Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
Transcript of Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
1/144
H A R M O N I C A N A L Y S I S A N D
P A R T I A L D I F F E R E N T I A L E Q U A T I O N S
B J R N E . J . D A H L B E R G
C A R L O S E . K E N I G
I S S N 0 3 4 7 - 2 8 0 9
D E P A R T M E N T O F M A T H E M A T I C S
C H A L M E R S U N I V E R S I T Y O F T E C H N O L O G Y
A N D T H E U N I V E R S I T Y O F G T E B O R G
G T E B O R G 1 9 8 5 / 1 9 9 6
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
2/144
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
3/144
F O R E W O R D
T h e s e l e c t u r e n o t e s a r e b a s e d o n a c o u r s e I g a v e r s t a t U n i v e r s i t y o f T e x a s , A u s t i n
d u r i n g t h e a c a d e m i c y e a r 1 9 8 3 - 1 9 8 4 a n d a t U n i v e r s i t y o f G t e b o r g i n t h e f a l l o f 1 9 8 4 .
M y p u r p o s e i n t h o s e l e c t u r e s w a s t o p r e s e n t s o m e o f t h e r e q u i r e d b a c k g r o u n d i n o r d e r
t o p r e s e n t t h e r e c e n t r e s u l t s o n t h e s o l v a b i l i t y o f b o u n d a r y v a l u e p r o b l e m s i n d o m a i n s
w i t h b a d b o u n d a r i e s . T h e s e n o t e s c o n c e n t r a t e o n t h e b o u n d a r y v a l u e p r o b l e m s f o r t h e
L a p l a c e o p e r a t o r f o r a c o m p l e t e s u r v e y o f r e s u l t s , w e r e f e r t o t h e s u r v e y a r t i c l e b y C a r l o s
K e n i g I a m v e r y g r a t e f u l f o r t h i s k i n d p e r m i s s i o n t o i n c l u d e i t h e r e . I t i s a l s o m y p l e a s u r e
t o a c k n o w l e d g e m y g r a t i t u d e t o P e t e r K u m l i n f o r e x c e l l e n t w o r k i n p r e p a r i n g t h e s e n o t e s
f o r p u b l i c a t i o n .
J a n u a r y 1 9 8 5
B j r n E . J . D a h l b e r g
i
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
4/144
i i
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
5/144
C o n t e n t s
0 I n t r o d u c t i o n 1
1 D i r i c h l e t P r o b l e m f o r L i p s c h i t z D o m a i n . T h e S e t u p 1 1
2 P r o o f s o f T h e o r e m 1 . 1 a n d T h e o r e m 1 . 2 1 9
3 P r o o f o f T h e o r e m 1 . 6 2 5
4 P r o o f o f T h e o r e m 1 . 3 3 7
5 P r o o f o f T h e o r e m 1 . 4 4 7
6 D i r i c h l e t P r o b l e m f o r L i p s c h i t z d o m a i n s . T h e n a l a r g u m e n t s f o r t h e
L
2
- t h e o r y 5 1
7 E x i s t e n c e o f s o l u t i o n s t o D i r i c h l e t a n d N e u m a n n p r o b l e m s f o r L i p s c h i t z
d o m a i n s . T h e o p t i m a l L
p
- r e s u l t s 5 7
I n d e x : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : 6 4
A p p e n d i x 1 C . E . K e n i g : R e c e n t P r o g r e s s o n B o u n d a r y V a l u e P r o b l e m s o n
L i p s c h i t z D o m a i n s : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : 6 7
A p p e n d i x 2 B . E . D a h l b e r g / C . E . K e n i g : H a r d y s p a c e s a n d t h e N e u m a n n
P r o b l e m i n L
p
f o r L a p l a c e ' s e q u a t i o n i n L i p s c h i t z d o m a i n s : : : : : : : : : 1 0 7
i i i
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
6/144
i v
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
7/144
C h a p t e r 0
I n t r o d u c t i o n
I n t h i s c o u r s e w e w i l l s t u d y b o u n d a r y v a l u e p r o b l e m s ( B V P : s ) f o r l i n e a r e l l i p t i c P D E : s
w i t h c o n s t a n t c o e c i e n t s i n L i p s c h i t z - d o m a i n s , i . e . , d o m a i n s w h e r e t h e b o u n d a r y @
l o c a l l y i s g i v e n b y t h e g r a p h o f L i p s c h i t z f u n c t i o n . W e r e c a l l t h a t a f u n c t i o n ' i s L i p s c h i t z
i f t h e r e e x i s t s a c o n s t a n t M
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
8/144
D i r i c h l e t p r o b l e m
u = 0 i n
u = f o n @
N e u m a n n p r o b l e m
u = 0 i n
@ u
@ n
= f o n @
t h e c l a m p e d p l a t e p r o b l e m
8
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
9/144
a n d t h a t
( ) s u p
y > 0
k u ( y ) k
p
k f k
p
T h u s w i t h X = L
p
( R
n
) a n d Y = f u : u h a r m o n i c i n R
n + 1
+
a n d u s a t i s e s ( ) g w e h a v e t h e
i m p l i c a t i o n
f 2 X ) u 2 Y
H o w e v e r , w e c a n a l s o r e v e r s e t h e i m p l i c a t i o n s i n c e a h a r m o n i c f u n c t i o n u w h i c h s a t i s e s
( ) h a s n o n - t a n g e n t i a l l i m i t s a . e . o n @ R
n + 1
+
, t h e l i m i t - f u n c t i o n u
0
= u ( 0 ) 2 L
p
( R
n
) a n d
u ( x y ) = p
y
u
0
( x )
S k e t c h o f a p r o o f . A s s u m e u h a r m o n i c f u n c t i o n i n R
n + 1
+
t h a t s a t i s e s ( ) . T h e s e m i g r o u p
p r o p e r t i e s o f f p
y
g
y 0
i m p l i e s
u ( x y + ) = p
y
u
( x ) > 0 y > 0
w h e r e u
( x ) = u ( x )
( ) ) u
n
* v i n L
p
( R
n
) a s
n
# 0
) p
y
u
n
( x ) ! p
y
v ( x ) a s
n
# 0 y > 0
B u t p
y
u
n
( x ) = u ( x y +
n
) a n d t h u s
u ( x y ) = p
y
v ( x ) w h e r e v 2 L
p
( R
n
)
F o r t h e p r o o f o f t h e e x i s t e n c e o f n o n - t a n g e n t i a l l i m i t s o f p
y
u
0
w e r e f e r t o e . g . S t e i n / W e i s s
2 ] .
T h e n o t i o n o f s o l u t i o n o f t h e D i r i c h l e t p r o b l e m a n d a n y o t h e r p r o b l e m , i s s o u n d o n l y
i f w e h a v e s u c h a m a t c h i n g b e t w e e n t h e b o u n d a r y v a l u e f o f u a n d t h e s o l u t i o n u i t s e l f ,
i . e . , w e s h o u l d n o t a c c e p t c o n c e p t s o f s o l u t i o n w h i c h a r e s o w e a k s u c h t h a t t h e r e v e r s e d
i m p l i c a t i o n i s i m p o s s i b l e .
N o w a s s u m e t h a t i s a b o u n d e d ( c o n n e c t e d ) d o m a i n i n R
n
n 3 w i t h C
2
b o u n d a r y . ( T o
a v o i d t e c h n i c a l i t i e s , w e h a v e a s s u m e d n 6= 2 ) . C o n s i d e r t h e D i r i c h l e t p r o b l e m
( D )
u = 0 i n
u
@
= f 2 C ( @ )
L e t r d e n o t e ( ; 1 ) ( t h e f u n d a m e n t a l s o l u t i o n ) o f t h e L a p l a c e o p e r a t o r i n R
n
, t h a t i s ,
r ( x ) = c
n
1
x
n ; 2
c
n
= ;
1
( 2 ; n ) !
n
;
1
2 ; n
;
( n = 2 )
2
n = 2
3
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
10/144
a n d s e t
R ( x y ) = r ( x ; y )
F o r f 2 C ( @ ) w e d e n e
D f ( P ) =
Z
@
@
@ n
Q
R ( P Q ) f ( Q ) d ( Q ) P =2 @
S f ( P ) =
Z
@
R ( P Q ) f ( Q ) d ( Q ) P =2 @
T h u s D f a n d S f d e n o t e t h e d o u b l e l a y e r p o t e n t i a l a n d s i n g l e l a y e r p o t e n t i a l r e s p . H e r e d
i s t h e s u r f a c e m e a s u r e o n @ a n d
@
@ n
Q
i s t h e d i r e c t i o n a l d e r i v a t i v e a l o n g t h e u n i t o u t w a r d
n o r m a l f o r @ a t Q . I t i s i m m e d i a t e t h a t
D f ( P ) = 0 P 2 R
n
n @
a n d D f w i l l b e o u r c a n d i d a t e f o r s o l u t i o n o f ( D ) . I t r e m a i n s t o s t u d y t h e b e h a v i o u r o f D f
a t @
P a r t o f t h a t s t o r y i s
L e m m a 1 . I f f 2 C ( @ ) , t h e n
1 ) D f 2 C (
)
2 ) D f 2 C ( { )
M o r e p r e c i s e l y : D f c a n b e e x t e n d e d a s a c o n t i n u o u s f u n c t i o n f r o m i n s i d e t o
a n d f r o m
o u t s i d e t o { . L e t D
+
f a n d D
;
f d e n o t e t h e r e s t r i c t i o n s o f t h e s e f u n c t i o n s t o @ r e s p .
S e t K ( P Q ) =
@
@ n
Q
R ( P Q ) f o r P 6= Q P Q 2 @ . W e n o t e t h a t
i ) K 2 C ( @ @ n f ( P P ) : P 2 @ g )
i i ) K ( P Q )
C
P ; Q
n 2
f o r P Q 2 @ a n d s o m e C
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
11/144
S i n c e ' i s a C
2
f u n c t i o n , w e h a v e t h a t
' ( x ) = ' ( y ) + h x ; y r ' ( y ) i + e ( x y ) w h e r e e ( x y ) = O ( x ; y
2
)
H e n c e
K ( P Q ) C
h P ; Q ( r ' ( y ) ; 1 ) i
P ; Q
n
C
e ( x y )
P ; Q
n
C
P ; Q
n ; 2
T h i s e s t i m a t e i s u n i f o r m i n P a n d Q s i n c e @ c o m p a c t .
F o r f 2 C ( @ ) d e n e
T f ( P ) =
Z
@
K ( P Q ) f ( Q ) d ( Q ) P 2 @
W e c a n n o w f o r m u l a t e
L e m m a 2 ( j u m p r e l a t i o n f o r D )
1 ) D
+
=
1
2
I + T
2 ) D
;
= ;
1
2
I + T
a n d
L e m m a 3 . T : C ( @ ) ! C ( @ ) i s c o m p a c t .
