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# Applications of fixed point theorems in the theory of invariant subspaces

*Fixed Point Theory and Applications*
**volume 2012**, Article number: 197 (2012)

## Abstract

We survey several applications of fixed point theorems in the theory of invariant subspaces. The general idea is that a fixed point theorem applied to a suitable map yields the existence of invariant subspaces for an operator on a Banach space.

**MSC:**47A15, 47H10.

## 1 Introduction

One of the most recalcitrant unsolved problems in operator theory is the invariant subspace problem. The question has an easy formulation. Does every operator on an infinite dimensional, separable complex Hilbert space have a nontrivial invariant subspace?

Despite the simplicity of its statement, this is a very difficult problem and it has generated a very large amount of literature. We refer the reader to the expository paper of Yadav [1] for a detailed account of results related to the invariant subspace problem.

In this survey we discuss some applications of fixed point theorems in the theory of invariant subspaces. The general idea is that a fixed point theorem applied to a suitable map yields the existence of invariant subspaces for an operator on a Banach space.

In Section 2 we consider the striking theorem of Lomonosov [2] about the existence of invariant subspaces for algebras containing compact operators. The proof of this theorem is based on the Schauder fixed point theorem.

In Section 3 we present a recent result of Lomonosov, Radjavi, and Troitsky [3] about the existence of invariant subspaces for localizing algebras. The proof of this result is based on the Ky Fan fixed point theorem for multivalued maps. The idea of using fixed point theorems for multivalued maps in the search for invariant subspaces was first introduced by Androulakis [4].

In Section 4 we consider an extension of Burnside’s theorem to infinite dimensional Banach spaces. This result is originally due to Lomonosov [5]. We present a proof of it in a special case that was obtained independently by Scott Brown [6] and that once again is based on the Schauder fixed point theorem.

In Section 5 we address the existence of invariant subspaces for operators on the Krein space of an indefinite product, and we present a result of Albeverio, Makarov, and Motovilov [7] whose proof uses the Banach fixed point theorem.

The rest of this section contains some notation, a precise statement of the invariant subspace problem, and a few historical remarks.

Let *E* be an infinite dimensional, complex Banach space, and let \mathcal{B}(E) denote the algebra of all bounded linear operators on *E*. A subspace of *E* is by definition a closed linear manifold in *E*.

A subspace M\subseteq E is said to be *invariant* under an operator T\in \mathcal{B}(E) provided that TM\subseteq M, and a subspace M\subseteq E is said to be *invariant* under a subalgebra \mathcal{R}\subseteq \mathcal{B}(H) provided that *M* is invariant under every R\in \mathcal{R}. A subalgebra \mathcal{R}\subseteq \mathcal{B}(H) is said to be *transitive* provided that the only subspaces invariant under ℛ are the trivial ones, M=\{0\} and M=E. This is equivalent to saying that the subspace \{Rx:R\in \mathcal{R}\} is dense in *E* for each x\in E\mathrm{\setminus}\{0\}.

The *commutant* of a set of operators \mathcal{S}\subseteq \mathcal{B}(E) is the subalgebra {\mathcal{S}}^{\mathrm{\prime}} of all operators R\in \mathcal{B}(E) such that SR=RS for all S\in \mathcal{S}. A subspace M\subseteq E is said to be *hyperinvariant* under an operator T\in \mathcal{B}(E) provided that *M* is invariant under {\{T\}}^{\mathrm{\prime}}.

The *invariant subspace problem* is the question of whether every operator in \mathcal{B}(E) has a nontrivial invariant subspace. This is one of the most important open problems in operator theory.

The origin of this question goes back to 1935, when von Neumann proved the unpublished result that any compact operator on a Hilbert space has a nontrivial invariant subspace. Aronszajn and Smith [8] extended this result in 1954 to general Banach spaces. Bernstein and Robinson [9] used nonstandard analysis to prove in 1966 that every polynomially compact operator on a Hilbert space has a nontrivial invariant subspace. Halmos [10] obtained a proof of the same result using classical methods.

