A NNALI DELLA
S CUOLA N ORMALE S UPERIORE DI P ISA Classe di Scienze
M ARTIN S CHECHTER
A generalization of the problem of transmission
Annali della Scuola Normale Superiore di Pisa, Classe di Scienze 3
esérie, tome 14, n
o3 (1960), p. 207-236
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OF TRANSMISSION (*)
MARTIN SOHEOHTER
(New York)
1.
Introduction.
In the
past
few years there has beenincreasing
interest in so called« transmission >>
problems
forelliptic equations
andsystems (cf.,
eg., Picone[12],
Lions[9, 10, 11], Stampacchia [17], Campanato [18, 19]).
Theseproblems
may be described as follows. There are
given
two domains in Euclidean n- space which have a
portion ~o
of their boundaries in common. A boun-dary
valueproblem
is thanposed
for each domain with theboundary
con-ditions on
Io being
double the usual number andinvolving
the solutionsof both
problems.
To
give
asimple example,
let andG~2~
be the domains inquestion
with boundaries
aGel)
anda G~2~, respectively. One might
ask to find func- tions U(l) and harmonic in andG(2) , respectively,
y for which I- - J -,
and are
prescribed
on while andare
given
on andrespectively (here
a W
,a 2 b2
aregiven
functionsand a an
denotes a normalderivative).
an
Problems of this
type
forgeneral
second orderelliptic equations
havebeen treated as well as
problems
for somesystems (cf.
the references men-tioned
above).
(*)
The work presented in this paper was supported by the Institute of Mathematical Sciences, New York University, under Contract AT (30-1)-1480 with the U.S. Atomic EnergyCommission.
An announcement of this work was presented to the American Mathematical Society, April, 1960, Abstract No. 568-6.
1. Atinali delza Scuola Norm. Sup. -
In this paper we consider a transmission
problem
forgeneral
m - thorder
elliptic equations
andgeneral boundary
conditions. Moreprecisely,
letA,
andA2
be twoelliptic operators
of order m =1,
withsmooth
complex
coefficients. On~~
we consider a setBl, , ~12 ? partial
differential
operators
with smooth coefficients which neodonly
be definedon A similar set
B21’ B22 ,
...,B2r
is to be definedOn Io
we
prescribe
4roperators C11 , C,2 ,
... , yC1,2r , °21 , °22 ,
...,02,2r
of the sametype.
Theproblem
we consider is thefollowing ;
Given two functions1(1) , f ~2~
defined inG~l~ and G~2~ respectively,
to find functions U(l) and u~2~sucli
that
.. ’ - - ’ ’
--’in in
on on
on
Our
assumptions
on theBij
andCz~
aremild, being
no more than thoseusually imposed
inregular elliptic problems (cf. [2, 7]) plus
acompatibility
condition at
points
where10 and 1, (or
meet(cf.
Section2).
We definean «
adjoint » problem
andshow,
among otherthings,
that existence of so-lution of the
original problem
isguaranteed by
theuniqueness
of solution of theadjoint problem (cf.
Section 2 for a moregeneral sta~tement).
Moreoverwe show the existence of solutions
which
are smooth up to theboundary except possibly
atpoints
where~o
andIi join
and which do not behavebadly
at suchpoints.
Ourtheorem,
whenspecialized
to second order equa- tionsgives
moregeneral
results than thosepreviously
obtained.For
simplicity
we consider the case when both and G(2) are bounded and smooth. Under such circumstances we can map the closure of (~~2~ onto the closure of and then consider bothboundary problems appertaining only
to C~1>. Our transmissionproblem
then becomes a « mixed >>boundary
value
problem
for asystem
ofequations (c£. [16]).
This isessentially
theway we treated the
problem, although
we retained theoriginal
notation andterminology.
’
Our method
employs
a coercivenessinequality specially adapted
to theproblem. Near points
ofIt
and no newinequalities
wereneeded,
theproper estimated
being already
available in the literature(cf. [1, 2, 14]).
