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http://dx.doi.org/10.4134/JKMS.2012.49.1.139

CROSS COMMUTATORS ON BACKWARD SHIFT INVARIANT SUBSPACES OVER THE BIDISK II

Kei Ji Izuchi and Kou Hei Izuchi

Abstract. In the previous paper, we gave a characterization of backward shift invariant subspaces of the Hardy space over the bidisk on which [Szn, Sw] = 0 for a positive integer n≥ 2. In this case, it holds that Szn= cI for some c∈ C. In this paper, it is proved that if [Sφ, Sw] = 0 and φ∈ Hz), then Sφ= cI for some c∈ C.

1. Introduction

Let Γ

2

be the 2-dimensional unit torus. We write (z, w) = (e

is

, e

it

) for variables in Γ

2

= Γ

z

× Γ

w

. Let L

2

= L

2

2

) be the usual Lebesgue space on Γ

2

with the norm

∥f∥

2

= ( ∫

0

0

|f(e

is

, e

it

) |

2

dsdt (2π)

2

)

1/2

.

With the usual inner product, L

2

is a Hilbert space. Let H

2

= H

2

2

) be the Hardy space over Γ

2

. We denote by H

2

z

) and H

2

w

) the Hardy spaces on the unit circle Γ in variables z and w, respectively. We think of H

2

z

) and H

2

w

) as closed subspaces H

2

. For each f ∈ H

2

, we can write f as

f =

i=0

⊕f

i

(w)z

i

, f

i

(w) ∈ H

2

w

).

Let P be the orthogonal projection from L

2

onto H

2

. For a closed subspace M of L

2

, we denote by P

M

the orthogonal projection from L

2

onto M . For a function ψ ∈ L

, the Toeplitz operator T

ψ

on H

2

is defined by T

ψ

f = P (ψf ) for f ∈ H

2

. It is well known that T

ψ

= T

ψ

, and T

φ(z)

T

ψ(w)

= T

ψ(w)

T

φ(z)

for every φ(z) ∈ H

z

) and ψ(w) ∈ H

w

). A function f ∈ H

2

is called inner if |f| = 1 on Γ

2

almost everywhere. A nonzero closed subspace M of H

2

is

Received September 20, 2010; Revised December 17, 2010.

2010 Mathematics Subject Classification. Primary 47A15, 32A35; Secondary 47B35.

Key words and phrases. backward shift invariant subspace, invariant subspace, Hardy space, cross commutator.

The first author is partially supported by Grant-in-Aid for Scientific Research (No.16340037), Japan Society for the Promotion of Science.

⃝2012 The Korean Mathematical Societyc 139

(2)

called invariant if zM ⊂ M and wM ⊂ M. In one variable case, the well known Beurling theorem [2] says that an invariant subspace M of H

2

z

) has a form M = q(z)H

2

z

), where q(z) is an inner function. In two variable case, the structure of invariant subspaces of H

2

is extremely complicated, see [3, 10].

Let M be an invariant subspace of H

2

with M ̸= {0} and M ̸= H

2

. Then T

z

(H

2

⊖ M) ⊂ H

2

⊖ M and T

w

(H

2

⊖ M) ⊂ H

2

⊖ M. In this paper, we write

N = H

2

⊖ M.

Usually, N is called a backward shift invariant subspace of H

2

. See [1, 9] for studies of backward shift invariant subspaces over the unit circle Γ.

For a function ψ ∈ L

, we denote by R

ψ

the operator on M defined by R

ψ

f = P

M

(ψf ) for f ∈ M. It holds R

ψ

= R

ψ

and R

z

= T

z

|

M

. We denote by [R

z

, R

w

] the cross commutator of R

z

and R

w

, that is, [R

z

, R

w

] = R

z

R

w

R

w

R

z

. In [8], Mandrekar proved that [R

z

, R

w

] = 0 if and only if M is Beurling type, that is, M = qH

2

for some inner function q on Γ

2

. This is a nice characterization of Beurling type invariant subspaces of H

2

. More generally, in [4] the authors proved that [R

z

, R

w

] = 0 if and only if [R

ψ1(z)

, R

ψ

2(w)

] = 0 for nonconstant functions ψ

1

(z), ψ

2

(w) ∈ H

(Γ).

