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ISBN 82-553-0586-6 September 23

THE ~ULNOR mJMBER FOR CURVES ON TORIC SURFACES

by

Jan Arthur Christophersen

;.To 6 1985

PRBPRINT SERIES - Matematisk institutt, Univ. i Oslo

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It is proved in [D] that the topological type of an isolated curve singularity on a toric surface depends only on its Newton filtra- tion. In this note we give as a corollary of Kouchnirenko's theorem

I

in

[K]

a similar formula for the Hilnor number of singularities defined by one analytic function on a normal affine two dimensional toric variety. I would like to thank James Damon for his helpful remarks.

1. The toric surface as quotient singularity

Any complex normal affine toric surface is isomorphic to cne of the type X= Spec(([A]) where A=~

n

7 2 1 ~ is a rational polyhedral cone in ~~ and ~[A] is the semigroup ring of A over ~.

(See [ 0])

Let be generated by M1

=

(m1 ~n1 )

M1 ,M

2

E2'~, gcd(milni)=l~ det(M 1 ,t-1 2 )>0 is well known that X= 2/G where

and ~={aM 1. 1 +aM !a ER }. 2 2 i + It

G is a finite cyclic group acting freely outside the origin. One way of seeing this is as fol- lows: Let G = {a 1H1+cc2 M2 JaiE!R1 O~cti <1}

n

~2 Then G is a cylic group of order d=det(M1 ,M2 ); the group addition is vector addition modulo <~11 , M2 > •

Define tvJO linear maps v11v 2 : 22 + 1 by v 1 (x) = det(x,M 2 ) 1 v2 (x)

= det(M 1 ,x). These restrict to v · G + {0,1 1 • • • 1d-1} and induce

-

i'

group isomorphisms vi: G + 2d, ~.(a) =\),(a) (mod d). r,;e have an

.l .l

action of G on c[x,y]; for aEG

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Let T = :12 ~ z2

a. x

=

e

a.y

=

e

- 2 -

-2rciv 2 (a) d

2rciv1 (a) d

X

y

be the linear transformation T(m,n) =

( n

2

-m2)

It's matrix is . Of course -n1 m1

~[T(A)] ~ 't[x,y] and one checks that

. G

[T (A ) ]

= ({:

[X, y] •

t: [A

J

=

On the other hand, given a cyclic group G ~ GL2(~£) and an action on

c2

one can easily construct a cone

2

Spec

~[crn~

2

] = ~

/G.

2. The Milnor number of a function on X

cr c= - ~2 + such that

Assume f is an analytic function f: X ~ <I! with an isolated cri- tical point at 0. We know that f has a Hilnor fibration [L], i.e. a C ""' fibration

induced by f, where radius s:>O and

o*

n (Here e denotes the

B is a

€: closed

~

o*

n regular is a punctured disc of embedding dimension of

ball in ICe with radius n in it.

X. ) If F is the typical Milnor fiber we can define

number of the curve f-l (0) at 0.

~(f) = rk H1 (F) to be the Nilnor

We are now in the following situation:

-

2

F c: I 0

is the natural

~

1t

1

wap rc: <1:2 ~ <r:2; G.

1t

F c:

x,o

<1:, 0

- -

Here f = f 0 1t and F is the t1i lnor fiber of f at the origin.

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The embedding <jl: X -+ <Ce is given by monomials in x rating ~[x,y] G . Call these generators for ~, , . . . ,~e

aeg ~ .. Then ~ = <jl o ~:

c2

+ ~e is the map ~(x,y)

=

~

and y and. put

(~ 1 (x,y), ... ,~e(x,y)). If N is any positive nuiLlber let

B I T\7

E: I L'

< E: I b.• v1. = N}.

~ ~

The C.iilnor fiber constructed from regular balls in <Ce is

gene-

diffeomorphic to the Milnor fiber using "weighted" balls of the forn B' for sui table choice of e:.

e: , N

Notice that:

1) The unit sphere in

c2

is compact so,

e 2b. e 2b.w.

I (

(x,v) 2b.

