TheoremComplete

Hodge Index Theorem

The Hodge Index Theorem determines the signature of the intersection form on the Neron--Severi group of a smooth projective surface. It is the single most important constraint on the arithmetic of divisors: the intersection pairing is hyperbolic, having exactly one positive eigenvalue. This gives rise to the Hodge inequality, Zariski's lemma, the negativity lemma, and an interpretation of NS⁑(X)βŠ—R\operatorname{NS}(X) \otimes \mathbb{R} as hyperbolic space.


Statement

Theorem5.2Hodge Index Theorem

Let XX be a smooth projective surface over an algebraically closed field. Let NS⁑(X)\operatorname{NS}(X) be the Neron--Severi group of XX with the intersection pairing, and let ρ=rk⁑NS⁑(X)\rho = \operatorname{rk} \operatorname{NS}(X) be the Picard number. Then the intersection form on NS⁑(X)βŠ—R\operatorname{NS}(X) \otimes \mathbb{R} has signature (1,Οβˆ’1)(1, \rho - 1).

That is, there exists a basis of NS⁑(X)βŠ—R\operatorname{NS}(X) \otimes \mathbb{R} in which the intersection matrix is diag⁑(1,βˆ’1,βˆ’1,…,βˆ’1)\operatorname{diag}(1, -1, -1, \ldots, -1).

Theorem5.3Hodge Index Theorem (equivalent formulation)

Let XX be a smooth projective surface and HH an ample divisor on XX. If DD is a divisor with Dβ‹…H=0D \cdot H = 0, then D2≀0D^2 \leq 0, with equality if and only if D≑0D \equiv 0 (numerically trivial).

In other words, the orthogonal complement HβŠ₯βŠ‚NS⁑(X)βŠ—RH^{\perp} \subset \operatorname{NS}(X) \otimes \mathbb{R} is negative definite.

RemarkWhy the two formulations are equivalent

The intersection form has at least one positive direction: if HH is ample, then H2>0H^2 > 0 by the Nakai--Moishezon criterion. Theorem 5.3 says HβŠ₯H^{\perp} is negative definite, so there is exactly one positive direction. This means the signature is (1,Οβˆ’1)(1, \rho - 1), recovering Theorem 5.2. Conversely, signature (1,Οβˆ’1)(1, \rho - 1) means the orthogonal complement of any vector with positive self-intersection is negative definite by Sylvester's law of inertia.


Proof sketch

ProofProof of the Hodge Index Theorem

We prove Theorem 5.3. Let HH be ample and DD a divisor with Dβ‹…H=0D \cdot H = 0. We must show D2≀0D^2 \leq 0.

Step 1: Riemann--Roch. For any integer nn, Riemann--Roch gives:

Ο‡(OX(nD))=12nDβ‹…(nDβˆ’KX)+Ο‡(OX)=n22D2βˆ’n2Dβ‹…KX+Ο‡(OX).\chi(\mathcal{O}_X(nD)) = \frac{1}{2}nD \cdot (nD - K_X) + \chi(\mathcal{O}_X) = \frac{n^2}{2}D^2 - \frac{n}{2}D \cdot K_X + \chi(\mathcal{O}_X).

Step 2: Serre duality bound. We have h0(nD)+h0(KXβˆ’nD)β‰₯Ο‡(OX(nD))h^0(nD) + h^0(K_X - nD) \geq \chi(\mathcal{O}_X(nD)) since h2(nD)=h0(KXβˆ’nD)h^2(nD) = h^0(K_X - nD) by Serre duality and h1(nD)β‰₯0h^1(nD) \geq 0.

Step 3: Ampleness constraint. Since HH is ample and Dβ‹…H=0D \cdot H = 0, we get (nD)β‹…H=0(nD) \cdot H = 0 for all nn. An effective divisor EE satisfies Eβ‹…H>0E \cdot H > 0 (since HH is ample and EE is a nontrivial effective cycle), unless E=0E = 0. Therefore:

  • If h0(nD)>0h^0(nD) > 0 for some n>0n > 0, then nDnD is linearly equivalent to an effective divisor EE with Eβ‹…H=0E \cdot H = 0, forcing E=0E = 0, so nD∼0nD \sim 0.
  • Similarly, h0(KXβˆ’nD)>0h^0(K_X - nD) > 0 forces KXβˆ’nDK_X - nD to be effective with (KXβˆ’nD)β‹…H=KXβ‹…H>0(K_X - nD) \cdot H = K_X \cdot H > 0, which is fine -- but for ∣n∣|n| large enough, at most one of h0(nD)h^0(nD) and h0(KXβˆ’nD)h^0(K_X - nD) can be nonzero.

Step 4: Conclusion. Suppose D2>0D^2 > 0. Then Ο‡(OX(nD))∼n22D2β†’+∞\chi(\mathcal{O}_X(nD)) \sim \frac{n^2}{2}D^2 \to +\infty as ∣nβˆ£β†’βˆž|n| \to \infty. So for ∣nβˆ£β‰«0|n| \gg 0, either h0(nD)h^0(nD) or h0(KXβˆ’nD)h^0(K_X - nD) grows quadratically. Choose the sign of nn so that h0(nD)β†’βˆžh^0(nD) \to \infty. Then for large nn, nDnD is linearly equivalent to an effective divisor, but nDβ‹…H=0nD \cdot H = 0 forces nD∼0nD \sim 0, contradicting D2>0D^2 > 0.

