Startseite Mathematik Introduction to the dynamical properties of Toeplitz operators on the Hardy space of the unit disc
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Introduction to the dynamical properties of Toeplitz operators on the Hardy space of the unit disc

  • Emmanuel Fricain EMAIL logo und Maëva Ostermann
Veröffentlicht/Copyright: 30. Januar 2026

Abstract

These notes are based on a mini-course given at the ACOTCA conference 2025. The goal is to present full proofs of the first two key results regarding hypercyclic Toeplitz operators, in a way that is accessible to beginners.

MSC 2020: 47B35; 47A16; 30H10; 30H15

1 Introduction

These notes are based on a short mini-course, consisting of three 50-min lectures, which the fist author delivered at the ACOTCA (XIX Advanced Course in Operator Theory and Complex Analysis) held in June 2025 in Clermont-Ferrand, France. The topic concerns the hypercyclicity of Toeplitz operators on the Hardy space H 2 of the open unit disc D .

These notes are intended neither as a comprehensive survey of the literature on this subject nor as a presentation of new results. Rather, their purpose is to provide an introductory account accessible to readers approaching the topic for the first time. To this end, the exposition is aimed at readers (participants) with a background corresponding to a standard master’s level course in functional analysis and complex analysis and includes complete proofs of most of the results discussed.

The central question addressed in these notes is the following: given a function ϕ L ( T ) , where T = D denotes the unit circle equipped with the normalized Lebesgue measure m, can one determine some necessary and/or sufficient conditions on ϕ to ensure that the associated Toeplitz operator T ϕ is hypercyclic on H 2?

The structure of this mini-course is as follows. Lecture 1 (Section 2) provides a brief introduction to the notion of hypercyclicity, restricted to the tools required for our purposes. In particular, we establish the classical Godefroy–Shapiro criterion and recall some basic and well-known obstructions to hypercyclicity. Lecture 2 (Section 3) contains a concise introduction to Hardy spaces and Toeplitz operators. Lecture 3 (Section 4) is devoted to the main question under consideration. Our discussion will focus on two fundamental results: the first one, due to Godefroy and Shapiro, characterizes hypercyclic Toeplitz operators with anti-analytic symbols; the second one, due to Shkarin, concerns tridiagonal Toeplitz operators. As will become apparent, even in this last restricted setting, the problem remains far from straightforward. The paper concludes with a brief mention of three more recent contributions to the study of hypercyclicity for Toeplitz operators.

To close this introduction, let us emphasize that the question of hypercyclicity for Toeplitz operators remains far from being completely resolved, and significant challenges persist. In particular, in [1], you could find some more specific open problems. We hope that these notes will motivate interested readers to pursue further investigation into this topic.

2 Hypercyclic operators

2.1 Definition of hypercyclicity

We usually imagine chaos as something that arises in nonlinear systems, while linear systems are thought to be predictable and “well-behaved”. But this intuition is not always correct. In fact, some natural linear operators can behave in a surprisingly chaotic way. One of their key features is the existence of a dense orbit: starting from a single point and repeatedly applying the operator, the trajectory can come arbitrarily close to every point in the space.

Definition 2.1.

More formally, let X be a Fréchet space, that is a complete topological vector space whose topology is generated by a countable family of seminorms, and let T: XX be a continuous and linear operator on X (in short T L ( X ) ) . The operator T is called hypercyclic on X if there exists a xX such that its orbit under T,

o r b ( T , x ) = { T n x ; n 0 } ,

is dense in X. In such a case, x is called a hypercyclic vector for T and the set of all hypercyclic vectors for T is denoted by HC(T).

Example 2.2.

The first known example of a hypercyclic operator was constructed by Birkhoff in 1929 [2], illustrating that such “chaotic” behavior can indeed occur even for linear operators. Let H o l ( C ) be the Fréchet space of entire functions, let a be any non zero complex number and let T a : H o l ( C ) H o l ( C ) be the associated translation operator defined by

( T a f ) ( z ) = f ( a + z ) , z C , f H o l ( C ) .

Then T a is hypercyclic on H o l ( C ) .

Example 2.3.

Another early example of a hypercyclic operator, still on the Fréchet space H o l ( C ) , was given by MacLane in 1952 [3]. Let D : H o l ( C ) H o l ( C ) be the differentiation operator defined by Df = f′. Then D is hypercyclic on H o l ( C ) as well.

Example 2.4.

On Banach spaces, the first known example is provided by Rolewicz in 1969 [4]. Let X = p ( N ) , 1 ≤ p < + ∞, or X = c 0 ( N ) . Let T be the backward shift operator on X defined by

T : X X ( x 0 , x 1 , ) ( x 1 , x 2 , )

Then λT is hypercyclic on X if and only if |λ| > 1.

Inspired by these early examples, researchers in the 1980s started studying the dynamical behavior of general linear operators, paying special attention to the phenomenon of hypercyclicity. This marked the beginning of a systematic exploration of “chaotic” behavior in linear settings. Some classical references for this area of research include:

  1. Erdmann – Peris, “Linear Chaos”, 2011 [5];

  2. Bayart – Matheron, “Dynamics of linear operators”, 2009 [6].

In particular, these references contain all the results discussed in this section, and we draw on them as a source of inspiration for this brief introduction to hypercyclicity.

2.2 Birkhoff’s transitivity theorem and Godefroy Shapiro criterion

The most useful characterization of hypercyclicity is an application of the Baire category theorem and is due to Birkhoff through the notion of topological transitivity. We first recall this notion.

Definition 2.5.

Let X be a Fréchet space and T L ( X ) . The operator T is called topologically transitive if for each pair of non-empty open sets (U, V) of X, there exists n N such that T n (U) ∩ V ≠ ∅.

Theorem 2.6

(Birkhoff’s transitivity theorem, 1922 [7]). Let X be a separable Fréchet space and T L ( X ) . The following assertions are equivalent.

  1. T is hypercyclic;

  2. T is topologically transitive.

See Figure 1 for an illustration of the notion of topological transitivity.

