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atoms with a prescribed moment order
Definition
Let , let and let satisfy . A -atom is a measurable function for which there is a nondegenerate axis-parallel cube (Axis-parallel rectangles in and their volume, so all side lengths are equal and positive) such that
- , where the support is the closure of ;
- for almost every ;
- for every multi-index with ( maps and multi-index derivative notation in Euclidean space).
The exponent in the size bound and the order are part of the datum, not free parameters of the function: a -atom is also a -atom for every , because the moment conditions for the smaller order are among those already imposed. The zero function satisfies all three conditions; zero terms may be omitted from atomic representations.
Under Countable Choice (The Axiom of Countable Choice ()), every moment in condition 3 is an absolutely convergent Lebesgue integral; the supporting cube has its finite volume by A box in with parameters is Lebesgue measurable of measure , whichever of its faces are included. Indeed vanishes a.e. off the bounded set and a.e. on , a bounded function on a set of finite measure; the monomial is continuous and hence Borel measurable by Continuous functions on Euclidean spaces are Borel measurable. Applying Arithmetic and lattice operations preserve measurability whenever they are defined to the real and imaginary parts of shows that is measurable, so the integral is defined and finite. The a.e. bound in condition 2 is an essential supremum bound, (The essential supremum of a measurable function with respect to a measure); replacing by another representative of its a.e. class preserves conditions 2 and 3 but can change the support in condition 1, so the support condition is imposed for the chosen representative.
The page fixes the order This is the least integer compatible with condition 3, and it is the order used by the sources: DKKP require moments through , Wang and Hiserote through . The threshold moves exactly at the integers: for , for , and so on. For the definition specialises to the classical atoms of : support in a cube, a.e. and (Conjugate exponents, including the endpoint conventions records the exponent convention used for the dual exponents invoked later on this page).
The ball-supported atoms of the sources differ from this convention only by fixed constants: a cube containing a ball with carries the same conditions up to the dimensional factor , and nondegeneracy rules out the degenerate cubes of zero volume that occur in moment conditions. The three conditions define the class without selecting representatives; the accompanying Lebesgue-integrability assertions use Countable Choice.
Depends on
- Axis-parallel rectangles in $\mathbb{R}^m$ and their volume
- The space $L^p(\mu)$ as the quotient by null functions
- A locally integrable function on $\mathbb{R}^n$
- Conjugate exponents, including the endpoint conventions
- $C^k$ maps and multi-index derivative notation in Euclidean space
- The essential supremum of a measurable function with respect to a measure
- The Axiom of Countable Choice ($\mathrm{AC}_\omega$)
- A box in $\mathbb{R}^n$ with parameters $a_i\le b_i$ is Lebesgue measurable of measure $\prod_{i<n}(b_i-a_i)$, whichever of its faces are included
- Arithmetic and lattice operations preserve measurability whenever they are defined
- Continuous functions on Euclidean spaces are Borel measurable
Used by
- Weighted-integrable Hᵖ functions have vanishing moments in the atomic range Corollary
- A compactly supported L¹ function of nonzero integral is not in H¹ Counterexample
- A normalised cube indicator is not an H¹ atom Counterexample
- An H¹ atom need not be smooth or continuous Counterexample
- A normalised mean-zero H¹ atom Example
- The Hilbert transform of an H¹ atom is integrable Example
- Atoms have uniformly bounded Hᵖ quasi-norm and uniformly bounded test pairings Lemma
- BMO classes are determined by their pairings with H1 atoms Lemma
- BMO functions pair uniformly with H1 atoms Lemma
- Bounded BMO functions dualise H1 boundedly Lemma
- Finite atomic sums are dense in H1 Lemma
- Level decomposition of an Hᵖ distribution produces atoms Lemma
- ℓᵖ sums of atoms converge in S' and in Hᵖ Lemma
- Atomic characterisation of real Hᵖ for 0<p≤1 Theorem
- BMO classes define bounded functionals on H1 Theorem
- Calderon-Zygmund operators map H¹ boundedly into L¹ Theorem
- Fourier transform decay of real Hᵖ elements Theorem
Dependency tree · two levels
47 results within two dependency steps of this one, each drawn at its shortest distance from it. An arrow runs from a result to what uses it, so the chart reads left to right and ends at this result, which carries a heavier outline. Every node is a link to that result. Click elsewhere on the chart to enlarge it.
Sources
- Shai Dekel, Gerard Kerkyacharian, George Kyriazis, Pencho Petrushev, A New Proof of the Atomic Decomposition of Hardy Spaces, Constructive Theory of Functions (Sozopol 2016), pp. 59-73 (standard reference, not scraped)
- Mark Williams, Notes on Harmonic Analysis (January 11, 2022) (standard reference, not scraped)
- Li-An Daniel Wang, Multiplier Theorems on Anisotropic Hardy Spaces (PhD dissertation, University of Oregon, 2012) (standard reference, not scraped)
- Martin Hiserote, A Characterization of Anisotropic H^1(R^N) by Smooth Homogeneous Multipliers (PhD dissertation, University of Oregon, 2019) (standard reference, not scraped)