This paper introduces a new domain called the extended symmetrized polydisc, characterizes points within it and the original symmetrized polydisc, and explores their geometric properties, revealing differences and similarities for various dimensions.
Contribution
The paper provides new characterizations of the symmetrized polydisc and introduces the extended symmetrized polydisc, establishing their relationship and geometric properties.
Findings
01
G_n= ilde{\u00a0G}_n for n=1,2
02
G_n is a proper subset of ilde{\u00a0G}_n for n
03
ilde{\u00a0G}_n is non-convex but polynomially convex, starlike about the origin, not circled
Abstract
We find new characterizations for the points in the \textit{symmetrized polydisc} Gnβ, a family of domains associated with the spectral interpolation, defined by \[ \mathbb G_n :=\left\{ \left(\sum_{1\leq i\leq n} z_i,\sum_{1\leq i<j\leq n}z_iz_j \dots, \prod_{i=1}^n z_i \right): \,|z_i|<1, i=1,\dots,n \right \}. \] We introduce a new family of domains which we call \textit{the extended symmetrized polydisc} Gnβ, and define in the following way: \begin{align*} \widetilde{\mathbb G}_n := \Bigg\{ (y_1,\dots,y_{n-1}, q)\in \mathbb C^n :\; q \in \mathbb D, \; y_j = \beta_j + \bar{\beta}_{n-j} q, \; \beta_j \in \mathbb C &\text{ and }\\ |\beta_j|+ |\beta_{n-j}| < {n \choose j} &\text{ for } j=1,\dots, n-1 \Bigg\}. \end{align*} We show that Gnβ=Gnβ for n=1,2 and that GnββGnβ for $n\geqβ¦
\displaystyle\widetilde{\mathbb{G}}_{n}:=\Bigg{\{}(y_{1},\dots,y_{n-1},q)\in\mathbb{C}^{n}:|q|<1,\>y_{j}=\beta_{j}+\bar{\beta}_{n-j}q\>\text{ with }\;|\beta_{j}|
\displaystyle\widetilde{\mathbb{G}}_{n}:=\Bigg{\{}(y_{1},\dots,y_{n-1},q)\in\mathbb{C}^{n}:|q|<1,\>y_{j}=\beta_{j}+\bar{\beta}_{n-j}q\>\text{ with }\;|\beta_{j}|
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Characterizations of the symmetrized polydisc via another family of domains
Sourav Pal
Mathematics Department, Indian Institute of Technology Bombay, Powai, Mumbai - 400076, India.
We find new characterizations for the points in the symmetrized polydiscGnβ, a family of domains associated with the spectral interpolation, defined by
[TABLE]
We introduce a new family of domains which we call the extended symmetrized polydiscGnβ, and define in the following way:
[TABLE]
We show that Gnβ=Gnβ for n=1,2 and that GnββGnβ for nβ₯3. We first obtain a variety of characterizations for the points in Gnβ and we apply these necessary and sufficient conditions to produce an analogous set of characterizations for the points in Gnβ. Also we obtain similar characterizations for the points in ΞnββGnβ, where Ξnβ=Gnββ. A set of nβ1 fractional linear transformations play central role in the entire program. We also show that for nβ₯2, Gnβ is non-convex but polynomially convex and is starlike about the origin but not circled.
The named author was supported by the Seed Grant of IIT Bombay, the CPDA of Govt. of India, the INSPIRE Faculty Award (Award No. DST/INSPIRE/04/2014/001462) of DST, India and the MATRICS Award of SERB, (Award No. MTR/2019/001010) of DST, India. The second named author was supported by a Ph.D fellowship from the University Grand Commission of India.
1. Introduction
The following notations and terminologies will be used throughout the paper. We denote by R and C the sets of real
numbers and complex numbers respectively. By D and
T we mean the open unit disc and
the unit circle respectively with centre at the origin of C. We follow the standard convention to denote by MmΓnβ(C) (or CmΓn) the space
of all mΓn complex matrices and Mnβ(C)
is used when m=n. For a matrix AβMnβ(C),
β₯Aβ₯ is the operator norm of A. Also, the spectrum and the spectral radius of a bounded operator T are
denoted by Ο(T) and r(T) respectively.
