Paraproducts in One and Several Variables M. Lacey and J. Metcalfe

Size: px
Start display at page:

Download "Paraproducts in One and Several Variables M. Lacey and J. Metcalfe"

Transcription

1 Paraproducts in One and Several Variables M. Lacey and J. Metcalfe Kelly Bickel Washington University St. Louis, Missouri IAS Workshop on Multiparameter Harmonic Analysis June 19, 2012

2 What is a Paraproduct?! A Paraproduct is a bilinear operator that is similar to, but nicer than, a product of two functions. Consider the following operator: Π(f, g)(s) := s f (t)g(t) dt, f, g C 1 0 (R). Then Π satisfies: Product Reconstruction: By Leibniz s rule, fg = Π(f, g) + Π(g, f ). Linearization Formula: For G C (R), we have G(f ) = G(0) + Π(f, G (f )). A Leibniz-type Rule: It follows immediately that Π(f, g) = f g. Then Π is almost a paraproduct. (generally, paraproducts also satisfy a Hölder s inequality.)

3 A Paraproduct is... A Paraproduct Π is a bilinear operator satisfying: product reconstruction, a linearization formula, a Hölder-type inequality, and a Leibniz-type rule: α Π(f, g) = Π ( α f, g). We study One-Parameter Model Paraproducts: Let I be an interval. Then φ I is a bump function adapted to I iff φ I 2 = 1 and D n φ I (x) I n 1/2 ( 1 + ) N x c(i ), n = 0, 1, I where c(i ) is the center of I and N is sufficiently large. Let D be the set of dyadic intervals. Define: B(f 1, f 2 ) := 2 I 1/2 φ 3,I f j, φ j,i, I D j=1 where, for each I, each φ j,i is adapted to I and two of the φ j,i have integral zero.

4 An Example For each dyadic interval I, the Haar function adapted to I is h I := I 1/2 (1 Il 1 Ir ), where I l is the left half of I, and I r is the right half of I. Moreover, define h 0 I := h I and h 1 I := h I. Then, the Haar Paraproducts are given by: B k1,k2,k3 (f 1, f 2 ) = I D I 1/2 f 1, h k1 I f 2, h k2 I h k3 I, where k j {0, 1} and two of the k j are zero. It can be shown that f 1 f 2 = B 1,0,0 (f 1, f 2 ) + B 0,1,0 (f 1, f 2 ) + B 0,0,1 (f 1, f 2 ).

5 Increase the Parameters! We also study Bi-parameter Model Paraproducts: Let R be the set of dyadic rectangles in R 2. A function φ R is adapted to the rectangle R, where R = R 1 R 2, if φ R (x) = φ R1 (x 1 )φ R2 (x 2 ), where each φ Rk is adapted to R k. The bi-parameter model paraproducts are of the form: B(f 1, f 2 ) = 2 R 1/2 φ 3,R f j, φ j,r, R R j=1 where each φ j,r is adapted to R and for each coordinate x k, k = 1, 2, there are two positions in j = 1, 2, 3 such that φ j,r (x 1, x 2 )dx k = 0 x i x k and R R. R Then we say B has x k zeros in the j th position (or {φ j,r } has x k zeros).

6 Main Results The main results proved in the paper are that both the one and bi-parameter model paraproducts satisfy a Hölder-type inequality: Theorem 1 (Coifman, Meyer 78), (Muscalu, Pipher, Tao, Thiele 04) Whenever 1 < p 1, p 2, 1/r = 1/p 1 + 1/p 2, and 0 < r <, B(f 1, f 2 ) r f 1 p1 f 2 p2.

7 Classical Coifman-Meyer Theorem Theorem 1 is a discrete version of the following one and bi-parameter results: Let m be a bounded function on R 2, smooth away from the origin and satisfying α m(ζ) 1 ζ α, for sufficiently many multi-indices α and define the bilinear operator T m (1) T m (1) (f, g) = m(ζ)ˆf (ζ 1 )ĝ(ζ 2 )e 2πix(ζ1+ζ2) dζ, R 2 for Schwartz functions f, g S(R). We can generalize this by allowing m to be defined on R 2n and f, g S(R n ). Theorem 2 (Coifman, Meyer, 78) If m is a symbol satisfying the above estimates, then the bilinear operator T (1) m maps L p L q L r whenever 1 < p, q, 1/r = 1/p + 1/q, and 0 < r <. by

8 Bi-parameter Coifman-Meyer Theorem Let m(ζ, η) be a bounded function on R 4, smooth away from {(ζ 1, η 1 ) = 0} {(ζ 2, η 2 ) = 0} and satisfying the estimate α ζ β η m(ζ, η) 1 (ζ 1, η 1 ) α1+β1 1 (ζ 2, η 2 ) α2+β2, for sufficiently many multi-indices α and β. Then we can define the bilinear operator T m (2) as follows: T m (2) (f, g) = m(ζ, η)ˆf (ζ)ĝ(η)e 2πix(ζ+η) dζdη, R 4 where f, g S(R 2 ). Theorem 3 (Muscalu, Pipher, Tao, Thiele 04) If m is a symbol satisfying the above estimates, then the bilinear operator T (2) m maps L p L q L r whenever 1 < p, q, 1/r = 1/p + 1/q, and 0 < r <.

9 Fractional Derivative Estimates Let f, g S(R 2 ) and for α > 0, define the fractional derivative D α by D α f (ζ) = ζ αˆf (ζ). There are paraproducts Π j for j = 0, 1, 2, 3 such that the Coifman-Meyer theorem applies to each Π j and 3 fg = Π j (f, g). j=0 Using the structure of the Π j, one can find paraproducts Π 1 and Π 2 with D α( Π 1 (f, g) ) = Π 1(f, D α g) and D α( Π 2 (f, g) ) = Π 2(D α f, g), and similar Π 0 and Π 3 paraproducts. Using the Coifman-Meyer theorem, calculate D α (fg) r 3 D α (Π j (f, g)) r j=0 D α f p g q + f p D α g q, for 1 < p, q, 1/r = 1/p + 1/q, and 0 < r <.

10 Fractional Partial Derivative Estimates For f S(R 2 ) and for α, β > 0, define the partial differential operator D α 1 Dβ 2 by D α 1 Dβ 2 f (ζ) = ζ 1 α ζ 2 βˆf (ζ). Then, for f, g S(R 2 ), using the bi-parameter Coifman-Meyer theorem and analogous manipulations of paraproducts, we have D α 1 D β 2 (fg) r D α 1 D β 2 f p g q + f p D α 1 D β 2 g q + D α 1 f p D β 2 g q + D β 2 f p D α 1 g q, for 1 < p, q, 1/r = 1/p + 1/q, and 0 < r <.

11 Square and Maximal Functions We are considering the following paraproducts: B(f 1, f 2 ) := I D 2 I 1/2 φ 3,I f j, φ j,i, where, for each I, each φ j,i is adapted to I and two of the φ j,i have integral zero. Without loss of generality,we can assume φ 2,I and φ 3,I always have integral zero. We will need the following variations of the maximal function and square function: g, φ 1,I M 1 g := sup 1 I I D I j=1 S j g := [ ] 1/2 g, φ j,i 2 1 I, for j = 2, 3. I I D

12 Maximal Function Bounds f, φ 1,I M 1 (f )(x) = sup 1 I Mf (x), I D I where M denotes the typical Hardy-Littlewood maximal function. Fix I D, say I = 2 K+1. Translate I so that it is centered at 0 and let y be in I. Then: f, φ I I 1 f (x) (1 + x / I ) 2 dx I I 1 R I f + I 1 R I f (x) (1 + x 2 / I 2 ) 1 dx Mf (y) + 2 K 1 f (x) dx( (j 1) /2 2(K+1) ) 1 j>k I j Mf (y) + 2 k j 1 2 j+1 f (x) dx j>k I j Mf (y), where I j is the interval centered around zero with length 2 j+1. As y I, it is clear that y I j.