We define the operator S

ψ

on N by S

ψ

f = P

N

(ψf ) for f ∈ N. Then we have S

ψ

= S

ψ

and S

z

= T

z

|

N

. In [6], it is proved that [S

z

, S

w

] = 0 if and only if N has one of the following forms;

· N = H

2

⊖ q

1

(z)H

2

,

· N = H

2

⊖ q

2

(w)H

2

,

· N = (H

2

⊖ q

1

(z)H

2

) ∩ (H

2

⊖ q

2

(w)H

2

)

for nonconstant one variable inner functions q

1

(z) and q

2

(w). In [7], it is shown that the condition [S

z2

, S

w

] = 0 does not imply [S

z

, S

w

] = 0. In [5], the authors proved that for n ≥ 2, [S

zn

, S

w

] = 0 if and only if one of the following conditions holds;

(i) [S

z

, S

w

] = 0, (ii) S

zn

S

w

= 0,

(iii) there exists a Blaschke product b(z) with b(z) =

n j=1

z − α

j

1 − α

j

z , 0 <

j

| < 1,

where α

i

̸= α

j

for every i, j with i ̸= j and α

n1

= α

n2

= · · · = α

nn

such that N ⊂ H

2

⊖ b(z)H

2

.

In [7, Theorem 2.2], it is proved that (ii) holds if and only if either N ⊂ H

2

z

) or N ⊂ H

2

⊖ z

n

H

2

. If N ⊂ H

2

z

), then we have [S

z

, S

w

] = 0. Moreover, in [5] it is proved that if [S

zn

, S

w

] = 0 and [S

z

, S

w

] ̸= 0, then M ∩ H

z

) = θ(z)H

z

) for an inner function θ(z), and z

n

∈ C + θ(z)H

z

). In this case, we have S

zn

= cI for some c ∈ C.

The purpose of this paper is to generalize the above phenomeron. Let

φ(z) ∈ H

z

) be a nonconstant function. Suppose that [S

φ(z)

, S

w

] = 0 and

(3)

[S

z

, S

w

] ̸= 0. In Section 2, we prove that M ∩H

z

) ̸= {0} and M ∩H

2

z

) ̸=

H

2

z

). Hence by the Beurling theorem, M ∩ H

2

z

) = θ(z)H

2

z

) for a non- constant inner function θ(z). Thus we get θ(z)H

2

⊂ M. Write

M

θ

= M ⊖ θ(z)H

2

.

We prove that M

θ

̸= {0} and T

φ(z)

M

θ

⊂ M

θ

. In another word, φ(z)N N ⊕ θ(z)H

2

holds. In Section 3, we study on the one variable Hardy space H

2

z

). Let N

1

, N

2

be backward shift invariant subspaces of H

2

z

) satisfying {0} ̸= N

2

⫋ N

1

̸= H

2

z

). It is proved that φ(z)N

2

⊂ N

2

⊕ (H

2

z

) ⊖ N

1

) if and only if φ(z) ∈ C+(H

2

z

) ⊖N

1

). As applications of these facts, in Section 4 we prove that φ(z) ∈ C + θ(z)H

z

) and S

φ

= cI for some c ∈ C.

2. Equivalent conditions for [S

φ(z)

, S

w

] = 0

Let N be a backward shift invariant subspace of H

2

with N ̸= {0} and N ̸=

H

2

, and let φ(z) ∈ H

z

) be a nonconstant function. We write operators T

φ

and T

w

on H

2

= M ⊕ N in the matrix forms as

T

φ

=

( ∗ P

M

T

φ

|

N

0 S

φ

)

, T

w

=

( 0

P

N

T

w

|

M

S

w

)

on H

2

=

M

N

 .

Let

A = P

M

T

φ

|

N

and B = P

N

T

w

|

M

. Since T

φ

T

w

= T

w

T

φ

on H

2

, we have

S

φ

S

w

= BA + S

w

S

φ

. Hence we get the following.

Lemma 2.1. [S

φ

, S

w

] = 0 if and only if BA = 0.

It is not difficult to see that

ker B = {f ∈ M : T

w

f ∈ M}

= {f ∈ M ⊖ wM : T

w

f = 0 } ⊕ wM

= (

M ∩ H

2

z

) )

⊕ wM and

range A = M ⊖ ker A

= M ⊖ {f ∈ M : T

φ

f ∈ M}.

Then by Lemma 2.1, we have the following.

Lemma 2.2. [S

φ

, S

w

] = 0 if and only if M ⊖ {f ∈ M : T

φ

f ∈ M} ⊂ (

M ∩ H

2

z

) )

⊕ wM.

Lemma 2.3. If [S

φ

, S

w

] = 0 and [S

z

, S

w

] ̸= 0, then M ∩H

2

z

) is a nontrivial

invariant subspace of H

2

z

).

(4)

Proof. Since M ̸= H

2

, trivially M ∩ H

2

z

) ̸= H

2

z

) holds. Suppose that M ∩ H

2

z

) = {0}. By Lemma 2.2,

M ⊖ {f ∈ M : T

φ

f ∈ M} ⊂ wM.

Hence

M ⊖ wM ⊂ {f ∈ M : T

φ

f ∈ M}.

Since T

w

T

φ

= T

φ

T

w

on H

2

, if f ∈ M and T

φ

f ∈ M, then T

φ

(w

n

f ) = w

n

T

φ

f M for every n ≥ 0, so that by the above we get

w

n

(M ⊖ wM) ⊂ {f ∈ M : T

φ

f ∈ M}.

