S ERGEY V. L UDKOVSKY
Quasi-invariant measures on non-archimedean groups and semigroups of loops and paths, their representations. I
Annales mathématiques Blaise Pascal, tome 7, n
o2 (2000), p. 19-53
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Quasi-invariant measures
onnon-Archimedean
groups and semigroups of loops and paths,
their representations. I.
Sergey V. Ludkovsky
permanent address: Theoretical
Department,
Institute of GeneralPhysics,
Str. Vavilov
38, Moscow, 117942,
Russia.Abstract
Loop
andpath
groups G andsemigroups S
as families of map- pings of one non-Archimedean Banach manifold M into another N with markedpoints
over the samelocally
compact field K of char-acteristic
char(K)
= 0 are considered.Quasi-invariant
measures onthem are constructed. Then measures are used to
investigate
irre-ducible representations of such groups.
1 Introduction.
Loop
andpath
groups are veryimportant
in differentialgeometry, algebraic topology
and theoreticalphysics [2, 5, 19, 25]. Moreover, quasi-invariant
measures are
helpful
for aninvestigation
of the group itself. In the case of real manifolds Gaussianquasi-invariant
measures onloop
groups and semi- groups were constructed and thenapplied
for theinvestigation
ofunitary representations
in[17].
,In
[12, 14, 16] quasi-invariant
measures on non-Archimedean Banachspaces X
anddiffeomorphism
groups wereinvestigated.
*Mathematics subject classification
(1991 Revision)
43A05, 43A$~ and 46S10.During
the recent time non-Archimedean functionalanalysis
and quan- tum mechanicsdevelop intensively [21, 27].
One of the reason for this is in thedivergence
of someimportant integrals
and series in the real or com-plex
cases and their convergence in the non-Archimedean case.Therefore,
itis
important
to consider non-Archimedeanloop semigroups
and groups, thatare new
objects.
There are manyprincipal
differences between classical func- tionalanalysis (over
the fields R orC)
and non-Archimedean(21., 22, 24, 28].
Then the names of
loop
groups andsemigroups
in the non-Archimedean case are used here inanalogy
with the case of manifolds over the real fieldR,
buttheir
meaning
isquite different,
because non-Archimedean manifolds M aretotally
disconnected with the small inductive dimensionind(M)
= 0(see §6.2
and Ch. 7 in
[8])
and real manifolds arelocally
connected withind(M)
> l.In the real case
loop
groups G arelocally
connected fordimRM dimnN,
but in the non-Archimedean case
they
are zero-dimensional withind(G)
=0,
where 1dimRN
oo is the dimension of the tangent Banach spaceT~N
over R for 1V.
Shortly
the non-Archimedeanloop semigroups
were con-sidered in
[15].
In this article
loop
groups andsemi groups
are considered. Theloop
semi-groups are
quotients
of families ofmappings f
from one non-Archimedean manifold M into another N withlimx~s0 03A603C5 f(x)
= 0 for av ~
tby
thecorresponding equivalence relations,
where so and 0 are markedpoints
in
M
and Nrespectively,
M =M B ~s~}, ~v f
are continuous extensions of thepartial
differencequotients ~~ f .
Besideslocally
compact manifolds alsonon-locally compact
Banach manifolds M and N are considered. This work presents results for manifolds At and N modelled on Banachspa.ces X
and Yover
locally
compact fields K such thatQp C K C Cp,
whereQp
is the fieldof
p-adic numbers, Cp
is the field ofcomplex
numbers with thecorresponding
non-Archimedean norm, that
is,
K are finitealgebraic
extensions ofQp.
More
interesting
are groups constructed with thehelp
of A. Grothendieckprocedure
of an Abelian group from an Abelian monoid. Thisproduces
the non-Archimedean
loop
group. Alsosemigroups
and groups ofpaths
areconsidered,
but it isonly
formalterminology.
