ProofComplete

Proof of Hodge Index Theorem

The Hodge Index Theorem constrains the signature of the intersection form on a smooth projective surface. It asserts that the intersection pairing on the orthogonal complement of an ample class is negative definite. This proof proceeds via Riemann--Roch and the ampleness properties of divisors, following the treatment in Hartshorne V.1.


Statement of the Theorem

Theorem5.1Hodge Index Theorem

Let XX be a smooth projective surface over an algebraically closed field kk, and let HH be an ample divisor on XX. If DD is a divisor such that Dβ‹…H=0D \cdot H = 0, then D2≀0D^2 \leq 0. Moreover, equality D2=0D^2 = 0 holds if and only if D≑0D \equiv 0 (i.e., DD is numerically trivial).

Equivalently: the intersection pairing on NS⁑(X)βŠ—R\operatorname{NS}(X) \otimes \mathbb{R} has signature (1,Οβˆ’1)(1, \rho - 1), where ρ\rho is the Picard number.

RemarkGeometric meaning

The theorem says that the intersection form on the Neron--Severi group is a Lorentzian form: it has exactly one positive eigenvalue. The "positive direction" is occupied by any ample class HH, and every direction orthogonal to HH is negative semi-definite (and negative definite modulo numerical equivalence). This is the algebraic analogue of the Hodge--Riemann bilinear relations in complex geometry.


Step 1: Setup and Riemann--Roch

ProofStep 1 β€” Asymptotic behavior via Riemann--Roch

Goal: Show that if D2>0D^2 > 0 and Dβ‹…H=0D \cdot H = 0, we reach a contradiction.

Assume DD is a divisor with Dβ‹…H=0D \cdot H = 0 and D2>0D^2 > 0. For any integer nn, consider the divisor nDnD. By the Riemann--Roch theorem for surfaces:

Ο‡(OX(nD))=12(nD)β‹…(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).

Since D2>0D^2 > 0, the leading term n22D2\frac{n^2}{2}D^2 dominates for ∣n∣|n| large. Therefore:

Ο‡(OX(nD))β†’+∞as ∣nβˆ£β†’βˆž.\chi(\mathcal{O}_X(nD)) \to +\infty \quad \text{as } |n| \to \infty.

Now recall that Ο‡(OX(nD))=h0(nD)βˆ’h1(nD)+h2(nD)\chi(\mathcal{O}_X(nD)) = h^0(nD) - h^1(nD) + h^2(nD). Since h1(nD)β‰₯0h^1(nD) \geq 0, we have:

h0(nD)+h2(nD)β‰₯Ο‡(OX(nD))β†’+∞.h^0(nD) + h^2(nD) \geq \chi(\mathcal{O}_X(nD)) \to +\infty.

So at least one of h0(nD)h^0(nD) or h2(nD)h^2(nD) must grow without bound as ∣nβˆ£β†’βˆž|n| \to \infty.

β– 
ExampleQuadratic growth of chi on a K3 surface

On a K3 surface (KX=0K_X = 0, Ο‡(OX)=2\chi(\mathcal{O}_X) = 2), take any divisor DD with D2=2d>0D^2 = 2d > 0. Then:

Ο‡(OX(nD))=n22β‹…2d+2=dn2+2.\chi(\mathcal{O}_X(nD)) = \frac{n^2}{2} \cdot 2d + 2 = dn^2 + 2.

For d=1d = 1, D2=2D^2 = 2: Ο‡(O(nD))=n2+2\chi(\mathcal{O}(nD)) = n^2 + 2. The values are 3,6,11,18,…3, 6, 11, 18, \ldots for n=1,2,3,4,…n = 1, 2, 3, 4, \ldots.

If DD were orthogonal to an ample class, the Hodge Index Theorem says this cannot happen. Indeed, on a K3, if Dβ‹…H=0D \cdot H = 0 for ample HH, then D2≀0D^2 \leq 0.


Step 2: Serre Duality and the Two Cases

ProofStep 2 β€” Ruling out large h^0 and h^2

By Serre duality, h2(OX(nD))=h0(OX(KXβˆ’nD))h^2(\mathcal{O}_X(nD)) = h^0(\mathcal{O}_X(K_X - nD)). So the conclusion of Step 1 says:

For ∣n∣|n| large, either h0(nD)β†’βˆžh^0(nD) \to \infty or h0(KXβˆ’nD)β†’βˆžh^0(K_X - nD) \to \infty.

Case A: h0(nD)β‰₯1h^0(nD) \geq 1 for some n>0n > 0. Then nDnD is linearly equivalent to an effective divisor, say nD∼Eβ‰₯0nD \sim E \geq 0. Since HH is ample and EE is effective, we have Eβ‹…H>0E \cdot H > 0 (an ample divisor has strictly positive intersection with every effective divisor). But Eβ‹…H=nDβ‹…H=n(Dβ‹…H)=0E \cdot H = nD \cdot H = n(D \cdot H) = 0, a contradiction.

Case B: h0(KXβˆ’nD)β‰₯1h^0(K_X - nD) \geq 1 for some n>0n > 0. Then KXβˆ’nD∼Fβ‰₯0K_X - nD \sim F \geq 0, so Fβ‹…H>0F \cdot H > 0 by ampleness. But Fβ‹…H=(KXβˆ’nD)β‹…H=KXβ‹…Hβˆ’n(Dβ‹…H)=KXβ‹…HF \cdot H = (K_X - nD) \cdot H = K_X \cdot H - n(D \cdot H) = K_X \cdot H. This is a fixed quantity (independent of nn), so this does not yet give a contradiction for a single nn.

