Transport along a scaling action

Its proofs are relative to the explicit sheaf-theoretic imports below; it does not close those imports or the Microlocal Sheaves course. The consulted antecedents are Kashiwara and Schapira, Microlocal Study of Sheaves, Astérisque 128 (1985), §2.1.1, printed p. 39, and Pierre Schapira, An Introduction to Sheaves on Grothendieck Topologies, version dated 1 August 2026, Definition 5.4.4 and Exercise 5.13, pp. 114 and 120. Their conic objects use positive rays in a real vector bundle. This unit also treats arbitrary continuous positive-real actions, so it proves the required transport and topology statements below instead of importing them from that vector-bundle setting. The final section compares the actual source hypotheses and proof mechanisms. No constructibility or finite-generation condition is imposed.

SH02-CON-CONTRACT — Objects, degree conventions, and imports

Fix a commutative ring AA of finite global dimension dd. All spaces called locally compact are Hausdorff. Write D+(X)D^+(X) for complexes of sheaves of AA-modules with cohomology bounded below. Bounds need not be zero and stalk modules need not be finitely generated. A shift satisfies Hq(K[r])=Hq+r(K)H^q(K[r])=H^{q+r}(K). In particular a module in cohomological degree one is written M[−1]M[-1]. Tensor products and internal Hom below are derived over the constant sheaf of rings, unless specified otherwise.

The action group is G=(0,∞)G=(0,\infty) under multiplication. Its orientation is the increasing coordinate log⁡t\log t. An action is a continuous map a:X×G→Xa:X\times G\to X with a(a(x,s),t)=a(x,st)a(a(x,s),t)=a(x,st) and a(x,1)=xa(x,1)=x. The action is not required to be free, proper, effective, or a vector-space action. Set

p:X×G⟶X,e:X⟶X×G,p(x,t)=x,e(x)=(x,1). p:X\times G\longrightarrow X,\qquad e:X\longrightarrow X\times G, \qquad p(x,t)=x,\quad e(x)=(x,1).

Here are the exact prerequisite results used. Their proof routes are identified below; the exceptional-operation and orientation contracts retain their separately stated scopes.

SH02-IMPORT-INTERVAL — Interval cohomology (SH-01 import contract)

A locally constant sheaf on an interval is constant; its ordinary cohomology in positive degrees vanishes. Evaluation at any point identifies its sections with its stalk. These statements hold for arbitrary AA-modules. They also give the analogous evaluation statement for a bounded-below complex with locally constant cohomology, by the hypercohomology spectral sequence. The interval-constancy and evaluation proof establishes all these statements for arbitrary module coefficients, including open, closed, half-open and unbounded intervals. Its complex comparison is the actual section-to-germ map, using the bounded-below hypercohomology proof and its canonical edge, not an unspecified isomorphism.

SH02-IMPORT-CONTINUITY — Closed-exhaustion continuity (SH-01 import contract)

Stalks and filtered colimits of AA-modules are exact. For a closed exhaustion Tn⊂Int⁡(Tn+1)T_n\subset\operatorname{Int}(T_{n+1}) of a space TT, the usual sheaf-cohomology continuity theorem and its Mittag-Leffler criterion apply. In particular, if the restriction maps Hq(Tm;K)→Hq(Tn;K)H^q(T_m;K)\to H^q(T_n;K) are isomorphisms for every qq and m≥nm\ge n, then Hq(T;K)→Hq(Tn;K)H^q(T;K)\to H^q(T_n;K) is an isomorphism. The same assertion is available after restriction to an open subset of a parameter space. The geometric derived-limit comparison and its degree-specific Milnor obstruction are proved in the closed-exhaustion comparison and its tower, Milnor and Mittag–Leffler proofs, specifically SH02-EXH-COMPARISON, SH02-EXH-MILNOR and SH02-EXH-STRIPS. That proof includes the noncompact strips used below.

SH02-IMPORT-DERIVED-SHEAVES — Derived sheaf operations (SH-01 import contract)

Exact inverse image, derived direct image, adjunction, derived sections, localization triangles, stalk detection of quasi-isomorphisms, and the bounded-below hypercohomology spectral sequence. Proper base change for Rf!Rf_! is part of this import; ordinary Rf*Rf_* base change is used below only when the relevant map is proper or when a separate proof is supplied. For the proper closed-strip projections in SH02-CON-CYLINDER, the proper-fibre and section-restriction proof supplies the exact ordinary direct-image comparison on locally compact Hausdorff spaces, for arbitrary module coefficients and bounded-below complexes. This does not assert ordinary base change for a general nonproper map.

SH02-IMPORT-SIX-FUNCTORS — Exceptional operations contract

If f!f_! has finite cohomological dimension, Rf!⊣f!Rf_!\dashv f^! on D+D^+, with its units and counits, composition, projection formula, and

Rf*Rℋom(K,f!L)≃Rℋom(Rf!K,L),f!Rℋom(B,C)≃Rℋom(f−1B,f!C). Rf_*R\mathcal Hom(K,f^!L) \simeq R\mathcal Hom(Rf_!K,L),\qquad f^!R\mathcal Hom(B,C) \simeq R\mathcal Hom(f^{-1}B,f^!C).

In these formulas the first internal-Hom argument is bounded above and the second is bounded below. All instances below meet these bounds. For an oriented topological submersion of relative dimension rr, f!L≃f−1L[r]f^!L\simeq f^{-1}L[r]. An oriented open interval has RΓc(I;A)≃A[−1]R\Gamma_c(I;A)\simeq A[-1], and integration identifies RΓc(I;A[1])→AR\Gamma_c(I;A[1])\to A with the identity in this identification. These assertions include the trace’s compatibility with proper base change.

The submersion comparison, SH02-MD-SUBMERSION, proves the oriented-submersion assertion for every bounded-below input on locally compact Hausdorff bases. Its product-chart argument checks the actual tensor comparison, not only the underlying objects. The compact-support generator, SH02-MD-EUCLIDEAN, and normalized trace and submersion base change, SH02-MD-TRACE, prove the interval calculation and its sign. They use the cylinder theorem above only at SH02-CON-CYLINDER, whose proof uses neither orientation nor exceptional inverse image.

For internal duality with a bounded first input and a bounded-below second input, SH02-EX-INTERNAL supplies the proof; that scope suffices for SH02-CON-INTERVAL-FIBRES. The opposite-bounded-range proof, (EXA.1)–(EXA.9), supplies the full bounded-above first-input contract displayed above under the same uniform proper-support dimension hypothesis. It uses the finite relative-soft model, the exact unbounded acyclic-model theorem and an explicit coefficient exchange, rather than assuming that a bounded-above/bounded-below tensor is bounded below.

SH02-IMPORT-PROPER-SUPPORTS — Proper-support sections contract

For a map f:Y→Bf:Y\to B of locally compact spaces, the stalks of Rqf!KR^qf_!K can be computed by the filtered system of HCq(f−1V;K)H^q_C(f^{-1}V;K), where VV runs through neighbourhoods of the base point and C⊂f−1VC\subset f^{-1}V is closed and proper over VV. For a closed embedding i:S↪Yi:S\hookrightarrow Y, i*i!K≃RΓSKi_*i^!K\simeq R\Gamma_S K, compatibly with inclusions of closed supports.

These are hypotheses on the available sheaf formalism, not additional geometric assumptions such as compactness of XX or constructibility of KK. Finite global dimension is a fixed convention of this unit; no noetherian assumption is added. Results about actual manifolds use finite dimension and countability at infinity, but the action and vector-bundle results below require only the stated locally compact spaces.

SH02-CON-CYLINDER — Descent across a contractible parameter

Lemma. Let BB be locally compact and let q:B×ℝ→Bq:B\times\mathbb R\to B. For K∈D+(B×ℝ)K\in D^+(B\times\mathbb R), assume every Hj(K)H^j(K) restricts to a locally constant sheaf on every fibre of qq. With s0(b)=(b,0)s_0(b)=(b,0), the evaluation and counit morphisms

Rq*K⟶s0−1K,q−1Rq*K⟶K Rq_*K\longrightarrow s_0^{-1}K, \qquad q^{-1}Rq_*K\longrightarrow K

are isomorphisms. Consequently q−1:D+(B)→D+(B×ℝ)q^{-1}:D^+(B)\to D^+(B\times\mathbb R) is fully faithful; its essential image consists exactly of those KK with fibrewise locally constant cohomology. Restriction by s0s_0 is an inverse on that image.

