The Hardy–Littlewood maximal function #
The centred Hardy–Littlewood maximal function of f is
M f x = ⨆ r > 0, ⨍⁻ y in ball x r, ‖f y‖ₑ ∂μ,
the largest average of ‖f‖ over a ball centred at x. This file defines it, records the two
endpoint bounds it satisfies, and proves the maximal inequality in both of its forms: the weak
type (1,1) bound
t * μ {x | t < M f x} ≤ 4 ^ n * ∫⁻ x, ‖f x‖ₑ ∂μ
and, for 1 < p < ∞, the strong type (p, p) bound ‖M f‖_p ≤ C(n, p) * ‖f‖_p, for μ an
additive Haar measure on a real normed space of finite dimension n.
The maximal inequality is the first item of Lane B of the PDE roadmap, the estimate that drives
the Calderón–Zygmund theory and, through it, the Lᵖ regularity theory for elliptic equations.
It is also where the classical asymmetric pair of endpoints originates: M is bounded on L^∞
(TauCeti.maximalFunction_le_eLpNormEssSup) but, in positive dimension, not on L¹ — a failure
not formalised here — so the correct L¹ statement is the weak-type bound, and the strong (p, p)
bounds are obtained from those two ends by Marcinkiewicz interpolation. The qualification matters:
the L¹ failure is a positive-dimensional phenomenon, since in dimension 0 every ball is the
whole space and the averages defining M f collapse to ‖f‖ₑ.
The proof #
The weak-type bound is the Vitali covering argument, isolated here as
TauCeti.mul_measure_le_of_forall_exists_ball: if every point of a set S is the centre of a ball
of radius at most R on which ∫⁻ g is at least t times the measure of the ball, then
t * μ S ≤ 4 ^ n * ∫⁻ g. Mathlib's
Vitali.exists_disjoint_subfamily_covering_enlargement_closedBall extracts a pairwise disjoint
subfamily of those balls whose fourfold enlargements still cover S; the enlargement costs the
factor 4 ^ n because a Haar measure scales a ball of radius r by r ^ n, and disjointness turns
the sum of the integrals over the selected balls into a single integral over their union.
Applying this to S = {x | t < M f x} needs a uniform bound on the radii it selects, and that is
where finiteness of ∫⁻ ‖f‖ₑ enters: a ball whose average exceeds t has measure less than
∫⁻ ‖f‖ₑ / t, which in positive dimension bounds its radius. In dimension 0 it does not — every
ball is the whole space — and that degenerate case is proved separately.
The strong type (p, p) bound then comes from
TauCeti.lintegral_rpow_le_of_mul_meas_lt_le_of_le_eLpNormEssSup, the operator-level diagonal
case of Marcinkiewicz interpolation. That theorem performs the reusable split at height c * t.
Here c = d = 2⁻¹, so the low part is bounded by t / 2, its maximal function never reaches
t, and the weak-type bound applied to the high part gives
t * μ {M f > t} ≤ 2 * 4 ^ n * ∫⁻ x in {‖f‖ₑ > t / 2}, ‖f x‖ₑ ∂μ.
Main declarations #
TauCeti.maximalFunction: the centred Hardy–Littlewood maximal function, withTauCeti.setLAverage_le_maximalFunction,TauCeti.maximalFunction_leandTauCeti.lt_maximalFunction_iffas its interface.TauCeti.maximalFunction_const: the maximal function of a constant is that constant, so the normalisation is the intended one.TauCeti.maximalFunction_mono_ae,TauCeti.maximalFunction_congr_ae:Mis monotone in‖f‖ₑalmost everywhere, soM fdepends onfonly through‖f‖ₑand only up to a null set.TauCeti.maximalFunction_enorm: replacing a function by its extended norm leaves its maximal function unchanged.TauCeti.maximalFunction_zero,TauCeti.maximalFunction_add_le,TauCeti.maximalFunction_const_smul:Mis sublinear. Subadditivity and the endpoint bounds feed directly intoTauCeti.lintegral_rpow_le_of_mul_meas_lt_le_of_le_eLpNormEssSup.TauCeti.maximalFunction_le_eLpNormEssSup: theL^∞endpoint.TauCeti.lowerSemicontinuous_maximalFunction,TauCeti.measurable_maximalFunction: the superlevel sets{x | t < M f x}are open, soM fis Borel measurable.TauCeti.mul_measure_le_of_forall_exists_ball: the Vitali covering estimate.TauCeti.mul_measure_lt_maximalFunction_le,TauCeti.measure_lt_maximalFunction_le: the maximal inequality, in product and in quotient form.TauCeti.ae_maximalFunction_lt_top: the maximal function of anL¹function is finite almost everywhere.TauCeti.lintegral_rpow_maximalFunction_le,TauCeti.eLpNorm_maximalFunction_le: the strong type(p, p)maximal inequality for1 < p < ∞, with an explicit constant.TauCeti.eLpNorm_maximalFunction_lt_top,TauCeti.ae_maximalFunction_lt_top_of_eLpNorm_ne_top: a function with finiteLᵖseminorm has a maximal function with finiteLᵖseminorm for1 < p ≤ ∞, and the maximal function is finite almost everywhere for every1 ≤ p ≤ ∞.
