C OMPOSITIO M ATHEMATICA
S TEFAN P ETERS
Convergence of riemannian manifolds
Compositio Mathematica, tome 62, n
o1 (1987), p. 3-16
<http://www.numdam.org/item?id=CM_1987__62_1_3_0>
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Convergence of Riemannian manifolds
STEFAN PETERS
Institut fur Mathematik, Universitiit Dortmund, Postfach 500 500, 4600 Dortmund 50, FRG
Received 27 August 1985
1. Introduction
In this paper we consider sequences of
compact
n-dimensional Riemannian manifolds. We aregoing
tostudy
the convergence of such sequences and theproperties
ofpossible
limit spaces. Inparticular,
we shallinvestigate
underwhich
assumptions
the limit spaceagain
carries the structure of a manifold of the same dimension.The
concept
of convergence of Riemannian manifolds was introducedby
M. Gromov
(see [7]).
We shall recall theprecise
definitions inChapter
3. Butlet us first consider a few
examples.
l.1
Example:
Take a sequence of smoothed truncated cones inR3, converging
to a cone. We observe that a
singularity
arises in thelimit,
due to the fact that the curvature does notstay
bounded.Let us therefore restrict our attention to sequences with bounded sectional
curvatures |KM| 2.
We also assume bounded diametersdiam(M) d,
otherwise thecompactness
is lost in the limit.1.2
Example:
Take a sequence of two-dimensional flat toribecoming
thinnerand
thinner, eventually collapsing
toS 1.
Here theassumptions
on the curva-ture
( = 0)
and the diameter aresatisfied,
but the limit space is of lower dimension. Thisphenomenon
ofcollapsing
is not asubject
of this paper, see e.g.[7],
or[11].
It can be ruled outby
a lower bound on the volumes of the manifolds.1.3
Definition:
LetTZ (n, d, A, V)
denote the class ofcompact
n-dimensional Riemannian manifolds M with diameterdiam(M) d,
volumevol(M) V,
and sectional
curvature |KM| A2.
l. 4 Remark: The
hypothesis vol(M)
V can bereplaced by i(M) i0,
wherei(M)
denotes theinjectivity
radius of M.(See
e.g.[14]).
Martinus Nijhoff Publishers, Dordrecht - Printed in the Netherlands
1.5. THEOREM:
Cheeger’s
Finiteness Theorem([5], [12]):
9N containsonly a finite
numberof diffeomorphism
classes. This number can be estimatedexplicitly
in terms
of n, d, A,
V.We now turn to the results on
compactness.
In[7],
thm.8.28,
M. Gromovstated the
following
theorem.(For
the definition of theLipschitz topology,
seeChapter
3 of thesenotes).
1.6. THEOREM: Gromov’s
Compactness
Theorem: Withrespect to
theLipschitz topology, 9X (n, d, A, V) is relatively compact in a larger
classof n-dimensional manifolds, namely C1,1-manifolds
withC0-metrics.
In Gromov’s
proof
of thistheorem,
he uses as a main tool a theorem about theequivalence
of Hausdorff andLipschitz
convergence([7],
thm.8.25),
but anumber of details remained open.
Recently,
A. Katsuda[10]
succeeded towork out Gromov’s
proof
of thm. 8.25 in full detail.Katsuda’s paper is rather
long.
Inchapter
3 of this paper, we shallgive
ashorter
proof
of this theorem(Thm. 3.9).
It is very similar to the author’sproof
of
Cheeger’s
Finiteness Theorem in[12].
Thelargest part
of the work hasalready
been done in[12].
In Gromov’s version of the
Compactness
Theorem1.6,
theregularity properties
are notoptimal. However,
as we shall see mChapter 2,
theregularity
of the limit metricplays
animportant
role for theapplications
ofthe theorem. In
Chapter 4,
we aregoing
to prove thefollowing improved
version of Thm. 1.6.
1.7. THEOREM: Let 0 03B1 1. Then any
sequence in
9N contains asubsequence converging
w. r. t. theLipschitz topology to an
n-dimensionaldifferentiable
mani-fold
M wi th metric gof Hôlder
classC1+03B1.