Therefore

M =

n=0

⊕w

n

(M ⊖ wM) ⊂ {f ∈ M : T

φ

f ∈ M}.

Thus we get T

φ

M ⊂ M. This shows that φ(z)N ⊂ N.

Let

A = {ψ(z) ∈ H

z

) : ψN ⊂ N}.

Then both functions 1 and φ(z) are contained in A. For ψ ∈ A and h ∈ N, we have

N ∋ T

z

(ψh) = (T

z

ψ)h + ψ(0)T

z

h.

Hence (T

z

ψ)N ⊂ N, so that T

z

A ⊂ A. It is easy to see that A is a weak-

closed subalgebra of H

z

). Let

L = {

f (z) ∈ H

1

z

) :

0

f (e

)ψ(e

)

= 0 for every ψ(z) ∈ A } . Then L is a closed subspace of H

1

z

). Since T

z

A ⊂ A and 1 ∈ A, we have zL ⊂ L.

Suppose that L ̸= {0}. By the Beurling theorem, L = q(z)H

1

z

) for an inner function q(z). Since 1 ∈ A, q(0) = 0. Hence zq(z) ∈ H

z

). Since φ(z)

n

∈ A for n ≥ 1,

0

e

−iθ

q(e

)φ(e

)

n

e

h(e

) =

0

q(e

)h(e

)φ(e

)

n

= 0 for every h(z) ∈ H

1

z

). Hence zq(z)φ(z)

n

∈ H

z

) for every n ≥ 1. By the Schneider theorem [11], we have φ(z) ∈ H

z

). This shows that φ(z) is constant. Since we assumed that φ(z) is nonconstant, this is a contradiction.

Therefore L = {0}. Hence A = H

z

). Especially, we have z ∈ A and zN ⊂ N. Then T

z

|

N

= S

z

. Since T

w

|

N

= S

w

and T

z

T

w

= T

w

T

z

on H

2

, we have S

z

S

w

= S

w

S

z

. This is a desired contradiction. □ In the rest of this section, we assume that M ∩H

2

z

) ̸= {0}. Since M ̸= H

2

, M ∩ H

2

z

) ̸= H

2

z

). By the Beurling theorem,

M ∩ H

2

z

) = θ(z)H

2

z

)

(5)

for some nonconstant inner function θ(z). Hence θ(z)H

2

⊂ M. Write M

θ

= M ⊖ θ(z)H

2

.

Then

M = M

θ

⊕ θ(z)H

2

and H

2

⊖ θ(z)H

2

= M

θ

⊕ N.

By the definition of M

θ

, we have wM

θ

⊂ M

θ

and M

θ

∩ H

2

z

) = {0}. Note that if [S

φ

, S

w

] = 0 and [S

z

, S

w

] ̸= 0, then M

θ

̸= {0}. For, if M

θ

= {0}, then M = θ(z)H

2

and N = H

2

⊖ θ(z)H

2

. Then we have [S

z

, S

w

] = 0, see [6], and this is a contradiction.

Lemma 2.4. Let f ∈ M

θ

. Then T

w

f ∈ M

θ

if and only if f ∈ wM

θ

. Proof. Suppose that T

w

f ∈ M

θ

. Then

f − f(z, 0) ∈ wM

θ

⊂ M

θ

.

Since f ∈ M

θ

, f (z, 0) ∈ M

θ

. Since M

θ

∩ H

2

z

) = {0}, f(z, 0) = 0. Hence

f ∈ wM

θ

. The converse is trivial. □

Let P

θ

be the orthogonal projection from H

2

onto H

2

⊖ θ(z)H

2

, and Q

φ

be the operator on H

2

⊖ θ(z)H

2

defined by Q

φ

f = P

θ

(φf ) for f ∈ H

2

⊖ θ(z)H

2

. We can write both operators Q

φ

and T

w

|

(H2⊖θH2)

as

Q

φ

=

( ∗ P

Mθ

T

φ

|

N

0 S

φ

)

on H

2

⊖ θ(z)H

2

=

M

θ

N

and

T

w

|

(H2⊖θH2)

=

( 0

P

N

T

w

|

Mθ

S

w

)

on H

2

⊖ θ(z)H

2

=

M

θ

N

 .

Let

A

θ

= P

Mθ

T

φ

|

N

and B

θ

= P

N

T

w

|

Mθ

. Lemma 2.5. [S

φ

, S

w

] = 0 if and only if B

θ

A

θ

= 0.

Proof. Let f ∈ H

2

⊖θ(z)H

2

= M

θ

⊕N. We have T

w

(φ(z)f ) = φ(z)T

w

f . Write φ(z)f = Q

φ

f ⊕ f

1

∈ (M

θ

⊕ N) ⊕ θ(z)H

2

.

