MORSE THEORY J . Milnor B Y Based on lecture notes by M. SPIVAK a nd R. WELLS PRINCETON, NEW JERSEY PRINCETON UNIVERSITY PRESS 1963
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M O R S E T H E O R Y
J. Milnor
BY
Based on lecture notes by
M. SPIVAK and R. WELLS
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Copyright 1963. by Princeton University Press
All Rights ReservedL. C. Card 63-13729
Printed in the United States of America
CONTENTS
I.
SMOOTH FUNCTIONS ON A MANIFOLD$ 1 . Introduction . . . . . . . . . . . . . . . . . . . . . . .
. Definit ions and Lemmas. . . . . . . . . . . . . . . . . .
$3 . Homotopy Type i n Terms of C ri ti ca l Values . . . . . . . .
$4 . Examples . . . . . . . . . . . . . . . . . . . . . . . . .
$5 . The Morse Inequali t ies. . . . . . . . . . . . . . . . . .
. Manifolds i n Euclidean Space: The Existence of
Non -degenerate Functions . . . . . . . . . . . . . . . . .
$7 . The Theorem on Hyperplane Sections . . . . . . .
PART . A COURSE I N
. Covariant Differentiat ion . . . . . . . . . . . . .
$ 9. The Curvature Tensor . . . . . . . . . . . . . . . .. Geodesics and Completeness . . . . . . . . . . . . .
. THE OF VARIATIONS APPLIED TO GEODESICS
.
§1 2 .
.$14 .
.
§1 6 ..
.
.
The Path Space of a Smooth Mani fold . . . . . . . . . . .
The Energy of a Path. . . . . . . . . . . . . . . . . . .
The Hessian of the Energy Function at a C r i t i c a l P a th . .
Jacobi Fie lds : The Null-space of . . . . . . . . . .
The Index Theorem . . . . . . . . . . . . . . . . . . . .A Fi ni te Dimensional Approximation t o . . . . . . . .
The Topology of the Path Space . . . . . . . . . . .of Non-conjugate Points . . . . . . . . . . . .
1
4
1 2
2 8
43
55
67
70
74
a3
93
Some Relations Between Topology and Curvature . . . . . . lo o
V
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CONTENTS
APPLICATIONS TO LIE GROUPS SPACES
. . . . . . . . . . . . . . . . . . . .$20. Symmetric Spaces
$ 2 1 . Lie Groups as Symmetric Spaces 1 1 2
Whole Manifolds of Minimal Geodesics 118
1 2 4
. . . . . . . . . . . . .
. . . . . . . . . .
$23 . The Periodicity Theorem for the Unitary Group . . .$24 . The Theorem for the Orthogonal Group . . . .
THE TYPE OF A UNION
v i
. . . . . . . . 14 9PART I
NON-DEGENERATE SMOOTH FUNCTIONS ON A MANIFOLD.
$ 1 . Introduction.
I n this sect ion we w i l l i l l u s t r a t e by a s p e c i f i c t h e s i t u -
a t i o n that we w i l l i n v e s t i g a t e l a t e r for arb i t r a ry m an ifo lds .
s i d e r a to rus M, tangent to the plane V, as ind ica ted in Diagram 1 .
Let us con-
Diagram
Let f : always denotes the r e al numbers) be the he ight
above the V plane, and let be the se t of a l l po in t s x M such that
a. Then the fol lowing are t rue :
then i s vacuous.
then i s homeomorphic t o a 2-cell .
(3 ) I f < a < then i s homeomorphic t o a cylinder :
a < then t o a compact
manifold of genus one having c i r c l e as boundary:
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DEFINITIONS LEMMASI . NON-DEGENERATE FUNCTIONS
completes the induction; and proves 2 . 2 .
Non-degenerate a re i so l a t ed .2 .3
Examples of degenerate cri ti ca l poin ts (f or on
are given below, together with pictur es of t he ir graphs.
7
9
are degenerate, i s the x axis, which i s a sub -manifold of
= The set of c r i t i c a l p o i n t s , a l l of which
(a) The or ig in ( b) .i s a d eg en e ra t e c r i t i c a l The origin i s a degenerate, and
no n- i so la t ed, c r i t i c a l p o i n t .
degenerate , consists of the of the x and axis, which i s
not even a sub-manifold of
We conclude this sect ion wi th a discussion of 1-parameter groups of
The set o f c r i t i c a l p o i n ts , a l l of which are
e n t i a l for more det a i l s .
The reader i s re fe r red t o K. Groups and Differ-
A group of of a manifold M i s a
- R e a l p a r t o f
( 0 .0 )
(x +
i s a d egen era te c r i t i c a l p o i n t (a "monkey saddle").