This result is
optimal
in terms of Hôlderconditions,
i.e. the theorem does nothold for
C1,1
instead ofC1+lX.
We shall prove this inChapter
5. At least it isquite
obvious that we cannotexpect
more thanC1,l
ingeneral,
as thefollowing example
illustrates.1.8.
Example:
Put twospherical caps
onto acylinder
inR3
Theresulting compact surface,
with the inducedmetric,
canobviously
be obtained as a limit of a sequence of smooth surfaces with bounded curvatures,diameters,
andvolumes.
Nevertheless,
the metric is notC2,
otherwise the curvature wouldhave to be continuous.
Remark
After the
preparation
of this paper, the author leamed that R.E. Greene and H. Wu obtained the same result as Theorem,1.7independently. (R.E.
Greeneand H.
Wu, Lipschitz
convergence of Riemannianmanifolds, preprint).
We wish to remark that a
preliminary
version of this paper wascompleted
in
February
1985. Thispreliminary
paper did inparticular
not containchapter 5,
which consists of more recent results.2.
Applications
2. l.
"Pinching just
below1/4" (Berger [2])
For any even number n, there exists
~(n)
> 0 such that anycompact simply
connected n-dimensional Riemannian manifold M with
1/4 - ~(n) KM
1is
homeomorphic
to the standardsphere sn,
ordiffeomorphic
toPnC, PnH,
or to the
Cayley plane P2Ca.
In
Berger’s proof,
he assumes to have a sequence of metrics withpinching
constants
converging
to1/4.
Thecompactness
theorem is used toyield
a1/4-pinched
limit metric. Then a well-knownrigidity
theorem can beapplied.
The main
difficulty
is to show the smoothness of the limitmetric,
which isonly C0
apriori according
to Gromov. So we see thatregularity properties
ofthe limit metrics are crucial for the
applications
of thecompactness
theorem.Let us mention two further
applications:
2.2.
"Diameter-pinching" (Brittain [3])
There exists an e > 0
depending only
on n,max | KM|,
and apositive
numberVo,
such that ifRic(M) n - 1, vol(M) VQ,
anddiam(M)
qr - E, then Mis
diffeomorphic
to sn.2.3.
"Volume -pinching" (Katsuda [11])
Let M be an n-dimensional
compact
Riemannian manifold withRic(M) n -
1and |KM| 2.
There exists E > 0depending
on n and Asuch that
vol(M) Vol(Sn)-~ implies
that M isdiffeomorphic
to sn.3. Hausdorf f and
Lipschitz topology
Let us recall the definitions of
Lipschitz
distance and Hausdorff distance of metric spaces(see [7]).
3.1.
Definition:
LetX,
Y be metric spaces,f :
X - Y aLipschitz
map. Then dilf:= sup d(f(x), d(x,x) f(x’))
is called dilatation off.
dil
f :=
supd(x, x ,)
is called dilatation off.
dL(X, Y) := inf{|ln
dilf| + ln
dilrI 1 | f bi-Lipschitz hom.}
is theLipschitz
distance between X andY,
ifbi-Lipschitz homeomorphisms
exist.Otherwise
dL(X, Y)
= oo .3.2. PROPOSITION: For compact metric spaces,
dL
is a distance.There is the
following important
result of A. Shikata[15]:
3.3. THEOREM: There exists an E > 0
depending only
on n suchthat
any twocompact
n-dimensional Riemannianmanifolds M,
M withdL(M, M)
,E arediffeomorphic. The explicit
estimatefor
E has beenimproved by
H. Karcher(see [9]).
We now turn to the Hausdorff distance.
3. 4.
Definition : (a)
Let Z be a metric space,A,
B c Z. LetU~(A) := {z ~ Z| d(z, A) ~}. dz(A, B) : inf{~
>01 U,(A) D
B andU~(B) ~ A}
is the classicalHausdorff
distance forsubspaces
of asingle
metricspace.
