Bounded mean oscillation

• The universally adopted notation used for the set of BMO functions on a given domain Ω is BMO(Ω): when Ω = Rⁿ, BMO(Rⁿ) is simply symbolized as BMO.
• The BMO norm of a given BMO function u is denoted by ||u||_BMO: in some instances, it is also denoted as ||u||_∗.

BMO functions are locally L^p if 0 < p < ∞, but need not be locally bounded. In fact, using the John-Nirenberg Inequality, we can prove that

${\displaystyle \|u\|_{BMO}\simeq \sup _{Q}\left({\frac {1}{|Q|}}\int _{Q}|u-u_{Q}|^{p}dx\right)^{1/p}}$.

Constant functions have zero mean oscillation, therefore functions differing for a constant c > 0 can share the same BMO norm value even if their difference is not zero almost everywhere. Therefore, the function ||u||_BMO is properly a norm on the quotient space of BMO functions modulo the space of constant functions on the domain considered.

As the name suggests, the mean or average of a function in BMO does not oscillate very much when computing it over cubes close to each other in position and scale. Precisely, if Q and R are dyadic cubes such that their boundaries touch and the side length of Q is no less than one-half the side length of R (and vice versa), then

${\displaystyle |f_{R}-f_{Q}|\leq C\|f\|_{BMO}}$

where C > 0 is some universal constant. This property is, in fact, equivalent to f being in BMO, that is, if f is a locally integrable function such that |f_R−f_Q| ≤ C for all dyadic cubes Q and R adjacent in the sense described above and f is in dyadic BMO (where the supremum is only taken over dyadic cubes Q), then f is in BMO.[7]

Fefferman (1971) showed that the BMO space is dual to H¹, the Hardy space with p = 1.[8] The pairing between f ∈ H¹ and g ∈ BMO is given by

${\displaystyle (f,g)=\int _{\mathbb {R} ^{n}}f(x)g(x)\,\mathrm {d} x}$

though some care is needed in defining this integral, as it does not in general converge absolutely.

The John–Nirenberg Inequality is an estimate that governs how far a function of bounded mean oscillation may deviate from its average by a certain amount.

For each ${\displaystyle f\in \operatorname {BMO} \left(\mathbb {R} ^{n}\right)}$, there are constants ${\displaystyle c_{1},c_{2}>0}$, such that for any cube ${\displaystyle Q}$ in ${\displaystyle \mathbb {R} ^{n}}$,

${\displaystyle \left|\left\{x\in Q:|f-f_{Q}|>\lambda \right\}\right|\leq c_{1}\exp \left(-c_{2}{\frac {\lambda }{\|f\|_{BMO}}}\right)|Q|.}$

Conversely, if this inequality holds over all cubes with some constant C in place of ||f||_BMO, then f is in BMO with norm at most a constant times C.

The John–Nirenberg inequality can actually give more information than just the BMO norm of a function. For a locally integrable function f, let A(f) be the infimal A>0 for which

${\displaystyle \sup _{Q\subseteq \mathbb {R} ^{n}}{\frac {1}{|Q|}}\int _{Q}e^{\frac {|f-f_{Q}|}{A}}\mathrm {d} x<\infty .}$

The John–Nirenberg inequality implies that A(f) ≤ C||f||_BMO for some universal constant C. For an L^∞ function, however, the above inequality will hold for all A > 0. In other words, A(f) = 0 if f is in L^∞. Hence the constant A(f) gives us a way of measuring how far a function in BMO is from the subspace L^∞. This statement can be made more precise:[9] there is a constant C, depending only on the dimension n, such that for any function f ∈ BMO(Rⁿ) the following two-sided inequality holds

${\displaystyle {\frac {1}{C}}A(f)\leq \inf _{g\in L^{\infty }}\|f-g\|_{BMO}\leq CA(f).}$

When the dimension of the ambient space is 1, the space BMO can be seen as a linear subspace of harmonic functions on the unit disk and plays a major role in the theory of Hardy spaces: by using definition 2, it is possible to define the BMO(T) space on the unit circle as the space of functions f : T → R such that

${\displaystyle {\frac {1}{|I|}}\int _{I}|f(y)-f_{I}|\,\mathrm {d} y<C<+\infty }$

i.e. such that its mean oscillation over every arc I of the unit circle[10] is bounded. Here as before f_I is the mean value of f over the arc I.

