REVIEW 3 major objections 3 minor 1 cited by
The H\"ormander--Bernhardsson function in higher dimensions
T0 review · 3 major / 3 minor · reviewed 2026-08-27 · deepseek-v4-flash
Pith's one-line read For every dimension d≥1, the radial extremal function of the point-evaluation problem in Paley–Wiener space satisfies an explicit third-order linear ODE with polynomial coefficients.
desk verdict Gonçalves–Radchenko–Ramos closes the even-dimensional gap with a genuinely different proof; the announced ODE holds, but Proposition 3's PW membership needs a written proof. 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 machinery is the interpolation formula of Proposition 4, which states that for every $f\in PW_{d-1}$, $$\frac{f(z)}{\varphi_d(z)}=f(0)+f'(0)z+\frac{$z^{2}$}{2c_d}\sum_{n\geq 1}(-1)^n $t_n^{{d-1}}$\left[\frac{f(t_n)}{z-t_n}-\frac{f(-t_n)}{z+t_n}\right],\qquad c_d=\frac{d}{4C_d}.$$ This formula encodes the Euler–Lagrange equation as a sampling series of interpolation type over the zero sequence $\{t_{d,n}\}$. Applying it to carefully truncated test functions modelled on $z^{-d-1}$ yields the reciprocal expansions of Propositions 6 and 7, which in turn motivate the dimension-dependent factorization $\varphi_d=\Phi_+\Phi_-$ into two entire functions of exponential type 1. Lemma 8 gives each factor a second-order ODE with an entire error term; growth estimates for entire functions of exponential type force that error to be a polynomial of degree at most $d+1$, and the asymptotic zero-counting law for the extremal function fixes its leading coefficient, so the symmetric square of the second-order equation is exactly the ODE of Theorem 1.
What would settle it
Decisive check: for $d=2$, compute $\varphi_2$ and its zeros numerically, take the even test function whose Fourier transform is $(1-\xi^2)^4$ on $[-1,1]$ (so it lies in $PW_1$ with strong decay), and compare $f(z)/\varphi_2(z)$ with the right-hand side of Proposition 4 at several non-real $z$. A mismatch beyond numerical round-off would refute the interpolation formula and with it the proof of Theorem 1; an accurate match would support the theorem.
Extended reading notes
Core claim
The central claim is Theorem 1: for every $d\geq 1$, the Hörmander–Bernhardsson function $\varphi_d$ — the unique even, real-entire, exponential-type-1 minimizer of the weighted one-dimensional problem (1), normalized by $\varphi_d(0)=1$ — satisfies $$$z^{{2d+2}}$\varphi_d'''(z)+3(d+1)$z^{{2d+1}}$\varphi_d''(z)+\bigl((d+1)(2d+1)$z^{{2d}}$-r(z)\bigr)\varphi_d'(z)-\tfrac12 r'(z)\varphi_d(z)=0,$$ where $r(z)=-z^{2d+2}+\frac{d^2}{4C_d^2}\sum_{j=0}^d \alpha_j z^{2j}$ and $\alpha_j$ is the coefficient of $z^{2j}$ in $1/\varphi_d(z)^2$. Equivalently, $\varphi_d$ satisfies the two first-order identities displayed in the theorem. The proof derives an interpolation formula (Proposition 4) from the Euler–Lagrange equation, uses it to obtain reciprocal expansions that suggest a factorization $\varphi_d=\Phi_+\Phi_-$, proves a second-order ODE for each factor, and recovers the third-order equation as the symmetric square. This is the first characterization of the extremizer that holds uniformly in even and odd dimensions.
Load-bearing premise
The load-bearing premise is that the auxiliary function $g_z(w)=\frac{z f(z)\varphi_0(w)-w f(w)\varphi_0(z)}{w^2-z^2}$ belongs to the admissible space $PW_{d-1}$ for every $z$; the paper asserts this without proof, and the interpolation formula built on it drives the reciprocal expansions and the entire ODE derivation.
Editorial extensions
If this is right
- In dimension $d=1$, Theorem 1 recovers the known third-order equation for the Hörmander–Bernhardsson function obtained from the factorization $\varphi_1(z)=\Phi(z)\Phi(-z)$, so the new statement contains the one-dimensional case.
