Papers
Topics
Authors
Recent
Search
2000 character limit reached

Takagi–Pfister Skew Eigenvectors

Updated 12 July 2026
  • Takagi–Pfister skew eigenvectors are defined as extremal solutions of an antilinear eigenvalue problem using truncated Toeplitz operators and reflection conjugation on polynomial subspaces of Hardy spaces.
  • They generate rational inner approximants of Padé type for bounded holomorphic functions, linking to Montessus de Ballore-type convergence on polydisks.
  • The framework connects to Agler–Herglotz–Nevanlinna interpolation, providing semialgebraic coefficient characterizations while addressing pole distribution challenges in several variables.

Searching arXiv for the specified paper and topic to ground the article in the cited source. Takagi–Pfister skew eigenvectors are extremal solutions of an antilinear eigenvalue problem associated with truncated Toeplitz operators and a reflection conjugation on polynomial subspaces of Hardy spaces over the disk or polydisk. In the framework developed in "The multivariate Herglotz-Nevanlinna class: Rational approximation" (Bhowmik et al., 19 Sep 2025), they generalize the one-variable Takagi variational principle to several complex variables through Pfister’s extension, and they generate rational inner approximants of Padé type for bounded holomorphic functions on DdD^d. The same framework connects these extremals to Montessus de Ballore-type convergence on polydisks, to constructive Cayley rational inner interpolation in the Agler–Herglotz–Nevanlinna class, and to semialgebraic descriptions of finite Taylor coefficient sets. A central unresolved issue is the distribution of poles arising from the reflected denominator polynomials in several variables (Bhowmik et al., 19 Sep 2025).

1. Variational and operator-theoretic definition

For a complex symmetric matrix SS with S=STS = S^T, Takagi’s factorization yields a decomposition S=UDUTS = U D U^T, where UU is unitary and DD is diagonal with nonnegative entries. Equivalently, the Takagi singular values are obtained from the antilinear eigenvalue equation

S u‾=σu,σ≥0.S\,\overline{u} = \sigma u, \qquad \sigma \ge 0.

In the analytic setting, this matrix model is replaced by a truncated Toeplitz/Hankel construction associated with a bounded holomorphic function (Bhowmik et al., 19 Sep 2025).

On the polydisk DdD^d, for each multi-index n∈N0dn \in \mathbb{N}_0^d, one considers the polynomial space

Cn[z]:={g(z) of multidegree ≤n},\mathbb{C}_n[z] := \{g(z)\text{ of multidegree }\le n\},

the orthogonal projection SS0 onto SS1 with respect to the Hardy SS2 inner product, the truncated Toeplitz operator

SS3

and the conjugation

SS4

These satisfy the symmetry relation

SS5

The Takagi–Pfister skew-eigenvector equation is then

SS6

With the SS7 inner product SS8, this is equivalent to

SS9

The extremal value is the operator norm,

S=STS = S^T0

and the paper states that S=STS = S^T1 (Bhowmik et al., 19 Sep 2025). In this sense, skew eigenvectors are extremizers for a Hardy-space variational principle.

Pfister’s multivariate extension is expressed through the maximization formula

S=STS = S^T2

and equivalently

S=STS = S^T3

Here S=STS = S^T4 denotes the trigonometric polynomials with Fourier support in S=STS = S^T5. This places the skew-eigenvector problem in a Hankel/kernel formulation on S=STS = S^T6 (Bhowmik et al., 19 Sep 2025).

2. Rational inner functions generated by skew eigenvectors

Given an extremal eigenpair S=STS = S^T7 for S=STS = S^T8, the decomposition

S=STS = S^T9

holds with remainder S=UDUTS = U D U^T0 orthogonal to S=UDUTS = U D U^T1. If S=UDUTS = U D U^T2, then the Taylor expansions at S=UDUTS = U D U^T3 of S=UDUTS = U D U^T4 and of

S=UDUTS = U D U^T5

match for all monomials up to multidegree S=UDUTS = U D U^T6 (Bhowmik et al., 19 Sep 2025).