However, we can be more precise. Since h0(nD)+h0(KXβˆ’nD)β‰₯Ο‡(OX(nD))β†’+∞h^0(nD) + h^0(K_X - nD) \geq \chi(\mathcal{O}_X(nD)) \to +\infty, and since h0(nD)=0h^0(nD) = 0 for all large nn (by Case A, any nonzero h0(nD)h^0(nD) leads to contradiction), we must have h0(KXβˆ’nD)β†’βˆžh^0(K_X - nD) \to \infty. In particular, h0(KXβˆ’nD)β‰₯1h^0(K_X - nD) \geq 1 for all sufficiently large nn.

Now apply the same argument to βˆ’D-D: since Dβ‹…H=0D \cdot H = 0 implies (βˆ’D)β‹…H=0(-D) \cdot H = 0, and (βˆ’D)2=D2>0(-D)^2 = D^2 > 0, replace DD by βˆ’D-D. Then the same reasoning gives h0(βˆ’nD)=0h^0(-nD) = 0 for all n>0n > 0 (by Case A for βˆ’D-D), and h0(KX+nD)β†’βˆžh^0(K_X + nD) \to \infty.

In particular, for nn large enough: KXβˆ’nD∼Fnβ‰₯0K_X - nD \sim F_n \geq 0 and KX+nD∼Gnβ‰₯0K_X + nD \sim G_n \geq 0. Adding: 2KX∼Fn+Gnβ‰₯02K_X \sim F_n + G_n \geq 0, which is independent of nn. But Fnβ‹…H=KXβ‹…Hβˆ’nDβ‹…H=KXβ‹…HF_n \cdot H = K_X \cdot H - nD \cdot H = K_X \cdot H and Gnβ‹…H=KXβ‹…H+nDβ‹…H=KXβ‹…HG_n \cdot H = K_X \cdot H + nD \cdot H = K_X \cdot H. So the effective decomposition Fn+Gn∼2KXF_n + G_n \sim 2K_X has bounded degree with respect to HH, yet FnF_n and GnG_n are both effective with Fn+GnF_n + G_n fixed. Since effective divisors of bounded degree on a projective surface form a bounded family, there are only finitely many possibilities. But this must hold for infinitely many nn, so Fn=FmF_n = F_m and Gn=GmG_n = G_m for some nβ‰ mn \neq m. Then (Fnβˆ’Fm)∼(nβˆ’m)D∼0(F_n - F_m) \sim (n - m)D \sim 0 as effective divisors, which implies nDβˆ’mDnD - mD is principal, hence (nβˆ’m)D∼0(n-m)D \sim 0 with nβ‰ mn \neq m, contradicting D2>0D^2 > 0.

This completes the proof that D2>0D^2 > 0 is impossible.

β– 
ExampleWhy effective divisors must intersect H positively

On P2\mathbb{P}^2 with HH a line: every effective divisor is E∼dHE \sim dH with d>0d > 0, so Eβ‹…H=d>0E \cdot H = d > 0.

On Bl⁑P(P2)\operatorname{Bl}_P(\mathbb{P}^2): take H=3Lβˆ’EH = 3L - E (anticanonical, ample). The exceptional curve EE satisfies Eβ‹…H=Eβ‹…(3Lβˆ’E)=0+1=1>0E \cdot H = E \cdot (3L - E) = 0 + 1 = 1 > 0. The strict transform L~\tilde{L} of a line through PP gives L~∼Lβˆ’E\tilde{L} \sim L - E, and L~β‹…H=3βˆ’1=2>0\tilde{L} \cdot H = 3 - 1 = 2 > 0.

In general, for ample HH and effective Eβ‰ 0E \neq 0: either EE is an irreducible curve (then Hβ‹…E>0H \cdot E > 0 by Nakai--Moishezon, since HH is ample), or E=βˆ‘aiCiE = \sum a_i C_i with ai>0a_i > 0, and Hβ‹…E=βˆ‘ai(Hβ‹…Ci)>0H \cdot E = \sum a_i (H \cdot C_i) > 0.


Step 3: The Equality Case

ProofStep 3 β€” D^2 = 0 implies D numerically trivial

Now suppose Dβ‹…H=0D \cdot H = 0 and D2=0D^2 = 0, and D≑̸0D \not\equiv 0. We derive a contradiction.

Since D≑̸0D \not\equiv 0, there exists a divisor CC with Dβ‹…Cβ‰ 0D \cdot C \neq 0. We may assume Dβ‹…C>0D \cdot C > 0 (replacing DD by βˆ’D-D if necessary, which preserves Dβ‹…H=0D \cdot H = 0 and D2=0D^2 = 0).

For integers m,nm, n, consider the divisor mH+nDmH + nD. Its self-intersection is:

(mH+nD)2=m2H2+2mn(Hβ‹…D)+n2D2=m2H2(mH + nD)^2 = m^2 H^2 + 2mn(H \cdot D) + n^2 D^2 = m^2 H^2

since Hβ‹…D=0H \cdot D = 0 and D2=0D^2 = 0. Also:

(mH+nD)β‹…H=mH2+n(Dβ‹…H)=mH2.(mH + nD) \cdot H = m H^2 + n(D \cdot H) = mH^2.

So for m>0m > 0, the divisor mH+nDmH + nD has positive self-intersection m2H2>0m^2 H^2 > 0 and positive intersection mH2>0mH^2 > 0 with the ample class HH. By Riemann--Roch:

Ο‡(O(mH+nD))=m2H22βˆ’m(Hβ‹…KX)+n(Dβ‹…KX)2+Ο‡(OX).\chi(\mathcal{O}(mH + nD)) = \frac{m^2 H^2}{2} - \frac{m(H \cdot K_X) + n(D \cdot K_X)}{2} + \chi(\mathcal{O}_X).