S k e t c h o f p r o o f o f L e m m a 3 . D e n e t h e o p e r a t o r s T
n
b y
T
n
f ( P ) =
Z
@
K
n
( P Q ) f ( Q ) d ( Q ) P 2 @
f o r f 2 C ( @ ) , w h e r e
K
n
( P Q ) = s i g n ( K ( P Q ) ) m i n ( n K ( P Q ) ) n 2 Z
+
T h u s K
n
i s c o n t i n u o u s o n @ @ a n d A r z e l a - A s c o l i ' s t h e o r e m i m p l i e s t h a t T
n
i s a c o m p a c t
o p e r a t o r o n C ( @ ) . F u r t h e r m o r e s i n c e k T
n
k s u p
Q 2 @
k K
n
( Q ) k
1
C
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
12/144
P r o o f o f L e m m a 1 a n d 2 . S o m e b a s i c f a c t s :
1 )
Z
@
@
@ n
Q
R ( P Q ) d ( Q ) = 1 , i f P 2
P r o o f : A p p l y G r e e n ' s f o r m u l a t o t h e h a r m o n i c f u n c t i o n R ( ; Q ) i n n B
( P ) f o r
> 0 s m a l l , w h e r e B
( P ) = f x 2 R
n
: P ; x g
2 )
Z
@
@
@ n
Q
R ( P Q ) d ( Q ) = 0 , i f P =2
P r o o f : E x e r c i s e .
3 )
Z
@
K ( P Q ) d ( Q ) =
1
2
, i f P 2 @
P r o o f : E x e r c i s e .
L e t P 2 @ . W e w a n t t o s h o w t h a t
D f ( Q ) !
1
2
f ( P ) + T f ( P ) a s 3 Q ! P
A : A s s u m e P =2 s u p p f : E a s y .
B : A s s u m e f ( P ) = 0 : W e n e e d .
4 ) 9 C > 0 :
Z
@
@
@ n
Q
R ( P Q )
d ( Q ) < C f o r a l l P =2 @
P r o o f : E x e r c i s e .
4 ) i m p l i e s t h e e s t i m a t e
k D f k
L
1
( R
n
n @ )
C k f k
L
1
( @ )
C h o o s e f f
k
g C ( @ ) w i t h P =2 s u p p f
k
s u c h t h a t
k f ; f
k
k
L
1
( @ )
! 0 a s k ! 1
T b o u n d e d o p e r a t o r i m p l i e s T f
k
( P ) ! T f ( P ) a s k ! 1 . H e n c e
D f ( Q ) ; T f ( P ) C k ( f ; f
k
) k
L
1
( R
n
n @ )
+ D f
k
( Q ) ; T f
k
( P ) +
+ T f
k
( P ) ; T f ( P ) ! 0 a s k ! 1 a n d 3 Q ! P
C : E n o u g h t o c h e c k f 1
T h e r e s u l t f o l l o w s f r o m b a s i c f a c t s 1 ) a n d 3 ) . H e n c e w e h a v e p r o v e d L e m m a 1 a n d 2 p a r t
1 ) . P a r t 2 ) f o l l o w s a n a l o g o u s l y .
6
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
13/144
W e n o w r e t u r n t o t h e s i n g l e l a y e r p o t e n t i a l a n d o b s e r v e t h a t S f i s h a r m o n i c i n R
n
n @
a n d c o n t i n u o u s i n R
n
i f f 2 C ( @ ) . N e x t w e w a n t t o c o m p a r e t h e n o r m a l d e r i v a t i v e o f
S f w i t h D f a t @ . S i n c e @ i s C
2
w e h a v e f o l l o w i n g r e s u l t :
F o r " > 0 s m a l l e n o u g h
; " " @ 3 ( t P ) ! P + t n
p
2 V
i s a d i e o m o r p h i s m , w h e r e n
p
i s t h e o u t w a r d u n i t n o r m a l o f @ a t P , a n d V i s a n e i g h -
b o r h o o d o f @ . F o r P 2 @ a n d t 2 ; " " s e t
D S f ( P + t n
p
) =
Z
@
@
@ n
p
R ( P + t n
p
Q ) f ( Q ) d ( Q )
T h e c l o s e r e l a t i o n s b e t w e e n D f a n d D S f i s f o r m u l a t e d i n
L e m m a 4 . I f f 2 C ( @ ) t h e n
1 ) D S f 2 C ( V \ )
2 ) D S f 2 C ( V \ { )
( C o m p a r e L e m m a 1 ) .
L e t D
+
S f b e t h e r e s t r i c t i o n t o @ o f t h e f u n c t i o n D S f e x t e n d e d t o V \ f r o m i n s i d e
a n d D
;
S f t h e r e s t r i c t i o n t o @ o f t h e f u n c t i o n D S f e x t e n d e d t o V \ { f r o m o u t s i d e .
B u t R ( P Q ) = R ( Q P ) s o w i t h R
n
( P Q ) = K ( Q P ) , w h i c h i s t h e r e a l - v a l u e d k e r n e l i n
T
f ( P ) =
Z
@
K
( P Q ) f ( Q ) d ( Q ) P 2 @
w e h a v e t h a t T
i s t h e a d j o i n t o p e r a t o r o f T
L e m m a 5 ( j u m p r e l a t i o n s f o r D S ) 1 ) D
+
S = ;
1
2
I + T
2 ) D
;
S =
1
2
I + T
P r o o f o f L e m m a 4 a n d 5 . L e t f 2 C ( @ ) a n d d e n e
w
f
( P ) =
D f ( P ) + D S f ( P ) P 2 V n @
T f ( P ) + T
f ( P ) P 2 @
C l a i m : w
f
2 C ( V )
P r o o f : w
f
c o n t i n u o u s o n V n @ a n d o n @ . H e n c e i t i s e n o u g h t o s h o w t a h t
w
f
( P + t n
p
) ! w
f
( P ) u n i f o r m l y f o r P 2 @ a s t ! 0
7
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
14/144
A s s u m e
0
2 C ( @ ) s u c h t h a t 0
0
1
0
= 1 i n a n e i g h b o r h o o d o f P a n d
s u p p
0
B
( P )
D e c o m p o s e f a s
f = f
1
+ f
2
0
f + ( 1 ;
0
) f
A : w
f
2
( P + t n
p
) ! w
f
2
( P ) a s t ! 0 . E a s y
B : A s s u m e t 6= 0
0 0 0 0 0 0 0 0 0 0 0 0 0 0
0 0 0 0 0 0 0 0 0 0 0 0 0 0
0 0 0 0 0 0 0 0 0 0 0 0 0 0
0 0 0 0 0 0 0 0 0 0 0 0 0 0
0 0 0 0 0 0 0 0 0 0 0 0 0 0
0 0 0 0 0 0 0 0 0 0 0 0 0 0
0 0 0 0 0 0 0 0 0 0 0 0 0 0
0 0 0 0 0 0 0 0 0 0 0 0 0 0
0 0 0 0 0 0 0 0 0 0 0 0 0 0
0 0 0 0 0 0 0 0 0 0 0 0 0 0
0 0 0 0 0 0 0 0 0 0 0 0 0 0
0 0 0 0 0 0 0 0 0 0 0 0 0 0
0 0 0 0 0 0 0 0 0 0 0 0 0 0
0 0 0 0 0 0 0 0 0 0 0 0 0 0
1 1 1 1 1 1 1 1 1 1 1 1 1 1
1 1 1 1 1 1 1 1 1 1 1 1 1 1
1 1 1 1 1 1 1 1 1 1 1 1 1 1
1 1 1 1 1 1 1 1 1 1 1 1 1 1
1 1 1 1 1 1 1 1 1 1 1 1 1 1
1 1 1 1 1 1 1 1 1 1 1 1 1 1
1 1 1 1 1 1 1 1 1 1 1 1 1 1
1 1 1 1 1 1 1 1 1 1 1 1 1 1
1 1 1 1 1 1 1 1 1 1 1 1 1 1
1 1 1 1 1 1 1 1 1 1 1 1 1 1
1 1 1 1 1 1 1 1 1 1 1 1 1 1
1 1 1 1 1 1 1 1 1 1 1 1 1 1
1 1 1 1 1 1 1 1 1 1 1 1 1 1
1 1 1 1 1 1 1 1 1 1 1 1 1 1
P
t
= P + t n
P
P
t
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
15/144
T h e r e f o r e
T f ( P ) + T
f ( P ) = D
+
f ( P ) + D
+
S f ( P ) = D
;
f ( P ) + D
;
S f ( P ) P 2 @
T h e j u m p r e l a t i o n s f o r D S f o l l o w .
W e n o w g i v e t h e n a l a r g u m e n t f o r t h e e x i s t e n c e o f a s o l u t i o n o f t h e D i r i c h l e t p r o b l e m i n
a n d t h a t i s
D
+
: C ( @ ) ! C ( @ )
i s o n t o .
S i n c e D
+
=
1
2
I + T , w h e r e T i s c o m p a c t , F r e d h o l m ' s A l t e r n a t i v e t h e o r e m c a n b e a p p l i e d .
H e n c e ,
1
2
I + T = D
+
o n t o
i
1
2
I + T
= D
;
S 1 ; 1
T o p r o v e D
;
S i s 1 ; 1 i s e a s y :
A s s u m e D
;
S f = 0 f o r s o m e f 2 C ( @ ) . S e t v = S f . T h e n
i ) v h a r m o n i c i n {
i i ) v ( P ) = O ( P
2 ; n
) a s P ! 1
i i i )
@ v
@ n
@
= 0
G r e e n ' s f o r m u l a i m p l i e s
Z
{
r v
2
=
Z
{
v v +
Z
@
v
@ v
@ n
d = 0
T h u s v = 0 i n {
. B u t v 2 C ( R
n
) a n d v = 0 i n
M a x i m u m p r i n c i p l e ) v = 0 i n R
n
) f = 0
R e m a r k : T h e p r o o f a b o v e i s v a l i d f o r d o m a i n s w i t h C
1 +
b o u n d a r i e s w h e r e > 0 , b u t
n o t f o r d o m a i n s w i t h b o u n d a r i e s w i t h l e s s r e g u l a r i t y .
R e m a r k : W e o b s e r v e t h a t t h e m e t h o d i s n o n - c o n s t r u c t i v e a s a c o n s e q u e n c e o f t h e s o f t
a r g u m e n t s ( i . e . , c o m p a c t n e s s a r g u m e n t s ) w e h a v e u s e d . H e n c e i t i s n o t p o s s i b l e t o s o l v e
t h e D i r i c h l e t p r o b l e m f o r , s a y L i p s c h i t z - d o m a i n s b y a p p r o x i m a t i n g w i t h C
2
d o m a i n s
k
, s o l v e s o m e D i r i c h l e t p r o b l e m s f o r t h e s e a n d o b t a i n a n a p p r o x i m a t i o n o f a s o l u t i o n f o r
, s i n c e w e d o n o t h a v e a n y e s t i m a t e s o f t h e i n v e r s e s o f t h e D
+
: s
9
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
16/144
R e f e r e n c e s
1 ] F o l l a n d , G : I n t r o d u c t i o n t o p a r t i a l d i e r e n t i a l e q u a t i o n s . M a t h . N o t e s 1 7 , P r i n c e t o n
U . P .
