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An algebraic cycle ZZZ of codimension ppp has a unique cohomology class cl(Z)∈H2p(X,C)\mathrm{cl}(Z)\in H^{2p}(X,\mathbb{C})cl(Z)∈H2p(X,C) dual to ∫Z\int_Z∫Z​

Open
HodgeConjecture.existsUnique_cycleClass

by korbonits · Sep 8, 2026 · Mathlib 0df444a (Lean v4.33.1)

algebraic-cyclesalgebraic-geometrycomplex-geometryhodge-conjecturehodge-theorymillennium-prize

Deligne (pp. 1–2): "If ZZZ is a closed analytic subspace of XXX, of complex codimension ppp, ZZZ is an integral cycle and, by Poincaré duality, defines a class cl(Z)\mathrm{cl}(Z)cl(Z) in H2p(X,Z)H^{2p}(X,\mathbb{Z})H2p(X,Z). The integration current on ZZZ is a closed (p,p)(p,p)(p,p)-form with generalized function coefficients, representing the image of cl(Z)\mathrm{cl}(Z)cl(Z) in H2p(X,C)H^{2p}(X,\mathbb{C})H2p(X,C)." By Chow's theorem (Remark (i)) algebraic cycles and closed analytic subspaces coincide.

Let X⊂PN(C)X\subset\mathbb{P}^N(\mathbb{C})X⊂PN(C) be non-singular of dimension nnn, let p≤np\le np≤n, and let Z⊂XZ\subset XZ⊂X be an irreducible algebraic subvariety of dimension n−pn-pn−p. Then there is exactly one class c∈H2p(X,C)c\in H^{2p}(X,\mathbb{C})c∈H2p(X,C) such that

∫Xc∧η=∫Zηfor every closed (2n−2p)-form η on X,\int_X c\wedge\eta=\int_Z\eta\qquad\text{for every closed }(2n-2p)\text{-form }\eta\text{ on }X,∫X​c∧η=∫Z​ηfor every closed (2n−2p)-form η on X,

where ∫Z\int_Z∫Z​ is the integral over the smooth locus of ZZZ with its complex orientation. This class is cl(Z)\mathrm{cl}(Z)cl(Z).

Existence says that the integration current of ZZZ is a closed current cohomologous to a smooth form (Lelong's theorem on the finiteness and closedness of the current of integration, plus de Rham's theorem for currents); uniqueness is Poincaré duality, the non-degeneracy of the pairing H2p×H2n−2p→CH^{2p}\times H^{2n-2p}\to\mathbb{C}H2p×H2n−2p→C. Without this theorem the predicate "is the class of ZZZ" used in the Hodge conjecture would have no witness.

Formalization Note ∫Zη\int_Z\eta∫Z​η integrates η\etaη evaluated on a positively oriented orthonormal frame of the tangent space of ZZZ against the 2(n−p)2(n-p)2(n−p)-dimensional normalised Hausdorff measure on the smooth locus of ZZZ; ∫Xc∧η\int_X c\wedge\eta∫X​c∧η uses a representative of ccc and the 2n2n2n-dimensional measure on XXX. Both quantities are independent of the choices involved, which is part of what a proof must establish.

Preamble
import Definitions.Def_HodgeConjecture
import Mathlib
Formal statement
namespace HodgeConjecture
theorem existsUnique_cycleClass (N n p : ℕ) (hp : p ≤ n) (X Z : ProjVariety N)
    (hX : X.IsNonsingular n) (hZX : Z.cone ⊆ X.cone) (hZ : Z.IsIrreducible) (hd : Z.dim = n - p) :
    ∃! c : X.Cohomology (2 * p), X.IsCycleClass Z n p c := by sorry
end HodgeConjecture
Source
P. Deligne, The Hodge Conjecture, Clay Mathematics Institute Millennium Prize Problem description (2000), https://www.claymath.org/wp-content/uploads/2022/06/hodge.pdf, pp. 1–2: 'Z is an integral cycle and, by Poincaré duality, defines a class cl(Z) in H^{2p}(X,ℤ). The integration current on Z is a closed (p,p)-form ... representing the image of cl(Z) in H^{2p}(X,ℂ)'; Remark (i), p. 2 (Chow's theorem)
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What the Lean code literally says, in plain math · claude-fable-5-1

Read-back: HodgeConjecture.existsUnique_cycleClass

Shape of the statement

For every choice of natural numbers N,n,pN, n, pN,n,p with p≤np \le np≤n, and every pair of "projective varieties" X,ZX, ZX,Z in the sense defined below (both living in the same ambient PN\mathbb{P}^NPN-model), if

