlas and constructs no CR atlas or compactification.

Facts & Assumptions

Given: Full AC and exactly the data and hypotheses of the Statement.

[F1]

Pardon implicit atlases and virtual fundamental class package specifies the exact atlas, orientation, relative regularity and boundary convention; it does not assert the construction proved here.

[F2]

Cellular chains compute local homology gives the natural cellular/singular comparison for a CW pair with one ambient local system.

[F3]

Excision and Mayer–Vietoris with local coefficients gives actual transported subdivision/prism excision and Mayer–Vietoris, with no countability hypothesis.

[F4]

Refinement-limit Cech cohomology computes sheaf cohomology on compact Hausdorff spaces gives the compact-Hausdorff refinement-limit comparison, natural including coefficient connectors under AC. The supported-chain local duality, finite-group/DNC construction and Thom normalization are proved below, rather than imported.

Proof

technique · direct, using the explicit local constructions below
1.1F1F2F3F4givenconstructalgebra

All ambient spaces in this section are Hausdorff and locally compact; the final base Z is compact Hausdorff. For a compact subset K, a complex F(K) is contravariant under inclusion of compact subsets. Call it a compact-support descent complex if:

2.1F1F2F3F4givenconstructalgebrastep 1.1

(a) F(empty) is acyclic; (b) F(K1∪K2)→F(K1) direct-sum F(K2)→F(K1∩K2) is an acyclic total complex; (c) for a filtered decreasing family of compact supports Ki, the map colim F(Ki)→F(∩Ki) is a quasi-isomorphism.

3.1F1F2F3F4givenconstructalgebrastep 2.1

The stalk is F({z}). These are homotopy compact-presheaf conditions, not an assertion that each chain group is a sheaf.

4.1F1F2F3F4givenconstructalgebrastep 3.1

Here is a STRICT comparison complex, avoiding a choice of refinement maps. Fix a well-order of the point set of compact K. A rigid closed cover assigns a closed neighbourhood Cx to each x∈K, has only finitely many DISTINCT Cx, and satisfies x∈interior Cx. Its index set is always K, even when two assigned sets agree. Covers are ordered by C'_x subset Cx for EVERY x; intersection gives a common refinement. Use products over increasing point-tuples of the coefficient groups on their Cx intersections, and the alternating restriction differential. Refinement maps use the identity of this fixed index set and compose strictly. Take the directed colimit of these complexes. To compare one rigid cover with its finitely many distinct sets, choose one representative index for each distinct set; forgetting and reinserting repeated copies are inverse up to the explicit alternating prism inserting the two index choices. Thus its Čech complex is homotopy equivalent to that of a finite cover. Compact Hausdorff normality gives closed shrinkings of finite open covers and open enlargements of finite closed covers. Consequently this strict model computes precisely the refinement-colimit Čech convention in the corrected Definition. The products are products of Q-vector spaces and hence exact under the stated AC. Below its totalization is used only after good truncation to nonnegative internal degrees, so each total degree involves finitely many bidegrees.

5.1F1F2F3F4givenconstructalgebrastep 4.1

For a fixed finite closed cover, the augmentation F(K)→Tot Čech(F) is a quasi-isomorphism. Prove this by induction on its number of sets: split off the last set and use (b) for its intersection with the union of the preceding ones; the three resulting finite-cover complexes are the mapping-cone form of that Mayer–Vietoris square. The one-set case is the identity. Condition (c) permits the neighbourhood refinements used in passing between open and closed covers. Thus F computes its own Čech hypercohomology.

6.1F1F2F3F4givenconstructalgebrastep 5.1

Here is the exact purity argument, including the boundedness needed for that conclusion. Suppose the stalk cohomology is concentrated in degree zero and F is locally weakly bounded below in COHOMOLOGY. A compact support has a finite closed cover on which bounds exist; repeated (b) gives a bound on that support. Induct upward from that bound through degrees i<0. Once Hi−1F is zero, the exact sequence from (b), together with (c), says HiF is an ordinary compact sheaf: its finite gluing sequence is exact, and its support-continuity is (c). Its zero stalks then force it to be zero: an element vanishes on a neighbourhood of each point, finitely many of these neighbourhoods cover its compact support, and finite gluing is injective. Consequently HiF(K)=0 for every i<0.