Both in the real and non-Archimedean cases
compositions
ofpathes
are defined not for allelements,
but
satisfying
the additional condition. Since the non-Archimedean field K is not directed(apart
fromR)
this condition is another in the non-Archimedeancase than in the real case. On the other
hand, semigroups
with units(that is,
monoids)
and groups ofloops
have indeed thealgebraic
structure of monoidsand groups
respectively. Quasi-invariant
measures on thesesemigroups
andgroups are constructed in
§3
of Part I and§2
of Part II. Then such measuresare used for the
investigation
of irreducibleunitary representations
ofloop
groups in
§3
of Part II.To construct real-valued and also
Qq-valued (for q ~ p) quasi-invariant
measures
specific
anti derivations andisomorphisms
of non-Archimedean Ba- nach spaces are considered.Apart
from the real-valued measures the notion ofquasi-invariance
forQq-valued
measures isquite
different and is based onthe results from
[24].
For this a Banach spaceL(p,)
ofintegrable
functionsdefined for a
tight
measure ~ on analgebra Bco~X )
ofclopen
subsets ofa Hausdorff space X with
ind(X)
= 8 is used. To construct measures westart from measures
equivalent
to Haar measures on K. The real-valued non-negative
Haar measure v on K as the additive group is characterisedby
theequation v(x
+A)
=v(A)
for each x E K and A E wheredenotes the Borel u-field of X
(see Chapter
VII in[4]).
Each bounded non-negative
Borel measure on aclopen compact
subset of K may containonly
countable number of atoms, but for it each atom may be
only
asingleton.
Therefore,
the Haar measure vcertainly
has not any atom. TheQq-valued
Haar measure w on K is characterised
by w(z
+A)
=w(A)
for each z E K and each A EBco(K) (see Chapter
8 in[21]).
In view ofMonna-Springer
Theorem 8.4
[21]
a non-zeroQq-valued
invariant measure w onBco(K)
existsfor
each q ~
p, but does not existfor q =
p.Pseudo-diSerentiability
of measures with values in R andsidered,
because in the non-Archimedean case there is not any non-trivial differentiable functionQq for q ~
p. This notion ofpseudo-differentiability
of real-valued measures is based on Vladimirov operator on thecorresponding
space of functionsf
K --~ R[26, 27].
Semigroups
and groups ofloops
andpaths
areinvestigated
in§2
and PartII
respectively.
Here real-valued and alsoQq-valued
measures are considered(for q ~ p). Unitary representations
ofloop
groups aregiven
in Part II.The
loop
groups are neither Banach-Lie norlocally compact
and have astructure of a non-Archimedean Banach manifold
(see
Theorem11.2.3).
A.Weil theorem states
that,
if there exists a non-trivialnon-negative quasi-
invariant measure on a
topological
group G relative to left shiftsLg
for allg E
G,
then G islocally compact,
whereLgh
=gh
for each g andh ~
G(see
also Corollaries111.12.4,5 [9]). Therefore,
theloop
group and theloop
semigroup
has not any non-zero Haar measure. In Part I manifolds withdisjoint
atlases modelled on Banach spaces are considered. This is sufficient for many purposes.Moreover,
in§II.3.4
it isshown,
thatarbitrary
atlases ofthe
corresponding
class of smoothness of the same manifolds preserveloop
groups and
semigroups
up toalgebraic topological isomorphisms.
In Part IIloop
andpath
groups for manifolds modelled onlocally
K-convex spaces alsoare discussed.
The notation is summarized in
§II.6.
2 Loop semigroups.
To avoid
misunderstandings
we firstgive
our definitions and notations.They
are
quite
necessary, but a readerwishing
toget
main resultsquickly
canbegin
to read from
§2.6
and then to findappearing
notions and notations in§§2.1-5.
2.1. Notation. Let K be a local
field,
thatis,
a finitealgebraic
extensionof the
p-adic
fieldQp
for thecorresponding prime
number p[28].
For b ER,
6 ~ b
1,
we consider thefollowing mapping:
~~~
;= E~p
for ~’ ~ 0,
:=0,
such thatjb(~~ :
: K --~Ap,
where K CCp, Cp
denotes the field of
complex
numbers with the non-Archimedean valuationextending
that ofQp, :=’~~~, Ap
is aspherically complete
fieldwith a valuation group
0 ~ x ~ p}
=(0, ~) ~
R such thatCp ~ Ap
~6, 21, 22, 28~.