  • XXX is "nonsingular of dimension nnn" (definition below),
  • the cone of ZZZ is contained in the cone of XXX (as subsets of CN+1\mathbb{C}^{N+1}CN+1),
  • ZZZ is "irreducible" (definition below), and
  • the "dimension" of ZZZ equals n−pn - pn−p (natural-number subtraction; harmless here because p≤np \le np≤n),

then there exists a unique element ccc of the complex vector space H2p(X)H^{2p}(X)H2p(X) (the custom cohomology defined below) such that ccc "is a cycle class of ZZZ" in the custom sense IsCycleClassX(Z,n,p,c)\mathrm{IsCycleClass}_X(Z, n, p, c)IsCycleClassX​(Z,n,p,c) spelled out below. Uniqueness means: any c′c'c′ in H2p(X)H^{2p}(X)H2p(X) satisfying the same property is equal to ccc as an element of the quotient space H2p(X)H^{2p}(X)H2p(X) (i.e. two closed representatives of ccc and c′c'c′ differ by an element of the "exact forms" submodule). Nothing else is asserted; in particular ccc ranges over the whole complex vector space H2p(X)H^{2p}(X)H2p(X) with no rationality, integrality or Hodge-type condition in the statement.

Everything below unfolds the custom notions to Mathlib primitives.

Ambient objects

  • Coordinates. CoordN:=CN+1\mathrm{Coord}_N := \mathbb{C}^{N+1}CoordN​:=CN+1 (functions {0,…,N}→C\{0,\dots,N\}\to\mathbb{C}{0,…,N}→C).
  • Polynomials. PolyN:=\mathrm{Poly}_N :=PolyN​:= polynomials over C\mathbb{C}C in the N+1N+1N+1 variables x0,…,xNx_0,\dots,x_Nx0​,…,xN​.
  • Ambient space. AmbN:=C(N+1)×(N+1)\mathrm{Amb}_N := \mathbb{C}^{(N+1)\times(N+1)}AmbN​:=C(N+1)×(N+1), the space of (N+1)×(N+1)(N+1)\times(N+1)(N+1)×(N+1) complex matrices with the ℓ2\ell^2ℓ2 (Hilbert–Schmidt/Frobenius) inner product ⟨A,B⟩=∑i,jAij‾Bij\langle A,B\rangle = \sum_{i,j}\overline{A_{ij}}B_{ij}⟨A,B⟩=∑i,j​Aij​​Bij​; it is a complex inner-product space of real dimension 2(N+1)22(N+1)^22(N+1)2.
  • Projection map. π:CN+1→AmbN\pi:\mathbb{C}^{N+1}\to \mathrm{Amb}_Nπ:CN+1→AmbN​,
π(v)ij=vi vj‾∑k∣vk∣2.\pi(v)_{ij} = \frac{v_i\,\overline{v_j}}{\sum_k |v_k|^2}.π(v)ij​=∑k​∣vk​∣2vi​vj​​​.

For v≠0v\neq 0v=0 this is the rank-one Hermitian projector onto the line Cv\mathbb{C}vCv; it is constant on complex lines through 000. For v=0v=0v=0 the denominator is 000 and division by zero in C\mathbb{C}C returns 000, so π(0)\pi(0)π(0) is the zero matrix (this case never arises below, since cones exclude 000).

  • JJJ-map. For matrices P,AP,AP,A: JP(A):=i (AP−PA)=i[A,P]J_P(A) := i\,(AP - PA) = i[A,P]JP​(A):=i(AP−PA)=i[A,P].
  • Real inner product. ⟨a,b⟩R:=Re⁡⟨a,b⟩\langle a,b\rangle_{\mathbb{R}} := \operatorname{Re}\langle a,b\rangle⟨a,b⟩R​:=Re⟨a,b⟩ on AmbN\mathrm{Amb}_NAmbN​.
  • Zero set. For a set SSS of polynomials, Z(S):={v∈CN+1:Q(v)=0 for all Q∈S}\mathcal{Z}(S) := \{v\in\mathbb{C}^{N+1} : Q(v)=0 \text{ for all } Q\in S\}Z(S):={v∈CN+1:Q(v)=0 for all Q∈S}.

"Projective varieties" and their attributes

A ProjVariety XXX over NNN is a set EXE_XEX​ of polynomials (no finiteness assumed) together with a proof that every Q∈EXQ\in E_XQ∈EX​ is homogeneous of some degree dQ∈Nd_Q\in\mathbb{N}dQ​∈N (each polynomial may have its own degree; degree 000, i.e. constants, including nonzero constants, is allowed; the zero polynomial counts as homogeneous). Nothing else is recorded.