(b)
LetX,
Y now bearbitrary
metric spaces.dH(X, Y) := inf{dZH(f(X), g(Y))},
where the inf is taken over all metric spaces Z and all isometriesf :
X -Z,
g : Y - Z.3.5. PROPOSITION: For compact metric spaces,
dH
is a distance.The reason for
introducing
both distances is that it is often easier first to prove d H-convergence - whiled L-convergence
isstronger:
3.6 PROPOSITION:
Any
sequenceof
compactdL-convergent
metric spaces is alsodH-convergent.
We will soon prove the
important
fact that in our classm(n, d, A, V )
bothtopologies
coincide - a theorem due to M. Gromov([7],
thm.8.25),
which iscrucial for his
proof
of thecompactness
theorem.But let us first introduce a notion that makes the Hausdorff distance much handier.
3.7.
Definition:
An E-net N in a metric space X is a subset N c X such thatU U~(x)
= X. In our context, E-nets willalways
be finite sets ofpoints
in axEN
compact
Riemannian manifold.Roughly speaking, dH-convergence
ofcompact
metric spaces reduces todL-convergence
of e-nets. Moreprecisely:
3.8. PROPOSITION:
If
X andXk, k = 1, 2,
... are compact metric spaces andif for
any E > 0 there exists an E-net Nof
X which is thed L-limit of
a sequenceof
E-nets
Nk of Xk,
thenXk
isdh-convergent
to X.All
proofs
of thepreceding propositions
can be found in[7].
3.9. THEOREM: In
9N (n, d, A, V)
theHausdorff
andLipschitz topologies
coincide. More
precisely:
Given p >0,
there existsa 03B6(n, d, A, V, p)
such
thatdH(M, M) 03B6 implies dL(M, M)
pfor
allM, M ~ m(n, d, A, V).
3.10. Remark: In
principle,
all estimates areexplicit,
inparticular f(n, d, A, V, p).
Nevertheless we omitexplicit
calculations for the sake ofbrevity.
Wemainly
have toverify
that thehypothesis
of the crucial Lemma 2 of[12]
is satisfied in thisslightly
different situation. Let usagain
state thatlemma.
Assume two manifolds M and M in 9X
being
coveredby
N convex balls ofradius
R,
such that theR/2-balls
still cover and theR/4-balls
aredisjoint.
Let z, and
Zl
be the centers, ul :Rn ~ Tz, M
andul :
Rn ~1; M
linear isome-tries, and ~i := expz 0
ul :BR(0)
c Rn ~BR(zi) ~ M, equally ~l,
normal coor-dinates.
Pij
dénotesparallel
translationalong
the shortestgeodesic joining
z, andzj.
3.11. LEMMA: There exist
R,
Eo, El in termsof
n,d, A,
V such that the conditions_ _
(i) d(~-1j~i, ~-1j~l) ~0 and
(ii) ~ u-1jPjiui - u-1jPijui~ ~1 for all i, j imply
that M and M arediffeomor- phic.
The
diffeomorphism
F is constructedby averaging
thelocally
defined diffeo-morphisms F
=~i~-1i.
From the calculations in[12]
it followsthat 11 dF 11
isarbitrarily
close to1, provided
R and E o are smallenough.
Hence we have:3.12. LEMMA: There exist
R,
E0, ~1 in termsof
n,d, A, V,
p such that conditions(i)
and(ii) imply dL(M, M)
p.Proof of
Theorem 3.9: Given n,d, A,
V and p, we aregoing
to show theexistence of an q such that
dH(M, M)
qimplies dL(M, M)
p. TakeR,
~0, E 1 as small as dictated
by
lemmas 3.11 and 3.12. Then choose a net ofcenters {zi}
c M such that theR/8-balls
aredisjoint
and theR/4-balls
coverM. The
problem
is now to find a net ofcenters {Zl}
c M and proper identifications of thetangent
spaces7§, M
and1;,M,
i.e. suitablemappings
u,,ui
such as tosatisfy
conditions( i )
and( ii ).
For that purpose we introduce anauxiliary
net{pk}
cM, containing {zi}
andbeing,
say,8-dense,
8 muchsmaller
than
R. IfdH(M, M)
is smallenough,
there exists a, say, 203B4-net{ pk}
c Mhaving arbitrary
smallLipschitz
distancefrom {pk} -
the latterholds in
particular
for thesubnet (zil
and thecorresponding subnet {zl}
c{pk}.