This produces a Padé-type approximation scheme. The paper identifies the matching condition as a multivariate S=UDUTS = U D U^T7-type matching of the formal series: the difference

S=UDUTS = U D U^T8

has no terms up to multidegree S=UDUTS = U D U^T9. The normality condition is supplied by choosing UU0 from the extremal variational problem. The boundary behavior is inner because UU1 is of polynomial/reflection form and therefore unimodular almost everywhere on UU2 (Bhowmik et al., 19 Sep 2025).

A related notation is

UU3

so that UU4. In these terms,

UU5

and

UU6

If UU7 and UU8, then UU9 is itself rational inner (Bhowmik et al., 19 Sep 2025).

The construction generalizes the one-variable relation between Takagi extremals and finite Blaschke products. A plausible implication is that the multivariate theory provides a structured inner rational approximation paradigm in which extremality, Taylor matching, and boundary unimodularity are encoded by the same skew-eigenvector data.

3. Montessus-type convergence and moving pole sets

The paper proves a Montessus de Ballore-type convergence theorem on the polydisk for the rational inner functions arising from Takagi–Pfister extremals (Bhowmik et al., 19 Sep 2025). Let DD0 be holomorphic with DD1, and for each multi-index DD2 let DD3 be an optimal solution with DD4 attaining

DD5

Assume that the zero function is not a weak limit point of the sequence DD6 in DD7 as DD8. Then there exist an analytic hypersurface DD9 and a subsequence S u‾=σu,σ≥0.S\,\overline{u} = \sigma u, \qquad \sigma \ge 0.0, with S u‾=σu,σ≥0.S\,\overline{u} = \sigma u, \qquad \sigma \ge 0.1, such that the rational functions

S u‾=σu,σ≥0.S\,\overline{u} = \sigma u, \qquad \sigma \ge 0.2

are unimodular almost everywhere on S u‾=σu,σ≥0.S\,\overline{u} = \sigma u, \qquad \sigma \ge 0.3, their poles accumulate on S u‾=σu,σ≥0.S\,\overline{u} = \sigma u, \qquad \sigma \ge 0.4, and S u‾=σu,σ≥0.S\,\overline{u} = \sigma u, \qquad \sigma \ge 0.5 uniformly on every compact subset S u‾=σu,σ≥0.S\,\overline{u} = \sigma u, \qquad \sigma \ge 0.6 (Bhowmik et al., 19 Sep 2025).

The associated remainder admits the estimate

S u‾=σu,σ≥0.S\,\overline{u} = \sigma u, \qquad \sigma \ge 0.7

On compact subsets of S u‾=σu,σ≥0.S\,\overline{u} = \sigma u, \qquad \sigma \ge 0.8 with S u‾=σu,σ≥0.S\,\overline{u} = \sigma u, \qquad \sigma \ge 0.9 and DdD^d0,

DdD^d1

Because DdD^d2 and DdD^d3, this decays uniformly on compact subsets avoiding zeros of DdD^d4 (Bhowmik et al., 19 Sep 2025).

The poles of the approximants are the zeros of DdD^d5 in DdD^d6. Along the convergent subsequence, these poles accumulate on

DdD^d7

where DdD^d8 is the nonzero weak limit in DdD^d9 of n∈N0dn \in \mathbb{N}_0^d0. Outside n∈N0dn \in \mathbb{N}_0^d1, the rational approximants are holomorphic and converge uniformly to n∈N0dn \in \mathbb{N}_0^d2 (Bhowmik et al., 19 Sep 2025). This identifies the singular geometry of the denominator sequence as the main obstruction to full-domain uniform convergence in several variables.

4. Relation to Schur, Herglotz–Nevanlinna, and Agler classes

The skew-eigenvector framework is embedded in a broader function-theoretic setting. The Schur class on n∈N0dn \in \mathbb{N}_0^d3 is

n∈N0dn \in \mathbb{N}_0^d4

and the Herglotz–Nevanlinna class is

n∈N0dn \in \mathbb{N}_0^d5

For a commuting n∈N0dn \in \mathbb{N}_0^d6-tuple of strict contractions n∈N0dn \in \mathbb{N}_0^d7 on an infinite-dimensional separable Hilbert space n∈N0dn \in \mathbb{N}_0^d8, one defines