2 ] S t e i n , E . M . / W e i s s , G : I n t r o d u c t i o n t o F o u r i e r A n a l y s i s o n E u c l i d e a n S p a c e s . P r i n c e -
t o n U . P .
1 0
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
17/144
C h a p t e r 1
D i r i c h l e t P r o b l e m f o r L i p s c h i t z
D o m a i n . T h e S e t u p
A f u n c t i o n ' : R
n
! R s u c h t h a t
' ( x ) ; ' ( y ) M x ; y f o r a l l x y 2 R
n
i s c a l l e d L i p s c h i t z f u n c t i o n . A b o u n d e d d o m a i n R
n + 1
i s c a l l e d L i p s c h i t z d o m a i n i f @
c a n b e c o v e r e d b y n i t e l y m a n y r i g h t c i r c u l a r c y l i n d e r s L w h o s e b a s e s a r e a t a p o s i t i v e
d i s t a n c e f r o m @ s u c h t h a t t o e a c h c y l i d e r L t h e r e i s a L i p s c h i t z f u n c t i o n ' : R
n
! R a n d
a c o o r d i n a t e s y s t e m ( x y ) x 2 R
n
y 2 R s u c h t h a t t h e y - a x i s i s p a r a l l e l t o t h e a x i s o f
s y m m e t r y o f L a n d L \ = L \ f ( x y ) : y > ' ( x ) g a n d L \ @ = L \ f ( x y ) : y = ' ( x ) g
A d o m a i n D R
n + 1
i s c a l l e d s p e c i a l L i p s c h i t z d o m a i n i f t h e r e i s a L i p s c h i t z f u n c t i o n
' : R
n
! R s u c h t h a t D = f ( x y ) : y > ' ( x ) g a n d @ D = f ( x y ) : y = ' ( x ) g . I n t h i s a n d
a l l p r o c e e d i n g c h a p t e r s w e r e s e r v e t h e n o t a t i o n f o r b o u n d e d L i p s c h i t z d o m a i n s a n d D
f o r s p e c i a l L i p s c h i t z d o m a i n s r e s p e c t i v e l y . W i t h a c o n e ; w e m e a n a c i r c u l a r c o n e w h i c h
i s o p e n . A c o n e ; w i t h v e r t e x a t a p o i n t P 2 @ C , w h e r e C R
n + 1
i s a d o m a i n , i s c a l l e d
a n o n t a n g e n t i a l c o n e i f t h e r e i s a c o n e ;
0
a n d a > 0 s u c h t h a t
6= (
; \ B
( P ) ) n f P g ;
0
\ B
( P ) C
B
r
( Q ) i s o u r s t a n d a r d n o t a t i o n f o r t h e b a l l f x 2 R
n
: x ; Q r g . W e s a y t h a t a f u n c t i o n
u d e n e d i n a d o m a i n C h a s n o n t a n g e n t i a l l i m i t L a t a p o i n t P 2 @ C i f
u ( Q ) ! L a s Q ! P Q 2 ;
f o r a l l n o n t a n g e n t i a l c o n e s ; w i t h v e r t i c e s a t P . F i n a l l y w e d e n e t h e n o n t a n g e n t i a l
m a x i m a l f u n c t i o n M
u f o r > 1 a n d f u n c t i o n u d e n e d i n L i p s c h i t z d o m a i n b y
M
u ( P ) = s u p f u ( Q ) : P ; Q < d i s t ( Q @ ) Q 2 g P 2 @
1 1
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
18/144
O n e o f t h e m a i n r e s u l t s i n t h i s c o u r s e w i l l b e t h e e x i s t e n c e o f a s o l u t i o n t o t h e D i r i c h l e t
p r o b l e m
u = 0 i n R
n + 1
u
@
= f 2 L
2
( @ )
w h e r e i s a b o u n d e d L i p s c h i t z d o m a i n . B y t h i s w e m e a n t h a t t h e r e e x i s t s a h a r m o n i c
f u n c t i o n u i n w h i c h c o n v e r g e s n o n t a n g e n t i a l l y t o f a l m o s t e v e r y w h e r e w i t h r e s p e c t t o
t h e s u r f a c e m e a s u r e d ( @ ) a n d t h a t t h e m a x i m a l f u n c t i o n M
u 2 L
2
( @ ) f o r > 1 . T h e
s t a r t i n g p o i n t f o r o u r e n t e r p r i s e o f p r o v i n g t h e e x i s t e n c e o f a s o l u t i o n t o D i r i c h l e t p r o b l e m
f o r t h e L i p s c h i t z d o m a i n i s t h e d o u b l e l a y e r p o t e n t i a l
D g ( P ) =
Z
@
@
@ n
Q
R ( P Q ) g ( Q ) d ( Q ) P 2
w h e r e R ( P Q ) i s t h e f u n d a m e n t a l s o l u t i o n f o r L a p l a c e e q u a t i o n i n R
n + 1
( m u l t i p l i e d w i t h
; 1 ) a n d g 2 L
2
( @ ) . S i n c e D g i s h a r m o n i c i n , w e a r e d o n e i f w e c a n s h o w t h a t
f o r s o m e c h o i c e o f g w e h a v e t h e r i g h t b e h a v i o u r o f D g a t @ . H o w e v e r , t h i s i s n o t
e a s y s i n c e f o r K ( P Q ) =
@
@ n
Q
R ( P Q ) P Q 2 @ P 6= Q , w e o n l y h a v e t h e e s t i m a t e
K ( P Q )
C
P ; Q
n 1
w h i c h c a n n o t b e i m p r o v e d i n g e n e r a l . T h u s w e h a v e t o r e l y o n t h e
c a n c e l l a t i o n p r o p e r t i e s o f K ( P Q ) , a n d t h e o p e r a t o r T w h i c h a p p e a r e d i n C h a p t e r 0 c a n
o n l y b e d e n e d a s a p r i n c i p a l v a l u e o p e r a t o r . B e f o r e w e s t u d y t h e c a s e w i t h a g e n e r a l
b o u n d e d L i p s c h i t z d o m a i n w e t r e a t t h e c a s e w i t h a s p e c i a l L i p s c h i t z d o m a i n D . F r o m
t h i s w e o b t a i n t h e r e s u l t f o r u s i n g s t a n d a r d p a t c h i n g t e c h n i q u e s ( s e e A p p e n d i x 2 ) .
C o n s i d e r
D g ( P ) =
Z
@ D
@
@ n
Q
R ( P Q ) g ( Q ) d ( Q ) P 2 D
w h e r e D = f ( x y ) : y > ' ( x ) g f o r a L i p s c h i t z f u n c t i o n ' : R
n
! R . W e r e m a r k t h a t
' L i p s c h i t z f u n c t i o n i m p l i e s t h a t '
0
e x i s t s a . e . s o t h e d e n i t i o n o f D g m a k e s s e n s e a n d
@
@ n
Q
R ( P Q ) = C
n
h n
Q
P ; Q i
P ; Q
n + 1
, w i t h n
Q
=
( r ' ( x ) ; 1 )
p
r ' ( x )
2
+ 1
f o r Q = ( x ' ( x ) ) , e x i s t s a . e .
d ( @ D ) . T o s t a t e t h e r s t p r o p o s i t i o n , w e n e e d s o m e m o r e n o t a t i o n : F o r e v e r y m e a s u r e
a n d e a c h - m e a s u r a b l e f u n c t i o n g a n d m e a s u r a b l e s e t A w i t h ( A ) 6= 0 w e l e t
R
A
g d ,
d e n o t e t h e m e a n v a l u e
1
( A )
Z
A
g d . F u r t h e r m o r e f o r g 2 L
1
o c
( @ D ) w e d e n e t h e m a x i m a l
f u n c t i o n M g b y
M g ( P ) = s u p
r > 0
Z
@ D \ B
r
( P )
g ( Q ) d ( Q ) P 2 @ D
T h e f o l l o w i n g r e s u l t i s c r u c i a l .
1 2
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
19/144
P r o p o s i t i o n 1 . 1 . L e t D = f ( x y ) : y > ' ( x ) g w h e r e ' : R
n
! R i s a L i p s c h i t z f u n c t i o n
w i t h k '
0
k
1
= A . L e t P = ( x y ) 2 D a n d P
2 ( x ' ( x ) ) 2 @ D a n d s e t = y ; ' ( x )
A s s u m e g 2 L
p
( @ D ) f o r s o m e p w h e r e 1 < p 0 s u c h t h a t
f x : M g ( x ) > g C
k g k
1
f o r a l l g 2 L
1
5 ) M i s b o u n d e d i n L
p
1 < p 0 s u c h t h a t
k M g k
p
C
p
k g k
p
f o r a l l g 2 L
p
H e r e 3 ) i s t r i v i a l , 4 ) c a n b e p r o v e n b y a c o v e r i n g l e m m a a r g u m e n t a n d 5 ) f o l l o w s f r o m 3 ) ,
4 ) a n d M a r c i n k i e w i c z ' i n t e r p o l a t i o n t h e o r e m ( s e e S t e i n 1 ] ) . F o r l a t e r r e f e r e n c e w e s t a t e
1 3
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
20/144
M a r c i n k i e w i c z ' i n t e r p o l a t i o n t h e o r e m . L e t 1 p < q 1 a n d l e t T b e a s u b a d -
d i t i v e o p e r a t o r d e n e d o n L
p
+ L
q
. A s s u m e T i s a w e a k ( p p ) o p e r a t o r a n d a w e a k ( q q )
o p e r a t o r . T h e n T i s b u n d e d o n L
r
w h e r e p < r < q . A n o p e r a t o r T i s a w e a k ( p p )
o p e r a t o r i f t h e r e e x i s t s a c o n s t a n t C > 0 s u c h t h a t
f x : T g ( x ) > g C
;
k g k
p
p
f o r a l l g 2 L
p
a n d > 0
H e n c e , i f T i s b o u n d e d o n L
p
, t h e n T i s a w e a k ( p p ) o p e r a t o r , b u t t h e c o n v e r s e i s n o t t r u e
i n g e n e r a l .
P r o o f o f P r o p o s i t i o n 1 . 1 .
0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0
0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0
0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0
0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0
0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0
0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0
0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0
0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0
0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0
0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0
0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0
0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0
0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0
0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
P
D
P
D g ( P ) ; T
g ( P
) C
Z
@ D \ f P
; Q > g
h n
Q
P ; Q i
P ; Q
n + 1
;
h n
Q
P
; Q i
P
; Q
n + 1
g ( Q ) d
+ C
Z
@ D n f P
; Q > g
h n
Q
P ; Q i
P ; Q
n + 1
g ( Q ) d ( Q )
C
Z
@ D \ f P
; Q > g
( + Q ; P
)
n + 1
g ( Q ) d ( Q ) +
+ C
Z
@ D n f P
; Q > g
1
n
g ( Q ) d ( Q )
w h e r e w e h a v e a p p l i e d t h e m e a n v a l u e t h e o r e m t o t h e r s t i n t e g r a l . T h e s e c o n d i n t e g r a l i s
C M g ( P
) a n d t h e r s t i n t e g r a l c a n a l s o b e e s t i m a t e d f r o m a b o v e w i t h t h e s a m e b o u n d
a c c o r d i n g t o
L e m m a 1 . 1 . L e t 0 b e a r a d i a l d e c r e a s i n g f u n c t i o n d e n e d i n R
n
. A s s u m e f 2 L
1
+ L
1
a n d s e t m f ( x ) = s u p
r > 0
R
B
r
( x )
f ( x ) d x f o r x 2 R
n
. T h e n f ( x ) B m f ( x ) f o r a l l x 2 R
n
w h e r e B =
R
( x ) d x
1 4
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
21/144
I f w e t a k e t h i s l e m m a f o r g r a n t e d f o r a m o m e n t a n d s e t
( x ) =
( x + )
n + 1
t h e r s t i n t e g r a l a b o v e i s b o u n d e d f r o m a b o v e b y C M g ( P
) a n d w e a r e d o n e .