For
10
we derive newinequalities
which areessentially
those forsystems (cf.
Section7).
Moregeneral
estimates of this nature will begiven
in thesecond
part
of[2]. Finally,
forpoints
where~o
andIt
intersect we obtainspecial inequalities peculiar
to thisparticular problem (cf.
Section8).
In Section 2 we state our
hypotheses
and main theorem(Theorem 2.1).
The coerciveness
inequality
isdescribed
in Section3,
and itsproof
isgiven
in Sections
5, 7,
and 8. Our existence andregularity proof
isgiven
in Sec.tion 4. In Section 6 some
algebraic
theorems which are needed for our e- stimates are discussed.2.
Assumptions
andResults.
We consider two bounded
domains,
y G(l) andG~2~
in Euclidean n space with boundaries anda G~2~
which are each of class C°°. We assumethat =
0,
but also thatnaG(2) -
the closure of a non-empty
setIo
open in thetopology of a G
ora G2.
We set ·° For any
appropriate
subsetcS
ofEn,’
° we let C°°(d)
denote the set ofcomplex
valued functions which areinfinitely
differentiable incS.
We shall deal with vector functions v =(v~l~,
where v(i) gC°° (G(i))
and thefollowing
norms and inner
products :
where is a multi-index with non
negative components, , and
By
aboundary triple (xo
7 T,v)
weshall
mean apoint
XO 8aO(I) fl a G(2) ,
areal vector 1
#
0tangent
to(or a G~2~)
at x° and a real vector v~
0normal to
(or G(2) )
at x°. We shall make thefollowing assumptions (re-
ferred to as
Hypotheses
1-9).
_
_
1. In each there is defined a
partial
differentialoperator
with
complex
coefficients in2. Each
Ai
iselliptic
ini.e.,
the characteristicpolynomial
of
Ai
does not vanish at anypoint
when~= (~1~ ~2~ ..,~ ~~)
is real3.
Each Ai
is_properly elliptic
in 6~).By
this we meam thatAi
is el-liptic
in aCi) and that for everyboundary triple (aP, 1:, v)
with x° 8 thepolynomial
in zhas
exactly r
roots withpositive
i-maginary parts.
When it> 2,
everyelliptic operator
isproperly elliptic.
I
’
4. On each there are defined r
partial
differentialwhere each mij 2r and the
complex
coefficients are in 5. The set coversAi.
This means that ifis the characteristic
polynomial
ofBij ,
then for everyboundary triple
(x°,
1:,v)
with x° E I:i thepolynomials
in z ,are
linearly independent
modulowhere the
I§I) (x°,
7:,v)
are theroots
of(2.3)
withpositive imaginary parts
(cf. Hypothesis 3).
6. The set is
normal, i.e.,
mij=)=
mikfor j ~ k
and noQij v)
vanishes for any XO s
Ii
and v=f:
0 normal toa G~i>
atxO.
7. There are 4r
boundary operators
defined on-YO
Each set is assumed normal.
8. Let
be the characteristic
polynomial
ofOij .
Then for anyboiindary triple with x° E .2o ,
the relationsimply
thatU1 (z), U2 (z)
andthe Aj
allvanish,
wherethe Ai
arecomplex constants,
theU1 (z)
arepolynomials,
thePi+ (z)
are definedby (2.7), _and
Before
stating
the laststipulation,
we mention several consequencesof - Hypotheses
1 - 8. ’REMARK 2.1. It follows from
Hypotheses
6 that to there core-sponds
a normal setcalled adjoint
to it relative toA,
such thathold whenever and vanish near
fo,
and(Here Ar
denotes the formaladjoint
ofAi).
Inaddition,
if satisfies(2.13)
for all which vanish near
~o
andsatisfy (2.15),
then(2.14)
holds. Con-versely,
if satisfies(2.13)
for all U(i) which vanish near20
andsatisfy
,
(2.14),
then(2.15)
holds(See [3, 15 J).