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30I. NON-DEGENERATE FUNCTIONS
rank h rank A - rank i
rank A - rank B + rank j
rank A - rank B + rank C - rank k
...rank A - rank B rank C - rank D .
the last express ion i sa t r i p l e X Y
0.
Now consider the homoiogy exact
Applying this computation t o th e homomorphism
we s ee that
rank - - + .. .
Collecting terms, this means that
which completes the
Applying this subaddit ive function to the s pacesa
C C M
we ob ta in the Morse ineq ua l i t i e s
or
- (M ) . C, +
T hese ine qua l i t i e s a r e de f in i t e ly s harper than the p rev ious ones.
I n f a c t , a d di n g (4 , ) and one obtains and comparingw i th f o r > n one obtains the equali ty ( 3 ) .
A s an i l l u s t r a t i o n of t h e u se of the Morse inequali t ies , suppose
that Then must be zero. Comparing the in eq ua li ti es
and we see that
- C, - C, .
Now suppose that i s al so zero. Then 0, arid a argu-
ment shows th a t
- R, - .
MORSE INEQUALITIES
Subtracting this from t h e e q u a l i t y above we ob ta in the fo l lowing :
5 . 4 . If = = 0 then C, and
= =
( O f course this would a l s o follow from Theorem 3 . 5 . )
Note thatthis corollary enables u s to fin d the homology of complex projective
space (see without use of Theorem 3.5 .
31
.
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46 RIEMANNIAN GEOMETRY
Now suppose t h a t M i s provided w i t h an af f ine connection . ThenDV
v e c t o r f i e l d V along c determines a new vector f i e l d a long c
the c o v a r i a n t d e r iv a t i v e of V. The operation
DV
character ized by the fo l lowing three axioms.
DV DW=
If i s a smooth real valued funct ion on R then
DV.
at
c ) If V i s induced by a v e c t o r f i e l d Y on M , that i s if dc
for each t , then i s e q u a l t o Y=
t h e c o v a r i a n t d e r iv a t i v e o f
v e lo c i t y v e c to r o f
Y i n t h e d i r e c t i o n o f t h e
DVV -0 . 1 .
w h i c h s a t i s f i e s these three c o n d i t i o n s .
There i s one and only one operation
PROOF: Choose a loca l coord inate system for M, a nd l e t
. denote the coord inate s of th e po in t The vector
f i e l d V can be expressed un iquely i n the fo rm
where
su b se t of R), and are t h e s t a n d a r d v e c to r f i e l d s o n t h e c o-
ordinate neighborhood. It follows from ( a ) , an d
,. . . are real valued funct ions on R (oran appropr ia te open
Converse ly , def in ing
that c o n d i t i o n s ( a ) , (b), and (c) are s a t i s f i e d .
by this formula, i t i s n o t d i f f i c u l t v e r i f y
A v e c t o r f i e l d V a lo n g c i s s a i d t o b e a p a r a l l e l v e c to r f i e l d
DVi f the c o v a r i a n t d e r iv a t i v e i s i d e n t i c a l l y z e r o .
a
8. COVARIANT DIFFERENTIATION 4 7
LEMMA Given a curve c and a t a n g e nt v e c t o r
a t t h e p o in t
v e c t o r f i e l d V alon g c which extends
t h e r e i s one and only one parallel
PROOF. The di ff er en ti al equati ons
have so lu t ions
a l l r e l e v a n t v a lu e s of t .
Real Va r i a b l e s ," p .
which are uniquely determined by the i n i t i a l v a lu es
Since these equat ions are l i n e a r , t h e so lu t i o n s c a n b e d ef in e d for
(Compare Graves, "The Theory of Funct ions of
The vector i s sa i d t o be ob ta ined f rom b y p a r a l l e l t r a n s-
l a t i o n a l on g c .
Now suppose that M i s a Riemannian manif old. The inner product
of two vectors w i l l be denoted by .
DEFINITION. A connection on M i s compatible with the Rieman-
n ia n m e t r i c i f p a r a l l e l t r a n s l a t i o n p r e se r ve s i n n e r p r o d u c t s . I n o th e r wor ds ,
fo r any parametrized curve c and any pa ir P, of' p a r a l l e l v e c t o r f i e l d s
a long c , the inner p roduct should be constan t .
LEMMA 8 . 3 . Suppose that the connect ion i s compat ib le wi th
the m e t r i c . L e t V, W b e an y two v e c to r f i e l d s a lo n g c .
Then
PROOF: Choose pa ra ll el vector f i el ds along c which
are orthonormal a t one po in t of c and hence a t every po in t of c. Then
t h e g i v en f i e l d s V an d W be expressed as and respec-
t i v e l y (where = i s a real valued funct ion on . It f o l -
lows that = a n d t h a t
or e
which the proof .