Since T

w

f

1

∈ θ(z)H

2

and T

w

(Q

φ

f ) ⊥ θ(z)H

2

, we get T

w

Q

φ

f = Q

φ

T

w

f . Thus Q

φ

T

w

= T

w

Q

φ

on M

θ

⊕ N. Similarly as Lemma 2.1, we can prove the

assertion. □

The following is a slight generalization of [7, Theorem 4.4].

Theorem 2.6. The following conditions are equivalent;

(i) [S

φ

, S

w

] = 0,

(ii) M

θ

⊖ {f ∈ M

θ

: T

φ

f ∈ M

θ

} ⊂ wM

θ

,

(iii) T

φ

M

θ

⊂ M

θ

,

(6)

(iv) φ(z)N ⊂ N ⊕ θ(z)H

2

. Proof. By Lemma 2.4,

ker B

θ

= {f ∈ M

θ

: T

w

f ∈ M

θ

} = wM

θ

. Also we have

range A

θ

= M

θ

⊖ ker A

θ

= M

θ

⊖ {f ∈ M

θ

: T

φ

f ∈ M

θ

}.

Hence by Lemma 2.5, we get (i) ⇔ (ii).

If (ii) holds, then

M

θ

⊖ wM

θ

⊂ {f ∈ M

θ

: T

φ

f ∈ M

θ

}.

Hence for each n ≥ 0, we have

T

φ(z)

w

n

(M

θ

⊖ wM

θ

) = w

n

T

φ(z)

(M

θ

⊖ wM

θ

) ⊂ w

n

M

θ

⊂ M

θ

. Since

M

θ

=

n=0

⊕w

n

(M

θ

⊖ wM

θ

), we have T

φ

M

θ

⊂ M

θ

. Thus we get (iii).

(iii) ⇒ (ii) is trivial.

It is not difficult to see that (iii) ⇔ (iv).

Suppose that [S

φ

, S

w

] = 0 and [S

z

, S

w

] ̸= 0. Then we proved that θ(z)H

2

⫋ M and φ(z)(H

2

⊖ M) ⊂ (H

2

⊖ M) ⊕ θ(z)H

2

.

Note that θ(z)H

2

and M are invariant subspaces of H

2

. Now we fix an inner function θ(z). Here we have a question for which φ(z) ∈ H

z

) satisfies the above condition. In the next section, we study a similar question in the one variable Hardy space H

2

z

). In Section 4, we revisit on this question.

3. A theorem on the unit circle In this section, we prove the following theorem.

Theorem 3.1. Let N

1

, N

2

be backward shift invariant subspaces of H

2

z

) with 0 ̸= N

2

⫋ N

1

̸= H

2

z

), and φ(z) ∈ N

1

. Then

φ(N

2

∩ H

z

)) ⊂ N

2

⊕ (H

2

z

) ⊖ N

1

)

if and only if φ(z) = cP

N1

1 for some c ∈ C. In this case, if we define the operator S

φ

on N

1

by S

φ

f = P

N1

(φf ) for f ∈ N

1

, then S

φ

= cI.

To prove the theorem, we need two lemmas which are not difficult to show.

Lemma 3.2. Let N be a backward shift invariant subspace of H

2

z

). Then N ∩ H

z

) is dense in N .

Lemma 3.3. Let N be a backward shift invariant subspace of H

2

z

) with N ̸= {0} and N ̸= H

2

z

). If φ ∈ H

2

z

) is a nonconstant function, then φ (

N ∩ H

z

) )

̸⊂ N.

(7)

Proof of Theorem 3.1. By the Beurling theorem, H

2

z

) ⊖ N

1

= θH

2

z

) for some nonconstant inner function θ.

First, suppose that

φ(N

2

∩ H

z

)) ⊂ N

2

⊕ (H

2

z

) ⊖ N

1

).

Since N

2

̸= {0}, by Lemma 3.2 there exists h

1

∈ N

2

∩ H

z

) with h

1

(0) = 1.

Write

(3.1) φh

1

= f

1

⊕ θg

1

∈ N

2

(

H

2

z

) ⊖ N

1

) = N

2

⊕ θH

2

z

).

Also for each h ∈ N

2

∩ H

z

), we can write

(3.2) φh = f ⊕ θg ∈ N

2

⊕ θH

2

z

).

When h(0) = 0, we shall prove that

(3.3) g(0) = 0.

Since

T

z

(φh) = φT

z

h + h(0)T

z

φ = φT

z

h, by (3.2) we have

φT

z

h = T

z

(φh) = T

z

(f + θg)

= T

z

f + θT

z

g + g(0)T

z

θ

= (T

z

f + g(0)T

z

θ) + θT

z

g.

Note that T

z

h ∈ N

2

∩H

z

) and T

z

f + g(0)T

z

θ ⊥ θH

2

z

). By the assump- tion, φT

z

h ∈ N

2

⊕ θH

2

z

). Hence

T

z

f + g(0)T

z

θ ∈ N

2

.