Lomonosov [2] proved in 1973 that any nonscalar operator on a Banach space that commutes with a nonzero compact operator has a nontrivial hyperinvariant subspace. The result of Lomonosov came into the scene like a lightning bolt in a clear sky, generalizing all the previously known results and introducing the use of the Schauder fixed point theorem as a new technique to produce invariant subspaces.

Enflo [11] constructed in 1976 the first example of an operator on a Banach space without nontrivial invariant subspaces. The example circulated in a preprint form and it did not appear published until 1987, when it was recognized as correct work [12]. In the meantime, Beauzamy [13] simplified the technique, and further examples were given by Read [14, 15].

Very recently, Argyros and Haydon [16] constructed an example of an infinite dimensional, separable Banach space such that every continuous operator is the sum of a compact operator and a scalar operator, so that every operator on it has a nontrivial invariant subspace.

However, after so many decades, the question about the existence of invariant subspaces for operators on Hilbert space is still an open problem.

## 2 Invariant subspaces for algebras containing compact operators

We start with a fixed point theorem that is the key to the main result in this section. The use of this result is one of the main ideas in the technique of Lomonosov. We shall denote by \overline{conv}(S) the closed convex hull of a subset S\subseteq E.

**Proposition 2.1** [[17], Proposition 1]

*Let* *E* *be a Banach space*, *let* C\subseteq E *be a closed convex set*, *and let* \mathrm{\Phi}:C\to E *be a continuous mapping such that* \mathrm{\Phi}(C) *is a relatively compact subset of* *C*. *Then there is a point* {x}_{0}\in C *such that* \mathrm{\Phi}({x}_{0})={x}_{0}.

*Proof* Let *Q* denote the closure of \mathrm{\Phi}(C). It follows from a theorem of Mazur that \overline{conv}(Q) is a compact, convex subset of *E*, and since *C* is closed and convex, we have \overline{conv}(Q)\subseteq C. Since \mathrm{\Phi}(C)\subseteq Q, we have \mathrm{\Phi}(\overline{conv}(Q))\subseteq Q\subseteq \overline{conv}(Q), and now the result follows from the Schauder fixed point theorem. □

**Theorem 2.2** [[17], Theorem 2]

*Let* \mathcal{R}\subseteq \mathcal{B}(E) *be a transitive algebra and let* K\in \mathcal{B}(E) *be a nonzero compact operator*. *Then there is an operator* R\in \mathcal{R} *and there is a vector* {x}_{1}\in E *such that* RK{x}_{1}={x}_{1}.

*Proof* We may assume, without loss of generality, that \parallel K\parallel =1. Choose an {x}_{0}\in E such that \parallel K{x}_{0}\parallel >1, so that \parallel {x}_{0}\parallel >1. Consider the closed ball B=\{x\in E:\parallel x-{x}_{0}\parallel \le 1\}. Then, for each R\in \mathcal{R}, consider the open set {G}_{R}=\{y\in E:\parallel Ry-{x}_{0}\parallel <1\}. Since ℛ is a transitive algebra, we have

Since *K* is a compact operator, \overline{KB} is a compact subset of *E*, and since \parallel K\parallel =1 and \parallel K{x}_{0}\parallel >1, we have 0\notin \overline{KB}. Thus, the family \{{G}_{R}:R\in \mathcal{R}\} is an open cover of \overline{KB}. Hence, there exist finitely many operators {R}_{1},\dots ,{R}_{n}\in \mathcal{R} such that

Next, for each y\in \overline{KB} and i=1,\dots ,n we define {\alpha}_{i}(y)=max\{0,1-\parallel {R}_{i}y-{x}_{0}\parallel \}. Then 0\le {\alpha}_{i}(y)\le 1, and for each y\in \overline{KB}, there is an i=1,\dots ,n such that y\in {G}_{{R}_{i}}, so that {\alpha}_{i}(y)>0. Thus, {\sum}_{i=1}^{n}{\alpha}_{i}(y)>0 for each y\in \overline{KB}, and we may define

for i=1,\dots ,n and y\in \overline{KB}. Now, each {\beta}_{i} is a continuous function from \overline{KB} into ℝ. Hence, we may define a continuous mapping \mathrm{\Phi}:B\to E by the expression

