Schwarz rearrangement #
For a measure μ on a normed space and f : E → ℝ≥0∞, the Schwarz rearrangement
schwarzRearrangement μ f is the radially nonincreasing function whose strict superlevel set
{t < f*} is {x | μ (ball 0 ‖x‖) < μ {t < f}}:
schwarzRearrangement μ f x = ⨆ {t | μ (ball 0 ‖x‖) < μ {f > t}}, t.
For an additive Haar measure on a nontrivial finite-dimensional real normed space, a superlevel
set of finite measure is the centered open ball with the same measure, while one of infinite
measure is the whole space. Equimeasurability also holds in dimension zero. For Lebesgue measure
on a Euclidean space this is the symmetric decreasing rearrangement.
The definition is made directly from the distribution function t ↦ μ {f > t}, with no
measurability, integrability or finiteness hypotheses. For an additive Haar measure, a superlevel
set of infinite measure is replaced by the whole space, and one of measure zero by the empty set.
Consequently the rearrangement depends only on the a.e. class of f, and it is defined pointwise
at every point, so no further choice of representative is involved.
Its strict superlevel sets are {x | μ (ball 0 ‖x‖) < μ {f > t}}
(TauCeti.setOf_lt_schwarzRearrangement). For an additive Haar measure on a
finite-dimensional real normed space these sets have the same measure as {f > t}:
the rearrangement is equimeasurable with f (TauCeti.addHaar_setOf_lt_schwarzRearrangement).
For a.e.-measurable f, the layer-cake formula then gives equality of all ∫⁻ f ^ p for
0 < p, hence of every eLpNorm with finite exponent, while equality of essential suprema gives
the case p = ∞. Rearrangement is monotone under a.e. inequality, idempotent, and it sends the
indicator of a set s to the indicator of {x | μ (ball 0 ‖x‖) < μ s}. In a nontrivial
finite-dimensional real normed space with additive Haar measure, this set is the centered open
ball of measure μ s when that measure is finite, and the whole space when it is infinite.
The Hardy--Littlewood inequality says that rearranging two nonnegative functions can only increase
the integral of their product.
Schwarz rearrangement is a contraction for every Lᵖ distance with 1 ≤ p ≤ ∞, measured by the
extended distance on ℝ≥0∞. Two rearranged superlevel sets are concentric, so the measure of
their difference is the truncated difference of the original level measures. A level-by-level
formula for ∫⁻ (f - g) then gives the one-sided L¹ contraction, and writing (f - g) ^ p as a
mixture of the hinges f - g - r extends it to 1 < p; adding a constant commutes with
rearrangement, which gives the case p = ∞.
Main definitions and results #
TauCeti.schwarzRearrangement: the Schwarz rearrangement of anℝ≥0∞-valued function.TauCeti.lt_schwarzRearrangement_iff: its superlevel sets.TauCeti.measurable_schwarzRearrangement: it is always measurable.TauCeti.schwarzRearrangement_mono_ae,TauCeti.schwarzRearrangement_congr_ae: order preservation and independence of the representative.TauCeti.addHaar_setOf_lt_schwarzRearrangement: equimeasurability.TauCeti.addHaar_inter_setOf_lt_schwarzRearrangement: intersections of two rearranged superlevel sets have the smaller of the original level measures.TauCeti.lintegral_rpow_schwarzRearrangement,TauCeti.eLpNorm_schwarzRearrangement,TauCeti.memLp_schwarzRearrangement_iff: equality of integrals of powers and ofLᵖseminorms, and preservation of everyLᵖclass.MeasureTheory.Integrable.ae_schwarzRearrangement_ofReal_ne_top,MeasureTheory.Integrable.toReal_schwarzRearrangement: almost-everywhere finiteness and integrability of the real-valued rearrangement of the positive part of an integrable function.TauCeti.lintegral_mul_le_lintegral_schwarzRearrangement_mul: the Hardy--Littlewood rearrangement inequality.TauCeti.schwarzRearrangement_add_const: rearrangement commutes with adding a constant.TauCeti.addHaar_sdiff_setOf_lt_schwarzRearrangement: differences of two rearranged superlevel sets have the truncated difference of the original level measures.TauCeti.lintegral_sub_rpow_schwarzRearrangement_le,TauCeti.lintegral_edist_rpow_schwarzRearrangement_le,TauCeti.edist_schwarzRearrangement_le_essSup,TauCeti.eLpNorm_edist_schwarzRearrangement_le: one-sided and two-sidedLᵖcontraction for1 ≤ p ≤ ∞.
