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International Congress of Mathematicians

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516 Miles Reiddeg Kc = 2g — 2. We see thatK C < 0 g = 0, K C = 0 g=l, K c > 0 g > 2.This trichotomy is basic for the study <strong>of</strong> a curve C from every point <strong>of</strong> view,including topology, differential geometry, complex function theory, moduli, all theway through to algebraic geometry and Diophantine number theory. To relatethis briefly to curvature as discussed in Section 1.2, for an arbitrary Riemannianmetric, the average value <strong>of</strong> curvature over C equals — deg Kc by the Gauss^Bonnettheorem; moreover, by the Riemann mapping theorem, there exists a metric on C inthe conformai class <strong>of</strong> the complex structure with constant positive, zero or negativecurvature in the three cases.2. Classification <strong>of</strong> 3-foldsThe great trichotomy also drives classification in higher dimensions. Themeaning <strong>of</strong> "higher dimensions" is time-dependent: dim 2 was worked out around1900 by Castelnuovo and Enriques, dim 3 during the 1980s by Mori and others, anddim 4 is just taking <strong>of</strong>f with Shokurov's current work. I concentrate on dim 3, wherethese issues first arose systematically.2.1. Preliminaries: the canonical class K xAn n-dimensional projective variety X can be embedded X ^y P^, and isgiven there by homogeneous polynomial equations; nonsingular means that at everypoint F e X, we can choose N — n <strong>of</strong> the defining equations so that the Jacobianmatrix -jfifi has rank N — n, with n linear coordinates <strong>of</strong> P^ providing local analyticcoordinates on X.The canonical class <strong>of</strong> X is Kx = iì x = /\ n ii x . It has many interpretations:it is the line bundle obtained as the top exterior power <strong>of</strong> the holomorphic cotangentbundle; it has transition functions on U n U' the Jacobian determinant det jfi 1 ,where x,x' are systems <strong>of</strong> local analytic coordinates on open sets U,U' C X; itssections are holomorphic n-forms; at a nonsingular point P £ X, its sections aregenerated by the holomorphic volume form d#i A- • • Adx n , so that ii x = Ox -dxi A• • • A dx n .For MMP to work in dim > 3, we are eventually forced to allow certain mildsingularities. The theory in dim 3 is now standard and not very hard (see [YPG] andcompare the foreword to [CR]). We always insist that the first Chern class <strong>of</strong> Kxrestricted to the nonsingular locus X° c X comes from an element <strong>of</strong> H 2 (X, Q),that I continue to denote by Kx- This ensures that the pullback f*Kx by amorphism /: Y —t X is defined, together with the intersection number KxC withevery curve C C X (obtained by evaluating Kx £ H 2 against the class [C] £H 2 (X,Q)). Note that —KxC is an integral or average value <strong>of</strong> Ricci curvature(a 2-form) calculated over a 2-cycle [C] corresponding to a holomorphic curve; wehave taken several steps back from varieties <strong>of</strong> constant curvature suggested by thecolloquial pictures in Section 1.

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