Then we denote :~ x for each .c ~ K.2.2. Note. Each continuous function
f :
: M --~ K has thefollowing decomposition
(1) f(x)= 03A3 03B1(m, f)Qm(x),
m~Nno
where M = 0,
l~
is the unit ball inKn,
are basic Amicepoly- nomials, a(m, f ~
E K areexpansion
coefficients(see
also§2.2 ~13~
and(1, 3j~.
Here
~y : d(x, y) ~ r}, B(.X, x, r~~ :_ ~y
eX:r~
are balls for a space X with a metricd,
zE X,
r >0,
N :=~1, 2, 3, ...}, No
:-~0,1, 2, 3, ...~.
.2.3. Definitions and Notes. Let us consider Banach spaces X and Y
over K.
Suppose
F : I~ --~ Y is amapping,
where U is an open bounded subset. Themapping
F is called differentiable if foreach (
EK,
a? E U andh E X with x +
(h
E U there exists a differential such that(1) DF(x, h)
:=dF(x
+|~=0:= lim{F(x
+03B6h)
-F(x)}/03B6
and
h)
is linearby h,
thatis, DF(z, h)
=: where.F’~~)
is abounded linear
operator (a derivative).
Let(2) h; ()
:= +~~)
-~’~~)~I ~
be a
partial
differencequotient
of order 1 for each a? +(h
EU, (h =~
o.If
h; ()
has a bounded continuous extension onto U x V x,~r
where U and V are open
neighbourhoods
of x and 0 inX,
U + V CU,
~ = B~K, o,1),
then(3) h;
= supI~~~~’Cx~ h;
~(x~U,h~V,03B6~S)
and =
F’(z)h.
Such F is calledcontinuously
diflerentiable onU. The space of such F is denoted
C(1,
U ~Y).
Let(4) h; ()
:=(F(z
+~h)
- EY~~
be
partial
differencequotients
of order b for 0 bI,
ac +(h
EU, ~h ~ o,
:~-
F,
whereY~p
is a Banach space obtained from Yby
extension of ascalar field from K to
Ap. By
inductionusing
Formulas(1 - 4)
we definepartial
differencequotients
of orders n + 1 and n + b:(5) ~~F(~~,.,.~~;Ci~~~+i)
:=+
(n+lhn+l; h1,
..,hn; 03B61,
...,03B6n) - 03A6nF(x; h1,
...;hn;
03B61, ..., 03B6n)}/03B6n+1
and =03A6b(03A6nF)
and derivatives = Then
C(t, U
--~Y)
is a space of functions F : ; U --~ Y for which there exist bounded continuous extensions~~F
for each z and x +(;h;
E U and each 4 vt,
such that each derivativeF~~~(x) :
:X~
--~ Y is a continuous k-linearoperator
for each a?E U
andare the
integral
and the fractionalparts
of t = n + brespectively.
The normin the Banach space
C(t,
U -+Y)
is thefollowing:
1s~ I~
~=hl~
~~~~1~
..., ,where o t ~
R, sign(y)
= -1 for y0, sign(y)
= 0 for y = 0 andBign(y)
= 1for y
> ~.Then the
locally
K-convex spaceC(oo,
U ~Y)
:=~~n=1 C(n,
U ~Y)
issupplied
with theultrauniformity given by
thefamily
of ultranormsil
*~C(n,U~Y).
2.4. Definitions and Notes. 1. . Let X be a Banach space over K.
Suppose
M is ananalytic
manifold modelled on X with an atlasAt(M) consisting
ofdisjoint clopen
charts(Uj,03C6j), j
EAM, M ~
N[18].
Thatis, ~I~
and areclopen
in ~I and Xrespectively, ~a
:U~
- arehomeomorphisms,
are bounded in X. Let X = where(1) co(a, K)
:={a-
=(~ :
: i E~))a’’
~K,
and for each e > 0 the set(i :
>e)
isfinite}
with(2) ~x~
:= suP|xi|
o0i
and the standard orthonormal base
(e, :
: i ~a) [21],
a is anordinal,
a>
1[11].