  • Cone. CX:={v∈CN+1:v≠0, v∈Z(EX)}C_X := \{v\in\mathbb{C}^{N+1} : v\neq 0,\ v\in\mathcal{Z}(E_X)\}CX​:={v∈CN+1:v=0, v∈Z(EX​)}, the nonzero common zeros of EXE_XEX​. It may be empty (e.g. if EXE_XEX​ contains a nonzero constant).
  • Points. ptsX:=π(CX)⊆AmbN\mathrm{pts}_X := \pi(C_X)\subseteq \mathrm{Amb}_NptsX​:=π(CX​)⊆AmbN​, the set of rank-one projectors onto lines of the cone (a model of the projective variety inside matrix space).
  • Vanishing set. IX:={Q∈PolyN:Q(v)=0 for all v∈CX}I_X := \{Q\in\mathrm{Poly}_N : Q(v)=0 \text{ for all } v\in C_X\}IX​:={Q∈PolyN​:Q(v)=0 for all v∈CX​}; all polynomials (homogeneous or not) vanishing on the cone. If CX=∅C_X=\emptysetCX​=∅ then IXI_XIX​ is all polynomials.
  • Jacobian form. For QQQ and vvv: the C\mathbb{C}C-linear map dQv:CN+1→CdQ_v:\mathbb{C}^{N+1}\to\mathbb{C}dQv​:CN+1→C, u↦∑i∂Q∂xi(v) uiu\mapsto\sum_i \frac{\partial Q}{\partial x_i}(v)\,u_iu↦∑i​∂xi​∂Q​(v)ui​.
  • Tangent cone. For any v∈CN+1v\in\mathbb{C}^{N+1}v∈CN+1 (not only v∈CXv\in C_Xv∈CX​),
TX(v):=⋂Q∈IXker⁡(dQv) ⊆ CN+1,T_X(v) := \bigcap_{Q\in I_X}\ker(dQ_v)\ \subseteq\ \mathbb{C}^{N+1},TX​(v):=Q∈IX​⋂​ker(dQv​) ⊆ CN+1,

a complex subspace (the Zariski tangent space of the affine cone at vvv, computed from the full vanishing set IXI_XIX​, not from EXE_XEX​).

  • IsNonsingular nnn. XXX is nonsingular of dimension nnn iff for every v∈CXv\in C_Xv∈CX​, dim⁡CTX(v)=n+1\dim_{\mathbb{C}} T_X(v) = n+1dimC​TX​(v)=n+1. This is vacuously true when CX=∅C_X=\emptysetCX​=∅.
  • Tangent space at a point. For P∈AmbNP\in\mathrm{Amb}_NP∈AmbN​,
TX(P):=∑v∈CXπ(v)=PDπv(TX(v)) ⊆ AmbN,\mathcal{T}_X(P) := \sum_{\substack{v\in C_X\\ \pi(v)=P}} D\pi_v\big(T_X(v)\big)\ \subseteq\ \mathrm{Amb}_N,TX​(P):=v∈CX​π(v)=P​∑​Dπv​(TX​(v)) ⊆ AmbN​,

the real subspace spanned by the images of the tangent cones TX(v)T_X(v)TX​(v) (viewed as real subspaces) under the real Fréchet derivative Dπv:CN+1→AmbND\pi_v:\mathbb{C}^{N+1}\to\mathrm{Amb}_NDπv​:CN+1→AmbN​ of π\piπ at vvv, summed over all vvv in the fibre of π\piπ over PPP lying in the cone. If no such vvv exists (in particular if P∉ptsXP\notin\mathrm{pts}_XP∈/ptsX​) this is the zero subspace. (π\piπ is smooth away from 000, so for v∈CXv\in C_Xv∈CX​ this is the genuine derivative; it kills the direction Cv\mathbb{C}vCv since π\piπ is constant on complex lines.)

  • IsIrreducible. XXX is irreducible iff CX≠∅C_X\neq\emptysetCX​=∅ and for all sets of polynomials S1,S2S_1,S_2S1​,S2​ (arbitrary, not necessarily homogeneous): if CX⊆Z(S1)∪Z(S2)C_X\subseteq\mathcal{Z}(S_1)\cup\mathcal{Z}(S_2)CX​⊆Z(S1​)∪Z(S2​) then CX⊆Z(S1)C_X\subseteq\mathcal{Z}(S_1)CX​⊆Z(S1​) or CX⊆Z(S2)C_X\subseteq\mathcal{Z}(S_2)CX​⊆Z(S2​).
  • Dimension.
dim⁡X:=(inf⁡{dim⁡CTX(v):v∈CX})  −˙  1,\dim X := \Big(\inf\{\dim_{\mathbb{C}} T_X(v) : v\in C_X\}\Big) \;\dot{-}\; 1,dimX:=(inf{dimC​TX​(v):v∈CX​})−˙​1,

where the infimum is over a set of natural numbers (so it is a minimum when CX≠∅C_X\neq\emptysetCX​=∅, and equals 000 by Mathlib's convention inf⁡∅=0\inf\emptyset = 0inf∅=0 when CX=∅C_X=\emptysetCX​=∅), and −˙\dot{-}−˙​ is truncated subtraction on N\mathbb{N}N (0−˙1=00\dot{-}1 = 00−˙​1=0). So dim⁡X=0\dim X = 0dimX=0 both when the cone is empty and when the minimum tangent rank is 000 or 111.

