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International Congress of Mathematicians

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178 S. S. Kudlawhere Z = J2ì n ìPì f° r dosed points Pi <strong>of</strong> M with residue field fc(Fj), is an isomorphism.Let r = u + iv £ SJ2, the Siegel space <strong>of</strong> genus 2, and for T £ Sym 2 (Z), letq T = e 27rrtr ( TT ). To define the generating series4> 2 (T)= Y. 2(2» g T ,T€Sym 2 (Z)we want to define classes Z(T,v) £ CH (M) for each T £ Sym 2 (Z) and v £Sym 2 (R) >0 .We begin by considering cycles on M which are defined by imposing pairs <strong>of</strong>endomorphisms. For T £ Sym 2 (Z) >0 a positive definite integral symmetric matrix,let Z(T) be the moduli stack over M consisting <strong>of</strong> triples (.4, i, x) where (.4, i) is asbefore, and x = [ari,a: 2 ] £ Y(A,i) 2 is a pair <strong>of</strong> special endomorphisms with matrix<strong>of</strong> inner products Q(x) = |((x»,Xj)) = T. We call T the fundamental matrix <strong>of</strong> thetriple (A,i,x). The following result <strong>of</strong> joint work with M. Rapoport describes thecases in which Z(T) is, in fact, a 0-cycle on M.Proposition 2. ([15]) Suppose thatT £ Sym 2 (Z) >0 . (i) The cycle Z(T) is eitherempty or is supported in the set <strong>of</strong> supersingular points in a fiber M p for a uniqueprime p determined by T. In particular, Z(T)Q = 0. The prime p is determinedby the condition that T is represented by the ternary quadratic space V^ = { x £F^ | tr(ar) = 0 }, with Q^(x) = —x 2 , where F^ is the definite quaternion algebraover Q with Bf ~ B( for all primes £ ^ p. If there is no such prime, then Z(T)is empty.(ii) (T regular) Let p be as in (i). Then, if p \ D(B) or if p | F(F) but p 2 \ T,then Z(T) is a 0-cycle in M p .(in) (T irregular) Letp be as in (i). If p | F(F) andp 2 | T, then Z(T) is a union,with multiplicities, <strong>of</strong> components <strong>of</strong> A4 P , cf. [15], 176.For T £ Sym 2 (Z) >0 regular, as in (ii) <strong>of</strong> Proposition 2, we letFor T = f1Z(T,v) := Z(T) = (Z(T),0) £ Gif (M).J £ Sym 2 (Z) >0 irregular, we use the results <strong>of</strong> [15], section8 (where the quadratic form is taken with the opposite sign). We must thereforeassume that p^2, although the results <strong>of</strong> the appendix to section 11 <strong>of</strong> [18] suggestthat it should be possible to eliminate this restriction. In this case, the vertical cycleZ(T) in the fiber M p is the union <strong>of</strong> those connected components <strong>of</strong> the intersectionZ(h) XM Z(t2) where the 'fundamental matrix', [15], is equal to T. Here Z(ti)and Z(t2) are the codimension 1 cycles defined earlier. Note that, by Proposition1, they can share some vertical components. We base change to Z p and setZ(T,v) := x(Z(T), O z(tl) ® h O z(t2) ) • log(p) G R ~ CH 2 (M),

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