• Aucun résultat trouvé

A t h e o r e m o n duality m a p p i n g s in B a n a c h s p a c e s

N/A
N/A
Protected

Academic year: 2022

Partager "A t h e o r e m o n duality m a p p i n g s in B a n a c h s p a c e s "

Copied!
7
0
0

Texte intégral

(1)

A R K I V F O R M A T E M A T I K B a n d 4 n r 32

R e a d 2 J u n e 1954

A t h e o r e m o n duality m a p p i n g s in B a n a c h s p a c e s

By ARNE BEURLING and A. E. LIVINGSTON

l. Introduction

The problem considered in this paper originates in the theory of Fourier series of functions belonging to a Lebesgue space L ~, where L p denotes the space of measurable functions with period 2 g a n d with n o r m

2 ~

II/11. = { f I/(~)I" d ~}".

0

F o r the Fourier coefficients of ], we shall use the notation

if

2yg

c,,

(t) = ~ e-'"" I (x)

0

d x .

A classical theorem such t h a t

asserts t h a t if { a n } ~ is a given sequence of numbers l a . [ 2 < oo,

n ~ - - O 0

then there is a unique element / E L ~ with the p r o p e r t y t h a t

c . (1) = a .

for n = 0 , __1, --+2, . . . .

The above theorem admits the following extension. Let S~, 0 < ~ < oo, denote the operator t a k i n g ' t h e complex n u m b e r z into I zl a:a z. We have

so t h a t the collection { Sa} forms a group. Furthermore, Sa performs a one- to-one m a p p i n g of the finite complex plane onto itself. Applied to a space L v, we see t h a t Sa ] will t a k e L ~ onto L p/a, 0 < a_< p. I n particular, Sv-1 ] will m a p L v onto its dual space L ~, q = p / ( p - 1 ) . We then have

T h e o r e m t . l e t the integers be partitioned into two disjoint sets A and A ' , neither o/ which is empty. Let p be a given exponent such that 1 < p < ~ . Let { a, ; n E A } and (bn ; n E A ' } be given sets o/ numSers such that, /or some h E L ~ and /or some k E L q, q = p / ( p - 1 ) , we have

(2)

A. B E U R L I N G , A. E . L I V I N G S T O N , Duality mappings in Banach s p a c e s

ca (h) = an, n fi A , cn (k) = b~, n 6 A ' . Then there is a unique element [ 6 L v such that

c,~(f)=an, n e A , c,,(Sv_l])=b,~, n E A ' .

(1)

For p = 2, the above statement reduces to the cited classical result, since, in this case, S~_1 f = f.

The proof of the uniqueness is quite easy. If there were two solutions ~1 and f3 of (1), then the difference F = [ 1 - [ 3 would be an element of L p and would have Fourier coefficients vanishing on A. Similarly, G = Sp-i ~1- Sv-1 [3 would be in L e and have Fourier coefficients zero on A'. Consequently, the Fourier coefficients of the continuous function

2n

! ~'(x+t)O(t)~t,

0

which are given by c, (E)5n (G), are zero for each n. Therefore,

2:z 21t

~! fllv I N ' ~ dr. (2)

~ f

0

I ("-'3), ,1

0

,3/

Setting fl = ]fi I e'~ s = Is e'~ we find t h a t the real part of the integrand in (2) is

Ihl ~ + 1/31"-(Ihl ]f3l n - l + 1/11 "-~ 1/31) cos (01-03)>_ (1111-1/31)(Ihl " - ~ - 1131"-1) >-0.

The vanishing of (2) therefore requires t h a t almost everywhere ]h [ = I f3l and cos ( 0 1 - 0~)= 1, and the uniqueness follows.

The above proof of the uniqueness is satisfactory, b u t it gives no indication of the nature of the problem. In particular, the role played b y the operator Sp_l is not at all clear. We shall see in the next section t h a t the operator Sp-1 is only one of a large class of operators on L v to L v/(v-1) which arise quite naturally from a consideration of what we call duality maps of a Banach space onto its first conjugate space.

2. Duality mappings

We will be dealing with a complex (or real) Banach space B and its conju- g a t e space B*. The null element of B will be denoted b y 0, of B* b y 0". The norm of an element x E B is IIxH--IIxIl., of

u B*

is Hull=lluiI~.. The unit- spheres in B and B* will be denoted b y S and S*, respectively.

