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An Lp theory for outer measures. Application to singular integrals.II Christoph Thiele Santander, September 2014

An Lp theory for outer measures. Application to singular integrals.II

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An Lp theory for outer measures. Application to singular integrals.II. Christoph Thiele Santander, September 2014. Recall Tents (or Carleson boxes). X is the open upper half plane, generating sets are tents T(x,s ) : Define outer measure on X by. Sizes. - PowerPoint PPT Presentation

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Page 1: An  Lp  theory for outer measures. Application to singular  integrals.II

An Lp theory for outer measures.Application to singular integrals.II

Christoph ThieleSantander, September 2014

Page 2: An  Lp  theory for outer measures. Application to singular  integrals.II

Recall Tents (or Carleson boxes)

X is the open upper half plane, generating sets are tents T(x,s) :

Define outer measure on X by

σ(T(x,s)) := s (= μ(T(x,s)))

Page 3: An  Lp  theory for outer measures. Application to singular  integrals.II

Sizes

Sp size of function on a tent

Alos Sinfty

S p ( f )(T(x,s)) = (1

sf (y, t)p dy

dt

tT (x,s)

∫∫ )1/ p

S∞( f )(T(x,s)) = sup(y,t )∈T (x,s) f (y, t)

Page 4: An  Lp  theory for outer measures. Application to singular  integrals.II

Outer essential supremum

Space of functions with finite out.ess.supremum

Outer essential supremum on a subset F:€

outess( f ) = sup{S( f )(E) : E ∈Σ}

L∞(X,μ,S)

outessF ( f ) = sup{S( f 1F )(E) : E ∈Σ}

Page 5: An  Lp  theory for outer measures. Application to singular  integrals.II

Outer Lp spaces

Define super level measures

Define Lp norms

Also weak Lp (Lorentz space) €

μ( f > λ ) := inf{μ(F) : outessF c f ≤ λ}

fLp (X ,μ ,S )

:= ( pλ p

0

∫ μ( f > λ )dλ /λ )1/ p

fLp ,∞ (X ,μ ,S )

:= supλ λ pμ( f > λ )

Page 6: An  Lp  theory for outer measures. Application to singular  integrals.II

Embedding theorems

Thm: Define for fixed Schwartz function ϕ

Then we have:

If φ has integral zero:

Fφ ( f )(y, t) := f (z)t−1φ(t−1(z − y))dz∫

Fφ ( f )Lp (X ,μ ,S ∞ )

≤ Cφ fp

Fφ ( f )Lp (X ,μ ,S 2 )

≤ Cφ fp

Page 7: An  Lp  theory for outer measures. Application to singular  integrals.II

Proof of embedding thm for Sinfty size

By Marcinkiewicz interpolation between

and

Fφ ( f )L∞ (X ,μ ,S ∞ )

≤ Cφ f∞

Fφ ( f )L1,∞ (X ,μ ,S ∞ )

≤ Cφ f1

Page 8: An  Lp  theory for outer measures. Application to singular  integrals.II

Linfty-Sinfty estimate

To show for all tents T(x,s)

But this follows from

S∞(Fφ )(T(x,s)) ≤ C f∞

sup(y,t )∈T (x,s) Fφ (y, t) ≤ sup(y,t ) Fφ (y, t)

=sup(y,t ) f (z)t−1φ(t−1(z − y))dzR

∫ ≤ φ 1 f∞

Page 9: An  Lp  theory for outer measures. Application to singular  integrals.II

Weak L1-Sinfty estimate

Ned for all lambda

Need to find a collection of tents T(xi,si) with union E such that for all x,s

S∞(Fφ1E c )(T(x,s)) ≤ Cλ

sii

∑ ≤ Cλ−1 f1

λ μ(Fφ > λ ) ≤ C f1

Page 10: An  Lp  theory for outer measures. Application to singular  integrals.II

Weak L1-Sinfty estimate

Hardy Littlewood maximal function

There is an open set where Mf is larger than lambda. Let (xi-si,xi+si) be the collection of connected components of this set. These are the tents. By Hardy Littlewood maximal thm

Mf (x) = supε

1

2εf (x + y)dy

−ε

ε

sii

∑ = x : Mf (x) > λ{ } ≤ Cλ−1 f1

Page 11: An  Lp  theory for outer measures. Application to singular  integrals.II

More on weak L1-Sinfty estimate

We haveSince F(y,t) is testing f against bump function at y of width t, may estimate by Hardy Littlewood

S∞(Fφ1E c )(T(x,s)) ≤ sup

(y,t )∈E c Fφ (y, t)

≤C supy −t ≤z≤y +t Mf (z) ≤ Cλ

Page 12: An  Lp  theory for outer measures. Application to singular  integrals.II