Proof. Put In=[−n,n]I_n=[-n,n], restrict KK to B×InB\times I_n, and denote the proper projection by qnq_n. It is proper because the inverse image of a compact C⊂BC\subset B is C×InC\times I_n, which is compact; the spaces are Hausdorff. The proper-fibre comparison with its actual restriction map identifies the stalk at bb of Rqn*(K|B×In)Rq_{n*}(K|_{B\times I_n}) with RΓ(In;K|{b}×In)R\Gamma(I_n;K|_{\{b\}\times I_n}). In the spectral sequence for these sections the terms in positive sheaf cohomology degree vanish by SH02-IMPORT-INTERVAL. The remaining terms are the stalks at (b,0)(b,0) of Hj(K)H^j(K). The spectral sequence is convergent because KK is bounded below, by HC1a–HC2. The interval evaluation theorem identifies this calculation with evaluation and proves that

Rqn*(K|B×In)⟶s0−1K Rq_{n*}(K|_{B\times I_n})\longrightarrow s_0^{-1}K

is a quasi-isomorphism. For m≥nm\ge n the restriction morphism between these direct images commutes with evaluation, so it too is an isomorphism.

For every open V⊂BV\subset B, this gives compatible isomorphisms

Hj(V×In;K)≃Hj(V;s0−1K). H^j(V\times I_n;K)\simeq H^j(V;s_0^{-1}K).

The closed strips V×InV\times I_n exhaust V×ℝV\times\mathbb R, each lying in the interior of the next. The transition maps on cohomology are isomorphisms, so SH02-IMPORT-CONTINUITY shows that evaluation Hj(V×ℝ;K)→Hj(V;s0−1K)H^j(V\times\mathbb R;K)\to H^j(V;s_0^{-1}K) is an isomorphism for every jj. This is the asserted isomorphism Rq*K→s0−1KRq_*K\to s_0^{-1}K.

For the counit, fix (b,t)(b,t) and choose n>|t|n>|t|. Its restriction to the strip fits into the adjunction diagram with the counit for qnq_n. On the stalk at (b,t)(b,t), the latter is evaluation from RΓ(In;K|{b}×In)R\Gamma(I_n;K|_{\{b\}\times I_n}) to K(b,t)K_{(b,t)}. The same spectral sequence calculation, now evaluated at tt, makes this an isomorphism. The map Rq*K→Rqn*(K|B×In)Rq_*K\to Rq_{n*}(K|_{B\times I_n}) was already shown to be an isomorphism. Thus the counit is an isomorphism on every stalk.

For K=q−1LK=q^{-1}L its cohomology is constant along fibres, and the unit L→Rq*q−1LL\to Rq_*q^{-1}L is inverse to evaluation: the composite is the identity by the adjunction identity. Hence this unit is an isomorphism. Adjunction now gives

Hom⁡(q−1L,q−1M)≃Hom⁡(L,Rq*q−1M)≃Hom⁡(L,M). \operatorname{Hom}(q^{-1}L,q^{-1}M) \simeq\operatorname{Hom}(L,Rq_*q^{-1}M) \simeq\operatorname{Hom}(L,M).

This proves full faithfulness and the remaining assertions. The same proof works after replacing ℝ\mathbb R by GG through log\log. Iterating it gives full faithfulness for B×Gr→BB\times G^r\to B for every finite rr. No finite-generation or upper-boundedness assertion was used. ▫\square

SH02-CON-DEFINITION — Which orbit topology is meant?

For a subset Z⊂XZ\subset X, restriction in this unit means F|Z=iZ−1FF|_Z=i_Z^{-1}F, where the subset has its induced topology. For a general action this must be distinguished from pullback along an orbit parameter. The distinction is invisible for an ordinary nonzero vector-bundle ray, whose induced and homogeneous-space topologies agree. Thus the raywise definitions in Astérisque 128, §2.1.1, and Schapira’s Definition 5.4.4 do not decide which definition to use for a dense orbit of a general action. We specify both and compare them directly.

For x∈Xx\in X, let bxb_x be its orbit with the topology induced from XX, and write ix:bx→Xi_x:b_x\to X and ox:G→Xo_x:G\to X, ox(t)=a(x,t)o_x(t)=a(x,t), for the inclusion and the orbit map. The induced-orbit sheaf category is the full subcategory

Mod⁡ind(AX)={L∈Mod⁡(AX):ix−1L is locally constant on bx for every x}. \operatorname{Mod}_{\mathrm{ind}}(A_X) =\{L\in\operatorname{Mod}(A_X): i_x^{-1}L\text{ is locally constant on }b_x\text{ for every }x\}.

Write Dind+(X)D_{\mathrm{ind}}^+(X) for the full subcategory of D+(X)D^+(X) whose cohomology sheaves belong to this category. These are definitions; they do not identify induced-orbit conicity with parameter conicity, or require bxb_x to be locally compact.

In this unit, conic means parameter-conic: F∈D+(X)F\in D^+(X) is conic if ox−1Hj(F)o_x^{-1}H^j(F) is locally constant on GG for every xx and jj. Write DG+(X)D_G^+(X) for this full subcategory. For an ordinary sheaf LL, the corresponding condition is local constancy of every ox−1Lo_x^{-1}L.

Equivalently, one can restrict to each orbit with its homogeneous-space topology. Here is the topology check, including nonembedded orbits. The stabilizer GxG_x is closed because XX is Hausdorff. Under log\log, a closed subgroup of ℝ\mathbb R is either 00, cℤc\mathbb Z for some c>0c>0, or ℝ\mathbb R. Indeed, if positive subgroup elements have infimum zero their integer multiples approximate every real number and closedness gives the whole line. Otherwise the positive infimum belongs to the closed subgroup, and division with remainder shows that it generates the subgroup. The remaining subgroup has no nonzero elements.

Thus G/GxG/G_x is a line, a circle, or a point. Except for the point case the quotient map has local sections and is a local homeomorphism. A sheaf on the homogeneous orbit is locally constant if and only if its pullback to GG is: one direction is functorial pullback, and the other follows by pulling back along a local section and using a neighbourhood on which the pulled-back sheaf is constant. In the point case both statements hold for every module. Inverse image is exact, so this applies separately to every cohomology sheaf.

Here pullback from a homogeneous orbit means pullback along the continuous map G/Gx→XG/G_x\to X induced by oxo_x, with G/GxG/G_x given its quotient topology. That map need not be an embedding, so its quotient topology cannot be silently replaced by the induced topology. The next example proves that Dind+(X)⊆DG+(X)D_{\mathrm{ind}}^+(X)\subseteq D_G^+(X) can be strict, while the homogeneous and parameter conditions are equivalent as just proved.

SH02-CON-EXAMPLE-DENSE-ORBIT — A topology distinction detected by supports

Take A=ℤA=\mathbb Z, choose an irrational real number λ\lambda, and put

X=S1×S1,j:ℝ⟶X,j(u)=(eiu,eiλu). X=S^1\times S^1,\qquad j:\mathbb R\longrightarrow X,\qquad j(u)=(e^{iu},e^{i\lambda u}).

Use the continuous action

a((z1,z2),t)=(eilog⁡tz1,eiλlog⁡tz2). a((z_1,z_2),t)=(e^{i\log t}z_1,e^{i\lambda\log t}z_2).

The map jj is injective: j(u)=j(v)j(u)=j(v) would give u−v=2πmu-v=2\pi m and λm∈ℤ\lambda m\in\mathbb Z, forcing m=0m=0. Its image bb is one orbit. It is dense. To see this, the closure of the subgroup ℤ+λℤ⊂ℝ\mathbb Z+\lambda\mathbb Z\subset\mathbb R contains 11 and λ\lambda. By the closed-subgroup classification above, a proper such closure would be cℤc\mathbb Z, making λ\lambda a ratio of integers. Thus this subgroup is dense, so the fractional parts of mλm\lambda are dense in the circle. At each fixed first coordinate, adding 2πm2\pi m to the parameter therefore gives a dense set of second coordinates. This proves density in XX. The nonconstancy argument below only needs the recurrence that we will also prove explicitly.

Let

F=j!ℤℝ. F=j_!\mathbb Z_{\mathbb R}.