For mm large and fixed nn, by Serre's vanishing theorem (or asymptotic Riemann--Roch), h0(mH+nD)>0h^0(mH + nD) > 0 for m≫0m \gg 0. So mH+nDmH + nD is linearly equivalent to an effective divisor for mm sufficiently large (depending on nn).

Write mH+nD∼Em,nβ‰₯0mH + nD \sim E_{m,n} \geq 0. Then:

Em,nβ‹…C=m(Hβ‹…C)+n(Dβ‹…C).E_{m,n} \cdot C = m(H \cdot C) + n(D \cdot C).

Since HH is ample and CC is a divisor, Hβ‹…CH \cdot C is some fixed integer. By choosing nn negative with ∣n∣|n| large and mm appropriately large (to ensure effectivity), we can make:

Em,nβ‹…C=m(Hβ‹…C)+n(Dβ‹…C)<0.E_{m,n} \cdot C = m(H \cdot C) + n(D \cdot C) < 0.

But Em,nE_{m,n} is effective, and if CC were also effective and ample, this would give a contradiction. More carefully: replace CC by a large multiple of HH plus a correction. Since Dβ‹…C>0D \cdot C > 0 and we can choose n<0n < 0 with ∣n∣|n| as large as we like (adjusting mm accordingly), the intersection Em,nβ‹…CE_{m,n} \cdot C can be made arbitrarily negative.

However, we can argue more directly. Apply the result from Steps 1--2 to the divisor D′=mH+nDD' = mH + nD for a suitable pair (m,n)(m, n). Specifically, choose n≠0n \neq 0 and set D′=nDD' = nD. Then D′⋅H=0D' \cdot H = 0 and (D′)2=n2D2=0(D')^2 = n^2 D^2 = 0. By Riemann--Roch:

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

This is linear in nn. If Dβ‹…KXβ‰ 0D \cdot K_X \neq 0, then for nβ†’+∞n \to +\infty or nβ†’βˆ’βˆžn \to -\infty, Ο‡(O(nD))β†’+∞\chi(\mathcal{O}(nD)) \to +\infty, and the same argument as in Step 2 produces a contradiction. If Dβ‹…KX=0D \cdot K_X = 0, then Ο‡(O(nD))=Ο‡(OX)\chi(\mathcal{O}(nD)) = \chi(\mathcal{O}_X) for all nn, and we use a refined argument with mH+nDmH + nD as above.

For the refined argument with Dβ‹…KX=0D \cdot K_X = 0: consider Dβ€²=H+tDD' = H + tD for large integer tt. Then Dβ€²β‹…H=H2>0D' \cdot H = H^2 > 0, (Dβ€²)2=H2>0(D')^2 = H^2 > 0, and for tt large, Dβ€²β‹…C=Hβ‹…C+t(Dβ‹…C)D' \cdot C = H \cdot C + t(D \cdot C). Since Dβ‹…C>0D \cdot C > 0, the divisor Dβ€²D' behaves like an ample class. Apply the Hodge Index Theorem (the part we already proved: the strict inequality D2≀0D^2 \leq 0 for Dβ‹…H=0D \cdot H = 0) to the divisor DD with respect to the "pseudo-ample" class Dβ€²D'. Formally: if Eβ‹…Dβ€²=0E \cdot D' = 0 and (Dβ€²)2>0(D')^2 > 0, then E2≀0E^2 \leq 0. Taking E=aDβ€²βˆ’bDE = aD' - bD for appropriate a,ba, b to ensure Eβ‹…Dβ€²=0E \cdot D' = 0 leads to E2≀0E^2 \leq 0, which forces D2≀0D^2 \leq 0. Since we assumed D2=0D^2 = 0, this is consistent but shows DD must be numerically proportional to any class it pairs nontrivially with, eventually forcing D≑0D \equiv 0.

A cleaner approach: by the already-proved inequality D2≀0D^2 \leq 0, the form restricted to HβŠ₯H^\perp is negative semi-definite. If D2=0D^2 = 0 and Dβ‹…H=0D \cdot H = 0, then for any divisor CC, consider Dβ€²=Cβˆ’Cβ‹…HH2HD' = C - \frac{C \cdot H}{H^2} H. Then Dβ€²β‹…H=0D' \cdot H = 0, so (Dβ€²)2≀0(D')^2 \leq 0, i.e., C2βˆ’(Cβ‹…H)2H2≀0C^2 - \frac{(C \cdot H)^2}{H^2} \leq 0. Now Dβ‹…C=Dβ‹…Dβ€²+Dβ‹…Cβ‹…HH2H=Dβ‹…Dβ€²D \cdot C = D \cdot D' + D \cdot \frac{C \cdot H}{H^2} H = D \cdot D'. By the Cauchy--Schwarz inequality for the negative semi-definite form on HβŠ₯H^\perp:

(Dβ‹…Dβ€²)2β‰₯(βˆ’D2)(βˆ’Dβ€²2)(withΒ reversedΒ sign,Β sinceΒ theΒ formΒ isΒ negativeΒ semi-definite).(D \cdot D')^2 \geq (-D^2)(-D'^2) \quad \text{(with reversed sign, since the form is negative semi-definite)}.