13 Square Function Bounds Sf is more or less large only where f is large, which is reflected by Sf p f p 1 < p <. Partially follows because φ I, φ I is usually small. In particular, if all {φ I } have integral zero, then φ I, φ I C. I D For p = 2, restrict to finite sums, let f 2 = 1 and calculate: f, φ I 2 f, φ I φ I 2, I using Cauchy-Schwarz and then calculate ( ) 2 f, φ I 2 I I I 2 I I f, φ I φ I, f φ I, φ I f, φ I 2 I φ I, φ I.

14 Proof of One-Parameter Result Recall: We are trying to show that B maps L p1 L p2 L r whenever 1 < p 1, p 2, 1/r = 1/p 1 + 1/p 2, and 0 < r <. Case 1: 1 < r < In this case, L.M. use a duality argument. We will need the following obvious fact: If {a j,i } I D are sequences such that {a 1,I } l, {a 2,I }, {a 3,I } l 2, then a 1,I a 2,I a 3,I a 1,I a 2,I 2 a 3,I 2, and in particular, ( 3 I D j=1 I D sup I D ) f j, φ j,i 1 I (x) I f 1, φ 1,I I 1 I (x) [ 3 f j, φ j,i 2 1 I (x) I j=2 = (M 1 f 1 )(S 2 f 2 )(S 3 f 3 )(x) I D ] 1/2

15 Proof of One-Parameter Result Case 1: 1 < r < Let r be dual to r, fix f 3 L r with f 3 r = 1, and calculate: B(f 1, f 2 ), f 3 = 2 I 1/2 φ 3,I f j, φ j,i f 3 I D j=1 3 I 3/2 f j, φ j,i 1 I I D j=1 (Mf 1 )(S 2 f 2 )(S 3 f 3 ) Mf 1 p1 S 2 f 2 p2 S 3 f 3 r f 1 p1 f 2 p2, where Hölder s inequality is used. Taking the supremum over all such f 3 yields: B(f 1, f 2 ) r f 1 p1 f 2 p2.

16 Proof of One-Parameter Result Case 2: 1/2 < r < 1 M.L. prove the following weak-type estimates: λ {B(f 1, f 2 ) > λ} 1/r f 1 p1 f 2 p2, (1) and multi-linear Marcinkiewicz interpolation yields the desired strong estimates. To get the weak estimates, use the following lemma: Lemma 1 (Auscher, Hofmann, Muscalu, Tao, Thiele 02) Let 0 < r <. If for all sets E with 0 < E <, there is subset E E with E E and f, 1 E A E 1/r then f r, A. In particular, let f = B(f 1, f 2 ) and A = f 1 p1 f 2 p2.

17 The Λ operator Consider the following multi-linear operator: Λ(f 1, f 2, f 3 ) := I D 3 I 1/2 f j, φ j,i. (2) Then, M.L. shows that for each f 1, f 2, and set E, there is a set E E with E E such that j=1 Λ(f 1, f 2, f 3 ) E 1/r f 1 p1 f 2 p2, for all f 3 supported in E and bounded by 1. (particularly, f 3 = 1 E.) By multi-linearity, we can assume f 1 p1 = f 2 p2 = 1. As the class of the multi-linear forms Λ is invariant under dilations by powers of two, we can assume E = 1. Specifically, if D λ is the dilation operator defined by (D λ f )(x) = f (λ 1 x) and Λ k (f 1, f 2, f 3 ) := 2 k Λ(D 2 k f 1, D 2 k f 2, D 2 k f 3 ), then Λ k is a multi-linear form of type (2) for k Z.

18 End! The End!

19 Paraproducts in One and Several Variables (Part II) M. Lacey and J. Metcalfe Kelly Bickel Washington University St. Louis, Missouri IAS Workshop on Multiparameter Harmonic Analysis June 19, 2012 Paraproducts in One and Several Variables (Part II) M. Lacey and J. Metca

20 Bi-parameter Paraproducts- Review Recall: for I be an interval, we say φ I is a bump function adapted to I iff φ I 2 = 1 and D n φ I (x) I n 1/2 ( 1 + ) N x c(i ), n = 0, 1, I where c(i ) is the center of I and N is sufficiently large. Last time, we considered paraproducts of the form: B(f 1, f 2 ) := I D 2 I 1/2 φ 3,I f j, φ j,i, where, for each I, each φ j,i is adapted to I and two of the φ j,i have integral zero. Let R be the set of dyadic rectangles in R 2. A function φ R is adapted to the rectangle R, where R = R 1 R 2, if where each φ Rk is adapted to R k. j=1 φ R (x) = φ R1 (x 1 )φ R2 (x 2 ), Paraproducts in One and Several Variables (Part II) M. Lacey and J. Metca

21 Bi-parameter Paraproducts- Review The bi-parameter model paraproducts are of the form: B(f 1, f 2 ) = R R R 1/2 φ 3,R 2 f j, φ j,r, where each φ j,r is adapted to R and for each coordinate x k, k = 1, 2, there are two positions in j = 1, 2, 3 such that φ j,r (x 1, x 2 )dx k = 0 x i x k and R R. R Then we say B has x k zeros in the j th position (or {φ j,r } has x k zeros). Theorem 2 (Muscalu, Pipher, Tao, Thiele 04) Whenever 1 < p 1, p 2, 1/r = 1/p 1 + 1/p 2, and 0 < r <, j=1 B(f 1, f 2 ) r f 1 p1 f 2 p2. Paraproducts in One and Several Variables (Part II) M. Lacey and J. Metca

22 Variants of Square and Maximal functions Again, M.L. use variants of square and maximal functions, adapted to the specific bump functions appearing in the given paraproduct B. Consider the following iterates of one-variable square and maximal functions: f, φ R MM(f ) := sup 1 R R R R S 1 M 2 (f ) := SS(f ) := [ sup R R 2 D 1 D [ R R ] 1/2 f, φ R1 R R, R = R 1 R 2 R ] 1/2 f, φ R 2 1 R, R where we can similarly define S 2 M 1, M 1 S 2, and M 2 S 1. If a square function is applied to the set {φ R } in the x k coordinate, we require the functions {φ R } to have x k zeros. Paraproducts in One and Several Variables (Part II) M. Lacey and J. Metca

23 Biparameter Proof: Case 1 As before, the interated square and maximal functions are bounded from L p L p, for 1 < p <. Specficically, if T is an operator on the previous slide, Tf p f p for 1 < p <. As before, we define the multilinear form Λ by for f 3 L r, and have: Λ(f 1, f 2, f 3 ) = R R R 1/2 B(f 1, f 2 ), f 3 Λ(f 1, f 2, f 3 ) 3 f j, φ j,r j=1 = 3 R 1/2 f j, φ j,r 1 R, R R j=1 We will use operators to bound the sum inside the integral. The operators we choose will depend on where B has zeros in each coordinate. Paraproducts in One and Several Variables (Part II) M. Lacey and J. Metca

24 Bi-parameter Proof Case 1 To illustrate, assume B has x 2 zeros in the j = 1, 2 positions and x 1 zeros in the j = 2, 3 positions. Then we have: R R j=1 3 R 1/2 f j, φ j,r 1 R sup R R 2 D 1 D f 3, φ 3,R R 1 R 2 j=1 ( R 2 D ) 1/2 f j, φ j,r 2 1 R R sup R 1 ( R 2 ) 1 ( 2 f 1, φ 1,R 2 1 R R R ) 1 ( f 2, φ 2,R 2 2 f 3, φ 3,R 2 1 R sup R R 2 R R 1 1 R ) 1 2 = (M 1 S 2 f 1 )(SSf 2 )(S 1 M 2 f 3 ) (S 2 M 1 f 1 )(SSf 2 )(S 1 M 2 f 3 ). Paraproducts in One and Several Variables (Part II) M. Lacey and J. Metca

25 Bi-parameter Proof Case 1 In general, there are 3 iterated square/maximal operators T j for j = 1, 2, 3 with B(f 1, f 2 ), f 3 Λ(f 1, f 2, f 3 ) = 3 R 1/2 f j, φ j,r 1 R R R j=1 T 1 f 1 T 2 f 2 T 3 f 3. Case 1: For 1 < r <, let r be dual to r and choose f 3 L r with f 3 r = 1. Then B(f 1, f 2 ), f 3 T 1 f 1 p1 T 2 f 2 p2 T 3 f 3 r which gives the result for 1 < r <. f 1 p1 f 2 p2, Paraproducts in One and Several Variables (Part II) M. Lacey and J. Metca

