The sharp constant in Hardy's inequality for complement of bounded domain
Nonlinear Analysis, Theory, Methods&Applications, Vol. 33, No. 2, pp. 105-120, 1998 @ 1998 Elsevier Science Ltd. All rights reserved Printed in Great ...
Nonlinear Analysis, Theory, Methods&Applications, Vol. 33, No. 2, pp. 105-120, 1998 @ 1998 Elsevier Science Ltd. All rights reserved Printed in Great Britain 0362-546X/98 $19.00+0.00
Pergamon PII: S0362-546X(97)00518-X
THE
SHARP CONSTANT FOR COMPLEMENT
IN HARDY'S OF BOUNDED
INEQUALITY DOMAIN
T. M A T S K E W l C H and P. E. SOBOLEVSKII H e b r e w U n i v e r s i t y , J e r u s a l e m , Israel
(Received 1 August 1996; received for publication 14 May 1997) Key words and phrases: T h e n e w c o o r d i n a t e s y s t e m f o r d o m a i n w i t h s m o o t h b o u n d a r y , generalized Hardy's functional. INTRODUCTION
This investigation is continuation of the work in Ref. [1]. We will consider the generalized H a r d y ' s functional
where f~ is an arbitrary domain in R 3, u ~ C~(f~) and is not identically equal to zero, P0a(x) is distance from the point x, belonging to f~ to the boundary of the domain Of~, l_ 3 inf
R 3
and its
3 lp(u, ~ ) = 1 - - .
Here constant 3 in the right side corresponds to the dimension of considered space. The analogous result (with a more simple proof) was also established for R 2 and we ~uppose that these results can be generalized to R n. The following sections o f this article contain the p r o o f of Theorem 1. The first section is devoted to a description of the new coordinate system. It appears :hat there exists such a subset 9l of fl that on ~ \ 9 1 it is possible to introduce correctly the aew coordinate system, such that in this system estimate from below for ip(u, fl) can be ,~stablished by investigation of some one-dimensional functional. It can be shown that we can choose such 91 that its Lebesgue measure is equal to zero. ?roof of this statement is given in the Appendix. 105
106
T. MATSKEWICH and P. E. SOBOLEVSKII
In the second section the estimate from below for Ip(U, f2) is established. This estimate holds for arbitrary domain f2 when its boundary O2f is C z smooth two-dimensional manifold. In the third section the estimate from above is established. In this section we will use the homothety transformation, which allows to reduce investigation of lp(u, £2) to the case when D = 101. In this section boundedness of the domain D is an essential condition. 1. I N T R O D U C T I O N
OF THE NEW COORDINATE
SYSTEM
Let us suppose that if2 is an arbitrary domain in R 3 and its boundary 0¢) is a C 2 two-dimensional compact manifold. We will say, that pair (y, t) where y • 0f~ and t some positive number corresponds to the point x • f2 i f y is the nearest to x point of O2f (or one of such points), t is the distance between x and y. Note that in this case vector x - y is perpendicular to 0f2 in the point y. For every y • Ot2 let us denote: n(y) is the unit inner normal to 0f2 in the point y, T(y) = inflt > 0, such that there exists Yt • c9f2, Yt ~ Y and d i s t ( y t , y + tn(y)) <_ dist(y, y + tn(y)) = t], i.e. T(y) is infimum among those t, that for y + tn(y) point y is not the unique nearest point of Of2.
