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474 PHILLIP A. GRIFFITHS<br />

el<br />

Z.Z *<br />

where A (Ai)<br />

e2<br />

U(2). From<br />

and<br />

we deduce that<br />

(-012<br />

-<br />

0) (dZl, e) A21(o]<br />

(de1, e)<br />

=- dA 1121 dA 1222 mod o*<br />

F*(dL) dp / tO(A, dA)<br />

and &*.<br />

where tO(A, dA) is a 2-form on U(2). The integral of tO over the fibre 7r-l(z) is a<br />

constant independent of z, and this implies (4.1).<br />

Proof #2. This is based on the Wirtinger theorem (3.14), and the analytic<br />

curve C will appear only at the very end.<br />

We begin by defining the incidence correspondence<br />

IC 2 x (1,2)<br />

to be {(z, L) z L}. The two projections<br />

2<br />

7/’1<br />

I<br />

j 7"/" 2<br />

(1, 2)<br />

have respective fibres 7/’-l(z) {lines through z}, and zr-l(L) {points on the<br />

line L}. Clearly I is a 3-dimensional complex manifold, and zr dL is a positive<br />

(2, 2) form on I. Integration over the fibres of the first projection gives<br />

(’W1):(’W dL)<br />

with the properties (a)" C, i) ( is a (1, l) form on and (ii) d) is invariant under the<br />

group of unitary motions z --) Az + b, A U(2). It follows easily that ( is a<br />

constant multiple of the standard Kfihler form<br />

Now setting B T/"I(C) and using (4.2) and r dLIB F* dL<br />

IB F* dL Ic (7rl), (F* dL)<br />

C t’ vol (C)

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