26 Bi-parameter Proof Case 2 Case 2: 1/2 < r < 1 M.L. prove the following weak-type estimates: λ {B(f 1, f 2 ) > λ} 1/r f 1 p1 f 2 p2, and multi-linear Marcinkiewicz interpolation yields the desired strong estimates. To get the weak estimates, show, that for each f 1, f 2 with f 1 p1 = f 2 p2 = 1 and set E with E = 1, there is a set E with E E with E E and Λ(f 1, f 2, f 3 ) 1, for every f 3 supported in E and bounded by 1. Further, we can assume each f j is smooth and compactly supported. Let T j, for j = 1, 2, 3, be the operators bounding B as in the previous slide. Paraproducts in One and Several Variables (Part II) M. Lacey and J. Metca

27 O Notation We will be estimating Λ(f 1, f 2, f 3 ) = R R R 1/2 3 f j, φ j,r. In particular, we will decompose R into several classes of rectangles. Let O be a class of dyadic rectangles. Then define sum(o) = R O R 1/2 j=1 3 f j, φ j,r. Recall that for each iterated operator T j we were summing (or sup-ing) over f, φ R, for R R. Let T O denote an iterated square or maximal function restricted to the class of dyadic rectangles O. For example, if T = SS, ( ) 1/2 f, φ R 2 T O f = 1 R. R R O Before we define E, we need to establish several bounds on sum(o) and T O 2 for classes of rectangles O satisfying special properties. j=1 Paraproducts in One and Several Variables (Part II) M. Lacey and J. Metca

28 Technical Lemma 1 Lemma 2 Let O R and let µ > 1 be a constant such that supp(f ) µr = R O, for a given function f. Then T O f 2 µ N f 2, where N = N N 0, where N is the integer in the definition of adapted for the {φ R } defining T, and N 0 is the smallest integer needed to get the L p bounds on the square and maximal functions. Idea of Proof Let {φ R } be adapted with integer N > 0. One can define a new set of adapted functions { φ R } adapted with integer N 0 such that φ R (x) = µ N φ R (x) x µr. Define T with the {φ R } and T with the { φ R }. If f satisfies the assumptions of the lemma, then T O f = µ N TO f, and the result follows since T is bounded on L 2, with bounds independent of µ. Paraproducts in One and Several Variables (Part II) M. Lacey and J. Metca

29 Technical Lemma 2 Lemma 3 Let c 1, c 2, c 3 > 0 be constants and O a collection of rectangles such that R {T j f j > c j } R for R O, j = 1, 2, 3. (3) Then we have the estimate: sum(o) c 1 c 2 c 3 sho. If (3) is not known for j = 3, we have: sum(o) c 1 c 2 sho 1/2 T 3O f 3 2. Idea of Proof: Let W = sh(o) 3 j=1 {T jf j < c j }, so that R W R. Then: 3 sum(o) R 1/2 f j, φ j,r 1 R W R O j=1 W T 1 f 1 T 2 f 2 T 3 f 3 sh(o) c 1 c 2 c 3. Paraproducts in One and Several Variables (Part II) M. Lacey and J. Metca

30 Definition of E Fix f 1, f 2, E with f 1 p1 = f 2 p2 = E = 1. Define 4ν = min(p 1, p 2 ) and let T 0 be the strong maximal function (in two parameters). Define Ω j,l := {T j f j > C2 l }, l Z, j = 1, 2, Ω l := 2 j=1ω j,l, Ω := l N {T 0 1 Ωl > 2 νl /100}, Ω := {T 0 1 Ω > 1/2}. Set E = Ω c E. We can choose C so that E 1/2 by choosing C so that Ω < 1/8. Using the L 2 boundedness oft 0 and L p j boundedness of the T j for j = 1, 2, we have Ω K 1 Ω l 2 2νl K 2 l N l N j=1 2 C p j 2 l(2ν p j ), which converges, and so we can choose C >> 0 to give Ω the desired size. Paraproducts in One and Several Variables (Part II) M. Lacey and J. Metca

31 Decomposition of R Recall, we are trying to show: Λ(f 1, f 2, f 3 ) = R R R 1/2 3 f j, φ j,r 1, where f 3 is bounded by one and supported on E. Then, for 1 < p 3 <, f 3 p3 1. We consider the sum restricted to specific classes of rectangles in R and split the rectangles into classes as follows: j=1 R is in class O j,l iff l is the greatest integer so that R Ω j,l = R {T j f j > C2 l } R. As the T j f j are bounded, every rectangle R is in precisely one O j,l for each j and so we can associate to each R a tuple l = (l 1, l 2, l 3 ) of integers. Paraproducts in One and Several Variables (Part II) M. Lacey and J. Metca

32 l with l1, l 2 0 Let L denote the tuples with l 1, l 2, l 3 0. Fix such an l = (l 1, l 2, l 3 ) and define Then for each R O l, and j = 1, 2, 3, O l = 3 j=1o j,lj. R Ω j,lj +1 = R {T j f j > C2 l j +1 } < R. and so Technical Lemma 2 yields: sum(o l ) sh(o l ) 2 l1+l2+l3. The L p j -boundedness of T j implies that, for θ 1 + θ 2 + θ 3 = 1, sh(o l ) sh(o 1,l1 ) θ1 sh(o 2,l2 ) θ2 sh(o 3,l3 ) θ3 2 p1l1θ1 p2l2θ2 p3l3θ3. Then we can calculate sum(o l ) 2 l1(1 p1θ1)+l2(1 p2θ2)+l3(1 p3θ3), l L l L which converges for θ 1, θ 2, θ 3 and p 3 > 0 with 1 p j θ j > 0. Paraproducts in One and Several Variables (Part II) M. Lacey and J. Metca

33 l with l1 > 0 or l 2 > 0 Let G denote the tuples with at least one of l 1, l 2 0. Fix such an l = (l 1, l 2, l 3 ) and define O l = 2 j=1o j,lj. Fix such an l and without loss of generality, assume l 1 > 0. Let R O l. Let 2 νl1/2 R be the rectangle obtained by dilating each side of R by a factor of 2 νl1/2 and keeping the same center. Then 1 2 νl1/2 R 2 νl 1 /2 R which implies 2 µl1/2 R Ω and so Technical Lemma 1 gives: for N sufficiently large. 1 Ωl1 = 2 νl1/2 R Ω l1 / 2 νl1/2 R R Ω l1 /2 νl1 R 2 νl1 /100, 2 νl1/2 R supp(f 3 ) = R O l. T Ol,3f N νl 1/2 f l1, Paraproducts in One and Several Variables (Part II) M. Lacey and J. Metca

34 l with l1 > 0 or l 2 > 0 Actually, we showed: Now, as each R O l satisfies: T Ol,3f 3 2 min(2 10l1, 2 10l2 ). R {T j f j > C2 l j +1 } R for R O l, j = 1, 2, Technical Lemma 2 implies: sum(o l ) 2 l1+l2 sho l 1/2 T Ol,3f l1+l2 min(2 10l1, 2 10l2 ), which is clearly summable over all tuples (l 1, l 2 ) with l 1 or l 2 positive. This covers the entire class of dyadic rectangles. Thus, we have proved: as desired. Λ(f 1, f 2, f 3 ) = R R R 1/2 3 f j, φ j,r 1, j=1 Paraproducts in One and Several Variables (Part II) M. Lacey and J. Metca

A SHORT PROOF OF THE COIFMAN-MEYER MULTILINEAR THEOREM

A SHORT PROOF OF THE COIFMAN-MEYER MULTILINEAR THEOREM A SHORT PROOF OF THE COIFMAN-MEYER MULTILINEAR THEOREM CAMIL MUSCALU, JILL PIPHER, TERENCE TAO, AND CHRISTOPH THIELE Abstract. We give a short proof of the well known Coifman-Meyer theorem on multilinear

More information

MULTI-PARAMETER PARAPRODUCTS

MULTI-PARAMETER PARAPRODUCTS MULTI-PARAMETER PARAPRODUCTS CAMIL MUSCALU, JILL PIPHER, TERENCE TAO, AND CHRISTOPH THIELE Abstract. We prove that the classical Coifman-Meyer theorem holds on any polydisc T d of arbitrary dimension d..