Itscardinality
is called a dimensioncard(a)
=:dimKc0(03B1,K)
over K.Then
C(t,
M -+Y)
for M with a finite atlasAt(M), card(AM) No,
denotes a Banach space of functions
f
: M -~ Y with an ultranorm(3) ~f~t
= sup~f|Uj~C(t,Uj~Y)
~,j~M
where Y :=
K)
is the Banach space overK,
0 t ER,
their restrictionsf|Uj
are inC(t, Uj
~Y)
for eachj, 03B2
> 1.2.4.2. Let
X,
Y and M be the same as in§2.4.1
for a local field K. When X or Y are infinite-dimensional overK,
then the Banach spaceC(t,
M ~Y)
is in
general
ofnon-separable type
over K for 0 t E R. For constructions ofquasi-invariant
measures it is necessary to have spaces ofseparable type.
Therefore, subspaces
oftype Co
are defined below. Their construction isanalogous
to that of Co from I°~by imposing
additional conditions(see
forcomparison [21]).
We denote
by Co(t,
M --~Y)
acompletion
of asubspace
ofcylindrical
functions restrictions of which on each chart
f|Ul
are finite K-linear com-binations of functions e
p, m}
relative to thefollowing
norm:
~~3
:= sup~)~
ii,m,l
where
multipliers m)
are defined as follows:(2) m)
v-=~Qm|Ul~C(t,03C6l(Ul)~Kn~K),
m ~
Qp)
withcomponents
~ ENo,
non-zerocomponets
of m are m;, ..., with n EN,
m := ..., for each0,
:=(~’~ ,
...,~~ )
EX, Qo
:= 1(see
aslo§2.2).
Lemma.
If f
eCo(t, M
--~Y),
then(3) (f|Uj)(x)
=i,m
for each j
EAM,
wherea(m, fi|Uj)
E K areexpansion coefficients
such thatfor
each e > 0 a set(4) ~(~~ m~~) ~
:f a(’m~ I J(t, m)
>finite
.Proof. This follows
immediately
from thedefinition,
since(5) f(x)
=03A3 fi(x)qi,
;e4
where
Co(t,
M -~K).
In view of Formulas
(1 2014 5)
the spaceCo(t,
M --~Y)
is ofseparable type
over
K,
whencard(a
x~
xA,~) ~ Evidently,
forcompact
M the spacesCo (t,
M -~Y)
andCo(t,
~I --~Y)
areisomorphic.
2.4.3.a. Now we define uniform spaces of the
corresponding mappings
from one manifold into
another,
which are necessary for thesubsequent
def-initions of
loop semi groups
and groups.Let N be an
analytic
manifold modelled on Y with an atlas(1) At(N)
=~{Y~~’~~)
: k E such that: V~~ --~ ~~{v~)
c Yare
homeomorphisms, card(AN) No
and B : M ~ N be aC(t’)-mapping,
also
card(AM) N0, where Vk
areclopen
inN, t’ ~ max(l, t)
is the index ofa class of
smoothness,
thatis,
for each admissible(i,j):
(2)
E~*(~, U;a
--~y)
with *
empty
or an index *taking
value 0respectively, (3) 8= =i
:= o awhere :=
[U;
n are non-voidclopen
subsets. We denoteby
M -
N) for 03BE
= t with 4t ~
oo a space ofmappings f
: M ~ Nsuch that
(4)
-B=,J
EC*(~y U=a
-~Y).
In view of Formulas
(1 2014 4)
wesupply
it with an ultrametric(5) 9)
= sup "gi,j~C*(03BE,Uj~Y)
i~1
for each
4 ~’
oo.2.4.3.b. For a construction of
quasi-invariant
measuresparticular types
of function spaces are necessary, which are obtainedby imposing simple
relations on vectors
h;
forpartial
differencequotients.
Let M and N be twoanalytic
manifolds with finiteatlases, dimKM
= n EN,
EC(~, Uj
~K)
for eachWe denote
by Cp {(t, s), M
-~N)
acompletion
of alocally
K-convexspace
(1) ~f
EN) :
tp~f’’1{,~~ ~)
o0and for each e > 0 a set
~{k, rrz) :
:~ ~a{m,, f ~-8~~)~J{{t, $), m)
> finite}
ta
’ ’
relative to an ultrametric
(2)
:= sup|a(m, f a
-s), m),
i,j,m,k
where 8
No, 0 ~
oo, ,(3) Jj((t, s), m)
:= maxh1,
...,03B61,
..., with(4) hi
= ... =h03B3
= e1, ..., = ... =hn03B3
= enfor each
integer 03B3
such that 1 03B3 s and foreach v E {[t] + 03B3n, t
+03B3n}.