Figure 1: 
Topological transitivity.
Figure 1:

Topological transitivity.

Proof.

(i) ⇒ (ii): Assume that T is hypercyclic and let x be a hypercyclic vector for T. Consider U and V be two non-empty open sets of X. Since orb(T, x) is dense in X, there is some k ≥ 0 such that T k xU. But the space X has no isolated points, and then the set {T m x; mk} is also dense in X. Hence there exists mk such that T m xV. Observe now that

T m x = T m k ( T k x ) T m k ( U ) V ,

meaning that T n (U) ∩ V ≠ ∅ with n = mk. Thus T is topologically transitive.

(ii) ⇒ (i): Assume now on the contrary that T is topologically transitive and let us prove that T is hypercyclic. Since X has a countable dense set {y j ; j ≥ 1} (remember that X is separable), then the open balls of radius 1/m around the y j , j, m ≥ 1, form a countable base ( V k ) k 1 of the topology of X. Hence, xHC(T) if and only if for every k ≥ 1, there is some n ≥ 0 such that T n xV k . In other words

H C ( T ) = k 1 n 0 T n ( V k ) .

By continuity of T, the sets

W k = n 0 T n ( V k )

are open sets for every k ≥ 1. Let’s prove that W k is dense for every k ≥ 1.

Let U be an open set of X. Since T is topologically transitive, there exists n ≥ 0 such that

T n ( U ) V k U T n ( V k ) .

Therefore W k is dense in X. By Baire category theorem, the set H C ( T ) = k 1 W k is dense in X and in particular, HC(T) ≠ ∅.□

Remark 2.7.

Let T L ( X ) and assume that T is invertible. Then T is hypercyclic if and only if T −1 is hypercyclic. Indeed it is sufficient to observe that

T n ( U ) V U T n ( V )

and to apply Birkhoff theorem.

As was observed by Godefroy and Shapiro, it turns out that if an operator has sufficiently many eigenvectors, then it is hypercyclic.

Theorem 2.8

(Godefroy – Shapiro citerion, 1991 [8]). Let X be a separable Fréchet space and T L ( X ) . Suppose that

H ( T ) = s p a n ker ( T λ ) ; | λ | < 1 and H + ( T ) = s p a n ker ( T λ ) ; | λ | > 1

are dense in X. Then T is hypercyclic on X.

Proof.

We shall prove that T is topologically transitive. Let U and V be two non-empty open subsets of X. By assumption, UH (T) ≠ ∅ and VH +(T) ≠ ∅. In other words, we can find

x = k = 1 m a k x k U and y = k = 1 m b k y k V

with Tx k = λ k x k with |λ k | < 1, Ty k = μ k y k with |μ k | > 1 and a k , b k C , 1 k m . Observe that

T n x = k = 1 m a k λ k n x k n 0

and

u n = k = 1 m b k 1 μ k n y k n 0 with T n u n = y , n 0 .

Taking into account the fact that U and V are open subsets, it follows that there is some N N so that, for all nN,

x + u n U and y + T n x V .

In other words, VT n (U) ≠ ∅ meaning that T is topologically transitive. According to Birkhoff’s theorem, we then deduce that T is hypercyclic.□

2.3 Some restrictions to hypercyclicity

We assume now that X is a complex separable Banach space.

Proposition 2.9.

Let T L ( X ) . If T is hypercyclic on X, then σ p (T*) = ∅.

Proof.

Let xHC(T) and argue by contradiction assuming that T*(x*) = μx* for some μ C and x* ∈ X*, x* ≠ 0. Then, we have, for every n N

x * , T n x = T * n x * , x = μ n x * , x .

Observe that the set { x * , T n x ; n 0 } is dense in C whereas clearly the set { μ n x * , x ; n 0 } is not dense. This yields the desired contradiction.□

Proposition 2.10.

Let T L ( X ) .

  1. If ‖T‖ ≤ 1 then T is not hypercyclic on X.

  2. If for every xX, ‖Tx‖ ≥ ‖x‖, then T is not hypercyclic on X.

Proof.

(a) If ‖T‖ ≤ 1, then for every xX and every n ≥ 1, we have ‖T n x‖ ≤ ‖x‖. Hence the orbit orb(T, x) is bounded, and then cannot be dense in X. Since this is true for every xX, then T is not hypercyclic.

(b) If for every xX, ‖Tx‖ ≥ ‖x‖, then for every xX and every n ≥ 0, we have ‖T n x‖ ≥ ‖x‖. Hence the orbit orb(T, x) stays away from 0 (if x ≠ 0) and then cannot be dense in X. One more time, T cannot be hypercyclic on X.□

In the context of Hilbert spaces, we will show that a hyponormal operator cannot be hypercyclic.

Definition 2.11.

Let H be a Hilbert space and T L ( H ) . We say that T is hyponormal if T*TTT* ≥ 0, that is

(1) x H , T x T * x .

Fact 2.12.

If T is hyponormal, then we have

x H , T x 2 T 2 x x .

Proof.

Write:

T x 2 = T x , T x = T * T x , x T * ( T x ) x by Cauchy Schwartz inequality T 2 x x by  ( 1 )  applied to T x .

Theorem 2.13.

Let T L ( H ) be hyponormal. Then T is not hypercyclic on H.

Proof.

Let xH, x ≠ 0.

Assume first that the sequence ( T n x ) n 0 is decreasing. Thus ‖T n x‖ ≤ ‖x‖ for all n ≥ 0 and x cannot be a hypercyclic vector.

Now, it remains to prove that when the sequence ( T n x ) n 0 is not decreasing, then the vector x cannot be hypercyclic as well.

By assumption, there exists N N such that ‖T N+1 x‖ > ‖T N x‖. In particular, it implies that T N+1 x ≠ 0 and then T N x ≠ 0. By Fact 2.12 applied to T N x, we obtain ‖T N+1 x2 ≤ ‖T N+2 x‖‖T N x‖, whence

T N + 2 x T N + 1 x 2 T N x = T N + 1 x T N + 1 x T N x > 1 > T N + 1 x .