We claim that \mathrm{\Phi}(B)\subseteq B. Indeed, for each x\in B, we have {\sum}_{i=1}^{n}{\beta}_{i}(Kx)=1 so that

If \parallel {R}_{i}Kx-{x}_{0}\parallel >1, then {\alpha}_{i}(Kx)=0 and therefore {\beta}_{i}(Kx)=0. Hence,

and this completes the proof of our claim. Finally, each operator {R}_{i}K is compact so that each {R}_{i}KB is relatively compact, and it follows from an earlier mentioned theorem of Mazur that Q=\overline{conv}{\bigcup}_{i=1}^{n}{R}_{i}KB is compact. Since \mathrm{\Phi}(B)\subseteq Q, the set \mathrm{\Phi}(B) is a relatively compact subset of *B*. Now, we apply Proposition 2.1 to find a vector {x}_{1}\in B such that \mathrm{\Phi}({x}_{1})={x}_{1}. Since 0\notin B, we have {x}_{1}\ne 0. Then we consider the operator defined by

and we conclude that R\in \mathcal{R} and RK{x}_{1}={x}_{1}, as we wanted. □

**Corollary 2.3** [2], [[17], Theorem 3]

*Every nonscalar operator that commutes with a nonzero compact operator has a nontrivial*, *hyperinvariant subspace*.

*Proof* Let T\in \mathcal{B}(E) be a nonscalar operator and suppose that *T* commutes with a nonzero compact operator *K*. We must show that the commutant {\{T\}}^{\mathrm{\prime}} is nontransitive. Suppose, on the contrary, that {\{T\}}^{\mathrm{\prime}} is transitive. We can apply Theorem 2.2 to find an operator R\in {\{T\}}^{\mathrm{\prime}} such that \lambda =1 is an eigenvalue of the compact operator *RK* with an associated finite dimensional eigenspace F=ker(RK-I). Since *T* commutes with *RK*, we observe that *T* maps *F* into itself, and therefore, *T* must have an eigenvalue. Since *T* is nonscalar, the corresponding eigenspace *M* cannot be the whole *E*, and it is invariant under {\{T\}}^{\mathrm{\prime}}. The contradiction has arrived. □

## 3 Invariant subspaces for localizing algebras

In this section we use the following fixed point theorem of Ky Fan [18]. Recall that if Ω is a topological space and \mathrm{\Phi}:\mathrm{\Omega}\to \mathcal{P}(\mathrm{\Omega}) is a point to set map from Ω to the power set of Ω, then Φ is said to be *upper semicontinuous* if for every {x}_{0}\in \mathrm{\Omega} and every open set U\subseteq \mathrm{\Omega} such that \mathrm{\Phi}({x}_{0})\subseteq U, there is a neighborhood *V* of {x}_{0} such that \mathrm{\Phi}(x)\subseteq U for every x\in V. In terms of convergence of nets, this definition is equivalent to saying that for every x\in \mathrm{\Omega}, for every net ({x}_{\alpha}) with {x}_{\alpha}\to x, and for every {y}_{\alpha}\in \mathrm{\Phi}({x}_{\alpha}) such that the net ({y}_{\alpha}) converges to some y\in \mathrm{\Omega}, we have y\in \mathrm{\Phi}(x).

**Theorem 3.1** (Ky Fan fixed point theorem [18])

*Let* *C* *be a compact convex subset of a locally convex space*, *and let* \mathrm{\Phi}:C\to \mathcal{P}(C) *be an upper semicontinuous mapping such that* \mathrm{\Phi}(x) *is a nonempty*, *closed convex set for every* x\in C. *Then there is an* {x}_{0}\in C *such that* {x}_{0}\in \mathrm{\Phi}({x}_{0}).