More information

Paraproducts and the bilinear Calderón-Zygmund theory

Paraproducts and the bilinear Calderón-Zygmund theory Paraproducts and the bilinear Calderón-Zygmund theory Diego Maldonado Department of Mathematics Kansas State University Manhattan, KS 66506 12th New Mexico Analysis Seminar April 23-25, 2009 Outline of

More information

arxiv:math.ca/ v1 23 Oct 2003

arxiv:math.ca/ v1 23 Oct 2003 BI-PARAMETER PARAPRODUCTS arxiv:math.ca/3367 v 23 Oct 23 CAMIL MUSCALU, JILL PIPHER, TERENCE TAO, AND CHRISTOPH THIELE Abstract. In the first part of the paper we prove a bi-parameter version of a well

More information

T (1) and T (b) Theorems on Product Spaces

T (1) and T (b) Theorems on Product Spaces T (1) and T (b) Theorems on Product Spaces Yumeng Ou Department of Mathematics Brown University Providence RI yumeng ou@brown.edu June 2, 2014 Yumeng Ou (BROWN) T (1) and T (b) Theorems on Product Spaces

More information

Characterization of multi parameter BMO spaces through commutators

Characterization of multi parameter BMO spaces through commutators Characterization of multi parameter BMO spaces through commutators Stefanie Petermichl Université Paul Sabatier IWOTA Chemnitz August 2017 S. Petermichl (Université Paul Sabatier) Commutators and BMO Chemnitz

More information

Michael Lacey and Christoph Thiele. f(ξ)e 2πiξx dξ

Michael Lacey and Christoph Thiele. f(ξ)e 2πiξx dξ Mathematical Research Letters 7, 36 370 (2000) A PROOF OF BOUNDEDNESS OF THE CARLESON OPERATOR Michael Lacey and Christoph Thiele Abstract. We give a simplified proof that the Carleson operator is of weaktype

More information

Duality of multiparameter Hardy spaces H p on spaces of homogeneous type

Duality of multiparameter Hardy spaces H p on spaces of homogeneous type Duality of multiparameter Hardy spaces H p on spaces of homogeneous type Yongsheng Han, Ji Li, and Guozhen Lu Department of Mathematics Vanderbilt University Nashville, TN Internet Analysis Seminar 2012

More information

Multi-Parameter Riesz Commutators

Multi-Parameter Riesz Commutators Multi-Parameter Riesz Commutators Brett D. Wick Vanderbilt University Department of Mathematics Sixth Prairie Analysis Seminar University of Kansas October 14th, 2006 B. D. Wick (Vanderbilt University)

More information

Analytic families of multilinear operators

Analytic families of multilinear operators Analytic families of multilinear operators Mieczysław Mastyło Adam Mickiewicz University in Poznań Nonlinar Functional Analysis Valencia 17-20 October 2017 Based on a joint work with Loukas Grafakos M.

More information

arxiv:math/ v2 [math.ca] 18 Jan 2006

arxiv:math/ v2 [math.ca] 18 Jan 2006 COMMUTATORS WITH REISZ POTENTIALS IN ONE AND SEVERAL PARAMETERS arxiv:math/0502336v2 [math.ca] 18 Jan 2006 MICHAEL T. LACEY GEORGIA INSTITUTE OF TECHNOLOGY Abstract. Let M b be the operator of pointwise

More information

A characterization of the two weight norm inequality for the Hilbert transform

A characterization of the two weight norm inequality for the Hilbert transform A characterization of the two weight norm inequality for the Hilbert transform Ignacio Uriarte-Tuero (joint works with Michael T. Lacey, Eric T. Sawyer, and Chun-Yen Shen) September 10, 2011 A p condition

More information

Bilinear pseudodifferential operators: the Coifman-Meyer class and beyond

Bilinear pseudodifferential operators: the Coifman-Meyer class and beyond Bilinear pseudodifferential operators: the Coifman-Meyer class and beyond Árpád Bényi Department of Mathematics Western Washington University Bellingham, WA 98225 12th New Mexico Analysis Seminar April

More information

MULTIPARAMETER RIESZ COMMUTATORS. 1. Introduction

MULTIPARAMETER RIESZ COMMUTATORS. 1. Introduction MULTIPARAMETER RIESZ COMMUTATORS MICHAEL T. LACEY 1, STEFANIE PETERMICHL 2, JILL C. PIPHER 3, AND BRETT D. WICK 4 Abstract. It is shown that product BMO of S.-Y. A. Chang and R. Fefferman, ined on the

More information

Teoría de pesos para operadores multilineales, extensiones vectoriales y extrapolación

Teoría de pesos para operadores multilineales, extensiones vectoriales y extrapolación Teoría de pesos para operadores multilineales, extensiones vectoriales y extrapolación Encuentro Análisis Funcional Sheldy Ombrosi Universidad Nacional del Sur y CONICET 8 de marzo de 208 If f is a locally

More information

1 I (x)) 1/2 I. A fairly immediate corollary of the techniques discussed in the last lecture is Theorem 1.1. For all 1 < p <

1 I (x)) 1/2 I. A fairly immediate corollary of the techniques discussed in the last lecture is Theorem 1.1. For all 1 < p < 1. Lecture 4 1.1. Square functions, paraproducts, Khintchin s inequality. The dyadic Littlewood Paley square function of a function f is defined as Sf(x) := ( f, h 2 1 (x)) 1/2 where the summation goes

More information

Dyadic structure theorems for multiparameter function spaces

Dyadic structure theorems for multiparameter function spaces Rev. Mat. Iberoam., 32 c European Mathematical Society Dyadic structure theorems for multiparameter function spaces Ji Li, Jill Pipher and Lesley A. Ward Abstract. We prove that the multiparameter (product)

More information

LOUKAS GRAFAKOS, DANQING HE, AND PETR HONZÍK

LOUKAS GRAFAKOS, DANQING HE, AND PETR HONZÍK THE HÖRMADER MULTIPLIER THEOREM, II: THE BILIEAR LOCAL L 2 CASE LOUKAS GRAFAKOS, DAQIG HE, AD PETR HOZÍK ABSTRACT. We use wavelets of tensor product type to obtain the boundedness of bilinear multiplier

More information

Weighted norm inequalities for singular integral operators

Weighted norm inequalities for singular integral operators Weighted norm inequalities for singular integral operators C. Pérez Journal of the London mathematical society 49 (994), 296 308. Departmento de Matemáticas Universidad Autónoma de Madrid 28049 Madrid,

More information

Weak Factorization and Hankel operators on Hardy spaces H 1.