In this article, we contribute to the understanding of the geometry of the symmetrized polydisc Gnβ by producing a set of necessary and sufficient conditions each of which characterizes a point in Gnβ, where Gnβ is the following family of domains:
[TABLE]
This family of domains {Gnβ} is naturally associated with the spectral Nevanlinna-Pick interpolation in the following way: a matrix T belongs to the spectral unit ball Bn1ββMnβ(C), i.e., r(T)<1 if and only if
Οnβ(ΞΎ1β,β¦,ΞΎnβ)βGnβ (see
[17]). Here ΞΎ1β,β¦,ΞΎnβ are the
eigenvalues of T and Οnβ is the symmetrization map on
Cn defined by
[TABLE]
For given distinct points Ξ·1β,β¦,Ξ·kβ in D and matrices T1β,β¦,TkββBn1β, the spectral Nevanlinna-Pick interpolation seeks necessary and sufficient conditions under which there exists an analytic function F:DβMnβ(C) that interpolates the data, that is, F(Ξ·iβ)=Tiβ for i=1,β¦,k. Apart from the derogatory matrices, the nΓn spectral Nevanlinna-Pick problem is equivalent to a similar interpolation problem for the symmetrized polydisc Gnβ (see [6], Theorem 2.1). Note that a bounded domain like Gnβ, which has complex-dimension n, is much easier to deal with than an unbounded n2-dimensional object like Bn1β. The symmetrized polydisc has attracted considerable attention in past two decades because of its rich function theory [3, 13, 19, 25, 29, 30], elegent complex geometry [4, 9, 10, 16, 18, 20, 21, 22] and associated operator theory [5, 8, 11, 12, 14, 23, 24, 28] (also see references there in). It is evident from the definition that G1β=D which is convex but for nβ₯2, Gnβ is non-convex but polynomially convex (see [5, 18]).
The symmetrized polydisc Gnβ and its closure Ξnβ are the image of polydisc Dn and the closed polydisc Dn respectively under the symmetrization map Οnβ. We obtain from the literature (see [17, 18]) that
[TABLE]
In [17], Costara describe the points in Gnβ and Ξnβ in the following way:
[TABLE]
[TABLE]
Taking cue from Costaraβs characterization, we introduce a new family of domains, namely the extended symmetrized polydiscGnβ, which we define in the following way:
[TABLE]
It is obvious that if (s1β,β¦,snβ1β,p)βGnβ, then β£siββ£<(inβ). So, if (Ξ²1β,β¦,Ξ²nβ1β)βGnβ1β,
then β£Ξ²jββ£+β£Ξ²nβjββ£<(jnβ1β)+(nβjnβ1β)=(jnβ). Therefore, it follows that GnββGnβ. It is evident that G1ββ=G1β=D and we shall prove that G2ββ=G2β and that GnββGnββ for nβ₯3. We first characterize the points in Gnβ and its closure Ξnβ in several different ways. Then we use these characterizations to obtain analogous characterizations for the points in Gnβ and its closure Ξnβ. To characterize the points in Gnβ and Ξnβ, we introduce nβ1 fractional linear transformations Ξ¦1β,β¦,Ξ¦nβ1β, which play pivotal role in this paper. Also we show that Ξnβ is neither convex nor circled but polynomially convex and starlike and hence is simply connected.
Note. This article is a part of authorsβ unpublished note [26]. The techniques that are employed in the proofs of Theorems 2.2 and 2.4 are generalization in several variables of the techniques that are used in the article [2].
2. Characterizations of the points in Gnβ and Ξnβ
For characterizing the points in Gnβ and Ξnββ, we introduce (nβ1) fractional linear transformations Ξ¦1β,β¦,Ξ¦nβ1β in the following way.
Definition 2.1**.**
For zβC, y=(y1β,β¦,ynβ1β,q)βCn and for any jβ{1,β¦,nβ1},
let us define a meromorphic map
[TABLE]
and
[TABLE]
where Hβ denotes the Banach space of bounded complex-valued analytic functions on D equipped with supremum norm.