Let (x, u) be the bilinear functional defined for x E B and u E B* and having the properties :

(3)

A]gKIV FOR MATEMATIK~ B d 4 nr 32 (a) I f 2 is a complex (or real) number, then

(~

x, u) = (x, ~ u) = ~ (x, u) ;

(b) (x 1 + x~, u) = (x 1, u) + (x,, u),

(x, u 1 + u2) = (x, u l ) + (x, us) ;

(c) II ll.. = sup os I(x,

Two elements x E S and x*E S* are said to be conjugate if (x, x * ) = 1. The sets (;t x ; 0 _ ~ < o~ } and {/~ x* ; 0 _</z < oo } win then be called conjugate rays.

Under the assumption t h a t each element on S (or S*) has a unique con- jugate on S* (or S), we will consider duality m a p s of B onto B* characterized b y the following properties: T is one-to-one and takes each r a y in B onto the conjugate r a y in B* and each sphere [[x[[=r in B onto a sphere [[u[[=Q in B*

in such a w a y t h a t r 1 < r 2 implies Q1 < 0z. F r o m this definition, it follows t h a t

T(~x)=~ (2)x*, 2>0,

x and x* being conjugate elements on the respective unit spheres and ~ (~) a continuous function t h a t is strictly increasing from 0 to oo with 2. (A special t y p e of duality m a p has previously been considered b y E. R. LORC~ [4].)

With regard to such mappings, we have

L e m n a a i . Let there exist a duality map o/ B onto B*. I / x, y E B, then the relation

( z - y , T x - T y ) = O (3)

implies that x = y.

To prove this, we observe t h a t z E B and u EB* will belong to conjugate rays if and only if (z, u)=[[zili[ul]. Consequently, the assumption x r

> 0, will imply t h a t

R e (x, T y ) < Itxll tiTyll, R e ( y , Tx)<ilYII IITxi], so t h a t upon taking the real p a r t of (3), we will have

0 > ( H x l l - H y I I ) (lITxii-iiTy[I)>-o.

Therefore x = ~y, and )t = 1.

We w a n t next to find conditions on the space B in order t h a t a duality m a p shall exist. F o r this purpose, we need to recall certain definitions.

The space B is said to be uniformly c o n v e x [ l ] if there corresponds to each e, 0 < e < l , a positive n u m b e r O(e) tending to zero with e and such t h a t

(4)

A. BEURLING, A. E. LIVINGSTON, Duality mappings i n Banach spaces imply t h a t

I n uniformly convex Banaeh spaces, each closed convex subset possesses a unique element of minimal norm.

We shall say t h a t B is differentiable if for a n y x E B, x r 0, a n d a n y y E B there is a finite complex (or real) number D = D (y, x) such t h a t

+ tytl - II ll= { t D } + o (Itl)

(4)

as the complex (or real) n u m b e r t tends to zero. I t is known [3] t h a t for differentiable spaces D (y, x) is a linear functional in y of norm unity. We observe t h a t (4) implies

j D ( y ,

)l<llyll; D(x, x)-II ll;

D ( y , X x ) = D ( y , x), 0 < 4 < ~o.

An important consequence of uniform convexity and differentiability in a Banach space is the, in principle, known

L e m n a a 2. I f B is a uni/ormly convex and di//erentiable Banach space, then each element on S (or S*) has a unique conjugate element on S* (or S).

Assume first t h a t x E S is given. We are to show the existence and the uniqueness of a linear functional L ( y ) = (y, x*) of norm unity and for which L ( x ) = 1. The existence of L (y) is clear, for we m a y t a k e L ( y ) = D (y, x). As for the uniqueness, we observe t h a t for a n y y E B and for a n y complex (or real) scalar t, we have

O<-]]x+ tyli - R e { L ( x + t y ) } = i i x + t y l [ - i ] x ] [ - R e {t L (y)}.

Combining this relation with (4) yields

O <_Re {t [i) (y, x) - L (y)]} + o (I

t])

from which it follows t h a t L (y)= D (y, x).

On the other hand, if x*E S* is given, its conjugate x E S can be characterized as the element of minimal norm in the closed and convex set {y; (y, x * ) = 1} c B . Therefore, x exists and is unique.