Weak Factorization and Hankel operators on Hardy spaces H 1. Weak Factorization and Hankel operators on Hardy spaces H 1. Aline Bonami Université d Orléans Bardonecchia, June 16, 2009 Let D be the unit disc (or B n C n ) the unit ball ), D its boundary. The Holomorphic

More information

A survey on l 2 decoupling

A survey on l 2 decoupling A survey on l 2 decoupling Po-Lam Yung 1 The Chinese University of Hong Kong January 31, 2018 1 Research partially supported by HKRGC grant 14313716, and by CUHK direct grants 4053220, 4441563 Introduction

More information

A Characterization of Product BM O by Commutators

A Characterization of Product BM O by Commutators arxiv:math/0104144v2 [math.ca] 22 Mar 2002 A Characterization of Product BM O by Commutators Michael T. Lacey Georgia Institute of Technology 1 Introduction Sarah H. Ferguson Wayne State University In

More information

arxiv: v3 [math.ca] 6 Oct 2009

arxiv: v3 [math.ca] 6 Oct 2009 SHARP A 2 INEQUALITY FOR HAAR SHIFT OPERATORS arxiv:09061941v3 [mathca] 6 Oct 2009 MICHAEL T LACEY, STEFANIE PETERMICHL, AND MARIA CARMEN REGUERA Abstract As a Corollary to the main result of the paper

More information

Chapter One. The Calderón-Zygmund Theory I: Ellipticity

Chapter One. The Calderón-Zygmund Theory I: Ellipticity Chapter One The Calderón-Zygmund Theory I: Ellipticity Our story begins with a classical situation: convolution with homogeneous, Calderón- Zygmund ( kernels on R n. Let S n 1 R n denote the unit sphere

More information

Contents. 1. Introduction Decomposition 5 arxiv:math/ v4 [math.ca] 9 Aug Complements The Central Lemmas 11

Contents. 1. Introduction Decomposition 5 arxiv:math/ v4 [math.ca] 9 Aug Complements The Central Lemmas 11 Contents 1. Introduction 2 2. Decomposition 5 arxiv:math/0307008v4 [math.ca] 9 Aug 2005 2.1. Complements 10 3. The Central Lemmas 11 3.1. Complements 14 4. The Density Lemma 14 4.1. Complements 15 5. The

More information

JUHA KINNUNEN. Harmonic Analysis

JUHA KINNUNEN. Harmonic Analysis JUHA KINNUNEN Harmonic Analysis Department of Mathematics and Systems Analysis, Aalto University 27 Contents Calderón-Zygmund decomposition. Dyadic subcubes of a cube.........................2 Dyadic cubes

More information

Weighted Littlewood-Paley inequalities

Weighted Littlewood-Paley inequalities Nicolaus Copernicus University, Toruń, Poland 3-7 June 2013, Herrnhut, Germany for every interval I in R let S I denote the partial sum operator, i.e., (S I f ) = χ I f (f L2 (R)), for an arbitrary family

More information

NEW MAXIMAL FUNCTIONS AND MULTIPLE WEIGHTS FOR THE MULTILINEAR CALDERÓN-ZYGMUND THEORY

NEW MAXIMAL FUNCTIONS AND MULTIPLE WEIGHTS FOR THE MULTILINEAR CALDERÓN-ZYGMUND THEORY NEW MAXIMAL FUNCTIONS AND MULTIPLE WEIGHTS FOR THE MULTILINEAR CALDERÓN-ZYGMUND THEORY ANDREI K. LERNER, SHELDY OMBROSI, CARLOS PÉREZ, RODOLFO H. TORRES, AND RODRIGO TRUJILLO-GONZÁLEZ Abstract. A multi(sub)linear

More information

U = 1 b. We fix the identification G a (F ) U sending b to ( 1 b

U = 1 b. We fix the identification G a (F ) U sending b to ( 1 b LECTURE 11: ADMISSIBLE REPRESENTATIONS AND SUPERCUSPIDALS I LECTURE BY CHENG-CHIANG TSAI STANFORD NUMBER THEORY LEARNING SEMINAR JANUARY 10, 2017 NOTES BY DAN DORE AND CHENG-CHIANG TSAI Let L is a global

More information

The Discrepancy Function and the Small Ball Inequality in Higher Dimensions

The Discrepancy Function and the Small Ball Inequality in Higher Dimensions The Discrepancy Function and the Small Ball Inequality in Higher Dimensions Dmitriy Georgia Institute of Technology (joint work with M. Lacey and A. Vagharshakyan) 2007 Fall AMS Western Section Meeting

More information

212a1214Daniell s integration theory.

212a1214Daniell s integration theory. 212a1214 Daniell s integration theory. October 30, 2014 Daniell s idea was to take the axiomatic properties of the integral as the starting point and develop integration for broader and broader classes

More information

Jordan Journal of Mathematics and Statistics (JJMS) 9(1), 2016, pp BOUNDEDNESS OF COMMUTATORS ON HERZ-TYPE HARDY SPACES WITH VARIABLE EXPONENT

Jordan Journal of Mathematics and Statistics (JJMS) 9(1), 2016, pp BOUNDEDNESS OF COMMUTATORS ON HERZ-TYPE HARDY SPACES WITH VARIABLE EXPONENT Jordan Journal of Mathematics and Statistics (JJMS 9(1, 2016, pp 17-30 BOUNDEDNESS OF COMMUTATORS ON HERZ-TYPE HARDY SPACES WITH VARIABLE EXPONENT WANG HONGBIN Abstract. In this paper, we obtain the boundedness

More information

Hardy spaces of Dirichlet series and function theory on polydiscs

Hardy spaces of Dirichlet series and function theory on polydiscs Hardy spaces of Dirichlet series and function theory on polydiscs Kristian Seip Norwegian University of Science and Technology (NTNU) Steinkjer, September 11 12, 2009 Summary Lecture One Theorem (H. Bohr)

More information

SOBOLEV SPACE ESTIMATES AND SYMBOLIC CALCULUS FOR BILINEAR PSEUDODIFFERENTIAL OPERATORS

SOBOLEV SPACE ESTIMATES AND SYMBOLIC CALCULUS FOR BILINEAR PSEUDODIFFERENTIAL OPERATORS SOBOLEV SPACE ESTIMATES AND SYMBOLIC CALCULUS FOR BILINEAR PSEUDODIFFERENTIAL OPERATORS Abstract. Bilinear operators are investigated in the context of Sobolev spaces and various techniques useful in the

More information

BOUNDS FOR A MAXIMAL DYADIC SUM OPERATOR

BOUNDS FOR A MAXIMAL DYADIC SUM OPERATOR L p BOUNDS FOR A MAXIMAL DYADIC SUM OPERATOR LOUKAS GRAFAKOS, TERENCE TAO, AND ERIN TERWILLEGER Abstract. The authors prove L p bounds in the range

More information

SCALE INVARIANT FOURIER RESTRICTION TO A HYPERBOLIC SURFACE

SCALE INVARIANT FOURIER RESTRICTION TO A HYPERBOLIC SURFACE SCALE INVARIANT FOURIER RESTRICTION TO A HYPERBOLIC SURFACE BETSY STOVALL Abstract. This result sharpens the bilinear to linear deduction of Lee and Vargas for extension estimates on the hyperbolic paraboloid

More information

Classical Fourier Analysis

Classical Fourier Analysis Loukas Grafakos Classical Fourier Analysis Second Edition 4y Springer 1 IP Spaces and Interpolation 1 1.1 V and Weak IP 1 1.1.1 The Distribution Function 2 1.1.2 Convergence in Measure 5 1.1.3 A First

More information

A new class of pseudodifferential operators with mixed homogenities

A new class of pseudodifferential operators with mixed homogenities A new class of pseudodifferential operators with mixed homogenities Po-Lam Yung University of Oxford Jan 20, 2014 Introduction Given a smooth distribution of hyperplanes on R N (or more generally on a

More information

MATH6081A Homework 8. In addition, when 1 < p 2 the above inequality can be refined using Lorentz spaces: f

MATH6081A Homework 8. In addition, when 1 < p 2 the above inequality can be refined using Lorentz spaces: f MATH68A Homework 8. Prove the Hausdorff-Young inequality, namely f f L L p p for all f L p (R n and all p 2. In addition, when < p 2 the above inequality can be refined using Lorentz spaces: f L p,p f

More information

A RELATIONSHIP BETWEEN THE DIRICHLET AND REGULARITY PROBLEMS FOR ELLIPTIC EQUATIONS. Zhongwei Shen

A RELATIONSHIP BETWEEN THE DIRICHLET AND REGULARITY PROBLEMS FOR ELLIPTIC EQUATIONS. Zhongwei Shen A RELATIONSHIP BETWEEN THE DIRICHLET AND REGULARITY PROBLEMS FOR ELLIPTIC EQUATIONS Zhongwei Shen Abstract. Let L = diva be a real, symmetric second order elliptic operator with bounded measurable coefficients.

