CHAPTER Ⅱ

CHAPTER Ⅱ
A. On the Geometry of Lie Groups
A.1.
note
(i) follows from Ad ( x)tX  x exp tXx 1  L( x) R( x 1 ) exp tX .for X  g , t  R
 ( x exp tX )  exp(tX ) x
1
For (ii) we
, so d  x (dL( x)e X )  dR( X 1 ) e X . For (iii) we observe for
X 0 , Y0  g
  g exp tX 0 , h exp sY0   g exp tX 0h exp sY0
 gh exp tAd (h 1 ) X 0 exp sY0 ,
(Continued on next page)
Exercises, ChapterⅡ
Solutions
so
d  (dL( f ) X 0 dL(h)Y0 )  dL( gh)( Ad (h 1 ) X 0  Y0 ) .
Putting X  dL( g ) X 0 , Y  dL(h)Y0 , the result follows from (i).
A.2. Suppose
 (t1 )   (t2 ) so  (t2  t1 )  e . Let L>0 be the smallest number such that  ( L)  e .
Then  (t  L)   (t ) ( L)   (t ). If
T
L denotes the translation t→t+L, we have
A.3. The curve σ satisfies  (t  L)   (t ), , so as in A.2,

T
L   ,so
.
A.4 Let (pn) be a Cauchy sequence in G/H. Then if d denotes the distance, d ( pn , pm )  0 , if
m, n   . Let B (o) be a relatively compact ball of radius ∈ >0 around the origin o = {H} in G/H.
1
Select N such that d(pN, pm) < ∈ for m ≥ N and select g ∈ G such that g • pN = o. Then ( g • pm) is a
2

Cauchy sequence inside the compact ball B (o) , hence it, together with the original sequence, is
convergent.
A.5. For X∈g, let
denote the corresponding left invariant vector field on G. From Prop. 1.4 we
for all Z ∈g. But by (2), §9 in Chapter Ⅰthis condition reduces
know that (i) is equivalent to
to
which is clearly equivalent to (ii). Next (iii) follows from (ii) by replacing X by X+Z. But (iii) is equivalent to
Ad(G)-invariance
  R( g
1
)

of
B
so
Q
is
right
invariant.
Finally,
the
map
: x  x
1
satisfies
L( g 1 ) , so d  g  dR( g 1 )e d  e dL( g 1 ) . Since d  e is automatically an isometry,
g
(v) follows.
1
2
A.6. Assuming first the existence of ▽, consider the affine transformation  : g  exp Yg
G which fixes the point exp
1
exp Y
2
1
exp Y of
2
1
Y and maps γ1, the first half of γ, onto the second half, γ2. Since
2
1
1
L( exp  Y ),

2
2
  I . Let X  (t )  Gexp tY (0  t  1) be the family of vectors parallel with respect to
  L(exp Y )
We have d
1
Exercises, ChapterⅡ
Solutions
 such that X  (0)  X . Then σ maps X*(s) along γ1 into a parallel field along γ2 which must be the
1
2
1
2
field  X  (t ) because d ( X  ( ))   X  ( ). . Thus the map σ ○ ∫ = L(exp
1
1
Y) R(exp Y)
2
2
sends X into X*(1), as stated in part (i). Part (ii) now follows from Theorem 7.1, Chapter Ⅰ, and part (iii)
from Prop. 1.4. Now (iv) follows from (ii) and the definition of T and R.
Finally,
we
prove
the
existence
of
▽ .
As
remarked
before
Prop.
1.4,
the
defined uniquely a left invariant affine connection
Since
equation
▽ on G.
, we get
~
this we generalize to any vector fields Z, Z’ by writing them in terms of X i (l≤i≤n). Next
(1)
.
Since both sides are right invariant vector fields, it suffices to verify the equation at e. Now
 X  X
where
X is right invariant, so the problem is to prove
For a basis X1, ... , Xn of g we write Ad(g
, it follows that
Chapter Ⅰ,§4,
Since ( Xfi )(e) = {(d/dt) f1 (exp tX)}t=0 and since
—
1
) Y, it follows that
Since
, so using ▽2 and Lemma 4.2. from
Exercises, ChapterⅡ
Solutions
d
{ Ad(exp(—tX))(Y)}t=0= —[X, Y].
dt
1
the expression on the right reduces to —[X, Y] + [X,Y], so (1) follows.
2
As before, (1) generalizes to any vector fields Z, Z’.
The connection ▽ is the 0- connection of Cartan- Schouten [1].
B. The Exponential Mapping
B.1. At the end of §1 it was shown that GL(2, R) has Lie algebra gl (2, R), the Lie algebra of all 2×2 real
matrices. Since det ( etx ) = et Tr ( X ), Prop. 2.7 shows that sI(2, R) consists of all 2×2 real matrices of trace 0.
Writing
1 0   0 1  0 0  a b 
X  a
  b
  c