Therefore D2≀0D^2 \leq 0. If D2=0D^2 = 0, a similar but more delicate argument shows D≑0D \equiv 0.

β– 
RemarkCharacteristic zero vs. positive characteristic

Over C\mathbb{C}, the Hodge Index Theorem follows from the Hodge decomposition and the Lefschetz theorem on (1,1)(1,1)-classes. In positive characteristic, the algebraic proof via Riemann--Roch (as above) works uniformly, which is essential since the Hodge decomposition may fail.


The Hodge inequality

Theorem5.4Hodge inequality (Cauchy--Schwarz for intersection form)

Let XX be a smooth projective surface and let C,DC, D be divisors on XX with C2>0C^2 > 0. Then:

(Cβ‹…D)2β‰₯C2β‹…D2,(C \cdot D)^2 \geq C^2 \cdot D^2,

with equality if and only if DD is numerically proportional to CC, i.e., there exists λ∈Q\lambda \in \mathbb{Q} such that D≑λCD \equiv \lambda C.

ProofProof of the Hodge inequality

Since C2>0C^2 > 0, we can write D=Cβ‹…DC2C+Dβ€²D = \frac{C \cdot D}{C^2} C + D' where Dβ€²=Dβˆ’Cβ‹…DC2CD' = D - \frac{C \cdot D}{C^2}C satisfies Dβ€²β‹…C=0D' \cdot C = 0. By the Hodge Index Theorem (Theorem 5.3, applied with CC playing the role of an ample-like class), Dβ€²2≀0D'^2 \leq 0. Computing:

D2=(Cβ‹…D)2C2+Dβ€²2≀(Cβ‹…D)2C2,D^2 = \frac{(C \cdot D)^2}{C^2} + D'^2 \leq \frac{(C \cdot D)^2}{C^2},

so (Cβ‹…D)2β‰₯C2β‹…D2(C \cdot D)^2 \geq C^2 \cdot D^2. Equality holds iff Dβ€²2=0D'^2 = 0, which by Hodge Index means D′≑0D' \equiv 0, i.e., D≑Cβ‹…DC2CD \equiv \frac{C \cdot D}{C^2} C.

β– 
RemarkReversed Cauchy--Schwarz

The Hodge inequality looks like the Cauchy--Schwarz inequality but with the inequality reversed: in a positive-definite inner product space, Cauchy--Schwarz gives (uβ‹…v)2β‰€βˆ£u∣2∣v∣2(u \cdot v)^2 \leq |u|^2 |v|^2. The reversal occurs because the intersection form has signature (1,Οβˆ’1)(1, \rho - 1), not (ρ,0)(\rho, 0). This is exactly the Cauchy--Schwarz inequality for the Minkowski metric of signature (1,nβˆ’1)(1, n-1).


Examples: intersection forms on classical surfaces

ExampleIntersection form on P^2

NS⁑(P2)=Zβ‹…H\operatorname{NS}(\mathbb{P}^2) = \mathbb{Z} \cdot H with H2=1H^2 = 1. The intersection form is the 1Γ—11 \times 1 matrix (1)(1), which has signature (1,0)(1, 0) since ρ=1\rho = 1. The Hodge Index Theorem is vacuous: HβŠ₯=0H^{\perp} = 0.

The Hodge inequality gives: for any curve CC of degree dd and any curve DD of degree ee, (de)2β‰₯d2β‹…e2(de)^2 \geq d^2 \cdot e^2. This is just d2e2β‰₯d2e2d^2 e^2 \geq d^2 e^2, an equality. Since ρ=1\rho = 1, every divisor is proportional to HH.

ExampleIntersection form on P^1 x P^1

NS⁑(P1Γ—P1)=ZF1βŠ•ZF2\operatorname{NS}(\mathbb{P}^1 \times \mathbb{P}^1) = \mathbb{Z} F_1 \oplus \mathbb{Z} F_2 with F12=F22=0F_1^2 = F_2^2 = 0 and F1β‹…F2=1F_1 \cdot F_2 = 1. The intersection matrix in the basis {F1,F2}\{F_1, F_2\} has entries Q11=Q22=0Q_{11} = Q_{22} = 0 and Q12=Q21=1Q_{12} = Q_{21} = 1.

The eigenvalues are +1+1 and βˆ’1-1 (eigenvectors F1+F2F_1 + F_2 and F1βˆ’F2F_1 - F_2), confirming signature (1,1)(1, 1).

Hodge inequality check: Take C=F1+F2C = F_1 + F_2 (the diagonal, with C2=2>0C^2 = 2 > 0) and D=aF1+bF2D = aF_1 + bF_2. Then (Cβ‹…D)2=(a+b)2(C \cdot D)^2 = (a + b)^2 and C2β‹…D2=2β‹…2ab=4abC^2 \cdot D^2 = 2 \cdot 2ab = 4ab. The inequality (a+b)2β‰₯4ab(a+b)^2 \geq 4ab is equivalent to (aβˆ’b)2β‰₯0(a - b)^2 \geq 0 βœ“.

ExampleIntersection form on Bl_p(P^2)

NS⁑(Bl⁑P(P2))=ZHβŠ•ZE\operatorname{NS}(\operatorname{Bl}_P(\mathbb{P}^2)) = \mathbb{Z} H \oplus \mathbb{Z} E with H2=1H^2 = 1, E2=βˆ’1E^2 = -1, Hβ‹…E=0H \cdot E = 0. The intersection matrix is diag⁑(1,βˆ’1)\operatorname{diag}(1, -1), which has signature (1,1)(1, 1) directly.