The ballsB(1;, R/16)
arecertainly disjoint
and the ballsB(1, , R/2)
cover M.
Finally
take{B(zi, R)}
and{B(zi, R)}
ascoverings
of M and M.On both
manifolds,
theR/2-balls
still cover, asrequired
for lemma 3.11. The fact thatonly
theR/16-balls
aredisjoint
instead of theR/4-balls,
leads to aworse estimate for the number of balls
(See [12]).
As a consequence, the above mentioned estimatefor ~dF~ requires
even smaller R and E o .([12],
p.80).
Assume R and E o to be chosen small
enough
from the start.We are now
looking
for suitable linear isometries ui,ui.
For the identifica- tions oftangent
spacesIi
=uiu-1i
we demand thatF
=~i~-1i = expz Ii exp-1zl
sends
{pk}
~B( zl, R )
almost onto thecorresponding
net in M. We aregoing
to show that
such h
exist and that the so defined localmappings F, satisfy
thehypothesis
of lemma 3.11.Roughly speaking,
if themappings
aregood
on avery dense net,
they
aregood enough everywhere.
Now fix an i. Consider the nets
{xk := exp-1zlpk} ~ B(0, R) ~ Rn
and{xk := expz-1zl pk}.
We arelooking
for a linearisometry h
that sends{xk}
almost onto
{xk}.
That is apurely
euclideanproblem,
which was solvedby
T.Yamaguchi ([17]).
Hisproof
was rathertechnical,
because hecomputed
allconstants
explicitly.
We willgive
a shorter version of theproof
at the end ofthis section.
3.13. LEMMA: Given v >
0,
there exists a 03B4 > 0 and a 03BC > 0 such thatfor
any two 03B4-nets{xk}
inB(0, R)
c Rn,
and{xk}
c Rn with the same numberof points, satisfying
xo =xo
= 0 andthere exists a linear
isometry
I EO(n)
such thatApplying Lemma
3.13 to the nets{xk} and {xk}
in the fixed euclidean spacesTz M
andTz M,
we can choose uiarbitrarily
and obtainui := hut.
The rest of the
proof
of Theorem 3.9 now follows from the next lemma.3.14. LEMMA:
There
exist constants in termsof
n,d, A,
V s. t.(i) d(~-1j~i, ~-1j~i) const0(03B4 + 03BD),
(ii) ~u-1jPijui- u-1jPijui| const1
+const2 R ’
8+vTherefore,
if R and then 8 are chosen smallenough
from the start and ifdH(M, M)
is so small as toyield
asufficiently
small vby
Lemma3.13,
Lemmas 3.11 and 3.12 can be
applied
tocomplete
theproof
of the theorem.a
Proof of
Lemma 3.14 : For technical reasons to be understood in(ii),
we prove( i )
forB(0, 2R)
instead ofB(0, R )
and assume that the choice ofh
has beenmade with
regard
to theselarger
balls.By
Lemma 3.13 and Rauch’scompari-
son
theorem,
whichyields
a boundon Il d expz, Il,
we haved(Fi(pk), pk)
=d(expzl Iixk, expzl xk)
const - v, where{pk},
asabove,
denotes theauxiliary
net.
By
thetriangle inequality,
Again by
Rauch’scomparison theorem,
Thus we have shown that
1 ~-1j~i-~-1j~i |
issmall on
thedil(~-1i)
8-dense net{u-1ixk}.
As we have a bound ondil(~-1j~i - ~-1j~i),
weobtain for ail x E
B(0, 2R):
(ii)
isproved by comparing parallel
translation on the manifold and in thetangent
space, see[3],
p.101,
where thefollowing
formula is derived from Jacobi field estimates:d(expz ( w
+exp-1zlzj),
expzJ Pijw) const" . R | w|,
where say,1 w|
R. Letw
= uiv.Then expzl(w
+exp-1zlzj)
=~i(v
+~-1i(zj))
and
expzj Pijw
=~i(u-1jPijuiv),
henceand therefore
where we have used
( i )
for x = v+ ~-1i(zj) ~ B(, 2R). Finally,
Proof
of Lemma3.13;
Assume without loss ofgenerality,
R > 1. Take anarbitrary
orthonormal frame{es}
of R n. There exists a subset{a1, ..., an}
ofthe net
{xk}
with1 as - es 03B4.