An induction shows that ( T n x ) n N is strictly increasing and in particular ‖T n x‖ > ‖T N x‖, ∀nN + 1. Hence x cannot be a hypercyclic vector.□

We finish this first lecture (section) by giving some spectral restrictions.

Theorem 2.14.

Let X be a complex separable Banach space and T L ( X ) . Assume that T is hypercyclic. Then σ ( T ) T .

Proof.

We argue by contradiction and suppose that σ ( T ) T = .

If σ ( T ) D then by the spectral radius formula r(T) < 1 and there exists ɛ > 0 and M > 0 such that

T n M ( 1 ε ) n n 0 ,

which contradicts the fact that T is hypercyclic.

If σ ( T ) C \ D ̄ , then T is invertible and T −1 is also hypercyclic. But since σ ( T 1 ) = σ ( T ) 1 D , we also get a contradiction.

Therefore σ 1 = σ ( T ) D and σ 2 = σ ( T ) C \ D ̄ form a partition of σ(T) into two non empty closed sets. By the Riesz decomposition theorem, there exists two non-trivial closed invariant subspaces M 1 and M 2 such that

X = M 1 M 2 and σ ( T | M j ) = σ j , 1 j 2 .

But it is not difficult to see that T | M 1 should be hypercyclic, which is again a contradiction because σ ( T | M 1 ) = σ 1 D .□

Kitai proved indeed a better result.

Theorem 2.15

(Kitai, 1982 [9]). Let X be a complex separable Banach space and T L ( X ) . Assume that T is hypercyclic. Then every connected component of σ(T) intersects T .

3 Toeplitz operators and Hardy spaces

3.1 Toeplitz matrices

Recall that a Toeplitz matrix on 2 ( N ) is a matrix of the form

T ( a ) = a 0 a 1 a 2 a 3 a 1 a 0 a 1 a 2 a 2 a 1 a 0 a 1 a 3 a 2 a 1 a 0

where a = ( a n ) n Z is a doubly infinite sequence of complex numbers. In other words A = ( a j , k ) j , k 0 is a Toeplitz matrix T(a) if a j,k = a jk , for every j, k ≥ 0. To study boundedness of a Toeplitz matrix on 2 ( N ) , it will be useful to adopt another point of view.

Let L 2 ( T ) be the Hilbert space of Lebesgue measurable function on the unit circle T equipped with the inner product

f , g 2 = 0 2 π f ( e i θ ) g ( e i θ ) ̄ d θ 2 π .

Let H 2 = f L 2 ( T ) ; f ̂ ( n ) = 0 , n < 0 be the Hardy space. It turns out that H 2 is a closed subspace of L 2 ( T ) and we denote by P + : L 2 ( T ) H 2 the orthogonal projection of L 2 ( T ) onto H 2, defined by

P + n Z c n e i n θ = n 0 c n e i n θ .

Note that

(2) ker ( P + ) = H 0 2 ̄ ,

where H 0 2 = e i θ H 2 . Moreover, the operator

U : 2 ( N ) H 2 ( a n ) n 0 n 0 a n e i n θ

is a unitary operator.

Hartman and Wintner in 1954 got a characterization of the Toeplitz matrices that give rise to bounded operators on 2 ( N ) .

Theorem 3.1

(Hartman – Wintner, 1954 [10]). The following assertions are equivalent:

  1. The operator T(a) is bounded on 2 ( N ) ;

  2. There exists a function ϕ L ( T ) such that a n = ϕ ̂ ( n ) , n Z .

Moreover, UT(a)U −1 = T ϕ , where T ϕ f = P +(ϕf) fH 2.

Proof of (ii) ⟹ (i).

First note that if ϕ L ( T ) , then, for every fH 2, we have

T ϕ f 2 = P + ( ϕ f ) 2 ϕ f 2 ϕ f 2 .

Hence T ϕ is bounded on H 2 and ‖T ϕ ‖ ≤ ‖ϕ.

Moreover, let ( e n ) n 0 be the canonical basis of 2 ( N ) . Then, for every n, k ≥ 0, on one hand, we have T ( a ) e n , e k = a k n , and on the other hand, we have

U 1 T ϕ U e n , e k = T ϕ U e n , e k = T ϕ z n , z k = P + ( ϕ z n ) , z k = ϕ z n , z k because  z k H 2 = ϕ , z k n = ϕ ̂ ( k n ) = a k n .

Hence, for every n, k ≥ 0, we have T ( a ) e n , e k = U 1 T ϕ U e n , e k , which proves that T(a) = U −1 T ϕ U is bounded on 2 ( N ) .

For the proof of (i) ⟹ (ii), we refer to the following book: “An introduction to operators on the Hardy-Hilbert space” by Rubén A. Martinez-Avendaño and Peter Rosenthal, 2007 [11].□

We will now discuss basic properties of Toeplitz operators T ϕ on H 2 when the symbol ϕ L ( T ) . Before, we recall some basic facts on H 2.

3.2 The Hardy space H 2

The space H 2 can be identified with the space H 2 ( D ) which consists of analytic functions f on the open unit disc D ,

f ( z ) = n = 0 + a n z n , z D ,

where Taylor coefficients ( a n ) n 0 2 ( N ) . The space H 2 ( D ) is equipped with the following scalar product

(3) f , g 2 = n = 0 + a n b n ̄ ,

where f ( z ) = n = 0 a n z n and g ( z ) = n = 0 b n z n . Then the operator

U : H 2 ( D ) H 2 f ( z ) = n = 0 a n z n f * ( e i θ ) = n = 0 a n e i n θ

is a unitary operator and f * ̂ ( n ) = a n , n 0 .

Using Parseval equality, it is not difficult to see that if f r (eiθ ) = f(reiθ ), 0 ≤ r < 1, θ R , then

lim r 1 f r f * L 2 ( T ) = 0 .

