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, S∗w] = 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, S∗w] = 0 and φ∈ H∞(Γz), then Sφ= cI for some c∈ C.
1. Introduction
Let Γ
2be 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(Γ
2) be the usual Lebesgue space on Γ
2with the norm
∥f∥
2= ( ∫
2π0
∫
2π 0|f(e
is, e
it) |
2dsdt (2π)
2)
1/2.
With the usual inner product, L
2is a Hilbert space. Let H
2= H
2(Γ
2) be the Hardy space over Γ
2. We denote by H
2(Γ
z) and H
2(Γ
w) the Hardy spaces on the unit circle Γ in variables z and w, respectively. We think of H
2(Γ
z) and H
2(Γ
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(Γ
w).
Let P be the orthogonal projection from L
2onto H
2. For a closed subspace M of L
2, we denote by P
Mthe orthogonal projection from L
2onto M . For a function ψ ∈ L
∞, the Toeplitz operator T
ψon H
2is defined by T
ψf = 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
∞(Γ
z) and ψ(w) ∈ H
∞(Γ
w). A function f ∈ H
2is called inner if |f| = 1 on Γ
2almost everywhere. A nonzero closed subspace M of H
2is
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
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(Γ
z) has a form M = q(z)H
2(Γ
z), where q(z) is an inner function. In two variable case, the structure of invariant subspaces of H
2is extremely complicated, see [3, 10].
Let M be an invariant subspace of H
2with 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
ψthe operator on M defined by R
ψf = P
M(ψf ) for f ∈ M. It holds R
∗ψ= R
ψand R
z= T
z|
M. We denote by [R
z, R
∗w] the cross commutator of R
zand R
w, that is, [R
z, R
∗w] = R
zR
∗w− R
∗wR
z. In [8], Mandrekar proved that [R
z, R
∗w] = 0 if and only if M is Beurling type, that is, M = qH
2for 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
∗ψ2(w)
] = 0 for nonconstant functions ψ
1(z), ψ
2(w) ∈ H
∞(Γ).
We define the operator S
ψon N by S
ψf = P
N(ψf ) for f ∈ N. Then we have S
ψ∗= S
ψand 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
znS
w∗= 0,
(iii) there exists a Blaschke product b(z) with b(z) =
∏
n j=1z − α
j1 − α
jz , 0 < |α
j| < 1,
where α
i̸= α
jfor every i, j with i ̸= j and α
n1= α
n2= · · · = α
nnsuch 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(Γ
z) or N ⊂ H
2⊖ z
nH
2. If N ⊂ H
2(Γ
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
∞(Γ
z) = θ(z)H
∞(Γ
z) for an inner function θ(z), and z
n∈ C + θ(z)H
∞(Γ
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
∞(Γ
z) be a nonconstant function. Suppose that [S
φ(z), S
w∗] = 0 and
[S
z, S
w∗] ̸= 0. In Section 2, we prove that M ∩H
∞(Γ
z) ̸= {0} and M ∩H
2(Γ
z) ̸=
H
2(Γ
z). Hence by the Beurling theorem, M ∩ H
2(Γ
z) = θ(z)H
2(Γ
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
θ̸= {0} and T
φ(z)∗M
θ⊂ M
θ. In another word, φ(z)N ⊂ N ⊕ θ(z)H
2holds. In Section 3, we study on the one variable Hardy space H
2(Γ
z). Let N
1, N
2be backward shift invariant subspaces of H
2(Γ
z) satisfying {0} ̸= N
2⫋ N
1̸= H
2(Γ
z). It is proved that φ(z)N
2⊂ N
2⊕ (H
2(Γ
z) ⊖ N
1) if and only if φ(z) ∈ C+(H
2(Γ
z) ⊖N
1). As applications of these facts, in Section 4 we prove that φ(z) ∈ C + θ(z)H
∞(Γ
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
2with N ̸= {0} and N ̸=
H
2, and let φ(z) ∈ H
∞(Γ
z) be a nonconstant function. We write operators T
φand T
w∗on H
2= M ⊕ N in the matrix forms as
T
φ=
( ∗ P
MT
φ|
N0 S
φ)
, T
w∗=
( ∗ 0
P
NT
w∗|
MS
∗w)
on H
2=
M
⊕ N
.