Let{a1,...,an}
denote thecorresponding points
in{xk}. {as}
and{as}
have smallLipschitz distance,
therefore{as}
isstill
linearly independent,
even "almostorthonormal",
because thetriangles (0,
as,al)
have almost the sameedgelengths
as(0, as, al).
The Schmidt orthonormalization process therefore
yields
an orthonormal frame{es}
close to{as}, say 1 as - es|
8. We define Iby I(es) := es.
ThusI is a linear
isometry
with|I(as)-as|03B4+03B4, s = 0, 1,...,n.
Now let xk be an
arbitrary
netpoint.
Thetriangle inequality yields Il |I(xk) - as|-|xk - as~ 03B4 + 03B4. Moreover,
the smallLipschitz
distance ofthe
given
netsimplies
the existence of a small 8’ such thatConsider the
mapping
Note that
a0 = a0 = 0.
(p isinjective
andcontinuous, B(0, R)
iscompact,
therefore~-1 : ~(B(0, R)) ~ B(0, R)
is continuous. Hence eachI(xk)
isarbitrarily
close toxk, provided 8
and J1. are smallenough.
Thatcompletes
theproof
of the lemma. 04. The
compactness
theorem4.1. Let us
again
state theorem 1.7:THEOREM: Let 0 a 1. Then any sequence in M contains a
subsequence
which is
dL-convergent
to an n-dimensionaldifferentiable manifold
M with metricg of class C1+03B1.
We obtain
optimal regularity properties by using "optimal coordinates", namely
harmonic coordinates.In
[8],
Jost and Karcherproved
the existence of harmonic coordinatesH: B(p, R) ~ TpM on a-priori
sized balls around anypoint
p EM,
wherethe radius R
depends only
ongeometrical quantities
of M(see
Thm.4.3).
These coordinates are called harmonic because the
component
functions are harmonic. Just as the well-knownexponential coordinates, they
are canoni-cally defined,
i.e. without anyarbitrary
choices. Harmonic coordinates areoptimal
in thefollowing
sense:4.2. THEOREM.
( J. Kazdan,
D. De Turck[6]): If a
Riemannianmetric is of
class
Ck+« in
somecoordinates,
so it is in harmonic coordinates.Crucial for our purpose are the
following properties
of harmonic coordi- nates(see [8], [16]).
4.3. THEOREM:
( J. Jost,
H. Karcher[8]):
Let M be acompact
Riemannianmanifold,
0 a 1. Aboutany point p E
M there exists a ballB( p, R) of fixed
radius
R,
on which harmonic coordinates exist and havethe following properties:
( i )
There exist auniform C2+03B1-Hölder bound for
the transitionfunctions, (ii) a uniform C1+03B1-bound for
themetric,
and(iii) a uniform C«-bound for
theChristoffel symbols,
where the radius and the Hölder boundsdepend
on thedimensional,
theinjectivity radius,
andcurvature bounds
of
M.Proof of
Theorem 1.7: AssumeR’
to be small that harmonic coordinates existon balls of
radius,
say,5R’
andsatisfy (i)-(iii)
of 4.3. LetHt
be thesecoordinates on balls
B(zki, R’)~Mk,
and set~ki := (Hki)-1uki,
whereuki
areagain
linear isometries Rn ~TzMk.
Now(~ki)-1(B(zki, R’))
is nolonger
aball,
but contains a ballB(0, R) ~ Rn, R
close toR’. ~ki(B(0, R))
isagain
not a
ball,
but contains a ball with radiusR", R"
close to R. Afterpassing
toa
subsequence,
we can assume each manifold to be coveredby
balls with radiusR",
such that theR"/2-balls
still cover and theR"/4-balls
aredisjoint.