Proof of embedding thm for S2 size

By Marcinkiewicz interpolation between

and

Fφ ( f )L∞ (X ,μ ,S 2 )

≤ Cφ f∞

Fφ ( f )L1,∞ (X ,μ ,S 2 )

≤ Cφ f1

Page 13: An  Lp  theory for outer measures. Application to singular  integrals.II

Use Calderon reproducing formula

Fφ (y, t)2

∫∫ dydt / t = f *ϕ t (y)2∫∫ dydt / t

= ˆ f ˆ ϕ t (η)2

∫∫ dη dt / t = ˆ f (η)2

ˆ ϕ (η / t)dt / t∫ dη ≤ C∫ ˆ f 2

dη∫

Fφ (y, t)2

T (x,s)

∫∫ dydt / t ≤ f 1[x −Cs,x +Cs]

2dη∫ ≤ Cs f

2

Page 14: An  Lp  theory for outer measures. Application to singular  integrals.II

Proof of Linfty-S2 estimate

Apply Calderon reproducing formula.If we integrate over arbitrary tent T(x,s), only

restriction of f to X-Cs,x+Cs matters if phi has compact support

Dividing by s yields the desired

Fφ (y, t)2

T (x,s)

∫∫ dydt / t ≤ f 1[x −Cs,x +Cs]

2dη∫ ≤ Cs f

2

S(Fφ )(T(x,s)) ≤ C f∞

2

Page 15: An  Lp  theory for outer measures. Application to singular  integrals.II

BMO estimate

Note that we have in fact proven for any m

Thus we have the stronger embedding theorem

For the space BMO, which is defined by

Fφ ( f )L∞ (X ,μ ,S 2 )

≤ Cφ fBMO

fBMO

2:= supI

1

I| f (x) − f I |2 dx

I

S(Fφ )(T(x,s) ≤1

sf (y) − m

2dy

x −Cs

x +Cs

Page 16: An  Lp  theory for outer measures. Application to singular  integrals.II

Weak L1-S2 estimate

Let (xi-si,x-+si) be the connected components of the set where Mf(x) is larger than lambda/2.

Let E be the union of tents T(xi,3si).Do Calderon Zygmund decomposition of f

Where g is bounded by lambda, and bi is supported on interval xi-si,xi+si and has integral zero.

f = g + bii

Page 17: An  Lp  theory for outer measures. Application to singular  integrals.II

Weak L1-S2 estimate

For the good function use Linfty estimate.

For bi, do a careful estimate and accounting using1) Partial integration of bi to use mean zero when

paired with a phi-t of large support2) Support considerations of bi and phi when paired

with phi-t of small support. .

Page 18: An  Lp  theory for outer measures. Application to singular  integrals.II

Summary of proof of embedding thm

Encodes much of singular integral theory:Hardy Littlewood maximal theorem, Vitali covering argumentsCalderon reproducing formula, BMO estimates, square function techniques, Calderon Zygmund decomposition

Page 19: An  Lp  theory for outer measures. Application to singular  integrals.II

Use to prove boundedness of operators

Suppose we have operator T mapping functions on real line to functions on real line.

Want to prove

(If T is commutes with dilations, it is forced thatBoth exponents are the same)

Tfp

≤ C fp

Page 20: An  Lp  theory for outer measures. Application to singular  integrals.II

Use to prove boundedness of operators

Duality implies

Hence it suffices to prove

Tfp

= supg p ' =1

Tf ,g

Tf ,g ≤ C fp

gp'

Page 21: An  Lp  theory for outer measures. Application to singular  integrals.II

Use to prove boundedness

Express <Tf,g> by Fphi and Gphi and prove

Where either S is S2 or Sinfty, as the case may beBy outer Hoelder suffices to prove

Which itself my be result of outer triangle ineq.

Tf ,g ≤ C Fφ Lp (X ,μ ,S )Gϕ Lp ' (X ,μ ,S )

Tf ,g ≤ C FφGϕ L1 (X ,μ ,S )

Page 22: An  Lp  theory for outer measures. Application to singular  integrals.II

Example identity operator

By polarization of Calderon reproducing f.:

Provided phi has mean zero and

Triangle ineq. and outer triangle ineq. imply€

f ,g = Fφ ,Gφ dydt / t

ˆ ϕ (η / t)2dt / t∫ =1

f ,g ≤ FφGφ L1 (X ,μ ,S1 )

Page 23: An  Lp  theory for outer measures. Application to singular  integrals.II

Cauchy projection operator

By polarization of Calderon reproducing f.:

Provided phi has mean zero and

Boundedness of identity operator and of Cauchy projection imply that of Hilbert transform

Πf ,g = Fφ ,Gφ

ˆ ϕ (η / t)2dt / t∫ =1(0,∞)(η)