(We point out t h a t x*E S* can be shown to have a unique conjugate x E S if we assume only t h a t B is strictly convex and t h a t the set {y; y E B , Ily]l_<l} is weakly compact. These two conditions are known to be weaker t h a n the requirement t h a t B be uniformly convex.)

I n the sequel, we will use the following definitions and notations: I f A is a closed linear subset of B, then its orthogonal complement in B* is the set A x of u E B * for which (x,u)---0 for every x E A . I f y is an element and C a set of elements, then C + y will denote the set {x; x = y + z for z E C I.

We are now r e a d y to prove

(5)

ARKIV F6R MATEMATIK. Bd 4 nr 32 T h e o r e m 2. Let B be a uni/ormly convex and di/[erentiable Banach space and T a duality m a p o/ B onto its conjugate B*. Let C be a closed, linear, and proper subset o/ B and C • its orthogonal complement in B*. 1] H E B and K C B* are given elements, then the sets C • + K and T (C + H) have one and only one element i n common.

(Note t h a t , b y v i r t u e of L e m m a 2, d u a l i t y m a p s of B o n t o B* do i n d e e d e x i s t .)

R e c a l l t h a t t h e d u a l i t y m a p T defines a c o n t i n u o u s f u n c t i o n r (~), 0_< 2 < c~, which is s t r i c t l y increasing from 0 t o c~ w i t h 2. Set

(~) = f ~ (u) d u , 0

a n d consider t h e f u n c t i o n a l

(5) = ~ (11 x II) - R e {(x, K ) }

for x E C + H . F o r Ilxll=r, we h a v e

F (x) >__ ~b (r) - r II K liB..

The r i g h t - h a n d m e m b e r of t h i s i n e q u a l i t y is a s t r i e t l y convex function of r, t e n d s t o i n f i n i t y as r - § ~ , a n d is b o u n d e d from below for r > 0. Hence,

M = inf { F (x) ; x 6 C + H }

is a finite n u m b e r . F u r t h e r m o r e , F ( x ) _ m + 1 i m p l i e s t h a t It x II < r0 < ~ - L e t {x,} c C + H be a m i n i m i z i n g sequence of F (x). W i t h o u t loss of g e n e r a l i t y , w e m a y a s s u m e t h a t II~nll t e n d s t o s o m e f i n i t e l i m i t ar (Actually, we need n o t m a k e t h i s a s s u m p t i o n , for t h e s t r i c t c o n v e x i t y of ~b (2), 0 _ 2 < c~, g u a r a n - tees t h a t II~nll t e n d s to a finite limit.) Since C + H is a c o n v e x set, we h a v e

Since r (r), r>_ O, is convex, we o b t a i n

~X m -}- Xn~

= 1 { F (~m) + F (~n)} - F ~ - - V - / = ~m n,

where emn-~0 as m, n-->c~. Therefore

lim O(ll ll)=O, ,

rn ~-~oo n--~oo

409

(6)

A . B E U R L I N G , A. E . L I V I N G S T O N ,

Duality mappings

in Banach spaces from which we d e d u c e t h a t

m--~ cr

B u t in a u n i f o r m l y c o n v e x space, t h i s i m p l i e s t h a t ( x , } is a C a u c h y sequence.

Since C + H is a closed s u b s e t of B, t h e r e is a n x o E C + H such t h a t I l x n - x o l l ~ O a n d F (xo) = M. C o n s e q u e n t l y ,

F (x o + t x) - F (Xo) > 0 for x EC a n d t a c o m p l e x (or real) scalar.

Since ~b is a d i f f e r e n t i a b l e function,

r (ll xo + t x il) - r (ll xo ID = r (ll xo lD R e { t D (x, xo) } + o (I t l)

= ~ (11 Xo II) R e {t D (x, ~o)} + o (I t I).

T h u s

R e (t [~ (H xo ]]) n (x, xo) - (x, K)]) + o (I t i) __ 0, f r o m w h i c h we conclude t h a t

([[ x o [[) D (x, Xo) - (x, K) = 0 (5)

for x E C . Since 6(HXoi})D(x, Xo) is a l i n e a r f u n c t i o n a l in x of n o r m ~b(Hxo] D, i t m a y be w r i t t e n in t h e f o r m (x, no), where u o is a n e l e m e n t on t h e sphere Ilulln.=~b (llXoH). S e t t i n g x = x o gives

(Xo, ~o) = + (11 Xo II) D (xo, Xo) = [I Xo II + (11 ~o II),

from w h i c h i t follows t h a t n o = T x o. Consequently, (5) m a y b e w r i t t e n as

(x, T x o - K ) = 0 (O)

for x E C, which i m p l i e s t h a t T x 0 E Cx + K .