REMARK 2.2.
Similarly, Hypothesis
7implies
that there are normalsets
such that ’’
for all and which vanish
near Ii,
where ds denotes the element of surface onREMARK 2.3. From
Hypothesis
8 it follows that for averyboundary triple (xo ,
z,v) with xo
c~ 0’
the relationsimply
thatUt (z), U2 (z),
and theÀj
allvanish,
whereThis follows from the fact that and
are
equal, respectively,
y toPij (z)
and for Hence relations(2.17)
and(2.18).
at aboundary triple imply
relations similar to(2.10)
and
(2.11)
for theboundary triple
-v).
Thusthe Aj
must vanish.The
following
notation will be useful infomulating
our last assump- tion. If is anypolynomial
ofdegree
S m andis any
(m + 1)
dimensionalcomplex vectors
we writeWe also write where the bar denotes
complex conjugation.
n~2013u
For every
boundary triple (:»°,
T,v)
we can define(cf. (2.7)). Hypothesis
9 can now be stated as follows.9. For every
point
and every v~
0 normal toat
X0,
there arepolynomials
in thecomponents
of isuch that
is
positive
for allcomplex
vectors and W(2)satisfyng
unless = W(2) = 0. Here
Rij
andQij
denote the characteristicpolyno-
mials of the
C~~
andBij,
yrespectively,
which are assumed of ordersm3
andy
respectively.
By
a solution ofproblem
17(A, f,
yCj)
we shall mean a vector fun-ction such that for every
compact
subset of which is bounded away
from S,
and such that in 1on
on
THEOREM 2.1. Assume that
Hypotheses
1-9 hold. Then asufficient
condi-tion
for problem
II(A, f, OJ)
to have a solution is that( f, v)
= 0for
everysolution v
of
IT(A*, 0, Bj , Cj’).
As an illustration we consider the
following generalization
of theproblem
mentioned in the introduction.
where v = ... , is a unit normal vector to the surface in
question
and the and are
complex
functions. We assume thatajk
= akj and that theAi
areproperly elliptic (cf. below).
We shall show that Theorem 2.1applies
when a certainexpression Z
defined below is real andnegative
First let us consider an
arbitrary boundary triple (XO, 7:, ’V)..
Thenwhere
We assume so that
Hypothesis
3 is satisfied. Mo-reover, If the
boundary triple
is onwhere Hence
can never vanish for z = and
Hypothesis
5 is satisfied.Next,
assume that theboundary triple
is onIo.
We must show thatthe identities
imply that 71
= 72 = 0. Here the arecomplex
constants and we have made use of the fact thatNow
(2.24) implies
thatwhere
Hence
the 7i
mustequal
zero if the de-terminant
does not vanish on
Io.
Finally,
y we assume that theboundary triple
is on S. We first note thatwhere
theb~z~~ depend
on the and theb(~).
ThusNow let be two
complex
vectors. ThusHence,
whenIn order to
satisfy Hypothesis
9 we must therefore show that there arepolynomials
es in t such that the realpart
of -is
positive
definite in the Moreover thepolynomials
Ci’.’" e4 must behomogeneous
in thecomponents
of z of orders3, 2, 2, 1, respectively.
Itis therefore clear
that C1 and e4
cannothelp
inmaking
theexpression positive
definite. We take them to be zero. We are then left withNow
by definition,
From this we caneasily
showthat the
expression
can be madepositive
in theis real and
negative
on S. For then we may takeFor then
both of which have
positive
realparts,
andMareover, if Z ~
0 on the whole offa,
then(2.25)
cannot vanish there.For otherwise we vould have
which is
impossible.
For theimaginary part
of theright
hand side ispositive,
while of the left hand side isnegative.
Thus Theorem 2.1applies
when
Z 0
onTo. Notice,
that when on 9 this criterionreduces to 0. ’
A
proof
of Theorem 2.1 will begiven
in Section 5 after we discuss abasic
inequality
in the next section.3.