In particular, there exists a sequence ( r n ) n ( 0,1 ) such that r n ⟶ 1 as n ⟶ ∞ and

lim n f ( r n e i θ ) = f * ( e i θ ) , a.e.  e i θ T .

In fact, a deep result of Fatou says much more: if f H 2 ( D ) , then

n t lim z e i θ f ( z ) = f * ( e i θ ) a.e.  e i θ T ,

where nt − lim denotes the non-tangential limit, that is the limit restricted to every Stolz region Δ α (see Figure 2).

Figure 2: 
A Stolz region.
Figure 2:

A Stolz region.

In the sequel, we will identify, as usual, H 2 and H 2 ( D ) and omit the star in f* when we talk about the non-tangential limit of a function in H 2 ( D ) . The space H 2 is a RKHS (reproducing kernel Hilbert space) where the kernels are given by

k λ ( z ) = 1 1 λ ̄ z , λ , z D .

Indeed, we have k λ ( z ) = n 0 λ ̄ n z n , and ( λ ̄ n ) n 0 2 ( N ) . Hence the function k λ belongs to H 2. Moreover, for every f H 2 , f ( z ) = n 0 a n z n , and for every λ D , taking account of [6], we have

f , k λ = n = 0 a n λ n = f ( λ ) .

3.3 Toeplitz operators on H 2

If we come back to Toeplitz operators on H 2, we have the following result on the norm.

Theorem 3.2

(Brown – Halmos, 1963 [12]). Let ϕ L ( T ) . Then T ϕ L ( H 2 ) and ‖T ϕ ‖ = ‖ϕ.

Proof.

We have already seen that T ϕ is bounded and ‖T ϕ ‖ ≤ ‖ϕ.

For the converse inequality, denote by k λ ̃ = k λ / k λ 2 the normalized reproducing kernel. We have

T ϕ k λ ̃ , k λ ̃ 2 T ϕ k λ ̃ 2 k λ ̃ 2 T ϕ .

Moreover, using that k λ 2 2 = k λ , k λ 2 = k λ ( λ ) = 1 1 | λ | 2 , we have

T ϕ k λ ̃ , k λ ̃ 2 = P + ( ϕ k λ ̃ ) , k λ ̃ 2 = ϕ k λ ̃ , k λ ̃ because  k λ ̃ H 2 = T ϕ ( e i θ ) | k λ ( e i θ ) | 2 k λ 2 2 d m ( e i θ ) = T ϕ ( e i θ ) 1 | λ | 2 | e i θ λ | 2 Poisson kernel d m ( e i θ ) = P ( ϕ ) ( λ ) ,

where P ( ϕ ) is the Poisson transform of ϕ. Hence we get that for every λ D , we have

(4) | P ( ϕ ) ( λ ) | T ϕ .

We will now use a well-known property of the Poisson integral (see [11], Corollary 1.1.27]) saying that

lim r 1 P ( ϕ ) ( r e i θ ) = ϕ ( e i θ ) a.e.  e i θ T

Hence, according to [7], it follows that for almost all e i θ T , we have

| ϕ ( e i θ ) | T ϕ .

Hence ‖ϕ ≤ ‖T ϕ ‖, which concludes the proof.□

Some observations.

Let ϕL . It is easy to see that

  1. T ϕ * = T ϕ ̄ . In particular, if S = T z is the shift operator on H 2, then S * = T z ̄ is the backward shift operator on H 2. For every fH 2, we have

S f ( z ) = z f ( z ) and S * f ( z ) = f ( z ) f ( 0 ) z .

  1. If ϕH , the algebra of bounded and analytic functions on D , then, for every λ D , we have

(5) T ϕ ̄ k λ = ϕ ( λ ) ̄ k λ .

Indeed, let fH 2, then

f , T ϕ ̄ k λ 2 = f , T ϕ * k λ 2 = T ϕ f , k λ 2 = P + ( ϕ f ) , f λ 2 = ϕ f , k λ 2 .

Now observe that since ϕH , then ϕfH 2 and we deduce that

f , T ϕ ̄ k λ 2 = ( ϕ f ) ( λ ) = ϕ ( λ ) f ( λ ) = f , ϕ ( λ ) ̄ k λ 2 .

Therefore, T ϕ ̄ k λ = ϕ ( λ ) ̄ k λ .

  1. In general, T ϕ T ψ T ϕψ but Brown and Halmos proved the following.□

Theorem 3.3

(Brown – Halmos, 1963 [12]). Let ϕ , ψ L ( T ) Then

T ϕ T ψ = T ϕ ψ either  ϕ ̄  or  ψ  is in  H .

We will do not really use this result so we will admit it. However, note that, in general, we have T ϕ n T ϕ n and there is no tractable formula for T ϕ n , which makes the question of hypercyclicity for general Toeplitz operators very difficult.

As we have seen in the first part, the question of eigenvectors is crucial in the study of hypercyclicity. We will now give two results in this direction.

Theorem 3.4

(Coburn, 1966 [13]). Let ϕ L ( T ) , ϕ 0 . Then either kerT ϕ = {0} or ker T ϕ * = { 0 } .

Proof.

Argue by contradiction and assume that there are two functions h 1 and h 2 in H , h 1, h 2 ≠ 0 such that T ϕ h 1 = 0 and T ϕ ̄ h 2 = 0 . Taking into account of [15], it means that ϕ h 1 H 0 2 ̄ and ϕ ̄ h 2 H 0 2 ̄ . It is an easy exercise to prove that if f H 0 2 and gH 2, then f g L 1 ( T ) and f g ̂ ( n ) = 0 , ∀n ≤ 0.