In view of Fbrmulas
(1 2014 3)
this space isseparable,
when N isseparable,
since M is
locally
compact.2.4.4. For infinite atlases we use the traditional
procedure
of inductive limits of spaces. Fbr M with the infiniteatlas, card(AM)
=N0,
and theBanach space Y over K we denote
by
M -+Y) for 03BE
= t with 4 t o0or
for {= (t, $)
alocally
K-convex space, which is the strict inductive limit(1) Y) :=
str -Y), ~, ~},
where E E
E, E
is thefamily
of all finite subsets of AM directedby
theinclusion E F if E C
F, UE
:=~j~E Uj (see
also§2.4 [13]).
For
mappings
from one manifold into anotherf
M -~ N we thereforeget the
corresponding
uniform spaces. Then as in§2.4.4(b) [13]
we denotethem
by
M --~N).
We introduce notations
(2) C(~~ M) ~=
--~M)
nHom(M), (3) M)
=C~(~~
M --~M)
nHom(M),
that are called groups of
diffeomorphisms (and homeomorphisms
for 0 t1 and s =
U),
8 =id, id(z)
= z for each x ~M,
whereHom(M)
:={f
:j
EC(0,
Af -~M), f
isbijective, ,~(M)
=M, f
andf -1
EC(0,
M -+M)}
denotes the usual
homeomorphism
group. For s == 0 we may omit it from thenotation,
which isalways accomplished
for M infinite-dimensional overK.
2.5. Notes.
Henceforth,
ultrametrizableseparable complete
manifoldsM
and N are considered. Since alarge
inductive dimensionInd(M)
= U(see
Theorem 7.3.3[8]),
henceM
has not boundaries in the usual sense.Therefore,
has a refinement which is countable and its charts
(Uj,
areclopen
and
disjoint
andhomeomorphic
with thecorresponding
ballsB(X,
ya,r~),
where
(2) ~.:
:U?
-+ foreach j
E~.~
are
homeomorphisms (see {8, 18j).
ForM
we fix suchAt’(M).
We define
topologies
of groupsG(~, M)
andlocally
K-convex spaces .C~(~’, ,~l --~ Y)
relative to where Y is the Banach space over K.Therefore,
we suppose also thatM
and N areclopen
subsets of the Banach spaces X and Yrespectively. Up
to theisomorphism
ofloop semigroups (see
below their
definition)
we can suppose that So = 0 EM
andy0 = 0
E N.For M =
M B ~a}
letAt(M)
consists of charts EAM,
whileAt’(M)
consists of charts(t~~, ~y), ,j
EA~,
where due to Formulas(1, 2)
wedefine
(3) t/i
=U1 B {0}, 03C61
== U; and 03C6j = 03C6j
foreach j
>1,
0 E
U1
,M
=U’1 B {0}
s03C6’1
= ,U’ ; = U’j
and03C6’j = 03C6’k
for
each j
>1, ,~
eA’M
=A’M, Ui
3 0.2.6. Definitions and Notes. 1. Let the spaces be the same as in
~2.4.4
(see
Formulas2.4.4.(1-3))
with the atlas of M definedby
Conditions2.5.(3).
Then we consider their
subspaces
ofmappings preserving
markedpoints:
(1)
~(N, y0)) := {f
EC03B80(03C9, M
~N)
: lim03A6v(f-
|03B61|+...+|03B6k|~0
h1,
...,hk; 03B61, ..., 03B6k)
= 0 for each v E{0, 1,
...,[t], t},
k = twhere for a > 0
and ~ == (t, s)
in addition Condition2.4.3.b.(4)
is satisfiedfor each
1 ~ 03B3
s and for each v E{[t]
+ +n03B3},
and the
following subgroup:
(2) Go(~~ M)
:=~f
EG(~~ M) /(so)
=so}
of the
diffeomorphism
group, where s ENo
fordimK M No
and a = o fordimKM
=N0.