Hf (x) = p.v. f (x − t)dt / t∫

Page 24: An  Lp  theory for outer measures. Application to singular  integrals.II

Paraproduct estimates

For three Schwartz functions

If two Schwartz functions have integral zero

Λ( f1, f2, f3) := ( Fφ i( f i)(y, t))dy

dt

ti=1

3

∏∫∫

Λ( f1, f2, f3) ≤ Fφ i( f i)

i=1

3

∏L1 (X ,μ ,S1 )

≤ C Fφ i( f i)

i=1

3

∏Lpi (X ,μ ,Sqi

)

≤ C f ii=1

3

∏Lpi

Page 25: An  Lp  theory for outer measures. Application to singular  integrals.II

Special paraproducts

Paraproducts ard trilinear forms which are dual to bilinear operators

If phi-2 has mean 1 and f2 is 1, then F2 is 1 And we are redued to previous case. In

particular there is a paraproduct withFixing h and considering as operator in f we haveAn operator with

Λ( f1, f2,.)

Λ(h,1,.) = h

T( f ) = Λ(h, f ,.)

T(1) = h

Page 26: An  Lp  theory for outer measures. Application to singular  integrals.II

Basic T(1) Theorem

Let T be a bounded operator in L2 with

whereFor some nonzero test function phi with mean

zero. Then for 1<p<infty we have for all f,

with universal constant Cp independent of T

Tφx,s,φy,t ≤min(t,s)

max(t,s, x − y )

Tfp

≤ Cp fp

φx,s(z) = s−1φ(s−1(z − x))

Page 27: An  Lp  theory for outer measures. Application to singular  integrals.II

Why T(1) theorem?

Usually have a different set of assumptions.If s<t<|x-y| then we write

and demand suitable pointwise estimates on the partial derivative of K (Calderon Zygmund kernel).

Symmetrically if t<s<|x-y|€

Tφx,s,φy,t = K(u,v)φx,s(u)φy,t (v)dudv∫∫

=− ∂1K(u,v)Φx,s(u)φy,t (v)dudv∫∫

Page 28: An  Lp  theory for outer measures. Application to singular  integrals.II

Why T(1) theorem?

We further demand T(1)=0If |x-y|<s and t<s, then we write

And again demand suitable bounds on K. Similarly we ask T*(1)=0 to address the case|x-y|<t, s<t

= K(u,v)(u − v)(φx,s(u) − φx,s(v))

u − vφy,t (v)dudv∫∫

K(u,v)(φx,s(u) − φx,s(v))φy,t (v)dudv∫∫

Page 29: An  Lp  theory for outer measures. Application to singular  integrals.II

More general T(1) theorem

It suffices to demand T(1)=h, T*(1)=0, for some h in BMO. One reduces to the previous case by subtracting a suitable paraproduct:

Similarly one can relax the condition on T* by subtracting a dual paraproduct.

′ T f ,g = Tf ,g − P(h, f ,g)

Page 30: An  Lp  theory for outer measures. Application to singular  integrals.II

Proof of T(1) theorem

By Calderons reproducing formula

At which time we use the assumption. To apply outer Hoelder, we break up the region, e.g

|x-y|<s, t<s where we obtain€

F(x,s) Tφx,s,φy,t∫∫ G(y, t)dxdyds /sdt / t∫∫€

Tf ,g =

≤ F(x,s)x −s

x +s

∫0

s

∫ G(y, t)dydt / tR

∫ dx0

∫ ds /s3

Page 31: An  Lp  theory for outer measures. Application to singular  integrals.II

Proof of T(1) theorem

Applying Fubini

Setting Gab(x,s)=G(x+as,bs) and using outer triangle inequality

≤ F(x,s)R

∫0

∫ G(x + as,bs)dxds /s−1

1

∫ da0

1

∫ db

≤ FGa,b L1 (X ,S1 )−1

1

∫ da0

1

∫ db

FGa,b L1 (X ,S 2 )

Page 32: An  Lp  theory for outer measures. Application to singular  integrals.II

Proof of T(1) theorem

Applying outer Hoelder

Integrating trivially:

≤ F Lp (X ,S 2 ) Ga,b Lp ' (X ,S 2 )−1

1

∫ da0

1

∫ db

≤C F Lp (X ,S 2 ) Ga,b Lp ' (X ,S 2 )

Page 33: An  Lp  theory for outer measures. Application to singular  integrals.II

Proof of T(1) theorem

Using embedding theorem (a modified one with tilted triangles for Gab)

Similarly one proves this estimate for the other regions other than|x-y|<s, t<s. €

≤C fp

gp'

Page 34: An  Lp  theory for outer measures. Application to singular  integrals.II