P r o o f o f L e m m a 1 . 1 . I t i s e n o u g h t o p r o v e t h e l e m m a f o r 0 f 2 C
1
0
2 C
1
0
a n d x = 0
S e t S
n
= @ B
1
( 0 ) a n d A ( r ) =
R
B
r
( 0 )
f ( x ) d x
W e o b t a i n
f ( 0 ) =
Z
R
n
( x ) f ( x ) d x =
Z
1
0
( r ) r
n ; 1
Z
S
n
f ( r w ) d ( w ) d r =
=
Z
1
0
( r ) A
0
( r ) d r = ;
Z
1
0
0
( r ) A ( r ) d r ;
Z
1
0
0
( r ) B
r
( 0 ) d r m f ( 0 )
S e t f 1 i n t h e c a l c u l a t i o n s a b o v e a n d w e g e t ;
R
1
0
0
( r ) B
r
( 0 ) d r = B . T h e l e m m a i s
p r o v e n .
I f w e d e n e t h e o p e r a t o r T
b y
T
g ( P
) = s u p
> 0
T
g ( P
) P
2 @ D
f o r g 2 L
p
( @ D ) , t h e n
D g ( P ) C ( T
g ( P
) + M g ( P
) )
f o r a l l P = ( x y ) 2 D a n d P
= ( x ' ( x ) ) 2 @ D . T h u s i f w e c a n p r o v e t h a t T
i s b o u n d e d
o n L
p
( @ D ) , t h e n D g ( P
) 0 a n d T
. T h i s c a l l s f o r s o m e d e n i t i o n s . L e t S ( R
n
) d e n o t e
t h e S c h w a r t z c l a s s ( i . e . , t h e s p a c e o f a l l C
1
- f u n c t i o n s i n R
n
w h i c h t o g e t h e r w i t h a l l t h e i r
d e r i v a t i v e s d i e o u t f a s t e r t h a n a n y p o w e r o f x a t i n n i t y ) w i t h t h e u s u a l t o p o l o g y .
T i s c a l l e d a s i n g u l a r i n t e g r a l o p e r a t o r ( S I O ) i f T : S ( R
n
) ; ! S ( R
n
)
i s l i n e a r a n d
c o n t i n u o u s a n d t h e r e e x i s t s a k e r n e l K s u c h t h a t f o r a l l ' , 2 C
1
0
( R
n
) w i t h s u p p ' \
s u p p =
h T ' i =
Z Z
K ( x y ) ' ( y ) ( x ) d y d x
1 5
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
22/144
w h e r e h i i s t h e u s u a l S ; S
p a r i n g . W e o b s e r v e t h a t K d o e s n o t d e t e r m i n e T u n i q u e l y .
C o n s i d e r f o r i n s t a n c e T f = f
0
f o r w h i c h K = 0 i s a k e r n e l .
W e s a y t h a t a k e r n e l K i s o f C a l d e r n - Z y g m u n d t y p e ( C Z - t y p e ) i f
1 ) K ( x y )
C
x ; y
n
2 ) r
x
K ( x y ) + r
y
K ( x y )
C
x ; y
n + 1
3 ) K ( x y ) = ; K ( y x )
T h e o p e r a t o r - k e r n e l s , w e w i l l s t u d y , w i l l b e o f t h e f o r m
K
i
( x y ) =
( ( x ' ( x ) ) ; ( y ' ( y ) ) )
i
( x ' ( x ) ) ; ( y ' ( y ) )
n + 1
i = 1 2 : : : n + 1
w h e r e ( a )
i
d e n o t e s t h e i - t h c o m p o n e n t o f a 2 R
n + 1
W e o b s e r v e t h a t t h e s e k e r n e l s a r e o f C Z - t y p e a n d a d o p t t h e c o n v e n t i o n t h a t w h e n e v e r
w e d i s c u s s k e r n e l s K , t h e y a r e a s s u m e d t o b e o f C Z - t y p e u n l e s s w e e x p l i c i t l y s t a t e t h e
c o n v e r s e . S t a r t i n g w i t h a k e r n e l K , w e c a n f o r m a w e l l - d e n e d S I O w i t h K a s t h e k e r n e l
n a m e l y t h e p r i n c i p a l v a l u e o p e r a t o r ( P V O ) T . N o t e t h a t f o r ' 2 S ( R
n
) )
Z Z
x ; y > "
K ( x y ) ' ( y ) ( x ) d y d x =
1
2
Z Z
x ; y > "
K ( x y ) ( ' ( y ) ( x ) ; ' ( x ) ( y ) ) d y d x
s i n c e K ( x y ) = ; K ( y x ) a n d t h u s
l i m
" ! 0
Z Z
x ; y > "
K ( x y ) ' ( y ) ( x ) d y d x
e x i s t s s i n c e ' ( y ) ( x ) ; ' ( x ) ( y ) = O ( x ; y ) a n d ' 2 S ( R
n
) d e c a y f a s t e n o u g h a t
i n n i t y .
H e n c e T : S ( R
n
) 3 ' ! T ' 2 S ( R
n
)
w h e r e
h T ' i = l i m
" ! 0
Z Z
x ; y > "
K ( x y ) ' ( y ) ( x ) d y d x
i s a S I O .
W e l e a v e t h e p r o o f o f c o n t i n u i t y o f T a s a n e x e r c i s e . F r o m n o w o n w e a s s u m e t h a t a l l
o p e r a t o r s T a r e P V O w i t h k e r n e l s K o f C Z - t y p e .
T o a c h i e v e o u r g o a l t o e s t a b l i s h t h e e x i s t e n c e o f a s o l u t i o n t o t h e D i r i c h l e t p r o b l e m f o r
L i p s c h i t z d o m a i n s , w e w i l l p r o v e t h e f o l l o w i n g s e q u e n c e o f t h e o r e m s
T h e o r e m 1 . 1 . I f T b o u n d e d o n L
2
, t h e n T i s a w e a k ( 1 1 ) o p e r a t o r .
T h i s i m p l i e s
1 6
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
23/144
T h e o r e m 1 . 1 ' . I f T b o u n d e d o n L
2
, t h e n T b o u n d e d o n L
p
f o r 1 < p
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
24/144
1 8
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
25/144
C h a p t e r 2
P r o o f s o f T h e o r e m 1 . 1 a n d T h e o r e m
1 . 2
W e r e c a l l t h a t T i s a P V O w i t h k e r n e l K o f C Z - t y p e . I n t h i s c h a p t e r w e g i v e a p r o o f o f
t h e f o l l o w i n g r e s u l t o f C a l d e r n - Z y g m u n d 1 ] .
T h e o r e m 1 . 1 : I f T b o u n d e d o n L
2
, t h e n T i s a w e a k ( 1 1 ) o p e r a t o r .
T h e f o l l o w i n g b o u n d o n T
i s d u e t o C o t l a r 3 ] .
T h e o r e m 1 . 2 : I f T b o u n d e d o n L
2
, t h e n T
i s b o u n d e d o n L
p
f o r 1 < p 0
s u c h t h a t
f x 2 R
n
: T f ( x ) > g C
k f k
1
f o r a l l f 2 L
1
a n d > 0
b y s p l i t t i n g f i n a g o o d p a r t g , w h i c h i s a L
2
- f u n c t i o n a n d a b a d p a r t b . T h i s i s d o n e w i t h
t h e f o l l o w i n g l e m m a
L e m m a ( C a l d e r n - Z y g m u n d d e c o m p o s i t i o n ) . L e t f 2 L
1
( R
n
) a n d > 0 . T h e n
t h e r e e x i s t c u b e s Q
j
j = 1 2 : : : s u c h t h a t
1 ) Q
j
\ Q
k
= 0 f o r j 6= k
2 ) f ( x ) a . e . f o r x 2 R
n
n
1
j = 1
Q
j
1 9
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
26/144
3 )
R
Q
j
f ( x ) d x g j j f x 2 R
n
: T g ( x ) >
2
g + f x 2 R
n
: T b ( x ) >
2
g
f x 2 R
n
: T g ( x ) >
2
g +
1
j = 1
2 Q
j
+ f x 2 R
n
n
1
j = 1
2 Q
j
: T b ( x ) >
2
g
w h e r e 2 Q
j
i s t h e c u b e w i t h t h e s a m e c e n t e r a s Q
j
, w h i c h w e d e n o t e y
j
, w i t h s i d e s p a r a l l e l
w i t h Q
j
a n d w i t h d o u b l e d s i d e l e n g t h s c o m p a r e d w i t h Q
j
. H e r e
f x 2 R
n
: T g ( x ) >
2
g
4
2
k T g k
2
C
2
k g k
2
C
1
k f k
1
a n d
1
j = 1
2 Q
j
2
n
1
X
j = 1
Q
j
2
n
k f k
1
s o i t r e m a i n s t o e s t i m a t e f x 2 R
n
n
1
j = 1
2 Q
j
: T b ( x ) >
2
g a n d t h i s i s t h e p o i n t w h e r e
w e u s e t h e p r o p e r t i e s o f t h e k e r n e l K . S e t
b
j
( x ) =
b ( x ) x 2 Q
j
0 o t h e r w i s e
F o r , x =2 2 Q
j
w e h a v e
T b
j
( x ) =
Z
Q
j
( K ( x y ) ; K ( x y
j
) ) b
j
( y ) d y
2 0
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
27/144
a n d t h u s
T b
j
( x ) C
Z
Q
j
y ; y
j
x ; y
n + 1
b
j
( y ) d y
w h e r e w e u s e d
Z
Q
j
b
j
( y ) d y = 0 . I n t e g r a t i n g t h e s e i n e q u a l i t i e s g i v e s
Z
R
n
n
1
j = 1
2 Q
j
T b ( x ) d x
1
X
j = 1
Z
R
n
n 2 Q j
T b
j
( x ) d x
C
1
X
j = 1
Z
Q
j
b
j
( y ) d y = C k b k
1
C k f k
1
a n d c o n s e q u e n t l y
f x 2 R
n
n
1
j = 1
2 Q j : T b ( x ) >
2
g
2
k T b k
L
1
( R
n
n
1
j = 1
2 Q j )
C
k f k
1
T h e p r o o f i s d o n e .