Here j!j_! is the direct image with proper supports for a continuous map between locally compact Hausdorff spaces. It does not require jj to be a locally closed embedding. Concretely, F(U)F(U) consists of locally constant integer-valued sections on j−1Uj^{-1}U whose closed support is proper over UU. Proper base change identifies the stalk of Rj!ℤℝRj_!\mathbb Z_{\mathbb R} at yy with compactly supported cohomology of j−1(y)j^{-1}(y). That fibre is one point for y∈by\in b and empty otherwise. Thus Rj!ℤℝRj_!\mathbb Z_{\mathbb R} is concentrated in degree zero, equals FF, and has stalk ℤ\mathbb Z on bb and zero off bb. The same fibre calculation for arbitrary sheaves on ℝ\mathbb R shows that j!j_! has cohomological dimension zero.

For y∈Xy\in X use the additive orbit parameter ry(s)=a(y,es)r_y(s)=a(y,e^s). If y=j(u0)y=j(u_0), the fibre product of ryr_y and jj is the graph {(s,u0+s):s∈ℝ}\{(s,u_0+s):s\in\mathbb R\}, with its usual graph topology. Projection to ss is a homeomorphism. If y∉by\notin b, the fibre product is empty. Proper base change for these squares gives the sheaf isomorphisms

ry−1F≃{ℤℝ,y∈b,0,y∉b. r_y^{-1}F\simeq \begin{cases} \mathbb Z_{\mathbb R},&y\in b,\\ 0,&y\notin b. \end{cases}

These are isomorphisms of sheaves, not merely identifications of stalk groups. Hence FF is conic according to SH02-CON-DEFINITION.

We now show that F|bF|_b is not locally constant when bb carries its topology as a subset of XX. Fix x=j(u0)x=j(u_0) and a section s∈F(U)s\in F(U) over an ambient open neighbourhood UU of xx. Choose a compact neighbourhood K⊂UK\subset U of xx. If C⊂j−1UC\subset j^{-1}U is the closed support of the section defining ss, properness makes C∩j−1KC\cap j^{-1}K compact in ℝ\mathbb R, hence bounded. Consequently there is RR such that the germ of ss at every j(u)∈Kj(u)\in K with |u|>R|u|>R is zero.

There are positive integers mk→∞m_k\to\infty such that the distance of mkλm_k\lambda to ℤ\mathbb Z tends to zero. Indeed, subdividing [0,1)[0,1) into NN equal intervals and comparing the N+1N+1 fractional parts of 0,λ,…,Nλ0,\lambda,\ldots,N\lambda gives an integer 1≤m≤N1\le m\le N with distance at most 1/N1/N. Such integers cannot stay in a finite set as the distance tends to zero, since λ\lambda is irrational. Passing to an unbounded subsequence proves the assertion. Therefore

uk=u0+2πmk⟶+∞,j(uk)⟶x. u_k=u_0+2\pi m_k\longrightarrow+\infty,\qquad j(u_k)\longrightarrow x.

For all sufficiently large kk, these points lie in the interior of KK and their germs of ss vanish. Every ambient section with nonzero germ at xx consequently has zero germs at points of bb arbitrarily near xx.

If F|bF|_b were locally constant near xx, a local trivialization and the nonzero element 1∈Fx=ℤ1\in F_x=\mathbb Z would provide a section with nonzero germ everywhere on some relative neighbourhood of xx. By the definition of inverse image to a subspace, that section is represented, after a further relative shrink around xx, by an ambient section of FF. The recurrent zero germs just proved give a contradiction.

Thus conicity along parameter maps, equivalently along homogeneous-space orbits, does not imply local constancy on an orbit with its induced subspace topology. Local constancy for the induced topology does imply the parameter condition, since the parameter map to that subspace is continuous and inverse image preserves locally constant sheaves. The implication is therefore strict. In particular, an equivalence formulated using parameter pullbacks cannot simply replace that condition by local constancy on induced-subspace orbits. This independently proved topology obstruction is distinct from the periodic-action failure in SH02-CON-RESTRICTION. ▫\square

The topology distinction in pictures. Specialize the example to λ=2\lambda=\sqrt2. The first figure shows the orbit on a standard embedded torus; the second separates long parameter travel from small return distance and shows why proper supports obstruct an induced-orbit trivialization.

A finite irrational orbit segment on a torus, with its initial point and a later return marked

The blue curve samples j(u)j(u) for 0≤u≤20π0\le u\le20\pi at 6,001 parameter values. It is shown through the embedding E(θ,ϕ)=((1.8+0.6cos⁡ϕ)cos⁡θ,(1.8+0.6cos⁡ϕ)sin⁡θ,0.6sin⁡ϕ)E(\theta,\phi)=((1.8+0.6\cos\phi)\cos\theta, (1.8+0.6\cos\phi)\sin\theta,0.6\sin\phi), with θ=u\theta=u and ϕ=2u\phi=\sqrt2u. The red point is j(0)j(0) and the gold point is j(10π)j(10\pi); the latter has second-circle angle 2π/(52+7)2\pi/(5\sqrt2+7) modulo 2π2\pi. The gray grid describes the ambient torus and is not sheaf support. Curve thickness is only a drawing aid.

Exact return samples and the proper-support mechanism in the dense-orbit counterexample

For the displayed pairs (m,n)=(5,7),(12,17),(29,41),(70,99),(169,239)(m,n)=(5,7),(12,17),(29,41),(70,99),(169,239), put u=2πmu=2\pi m and ϵ=m2−n=(2m2−n2)/(m2+n)\epsilon=m\sqrt2-n=(2m^2-n^2)/(m\sqrt2+n). The first circle coordinate of j(u)j(u) is exactly 11. The right panel magnifies the second circle; its labelled distance is the Euclidean chord |e2πiϵ−1|=2|sin⁡(πϵ)||e^{2\pi i\epsilon}-1|=2|\sin(\pi\epsilon)|, not an intrinsic metric on the orbit. The lower panel depicts the proof above: properness of a section’s support over a compact neighbourhood bounds the parameters of its nonzero germs, while recurrence supplies arbitrarily large parameters whose images return near the basepoint. Those returning germs must vanish. No numerical bound for an arbitrary section is asserted.

These are finite illustrations of SH02-CON-EXAMPLE-DENSE-ORBIT. The full density, recurrence and sheaf arguments remain above. The proper-support definition used in that proof is compared with Schapira’s Definition 4.2.2 and Remark 4.2.5, pp. 85–86: compactness over each compact subset of the target bounds the returning parameters of any one section’s support. The dense-orbit example and its drawings are independently authored course material illustrating the mathematical distinction proved here. A vector copy of the return and support panels preserves the exact labels.

SH02-CON-COMPARISON — Canonical transport and its normalization

For any F∈D+(X)F\in D^+(X) let K=a−1FK=a^{-1}F. Define

uF:Rp*K⟶F u_F:Rp_*K\longrightarrow F

by applying Rp*Rp_* to the unit K→Re*e−1KK\to Re_*e^{-1}K and using p∘e=a∘e=id⁡Xp\circ e=a\circ e=\operatorname{id}_X. There are two specified maps

αF:p−1Rp*a−1F⟶a−1F,βF=p−1uF:p−1Rp*a−1F⟶p−1F, \alpha_F:p^{-1}Rp_*a^{-1}F\longrightarrow a^{-1}F, \qquad \beta_F=p^{-1}u_F:p^{-1}Rp_*a^{-1}F\longrightarrow p^{-1}F,

where αF\alpha_F is the counit for p−1⊣Rp*p^{-1}\dashv Rp_*. These definitions specify the maps, not just their source and target objects.

Theorem. The following conditions on FF are equivalent:

  1. FF is conic.
  2. Every Hj(a−1F)H^j(a^{-1}F) is locally constant on every fibre of pp.
  3. Both αF\alpha_F and βF\beta_F are isomorphisms.
  4. There exists an isomorphism p−1F≃a−1Fp^{-1}F\simeq a^{-1}F in D+(X×G)D^+(X\times G).
  5. There exists an isomorphism p!F≃a!Fp^!F\simeq a^!F.

When these conditions hold, there is a canonical transport isomorphism

θF=αF∘βF−1:p−1F⟶a−1F.(SH02-CON-THETA) \theta_F=\alpha_F\circ\beta_F^{-1}: p^{-1}F\longrightarrow a^{-1}F. \qquad\text{(SH02-CON-THETA)}

It is natural in FF and its restriction along ee is the identity.