  • Regular points. regX:=π({v∈CX:dim⁡CTX(v)=dim⁡X+1})\mathrm{reg}_X := \pi\big(\{v\in C_X : \dim_{\mathbb{C}}T_X(v) = \dim X + 1\}\big)regX​:=π({v∈CX​:dimC​TX​(v)=dimX+1}): images of cone points whose tangent-cone rank is exactly dim⁡X+1\dim X + 1dimX+1. If the minimum rank mmm over the cone is ≥1\ge 1≥1, then dim⁡X+1=m\dim X + 1 = mdimX+1=m and regX\mathrm{reg}_XregX​ is the (nonempty) image of the rank-minimising locus. If CX=∅C_X=\emptysetCX​=∅, regX=∅\mathrm{reg}_X=\emptysetregX​=∅; if m=0m=0m=0 then dim⁡X+1=1≠m\dim X+1 = 1\ne mdimX+1=1=m and regX\mathrm{reg}_XregX​ could be empty. (For vvv in a cone, vvv itself lies in ker⁡dQv\ker dQ_vkerdQv​ for every QQQ vanishing on the cone, by Euler's relation applied to the homogeneous components, so in fact m≥1m\ge 1m≥1 whenever the cone is nonempty; the definition does not rely on this.)

Forms and the custom cohomology

  • kkk-forms. ΩNk:=\Omega^k_N := ΩNk​:= all functions ω:AmbN→AltRk(AmbN;C)\omega:\mathrm{Amb}_N\to \mathrm{Alt}^k_{\mathbb{R}}(\mathrm{Amb}_N;\mathbb{C})ω:AmbN​→AltRk​(AmbN​;C), where the target is the space of continuous real-multilinear alternating maps (AmbN)k→C(\mathrm{Amb}_N)^k\to\mathbb{C}(AmbN​)k→C. No regularity is built in; forms live on the whole ambient matrix space, not on XXX. A 000-form is just a function AmbN→C\mathrm{Amb}_N\to\mathbb{C}AmbN​→C. ΩNk\Omega^k_NΩNk​ is a complex vector space (scalars act on values).
  • Vanishes on XXX. ω∈ΩNk\omega\in\Omega^k_Nω∈ΩNk​ vanishes on XXX iff for every P∈ptsXP\in\mathrm{pts}_XP∈ptsX​ and every kkk-tuple (v1,…,vk)(v_1,\dots,v_k)(v1​,…,vk​) with all vi∈TX(P)v_i\in\mathcal{T}_X(P)vi​∈TX​(P), ωP(v1,…,vk)=0\omega_P(v_1,\dots,v_k)=0ωP​(v1​,…,vk​)=0. (For k=0k=0k=0 this says ω(P)=0\omega(P)=0ω(P)=0 for all P∈ptsXP\in\mathrm{pts}_XP∈ptsX​.)
  • Exterior derivative. dω∈ΩNk+1d\omega\in\Omega^{k+1}_Ndω∈ΩNk+1​ is Mathlib's extDeriv: at each point, the alternating (k+1)(k+1)(k+1)-form obtained from the real Fréchet derivative of ω\omegaω, (dω)P(v0,…,vk)=∑i(−1)i (DωP⋅vi)(v0,…,vi^,…,vk)(d\omega)_P(v_0,\dots,v_k)=\sum_i (-1)^i\,(D\omega_P\cdot v_i)(v_0,\dots,\widehat{v_i},\dots,v_k)(dω)P​(v0​,…,vk​)=∑i​(−1)i(DωP​⋅vi​)(v0​,…,vi​​,…,vk​); at points where ω\omegaω is not differentiable the derivative is 000. (It is used only inside "vanishes on XXX" conditions, which are insensitive to nonzero normalisation constants.)
  • Smooth. "ω\omegaω is smooth" means C∞C^\inftyC∞ over R\mathbb{R}R as a map from all of AmbN\mathrm{Amb}_NAmbN​ into the normed space of alternating maps.
  • IsClosedForm. ω∈ΩNk\omega\in\Omega^k_Nω∈ΩNk​ is closed for XXX iff ω\omegaω is smooth and dωd\omegadω vanishes on XXX (in the tangential sense above). Note ω\omegaω itself is not required to vanish or be anything on XXX; closedness is tested only on TX(P)\mathcal{T}_X(P)TX​(P) for P∈ptsXP\in\mathrm{pts}_XP∈ptsX​.
  • IsExactForm. For k=0k=0k=0: ω\omegaω is smooth and vanishes on XXX. For k≥1k\ge1k≥1: ω\omegaω is smooth and there exists a smooth α∈ΩNk−1\alpha\in\Omega^{k-1}_Nα∈ΩNk−1​ with ω−dα\omega - d\alphaω−dα vanishing on XXX.
  • Closed / exact submodules. CXk:=span⁡C{ω:ω closed for X}\mathcal{C}^k_X := \operatorname{span}_{\mathbb{C}}\{\omega : \omega \text{ closed for } X\}CXk​:=spanC​{ω:ω closed for X} and EXk:=span⁡C{ω:ω exact for X}\mathcal{E}^k_X := \operatorname{span}_{\mathbb{C}}\{\omega : \omega \text{ exact for } X\}EXk​:=spanC​{ω:ω exact for X}, both complex subspaces of ΩNk\Omega^k_NΩNk​.
  • Cohomology. Hk(X):=H^k(X) :=Hk(X):= the image of CXk\mathcal{C}^k_XCXk​ under the canonical quotient map ΩNk→ΩNk/EXk\Omega^k_N\to\Omega^k_N/\mathcal{E}^k_XΩNk​→ΩNk​/EXk​; a complex subspace of that quotient. Its elements are classes [ω][\omega][ω] with ω∈CXk\omega\in\mathcal{C}^k_Xω∈CXk​, and [ω]=[ω′][\omega]=[\omega'][ω]=[ω′] iff ω−ω′∈EXk\omega-\omega'\in\mathcal{E}^k_Xω−ω′∈EXk​. (Nothing in the definition forces EXk⊆CXk\mathcal{E}^k_X\subseteq\mathcal{C}^k_XEXk​⊆CXk​.)
  • Class. For ω∈CXk\omega\in\mathcal{C}^k_Xω∈CXk​, clsX(ω):=[ω]∈Hk(X)\mathrm{cls}_X(\omega) := [\omega]\in H^k(X)clsX​(ω):=[ω]∈Hk(X).