n∈N0dn \in \mathbb{N}_0^d9

The Agler–Schur class Cn[z]:={g(z) of multidegree ≤n},\mathbb{C}_n[z] := \{g(z)\text{ of multidegree }\le n\},0 consists of holomorphic Cn[z]:={g(z) of multidegree ≤n},\mathbb{C}_n[z] := \{g(z)\text{ of multidegree }\le n\},1 with Cn[z]:={g(z) of multidegree ≤n},\mathbb{C}_n[z] := \{g(z)\text{ of multidegree }\le n\},2, while the Agler–Herglotz–Nevanlinna class Cn[z]:={g(z) of multidegree ≤n},\mathbb{C}_n[z] := \{g(z)\text{ of multidegree }\le n\},3 consists of holomorphic Cn[z]:={g(z) of multidegree ≤n},\mathbb{C}_n[z] := \{g(z)\text{ of multidegree }\le n\},4 with

Cn[z]:={g(z) of multidegree ≤n},\mathbb{C}_n[z] := \{g(z)\text{ of multidegree }\le n\},5

for all such Cn[z]:={g(z) of multidegree ≤n},\mathbb{C}_n[z] := \{g(z)\text{ of multidegree }\le n\},6. The paper notes that in Cn[z]:={g(z) of multidegree ≤n},\mathbb{C}_n[z] := \{g(z)\text{ of multidegree }\le n\},7 and Cn[z]:={g(z) of multidegree ≤n},\mathbb{C}_n[z] := \{g(z)\text{ of multidegree }\le n\},8 these coincide with the classical Schur and Herglotz classes, while for Cn[z]:={g(z) of multidegree ≤n},\mathbb{C}_n[z] := \{g(z)\text{ of multidegree }\le n\},9 they are strict subclasses (Bhowmik et al., 19 Sep 2025).

For SS00, the Korányi–Pukanszky representation gives a unique positive regular Borel measure SS01 on SS02 satisfying the moment vanishing constraints

SS03

unless either all SS04 or all SS05, such that

SS06

This supplies the kernel representation linking positive-real-part functions to Hardy-space techniques (Bhowmik et al., 19 Sep 2025).

The Cayley transform implements a bijection between Schur and Herglotz classes:

SS07

The same formulas connect the corresponding Agler subclasses (Bhowmik et al., 19 Sep 2025). Within the article’s framework, this transform is the mechanism through which rational inner objects on the Schur side correspond to Cayley rational inner objects on the Herglotz side.

5. Cayley rational inner interpolation and semialgebraic coefficient sets

A constructive theorem in the Agler–Herglotz–Nevanlinna setting states that if truncated Taylor data

SS08

is solvable by some SS09, then there exists a Cayley rational inner solution of multidegree at most

SS10

matching SS11 for all SS12. The solution is rational, has poles off SS13, and satisfies SS14 almost everywhere on SS15 (Bhowmik et al., 19 Sep 2025).

The construction uses Woerdeman’s Agler matrix identity. One finds positive matrices SS16 on SS17 satisfying

SS18

where SS19 encodes the shift in polynomial coordinates, SS20 stacks the data SS21, and SS22 stacks the basepoint. Extending an induced isometry to a unitary

SS23

and setting

SS24

one obtains

SS25

with

SS26

The paper states that this SS27 belongs to SS28, matches the truncated Taylor data, has poles off SS29 since SS30 on SS31, and satisfies

SS32

whose radial limit on SS33 is zero almost everywhere (Bhowmik et al., 19 Sep 2025).

The same Hilbert-space proof yields a structural result for finite Taylor sections. For each SS34,

SS35

The paper proves that SS36 is semialgebraic (Bhowmik et al., 19 Sep 2025). The argument expresses positivity constraints using factorizations SS37 and then applies Tarski–Seidenberg after projection onto coefficient coordinates. The same source states that SS38 is closed, convex, has nonempty interior, and is compact, with boundedness derived from the Korányi–Pukanszky integral representation giving SS39.

In the bidisk with SS40, writing the data as SS41, the paper gives the explicit characterization

SS42

if and only if

SS43

and

SS44

It further notes that these are polynomial inequalities in the real and imaginary parts of SS45 (Bhowmik et al., 19 Sep 2025).