Wait -- for a negative semi-definite form qq, the Cauchy--Schwarz inequality gives q(x,y)2≀q(x,x)β‹…q(y,y)q(x,y)^2 \leq q(x,x) \cdot q(y,y), i.e., (Dβ‹…Dβ€²)2≀D2β‹…(Dβ€²)2(D \cdot D')^2 \leq D^2 \cdot (D')^2. But D2=0D^2 = 0, so (Dβ‹…Dβ€²)2≀0(D \cdot D')^2 \leq 0, hence Dβ‹…Dβ€²=0D \cdot D' = 0, hence Dβ‹…C=0D \cdot C = 0 for all CC. This means D≑0D \equiv 0. β– \blacksquare

β– 
ExampleEquality case on P^1 x P^1

On P1Γ—P1\mathbb{P}^1 \times \mathbb{P}^1, take H∼F1+F2H \sim F_1 + F_2 (the diagonal class, which is ample with H2=2H^2 = 2). Consider D=F1βˆ’F2D = F_1 - F_2. Then:

  • Dβ‹…H=(F1βˆ’F2)β‹…(F1+F2)=0+1βˆ’1βˆ’0=0D \cdot H = (F_1 - F_2) \cdot (F_1 + F_2) = 0 + 1 - 1 - 0 = 0.
  • D2=(F1βˆ’F2)2=0βˆ’1βˆ’1+0=βˆ’2<0D^2 = (F_1 - F_2)^2 = 0 - 1 - 1 + 0 = -2 < 0.

So D2<0D^2 < 0, consistent with the theorem. And D≑̸0D \not\equiv 0 since Dβ‹…F1=1β‰ 0D \cdot F_1 = 1 \neq 0.

The form on HβŠ₯=span⁑(F1βˆ’F2)H^\perp = \operatorname{span}(F_1 - F_2) is ⟨F1βˆ’F2,F1βˆ’F2⟩=βˆ’2<0\langle F_1 - F_2, F_1 - F_2 \rangle = -2 < 0, confirming negative definiteness.


Complete Self-Contained Proof

ProofComplete proof of the Hodge Index Theorem

Theorem. Let XX be a smooth projective surface, HH an ample divisor. If Dβ‹…H=0D \cdot H = 0, then D2≀0D^2 \leq 0, with equality iff D≑0D \equiv 0.

Proof. Suppose Dβ‹…H=0D \cdot H = 0.

(i) Proving D2≀0D^2 \leq 0. Assume for contradiction that D2>0D^2 > 0. By Riemann--Roch:

Ο‡(OX(nD))=n22D2βˆ’n2Dβ‹…KX+Ο‡(OX)β†’+∞\chi(\mathcal{O}_X(nD)) = \frac{n^2}{2} D^2 - \frac{n}{2} D \cdot K_X + \chi(\mathcal{O}_X) \to +\infty

as ∣nβˆ£β†’βˆž|n| \to \infty, since the n2n^2 term dominates. So h0(nD)+h0(KXβˆ’nD)β‰₯Ο‡(OX(nD))β†’+∞h^0(nD) + h^0(K_X - nD) \geq \chi(\mathcal{O}_X(nD)) \to +\infty.

If h0(nD)β‰₯1h^0(nD) \geq 1 for some n>0n > 0, then nDnD is effective, so nDβ‹…H>0nD \cdot H > 0 by ampleness of HH. But nDβ‹…H=0nD \cdot H = 0, contradiction.

If h0(βˆ’nD)β‰₯1h^0(-nD) \geq 1 for some n>0n > 0, then βˆ’nD-nD is effective, so (βˆ’nD)β‹…H>0(-nD) \cdot H > 0, giving βˆ’n(Dβ‹…H)>0-n(D \cdot H) > 0, i.e., 0>00 > 0, contradiction.

Therefore h0(nD)=0h^0(nD) = 0 for all nβ‰ 0n \neq 0. Then h0(KXβˆ’nD)β†’βˆžh^0(K_X - nD) \to \infty, so KXβˆ’nDK_X - nD is effective for large n>0n > 0, and KX+nDK_X + nD is effective for large n>0n > 0. Adding: Fn+Gn∼2KXF_n + G_n \sim 2K_X with Fn=KXβˆ’nDβ‰₯0F_n = K_X - nD \geq 0 and Gn=KX+nDβ‰₯0G_n = K_X + nD \geq 0. Since the set of effective decompositions of 2KX2K_X is finite (bounded family), for large n,mn, m with nβ‰ mn \neq m: Fn=FmF_n = F_m, giving (nβˆ’m)D∼0(n - m)D \sim 0, so D2=0D^2 = 0, contradicting D2>0D^2 > 0.

(ii) Proving equality implies D≑0D \equiv 0. Suppose Dβ‹…H=0D \cdot H = 0 and D2=0D^2 = 0. By part (i), the intersection form is negative semi-definite on HβŠ₯H^\perp. For any divisor CC, set Cβ€²=Cβˆ’Cβ‹…HH2H∈HβŠ₯βŠ—QC' = C - \frac{C \cdot H}{H^2} H \in H^\perp \otimes \mathbb{Q}. Then Dβ‹…C=Dβ‹…Cβ€²D \cdot C = D \cdot C' (since Dβ‹…H=0D \cdot H = 0). By Cauchy--Schwarz for the negative semi-definite form:

(Dβ‹…Cβ€²)2≀D2β‹…(Cβ€²)2=0β‹…(Cβ€²)2=0.(D \cdot C')^2 \leq D^2 \cdot (C')^2 = 0 \cdot (C')^2 = 0.