Needless to mention that for a fixed y=(y1β,β¦,ynβ1β,q)βCn, the function Ξ¦jβ(.,y) is a MΓΆbius transformation. It is evident from the definition that Ξ¦jβ(.,y)=Ξ¦nβjβ(.,y~β),
where
[TABLE]
which is obtained by interchanging the i-th and the j-th coordinates of y. It can be shown by a few steps of calculations that if β£ynβjββ£ξ =(jnβ), then the image set Ξ¦jβ(T,y) is a circle whose center and radius are
[TABLE]
respectively. If β£ynβjββ£<(jnβ), then Ξ¦jβ(.,y) is bounded on D. By the maximum modulus principle, the set Ξ¦jβ(D,y) must be lying inside the circle Ξ¦jβ(T,y) for that jβ{1,β¦,nβ1}. Now by continuity of the function Ξ¦jβ(.,y), the set Ξ¦jβ(D,y) is the open disc with boundary Ξ¦jβ(T,y). Hence for a point y=(y1β,β¦,ynβ1β,q)βCn and jβ{1,β¦,nβ1} if β£ynβjββ£<(jnβ), then the function Ξ¦jβ(.,y) maps D to the open disc with center and radius as in (2.3). Note that the point of maximum modulus of a closed disc with center a and radius r has modulus β£aβ£+r. Hence
[TABLE]
2.1. Characterizations for the points in Gnβ
Being armed with the functions Ξ¦jββs and Djββs, we now characterize the points in Gnβ.
Theorem 2.2**.**
For a point y=(y1β,β¦,ynβ1β,q)βCn, the following are equivalent:
(1)
yβGnβ;
2. (2)
(jnβ)βyjβzβynβjβw+(jnβ)qzwξ =0, for all z,wβD and for all j=1,β¦,[2nβ];
3. (3)
for all j=1,β¦,[2nβ],
[TABLE]
4. (3β²)
for all j=1,β¦,[2nβ],
[TABLE]
5. (4)
for all j=1,β¦,[2nβ],
[TABLE]
6. (4β²)
for all j=1,β¦,[2nβ],
[TABLE]
7. (5)
for all j=1,β¦,[2nβ],
[TABLE]
8. (5β²)
for all j=1,β¦,[2nβ],
[TABLE]
9. (6)
β£qβ£<1* and β£yjββ£2+β£ynβjββ£2β(jnβ)2β£qβ£2+2βyjβynβjββ(jnβ)2qβ<(jnβ)2 for all j=1,β¦,[2nβ];*
10. (7)
β£ynβjββyΛβjβqβ£+β£yjββyΛβnβjβqβ£<(jnβ)(1ββ£qβ£2)* for all j=1,β¦,[2nβ];*
11. (8)
there exist [2nβ] number of 2Γ2 matrices B1β,β¦,B[2nβ]β such that β₯Bjββ₯<1, yjβ=(jnβ)[Bjβ]11β, ynβjβ=(jnβ)[Bjβ]22β for all j=1,β¦,[2nβ] and
[TABLE]
12. (9)
there exist [2nβ] number of 2Γ2 symmetric matrices B1β,β¦,B[2nβ]β such that β₯Bjββ₯<1, yjβ=(jnβ)[Bjβ]11β, ynβjβ=(jnβ)[Bjβ]22β for all j=1,β¦,[2nβ] and
[TABLE]
Proof.
First we prove the equivalence of the conditions (2)β(6) and (8),(9).
Case-A: We first consider the case when yjβynβjβ=(jnβ)2q. In this case, each of the conditions (2)β(6) and (8),(9) is equivalent to the pair of conditions β£yjββ£<(jnβ) and β£ynβjββ£<(jnβ).
(2)
: Since we have
[TABLE]
the condition (2) is equivalent to (1). Otherwise if β£yjββ£β₯(jnβ)β£, we may take z=(jnβ)yjβ1ββD or if β£ynβjββ£β₯(jnβ), we may take w=(jnβ)ynβjβ1ββD to reach a contradiction to the equation (2).
2. (3)
: For the case yjβynβjβ=(jnβ)2q, we have Ξ¦jβ(.,y)=(jnβ)yjββ. Thus β₯Ξ¦jβ(.,y)β₯<1 if and only if
β£yjββ£<(jnβ).
3. (3β²)
: In this case, Ξ¦nβjβ(.,y)=(jnβ)ynβjββ.
Thus β₯Ξ¦nβjβ(.,y)β₯<1 if and only if β£ynβjββ£<(jnβ).
4. (4)
: Since yjβynβjβ=(jnβ)2q, the statement (4) is equivalent to
[TABLE]
which is equivalent to β£ynβjββ£<(jnβ)Β andΒ β£yjββ£<(jnβ). The reason of the forward implication is that, if β£ynβjββ£>(jnβ),
then the left hand side of the inequality \eqref1 becomes positive while
the right hand side becomes negative, a contradiction. Also, the inequality
\eqref1 is not valid for the case β£ynβjββ£=(jnβ).