- For odd $d$, the reciprocal formula in Proposition 6 is equivalent to the quadratic functional identity of [9, Theorem 1(a)], so the new derivation is consistent with the existing odd-dimensional characterization while also covering even dimensions.
- Proposition 4 shows that every admissible function in $PW_{d-1}$ is determined by its values at the zeros $t_{d,n}$ through a sampling series of interpolation type, so the zero sequence gives complete sampling information in the weighted space for all $d$.
- The factorization $\varphi_d=\Phi_+\Phi_-$ holds in every dimension, with the factors built from alternating or parity-split subsequences of the zeros, and each factor has exponential type 1.
Reading between the lines
- Since Remark 5 states that every result through the interpolation formulas holds for real $d>0$, the same proof scheme may yield a continuous family of ODEs for weights $|x|^s$ with non-integer $s$, unifying the even/odd split into one analytic family.
- A numerical test of the ODE of Theorem 1 for $d=2$ or $d=4$ could determine whether the equation, together with $\varphi_d(0)=1$ and the known zero spacing, uniquely determines the extremizer; if it does, the ODE becomes a practical tool for computing $C_d$ to high precision and for conjecturing its asymptotic rate.
- The reciprocal formulas for even $d$ split the zeros into two alternating subsequences; a natural next step is to derive discrete equations for these subsequences, which may expose finer spacing statistics of the extremal zeros than the infinite product factorization does.
Signed reviews
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper studies the norm of the point evaluation functional on the Paley--Wiener space PW^1(R^d), reduces the problem to a weighted one-dimensional problem, and studies the unique extremizer φ_d, called the Hörmander–Bernhardsson function. The main result, Theorem 1, states that φ_d satisfies a third-order linear ODE with polynomial coefficients for every d ≥ 1, extending Gorbachev's odd-dimensional result. The proof proceeds by deriving a summation formula (Proposition 2), an interpolation formula (Propositions 3–4), reciprocal formulas (Propositions 6–7), a factorization φ_d = Φ_+ Φ_-, and finally the ODE by a symmetric-square argument. Lemma 10 identifies the polynomial r(z) by a power-series comparison and a zero-counting asymptotic.
Significance. If the gaps identified below are repaired, Theorem 1 is a substantial advance: it supplies the first unified differential-equation characterization of the extremal function in both even and odd dimensions, and the interpolation and reciprocal formulas are likely to be reusable tools. The proof is genuinely variational rather than tautological: the ODE is derived from the Euler–Lagrange equation, and the coefficients of r(z) are identified from the extremizer itself. The paper is also commendable for treating the parity issue explicitly and for attempting to be self-contained.
major comments (3)
- [Section 3.2, Proposition 3] The assertion that the divided-difference function g_z(w) = (z f(z) φ_0(w) − w f(w) φ_0(z))/(w^2 − z^2) lies in PW_{d−1} is stated without proof. This is not a formal consequence of f, φ ∈ PW_{d−1}: at infinity g_z(w) behaves like (f(z)φ(w) − f(w)φ(z))/w, and the stated hypotheses do not by themselves guarantee integrability against |w|^{d−1} dw. Since Proposition 2 is an identity valid only for functions in PW_{d−1}, and Proposition 3 feeds directly into the reciprocal formulas, Lemma 8, and the ODE of Theorem 1, this missing membership estimate is load-bearing. Please add an explicit lemma with a quantitative decay estimate, or provide an approximation argument that justifies applying the summation formula to g_z.
- [Section 3.2, Eq. (5), and Section 3.1] The derivation of equation (5) applies Proposition 2 to f_n(z) = φ_0(z)/(z^2 − t_n^2). The function f_n is entire of exponential type, but on the real line it behaves like φ(x)/x; membership in PW_{d−1} is not established and is not implied by φ ∈ PW_{d−1}. For d = 1 this would require ∫ |φ(x)|/|x| dx < ∞, which is stronger than φ ∈ L^1. The same unproved division by a linear factor occurs in the derivation of Proposition 2 itself, where identity (4) is applied to f(x)/x. These steps are not merely technical: without a division lemma or a limiting argument, the summation formula and all later interpolation identities rest on an unverified premise.