More information

RESULTS ON FOURIER MULTIPLIERS

RESULTS ON FOURIER MULTIPLIERS RESULTS ON FOURIER MULTIPLIERS ERIC THOMA Abstract. The problem of giving necessary and sufficient conditions for Fourier multipliers to be bounded on L p spaces does not have a satisfactory answer for

More information

MULTILINEAR CALDERÓN ZYGMUND SINGULAR INTEGRALS

MULTILINEAR CALDERÓN ZYGMUND SINGULAR INTEGRALS MULTILINEAR CALDERÓN ZYGMUND SINGULAR INTEGRALS LOUKAS GRAFAKOS Contents 1. Introduction 1 2. Bilinear Calderón Zygmund operators 4 3. Endpoint estimates and interpolation for bilinear Calderón Zygmund

More information

HAAR SHIFTS, COMMUTATORS, AND HANKEL OPERATORS

HAAR SHIFTS, COMMUTATORS, AND HANKEL OPERATORS REVISTA DE LA UNIÓN MATEMÁTICA ARGENTINA Volumen 50, Número 2, 2009, Páginas 3 HAAR SHIFTS, COMMUTATORS, AND HANKEL OPERATORS MICHAEL LACEY Abstract. Hankel operators lie at the junction of analytic and

More information

Locally convex spaces, the hyperplane separation theorem, and the Krein-Milman theorem

Locally convex spaces, the hyperplane separation theorem, and the Krein-Milman theorem 56 Chapter 7 Locally convex spaces, the hyperplane separation theorem, and the Krein-Milman theorem Recall that C(X) is not a normed linear space when X is not compact. On the other hand we could use semi

More information

Borderline variants of the Muckenhoupt-Wheeden inequality

Borderline variants of the Muckenhoupt-Wheeden inequality Borderline variants of the Muckenhoupt-Wheeden inequality Carlos Domingo-Salazar Universitat de Barcelona joint work with M Lacey and G Rey 3CJI Murcia, Spain September 10, 2015 The Hardy-Littlewood maximal

More information

Hardy spaces associated to operators satisfying Davies-Gaffney estimates and bounded holomorphic functional calculus.

Hardy spaces associated to operators satisfying Davies-Gaffney estimates and bounded holomorphic functional calculus. Hardy spaces associated to operators satisfying Davies-Gaffney estimates and bounded holomorphic functional calculus. Xuan Thinh Duong (Macquarie University, Australia) Joint work with Ji Li, Zhongshan

More information

MULTILINEAR HARMONIC ANALYSIS. 1. Introduction

MULTILINEAR HARMONIC ANALYSIS. 1. Introduction MULTILINEAR HARMONIC ANALYSIS LOUKAS GRAFAKOS Abstract. This article contains an expanded version of the material covered by the author in two 90-minute lectures at the 9th international school on Nonlinear

More information

Decouplings and applications

Decouplings and applications April 27, 2018 Let Ξ be a collection of frequency points ξ on some curved, compact manifold S of diameter 1 in R n (e.g. the unit sphere S n 1 ) Let B R = B(c, R) be a ball with radius R 1. Let also a

More information

ABSTRACT SCATTERING SYSTEMS: SOME SURPRISING CONNECTIONS

ABSTRACT SCATTERING SYSTEMS: SOME SURPRISING CONNECTIONS ABSTRACT SCATTERING SYSTEMS: SOME SURPRISING CONNECTIONS Cora Sadosky Department of Mathematics Howard University Washington, DC, USA csadosky@howard.edu Department of Mathematics University of New Mexico

More information

for all subintervals I J. If the same is true for the dyadic subintervals I D J only, we will write ϕ BMO d (J). In fact, the following is true

for all subintervals I J. If the same is true for the dyadic subintervals I D J only, we will write ϕ BMO d (J). In fact, the following is true 3 ohn Nirenberg inequality, Part I A function ϕ L () belongs to the space BMO() if sup ϕ(s) ϕ I I I < for all subintervals I If the same is true for the dyadic subintervals I D only, we will write ϕ BMO

More information

WEAK HARDY SPACES LOUKAS GRAFAKOS AND DANQING HE

WEAK HARDY SPACES LOUKAS GRAFAKOS AND DANQING HE WEAK HARDY SPACES LOUKAS GRAFAKOS AND DANQING HE Abstract. We provide a careful treatment of the weak Hardy spaces H p, (R n ) for all indices 0 < p

More information

4 Sobolev spaces, trace theorem and normal derivative

4 Sobolev spaces, trace theorem and normal derivative 4 Sobolev spaces, trace theorem and normal derivative Throughout, n will be a sufficiently smooth, bounded domain. We use the standard Sobolev spaces H 0 ( n ) := L 2 ( n ), H 0 () := L 2 (), H k ( n ),

More information

DISCRETE LITTLEWOOD-PALEY-STEIN THEORY AND MULTI-PARAMETER HARDY SPACES ASSOCIATED WITH FLAG SINGULAR INTEGRALS

DISCRETE LITTLEWOOD-PALEY-STEIN THEORY AND MULTI-PARAMETER HARDY SPACES ASSOCIATED WITH FLAG SINGULAR INTEGRALS DSCRETE LTTLEWOOD-PALEY-STEN THEORY AND MULT-PARAMETER HARDY SPACES ASSOCATED WTH LAG SNGULAR NTEGRALS Yongsheng Han Department of Mathematics Auburn University Auburn, AL 36849, U.S.A E-mail: hanyong@mail.auburn.edu

More information

Variational estimates for the bilinear iterated Fourier integral

Variational estimates for the bilinear iterated Fourier integral Variational estimates for the bilinear iterated Fourier integral Yen Do, University of Virginia joint with Camil Muscalu and Christoph Thiele Two classical operators in time-frequency analysis: (i) The

More information

Carleson Measures for Besov-Sobolev Spaces and Non-Homogeneous Harmonic Analysis

Carleson Measures for Besov-Sobolev Spaces and Non-Homogeneous Harmonic Analysis Carleson Measures for Besov-Sobolev Spaces and Non-Homogeneous Harmonic Analysis Brett D. Wick Georgia Institute of Technology School of Mathematics & Humboldt Fellow Institut für Mathematik Universität

More information

arxiv: v2 [math.ca] 29 Apr 2015

arxiv: v2 [math.ca] 29 Apr 2015 AN L 4 ESTIMATE FO A SINGULA ENTANGLED QUADILINEA FOM POLONA DUCIK arxiv:42.2384v2 [math.ca] 29 Apr 25 Abstract. The twisted paraproduct can be viewed as a two-dimensional trilinear form which appeared

More information

HIGHER INTEGRABILITY WITH WEIGHTS

HIGHER INTEGRABILITY WITH WEIGHTS Annales Academiæ Scientiarum Fennicæ Series A. I. Mathematica Volumen 19, 1994, 355 366 HIGHER INTEGRABILITY WITH WEIGHTS Juha Kinnunen University of Jyväskylä, Department of Mathematics P.O. Box 35, SF-4351

More information

Boundedness of Fourier integral operators on Fourier Lebesgue spaces and related topics

Boundedness of Fourier integral operators on Fourier Lebesgue spaces and related topics Boundedness of Fourier integral operators on Fourier Lebesgue spaces and related topics Fabio Nicola (joint work with Elena Cordero and Luigi Rodino) Dipartimento di Matematica Politecnico di Torino Applied

More information

Sharp Bilinear Decompositions of Products of Hardy Spaces and Their Dual Spaces

Sharp Bilinear Decompositions of Products of Hardy Spaces and Their Dual Spaces Sharp Bilinear Decompositions of Products of Hardy Spaces and Their Dual Spaces p. 1/45 Sharp Bilinear Decompositions of Products of Hardy Spaces and Their Dual Spaces Dachun Yang (Joint work) dcyang@bnu.edu.cn

More information

M ath. Res. Lett. 16 (2009), no. 1, c International Press 2009

M ath. Res. Lett. 16 (2009), no. 1, c International Press 2009 M ath. Res. Lett. 16 (2009), no. 1, 149 156 c International Press 2009 A 1 BOUNDS FOR CALDERÓN-ZYGMUND OPERATORS RELATED TO A PROBLEM OF MUCKENHOUPT AND WHEEDEN Andrei K. Lerner, Sheldy Ombrosi, and Carlos

