SLIDE 1 Factorization of the identity
Joint work with N. J. Laustsen and P. F. X. Müller
- J. Kepler University, Linz
Bedlewo, July 19, 2016
SLIDE 2
Overview
1 Operators with large diagonal 2 Mixed-norm Hardy spaces Hp(Hq)
SLIDE 3
Overview
1 Operators with large diagonal 2 Mixed-norm Hardy spaces Hp(Hq)
SLIDE 4 A description of the problem class
- Let X be a Banach space and T : X → X a linear operator.
Find conditions on X and T such that the identity Id on X factors through T i.e. X
Id
X
T
X
P
- EP ≤ C.
- The problem has finite dimensional (quantitative) and infinite
dimensional (qualitative) aspects.
- Classical examples for X include: ℓp (Pełczyński), ℓ∞ (Lindenstrauss),
L1 (Enflo-Starbird), Lp (Johnson-Maurey-Schechtman-Tzafriri), ℓp
n
(Bourgain-Tzafriri).
- Two parameters: Lp(Lq), 1 < p, q < ∞ (Capon).
SLIDE 5 A description of the problem class
- Let X be a Banach space and T : X → X a linear operator.
Find conditions on X and T such that the identity Id on X factors through T i.e. X
Id
X
T
X
P
- EP ≤ C.
- The problem has finite dimensional (quantitative) and infinite
dimensional (qualitative) aspects.
- Classical examples for X include: ℓp (Pełczyński), ℓ∞ (Lindenstrauss),
L1 (Enflo-Starbird), Lp (Johnson-Maurey-Schechtman-Tzafriri), ℓp
n
(Bourgain-Tzafriri).
- Two parameters: Lp(Lq), 1 < p, q < ∞ (Capon).
SLIDE 6 A description of the problem class
- Let X be a Banach space and T : X → X a linear operator.
Find conditions on X and T such that the identity Id on X factors through T i.e. X
Id
X
T
X
P
- EP ≤ C.
- The problem has finite dimensional (quantitative) and infinite
dimensional (qualitative) aspects.
- Classical examples for X include: ℓp (Pełczyński), ℓ∞ (Lindenstrauss),
L1 (Enflo-Starbird), Lp (Johnson-Maurey-Schechtman-Tzafriri), ℓp
n
(Bourgain-Tzafriri).
- Two parameters: Lp(Lq), 1 < p, q < ∞ (Capon).
SLIDE 7 A description of the problem class
- Let X be a Banach space and T : X → X a linear operator.
Find conditions on X and T such that the identity Id on X factors through T i.e. X
Id
X
T
X
P
- EP ≤ C.
- The problem has finite dimensional (quantitative) and infinite
dimensional (qualitative) aspects.
- Classical examples for X include: ℓp (Pełczyński), ℓ∞ (Lindenstrauss),
L1 (Enflo-Starbird), Lp (Johnson-Maurey-Schechtman-Tzafriri), ℓp
n
(Bourgain-Tzafriri).
- Two parameters: Lp(Lq), 1 < p, q < ∞ (Capon).
SLIDE 8 A description of the problem class
- Let X be a Banach space and T : X → X a linear operator.
Find conditions on X and T such that the identity Id on X factors through T i.e. X
Id
X
T
X
P
- EP ≤ C.
- The problem has finite dimensional (quantitative) and infinite
dimensional (qualitative) aspects.
- Classical examples for X include: ℓp (Pełczyński), ℓ∞ (Lindenstrauss),
L1 (Enflo-Starbird), Lp (Johnson-Maurey-Schechtman-Tzafriri), ℓp
n
(Bourgain-Tzafriri).
- Two parameters: Lp(Lq), 1 < p, q < ∞ (Capon).
SLIDE 9 A description of the problem class
- Let X be a Banach space and T : X → X a linear operator.
Find conditions on X and T such that the identity Id on X factors through T i.e. X
Id
X
T
X
P
- EP ≤ C.
- The problem has finite dimensional (quantitative) and infinite
dimensional (qualitative) aspects.
- Classical examples for X include: ℓp (Pełczyński), ℓ∞ (Lindenstrauss),
L1 (Enflo-Starbird), Lp (Johnson-Maurey-Schechtman-Tzafriri), ℓp
n
(Bourgain-Tzafriri).
- Two parameters: Lp(Lq), 1 < p, q < ∞ (Capon).
SLIDE 10 Operators with large diagonal
- Let X be a Banach space and T : X → X a linear operator.