- [Section 2.1] The paper states that 'a standard argument shows that extremizers of (3) must exist' but gives neither the argument nor a specific reference. The existence of a minimizer is a prerequisite for defining φ_d and hence for the uniqueness and ODE arguments. If existence is already proved in [7] or [9], please cite the precise statement; otherwise include the compactness argument (for example, via the Paley–Wiener description and weak-* compactness of the relevant unit ball).
minor comments (3)
- [Section 5] The appendix proves Proposition 2 via a distributional identity and then says a 'routine approximation argument' completes the extension to PW_{d−1}; please spell out the approximation, since the interpolation formulas in Section 3 are applied to functions that are not compactly supported in frequency and need the full summability statement.
- [Section 4, Lemma 10] In the proof of Lemma 10 the notation φ1 is used for the derivative without a local definition; please write φ' consistently.
- [General] The title and abstract contain several broken spacing artifacts ('H ¨ormander'), and the paper would benefit from a final proofreading pass to normalize such typographical issues.
Circularity Check
No circularity: the ODE is derived from the variational Euler-Lagrange system, and the main proof dependencies do not reduce to self-citations or fitted inputs; the unproved g_z membership in Section 3.2 is a correctness gap, not a circular one.
full rationale
No circular step is present. Theorem 1 is derived from the Euler-Lagrange/first-variation identity (4) through Proposition 2, the interpolation formula (Proposition 3), the reciprocal formulas (Propositions 6 and 7), and the symmetric-square argument in Section 4. The coefficients alpha_j and the constant C_d are defined from the extremizer and the extremal constant, not fitted to force the ODE; Lemma 10 identifies r(z) by coefficient comparison inside the already-proved differential identity, which is a characterization rather than a tautology. The only self-citations to [4] and [7] are contextual, and the cited properties are either reproved in Section 2 or used only as background, so no load-bearing self-citation occurs. The manuscript does contain a genuine technical gap at Section 3.2, where the divided-difference function g_z(w) = (z f(z) phi_0(w) - w f(w) phi_0(z))/(w^2 - z^2) is asserted to lie in PW_{d-1} without proof, and Section 2.1 delegates existence of extremizers to 'a standard argument'. These are correctness risks that could invalidate the proof if false, but they are not cases of a prediction reducing to its inputs, so they do not affect the circularity score.
Assumptions & free parameters
assumptions (5)
- domain assumption Existence of an extremizer for the weighted L1 variational problem (1)
- domain assumption First-variation identity (4) applies to derivatives and divided differences of functions in PW_{d-1}
- standard math Krein's factorization theorem: a real entire function of exponential type that is nonnegative on R factorizes as h(z)h(conj z) with h of half the type
- standard math A ratio of two entire functions of exponential type, when entire, has exponential type (Lindelöf)
- standard math For a type-1 entire function bounded on R with only real zeros, the zero-counting function satisfies n(r)=r/π+o(r)
Cite this review
Pith. "Pith review of The H\"ormander--Bernhardsson function in higher dimensions." pith.science (2026). https://pith.science/paper/NU4ZZNYB
@misc{pith2026260822198,
author = {Pith},
title = {Pith review of: The H\"ormander--Bernhardsson function in higher dimensions},
year = {2026},
howpublished = {\url{https://pith.science/paper/NU4ZZNYB}},
note = {Machine review of arXiv:2608.22198}
}
abstract
We study the problem of finding the norm of the point evaluation operator in the Paley--Wiener space $PW^{1}(\r^d)$, consisting of $d$-variable functions of spherical exponential type that are integrable on $\r^d$. The extremal functions can be taken radial, which naturally leads us to consider a related extremal problem in a weighted Paley--Wiener space of single-variable functions. We establish that the radial extremal function must satisfy a third-order linear ODE with polynomial coefficients for every $d \geq 1$, extending Gorbachev's recent odd-dimensional result. Along the way, we prove interpolation and reciprocal formulas involving the zeros of the extremizer.
Forward citations
Cited by 1 Pith paper
-
Exact Asymptotics of the Multidimensional Nikolskii Constant
As d tends to infinity, 2^d times the normalized L1 Nikolskii constant converges to π/2, and the rescaled zeros of the extremal function converge to an explicit Bessel-type measure.