Proof. Since inverse image is exact, restriction of Hj(a−1F)=a−1Hj(F)H^j(a^{-1}F)=a^{-1}H^j(F) to {x}×G\{x\}\times G is exactly ox−1Hj(F)o_x^{-1}H^j(F). This proves the equivalence of the first two conditions. Under the second condition SH02-CON-CYLINDER applies to K=a−1FK=a^{-1}F: its evaluation is uFu_F and its counit is αF\alpha_F. Both are isomorphisms, hence so is βF\beta_F. The third condition gives the fourth by the displayed definition of θF\theta_F. Conversely, any isomorphism in the fourth condition identifies the cohomology of a−1Fa^{-1}F, on each pp-fibre, with the constant cohomology of p−1Fp^{-1}F, giving condition two.

For condition five, the homeomorphism

h:X×G⟶X×G,h(x,t)=(a(x,t),t) h:X\times G\longrightarrow X\times G,\qquad h(x,t)=(a(x,t),t)

has inverse (y,t)↦(a(y,t−1),t)(y,t)\mapsto(a(y,t^{-1}),t), and a=p∘ha=p\circ h. Thus both pp and aa are topological submersions of relative dimension one. Orient their fibres by the coordinate log⁡t\log t; hh preserves that coordinate. The submersion identity gives p!F≃p−1F[1]p^!F\simeq p^{-1}F[1] and a!F≃a−1F[1]a^!F\simeq a^{-1}F[1]. Shifting by [−1][-1] proves the equivalence with condition four, without an orientation sign change.

Finally, restriction of the counit αF\alpha_F by e−1e^{-1} is precisely uFu_F. The same is true of e−1βFe^{-1}\beta_F, by e−1p−1=ide^{-1}p^{-1}=\mathrm{id}. Their quotient is the identity. Every construction used a unit, counit, or its inverse naturally, proving naturality. ▫\square

The precise reach of the transport tests. Let I(F)I(F) mean induced-orbit conicity, P(F)P(F) parameter conicity, and H(F)H(F) homogeneous-orbit conicity. The existing topology comparison and the theorem give, under exactly the hypotheses of SH02-CON-CONTRACT,

I(F)⟹P(F)⟺H(F)⟺(2)⟺(3)⟺(4)⟺(5). I(F)\Longrightarrow P(F)\Longleftrightarrow H(F) \Longleftrightarrow (2)\Longleftrightarrow (3) \Longleftrightarrow (4)\Longleftrightarrow (5).

To make the logical issue explicit, consider a proposed three-condition criterion labelled (i) induced-orbit conicity, (ii) invertibility of the comparison maps, and (iii) fibrewise local constancy. Conditions (ii) and (iii) are conditions three and two above. With condition (i) read as I(F)I(F), none of the four transport tests implies I(F)I(F) in the stated generality. The same sheaf in SH02-CON-EXAMPLE-DENSE-ORBIT satisfies all four tests and fails I(F)I(F).

The fibre-pullback identity in the first sentence of our proof is valid for every FF and proves (2)⟺P(F)(2)\Longleftrightarrow P(F). Together with I(F)⇒P(F)I(F) \Rightarrow P(F) it proves the forward implication (i)⇒\Rightarrow(iii) in that proposed criterion, but not the false converse (iii)⇒\Rightarrow(i). Thus the theorem supplies the full parameter/homogeneous equivalence and all valid induced-orbit implications, without adding an embedded-orbit hypothesis. These are independently proved implications between the definitions in this unit; they make no claim about the wording or intended meaning of an unconsulted source.

Corollary. DG+(X)D_G^+(X) is closed under shifts, cones of morphisms between its objects, and cohomological truncations.

Proof. Truncations and shifts preserve the defining orbital-pullback condition. For cones, use the natural transformations α\alpha and β\beta: their source and target functors are triangulated. In the comparison of the two distinguished triangles, isomorphisms at the first two vertices force an isomorphism at the third. SH02-CON-COMPARISON applies to the cone. ▫\square

SH02-CON-COCYCLE — What the canonical transport actually proves

Proposition. θF\theta_F is the unique isomorphism p−1F→a−1Fp^{-1}F\to a^{-1}F whose restriction at t=1t=1 is the identity. On X×G×GX\times G\times G it satisfies

θF(x,st)=θF(a(x,s),t)∘θF(x,s).(SH02-CON-COCYCLE-EQ) \theta_F(x,st)=\theta_F(a(x,s),t)\circ\theta_F(x,s). \qquad\text{(SH02-CON-COCYCLE-EQ)}

Here the formula denotes equality of the corresponding pullback morphisms in the derived category, not a formula between chosen complexes of stalks.

Proof. For any other normalized isomorphism ϕ\phi, the composite θF−1ϕ\theta_F^{-1}\phi is an automorphism of p−1Fp^{-1}F. Full faithfulness in SH02-CON-CYLINDER says it is the pullback of one automorphism of FF; applying e−1e^{-1} identifies that automorphism with the identity. This proves uniqueness.

For the second assertion, the two sides are maps from q−1Fq^{-1}F to c−1a−1Fc^{-1}a^{-1}F, where q(x,s,t)=xq(x,s,t)=x and c(x,s,t)=(x,st)c(x,s,t)=(x,st). The left side is an isomorphism, and both sides restrict to the identity at (s,t)=(1,1)(s,t)=(1,1). Compose the right side with the inverse of the left side. The result is an endomorphism of q−1Fq^{-1}F. Full faithfulness for X×G2→XX\times G^2\to X and restriction at (1,1)(1,1) make it the identity. This is the required equality. ▫\square

This proves normalized action data and its cocycle equality in the ordinary derived category. It makes no claim about a chosen dg or infinity-categorical equivariant enhancement or about higher coherences. Those are different constructions and have not been imported by the mere existence of an isomorphism in condition four.

SH02-CON-INTERVAL-FIBRES — An open-submersion calculation

Lemma. Let BB be locally compact Hausdorff, let WW be an open subset of B×ℝB\times\mathbb R, and let r:W→Br:W\to B be the projection. Suppose each fibre WbW_b is a nonempty interval. For every L∈D+(B)L\in D^+(B) the unit L→Rr*r−1LL\to Rr_*r^{-1}L is an isomorphism.

Proof. The map rr is an oriented topological submersion of relative dimension one and has finite cohomological dimension for proper direct image. Its relative dualizing object is ωr=r!AB≃AW[1]\omega_r=r^!A_B\simeq A_W[1]. Consider the trace

tr⁡:Rr!ωr⟶AB. \operatorname{tr}:Rr_!\omega_r\longrightarrow A_B.

By proper base change its stalk at bb is the integration morphism RΓc(Wb;A[1])→AR\Gamma_c(W_b;A[1])\to A. A nonempty open interval, bounded or unbounded, is orientation-preservingly homeomorphic to ℝ\mathbb R, so this is an isomorphism by the positive-interval trace normalization and submersion base-change identity. Stalk detection proves that the trace is an isomorphism.

The submersion formula and the bounded-first-input internal duality proof identify

Rr*r−1L≃Rr*Rℋom(ωr,r!L)≃Rℋom(Rr!ωr,L)≃Rℋom(AB,L)≃L. \begin{aligned} Rr_*r^{-1}L &\simeq Rr_*R\mathcal Hom(\omega_r,r^!L)\\ &\simeq R\mathcal Hom(Rr_!\omega_r,L)\\ &\simeq R\mathcal Hom(A_B,L)\simeq L. \end{aligned}

The first identity cancels the common shift [1][1] in the two internal-Hom arguments; AWA_W is the tensor unit, so it needs no stalk-finiteness assumption. Under the second identity, precomposition with the trace is the unit L→Rr*r−1LL\to Rr_*r^{-1}L: this is the tensor-Hom adjunction identity for the counit Rr!r!AB→ABRr_!r^!A_B\to A_B. Thus the displayed isomorphism proves the assertion for the specified unit.

Here is the map check with its tensor order explicit. Write ϵr(L):Rr!r!L→L\epsilon_r(L):Rr_!r^!L\to L for the counit, and let θ:ωr⊗r−1L→r!L\theta:\omega_r\otimes r^{-1}L\to r^!L be the submersion tensor isomorphism, with the relative dualizing factor first. Its defining trace identity, (EX.24), identifies the composite

Rr!ωr⊗L→πRr!(ωr⊗r−1L)→Rr!θRr!r!L→ϵr(L)L Rr_!\omega_r\otimes L \xrightarrow{\pi}Rr_!(\omega_r\otimes r^{-1}L) \xrightarrow{Rr_!\theta}Rr_!r^!L \xrightarrow{\epsilon_r(L)}L

with ϵr(AB)⊗1L\epsilon_r(A_B)\otimes1_L, followed by AB⊗L≃LA_B\otimes L\simeq L.