- Suppose that X has an unconditional basis (bn), and let b∗
n ∈ X∗ be so
that bn, b∗
m = 0, m = n, and bn, b∗ n = 1.
- We say that T has large diagonal (relative to (bn)) if
infn∈N |Tbn, b∗
n| > 0.
- For many Banach spaces X we know that the identity factors through
- perators T with large diagonal, i.e.
X
Id
X
T
X
P
- EP ≤ C.
- X = ℓp with the unit vector basis (Pełczyński)
- X = Lp (Andrew), X = Lp(Lq) (Capon) with the Haar basis
SLIDE 11 Operators with large diagonal
- Let X be a Banach space and T : X → X a linear operator.
- Suppose that X has an unconditional basis (bn), and let b∗
n ∈ X∗ be so
that bn, b∗
m = 0, m = n, and bn, b∗ n = 1.
- We say that T has large diagonal (relative to (bn)) if
infn∈N |Tbn, b∗
n| > 0.
- For many Banach spaces X we know that the identity factors through
- perators T with large diagonal, i.e.
X
Id
X
T
X
P
- EP ≤ C.
- X = ℓp with the unit vector basis (Pełczyński)
- X = Lp (Andrew), X = Lp(Lq) (Capon) with the Haar basis
SLIDE 12 Operators with large diagonal
- Let X be a Banach space and T : X → X a linear operator.
- Suppose that X has an unconditional basis (bn), and let b∗
n ∈ X∗ be so
that bn, b∗
m = 0, m = n, and bn, b∗ n = 1.
- We say that T has large diagonal (relative to (bn)) if
infn∈N |Tbn, b∗
n| > 0.
- For many Banach spaces X we know that the identity factors through
- perators T with large diagonal, i.e.
X
Id
X
T
X
P
- EP ≤ C.
- X = ℓp with the unit vector basis (Pełczyński)
- X = Lp (Andrew), X = Lp(Lq) (Capon) with the Haar basis
SLIDE 13 Operators with large diagonal
- Let X be a Banach space and T : X → X a linear operator.
- Suppose that X has an unconditional basis (bn), and let b∗
n ∈ X∗ be so
that bn, b∗
m = 0, m = n, and bn, b∗ n = 1.
- We say that T has large diagonal (relative to (bn)) if
infn∈N |Tbn, b∗
n| > 0.
- For many Banach spaces X we know that the identity factors through
- perators T with large diagonal, i.e.
X
Id
X
T
X
P
- EP ≤ C.
- X = ℓp with the unit vector basis (Pełczyński)
- X = Lp (Andrew), X = Lp(Lq) (Capon) with the Haar basis
SLIDE 14 Operators with large diagonal
- Let X be a Banach space and T : X → X a linear operator.
- Suppose that X has an unconditional basis (bn), and let b∗
n ∈ X∗ be so
that bn, b∗
m = 0, m = n, and bn, b∗ n = 1.
- We say that T has large diagonal (relative to (bn)) if
infn∈N |Tbn, b∗
n| > 0.
- For many Banach spaces X we know that the identity factors through
- perators T with large diagonal, i.e.
X
Id
X
T
X
P
- EP ≤ C.
- X = ℓp with the unit vector basis (Pełczyński)
- X = Lp (Andrew), X = Lp(Lq) (Capon) with the Haar basis
SLIDE 15 Operators with large diagonal
- Let X be a Banach space and T : X → X a linear operator.
- Suppose that X has an unconditional basis (bn), and let b∗
n ∈ X∗ be so
that bn, b∗
m = 0, m = n, and bn, b∗ n = 1.
- We say that T has large diagonal (relative to (bn)) if
infn∈N |Tbn, b∗
n| > 0.
- For many Banach spaces X we know that the identity factors through
- perators T with large diagonal, i.e.
X
Id
X
T
X
P
- EP ≤ C.
- X = ℓp with the unit vector basis (Pełczyński)
- X = Lp (Andrew), X = Lp(Lq) (Capon) with the Haar basis
SLIDE 16 Operators with large diagonal
- Let X be a Banach space and T : X → X a linear operator.
- Suppose that X has an unconditional basis (bn), and let b∗
n ∈ X∗ be so
that bn, b∗
m = 0, m = n, and bn, b∗ n = 1.
- We say that T has large diagonal (relative to (bn)) if
infn∈N |Tbn, b∗
n| > 0.