Statement 1 (proof of this statement is given in the Appendix). For every bounded domain f2 such that Of2 is a C 2 smooth two-dimensional manifold transformation: (y, t) --, y + tn(y), where y e f2 and t e [0; T(y)) defines bijection between a set of such pairs and f2\9l, where 9Z is subset of f2 such that its Lebesgue measure is equal to zero. Now let us consider arbitrary domain f2 (bounded or unbounded) such that 0f2 is a C 2 smooth compact two-dimensional manifold. Suppose, that Of~ is described by the set of maps ~Pi: Ui --" V~, i = 0 . . . . . k, where Ui C R E is an open bounded domain, LJki=1VR • 0f2, ~ i ; (~-1 • C 2 and let {Xi(Y)ff= 1 is the partition of unity, corresponding to Iv, I/~= 1. For arbitrary u e C~(f2) if f2 is bounded then f r o m Statement 1 it follows that l,~(u, ~ ) =
i~\~zlVulPdx ~ \ ~ lu/po~l dx
Iyeaei~tY) l V u l p E k = l X i J ' d y d t
~y ~ ae I~(y) [u/PaelPJ' dY dt
~/k=l ~y ev~Zi(Y) fro(y) IVul pJ' dy dt ~/k=l Iy ev~Xi(Y) i T(y) lu/pa~l pJ' dy a t ' where J ' is Jacobian, corresponding to conversion from standard Euclidean coordinates to coordinates (y, t). But let us note that if f2 is not bounded then for every u • C~(f2) we can define ~ as the intersection of f2 with sufficiently large ball B, such that B contains af2 (and so the boundary of 0f2 is also the C 2 manifold) and such that for every x belonging to the support of u the distance f r o m this point to a ~ is equal to the distance from x to 0f2. Then lp(u, f2) = Ip(u,~) and all following discussions can be done for the bounded domain ~ . Let us consider now one of the maps describing 0f2: {0: U--, V, U C R 2, V C tgf2. We will denote by (~, r/) coordinates in the plane domain U, then (0 defines C2-smooth diffeomorphism between (~, r/) • U and y e V. Now we denote by X(Y) one of the functions
The sharp constant in Hardy's inequality
107
from unity partition, corresponding to the chosen map. Then
Iy ~ vX(y) Ire')
[vulPJ ' dt dy J'y ~ vX(Y) Jo:r°') lu/po.lPJ ' dt dy
j(~,,) ~ v Z((o(g, 8)) Jor(~c*'~)) [Vul pJdt d~ d8
where J is the Jacobian that corresponds to conversion from the original Euclidean coordinates x = (xl, x2, x3) to the new coordinate system (4, 8, t).
Statement 2. In the notations described above J(~,~) ~ u Z((o(~, 8)) jT(~(~.~))]Vu]PJ dt d~ d8 ~(~,.) ~ uX(¢O(~, 8)) Ior(~(~'n)) [u/Po~ IpJ dt d~ d8 >_
where E, G, F, L, M, N are coefficients of the first and second fundamental forms of O~, H is mean curvature, K is Gaussian curvature (see [3]).
Proof. (1) In what follows we will denote the standard scalar product by ( , ) and the cross product by ×. Then J = det O(xl,0(~,8, t)xz,x3)[
,-77 ~ 7 _ / -#7 0Oxx
Ox)
v
but x = ¢o(~, 8) + tn(~, 8), so we obtain: J=
n,
+t
×
Using the formula n = ,/x/EG
+t
-
FZ(O(p/O~
×
O(p/08) we get:
J = ffEG - F2(1 - t L G + E N - 2MF tzLN - Mz~ EG - F 2 + EG - Fz J = ~/EG - F2(I - 2Ht + Kt2). (2) A little later it will be shown, that J is always positive. So the inverse mapping is defined and its Jacobian is equal to
/ OXl Oxz Ox3 04 04 04
o ( 4 , . , t) ) =
, \ 0(4, 8, t) i
O×1
O×2
O×3
1
O×
Ox
Ox
Ox
=7 -bT×
= 7 Ox~ Ox2 Ox3 Ot Ot Ot
Ox
Ox
108
T. MATSKEWICH and P. E. SOBOLEVSKII
Further, in the new coordinate system:
(~uy
~ . ~ : ( ~ . y + l~uy + \ax,/
\ax2,/
= \aC/\ax'
\ax3,/
+ \a,7,/kay' ~
+ \ a t } \Ox'
+ 2~-~
+ 2 -~ ~
Ox
+ 2-~-~
' ~x ~x
O~ O~
=
°x+~
~
=~
×~,~×
\~,/~,
+l-#X~
because
~,~
=)~\\~'~J\~'~
-
~'~
\an ~
'
but ,
=
n, ~
and so
+ t
= 0,
(0~ 0,) \ ~ T x =o
and analogously it can be shown, that
~
=0.
So,
1 o ox[ Co.Y
JVu[2 >- ~
~
\-~/
jo ,o: ox, o,j iouy> ;o y
= ()2 \at'~
- \at,/ "
Finally let us note, that in the new coordinate system
and so Statement 2 is proved.
Statement 3. Let us consider point y, belonging to a l l Denote by k I and k 2 the principal curvatures of Of~ in this point. Then (1) I f k 1 or k2 is greater than zero, thenT(y) _< 1/max(kl, k2). (2) In any case, independently on the signs of k~ and k2 for every t e [0; T(y)) J = ~/EG - F2(1 - 2Ht + Kt 2 ) > 0 .