Let now define ψ = h 1 ϕ h 2 ̄ . Since ϕ h 2 ̄ H 0 2 and h 1H 2, then ψ L 1 ( T ) and ψ ̂ ( n ) = 0 , ∀n ≤ 0. Moreover ψ ̄ = h 1 ϕ ̄ h 2 , with h 1 ϕ ̄ H 0 2 and h 2H 2. Hence ψ ̄ ̂ ( n ) = 0 , ∀n ≤ 0, which give that ψ ̂ ( n ) = 0 , ∀n ≥ 0. Therefore ψ ̂ ( n ) = 0 , n Z and thus ψ ≡ 0. But a standard property of Hardy spaces (see [11], Corollary 2.7.2]) shows that, since h 1, h 2 ≠ 0, then h 1 and h 2 are non-zero almost everywhere. Hence ϕ ≡ 0 a.e. which is a contradiction.□

When the symbol ϕ is continuous, we can link the spectral properties of T ϕ with the winding number of ϕ. Recall that if ϕ C ( T ) and λ ϕ ( T ) , then its winding number is defined as

w i n d ϕ ( λ ) = 1 2 i π ϕ ( T ) 1 u λ d u = 1 2 i π T ϕ ( ζ ) ϕ ( ζ ) z d ζ if  ϕ C 1 ( T ) .

Furthermore, recall that an operator T L ( H ) is said to be Fredholm is:

  1. Im(T) is closed;

  2. ker(T) and ker(T*) are both finite dimensional.

In this case, the index of T is defined as

j ( T ) = dim ( ker T ) dim ( ker T * ) .

When ϕ is continuous, we have the following description of the spectrum.

Theorem 3.5.

Let ϕ C ( T ) .

  1. T ϕ is a Fredholm operator on H 2 if and only if ϕ does not vanish on T . In this case,

j ( T ϕ ) = w i n d ϕ ( 0 ) .

  1. We have

σ ( T ϕ ) = ϕ ( T ) { λ C \ ϕ ( T ) ; w i n d ϕ ( λ ) 0 } .

This beautiful theorem is the combined work of several mathematicians: Krein, Calderón, Spitzer, Widom, Devinatz. Since we will not really use this result in the sequel, we will admit it. However, we refer to the book of Martinez-Avendaño – Rosenthal [11] for its proof and more details.

Figure 3: 
The spectrum of a Toeplitz operator.
Figure 3:

The spectrum of a Toeplitz operator.

Observe that if λ C \ ϕ ( T ) with wind ϕ (λ) < 0, then

w i n d ϕ ( λ ) = j ( T ϕ λ ) = dim ker ( T ϕ λ ) dim ker T ϕ * λ ̄

so, we necessary have dimker(T ϕ λ) > 0. Hence

{ λ C \ ϕ ( T ) ; w i n d ϕ ( λ ) < 0 } σ p ( T ϕ ) ,

and

(6) { λ C \ ϕ ( T ) ; w i n d ϕ ( λ ) > 0 } σ p T ϕ * .

Example 3.6.

  1. If S denotes the shift operator on H 2, it can be easily proved that σ ( S * ) = D ̄ and σ p ( S * ) = D .

  2. Let ϕ be a continuous symbol such that ϕ ( T ) is represented as in Figure 3. In this example, the spectrum is the union of the curve and the two components of index $-1$ and $-2$.

4 Hypercyclicity of Toeplitz operators

Recall that we are interested in the following question: given a function ϕ L ( T ) , where T = D denotes the unit circle equipped with the normalized Lebesgue measure m, can one determine some necessary and/or sufficient conditions on ϕ to ensure that the associated Toeplitz operator T ϕ is hypercyclic on H 2? As already said in the introduction, we will focus on two key results where we have a complete characterization. The first one concerns the case where the symbol ϕ is anti-analytic (meaning that ϕ H ̄ ). The second one concerns the case where the symbol ϕ is of the form ϕ(z) = a/z + b + cz, z T (which corresponds to tridiagonal Toeplitz matrices).

4.1 Analytic and anti-analytic symbols

We start with a simple observation. If ϕH , then T ϕ is not hypercyclic on H 2. Indeed, since ϕH , then for every λ D , we have

T ϕ * k λ = T ϕ ̄ k λ = ϕ ( λ ) ̄ k λ ,

(see [2]) and in particular σ p T ϕ * . Thus T ϕ cannot be hypercyclic by Proposition 2.9.

The case of anti-analytic symbol was studied by Godefroy and Shapiro.

Theorem 4.1

(Godefroy – Shapiro, 1991 [8]). Let ϕH . The following assumptions are equivalent.

  1. T ϕ ̄ is hypercyclic on H 2;

  2. ϕ is non-constant and ϕ ( D ) T .

Proof.

(ii) ⟹ (i). Since ϕ is non constant, by the open mapping theorem, ϕ ( D ) is an open connected set which intersects T (see Figure 4).

Let U = { z D ; | ϕ ( z ) | < 1 } and V = { z D ; | ϕ ( z ) | > 1 } . Then U and V are two open sets which are both non empty. On the other hand, it follows from [2] that

s p a n { k z ; z U } H ( T ϕ ̄ ) and s p a n { k z ; z V } H + ( T ϕ ̄ ) ,

where we recall that

H ( T ) = s p a n ker ( T λ ) ; | λ | < 1 and H + ( T ) = s p a n ker ( T λ ) ; | λ | > 1

According to Godefroy – Shapiro Criterion, it is sufficient to prove that if Ω is a non empty open subset of D , then span{k z ; z ∈ Ω} is dense in H 2. Thus let fH 2 such that f ⊥ k z , ∀ z ∈ Ω. Hence

f ( z ) = f , k z = 0 , for every  z Ω .

But since Ω is a non-empty open subset of D , the uniqueness principle for analytic functions implies that f ≡ 0. Hence H ( T ϕ ̄ ) and H + ( T ϕ ̄ ) are both dense in H 2, which implies that T ϕ ̄ is hypercyclic on H 2.

