A NNALES DE L ’I. H. P., SECTION C
M ARIANO G IAQUINTA G IUSEPPE M ODICA J I ˇ RÍ S OU ˇ CEK
Connectivity properties of the range of a weak diffeomorphism
Annales de l’I. H. P., section C, tome 12, n
o1 (1995), p. 61-73
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Connectivity properties of the range of
aweak diffeomorphism (*)
Mariano
GIAQUINTA, Giuseppe
MODICA Dipartimento di Matematica ApplicataUniversita di Firenze Via S. Marta, 3 50139 Firenze, Italy.
Ji0159í
SOU010DEK
Akademie ved Ceske republiky Matematicky Ustav
Xitna,
25 11567 Praha, CR.Vol. 12, n° 1, 1995, p. 61-73. Analyse non linéaire
ABSTRACT. - We discuss
connectivity properties
of the range of Sobolevmaps, and of weak
diffeomorphisms
orequivalently
of elastic deformations.Key words: Calculus of variations, finite elasticity.
RESUME. - On
presente
des resultats sur la connexion del’image
d’undiffeomorphisme
faible.In this paper we shall
study
someproperties
of the range of aweak
diffeomorphism
u, where f2 is an open connected domain in R’~ . We denoteby Rn
another copy of Rn and werecall,
compare[3] [2],
that aClassification A.M.S.: 49 Q 20, 73 C 50.
(*) This work has been partially supported by the Ministero dell’Universita e della Ricerca Scientifica, by C.N.R. contract n. 91.01343.CT01, by the European Research Project GADGET, and by Grant n.11957 of the Czech Acad. of Sciences. The second author would like to
aknowledge hospitality of the Mathematisches Institut of ETH Zurich during the preparation of this work.
Annales de l’lnstitut Henri Poincaré - Analyse non linéaire - 0294-1449 Vol. 12/95/01/$ 4.00/@ Gauthier-Villars
function u E
W 1’ 1 ( SZ, Rn )
is said tobelong
to ifwhere
M(Du)
denotes the n-vector inAnRn
xRn
ei,..., en
being
the canonical basis ofRn,
and moreoverwhere
Gu
denotes the n-dimensional rectifiable current in Rn x Rn carriedby
thegraph
of u. Ifand
then
where M := E and is the n-vector
orienting
Mcompare
[5].
The class of weak
diffeomorphisms
is then defined as the class ofu E
cart 1 (03A9, Rn )
such that(i)
det Du > 0 a.e. inSZ,
(ii) u
isglobally
invertible in the sense thatholds for
all §
E xRn ) with §
> 0.Annales de l’lnstitut Henri Poincaré - Analyse non linéaire
In the
physical
case n = 3 such a class arisesnaturally
in finiteelasticity,
and in fact characterizes elastic
deformations
in the sense of[4].
In order to discuss
properties
of the rangeof u,
of course we should firstidentify u(f2).
First we consider Sobolev maps u ERn),
p >l,
and we do it in terms of
approximate continuity,
compare e.g.[ 1 ] .
Givena
point x
E H at which H haspositive density, o(SZ, x)
>0,
one says thatz E is the
approximate
limit ofu(y) for y -
x,if for every r > 0 the
point x
is a zerodensity point
for the setu-1(Rn B B(z, r)).
Here thedensity
is defined in terms ofLebesgue
measure
It turns out that for a.e. x G H the
approximate
limit ofu(y)
exists and agrees with
Lebesgue’s
value of u. Moreprecisely, setting
we have
and
finally,
compare[7], [13]
consequently
We shall now work with the
approximately
continuousrepresentative 11
on
Au
of u and prove that theimage
of a connected set f2by
aW1,p
map is connected.DEFINITION 1. - We say that A C R" is
d-open if and only if 0 (A, x)
= 1for
all x E A.Vol. 12, n° 1-1995.
The collection of
d-open
sets defines the so-calledd-topology;
it is in facteasily
seen that unions and finite intersections ofd-open
sets ared-open
sets. Such a
topology
is studied for instance in[8] [9]
and[10],
where the notion ofdo-connectedness
is introduced.LEMMA 1. - Let H
C Rn
be open and connected and let A C SZ be a setof positive
measure withfinite perimeter
in S~for
which~A~
> 0 and= 0. Then
~SZ B A) =
0.Proof. -
Fromwe infer that the distribution xA has zero derivatives in
H,
hence xA is constant inH,
as H is connected. DWe can now state
THEOREM 1. - Let Q be an open connected set in Rn and let u E
RN),
p > l. Then the set nAu)
is connected.Proof - Suppose
that B :=u(A
nAu)
is not connected. Then there aredisjoint
open setsU1
andU2
inR~
such thatSince u is
approximately
continuous onAu
the setsare contained in
Au
andd-open
in Rn .From B C
Ui
UU2
we then deduce thatAu
=Ai
UA2,
henceAs B
n Ui
we haveAi ~ 0, hence IAi (
>0,
since the ared-open.