Let
A = P
MT
φ|
Nand B = P
NT
w∗|
M. Since T
φT
w∗= T
w∗T
φon H
2, we have
S
φS
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(Γ
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(Γ
z) )
⊕ wM.
Lemma 2.3. If [S
φ, S
w∗] = 0 and [S
z, S
w∗] ̸= 0, then M ∩H
2(Γ
z) is a nontrivial
invariant subspace of H
2(Γ
z).
Proof. Since M ̸= H
2, trivially M ∩ H
2(Γ
z) ̸= H
2(Γ
z) holds. Suppose that M ∩ H
2(Γ
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
wT
φ∗= T
φ∗T
won H
2, if f ∈ M and T
φ∗f ∈ M, then T
φ∗(w
nf ) = w
nT
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
∞(Γ
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
∞(Γ
z). Let
L = {
f (z) ∈ H
1(Γ
z) :
∫
2π 0f (e
iθ)ψ(e
iθ) dθ
2π = 0 for every ψ(z) ∈ A } . Then L is a closed subspace of H
1(Γ
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(Γ
z) for an inner function q(z). Since 1 ∈ A, q(0) = 0. Hence zq(z) ∈ H
∞(Γ
z). Since φ(z)
n∈ A for n ≥ 1,
∫
2π 0e
−iθq(e
iθ)φ(e
iθ)
ne
iθh(e
iθ) dθ 2π =
∫
2π 0q(e
iθ)h(e
iθ)φ(e
iθ)
ndθ 2π = 0 for every h(z) ∈ H
1(Γ
z). Hence zq(z)φ(z)
n∈ H
∞(Γ
z) for every n ≥ 1. By the Schneider theorem [11], we have φ(z) ∈ H
∞(Γ
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
∞(Γ
z). Especially, we have z ∈ A and zN ⊂ N. Then T
z|
N= S
z. Since T
w∗|
N= S
w∗and T
zT
w∗= T
w∗T
zon H
2, we have S
zS
w∗= S
w∗S
z. This is a desired contradiction. □ In the rest of this section, we assume that M ∩H
2(Γ
z) ̸= {0}. Since M ̸= H
2, M ∩ H
2(Γ
z) ̸= H
2(Γ
z). By the Beurling theorem,
M ∩ H
2(Γ
z) = θ(z)H
2(Γ
z)
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
2and H
2⊖ θ(z)H
2= M
θ⊕ N.
By the definition of M
θ, we have wM
θ⊂ M
θand M
θ∩ H
2(Γ
z) = {0}. Note that if [S
φ, S
w∗] = 0 and [S
z, S
w∗] ̸= 0, then M
θ̸= {0}. For, if M
θ= {0}, then M = θ(z)H
2and 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
θif 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(Γ
z) = {0}, f(z, 0) = 0. Hence
f ∈ wM
θ. The converse is trivial. □
Let P
θbe the orthogonal projection from H
2onto H
2⊖ θ(z)H
2, and Q
φbe the operator on H
2⊖ θ(z)H
2defined by Q
φf = P
θ(φf ) for f ∈ H
2⊖ θ(z)H
2. We can write both operators Q
φand T
w∗|
(H2⊖θH2)as
Q
φ=
( ∗ P
MθT
φ|
N0 S
φ)
on H
2⊖ θ(z)H
2=
M
θ⊕ N
and
T
w∗|
(H2⊖θH2)=
( ∗ 0
P
NT
w∗|
MθS
w∗)
on H
2⊖ θ(z)H
2=
M
θ⊕ N
.
Let
A
θ= P
MθT
φ|
Nand B
θ= P
NT
w∗|
Mθ. Lemma 2.5. [S
φ, S
w∗] = 0 if and only if B
θA
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
φf ⊕ f
1∈ (M
θ⊕ N) ⊕ θ(z)H
2.
