REVIEW 1 major objections 4 minor 15 references
A note on a Pohozaev identity for the fractional Green function
T0 review · 1 major / 4 minor · reviewed 2026-08-07 · deepseek-v4-flash
Pith's one-line read The paper proves that in bounded $C^{1,1}$ domains with $N>2s$, the fractional Robin function $R_s(x)$ equals $\Gamma^2(1+s)/(N-2s)$ times the boundary integral of $(G_s(x,\cdot)/\delta^s)^2\langle\cdot-x,\nu\rangle$, extending the…
desk verdict A genuinely new fractional Pohozaev identity for the Robin function, proved mostly carefully, but the one-line y→x limit in Theorem 1.1 is a real gap that needs filling. read the letter →
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
The reading
What carries the argument
The load-bearing object is the generalized fractional integration-by-parts identity (1.10) with vector field $X=\mathrm{id}-\xi$, quoted from [8]: it converts sums of weighted gradient terms into a boundary term $\Gamma(1+s)^2\int_{\partial\Omega}(u/\delta^s)(v/\delta^s)\langle X,\nu\rangle\,d\sigma$ plus a double-integral remainder. The proof feeds the Green functions through cut-off approximations $\eta_k\psi_{\mu,x}G_s(x,\cdot)$ that vanish near the boundary and near the singularity, so the identity can be applied; then Lemmas 2.1--2.9 transfer the limits $k\to\infty$, $\mu\to0^+$, $\gamma\to0^+$ to recover exactly the boundary term and the regular parts $H_s$. Sharp two-sided estimates for $G_s$ and $\nabla G_s$ from [5, 13, 2] justify the needed integrability for these limits.
What would settle it
Take $\Omega$ to be the unit ball in $\mathbb{R}^3$ and choose $s=3/4$. The fractional Green function and its regular part are known explicitly for the ball, so one can numerically evaluate both sides of (1.7) at an off-center point $x$; agreement to machine precision would support the claim, and any systematic mismatch would refute it. A cheaper check is the endpoint test: as $s\to1^-$, the right side of (1.7) should reduce to the classical identity for the Laplacian.
Extended reading notes
Core claim
The central claim is Theorem 1.1: for bounded $C^{1,1}$ domains and $N>2s$, the fractional Robin function $R_s(x)=H_s(x,x)$ equals the boundary integral in (1.7), so the regular part of the fractional Green function is fully determined by a boundary trace. The identity is derived as the limit $y\to x$ of a two-point identity (Theorem 1.2) that expresses $(N-2s)H_s(x,y)+\langle\nabla_y H_s(x,y),y-x\rangle$ as the same kind of boundary integral. For $s>1/2$ the two-point identity holds with an arbitrary center $\xi$; for $s\le 1/2$ it holds with $\xi=x$, and taking $\xi=x$ in the former gives the full range. The proof applies a generalized fractional Pohozaev identity to regularized cutoff versions of the Green functions and passes to the limit using sharp boundary estimates; the same method yields the local identity (1.11), which the paper notes has no known counterpart even in the classical case.
Load-bearing premise
The identity is proved only for bounded $C^{1,1}$ domains and depends on sharp two-sided estimates for the fractional Green function and its gradient near the boundary; if the boundary is less regular than $C^{1,1}$, those estimates are not available and the limiting passages that produce the identity break down.
Editorial extensions
If this is right
- The regular part of the fractional Green function, and hence the Robin function, is completely determined by a boundary trace of the Green function itself; no interior information is needed beyond the domain geometry.
- The two-point identity (1.8) gives an explicit formula for $(N-2s)H_s(x,y)+\langle\nabla_y H_s(x,y),y-x\rangle$ in the whole range $s\in(0,1)$.
- For $s>1/2$, the stronger identity (1.9) yields separate control of both gradient terms and, by subtraction at $\xi=x$ and $\xi=y$, a new boundary formula for $\langle\nabla_x H_s(y,x)+\nabla_y H_s(x,y),x-y\rangle$.