Hence β£ynβjββ£<(jnβ) and consequently, by \eqref1, β£yjββ£<(jnβ).
5. (4β²)
: Similarly, statement (4β²) is equivalent to the pair
of conditions β£yjββ£<(jnβ) and β£ynβjββ£<(jnβ).
6. (5)
:
[TABLE]
Also by hypothesis, β£ynβjββ£<(jnβ). Hence statement (5) implies β£yjββ£<(jnβ) and β£ynβjββ£<(jnβ), when yjβynβjβ=(jnβ)2q. On the other hand
[TABLE]
Hence β£yjββ£<(jnβ) and β£ynβjββ£<(jnβ) together imply statement (5) for the case yjβynβjβ=(jnβ)2q.
7. (5β²)
: Similarly, statement (5β²) is equivalent to the pair of conditions β£yjββ£<(jnβ) and β£ynβjββ£<(jnβ).
8. (6)
: The fact that β£yjββ£2+β£ynβjββ£2β(jnβ)2β£qβ£2+2βyjβynβjββ(jnβ)2qβ<(jnβ)2 is equivalent to (jnβ)2β1β(jnβ)2β£yjββ£2ββ+β£ynβjββ£2β1β(jnβ)2β£yjββ£2ββ>0, which holds if and only if
[TABLE]
Also β£qβ£<1ββ£yjββ£β£ynβjββ£<(jnβ)2. Hence in this case, statement (6) holds if and only if
[TABLE]
The first inequality of \eqref5 holds only if β1β(jnβ)2β£yjββ£2ββ and β1β(jnβ)2β£ynβjββ£2ββ have same sign (positive or negative). Then the second inequality of \eqref5 leads to the fact that both the inequalities in \eqref5 hold only if β£ynβjββ£<(jnβ) and β£yjββ£<(jnβ). If β£ynβjββ£<(jnβ) and β£yjββ£<(jnβ) hold then clearly \eqref5 holds. Therefore, the statement (5) holds if and only if β£ynβjββ£<(jnβ) and β£yjββ£<(jnβ).
9. (8)
: Suppose condition (8) holds. Then the matrix Bjβ, as mentioned in the statement of (8), is of the form
[TABLE]
where ajβ,bjββC such that detBjβ+ajβbjβ=(jnβ)2yjβynβjββ. Then ajβbjβ=(jnβ)2yjβynβjβββdetBjβ=(jnβ)2yjβynβjβββq=0. Therefore, Bjβ is one of the following matrices
[TABLE]
In any case β₯Bjββ₯<1 if and only if β£ynβjββ£<(jnβ) and β£yjββ£<(jnβ).
10. (9)
:
Suppose condition (9) holds. Then we must have
[TABLE]
Note that, β₯Bjββ₯<1 if and only if β£ynβjββ£<(jnβ) and β£yjββ£<(jnβ).
Case-B: Next we consider the other case when yjβynβjβξ =(jnβ)2q.
First we prove the following :
[TABLE]
(2)β(3):
Fix a jβ{1,β¦,nβ1}. Condition (2) then implies that
[TABLE]
which is equivalent to
[TABLE]
The above mentioned condition holds only if 1β(jnβ)ynβjββwξ =0 for all wβD, otherwise the choice z=0 will lead to a contradiction. If β£ynβjββ£<(jnβ), then β(jnβ)ynβjββwβ<1 for all wβD and consequently 1β(jnβ)ynβjββwξ =0 for all wβD. If β£ynβjββ£β₯(jnβ), then for w=ynβjβ(jnβ)ββD we have 1β(jnβ)ynβjββw=0. Hence, 1β(jnβ)ynβjββwξ =0 for all wβD if and only if β£ynβjββ£<(jnβ). Therefore, condition (1) holds if and only if
(2)β(3β²):
Fixed a jβ{1,β¦,nβ1}. Since condition (2) is equivalent to
[TABLE]
by a similar argument as above, condition (2) holds if and only if
[TABLE]
that is if and only if Ξ¦nβjβ(D,y) does not intersect the complement of D which is same as saying β₯Ξ¦nβjβ(.,y)β₯<1.
