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Weak Shanks Conjecture in Bidisk Hardy Spaces

Updated 9 July 2026
  • The Weak Shanks Conjecture is a hypothesis in bidisk Hardy spaces that asserted optimal polynomial approximants for zero-free functions would be zero-free, but explicit counterexamples have disproven it.
  • It originated from investigations in least-squares inverse problems and cyclicity in Hardy spaces, linking polynomial approximation methods with digital filter design stability.
  • Recent Fourier-analytic techniques and hypergeometric formulations have led to new counterexample families, providing a refined framework for understanding zero behavior in multivariable function theory.

Searching arXiv for recent and foundational papers on the Weak Shanks Conjecture and closely related work. The Weak Shanks Conjecture is a conjecture in the function theory of the bidisk concerning zeros of optimal polynomial approximants in H2(D2)H^2(\mathbb D^2). In its weak or “weakest” form, it asserts that if a polynomial ff is nonvanishing on D2\overline{\mathbb D^2}, then the optimal polynomial approximants to $1/f$ should be zero-free in D2\mathbb D^2. A closely related formulation quoted from Delsarte–Genin–Kamp assumes only that ff has no zeros in D2\mathbb D^2. This conjecture arose from least-squares inverse problems for two-variable filters and from the study of cyclicity and invariant subspaces in Hardy spaces. It is now known to be false: a first disproof was given by a degree-one counterexample in 2024, and a 2025 Fourier-analytic paper embedded that example in a broader parametric family, derived explicit hypergeometric formulas for the relevant Fourier data, and produced additional counterexamples (Bénéteau et al., 2024, Geronimo et al., 21 Aug 2025).

1. Statement and mathematical setting

The ambient space is the Hardy space H2(D2)H^2(\mathbb D^2), where D={zC:z<1}\mathbb D=\{z\in\mathbb C:|z|<1\}. For

g(z1,z2)=k,l0ak,lz1kz2l,g(z_1,z_2)=\sum_{k,l\ge 0} a_{k,l} z_1^k z_2^l,

the norm is

ff0

so the monomials ff1 form an orthonormal basis. For each ff2, let ff3 denote the two-variable polynomials spanned by monomials ff4 with ff5. Given ff6, an optimal polynomial approximant (OPA) of degree ff7 to ff8 is a polynomial ff9 minimizing

D2\overline{\mathbb D^2}0

Equivalently, D2\overline{\mathbb D^2}1 is the orthogonal projection of D2\overline{\mathbb D^2}2 onto the finite-dimensional subspace D2\overline{\mathbb D^2}3 (Bénéteau et al., 2024).

In the bidisk literature, the weak conjecture is usually stated as follows: if D2\overline{\mathbb D^2}4 is a polynomial with no zeros in D2\overline{\mathbb D^2}5, then its OPAs are zero-free in D2\overline{\mathbb D^2}6. The 2024 counterexample paper describes this as the “weakest” form, contrasting it with stronger earlier variants that did not assume D2\overline{\mathbb D^2}7 itself was zero-free in the bidisk (Bénéteau et al., 2024). A related formulation quoted in the 2025 Fourier-analytic paper is: if D2\overline{\mathbb D^2}8 is a polynomial with no zeros in D2\overline{\mathbb D^2}9, then its OPAs are zero-free in $1/f$0 (Geronimo et al., 21 Aug 2025). In the stable-polynomial terminology used in related structural work, a polynomial is stable if it has no zeros in $1/f$1 and strongly stable if it has no zeros in $1/f$2; the weak conjecture then becomes the assertion that strongly stable polynomials have OPAs that are stable (Felder, 2024).

2. Historical origin and pre-disproof structure

The conjecture belongs to the theory of least-squares inverse polynomials in two variables, with applications to recursive digital filter design. In one variable, the analogous zero-exclusion phenomenon is true: OPAs are zero-free in the closed unit disk. That one-variable fact suggested a bidisk analogue and partly explains why the conjecture persisted. The same minimization problem is also tied to cyclicity in Hardy spaces, because a function $1/f$3 is cyclic exactly when there exist polynomials $1/f$4 such that

$1/f$5

(Bénéteau et al., 2024).

Before the disproof, structural work emphasized several positive or restrictive results. One paper distinguished a strong Shanks conjecture—asserting zero-exclusion for OPAs of arbitrary polynomial $1/f$6—from the weaker form restricted to strongly stable $1/f$7, and it studied the zero geometry of OPAs through Gram matrices, reproducing kernels, and polynomial reflection (Felder, 2024). That paper also proved positive classes: if $1/f$8 for a one-variable $1/f$9 and a monomial D2\mathbb D^20, then every OPA is zero-free in the closed bidisk, so “one-variable functions in disguise” cannot furnish counterexamples. It further derived a determinantal criterion: for D2\mathbb D^21 zero-free in D2\mathbb D^22, the condition that D2\mathbb D^23 have no zeros in D2\mathbb D^24 is equivalent to the nonvanishing of a kernel-modified Gram determinant for every D2\mathbb D^25 (Felder, 2024).