C o r o l l a r y : I f T i s b o u n d e d o n L
2
, t h e n T i s b o u n d e d o n L
p
f o r 1 < p
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
28/144
a n d f
2
( x ) = f ( x ) ; f
1
( x ) . T h u s T
"
f ( 0 ) = T f
2
( 0 ) . T h e s t r a t e g y i s t o p r o v e t h a t f o r x "
"
y
n + 1
f ( y ) d y C
Z
m i n
;
"
y
n + 1
"
; n
f ( y ) d y C M f ( 0 )
f o r x
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
29/144
R e f e r e n c e s
1 ] A . P . C a l d e r o n / A . Z y g m u n d : O n t h e e x i s t e n c e o f c e r t a i n s i n g u l a r i n t e g r a l s , A c t a
M a t h . 8 8 ( 1 9 5 2 ) p p . 8 5 - 1 3 9 .
2 ] E . M . S t e i n : S i n g u l a r i n t e g r a l s a n d d i e r e n t i a b i l i t y p r o p e r t i e s o f f u n c t i o n s . P r i n c e t o n
U n i v e r s i t y P r e s s 1 9 7 0 .
3 ] M . C o t l a r : S o m e g e n e r a l i z a t i o n s o f t h e H a r d y - L i t t l e w o o d m a x i m a l t h e o r e m R e v .
M a t . C u y a n a 1 ( 1 9 5 5 ) p p . 8 5 - 1 0 4 .
2 3
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
30/144
2 4
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
31/144
C h a p t e r 3
P r o o f o f T h e o r e m 1 . 6
W e b e g i n t h i s s e c t i o n b y i n t r o d u c i n g s o m e o f t h e t o o l s w e n e e d t o p r o v e t h e L
2
- b o u n d e d n e s s
o f T
B M O
p
( R
n
) : F o r f 2 L
1
o c
( R
n
) w e s e t
k f k
p
= s u p
Q c u b e
;
Z
Q
f ( x ) ; f
Q
p
d x
1
p
1 p
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
32/144
a n d w i t h r a t i o n a l s i d e l e n g t h s . S e t E =
j
@ Q
j
. F o r e a c h p a i r ( x
1
x
2
) 2 ( R
n
n E ) ( R
n
n E )
c h o o s e a c u b e Q 2 f Q
j
g s u c h t h a t x
1
x
2
2 Q . S e t f
1
= f
2 Q
a n d f
2
= f ; f
1
. D e n e
F ( x
1
x
2
) = T f
1
( x
1
) ; T f
1
( x
2
) +
Z
R
n
( K ( x
1
y ) ; K ( x
2
y ) ) f
2
( y ) d y
W e n o t e t h a t F i s d e n e d a . e . a n d t h a t F i s i n d e p e n d e n t o f Q ( a s l o n g a s x
1
x
2
2 Q )
C h e c k i t ! F u r t h e r m o r e , f o r a . e . x
1
2 R
n
a n d x
2
2 R
n
F ( x x
1
) ; F ( x x
2
) i s a c o n s t a n t
( r e g a r d e d a s a f u n c t i o n o f x ) . W e n o w d e n e T f a s t h e c l a s s x ! F ( x x
1
) f o r a . e . x
1
2 R
n
I t r e m a i n s t o s h o w t h a t T : L
1
! B M O i s b o u n d e d . I t i s e n o u g h t o s h o w t h a t
Z
Q
F ( x x
Q
) ; T f
1
( x
Q
) d x C k f k
L
1
f 2 L
1
( R
n
)
f o r a l l c u b e s Q 2 f Q
j
g
B u t
Z
Q
T f
1
( x ) d x (
Z
Q
T f
1
( x )
2
d x )
1 = 2
C (
Z
Q
f
1
( x )
2
d x )
1 = 2
C k f k
1
s i n c e
Z
R
n
( K ( x y ) ; K ( x
Q
y ) ) f
2
( y ) d y
Z
R
n
n 2 Q
K ( x y ) ; K ( x
Q
y ) f ( y ) d y
C
Z
R
n
n 2 Q
x ; x
Q
y ; x
Q
n + 1
d y k f k
1
C k f k
1
f o r x 2 Q
T h e p r o p o s i t i o n f o l l o w s .
F a c t 2 : J o h n - N i r e n b e r g i n e q u a l i t y
T h e o r e m : L e t ' 2 B M O ( R
n
) . T h e n t h e r e e x i s t s c o n s t a n t s , C > 0 > 0 , d e p e n d i n g
o n l y o n n , s u c h t h a t
f x 2 Q : ' ( x ) ; '
Q
> g C Q e x p
;
;
k ' k
f o r a l l > 0 a n d c u b e s Q
S k e t c h o f a p r o o f . I t i s e n o u g h t o s h o w t h a t
s u p
Q c u b e
Z
Q
e x p
;
k ' k
' ( x ) ; '
Q
d x C
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
33/144
A s s u m e k ' k
= 1 a n d ' 2 L
1
. S i n c e t h e c o n s t a n t s C a n d w i l l b e i n d e p e n d e n t o f k ' k
1
,
t h e r e s u l t f o l l o w s f o r a g e n e r a l ' . F i x a c u b e Q . C o n s i d e r a l l c u b e s Q
j
i n t h e d y a d i c m e s h
o f Q a n d c h o o s e a t > 1 . L e t
~
Q
j
d e n o t e t h o s e d y a d i c c u b e s w h i c h a r e m a x i m a l w i t h r e s p e c t
t o i n c l u s i o n s a t i s f y i n g
Z
~
Q
j
' ( x ) ; '
Q
d x > t
a n d
' ( x ) ; '
Q
t a . e . f o r x 2 Q n
1
j = 1
~
Q
j
C l e a r l y
~
Q
j
Q a n d
1
j = 1
~
Q
j
1
t
k ' ; '
Q
k
L
1
( Q )
1
t
Q
T h e m a x i m a l i t y o f
~
Q
j
i m p l i e s t h a t
Z
Q
j
' ( x ) ; '
Q
d x t
w h e r e
Q
j
i s t h e m i n i m a l c u b e i n t h e d y a d i c m e s h o f Q w i t h r e s p e c t t o i n c l u s i o n f o r w h i c h
~
Q
j
6
Q
j
. F u r t h e r m o r e
Q
Q
j
~
Q
j
'
~
Q
j
; '
Q
'
~
Q
j
; '
Q
j
+ '
Q
j
; '
Q
Z
~
Q
j
' ( x ) ; '
Q
j
d x + t
2
n
Z
Q
j
' ( x ) ; '
Q
j
d x + t
( 2
n
+ 1 ) t
S e t X ( Q ) = s u p
Q
j
2 d y a d i c m e s h o f Q
R
Q
j
e x p ( ' ( x ) ; '
Q
j
) d x w h i c h i s
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
34/144
T a k e s u p r e m u m o v e r a l l c u b e s Q . T h u s
s u p
Q c u b e
X ( Q ) 1 ;
1
t
e x p ( t ( 2
n
+ 1 ) ) ] e
t
w h i c h i m p l i e s s u p
Q c u b e
X ( Q ) C i f > 0 s m a l l e n o u g h . T h e p r o o f i s d o n e .
R e m a r k : I t i s a n e a s y c o n s e q u e n c e o f J o h n - N i r e n b e r g ' s i n e q u a l i t y t h a t t h e n o r m s k k
p
a n d k k
k k
1
a r e e q u i v a l e n t f o r 1 < p 0 s u c h t h a t x
p
C e x p ( x ) f o r
x > 0 . C h o o s e =
2
a n d a p p l y t h e i n e q u a l i t y a b o v e . H e n c e
k
'
k ' k
k
p
C s u p
Q c u b e
Z
Q
e x p
;
2
' ( x ) ; '
Q
k ' k
d x =
= C s u p
Q c u b e
1
Q
Z
1
0
e x p
;
2
t
d
;
f x 2 Q :
' ( x ) ; '
Q
k ' k
> t g
C s u p
Q c u b e
1
Q
Z
1
0
e x p
;
2
t
C Q e x p ( ; t ) ( ; ) d t = C
a n d k ' k
p
C k ' k
. T h e i n e q u a l i t y k ' k
k ' k
p
f o l l o w s f r o m H l d e r ' s i n e q u a l i t y .
F a c t 3 : C o n n e c t i o n b e t w e e n B M O a n d C a r l e s o n m e a s u r e s .
C a r l e s o n m e a s u r e s o r i g i n a l l y a p p e a r e d a s a n s w e r s t o t h e f o l l o w i n g q u e s t i o n .
Q u e s t i o n : W h i c h p o s i t i v e m e a s u r e s o n R
n + 1
+
h a v e t h e p r o p e r t y
Z Z
R
n + 1
+
P
y
f ( x )
2
d ( x y ) C ( ) k f k
2
2
f o r a l l f 2 L
2
( R
n
)
w h e r e P
y
f ( x ) = p
y
f ( x ) w i t h t h e P o i s s o n k e r n e l p
y
( x ) = c
n
y
( x
2
+ y
2
)
n + 1
2
?
T o o b t a i n a n e c e s s a r y c o n d i t i o n o n c o n s i d e r f =
Q
, i . e . , f i s t h e c h a r a c t e r i s t i c f u n c t i o n
f o r a c u b e Q R
n
. W e i m m e d i a t e l y o b s e r v e t h a t P
y
f ( x ) C > 0 f o r f ( x y ) : x 2
1
2
Q 0
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
35/144
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
36/144
R e m a r k : T h e o r e m 3 . 1 i s a l s o v a l i d f o r a l l o p e r a t o r s o f t h e f o r m
P
t
f ( x ) = '
t
f ( x )
w h e r e ' i s a s m o o t h f u n c t i o n w h i c h d e c a y s a t i n n i t y a n d s u c h t h a t ' ( x ) ( x ) f o r s o m e
r a d i a l f u n c t i o n 2 L
1
( R
n
) '
t
( x ) d e n o t e s
1
t
n
'
;
x
t
. W e l e a v e t h e p r o o f o f t h i s r e m a r k a s
a n e x e r c i s e .
W e n o w i n t r o d u c e t w o f a m i l i e s o f o p e r a t o r s d e n o t e d P
t
a n d Q
t
o f w h i c h t h e r s t i s a n
a p p r o x i m a t i o n o f t h e i d e n t i t y a n d t h e s e c o n d i s a n a p p r o x i m a t i o n o f t h e z e r o o p e r a -
t o r . L e t ' b e s m o o t h f u n c t i o n s t h a t d e c a y a t i n n i t y s u c h t h a t
R
R
n
' ( x ) d x = 1 a n d
R
R
n
( x ) d x = 0 . D e n e P
t
a n d Q
t
b y
d
P
t
f ( ) = ^' ( t )
^
f ( )
d
Q
t
f ( ) =
^
( t )
^
f ( )
f o r n i c e f u n c t i o n s f i n R
n
. W e i m m e d i a t e l y o b s e r v e
L e m m a 3 . 2 . I f f 2 L
2
( R
n
) , t h e n
Z
1
0
k Q
t
f k
2
2
d t
t
C ( ) k f k
2
2
P r o o f . A p p l y P l a n c h e r e l ' s f o r m u l a .