- The same scheme proves the local identity (1.11), a new result even for the classical Laplacian, refining the classical asymptotics framework.
- Applied to fractional Sobolev-critical boundary value problems, the formula should give sharp asymptotic characterizations of solutions, improving the known profile results.
Reading between the lines
- The boundary-only character of (1.7) suggests that $R_s$ satisfies stronger geometric monotonicity than is currently known; for instance, in the ball one would expect $R_s(x)$ to be radial and increasing in $|x|$, which could be tested directly from the explicit Green function.
- Differentiating (1.7) under the integral sign (where justified) should produce gradient formulas for $H_s(x,\cdot)$ consistent with the representation formula in the cited work, without additional regularity assumptions.
- A density argument from $C^{1,1}$ domains to rougher boundaries is a natural next step: if the boundary trace $(G_s/\delta^s)^2$ remains integrable, the identity might extend to Lipschitz domains; a counterexample there would show the regularity threshold is essential.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper derives a fractional analogue of the Brezis–Peletier identity. Theorem 1.2 establishes, for x≠y in Ω, the two-point identity (1.8) relating the boundary integral of (G_s(x,·)/δ^s)(G_s(y,·)/δ^s) to the regular part H_s, and a variant (1.9) valid for s>1/2. Theorem 1.1 then asserts that letting y→x in (1.8) yields the Robin-function representation (1.7). The proof of Theorem 1.2 uses the generalized fractional Pohozaev identity from [8], approximates the Green functions by cut-offs ψ_{μ,x}G_s(x,·), and passes to the limit using estimates from [2,5,7,9,13]. A local s=1 counterpart is proved in Theorem 1.3. The central issue is the one-line proof of Theorem 1.1.
Significance. If the gap in the passage y→x is filled, the results are significant: the identity (1.7) generalizes the classical Brezis–Peletier formula to all s∈(0,1), determining the fractional Robin function from a boundary trace, and the two-point identities (1.8)–(1.9) are new tools for studying the gradient of the Robin function. The proof of Theorem 1.2 is careful and self-contained up to imported estimates; the split s≤1/2 vs s>1/2 is handled with explicit integrability computations (Remark 2.5). Theorem 1.3 correctly reproduces the local analogue. Nevertheless, the main theorem is currently not proven as written.
major comments (1)
- [Section 3, Proof of Theorem 1.1] The proof of Theorem 1.1 consists of the single sentence 'It is enough to observe that, fixing x∈Ω in (1.8), and letting y go to x, (1.7) follows.' This limit passage is load-bearing and is not justified. In (1.8) the left-hand side contains G_s(y,·)/δ^s under a boundary integral; passing y→x requires a trace theorem for the boundary quotient G_s(z,·)/δ^s on ∂Ω and continuity of that trace in the pole z, together with a uniform integrable bound to apply dominated convergence. The estimate (2.19) is an interior two-sided bound and does not by itself control the boundary quotient as the pole approaches x, nor is any reference given for such a trace result. On the right-hand side one also needs H_s(x,y)→R_s(x) and ⟨∇_yH_s(x,y), y−x⟩→0; these are plausible but are not stated or proved. Without this step, (1.8) alone does not imply the stated formula (1.7). I recommend that the authors supply a proof (or a precise citation) of the convergence of G_s(y,·)/δ^s to G_s(x,·)/δ^s on ∂Ω as y→x, uniformly over the boundary, and verify the RHS limit.
minor comments (4)
- [Lemma 2.3] Lemma 2.3 states w∈C(Ω), but the proof uses the L∞ norm of w (e.g., in the bound (2.18)). Since Ω is bounded, the assumption should be w∈C(Ω)∩L∞(Ω) or w∈C(Ω̅), and the applications indeed have bounded w.
