The Lᵖ integral is bounded by the p-th power of the Lᵖ seminorm #
For a finite exponent p ≠ 0, Mathlib's MeasureTheory.eLpNorm_nnreal_pow_eq_lintegral identifies
eLpNorm f p μ ^ p with ∫⁻ ‖f‖ₑ ^ p ∂μ for an almost everywhere strongly measurable f. Without
measurability the seminorm is ∞ by convention, so the inequality
∫⁻ ‖f‖ₑ ^ p ∂μ ≤ eLpNorm f p μ ^ p holds for every f
(TauCeti.lintegral_rpow_enorm_le_rpow_eLpNorm). This is the form in which a bound on the Lᵖ
seminorm is used to bound an integral, with no measurability side condition. For a natural
exponent n ≠ 0 and measurable f the identity reads ∫⁻ ‖f‖ₑ ^ n ∂μ = eLpNorm f n μ ^ n
(TauCeti.lintegral_enorm_pow_eq_eLpNorm_pow).
Consequently a function in Lᵖ for p ≠ 0 is finite almost everywhere
(MeasureTheory.MemLp.ae_enorm_lt_top), including for p = ∞.
The same identification gives monotone convergence for the seminorm: the Lᵖ seminorm of the
supremum of an increasing sequence of functions with values in [0, ∞] is the supremum of their
seminorms (MeasureTheory.eLpNorm_iSup_eq_iSup_eLpNorm), also for p = ∞.
For p ≠ 0, the integral ∫⁻ ‖f‖ₑ ^ p ∂μ is at most eLpNorm f p μ ^ p, whether or not f is
almost everywhere strongly measurable.
For n ≠ 0, the n-th power of the Lⁿ seminorm of an almost everywhere strongly measurable
function is the integral of ‖f‖ₑ ^ n.
Monotone convergence for the Lᵖ seminorm. The Lᵖ seminorm of the pointwise supremum
of an almost everywhere increasing sequence of almost everywhere measurable functions with values
in [0, ∞] is the supremum of their Lᵖ seminorms.
A function in Lᵖ with p ≠ 0 is finite almost everywhere.