6. Pole distribution, examples, and computational issues

The principal open problem identified in the paper is the zero set problem for extremal skew eigenvectors (Bhowmik et al., 19 Sep 2025). In several variables, an extremal eigenfunction SS46 may have its reflection SS47 vanish inside SS48, so that the rational inner function SS49 develops poles in the domain. This prevents full-domain uniform convergence even when Taylor matching and boundary unimodularity hold. The paper formulates the open question as follows: describe asymptotically, along increasing multidegrees, the pole distribution of the Takagi–Pfister rational inner interpolants SS50, equivalently the zero set of SS51, and identify conditions guaranteeing that poles avoid SS52 (Bhowmik et al., 19 Sep 2025).

A concrete bidisk example illustrates the difficulty. For

SS53

the maximal eigenvalue is

SS54

with eigenfunction

SS55

and reflected polynomial

SS56

The zero set of SS57 intersects SS58, and SS59 and SS60 are relatively prime. The corresponding rational inner approximant

SS61

matches Taylor data up to degree SS62 but has poles in SS63 (Bhowmik et al., 19 Sep 2025).

By contrast, for tensor products SS64, the paper states that products of one-variable Takagi extremals yield poles outside the closed bidisk by the one-variable theorem, giving inner approximants with good pole control (Bhowmik et al., 19 Sep 2025). This suggests that separable structure may ameliorate the denominator-zero problem, although no general theorem of that form is stated beyond the given setting.

The paper also includes a one-variable example. For SS65 and SS66, writing SS67, one computes

SS68

so

SS69

The skew-eigenvector equation

SS70

forces

SS71

The paper states that for SS72 or larger, nontrivial eigenpairs appear and the approximant SS73 matches Taylor coefficients up to degree SS74. In one variable, if SS75 at some SS76, then SS77 is a finite Blaschke product; otherwise SS78 and SS79 uniformly on compact sets (Bhowmik et al., 19 Sep 2025).

The computational procedure described in the paper is finite-dimensional. One inputs SS80 and a multidegree SS81, forms the truncated Toeplitz matrix of SS82 in the monomial basis, defines SS83 by reflection, and constructs the antilinear operator

SS84

One then computes its Takagi singular values and skew eigenvectors by solving

SS85

selects the maximal SS86 and its corresponding SS87, and forms

SS88

Pole verification is reduced to locating the zeros of SS89 in SS90; in the Agler/Herglotz setting, one instead solves the semidefinite feasibility problem for the matrices SS91 and constructs the realization

SS92

(Bhowmik et al., 19 Sep 2025).

7. Conceptual placement within interpolation and Padé theory

The article situates the skew-eigenvector method at the intersection of several classical theories (Bhowmik et al., 19 Sep 2025). First, it is described as a Hilbert-space realization of Carathéodory–Fejér interpolation and Nevanlinna–Pick theory. In one variable, solvability is encoded by contractivity or positivity of Toeplitz and Hankel matrices formed from the data; in several variables, the Agler framework provides positivity certificates and realizations through operator-theoretic decompositions.

Second, the Takagi–Pfister eigenproblem

SS93

is the Hardy-space analogue of the matrix equation

SS94

from Takagi factorization. The conjugation SS95 plays the role of the symmetric reflection, and the extremal eigenpairs maximize the corresponding Hankel form (Bhowmik et al., 19 Sep 2025).

Third, the resulting rational functions are explicitly Padé-type. They match finite Taylor sections while controlling denominator degree and preserving an inner boundary condition. The paper characterizes them as multivariate SS96 inner rational approximants, with a Montessus-type convergence theorem valid away from a moving pole set (Bhowmik et al., 19 Sep 2025).

Finally, the Agler-side realization theory complements the skew-eigenvector construction by giving a separate but connected route to rational interpolation with positivity constraints. The Cayley transform

SS97

converts between Schur and Herglotz–Nevanlinna formulations, while Woerdeman’s positive matrix identity yields realizable finite sections and semialgebraic coefficient bodies. Taken together, these ingredients form what the source presents as a cohesive framework for rational approximation on polydisks, centered on Takagi–Pfister extremals and their denominator geometry (Bhowmik et al., 19 Sep 2025).

Definition Search Book Streamline Icon: https://streamlinehq.com
References (1)

Topic to Video (Beta)

No one has generated a video about this topic yet.

Whiteboard

No one has generated a whiteboard explanation for this topic yet.

Follow Topic

Get notified by email when new papers are published related to Takagi-Pfister Skew Eigenvectors.