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1 1 6 APPLICATIONS$2 1 . LI E GROUPS 11 7
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some (See Chevalley, of Lie Groups.")
proof.
T h i s completes the
THEOREM 21 .7 ( B o t t ) . L e t G be a compact, simply con-
nected Lie group. Then the loop space has the
homotopy type of a with no odd dimensional
c e l l s , and with only f in i t el y many for each
even value of
Thus the X-th homology groups of i s zero fo r A odd, i s
f r ee abe l i an of f in i t e r ank for X even.
REMARK 1 . T h i s CW-complex w i l l always be inf ini te dimensional . A s
example, i f G i s the group of u n i t quate rnions , then we have seen
that the homology group i s i n f i n i t e c y c l ic a l l even va lues of
REMARK 2. Th i s theorem remains t r u e even for a non-compact group.
In f ac t any connected Lie group cont ains a compact subgroup as deformation
r e t r a c t . ( S e e K. Iwasawa, On some typ es of topological A n n a l s of
Mathematics 50 Theorem 6. )
we have
Ad =
- (Ad (A d .
The li ne ar trans forma tion Ad V i s skew-symmetric; that i s
< Ad > - < > .
This fol lows immediately f rom the identi ty Therefore we can choose
an or thonormal bas is for G so that the m at r ix of Ad V takes the form
PROOF of Choose two poi nt s p and q i n G which are not
conj ugat e alon g any geod esic . By Theorem 17.3 , has the homotopy
type of a with one ce ll of dimension A for each geodes ic f rom
p t o q of index X . By ther e are only f i ni te ly many A-cells for
each Thus i t only remains t o prove that the index X of a geodesic is
always even.
Consider a geodes ic 7 s t a r t i n g a t p w i th ve loc i ty vec to r
vP
According to 6 2 0 . 5 the conjugate points of p on are determined by the
eigenvalues of the l inea r t r ans fo rm at ion
def ined by
.
Defining the homomorphism
Ad V:
It fol lows that the
matr ix
. .
composite li ne ar trans forma tion (Ad (Ad V) ha s
Therefore the non-zero eigenvalues of
occu r i n pa i r s .
- are pos i t ive , and
It follows from 20.5 that the conjugate points of p along a l s o
In ot her words every conjugate point has even m ul t ip l i c i ty .occu r in pa i r s .
Together with the Index Theorem, this implies that the index X of an y
geodesic from p t o q i s even. Th i s completes the proof.
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1 2 2 APPLICATIONS 2 2 . MANIFOLDS OF MINIMAL GEODESICS
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( 2 ) The index of g a t each c r i t i c a l po in t wh ich l i e s i n the com-
p a c t s e t i s
It follows from 2 2 . 4 that any g which approxim ates
s u f f i c ien t l y c los e ly , the f i r s t and s econd der iva t ives a l s o be ing approx i-
mated, w i l l s a t i s f y ( 2 ) . In fa ct the compact se t can be
covered by fi ni te ly many compact s e t
nate neighborhood.
each of which l ies i n a coordi-
22.4 can then be applied to eachThe function i sThe proof of 22.5 now proceeds as fol lows.
smooth on the compact region
po in t s a r e non-degenerate, with index Hence the manifold
has the homotopy type of w i t h c e l l s of dimension
attached.
c and c r i t i c a l
Now cons ider t he map
0 h: C .
Since < it follows that h i s homotopic within t o
0 h ’ : .
But this l a s t p a i r i s contained in and U can be deformed in to
w i th in M. It fo l low s tha t i s homotopic within t o a map
h ” : - T h i s completes the proof of 2 2 . 5 .
The original theorem, 2 2 . 1 , now can be proved as fol lows. Clear ly
it i s s u f f i c i e n t t o p ro ve t h a t
o
f o r a r b i t r a r i l y l a r g e v a l u e s of c . A s i n the space I nt contains
a smooth manifold In t . . as deformation re tr ac t. The space
of minimal geodesics i s contained i n this smooth manifold.
The energy function E: w hen r es t r i c ted to
I n t a lmos t s a t i s f i e s the hypo thes is of 22.5. The only
d i f f i c u l t y i s t h a t ranges over the int erv al d E < c , in s tead of
the r equ i r ed in te rva l To c o r r e c t this, l e t
F:
be any
Then
F R
s a t i s f i e s the hypo thes i s of 22.5. Hence
d
< Th i s completes the proof.
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7/31/2019 Milnor J. Morse Theory (Princeton, 1963)
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7/31/2019 Milnor J. Morse Theory (Princeton, 1963)
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7/31/2019 Milnor J. Morse Theory (Princeton, 1963)
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7/31/2019 Milnor J. Morse Theory (Princeton, 1963)
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7/31/2019 Milnor J. Morse Theory (Princeton, 1963)
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