Since T

z

f ∈ N

2

, g(0)T

z

θ ∈ N

2

. To prove (3.3), suppose that g(0) ̸= 0. Then T

z

θ ∈ N

2

. Let N be a backward shift invariant subspace generated by T

z

θ.

Since N

1

= H

2

z

) ⊖ θH

2

z

), we have N = N

1

. Since T

z

θ ∈ N

2

, N ⊂ N

2

. This contradicts N

2

⫋ N

1

. Therefore g(0) = 0. Thus we get (3.3).

By (3.1) and (3.2),

φ(h − h(0)h

1

) = (f − h(0)f

1

) ⊕ θ(g − h(0)g

1

) ∈ N

2

⊕ θH

2

z

).

Since (h − h(0)h

1

)(0) = 0, by (3.3) we get

(3.4) g(0) = h(0)g

1

(0).

By (3.2) again,

φT

z

h + h(0)T

z

φ = T

z

(φh) = (T

z

f + g(0)T

z

θ) + θT

z

g, so that

φT

z

h = (

− h(0)T

z

φ + T

z

f + g(0)T

z

θ )

⊕ θT

z

g.

Since T

z

h ∈ N

2

∩ H

z

) and φ ⊥ θH

2

z

), by the assumption we have

−h(0)T

z

φ + T

z

f + g(0)T

z

θ ∈ N

2

.

(8)

Similarly we have φT

z∗2

h =

( − (T

z

h)(0)T

z

φ − h(0)T

z∗2

φ + T

z∗2

f + g(0)T

z∗2

θ

+(T

z

g)(0)T

z

θ

) ⊕ θT

z∗2

g.

Repeating the same argument, we get φT

z∗n

h =

[ (

n

−1

j=0

( T

z∗(n−j−1)

h )

(0)T

z∗(j+1)

φ )

+ T

z∗n

f

+ (

n

−1

j=0

(T

z∗j

g)(0)T

z∗(n−j)

θ

)] ⊕ θT

z∗n

g.

Since h ∈ N

2

∩ H

z

), T

z∗n

h ∈ N

2

∩ H

z

). Hence by (3.2) and (3.4), (T

z∗n

g)(0) = (T

z∗n

h)(0)g

1

(0)

for every n ≥ 0. This shows that g = g

1

(0)h. By (3.2), we obtain − g

1

(0)θ)h = f ∈ N

2

for every h ∈ N

2

∩ H

z

). By Lemma 3.3, φ − g

1

(0)θ is constant. Write φ − g

1

(0)θ = c. Since φ ∈ N

1

, we have φ = cP

N1

1.

Next, suppose that φ = cP

N1

1. Then

φ = cP

N1

1 = c(1 − θ(0)θ).

Hence for f ∈ N

2

∩ H

z

), we have

φf = cf − cθ(0)θf ∈ N

2

⊕ θH

2

z

).

Thus we get φ (

N

2

∩ H

z

) )

⊂ N

2

⊕ (H

2

z

) ⊖ N

1

). □ Corollary 3.4. Let N

1

, N

2

be backward shift invariant subspaces of H

2

z

) with {0} ̸= N

2

⫋ N

1

̸= H

2

z

), and φ(z) ∈ L

z

). Define the operator S

φ

on N

1

by S

φ

h = P

N1

(φh) for h ∈ N

1

. Then S

φ

N

2

⊂ N

2

if and only if φ ∈ C + H

2

z

)

+ (H

2

z

) ⊖ N

1

) = H

2

z

) + (H

2

z

) ⊖ N

1

).

Proof. Write H

2

z

) ⊖ N

1

= θH

2

z

) for some inner function θ. Let φ = φ

1

⊕ φ

2

⊕ θφ

3

∈ H

2

z

)

⊕ N

1

⊕ θH

2

z

).

It is easy to see that P

N1

( φ

1

(N

2

∩ H

z

)) )

⊂ N

2

and

P

N1

( θφ

3

(N

2

∩ H

z

)) )

= {0}.

(9)

Hence S

φ

N

2

⊂ N

2

if and only if P

N1

(

φ

2

(N

2

∩ H

z

)) )

⊂ N

2

. By Theorem 3.1, S

φ

N

2

⊂ N

2

if and only if

φ = φ

1

+ cP

N1

1 + θφ

3

= φ

1

+ c(1 − θ(0)θ) + θφ

3

= φ

1

+ c + θ(φ

3

− cθ(0)).

This completes the proof. □

The following corollaries follow from Corollary 3.4 directly.

Corollary 3.5. Let N

1

, N

2

be backward shift invariant subspaces of H

2

z

) with {0} ̸= N

2

⫋ N

1

̸= H

2

z

), and φ(z) ∈ H

z

). Then φN

2

⊂ N

2

(H

2

z

) ⊖ N

1

) if and only if φ ∈ C + (H

2

z

) ⊖ N

1

).

