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 nh 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 y01 ) I ( y0 ) L( x01 , y01 ),
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 2e
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.
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