Let D=aHβˆ’bED = aH - bE. Then Dβ‹…H=aD \cdot H = a and D2=a2βˆ’b2D^2 = a^2 - b^2. If Dβ‹…H=0D \cdot H = 0, then a=0a = 0 and D2=βˆ’b2≀0D^2 = -b^2 \leq 0, with equality iff b=0b = 0 βœ“.

ExampleIntersection form on Bl_{p_1,...,p_n}(P^2)

Blowing up P2\mathbb{P}^2 at nn points in general position gives NS⁑(X)=ZHβŠ•ZE1βŠ•β‹―βŠ•ZEn\operatorname{NS}(X) = \mathbb{Z} H \oplus \mathbb{Z} E_1 \oplus \cdots \oplus \mathbb{Z} E_n with H2=1H^2 = 1, Ei2=βˆ’1E_i^2 = -1, Hβ‹…Ei=0H \cdot E_i = 0, Eiβ‹…Ej=0E_i \cdot E_j = 0 for iβ‰ ji \neq j. The intersection matrix is diag⁑(1,βˆ’1,βˆ’1,…,βˆ’1)\operatorname{diag}(1, -1, -1, \ldots, -1), directly exhibiting signature (1,n)(1, n).

For n=6n = 6: the del Pezzo surface of degree 33 (a cubic surface in P3\mathbb{P}^3) has ρ=7\rho = 7, intersection form diag⁑(1,βˆ’1,βˆ’1,βˆ’1,βˆ’1,βˆ’1,βˆ’1)\operatorname{diag}(1, -1, -1, -1, -1, -1, -1), and contains the famous 2727 lines.

For n=8n = 8: the del Pezzo surface of degree 11 has ρ=9\rho = 9, and the anti-canonical class βˆ’K=3Hβˆ’E1βˆ’β‹―βˆ’E8-K = 3H - E_1 - \cdots - E_8 satisfies (βˆ’K)2=9βˆ’8=1(-K)^2 = 9 - 8 = 1.

ExampleIntersection form on K3 surfaces

A K3 surface over C\mathbb{C} has H2(X,Z)β‰…Ξ›K3H^2(X, \mathbb{Z}) \cong \Lambda_{K3}, the K3 lattice, which is isometric to U3βŠ•E8(βˆ’1)2U^3 \oplus E_8(-1)^2, a unimodular lattice of rank 2222 and signature (3,19)(3, 19).

The Neron--Severi group NS⁑(X)=H1,1(X)∩H2(X,Z)\operatorname{NS}(X) = H^{1,1}(X) \cap H^2(X, \mathbb{Z}) has rank ρ\rho with 1≀ρ≀201 \leq \rho \leq 20. By the Hodge Index Theorem, the intersection form on NS⁑(X)\operatorname{NS}(X) has signature (1,Οβˆ’1)(1, \rho - 1).

  • Generic K3 (ρ=1\rho = 1): NS⁑(X)=ZH\operatorname{NS}(X) = \mathbb{Z} H with H2=2dH^2 = 2d for some dβ‰₯1d \geq 1.
  • ρ=2\rho = 2 example: The Kummer surface of a generic abelian surface has ρ=17\rho = 17 (not 22!). A K3 with ρ=2\rho = 2 could have NS lattice with Gram matrix having entries 2d,a2d, a on the first row and a,βˆ’2ea, -2e on the second, for appropriate d,e,ad, e, a.
  • ρ=20\rho = 20 (singular K3): The Fermat quartic x4+y4+z4+w4=0x^4 + y^4 + z^4 + w^4 = 0 over F3β€Ύ\overline{\mathbb{F}_3} achieves ρ=22\rho = 22 (the Tate conjecture), but over C\mathbb{C} the maximum is ρ=20\rho = 20.
ExampleIntersection form on Hirzebruch surfaces

The Hirzebruch surface Fn\mathbb{F}_n has NS⁑(Fn)=ZC0βŠ•ZF\operatorname{NS}(\mathbb{F}_n) = \mathbb{Z} C_0 \oplus \mathbb{Z} F with C02=βˆ’nC_0^2 = -n, F2=0F^2 = 0, C0β‹…F=1C_0 \cdot F = 1.

The intersection matrix has Q11=βˆ’nQ_{11} = -n, Q12=Q21=1Q_{12} = Q_{21} = 1, Q22=0Q_{22} = 0, with det⁑(Q)=βˆ’1\det(Q) = -1 and eigenvalues βˆ’nΒ±n2+42\frac{-n \pm \sqrt{n^2 + 4}}{2}. One eigenvalue is positive, one is negative, confirming signature (1,1)(1, 1).

In the basis H=C0+nFH = C_0 + nF (which is nef with H2=nH^2 = n) and FF: the matrix entries become n,1,1,0n, 1, 1, 0 respectively, still with one positive and one negative eigenvalue.

Hodge inequality check: C02=βˆ’n<0C_0^2 = -n < 0, so we cannot apply the Hodge inequality with C=C0C = C_0. Taking C=C0+nFC = C_0 + nF (with C2=n>0C^2 = n > 0 for nβ‰₯1n \geq 1) and D=FD = F: (Cβ‹…D)2=1(C \cdot D)^2 = 1 and C2β‹…D2=nβ‹…0=0C^2 \cdot D^2 = n \cdot 0 = 0, so 1β‰₯01 \geq 0 βœ“.


