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Smooth half-space trace power bounded by the Holder product of its zero-order and normal-derivative energies

Proved
HunterPDE.Compactness.smooth_halfSpace_trace_power_le_holder

by Mazecto · Oct 17, 2026 · Mathlib 0df444a (Lean v4.33.1)

pdesobolev-spacestrace

The LpL^pLp power of the boundary restriction of a smooth half-space function is bounded by the Holder product of its zero-order LpL^pLp energy and the LpL^pLp energy of its normal weak derivative.

Let m≥0m\ge0m≥0, let 1≤p<∞1\le p<\infty1≤p<∞, and let H={x∈Rm+1:xm+1>0}H=\{x\in\mathbb{R}^{m+1}:x_{m+1}>0\}H={x∈Rm+1:xm+1​>0} be the open upper half-space in dimension m+1m+1m+1. Let f:Rm+1→Rf:\mathbb{R}^{m+1}\to\mathbb{R}f:Rm+1→R be smooth up to the boundary of HHH and vanish on the closed half-space outside an ambient compact set. Write D0fD_0fD0​f and DnfD_nfDn​f for the chosen weak derivatives of orders zero and one in the last (normal) coordinate, and identify ∂H\partial H∂H with Rm\mathbb{R}^mRm through x′↦(x′,0)x'\mapsto(x',0)x′↦(x′,0). Then

∥f(⋅,0)∥pp≤p ∥D0f∥Lp(H)p−1 ∥Dnf∥Lp(H),\|f(\cdot,0)\|_p^p\le p\,\|D_0f\|_{L^p(H)}^{p-1}\,\|D_nf\|_{L^p(H)},∥f(⋅,0)∥pp​≤p∥D0​f∥Lp(H)p−1​∥Dn​f∥Lp(H)​,

where both norms on the right use Lebesgue measure restricted to the open half-space, and the exponents p−1p\frac{p-1}{p}pp−1​ and 1p\frac1pp1​ accompany the zero-order and normal-derivative energies respectively. The bound is uniform in the dimension and includes p=1p=1p=1 and m=0m=0m=0; no vanishing of fff on the boundary is assumed.

This is the first (Holder) half of the anisotropic smooth trace estimate that underlies Hunter's trace theorem for W1,pW^{1,p}W1,p on the half-space, stated in the form in which it is combined with Young's inequality.

Formalization Note The weak derivatives are the chosen representatives weakDeriv; they agree almost everywhere with the classical derivatives of the smooth function. The boundary power and both energies are written with eLpNorm raised to the real exponent p.toReal.

Preamble
import Definitions.Def_HunterPDE_Compactness_Sobolev
import Definitions.Def_HunterPDE_Compactness_HalfSpace
import Mathlib.MeasureTheory.Function.LpSeminorm.Basic
open MeasureTheory HunterPDE.Compactness
open scoped ENNReal NNReal
set_option autoImplicit false
Formal statement
theorem HunterPDE.Compactness.smooth_halfSpace_trace_power_le_holder {m : ℕ}
    (p : ℝ≥0∞) (hp : 1 ≤ p) (hp' : p ≠ ∞)
    (f : EuclideanSpace ℝ (Fin (m + 1)) → ℝ)
    (hf : IsSmoothCompactClosedHalfSpace f) :
    eLpNorm (fun x' => f (boundaryPoint x')) p volume ^ p.toReal ≤
      ENNReal.ofReal p.toReal *
        (eLpNorm (HunterPDE.Shared.weakDeriv (upperHalfSpace m) 0 f)
            p (volume.restrict (upperHalfSpace m)) ^ p.toReal) ^ ((p.toReal - 1) / p.toReal) *
        (eLpNorm (HunterPDE.Shared.weakDeriv (upperHalfSpace m)
            (Pi.single (Fin.last m) 1) f)
            p (volume.restrict (upperHalfSpace m)) ^ p.toReal) ^ (1 / p.toReal) := by sorry
Source
J. K. Hunter, Notes on Partial Differential Equations, revised 6/18/2014, https://www.math.ucdavis.edu/~hunter/pdes/ch3.pdf, proof of Theorem 3.44, printed p. 72 (normal fundamental theorem, Fubini and Holder step). Anisotropic Holder form of the smooth trace estimate; it is the first half of the derivation of the two-energy bound.

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