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Using Bott's "Vanishing Theorem" one can, in a certain sense invert the preceding result obtaining

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(1)

- 2 -

one hM

P(iJ.)=O

![ -.(

Using Bott's "Vanishing Theorem" one can, in a certain sense invert the preceding result obtaining

THEOREM B

Le.t M be a iUemamu.an

~moo.th

oiUen.tab.te marù6o.td oli d..ùnen6-<-on

11.

.the bund.te Q.

=

TM/E.

.( (

q.=n-n . .

( .(

and

E. c nl and tu

.(

q. t'k.th

.(

PhIQ.)p lE.) = O

.( ~ { Vh.~ > J

and h+.'=1[

In order to glve a self-contained presentation we recall the necessary preliminaries.

l. Preliminaries

Let M be a smooth (paracompact) manifold and let E be a vector mq-bun dle on M. As is well known, the total (real) Pontrjagin class

is defined by

p(E) of E

where

lS

the curvature of an arbitrary connection on E and p (E)EH 4r (M;IR)

r

(2)

- 3 -

'*

where H (M; ffi) is the de Rham cohomo1ogy ring of Mo the r-the Pontrjagin c1ass of Eo

P (E)

r i s ca 11 ed

C1ear1y p (E) = O for 4r > n if n = dim Mo Moreover if E

1S

an onen r

ted bund1e of even dimension q, then the c1ass p (E), which

1S

l oca lly

q/2

represented by the c10sed form (21T)-q det n, equa1s the square of the Eu1er c1ass; this 1atter is strict1y connected with the Euler-Poincaré cha racteristic of the manifo1d under consideration, if E - TMo

If E 15 the tangent bund1e TM, then the c1asses are also cal1ed Pon- trjagin c1ass of M and are often denoted by P (M)o

r

Let n is the curvature form of a connection on the principal fibre bundle of orthonorma1 frames, then the explicit expression of Pontrjagin classes is give by(1)

( 1. l )

where

P (TM) r

(1.2) l: 6(i. ooo,i ;j • oo.j )n . . 1\0' 0/\ n. .

(i) 1 5 ] 5 J]J2 J5-] Js

s is an even integer and 6(i

1 ,. 00 ,i

s ; jl'o o. ,js) is the genera1ysed Kronecker symbo1o

For n even, the n-form

(1.3) c.

l • • • l

." n. .

l l

] n ] 2

o • •

"n,

l

n-l

, l

n

cal1ed Gauss curvature form of M, is a representative of the Euler class of

- - - -

I)See JoA. Thorpe l6J

(3)

- 4 -

TM and if M is compact and orientable, the Gauss-Bonnet theorem says that

f f~ n(n) = x(M)

M

where X(M) is the Eu1er-Poincaré characteristic of M and f:M

-> "-

G (M)

n

15

an orientation of M,

n-p1anes tangent to M.

2. A vanishing theorem

"-

G (M)

n being the Grassmann bund1e of the oriented

We can now prove the fo 11 owi ng theorem ([3J)

(2. l). Theorem

admU.6 k c.omptemerttalty (òmooth) fu .tJUbu.V.o

nI.>

(~

: l, ... ,k). Then the

~eat Po~ja9~n

c.laJ.>òeJ.>

Proof.

06

o~ented

p (M) Me

iL

n .- pfuneJ.>

.(,

nute 60iL 2iL>max(n

1 , •. ,n k )

'"

Let E be the principa1 fibre bund1e of the orthonorma1 frames (associated

"-

to the tangent). Its structura1 group

15

G - SO(n) (the rotation group). We

""

reca11 that the Lie algebra ~ of SO(n) can be identified with space of the skew-symmetric matrices of order n.

"-

Let us consider the subbund1e E of E formed of the frames "adapted"

to the distributions, viz. the orthogona1 frames vectors

le. }(i=l, ... ,n)

l

so that the

{e }

a. J

a - n +... +n . +l , ... , n +... +n .

J l J-l l J

form a basis for T J . The bund1e E can be regarded as having structura1 group

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