Since T
w∗f
1∈ θ(z)H
2and T
w∗(Q
φf ) ⊥ θ(z)H
2, we get T
w∗Q
φf = Q
φT
w∗f . Thus Q
φT
w∗= T
w∗Q
φon 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,
(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
nT
φ(z)∗(M
θ⊖ wM
θ) ⊂ w
nM
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
2and 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
∞(Γ
z) satisfies the above condition. In the next section, we study a similar question in the one variable Hardy space H
2(Γ
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
2be backward shift invariant subspaces of H
2(Γ
z) with 0 ̸= N
2⫋ N
1̸= H
2(Γ
z), and φ(z) ∈ N
1. Then
φ(N
2∩ H
∞(Γ
z)) ⊂ N
2⊕ (H
2(Γ
z) ⊖ N
1)
if and only if φ(z) = cP
N11 for some c ∈ C. In this case, if we define the operator S
φon N
1by S
φf = 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(Γ
z). Then N ∩ H
∞(Γ
z) is dense in N .
Lemma 3.3. Let N be a backward shift invariant subspace of H
2(Γ
z) with N ̸= {0} and N ̸= H
2(Γ
z). If φ ∈ H
2(Γ
z) is a nonconstant function, then φ (
N ∩ H
∞(Γ
z) )
̸⊂ N.
Proof of Theorem 3.1. By the Beurling theorem, H
2(Γ
z) ⊖ N
1= θH
2(Γ
z) for some nonconstant inner function θ.
First, suppose that
φ(N
2∩ H
∞(Γ
z)) ⊂ N
2⊕ (H
2(Γ
z) ⊖ N
1).
Since N
2̸= {0}, by Lemma 3.2 there exists h
1∈ N
2∩ H
∞(Γ
z) with h
1(0) = 1.
Write
(3.1) φh
1= f
1⊕ θg
1∈ N
2⊕ (
H
2(Γ
z) ⊖ N
1) = N
2⊕ θH
2(Γ
z).
Also for each h ∈ N
2∩ H
∞(Γ
z), we can write
(3.2) φh = f ⊕ θg ∈ N
2⊕ θH
2(Γ
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
∞(Γ
z) and T
z∗f + g(0)T
z∗θ ⊥ θH
2(Γ
z). By the assump- tion, φT
z∗h ∈ N
2⊕ θH
2(Γ
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(Γ
z) ⊖ θH
2(Γ
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(Γ
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
∞(Γ
z) and φ ⊥ θH
2(Γ
z), by the assumption we have
−h(0)T
z∗φ + T
z∗f + g(0)T
z∗θ ∈ N
2.
Similarly we have φT
z∗2h =
( − (T
z∗h)(0)T
z∗φ − h(0)T
z∗2φ + T
z∗2f + g(0)T
z∗2θ
+(T
z∗g)(0)T
z∗θ
) ⊕ θT
z∗2g.
Repeating the same argument, we get φT
z∗nh =
[ − (
n∑
−1j=0
( T
z∗(n−j−1)h )
(0)T
z∗(j+1)φ )
+ T
z∗nf
+ (
n∑
−1j=0
(T
z∗jg)(0)T
z∗(n−j)θ
)] ⊕ θT
z∗ng.
Since h ∈ N
2∩ H
∞(Γ
z), T
z∗nh ∈ N
2∩ H
∞(Γ
z). Hence by (3.2) and (3.4), (T
z∗ng)(0) = (T
z∗nh)(0)g
1(0)
for every n ≥ 0. This shows that g = g
1(0)h. By (3.2), we obtain (φ − g
1(0)θ)h = f ∈ N
2for every h ∈ N
2∩ H
∞(Γ
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
N11.
Next, suppose that φ = cP
N11. Then
φ = cP
N11 = c(1 − θ(0)θ).
Hence for f ∈ N
2∩ H
∞(Γ
z), we have
φf = cf − cθ(0)θf ∈ N
2⊕ θH
2(Γ
z).