The Inequality.
,’
’
An
important
tool inestablishing
our existence theorem will be acoerciveness
inequality adapted
to thisparticular problem.
In it weemploy
a
boundary
normwhich,
while not needed inobtaining
a weaksolution,
enables us to prove smoothness up to the
boundary.
We shall follow the methods of[15, 16 J
veryclosely.
- -Let x° be any
point
of(x°
may be either inIo
or SinceaG(l)
is of classC °°,
there is aneighborhood
of x° such thatn cm (XO)
can bemapped
in a one-to-one C °° way onto thehyperplane tangent
toa G~l~
at x°.Let 99
be a smoothcomplex
valued function defined on andhaving compact support
inaG(l) (xO). By the mapping
we may
consider g
defined onpart of C (x°). Defining
it to be zero on therest we set
where irs a coordinate
system
onand is the
image
of,under the
mapping.
We then setfor any two functions cp, y, where
Fi
denotes thecomplex conjugate
ofF, [y]. Similarly
we setAnalogous
definitions are to be made forpoints x°
ona G(2).-
Next assume in addition
that § and y
vanish near S =~o (this
is
automatically
the casewhen cm (x°)
n S =0).
If .E(~’)
is anypolynomial
in the
components
of~’,
we claim thatIn
fact,
if weapply
Parseval’sidentity
to(3.5),
we obtainwhere .E
(D’)
is atangential
differentialoperator,
990 is the function whichequals 99
on10
andequals
zero on-Y, ,
while 1Jlt has theopposite relationship to y. Thus
vanishesthroughout IC (xO) making (3.6) equal
zero.Now it follows from
(3.5)
thatand
hence,
if E(e’)
ishomogeneous in e’
ofdegree s,
we haveby
the Sch-warz
inequality
’
, - ,
It should be borne in mind that when
corresponding
definitions are made forpoints
ofâG(2B
all of the aboverelationships
hold with thesubscript
1replaced by
2.For any subset
d
let be the collection of allwhich vanish near the
boundary
ofd.
It follows from considerations in[ly 14]
that there is a constant Kdepending only on 9L (~O)
and s such thatfor all v g
Co~ (£1°)).
From this it follows thatwbenever and is bounded away from S.
Let C°°((7)
be the set of all vector functions such that each and vanishes near S. Assume that all of thehypotheses
of Theorem 2.1 are satisfied. We are
going
to show for everypoint
there is a
neighborhood
such that for every and every there is a constant K such thatfor all u ~
C °° (G).
As beforemij
is the order ofBij and mj
is the order of bothOij
andBy
thecompactness
of the we know that there is afinite set of
points
such that Letbe a
partition
ofunity
subordinate to thiscovering.
We may assume thatthe ek
areinfinitely
" differentiable.Taking s1- 2p
in(3.10)
we havewhere
Thus
This is the
appropriate
coercivenessinequality
which will be used in thenext section in our existence and
regularity proof.
As we havejust
seen, it can beproved by establishing inequality (3.10)
at eachpoint x°
ofU
G~2~. This program will be carried out in Sections5, 7,
and 8.4.
Existence and Regul arity of
theSolution.
In this section we
give
aproof
of Theorem2.1.
The main tool in ourapproach
in the coercivenessinequality (3.12).
Let H* be the
completion
ofC°° (G)
withrespect
to the normClearly,
H~ is a Hilbert space which may be identified with a subset of thecompletion
of withrespect
tot he normWe also set
It is
easily
seen from(3.12)
that[u, v]*
is defined foru, v 8 H*
and thatthere is a constant c
>
0 such thatfor all Let
N*
be the set of all such that[v, v]* = 0.
It fol-.lows from
(4.3)
and Rellich’s lemma thatN*
is finite dimensional. Hence N* is closed in bothH*
and.L2 (G(l»)
XL2 (G(2)).