(i) ⟹ (ii). Assume now that T ϕ ̄ is hypercyclic on H 2. Then, of course, ϕ is non-constant and T ϕ ̄ is not a contraction. In particular, ϕ = T ϕ = T ϕ ̄ > 1 . Moreover, we also have inf z D | ϕ ( z ) | < 1 . Indeed, if inf z D | ϕ ( z ) | 1 , then 1/ϕH and T 1 / ϕ * is not hypercyclic because T 1 / ϕ * = T 1 / ϕ = 1 / ϕ 1 . But since T 1/ϕ T ϕ = T ϕ T 1/ϕ = I, the operator T ϕ is invertible and T ϕ 1 = T 1 / ϕ . Thus T ϕ * 1 = T 1 / ϕ * . Now, since T 1 / ϕ * is not hypercyclic, it follows from Remark 2.7 that T ϕ * = T ϕ ̄ is not hypercyclic as well, which is absurd. Hence we have

inf z D | ϕ ( z ) | < 1 < sup z D | ϕ ( z ) | .

Now, a simple connectedness argument implies that ϕ ( D ) T .□

Figure 4: 
Hypercyclic operator.
Figure 4:

Hypercyclic operator.

We immediately recover the result of Rolewicz.

Corollary 4.2

(Rolewicz, 1969 [4]). Let λ C .Then

λ S * = T λ z ̄  is hypercyclic on  H 2 | λ | > 1 .

4.2 Tridiagonal Toeplitz operators

In [14], Shkarin characterized hypercyclic Toeplitz operators T F with symbols of the form

F ( e i θ ) = a e i θ + b + c e i θ , a , b , c C , c 0 .

They correspond to the following Toeplitz matrices which are tridiagonal.

b a c b a ( 0 ) c b a ( 0 )

Observe that T F = aS* + bI + cS and then T F * = a ̄ S + b ̄ I + c ̄ S * . Using that S*S = I, we get

T F * T F T F T F * = ( a ̄ S + b ̄ I + c ̄ S * ) ( a S * + b I + c S ) ( a S * + b I + c S ) ( a ̄ S + b ̄ I + c ̄ S * ) = ( | a | 2 | c | 2 ) S S * + | c | 2 | a | 2 = ( | c | 2 | a | 2 ) ( I S S * ) .

Since S* is a contraction, we have ISS* ≥ 0. Thus if |c| ≥ |a|, we get T F * T F T F T F * 0 meaning that T F is hyponormal. In particular, if |c| ≥ |a| then T F cannot be hypercyclic (see Theorem 2.13). It is also possible to check that if |c| > |a|, then there exists λ C \ F ( T ) , such that wind F (λ) > 0 (see [1], Fact 5.3]). Then, according to [12], we get σ p T F * , which implies, by Proposition 2.9, that T F cannot be hypercyclic on H 2. Note that this last argument extends to the Banach setting H p but not to the case |a| = |c|.

Thus we may assume that |c| < |a|. We need now two lemmas.

Lemma 4.3.

Let F ( z ) = a z + b + c z , | a | > | c | > 0 . Then

  1. F ( T ) is an ellipse;

  2. The interior E of the ellipse satisfies

E = F z C ; 1 < | z | < a c .

See Figure 5.

Figure 5: 
Shkarin Toeplitz operators.
Figure 5:

Shkarin Toeplitz operators.

Proof.

Let a = |a|eiα , c = |c|eiγ and consider F ̃ ( z ) = | a | z + | c | z . Then

F ( z ) = b + | a | z e i α + | c | e i γ z = b + e i α + γ 2 | a | z e i α γ 2 + | c | e i γ α 2 z = b + e i α + γ 2 F ̃ e i γ α 2 z .

This formula shows that we can assume, without loss of generality, that b = 0 and a and c are real with a > c > 0.

(a) F(eiθ ) = ae−iθ + ceiθ = (a + c)cosθ + i(ca)sinθ. Hence

F ( T ) = x + i y C ; x 2 ( a + c ) 2 + y 2 ( a c ) 2 = 1

and thus F ( T ) is an ellipse centered at 0 whose foci are ( ± 2 a c , 0 ) and the length of the axis are 2(a + c) and 2(ac).

(b) We have

E = x + i y C ; x 2 ( a + c ) 2 + y 2 ( a c ) 2 < 1 .

Let us first check that F z C ; 1 < | z | < a c E . Let z = reiθ , 1 < r < a/c. Thus

(7) F ( r e i θ ) = a r e i θ + c r e i θ = a r + c r cos θ + i c r a r sin θ .

If we denote by ϕ ( r ) = a r + c r , then it is easy to see that

Hence for all 1 < r < a c , we have 0 < a r + c r < a + c . Similarly, if we denote by ψ ( r ) = c r a r , then

Hence for all 1 < r < a c , we have c r a r < a c . Thus

a r + c r 2 cos 2 θ ( a + c ) 2 + c r a r 2 sin 2 θ ( a c ) 2 < cos 2 θ + sin 2 θ = 1 ,

which means that F ( r i θ ) E .

Let us now check that E F z C ; 1 < | z | < a c . Let x + i y E then x 2 ( a + c ) 2 + y 2 ( a c ) 2 < 1 . According to [13], we need to prove that there exists r 0 with 1 < r 0 < a/c and θ R such that

x = a r 0 + c r 0 cos θ ; y = c r 0 a r 0 sin θ .

Let ϕ 1 ( r ) = x 2 a r + c r 2 + y 2 c r a r 2 for r a c . The function ϕ 1 is continuous and differentiable on 1 , a c \ a c and we have

ϕ 1 ( r ) = 2 x 2 c a r 2 a r + c r 3 2 y 2 c + a r 2 c r a r 3 = 2 x 2 c a r 2 c r a r 3 2 y 2 c + a r 2 a r + c r 3 a r + c r 3 c r a r 3 = 2 x 2 r 3 c a r 2 4 + 2 y 2 c + a r 2 a r + c r 3 a r + c r 3 c r a r 3 .

Observe that ϕ 1 ( r ) 0 c r a r 0 r < a c . It follows that we have the monotonicity table

Moreover ϕ 1 ( 1 ) = x 2 ( a + c ) 2 + y 2 ( a c ) 2 < 1 . So, by the mean value principle, there exists a r 0 1 , a c such that ϕ(r 0) = 1, which means that

x 2 a r 0 + c r 0 2 + y 2 c r 0 a r 0 2 = 1 .