Thus we get φ (
N
2∩ H
∞(Γ
z) )
⊂ N
2⊕ (H
2(Γ
z) ⊖ N
1). □ Corollary 3.4. Let N
1, N
2be backward shift invariant subspaces of H
2(Γ
z) with {0} ̸= N
2⫋ N
1̸= H
2(Γ
z), and φ(z) ∈ L
∞(Γ
z). Define the operator S
φon N
1by S
φh = P
N1(φh) for h ∈ N
1. Then S
φN
2⊂ N
2if and only if φ ∈ C + H
2(Γ
z)
⊥+ (H
2(Γ
z) ⊖ N
1) = H
2(Γ
z) + (H
2(Γ
z) ⊖ N
1).
Proof. Write H
2(Γ
z) ⊖ N
1= θH
2(Γ
z) for some inner function θ. Let φ = φ
1⊕ φ
2⊕ θφ
3∈ H
2(Γ
z)
⊥⊕ N
1⊕ θH
2(Γ
z).
It is easy to see that P
N1( φ
1(N
2∩ H
∞(Γ
z)) )
⊂ N
2and
P
N1( θφ
3(N
2∩ H
∞(Γ
z)) )
= {0}.
Hence S
φN
2⊂ N
2if and only if P
N1(
φ
2(N
2∩ H
∞(Γ
z)) )
⊂ N
2. By Theorem 3.1, S
φN
2⊂ N
2if and only if
φ = φ
1+ cP
N11 + 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
2be backward shift invariant subspaces of H
2(Γ
z) with {0} ̸= N
2⫋ N
1̸= H
2(Γ
z), and φ(z) ∈ H
∞(Γ
z). Then φN
2⊂ N
2⊕ (H
2(Γ
z) ⊖ N
1) if and only if φ ∈ C + (H
2(Γ
z) ⊖ N
1).
Corollary 3.6. Let N
1, N
2be backward shift invariant subspaces of H
2(Γ
z) with {0} ̸= N
2⊂ N
1̸= H
2(Γ
z), and φ(z) ∈ H
∞(Γ
z). If φN
2⊂ N
2⊕(H
2(Γ
z) ⊖ N
1), then N
1= N
2if and only if φ / ∈ C + (H
2(Γ
z) ⊖ N
1).
Corollary 3.7. Let M
1, M
2be invariant subspaces of H
2(Γ
z) with {0} ̸= M
1⫋ M
2̸= H
2(Γ
z), and φ(z) ∈ H
∞(Γ
z). Then T
φ∗(M
2⊖ M
1) ⊂ M
2⊖ M
1if and only if φ ∈ C + M
1.
Corollary 3.8. Let M
1, M
2be invariant subspaces of H
2(Γ
z) with {0} ̸= M
1⫋ M
2⊂ H
2(Γ
z), and φ(z) ∈ H
∞(Γ
z). If T
φ∗(M
2⊖ M
1) ⊂ M
2⊖ M
1, then φ / ∈ C + M
1if and only if M
2= H
2(Γ
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
2with N ̸=
{0} and N ̸= H
2. Let φ(z) ∈ H
∞(Γ
z) be a nonconstant function. If [S
φ, S
w∗] = 0 and [S
z, S
w∗] ̸= 0, then φ(z) − c ∈ M ∩ H
∞(Γ
z) for some c ∈ C and S
φ= cI.
Proof. By Lemma 2.3, M ∩ H
2(Γ
z) = θ(z)H
2(Γ
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
θ̸= {0}. By Theorem 2.6,
(4.2) φ(z)N ⊂ N ⊕ θ(z)H
2and
(4.3) T
φ∗M
θ⊂ M
θ.
To prove the assertion, we assume that
(4.4) φ(z) − c /∈ θ(z)H
∞(Γ
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.
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
2for 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(Γ
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(Γ
w) ⊂ N. For each nonnegative integer n, let
L
n= {
f (z) ∈ H
2(Γ
z) ⊖ θ(z)H
2(Γ
z) : w
nf (z) ∈ N } .
Then 1 ∈ L
n, L
nis a nonzero closed subspace of H
2(Γ
z) ⊖ θ(z)H
2(Γ
z), and T
z∗L
n⊂ L
n. By (4.2),
w
nφ(z)L
n⊂ φ(z)N ⊂ N ⊕ θ(z)H
2, so we have
φ(z)L
n⊂ L
n⊕ θ(z)H
2(Γ
z).