- For many Banach spaces X we know that the identity factors through
- perators T with large diagonal, i.e.
X
Id
X
T
X
P
- EP ≤ C.
- X = ℓp with the unit vector basis (Pełczyński)
- X = Lp (Andrew), X = Lp(Lq) (Capon) with the Haar basis
SLIDE 17 Can the identity operator on X be factored through each
- perator on X with large diagonal for all Banach spaces X
with an unconditional basis?
Answer:
Theorem (N. J. Laustsen, R. L., P. F. X. Müller)
There is an operator T on a Banach space X with an unconditional basis such that T has large diagonal, but the identity operator on X does not factor through T. Main ingredients for the proof:
- X is Gowers’ space with an unconditional basis (Gowers–Maurey).
- Fredholm theory.
Theorem (N. J. Laustsen, R. L., P. F. X. Müller)
The identity on mixed-norm Hardy spaces Hp(Hq), 1 ≤ p, q < ∞, factors through any operator T with large diagonal relative to the bi–parameter Haar basis. (1 < p, q < ∞ = Capon).
SLIDE 18 Can the identity operator on X be factored through each
- perator on X with large diagonal for all Banach spaces X
with an unconditional basis?
Answer:
Theorem (N. J. Laustsen, R. L., P. F. X. Müller)
There is an operator T on a Banach space X with an unconditional basis such that T has large diagonal, but the identity operator on X does not factor through T. Main ingredients for the proof:
- X is Gowers’ space with an unconditional basis (Gowers–Maurey).
- Fredholm theory.
Theorem (N. J. Laustsen, R. L., P. F. X. Müller)
The identity on mixed-norm Hardy spaces Hp(Hq), 1 ≤ p, q < ∞, factors through any operator T with large diagonal relative to the bi–parameter Haar basis. (1 < p, q < ∞ = Capon).
SLIDE 19 Can the identity operator on X be factored through each
- perator on X with large diagonal for all Banach spaces X
with an unconditional basis?
Answer:
Theorem (N. J. Laustsen, R. L., P. F. X. Müller)
There is an operator T on a Banach space X with an unconditional basis such that T has large diagonal, but the identity operator on X does not factor through T. Main ingredients for the proof:
- X is Gowers’ space with an unconditional basis (Gowers–Maurey).
- Fredholm theory.
Theorem (N. J. Laustsen, R. L., P. F. X. Müller)
The identity on mixed-norm Hardy spaces Hp(Hq), 1 ≤ p, q < ∞, factors through any operator T with large diagonal relative to the bi–parameter Haar basis. (1 < p, q < ∞ = Capon).
SLIDE 20 Can the identity operator on X be factored through each
- perator on X with large diagonal for all Banach spaces X
with an unconditional basis?
Answer:
Theorem (N. J. Laustsen, R. L., P. F. X. Müller)
There is an operator T on a Banach space X with an unconditional basis such that T has large diagonal, but the identity operator on X does not factor through T. Main ingredients for the proof:
- X is Gowers’ space with an unconditional basis (Gowers–Maurey).
- Fredholm theory.
Theorem (N. J. Laustsen, R. L., P. F. X. Müller)
The identity on mixed-norm Hardy spaces Hp(Hq), 1 ≤ p, q < ∞, factors through any operator T with large diagonal relative to the bi–parameter Haar basis. (1 < p, q < ∞ = Capon).
SLIDE 21 Can the identity operator on X be factored through each
- perator on X with large diagonal for all Banach spaces X
with an unconditional basis?
Answer:
Theorem (N. J. Laustsen, R. L., P. F. X. Müller)
There is an operator T on a Banach space X with an unconditional basis such that T has large diagonal, but the identity operator on X does not factor through T. Main ingredients for the proof:
- X is Gowers’ space with an unconditional basis (Gowers–Maurey).
- Fredholm theory.
Theorem (N. J. Laustsen, R. L., P. F. X. Müller)
The identity on mixed-norm Hardy spaces Hp(Hq), 1 ≤ p, q < ∞, factors through any operator T with large diagonal relative to the bi–parameter Haar basis. (1 < p, q < ∞ = Capon).
SLIDE 22 Can the identity operator on X be factored through each
- perator on X with large diagonal for all Banach spaces X
with an unconditional basis?