Now, we can find θ R such that

x = a r 0 + c r 0 cos θ and y = c r 0 a r 0 sin θ .

Hence x + i y = F r 0 e i θ and 1 < r 0 < |a/c|. Finally, we get

E = F z C ; 1 < | z | < a c .

Lemma 4.4.

Let d C , | d | < 1 and let

A W = { z D ; | d | < | z | < 1 } .

Assume that A has an accumulation point in W (see Figure 6). Let q : D C be an analytic function such that q ( z ) = q d z for all zA. Then q is constant.

Figure 6: 
The annulus W.
Figure 6:

The annulus W.

Proof.

Observe that zq(z) and z q d z are analytic on W and coincide on A. By the uniqueness principle for analytic functions (since A has an accumulation point in W), we get that for every zW, q ( z ) = q d z . Define now

q ̃ ( z ) = q ( z ) , z D ; q d z , | z | > d .

Then q ̃ is a well defined analytic function on C . Moreover, we have

lim | z | q ̃ ( z ) = lim | z | q d z = q ( 0 ) .

Hence q ̃ is bounded and, by Liouville’s theorem, we get that q ̃ is constant. Thus q is constant as well.□

We can now give the Shkarin’s characterization for hypercyclicity of tridiagonal Toeplitz operators.

Theorem 4.5

(Shkarin, 2012 [14]). Let F(eiθ ) = ae−iθ + b + ceiθ , where a , b , c C , c ≠ 0. Then the following assertions are equivalent.

  1. T F is hypercyclic on H 2;

  2. the following two conditions are satisfied:

    1. |a| > |c|;

    2. E T , where E is the interior of the elliptic curve F ( T ) .

Proof.

(1) ⟹ (2): let us first assume that T F is hypercyclic on H 2. We have already seen that (i) is necessary (because if |a| ≤ |c|, then T F is hyponormal and hence not hypercyclic). Let us now check (ii). Argue by contradiction and assume that E T = (see Figure 7).

We have E C \ D ̄ . Indeed if not, then E D , which implies that ‖T F ‖=‖F ≤ 1. In particular, T F cannot be hypercyclic.

Hence, there exists θ 0 R such that Re ( e i θ 0 F ( z ) ) 1 for every z T . In particular, for every fH 2, we have:

Re e i θ 0 T F f , f 2 = Re T e i θ 0 F ( z ) | f ( z ) | 2 d m ( z ) = T Re ( e i θ 0 F ( z ) ) | f ( z ) | 2 d m ( z ) T | f ( z ) | 2 d m ( z ) = f 2 2 .

Hence, by Cauchy–Schwartz’ inequality, we get T F f 2 f 2 f 2 2 . In particular, for every fH 2, f ≠ 0, we have ‖T F f2 ≥ ‖f2. In Proposition 2.10, we have seen that this contradicts the hypercyclicity of T F and this gives a contradiction. Si E T .

(2) ⟹ (1): let us now assume that (i) and (ii) are satisfied and let us check that T F is hypercyclic on H 2. By Lemma 4.3, we know that F ( T ) is an elliptic curve and its interior E is such that

E = F z C ; 1 < | z | < a c .

See Figure 8.

We are going to prove that every point in E is an eigenvalue of T F and we will describe the associated eigenspace. So take μ = F ( z 0 ) E for some z 0 C with 1 < | z 0 | < a c . Let fH 2. Since T F = aS* + bI + cS, we have

f ker ( T F μ I ) T F f = F ( z 0 ) f z D , a f ( z ) f ( 0 ) z + b f ( z ) + c z f ( z ) = F ( z 0 ) f ( z ) z D , a ( f ( z ) f ( 0 ) ) + b z f ( z ) + c z 2 f ( z ) = z F ( z 0 ) f ( z ) z D , a + b F ( z 0 ) z + c z 2 f ( z ) = a f ( 0 ) z D , a a z 0 + c z 0 z + c z 2 f ( z ) = a f ( 0 ) z D , z 2 a c z 0 + z 0 z + a c f ( z ) = a c f ( 0 ) .

Now observe that

z 2 a c z 0 + z 0 z + a c = ( z z 0 ) z a c z 0

and since 1 < | z 0 | < a c , the function

z 1 ( z z 0 ) z a c z 0

belongs to H 2. Thus

ker ( T F μ I ) = C 1 ( z z 0 ) z a c z 0

where μ = F(z 0) and 1 < | z 0 | < a c . Since E T , the two open sets O 1 = E D and O 2 = E ( C \ D ̄ ) are non empty. Write Ω 1 = F 1 ( O 1 ) and Ω 2 = F 1 ( O 2 ) . Then Ω1 and Ω2 are two non empty open subsets of 1 < | z 0 | < a c and

s p a n 1 ( z z 0 ) z a c z 0 ; z 0 Ω 1 H ( T F ) ,

s p a n 1 ( z z 0 ) z a c z 0 ; z 0 Ω 2 H + ( T F ) .

By Godefroy – Shapiro Criterion, it is sufficient to check that if Ω is a non empty open set of 1 < | z 0 | < a c then

s p a n 1 ( z z 0 ) z a c z 0 ; z 0 Ω is dense in H 2 .

So let hH 2 such that for every z 0 ∈ Ω, we have

h 1 ( z z 0 ) z a c z 0 .

Note that if z 0 2 a / c , we have

1 ( z z 0 ) z a c z 0 = 1 z 0 a c z 0 1 z z 0 1 z a c z 0 = 1 z 0 a c z 0 1 / z 0 1 z z 0 + c z 0 / a 1 c z 0 a z = 1 z 0 a c z 0 1 z 0 k 1 z 0 ̄ + c z 0 a k c z 0 ̄ a ̄ ,

where we recall that k w denotes the reproducing kernel at w of H 2 (observe that 1 z 0 ̄ D and c z 0 ̄ a ̄ D ). Hence for every z 0 ∈ Ω with z 0 2 a / c , we have

0 = h , 1 z 0 k 1 z 0 ̄ + c z 0 a k c z 0 ̄ a ̄ = 1 z 0 ̄ h 1 z 0 ̄ + c z 0 ̄ a ̄ h c z 0 ̄ a ̄ .