7.1F1F2F3F4givenconstructalgebrastep 6.1

There is now an actual canonical comparison ROOF (use the strict rigid-cover complex just defined) F(K) → τ≥0F(K) → Cˇech⁡(τ≥0F)(K) ← Cˇech⁡(H0F)(K). (C)

8.1F1F2F3F4givenconstructalgebrastep 7.1

The first arrow is good truncation, the second is the cover augmentation, and the last is the inclusion of degree-zero cycles in the good truncation. Strong negative vanishing proves the first is an objectwise quasi-isomorphism. Good truncation therefore inherits descent; the finite-cover argument and repeated-index prism prove the second is a quasi-isomorphism. For the last, its cone is bounded below and stalk-acyclic. A total Čech cocycle in fixed degree is killed after refinement: its lowest Čech-degree component is an internal cocycle; choose local internal primitives, take a finite closed refinement of their neighbourhoods and subtract their total coboundary. This removes that component and creates only the next Čech-degree component. Repeat; only finitely many degrees occur because the internal complex is bounded below. In its bottom internal degree the zero stalk kernel makes the remaining local cocycle zero after refinement. This proves acyclicity without assuming a global primitive or interchanging an unbounded spectral sequence. Thus (C) is a functorial quasi-isomorphism roof and gives Hq F(K)=Čech Hq(K;H0F).

9.1F1F2F3F4givenconstructalgebrastep 8.1

The argument also applies to bounded mapping cones of such complexes. Accordingly it preserves pair triangles and their connecting maps. In particular it is stronger than an arbitrary vector-space isomorphism after taking cohomology.

10.1F1F2F3F4givenconstructalgebrastep 9.1

Let M be ANY Hausdorff topological n-manifold with boundary. No second-countability or paracompactness assumption is imposed on M. Let N be a closed tame codimension-zero submanifold-with-boundary of its boundary: locally N is absent, the full boundary, or one half of the boundary. Let Y be a closed subset of M, let j:M interior union N interior→M, and let L be a rank-one local coefficient system. Put, with k=n−q, FYq(K)=Ck(M,M∖(K∩Y);L) ⊕Ck−1(N,N∖(K∩Y);L).

11.1F1F2F3F4givenconstructalgebrastep 10.1

The differential is (a,b)↦(boundary a+i∗b,−∂ b). This is the ordinary homological cone of the inclusion from N, regraded cohomologically. It is viewed on the one-point compactification Y+; a compact K containing infinity means K intersection Y, so infinity has zero stalk.

12.1F1F2F3F4givenconstructalgebrastep 11.1

The descent conditions of §1 hold directly. Relative singular chains give (a). For (b), barycentric subdivision makes chains small for the two complement opens; the subdivision prism is a chain homotopy to the identity. The resulting ordinary Mayer–Vietoris complex is exact, and taking its relative quotient gives the asserted total acyclicity. For (c), a finite chain disjoint from the intersection of a filtered family of closed supports is disjoint from one member: its compact image has a finite subcover by the complement opens, and filteredness combines those finitely many indices. Thus the colimit map is in fact an isomorphism of relative chain groups. These arguments apply also to the N summand and its mapping cone.

13.1F1F2F3F4givenconstructalgebrastep 12.1

The weak lower bound uses no countable exhaustion. First an open subset U of Rn has Hk(U;L)=0 for k≥n, with the usual exception of degree zero when n=0. A sufficiently fine grid has a finite union of closed cubes inside U containing the compact image of the given cycle. On that finite CW complex the actual published local cellular/singular comparison applies. There are no cells above dimension n; a finite n-cycle in Rn is zero, since cancellation across adjacent n-cell faces transports its coefficients unchanged and a nonzero coefficient must propagate to an outer face, where it cannot cancel. This proves the assertion, also with local coefficients by their invertible face transports. The relative sequence then gives Hk(U,U∖Y;L)=0 for k>n. The same finite cubical argument in half-space charts and their boundary proves the corresponding bound for boundary and tame-half-boundary cone pairs. This uses a grid only in coordinate domains, never a triangulation of the whole topological manifold.