A subalgebra \mathcal{R}\subseteq \mathcal{B}(H) is said to be *strongly compact* if its unit ball is precompact in the strong operator topology. An important example of a strongly compact algebra is the commutant of a compact operator with a dense range. We shall denote by ball(\mathcal{R}) the unit ball of ℛ.

This notion was introduced by Lomonosov [19] as a means to prove the existence of invariant subspaces for essentially normal operators on Hilbert spaces. Recall that an operator *T* on a Hilbert space is said to be *essentially normal* if {T}^{\ast}T-T{T}^{\ast} is a compact operator. Lomonosov showed that if an essentially normal operator *T* has the property that both its commutant {\{T\}}^{\mathrm{\prime}} and the commutant of its adjoint {\{{T}^{\ast}\}}^{\mathrm{\prime}} fail to be strongly compact, then *T* has a nontrivial invariant subspace.

Thus, in order to solve the invariant subspace problem for essentially normal operators, it suffices to consider only operators with a strongly compact commutant.

Lomonosov, Radjavi, and Troitsky [3] obtained a result about the existence of invariant subspaces for an operator with a strongly compact commutant under the additional assumption that the commutant of the adjoint is a localizing algebra.

A subalgebra \mathcal{R}\subseteq \mathcal{B}(E) is said to be *localizing* provided that there is a closed ball B\subseteq E such that 0\notin B and such that for every sequence ({x}_{n}) in *B* there is a subsequence ({x}_{{n}_{j}}), and a sequence of operators ({R}_{j}) in ℛ such that \parallel {R}_{j}\parallel \le 1 and ({R}_{j}{x}_{{n}_{j}}) converges in norm to some nonzero vector. An important example of a localizing algebra is any algebra containing a nonzero compact operator.

**Proposition 3.2** [[3], Proof of Theorem 2.3]

*Let* \mathcal{R}\subseteq \mathcal{B}(E) *be a transitive localizing algebra*, *let* B\subseteq E *be a closed ball as above*, *and let* T\in {\mathcal{R}}^{\mathrm{\prime}} *be a nonzero operator*. *Then there exists an* r>0 *such that for every* x\in B *we have* rball(\mathcal{R})(Tx)\cap B\ne \mathrm{\varnothing}.

*Proof* First, *T* is one-to-one because ℛ is transitive and ker*T* is invariant under ℛ. If this is not so, then for every n\ge 1, there is a vector {x}_{n}\in B such that \parallel R\parallel \ge n, whenever R\in \mathcal{R} and RT{x}_{n}\in B. Since ℛ is localizing, there is a subsequence ({x}_{{n}_{j}}) and a sequence ({R}_{j}) in ℛ such that \parallel {R}_{j}\parallel \le 1 and ({R}_{j}{x}_{{n}_{j}}) converges in norm to some nonzero vector x\in X. We have T{R}_{j}={R}_{j}T for all j\ge 1, so that ({R}_{j}T{x}_{{n}_{j}}) converges to *Tx* in norm. Now Tx\ne 0 because *T* is injective and x\ne 0. Since ℛ is transitive, there is an operator R\in \mathcal{R} such that RTx\in intB. It follows that there is a {j}_{0}\ge 1 such that R{R}_{j}T{x}_{{n}_{j}}\in intB for every j\ge {j}_{0}. Since R{R}_{j}\in \mathcal{R}, the choice of the sequence ({x}_{n}) implies that \parallel R{R}_{j}\parallel \ge {n}_{j} for every j\ge {j}_{0}, and this is a contradiction because \parallel R{R}_{j}\parallel \le \parallel R\parallel for every j\ge 1. □

If *E* is a Banach space, then {E}^{\ast} denotes its dual space. If \mathcal{R}\subseteq \mathcal{B}(E) is a subalgebra, then {\mathcal{R}}^{\ast} denotes the subalgebra of \mathcal{B}({E}^{\ast}) of the adjoints of the elements of ℛ, that is, {\mathcal{R}}^{\ast}=\{{R}^{\ast}:R\in \mathcal{R}\}.