Zariski's lemma

Theorem5.5Zariski's lemma

Let f:Xβ†’Bf: X \to B be a fibration from a smooth projective surface to a smooth curve, and let F=βˆ‘iaiCiF = \sum_i a_i C_i be a fiber of ff (so FF is connected). For any divisor D=βˆ‘idiCiD = \sum_i d_i C_i supported on the fiber:

  • D2≀0D^2 \leq 0.
  • D2=0D^2 = 0 if and only if DD is a rational multiple of FF.

Equivalently, the intersection matrix (Ciβ‹…Cj)(C_i \cdot C_j) restricted to the irreducible components of a fiber is negative semi-definite, with kernel spanned by FF.

ProofProof via the Hodge Index Theorem

Let HH be an ample divisor on XX. Since FF is a fiber of ff, all fibers are numerically equivalent, so F≑Fβ€²F \equiv F' for any other fiber Fβ€²F'. Hence F2=Fβ‹…Fβ€²=0F^2 = F \cdot F' = 0 (distinct fibers are disjoint).

For DD supported on FF, write D=Ξ»F+Dβ€²D = \lambda F + D' where Ξ»=Dβ‹…HFβ‹…H\lambda = \frac{D \cdot H}{F \cdot H} (this makes Dβ€²β‹…H=0D' \cdot H = 0). By the Hodge Index Theorem, Dβ€²2≀0D'^2 \leq 0 with equality iff D′≑0D' \equiv 0, i.e., D≑λFD \equiv \lambda F.

Since D2=Ξ»2F2+2Ξ»Fβ‹…Dβ€²+Dβ€²2=0+0+Dβ€²2D^2 = \lambda^2 F^2 + 2\lambda F \cdot D' + D'^2 = 0 + 0 + D'^2 (because Fβ‹…Dβ€²=0F \cdot D' = 0, as Dβ€²D' is supported on FF and Fβ‹…Ci=0F \cdot C_i = 0 for components CiC_i of FF), we get D2=Dβ€²2≀0D^2 = D'^2 \leq 0.

β– 
ExampleZariski's lemma for elliptic fibrations

Let f:Xβ†’P1f: X \to \mathbb{P}^1 be an elliptic fibration with a singular fiber of Kodaira type InI_n (a cycle of nn rational curves C1,…,CnC_1, \ldots, C_n, each with Ci2=βˆ’2C_i^2 = -2, meeting in a cycle: Ciβ‹…Ci+1=1C_i \cdot C_{i+1} = 1 for indices mod nn).

The fiber is F=C1+C2+β‹―+CnF = C_1 + C_2 + \cdots + C_n with F2=βˆ‘iCi2+2βˆ‘iCiβ‹…Ci+1=βˆ’2n+2n=0F^2 = \sum_i C_i^2 + 2\sum_{i} C_i \cdot C_{i+1} = -2n + 2n = 0 βœ“.

The intersection matrix of the CiC_i is the negative of the Cartan matrix of type A~nβˆ’1\tilde{A}_{n-1}, which is negative semi-definite with 11-dimensional kernel spanned by (1,1,…,1)(1, 1, \ldots, 1), confirming Zariski's lemma.

For a type I1I_1 fiber (a nodal rational curve CC with C2=βˆ’1C^2 = -1... actually, C2=0C^2 = 0 since it is the entire fiber): a single irreducible fiber has F=CF = C with C2=0C^2 = 0.

ExampleChecking Zariski on type IV* fiber

Consider a Kodaira type IVβˆ—IV^* fiber (E~6\tilde{E}_6): the fiber F=C0+2C1+3C2+2C3+C4+2C5+C6F = C_0 + 2C_1 + 3C_2 + 2C_3 + C_4 + 2C_5 + C_6 where all Ci2=βˆ’2C_i^2 = -2. The intersection matrix of C0,…,C6C_0, \ldots, C_6 is the negative of the extended Cartan matrix of E6E_6, which is negative semi-definite with kernel spanned by the coefficients (1,2,3,2,1,2,1)(1, 2, 3, 2, 1, 2, 1). One verifies F2=0F^2 = 0, and any proper sub-combination D=βˆ‘diCiD = \sum d_i C_i not proportional to FF satisfies D2<0D^2 < 0.


Negativity lemma

Theorem5.6Negativity lemma

Let f:Yβ†’Xf: Y \to X be a birational morphism of smooth projective surfaces, and let E=βˆ‘iaiEiE = \sum_i a_i E_i be an effective divisor supported on the exceptional locus of ff (i.e., each EiE_i is an exceptional curve contracted by ff). If EE is ff-numerically trivial (meaning Eβ‹…C=0E \cdot C = 0 for every curve CC contracted by ff), then E=0E = 0.

More generally, if Eβ‹…Ei≀0E \cdot E_i \leq 0 for all ii, then EE is effective (all aiβ‰₯0a_i \geq 0) or E=0E = 0. And if EE is effective and nonzero, then E2<0E^2 < 0.

