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The space JNp: Nontriviality and duality

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TLDR
In this paper, the authors studied a function space J N p based on a condition introduced by John and Nirenberg as a variant of BMO and showed that the two spaces are not the same.
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This article is published in Journal of Functional Analysis.The article was published on 2018-08-01 and is currently open access. It has received 42 citations till now. The article focuses on the topics: Bounded mean oscillation.

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The L^p-to-L^q boundedness of commutators with applications to the Jacobian operator

TL;DR: In this paper, the Calderon-Zygmund operator was shown to be sufficient for the boundedness of commutators of pointwise multiplication and Calderon Zygmund operators.
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The L-p-to-L-q boundedness of commutators with applications to the Jacobian operator

TL;DR: In this article, it was shown that b ∈ BMO is necessary and sufficient for the L p -boundedness of commutators of pointwise multiplication and Calderon-Zygmund operators under minimal non-degeneracy hypotheses.
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John–Nirenberg–Campanato Spaces

TL;DR: In this paper, the authors introduced the John-Nirenberg-Campanato space J N (p, q, s ) α (X ), where X is R n or any cube Q 0 ⫋ R n, which when α = 0 and s = 0 coincides with the J N p -space introduced by F. John and L. Nirenberg in the sense of equivalent norms.
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BMO on shapes and sharp constants

TL;DR: In this paper, the authors consider a general definition of BMO on a domain in the sense that the mean oscillation is taken with respect to a basis of shapes, i.e. a collection of open sets covering the domain.
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A bridge connecting Lebesgue and Morrey spaces via Riesz norms

TL;DR: In this paper, the Riesz-Morrey space was introduced and studied via combining riesz norms with Morrey norms, which differs from the John-Nirenberg-Campanato space in subtracting integral means.
References
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Book

Harmonic Analysis: Real-variable Methods, Orthogonality, and Oscillatory Integrals

TL;DR: In this article, the authors introduce the Heisenberg group and describe the Maximal Operators and Maximal Averages and Oscillatory Integral Integrals of the First and Second Kind.
Book

Wavelets and Operators

TL;DR: In this article, Yves Meyer stands the theory of wavelets firmly upon solid ground by basing his book on the fundamental work of Calderon, Zygmund and their collaborators.
Book

Weighted norm inequalities and related topics

TL;DR: Theories de la factorisation and inegalites en norme ponderees of Hardy as mentioned in this paper have been studied in the context of factorization, and a variable reelle des espaces de Hardy has been proposed.
Related Papers (5)
Frequently Asked Questions (8)
Q1. what is the norm in the Lorentz space?

The norm in the Lorentz space Lp,q is given by‖f‖qLp,q =ˆ ∞0( t|{f > t}|1/p )q dtt≥ ∞ ∑i=0ˆ hi+1hitq−1 dt · |{f = hi+1}| q/p&∞ ∑i=0(hqi+1 − h q i ) · 2 −(i+1)2q/p=∞ ∑i=0(2(i+1) 2q/p − 2i 2q/p) · 2−(i+1) 2q/p= ∞ ∑i=0(1 − 2−(2i+1)q/p). 

Since further ‖f‖JNr′‖(aij) ∞ j=1‖(r,s) is summable over i by assumption, yet another application of dominated convergence proves thatΛfg = ∑i〈f, gi〉 = lim N→∞∑iˆQ0fNgi = lim N→∞ˆQ0fNg. 

The only place in the above argument where the properties of real numbers beyond their Banach space structure were used was the representation of Λ̃ ∈ (Ls0(Q0)) ∗ by a function f ∈ Ls ′(Q0). 

If the authors take, without loss of generality, The author′ to be the left half of I, this minimal distance is achieved by always choosing the descendants The author′′ of The author′ on the right, so that Î ′′ gets closer and closer to Î. 

In order to have an access to the simple duality of the reflexive Lp spaces (in contrast to the more complicated situation of L∞), the authors first establish the following reduction to finite indices in their candidate predual space:6.4. 

Since δI > 0 is the minimal distance of supp fI from any supp fI′′ with I′′ ( I, the authors see that each fI is disjointly supported from its descendants fI′′ with I′′ ( I. 

In contrast, the Chang–Fefferman atoms, while beingthe larger structures in their expansion, have properties closely analogous to those of classical atoms, whereas their elementary particles have additional smoothness properties, which are neither present in the classical H1 theory nor in their new spaces. 

That is, the authors need to estimate∞ ∑k=0‖gk‖(r,∞) ≤ ∞ ∑k=0(∑ℓ,j|Qℓk,j |‖a ℓ kj‖ r ∞)1/r.∞ ∑k=0Ck ( ∑ℓ,j|Qℓk,j |(Qℓ|Aℓ| s)r/s)1/r.∞ ∑k=1Ck [ ∑ℓ∣ ∣ ∣ { MQℓAℓ > C k(Qℓ|Aℓ| s)1/s} ∣∣ ∣ (Qℓ|Aℓ| s)r/s]1/r+ ( ∑ℓ|Qℓ|(Qℓ|Aℓ| s)r/s)1/r,where the authors separated the easier term corresponding to k = 0.