**Theorem 3.3** [[3], Theorem 2.3]

*Let* *E* *be a complex Banach space*, *let* \mathcal{R}\subseteq \mathcal{B}(E) *be a strongly compact subalgebra such that* {\mathcal{R}}^{\ast} *is a transitive localizing algebra and it is closed in the weak*-∗ *operator topology*. *If* T\in {\mathcal{R}}^{\mathrm{\prime}} *is a nonzero operator*, *then there is an operator* R\in \mathcal{R} *and there is a nonzero vector* {x}^{\ast}\in {E}^{\ast} *such that* {R}^{\ast}{T}^{\ast}{x}^{\ast}={x}^{\ast}. *Moreover*, *the operator* {T}^{\ast} *has a nontrivial invariant subspace*.

*Proof* We shall apply Proposition 3.2 to the algebra {\mathcal{R}}^{\ast}. Let {B}^{\ast}\subseteq {E}^{\ast} be a closed ball as in the definition of a localizing algebra, let r>0 be a positive number as in Proposition 3.2, and define a multivalued map \mathrm{\Phi}:{B}^{\ast}\to \mathcal{P}({B}^{\ast}) by the expression

Then, \mathrm{\Phi}({x}^{\ast}) is a nonempty, convex subset of {B}^{\ast}. Also, \mathrm{\Phi}({x}^{\ast}) is weak-∗ closed because ball({\mathcal{R}}^{\ast})({T}^{\ast}{x}^{\ast}) is weak-∗ compact as the image of ball({\mathcal{R}}^{\ast}) under the map {R}^{\ast}\to {R}^{\ast}{T}^{\ast}{x}^{\ast}, which is continuous from \mathcal{B}({E}^{\ast}) with the weak-∗ operator topology into {E}^{\ast} with the weak-∗ topology, and ball({\mathcal{R}}^{\ast}) is compact in the weak-∗ operator topology.

We claim that Φ is upper semicontinuous for the weak-∗ topology. Indeed, let {x}^{\ast},{y}^{\ast}\in {B}^{\ast}, and let ({x}_{\alpha}^{\ast}) and ({y}_{\alpha}^{\ast}) be two nets in {B}^{\ast} with {x}_{\alpha}^{\ast}\to {x}^{\ast}, {y}_{\alpha}^{\ast}\to {y}^{\ast} in the weak-∗ topology and such that {y}_{\alpha}^{\ast}\in \mathrm{\Phi}({x}_{\alpha}^{\ast}). We must show that {y}^{\ast}\in \mathrm{\Phi}({x}^{\ast}). Since {y}_{\alpha}^{\ast}\in \mathrm{\Phi}({x}_{\alpha}^{\ast}), there is an {R}_{\alpha}^{\ast}\in ball({\mathcal{R}}^{\ast}) such that {y}_{\alpha}^{\ast}=r{R}_{\alpha}^{\ast}{T}^{\ast}{x}_{\alpha}^{\ast}. Since ball(\mathcal{R}) is precompact in the strong operator topology, there exists a subnet ({R}_{{\alpha}_{\beta}}) that converges in the strong operator topology to some R\in \mathcal{B}(E). Thus, {R}_{{\alpha}_{\beta}}^{\ast}\to {R}^{\ast} in the weak-∗ operator topology. Notice that ball({\mathcal{R}}^{\ast}) is compact in this topology because ball(\mathcal{B}({E}^{\ast})) is compact in this topology and {\mathcal{R}}^{\ast} is closed in this topology. It follows that {R}^{\ast}\in ball({\mathcal{R}}^{\ast}). Let x\in E and notice that \parallel T{R}_{{\alpha}_{\beta}}x-TRx\parallel \to 0. Then

We have \u3008T{R}_{{\alpha}_{\beta}}x-TRx,{x}_{{\alpha}_{\beta}}^{\ast}\u3009\to 0 and \u3008TRx,{x}_{{\alpha}_{\beta}}^{\ast}\u3009\to \u3008TRx,{x}^{\ast}\u3009=\u3008x,{R}^{\ast}{T}^{\ast}{x}^{\ast}\u3009, so that

Since x\in E is arbitrary, {y}_{{\alpha}_{\beta}}^{\ast}\to r{R}^{\ast}{T}^{\ast}{x}^{\ast} in the weak-∗ topology, and it follows that {y}^{\ast}=r{R}^{\ast}{T}^{\ast}{x}^{\ast}. This shows that {y}^{\ast}\in \mathrm{\Phi}({x}^{\ast}), and the proof of our claim is complete.