Now let M~ be the set ofall v ~ H* such that
(v, N*)
= 0(i.e., (v, w)
= 0 for all w 8N*).
Itfollows
again
from(4.3)
and Rellich’s lemma that there is aconstant c1 >
0 such thatfor all v E M*
(cfr. [15]).
Now assume for the moment that
f
isgiven
and thatIn view of
(4.4)
we may substitute[u, v]*
for the innerproduct
of the Hil-bert, space M*.
Since(v, f )
is a bounded linear functional inM*,
there issuch that
for all
Moreover,
we claim that(4.5) implies
that(4.6)
holds for allTo see
this,
we first note thatby (4.3)
the norm([v, v]* + II
vis
equivalent
toH v 11*
in H*.Furthermore,
since N* is closed inH*,
everyelement v s H * can be
decomposed
into the form v = v’+ v",
wherev" 8N*
andBut =
07
thefirst term
vanishesshowing
M*. Now(4.5)
and(4.6) imply
thatfor all v 8
H*,
as was asserted.Taking
thespecial
cases when or withwe see that
for all such v. It now follows from the interior
regularity theory
forstrongly elliptic equations (cf. [4, 5, 6. 7, 11])
that theg~i’
are in 000(G(i))
after cor-rection on a set of measure zero.
Integration by parts
then shows thatu(i)
- satisfiesAiu(i)
=f
(i) in’ We next consider the
special
cases when v =0), v
=(0, v~2~)
wherethe are in 000
(G(i))
and vanish nearIo.
Then°
for all such v. It now follows from the
regularity theory
of[15]
that isin C°°
(G(i) U Ii). Moreover, (4.9) implies
thatfor all v(i) 8
(G(~)) satisfying B! -
v(i) = 0 on~2
andvanishing
near~o . By
Remark 2.1 this
implies
thatBij
= 0on -Yi .
__Finally,
we consider the case when v =-==(~~1~, V(2))
with v(1) 8 C°°(G(i))
va-nishing
near This time we haveBy working
with thepair
of functionsg~l~ , g~2~ simultaneously,
We can foll-ow the
reasoning
of[15] step by step
and show that each is in Since no new ideas areinvolved,
we do notprovide
the de-tails. Once the
regularity
isknown, (4.10) implies
thatwhenever E C°°
(G(i))
vanishes nearli
and satisfieswhere
Hence, by (2.16),
for all such v. Thus
by (4.11)
Since is otherwise
arbitrary,
this means thaton
Hence u is a solution of
problem
1I(A, f,
yC~~.
Since our
argument
was based onassumption (4.5),
ourproof
will becomplete
if we can show thatN*
is contained in the set of solutions of77(A~’(~ ~ ~ CJ).
This latterfact, however,
hasessentially
beenproved.
Forwe have shown that
if g
satisfies(4.7)
for all then eachU U ~2 U provided f 8
C°°(G).
This is the case, inparticular,
if we takef
= 0.Moreover, [g, g]*
= 0implies
But when the have the above mentioned
regularity properties,
these condi- tionsimply that g is a
solution ofproblem (A~, 0, 0/). Hence
everyelement of N* is a solution of a
(A*7 0, 0/),
and theproof
iscomplete.
REMARK 4.1. In
general,
not every solution(A*, 0, B~ , Cj’)
is inN*. For every element of N* is in
(G),
while no suchrequirement
ismade on solutions of yr
(A*, 0, 0/)-
Thissuggests
one way in whichour theorem can be
strengthened.
5.
Poi nts of G(i) U Zi -
From the consideration of Section
3,
we see that it remainsonly
toprove
(3.10)
for eachpoint XO 8
U G(2). In this section we shall show that forpoints
ofG(i)
UIi, (3.10)
follows from known results(cf. [1, 2, 14]).