Answer:
Theorem (N. J. Laustsen, R. L., P. F. X. Müller)
There is an operator T on a Banach space X with an unconditional basis such that T has large diagonal, but the identity operator on X does not factor through T. Main ingredients for the proof:
- X is Gowers’ space with an unconditional basis (Gowers–Maurey).
- Fredholm theory.
Theorem (N. J. Laustsen, R. L., P. F. X. Müller)
The identity on mixed-norm Hardy spaces Hp(Hq), 1 ≤ p, q < ∞, factors through any operator T with large diagonal relative to the bi–parameter Haar basis. (1 < p, q < ∞ = Capon).
SLIDE 23
Overview
1 Operators with large diagonal 2 Mixed-norm Hardy spaces Hp(Hq)
SLIDE 24 Mixed-norm Hardy spaces Hp(Hq)
2n , k 2n [ : n ≥ 0, 1 ≤ k ≤ 2n} denotes the dyadic intervals on
the unit interval,
- R = {I × J : I, J ∈ D} denotes the dyadic rectangles on the unit
square,
- (hI : I ∈ D) the L∞-normalized Haar system.
- hI×J(x, y) = hI(x)hJ(y) the L∞-normalized tensor product Haar
function, I × J ∈ R.
I×J∈R aI×JhI×J be a finite linear combination,
- Given 1 ≤ p, q < ∞, the space Hp(Hq) is the closure of
span{hR : R ∈ R} under the norm
aRhRHp(Hq) = 1 1
R∈R
a2
Rh2 R(x, y)
q/2 dy p/q dx 1/p .
SLIDE 25 Mixed-norm Hardy spaces Hp(Hq)
2n , k 2n [ : n ≥ 0, 1 ≤ k ≤ 2n} denotes the dyadic intervals on
the unit interval,
- R = {I × J : I, J ∈ D} denotes the dyadic rectangles on the unit
square,
- (hI : I ∈ D) the L∞-normalized Haar system.
- hI×J(x, y) = hI(x)hJ(y) the L∞-normalized tensor product Haar
function, I × J ∈ R.
I×J∈R aI×JhI×J be a finite linear combination,
- Given 1 ≤ p, q < ∞, the space Hp(Hq) is the closure of
span{hR : R ∈ R} under the norm
aRhRHp(Hq) = 1 1
R∈R
a2
Rh2 R(x, y)
q/2 dy p/q dx 1/p .
SLIDE 26 Mixed-norm Hardy spaces Hp(Hq)
2n , k 2n [ : n ≥ 0, 1 ≤ k ≤ 2n} denotes the dyadic intervals on
the unit interval,
- R = {I × J : I, J ∈ D} denotes the dyadic rectangles on the unit
square,
- (hI : I ∈ D) the L∞-normalized Haar system.
- hI×J(x, y) = hI(x)hJ(y) the L∞-normalized tensor product Haar
function, I × J ∈ R.
I×J∈R aI×JhI×J be a finite linear combination,
- Given 1 ≤ p, q < ∞, the space Hp(Hq) is the closure of
span{hR : R ∈ R} under the norm
aRhRHp(Hq) = 1 1
R∈R
a2
Rh2 R(x, y)
q/2 dy p/q dx 1/p .
SLIDE 27 Mixed-norm Hardy spaces Hp(Hq)
2n , k 2n [ : n ≥ 0, 1 ≤ k ≤ 2n} denotes the dyadic intervals on
the unit interval,
- R = {I × J : I, J ∈ D} denotes the dyadic rectangles on the unit
square,
- (hI : I ∈ D) the L∞-normalized Haar system.
- hI×J(x, y) = hI(x)hJ(y) the L∞-normalized tensor product Haar
function, I × J ∈ R.
I×J∈R aI×JhI×J be a finite linear combination,
- Given 1 ≤ p, q < ∞, the space Hp(Hq) is the closure of
span{hR : R ∈ R} under the norm
aRhRHp(Hq) = 1 1
R∈R
a2
Rh2 R(x, y)
q/2 dy p/q dx 1/p .
SLIDE 28 Mixed-norm Hardy spaces Hp(Hq)
2n , k 2n [ : n ≥ 0, 1 ≤ k ≤ 2n} denotes the dyadic intervals on
the unit interval,
- R = {I × J : I, J ∈ D} denotes the dyadic rectangles on the unit
square,
- (hI : I ∈ D) the L∞-normalized Haar system.
- hI×J(x, y) = hI(x)hJ(y) the L∞-normalized tensor product Haar
function, I × J ∈ R.