To see the unit explicitly, put H=Rℋom(ωr,r!L)H=R\mathcal Hom(\omega_r,r^!L) and let λ:r−1L→H\lambda:r^{-1}L\to H be the curry of θ\theta. The submersion formula makes λ\lambda an isomorphism. Write ηL:L→Rr*r−1L\eta_L:L\to Rr_*r^{-1}L and δH:r−1Rr*H→H\delta_H:r^{-1}Rr_*H\to H for the ordinary unit and counit. The map in question, after internal duality, is

L→ηLRr*r−1L→Rr*λRr*H⟶Rℋom(Rr!ωr,L). L\xrightarrow{\eta_L}Rr_*r^{-1}L \xrightarrow{Rr_*\lambda}Rr_*H \longrightarrow R\mathcal Hom(Rr_!\omega_r,L).

Uncurry using the evaluated construction (EX.22). Naturality of the ordinary counit and its triangle identity give

δH∘r−1Rr*λ∘r−1ηL=λ∘δr−1L∘r−1ηL=λ. \delta_H\circ r^{-1}Rr_*\lambda\circ r^{-1}\eta_L =\lambda\circ\delta_{r^{-1}L}\circ r^{-1}\eta_L =\lambda.

Evaluation of ωr⊗λ\omega_r\otimes\lambda is θ\theta, so this uncurry is precisely the displayed projection–tensor–trace composite. Currying the equal composite ϵr(AB)⊗1L\epsilon_r(A_B)\otimes1_L is exactly precomposition with the trace. Thus the identity concerns the original unit, with the signs fixed by the same tensor order. Here ωr≃AW[1]\omega_r\simeq A_W[1] is bounded, so the bounded-first-input internal-Hom proof, (EX.20)–(EX.22), applies with the arbitrary bounded-below second input LL; no unbounded internal-Hom extension is used.

This proof uses proper base change for Rr!Rr_!; it never invokes unrestricted nonproper base change for Rr*Rr_*. ▫\square

SH02-CON-RESTRICTION — Restricting sections without losing a winding

For an open U⊂XU\subset X and x∈Xx\in X define the open subset of the parameter group

Tx(U)={t>0:a(x,t−1)∈U}. T_x(U)=\{t>0:a(x,t^{-1})\in U\}.

Theorem. Suppose Tx(U)T_x(U) is a nonempty interval in the coordinate log⁡t\log t for every xx. For conic F∈DG+(X)F\in D_G^+(X) the restriction map

RΓ(X;F)⟶RΓ(U;F|U) R\Gamma(X;F)\longrightarrow R\Gamma(U;F|_U)

is an isomorphism.

Proof. Let b:U×G→Xb:U\times G\to X be the restricted action. The change of coordinates hh used above identifies this map with the projection from

W={(x,t)∈X×G:a(x,t−1)∈U} W=\{(x,t)\in X\times G:a(x,t^{-1})\in U\}

to XX. This is open because UU is open and the inverse action is continuous. Its fibre at xx is Tx(U)T_x(U). SH02-CON-INTERVAL-FIBRES therefore makes the unit F→Rb*b−1FF\to Rb_*b^{-1}F an isomorphism.

Restrict θF\theta_F to U×GU\times G. It identifies b−1Fb^{-1}F with pU−1(F|U)p_U^{-1}(F|_U), where pU:U×G→Up_U:U\times G\to U. The cylinder lemma and composition of direct images give isomorphisms

RΓ(X;F)⟶RΓ(U×G;b−1F)≃RΓ(U×G;pU−1(F|U))⟶RΓ(U;F|U). R\Gamma(X;F) \longrightarrow R\Gamma(U\times G;b^{-1}F) \simeq R\Gamma(U\times G;p_U^{-1}(F|_U)) \longrightarrow R\Gamma(U;F|_U).

The first map is pullback along bb and the last is evaluation along u↦(u,1)u\mapsto(u,1). Since θF\theta_F is the identity along that section, the composite is exactly pullback along U↪XU\hookrightarrow X, that is, restriction. Hence it is the required isomorphism. ▫\square

Why the parameter fibre matters. A contractible intersection of an open set with the image of an orbit does not suffice for a general action. Take A=ℤA=\mathbb Z, X=S1X=S^1, and

a(z,t)=eilog⁡tz,U=S1\{1},F=ℤX. a(z,t)=e^{i\log t}z,\qquad U=S^1\setminus\{1\},\qquad F=\mathbb Z_X.

There is one orbit, its intersection with UU is a nonempty contractible open arc, and FF is conic. Nevertheless

H1(X;F)=ℤ,H1(U;F|U)=0. H^1(X;F)=\mathbb Z,\qquad H^1(U;F|_U)=0.

For completeness, cover the circle by two contractible arcs whose intersection has two contractible components. Their constant-sheaf Cech complex has ℤ2\mathbb Z^2 in degrees zero and one, with differential, after compatible trivializations, (a,b)↦(b−a,b−a)(a,b)\mapsto(b-a,b-a). Its kernel and cokernel are both ℤ\mathbb Z; interval acyclicity makes this Cech computation valid. The arc UU is acyclic by SH02-IMPORT-INTERVAL. Thus the restriction in degree one is the zero map from a nonzero group.

In this example log⁡Tx(U)\log T_x(U) is a disjoint union of infinitely many open intervals, rather than one interval. The same computation works with any nonzero allowed coefficient ring. An orbit-image version of the criterion is therefore false as a statement for arbitrary positive-real actions. SH02-CON-RESTRICTION states and proves a sufficient condition on the actual parameter fibres. The counterexample is retained with its complete cohomology calculation; no correspondence with an unconsulted source or errata entry is needed for the conclusion. For vector-bundle scaling the parameter fibres required below really are intervals.

SH02-CON-RADIAL-STAR — Ordinary contraction to the zero section

Let τ:E→Z\tau:E\to Z be a real vector bundle of finite rank nn over a locally compact space. Give EE the action (v,t)↦tv(v,t)\mapsto tv, and let i:Z↪Ei:Z\hookrightarrow E be its zero section. No orientation of EE or ZZ is chosen. For F∈DG+(E)F\in D_G^+(E) define

ρF:Rτ*F⟶i−1F \rho_F:R\tau_*F\longrightarrow i^{-1}F

by restricting the counit τ−1Rτ*F→F\tau^{-1}R\tau_*F\to F to ii.

Theorem. ρF\rho_F is an isomorphism.

Proof. This can be checked on stalks at z∈Zz\in Z. Trivialize the bundle over an open neighbourhood of zz and use a Euclidean norm on that trivialization. For an open VV in the trivializing neighbourhood and ε>0\varepsilon>0, set UV,ε=V×Bε⊂V×ℝnU_{V,\varepsilon}=V\times B_\varepsilon\subset V\times\mathbb R^n. For (v,w)(v,w) with w≠0w\ne0, the parameter fibre in the restriction theorem is

{t>0:|w|/t<ε}=(|w|/ε,∞). \{t>0:|w|/t<\varepsilon\}=(|w|/\varepsilon,\infty).

For w=0w=0 it is all of GG. Thus SH02-CON-RESTRICTION gives

RΓ(τ−1V;F)⟶RΓ(UV,ε;F) R\Gamma(\tau^{-1}V;F)\longrightarrow R\Gamma(U_{V,\varepsilon};F)

as an isomorphism. These are actual restrictions, so the isomorphisms are compatible as VV and ε\varepsilon shrink. The sets UV,εU_{V,\varepsilon} form a neighbourhood basis of i(z)i(z): in a product topology, every neighbourhood of (z,0)(z,0) contains such a product.

For each degree qq, taking filtered colimits yields

Hq(Rτ*F)z=lim→V∋zHq(τ−1V;F)≃lim→V∋z,ε>0Hq(UV,ε;F)=Hq(F)i(z). \begin{aligned} H^q(R\tau_*F)_z &=\underset{\rightarrow}{\lim}_{V\ni z}H^q(\tau^{-1}V;F)\\ &\simeq\underset{\rightarrow}{\lim}_{V\ni z,\,\varepsilon>0} H^q(U_{V,\varepsilon};F) =H^q(F)_{i(z)}. \end{aligned}

Exactness of filtered colimits justifies passage to cohomology. The map in this display is induced by restriction to germs, hence is Hq(ρF)zH^q(\rho_F)_z. It is an isomorphism for every qq and zz. ▫\square

The proof is local on the base and therefore needs neither a global bundle metric nor a paracompactness assumption on ZZ. It also explains why a nonproper map τ\tau is allowed: no properness of τ\tau was invoked.