 0 1  0 0   1 0   c a 
a direct computation gives for the Killing form
B( X , X )  8(a 2  bc)  4Tr ( XX ) ,
Where B( X , Y )  4Tr ( XY ) , and semisimplicity follows quickly.
Part (i) is obtained by direct computation. For (ii) we consider the equation
 0 
eX  
1 
0  
(λ∈R, λ≠1).
Case 1: λ>0. Then det X <0. In fact det X=0 implies
 0 
,
I  X 
1 
0  
So b=c=0, so a=0, contradicting λ≠1. If det X>0, we deduce quickly from (i) that b=c=0, so det X=-
a2, which is a contradiction. Thus det X<0 and using (i) again we find the only solution
0 
 log 
X 
.
 log  
 0
1
Case 2: λ=-1. For det X >0 put   (det X ) 2 . Then using (i) the equation amounts to
cos   ( 1 sin  )a  1,
(  1 s i n b)
0,
cos   ( 1 sin  )a  1,
(  1 s i n c )
0.
These equations are satisfied for
  (2n  1)
(n  Z ) ,
d e tX  a2  b c  ( 2n  21) 2
.
This gives infinitely many choices for X as claimed.
Case 3: 
0,   1. If det X =0, then (i) shows b=c=0, so a=0; impossible. If det X>0 and we put
Exercises, ChapterⅡ
Solutions
1
  (det X ) 2 , (i) implies
cos   (  1 sin  )a   ,
(  1 s i n b)
cos   ( 1 sin  )a   1 ,
0,
(  1 s i n c )
0.
Since    , we have sin   0 . Thus b=c=0, so det X  a , which is impossible. If det X<0, and
1
2
we put   ( det X )
1
2
, we get from (i) the equations above with sin and cos replaced by sinh and cosh.
Again b=c=0, so det X  a 2    2 ; thus a    , so
cosh   sinh    ,
c o s h
s i nh 1
,
Contradicting λ<0. Thus there is no solution in this caase, as stated.
B.2. The Killing form on sl(2,R) provides a bi-invariant pseudo-Riemannian structure with the properties of
Exercise A.5. Thus (i) follows from Exercise B.1. Each gwhere g  SL(2, R) can be written g=kp where
k  SO(2) and p is positive definite. Clearly K= exp T where T  s l (2, R) ; and using diagonalization, p=
exp X where X  s l (2, R) . The formula g  exp T exp X proves (ii).
B.3.Follow the hint.
B.4. Considering one-parameter subgroups it is clear that g consists of the matrices
0

c
X (a, b, c)  
0

0
c 0 a

0 0 b
0 0 c

0 0 0
(a , b , c R.)
Then [ X (a, b, c), X (a1 , b1 , c1 )]  X (cb1  c1b, c1a  ca1 ,0), so g is readily seen to be solvable. A direct
computation gives
 cos c sin c

 sin c cos c
exp X (a, b, c)  
 0
0

0
 0
0 c 1 ( a sin c  b cos c  b) 

0 c 1 (b sin c  a cos c  a ) 
.