The sharp constant in Hardy's inequality
109
Proof. (1) Let us suppose, that k I > k 2 > 0. Then there exists a n o r m a l section with curvature kl. This section can be obtained as the intersection o f Of2 with some n o r m a l plane, passing t h r o u g h y. We suppose further that in the n o r m a l plane this section can be described as a plane curve by equation r(t) = (0/(0, p(t)); such that y = r(to). Let us show that for every point o f the f o r m x = y + tn(y), where t > 1/kl, there exists m o r e nearer than y points o f this curve, and so such point o f the surface 0f2. Then f r o m the definition o f T(y) the first part o f the statement follows. Really, let us consider point x = y + (1/kl + O)n(y), where ~ > 0. A n d let us denote by H(e) the square o f the distance f r o m this point to the point o f considered curve, sufficiently close to y = r(to): H(e) = distZ(x, r(to + e)), then H(e) = r(to) - r(t o + e) +
+ 6 n(y)
= 2(r(t0) - r(to + e), r(t o) - r(to + e)>
+ 2(~-~a + cY)(r(to) - r(to + e),n(Y)) + ( ~ 1 + ~) 2. It is sufficient to prove, that H ' ( 0 ) = 0 and H"(0) < 0. In fact
H'(e) = - 2 ( r ' ( t o + e), r(t o) - r(t o + e)> > =
-
+
n>
=
+ ~ (r'(t o + e), n>;
O.
H"(e) = - 2 < ( r " ( t o + e), r(t o) - r(t o + e)> + 2(r'(to + e), r'(t o + e)> ¢
H"(O) = 2(r'(to), r'(to)> - 2
+ ~ .
But if r(t) = (0/(0, fl(t)), then curvature o f the curve can be c o m p u t e d by the following formula 1 ((0/,)2 -- =
kI
0/'fl"
+ (flt)2)3/2 -
-
(-~',
> O;
fl'0/" 0/ ')
r/ = ( ( 0 / ' ) 2 + ( , ~ t ) 2 ) 1 / 2 '
~hen
H,,(O)
=
2((0/,)2+(fl,)2)2(_~l -
=2((0/')2+(fl')2)(1-
+ ~
)-0/"fl'+odfl" ((0/,)2 + (fl,)2)1/2
(~1+~)kl)
= -2((or') 2 + (fl')2)~k" 1 < O.
110
T. MATSKEWICH and P. E. SOBOLEVSKII
(2) J = x/EG - F2(1 - 2Ht + Kt 2) = ~/EG - F2(1 - (kl + k2)t + klk2t2). If k I o r ](2 (for example ka) is equal to zero, then J = 1 - kEg and in this case if k 2 <_ 0 then J _> 1; if k2 > 0 then t < T <_ k 2 / 1 and J is again greater than 0. If k~, k 2 ;~ 0 then J = [kl(l/k~ - t ) ] [ k 2 ( l / k 2 - t)]. Let us note that if ki > 0 (i = 1, 2) then t < T <_ l / k i and so [ki(1/ki - t)] is always positive. • 2. E S T I M A T E FROM BELOW FOR lp(u, f2)
N o w let us estimate f r o m below the ratio between inner integrals in the f o r m u l a obtained in Statement 2 when y = ~0({, r/) e Of~ is fixed, i.e. the following ratio will be considered:
I TCv) IOu/OtlP(1 - 2Ht + Kt z) dt I(y) = ~ro~y) [u/tlp(1 _ 2Ht + Kt 2) dt ' where T, H , K are the same as in the previous part, u e C=[0; T], u(0) = 0 and T(y) is denoted by T for m o r e simplicity. Note, that if k~ # 0, k2 # 0, then
I(y) =
I r lau/OtF(t - 1/kl)(t - 1/k2) dt I r lu/tF(t - 1/kl)(t - l/k2) dt
LEMMA la. If kl, k2 < 0 then for p > 3 I(y) >_ ((p - 3)/p) p.