Definition 3. An Analytic function on the unit disk is said to belong to the Harmonic BMO or in the BMOH space if and only if it is the Poisson integral of a BMO(T) function. Therefore, BMOH is the space of all functions u with the form:

${\displaystyle u(a)={\frac {1}{2\pi }}\int _{\mathbf {T} }{\frac {1-|a|^{2}}{|a-e^{i\theta }|^{2}}}f(e^{i\theta })\,\mathrm {d} \theta }$

equipped with the norm:

${\displaystyle \|u\|_{BMOH}=\sup _{|a|<1}\left\{{\frac {1}{2\pi }}\int _{\mathbf {T} }{\frac {1-|a|^{2}}{|a-e^{i\theta }|^{2}}}|f(e^{i\theta })-u(a)|\,\mathrm {d} \theta \right\}}$

The subspace of analytic functions belonging BMOH is called the Analytic BMO space or the BMOA space.

Charles Fefferman in his original work proved that the real BMO space is dual to the real valued harmonic Hardy space on the upper half-space Rⁿ × (0, ∞].[11] In the theory of Complex and Harmonic analysis on the unit disk, his result is stated as follows.[12] Let H^p(D) be the Analytic Hardy space on the unit Disc. For p = 1 we identify (H¹)* with BMOA by pairing f ∈ H¹(D) and g ∈ BMOA using the anti-linear transformation T_g

${\displaystyle T_{g}(f)=\lim _{r\rightarrow 1}\int _{-\pi }^{\pi }{\bar {g}}(e^{i\theta })f(re^{i\theta })\,\mathrm {d} \theta }$

Notice that although the limit always exists for an H¹ function f and T_g is an element of the dual space (H¹)*, since the transformation is anti-linear, we don't have an isometric isomorphism between (H¹)* and BMOA. However one can obtain an isometry if they consider a kind of space of conjugate BMOA functions.

The space VMO of functions of vanishing mean oscillation is the closure in BMO of the continuous functions that vanish at infinity. It can also be defined as the space of functions whose "mean oscillations" on cubes Q are not only bounded, but also tend to zero uniformly as the radius of the cube Q tends to 0 or ∞. The space VMO is a sort of Hardy space analogue of the space of continuous functions vanishing at infinity, and in particular the real valued harmonic Hardy space H¹ is the dual of VMO.[13]

A locally integrable function f on R is BMO if and only if it can be written as

${\displaystyle f=f_{1}+Hf_{2}+\alpha }$

where f_i ∈ L^∞, α is a constant and H is the Hilbert transform.

The BMO norm is then equivalent to the infimum of ${\displaystyle \|f_{1}\|_{\infty }+\|f_{2}\|_{\infty }}$ over all such representations.

Similarly f is VMO if and only if it can be represented in the above form with f_i bounded uniformly continuous functions on R.[14]

Let Δ denote the set of dyadic cubes in Rⁿ. The space dyadic BMO, written BMO_d is the space of functions satisfying the same inequality as for BMO functions, only that the supremum is over all dyadic cubes. This supremum is sometimes denoted ||•||_BMOd.

This space properly contains BMO. In particular, the function log(x)χ_[0,∞) is a function that is in dyadic BMO but not in BMO. However, if a function f is such that ||f(•−x)||_BMOd ≤ C for all x in Rⁿ for some C > 0, then by the one-third trick f is also in BMO. In the case of BMO on Tⁿ instead of Rⁿ, a function f is such that ||f(•−x)||_BMOd ≤ C for n+1 suitably chosen x, then f is also in BMO. This means BMO(Tⁿ ) is the intersection of n+1 translation of dyadic BMO. By duality, H¹(Tⁿ ) is the sum of n+1 translation of dyadic H¹.[15]

Although dyadic BMO is a much narrower class than BMO, many theorems that are true for BMO are much simpler to prove for dyadic BMO, and in some cases one can recover the original BMO theorems by proving them first in the special dyadic case.[16]