With the
help
of them we define thefollowing equvalence
relationsK~:
if and
only
if there exist sequences{03C8n
E n~ N},
{fn
E -+N)
: n EN}
and~9n
E -.~’) :
n EN}
such that(3) f n(x)
= for each x E M and lim n~~f n
=f
and n~~lim gn = g.Due to Condition
(3)
theseequivalence
classes areclosed,
since(g(03C8(x))’
== sa, = 0 for t + s > 1. We denote them
by f > K,03BE.
Then for g Ef > K,03BE
we writegK03BEf
also. Thequotient
space(M, so)
~(N, y0))/K03BE
we denoteby N),
where03B8(M)
={y0}.
2.6.2. Let as
usually
AV B := A x{b0}
U{a0}
x B ~ A x B be thewedge product
ofpointed
spaces(A, ao)
and(B, 60),
where A and B aretopological
spaces with marked
points a0 ~ A
andbQ
E B. Then thecomposition g o f
of two elements
f , g
E~(~’, (~’, so)
-~ is defined on the domainM V
s0}
=: M V M..Let M =
M B ~0}
be as in§2.5.
We fix an infinite atlas :=~(Uj, ~’3) : ~ EN}
such that: U~
-~B(K, y’~, r’a)
arehomeomorphisms,
lim r’j(k)
= o andlim
= ofor an infinte sequence
{j(k) E N :
: k EN}
such thatclM[~~k=1 ’j(k)]
is aclopen neighbourhood
of 0 inM,
whereclMA
denotes the closure of a subset A inM.
In M V M we choose thefollowing
atlas VM)
= :l E
N}
suchthat ~ :
-~B(X,
~,o~)
arehomeomorphisms,
lim
al(k)
= 0 and lim k~~zl(k)
= 0for an infinite sequence
EN:
k EN}
such that is aclopen neighbourhood
of 0 x 0 inM
VM
andcard(N B {l(k) :
kEN})
=card(N 1 {j(k) :
k~ N}).
Then we fix a
C(~)-diffeomorphisms ~ :
M V M ~ M such that(1)
= for each k e N and(2)
= for each ! E(N B ~1(k) :
k EN}),
where(3) It :
k EN})
-+ k EN})
is a
bijective mapping
for which(4) p~~
p andpVl
p.This induces the continuous
injective homomorphism
(5) x* : C03B80(03BE, (MV M, s0 s0)
-+(N, y0))
~C03B80(03BE, (M, so)
~(!’V, y0))
such that(s)
Vf )(x)
=(g V ~)~x~lC~))
for each x E
M,
where(g
Vf )(y)
=f(y)
for y EM2
and(g
Vf )(y)
=g(y)
for y E
Mx, M1
VM2
= M VM, Mi
= M for d =I, 2.
Therefore(~)9°f
may be considered as defined on M
also,
thatis,
to g of
therecorresponds
the
unique
element inCo (~, (M, se)
--~(N, yo)~.
2.8.8. The
composition
inN~
is defined due to thefollowing
inclusion g
o j
ECa(~, (M, so)
-+(N, (see
Formulas2.B.2.(1-7))
andthen
using
theequivalence
relationsK~ (see
Condition2.6.1.(3)~.
It is shown below that
S~~(~l,
is themonoid,
which we call theloop
monoid.
2.7. Theorem. The space
from §2.6
is thecomplete
sep-arable Abelian
topological Hausdorff
monoid.Moreover,
it asnon-discrete, topologically perfect
and has thecardinality
c :=card(R).
.Proof. We have E
(M, so)
~(N, y0))
for eachf
EC03B80(03BE, (M, so)
~and
~G
E(see
also[16, 18~j.
Thediffeomorphism
x :M V M --~ M is of class
C(oo)
and from Condition2.6.1.(1)
forf;
E--~ it follows that for
f
~x* ( f x
Vf ~)
also Condition2.fi.1.(1~
issatisfied,
since X fulfils Conditions2.fi.2.(1-4~,
where i E~l, 2~,
E M for each
j,
n =h~
E~, ~J
E K. Due to Condition2.6.2(4)
thecomposition
inC03B80(03BE, (M, so)
~(N, y0))
isevidently continuous,
since
I!f ~ Pd
Xmax{~f~C03B80(03BE,M~Y), ~g~C03B80(03BE,M~Y)}
for finite
At(M)
andusing
the strict inductive limit for infinteAt(M~,
whent oo and d =
[t]
+ 1for 03BE =
t withdimKM N0,
d =[t]
+ I + sa for03BE
=(t, s)
with a =dimKM No,
where o t E R and s ENo.