Corollary 3.6. Let N

1

, N

2

be backward shift invariant subspaces of H

2

z

) with {0} ̸= N

2

⊂ N

1

̸= H

2

z

), and φ(z) ∈ H

z

). If φN

2

⊂ N

2

⊕(H

2

z

) N

1

), then N

1

= N

2

if and only if φ / ∈ C + (H

2

z

) ⊖ N

1

).

Corollary 3.7. Let M

1

, M

2

be invariant subspaces of H

2

z

) with {0} ̸= M

1

M

2

̸= H

2

z

), and φ(z) ∈ H

z

). Then T

φ

(M

2

⊖ M

1

) ⊂ M

2

⊖ M

1

if and only if φ ∈ C + M

1

.

Corollary 3.8. Let M

1

, M

2

be invariant subspaces of H

2

z

) with {0} ̸= M

1

M

2

⊂ H

2

z

), and φ(z) ∈ H

z

). If T

φ

(M

2

⊖ M

1

) ⊂ M

2

⊖ M

1

, then φ / ∈ C + M

1

if and only if M

2

= H

2

z

).

4. The main theorem

As applications of the results in Sections 2 and 3, we prove the following.

Theorem 4.1. Let N be a backward shift invariant subspace of H

2

with N ̸=

{0} and N ̸= H

2

. Let φ(z) ∈ H

z

) be a nonconstant function. If [S

φ

, S

w

] = 0 and [S

z

, S

w

] ̸= 0, then φ(z) − c ∈ M ∩ H

z

) for some c ∈ C and S

φ

= cI.

Proof. By Lemma 2.3, M ∩ H

2

z

) = θ(z)H

2

z

) for a nonconstant inner function θ(z). Since θ(z)H

2

⊂ M, as in Section 2 we write

(4.1) M

θ

= M ⊖ θ(z)H

2

.

Since [S

z

, S

w

] ̸= 0, we have M

θ

̸= {0}. By Theorem 2.6,

(4.2) φ(z)N ⊂ N ⊕ θ(z)H

2

and

(4.3) T

φ

M

θ

⊂ M

θ

.

To prove the assertion, we assume that

(4.4) φ(z) − c /∈ θ(z)H

z

)

for every c ∈ C. We shall prove that [S

z

, S

w

] = 0. This will be a desired

contradiction. We consider two cases θ(0) = 0 and θ(0) ̸= 0 separately.

(10)

Case 1. Suppose that θ(0) = 0. If θ(z) = cz for some constant c with |c| = 1, then it is easy to see that

M = θ(z)H

2

+ q(w)H

2

for either a nonconstant inner function q(w) or q(w) = 0. In this case, by [6]

we have [S

z

, S

w

] = 0. So, we may assume that θ(z) = zθ

1

(z) for a nonconstant inner function θ

1

(z). Then

(4.5) H

2

⊖ θ(z)H

2

= H

2

w

) ⊕ z (

H

2

⊖ θ

1

(z)H

2

) . We divide the proof into two subcases.

Subcase 1.1. Assume that θ

1

(z)M

θ

⊂ θ(z)H

2

. Then M

θ

⊂ zH

2

. Hence H

2

w

) ⊂ N. For each nonnegative integer n, let

L

n

= {

f (z) ∈ H

2

z

) ⊖ θ(z)H

2

z

) : w

n

f (z) ∈ N } .

Then 1 ∈ L

n

, L

n

is a nonzero closed subspace of H

2

z

) ⊖ θ(z)H

2

z

), and T

z

L

n

⊂ L

n

. By (4.2),

w

n

φ(z)L

n

⊂ φ(z)N ⊂ N ⊕ θ(z)H

2

, so we have

φ(z)L

n

⊂ L

n

⊕ θ(z)H

2

z

).

By (4.4) and Corollary 3.6, L

n

= H

2

z

) ⊖ θ(z)H

2

z

). Hence w

n

(

H

2

z

) ⊖ θ(z)H

2

z

) )

⊂ N for every n ≥ 0. Therefore

H

2

⊖ θ(z)H

2

=

n=0

⊕w

n

(

H

2

z

) ⊖ θ(z)H

2

z

) )

⊂ N.

By (4.1), H

2

⊖θ(z)H

2

= M

θ

⊕N, so that M

θ

= {0}. This contradicts [S

z

, S

w

] ̸=

0.