Frames, measures, wedge, pairing, integral

  • JJJ-frame. Given a real subspace T⊆AmbNT\subseteq\mathrm{Amb}_NT⊆AmbN​, a matrix PPP, and u=(u0,…,um−1)u=(u_0,\dots,u_{m-1})u=(u0​,…,um−1​) in AmbN\mathrm{Amb}_NAmbN​: uuu is a JJJ-frame for (T,P)(T,P)(T,P) iff (i) every ui∈Tu_i\in Tui​∈T; (ii) ⟨ui,uj⟩R=δij\langle u_i,u_j\rangle_{\mathbb{R}}=\delta_{ij}⟨ui​,uj​⟩R​=δij​ (real orthonormality for Re⁡⟨⋅,⋅⟩\operatorname{Re}\langle\cdot,\cdot\rangleRe⟨⋅,⋅⟩); (iii) ⟨ui,JPuj⟩R=0\langle u_i, J_P u_j\rangle_{\mathbb{R}} = 0⟨ui​,JP​uj​⟩R​=0 for all i,ji,ji,j. It is not required that JPuj∈TJ_P u_j\in TJP​uj​∈T, nor that the family span anything. For m=0m=0m=0 the empty family is trivially a JJJ-frame.
  • Chosen frame. frame(T,P,d)∈(AmbN)d\mathrm{frame}(T,P,d)\in(\mathrm{Amb}_N)^dframe(T,P,d)∈(AmbN​)d is built as follows. Let u=(u0,…,u⌊d/2⌋−1)u=(u_0,\dots,u_{\lfloor d/2\rfloor-1})u=(u0​,…,u⌊d/2⌋−1​) be some JJJ-frame for (T,P)(T,P)(T,P) of length ⌊d/2⌋\lfloor d/2\rfloor⌊d/2⌋, chosen by Hilbert's ε\varepsilonε-operator (Classical.epsilon): if at least one such frame exists, uuu is an unspecified one of them; if none exists, uuu is an unspecified arbitrary family in (AmbN)⌊d/2⌋(\mathrm{Amb}_N)^{\lfloor d/2\rfloor}(AmbN​)⌊d/2⌋ with no properties at all. The choice is a fixed but unknown function of (T,P,d)(T,P,d)(T,P,d), with no continuity or measurability in PPP. Then, for index k∈{0,…,d−1}k\in\{0,\dots,d-1\}k∈{0,…,d−1}:
frame(T,P,d)k={uk/2k even, ⌊k/2⌋<⌊d/2⌋,JP u(k−1)/2k odd, ⌊k/2⌋<⌊d/2⌋,0otherwise (only when d is odd and k=d−1).\mathrm{frame}(T,P,d)_k = \begin{cases} u_{k/2} & k \text{ even},\ \lfloor k/2\rfloor<\lfloor d/2\rfloor,\\ J_P\,u_{(k-1)/2} & k \text{ odd},\ \lfloor k/2\rfloor<\lfloor d/2\rfloor,\\ 0 & \text{otherwise (only when } d \text{ is odd and } k=d-1).\end{cases}frame(T,P,d)k​=⎩⎨⎧​uk/2​JP​u(k−1)/2​0​k even, ⌊k/2⌋<⌊d/2⌋,k odd, ⌊k/2⌋<⌊d/2⌋,otherwise (only when d is odd and k=d−1).​

So the frame is the interleaved family (u0,JPu0,u1,JPu1,… )(u_0, J_Pu_0, u_1, J_Pu_1, \dots)(u0​,JP​u0​,u1​,JP​u1​,…), with a trailing zero vector when ddd is odd. In this theorem the frames used have even length (2n2n2n and 2(n−p)2(n-p)2(n−p)), so no zero entry occurs.