SH02-CON-RADIAL-SUPPORT — Proper-support contraction

Define a natural morphism in the other direction by the closed-embedding counit:

σF:i!F≃Rτ!i*i!F⟶Rτ!F. \sigma_F:i^!F\simeq R\tau_!i_*i^!F\longrightarrow R\tau_!F.

Here ii is proper and τ∘i=id⁡Z\tau\circ i=\operatorname{id}_Z. The rank of τ\tau is finite, so τ!\tau_! has finite cohomological dimension and all displayed functors are defined on D+D^+.

Theorem. For every F∈DG+(E)F\in D_G^+(E), σF\sigma_F is an isomorphism.

Proof. First assume n>0n>0 and work in a local trivialization over VV. Write

YV=V×ℝn,SV=V×{0},CV,R=V×B¯R(R>0). Y_V=V\times\mathbb R^n,\quad S_V=V\times\{0\},\quad C_{V,R}=V\times\overline B_R\qquad(R>0).

On the invariant open space YV\SVY_V\setminus S_V, take the open subset YV\CV,RY_V\setminus C_{V,R}. Every point (v,w)(v,w) of the former has w≠0w\ne0, and its parameter fibre for the latter is (0,|w|/R)(0,|w|/R). It is a nonempty interval. SH02-CON-RESTRICTION therefore shows that

RΓ(YV\SV;F)⟶RΓ(YV\CV,R;F) R\Gamma(Y_V\setminus S_V;F)\longrightarrow R\Gamma(Y_V\setminus C_{V,R};F)

is an isomorphism. Compare the two localization triangles

RΓSV(YV;F)⟶RΓ(YV;F)⟶RΓ(YV\SV;F)⟶,RΓCV,R(YV;F)⟶RΓ(YV;F)⟶RΓ(YV\CV,R;F)⟶. \begin{aligned} R\Gamma_{S_V}(Y_V;F)&\longrightarrow R\Gamma(Y_V;F) \longrightarrow R\Gamma(Y_V\setminus S_V;F) \longrightarrow,\\ R\Gamma_{C_{V,R}}(Y_V;F)&\longrightarrow R\Gamma(Y_V;F) \longrightarrow R\Gamma(Y_V\setminus C_{V,R};F) \longrightarrow. \end{aligned}

The vertical maps are inclusion of supports, the identity, and restriction. The last two are isomorphisms, hence so is

RΓSV(YV;F)⟶RΓCV,R(YV;F).(SH02-CON-DISK-SUPPORT) R\Gamma_{S_V}(Y_V;F)\longrightarrow R\Gamma_{C_{V,R}}(Y_V;F). \qquad\text{(SH02-CON-DISK-SUPPORT)}

It remains to check the support limit, since fibre compactness alone is not global properness. Each CV,R→VC_{V,R}\to V is proper. Conversely, take a closed support C⊂YVC\subset Y_V proper over VV, and fix z∈Vz\in V. Choose a smaller neighbourhood V′V' of zz whose closure is compact and contained in VV; local compactness and the Hausdorff condition provide it. Properness makes C∩τ−1(V′¯)C\cap\tau^{-1}(\overline{V'}) compact. The norm in the trivialization is bounded on this compact set, so after choosing RR we have C∩τ−1V′⊂CV′,RC\cap\tau^{-1}V'\subset C_{V',R}. Thus closed disk supports are cofinal in the system of proper supports after passage to the stalk at zz.

By SH02-IMPORT-PROPER-SUPPORTS and this cofinality,

Hq(i!F)z=lim→V∋zHSVq(YV;F),Hq(Rτ!F)z=lim→V∋z,R>0HCV,Rq(YV;F). \begin{aligned} H^q(i^!F)_z &=\underset{\rightarrow}{\lim}_{V\ni z}H^q_{S_V}(Y_V;F),\\ H^q(R\tau_!F)_z &=\underset{\rightarrow}{\lim}_{V\ni z,\,R>0}H^q_{C_{V,R}}(Y_V;F). \end{aligned}

The first equality also uses i*i!F=RΓi(Z)Fi_*i^!F=R\Gamma_{i(Z)}F. The compatible isomorphisms (SH02-CON-DISK-SUPPORT) identify these two colimits. Their map is inclusion of zero-section support into proper support, hence is exactly Hq(σF)zH^q(\sigma_F)_z. This proves the theorem.

If n=0n=0, then E=ZE=Z and i=τ=idi=\tau=\mathrm{id}. Both ρF\rho_F and σF\sigma_F are the identity. This also avoids inserting a fictitious sphere or punctured fibre into the argument. If Z=⌀Z=\varnothing, all objects and maps are zero and both assertions hold. ▫\square

There is no orientation twist or shift in either contraction comparison. Orientation and shifts enter only when the resulting stalk or costalk is subsequently computed. The proof of proper-support contraction did not use Verdier double-dual reflexivity, which would require unjustified finiteness hypotheses for the objects allowed here.

SH02-CON-FUNCTORS — Transport through sheaf operations

Let f:Y→Xf:Y\to X be a continuous equivariant map of locally compact GG-spaces. In this section assume f!f_! has finite cohomological dimension, so that f!f^! is available in the stated formalism. Set f̃=f×idG\widetilde f=f\times\mathrm{id}_G. Its proper direct image has the same finite cohomological-dimension bound, by proper base change on the identical fibres.

Theorem. If F∈DG+(X)F\in D_G^+(X) and K∈DG+(Y)K\in D_G^+(Y), then

f−1F,f!F∈DG+(Y),Rf*K,Rf!K∈DG+(X). f^{-1}F,\ f^!F\in D_G^+(Y),\qquad Rf_*K,\ Rf_!K\in D_G^+(X).

If F1,F2∈DG+(X)F_1,F_2\in D_G^+(X), their derived tensor product is conic. If in addition F1∈D−(X)F_1\in D^-(X), then Rℋom(F1,F2)R\mathcal Hom(F_1,F_2) is conic and belongs to D+(X)D^+(X). Since F1F_1 was already bounded below, this last hypothesis makes F1F_1 bounded; it does not say that it is perfect or has finite-rank stalks.

Proof. We check each comparison and its required base change.

For inverse image, equivariance and pXf̃=fpYp_X\widetilde f=fp_Y give

aY−1f−1F≃f̃−1aX−1F≃f̃−1pX−1F≃pY−1f−1F. a_Y^{-1}f^{-1}F \simeq\widetilde f^{-1}a_X^{-1}F \simeq\widetilde f^{-1}p_X^{-1}F \simeq p_Y^{-1}f^{-1}F.

The middle map is transport for FF, with its direction inverted as needed. SH02-CON-COMPARISON proves conicity.

For extraordinary inverse image, functoriality of !! for the two commuting composites gives

aY!f!F≃f̃!aX!F≃f̃!pX!F≃pY!f!F. a_Y^!f^!F\simeq\widetilde f^!a_X^!F \simeq\widetilde f^!p_X^!F\simeq p_Y^!f^!F.

The middle isomorphism is the shift of transport by [1][1]. The orientations used for aY,pY,aX,pXa_Y,p_Y,a_X,p_X all use log⁡t\log t, preserved by f̃\widetilde f. Hence their relative shifts agree and no minus sign is introduced. The extraordinary version of SH02-CON-COMPARISON applies.

For proper direct image, both squares with horizontal maps pY,pXp_Y,p_X and with horizontal maps aY,aXa_Y,a_X are Cartesian. For the action square this deserves verification: given (x,t)(x,t) and yy with aX(x,t)=f(y)a_X(x,t)=f(y), the unique preimage is (aY(y,t−1),t)(a_Y(y,t^{-1}),t), because equivariance gives f(aY(y,t−1))=xf(a_Y(y,t^{-1}))=x. Proper base change therefore supplies

aX−1Rf!K≃Rf̃!aY−1K≃Rf̃!pY−1K≃pX−1Rf!K. a_X^{-1}Rf_!K\simeq R\widetilde f_!a_Y^{-1}K \simeq R\widetilde f_!p_Y^{-1}K \simeq p_X^{-1}Rf_!K.

Here ff need not be proper: base change is for Rf!Rf_!, whose supports are already proper over the target.