- [Lemma 2.4] In the proof of Lemma 2.4 there is a typo: 'Lt us recall' should read 'Let us recall'.
- [Section 4, Theorem 1.3] The Pohozaev identity (4.1) is applied to the solutions u_{ρ,x}, u_{ρ,y} of (4.5), which are only C^1 (W^{2,p} for all p<∞) rather than C^2. The identity should be justified for such functions, for example by approximation or by noting that (4.1) extends to W^{2,p} functions. This is a standard technicality, but the manuscript currently does not address it.
- [Remark 2.5] The sentence about [3, Lemma 9] is ambiguous: the paper itself proves (2.23) for all s∈(0,1) (without uniformity in x), so clarify that only the uniform-in-x versions from [3] are restricted to s>1/2.
Circularity Check
No significant circularity: the central identity is derived from an independent external Pohozaev identity via approximation and limiting arguments; the one-line y→x passage is a possible gap, not a circular reduction.
full rationale
The proof chain is not circular. Theorem 1.2 is established by applying the generalized fractional Pohozaev identity (2.37), imported from Djitte–Fall–Weth [8], to regularized functions η_k ψ_{γ,y}G_s(y,·) and η_k ψ_{μ,x}G_s(x,·), and then passing to the limits k→∞, μ→0+, γ→0+ with the help of boundary estimates from Chen–Song [5], Kulczycki [13], Bogdan–Kulczycki–Nowak [2], and approximation lemmas from Djitte–Fall–Weth [7] and Djitte–Sueur [9]. None of these cited sources shares authors with the present paper, and none of the target identities (1.7)–(1.9) is assumed among the hypotheses. Theorem 1.1 is then obtained by fixing x in (1.8) and letting y→x. That one-sentence limit passage is asserted without detailed justification, so the proof may have an analytic gap, but a missing justification is not circularity: the boundary integral representation is not inserted as an input, and no fitted parameter or normalizing convention makes the conclusion true by definition. The only reference involving a present author, the forthcoming paper [6], is mentioned only as an intended application and is not load-bearing for any proof. Under the stated C^{1,1} and N>2s assumptions, the representation (1.7) has independent mathematical content relative to the external Pohozaev identity and estimates on which the derivation rests.
Assumptions & free parameters
assumptions (5)
- domain assumption Generalized fractional Pohozaev identity (Djitte-Fall-Weth [8, Theorem 1.3], reproduced as Lemma 2.10) holds for the regularized Green functions.
- domain assumption The fractional Green function satisfies the two-sided boundary estimate (2.19) and gradient estimate (2.21) in C^{1,1} domains, from [5,13] and [2].
- domain assumption The regularized functions ψμ,x Gs(x,·) satisfy the regularity and limit properties from [9, Lemma 2.2] and Lemmas 2.7-2.9.
- domain assumption The boundary distance function δ is C^{1,1} near ∂Ω and the Fermi map Ψ is bi-Lipschitz, allowing a change of variables near the boundary.
- domain assumption The product rule (2.5) for the fractional Laplacian and the approximation results from [7, Corollary 6.4] and [7, Lemma 6.8] are valid.
Cite this review
Pith. "Pith review of A note on a Pohozaev identity for the fractional Green function." pith.science (2026). https://pith.science/paper/4NUMJP3H
@misc{pith2026250602806,
author = {Pith},
title = {Pith review of: A note on a Pohozaev identity for the fractional Green function},
year = {2026},
howpublished = {\url{https://pith.science/paper/4NUMJP3H}},
note = {Machine review of arXiv:2506.02806}
}
read the original abstract
We get a Pohozaev-type identity for the fractional Green function, which extends to the fractional setting a classical result by Brezis and Peletier. Our result complements with some more recent ones obtained by Djitte and Sueur concerning a representation formula for the gradient of the fractional Robin function.
Reference graph
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Reviewed August 7, 2026 · model on record in the stance chip above.
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