  • Volume measure. On AmbN\mathrm{Amb}_NAmbN​,
μd:=π⌊d/2⌋⌊d/2⌋!  2d ⋅ Hd,\mu_d := \frac{\pi^{\lfloor d/2\rfloor}}{\lfloor d/2\rfloor!\; 2^{d}}\ \cdot\ \mathcal{H}^{d},μd​:=⌊d/2⌋!2dπ⌊d/2⌋​ ⋅ Hd,

where Hd\mathcal{H}^dHd is Mathlib's ddd-dimensional Hausdorff measure on the metric space AmbN\mathrm{Amb}_NAmbN​ (Hilbert–Schmidt metric), which carries no intrinsic normalisation. For even d=2md=2md=2m the constant is πm/(m! 22m)\pi^m/(m!\,2^{2m})πm/(m!22m), i.e. (volume of the unit ddd-ball)/2d/2^d/2d, the classical factor that rescales unnormalised Hausdorff measure to Lebesgue measure on ddd-dimensional Euclidean subspaces; for odd ddd the floor makes the constant differ from that classical factor (odd ddd does not occur in this theorem). For d=0d=0d=0, μ0=H0\mu_0=\mathcal{H}^0μ0​=H0 is counting measure.

  • Wedge value. For ω∈ΩNk\omega\in\Omega^k_Nω∈ΩNk​, η∈ΩNl\eta\in\Omega^l_Nη∈ΩNl​, a point PPP and a family f=(f0,…,fk+l−1)f=(f_0,\dots,f_{k+l-1})f=(f0​,…,fk+l−1​):
(ω∧η)P(f):=1k! l!∑σ∈Sk+lsgn⁡(σ) ωP(fσ(0),…,fσ(k−1)) ηP(fσ(k),…,fσ(k+l−1)).(\omega\wedge\eta)_P(f) := \frac{1}{k!\,l!}\sum_{\sigma\in S_{k+l}}\operatorname{sgn}(\sigma)\ \omega_P\big(f_{\sigma(0)},\dots,f_{\sigma(k-1)}\big)\ \eta_P\big(f_{\sigma(k)},\dots,f_{\sigma(k+l-1)}\big).(ω∧η)P​(f):=k!l!1​σ∈Sk+l​∑​sgn(σ) ωP​(fσ(0)​,…,fσ(k−1)​) ηP​(fσ(k)​,…,fσ(k+l−1)​).
  • Pairing on XXX. For ω∈ΩNk\omega\in\Omega^k_Nω∈ΩNk​, η∈ΩNl\eta\in\Omega^l_Nη∈ΩNl​:
⟨ω,η⟩X:=∫P∈ptsX(ω∧η)P(frame(TX(P),P,k+l)) dμk+l(P) ∈C,\langle\omega,\eta\rangle_X := \int_{P\in\mathrm{pts}_X} (\omega\wedge\eta)_P\big(\mathrm{frame}(\mathcal{T}_X(P),P,k+l)\big)\ d\mu_{k+l}(P)\ \in\mathbb{C},⟨ω,η⟩X​:=∫P∈ptsX​​(ω∧η)P​(frame(TX​(P),P,k+l)) dμk+l​(P) ∈C,

a Bochner integral over the set ptsX\mathrm{pts}_XptsX​ (all points of XXX, singular or not) of the complex number obtained by evaluating ω∧η\omega\wedge\etaω∧η at PPP on the chosen JJJ-frame of TX(P)\mathcal{T}_X(P)TX​(P) of length k+lk+lk+l. By Mathlib's convention the integral is 000 if the integrand is not integrable (including not almost-everywhere strongly measurable) with respect to μk+l\mu_{k+l}μk+l​ restricted to ptsX\mathrm{pts}_XptsX​.

  • Integral over ZZZ. For η∈ΩNl\eta\in\Omega^l_Nη∈ΩNl​:
∫Zη:=∫P∈regZηP(frame(TZ(P),P,l)) dμl(P) ∈C,\int_Z\eta := \int_{P\in\mathrm{reg}_Z}\eta_P\big(\mathrm{frame}(\mathcal{T}_Z(P),P,l)\big)\ d\mu_l(P)\ \in\mathbb{C},∫Z​η:=∫P∈regZ​​ηP​(frame(TZ​(P),P,l)) dμl​(P) ∈C,

integrating only over the regular points of ZZZ against μl\mu_lμl​, using ZZZ's own tangent spaces and frames; same 000-for-non-integrable convention.