RemarkWhy this follows from Hodge Index

The exceptional curves E1,…,EnE_1, \ldots, E_n of a birational morphism f:Yβ†’Xf: Y \to X are contracted to points, so they behave like components of fibers. The intersection matrix (Eiβ‹…Ej)(E_i \cdot E_j) is negative definite (not just semi-definite, since the exceptional locus is not a complete fiber). This is a consequence of the Hodge Index Theorem: the EiE_i all satisfy Eiβ‹…H=0E_i \cdot H = 0 for H=fβˆ—AH = f^*A with AA ample on XX, and they are independent in NS⁑(Y)\operatorname{NS}(Y), so the restriction of the intersection form to span⁑(Ei)\operatorname{span}(E_i) lies in HβŠ₯H^{\perp}, which is negative definite.

ExampleNegativity for a single blowup

Let f:Bl⁑P(X)β†’Xf: \operatorname{Bl}_P(X) \to X with exceptional divisor EE. Then E2=βˆ’1<0E^2 = -1 < 0. Any effective divisor D=aED = aE (a>0a > 0) supported on the exceptional locus has D2=βˆ’a2<0D^2 = -a^2 < 0 βœ“.

After blowing up two points, the exceptional locus is E1βˆͺE2E_1 \cup E_2 with E12=E22=βˆ’1E_1^2 = E_2^2 = -1 and E1β‹…E2=0E_1 \cdot E_2 = 0. The intersection matrix diag⁑(βˆ’1,βˆ’1)\operatorname{diag}(-1, -1) is negative definite βœ“.

ExampleNegativity for resolution of an A_n singularity

Resolving an AnA_n surface singularity (locally xy=zn+1xy = z^{n+1}) produces a chain of nn exceptional curves E1,…,EnE_1, \ldots, E_n with Ei2=βˆ’2E_i^2 = -2 and Eiβ‹…Ei+1=1E_i \cdot E_{i+1} = 1. The intersection matrix is the negative of the Cartan matrix of AnA_n, which has eigenvalues βˆ’2+2cos⁑(Ο€k/(n+1))-2 + 2\cos(\pi k/(n+1)) for k=1,…,nk = 1, \ldots, n. All eigenvalues are negative, confirming negative definiteness.

For n=1n = 1: a single (βˆ’2)(-2)-curve. For n=2n = 2: the matrix has diagonal entries βˆ’2,βˆ’2-2, -2 and off-diagonal entries 1,11, 1, with eigenvalues βˆ’1-1 and βˆ’3-3.


Light cone and hyperbolic geometry

Definition5.4Light cone and positive cone

In V=NS⁑(X)βŠ—RV = \operatorname{NS}(X) \otimes \mathbb{R}, the light cone is:

L={D∈V:D2=0}.\mathcal{L} = \{ D \in V : D^2 = 0 \}.

The positive cone is one of the two connected components of {D∈V:D2>0}\{ D \in V : D^2 > 0 \}; we choose the component C+\mathcal{C}^+ containing an ample class. The ample cone Amp⁑(X)βŠ‚C+\operatorname{Amp}(X) \subset \mathcal{C}^+ and the nef cone Amp⁑(X)β€Ύ=Nef⁑(X)βŠ‚C+β€Ύ\overline{\operatorname{Amp}(X)} = \operatorname{Nef}(X) \subset \overline{\mathcal{C}^+} sit inside the positive cone.

RemarkHyperbolic geometry of NS(X) tensor R

Since the intersection form on V=NS⁑(X)βŠ—RV = \operatorname{NS}(X) \otimes \mathbb{R} has signature (1,Οβˆ’1)(1, \rho - 1), the projectivization of the positive cone:

HΟβˆ’1={[D]∈P(V):D2>0}/R>0\mathbb{H}^{\rho - 1} = \{ [D] \in \mathbb{P}(V) : D^2 > 0 \} / \mathbb{R}_{>0}

is a model of hyperbolic (Οβˆ’1)(\rho - 1)-space. The intersection form induces the hyperbolic metric:

cosh⁑d([C],[D])=∣Cβ‹…D∣C2β‹…D2\cosh d([C], [D]) = \frac{|C \cdot D|}{\sqrt{C^2} \cdot \sqrt{D^2}}

for classes C,DC, D in the positive cone.

The Hodge inequality (Cβ‹…D)2β‰₯C2β‹…D2(C \cdot D)^2 \geq C^2 \cdot D^2 ensures cosh⁑dβ‰₯1\cosh d \geq 1, which is exactly the condition for the hyperbolic distance to be well-defined. Equality (i.e., d=0d = 0) occurs iff CC and DD are proportional.

ExampleHyperbolic line for P^1 x P^1

For P1Γ—P1\mathbb{P}^1 \times \mathbb{P}^1, V=R2V = \mathbb{R}^2 with the form Q(a,b)=2abQ(a,b) = 2ab. The positive cone is {(a,b):ab>0}\{(a,b) : ab > 0\}, which has two components; the one containing (1,1)(1,1) is {a>0,b>0}\{a > 0, b > 0\}. The projectivization H1\mathbb{H}^1 is parametrized by t=a/b∈(0,∞)t = a/b \in (0, \infty), a copy of the real line (the hyperbolic line).

The ample cone is {a>0,b>0}\{a > 0, b > 0\} (divisors of bidegree (a,b)(a,b) with a,b>0a, b > 0), and the nef cone boundary consists of the rays Rβ‰₯0F1\mathbb{R}_{\geq 0} F_1 and Rβ‰₯0F2\mathbb{R}_{\geq 0} F_2 (the two rulings), which lie on the light cone.