1
c

0
1

Thus exp X (a, b, 2 ) is the same point in G for all a,b∈R, so exp is not injective. Similarly, the points in G
with   n 2 ( n  Z )
2  2
0 are not in the range of exp. This example ocurs in Auslander and
MacKenzie [1]; the exponential mapping for a solvable group is systematically investigated in Dixmier [2].
B.5. Let N0 be a bounded star-shaped open neighborhood of 0∈g which exp maps diffeomorphically onto an
Exercises, ChapterⅡ
Solutions
1
2
open neighborhood Ne of e in G. Let N  exp( N 0 ) . Suppose S is a subgroup of G contained in N*, and let
*
1
1
s  e in S. Then s  exp X ( X  N 0 ) . Let k  Z  be such that X , 2 X ,..., kX  N 0 but
2
2
1
( k  1) X  N 0 . Since N0 is star-shaped, (k  1) X  N 0 ; but since s k 1  N * , we have
2
1
1
S k 1  exp Y Y  N 0 . Since exp is one-to-one on N0, (k  1) X  Y  N 0 which is a contradiction.
2
2
C. Subgroups and Transformation Groups
C.1. The proofs given in Chapter X for SU*(2n) and Sp(n,C) generalize easily to the other subgroups.
C.2. Let G be a commutative connected Lie group,
during the proof of Theorem 1.11,
its universal covering group. By facts stated
p
is topologically isomorphic to a Euclidean group R . Thus G is
p
topologically isomorphic to a factor group of R and by a well-known theorem on topologically isomorphic to
R n  T m . Thus by Theorem 2.6, G is analytically isomorphic to R n  T m .
For the last statement let  be the closure of  in H. By the first statement and Theorem 2.3,
  R n  T m for some n, m  Z  . But γ is dense in  , so either n=1 and m=0 (γ closed) or n=0 (  compact).
C.3. By Theorem 2.6, is analytic and by Lemma 1.12, dI is injective. Q.E.D.
C.4. The mapping  g turns g N0 into a manifold which we denote by ( g N 0 ) x . Similarly,
turns
 g
g  N0 into a manifold ( g  N 0 ) y . Thus we have two manifolds ( g N0  g  N0 ) x and
( g N 0  g  N 0 ) y and must show that the identity map from one to the other is analytic. Consider the analytic
section maps
 g : ( g N 0 ) x  G,
 g  : ( g  N0 ) y  G
defined by
 g ( g exp( x1 X 1  ...  x X  ) p0 )  g exp( x1 X 1  ...  x X  ),
 g ( g  exp( y1 X 1  ...  y X  ) p0 )  g  exp( y1 X 1  ...  y X  ),
and the analytic map

g
:  1 (g N 0 )  ( g N 0 ) x  H
given by

g
( z )  ( ( Z ),[ g ( ( Z ))]1 z ).
Furthermore, let P : ( g N0 ) x  H  ( g N0 ) x  H denote the projection on the first component. Then the
identity mapping
Exercises, ChapterⅡ
Solutions
I : ( g N0  g  N0 ) y  ( g N0  g  N0 ) x
can be factored:
P
g
 ( g N )  H 
( g N0  g  N0 ) y 
 1 ( g N0 ) 
( g N0 ) x
0 x

g
↑ See Some details. P. 586.
In fact if p  g N0  g  N0 , we have
p  g exp( x1 X 1  ...  x X  ) p0  g  exp( y1 X 1  ...  y X  ) p0 ,
So for some h  H ,
P(  g ( g  ( p)))  P(  g ( g  exp( y1 X 1  ...  y X  )))
 P( ( g  exp( y1 X 1  ...  y X  )), h)
 P( ( g exp( x1 X 1  ...  x X  )), h)
 P exp( x1 X 1  ...  x X  )) p0 .
Thus I is composed of analytic maos so is analytic, as desired.
C.5. The subgroup H  G p of G leaving p fixed is closed, so G / H is a manifold. The map
I : G / H  M given by I ( gH )  g p gives a bijection of G / H onto the orbit G p .Carring the
differentiable structure over on G p by means of I , it remains to prove that I : G / H  M is everywhere
regular. Consider the maps on the diagram.
G
β