The cycle-class property

For c∈H2p(X)c\in H^{2p}(X)c∈H2p(X): IsCycleClassX(Z,n,p,c)\mathrm{IsCycleClass}_X(Z,n,p,c)IsCycleClassX​(Z,n,p,c) holds iff

∀ ω∈CX2p with [ω]=c,∀ η∈ΩN2n−2p closed for X:⟨ω,η⟩X=∫Zη.\forall\,\omega\in\mathcal{C}^{2p}_X \text{ with } [\omega]=c,\quad \forall\,\eta\in\Omega^{2n-2p}_N \text{ closed for } X:\qquad \langle\omega,\eta\rangle_X = \int_Z\eta .∀ω∈CX2p​ with [ω]=c,∀η∈ΩN2n−2p​ closed for X:⟨ω,η⟩X​=∫Z​η.

Here 2n−2p2n-2p2n−2p is natural-number subtraction (equal to 2(n−p)2(n-p)2(n−p) because p≤np\le np≤n), the pairing uses frames of length 2p+(2n−2p)=2n2p+(2n-2p)=2n2p+(2n−2p)=2n in TX(P)\mathcal{T}_X(P)TX​(P) against μ2n\mu_{2n}μ2n​ on ptsX\mathrm{pts}_XptsX​, and the right-hand side uses frames of length 2(n−p)2(n-p)2(n−p) in TZ(P)\mathcal{T}_Z(P)TZ​(P) against μ2(n−p)\mu_{2(n-p)}μ2(n−p)​ on regZ\mathrm{reg}_ZregZ​. The quantifier runs over every closed representative ω\omegaω of ccc (not just one), and over every η\etaη that is closed for XXX (smooth on AmbN\mathrm{Amb}_NAmbN​ with dηd\etadη vanishing on XXX's tangent spaces); η\etaη is then integrated over ZZZ using ZZZ's tangent data.

Full statement, assembled

∀N,n,p∈N, p≤n, ∀X,Z ProjVarieties over N:[∀v∈CX, dim⁡CTX(v)=n+1] ∧ CZ⊆CX ∧ Z irreducible ∧ dim⁡Z=n−p\forall N,n,p\in\mathbb{N},\ p\le n,\ \forall X,Z\ \text{ProjVarieties over } N:\quad \Big[\forall v\in C_X,\ \dim_{\mathbb{C}}T_X(v)=n+1\Big]\ \wedge\ C_Z\subseteq C_X\ \wedge\ Z\ \text{irreducible}\ \wedge\ \dim Z = n-p∀N,n,p∈N, p≤n, ∀X,Z ProjVarieties over N:[∀v∈CX​, dimC​TX​(v)=n+1] ∧ CZ​⊆CX​ ∧ Z irreducible ∧ dimZ=n−p ⟹∃! c∈H2p(X): ∀ ω∈CX2p, [ω]=c⇒∀ η∈ΩN2n−2p closed for X, ⟨ω,η⟩X=∫Zη.\Longrightarrow\quad \exists!\,c\in H^{2p}(X):\ \forall\,\omega\in\mathcal{C}^{2p}_X,\ [\omega]=c \Rightarrow \forall\,\eta\in\Omega^{2n-2p}_N \text{ closed for } X,\ \langle\omega,\eta\rangle_X=\int_Z\eta .⟹∃!c∈H2p(X): ∀ω∈CX2p​, [ω]=c⇒∀η∈ΩN2n−2p​ closed for X, ⟨ω,η⟩X​=∫Z​η.