This pre-disproof work clarified the real difficulty. The central issue was not the existence of OPAs or the linear algebra of the optimality equations, but the relation between the zero set of D2\mathbb D^26 and the zero sets of the approximants. The determinantal formulation made that difficulty explicit, but it did not resolve the conjecture.

3. The 2024 counterexample

The first disproof exhibits the explicit function

D2\mathbb D^27

Because D2\mathbb D^28 on D2\mathbb D^29, the principal branch is analytic on a neighborhood of ff0; hence ff1 is holomorphic and nonzero on the closed bidisk. The degree-one OPA to ff2 has the symmetric affine form

ff3

with ff4, since ff5 is symmetric in ff6 and has real Taylor coefficients (Bénéteau et al., 2024).

The proof reduces the bidisk minimization problem to a one-variable weighted Hilbert space ff7. Writing

ff8

the relevant weights are

ff9

The normal equations become

D2\mathbb D^20

and, using D2\mathbb D^21, reduce to

D2\mathbb D^22

From these, the paper derives the criterion

D2\mathbb D^23

If D2\mathbb D^24, then the diagonal restriction D2\mathbb D^25 changes sign on D2\mathbb D^26, so D2\mathbb D^27 vanishes at

D2\mathbb D^28

(Bénéteau et al., 2024).

The verification is analytic rather than symbolic. The coefficients of

D2\mathbb D^29

satisfy

H2(D2)H^2(\mathbb D^2)0

and the comparison H2(D2)H^2(\mathbb D^2)1 is proved by reducing it to a finite-sum inequality with explicit tail bounds. In particular, the paper states

H2(D2)H^2(\mathbb D^2)2

and obtains

H2(D2)H^2(\mathbb D^2)3

which yields H2(D2)H^2(\mathbb D^2)4 (Bénéteau et al., 2024).

Strictly speaking, this H2(D2)H^2(\mathbb D^2)5 is not a polynomial. The same paper addresses that point directly. OPAs depend continuously on H2(D2)H^2(\mathbb D^2)6, and the Taylor polynomials H2(D2)H^2(\mathbb D^2)7 converge uniformly to H2(D2)H^2(\mathbb D^2)8 on H2(D2)H^2(\mathbb D^2)9. Hence, for sufficiently large D={zC:z<1}\mathbb D=\{z\in\mathbb C:|z|<1\}0, the polynomial D={zC:z<1}\mathbb D=\{z\in\mathbb C:|z|<1\}1 remains zero-free on D={zC:z<1}\mathbb D=\{z\in\mathbb C:|z|<1\}2, and the degree-one OPA to D={zC:z<1}\mathbb D=\{z\in\mathbb C:|z|<1\}3 remains close enough to D={zC:z<1}\mathbb D=\{z\in\mathbb C:|z|<1\}4 to retain a zero in D={zC:z<1}\mathbb D=\{z\in\mathbb C:|z|<1\}5. This converts the analytic example into an actual polynomial counterexample satisfying the conjecture’s stated hypotheses (Bénéteau et al., 2024).

4. Fourier-analytic reformulation and the 2025 strengthening

The 2025 paper does not provide the first disproof; rather, it develops a systematic Fourier-analytic framework that produces additional counterexamples and reorganizes the mechanism behind the 2024 example. Its central family is

D={zC:z<1}\mathbb D=\{z\in\mathbb C:|z|<1\}6

The condition D={zC:z<1}\mathbb D=\{z\in\mathbb C:|z|<1\}7 places the singularity set D={zC:z<1}\mathbb D=\{z\in\mathbb C:|z|<1\}8 outside the closed bidisk, so D={zC:z<1}\mathbb D=\{z\in\mathbb C:|z|<1\}9 is holomorphic on a neighborhood of g(z1,z2)=k,l0ak,lz1kz2l,g(z_1,z_2)=\sum_{k,l\ge 0} a_{k,l} z_1^k z_2^l,0. The OPA problem is then encoded by the Fourier coefficients of g(z1,z2)=k,l0ak,lz1kz2l,g(z_1,z_2)=\sum_{k,l\ge 0} a_{k,l} z_1^k z_2^l,1 on g(z1,z2)=k,l0ak,lz1kz2l,g(z_1,z_2)=\sum_{k,l\ge 0} a_{k,l} z_1^k z_2^l,2 (Geronimo et al., 21 Aug 2025).