T h e o r e m 3 . 2 . I f f 2 B M O ( R
n
) , t h e n
d ( x t ) = Q
t
f ( x )
2
d x d t
t
i s a C a r l e s o n m e a s u r e w i t h C a r l e s o n n o r m C ( ) k f k
2
T o c a r r y t h r o u g h t h e a r g u m e n t i n t h e p r o o f o f t h i s t h e o r e m , w e n e e d a l e m m a .
L e m m a 3 . 3 . I f f 2 B M O ( R
n
) a n d Q
0
i s t h e u n i t c u b e ( c e n t e r e d a t 0 ) , t h e n
Z
R
n
f ( x ) ; f
Q
0
1 + x
n + 1
d x C k f k
w h e r e C o n l y d e p e n d s o n n
P r o o f . F o r a > 0 l e t a Q d e n o t e t h e c u b e w i t h s i d e s p a r a l l e l w i t h t h e s i d e s o f Q a n d o f
l e n g t h s a t i m e s t h e s i d e l e n g t h s o f Q a n d w i t h t h e s a m e c e n t e r a s Q . W e o b s e r v e t h a t f o r
e v e r y c u b e Q R
n
f
Q
; f
2 Q
1
Q
Z
Q
f ( x ) ; f
2 Q
d x
2
n
2 Q
Z
2 Q
f ( x ) ; f
2 Q
d x 2
n
k f k
3 0
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
37/144
S e t Q
j
= 2
j
Q
0
f o r j 2 N a n d a s s u m e k f k
= 1 . H e r e
f
Q
j + 1
; f
Q
j
2
n
f o r j 2 N
w h i c h i m p l i e s
f
Q
j + 1
; f
Q
0
( j + 1 ) 2
n
f o r j 2 N
H e n c e
Z
R
n
f ( x ) ; f
Q
0
1 + x
n + 1
d x =
1
X
j = 0
Z
Q
j + 1
n Q
j
f ( x ) ; f
Q
0
1 + x
n + 1
d x +
+
Z
Q
0
f ( x ) ; f
Q
0
1 + x
n + 1
d x
1
X
j = 0
;
Z
Q
j + 1
f ( x ) ; f
Q
j + 1
2
j ( n + 1 )
d x +
+
Z
Q
j + 1
f
Q
j + 1
; f
Q
0
2
j ( n + 1 )
d x
+ 1
1
X
j = 0
( 2
n ; j
+ ( j + 1 ) 2
2 n ; j
) + 1 = C
w h i c h c o m p l e t e s t h e p r o o f .
P r o o f o f T h e o r e m 3 . 2 . Q
t
f ( x ) i s a w e l l - d e n e d f u n c t i o n i n R
n + 1
+
s i n c e Q
t
1 = 0 . W e w a n t
t o p r o v e t h a t f o r e a c h c u b e Q R
n
( )
Z Z
~
Q
Q
t
f ( x )
2
d x d t
t
C ( ) k f k
2
Q
I t i s e n o u g h t o c o n s i d e r Q = u n i t c u b e Q
0
s i n c e B M O i s s c a l e - a n d t r a n s l a t i o n i n v a r i a n t ,
i . e . , k f k
= k f
s
t
k
w h e r e f
s
t
( x ) = f ( t ( x ; s ) ) a n d
d t
t
i s s c a l e i n v a r i a n t . F u r t h e r m o r e w e m a y
a s s u m e f
2 Q
0
= 0 s i n c e Q
t
1 = 0 . T h u s w e h a v e t o p r o v e ( ) f o r Q = Q
0
a n d a l l f 2 B M O
w i t h f
2 Q
0
= 0 . S e t f
1
= f
2 Q
0
a n d f
2
= f ; f
1
T h e n Q
t
f = Q
t
f
1
+ Q
t
f
2
a n d w e o b t a i n
Z Z
Q
0
Q
t
f
1
2
d x d t
t
Z Z
R
n + 1
+
Q
t
f
1
2
d x d t
t
C ( ) k f
1
k
2
2
C ( ) k f k
2
f r o m l e m m a 3 . 2 a n d f o r ( x t ) 2
~
Q
0
w e o b t a i n
Q
t
f
2
( x )
Z
R
n
n 2 Q
0
1
t
n
;
x ; z
t
f
2
( z ) d z
C ( )
Z
R
n
n 2 Q
0
t
t
n + 1
+ x ; z
n + 1
f
2
( z ) d z
C ( ) t
Z
R
n
f ( z )
1 + z
n + 1
d z C ( ) t k f k
a c c o r d i n g t o l e m m a 3 . 3 . T h i s c o m p l e t e s t h e p r o o f .
W e h a v e n o w p r e p a r e d t h e t o o l s w e n e e d t o p r o v e t h e t h e o r e m o f D a v i d a n d J o u r n .
3 1
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
38/144
T h e o r e m 1 . 6 : I f T i s a P V O w i t h C Z t y p e k e r n e l K , t h e n
T i s b o u n d e d o n L
2
i T 1 2 B M O
H e r e t h e o n l y i f - p a r t f o l l o w s f r o m P r o p o s i t i o n 3 . 1 . T h e i f - p a r t i s t h e h a r d p a r t . T h e
p r o o f w e p r e s e n t i s d u e t o C o i f m a n / M e y e r 1 ] . C h o o s e ' 2 C
1
0
( R
n
) s u c h t h a t ' r a d i a l
w i t h s u p p o r t i n t h e u n i t b a l l B
1
( 0 ) a n d s u c h t h a t
^' ( ) = 1 + O (
4
) a s ! 0
D e n e P
t
a s a b o v e b y
d
P
t
f ( ) = ^' ( t )
^
f ( ) . A n a l o g o u s l y d e n e Q
t
b y
d
Q
t
f ( ) = ( t )
2
' ( t ) f ( )
a n d R
t
b y
d
R
t
f ( ) = ( )
; 1
^'
0
( t )
^
f ( ) . H e n c e P
t
Q
t
a n d R
t
c o m m u t e s a n d
d
d t
P
2
t
=
2
t
R
t
Q
t
T h i s i m p l i e s
1
2
d
d t
P
2
t
T P
2
t
=
1
t
( R
t
Q
t
T P
2
t
+ P
2
t
T R
t
Q
t
)
T h e i d e a i s a s f o l l o w s : W e w a n t t o s h o w
h
1
T
2
i C k
1
k
2
k
2
k
2
f o r a l l
1
2
2 S ( R
n
)
W e n o t e t h a t h
1
P
2
t
T P
2
t
2
i ! 0 a s t ! 1 a n d h e n c e i t i s e n o u g h t o p r o v e
Z
1
0
d
d t
h
1
P
2
t
T P
2
t
2
i d t C k
1
k
2
k
2
k
2
f o r a l l
1
2
2 S ( R
n
)
s i n c e P
0
i s t h e i d e n t i t y o p e r a t o r .
F u r t h e r m o r e , i t i s e n o u g h t o p r o v e
Z
1
0
h
1
R
t
Q
t
T P
2
t
2
i
d t
t
C k
1
k
2
k
2
k
2
f o r a l l
1
2
2 S ( R
n
)
s i n c e P
t
Q
t
R
t
a r e s e l f a d j o i n t o p e r a t o r s a n d T
= ; T . W e n e e d t h e f o l l o w i n g e s t i m a t e .
L e m m a 3 . 4 . L e t ' 2 C
1
0
( R
n
) w i t h s u p p o r t i n t h e u n i t b a l l B
1
( 0 ) a n d a s s u m e
Z
R
n
( x ) d x = 0
T h e n
h
x
t
T '
y
t
i C p
t
( x ; y )
w h e r e
x
t
( z ) =
1
t
n
;
z ; x
t
'
y
t
( z ) =
1
t
n
'
;
z ; y
t
a n d p
t
i s t h e P o i s s o n k e r n e l .
3 2
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
39/144
P r o o f . T h e a r g u m e n t c o n s i s t s o f a s t r a i g h t f o r w a r d c a l c u l a t i o n w h e r e w e u s e t h e C Z t y p e
p r o p e r t i e s o f t h e k e r n e l K
2 h
x
t
T '
y
t
i = l i m
" # 0
Z Z
; > "
K ( ) (
x
t
( ) '
y
t
( ) ;
x
t
( ) '
y
t
( ) ) d d
= l i m
" # 0
Z Z
; > "
K ( t + y t + y )
;
x y
t
1
( ) ' ( ) ;
x y
t
1
( ) ' ( ) ) d d :
H e n c e , i t i s e n o u g h t o p r o v e t h e l e m m a f o r y = 0
A s s u m e x
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
40/144
H e r e
I =
Z
1
0
k
^'
0
( t )
t
^
1
( ) k
2
2
d t
t
C k ^
1
k
2
2
= C k
1
k
2
2
T o c o p e w i t h I I , w e r e w i r t e Q
t
T P
2
t
2
= L
t
P
t
2
a s
( ( L
t
P
t
)
2
) ( x ) = L
t
P
t
2
; P
t
2
( x ) ( x ) + P
t
2
( x ) L
t
1 ( x ) =
= L
t
P
t
2
; P
t
2
( x ) ( x ) + P
t
2
( x ) Q
t
T 1 ( x )
B u t T 1 2 B M O i m p l i e s Q
t
T 1
2
d x d t
t
i s a C a r l e s o n m e a s u r e a c c o r d i n g t o T h e o r e m 3 . 2 a n d
h e n c e
Z
1
0
k P
t
2
( x ) Q
t
T 1 k
2
2
d t
t
=
Z Z
R
n + 1
+
P
t
2
( x )
2
Q
t
T 1
2
d x d t
t
C k
2
k
2
2
w h e r e w e h a v e u s e d t h e r e m a r k t o T h e o r e m 3 . 1 . F u r t h e r m o r e u s i n g J e n s e n ' s i n e q u a l i t y
A ( x t ) L
t
( P
t
2
; P
t
2
( x ) ) ( x )
2
=
=
Z
R
n
1
t
( x y ) ( P
t
2
( y ) ; P
2
2
( x ) ) d y
2
C
Z
R
n
p
t
( x ; y ) P
t
2
( y ) ; P
t
2
( x )
2
d y
a n d t h u s
Z
1
0
k L
t
P
t
2
; P
t
2
( x ) ( x ) k
2
2
d t
t
=
Z
1
0
Z
R
n
A ( x t )
d x d t
t
C
Z
1
0
Z
R
n
Z
R
n
p
t
( x ; y ) P
t
2
( x ) ; P
t
2
( y )
2
d y d x
d t
t
=
= C
Z
1
0
Z
R
n
Z
R
n
p
t
( x ) P
t
2
( x + y ) ; P
t
2
( y )
2
d x d y
d t
t
= C
Z
1
0
Z
R
n
Z
R
n
p
t
( x )
\
( P
t
2
( + x ) ; P
t
2
( ) ) ( )
2
d d x
d t
t
=
= C
Z
1
0
Z
R
n
Z
R
n
p
t
( x ) ^' ( t )
2
1 ; e
i h x i 2
^
2
( )
2
d d x
d t
t
B u t
Z
R
n
p
t
( x ) 1 ; e
i h x i 2
d x = 2 ; 2 e
; t
T h u s
Z
1
0
k L
t
P
t
2
; P
t
2
( x ) ( x ) k
2
2
d t
t
C
Z
R
n
Z
1
0
2 ( 1 ; e
; t
) ^' ( t )
2
d t
t
^
2
( )
2
d
C
Z
R
n
;
Z
1
0
( 1 ; e
; t
)
d t
t
+
Z
1
1
^' ( t )
2
d t
t
^
2
( )
2
d
C k
2
k
2
2
T h i s c o m p l e t e s t h e p r o o f .