By (4.4) and Corollary 3.6, L
n= H
2(Γ
z) ⊖ θ(z)H
2(Γ
z). Hence w
n(
H
2(Γ
z) ⊖ θ(z)H
2(Γ
z) )
⊂ N for every n ≥ 0. Therefore
H
2⊖ θ(z)H
2=
∑
∞ n=0⊕w
n(
H
2(Γ
z) ⊖ θ(z)H
2(Γ
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
θ̸⊂ θ(z)H
2. By (4.5), for every g ∈ M
θwe can write
(4.6) g = f
g(w) ⊕ zh
g(z, w),
where f
g∈ H
2(Γ
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
θ̸⊂ 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(Γ
w). Hence there is a one variable inner function q(w) such that
(4.7) q(w)H
2(Γ
w) = {f
g(w) : g ∈ M
θ}.
Since θ
1(z) {f
g(w) : g ∈ M
θ} ⊂ M
θ, we have (4.8) θ
1(z)q(w)H
2(Γ
w) ⊂ M
θ. If q(w) is constant, then θ
1(z) ∈ M
θand
θ(z)H
2(Γ
z) ⫋ C · θ
1(z) + θ(z)H
2(Γ
z) ⊂ M ∩ H
2(Γ
z),
so that θ(z)H
2(Γ
z) ̸= M ∩ H
2(Γ
z). This is a contradiction. Hence q(w) is nonconstant. By (4.6) and (4.7), we get
(4.9) (
H
2(Γ
w) ⊖ q(w)H
2(Γ
w) )
⊥ M
θ. For each nonnegative integer n, let
L
n= {
f (z) ∈ H
2(Γ
z) ⊖ θ(z)H
2(Γ
z) : f (z)w
nq(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(Γ
z) is an invariant subspace of H
2(Γ
z). By (4.3), we have T
φ∗L
n⊂ L
n. By (4.4) and Corollary 3.8, L
n= H
2(Γ
z) ⊖ θ(z)H
2(Γ
z). Hence
w
nq(w) (
H
2(Γ
z) ⊖ θ(z)H
2(Γ
z) )
⊂ M
θfor every n ≥ 0. Thus we get
(4.10) q(w) (
H
2⊖ θ(z)H
2)
⊂ M
θ.
By (4.9), H
2(Γ
w) ⊖q(w)H
2(Γ
w) ⊂N. For each ψ(w)∈H
2(Γ
w) ⊖q(w)H
2(Γ
w), let
L
ψ= {
f (z) ∈ H
2(Γ
z) ⊖ θ(z)H
2(Γ
z) : f (z)ψ(w) ∈ N } .
Then 1 ∈ L
ψ, and in the same way as Subcase 1.1, L
ψis a nonzero closed subspace of H
2(Γ
z) ⊖ θ(z)H
2(Γ
z) such that T
z∗L
ψ⊂ L
ψand φ(z)L
ψ⊂ L
ψ⊕ θ(z)H
2(Γ
z). Hence by (4.4) and Corollary 3.6, L
ψ= H
2(Γ
z) ⊖ θ(z)H
2(Γ
z).
Therefore
ψ(w) (
H
2(Γ
z) ⊖ θ(z)H
2(Γ
z) )
⊂ N for every ψ(w) ∈ H
2(Γ
w) ⊖ q(w)H
2(Γ
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(Γ
z) ⊖ θH
2(Γ
z) and φ
2∈ H
2(Γ
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.
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
θ∗2−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(Γ
z) ⊖ θ(z)H
2(Γ
z) )
⊂ N ⊂ H
2⊖ θ(z)H
2for 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(Γ
w), so that
{h(0, w) : h ∈ N} = H
2(Γ
w) ⊖ q(w)H
2(Γ
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.
For every f ∈ N, write
f =
∑
∞ n=0⊕f
n(w)z
n.
Since T
z∗N ⊂ N, f
n(w) ∈ H
2(Γ
w) ⊖ q(w)H
2(Γ
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
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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]