Thus for every z 0 ∈ Ω with z 0 2 a / c , we have

1 z 0 h 1 z 0 ̄ ̄ = c z 0 a h c z 0 ̄ a ̄ ̄ .

Denote by q ( z ) = z h ( z ̄ ) ̄ for z D . We know that q is analytic on D and if A = z 0 1 ; z 0 Ω , z 0 2 a / c , then A is a nonempty open subset of W = { z C ; | c / a | < | z | < 1 } and for all zA, q ( z ) = q a c z . According to Lemma 4.4, we conclude that q is constant. But q(0) = 0, whence q ≡ 0 and therefore h ≡ 0.□

Figure 7: 
Non hypercyclic Toeplitz operator.
Figure 7:

Non hypercyclic Toeplitz operator.

Figure 8: 
Hypercyclic Toeplitz operator.
Figure 8:

Hypercyclic Toeplitz operator.

4.3 Some more recent results

To go a little bit further, we conclude by mentioning three recent papers.

The first one is by Baranov – Lishanskii, 2016 [15]. They investigate the more general case where F has the form

F ( e i θ ) = P ( e i θ ) + ϕ ( e i θ ) ,

where P is an analytic polynomial and ϕ A ( D ) . They provided some necessary conditions (of a spectral kind) for T F to be hypercyclic on H 2 as well as some sufficient conditions based on an explicit description of the eigenvectors of T F and on the Godefroy – Shapiro criterion. A novel feature of their conditions is the role of univalence or N-valence (where N is the degree of P) of the symbol. The same line of approach was taken in the subsequent work [16] of Abakumov, Baranov, Charpentier and Lishanskii where they extended results of [15] to the case of more general symbols F of the form

F ( e i θ ) = R ( e i θ ) + ϕ ( e i θ ) ,

where R is a rational function without poles in D ̄ and ϕ A ( D ) . The novel feature of the approach taken in [16] is the use of deep results of Solomyak providing necessary and sufficient conditions for finite sets of functions to be cyclic in H 2.

Finally, using the model theory for Toeplitz operators with smooth symbols developed by D. Yakubovich in the 80s, Fricain – Grivaux – Ostermann obtained in [1] some new necessary and sufficient conditions for Toeplitz operators to be hypercyclic on H p , 1 < p < ∞. We will take some time to discuss the flavor of some results obtained in [1]. Let q be the conjugate exponent of p, that is 1 p + 1 q = 1 . Consider the following conditions on the symbol F:

  1. F belongs to the class C 1 + ε ( T ) for some ɛ > max(1/p, 1/q), and its derivative F′ does not vanish on T here C 1 + ε ( T ) denotes the set of C 1 functions whose derivatives is ε-Hölder continuous;

  2. the curve F ( T ) self-intersects a finite number of times, i.e. the unit circle T can be partitioned into a finite number of closed arcs α 1, …, α m such that

    1. F is injective on the interior of each arc α j , 1 ≤ jm;

    2. for every ij, 1 ≤ i, jm, the sets F(α j ) and F(α j ) have disjoint interiors;

  3. for every λ C \ F ( T ) , wind F (λ) ≤ 0, where we recall that wind F (λ) denotes the winding number of the curve F ( T ) around λ.

Recall that σ ( T F ) = F ( T ) { λ C \ F ( T ) ; w i n d F ( λ ) < 0 } , and according to [12], the condition (H3) is a necessary condition for hypercyclicity. We denote by C the set of all connected component of σ ( T F ) \ F ( T ) . As we have seen in Theorem 2.14, if T is a hypercyclic operator on a separable Banach space X, every component of the spectrum of T must intersect T . It turns out that, in our current setting, a stronger property must hold.

Theorem 4.6

(Fricain – Grivaux – Ostermann, 2025 [1]). Let p > 1 and let F satisfy (H1), (H2) and (H3). If T F is hypercyclic on H p , then every component of the interior of the spectrum of T F must intersect T .

The proof of Theorem 4.6 relies on the fact that under conditions (H1), (H2) and (H3), the operator T F has an H -functional calculus on the interior of its spectrum.

In the other direction, we have the following result.

Theorem 4.7

(Fricain – Grivaux – Ostermann, 2025 [1]). Let p > 1 and let F satisfy (H1), (H2) and (H3). Suppose that, for every Ω C , Ω T . Then T F is hypercyclic on H p .

When the set σ ( T F ) \ F ( T ) is connected, we then deduce the following complete characterization.

Corollary 4.8

(Fricain – Grivaux – Ostermann, 2025 [1]). Let p > 1 and let F satisfy (H1), (H2) and (H3). Suppose that σ ( T F ) \ F ( T ) is connected. Then, the following are equivalent:

  1. T F is hypercyclic on H p ;

  2. T σ ( T F ) .

We refer to [1] for more deep results and proofs of all the previous results.


Corresponding author: Emmanuel Fricain, University of Lille, CNRS, UMR 8524 – Laboratoire Paul Painlevé, F-59000 Lille, France, E-mail: 

  1. Funding information: This work was supported in part by the project COMOP of the French National Research Agency (grant ANR-24-CE40-0892-01) and a variety of sponsors of the ACOTCA conference you could find here: https://indico.math.cnrs.fr/event/13430/. The authors acknowledge the support of the CDP C2EMPI, as well as of the French State under the France-2030 program, the University of Lille, the Initiative of Excellence of the University of Lille, and the European Metropolis of Lille for their funding and support of the R-CDP-24-004-C2EMPI project. The second author also acknowledges the support of the CNRS.

  2. Author contributions: The author confirms the sole responsibility for the conception of the study, presented results, and manuscript preparation.

  3. Conflict of interest: The author states no conflict of interest.

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Received: 2025-08-25
Accepted: 2025-11-03
Published Online: 2026-01-30

© 2026 the author(s), published by De Gruyter, Berlin/Boston

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