AlsoConsider now the reduced
boundary c~~ Ai
ofAi
in H. We haveAnnales de l’lnstitut Henri Poincaré - Analyse non linéaire
hence
so that
From Lemma 1 we therefore
deduce S2 B All
= 0 which contradicts> o. D
Remark 1. - It is
easily
seen that in fact Theorem 1 holds for anyrepresentative v
of u which isapproximately
continuous in with,~n (SZ B Av)
=0, replacing Au
and urespectively
with and v.Remark 2. - The choice of a
representative
of u in Theorem 1 isessential. For
example
consider the functionThen
u(B(0, 1)) _ (-1, 0)
U(0,1)
U{2},
i.e.u(B(O, 1))
is not connected.Only carefully redefining u
on?~l"-1-a.e. point
of the line{0}
x(-1,1)
CB(0, 1)
in terms of anapproximately
continuousrepresentative v
we caninfer that
v(B(0, 1))
is connected.We are now
ready
to discussconnectivity properties
of the range af weakdiffeomorphisms u
Edif (0, Rn).
Since has the double Lusin’sproperty,
from[4]
we known that there exists a null setNu
CH, INul
=0,
such that u is one to one on
Ru B Nu
andIn fact this holds for any Lusin’s
representative
of u,and,
moreover, we can assume that be defined in all of H.We shall now introduce a variant of the notion of
connectivity
whichis suited
,for
our purposes. Given two subsets A and B of Rn we define their essential distanceby
We then set
DEFINITION 2. - A set A
C Rn is
said to beessentially connected, ess-connected, iff
Vol. 12, n° 1-1995.
We have
THEOREM
2. -
Let SZ ~ Rn be a bounded connected domain and letu C
1,1 SZ, Rn).
Thenu(SZ)
isess-connected for
any Lusinrepresentative
ic
of
u.Proof - Suppose ic(SZ)
is not ess-connected. Then we can findB1, B2
Cic ( SZ )
such thatConsider now an open set U D
Bi
with smoothboundary
~Lf such thatdist
(U, B2)
>0,
and the functionA(y)
isLipschitz-continuous
and for some~o
> 0Finally
we extend A to all of R" xRn by setting
Setting
we see as consequence of the double Lusin’s
property
of ù(in
fact fromI
= 0 if~A~
=0)
thatNow we slice the current
Gu by A,
compare[11].
For a.e.8,
0b $o
the slice
Gu, ~, b
> exists as a(n - 1)-rectifiable
current andon
(n - 1 )-forms
withcompact support
in 03A9 x R n. On the other handand
Annales de l ’lnstitut Henri Poincaré - Analyse non linéaire
so that
Since
Rn
=0,
weget
and therefore
This
implies
as
o~~ A1 ~ _ Al
xRn)
=0,
where ~ is the map(x, y)
--~ x.This
gives
a contradiction sinceby
Lemma 1 we then have|A2|
= 0. DWe shall now show that maps in dif
(Q,
do not cavitate. Resultsof these
type
arerelatively simple
if one has some control on theboundary.
Indeed we have
PROPOSITION l. - Let SZ be a bounded open connected set in Rn and let
u E
dif 1 ( SZ, Rn). Suppose
thatis
compact
and letthe
decomposition of
thecomplement of
K into connectedcomponents,
whereUo
is the unbounded component. Thenand for each I
=1,
...,m we have either |(03A9)~Ui|
= = 0.In
particular, if
m -1,
thenVol. 12, n° 1-1995.
Proof. -
It is an easyapplication
of theconstancy theorem,
see e.g.[11].
In factis an n-dimensional rectifiable current in
Rn
withmultiplicity
one and~ u(S2) n Ui]
isboundaryless
inUi.
The last statement follows then at onceas
]
> 0 because of det Du > 0 a.e. 0Remark 3. - A
simple
consequence ofProposition
1 is the result in[12].
In fact oneeasily
sees that the classAp,q
introduced in[12]
is asubclass of dif
and,
if is the current carriedby
thegraph
of a continuous map u, then K C
Our last theorem concerns the
regularity,
in the sense ofnon-cavitation,
of weakdiffeomorphisms
without any control on theboundary.
Weconsider a bounded and
simply
connected domain H in R n. We denoteby
d : S~ ~
(0,oo)
aWhitney’s regularized
distancefunction, i.e.,
a smooth functiond(x)
which isequivalent
to dist(x,
for x E H. We thenassume that
(S)
For somebo
> 0 the open setsare connected
for
all b with 0 bbo.