Due toFormulas
2.6.1.(1-3)
and2.6.2.(5-7) f >x,~
o g>x,~= f o g >x,~
for each
f and g
ECo (~, (M, so)
"~(N, yo~),
since iff n(x)
= andgn(~)
~ for each 2 EM,
then( f n
V = V ,where ~n and (n
EG0(03BE, M).
Hence thecomposition
is continuous for thequotient
space.In view of Formulas
2.6.2.(1-3) M1M2
andM2VM1
areC(oo)-diffeomorphic,
hence these
semigroups
are Abelian.Evidently,
thiscomposition
is associa-tive,
since M V(M
VM)
isC(~)-diffeomorphic
with(M
VM)
V M. Inview of Conditions
2.6.1.(1-3)
for eachf
EC03B80(03BE,(M,s0) ~ (N, y0))
thereexist sequences
{03C8n : n
EN},
EN}
EN}
inG0(03BE, M), N}, N}
and {gn : nN}
in(M, so)
~(N, y0))
such that V
fn](03C8n
V = where(1) lim diam{x
EM: : V V =y0} = 0,
(2)
limfn
=f,
lim gn =f,
(3)
lim 03C90,n = 03C90, fn(x) ~ yQ for each a? EM,
(4) diam(A) :=
sup~x1
-x2~X,
x1,x2~A
A C M C X. On the other
hand,
fromlimn~~(fn
Vgn)
=f
V g it followsthat
limn~~ fn
=f
andlimn~~
g" = g.Using
Formulas(1 - 4)
we get’~o o
f >x,~= f >x,~
and wo>x,~=
e is the unit element in~V)~
since
f >x,~
° g>x,~= fog >x,~
for eachf
and g ECo (f , (M, so)
"~(~: ~oj)~
For each
f , h
and g E(N, yo)j
fromf
V g =f
V h itfollows
that g
= h. If thereexists 03C8
EG0(03BE, M)
such thatX*(j
V =V
h)(x)
for each x EM,
then thereexists 03C8
EG0(03BE, M
VM)
for which( f
Vgj(~(~)j
=( f
Vh)(z)
for each z E M V M andf (~~~~ )(xj
= foreach :B E
Mi, M~
=M2
=M,
henceg(z)
= for each x EA-f,
where03C8
Ecorresponds to 03C8|M2
. Then(5) f
o 9’>x~~=’~ f >x~~
o himplies
g
>K,03BE =
h >K,03BE,since it is true for
representatives
of these classes.Implication (5)
is caJled thecancellation
property. Therefore,
thecomposition
inN)
isassociative,
commutative and there is the unit element e,
consequently, N)
is themonoid with the cancellation
property.
To show that
S~~ (M, N)
is the Hausdorfl space it is sufficient to consider M with a finiteatlas,
since~I N~
is defined with thehelp
of inductive limit. In view of the monoid structure it is sufficient to consider two elements~ and e
with ~ 5~
e. . Let~= inf
(g~g,f~f)
be apseudoultrametric
in thatis,
(8) Pn(9~ f )
>t~, f)
=~~
(7) 03C103BE03A9(g, f )
= and(8)
G for eachf, g
andhE
where 9
and/
ECo (~~ (M~ $o)
--~(Ns ~o))t ~ 9 >x,~=
9~f >x,~= f
tf
and g EN). Evidently, N)
is continuous relative to thequotient topology (see §2.4
and§4.1 (8~).
If =0,
then there existGo(/, M)
and9n
E 9 such that(9) lim {sup
n~~~03C8j gn 03C6n~C0(03BE,M~Y)}
= 0j~N
(see
Formulas2.4.2.(3-5)
and2.4.3.a.(l)).
In view of Conditions2.6.1(1), 2.6.2(4)
and Formula(9)
for eachf E N)
there arein
Ef , ~~,
and~"
EGo(~, M)
such thatlim {sup ~03C8j
° V ° =0,
n~~ j
consequently, f o g
=f
= g of
for eachf
EN),
hence g = e.This contradicts the
assumption
g~
e,consequently,
E :=pn(g, e)
> o andWg n We
= 0 forW,
:={h
E~~p},
whereW,
areopen subsets of
N).
