theoremnovelstructure_uncertain
Local smoothing on one frequency annulus
Bounds on at with loss
single-annulus estimate behind all the corollaries
Theorem·
thm:main·§1.3 An estimate on one frequency annulusStatement (paper)
Let , , and .
For set . Then
In plain English
For and , the wave propagator applied to a function with frequencies in the annulus (cut off by ) satisfies .
Why it's here
This is the paper's main estimate: at the critical exponent, local smoothing holds on a single dyadic annulus with only a logarithmic loss in . It rests on the periodic cap estimate, which supplies the factor and is brought to . The Euclidean local smoothing theorem, the logarithmic Sobolev corollary, and the extension and Kakeya corollaries then use it.
Classified novel:
The main new estimate: sharp local smoothing at the critical exponent p_c on a single frequency annulus, with only a [log N]^{2/p} loss. This improves the N^ε loss in the Guth–Wang–Zhang (n=2) and Bourgain–Demeter decoupling approaches, and is obtained by transferring the periodic cap estimate to R^n.
Uses
Used by
thmSobolev local smoothing for the wave equationcorLogarithmic Sobolev local smoothing estimatecorQuantitative extension and Kakeya boundscorGlobal spherical and cone extension estimatescorParaboloid extension and Schrödinger local smoothingpropAngular polynomial local smoothing boundlemLocal smoothing bound on small ballsclaimKakeya maximal estimate by dualityclaimLocal paraboloid extension with logarithmic lossclaimShell profile operator approximates propagatorclaimStrong bound for unselected angular bandsclaimPeriodic cap estimate gives Euclidean pencil estimate
Sources
PaperOpen
- Section
- §1.3 An estimate on one frequency annulus
- Page
- —
- Label
thm:main- Line
sections/introduction.tex:97
Leannot aligned
Phase 2 aligns this node to a Lean declaration.
Friction
- infostructure_uncertainAppendix D (sections/planar.tex) gives an alternative proof of the n=2 case via a linear Dirichlet problem, reproving Proposition 5.1's inequalities for a planar energy; it has no statement of its own.