I×J∈R aI×JhI×J be a finite linear combination,
- Given 1 ≤ p, q < ∞, the space Hp(Hq) is the closure of
span{hR : R ∈ R} under the norm
aRhRHp(Hq) = 1 1
R∈R
a2
Rh2 R(x, y)
q/2 dy p/q dx 1/p .
SLIDE 29 Mixed-norm Hardy spaces Hp(Hq)
2n , k 2n [ : n ≥ 0, 1 ≤ k ≤ 2n} denotes the dyadic intervals on
the unit interval,
- R = {I × J : I, J ∈ D} denotes the dyadic rectangles on the unit
square,
- (hI : I ∈ D) the L∞-normalized Haar system.
- hI×J(x, y) = hI(x)hJ(y) the L∞-normalized tensor product Haar
function, I × J ∈ R.
I×J∈R aI×JhI×J be a finite linear combination,
- Given 1 ≤ p, q < ∞, the space Hp(Hq) is the closure of
span{hR : R ∈ R} under the norm
aRhRHp(Hq) = 1 1
R∈R
a2
Rh2 R(x, y)
q/2 dy p/q dx 1/p .
SLIDE 30 Large diagonal relative to the bi-parameter Haar system
Theorem (N. J. Laustsen, R. L., P. F. X. Müller)
Let 1 ≤ p, q < ∞, δ > 0 and T : Hp(Hq) → Hp(Hq) be a linear operator with large diagonal, i.e. ThI×J, hI×J ≥ δ|I × J|. Then we have Hp(Hq)
Id
Hp(Hq)
T
Hp(Hq)
P
where C = 1 + 1/10000. By Capon’s bi–parameter construction (BI×J) and a random choice of signs εI×J, there exists a block basis b(ε)
I×J = K∈BI×J εK×LhK×L such that:
I×J) is equivalent to (hI×J),
I×J = αI×Jb(ε) I×J + small error, with αI×J ≥ δ,
I∈D f,b(ε)
I×J
b(ε)
I×J2 2
b(ε)
I×J is bounded on Hp(Hq).
SLIDE 31 Large diagonal relative to the bi-parameter Haar system
Theorem (N. J. Laustsen, R. L., P. F. X. Müller)
Let 1 ≤ p, q < ∞, δ > 0 and T : Hp(Hq) → Hp(Hq) be a linear operator with large diagonal, i.e. ThI×J, hI×J ≥ δ|I × J|. Then we have Hp(Hq)
Id
Hp(Hq)
T
Hp(Hq)
P
where C = 1 + 1/10000. By Capon’s bi–parameter construction (BI×J) and a random choice of signs εI×J, there exists a block basis b(ε)
I×J = K∈BI×J εK×LhK×L such that:
I×J) is equivalent to (hI×J),
I×J = αI×Jb(ε) I×J + small error, with αI×J ≥ δ,
I∈D f,b(ε)
I×J
b(ε)
I×J2 2
b(ε)
I×J is bounded on Hp(Hq).
SLIDE 32 Large diagonal relative to the bi-parameter Haar system
Theorem (N. J. Laustsen, R. L., P. F. X. Müller)
Let 1 ≤ p, q < ∞, δ > 0 and T : Hp(Hq) → Hp(Hq) be a linear operator with large diagonal, i.e. ThI×J, hI×J ≥ δ|I × J|. Then we have Hp(Hq)
Id
Hp(Hq)
T
Hp(Hq)
P
where C = 1 + 1/10000. By Capon’s bi–parameter construction (BI×J) and a random choice of signs εI×J, there exists a block basis b(ε)
I×J = K∈BI×J εK×LhK×L such that:
I×J) is equivalent to (hI×J),
I×J = αI×Jb(ε) I×J + small error, with αI×J ≥ δ,
I∈D f,b(ε)
I×J
b(ε)
I×J2 2
b(ε)
I×J is bounded on Hp(Hq).
SLIDE 33 Large diagonal relative to the bi-parameter Haar system
Theorem (N. J. Laustsen, R. L., P. F. X. Müller)
Let 1 ≤ p, q < ∞, δ > 0 and T : Hp(Hq) → Hp(Hq) be a linear operator with large diagonal, i.e. ThI×J, hI×J ≥ δ|I × J|. Then we have Hp(Hq)
Id
Hp(Hq)
T
Hp(Hq)
P
where C = 1 + 1/10000. By Capon’s bi–parameter construction (BI×J) and a random choice of signs εI×J, there exists a block basis b(ε)
I×J = K∈BI×J εK×LhK×L such that:
I×J) is equivalent to (hI×J),
I×J = αI×Jb(ε) I×J + small error, with αI×J ≥ δ,
I∈D f,b(ε)
I×J
b(ε)
I×J2 2
b(ε)
I×J is bounded on Hp(Hq).