More information

FRACTIONAL DIFFERENTIATION: LEIBNIZ MEETS HÖLDER

FRACTIONAL DIFFERENTIATION: LEIBNIZ MEETS HÖLDER FRACTIONAL DIFFERENTIATION: LEIBNIZ MEETS HÖLDER LOUKAS GRAFAKOS Abstract. Abstract: We discuss how to estimate the fractional derivative of the product of two functions, not in the pointwise sense, but

More information

1 The Continuous Wavelet Transform The continuous wavelet transform (CWT) Discretisation of the CWT... 2

1 The Continuous Wavelet Transform The continuous wavelet transform (CWT) Discretisation of the CWT... 2 Contents 1 The Continuous Wavelet Transform 1 1.1 The continuous wavelet transform (CWT)............. 1 1. Discretisation of the CWT...................... Stationary wavelet transform or redundant wavelet

More information

V. CHOUSIONIS AND X. TOLSA

V. CHOUSIONIS AND X. TOLSA THE T THEOEM V. CHOUSIONIS AND X. TOLSA Introduction These are the notes of a short course given by X. Tolsa at the Universitat Autònoma de Barcelona between November and December of 202. The notes have

More information

SCHWARTZ SPACES ASSOCIATED WITH SOME NON-DIFFERENTIAL CONVOLUTION OPERATORS ON HOMOGENEOUS GROUPS

SCHWARTZ SPACES ASSOCIATED WITH SOME NON-DIFFERENTIAL CONVOLUTION OPERATORS ON HOMOGENEOUS GROUPS C O L L O Q U I U M M A T H E M A T I C U M VOL. LXIII 1992 FASC. 2 SCHWARTZ SPACES ASSOCIATED WITH SOME NON-DIFFERENTIAL CONVOLUTION OPERATORS ON HOMOGENEOUS GROUPS BY JACEK D Z I U B A Ń S K I (WROC

More information

MULTILINEAR SINGULAR INTEGRAL OPERATORS WITH VARIABLE COEFFICIENTS

MULTILINEAR SINGULAR INTEGRAL OPERATORS WITH VARIABLE COEFFICIENTS REVISTA DE LA UNIÓN MATEMÁTICA ARGENTINA Volumen 50, Número 2, 2009, Páginas 157 174 MULTILINEAR SINGULAR INTEGRAL OPERATORS WITH VARIABLE COEFFICIENTS RODOLFO H. TORRES Abstract. Some recent results for

More information

VARIATIONS ON THE THEME OF JOURNÉ S LEMMA. 1. Introduction, Journé s Lemma

VARIATIONS ON THE THEME OF JOURNÉ S LEMMA. 1. Introduction, Journé s Lemma VARIATIONS ON THE THEME OF JOURNÉ S LEMMA CARLOS CABRELLI, MICHAEL T. LACEY, URSULA MOLTER, AND JILL C. PIPHER arxiv:math/0412174v2 [math.ca] 9 Mar 2005 Abstract. Journé s Lemma [11] is a critical component

More information

The Calderon-Vaillancourt Theorem

The Calderon-Vaillancourt Theorem The Calderon-Vaillancourt Theorem What follows is a completely self contained proof of the Calderon-Vaillancourt Theorem on the L 2 boundedness of pseudo-differential operators. 1 The result Definition

More information

L. Levaggi A. Tabacco WAVELETS ON THE INTERVAL AND RELATED TOPICS

L. Levaggi A. Tabacco WAVELETS ON THE INTERVAL AND RELATED TOPICS Rend. Sem. Mat. Univ. Pol. Torino Vol. 57, 1999) L. Levaggi A. Tabacco WAVELETS ON THE INTERVAL AND RELATED TOPICS Abstract. We use an abstract framework to obtain a multilevel decomposition of a variety

More information

Both these computations follow immediately (and trivially) from the definitions. Finally, observe that if f L (R n ) then we have that.

Both these computations follow immediately (and trivially) from the definitions. Finally, observe that if f L (R n ) then we have that. Lecture : One Parameter Maximal Functions and Covering Lemmas In this first lecture we start studying one of the basic and fundamental operators in harmonic analysis, the Hardy-Littlewood maximal function.

More information

Fascículo 4. Some Topics in Dyadic Harmonic Analysis. Michael T. Lacey. Cursos y seminarios de matemática Serie B. Universidad de Buenos Aires

Fascículo 4. Some Topics in Dyadic Harmonic Analysis. Michael T. Lacey. Cursos y seminarios de matemática Serie B. Universidad de Buenos Aires Fascículo 4 Cursos y seminarios de matemática Serie B ISSN 1851-149X Michael T. Lacey Some Topics in Dyadic Harmonic Analysis Departamento de Matemática Facultad de Ciencias i Exactas y Naturales Universidad

More information

Herz (cf. [H], and also [BS]) proved that the reverse inequality is also true, that is,

Herz (cf. [H], and also [BS]) proved that the reverse inequality is also true, that is, REARRANGEMENT OF HARDY-LITTLEWOOD MAXIMAL FUNCTIONS IN LORENTZ SPACES. Jesús Bastero*, Mario Milman and Francisco J. Ruiz** Abstract. For the classical Hardy-Littlewood maximal function M f, a well known

More information

Bilinear operators, commutators and smoothing

Bilinear operators, commutators and smoothing Bilinear operators, commutators and smoothing Árpád Bényi Department of Mathematics Western Washington University, USA Harmonic Analysis and its Applications Matsumoto, August 24-28, 2016 Á. B. s research

More information

Multilinear And Multiparameter Pseudo- Differential Operators And Trudinger-Moser Inequalities

Multilinear And Multiparameter Pseudo- Differential Operators And Trudinger-Moser Inequalities Wayne State University Wayne State University Dissertations --06 Multilinear And Multiparameter Pseudo- Differential Operators And Trudinger-Moser Inequalities Lu Zhang Wayne State University, Follow this

More information

8 Singular Integral Operators and L p -Regularity Theory

8 Singular Integral Operators and L p -Regularity Theory 8 Singular Integral Operators and L p -Regularity Theory 8. Motivation See hand-written notes! 8.2 Mikhlin Multiplier Theorem Recall that the Fourier transformation F and the inverse Fourier transformation

More information

MULTILINEAR SINGULAR INTEGRALS. Christoph M. Thiele

MULTILINEAR SINGULAR INTEGRALS. Christoph M. Thiele Publ. Mat. (2002), 229 274 Proceedings of the 6 th International Conference on Harmonic Analysis and Partial Differential Equations. El Escorial, 2000. MULTILINEAR SINGULAR INTEGRALS Christoph M. Thiele

More information

General Franklin systems as bases in H 1 [0, 1]

General Franklin systems as bases in H 1 [0, 1] STUDIA MATHEMATICA 67 (3) (2005) General Franklin systems as bases in H [0, ] by Gegham G. Gevorkyan (Yerevan) and Anna Kamont (Sopot) Abstract. By a general Franklin system corresponding to a dense sequence

More information

Algebras of singular integral operators with kernels controlled by multiple norms

Algebras of singular integral operators with kernels controlled by multiple norms Algebras of singular integral operators with kernels controlled by multiple norms Alexander Nagel Conference in Harmonic Analysis in Honor of Michael Christ This is a report on joint work with Fulvio Ricci,

More information

Compactness for the commutators of multilinear singular integral operators with non-smooth kernels

Compactness for the commutators of multilinear singular integral operators with non-smooth kernels Appl. Math. J. Chinese Univ. 209, 34(: 55-75 Compactness for the commutators of multilinear singular integral operators with non-smooth kernels BU Rui CHEN Jie-cheng,2 Abstract. In this paper, the behavior

More information

On a class of pseudodifferential operators with mixed homogeneities

On a class of pseudodifferential operators with mixed homogeneities On a class of pseudodifferential operators with mixed homogeneities Po-Lam Yung University of Oxford July 25, 2014 Introduction Joint work with E. Stein (and an outgrowth of work of Nagel-Ricci-Stein-Wainger,

