Fourier restriction conjecture for the sphere

OPENLandmarkConjectureProposed c. 1967 · Standard version

Canonical statement

Let n3n\ge3, let dσd\sigma be surface measure on Sn1S^{n-1}, and for 1p,q<1\le p,q<\infty define
Eg(x)=Sn1e2πixωg(ω)dσ(ω). Eg(x)=\int_{S^{n-1}}e^{2\pi i x\cdot\omega}g(\omega)\,d\sigma(\omega).
If
q>2nn1andn+1qn1p,p=pp1 q>\frac{2n}{n-1} \quad\text{and}\quad \frac{n+1}{q}\le\frac{n-1}{p'}, \qquad p'=\frac{p}{p-1}
(with p=p'=\infty for p=1p=1), then there is C=C(n,p,q)C=C(n,p,q) such that EgLq(Rn)CgLp(Sn1,dσ)\|Eg\|_{L^q(\mathbb R^n)}\le C\|g\|_{L^p(S^{n-1},d\sigma)} for every gLp(Sn1,dσ)g\in L^p(S^{n-1},d\sigma).
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Let \(n\ge3\), let \(d\sigma\) be surface measure on \(S^{n-1}\), and for \(1\le p,q<\infty\) define \[ Eg(x)=\int_{S^{n-1}}e^{2\pi i x\cdot\omega}g(\omega)\,d\sigma(\omega). \] If \[ q>\frac{2n}{n-1} \quad\text{and}\quad \frac{n+1}{q}\le\frac{n-1}{p'}, \qquad p'=\frac{p}{p-1} \] (with \(p'=\infty\) for \(p=1\)), then there is \(C=C(n,p,q)\) such that \(\|Eg\|_{L^q(\mathbb R^n)}\le C\|g\|_{L^p(S^{n-1},d\sigma)}\) for every \(g\in L^p(S^{n-1},d\sigma)\).

The restriction conjecture concerns the extension operator Eg(x)=Sn1e2πixωg(ω)dσ(ω)Eg(x)=\int_{S^{n-1}}e^{2\pi i x\cdot\omega}g(\omega)\,d\sigma(\omega) associated with the sphere: it predicts that EE maps Lp(Sn1)L^p(S^{n-1}) boundedly into Lq(Rn)L^q(\mathbb R^n) exactly in the range of exponents forced by stationary-phase decay and by Knapp's cap examples, the key constraint being q>2n/(n1)q>2n/(n-1). The problem grew out of Stein's late-1960s work on restricting the Fourier transform to curved surfaces [Stein1993HarmonicAnalysis].

In two dimensions the conjecture is a classical theorem. In dimensions n3n\ge3 the necessary conditions are known to be sufficient on large subranges of exponents: methods including decoupling and polynomial partitioning have successively enlarged the known range [Tao2003RestrictionSurvey], with sharp oscillatory-integral estimates via polynomial partitioning among the strongest results in this direction [GuthHickmanIliopoulou2019Oscillatory].

Despite this progress, the full conjectured range is not established in any dimension n3n\ge3. The conjecture is closely linked to the Kakeya and Bochner–Riesz problems, and completing the remaining range is one of the central open goals of modern harmonic analysis.

The boxed statement is the canonical open formulation — not a stronger variant or a related research program. The status reflects the catalog's last review; do your own literature search before investing serious effort.