SLIDE 34 Large diagonal relative to the bi-parameter Haar system
Theorem (N. J. Laustsen, R. L., P. F. X. Müller)
Let 1 ≤ p, q < ∞, δ > 0 and T : Hp(Hq) → Hp(Hq) be a linear operator with large diagonal, i.e. ThI×J, hI×J ≥ δ|I × J|. Then we have Hp(Hq)
Id
Hp(Hq)
T
Hp(Hq)
P
where C = 1 + 1/10000. By Capon’s bi–parameter construction (BI×J) and a random choice of signs εI×J, there exists a block basis b(ε)
I×J = K∈BI×J εK×LhK×L such that:
I×J) is equivalent to (hI×J),
I×J = αI×Jb(ε) I×J + small error, with αI×J ≥ δ,
I∈D f,b(ε)
I×J
b(ε)
I×J2 2
b(ε)
I×J is bounded on Hp(Hq).
SLIDE 35 Large diagonal relative to the bi-parameter Haar system
Theorem (N. J. Laustsen, R. L., P. F. X. Müller)
Let 1 ≤ p, q < ∞, δ > 0 and T : Hp(Hq) → Hp(Hq) be a linear operator with large diagonal, i.e. ThI×J, hI×J ≥ δ|I × J|. Then we have Hp(Hq)
Id
Hp(Hq)
T
Hp(Hq)
P
where C = 1 + 1/10000. By Capon’s bi–parameter construction (BI×J) and a random choice of signs εI×J, there exists a block basis b(ε)
I×J = K∈BI×J εK×LhK×L such that:
I×J) is equivalent to (hI×J),
I×J = αI×Jb(ε) I×J + small error, with αI×J ≥ δ,
I∈D f,b(ε)
I×J
b(ε)
I×J2 2
b(ε)
I×J is bounded on Hp(Hq).
SLIDE 36 Proof – ordering of R
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48
Figure: Order of the first 49 rectangles.
I ∈ D is such that I ⊃ I and | I| = 2|I|.
number of I × J.
I × J) < O⊳ (I × J)
J) < O⊳ (I × J)
2], then
I × J) = 3,
J) = 1.
SLIDE 37 Proof – ordering of R
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48
Figure: Order of the first 49 rectangles.
I ∈ D is such that I ⊃ I and | I| = 2|I|.
number of I × J.
I × J) < O⊳ (I × J)
J) < O⊳ (I × J)
2], then
I × J) = 3,
J) = 1.
SLIDE 38 Proof – ordering of R
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48
Figure: Order of the first 49 rectangles.
I ∈ D is such that I ⊃ I and | I| = 2|I|.
number of I × J.
I × J) < O⊳ (I × J)
J) < O⊳ (I × J)
2], then
I × J) = 3,
J) = 1.
SLIDE 39 Proof – ordering of R
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48
Figure: Order of the first 49 rectangles.
I ∈ D is such that I ⊃ I and | I| = 2|I|.
number of I × J.
I × J) < O⊳ (I × J)
J) < O⊳ (I × J)
2], then
I × J) = 3,
J) = 1.
SLIDE 40 Proof – ordering of R
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48
Figure: Order of the first 49 rectangles.
I ∈ D is such that I ⊃ I and | I| = 2|I|.
number of I × J.
I × J) < O⊳ (I × J)
J) < O⊳ (I × J)
2], then
I × J) = 3,
J) = 1.
SLIDE 41 Proof – ordering of R
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48
Figure: Order of the first 49 rectangles.
I ∈ D is such that I ⊃ I and | I| = 2|I|.
number of I × J.
I × J) < O⊳ (I × J)
J) < O⊳ (I × J)
2], then
I × J) = 3,
J) = 1.
SLIDE 42 Proof – ordering of R
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48
Figure: Order of the first 49 rectangles.
I ∈ D is such that I ⊃ I and | I| = 2|I|.
number of I × J.
I × J) < O⊳ (I × J)
J) < O⊳ (I × J)
2], then
I × J) = 3,
J) = 1.