Hence Dβ‹…Cβ€²=0D \cdot C' = 0, so Dβ‹…C=0D \cdot C = 0 for all divisors CC. Therefore D≑0D \equiv 0. β– \blacksquare

β– 

Verification on Standard Surfaces

ExampleVerification on P^2

On P2\mathbb{P}^2: NS⁑(P2)=Zβ‹…H\operatorname{NS}(\mathbb{P}^2) = \mathbb{Z} \cdot H with H2=1H^2 = 1, ρ=1\rho = 1.

The orthogonal complement HβŠ₯H^\perp in NS⁑(P2)βŠ—R\operatorname{NS}(\mathbb{P}^2) \otimes \mathbb{R} is {0}\{0\}, since the lattice is rank 11. So the theorem is vacuously true: the only divisor with Dβ‹…H=0D \cdot H = 0 is D≑0D \equiv 0, and indeed 02=00^2 = 0. The signature is (1,0)(1, 0).

ExampleVerification on Bl_P(P^2)

On Bl⁑P(P2)\operatorname{Bl}_P(\mathbb{P}^2) with NS⁑=ZLβŠ•ZE\operatorname{NS} = \mathbb{Z} L \oplus \mathbb{Z} E, where L2=1L^2 = 1, E2=βˆ’1E^2 = -1, Lβ‹…E=0L \cdot E = 0. The Picard number is ρ=2\rho = 2.

Take H=2Lβˆ’EH = 2L - E (ample, since H2=4βˆ’1=3>0H^2 = 4 - 1 = 3 > 0 and Hβ‹…L=2>0H \cdot L = 2 > 0, Hβ‹…E=1>0H \cdot E = 1 > 0).

Find D∈HβŠ₯D \in H^\perp: D=aL+bED = aL + bE with Dβ‹…H=2aβˆ’b=0D \cdot H = 2a - b = 0, so b=2ab = 2a. Take D=L+2ED = L + 2E. Then:

D2=1+4(βˆ’1)=βˆ’3<0D^2 = 1 + 4(-1) = -3 < 0.

The form on HβŠ₯=Rβ‹…(L+2E)H^\perp = \mathbb{R} \cdot (L + 2E) is (L+2E)2=βˆ’3<0(L + 2E)^2 = -3 < 0. Signature of full form: (1,1)(1, 1).

ExampleVerification on Hirzebruch surfaces F_n

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

Take H=C0+(n+1)FH = C_0 + (n+1)F (ample for nβ‰₯0n \geq 0). Then H2=βˆ’n+2(n+1)=n+2>0H^2 = -n + 2(n+1) = n + 2 > 0.

Find D=aC0+bFD = aC_0 + bF with Dβ‹…H=0D \cdot H = 0: a(βˆ’n+n+1)+b(1)=a+b=0a(-n + n + 1) + b(1) = a + b = 0, so b=βˆ’ab = -a. Take D=C0βˆ’FD = C_0 - F. Then:

D2=(C0βˆ’F)2=βˆ’nβˆ’2<0D^2 = (C_0 - F)^2 = -n - 2 < 0 for all nβ‰₯0n \geq 0.

On HβŠ₯H^\perp: the restriction of the form is βˆ’nβˆ’2<0-n - 2 < 0. Signature: (1,1)(1, 1).

For F0=P1Γ—P1\mathbb{F}_0 = \mathbb{P}^1 \times \mathbb{P}^1: D2=βˆ’2D^2 = -2. For F1=Bl⁑P(P2)\mathbb{F}_1 = \operatorname{Bl}_P(\mathbb{P}^2): D2=βˆ’3D^2 = -3. For F2\mathbb{F}_2: D2=βˆ’4D^2 = -4.

ExampleVerification on a K3 surface with rho = 2

Consider a K3 surface with NS⁑(X)β‰…ZHβŠ•ZD\operatorname{NS}(X) \cong \mathbb{Z} H \oplus \mathbb{Z} D where H2=4H^2 = 4, D2=βˆ’2D^2 = -2, Hβ‹…D=0H \cdot D = 0. (This arises, for example, from a quartic in P3\mathbb{P}^3 containing a line DD.)

Here DD is already in HβŠ₯H^\perp, and D2=βˆ’2<0D^2 = -2 < 0, confirming the theorem.

The intersection matrix is diag⁑(4,βˆ’2)\operatorname{diag}(4, -2) with signature (1,1)(1, 1).

The class DD is realized by a smooth rational (βˆ’2)(-2)-curve. It cannot be effective and satisfy Dβ‹…H=0D \cdot H = 0 simultaneously -- but wait, DD is effective (it is a line on the quartic) and Dβ‹…H=0D \cdot H = 0. This seems to contradict ampleness. The resolution: HH is not ample if Hβ‹…D=0H \cdot D = 0 for an effective curve DD. The class HH here is nef but not ample. To apply the Hodge Index Theorem, we need HH genuinely ample, e.g., replace HH by Hβ€²=H+Ο΅Dβ€²H' = H + \epsilon D' for some correction. In fact, on this K3, the ample cone excludes the boundary Hβ‹…D=0H \cdot D = 0. Taking Hβ€²=H+DH' = H + D (not ample either, since (H+D)β‹…D=βˆ’2<0(H + D) \cdot D = -2 < 0). Instead take Hβ€²=2H+DH' = 2H + D: (Hβ€²)2=16βˆ’2=14>0(H')^2 = 16 - 2 = 14 > 0, Hβ€²β‹…D=βˆ’2<0H' \cdot D = -2 < 0 (still not ample).

