T.FI aiinxi II. biua · ) 7 MCA + ercx) kxe 213,26). @ r. 0¥ RCKD µ •. TJBGMD°←¥in• JR Xo...
Transcript of T.FI aiinxi II. biua · ) 7 MCA + ercx) kxe 213,26). @ r. 0¥ RCKD µ •. TJBGMD°←¥in• JR Xo...
Maximum Principles
Consider the coefficients of L,
the function f and
the set r regular enough so that we C2Cn) n C CI ).
Because of the regularity assumptions the Pole can
be equivalently written in divergence or non - divergence
form ( already remarked ) .We find it convenient to
choose the form
Lu = T.FI,
aiinxi,
+ II. biua.
+ cu
Since the proof we are going to do works under
weaker regularity assumptions onaid
,bi
,C
,
namely that aid,
bi,
c e C CR ),
we will only assume
that and further suppose that he Ctcnnccr ) .
We will work under the assumption aid'
= aji,
RCR"
bounded and open .
Theorem ( Week maximum principle )
Assume we Ctcr ) n CCI ) and czo in R.
( ^ ) Lee e 0,
CIO =p mox in = moxie
( u is said to be a of ZR
sub solution )
(2) 4,
C Z 0 =D
hexin E Max µ+
r anwhere utcx ) = mex { uCx3o] .
To prove the theorem we first need the following result
from linear algebra :
Lemma;
A,
B positive semi - definite symmetric uxu
n
matrices.
Then I aid'
bit zo .
Proof ,
ijae
F Re Ocn ) : A = RTDR for some D= okay 6h,
- ,dn)with di 30 . Being B positive semi - definite ,
the
metric C : = RBRT is positive semi - definite ,too
.
This implies that Cii 30,
it { 1,2,
- in } .
Now using the invariance of the trace under. .
transposition and under commutation namely the
fact that tr ( JK ) = tr ( KJ ) = tr KKJJT ) we have
A=AT
p
£
aid
bid'
=tr ( ABT ) = tr ( BAT )=tr(# B) = tr # B) =
iij 1 ↳v commutation
transposition .
= tr ( EDRB ) = tr ( DRBRT ) = to CDC ) =
Lo commutation
=
.§ dicii zo
Da
Proof of the theorem
ake E > 0 and t > o so big that
- 0×2+11 ball at + Uc Ha < °. Define rfk ) : = ucx ) + set "
and note that
Lrf = Lute e
"'
( T.gl aijoeisnjt'
+ bat c)
s o + set 't
( - 05+11 ballot + Hello ) < °
If F x. e R : 0 s E ( xD=
mzex nf =D
Lrrecxo ) =-
;§aiicx
. ) NI.
,( ×
. ) t ? bicx. ) which )tcQ° ) ntcx
. )
Z ccx . ) Nscxo )
Z ° because in a mex point TN{xo ) - 0
thanks to the lemme applied to A = @iicxo) )ijand B = - DIE Ho ) noting that A is pos ohfby the uniform elliphieity and the B is
positive definite since at ×.
DTEKO) is non - pos .
definite as this is a mex point .
This contradiction yields , mox we=/° %) < °
-e
R\ wax or
2R
Now mox u s wax NE f° 4×0 ) - ° E utans ngonxut
- -
+r R
mexv 's mex @E)an ar
The thesis follows as s -00 since Nz → u
uniformly in I.
=D met U £ me × µ+.
.
r an
Note that if CIO there is no need of introducing @4+
Ten fact mex u = gains nog×NE = max we → mexu
an an e→o are
and the chain of inequalities is actually a chain ofequalities .
Riney : Of course one has also an equivalentstatement for min instead of mex .
This reads as
( 1'
) Luz 0 in R,
c=o ⇒ min u =
minusan
( 2' ) "
, CZO =D min re z - maxein an
where ii. - win { Mio } .
Theorem ( Strong maximum Principle )
let CZO in RCIR"
openand connected
.
Assume
we C2Cn)n CCI ) be such that Lee so.