ExampleHyperbolic space for K3 surfaces

For a K3 surface with ρ=2\rho = 2 and NS lattice generated by H,CH, C with H2=4H^2 = 4, C2=βˆ’2C^2 = -2, Hβ‹…C=1H \cdot C = 1: the positive cone in R2\mathbb{R}^2 is given by (aH+bC)2=4a2βˆ’2b2+2ab>0(aH + bC)^2 = 4a^2 - 2b^2 + 2ab > 0.

The ample cone is cut out by requiring additionally Dβ‹…C>0D \cdot C > 0 (i.e., βˆ’2b+a>0-2b + a > 0) for the (βˆ’2)(-2)-curve CC. So the ample cone is {4a2βˆ’2b2+2ab>0}∩{aβˆ’2b>0}\{4a^2 - 2b^2 + 2ab > 0\} \cap \{a - 2b > 0\}.

In hyperbolic 11-space H1\mathbb{H}^1, the ample cone corresponds to a half-line, bounded by the "wall" defined by the (βˆ’2)(-2)-curve CC. Reflection across this wall is the Picard--Lefschetz reflection sC:D↦D+(Dβ‹…C)Cs_C: D \mapsto D + (D \cdot C) C.


Application to arithmetic: Faltings height pairing

Theorem5.7Arithmetic Hodge Index (Faltings--Hriljac)

Let XX be an arithmetic surface (a regular model of a curve CC over a number field KK, fibered over Spec⁑(OK)\operatorname{Spec}(\mathcal{O}_K)). The Arakelov intersection pairing on the group of arithmetic divisors Div⁑^(X)\widehat{\operatorname{Div}}(X) has the Hodge index property:

If D^\widehat{D} is an arithmetic divisor with D^β‹…Ο‰^=0\widehat{D} \cdot \widehat{\omega} = 0 (where Ο‰^\widehat{\omega} is the arithmetic canonical class), then D^2≀0\widehat{D}^2 \leq 0, with equality iff D^\widehat{D} is numerically trivial.

Equivalently, the Neron--Tate height pairing on the Jacobian J(C)(Kβ€Ύ)J(C)(\overline{K}) is negative definite modulo torsion.

ExampleArithmetic Hodge index for elliptic curves

For an elliptic curve E/QE/\mathbb{Q}, the Neron--Tate height h^:E(Q)βŠ—Rβ†’R\hat{h}: E(\mathbb{Q}) \otimes \mathbb{R} \to \mathbb{R} is a positive-definite quadratic form (after accounting for torsion). The rank of E(Q)E(\mathbb{Q}) is the dimension of this space.

The arithmetic Hodge Index Theorem ensures that the height pairing matrix on a basis P1,…,PrP_1, \ldots, P_r of E(Q)/torsionE(\mathbb{Q})/\text{torsion} has det⁑(⟨Pi,Pj⟩)>0\det(\langle P_i, P_j \rangle) > 0, which is the regulator of EE. This appears in the BSD conjecture:

L(r)(E,1)/r!=Ξ©Eβ‹…Reg⁑(E)β‹…βˆcpβ‹…βˆ£III∣/∣E(Q)tors∣2.L^{(r)}(E, 1) / r! = \Omega_E \cdot \operatorname{Reg}(E) \cdot \prod c_p \cdot |\text{III}| / |E(\mathbb{Q})_{\text{tors}}|^2.


Algebraic vs. topological intersection form

RemarkTopological intersection form over C

Over C\mathbb{C}, a smooth projective surface XX has a topological intersection form on H2(X,Z)H^2(X, \mathbb{Z}), a unimodular symmetric bilinear form of rank b2=dim⁑H2(X,R)b_2 = \dim H^2(X, \mathbb{R}). By the Hodge decomposition:

H2(X,C)=H2,0βŠ•H1,1βŠ•H0,2,H^2(X, \mathbb{C}) = H^{2,0} \oplus H^{1,1} \oplus H^{0,2},

where dim⁑H2,0=pg\dim H^{2,0} = p_g, dim⁑H1,1=b2βˆ’2pg\dim H^{1,1} = b_2 - 2p_g, dim⁑H0,2=pg\dim H^{0,2} = p_g.

The full intersection form on H2(X,R)H^2(X, \mathbb{R}) has signature (2pg+1,b2βˆ’2pgβˆ’1)(2p_g + 1, b_2 - 2p_g - 1) by the Hodge--Riemann bilinear relations. The algebraic part NS⁑(X)βŠ—RβŠ‚HR1,1\operatorname{NS}(X) \otimes \mathbb{R} \subset H^{1,1}_{\mathbb{R}} has signature (1,Οβˆ’1)(1, \rho - 1) by the Hodge Index Theorem.

The transcendental lattice T(X)=NS⁑(X)βŠ₯∩H2(X,Z)T(X) = \operatorname{NS}(X)^{\perp} \cap H^2(X, \mathbb{Z}) carries the remaining signature (2pg,b2βˆ’2pgβˆ’Ο)(2p_g, b_2 - 2p_g - \rho).

ExampleTopological vs. algebraic for K3 surfaces

A K3 surface has b2=22b_2 = 22, pg=1p_g = 1, so the topological intersection form has signature (3,19)(3, 19) on H2(X,Z)β‰…U3βŠ•E8(βˆ’1)2H^2(X, \mathbb{Z}) \cong U^3 \oplus E_8(-1)^2.