THEOREM 3. - Let 03A9 C Rn be a connected domain
satisfying (S)
and letu E
dif 1 ( SZ, Rn).
Thenfor
almost everyb,
0 bbo,
theimage ic ( SZs ) of SZs
andR n B
are bothessentially
connected.Proof. -
SetOb
:=ic(SZs),
0 bbo.
We know thatic(S2s)
is ess-connected. Assume on the
contrary
thatR n B Os
is not ess-connected fora non zero measure set of b’ s. For almost every such S’ s
is of course a rectifiable current with finite mass,
consequently Ob
is aCaccioppoli
set, as7r
being
the map(x, y)
-~ y. Fix now one such a 8. We claim that for almost every81
with 081 b
we haveAnnales de l ’lnstitut Henri Poincaré - Analyse non linéaire
and moreover
In order to prove
(10)
we first observe thatwhere
because f satisfies the double Lusin
property.
From this weeasily
inferwhere
On the other hand the trace u of u on
~03A903B41 belongs
for a.e.81
toW1,1(~03A903B41, n), Hn-1
almost everypoint
in~03A903B41
is aregular point
foru and ~c, and
moreover
compare e.g.
[6]. Denoting
the Lusinrepresentative of u,
we theninfer that
consequently
Since the set
{x
E~03A903B41 n Ru
E 9039403B4}
differs formE81 by
a null setand n has the Lusin
property
on~03A903B41,
wefinally
infer( 10)
from( 11 ).
We now choose
81
in such a way that(9)
and(10)
hold.Setting
Vol. 12, n° 1-1995.
(10) yields
On account or our
assumption,
R :=Rn B
is not ess-connected.We can then find
disjoint
open setsU1, U2 C Rn
such thatBeing ic
one-to-one in H we haveand
if we take into account
(13)
and(14).
From Theorem 2 we know that C is
ess-connected,
hence one of the addenda of(15),
say Cnul,
must be a null setconsequently
From
(12)
we therefore obtainNow we define
and
observing
thatB, U1, U2
is acovering
ofRn,
weget
consequently
~- ~ _0,
if we take into account(16).
We therefore conclude that either B = R" a.e. or = 0. Because of(13)
wefinally
inferB =
Rn
a.e.and,
because of(17),
thatwhich
contradicts
0 in(13).
QAnnales de l ’lnstitut Henri Poincaré - Analyse non linéaire
We shall now show
by
means of a fewexamples
that Theorems 2 and3 are in some sense
optimal.
Our firstexample
shows thatu(S2)
may be disconnected.Example
1. - Let 52 =(-1, 1)2
CR2
and let a E(0,1).
Consider the map u : S2 ~R 2
definedby
- 1,1 -
We have u E
dif 1 SZ, Rn
In factG u
where u~ is thefamily
of maps defined
by
It is
immediately
seen thatis not
connected,
but it is ess-connected. Notice that instead for theapproximately
continuousrepresentative u
of u we havein tact x
(-1,1)
ismapped
to zero andby
the Hausdorff estimates of thesingular
set of u we cannot have~0}
x(-1,1)
CS2 ~
We thereforesee that is connected
according
to Theorem 1.Finally
we notice that Theorem 2 does not hold for Cartesian maps as it is shownby
thefollowing
variant of theprevious example.
Setand
Then it is
easily
seen thatis not ess-connected while it is connected in the usual sense.
Vol. 12, n° 1-1995.
Example
2. - Weidentify R2
with thecomplex plane C,
we setand we consider
u(z) .- z2
for z E H. In the a.e. sense we haveClearly
is notessentially connected,
whilen Ru)
is
essentially
connected for all 6 > 0.The map u is of course of class
C1
in H and its exactimage (not
thea.e.
image)
isgiven by
n
Au)
which is
simply
connected in the usual sense.The next
example
of a discontinuous weakdeffeomorphism
shows thatin
general R2 B
nAu)
need not be connected(in
the usualsense).
Example
3. -LetH=B(0, 2) C R2, Q = ~(~1, ~2)
-~-] 1~,
and u =
(u1, U2) : B(0,2)
-~R2 given by
One can show that u E
dif ( SZ, R2 ) (in
fact u for allp, q
2), by approximating u by
a sequence of smooth maps for instanceOne then sees that
while u is not
approximately
continuous at(0, 0) .
Thus we havewhich is not
simply connected,
but n andR2 ~
nLu)
areboth
essentially
connected.Example
3 shows that weakdiffeomorphisms
may create holes of zero measure.Annales de l ’lnstitut Henri Poincaré - Analyse non linéaire
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(Manuscript received November 18, 1993.)
Vol. 12, n° 1-1995.