Scientists / Open questions

查尔斯·费弗曼

Charles Louis Fefferman

调和分析、偏微分方程

1978 年菲尔兹奖

13 个问题

  1. Sharp critical coupling and sharp stability constants for the pseudo-relativistic many-body Coulomb Hamiltonian

  2. Linear extension operators for Sobolev spaces on weighted trees: the endpoint cases p=1p=1 and p=∞p=\infty, the inhomogeneous space W1,p(T)W^{1,p}(T), non-radially-symmetric weights, and the planar W˙2,p(R2)\dot W^{2,p}(\mathbb{R}^2) extension problem for 1<p<21<p<2

  3. Rigorous justification of vortex-line dynamics in the 3D Euler equations: construction of almost-sharp vortex tubes and derivation of the vortex filament equation

  4. The sharp HH-stability constant of many-body Pauli--Fierz matter: the ε(Z)≤const⋅Z\varepsilon(Z)\le\mathrm{const}\cdot Z conjecture

  5. The omitted details in Fefferman's linear interpolation and extrapolation operators: an explicit bounded-depth construction for finite sets and the m=1m=1 case of the Banach-limit passage

  6. The oscillatory fourth term in the ground-state energy of large atoms: open quantitative problems on the Weyl sums of Córdoba–Fefferman–Seco (1995)

  7. Semialgebraic sections of semialgebraic CmC^m-jet bundles in dimensions n≥3n \ge 3 at fixed smoothness m≥2m \ge 2

  8. Logarithmic and nonlocal terms in the boundary asymptotic expansion of the harmonic projection kernels of the Bergman metric on strictly pseudoconvex domains

  9. The spin of the ground state of a large atom: sharp bounds and extensions to molecules

  10. Bounded linear Sobolev L2,pL^{2,p} extension for arbitrary finite subsets of the plane when 1<p<21<p<2

  11. The Sharp Interpolation Algorithm for Cm(Rn)C^m(\mathbb{R}^n) (Fefferman's Conjecture 2): computing (1+ϵ)(1+\epsilon)-optimal interpolants of finite data with near-linear work

  12. Finite-time pinch-off of capillary jets in the Navier–Stokes equations with surface tension

  13. Uniform-in-surface-tension local well-posedness and desingularization control for 2D water waves with surface tension beyond the Rayleigh–Taylor-positive regime

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