Edge cases, degenerate inputs, junk values

  • Nonemptiness forced. Irreducibility of ZZZ includes CZ≠∅C_Z\neq\emptysetCZ​=∅; with CZ⊆CXC_Z\subseteq C_XCZ​⊆CX​ this forces CX≠∅C_X\neq\emptysetCX​=∅, so the nonsingularity hypothesis on XXX is not vacuous, dim⁡X=(n+1)−˙1=n\dim X = (n+1)\dot{-}1 = ndimX=(n+1)−˙​1=n, and regX=ptsX\mathrm{reg}_X = \mathrm{pts}_XregX​=ptsX​. The hypotheses are jointly satisfiable (e.g. XXX a linear Pn⊆PN\mathbb{P}^n\subseteq\mathbb{P}^NPn⊆PN cut out by linear forms and ZZZ a linear subspace of dimension n−pn-pn−p).
  • Natural subtraction. n−pn-pn−p and 2n−2p2n-2p2n−2p are genuine because p≤np\le np≤n. dim⁡Z=m−˙1\dim Z = m\dot{-}1dimZ=m−˙​1 with mmm the minimum tangent rank on CZC_ZCZ​; the hypothesis dim⁡Z=n−p\dim Z = n-pdimZ=n−p reads m−˙1=n−pm\dot{-}1 = n-pm−˙​1=n−p, i.e. m=n−p+1m = n-p+1m=n−p+1 when m≥1m\ge1m≥1; if mmm were 000 it would force p=np=np=n and regZ\mathrm{reg}_ZregZ​ could be empty (then ∫Zη=0\int_Z\eta=0∫Z​η=0 for all η\etaη). inf⁡∅=0\inf\emptyset=0inf∅=0 does not arise since CZ≠∅C_Z\ne\emptysetCZ​=∅.
  • p=np=np=n. Then η\etaη is a 000-form (a smooth function with dηd\etadη vanishing on XXX's tangents), ∫Zη\int_Z\eta∫Z​η is the integral of η\etaη over regZ\mathrm{reg}_ZregZ​ against counting measure μ0\mu_0μ0​ (a finite sum if regZ\mathrm{reg}_ZregZ​ is finite; 000 if η\etaη is not integrable for counting measure on regZ\mathrm{reg}_ZregZ​), and (ω∧η)P(f)=ωP(f) η(P)(\omega\wedge\eta)_P(f)=\omega_P(f)\,\eta(P)(ω∧η)P​(f)=ωP​(f)η(P).
  • p=0p=0p=0. ccc is a class of 000-forms modulo EX0\mathcal{E}^0_XEX0​ (smooth functions vanishing on ptsX\mathrm{pts}_XptsX​); ω\omegaω is a smooth function whose derivative vanishes on TX(P)\mathcal{T}_X(P)TX​(P) at points of XXX; frames of length 2n2n2n are used on both sides (dim⁡Z=n\dim Z=ndimZ=n).
  • N=0N=0N=0. Amb0=C\mathrm{Amb}_0=\mathbb{C}Amb0​=C, π(v)=1\pi(v)=1π(v)=1 for v≠0v\neq0v=0, so ptsX⊆{1}\mathrm{pts}_X\subseteq\{1\}ptsX​⊆{1}; only n=p=0n=p=0n=p=0 is compatible with tangent rank 111.
  • Frame junk. If for some PPP no JJJ-frame of the required length exists in TX(P)\mathcal{T}_X(P)TX​(P) (or TZ(P)\mathcal{T}_Z(P)TZ​(P)), the ε\varepsilonε-operator returns an arbitrary family with no orthonormality or membership properties, and the integrand at PPP is whatever the form gives on that family. Even when frames exist, the choice P↦frame(⋅,P,⋅)P\mapsto\mathrm{frame}(\cdot,P,\cdot)P↦frame(⋅,P,⋅) is unspecified and need not be measurable; if the resulting integrand fails to be a.e.-strongly measurable or integrable, the Bochner integral is 000 by convention, on either side of the equation independently.
  • Frame ordering/orientation. Evaluation of a top-degree alternating form on the frame depends on the interleaved order (u0,JPu0,u1,JPu1,… )(u_0,J_Pu_0,u_1,J_Pu_1,\dots)(u0​,JP​u0​,u1​,JP​u1​,…) and on which JJJ-frame ε\varepsilonε selects; the definition fixes one such choice per (T,P,d)(T,P,d)(T,P,d) once and for all.
  • Measure normalisation. Both integrals use Hausdorff measure scaled by πm/(m! 4m)\pi^{m}/(m!\,4^{m})πm/(m!4m) with d=2md=2md=2m; the scale on the left is for d=2nd=2nd=2n and on the right for d=2(n−p)d=2(n-p)d=2(n−p).
  • Domain of integration. The pairing integrates over all of ptsX\mathrm{pts}_XptsX​; the right-hand side integrates over regZ⊆ptsZ⊆ptsX\mathrm{reg}_Z\subseteq\mathrm{pts}_Z\subseteq\mathrm{pts}_XregZ​⊆ptsZ​⊆ptsX​, the points of ZZZ of minimal tangent rank, using ZZZ's tangent spaces TZ(P)\mathcal{T}_Z(P)TZ​(P) (computed from ZZZ's own vanishing set IZI_ZIZ​), not XXX's.
  • Forms are ambient. All forms are functions on the entire matrix space AmbN\mathrm{Amb}_NAmbN​ with real-multilinear alternating values in C\mathbb{C}C; smoothness is required everywhere on AmbN\mathrm{Amb}_NAmbN​, while "closed" and "exact" are tested only tangentially along XXX.
  • Cohomology is complex. H2p(X)H^{2p}(X)H2p(X) is a C\mathbb{C}C-vector space (spans over C\mathbb{C}C); the unique ccc is an element of it, and uniqueness is equality modulo EX2p\mathcal{E}^{2p}_XEX2p​.

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