(3)β(4): Note that
[TABLE]
Therefore β₯Ξ¦jβ(.,y)β₯Hββ<1 if and only if
[TABLE]
Thus conditions (3) and (4) are equivalent.
(3β²)β(4β²): Similarly, this equivalence is clear from the following fact
[TABLE]
(3)β(5):
Fix a jβ{1,β¦,nβ1}. Suppose condition (3) holds. Since yjβynβjβξ =(jnβ)2q, the inequality β₯Ξ¦jβ(.,y)β₯<1 (that is Ξ¦jβ(.,y) is bounded on D) implies β£ynβjββ£<(jnβ). Again if
β£ynβjββ£<(jnβ) holds, then ynβjβzβ(jnβ)ξ =0 for any zβD and consequently the inequality
[TABLE]
implies β₯Ξ¦jβ(.,y)β₯<1. Then by the maximum modulus principle, condition (2) holds if and only if
[TABLE]
Note that:
[TABLE]
(since β£xβ£<k if and only if Re(zx)<k for all zβT.)
Hence condition (3) holds if and only if β£ynβjββ£<(jnβ) and inequality \eqref6 hold, that is, if and only if condition (5) holds.
(3β²)β(5β²):
Using the same line of argument we can show it.
Thus for the case yjβynβjβξ =(jnβ)2q conditions (2),(3),(3β²),(4),(4β²),(5),(5β²) are equivalent. To complete the first part of the proof we show the equivalence of (2),(6),(8) and (9).
(2)β(6): write y^β=(y^β1β,...,y^βnβ1β,qβ), where y^βkββ=ykββ for all kξ =nβj, y^βnβjβ=(jnβ)qΛβ and qβ=(jnβ)yΛβnβjββ. That is,
[TABLE]
First note that replacing ynβjβ and q by (jnβ)qΛβ and (jnβ)yΛβnβjββ respectively, makes no difference in the inequality in condition (5β²). Thus, condition (5β²) holds for the point y ( and for the chosen j) if and only if (5β²) holds for the point y^β. Since we already proved the equivalence of (2), (5) and (5β²), we can conclude that the inequality in condition (2) holds for the point y if and only if the inequalities in (5) hold for the point y^β. Thus, condition (2) holds if and only if the following holds :
[TABLE]
which is same as saying that
[TABLE]
Hence (2)β(6). To complete the rest of the proof we need the following lemma, which can be proved by simple calculations.
Lemma 2.3**.**
If
[TABLE]
where bjβcjβ=(jnβ)2yjβynβjβββq. Then detBjβ=q,
where kjβ is the square root(any) of β(jnβ)2yjβynβjβββqβ. Then detBjβ=q. By Lemma 2.3, the diagonals of 1βBjββBjβ are the following :
[TABLE]
We have proved that condition (2) is equivalent to conditions (4),(4β²) and (6). Thus if condition (6) holds, then conditions (4) and (4β²) also hold. Then by conditions (4) and (4β²), we have
[TABLE]
that is, the diagonals of 1βBjββBjβ are positive. Again by Lemma 2.3 and condition (6), we have
[TABLE]
Thus β₯Bjββ₯<1. Also we have yjβ=(jnβ)[Bjβ]11β and ynβjβ=(jnβ)[Bjβ]22β. Hence condition (9) is satisfied.
(9)β(8) : Obvious.
(8)β(6) : Suppose (8) holds. Then Bjβ is a 2Γ2 matrix such that [Bjβ]11β=(jnβ)yjββ, [Bjβ]22β=(jnβ)ynβjββ and [Bjβ]12β[Bjβ]21β=(jnβ)2yjβynβjβββq. Since (β£[Bjβ]12ββ£ββ£[Bjβ]21ββ£)2β₯0, we have
[TABLE]
Since β₯Bjββ₯<1, by lemma 2.3 we have
[TABLE]
Therefore,
[TABLE]
The fact β₯Bjββ₯<1 implies β£detBjββ£<1, and thus β£qβ£<1. Hence (6) holds and the first part of the proof is complete.
To complete the rest of the proof we show the following : (1)β(2)β(7)β(1).