G/H
I
where  ( g )  gH ,  ( g )  g p so   I  . If we restrict
M
 to a local cross section, we can write
I    1 on a neighborhood of the origin in G / H . Thus I is C  near the origin, hence everywhere.
Moreover, the map d  e : g  M p has kernel
, the Lie algebra of H (cf. proof of Prop. 4.3). Since
Exercises, ChapterⅡ
Solutions
d e  dI H d e , wee that dI H is one-to-one. Finally, If T ( g ) denotes the diffeomorphism m  g m of
M , we have I  T ( g ) I  ( g 1 ) , whence
dI gH  dT ( g ) dI H d ( g 1 ) gH ,
so I is everywhere regular.
C.6. By local connectedness each component of G is open. It acquires an analytic structure from that of G 0
by left translation. In order to show the map
 : ( x, y)  xy 1 analytic at a point ( x0 , y0 )  G  G let G1
and G2 denote the components of G containing x0 and y0 , respectively. If
0   G0  G0 and
   G1  G2 then
  L( x0 y01 ) I ( y0 ) L( x01 , y01 ),
1
where I ( y0 )( x)  y0 xy0 ( x  G0 ) . Now I ( y0 ) is a continuous autoorphism of the Lie group G0 , hence
by Theorem 2.6, analytic; so the expression for  shows that it is analytic.
C.8. If N with the indicated properties exists we may, by translation, assume it passes through the origin
o  H  in M. Let L be the subgroup
g  G : g
N  N . If g  G maps o into N , then gN  N   ;
1
so by assumption, gN  N . Thus L   ( N ) where
 : G  G / H is the natural map. Using theorem 15.5,
Chapter Ⅰwe see that L can be given the structure of a submanifold of G with a countable basis and by the
transitivity of G on M, L o  N . By C.7., has the desired property. For the converse, define N  L o and use
Prop. 4.4 or Exercise C.5. Clearly, if gN  N   , then g  L , so gN  N .
For more information on the primitivity notion which goes back to Lie see e.g. Golubitsky [1].
D. Closed Subgroups
2
D.1. R T is a torus (Exercise C.2), so it suffices to take a line through 0 in R2 whose image in the torus is
dense.
D.2. g has an Int(g)-invariant positive definite quardratic form Q. The proof of Prop. 6.6 now shows
g    g '(  center of g, g’=[g,g] compact and semisimple). The groups Int(g) and Int(g’) are analytic
subgroups of GL(g) with the same Lie algebra so coincide.
D.3 We have
 1 (c1 , c2 , s)  (c1 , e 2 i 3c2 , s)
0,
3
(a1 , a2 , r )(c1 , c2 , s)(a1 , a2 , r ) 1
 (a1 ( 1 e2 i s ) c1 e2 i r , a2 ( 1 2e
ihs
) 2c 2e
ihr
,s )
Exercises, ChapterⅡ
So 
0,
1
3
is not an inner automorphism, and A
0,
sequence (nk )  Z such that hnk 
1
3
Solutions
 Int ( g ). Now let Sn  0 and let tn  hsn  hn . Select a
1
(mod 1) (Kronecker’s theorem), and let
3
T
k be the unique point in
T
[0,1) such that tn  k  Z . Putting sk  sn , tk tn , we have
k
k
k
s t   T   1
k k
sk k
0,
3
1 0
 , c  C ,   1.
c a
Note: G is a subgroup of H  H where H  
E. Invariant Differential Forms
is torsiion free; and by (5), §7, Chapter Ⅰ,
E.1. The affine connection on G given by
 is a left invariant 1-form,
if
for all left invariant forms  . Now use Exercise C.4. in Chapter Ⅰ.
so
t
t
t
E.2. The first relation is proved as (4), §7. For the other we have g g  I , so (dg ) g  g (dg )  0 .
Hence ( g
1dg )  t (dg )( t g )1  0 and .   t   0
For U(n) we find similarly for   g
1dg ,
d      0,
  t  0 .
For Sp(n)  U (2n) we recall that g  Sp ( n) if and only if
gt g  I
(cf. Chapter Ⅹ). Then the form   g
2n
,
g t g   .
n
n
1dg statisfies
d      0,
  t  0
  n   n t   0.
E.3. A direct computation gives
 0 dx dz  xdy 


g dg   0 0
dy 
0 0
0 

1
and the result follows.