The. main
difficulty
lies inconsidering points
of~° and 8,
and these caseswill be treated
seperately
in Section 7 and 8.First
suppose x°
E G11. We can take theneighborhood 9l (x°)
so smallthat its closure does not intersect For such
points
theellipticity
ofA ~ implies
for all and
(cf. [13]). By
standardprocedures
this can be transformed into
where .g’
depends
alsoon ~ and
8.Inequality (5.2) immediately implies
(3.10)
forx°.
A similarargument
holds forpoints
of G(2).Next assume that x° We take
9l(z°)
so small that its closure does not intersectTo U ¿2.
We then havefor
all I
sCo (x°))
and u(l) s 000(G(l)).
This follows from.[14]
once weknow the
fact, proved
in[15],
that the set conyersA1
wheneverJB~)~
1 coversA1 .
That coversA~ ,
was assumed(Hypothesis 5).
Hence
(5.3)
holds.Again
we may transform theinequality
intowhich
implies (3.10)
for x°. A similarinequality
holds forpoints
of’¿2.
In Section 7 we shall show that for
points x°
E~o
there is aneighbor-
hood
(x°)
such thatwhen and
In
addition
we shall prove in Section 8 thatat
points
where the are thepolynomials
mentioned inHypo-
thesis 9.
By (3. 7)
and(3.9)
it followsby
standard methods that each of theinequalities (5.5)
and(5.6) implies (3.10)
on theirrespective portions
ofthe
boundary (cf. [15, 16]). Moreover, by
the usual trick oftransforming
into a
semisphere
andapproximating
theAT, Oil by
homo.geneous
operators
with constant coefficients whichequal
theirprinciple
2. Artnali della Scuola Norm. Sup.. Pisa.
parts
atx°,
it iseasily
shown that either(5.5)
or(5.6)
holds in9L (x°)
if and
only
if it holds forhomogeneous constant
coefficientoperators
in asemisphere.
It therefore remains to prove(5.5)
and(5.6)
in such « canonical » situations. This will be carried out in Sections 7 and 8 after wedegress
in
the
next section to thestudy
of certainalgebraic
theorems which willbe needed. , .
6.
Preliminaries.
We now consider a few unrelated
topics
whichpresent
themselves in theproofs
of the next few sections. Westate,
them here for future reference.LEMMA 6.1. Let
P (z)
be apolynomial of degree
m withleading coeffi- cient ao
andhaving
no real roots. Let H(z)
be apolynomial of degree
m - Iwhich has all the roots
of
P(z)
which lie above the i-eal axis.If bo
is theleading coefficient of
H(z),
then ,where the
-integ1’al
i~s taken in theC’auck y principle
va,lue sense.Next consider the
polynomials
.where the are such that
If
0,)(,) ~ m2)
aretwo, complex vectors,
and we
employ
the notationLEMMA
6.2. If
implies
that eachAj
=0,
thenimply
ro(1) = ro(2) =0,
and vice versa.The
proof
of Lemma 6.2 follows from the fact that thefollowing
threestatements are
equivalent.
implies
implies
implies
Next consider the
polynomial
and set
where
Now assume that where and are
polynomials
ofdegree r
mand m - r, respectively.
SetFor each
polynomial Hj (z)
we can defineT~ (~~ ~) corresponding
toT (z, I) by
means of a formula similar to(6.I). Moreover,
it iseasily
checked that for anycomplex
vector w = c~~, ..., thepolynomial Hj (z) T (z, w) - P (z) w)
is ofdegree
m -1.Furthermore,
the coefficient of Zm-1 isHence, by
Lemma 6.1 we haveLEMMA 6.3.
If P (z)
has no real andP+ (z)
has all the rootsof P (z) (with multiplicities)
which lie above the reaclaxis,
thenwhere the
integral
is taken in theCauchy principle
value sense.LEMMA 6.4- The relation
I
is
equivalent
toProof : It is
easily
shownby
induction thatwhen zo is a root of
P (z)
ofmultiplicity greater
than t.Moreover,
ifk =1, 2,
..., p, are the distinct roots ofP- (z)
Withmultiplicities
y/c?then
(6.3) implies
Set
It is
easily
checked that theTkt (z)
arelinearly independent
and since thereare r of
them,
there are numbers such thatNow set
by (6.5).