More information

PROBLEMS. (b) (Polarization Identity) Show that in any inner product space

PROBLEMS. (b) (Polarization Identity) Show that in any inner product space 1 Professor Carl Cowen Math 54600 Fall 09 PROBLEMS 1. (Geometry in Inner Product Spaces) (a) (Parallelogram Law) Show that in any inner product space x + y 2 + x y 2 = 2( x 2 + y 2 ). (b) (Polarization

More information

Overview of normed linear spaces

Overview of normed linear spaces 20 Chapter 2 Overview of normed linear spaces Starting from this chapter, we begin examining linear spaces with at least one extra structure (topology or geometry). We assume linearity; this is a natural

More information

In this note we give a rather simple proof of the A 2 conjecture recently settled by T. Hytönen [7]. Theorem 1.1. For any w A 2,

In this note we give a rather simple proof of the A 2 conjecture recently settled by T. Hytönen [7]. Theorem 1.1. For any w A 2, A SIMPLE PROOF OF THE A 2 CONJECTURE ANDREI K. LERNER Abstract. We give a simple proof of the A 2 conecture proved recently by T. Hytönen. Our proof avoids completely the notion of the Haar shift operator,

More information

L p -boundedness of the Hilbert transform

L p -boundedness of the Hilbert transform L p -boundedness of the Hilbert transform Kunal Narayan Chaudhury Abstract The Hilbert transform is essentially the only singular operator in one dimension. This undoubtedly makes it one of the the most

More information

MODULATION INVARIANT BILINEAR T(1) THEOREM

MODULATION INVARIANT BILINEAR T(1) THEOREM MODULATION INVARIANT BILINEAR T(1) THEOREM ÁRPÁD BÉNYI, CIPRIAN DEMETER, ANDREA R. NAHMOD, CHRISTOPH M. THIELE, RODOLFO H. TORRES, AND PACO VILLARROYA Abstract. We prove a T(1) theorem for bilinear singular

More information

Sobolev Spaces. Chapter Hölder spaces

Sobolev Spaces. Chapter Hölder spaces Chapter 2 Sobolev Spaces Sobolev spaces turn out often to be the proper setting in which to apply ideas of functional analysis to get information concerning partial differential equations. Here, we collect

More information

Wave operators with non-lipschitz coefficients: energy and observability estimates

Wave operators with non-lipschitz coefficients: energy and observability estimates Wave operators with non-lipschitz coefficients: energy and observability estimates Institut de Mathématiques de Jussieu-Paris Rive Gauche UNIVERSITÉ PARIS DIDEROT PARIS 7 JOURNÉE JEUNES CONTRÔLEURS 2014

More information

arxiv:math/ v3 [math.ca] 9 Oct 2007

arxiv:math/ v3 [math.ca] 9 Oct 2007 BCR ALGORITHM AND THE T(b) THEOREM P. AUSCHER AND.X.YANG arxiv:math/0702282v3 [math.ca] 9 Oct 2007 Abstract. We show using the Beylkin-Coifman-Rokhlin algorithm in the Haar basis that any singular integral

More information

MATH 722, COMPLEX ANALYSIS, SPRING 2009 PART 5

MATH 722, COMPLEX ANALYSIS, SPRING 2009 PART 5 MATH 722, COMPLEX ANALYSIS, SPRING 2009 PART 5.. The Arzela-Ascoli Theorem.. The Riemann mapping theorem Let X be a metric space, and let F be a family of continuous complex-valued functions on X. We have

More information

Finite-dimensional spaces. C n is the space of n-tuples x = (x 1,..., x n ) of complex numbers. It is a Hilbert space with the inner product

Finite-dimensional spaces. C n is the space of n-tuples x = (x 1,..., x n ) of complex numbers. It is a Hilbert space with the inner product Chapter 4 Hilbert Spaces 4.1 Inner Product Spaces Inner Product Space. A complex vector space E is called an inner product space (or a pre-hilbert space, or a unitary space) if there is a mapping (, )

More information

NEW CONSTRUCTIONS OF PIECEWISE-CONSTANT WAVELETS

NEW CONSTRUCTIONS OF PIECEWISE-CONSTANT WAVELETS NEW CONSTRUCTIONS OF PIECEWISE-CONSTANT WAVELETS YOUNGMI HUR AND AMOS RON Abstract. The classical Haar wavelet system of L 2 (R n ) is commonly considered to be very local in space. We introduce and study

More information

MULTILINEAR SQUARE FUNCTIONS AND MULTIPLE WEIGHTS

MULTILINEAR SQUARE FUNCTIONS AND MULTIPLE WEIGHTS MULTILINEA SUAE FUNCTIONS AND MULTIPLE WEIGHTS LOUKAS GAFAKOS, PAASA MOHANTY and SAUABH SHIVASTAVA Abstract In this paper we prove weighted estimates for a class of smooth multilinear square functions

More information

ALMOST ORTHOGONALITY AND A CLASS OF BOUNDED BILINEAR PSEUDODIFFERENTIAL OPERATORS

ALMOST ORTHOGONALITY AND A CLASS OF BOUNDED BILINEAR PSEUDODIFFERENTIAL OPERATORS ALMOST ORTHOGONALITY AND A CLASS OF BOUNDED BILINEAR PSEUDODIFFERENTIAL OPERATORS Abstract. Several results and techniques that generate bilinear alternatives of a celebrated theorem of Calderón and Vaillancourt

More information

arxiv: v1 [math.ca] 3 Nov 2018

arxiv: v1 [math.ca] 3 Nov 2018 SPARSE DOMINATION AND THE STRONG MAXIMAL FUNCTION ALEX BARRON, JOSÉ M. CONDE-ALONSO, YUMENG OU, AND GUILLERMO REY arxiv:1811.01243v1 [math.ca] 3 Nov 2018 Abstract. We study the problem of dominating the

More information

HARMONIC ANALYSIS. Date:

HARMONIC ANALYSIS. Date: HARMONIC ANALYSIS Contents. Introduction 2. Hardy-Littlewood maximal function 3. Approximation by convolution 4. Muckenhaupt weights 4.. Calderón-Zygmund decomposition 5. Fourier transform 6. BMO (bounded

More information

Some recent works on multi-parameter Hardy space theory and discrete Littlewood-Paley Analysis

Some recent works on multi-parameter Hardy space theory and discrete Littlewood-Paley Analysis Some recent works on multi-parameter Hardy space theory and discrete Littlewood-Paley Analysis Yongsheng Han and Guozhen Lu Dedicated to Professor Guangchang Dong on the occasion of his 80th birthday Abstract

More information

An introduction to some aspects of functional analysis

An introduction to some aspects of functional analysis An introduction to some aspects of functional analysis Stephen Semmes Rice University Abstract These informal notes deal with some very basic objects in functional analysis, including norms and seminorms

More information

Function spaces and multiplier operators

Function spaces and multiplier operators University of Wollongong Research Online Faculty of Informatics - Papers (Archive Faculty of Engineering and Information Sciences 2001 Function spaces and multiplier operators R. Nillsen University of

More information

CHAPTER 6. Differentiation

CHAPTER 6. Differentiation CHPTER 6 Differentiation The generalization from elementary calculus of differentiation in measure theory is less obvious than that of integration, and the methods of treating it are somewhat involved.

More information

ON THE BEHAVIOR OF THE SOLUTION OF THE WAVE EQUATION. 1. Introduction. = u. x 2 j

ON THE BEHAVIOR OF THE SOLUTION OF THE WAVE EQUATION. 1. Introduction. = u. x 2 j ON THE BEHAVIO OF THE SOLUTION OF THE WAVE EQUATION HENDA GUNAWAN AND WONO SETYA BUDHI Abstract. We shall here study some properties of the Laplace operator through its imaginary powers, and apply the

More information

Hartogs Theorem: separate analyticity implies joint Paul Garrett garrett/

Hartogs Theorem: separate analyticity implies joint Paul Garrett  garrett/ (February 9, 25) Hartogs Theorem: separate analyticity implies joint Paul Garrett garrett@math.umn.edu http://www.math.umn.edu/ garrett/ (The present proof of this old result roughly follows the proof

More information