14.1F1F2F3F4givenconstructalgebrastep 13.1

For an arbitrary manifold, any finite chain and finite chain witnessing its relative boundary lie in a finite union of coordinate charts. That open union is second countable and normal, regardless of the whole M. Shrink this FINITE cover to closed sets, intersect with Y, and use the supported Mayer–Vietoris sequence. Each piece and each successive intersection lies in a chart; induction preserves the bound Hk=0 for k>n. Excision identifies the chart-supported pairs with their pairs in the union. Thus the supported cone is weakly bounded below. This is a finite-chain argument; no global countable atlas or global collar was used.

15.1F1F2F3F4givenconstructalgebrastep 14.1

Its stalks are calculated in a ball, half-ball or tame quarter-ball by radial deformation of a punctured chart. At a point of M interior the only local group is the orientation line oM tensor L in q=0. At a point of N interior the boundary-to-interior cone gives the same line with its outward-normal-first orientation. At a boundary point not in N interior, including the edge of N, that local cone contracts and its groups vanish. At infinity the stalk is zero. These chart computations commute with chart changes by their action on the top local homology line. They therefore identify the degree-zero sheaf with extension by zero of (oM⊗L)|_{M interior union N interior}, restricted to Y.

16.1F1F2F3F4givenconstructalgebrastep 15.1

Applying the PROVED roof (C), and the finite-cover definition of compactly supported Čech cohomology on Y as relative cohomology of Y+ at infinity, gives Hq FY(Y+)=Cˇech⁡ Hcq(Y;j!j∗(oM⊗L)∣Y). (LD)

17.1F1F2F3F4givenconstructalgebrastep 16.1

The maps in (LD) are natural for open restriction, inclusions of supports, the boundary cone, and products with oriented coordinate vector spaces. These assertions hold at the chain and orientation-sheaf level used in (C). In particular (LD) is not an invocation of a published duality theorem whose Statement assumed second countability.

18.1F1F2F3F4givenconstructalgebrastep 17.1

If a finite group G acts on a locally compact Hausdorff space Y, the quotient map q is closed and proper. For a sheaf F, the stalk (q∗F)x is the finite direct sum of Fy over the orbit above x: choose pairwise disjoint neighbourhoods of its finitely many points and shrink the quotient neighbourhood using closedness of q. Hence q∗ is exact. Rational G-invariants are exact by the averaging idempotent ∣G∣−1∑g g, also on complexes and local systems. If F=q∗L with its descent action, (q∗F)G=L. These identities with compact supports and the comparison construction (C) give Čech Hc∗(Y;q∗L)G = Čech Hc∗(Y/G;L).

19.1F1F2F3F4givenconstructalgebrastep 18.1

This proof permits isotropy; freeness is required only for the relative chart covering degrees used below. The corrected local-orientability axiom ensures that the virtual orientation system is such a descended system even when G itself has stabilizers.

20.1F1F2F3F4givenconstructalgebrastep 19.1

For any locally compact Y and local system L there is a canonical orientation-twisted suspension isomorphism Čech Hcq+r(Y×R>0r;L⊗oR⊗r) =Hˇcq(Y;L).

21.1F1F2F3F4givenconstructalgebrastep 20.1

For r=1, compactify the positive line at its two ends and use the relative interval cochain complex modulo its ends. Its sole reduced cohomology is the orientation line in degree one; the two-cone Mayer–Vietoris contraction gives the displayed shift for any Čech coefficient complex. Iterate, using the ordered super tensor convention. This proves precisely the sphere-suspension case needed here, not an unproved general Künneth theorem.