As in[12]
we can achieve that thecoverings
all have the same nerve.The Hôlder bounds of 4.3 are now universal for the whole sequence. The transition functions can be considered as
mappings ~kij: B(0, R) ~ B(0, cR) c IR n,
c a constant. But different from[12],
we do notonly
have a uniformC1-bound
forthe ~kij,
but a uniformC2+03B1-bound,
because harmonic coordi-nates are that much better than
exponential
coordinates.By
Ascoli’s theoremthere exists a
subsequence
such that for allpairs (i, j)
for which transition functionsexist, they
converge in theC2-topology
to limit functions~~ij : B(0, R) ~ B(0, cR )
of classc2+a.
Once moretaking
asubsequence
andonce more
applying
Ascoli’stheorem,
the metrics also converge - consideredas functions on
B(0, R )-
to limit "metrics"g~i
of classC1+03B1
on eachcoordinate
ball,
i.e. on each copy ofJ?(0, R).
The distinctcopies
ofJ?(0, R )
are now
glued together
via the transition functions~~ij.
Consider the restric- tionsij := ~~ij| (B(0, R ))
~B(0, R )
anddefine x - y:
~ij
s.t.ij(x)
=y. Set M°° :=
U B(0, R)/~.
If~~i
denotes the canonicalprojection,
re-stricted to the i-th copy of
B(0, R),
M°° becomes aC2+03B1-manifold
with the~~i
as coordinates.~~j(~~i)-1=ij
are the transition functions. Asthey
converge in
Cl (even C2),
the limit "metrics"g~i
have theright
transforma- tionbehavior,
i.e.they
define a(0, 2)-tensor
fieldg°°
on M°°.Clearly g°°
issymmetric.
As the metricsgki
are close to the euclidean metric onB(0, R),
this is also true for
g~i.
Inparticular,
thegr
arepositive
definite. Sog~
isagain
ametric,
butonly
of classC1+03B1.
We are nowgoing
to show that( Mk, gk)
isdH-convergent
to( M°°, g~). Let {p~l}
be a 8-net in M°° . Wecan find a
8’-net {pkl}
inMk, 8’ arbitrarily
close to8,
suchthat |d(p~l, pm )
-d(pkl, pkm)|
isarbitrarily
small if k islarge enough.
Just take anypoint
(~~i)-1pl representing PIE
M°° and letpkl = ~ki(~~i)-1pl. {p~l}
is a finite net,and therefore
d(p~l, pm )
is bounded away from zero.Thus
goes to1,
i.e.{pkl}
isdL-convergent
to( p’ 1.
HenceMk
isdh-convergent
to M°°.In
particular, (Mkl
is adH-Cauchy
sequence.By
theorem3.9,
it is also ad L-Cauchy
sequence, henced L-convergent
to some metric space, which can benothing
but thedh-limit
spaceM°°,
because forcompact
metric spacesX, Y, dH(X, Y )
= 0implies X
and Y are isometric(Prop. 3.5).
Crucial is the non smoothness of the limit
metric,
whereas the non-smooth-ness of M°° itself is not
essential,
becauseby
a classical result ofWhitney’s,
the maximal
C2-atlas
definedby
ourC2-atlas
on M°° contains a smoothsub-atlas,
which defined a C°°-structure on M°°.By
M we denote M°°endowed with this C°°-structure.
We are now
going
topresent
a reformulation of thecompactness
theorem(suggested by
D.Brittain),
which avoids the notions of Hausdorff andLipschitz topology,
and state some more facts that areimportant
for theapplications
ofthe theorem.
4.4. THEOREM: Let
{(Mk, gk)}
be a sequenceof manifolds
inm(n, d, A, V),
0 03B1 1. There exists a
subsequence «Ml, gl)l
with thefollowing properties:
( i )
EachMI is diffeomorphic
to asingle fixed manifold
M.(ii)
There existdiffeomorphism FI : M ~ Ml
suchthat {(Fl) *gl}
convergesin
Cl to a C1+03B1-metric
g on M.(iii) diam ( Ml )
converges todiam(M).