W e h a v e t h e r e f o r e shown t h a t T ( C + H ) a n d C ~ + K h a v e a t l e a s t one ele- m e n t in c o m m o n .

I f x E C + H a n d T x E C j . + K , t h e n (6) i m p l i e s t h a t (x o - x, T x 0 - T x) = 0.

A n a p p l i c a t i o n of L e m m a 1 shows t h a t x = x o a n d , hence, t h a t T ( C + H ) a n d C ~ + K h a v e a t m o s t one e l e m e n t in c o m m o n .

The p r o o f of t h e t h e o r e m i s now complete.

W e wish t o p o i n t o u t t h a t t h e conclusion of T h e o r e m 2 r e m a i n s v a l i d if we a g a i n a s s u m e o n l y t h a t B is s t r i c t l y c o n v e x a n d t h a t ( y ; y E B , HyH_<I} is w e a k l y c o m p a c t .

I n o r d e r t o d e d u c e T h e o r e m 1 from T h e o r e m 2, we set B = L ~', B * = L ~, a n d let C b e t h e set of f u n c t i o n s in L p w i t h F o u r i e r coefficients v a n i s h i n g for n E A . I f

410

(7)

ARKIV FOR MATEMATIK. B d 4 n r 3 2

2 ~

(x, u)= f x(t) u(t)dt

0

for xEL p, uEL e, t h e o r t h o g o n a l c o m p l e m e n t C ~ of C consists of t h o s e uEL '~

for which ~ h a s F o u r i e r coefficients zero on A ' .

I t is k n o w n t h a t L ~, 1 < p < ~ , is u n i f o r m l y c o n v e x [1] a n d d i f f e r e n t i a b l e [2], a n d it is clear t h a t Tx=Sp_l~=ixi~/x is a d u a l i t y m a p of L ~ o n t o L ~. The d e s i r e d r e s u l t n o w follows f r o m T h e o r e m 2 if we set H = h a n d K = k.

R E F E R E N C E S

1. J. A. CLARKSON, U n i f o r m l y convex spaces. T r a n s a c t i o n s of t h e Amer. Math. Soc. 40 (1936), 396-414.

2. R. C. JAMES, O r t h o g o n a l i t y a n d linear functionals in n o r m e d linear spaces. T r a n s a c t i o n s of t h e Amer. Math. Soe. 61 (1947), 265-292.

3. - - - - L i n e a r functionals a s differentials of a n o r m . M a t h e m a t i c s Magazine 24 (1950-51), 237-244.

4. E. R. LORCH, A c u r v a t u r e s t u d y of c o n v e x bodies in B a n a c h spaces. Annali di M a t e m a t i c a P u r a ed A p p l i e a t a 34 (1953), 105-112.

Tryckt den 24 januari 1962

Uppsala 1962. Almqvist & Wiksells Boktryckeri AB

4 1 1

Références

Documents relatifs

For stable spaces (~hat is, for spaces isomorphic to its square) one has the following stronger result.. isomorphic for every

Later on the identity (6) was used to obtain estimates from below for analytic capacity [Me] and to describe uniform rectifiability via the mapping properties

Last on the agenda, the Lasry-Lions approximates of functions f (defined on Hilbert space) which are locally convex up to a positive multiple of the square of

This test is related to other integral tests due to Benedicks and Chevallier, the former in the special case of a Denjoy domain.. We then generalise our test,

There exists a coarse moduli scheme M for the equivalence classes of semistable parabolic vector bundles (on an irreducible nonsingular complete curve X}.. of

construct a reflexive sheaf from Y using the Serre construction, and then to describe this sheaf by means of a monad, where the family of monads involved

Nous 6nonr ~t la fin du second paragraphe, le r6sultat d'approximation dans le eas particulier des points minimaux, et, dans le troisi6me paragraphe, nous l'appli- quons pour

Wojtasz- czyi( that he has used the theory of molecules to study basis properties of the Franklin system.. We remark that the theory of molecules can be used also for