COMPLEX GEOMETRY NOTES 1. Characteristic Numbers Of

COMPLEX GEOMETRY NOTES 1. Characteristic Numbers Of

COMPLEX GEOMETRY NOTES JEFF A. VIACLOVSKY 1. Characteristic numbers of hypersurfaces Let V ⊂ Pn be a smooth complex hypersurface. We know that the line bundle [V ] = O(d) for some d ≥ 1. We have the exact sequence (1,0) (1,0) 2 (1.1) 0 → T (V ) → T P V → NV → 0. The adjunction formula says that (1.2) NV = O(d) V . We have the smooth splitting of (1.1), (1,0) n (1,0) (1.3) T P V = T (V ) ⊕ O(d) V . Taking Chern classes, (1,0) n (1,0) (1.4) c(T P V ) = c(T (V )) · c(O(d) V ). From the Euler sequence [GH78, page 409], ⊕(n+1) (1,0) n (1.5) 0 → C → O(1) → T P → 0, it follows that (1,0) n n+1 (1.6) c(T P ) = (1 + c1(O(1))) . Note that for any divisor D, (1.7) c1([D]) = ηD, where ηD is the Poincar´edual to D. That is Z Z (1.8) ξ = ξ ∧ ηD, n D P 2n−2 for all ξ ∈ H (P), see [GH78, page 141]. So in particular c1(O(1)) = ω, where ω is the Poincar´edual of a hyperplane in Pn (note that ω is integral, and is some multiple of the Fubini-Study metric). Therefore (1,0) n n+1 (1.9) c(T P ) = (1 + ω) . ⊗d Also c1(O(d)) = d · ω, since O(d) = O(1) . The formula (1.4) is then n+1 (1.10) (1 + ω) V = (1 + c1 + c2 + ... )(1 + d · ω V ). Date: November 21, 2006. 1 2 JEFF A. VIACLOVSKY 2. Dimension n = 2 Consider a curve in P2. The formula (1.10) is (2.1) (1 + 3ω) V = (1 + c1)(1 + d · ω V ), which yields (2.2) c1 = (3 − d)ω V . The top Chern class is the Euler class, so we have Z (2.3) χ(V ) = (3 − d)ω V Z = (3 − d) ω ∧ (d · ω)(2.4) 2 ZP (2.5) = d(3 − d) ω2 = d(3 − d). 2 P Here we used the fact that d · ω is Poincar´edual to V , and ω2 is a positive generator of H4(P2, Z). Equivalently, we can write Z Z Z (2.6) ω = ω ∧ ηV = ηH ∧ ηV . 2 2 V P P Since cup product is dual to intersection under Poincar´eduality, the integral simply counts the number of intersection points of V with a generic hyperplane. In term of the genus g, (d − 1)(d − 2) (2.7) g = . 2 3. Dimension n = 3 We consider a hypersurface in P3, which is topologically a 4-manifold. The formula (1.10) is 2 (3.1) (1 + 4ω + 6ω ) V = (1 + c1 + c2) · (1 + d · ω V ), so that (3.2) c1 = (4 − d)ω V , and then 2 (3.3) c2 = (6 − d(4 − d))ω V . Since the top Chern class is the Euler class, Z (3.4) χ(V ) = (6 − d(4 − d))ω2 V Z = (6 − d(4 − d)) ω2 ∧ (d · ω)(3.5) 3 P (3.6) = d(6 − d(4 − d)), again using the fact that d·ω is Poincar´edual to V , and that ω3 is a positive generator of H6(P3, Z). COMPLEX GEOMETRY NOTES 3 It follows from the Lefschetz Hyperplane Theorem [GH78, page 156], that M has 1,0 0,1 b1 = 0, therefore b = b = 0. 3.1. Hirzebruch Signature Theorem. We think of V as a real 4-manifold, with complex structure given by J. Then the kth Pontrjagin Class is defined to be k pk(V ) = (−1) c2k(TV ⊗ C)(3.7) Since (V, J) is complex, we have that (3.8) TV ⊗ C = TV ⊕ TV, so c(TV ⊗ C) = c(TV ) · c(TV )(3.9) = (1 + c1 + c2) · (1 − c1 + c2)(3.10) 2 (3.11) = 1 + 2c2 − c1, which yields 2 (3.12) p1(V ) = c1 − 2c2. Consider next the intersection pairing H2(V ) × H2(V ) → R, given by Z (3.13) (α, β) → α ∧ β ∈ R. + − Let b2 denote the number of positive eigenvalues, and b2 denote the number of negative eigenvalues. By Poincar´eduality the intersection pairing is non-degenerate, so + − (3.14) b2 = b2 + b2 . The signature of V is defined to be + − (3.15) τ = b2 − b2 . The Hirzebruch Signature Theorem [MS74, page 224] states that 1 Z τ = p1(V )(3.16) 3 V Z 1 2 (3.17) = (c1 − 2c2). 3 V Rewriting this, Z 2 (3.18) 2χ + 3τ = c1. V Remark. This implies that S4 does not admit any almost complex structure, since the left hand side is 4, but the right hand side trivially vanishes. Pointwise, let + 2 (3.19) Λ2 = {α ∈ Λ (M, R): ∗α = α} − 2 (3.20) Λ2 = {α ∈ Λ (M, R): ∗α = −α}. 