Since the map Φ is upper semicontinuous and {B}^{\ast} is compact in the weak-∗ topology, it follows from the Ky Fan fixed point theorem that there is a vector {x}^{\ast}\in {B}^{\ast} such that {x}^{\ast}\in \mathrm{\Phi}({x}^{\ast}); that is, there is an operator R\in ball(\mathcal{R}) such that {x}^{\ast}=r{R}^{\ast}{T}^{\ast}{x}^{\ast}.

Finally, consider the closed subspace defined as M=ker({R}^{\ast}{T}^{\ast}-I). Notice that *M* is invariant under {T}^{\ast} and M\ne \{0\}. If {T}^{\ast} is not invertible then M\ne E and we are done. If {T}^{\ast} is invertible, pick any \lambda \in \sigma ({T}^{\ast}) and put S=\lambda -{T}^{\ast}. Then *S* is not invertible and the preceding argument applied to *S* shows that *S* has a nontrivial invariant subspace. It is clear that such subspace is also invariant under {T}^{\ast}. □

**Corollary 3.4** [[3], Corollary 2.4]

*Let* T\in \mathcal{B}(E) *be an operator such that* {\{T\}}^{\mathrm{\prime}} *is a strongly compact algebra and* {\{{T}^{\ast}\}}^{\mathrm{\prime}} *is a localizing algebra*. *Then* {T}^{\ast} *has a nontrivial invariant subspace*.

*Proof* If {T}^{\ast} has a hyperinvariant subspace then there is nothing to prove, and otherwise {\{{T}^{\ast}\}}^{\mathrm{\prime}} is a transitive algebra so that Theorem 3.3 applies. □

Notice that the assumptions of Corollary 3.4 are met whenever *T* is a compact operator with a dense range.

## 4 An infinite dimensional version of Burnside’s theorem

Burnside’s classical theorem is the assertion that for a finite dimensional linear space *F*, the only transitive subalgebra of \mathcal{B}(F) is the whole algebra \mathcal{B}(F). Lomonosov [5] obtained a generalization of Burnside’s theorem to infinite dimensional Banach spaces. Scott Brown [6] proved the same result independently for the special case of a Hilbert space and a commutative algebra. Lindström and Schlüchtermann [20] provided a relatively short proof of the Lomonosov result in full generality. In this section we present a proof of the Scott Brown result that is based on the Schauder fixed point theorem.

Let *H* be a complex, infinite dimensional, and separable Hilbert space. Let T\in \mathcal{B}(H), and let {\parallel T\parallel}_{e} denote the essential norm of *T*, that is, the distance from *T* to the space of compact operators.

**Theorem 4.1** [[6], Theorem 1.1]

*Let* ℛ *be a commutative subalgebra of* \mathcal{B}(H). *Then there exist nonzero vectors* x,y\in H *such that for any* R\in \mathcal{R} *we have* |\u3008Rx,y\u3009|\le {\parallel R\parallel}_{e}.

