300 L. C. JEFFREY, HAMILTONIAN GROUP ACTIONS
t E t* of the moment map μ; the space Mt is a symplectic orbifold for any regular
value t ofμ.
Example 1.11. Let U(l) act diagonally on cn+l equipped with the standard sym-
plectic structure. The moment map for this action is
1 n
μ(zo, ···,Zn)= -2 2..: lz11
2
,
j=O
so the symplectic quotient μ-^1 (-~)/U(l) is complex projective space
s2n+1 /U(l) ~ <CPn.
More generally we may consider the reduced space M>-. = μ-^1 (0>-.)/G when
0 >-. is the orbit in g* through .A E g* ( coadjoint orbit) All such orbits may be
parametrized by .A E t~ where t~ is a chosen positive Weyl chamber in t*.
Example 1.12. The shifting trick. Let .A E g*. We define a symplectic structure
w^0 >- on the coadjoint orbit 0 >-. (in terms of the vector fields X#, y# generated
by the action of X, YE g) by wf >-(X# >-., y# >-.) = -.A([X, Y]) at the point .A E 0>-.
(and everywhere else on the orbit by equivariance). The moment map for the action
of G on 0 >-. with respect to this symplectic structure is the inclusion of 0 >-. in g*.
(The symplectic structure on the orbit was found by Kirillov and Kostant; see for
instance Section 7.5 of [6].)
Define a symplectic structure D on M x 0 >-. by
D=wM -w^0 >-.
Then for the moment map with respect to the induced action of G on M x 0 >-. we
have
M>-. ~ (M x 0>-.)o.
Corollary 1.13. Combining Example 1.9 with Proposition 1.6 (b) we see that for
any linear action of a group G on cpn-^1 (i.e. an action factoring through a
representation G---+ U(n)) the moment map factors as
μ=nofl
where fl : cpn-l ---+ u( n) was given in ( 1. 1) and 7f : u( n) ---+ g* is the projection
map.
In particular one often demands for a projective manifold M (i.e. a compact
complex manifold with an embedding into <e,pn-l) that the action of G extends to
a linear action on <e,pn-l. Thus moment maps for such linear actions are given by
(1.1) composed with n and with the embedding of M into cpn-^1.
1.3. The normal form theorem
There is a neighbourhood of μ-^1 (0) on which the symplectic form is given in a
standard way related to the symplectic form w 0 on Mre d (see for example sections
39-41 of [21]).