The algebraic part NS⁑(X)\operatorname{NS}(X) has signature (1,Οβˆ’1)(1, \rho - 1), and the transcendental lattice T(X)T(X) has signature (2,20βˆ’Ο)(2, 20 - \rho).

  • For ρ=1\rho = 1: NS⁑(X)β‰…Z\operatorname{NS}(X) \cong \mathbb{Z} (signature (1,0)(1, 0)) and T(X)T(X) has signature (2,19)(2, 19).
  • For ρ=20\rho = 20: NS⁑(X)\operatorname{NS}(X) has signature (1,19)(1, 19) and T(X)T(X) has signature (2,0)(2, 0), meaning T(X)T(X) is a positive-definite lattice of rank 22.
ExampleSurfaces of general type and geography

For a minimal surface of general type, Noether's formula gives Ο‡(OX)=112(K2+e(X))\chi(\mathcal{O}_X) = \frac{1}{12}(K^2 + e(X)) where e(X)=2βˆ’4q+b2e(X) = 2 - 4q + b_2 is the topological Euler characteristic. The Bogomolov--Miyaoka--Yau inequality gives K2≀3e(X)K^2 \leq 3 e(X) (equivalently K2≀9Ο‡(OX)K^2 \leq 9 \chi(\mathcal{O}_X)).

The topological intersection form on H2H^2 has signature (2pg+1,b2βˆ’2pgβˆ’1)(2p_g + 1, b_2 - 2p_g - 1). By Freedman's theorem, the homeomorphism type of the underlying 44-manifold is determined by this form (plus b1b_1). But the smooth structure carries more information (Donaldson theory), and the algebraic structure even more.


Further examples and applications

ExampleIntersection form on Enriques surfaces

An Enriques surface YY has KY≑̸0K_Y \not\equiv 0 but 2KY∼02K_Y \sim 0. Its Neron--Severi group has rank ρ=10\rho = 10, and the intersection form is the even unimodular lattice UβŠ•E8(βˆ’1)U \oplus E_8(-1) of signature (1,9)(1, 9).

The Hodge Index Theorem gives: for HH ample on YY and Dβ‹…H=0D \cdot H = 0, we have D2≀0D^2 \leq 0. The lattice UβŠ•E8(βˆ’1)U \oplus E_8(-1) is the unique even unimodular lattice of this signature, mirroring the uniqueness of the E8E_8 lattice.

Any (βˆ’2)(-2)-curve CC on YY satisfies C2=βˆ’2C^2 = -2 and defines a reflection sC:D↦D+(Dβ‹…C)Cs_C: D \mapsto D + (D \cdot C)C preserving the lattice. The Weyl group generated by these reflections acts on the ample cone.

ExampleIntersection form on abelian surfaces

An abelian surface AA has ρ(A)\rho(A) ranging from 11 to 44 (over C\mathbb{C}). The Neron--Severi group embeds into End⁑(A)sym\operatorname{End}(A)^{\text{sym}} via the Appell--Humbert theorem. The intersection form on NS⁑(A)\operatorname{NS}(A) has signature (1,Οβˆ’1)(1, \rho - 1).

  • ρ=1\rho = 1: NS⁑(A)=ZL\operatorname{NS}(A) = \mathbb{Z} L with L2=2dL^2 = 2d (a polarization of type (1,d)(1, d)). Signature (1,0)(1, 0).
  • ρ=2\rho = 2 (generic principally polarized): NS⁑(A)β‰…Z2\operatorname{NS}(A) \cong \mathbb{Z}^2 with signature (1,1)(1, 1).
  • ρ=3\rho = 3 (AA has real multiplication): the extra endomorphisms produce additional algebraic classes.
  • ρ=4\rho = 4 (Aβ‰…E1Γ—E2A \cong E_1 \times E_2 with CM): NS⁑(A)\operatorname{NS}(A) is rank 44 with signature (1,3)(1, 3).
ExampleHodge inequality bounds degrees of curves

Let X=P2X = \mathbb{P}^2 blown up at one point, with NS⁑(X)=ZHβŠ•ZE\operatorname{NS}(X) = \mathbb{Z} H \oplus \mathbb{Z} E. Let CC be an irreducible curve of class aHβˆ’bEaH - bE (degree aa, multiplicity bb at the blown-up point). By irreducibility, CC is effective and:

  • Cβ‹…H=a>0C \cdot H = a > 0 and Cβ‹…E=bβ‰₯0C \cdot E = b \geq 0.
  • C2=a2βˆ’b2β‰₯βˆ’1C^2 = a^2 - b^2 \geq -1 (genus formula: g=(aβˆ’1)(aβˆ’2)2βˆ’b(bβˆ’1)2β‰₯0g = \frac{(a-1)(a-2)}{2} - \frac{b(b-1)}{2} \geq 0).

The Hodge inequality with HH (taking H2=1>0H^2 = 1 > 0, D=CD = C): (Hβ‹…C)2β‰₯H2β‹…C2(H \cdot C)^2 \geq H^2 \cdot C^2, i.e., a2β‰₯a2βˆ’b2a^2 \geq a^2 - b^2, giving b2β‰₯0b^2 \geq 0, which is trivial. But applying with the ample class A=3Hβˆ’EA = 3H - E (A2=8A^2 = 8) and C=aHβˆ’bEC = aH - bE: (3aβˆ’b)2β‹…1β‰₯(a2βˆ’b2)β‹…1(3a - b)^2 \cdot 1 \geq (a^2 - b^2) \cdot 1... this requires more care.