For ordinary direct image we justify the product base-change map instead of applying nonproper base change indiscriminately. The canonical map

pX−1Rf*K⟶Rf̃*pY−1K p_X^{-1}Rf_*K\longrightarrow R\widetilde f_*p_Y^{-1}K

is an isomorphism on stalks. Indeed, rectangles V×IV\times I with II an open interval form a neighbourhood basis at (x,t)(x,t). The right-hand stalk is the filtered colimit of Hj(f−1V×I;pY−1K)H^j(f^{-1}V\times I;p_Y^{-1}K), which the cylinder lemma identifies naturally with Hj(f−1V;K)H^j(f^{-1}V;K), with the canonical pullback map providing that identification. Their colimit is Hj(Rf*K)xH^j(Rf_*K)_x, the left-hand stalk. The same holds for the action square by applying the homeomorphisms hX,hYh_X,h_Y; equivariance gives hXf̃=f̃hYh_X\widetilde f=\widetilde f h_Y. Thus

aX−1Rf*K≃Rf̃*aY−1K≃Rf̃*pY−1K≃pX−1Rf*K, a_X^{-1}Rf_*K\simeq R\widetilde f_*a_Y^{-1}K \simeq R\widetilde f_*p_Y^{-1}K \simeq p_X^{-1}Rf_*K,

and conicity follows. The rectangle argument is valid for bounded-below complexes because inverse image and stalk formation are exact and the cylinder lemma was proved in D+D^+.

For tensor products, exact inverse image commutes with derived tensor, and therefore

aX−1(F1⊗LF2)≃aX−1F1⊗LaX−1F2≃pX−1F1⊗LpX−1F2≃pX−1(F1⊗LF2). a_X^{-1}(F_1\otimes^L F_2) \simeq a_X^{-1}F_1\otimes^L a_X^{-1}F_2 \simeq p_X^{-1}F_1\otimes^L p_X^{-1}F_2 \simeq p_X^{-1}(F_1\otimes^L F_2).

If the two lower cohomological bounds are b1,b2b_1,b_2, finite global dimension dd gives lower bound b1+b2−db_1+b_2-d for their derived tensor product. Thus it really is an object of D+D^+, as required by the conicity criterion.

For internal Hom, put H=Rℋom(F1,F2)H=R\mathcal Hom(F_1,F_2). If F1F_1 has upper bound cc and F2F_2 lower bound bb, derived Hom has lower bound b−cb-c. The extraordinary inverse-image/internal-Hom comparison, (EXA.2), gives

aX!H≃Rℋom(aX−1F1,aX!F2)≃Rℋom(pX−1F1,pX!F2)≃pX!H. \begin{aligned} a_X^!H &\simeq R\mathcal Hom(a_X^{-1}F_1,a_X^!F_2)\\ &\simeq R\mathcal Hom(p_X^{-1}F_1,p_X^!F_2) \simeq p_X^!H. \end{aligned}

This proves conicity by the extraordinary comparison criterion. It does not assume that arbitrary inverse image commutes with internal Hom, an identity which would require additional justification. ▫\square

All comparisons in this proof are composites of specified units, counits, base-change maps, functor-composition maps, and θ\theta. Their restrictions at t=1t=1 are identities by the adjunction and base-change identities. Hence they give the canonical transport on the resulting conic object by SH02-CON-COCYCLE. In particular this compatibility statement is independent of a chosen isomorphism witnessing condition four.

External products. If F∈DG+(X)F\in D_G^+(X) and K∈DG+(Y)K\in D_G^+(Y), put F⊠LK=prX−1F⊗LprY−1KF\boxtimes^L K=\mathrm{pr}_X^{-1}F\otimes^L\mathrm{pr}_Y^{-1}K. It is invariant under the two scaling parameters independently: pullback by (x,y,s,t)↦(aX(x,s),aY(y,t))(x,y,s,t)\mapsto(a_X(x,s),a_Y(y,t)) is identified with pullback by the projection using the two transport isomorphisms and tensor. Thus its cohomology is locally constant along each parametrized G2G^2-orbit. This is what biconic means here. Pulling this isomorphism back along s=ts=t proves conicity for the diagonal action. Finite global dimension gives the same lower bound as for tensor, so the external product remains in D+D^+.

SH02-CON-EXAMPLE — A large angular family with zero ordinary sections

Let E=Z×ℝ2E=Z\times\mathbb R^2 and let j:Z×(ℝ2\{0})↪Ej:Z\times(\mathbb R^2\setminus\{0\})\hookrightarrow E be the open embedding. Define

q:Z×(ℝ2\{0})⟶Z×S1,q(z,v)=(z,v/|v|), q:Z\times(\mathbb R^2\setminus\{0\})\longrightarrow Z\times S^1, \qquad q(z,v)=(z,v/|v|),

and let s:Z×S1→Zs:Z\times S^1\to Z. For an arbitrary L∈D+(Z×S1)L\in D^+(Z\times S^1) set F=j!q−1LF=j_!q^{-1}L. The angular data LL need not be locally constant, constructible, or of finite rank.

The action on Z×S1Z\times S^1 is trivial. Every object there is conic, because each parametrized orbit is a constant map. Both qq and jj are equivariant; the fibres of qq are one-dimensional and j!j_! is exact, so the functor theorem proves that FF is conic. Since extension by zero has zero stalks along the complement of its open domain, i−1F=0i^{-1}F=0. Ordinary contraction therefore gives

Rτ*F=0. R\tau_*F=0.

Polar coordinates identify qq with projection from (Z×S1)×(0,∞)(Z\times S^1)\times(0,\infty), with radial orientation drdr. The projection formula and interval integration give Rq!q−1L≃L[−1]Rq_!q^{-1}L\simeq L[-1]. Composition of proper direct images, and properness of ss, now give

Rτ!F≃Rs*L[−1],i!F≃Rs*L[−1]. R\tau_!F\simeq Rs_*L[-1],\qquad i^!F\simeq Rs_*L[-1].

This displays a conic sheaf whose ordinary direct image vanishes while its proper direct image can be large. It also tests the direction of both contraction maps: the ordinary one reads a stalk, while the proper one reads a costalk.

For a concrete non-finite module, take ZZ to be a point, A=ℤA=\mathbb Z, and L=MS1L=M_{S^1} with M=ℚ⊕⨁m≥1ℤ/2ℤM=\mathbb Q\oplus\bigoplus_{m\ge1}\mathbb Z/2\mathbb Z. The two-arc Cech complex used above is now [M2→(a,b)↦(b−a,b−a)M2][M^2\xrightarrow{(a,b)\mapsto(b-a,b-a)}M^2]. Splitting its source into diagonal and difference coordinates and its target into diagonal and a complementary coordinate gives one copy of MM in degree zero, one in degree one, and a contractible identity summand. Consequently

RΓ(S1;MS1)≃M⊕M[−1],RΓc(E;F)≃M[−1]⊕M[−2]. R\Gamma(S^1;M_{S^1})\simeq M\oplus M[-1],\qquad R\Gamma_c(E;F)\simeq M[-1]\oplus M[-2].

Every use of interval acyclicity in this calculation applies to this arbitrary module. No finite-rank substitute was made.

SH02-CON-EXERCISE-MONODROMY — Transport after one period

Exercise. Give S1S^1 the action a(z,t)=eilog⁡tza(z,t)=e^{i\log t}z. Let NN be any AA-module and let T:N→NT:N\to N be an automorphism. Let LTL_T be the locally constant sheaf whose positive monodromy is TT. Compute its cohomology and the restriction to U=S1\{1}U=S^1\setminus\{1\}. Determine the canonical action transport at t=e2πt=e^{2\pi} after identifying the fibre at one chosen point with NN.

Solution. Trivialize on two arcs as in the circle calculation, using one intersection component to identify the trivializations and the other to record TT. The Cech differential is, with one choice of ordering,

N⊕N⟶N⊕N,(u,v)⟼(v−u,v−Tu). N\oplus N\longrightarrow N\oplus N, \qquad (u,v)\longmapsto(v-u,v-Tu).

Subtract the first target coordinate from the second, and write the source in coordinates (u,w=v−u)(u,w=v-u). The differential becomes (u,w)↦(w,(1−T)u)(u,w)\mapsto(w,(1-T)u). The identity map on the ww coordinate is a contractible summand, leaving the two-term complex [N→1−TN][N\xrightarrow{1-T}N] in degrees zero and one. All intersections are acyclic for a locally constant sheaf by the interval import, so this complex computes derived sections. Hence

H0(S1;LT)=ker⁡(T−1),H1(S1;LT)=coker⁡(T−1),Hj=0(j≠0,1). H^0(S^1;L_T)=\ker(T-1),\quad H^1(S^1;L_T)=\operatorname{coker}(T-1),\quad H^j=0\ (j\ne0,1).