Subcase 1.2. Assume that θ

1

(z)M

θ

̸⊂ θ(z)H

2

. By (4.5), for every g ∈ M

θ

we can write

(4.6) g = f

g

(w) ⊕ zh

g

(z, w),

where f

g

∈ H

2

w

) and h

g

∈ H

2

⊖ θ

1

(z)H

2

. Since θ

1

(z)M

θ

⊂ M, we have θ

1

(z)g = θ

1

(z)f

g

(w) ⊕ zθ

1

(z)h

g

(z, w) ∈ M = M

θ

⊕ θ(z)H

2

,

so that θ

1

(z)f

g

(w) ∈ M

θ

. Since θ

1

(z)M

θ

̸⊂ θ(z)H

2

, f

g

(w) ̸= 0 for some g ∈ M

θ

. Then {f

g

(w) : g ∈ M

θ

} ̸= {0}. Since wM

θ

⊂ M

θ

, by (4.6) {f

g

(w) : g ∈ M

θ

} is a nonzero T

w

-invariant subspace of H

2

w

). Hence there is a one variable inner function q(w) such that

(4.7) q(w)H

2

w

) = {f

g

(w) : g ∈ M

θ

}.

(11)

Since θ

1

(z) {f

g

(w) : g ∈ M

θ

} ⊂ M

θ

, we have (4.8) θ

1

(z)q(w)H

2

w

) ⊂ M

θ

. If q(w) is constant, then θ

1

(z) ∈ M

θ

and

θ(z)H

2

z

) ⫋ C · θ

1

(z) + θ(z)H

2

z

) ⊂ M ∩ H

2

z

),

so that θ(z)H

2

z

) ̸= M ∩ H

2

z

). This is a contradiction. Hence q(w) is nonconstant. By (4.6) and (4.7), we get

(4.9) (

H

2

w

) ⊖ q(w)H

2

w

) )

⊥ M

θ

. For each nonnegative integer n, let

L

n

= {

f (z) ∈ H

2

z

) ⊖ θ(z)H

2

z

) : f (z)w

n

q(w) ∈ M

θ

} .

By (4.8), θ

1

(z) ∈ L

n

. Since zM

θ

⊂ M

θ

⊕ θ(z)H

2

, L

n

⊕ θ(z)H

2

z

) is an invariant subspace of H

2

z

). By (4.3), we have T

φ

L

n

⊂ L

n

. By (4.4) and Corollary 3.8, L

n

= H

2

z

) ⊖ θ(z)H

2

z

). Hence

w

n

q(w) (

H

2

z

) ⊖ θ(z)H

2

z

) )

⊂ M

θ

for every n ≥ 0. Thus we get

(4.10) q(w) (

H

2

⊖ θ(z)H

2

)

⊂ M

θ

.

By (4.9), H

2

w

) ⊖q(w)H

2

w

) ⊂N. For each ψ(w)∈H

2

w

) ⊖q(w)H

2

w

), let

L

ψ

= {

f (z) ∈ H

2

z

) ⊖ θ(z)H

2

z

) : f (z)ψ(w) ∈ N } .

Then 1 ∈ L

ψ

, and in the same way as Subcase 1.1, L

ψ

is a nonzero closed subspace of H

2

z

) ⊖ θ(z)H

2

z

) such that T

z

L

ψ

⊂ L

ψ

and φ(z)L

ψ

⊂ L

ψ

θ(z)H

2

z

). Hence by (4.4) and Corollary 3.6, L

ψ

= H

2

z

) ⊖ θ(z)H

2

z

).

Therefore

ψ(w) (

H

2

z

) ⊖ θ(z)H

2

z

) )

⊂ N for every ψ(w) ∈ H

2

w

) ⊖ q(w)H

2

w

), and hence

(4.11) (

H

2

⊖ θ(z)H

2

)

⊖ q(w) (

H

2

⊖ θ(z)H

2

)

⊂ N.

Since H

2

⊖ θ(z)H

2

= M

θ

⊕ N, by (4.10) and (4.11) we get N = (

H

2

⊖ θ(z)H

2

)

⊖ q(w) (

H

2

⊖ θ(z)H

2

) . By [6], this shows that [S

z

, S

w

] = 0.

Case 2. Suppose that θ(0) ̸= 0. Let φ

(z) = φ(z) − ⟨φ, θ⟩θ(z). Then S

φ

= S

φ

, so that we may assume that φ ⊥ θ. Write

(4.12) φ(z) = φ

1

(z) + θ(z)zφ

2

(z),

where φ

1

∈ H

2

z

) ⊖ θH

2

z

) and φ

2

∈ H

2

z

). By (4.4), φ

1

(z) ̸= 0. Since θ(0) ̸= 0, T

z

φ

1

(z) ̸= 0. For each h ∈ N, by (4.2) we can write

φh = f

h

+ θg

h

∈ N ⊕ θH

2

.

(12)

Applying T

z

for the both side of the above, we have

φT

z

h + h(0, w)T

z

φ = T

z

f

h

+ g(0, w)T

z

θ + θT

z

g

h

. Hence by (4.12),

φT

z

h = −h(0, w)T

z

φ + T

z

f

h

+ g

h

(0, w)T

z

θ + θT

z

g

h

= −h(0, w)T

z

φ

1

+ T

z

f

h

+ g

h

(0, w)T

z

θ + θ(T

z

g

h

− h(0, w)φ

2

).