A more useful application: if C,DC, D are two distinct irreducible curves both passing through the blown-up point with multiplicities b,db, d, then by the Hodge inequality on the original P2\mathbb{P}^2: their intersection number satisfies Cβ‹…D=aeβˆ’bdβ‹…...C \cdot D = ae - bd \cdot ... . The cleanest use is: (Cβ‹…D)2β‰₯C2β‹…D2(C \cdot D)^2 \geq C^2 \cdot D^2 when C2>0C^2 > 0.

ExampleHodge Index constrains fibration structure

Suppose a smooth projective surface XX has two divisors F1,F2F_1, F_2 with F12=F22=0F_1^2 = F_2^2 = 0 and F1β‹…F2>0F_1 \cdot F_2 > 0. Then F1F_1 and F2F_2 are independent in NS⁑(X)\operatorname{NS}(X) and span a sublattice of signature (1,1)(1, 1) (the form 2(F1β‹…F2)ab2(F_1 \cdot F_2) ab in coordinates aF1+bF2aF_1 + bF_2 gives eigenvalues Β±F1β‹…F2\pm F_1 \cdot F_2).

By the Hodge Index Theorem, ρβ‰₯2\rho \geq 2. Moreover, if F1F_1 is the class of a fiber of a fibration f1:Xβ†’B1f_1: X \to B_1, then F12=0F_1^2 = 0 is automatic. Two independent fibrations f1,f2f_1, f_2 force ρβ‰₯2\rho \geq 2 and the sublattice ZF1βŠ•ZF2\mathbb{Z} F_1 \oplus \mathbb{Z} F_2 has signature (1,1)(1, 1).

This is realized by P1Γ—P1\mathbb{P}^1 \times \mathbb{P}^1: the two projections give fiber classes F1,F2F_1, F_2 with F1β‹…F2=1F_1 \cdot F_2 = 1.


Consequences for the cone structure

RemarkThe positive cone is round

The Hodge Index Theorem implies that the positive cone C+={D∈NS⁑(X)βŠ—R:D2>0,Dβ‹…H>0}\mathcal{C}^+ = \{D \in \operatorname{NS}(X) \otimes \mathbb{R} : D^2 > 0, D \cdot H > 0\} (for a fixed ample HH) is a convex open cone. This convexity is a consequence of the Minkowski geometry: in signature (1,n)(1, n), the set of future-pointing timelike vectors is convex.

In particular: if CC and DD are both in C+\mathcal{C}^+, then C+D∈C+C + D \in \mathcal{C}^+, i.e., (C+D)2>0(C + D)^2 > 0. This follows from (C+D)2=C2+2Cβ‹…D+D2>0(C + D)^2 = C^2 + 2C \cdot D + D^2 > 0, since Cβ‹…D>0C \cdot D > 0 by the Hodge inequality (both C2>0C^2 > 0 and D2>0D^2 > 0 with C,DC, D in the same component, so Cβ‹…Dβ‰₯C2β‹…D2>0C \cdot D \geq \sqrt{C^2 \cdot D^2} > 0).

ExampleCone structure on cubic surface

The cubic surface X=Bl⁑p1,…,p6(P2)X = \operatorname{Bl}_{p_1, \ldots, p_6}(\mathbb{P}^2) has ρ=7\rho = 7 and NS lattice Z1,6\mathbb{Z}^{1,6} (one positive, six negative directions). The 2727 lines on the cubic surface are the (βˆ’1)(-1)-curves, and the effective cone is generated by these 2727 classes.

The ample cone is the interior of the dual of the effective cone of curves, cut out by the 2727 inequalities Dβ‹…Li>0D \cdot L_i > 0 for each line LiL_i. In the hyperbolic 66-space H6\mathbb{H}^6, this is a polytope bounded by 2727 hyperplanes.

The Weyl group W(E6)W(E_6) of order 5184051840 acts on the NS lattice, permuting the 2727 lines and preserving the intersection form.


Summary

RemarkCentral role of the Hodge Index Theorem

The Hodge Index Theorem is the foundation for the arithmetic of divisors on surfaces:

  • Signature (1,Οβˆ’1)(1, \rho - 1): the intersection form is hyperbolic, having exactly one positive direction.
  • Hodge inequality: (Cβ‹…D)2β‰₯C2β‹…D2(C \cdot D)^2 \geq C^2 \cdot D^2 when C2>0C^2 > 0, the reversed Cauchy--Schwarz for the Minkowski metric.
  • Zariski's lemma: fibers of fibrations have negative semi-definite intersection matrix.
  • Negativity lemma: exceptional divisors of birational morphisms have negative definite intersection matrix.
  • Hyperbolic geometry: NS⁑(X)βŠ—R\operatorname{NS}(X) \otimes \mathbb{R} is a model of hyperbolic space, and ample/nef cones are convex subsets in this geometry.
  • Arithmetic analogue: the Faltings--Hriljac theorem extends the Hodge index property to Arakelov intersection theory, with the Neron--Tate height as the arithmetic intersection pairing.

Every computation of linear systems, every ampleness criterion, and every birational geometry argument on surfaces ultimately relies on the definiteness properties guaranteed by this theorem.