The restriction to UU is constant with fibre NN. In degree zero the map is evaluation of invariant sections, namely ker⁡(T−1)↪N\ker(T-1)\hookrightarrow N; in degree one it maps coker⁡(T−1)\operatorname{coker}(T-1) to zero. Thus this restriction need not be an isomorphism even though UU meets the orbit in a contractible arc.

On the parametrized orbit ℝ→S1\mathbb R\to S^1, increasing log⁡t\log t traces the positive path. Local-system transport along that path defines a map p−1LT→a−1LTp^{-1}L_T\to a^{-1}L_T restricting to the identity at t=1t=1. By SH02-CON-COCYCLE it equals θLT\theta_{L_T}. After one period its value is therefore TT, although the underlying homeomorphism of S1S^1 at that parameter is the identity. A periodic point is not a reason to force the action transport to be the identity. ▫\square

SH02-CON-EXERCISE-BOUNDARY — Zero rank and a trivial action

Exercise. Check the comparison maps for a trivial action and for a rank-zero bundle. Explain why a radial shift [n][n] must not be inserted into either contraction theorem.

Solution. For a trivial action a=pa=p, and a−1F=p−1Fa^{-1}F=p^{-1}F for every F∈D+(X)F\in D^+(X). The unit F→Rp*p−1FF\to Rp_*p^{-1}F and evaluation are inverse by the cylinder lemma. The counit and evaluation in the definition of θF\theta_F consequently give the identity of p−1Fp^{-1}F; this also follows from uniqueness of normalized transport. No condition on the cohomology of FF in the XX direction appears. The restriction criterion in this case requires U=XU=X: if x∉Ux\notin U, then Tx(U)T_x(U) is empty.

For rank zero, E=ZE=Z and both maps ii and τ\tau are identities. Their units and counits are identities, so ρF\rho_F and σF\sigma_F are identities. In positive rank the two theorems identify direct images with the actual inverse and extraordinary inverse images along the zero section; any codimension shift is already contained in a separate computation of i!Fi^!F. For example, the costalk in SH02-CON-EXAMPLE has degrees one and two although its ordinary stalk is zero. Inserting another radial shift would contradict that computed proper cohomology. ▫\square

SH02-CON-BOUNDARY — Scope and remaining proof dependencies

What the consulted sources establish. The comparisons here use the 1985 Astérisque 128 edition, §2.1.1, printed pp. 39–41 (PDF pp. 42–44), and Schapira’s An Introduction to Sheaves on Grothendieck Topologies, 1 August 2026 version. They concern the actual passages listed below, not the other works cited within those passages. No statement about an excluded book’s definitions, theorem numbering or errata is needed for the results of this unit.

Step in this unit Consulted passage and its scope Argument supplied here
Positive-ray conicity Astérisque 128, §2.1.1, p. 39, uses bounded-below complexes on a real vector bundle over a locally compact base, with locally constant cohomology on half-lines. Schapira, Definition 5.4.4, p. 114, uses bounded complexes on a finite-dimensional vector bundle over a real manifold. SH02-CON-DEFINITION specifies parameter pullbacks for general continuous actions. The stabilizer classification proves equivalence with homogeneous-orbit pullback. The proper-support dense-orbit example proves that the induced-subspace condition can be strictly stronger.
Cylinder descent and its maps Schapira, Proposition 3.5.3 and Lemma 3.6.4, pp. 73–75, prove interval constancy and the compact-interval product unit. Exercise 3.18, pp. 78–79, proposes a proper contractible exhaustion argument for bounded complexes. SH02-CON-CYLINDER first applies proper base change to closed strips, then uses the separate closed-exhaustion bridge for their noncompact open-base restrictions. It checks the evaluation, counit and unit individually. The degreewise spectral sequence is bounded below; a uniform upper bound is unnecessary.
Open interval fibres and restriction Schapira, Theorem 4.5.3 and equation (4.5.4), p. 93, give proper-direct-image base change and its compact-support fibre formula. Proposition 4.6.6, pp. 95–96, identifies internal duality by the counit; Proposition 5.1.9, pp. 107–108, identifies the submersion dualizing object for bounded-below input. SH02-CON-INTERVAL-FIBRES applies base change to the trace, then internal duality to identify the specified ordinary unit. SH02-CON-RESTRICTION computes the action map’s actual fibres and checks that the composite is restriction. The periodic circle and monodromy solution detect why an orbit-image test loses winding.
The two radial contractions Schapira, Exercise 5.13, p. 120, states both contractions for bounded conic objects over a locally compact base of finite soft dimension. It is an exercise, not a proof of the larger scope used here. SH02-CON-RADIAL-STAR uses a local product-ball basis and compatible restrictions. SH02-CON-RADIAL-SUPPORT compares localization triangles, then proves disk supports cofinal after shrinking at a base point. Both identify the actual maps. Neither uses a global metric, a finite-soft-dimension base, double-dual reflexivity, finite generation, or an extra radial shift.
Equivariant operations Schapira, §§4.4–4.6, pp. 90–98, supplies projection, base-change and adjunction machinery; Proposition 4.6.5 prints the exceptional internal-Hom identity for bounded inputs. Astérisque 128, Propositions 2.1.5–2.1.6, p. 41, concerns vector-bundle Fourier functoriality. SH02-CON-FUNCTORS proves each action comparison separately, including the Cartesian action square and ordinary product base change by rectangles. Its internal-Hom conclusion uses the explicit exceptional-operation contract at the stated bounds, not an unsupported inverse-image/internal-Hom interchange or a wholesale import of vector-bundle Fourier functoriality.

The proper-support calculation deserves a further distinction. Schapira’s Definition 4.2.2 and Remark 4.2.5, pp. 85–86, identify sections of proper direct image by closed supports proper over the target open set. They do not permit replacing properness by compactness of each individual fibre. That is why the dense-orbit proof bounds a section’s support over a compact target neighbourhood, and the radial proof shrinks the base before choosing a disk radius. The support-to-stalk comparison and its derived version are still named imports in SH02-CON-CONTRACT; the new geometric cofinality argument is supplied in full here.

The contraction statements themselves are established antecedents, and no priority claim is made for them or for a restriction criterion. The general action formulation, normalized maps, topology comparison and counterexamples are justified by the complete arguments in this reader, under the explicit definitions and hypotheses stated here. The independently authored course prose, proofs and figures remain under the edition’s CC0 dedication. The linked human works retain their own terms; in particular Astérisque 128 carries the Société mathématique de France 1985 copyright notice. Access for consultation does not relicense those works.

This unit proves the parametrized-orbit criterion, its canonical comparisons and ordinary derived-category cocycle, the actual-parameter restriction theorem with a counterexample to the overly broad orbit-image assertion, all listed equivariant operations with their stated boundedness, and both vector-bundle contractions. Fixed points, periodic actions, nonembedded orbits under the declared topology, zero rank, empty base, nonproper bundle projections, and arbitrary coefficient modules are accounted for.

The five prerequisite families in SH02-CON-CONTRACT remain explicit. The interval evaluation theorem, the closed-exhaustion comparison with its limit proofs, and the proper-fibre and hypercohomology proofs supply the cylinder inputs at the stated bounded-below scope. The closed-exhaustion argument includes noncompact strips; a bounded-complex exercise alone would not establish that scope. SH02-MD-SUBMERSION and SH02-MD-TRACE supply the orientation/trace package, its normalization and submersion base-change compatibility. Other parts of the derived sheaf formalism and the derived proper-support stalk formula retain their explicitly stated contracts. The exceptional internal-Hom contract with bounded-above first input and bounded-below second input is supplied by SH02-EX-BOUNDED-ABOVE at exactly that scope. Its finite resolution proof does not impose an upper bound on the second input. The separate unbounded supported-evaluation proof supplies the support-forgetting comparison without narrowing its first input; it is not needed to replace the interval argument above. Other declared prerequisites retain their own proof obligations. SH02-CON-EXAMPLE-DENSE-ORBIT proves that an induced-subspace interpretation of nonembedded orbits can give a strictly smaller category. This unit supplies no Fourier-Sato equivalence, specialization, microlocalization, microsupport estimate, or involutivity proof; these are subsequent course obligations. The source comparisons above do not by themselves admit the course or discharge its remaining proof dependencies.