Thus(6.6) implies
But from
(6.2)
and(6.7),
we haveHence
(6.8) implies
Conversely, (6.4) implies (6.8),
whichgives
in turn(6.6)
and(6.3).
Thiscompletes
theproof.
Now consider the
polynomials
where
=~= 0, j =1, 2,
..., m. Oneeasily
finds coefficientsPsj
such thatThus
where
bj~
is the Kronecker delta. ’LEMMA 6.5. For any
given
sety 221
"’ .9of complex numbers,
there isa
complex
vector co =(wo’
..., such thatProof : We set
Then
which was to be
proved.
LEMMA 6.6.
If
we setwhere
Q (z)
denotes thepolynomial
withcoefficients
which are thecomplex
coefficients of
thoseof Q (z),
then -Proof :
by (6.1)
and(6.9)
Finally,
y we consider twopolynomials
For each of then we can define
(z, ~)
and theY~ (z) by
means of for-mula
(6.1). Also,
if we aregiven
two sets ofpolynomials
we can find coefficients
flij
such thatNote that in these and future formulas we shall not
employ
the summation convention. Assume thatPi (z) = pt (z) P i (z),
where thedegree
ofP± (z)
is r.Then
defined
and
We now have
THEOREM 6.1. Assume In = 2r.
If
implies
that all theyAj vanish,
thenimplies
that all theÂj vanish,
and vice versa,.Proof : Assume that
(6.11) implies
that all of theÀj
vanish and that(6.12)
holds. We shall prove that all of theÂj
vanish.By
Lemma 6.5Moreover,
Lemma 6.5 shows that there arecomplex
vectorsW(l)
andW(2)
such that
Thus
by (6.12)
and(6.13).
But this isequivalent, by
Lemma6.4,
toBut it follows from Lemma 6.2 that
(6.14)
and(6.15) imply W(I)
=W(2)
= 0.Hence
the 2j’
vanish and the first stratement isproved.
The converse is pro-ved in similar fashion.
7.
Points
of~o .
In this section we shall prove
(5.5)
when is thesemisphere xn > 0,
C 1, G(2)
is thesemisphere 0, 1 x I 1,
and the coefficients of theAi
and theC~~
are constants. In such a case(5.5) readily
follows formholding
for all E C°°(G(i~)
which vanishnear x ~ =1.
Here theboundary
norm is taken over
~o,
which in this case is the setI x I 1,
xn = 0. Toconvert
(7.1)
into(5.5),
we substitute-v = u,
where U(i) 8 C°°(G(i)) and C
isa C°° function which vanishes
near =1.
The error terms are the han-dley by
standardtechniques (cf. [14, 16]).
We next note that Theorem 6.1 shows that the
C~~ satisfy Hypothesis
8 with
respect
to theAt.
Hence(7.1)
will beproved
if we canshow,
em-ploying only Hypothesis 8,
that a similarinequality
holds for theAi
andC~~ .
Thus the asterisks may bedropped
in(7.1).
Define 1J(i) to be
identically
zero outside and consider v =v2»
as a vector function defined on En . Let
’
be the Fourier transform
of v, where $’
=(~1, ~2 ,
... ,~n-1) corresponds
to;x’ =
(xl 1 X2
... ,and q corresponds
to xn . Set(cf. (2.7)),
andIn
addition,
weput
where
and
- (of. [14]).
It wasproved
in[14]
that for any functionvanishing
near I x ( =1
and outsideG~~~
If is a
polynomial in q,
weemploy
the notationwit similar definitions
for g (~’, W(~)) and g (~’, y2~).