References #
- E. H. Lieb and M. Loss, Analysis, 2nd ed., Graduate Studies in Mathematics 14, AMS, 2001, Sections 3.3--3.5; Theorem 3.5 is the nonexpansivity of rearrangement.
Right continuity of the distribution function. The measure of a strict superlevel set
{t < f} is approached by those of strictly higher levels, so anything below it is already below
μ {s < f} for some s > t.
The Schwarz rearrangement of f : E → ℝ≥0∞ with respect to μ: the radially
nonincreasing function whose superlevel set {t < f*} is {x | μ (ball 0 ‖x‖) < μ {t < f}}.
For an additive Haar measure on a nontrivial finite-dimensional real normed space, this is the
centered open ball of the same measure when μ {t < f} is finite, and the whole space when it is
infinite.
Instances For
The defining formula of the Schwarz rearrangement.
Superlevel sets of the Schwarz rearrangement.
The strict superlevel sets of the Schwarz rearrangement, as sets.
Superlevel sets of Schwarz rearrangements are nested according to the measures of the original superlevel sets.
The Schwarz rearrangement is radially nonincreasing.
The Schwarz rearrangement is radial.
The Schwarz rearrangement is always measurable: its superlevel sets are preimages under the
norm of sublevel sets of the monotone function r ↦ μ (ball 0 r).
Order preservation. An a.e. inequality between functions gives a pointwise inequality between their Schwarz rearrangements.
Order preservation, pointwise form.
The Schwarz rearrangement depends only on the a.e. class of the function.
The Schwarz rearrangement is unchanged when the measure is multiplied by a nonzero finite constant: both sides of each defining comparison scale by that constant.
The Schwarz rearrangement of the indicator of a set is the indicator of
{x | μ (ball 0 ‖x‖) < μ s}. For an additive Haar measure on a nontrivial finite-dimensional real
normed space, this is the centered open ball of measure μ s when that measure is finite, and the
whole space when it is infinite.
At the origin the Schwarz rearrangement takes the value essSup f μ.
The Schwarz rearrangement is bounded by the essential supremum of f.
Equimeasurability. For an additive Haar measure, every strict superlevel set of the
Schwarz rearrangement has the same measure as the corresponding superlevel set of f. No
measurability or finiteness hypothesis is needed.
Two superlevel sets of Schwarz rearrangements are concentric, so their intersection has the smaller of the two original superlevel measures. No measurability or finiteness hypothesis is needed.
The Schwarz rearrangement is idempotent.
The Schwarz rearrangement has the same essential supremum as f.
Layer cake for the Schwarz rearrangement. For 0 < p, the Schwarz rearrangement has the
same integral of p-th powers as f.
The Schwarz rearrangement has the same integral as f.
The extended integral of the Schwarz rearrangement of the positive part of an integrable real function is finite.
The Schwarz rearrangement of the positive part of an integrable real function is finite almost everywhere.
The real-valued Schwarz rearrangement of the positive part of an integrable function is
integrable. The extended rearrangement is finite almost everywhere, so taking toReal changes
only its values on a null set.
The Schwarz rearrangement has the same Lᵖ seminorm as f, for every exponent
p ∈ [0, ∞].
The Schwarz rearrangement of an a.e.-measurable function lies in Lᵖ exactly when the function
does, for every exponent p ∈ [0, ∞].
Hardy--Littlewood rearrangement inequality. For two nonnegative a.e.-measurable functions on a finite-dimensional real normed space, Schwarz rearrangement can only increase the integral of their product. The statement includes infinite integrals and dimension zero.
Adding a constant commutes with Schwarz rearrangement.
The difference of two superlevel sets of Schwarz rearrangements has measure equal to the truncated difference of the two original level measures, since the two sets are concentric. No measurability or finiteness hypothesis is needed.
One-sided Lᵖ contraction of Schwarz rearrangement. For 1 ≤ p, the integral of the
p-th power of the truncated difference f - g can only decrease under Schwarz rearrangement.
Lᵖ contraction of Schwarz rearrangement, integral form. For 1 ≤ p, the integral of
the p-th power of the extended distance between two nonnegative functions can only decrease
under Schwarz rearrangement.
L^∞ contraction of Schwarz rearrangement. The extended distance between two Schwarz
rearrangements is bounded everywhere by the essential supremum of the distance between the two
functions. No measurability hypothesis is needed.
Lᵖ contraction of Schwarz rearrangement. For every exponent 1 ≤ p ≤ ∞, the Lᵖ
seminorm of the extended distance between two nonnegative functions can only decrease under
Schwarz rearrangement.