Lower integrals of a real power, and the layer cake formula in ℝ≥0∞ #
This file collects the two lower integrals of t ↦ t ^ s on a half-line that the real
interpolation method needs, and uses them to transport Mathlib's layer cake formula from
real-valued to ℝ≥0∞-valued functions.
For -1 < s the function t ↦ t ^ s is integrable near 0 and not integrable near ∞, and the
two computations below are the two halves of that dichotomy:
TauCeti.lintegral_ofReal_rpow_Ioo evaluates ∫⁻ t in (0, a), t ^ s to the expected
antiderivative for such an s, while TauCeti.lintegral_ofReal_rpow_Ioi records that
∫⁻ t in (0, ∞), t ^ s diverges — the latter for every exponent s, since a power that is
integrable at the origin is not integrable at infinity and conversely.
TauCeti.lintegral_indicator_ofReal_rpow_Ioi packages the two together as the single formula the
real interpolation method uses: the integral over (0, ∞) of t ^ s cut off at the height where
c * t reaches a threshold a : ℝ≥0∞, which is the finite antiderivative when a is finite and
∞ when it is not.
TauCeti.lintegral_indicator_le_ofReal_rpow_Ioi is the companion over the complementary region,
where c * t has already passed the threshold. There the roles of the two endpoints are
exchanged: the integral converges at infinity and diverges at the origin, so the exponent range is
s < -1 and the value is ∞ exactly when the threshold is 0. The two together are what the
real interpolation method between two finite exponents integrates against, the first for the part
of a function above a height and the second for the part below it.
The layer cake formula ∫⁻ u ^ p = p * ∫⁻ t in (0, ∞), ν {u > t} * t ^ (p - 1) is in Mathlib as
MeasureTheory.lintegral_rpow_eq_lintegral_meas_lt_mul, but only for a nonnegative real-valued
u. Analysis in ℝ≥0∞ — where the operators of interpolation theory naturally land, since a
supremum of averages such as the Hardy–Littlewood maximal function is defined without any
finiteness hypothesis — needs the version for u : β → ℝ≥0∞, which is
TauCeti.lintegral_rpow_eq_lintegral_meas_ofReal_lt_mul below. The superlevel sets there are cut
at the ℝ≥0∞-valued threshold ENNReal.ofReal t, which is what distinguishes the statement from
Mathlib's.
The passage between the two is by ENNReal.toReal, which is faithful exactly where u is finite.
Where u = ∞ on a set of positive measure both sides are ∞: the left because u ^ p = ∞
there, and the right because every superlevel set then has measure at least that of {u = ∞},
and ∫⁻ t in (0, ∞), t ^ (p - 1) diverges. That is where TauCeti.lintegral_ofReal_rpow_Ioi is
used, and it is why the statement needs no finiteness hypothesis on u.
Main declarations #
TauCeti.lintegral_ofReal_rpow_Ioo:∫⁻ t in (0, a), t ^ s = a ^ (s + 1) / (s + 1)for-1 < sand0 ≤ a.TauCeti.lintegral_ofReal_rpow_Ioi:∫⁻ t in (0, ∞), t ^ s = ∞, for everys.TauCeti.lintegral_indicator_ofReal_rpow_Ioi: the same integral truncated at the height wherec * treachesa : ℝ≥0∞, evaluated toc ^ (-(s + 1)) / (s + 1) * a ^ (s + 1).TauCeti.lintegral_indicator_le_ofReal_rpow_Ioi: the integral over the complementary region, wherec * tis at leasta, evaluated toc ^ (-(s + 1)) / (-(s + 1)) * a ^ (s + 1)fors < -1.TauCeti.setLIntegral_Ioc_ite_rpow_le: an upper-tail bound for a negative power restricted by a linear threshold.TauCeti.setLIntegral_Ioc_rpow_mul_ite_le: the same bound with constant and linear weights.TauCeti.lintegral_rpow_eq_lintegral_meas_ofReal_lt_mul: the layer cake formula for anℝ≥0∞-valued function.TauCeti.sigmaFinite_restrict_pos_of_lintegral_rpow_ne_top: a function with finite positive power integral is carried by a σ-finite part of the measure.
References #
- L. Grafakos, Classical Fourier Analysis, Proposition 1.1.4.
The lower integral of t ^ s over a bounded interval (0, a), for -1 < s and 0 ≤ a: the
power is integrable at the origin and the value is the expected antiderivative.
Nonnegativity of a is needed: for a < 0 the interval is empty while a ^ (s + 1), a real power
at a negative base, need not vanish.
The tail integral ∫_{r / D}^∞ t ^ (-n - 1) dt = D ^ n r ^ (-n) / n bounds the integral of
t ^ (-n - 1) over those t ∈ (0, 1] with r ≤ t * D.
The bound of setLIntegral_Ioc_ite_rpow_le, multiplied by the length r of a segment and by
a weight a, gives the kernel r ^ (1 - n).
The lower integral of t ^ s over (0, ∞), truncated at the height where c * t reaches a
threshold a : ℝ≥0∞: for -1 < s and 0 < c,
∫⁻ t in (0, ∞), [c * t < a] * t ^ s = c ^ (-(s + 1)) / (s + 1) * a ^ (s + 1).
For a finite a the cut-off makes this the integral over (0, a / c) evaluated by
TauCeti.lintegral_ofReal_rpow_Ioo; for a = ∞ the cut-off is vacuous and both sides are ∞, by
TauCeti.lintegral_ofReal_rpow_Ioi. This is the inner integral of the real interpolation method,
where a is the value of the function being interpolated at a point.
The lower integral of t ^ s over (0, ∞), restricted to the heights at which c * t has
already reached a threshold a : ℝ≥0∞: for s < -1 and 0 < c,
∫⁻ t in (0, ∞), [a ≤ c * t] * t ^ s = c ^ (-(s + 1)) / (-(s + 1)) * a ^ (s + 1).
For a nonzero a this is the convergent tail integral over [a / c, ∞); for a = 0 the
restriction is vacuous and both sides are ∞, by TauCeti.lintegral_ofReal_rpow_Ioi, while for
a = ∞ the region is empty and both sides vanish. This is the inner integral that the real
interpolation method pairs with the part of a function below the height c * t, the exponent
range s < -1 being the one in which the power is integrable at infinity; the complementary
region is TauCeti.lintegral_indicator_ofReal_rpow_Ioi.
A function with a finite L^p norm is carried by a σ-finite part of the measure: the level
sets {f ≥ 1 / (n + 1)} have finite measure by Chebyshev's inequality applied to f ^ p, and they
exhaust {f > 0}.
The layer cake formula for an ℝ≥0∞-valued function: for 0 < p,
∫⁻ u ^ p ∂ν = p * ∫⁻ t in (0, ∞), ν {u > t} * t ^ (p - 1),
where the superlevel set is cut at the threshold ENNReal.ofReal t.
This is MeasureTheory.lintegral_rpow_eq_lintegral_meas_lt_mul for a function that is allowed to
take the value ∞; no finiteness hypothesis is needed, because both sides are ∞ as soon as
{u = ∞} has positive measure.