22.1F1F2F3F4givenconstructalgebrastep 21.1

Fix a FINITE subatlas A of the corrected Definition and put EA=⨁ Eα, ΓA=∏ Γα, and m=d+dim⁡ EA. For I subset J subset A define DIJ to be the set of

23.1F1F2F3F4givenconstructalgebrastep 22.1

(e,t,x) in EA times R≥0A times ZJreg

24.1F1F2F3F4givenconstructalgebrastep 23.1

with tα=0 outside I, sα(x)=tα eα for alpha in J, and ψK,J(x) in ZKreg for K={α:tα>0}. Let DIJ(K0) be its closed subset e=0 and ψ∅,J(x) in K0, for compact K0 subset Z. Denote by NIJ the part with x on the atlas boundary.

25.1F1F2F3F4givenconstructalgebrastep 24.1

The RELATIVE submersion axiom, not transversality of sJ itself, gives DIJ a manifold-with-corners structure of dimension m+|I|. To check at a face with positive parameters exactly K, use the local product coordinates for sJ∖K near ψK,J−1(ZKreg). Its extra coordinates are solved by zα=tα eα; the remaining variables are the regular K-chart coordinates, free e outside K, and the nonnegative t in I. This has exactly the displayed dimension and corner faces. At positive tα, solve eα=sα(x)/tα instead. These descriptions agree on overlap. The boundary part NIJ is tame and its complementary boundary faces are tα=0. Corners may be straightened as topological manifold boundary; their ordering is retained in the orientation line. That orientation line is oZJreg tensor oEA tensor oEJdual tensor oR⊗I.

26.1F1F2F3F4givenconstructalgebrastep 25.1

Define the RELATIVE virtual partial complex by AIJq(K0)=Cm−q(DIJ,DIJ∖DIJ(K0);oEAdual)ΓA.

27.1F1F2F3F4givenconstructalgebrastep 26.1

Define its ABSOLUTE version by adding the boundary cone summand Cm−q−1(NIJ,NIJ∖DIJ(K0);oEAdual) with differential (a,b)↦(boundary a+i∗b,−∂ b). The finite-group invariant functor is exact over Q, so the conclusions of §§1–3 apply.

28.1F1F2F3F4givenconstructalgebrastep 27.1

Let VI=ψ∅,I(sI−1(0)∩ZIreg), and let jIJ:VI intersection VJ→Z. Apply (LD) to the closed support DIJ(K0). Removing the unselected t-boundary leaves the support ψ∅,J−1(K0∩VI∩VJ) times R>0I.

29.1F1F2F3F4givenconstructalgebrastep 28.1

The orientation formula above cancels oEA against its dual; Euclidean suspension cancels the |I| shift. Finite-group descent then gives Hq AIJ(K0) = Čech Hq(K0;(jIJ)!(jIJ)∗oZ)

30.1F1F2F3F4givenconstructalgebrastep 29.1

for the absolute version, and the same with oZrel∂=j!j∗oZ for the relative version. This calculation proves in particular that the partial complexes are pure compact-support descent complexes. Its local map sends a normal relative fundamental class to its virtual orientation germ; it is a specified comparison, not a dimension count.

31.1F1F2F3F4givenconstructalgebrastep 30.1

For I subset I' subset J' subset J there is an actual map DIJ→DI′J′ given by x↦ψJ′,J(x), with e unchanged and newly allowed parameters still zero. Its relative singular-chain pushforward is multiplied by ∣ΓJ∖J′|^{-1}.

32.1F1F2F3F4givenconstructalgebrastep 31.1

These weighted maps compose exactly. They preserve the absolute/relative boundary cone. On a common zero-footprint stalk the raw pushforward is the orientation map times the degree ∣ΓJ∖J′|, because the RELATIVE group acts freely there. The displayed factor makes the induced orientation-sheaf map the identity. Maps outside the relevant footprints are extension by zero. This verifies the needed normalization and compatibility explicitly.

33.1F1F2F3F4givenconstructalgebrastep 32.1

The virtual cochain complex is the following FINITE bar totalization: Cvirq(K0)=⨁ over I0 strictly-subset ... strictly-subset Ip subset A AI0,Ipq+p(K0).

34.1F1F2F3F4givenconstructalgebrastep 33.1

Use internal differential (-1)^p d and the alternating face differential deleting an Ii. For an endpoint use its weighted structure map; for an internal face use the identity. The two differentials anticommute and the simplicial faces square to zero, so this is an actual complex. It agrees with the finite-poset hocolim, but the displayed formula fixes its degrees and signs. Use the analogous relative partial complexes for Cvir(K0rel∂).