Note that

−h(0, w)T

z

φ

1

+ T

z

f

h

+ g

h

(0, w)T

z

θ ⊥ θH

2

. Since h ∈ N, we have T

z

h ∈ N, so that by (4.2) we have

−h(0, w)T

z

φ

1

+ T

z

f

h

+ g

h

(0, w)T

z

θ ∈ N.

Since f

h

∈ N, also we have T

z

f

h

∈ N and

(4.13) −h(0, w)T

z

φ

1

+ g

h

(0, w)T

z

θ ∈ N.

Write

Θ(z) = θ

2

(z) − θ(0)θ(z).

We have

T

θθ−θ(0)z

T

z

= T

θ2−θ(0)θ

= T

Θ

. Since

T

θθ−θ(0)z

N ⊂ N,

−h(0, w) (

T

Θ

φ

1

+ aT

Θ

θ )

+ g(0, w)T

Θ

θ ∈ N.

Since φ

1

∈ N ⊂ H

2

⊖ θH

2

, we have T

Θ

φ

1

= 0. Since T

Θ

θ = −θ(0), we get aθ(0)h(0, w) − θ(0)g(0, w) ∈ N.

Since θ(0) ̸= 0,

ah(0, w) − g(0, w) ∈ N.

Thus we get

ah(0, w) − g(0, w) ⊥ θ(z)H

2

.

Because θ(0) ̸= 0, we have ah(0, w) − g(0, w) = 0. Hence by (4.9),

−h(0, w)T

z

φ

1

(z) ∈ N.

Note that T

z

φ

1

(z) ̸= 0. In the same way as Subcase 1.2, h(0, w) (

H

2

z

) ⊖ θ(z)H

2

z

) )

⊂ N ⊂ H

2

⊖ θ(z)H

2

for every h ∈ N. Since T

w

N ⊂ N and N ̸= {0}, {h(0, w) : h ∈ N} is a nontrivial T

w

-invariant subspace of H

2

w

), so that

{h(0, w) : h ∈ N} = H

2

w

) ⊖ q(w)H

2

w

) for either nontrivial inner function q(w) or q(w) = 0. Hence

(H

2

⊖ θ(z)H

2

) ⊖ q(w)(H

2

⊖ θ(z)H

2

) ⊂ N.

(13)

For every f ∈ N, write

f =

n=0

⊕f

n

(w)z

n

.

Since T

z

N ⊂ N, f

n

(w) ∈ H

2

w

) ⊖ q(w)H

2

w

) for every n ≥ 0. Hence N ⊂ (H

2

⊖ θ(z)H

2

) ⊖ q(w)(H

2

⊖ θ(z)H

2

).

Therefore

N = (H

2

⊖ θ(z)H

2

) ⊖ q(w)(H

2

⊖ θ(z)H

2

).

This shows that [S

z

, S

w

] = 0. This completes the proof. □ References

[1] H. Bercovici, Operator Theory and Arithmetic in H, Mathematical Surveys and Mono- graphs, 26. American Mathematical Society, Providence, RI, 1988.

[2] A. Beurling, On two problems concerning linear transformations in Hilbert space, Acta Math. 81 (1948), 239–255.

[3] X. Chen and K. Guo, Analytic Hilbert Modules, Chapman & Hall/CRC, Boca Raton, FL, 2003.

[4] K. J. Izuchi and K. H. Izuchi, Commutativity in two variable Jordan blocks on the Hardy space, preprint.

[5] , Cross commutators on backward shift invariant subspaces over the bidisk, Acta Sci. Math. (Szeged) 72 (2006), no. 1-2, 251–270.

[6] K. J. Izuchi, T. Nakazi, and M. Seto, Backward shift invariant subspaces in the bidisc.

II, J. Operator Theory 51 (2004), no. 2, 361–376.

[7] , Backward shift invariant subspaces in the bidisc. III, Acta Sci. Math. (Szeged) 70 (2004), no. 3-4, 727–749.

[8] V. Mandrekar, The validity of Beurling theorems in polydiscs, Proc. Amer. Math. Soc.

103 (1988), no. 1, 145–148.

[9] N. Nikol’skiˇi, Treatise on the Shift Operator, Springer-Verlag, Berlin, 1986.

[10] W. Rudin, Function Theory in Polydiscs, Benjamin, New York, 1969.

[11] R. Schneider, Isometries of Hp(Un), Canad. J. Math. 25 (1973), 92–95.

Kei Ji Izuchi

Department of Mathematics Niigata University

Niigata 950-2181, Japan

E-mail address: [email protected]

Kou Hei Izuchi Faculty of Education Yamaguchi University Yamaguchi 753-8513, Japan

E-mail address: [email protected]

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