In mathematics, singular integrals are central to abstract harmonic analysis and are intimately connected with the study of partial differential equations. Broadly speaking a singular intetgral is an integral operator
:
whose kernel function "K" : R"n"×R"n" → R"n" is singular along the diagonal "x" = "y". Specifically, the singularity is such that |"K"("x","y")| is of size |"x"−"y"|−"n" asymptotically as |"x" − "y"| → 0. Since such integrals may not in general be absolutely integrable, a rigorous definition must define them as the limit of the integral over |"y" − "x"| > ε as ε → 0, but in practice this is a technicality. Usually further assumptions are required to obtain results such as their boundedness on "L""p"(R"n").
The Hilbert transform
The archetypal singular integral operator is the Hilbert transform "H". It is given by convolution against the kernel "K"("x") = 1/(π"x") for "x" in R. More precisely,
:
and the "cancellation" condition
:
Then we know that "T" is bounded on "L"p(R"n") and satisfies a weak-type (1,1) estimate. Observe that these conditions are satisfied for the Hilbert and Reisz transforms, so this result is an extension of those result. [cite book | last = Grakakos | first = Loukas | coauthors = | title = Classical and Modern Fourier Analysis | chapter = 7 | work = | pages = | language = | publisher = Pearson Education, Inc. | place = New Jersey| date = 2004 | url = | accessdate = ] ]ingular integrals of non-convolution type
These are even more general operators. However, since our assumptions are so weak, it is not necessarily the case that these operators are bounded on "L'p.
Calderón-Zygmund kernels
A function "K" : R"n"×R"n" → R is said to be "Calderón-Zygmund kernel" if it satisfies the following conditions for some constants "C" > 0 and δ > 0.:
:
:
ingular Integrals of non-convolution type
A "singular integral of non-convolution type" is an operator "T" associated to a Calderón-Zygmund kernel "K" is an operator which is such that
:
whenever "f" and "g" are smooth and have disjoint support.[ Such operators need not be bounded on "L""p"]Calderón-Zygmund operators
A singular integral of non-convolution type "T" associated to a Calderón-Zygmund kernel "K" is called a "Calderón-Zygmund operator" when it is bounded on "L"2, that is, there is a "C">0 such that
:
for all smooth compactly supported ƒ.
It can be proved that such operators are, in fact, also bounded on all "L""p" with 1 < "p" < ∞.
The "T"("b") theorem
The "T"("b") theorem provides sufficient conditions for a singular integral operator to be a Calderón-Zygmund operator, that is for a singular integral operator associated to a Calderón-Zygmund kernel to be bounded on "L"2. In order to state the result we must first define some terms.
A "normalised bump" is a smooth function φ on R"n" supported in a ball of radius 10 and centred at the origin such that |∂α φ("x")| ≤ 1, for all multi-indices |α| ≤ "n" + 2. Denote by τ"x"(φ)("y") = φ("y" − "x") and φ"r"("x") = "r"−nφ("x"/"r") for all "x" in R"n" and "r" > 0. An operator is said to be "weakly bounded" if there is a constant "C" such that
:
for all normalised bumps φ and ψ. A function is said to be "accretive" if there is a constant "c" > 0 such that Re("b")("x") ≥ "c" for all "x" in R. Denote by "M""b" the operator given by multiplication by a function "b".
The "T"("b") theorem states that a singular integral operator "T" associated to a Calderón-Zygmund kernel is bounded on "L"2 if it satisfies all of the following three conditions for some bounded accretive functions "b"1 and "b"2: [cite article | last = David | first = | coauthors = Journé | coauthors = Semmes | title = Opérateurs de Calderón-Zygmund, fonctions para-accrétives et interpolation | publisher = Revista Matemática Iberoamericana | volume = 1 | pages = 1–56| language = French | date = 1985 | url = | accessdate = ]
(a) is weakly bounded;
(b) is in BMO;
(c) is in BMO, where "T""t" is the transpose operator of "T".
Notes