35.1F1F2F3F4givenconstructalgebrastep 34.1

Its p-filtration is finite. At a base point z the partial cohomology is oZ,z if z belongs to VI intersection VJ and zero otherwise. The atlas axioms give:

36.1F1F2F3F4givenconstructalgebrastep 35.1

VI intersection VK subset VJ when I subset J subset K; VI intersection VI′ subset VI∪I′.

37.1F1F2F3F4givenconstructalgebrastep 36.1

Thus the set Sz={I:z∈VI} is nonempty, interval-convex in 2^A and closed under unions. It has the maximum Iz=⋃Sz. Its nerve contracts by adjoining that maximum to a chain, with the alternating last-vertex cone homotopy. The stalk bar complex is therefore oZ,z tensor the contractible nerve chain complex. It has just oZ,z in degree zero. The local orientation inclusions from AII patch, since the weighted maps were checked to be identity. Finite filtration preserves descent and weak lower boundedness. The purity comparison (C) now yields a NATURAL quasi-isomorphism roof Cvir(K0) ~= Cˇech⁡(K0;oZ), Cvir(K0rel∂) ~= Cˇech⁡(K0;oZrel∂). (V)

38.1F1F2F3F4givenconstructalgebrastep 37.1

This constructs the full comparison, including its functorial maps and finite-filtration convergence. It is not an assumed Pardon Theorem 4.3.4.

39.1F1F2F3F4givenconstructalgebrastep 38.1

Put T(EA)=Cdim⁡EA+∗(EA,EA∖0;oEAdual)ΓA. It has cohomology/homology Q in its zero degree and zero otherwise, with canonical generator [EA]. This follows by radial contraction of a punctured vector space to its sphere and the elementary relative ball computation. The coefficient orientation dual makes [EA] canonical without choosing an orientation of EA.

40.1F1F2F3F4givenconstructalgebrastep 39.1

For K0=Z, projection DII→EA is a map of the support pairs. On the p=0 summand AII, define the Thom augmentation by ϵI=∣ΓI∣−1(projectiontoEA)∗.

41.1F1F2F3F4givenconstructalgebrastep 40.1

Set it zero on p>0. It maps Cvird+∗(Zrel∂) to T(EA) with the reversed homological degree. This is a CHAIN MAP. Indeed, for an IJ edge its endpoint composites are both ∣ΓJ∣−1 times the SAME raw projection: the II endpoint includes ∣ΓJ∖I|^{-1}, whereas the JJ endpoint already has coefficient ∣ΓJ∣−1. They cancel in the alternating boundary. For higher simplices the output is zero or is the same cancellation after deleting an interior face. The internal differential commutes with projection. This also fixes the normalization hidden by the phrase “induced by projection”: unweighted projections are not an augmentation for the weighted faces.

42.1F1F2F3F4givenconstructalgebrastep 41.1

As a check, a point with one zero-dimensional obstruction chart, trivial action of Gamma on that chart, and empty empty-index regular locus has weight 1/|Gamma|. The ordinary regular empty-index atlas has weight one. These are consistent atlas-weight normalizations; no freeness of the full covering group was assumed.

43.1F1F2F3F4givenconstructalgebrastep 42.1

For finite A subset A', shuffle cross product with the canonical relative class [EA′∖A] and the map

44.1F1F2F3F4givenconstructalgebrastep 43.1

DIJ,A times EA′∖A→DIJ,A′

45.1F1F2F3F4givenconstructalgebrastep 44.1

set the extra t's to zero and give the atlas-refinement morphism in the derived category. One can choose any invariant relative cycle representing the class by averaging. Two choices differ by a boundary, so their chain maps differ by the explicit cross-product chain homotopy. Local duality identifies this morphism with the identity on oZ; hence it is a quasi-isomorphism by (V). The weighted endpoint factors stay ∣ΓI∣−1, so the augmentation commutes with this product, and [EA] times [EA′∖A]=[EA′]. This is the actual finite-subatlas independence proof.