Actually, the correct ample class should satisfy Hβ€²β‹…C>0H' \cdot C > 0 for all effective curves. On this K3, the only (βˆ’2)(-2)-curve is DD, so Hβ€²=H+DH' = H + D gives Hβ€²β‹…D=0βˆ’2<0H' \cdot D = 0 - 2 < 0: not ample. We need Hβ€²β‹…D>0H' \cdot D > 0, so try Hβ€²=Hβˆ’Ξ±DH' = H - \alpha D for Ξ±>0\alpha > 0: Hβ€²β‹…D=2Ξ±>0H' \cdot D = 2\alpha > 0, (Hβ€²)2=4βˆ’2Ξ±2(H')^2 = 4 - 2\alpha^2. For Ξ±=1\alpha = 1: (Hβ€²)2=2>0(H')^2 = 2 > 0, Hβ€²β‹…D=2>0H' \cdot D = 2 > 0, so Hβ€²=Hβˆ’DH' = H - D is ample. Then Hβ€²βŠ₯H'^\perp: aH+bDaH + bD with a(Hβ‹…Hβ€²)+b(Dβ‹…Hβ€²)=aβ‹…6+bβ‹…2=0a(H \cdot H') + b(D \cdot H') = a \cdot 6 + b \cdot 2 = 0, so b=βˆ’3ab = -3a. Take E=Hβˆ’3DE = H - 3D: E2=4βˆ’18=βˆ’14<0E^2 = 4 - 18 = -14 < 0. Confirmed.


Alternative Proof over C: Hodge Theory

ProofAnalytic proof via Hodge decomposition (over C)

Over C\mathbb{C}, a more conceptual proof uses the Hodge decomposition.

Setup. Let XX be a smooth projective surface over C\mathbb{C}. The second cohomology decomposes as:

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

The intersection form is given by the cup product pairing on H2(X,Z)H^2(X, \mathbb{Z}).

The Hodge--Riemann bilinear relations. Let Ο‰βˆˆH1,1(X)\omega \in H^{1,1}(X) be the class of a Kahler form (i.e., an ample class). Define the primitive cohomology P1,1=ker⁑(Ο‰βˆ§βˆ’:H1,1β†’H3,3)=(Ο‰)βŠ₯∩H1,1P^{1,1} = \ker(\omega \wedge -: H^{1,1} \to H^{3,3}) = (\omega)^\perp \cap H^{1,1}. The Hodge--Riemann relations state:

  • The pairing is positive definite on H2,0βŠ•H0,2H^{2,0} \oplus H^{0,2} (after adjusting signs).
  • The pairing restricted to Rβ‹…Ο‰\mathbb{R} \cdot \omega is positive definite (since Ο‰2=∫XΟ‰βˆ§Ο‰>0\omega^2 = \int_X \omega \wedge \omega > 0).
  • The pairing restricted to PR1,1=Ο‰βŠ₯∩HR1,1P^{1,1}_{\mathbb{R}} = \omega^\perp \cap H^{1,1}_{\mathbb{R}} is negative definite.

Deducing the algebraic statement. The Neron--Severi group NS⁑(X)\operatorname{NS}(X) embeds into H1,1(X)∩H2(X,Z)H^{1,1}(X) \cap H^2(X, \mathbb{Z}). The ample class HH maps to a Kahler class Ο‰\omega, and Dβ‹…H=0D \cdot H = 0 in the algebraic sense translates to [D]∈P1,1[D] \in P^{1,1}. The negative definiteness of the pairing on P1,1P^{1,1} gives D2<0D^2 < 0 for [D]β‰ 0[D] \neq 0, and D2=0D^2 = 0 iff [D]=0[D] = 0 in H1,1H^{1,1}.

Since NS⁑(X)\operatorname{NS}(X) injects into H1,1H^{1,1} modulo torsion, [D]=0[D] = 0 in H1,1H^{1,1} iff D≑0D \equiv 0 numerically.

β– 
RemarkComparison of the two proofs

The algebraic proof (Steps 1--3) works over any algebraically closed field and uses only Riemann--Roch plus basic properties of ample divisors. Its key insight is that if D2>0D^2 > 0 and Dβ‹…H=0D \cdot H = 0, then the Euler characteristic grows quadratically, forcing effective divisors orthogonal to HH to exist, which is impossible.

The analytic proof over C\mathbb{C} is more conceptual: it derives the theorem from the definiteness properties of the Hodge--Riemann bilinear relations, which are themselves consequences of the Kahler identities and the Hard Lefschetz theorem. The analytic proof also immediately gives the signature of the full lattice H2(X,Z)H^2(X, \mathbb{Z}), not just the Neron--Severi group.


Consequence 1: The Hodge Inequality

TheoremHodge inequality (algebraic form)

Let XX be a smooth projective surface, and let C,DC, D be divisors on XX. Then:

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

with equality if and only if CC and DD are numerically proportional (i.e., aC≑bDaC \equiv bD for some integers a,ba, b not both zero).

This is the Cauchy--Schwarz inequality for the intersection form, valid because the form has signature (1,Οβˆ’1)(1, \rho - 1).

ProofDeriving the Hodge inequality from the index theorem

If D2≀0D^2 \leq 0 or C2≀0C^2 \leq 0, the right side is ≀0\leq 0 and the inequality is trivially satisfied (since (Cβ‹…D)2β‰₯0(C \cdot D)^2 \geq 0).

Suppose C2>0C^2 > 0. By Nakai--Moishezon, if also Cβ‹…E>0C \cdot E > 0 for all curves EE, then CC is ample and we can use CC as the ample class. Set Dβ€²=Dβˆ’Dβ‹…CC2CD' = D - \frac{D \cdot C}{C^2} C. Then:

Dβ€²β‹…C=Dβ‹…Cβˆ’Dβ‹…CC2β‹…C2=0.D' \cdot C = D \cdot C - \frac{D \cdot C}{C^2} \cdot C^2 = 0.