If

g(z1,z2)=k,l0ak,lz1kz2l,g(z_1,z_2)=\sum_{k,l\ge 0} a_{k,l} z_1^k z_2^l,3

and

g(z1,z2)=k,l0ak,lz1kz2l,g(z_1,z_2)=\sum_{k,l\ge 0} a_{k,l} z_1^k z_2^l,4

then the degree-g(z1,z2)=k,l0ak,lz1kz2l,g(z_1,z_2)=\sum_{k,l\ge 0} a_{k,l} z_1^k z_2^l,5 OPA

g(z1,z2)=k,l0ak,lz1kz2l,g(z_1,z_2)=\sum_{k,l\ge 0} a_{k,l} z_1^k z_2^l,6

satisfies the Toeplitz-like linear system

g(z1,z2)=k,l0ak,lz1kz2l,g(z_1,z_2)=\sum_{k,l\ge 0} a_{k,l} z_1^k z_2^l,7

The paper’s main technical theorem computes the Fourier coefficients g(z1,z2)=k,l0ak,lz1kz2l,g(z_1,z_2)=\sum_{k,l\ge 0} a_{k,l} z_1^k z_2^l,8 and g(z1,z2)=k,l0ak,lz1kz2l,g(z_1,z_2)=\sum_{k,l\ge 0} a_{k,l} z_1^k z_2^l,9 in closed ff00 form. The derivation is entirely Fourier-analytic and hypergeometric: expand ff01, multiply by its conjugate expansion, collect coefficients, and reduce the finite combinatorial sums by factorial identities and the Chu–Vandermonde formula. This converts the OPA computation into an explicit special-function problem (Geronimo et al., 21 Aug 2025).

For degree ff02, symmetry reduces the OPA to

ff03

Writing

ff04

the paper gives

ff05

ff06

ff07

Because ff08, the root condition simplifies to

ff09

so the degree-one OPA has a zero in ff10 exactly when

ff11

Equivalently,

ff12

This scalar inequality is the effective counterexample criterion (Geronimo et al., 21 Aug 2025).

The same paper also derives an integral reformulation of the degree-one root condition as a triple integral inequality involving ff13 kernels, and remarks that this form may be more conducive to analysis in ff14. It thereby reframes the zero problem not only in Fourier and Toeplitz terms but also in integral-special-function terms (Geronimo et al., 21 Aug 2025).

5. Explicit families and numerical optimization

The Fourier-analytic framework recovers the 2024 counterexample and supplies additional parameter choices. It first reproduces the original example by taking

ff15

for which the numerical check is

ff16

Thus the degree-one OPA for

ff17

has a zero in ff18, matching the earlier disproof (Geronimo et al., 21 Aug 2025).

The paper then gives additional examples, including two rational-function families with integer ff19. These are not themselves polynomial inputs, but, exactly as in the 2024 disproof, sufficiently high Taylor truncations yield polynomial counterexamples.

Parameters ff20 Verified inequality Consequence
ff21 ff22 Recovers the first counterexample
ff23 ff24 New explicit counterexample family
ff25 ff26 New explicit counterexample family

The same paper introduces the quotient

ff27

The bidisk-root condition is that this quotient be ff28. Minimizing it over ff29 therefore seeks degree-one OPAs whose zeros lie as close to the origin as possible. Using Matlab’s fmincon, the reported minimizer is

ff30

with minimal quotient

ff31

For these values, the OPA is approximately

ff32

which has a root, for instance, at

ff33

The authors interpret this as producing roots “the closest (in ff34, for instance) to the origin” (Geronimo et al., 21 Aug 2025).

6. Current status, significance, and terminology

The current status is definitive: the conjecture is false. What failed is the blanket assertion that zero-freeness of a polynomial ff35 on the bidisk, or on the closed bidisk in the weakest formulation, forces zero-freeness of all OPAs to ff36. The 2024 paper settled the problem by a degree-one counterexample, and the 2025 paper strengthened that disproof by placing the phenomenon inside a larger family

ff37

computing the relevant Fourier coefficients explicitly, and giving a practical optimization scheme for the parameters ff38 (Bénéteau et al., 2024, Geronimo et al., 21 Aug 2025).

A recurrent misconception in later summaries is that the Fourier-analytic paper supplies the first disproof. It does not. Its contribution is different: additional counterexamples, explicit hypergeometric formulas for the Fourier coefficients of ff39, a scalar degree-one criterion, an integral reformulation, and a numerical search strategy. Conversely, the fact that the first example is nonpolynomial is not an obstruction to the conjecture’s disproof, because sufficiently high Taylor truncations preserve zero-freeness on ff40 and inherit the zero-producing degree-one OPA behavior by continuity (Bénéteau et al., 2024, Geronimo et al., 21 Aug 2025).

The broader significance of the conjecture lies in two directions. Function-theoretically, it probes how orthogonal projection in ff41 interacts with the zero geometry of multivariable holomorphic functions. From the engineering side, the problem comes from least-squares inverse polynomials in two variables, where zero-freeness of approximants corresponds to a stability property in recursive digital filter design (Bénéteau et al., 2024). The disproof therefore marks a sharp departure from the one-variable Hardy-space picture.

The phrase “Weak Shanks Conjecture” is not unique across mathematics. In unrelated arithmetic literature, one paper uses it for a conjectural statement about ff42-Shanks primes and shows, under hypotheses including irreducibility of ff43 modulo ff44, that

ff45

(Jones, 2023). That number-theoretic usage is distinct from the bidisk Hardy-space conjecture discussed here.

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