46.1F1F2F3F4givenconstructalgebrastep 45.1

Using (V), the augmentation and [EA]↦1 define [Z]^vir : Čech Hd(Z;oZrel∂)→Q.

47.1F1F2F3F4givenconstructalgebrastep 46.1

Every atlas has a finite covering subatlas by compactness. Two such finite choices are contained in their union, so the functional is independent of the choice. Open shrinking of charts gives pushforward on supported chain pairs; its local orientation map is identity and it commutes with epsilon. Therefore it gives the same functional. The construction is for a specified atlas, not a claim that arbitrary unrelated implicit atlases yield the same functional.

48.1F1F2F3F4givenconstructalgebrastep 47.1

The absolute partial complex was the boundary inclusion cone. Taking its finite bar totalization preserves that cone, giving the chain triangle Cvir(Z rel ∂)→Cvir(Z)→Cvir(∂Z)→Cvir(Z rel ∂)[1].

49.1F1F2F3F4givenconstructalgebrastep 48.1

The orientation coefficient sequence is

50.1F1F2F3F4givenconstructalgebrastep 49.1

0→oZ rel ∂→oZ→i∗o∂ Z→0,

51.1F1F2F3F4givenconstructalgebrastep 50.1

with the outward-normal line and its parity retained. In the half-ball calculation of §2 the cone projection is exactly restriction to the outward-normal-first boundary orientation germ. Therefore the comparison roof (C) identifies the chain triangle with the Čech coefficient triangle, including its LAST connecting morphism, not only the first two maps. This follows also by applying the same roof to the mapping cone itself; its maps are the actual inclusion and projection. The augmentation commutes with the boundary connecting chain map, since projection to EA does, and the endpoint group factors are identical for the boundary atlas. Hence [boundary Z]^vir(a)=[Z]^vir(delta a)

52.1F1F2F3F4givenconstructalgebrastep 51.1

for a in Čech Hd−1(∂Z;o∂). The composite delta after restriction from Z is zero by the cochain short-exact-sequence connector formula. Thus i∗[∂Z]^vir=0.

53.1F1F2F3F4givenconstructalgebrastep 52.1

If an oriented atlas bordism B of dimension d+1 has boundary Z1 disjoint-union (−Z0), then for every continuous F:B→Y, (F∣Z1)∗[Z1]vir=(F∣Z0)∗[Z0]vir

54.1F1F2F3F4givenconstructalgebrastep 53.1

as functionals on Čech Hd(Y;Q). Indeed evaluate on a, use the preceding boundary identity and δ(F∣∂)∗a=0. This proves the topological bordism package GIVEN a compatible oriented bordism atlas. It does not construct an atlas over a path of almost-complex structures.

55.1F1F2F3F4givenconstructalgebrastep 54.1

For a genuinely regular compact oriented d-manifold, the empty-index atlas already covers. Its complex is Cd−∗(Z,Z∖Z)=Cd−∗(Z), with the boundary cone in the boundary case. Formula (LD) identifies its augmentation to a point with the ordinary fundamental-class pairing. Thus the normalization is the ordinary oriented fundamental class. Disjoint union is direct sum on all the chain complexes and on the augmentation, giving additivity.

56.1F1F2F3F4givenconstructalgebrastep 55.1∎

For a continuous f:Z→Y, define covariant pushforward ONLY by precomposition with Čech pullback: (f∗[Z]vir)(a)=[Z]vir(f∗a). Functoriality is literal composition of cochain pullbacks, and bordism invariance follows above. No BF Chow class, singular-homology identification for an arbitrary compact Hausdorff Z, fibre-product formula, Kontsevich–Manin axiom or localization theorem is inferred.

Remarks

A5 was authored by the complementary lane after actual reading of the saved Pardon text §§4.2–5.2 and Appendix A.5–A.8, with relevant compact-presheaf definitions in A.1–A.2. The three published basic interfaces are the actual pinned physics imports. No independent full geometric-atlas acceptance is implied; that atlas is a hypothesis of this abstract theorem.

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