4 JEFF A. VIACLOVSKY On any K¨ahler manifold, + (2,0) (0,2) (3.21) Λ2 ⊗ C = (C · ω) ⊕ Λ ⊕ Λ , − (1,1) ⊥ (1,1) (3.22) Λ2 ⊗ C = Λo = (C · ω) ∩ Λ . (1,1) (Recall that Λo is by definition the primitive (1, 1)-forms.) Observe that this is a real decomposition, that is + (2,0) (2,0) (3.23) Λ2 = (R · ω) ⊕ {Λ ⊕ Λ }, (3.24) Λ− = Λ(1,1) = ( · ω)⊥ ∩ Λ1,1. 2 o,R R This decomposition follows from the proof of the Hodge-Riemann bilinear relations [GH78, page 123]. Applying this to the intersection form, we have the identities + 2,0 (3.25) b2 = 1 + 2b − 1,1 (3.26) b2 = b − 1. So we have that 1,1 2,0 (3.27) χ = 2 + b2 = 2 + b + 2b (3.28) τ = 2 + 2b2,0 − b1,1. Remark. Notice that (3.29) χ + τ = 4(1 + b2,0), so in particular, the integer χ + τ is divisible by 4 on a K¨ahler manifold with b1 = 0. This is in fact true for any almost complex manifold of real dimension 4, this follows from a version of Riemann-Roch Theorem which holds for almost complex manifolds, see [Gil95, Lemma 3.5.3]. Applying these formulas to our example, we find that Z (3.30) 2χ + 3τ = (4 − d)2 ω2 = d(4 − d)2. V Using the formula for the Euler characteristic form above, (3.31) χ = d(6 − d(4 − d)), we find that 1 (3.32) τ = − d(d + 2)(d − 2). 3 COMPLEX GEOMETRY NOTES 5 Some arithmetic shows that 3 2 b2 = d − 4d + 6d − 2(3.33) 1 b+ = (d3 − 6d2 + 11d − 3)(3.34) 2 3 1 b− = (d − 1)(2d2 − 4d + 3)(3.35) 2 3 1 b2,0 = b0,2 = (d − 3)(d − 2)(d − 1)(3.36) 6 1 b1,1 = d(2d2 − 6d + 7)(3.37) 3 (3.38) b1,0 = b0,1 = 0. + − For d = 2, we find that b2 = 1, b2 = 1. This is not surprising, as any non- degenerate quadric is biholomorphic to P1 ×P1 [GH78, page 478]. The Hodge numbers are b1,1 = 2, b0,2 = b2,0 = 0. + − For d = 3, we find b2 = 1, b2 = 6. This is expected, since any non-degenerate cubic is biholomorphic to P2 blown up at 6 points, and is therefore diffeomorphic to P2#6P2 [GH78, page 489]. The Hodge numbers in this case are b1,1 = 7, b0,2 = b2,0 = 0. + − For d = 4, this is a K3 surface [GH78, page 590]. We find b2 = 3, b2 = 19, so χ = 24, and τ = −16. The intersection form is given by 0 1 (3.39) 2E ⊕ 3 . 8 1 0 Since c1 = 0, the canonical bundle is trivial. The Hodge numbers in this case are b1,1 = 20, b0,2 = b2,0 = 1. + − For d = 5, we find b2 = 9, b2 = 44, so χ = 55, and τ = −35. From Freedman’s topological classification of simply-connected 4-manifolds, V must be homeomorphic to 9P2#44P2, see [FQ90]. By the work of Gromov-Lawson [GL80], this latter smooth manifold admits a metric of positive scalar curvature, and therefore all of its Seiberg- Witten invariants vanish [Wit94]. But V is K¨ahler,so it has some non-zero Seiberg- Witten invariant [Mor96, Theorem 7.4.4]. We conclude that V is homeomorphic to 9P2#44P2, but not diffeomorphic. 4. Riemann-Roch Theorem Instead of using the Hirzebruch signature Theorem to compute these characteristic numbers, we can use the Riemann-Roch formula for complex manifolds. Let E be a complex vector bundle over V of rank k. Assume that E splits into a sum of line bundles (4.1) E = L1 ⊕ · · · ⊕ Lk. Let ai = c1(Li). Then (4.2) c(E) = (1 + a1) ··· (1 + ak), 6 JEFF A. VIACLOVSKY which shows that cj(E) is given by the elementary symmetric functions of the ai, that is X (4.3) cj(E) = ai1 ··· aik . i1<···<ik Any other symmetric polynomial can always be expressed as a polynomial in the elementary symmetric functions. We define the Chern character as (4.4) ch(E) = eai + ··· + eak . Re-expressing in terms of the Chern classes, we have the first few terms of the Chern character: 1 (4.5) ch(E) = rank(E) + c (E) + c (E)2 − 2c (E) + .... 1 2 1 2 The Todd Class is associated to a a (4.6) T d(E) = 1 ··· k 1 − e−a1 1 − e−ak Re-expressing in terms of the Chern classes, we have the first few terms of the Todd class: 1 1 1 (4.7) T d(E) = 1 + c (E) + c (E)2 + c (E) + c (E)c (E) + ...

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