*Proof* Consider the set \mathcal{E}=\{R\in \mathcal{R}:{\parallel R\parallel}_{e}\le 1/16\}. We claim that there is some x\in H\mathrm{\setminus}\{0\} such that the set \mathcal{E}x is not dense in *H*. The result then follows easily because in that case there is some y\in H\mathrm{\setminus}\{0\} such that |\u3008Rx,y\u3009|\le 1 for all R\in \mathcal{E}. Now, for the proof of our claim, we proceed by contradiction. Suppose that the set \mathcal{E}x is dense in *H* for every x\in H\mathrm{\setminus}\{0\}. Choose {x}_{0}\in H with \parallel {x}_{0}\parallel =2 and consider the closed ball B=\{x\in H:\parallel x-{x}_{0}\parallel \le 1\}. Then, for every vector x\in B, there is an operator {R}_{x}\in \mathcal{E} such that \parallel {R}_{x}x-{x}_{0}\parallel <1/2. Next, there is a bounded operator {T}_{x} and a compact operator {K}_{x} such that {R}_{x}={T}_{x}+{K}_{x} and \parallel {T}_{x}\parallel \le 1/8. Since {K}_{x} is a compact operator, it is weak-to-norm continuous on bounded sets so that there exists an open neighborhood of *x* in the weak topology, say {V}_{x}\subseteq H, such that \parallel {K}_{x}y-{K}_{x}x\parallel <1/4 for all y\in {V}_{x}\cap B. Then consider the set {U}_{x}={V}_{x}\cap B and notice that {U}_{x} is an open neighborhood of *x* in the weak topology relative to *B*. Moreover, for y\in {U}_{x} we have

and therefore \parallel {R}_{x}y-{x}_{0}\parallel <1. Hence, {R}_{x}{U}_{x}\subseteq B. Since *B* is compact in the weak topology, there exist finitely many vectors {x}_{1},\dots {x}_{n}\in B such that

Choose some weakly continuous functions {f}_{1},\dots ,{f}_{n} on *B* such that , 0\le {f}_{j}(x)\le 1, and

Define a weakly continuous mapping \mathrm{\Phi}:B\to B by the expression

and apply the Schauder fixed point theorem to find a vector {y}_{0}\in B such that \mathrm{\Phi}({y}_{0})={y}_{0}. Finally, consider the operator R\in \mathcal{R} defined by the expression

Hence, R{y}_{0}={y}_{0}. Notice that R\ne I because {\parallel R\parallel}_{e}\le 1/8. Then, the eigenspace M=\{x\in H:Rx=x\} is a closed nontrivial invariant subspace for the algebra ℛ. Thus, any vector x\in M has the property that the set \mathcal{E}x is not dense in *H*. The contradiction has arrived. □

## 5 Invariant subspaces for operators on the Krein space

Let {H}_{1}, {H}_{2} be two Hilbert spaces and consider the orthogonal direct sum H={H}_{1}\oplus {H}_{2}. Let {P}_{1}, {P}_{2} denote the orthogonal projections from *H* onto {H}_{1}, {H}_{2}, respectively. Consider the operator J:={P}_{1}-{P}_{2}. The *Krein space* is the space *H* provided with the indefinite product

Notice that *J* is a selfadjoint involution, that is, {J}^{\ast}=J and {J}^{2}=I. The operator *J* is sometimes called the *fundamental symmetry* of the Krein space.

A vector x\in H is said to be *nonnegative* provided that [x,x]\ge 0, and a subspace M\subseteq H is said to be *nonnegative* provided that [x,x]\ge 0 for all x\in M.

Every operator T\in \mathcal{B}(H) has a matrix representation

with respect to the decomposition H={H}_{1}\oplus {H}_{2}.

There is a natural, one-to-one and onto correspondence between the maximal nonnegative invariant subspaces *M* of an operator T\in \mathcal{B}(H) and the contractive solutions X\in \mathcal{B}({H}_{1},{H}_{2}) of the so-called *operator Riccati equation*

The correspondence X\leftrightarrow M is given by M=\{{x}_{1}\oplus X{x}_{1}:{x}_{1}\in {H}_{1}\}, where \parallel X\parallel \le 1. The operator *T* is usually called the *Hamiltonian operator* of the operator Ricatti equation.

An operator T\in \mathcal{B}(H) is said to be *J*-*selfadjoint* provided that [Tx,y]=[x,Ty] for every x,y\in H. This is equivalent to saying that JT={T}^{\ast}J, or in other words, {T}_{11}^{\ast}={T}_{11}, {T}_{22}^{\ast}={T}_{22}, and {T}_{12}^{\ast}=-{T}_{21}.