3 4
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
41/144
R e f e r e n c e s
1 ] R . R . C o i f m a n / Y . M e y e r : p e r s o n a l c o m m u n i c a t i o n .
3 5
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
42/144
3 6
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
43/144
C h a p t e r 4
P r o o f o f T h e o r e m 1 . 3
I n t h i s s e c t i o n w e p r o v e
T h e o r e m 1 . 3 : I f ' : R ! R L i p s c h i t z f u n c t i o n a n d K
'
( x y ) =
1
x ; y + i ( ' ( x ) ; ' ( y ) )
,
t h e n t h e c o r r e s p o n d i n g o p e r a t o r T
'
i s b o u n d e d o n L
2
a n d k T
'
k C ( k '
0
k
1
)
W e i m m e d i a t e l y o b s e r v e t h a t t h e k e r n e l K
'
i s o f C Z t y p e a n d t h u s t h e L
2
b o u n d e d n e s s
o f t h e P V O T
'
c a n b e p r o v e d u s i n g T h e o r e m 1 . 6 , i . e . , i t i s e n o u g h t o p r o v e T
'
1 2 B M O .
H o w e v e r , t h i s i s n o t e a s y .
W e g i v e t h e p r o o f i n t w o s t e p s .
A : T h e r e e x i s t s a n "
0
> 0 s u c h t h a t i f k '
0
k
1
"
0
t h e n k T
'
k C ( k '
0
k
1
)
B : R e m o v a l o f t h e c o n s t r a i n t k '
0
k
1
"
0
P a r t A w a s p r o v e d b y C a l d e r n 1 ] . P a r t B w a s p r o v e d b y C o i f m a n / M c I n t o s h / M e y e r 2 ] .
T h e p r o o f w e p r e s e n t i s d u e t o D a v i d 3 ] .
P r o o f o f A : A s s u m e ' 2 C
1
0
( R
n
) a n d d e n e
K
N
( x y ) =
( ' ( x ) ; ' ( y ) )
N
( x ; y )
N + 1
N = 0 1 2 : : : :
T
N
c o r r e s p o n d i n g P V O w i t h k e r n e l K
N
W e r e m a r k t h a t t h e T
N
' s a r e c a l l e d c o m m u t a t o r s a n d a r i s e n a t u r a l l y w h e n o n e t r i e s t o
c o n s t r u c t a c a l c u l u s o f s i n g u l a r i n t e g r a l o p e r a t o r s t o h a n d l e d i e r e n t i a l e q u a t i o n s w i t h n o n -
s m o o t h c o e c i e n t s . W e r e f e r t o C a l d e r n 4 ] f o r a n e x t e n s i v e d i s c u s s i o n o f c o m m u t a t o r s
a n d P D E ' s . S i n c e T =
P
1
N = 0
( ; i )
N
T
N
, i t i s e n o u g h t o p r o v e t h a t
k T
N
k C
N + 1
k '
0
k
N
1
N = 0 1 2 : : : :
3 7
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
44/144
W e a l s o n o t e t h a t i t i s e n o u g h t o p r o v e t h a t t h e r e e x i s t s a n "
1
> 0 s u c h t h a t i f k '
0
k
1
"
1
,
t h e n
k T
N
k C
N
N = 1 2 : : : :
s i n c e T
0
i s t h e H i l b e r t t r a n s f o r m a n d t h i s o p e r a t o r i s L
2
b o u n d e d . T h e r e a r e m a n y p r o o f s
o f t h i s f a c t a n d o n e p r o o f i s s u p p l i e d b y T h e o r e m 1 . 6 . T o p r o v e t h a t T
N
N = 1 2 : : : a r e
L
2
b o u n d e d w e m a k e t h e f o l l o w i n g o b s e r v a t i o n .
L e m m a 4 . 1 . I f ' 2 C
1
0
, t h e n
T
N + 1
( 1 ) = T
N
( '
0
) N = 0 1 : : : :
P r o o f . T h e l e m m a i s a c o n s e q u e n c e o f t h e i d e n t i t y
d
d y
;
' ( x ) ; ' ( y )
x ; y
N + 1
= ( N + 1 )
( ' ( x ) ; ' ( y ) )
N + 1
( x ; y )
N + 2
; ( N + 1 )
( ' ( x ) ; ' ( y ) )
N
( x ; y )
N + 1
'
0
( y )
a n d
T
N + 1
1 ( x ) = l i m
" # 0
Z
x ; y > "
( ' ( x ) ; ' ( y ) )
N + 1
( x ; y )
N + 2
d y =
= l i m
" # 0
1
N + 1
;
' ( x ) ; ' ( x ; " )
"
;
' ( x ) ; ' ( x + " )
; "
+ T
N
'
0
( x ) = T
N
'
0
( x )
A r e c u r s i o n a r g u m e n t u s i n g P r o p o s i t i o n 3 . 1 , L e m m a 4 . 1 a n d t h e f a c t t h a t ' L i p s c h i t z
f u n c t i o n i m p l i e s '
0
2 L
1
s h o w s t h a t T
N
N = 0 1 2 : : : a r e L
2
b o u n d e d . W h a t r e m a i n s
t o b e d o n e i s t o s h o w t h a t
k T
N
k C
N
N = 1 2 : : :
f o r s o m e c h o i c e o f C > 0 . H e r e , o f c o u r s e , k k d e n o t e s t h e n o r m k k
L
2
! L
2
. T o c o n c l u d e t h e
p r o o f o f A w e n o t e t h a t
1 : I f K i s a k e r n e l o f C Z t y p e s u c h t h a t
K ( x y ) + ( r
x
K ( x y ) + r
y
K ( x y ) ) x ; y
C
1
x ; y
n
a n d i f k T 1 k
C
2
, t h e n
k T k D
n
( C
1
+ C
2
)
f o r s o m e c o n s t a n t D
n
w h i c h o n l y d e p e n d s o n d i m e n s i o n n
3 8
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
45/144
2 : U n d e r t h e s a m e a s s u m p t i o n s a s i n 1
k T k
L
1
! B M O
D
n
( k T k + C
1
)
T h i s f o l l o w s f r o m t h e p r o o f s o f P r o p o s i t i o n 3 . 1 a n d T h e o r e m 1 . 6 . H e n c e
k T
N + 1
k C
1
+ C
2
k T
N
k N = 0 1 2 : : :
f o r s o m e c o n s t a n t s C
1
C
2
i n d e p e n d e n t o f N a n d
k T
N
k C
N
N = 1 2 : : :
f o r s o m e c o n s t a n t C > 0 f o l l o w s . T h e p r o o f o f A i s c o m p l e t e d .
P r o o f o f B : W e s t a r t w i t h t h r e e l e m m a s .
L e m m a 4 . 2 . T h e r e e x i s t s a n "
0
> 0 s u c h t h a t i f
' ( x ) = A x + ( x ) x 2 R
w h e r e A 2 R a n d : R ! R L i p s c h i t z f u n c t i o n w i t h k
0
k
1
"
0
t h e n
k T
'
k C
0
f o r s o m e c o n s t a n t C
0
> 0 w h i c h i s i n d e p e n d e n t o f A .
P r o o f . R e p e a t i n g t h e a r g u m e n t a b o v e , w e s e e t h a t i f h : R ! C L i p s c h i t z f u n c t i o n w i t h
k h
0
k
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
46/144
R e m a r k :
~
L 2 L ; M L + M
P r o o f . W i t h o u t l o s s o f g e n e r a l i t y w e c a n a s s u m e t h a t I = 0 1 M = 1 L = ;
4
5
U
f x 2 I : '
0
( x ) + L 0 g h a s m e a s u r e
1
2
. C h e c k t h i s !
H e n c e ;
1
5
'
0
9
5
D e n e ~' : R ! R b y
~' ( x ) =
8
0 s u c h t h a t x x + h 2 0 1 . T h u s 0 ~'
0
9
5
a n d ~' s a t i s e s ( i i ) w i t h
~
L =
; 9
1 0
R e m a i n s t o c h e c k t h a t ( i ) i s s a t i s e d . S e t
E = f x 2 I : ' ( x ) = ~' ( x ) g
T h e n 0 2 E a n d E c l o s e d i m p l i e s t h a t
I n E =
k
I
k
w h e r e t h e c o m p o n e n t s I
k
a r e o f t h e f o r m a
k
b
k
o r a
k
1 w h e r e 0 < a
k
< b
k
1 . B u t ~'
i s c o n s t a n t o n e a c h i n t e r v a l I
k
a n d t h u s
' ( a
k
) = ~' ( a
k
) = ~' ( b
k
) = ' ( b
k
) i f I
k
= a
k
b
k
' ( a
k
) = ~' ( a
k
) = ~' ( 1 ) ' ( 1 ) i f I
k
= a
k
1
H e n c e
Z
I
k
'
0
( x ) d x 0 f o r e a c h k a n d w e o b t a i n
Z
'
0
( x ) d x 0
F i n a l l y
0
Z
'
0
( x ) d x =
Z
\ U
'
0
( x ) d x +
Z
\ ( I n U )
'
0
( x ) d x
4
5
\ U ;
1
5
\ ( I n U )
i m p l i e s
\ U
1
4
\ ( I n U )
4 0
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
47/144
a n d t h i s g i v e s u s
= \ U + \ ( I n U )
5
4
\ ( I n U )
5
8
H e n c e
E
3
8
a n d t h e p r o o f i s d o n e .
L e m m a 4 . 4 ( J o h n 6 ] ) . A s s u m e f : R ! R m e a s u r a b l e . A s s u m e t h e r e e x i s t s a n > 0
a n d a c o n t i n u o u s f u n c t i o n C : ! R , w h e r e = f ( a b ) 2 R
2
: a < b g , s u c h t h a t
f x 2 I : f ( x ) ; C ( I ) < g >
1
3
I f o r e a c h i n t e r v a l I = ( a b ) . T h e n f 2 B M O ( R ) a n d
k f k
C w h e r e C i s i n d e p e n d e n t o f f a n d t h e f u n c t i o n C
P r o o f . I t i s e n o u g h t o p r o v e t h e l e m m a f o r = 1 . T h e a r g u m e n t s a r e s i m i l a r t o t h o s e o n e
u s e s t o p r o v e J o h n - N i r e n b e r g ' s i n e q u a l i t y o n c e w e h a v e p r o v e d t h e f o l l o w i n g
C l a i m : I f I J R a r e i n t e r v a l s s u c h t h a t J = 2 I , t h e n C ( I ) ; C ( J ) 1 5
P r o o f o f c l a i m : L e t d e n o t e t h e i n t e r v a l w i t h e n d p o i n t s C ( I ) a n d C ( J ) a n d a s s u m e t o
o b t a i n a c o n t r a d i c t i o n t h a t > 1 5 . T h e n t h e r e e x i s t s p o i n t s z
k
2 k = 1 2 : : : 6 s u c h
t h a t z
k
2 a n d m i n
k 6= 1
z
k
; z
1
> 2 . S e t M
k
= f x 2 J : f ( x ) ; z
k
P
6
k = 1
M
k
S i n c e C : ! R i s c o n t i n u o u s , t h e r e e x i s t i n t e r v a l s I
k
k = 1 2 : : : 6 s u c h t h a t I I
k
J
a n d C ( I
k
) = z
k
. H e n c e
J >
6
X
k = 1
M
k
6
X
k = 1
M
k
\ I
k
6
1
3
I = 2 I
T h i s c o n t r a d i c t s J = 2 I a n d c l a i m i s p r o v e n .