Then03A903BE(M, N)
isHausdorff,
since(10) 03C103BE03A9(g,f) > 0 for each g ~ f
and
p~(g, f ) satisfying (6 - 8, 10)
is the ultrametric.The space
Ca (~, {M, so)
--~{N, y4))
isseparable
andcomplete (see ~~2.4
and
2.6)
such that for eachCauchy
sequence in theloop
monoid there exists aCauchy
sequence inCp (~, {~1, as)
--~(N, ys)),
hence this monoid iscomplete.
For each
pair
of elementsf and g
EC03B80(03BE, (M, so)
-(N, y0))
with differ-ent
images I(M) ~ g(M)
we havef
g>,~,~.
Since N is embedded into the Banach space Y and N isclopen
in Y it ispossible
to consider shiftsalong
the basic vectors and retractions ofimages f(M)
within N of thecorresponding
class ofsmoothness,
hence this monoid is non-discrete. The manifolds M and N and the spaceC03B80(03BE, (M, s0)
~(N, y0))
areseparable,
hence c =
card{N)
-~ = c.For
each g
EN)
there exists aCauchy
sequence~gs
: i EN} ~ N) B {g}
such thatlimi-+-co Ii
= g, since this is true forC03B80(03BE,
M ~N)
and
choosing representatives
in classes. HenceN)
is dense in itselfand
perfect
as thetopological
space.2.8. Note. For each chart of
At(N) (see Equality 2.4.3.a. (1 ))
there are local normal
coordinates y
=(~ : j
E~3)
EB{Y,
a;,r;),
Y =Moreover, T~
=~
xY, consequently,
TN has thedisjoint
atlasAt{TN~
= x xI)
: i E whereIy
: Y - Y is the unitmapping, AN C N,
TN is thetanget
vector bundle over N.Suppose
V is ananalytic
vector field on N(that is, by
definitionV|Vi
areanalytic
for each chart and V o has the natural extension from onthe balls
B(X,
ai,r;)).
Thenby analogy
with the classical case we can define thefollowing mapping
expy(zV)
= y +zV(y)
for which~2 expy(zV(y))/~z2
= Q(this
is theanalog
of thegeodesic),
where for y EY
andis also denoted
by
y, z EK, V(y)
E Y.Moreover,
there exists arefinement
At"(N) = ~(Y~i, ~";) :
: i E ofAt(N).
This isembedded into
At(N) by
charts such that it is alsodisjoint
andanalytic
andare K-convex in Y. The latter means that
for each E
~r"={Y";)
and each a EB(K, U,1). Evidently,
we can considerExp, injective
onY";, y
EY";.
The atlasAt" (N)
can be chosen such thatV"
xB(Y, 0, r,)
-+Y"~
ito be the
analytic homeomorphism
for each a ~ A" ~, where oo >~_
>0, expy : ({y}
X4! i))
~V"=
iis the
isomorphism. Therefore,
ezp is thelocally analytic mapping,
exp :TN
~N,
whereTN
is thecorresponding neighbourhood
of N in TN.Then
(1)
M ~ N) ={g
EC(03B8,0)*(03BE,
M ~TN):
: 03C0N o g =f}, consequently,
(2)
-~TN) = U
--~N)
= --~N),
f~C03B8*(03BE,M~N)
where 03C0N : TN ~ N is the natural
projection, *
= 0 or * = 0(0
isomitted).
Therefore,
thefollowing mapping
(3)
:~V) -~ N)
is defined
by
the formulagiven
below(4)
= og(x),
,that
gives
charts on Nf --~N)
inducedby
charts onC~(~,
M .-~TN).
2.9.
Definition and Note. In view ofEqualities 2.8.(1,2)
the space-~
N)
isisomorphic
with --~ x where yo = 0 is the markedpoint
of N. Hered
_
(1) N~
:= ~V 0(@
’~Y))
for t ENo
with t + s>~ 0;
;=1
(2) for t + s = 0;
(3) N03BE
= N ~(~ 03BE(Xj ~ Y)) ~ CQ (o, Mk
~Y03BB)
far t ER B N,
;~a
where