By the Hodge Index Theorem applied with the ample class replaced by a suitable positive multiple of CC:

Dβ€²2≀0.D'^2 \leq 0.

Expanding: Dβ€²2=D2βˆ’2Dβ‹…CC2(Dβ‹…C)+(Dβ‹…C)2(C2)2C2=D2βˆ’(Dβ‹…C)2C2≀0.D'^2 = D^2 - 2 \frac{D \cdot C}{C^2}(D \cdot C) + \frac{(D \cdot C)^2}{(C^2)^2} C^2 = D^2 - \frac{(D \cdot C)^2}{C^2} \leq 0.

Rearranging: (Cβ‹…D)2β‰₯C2β‹…D2(C \cdot D)^2 \geq C^2 \cdot D^2. Equality holds iff D′≑0D' \equiv 0, iff D≑Dβ‹…CC2CD \equiv \frac{D \cdot C}{C^2} C, iff CC and DD are numerically proportional. β– \blacksquare

β– 
ExampleHodge inequality on P^2

On P2\mathbb{P}^2 with C∼aHC \sim aH, D∼bHD \sim bH: (Cβ‹…D)2=(ab)2=a2b2=C2β‹…D2(C \cdot D)^2 = (ab)^2 = a^2 b^2 = C^2 \cdot D^2. Equality holds because all divisors are numerically proportional (Picard number ρ=1\rho = 1).

ExampleHodge inequality on P^1 x P^1

On P1Γ—P1\mathbb{P}^1 \times \mathbb{P}^1: C∼(a,b)C \sim (a, b) and D∼(c,d)D \sim (c, d).

(Cβ‹…D)2=(ad+bc)2(C \cdot D)^2 = (ad + bc)^2 and C2β‹…D2=(2ab)(2cd)=4abcdC^2 \cdot D^2 = (2ab)(2cd) = 4abcd.

The inequality (ad+bc)2β‰₯4abcd(ad + bc)^2 \geq 4abcd is equivalent to (adβˆ’bc)2β‰₯0(ad - bc)^2 \geq 0, which always holds. Equality iff ad=bcad = bc, i.e., a/c=b/da/c = b/d, i.e., CC and DD are numerically proportional.


Consequence 2: Negative Definiteness of Exceptional Divisors

TheoremNegative definiteness of exceptional configurations

Let f:Xβ†’Yf: X \to Y be a birational morphism of smooth projective surfaces, and let E1,…,ErE_1, \ldots, E_r be the irreducible components of the exceptional locus. Then the intersection matrix (Eiβ‹…Ej)1≀i,j≀r(E_i \cdot E_j)_{1 \leq i,j \leq r} is negative definite.

ProofProof using the Hodge Index Theorem

Let HYH_Y be an ample divisor on YY, and let H=fβˆ—HYH = f^* H_Y. Then HH is nef and big on XX (it is the pullback of an ample divisor), and Hβ‹…Ei=HYβ‹…fβˆ—Ei=0H \cdot E_i = H_Y \cdot f_* E_i = 0 for each ii (since fβˆ—Ei=0f_* E_i = 0 as a cycle on YY, because EiE_i is contracted by ff).

Any divisor D=βˆ‘aiEiD = \sum a_i E_i supported on the exceptional locus satisfies Dβ‹…H=βˆ‘ai(Eiβ‹…H)=0D \cdot H = \sum a_i (E_i \cdot H) = 0. By the Hodge Index Theorem (extended to nef and big classes by a limit argument, or by perturbing HH to a nearby ample class H+Ο΅AH + \epsilon A):

D2≀0,withΒ equalityΒ iffΒ D≑0.D^2 \leq 0, \quad \text{with equality iff } D \equiv 0.

But on a smooth surface, D=βˆ‘aiEi≑0D = \sum a_i E_i \equiv 0 with all EiE_i exceptional implies all ai=0a_i = 0 (since the EiE_i are linearly independent in NS⁑(X)\operatorname{NS}(X)). Therefore the quadratic form D↦D2D \mapsto D^2 is strictly negative definite on ⨁ZEi\bigoplus \mathbb{Z} E_i. β– \blacksquare

β– 
ExampleBlowup of P^2 at two points

Let X=Bl⁑P,Q(P2)X = \operatorname{Bl}_{P,Q}(\mathbb{P}^2) with exceptional divisors E1,E2E_1, E_2. The intersection matrix (Eiβ‹…Ej)(E_i \cdot E_j) has entries:

  • E12=βˆ’1E_1^2 = -1, E22=βˆ’1E_2^2 = -1, E1β‹…E2=0E_1 \cdot E_2 = 0.

So the matrix is βˆ’I2-I_2 (the negative of the 2Γ—22 \times 2 identity), which is negative definite. The eigenvalues are both βˆ’1-1.

ExampleResolution of an A_n singularity

The minimal resolution of the AnA_n surface singularity x2+y2+zn+1=0x^2 + y^2 + z^{n+1} = 0 has nn exceptional curves E1,…,EnE_1, \ldots, E_n, each isomorphic to P1\mathbb{P}^1, forming a chain: Eiβ‹…Ej=1E_i \cdot E_j = 1 if ∣iβˆ’j∣=1|i - j| = 1, Ei2=βˆ’2E_i^2 = -2, and Eiβ‹…Ej=0E_i \cdot E_j = 0 if ∣iβˆ’j∣β‰₯2|i - j| \geq 2.