W e n o w s h o w t h a t u n d e r t h e h y p o t h e s i s i n t h e l e m m a w i t h = 1
Z
I
f ( x ) ; C ( I ) d x C I
f o r e a c h i n t e r v a l I R . O b s e r v e t h a t w e d o n o t k n o w w h e t h e r f 2 L
1
o c
o r n o t . S i n c e t h e
a s s u m p t i o n s o n f a r e s c a l e - a n d t r a n s l a t i o n i n v a r i a n t w e c a n a s s u m e I = 0 1 . W e c a n a l s o
a s s u m e C ( I ) = 0
N o w , s e t
k
= 1 0 0 k k = 1 2 : : : a n d l e t
k
=
j
I
k
j
b e t h e u n i o n o f t h o s e i n t e r v a l s
i n t h e d y a d i c m e s h o f I w h i c h a r e m a x i m a l w i t h r e s p e c t t o i n c l u s i o n w i t h t h e p r o p e r t y
C ( I
k
j
) >
k
. W e s e e t h a t I =2
1
a n d
1
2
3
. F o r e a c h I
k
j
i n
k
t h e r e e x i s t s
4 1
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
48/144
a n i n t e r v a l
~
I
k
j
i n t h e d y a d i c m e s h o f I w h i c h i s m i n i m a l w i t h r e s p e c t t o i n c l u s i o n a n d w i t h
t h e p r o p e r t y I
k
j
*
~
I
k
j
. H e n c e C (
~
I
k
j
)
k
a n d t h e c l a i m a b o v e i m p l i e s
k
k
+ 2 g w h i c h i s a m e a s u r a b l e s e t a n d t a k e a p o i n t
o f d e n s i t y x
0
2 A
k
. T h e n t h e r e e x i s t s a s u c i e n t l y s m a l l i n t e r v a l J i n t h e d y a d i c m e s h o f
I s u c h t h a t x
0
2 J a n d
f x 2 J : f ( x ) >
k
+ 2 g
9 9
1 0 0
J
T h i s i m p l i e s C ( J ) >
k
a n d t h u s x
0
2 J
k
. H e n c e A
k
k
e x c e p t f o r a s e t o f m e a s u r e
0 a n d
A
k
k
B u t
k + 6
1
2
k
i m p l i e s t h a t t h e r e e x i s t c o n s t a n t s B C > 0 s u c h t h a t
A
k
B e
; C (
k
+ 2 )
k = 1 2 : : : :
C h o o s i n g a s l i g h t l y l a r g e r c o n s t a n t C w e g e t
f x 2 I : f ( x ) > g B e
; C
T h e r e m a i n i n g a r g u m e n t i s t h e s a m e a s i n t h e p r o o f o f t h e r e m a r k o n p a g e 2 9 .
F i n a l l y w e g i v e t h e a r g u m e n t f o r
k + 6
1
2
k
P r o o f . S e t E
k
= f x 2 I : f ( x ) ;
k
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
49/144
b y t a k i n g t h e u n i o n o v e r a l l I
k
j
I
k
0
j
0
a n d u s i n g E
k
\ I
k
j
1
3
I
k
j
. H e n c e
I
k
0
j
0
X
k
0
< k k
0
+ 6
I
k
0
j
0
\ E
k
1
3
X
k
0
< k k
0
+ 6
I
k
0
j
0
\
k
2 I
k
0
j
0
\
k
0
+ 6
w h i c h i m p l i e s
k + 6
1
2
k
W e h a v e n o w p r e p a r e d a l l t h e m a c h i n e r y w e n e e d t o p r o v e p a r t B . T h e i d e a i s t o m a k e a n
i n d u c t i o n a r g u m e n t w h e r e p a r t A i s t h e b a s e a n d t h e i n d u c t i o n s t e p i s t h e f o l l o w i n g : L e t
M > 0 . I f t h e r e e x i s t s a c o n s t a n t
C = C
;
9
1 0
M
s u c h t h a t k T
~'
k C f o r a l l L i p s c h i t z f u n c t i o n s ~' w i t h o s c ~'
9
1 0
M t h e n t h e r e e x i s t s a
c o n s t a n t C = C ( M ) s u c h t h a t k T
'
k C f o r a l l L i p s c h i t z f u n c t i o n s ' w i t h o s c ' M
H e r e w e l e t o s c ' d e n o t e i n f f M : ' ( x ) + L x ; ( ' ( y ) + L y ) M x ; y f o r a l l x 6= y a n d
s o m e L 2 R g
W e r e m a r k t h a t L e m m a 4 . 2 i m p l i e s t h a t k T
'
k o n l y d e p e n d s o n o s c ' a n d n o t o n k '
0
k
1
W e
o b s e r v e t h a t i t i s e n o u g h t o p r o v e t h e i n d u c t i o n s t e p f o r L i p s c h i t z - f u n t i o n s ' w i t h ' 2 C
1
a n d i t i s e n o u g h t o p r o v e t h a t t h e r e e x i s t s a c o n s t a n t C = C ( M ) s u c h t h a t
k T
'
k
L
1
! B M O
C
f o r a l l L i p s c h i t z - f u n c t i o n s ' 2 C
1
w i t h o s c ' M . T a k e f 2 L
1
w i t h k f k
1
= 1 . L e t
I b e a n i n t e r v a l a n d l e t x
I
d e n o t e t h e c e n t e r o f I . S e t z ( x ) = x + i ' ( x ) . D e c o m p o s e
f i n f
1
a n d f
2
w h e r e f
1
= f
I
a n d f
2
= f ; f
1
. F i n a l l y s e t C
f
( I ) = T
'
f
2
( x
I
) W e
s e e t h a t C i s a c o n t i n u o u s f u n c t i o n w i t h r e s p e c t t o t h e e n d p o i n t s o f I . W i t h o u t l o s s o f
g e n e r a l i t y w e a s s u m e I = 0 1 . F r o m L e m m a 4 . 3 w e o b t a i n a L i p s c h i t z f u n c t i o n s u c h
t h a t o s c
9
1 0
M a n d E f x 2 I : ' ( x ) = ( x ) g h a s m e a s u r e
3
8
. S e t z
( x ) = x + i ( x )
O u r p u r p o s e i s t o u s e t h e c h a r a c t e r i z a t i o n o f B M O f u n c t i o n s w h i c h i s g i v e n i n L e m m a 4 . 4
b y s h o w i n g t h a t
f x 2 I : T
'
f ( x ) ; C
f
( I ) < C ( M ) g >
1
3
f o r c o n s t a n t C = C ( M ) c h o s e n l a r g e e n o u g h a n d w h i c h i s i n d e p e n d e n t o f f . I f t h i s i s d o n e ,
T h e o r e m 1 . 3 f o l l o w s . W e s t a r t w i t h
T
'
f ( x ) ; C
f
( I ) = T
'
f ( x ) ; T
'
f
2
( x
I
)
T
'
f
2
( x ) ; T
'
f
2
( x
I
) + T
'
f
1
( x ) ; T
f
1
( x ) + T
f
1
( x )
w h e r e x b e l o n g s t o a s u b s e t o f I w h i c h w e w i l l d e n e l a t e r .
4 3
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
50/144
F o r x 2 I ,
T
'
f
2
( x ) ; T
'
f
2
( x
I
)
Z
R n I
z ( x ) ; z (
1
2
)
( z ( x ) ; z ( y ) ) ( z (
1
2
) ; z ( y ) )
f ( y ) d y
C
0
( M )
Z
R n I
d y
x ; y
1
2
; y
w h i c h i m p l i e s
Z
I
T
'
f
2
( x ) ; T
'
f
2
( x
I
) d x C
0
( M )
F o r x 2 E I ,
T
'
f
1
( x ) ; T
f
1
( x )
Z
I n E
z ( y ) ; z
( y )
( z ( x ) ; z ( y ) ) ( z
( x ) ; z
( y ) )
f ( y ) d y
B u t I n E = I
k
w h e r e t h e c o m p o n e n t s I
k
a r e i n t e r v a l s a n d
z ( y ) ; z
( y ) C
0
( M ) I
k
f o r y 2 I
k
H e n c e
T
'
f
1
( x ) ; T
f
1
( x )
X
k
Z
I
k
C
0
( M ) I
k
x ; y
2
d y x 2 E
S e t J
k
=
1 0 0 1
1 0 0 0
I
k
a n d E
= E \ { (
k
J
k
)
I
k 1
J
k 1
E
E
J
k
I
k
T h e n E n E
1
1 0 0 0
a n d
Z
E
T
'
f
1
( x ) ; T
f
1
( x ) d x C
0
( M )
X
k
Z
I
k
Z
J
k
I
k
x ; y
2
d x d y C
0
( M )
X
k
Z
I
k
d y C
0
( M )
F i n a l l y , f r o m t h e h y p o t h e s i s i n t h e i n d u c t i o n s t e p
Z
I
T
f
1
( x ) d x
;
Z
I
T
f
1
( x )
2
d x
1 = 2
C
;
9
1 0
M
B u t
f x 2 I : T
'
f
2
( x ) ; T
'
f
2
( x
I
)
C
0
( M )
3
g
1
1 0 0 0
f x 2 E
: T
'
f
1
( x ) ; T
f
1
( x )
C
0
( M )
3
g
1
1 0 0 0
f x 2 I : T
f
1
( x )
C
0
( M )
3
g
1
1 0 0 0
4 4
-
7/30/2019 Dahlberg B.E.J., Kenig C.E. Harmonic Analysis and Partial Differential Equations (1996)(en)(138s)
51/144
i f C
0
( M ) l a r g e e n o u g h . H e n c e f x 2 E
: T
'
f ( x ) ; T f
2
( x
I
) < C
0
( M ) g j j E ;
4
1 0 0 0
>
1
3
i f C
0
( M ) l a r g e e n o u g h a n d w h e r e C
0
( M ) i s i n d e p e n d e n t o f f . ( N o t e t h a t w e h a v e a s s u m e d
k f k
1
= 1 . ) L e m m a 4 . 4 c o n c l u d e s t h a t
k T
'
k C C
0
( M ) = C ( M )
a n d t h e i n d u c t i o n s t e p i s p r o v e d .
R e f e r e n c e s
1 : A .