( iv )
For theinjectivity
radii we have lim supi(Ml) i(M).
(v) If expl
denotes theexponential
mapof Ml,
exp thatof (M, g),
andepl = (Fl)* expl,
theneplp
converges toexpp uniformly
oncompact
subsetsof TpM,
andexpp
isLipschitz.
Proof: (i)
We define thediffeomorphisms Fl :
M°° -MI
as in[12]
and in theProof of Theorem
3.9, namely Fl(p)
is defined as the center of mass of thepoints Fli(p) := ~li(~~i)-1(p), weighted appropriately. ( i )
of Lemma 3.10 isobviously satisfied,
because the transition functions~lij
converge inC0
to~~ij.
Condition
(ii)
of 3.10 had been used toestimate ~dFli - d Flj ~,
but now, withharmonic
coordinates,
such an estimate followsdirectly
from theCl-conver-
gence of
~lij,
for(~lj)-1~li~(~~j)-1~~i
ine1 implies ~li(~~i)-1
isC 1 -close
to~lj(~~j)-1
if l islarge enough.
Thus the construction of[12] yields
a diffeomor-phism FI :
M°° -Ml.
(ii)
isproved
in local coordinates. Setl : (Fl)*gl.
Incoordinates, li :=
(cpf)*gl,
whileI
=(~li)*gl.
Thusgf
=[(~li)-1Fl~~i]*gli
is the transformation formula for the metrics in coordinates.Therefore,
if(~li)-1Fl~~i
isC -close
tothe
identity, then gi’
isC 1-close
togl .
But(~li)-1F1~~i = (~~i)-1(Fli)-1Fl~~i,
therefore it suffices to show that
Fl
isC2-close
toFl.
This follows from thefact that the transition functions are even
C2-convergent,
whenceFI
isC2-close
to anyFl. Unfortunately
this does notyet imply
thatFil
is alsoC2-close
to the averageF1,
becauseFl(p)
is defined as theunique
zero y ofN
exp-1yFlj(p)03C8lj(p). Therefore,
in the definition of the center of mass too, theexponential mapping
needs to bereplaced by
the canonical harmonic coordinatemapping
With this
improved definition,
all formerarguments
remain true, but now the center becomesC 2-close
toFli(p).
So far we have shown that
gl
isCl-close
togli
if 1 islarge enough.
As themetrics
gl
converge inCl
tog°°,
this is also true for thegl.
Hencegl
isC 1-convergent
tog~.
(iii)
and( iv )
areproved
in[13]
forC1-convergent
metrics.( v )
The uniform convergence followsagain
from Ascoli’stheorem,
for Rauch’scomparison
theorem
yields
a universal boundon ~d eplp~ on
eachball Bl(0, R )
inTp M°°,
w.r.t. the metricg l.
Asl
-g~,
we may take fixed ballsB(0, r )
w.r.t.the metric
g~.
Afterchoosing
asubsequence, eplp
convergesuniformly
onB(0, r),
but for different r’s we obtain different Rauch-bounds and thus also differentsubsequences. Taking
for r allintegers successively
andchoosing
each sequence as a
subsequence
of thepreceding
one, we obtain a sequence of sequences, from which wefinally
extract thediagonal sequence. Assume {Ml}
to this sequence.
Any compact
K cTpM~
is contained inB(0, n )
for all ngreater
than some n K, thereforeekplp
convergesuniformly
on K to amapping
which must be
exp§i.
The universalLipschitz
bound onB(0, n K )
passes to the limit.Sakai
[13]
proves the convergence ofgeodesics
with methods fromordinary
differential
equations,
under theassumption
ofCl-convergence
of the metrics.To prove convergence of d
explp,
he needsC2-convergence
of themetrics,
which is not satisfied in our situation.
Finally,
we noteagain
that the non-smoothness of M°° is not essential. Let M be M°° with the above mentioned C~-structure andpull
back all the metrics to M.5.
Sharpness
of theC1+a
resultIn this
chapter
we aregoing
to show that theC1+03B1
result on the limit metrics issharp
in terms of Hôlder conditions. Moreprecisely,
we willpresent
a verysimple counterexample
of a limit metric that isC1+03B1
for any a 1 but notC1,l.