SLIDE 43 Proof – ordering of R
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48
Figure: Order of the first 49 rectangles.
I ∈ D is such that I ⊃ I and | I| = 2|I|.
number of I × J.
I × J) < O⊳ (I × J)
J) < O⊳ (I × J)
2], then
I × J) = 3,
J) = 1.
SLIDE 44 Proof – ordering of R
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48
Figure: Order of the first 49 rectangles.
I ∈ D is such that I ⊃ I and | I| = 2|I|.
number of I × J.
I × J) < O⊳ (I × J)
J) < O⊳ (I × J)
2], then
I × J) = 3,
J) = 1.
SLIDE 45 Proof – case J = [0, 1]
Figure: Darkgray=past, lightgray=present, white=future.
I×[0,1]
SLIDE 46 Proof – case J = [0, 1]
Figure: Darkgray=past, lightgray=present, white=future.
I×[0,1]
[0, 1] K0 K K′ K K′′ K K′′′ K
SLIDE 47
The Gamlen-Gaudet construction (1973)
Figure: On the left side: construction of bI. On the right side: the corresponding index intervals I.
SLIDE 48
The Gamlen-Gaudet construction (1973)
Figure: On the left side: construction of bI. On the right side: the corresponding index intervals I.
SLIDE 49
The Gamlen-Gaudet construction (1973)
Figure: On the left side: construction of bI. On the right side: the corresponding index intervals I.
SLIDE 50
The Gamlen-Gaudet construction (1973)
Figure: On the left side: construction of bI. On the right side: the corresponding index intervals I.
SLIDE 51
The Gamlen-Gaudet construction (1973)
Figure: On the left side: construction of bI. On the right side: the corresponding index intervals I.
SLIDE 52
The Gamlen-Gaudet construction (1973)
Figure: On the left side: construction of bI. On the right side: the corresponding index intervals I.
SLIDE 53
The Gamlen-Gaudet construction (1973)
Figure: On the left side: construction of bI. On the right side: the corresponding index intervals I.
SLIDE 54 Proof – case J = [0, 1], I = [0, 1]
Figure: Darkgray=past, lightgray=present, white=future.
J
SLIDE 55 Proof – case J = [0, 1], I = [0, 1]
Figure: Darkgray=past, lightgray=present, white=future.
J
L0 L [0, 1] L′ L
SLIDE 56 Proof – case J = [0, 1], I = [0, 1]
Figure: Darkgray=past, lightgray=present.
- K0 × [0, 1] ∈ BI×[0,1]
- K1 × L1 ∈ B
I×J (⇒ K1 × [0, 1] ∈ B I×[0,1])
SLIDE 57 Proof – case J = [0, 1], I = [0, 1]
Figure: Darkgray=past, lightgray=present.
- K0 × [0, 1] ∈ BI×[0,1]
- K1 × L1 ∈ B
I×J (⇒ K1 × [0, 1] ∈ B I×[0,1])
L1 K0 L K1 L′
1
K0 L K′
1
L K′′
1
- The lightgray area is given by
BI×
J
B
I×J
SLIDE 58 Proof – case J = [0, 1], I = [0, 1]
Figure: Darkgray=past, lightgray=present.
- K0 × [0, 1] ∈ BI×[0,1]
- K1 × L1 ∈ B
I×J (⇒ K1 × [0, 1] ∈ B I×[0,1])
L1 K0 L K1 L′
1
K0 L K′
1
L K′′
1
- The lightgray area is given by
BI×
J
B
I×J
SLIDE 59 Proof – case J = [0, 1], I = [0, 1]
Figure: Darkgray=past, lightgray=present.
- K0 × [0, 1] ∈ BI×[0,1]
- K1 × L1 ∈ B
I×J (⇒ K1 × [0, 1] ∈ B I×[0,1])
L1 K0 L K1 L′
1
K0 L K′
1
L K′′
1
- The lightgray area is given by
BI×
J
B
I×J
SLIDE 60 What does BI×J look like?
K∈XI
- L∈YJ(K) K × L
- XI = {K0, K1, K2}
SLIDE 61 What does BI×J look like?
K∈XI
- L∈YJ(K) K × L
- XI = {K0, K1, K2}
SLIDE 62 Yes, but how does BI×J REALLY look like?
- XI = {K0, K1, K2},
- BI×J =
K∈XI
- L∈YJ(K) K × L,
- J, J0, J1 ∈ D are such that J0 ∪ J1 = J and J0 ∩ J1 = ∅,
- BI×J in the top layer,
- BI×J0 and BI×J1 in the bottom layer.