The intersection matrix is the negative of the Cartan matrix of type AnA_n:

  • n=1n = 1: (βˆ’2)(-2), eigenvalue βˆ’2-2.
  • n=2n = 2: diagonal entries βˆ’2-2, off-diagonal 11. Eigenvalues: βˆ’2Β±1=βˆ’1,βˆ’3-2 \pm 1 = -1, -3. Both negative.
  • n=3n = 3: eigenvalues βˆ’2+2cos⁑(kΟ€/4)-2 + 2\cos(k\pi/4) for k=1,2,3k = 1, 2, 3, giving approximately βˆ’0.59,βˆ’2,βˆ’3.41-0.59, -2, -3.41. All negative.

In general, the eigenvalues of the AnA_n Cartan matrix are 2βˆ’2cos⁑(kΟ€/(n+1))2 - 2\cos(k\pi/(n+1)) for k=1,…,nk = 1, \ldots, n, all positive, so the intersection matrix (its negative) is negative definite.


Consequence 3: Signature Constraints

RemarkThe signature (1, rho - 1)

The Hodge Index Theorem determines the signature of the intersection form on NS⁑(X)βŠ—R\operatorname{NS}(X) \otimes \mathbb{R} completely: it is (1,Οβˆ’1)(1, \rho - 1).

Proof of signature claim. Let HH be ample. Then H2>0H^2 > 0, so the form has at least one positive eigenvalue. By the theorem, HβŠ₯H^\perp is negative definite, so there are no other positive eigenvalues. Since the form is non-degenerate on NS⁑(X)/torsion\operatorname{NS}(X) / \text{torsion} (by definition of numerical equivalence), we get exactly one positive and Οβˆ’1\rho - 1 negative eigenvalues.

This is a strong constraint: knowing ρ\rho and the lattice structure determines the intersection form up to finitely many possibilities (by the theory of indefinite lattices).

ExampleSignatures for classical surfaces
  • P2\mathbb{P}^2: ρ=1\rho = 1, signature (1,0)(1, 0). Form: (1)(1).
  • P1Γ—P1\mathbb{P}^1 \times \mathbb{P}^1: ρ=2\rho = 2, signature (1,1)(1, 1). Form: the hyperbolic plane UU.
  • Bl⁑k(P2)\operatorname{Bl}_k(\mathbb{P}^2) (kk points blown up): ρ=k+1\rho = k + 1, signature (1,k)(1, k). Form: ⟨1βŸ©βŠ•βŸ¨βˆ’1⟩k\langle 1 \rangle \oplus \langle -1 \rangle^k.
  • K3 with ρ=1\rho = 1: signature (1,0)(1, 0). The full lattice H2(X,Z)H^2(X, \mathbb{Z}) has signature (3,19)(3, 19) (from the Hodge decomposition: h2,0=h0,2=1h^{2,0} = h^{0,2} = 1 contribute two more positive directions), but the Neron--Severi part has signature (1,0)(1, 0).
  • K3 with ρ=20\rho = 20: signature (1,19)(1, 19) on NS⁑\operatorname{NS}, and the transcendental lattice has signature (2,0)(2, 0).

Application: Why Negative Curves are Rigid

RemarkRigidity of negative curves

The Hodge Index Theorem explains why curves with negative self-intersection are rigid (cannot be deformed):

If CC is an irreducible curve with C2<0C^2 < 0, then ∣C∣|C| has no other member: h0(O(C))=1h^0(\mathcal{O}(C)) = 1. Indeed, if D∼CD \sim C with Dβ‰ CD \neq C, then Dβˆ’C∼0D - C \sim 0 but Dβˆ’Cβ‰ 0D - C \neq 0 as a divisor, meaning D=CD = C as divisor classes. More precisely, if Dβ‰₯0D \geq 0, D∼CD \sim C, and Dβ‰ CD \neq C, then C≀DC \leq D (since CC is irreducible and appears in DD, or CC and DD share no component). In the latter case, Cβ‹…Dβ‰₯0C \cdot D \geq 0 (two effective divisors with no common component meet non-negatively), but Cβ‹…D=C2<0C \cdot D = C^2 < 0, contradiction.

This applies to:

  • (βˆ’1)(-1)-curves on blowups (exceptional divisors).
  • (βˆ’2)(-2)-curves on K3 surfaces and rational surfaces.
  • Negative sections C0C_0 on Hirzebruch surfaces Fn\mathbb{F}_n with n>0n > 0.

Summary of the Proof Strategy

RemarkProof architecture

The proof of the Hodge Index Theorem has a clean two-part structure:

Part 1 (D2≀0D^2 \leq 0): Assume D2>0D^2 > 0 and Dβ‹…H=0D \cdot H = 0. Riemann--Roch gives quadratic growth of Ο‡(O(nD))\chi(\mathcal{O}(nD)), forcing either nDnD or KXβˆ’nDK_X - nD to be effective for large nn. But effectivity contradicts Dβ‹…H=0D \cdot H = 0 and the ampleness of HH (ample divisors pair positively with effective divisors). A more delicate argument using the finiteness of decompositions of a fixed class handles the case where KXβˆ’nDK_X - nD is effective.

Part 2 (D2=0D^2 = 0 implies D≑0D \equiv 0): Once negative semi-definiteness on HβŠ₯H^\perp is established, a Cauchy--Schwarz argument shows that any class DD with D2=0D^2 = 0 in HβŠ₯H^\perp pairs trivially with all other classes, hence is numerically trivial.

The theorem is the algebraic counterpart of the Hodge--Riemann bilinear relations and is fundamental to the classification theory of algebraic surfaces.