A classical theorem of Krein is the assertion that if the Hamiltonian operator *T* is *J*-selfadjoint and the corner operator {T}_{12} is compact, then there exists a maximal nonnegative invariant subspace for *T*.

Albeverio, Makarov, and Motovilov [7] addressed the question of the existence and uniqueness of contractive solutions to the operator Riccati equation under the condition that the diagonal entries in the Hamiltonian operator have disjoint spectra, that is, \sigma ({T}_{11})\cap \sigma ({T}_{22})=\mathrm{\varnothing}. They proved the following

**Theorem 5.1** [[7], Theorem 3.6 and Lemma 3.11]

*There is some universal constant*
c>0
*such that whenever the corner operator*
{T}_{12}
*satisfies the condition*

*there is a unique solution* *X* *to the operator Riccati equation with* \parallel X\parallel \le 1.

An earlier result in this direction was given by Motovilov [[21], Corollary 1] with the stronger assumption that the corner operator {T}_{12} is Hilbert-Schmidt. Adamjan, Langer, and Tretter [22] extended the technique to the case that the Hamiltonian operator is not *J*-selfadjoint. Kostrykin, Makarov, and Motovilov [23] adopted the assumption that \sigma ({T}_{11}) lies in a gap of \sigma ({T}_{22}) and they showed that the best constant, in that context, is c=\sqrt{2}.

We present a proof of Theorem 5.2 that is based on the Banach fixed point theorem. This method can be found in the paper of Albeverio, Motovilov, and Shkalikov [[24], Theorem 4.1]. A basic tool is the bounded linear operator *R* defined for X\in \mathcal{B}({H}_{1},{H}_{2}) by the expression

It follows from the Rosenblum theorem that the map *R* is invertible. The main result is the following

**Theorem 5.2** [[24], Theorem 4.1]

*If the operators* {T}_{11}, {T}_{22} *have disjoint spectra and the corner operator* {T}_{12} *satisfies the estimate*

*then there is a unique solution* *X* *to the operator Riccati equation with* \parallel X\parallel \le 1.

The following upper bound on the norm of the inverse {R}^{-1} can be found in the work of Albeverio, Makarov, and Motovilov [[7], Theorem 2.7]. See also the paper by Bhatia and Rosenthal [[4], p.15] for this interesting result and other related issues.

**Theorem 5.3** [[7], Theorem 2.7]

*If the operators* {T}_{11}, {T}_{22} *have disjoint spectra*, *then*

Notice that Theorem 5.1 becomes a corollary of Theorem 5.2 and Theorem 5.3 with the constant c=1/\pi.

*Proof of Theorem 5.2* Consider the quadratic map *Q* defined for X\in \mathcal{B}({H}_{1},{H}_{2}) by the expression

It is clear that the operator Riccati equation can be expressed as

or equivalently, X={R}^{-1}(Q(X)). Thus, the solutions of the operator Riccati equation are the fixed points of the map S:={R}^{-1}\circ Q. Now, let us check that the map *S* takes the unit ball of \mathcal{B}({H}_{1},{H}_{2}) into itself. Indeed, if \parallel X\parallel \le 1, then

Also, the map *S* is contractive, for if \parallel X\parallel ,\parallel Y\parallel \le 1, then

and from this inequality it follows that

so that the map *S* satisfies a Lipschitz condition with a Lipschitz constant 2\parallel {R}^{-1}\parallel \cdot \parallel {T}_{12}\parallel <1. The result now follows at once as a consequence of the Banach fixed point theorem. □

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## Acknowledgements

This research was partially supported by Junta de Andalucía under projects FQM-127 and FQM-3737, and by Ministerio de Educación, Cultura y Deporte under projects MTM2012-34847C02-01 and MTM2009-08934.

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Espínola, R., Lacruz, M. Applications of fixed point theorems in the theory of invariant subspaces.
*Fixed Point Theory Appl* **2012**, 197 (2012). https://doi.org/10.1186/1687-1812-2012-197

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DOI: https://doi.org/10.1186/1687-1812-2012-197