SLIDE 63 Yes, but how does BI×J REALLY look like?
- XI = {K0, K1, K2},
- BI×J =
K∈XI
- L∈YJ(K) K × L,
- J, J0, J1 ∈ D are such that J0 ∪ J1 = J and J0 ∩ J1 = ∅,
- BI×J in the top layer,
- BI×J0 and BI×J1 in the bottom layer.
SLIDE 64 Yes, but how does BI×J REALLY look like?
- XI = {K0, K1, K2},
- BI×J =
K∈XI
- L∈YJ(K) K × L,
- J, J0, J1 ∈ D are such that J0 ∪ J1 = J and J0 ∩ J1 = ∅,
- BI×J in the top layer,
- BI×J0 and BI×J1 in the bottom layer.
SLIDE 65 And one more
- XI = {K0, K1, K2}
- I, J0, J1, J2, J3 ∈ D
- J0 ⊂ J1 ⊂ J2 ⊂ J3
- |J3| = 2|J2| = 4|J1| =
8|J0|
- BI×Jj in layer j
- The shaded vertical
plane connects the lines ℓ = {(x, y0) : x ∈ [0, 1)}
SLIDE 66 And one more
- XI = {K0, K1, K2}
- I, J0, J1, J2, J3 ∈ D
- J0 ⊂ J1 ⊂ J2 ⊂ J3
- |J3| = 2|J2| = 4|J1| =
8|J0|
- BI×Jj in layer j
- The shaded vertical
plane connects the lines ℓ = {(x, y0) : x ∈ [0, 1)}
SLIDE 67 Summary
The identity factors through operators with large diagonal (with respect to the bi–parameter Haar system) in the following Hardy spaces:
- Capon: Hp(Hq) for 1 < p, q < ∞,
- P. F. X. Müller: H1(H1),
- R. L., P. F. X. Müller: H1
n(H1 n),
- N. J. Laustsen, R. L., P. F. X. Müller: Hp(Hq) for 1 ≤ p, q < ∞.
Coming soon...
n(Hq n).
SLIDE 68 Summary
The identity factors through operators with large diagonal (with respect to the bi–parameter Haar system) in the following Hardy spaces:
- Capon: Hp(Hq) for 1 < p, q < ∞,
- P. F. X. Müller: H1(H1),
- R. L., P. F. X. Müller: H1
n(H1 n),
- N. J. Laustsen, R. L., P. F. X. Müller: Hp(Hq) for 1 ≤ p, q < ∞.
Coming soon...
n(Hq n).
SLIDE 69 Summary
The identity factors through operators with large diagonal (with respect to the bi–parameter Haar system) in the following Hardy spaces:
- Capon: Hp(Hq) for 1 < p, q < ∞,
- P. F. X. Müller: H1(H1),
- R. L., P. F. X. Müller: H1
n(H1 n),
- N. J. Laustsen, R. L., P. F. X. Müller: Hp(Hq) for 1 ≤ p, q < ∞.
Coming soon...
n(Hq n).
SLIDE 70 Summary
The identity factors through operators with large diagonal (with respect to the bi–parameter Haar system) in the following Hardy spaces:
- Capon: Hp(Hq) for 1 < p, q < ∞,
- P. F. X. Müller: H1(H1),
- R. L., P. F. X. Müller: H1
n(H1 n),
- N. J. Laustsen, R. L., P. F. X. Müller: Hp(Hq) for 1 ≤ p, q < ∞.
Coming soon...
n(Hq n).
SLIDE 71 Summary
The identity factors through operators with large diagonal (with respect to the bi–parameter Haar system) in the following Hardy spaces:
- Capon: Hp(Hq) for 1 < p, q < ∞,
- P. F. X. Müller: H1(H1),
- R. L., P. F. X. Müller: H1
n(H1 n),
- N. J. Laustsen, R. L., P. F. X. Müller: Hp(Hq) for 1 ≤ p, q < ∞.
Coming soon...
n(Hq n).
SLIDE 72
- N. J. Laustsen, R. Lechner, and P. F. X. Müller.
Factorization of the identity through operators with large diagonal. ArXiv e-prints, September 2015. Richard Lechner and Paul F. X. Müller. Localization and projections on bi-parameter BMO.
- Q. J. Math., 66(4):1069–1101, 2015.