Nevertheless we are able to derive astronger result,
in terms of Sobolevspaces.
5.1.
Example:
Consider thefollowing
function of two realvariables,
wherex = (x1, X2)-
E is
obviously positive,
limE(x)
=1,
limgradxE
=0,
andapart
from theorigin, E
is C 00 .In
polar coordinates,
theexpression
for E readsAt
This
expression
tends to zero for any a1,
but toinfinity
for a = 1.The function E is now used to define metrics.
By
g11 = g22 =E,
g12 =0,
ametric on
R2
isdefined, expressed
in isothermal coordinates. It isimportant
that the coordinates xl, x2 are harmonic with
respect
to g, forby
theorem 4.2this rules out the
possibility
ofmaking
the metric smootherby reparametriza-
tion.
It remains to show that the curvature of g
stays
bounded in theneighbor-
hood of zero,
although
it is not defined at theorigin
itself. In isothermalcoordinates,
the Gaussian curvature readsIn our case, A In E = 8 cos
2,W,
so K is indeed bounded.In order to obtain a sequence of metrics
g’ converging
to g, weapply
mollifiers
JEk
to g, with fk ~ 0. Since thissmoothing
process,namely
convolu-tion with narrow
kernels,
preserves Hôlderconditions,
we obtain a sequencegk = J~k g
of C’-metrics with uniform Hôlderbounds, converging
to g in theC1+03B1 topology. Clearly
the bound on K carries over.So far we have shown that the
C1+03B1-estimates
for the metric in terms of curvature bounds which Jost and Karcher obtained in[8]
cannot besharpened
to a = 1. The desired
example
for thecompactness
theorem is noweasily
established. We consider any
compact,
two-dimensional Riemannian mani-fold,
and in somearbitrary neighborhood
wereplace
thegiven
metricby gk,
putting
the two metricstogether by
apartition
of 1 in the usual way. Let us now dérive our final resultconcerning
theregularity
of limit metrics. It is animmediate consequence of the
following
theorem.5.2. THEOREM:
(I.G.
Nikolaev[19]).
Let M be a spaceof bounded
curvature, 03A9a domain in which harmonic coordinates are
defined.
Then in Q the componentsgiJ of the
metricare functions of class H2p(03A9) for all p
1.Bounded curvature
K1
KK2
is here to be understood in ageneralized
sense,
namely
in terms of theangular
excess oftriangles, compared
withtriangles
of the sameedgelenghs
in the space forms of curvatureK1
andK2.
On
compact
differentiablemanifolds, C1-limits
of smooth Riemannian metrics with bounded curvature|K| 2 satisfy
this condition.Moreover,
if all metrics in aC1-convergent
sequence areexpressed
inharmonic
coordinates,
then this must also hold for the limitmetric,
becausethe condition for harmonie coordinates reads
gij0393lij = 0, l =1, ...,n.
In our
proof
of thecompactness theorem,
the limit metric was in fact obtainedas a
C1-limit
of a sequence of smooth metrics with bounded curvature,expressed
in harmonic coordinates. Hence itscomponents
areH2p-functions by
Nikolaev’s theorem. Thus we have shown:
5.3. THEOREM: In the
compactness
theorem 1.6 or4.4,
the componentsof
thelimit
metric, expressed in
harmoniccoordinates,
are contained in the Sobolev spacesHp for
any p 1. Inparticular,
all notions or curvature are almosteverywhere defined.
Acknowledgements
The author
profited
very much from fruitful discussions with D.Brittain,
R.E.Greene,
K.Grove,
H.Karcher, Min-Oo,
E.A.Ruh,
W. Ziller and several othersduring
a conference in Marseille1984,
and he wishes to thank theorganizers
of themeeting,
M.Berger
and S. Gallot. Aboveall,
he is much indebted to the referee of the paper, J.P.Bourguignon,
for a number ofhelpful suggestions,
and to the thesisadvisor,
ErnstRuh,
for this advice and encoura-gement.
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