Ifis a matrix in which
each gil (~’~ ~)
is apolynomial in V,
we setwith similar notation for i From
(7.7)
we haveBy (7.3)
we havewhere and
(cf. [14~). Similarly,
where the
T~
are similar to 2’. We therefore havewhere the asterisk denotes the
conjugate transpose
of amatrix,
(~’, 1),
andthe Aj
are vector functionsof ~’
to be chosen later. We have also setand made use of the fact that i
Anticipating
our nextstep,
we note thatHence, by
Lemma6.3,
Integrating (7.12)
withrespect to q,
we haveby (7.8)
and(7.13)
We now
pick
where 8
>
0 is a constant to be chosen later. We then haveNow the last term on the
right
hand side of(7.14)
is aquadratic
form inthe Åj. Moreover,
each coefficient is ahomogeneous
function ofdegree
- 1
(cf. [14]).
Hence there is a constant 8>
0 such thatfor all
possible
values of theÅj. Inserting
this value of s in(7.14) gives
The
stage
is now set forapplying
Lemma 6.4 of[14].
We needonly
torecall that
We then have
All of the
homogeneity requirements
are satisfied. Itonly
remains to showthat the sum of the last two terms on the
right
hand side of(7.16)
cannotvanish
for $’ ~
0 unlessJY1>
=W ~2~
= 0. This isindeed
so. For the va-nishing
ofthe Âj implies
,The
vanishing
of the last termimplies
But
by
Lemma 6.2, Hypotesis 8
thenimplies
=W ~2~
= 0. This com-pletes proof.
8.
Points
on.S.
In this section we shall prove
(5.6)
forpoints
xo 8 S.By hypothesis,
forevery such
point x°
there is aneighborhood 9~ (x°)
such thatfl 9l (x°)
can be
mapped
in a one-to-one C°° way onto thesemisphere 0, ] x
1.Similarly, G(2) n fl (x°)
can bemapped
in such a way0,x
1.We may assume that
points
ofZo
have the sameimages
under both map-pings. By
the usualprocedure
we reduce theproblem
toproving
for vector functions V =
(v~1 ~, V(2))
which vanish near theimage
ofCk (xo)
and
near x I =1,
where A* and theC~~
andB’k
have constant coefficients.The
($’)
are thehomogeneous
functions mentioned inHypothesis
9.We
employ
theanalague
of(7.15)
forA*, namely
where M’ and
the I§
have the samerelationship
to A* as M and thehave to A. We now obtain our result
by showing
that’
never vanishes
for ~’ #
0 unless= W(2)
=0,
where Jrepresents
thesecond term on the
right
hand side of(8.1)
anda >
0 is to be chosen.Let
E
be thecompact
set in 8 r+ n -
1 Euclidean space for which(The $k
are real while the arecomplex.)
Let12’
be the sdbsetof 12
ofs
those
points
forwhich -Y I Ail 12
=0,
i. e. thosepoints
for whichFor such
points
J ispositive by Hypothesis
9.By continuity,
y J>
0 onsome open set
m containing L’. Moreover, since L - M
iscompact,
thereis a
positive
constant a > 0 such thaton E - 9rl.
Hence(8.3)
isgreater
than onwhile it is
greater
than ~J>
0 on9N.
Hence(8.3)
ispositive
on the wholecompact
set~6. By homogeneity (which
iseasily checked)
it ispositive
forall
~’ # 0, #
0 and (ù(2)#
0. We nowapply
Lemma 6.4 of[14]
and theproof
iscomplete.
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Note added in proof. In the case of second order equations several authors have
proved
that u(i) satisfies a Holder condition in(Stampaaohia, Campanato,
Nikolsky)even when the bG(9 are not smooth. ,
Peetre (mimeogra,phed notes) has also extended the problem to higher order equations (indeed be oonsiders N equations in N domains). His method works for strongly elliptic equations and boundary conditions satisfying somewhat stronger hypotheses than those of the
present
paper.°