The maximal function defined here is the centred one, whose averages are over the balls centred at the point. The uncentred variant, over all balls containing the point, is comparable to it with a dimensional constant and is not needed downstream.
References #
- E. Stein, Singular Integrals and Differentiability Properties of Functions, Chapter I.
- L. Grafakos, Classical Fourier Analysis, Section 2.1.
The centred Hardy–Littlewood maximal function of f with respect to μ: the supremum
over the radii r > 0 of the average of ‖f‖ₑ over the ball of radius r centred at x.
The averages are taken in ℝ≥0∞, so this is defined for every f, taking the value ∞ at the
points where the averages are unbounded.
Equations
Instances For
Every ball average is at most the maximal function: the introduction rule.
A bound holding for every ball average bounds the maximal function: the elimination rule.
The maximal function exceeds t exactly when some ball average does.
If ‖f‖ₑ ≤ ‖g‖ₑ almost everywhere, then M f ≤ M g.
Functions whose norms agree almost everywhere have the same maximal function.
Replacing a function by its extended norm leaves its maximal function unchanged.
The L^∞ endpoint of the maximal inequality: the maximal function of f is bounded by the
essential supremum of ‖f‖, with constant 1.
The maximal function of a constant is that constant: the averages defining it are normalised, so no factor of the measure of a ball is left behind.
The maximal function is positively homogeneous: scaling f by c scales M f by ‖c‖ₑ.
This is the first half of the sublinearity of M, the second being
TauCeti.maximalFunction_add_le.
The maximal function of the zero function is zero.
The maximal function is subadditive, the second half of that sublinearity. Only the norm of the first summand need be measurable.
The Vitali covering estimate. If every point of S is the centre of a ball of radius at
most R on which ∫⁻ g is at least t times the measure of the ball, then
t * μ S ≤ 4 ^ n * ∫⁻ g, with n the dimension of the space.
The factor 4 ^ n is the cost of passing from a pairwise disjoint subfamily of those balls to its
fourfold enlargement, which still covers S.
The superlevel sets of the maximal function are open: enlarging the radius slightly keeps the
average of ‖f‖ₑ above t, at every nearby centre.
The maximal function is Borel measurable, being lower semicontinuous. No hypothesis on f is
needed: the supremum defining M f is over balls, not over values of f.
The Hardy–Littlewood maximal inequality, the weak-type (1,1) bound: the measure of the
set where the maximal function exceeds t, multiplied by t, is at most 4 ^ n times the L¹
norm of f, with n the dimension of the space.
No integrability hypothesis is needed: the bound is vacuous when ∫⁻ x, ‖f x‖ₑ ∂μ = ∞.
The Hardy–Littlewood maximal inequality, in quotient form.
The maximal function of an L¹ function is finite almost everywhere: the maximal inequality
with t → ∞.
The Hardy–Littlewood maximal inequality, the strong-type (p, p) bound for 1 < p < ∞,
as an inequality between the integrals ∫⁻ ‖·‖ₑ ^ p:
∫⁻ (M f) ^ p ∂μ ≤ (2 * p * 2 ^ (p - 1) / (p - 1)) * 4 ^ n * ∫⁻ ‖f‖ₑ ^ p ∂μ.
The constant degenerates as p → 1, as it must in positive dimension, where M is not bounded on
L¹.
The Hardy–Littlewood maximal inequality, the strong-type (p, p) bound for 1 < p < ∞,
in terms of representative-level Lᵖ seminorms.
Together with TauCeti.maximalFunction_le_eLpNormEssSup (the case p = ∞) and
TauCeti.mul_measure_lt_maximalFunction_le (the weak-type substitute at p = 1), this gives the
representative-level strong estimate for the maximal function. The resulting finiteness statement
is recorded by
TauCeti.eLpNorm_maximalFunction_lt_top below.
The maximal function of an Lᵖ function has finite Lᵖ seminorm when 1 < p ≤ ∞.
The maximal function of a function with finite Lᵖ seminorm is finite almost everywhere
when 1 ≤ p, including both endpoints.