Reference graph
Works this paper leans on
-
[7]
F. Dai, D. Gorbachev, and S. Tikhonov, Estimates of the asymptotic Nikolskii constants for spher- ical polynomials, J. Complexity65(2021), 101553
work page 2021
-
[9]
D. V. Gorbachev, The Nikolskii constant in odd dimensions, preprint at arXiv:2608.15674 (2026)
work page Pith review arXiv 2026
-
[1]
N. N. Andreev, S. V. Konyagin, and A. Yu. Popov, Extremal problems for functions with small support, Math. Notes60(1996), no. 3, 241–247
work page 1996
-
[2]
Bergman, H¨ ormander’s inequality and point evaluations in de Branges space, Rev
A. Bergman, H¨ ormander’s inequality and point evaluations in de Branges space, Rev. Mat. Iberoam. 42(2026), no. 2, 551–572
work page 2026
-
[3]
A. Bondarenko, J. Ortega-Cerd` a, D. Radchenko, and K. Seip, The H¨ ormander–Bernhardsson ex- tremal function: a preliminary study, inRecent advances in approximation and potential theory, pp. 77–88, Birkh¨ auser, Cham, 2026
work page 2026
-
[4]
A. Bondarenko, J. Ortega-Cerd` a, D. Radchenko and K. Seip, The H¨ ormander–Bernhardsson ex- tremal function, preprint at arXiv:2504.05205
-
[5]
O. F. Brevig, A. Chirre, J. Ortega-Cerd` a, and K. Seip, Point evaluation in Paley–Wiener spaces, J. Anal. Math.153(2024), no. 2, 595–670
work page 2024
-
[6]
E. Carneiro, M. B. Milinovich, and K. Soundararajan, Fourier optimization and prime gaps, Com- ment. Math. Helv.94(2019), no. 3, 533–568
work page 2019
Show all 17 references
-
[8]
D. V. Gorbachev, An integral problem of Konyagin and thepC, Lq-constants of Nikolskii, Proc. Steklov Inst. Math.2005, Function Theory, S117–S138
2005
-
[10]
H¨ ormander and B
L. H¨ ormander and B. Bernhardsson, An extension of Bohr’s inequality, Boundary Value Problems for Partial Differential Equations and Applications, RMA Res. Notes Appl. Math., vol. 29, Masson, Paris, 1993, pp. 179–194
1993
-
[11]
Koosis,The logarithmic integral
P. Koosis,The logarithmic integral. Vol. I, Cambridge Studies in Advanced Mathematics, vol. 12, Cambridge University Press, Cambridge, 1988
1988
-
[12]
B. Ya. Levin,Lectures on entire functions, Translations of Mathematical Monographs, vol. 150, American Mathematical Society, Providence, RI, 1996
1996
-
[13]
Levin and D
E. Levin and D. Lubinsky,L p Christoffel functions,L p universality, and Paley–Wiener spaces, J. Anal. Math.125(2015), 243–283
2015
-
[14]
D. S. Lubinsky, Scaling limits of polynomials and entire functions of exponential type, inApprox- imation Theory XV: San Antonio 2016, Springer, Cham, 2017, pp. 219–238
2016
-
[15]
Plancherel and G
M. Plancherel and G. P´ olya, Fonctions entieres et integrales de Fourier multiples. Comment. Math. Helv.9, 224–248 (1937)
1937
-
[16]
Plancherel and G
M. Plancherel and G. P´ olya, Fonctions entieres et integrales de Fourier multiples. Comment. Math. Helv.10, 110–163 (1938)
1938
-
[17]
G. N. Watson,A treatise on the theory of Bessel functions, 2nd ed., Cambridge University Press, London, 1966, vii+804 pp. IMPA - Instituto de Matem´atica Pura e Aplicada, Rio de Janeiro, 22460-320, Brazil. Email address:goncalves@impa.br Institut des Hautes ´Etudes Scientifiqu...
1966
Reviewed August 27, 2026 · model on record in the stance chip above.
Discussion (0). Continue with ORCID to comment.