Proof. Really, in this case ( t - 1 / k l ) ( t - 1//<2)= (t + I1/kll)(t + I1/kzl). Let us denote a = [1/k~[, b = [1/k2l, a , b > 0. Then
luF (t
+ a)(t + b ) d t = o
+ a)(t + b ) d t
go
=
tP
ulul p-2
o
d0
+
"t'P
Let us estimate the inner integral:
l r (r + a)(z + b) dz t
Tp .l~l- P
--(r 1-p
+ a)(r + b)lrt -
b)-
+ a)(t + b) +
t a-p (
p-3
+
(p--l-~-
3) + ( a + b ) ( p
r2-p -
tl-P
-,;2-3
rl-P (2z + (a + b ) ) d r
tl-P
tl-p (t+a)(t+ p--1 <_--(t p-1
IT
2
2t 3-p (p - 1)(p - 3)
1)(p
-
2i
t 2-p + (a + b)
(p - l ) ( p - 2)
+ b) + p - 3 "] < t~_P (t + a)(t + b). p - 1 ab/ -p - 3
The sharp constant in Hardy's inequality
111
T h e n using H 6 1 d e r ' s i n e q u a l i t y o n e o b t a i n s :
I T t P(t + a)(t + b ) d t
0
<
3
fTt
p-I
o
P p-3
((t + a)(t +
b))Go+l)/pOu
Ot ((t
(t + a)(t + b ) d t
0
t h a t c o m p l e t e s p r o o f o f the l e m m a .
0
+ a)(t + b)) lip
Ot
(t + a)(t + b) dt
,
•
LEMMA l b . I f k l , k 2 > 0 a n d p > 1 then I(y) > ((p - 1)/py °.
Proof. Really, in this case if we d e n o t e a = 1 / k 1, b -- 1 / k 2, t h e n I(y) =
Sff IOu/Otf(a
- t)(b - t) dt
~r o lu/tlP(a - t)(b - t) dt
a n d f r o m S t a t e m e n t 3 it follows, t h a t T _< min(a, b). In exactly the s a m e w a y as in L e m m a l a we o b t a i n :
0
p( a -
t)(b
-
t)dt
=
i ip ulul "-2 0
.At
rP
F u r t h e r let us n o t e t h a t
0 _<
i
t(a_
r)(b-
r)
t
T 2.1-p
rl-v [r dr = (a -
r)(b -
Tp
r ) ~ 1--//
tl-P <-- (a - t)(b - t ) - p-l'
It
+ t
- -
Jtp-1
(2r - (a + b)) d r
b e c a u s e for every z ~ [t, T) we have 2 r - (a + b) < 0. T h e n L e m m a l c follows f r o m H61der's inequality. •
LEMMA lC. I f kl > 0, k 2 < 0 a n d p > 2 then I(y) >_ ((p - 2)/p) p.
Proof. Let us d e n o t e a = l / k ~ , b = I1/k2[, then
j~ IOu/atlP(a - t)(t + b) dt I(y) = jr° [u/t[P(a _ t)(t + b) dt a n d f r o m S t a t e m e n t 3 it follows t h a t T_< a.
112
T. MATSKEWlCH and P. E. SOBOLEVSKII
Again it is sufficient to obtain the following estimate: 0 <_
i
ra_
r ) ( r + b) dr rp
t
= 1rl---~p -p (a-
r ) ( r + b)ltr -
I 1
t 1-p
<_--(ap-1
t
p
t)(t + b) +
-
1 (a -- t)(t + b) +
~r I (at
p-1
I-p
l
r)r 1-p dr
-
p-1
p-2
liT ) r 2-p dr p-2 t
1
t l-P
t)(t + b) + ( p _
( a - t) t + p - 2 b
p-2
1)(p- 2)(a-
)
p-1
=
k2
=
tl-P
<--(a-
t)t 2-p
t)(t+ b).
p-2
And so Lemma l c is also established. LEMMA ld. If kl
( r + b))l - p
( (a--r)'c2-P ;
t 1-p <-p--- l ( a -
-
T I - p dr
T
t ((a- r)-
•
0 then for every p > 1 I(y) >_ ((p - 1)/p) p.
This lemma immediately follows from the classical one-dimensional Hardy's inequality. LEMMA le. If kl = 0 and k 2 > 0 then for every p > 1 I(y) >_ ((p - 1)/p) p. Proof. Really, for a -- l / k 2 we obtain: z(y) =
fro IOu/OtlP(a - t) dt lfflu/tl(a
o 7 (a - t) dt =
- t) dt
o pulul p-2 ~
\jr
rp dr
at
and exactly as in the previous lemma it is sufficient to estimate f f ((a - r ) / z p) dr in the following way
f Ta-
3t rP r d r -
./.1-p
p-
1
and then we apply H61der's inequality.
I"T rl-P
r)ll- It p------i dr
< tl-P ( a -- p----i --
t),
•
LEMMA lf. I f k I = 0 and k 2 < 0 then for e v e r y p > 2 I(y) >_ ((p - 2)/p) p.
The sharp constant in Hardy's inequality
113
Proof. For a = I1/k2] it is sufficient to obtain the following estimate: -