F Xo ER : ucxo ) = mgxw > 0 =D U = const in R
r
Jn the case CEO : F xo c- Rieecxo ) = moxie =D u= const in RI
Jn order to provethis result we make use of
the following Lemme by Hopf .
Hopf lemme
Let czo in R,
we C2Cn)n Ctr ) and Luso . let xo ← 2R
such that Ucxo ) > UCH Fx E R. Suppose moreover that
F B CR such that x. ← JB ( we also saythat R satisfy
an interior ball condition at xo ) .Then
u( xo ) 70 =D 21 ( x . ) > 0,
%o
where V×.
is the unitary outer normal to B at xo.
In the case CIO then 21 ( ×. ) > o holds without
2v
assuming be ( x. ) 30
.
×0
Proof of the twpt lemme
without loss of generality wemay assume that
�1� = B Car ) for some r > 0.
We set vcx ) :=£tk[ It r2
txe B ( qr ) with X to be chosen later.
By uniform elliptieihy : P.g.,
aii 5i5j 301512
Using that ¢" "1) × ,= - ztxi it * 12
and that
( it " 2)a g.
= 47k.
.×
;it ""
2
- ztoijetk"
we have that Lv = - PL,
aiirxixj to¥,
birxitc =
= e-" " "
III. aid ( -41in .× ; tztoi ;) -ITYIETbizxa . + of it "Ie→m)
g e-" *
( -451×120+21 ltrA 1+271511×1 + Icl )
where A= ( ais )..j
and b = ( be,
- ,b" ) .
Consider now the region Ri= BG ,r)\B%, %) : txcr rz < kkr
Lira e-" " "
( -4×2 ⇐ To tztlltrallatztllbllortlkll .)
Provided 1 is big enough we have Lrrso. O*
By the assumption ucx . ) > lecx ) txer we have that
F e > ° such that ulx. ) 7 MCA + ercx ) kxe 213,26) . @
r.
RCKD
0¥ •µ.
TJBGMD°←¥in•JR Xo I i >
• rg r 1×1
Moreover,
since v = 0 we have UK.) 3 Uk ) + e Ncx ) �2�
12136 ,r)
ttxe 2136, r ) .We now have that tx€R
L ( utsr - ucxo ) ) = Keyt ELCN ) - Lcucxoj ) = - cucxo ) EO
A /×" either CEO
O 0 CUCXO ) or czo ,MK
. ) > 0by assumptionby *O
By the weak maximum principle
mfx ( utev - ucx . ) ) E wax ( let er - ucxo ))+ = O
a ar" by @& �2�
2136 ,r)U2Bl9%)
As a result we now have that txe R went even ) Eucx. )
Since for ×=×.
we have ll(xo)+ ENCX. ) = llcx
. ) we
:can write
( ucxteyrcx) -uCxo))y,
?ucx ) + ercx ) - ucx
. ) t×eR
0
Fnperlienlor Ju ( n + Ev - ucx . ) )| 30 or in other
x=Xo
words 2g ( ×. ) + Efg ( × . ) 30 ⇐D ( here w×o=×f )
- In
2£ ( x . ) 3- E @s ;×f)= Zetre > 0
-
zµc⇒=-Heitktx Tvcx. ) = -
zietkdx.
)@vk.7.ge )= - zxe→r4×÷P= -
siren↳ ix. 12am
a
Proof ( of the Strong maximum principle )
Let m : =
mgxin and set M :-. { xer : uk ) = in } .
r
Zf u¥ m consider N : = { xeri ucx ) < m } .
Pick a
point in N such that dist ( y ,M ) < dint ( q ,
24.
Such a point y exists since N is supposed Ntf
andR
is connectedNote that N is open by the continuity of n .
Joke the
largest ball centered aty
and contained in N
( the set of such balls is von empty again by the feet
that N isopen ) .
Denote such a ball by B.
There exists x. e Mr JB.
At the point xo N satisfies
an in tenor ball condition and by Hopf 's lemme
N.N2£yC xD 20 .
But this contradicts the fact that
u attains a wax point at xo.
BeThe contradiction implies re = in
.