2)

l:

I<P.(x,y)l ~ =

I I

(x,y) I J. J. ~i

I

(x,y)

I ) I

J.

i=l J.

i=1

2N e

I

(x,v) I 2b.

l:

J.

=

I

(x,y) I ~i(l(x,y)l)

i=1

It follows that for appropriate e: and N, <P maps a regular ball of ~2 onto X

n

B'. This means we can assume that F =

F

/G;

e:

hence x(F)

=

(ord G) • x(F), where x is the Euler characteristic.

But since we are dealing with curves,

- -

x (

F ) = 1 - ~ ( f ) and

x (

F ) = 1 - !J. ( f) , so

!J.(f) = 1 + tdf)-1 d

Recall Kouchnirenko' s formula for the ~-1ilnor number of a plane curve at the origin. A power series g E ~ [ [x 1 ,x 2 ]] is "commode" if the

. 1 m

monomJ. a s x 1 and x2 , m, n n ~ 1, appear in g with non zero

coefficients. If m and n are the minima 1 such nuru.bers, then the

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- 4 -

Newton number v(g) is defined as 2A-m-n+l where A is the area bounded by the Newton polygon NP(g) of g. If g is not "comi:'.ocie"

then v(g) is defined by v(g) =sup v(g+Ix~) mE N l

where the sum is now taken over the variables, a power of which does not appear alone in g. The theorem then states that if g has an isolated critical point at 0 and if g is nondegenerate (see [K], page 7, for the definition) then ~(g) = v(g).

Identifying an analytic f: X + C with a power series in the

monomials of

C[A],

we can define its Newton polygon as follows. If

\ i J'

f

=

f... C . . X Y 1

(i,j)EA lJ

let

r

be the convex hull in of u{ (i, j)+cr}

where (i,j)E{(i,j) jcij:J:O}. Call f commode if the monomials m1 n.

1 m

(x y ) and m2 n2 n

(x y ) appear with non zero coefficients. If f

i~ commode then define the Newton polygon NP(f) to be the polygon given by the boundary of

r

and the rays through

..

~~.

,

Define the Newton number as

v(f)=2S-m -n+l where S is the area bounded by NP(f) and m and n are chosen minimally as above. If f is not commode, then define v(f) as in the case of plane curves above.

To make the definitions simple we will say that f is non- degenerate if f = foTI is nondegenerate.

Theorem Let f: X + ~ be an analytic function with an isolated critical point at the origin. If f is nondegenerate, then f,l(f)

=

v (f) •

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Proof. Each monomial in f is Just the image of the corresponding monomial in f by the mapping !£[A]: IC[T(A)] ~ IC[x,yJ. So ~'-JP(f) is just the image of UP(f) by

If f is commode,

m1 n1 m m n n

f=(x y ) + (x 2y 2 ) + ... , then the area bounded by NP(f)

T ( nr-12 ) = ( 0, nd) ,

Consequently

is (det T) •S = d•S. Since T(mt-11 )=(md,O),

~(f) = v(f) = 2Sd- rod- nd + 1

~

( f ) = 1 +

~

( f ) - 1

=

2S - m - n+ l = v ( f) d

The same argument obviously holds in the non-commode case. 0

References

[D] James Damon: "Newton filtrations, monomial algebras and non- isolated and equivariant singularities". In Singularities, AMS Proc. of Symp. in Pure Math. Vol. 40, (1981 ), 267-276.

[K] Kouchnirenko, A.G.: "Polyedres de NevJton et nombres de t-1il- nor", Inv. Math 32, 1-32 (1976).

[6] L~, D.T.: "Some Remark on Relative Honodrony" in Real and Com- plex singularities, Oslo 1976, P. Holm (ed.), Sifthoff & Nord- hoff, Alphen aan den Rijn (1977), 397-403.

[o]

Oda, T.: Lectures on Torus Embeddings and Applications, Tata Inst., Bombay (1978).

University of Oslo Inst. of Mathematics P.B. 1053, Blindern 0316 Oslo 3

NOR hAY

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