(1)β(2):
Suppose y=(y1β,β¦,ynβ1β,q)βGnβ. Then β£qβ£<1, and there exists (Ξ²1β,β¦,Ξ²nβ1β)βCnβ1 such that for each jβ{1,β¦,[2nβ]}
[TABLE]
Hence
[TABLE]
Then, for each j=1,β¦,[2nβ],
[TABLE]
and
[TABLE]
Hence, for all j=1,β¦,[2nβ],
[TABLE]
Thus, for all j=1,β¦,[2nβ],
[TABLE]
Therefore, condition (5) holds. Then by equivalence of conditions (2) and (5), we have
[TABLE]
Hence (2) holds.
(2)β(7):
Suppose condition (2) holds. Then by conditions (5) and (5β²),
[TABLE]
By adding the above two inequalities we get
[TABLE]
Since j is chosen arbitrarily, inequality 2.12 holds for each jβ{1,β¦,[2nβ]}. Hence (2)β(7). Further note that if inequation in condition (2) holds for some jβ{1,β¦,[2nβ]}, then the inequality in condition (7) holds for the same j.
(7)β(1):
Suppose condition (7) holds. Clearly β£qβ£<1. For each j=1,β¦,[2nβ], consider
[TABLE]
Then
Ξ²jβ+Ξ²Λβnβjβq=yjβandΞ²nβjβ+Ξ²Λβjβq=ynβjβ,
for all j=1,β¦,[2nβ] which is same as saying that Ξ²jβ+Ξ²Λβnβjβq=yjβ,
for all j=1,β¦,nβ1. By condition (7) of this theorem, we have
[TABLE]
Hence for the point y=(y1β,β¦,ynβ1β,q)βCn, there exists (Ξ²1β,β¦,Ξ²nβ1β)βCnβ1 such that yjβ=Ξ²jβ+Ξ²Λβnβjβq and β£Ξ²jββ£+β£Ξ²nβjββ£<(jnβ) for all j=1,β¦,nβ1. Therefore yβGnβ, and the proof is complete.
2.2. Characterizations of a point in Ξnβ
In this subsection, we state and prove an analog of Theorem 2.2 for Ξnβ(=Gnββ).
Theorem 2.4**.**
For a point y=(y1β,β¦,ynβ1β,q)βCn, the following are equivalent:
(1)
yβΞnβ;
2. (2)
(jnβ)βyjβzβynβjβw+(jnβ)qzwξ =0, for all z,wβD and for all j=1,β¦,[2nβ];
3. (3)
for all j=1,β¦,[2nβ],
[TABLE]
4. (3β²)
for all j=1,β¦,[2nβ],
[TABLE]
5. (4)
for all j=1,β¦,[2nβ],
[TABLE]
6. (4β²)
for all j=1,β¦,[2nβ]
[TABLE]
7. (5)
for all j=1,β¦,[2nβ],
[TABLE]
8. (5β²)
for all j=1,β¦,[2nβ]
[TABLE]
9. (6)
β£qβ£β€1* and β£yjββ£2+β£ynβjββ£2β(jnβ)2β£qβ£2+2βyjβynβjββ(jnβ)2qββ€(jnβ)2 for all j=1,β¦,[2nβ];*
10. (7)
β£ynβjββyΛβjβqβ£+β£yjββyΛβnβjβqβ£β€(jnβ)(1ββ£qβ£2)* for all j=1,β¦,[2nβ], and if β£qβ£=1 then, in addition, β£yjββ£β€(jnβ) for all j=1,β¦,[2nβ];*
11. (8)
there exist [2nβ] number of 2Γ2 matrices B1β,β¦,B[2nβ]β such that β₯Bjββ₯β€1, yjβ=(jnβ)[Bjβ]11β, ynβjβ=(jnβ)[Bjβ]22β for all j=1,β¦,[2nβ] and
[TABLE]
12. (9)
there exist [2nβ] number of 2Γ2 symmetric matrices B1β,β¦,B[2nβ]β such that β₯Bjββ₯β€1, yjβ=(jnβ)[Bjβ]11β, ynβjβ=(jnβ)[Bjβ]22β for all j=1,β¦,[2nβ] and
[TABLE]
Proof.
(1)β(2):
Suppose (2) holds. For any ΞΆ,Ξ·βD and for any rβ(0,1) we have rΞΆ,rΞ·βD. Hence
[TABLE]
Since the above is true for any ΞΆ,Ξ·βD and any rβ(0,1), by Theorem 2.2, we have
[TABLE]
for any rβ(0,1). Therefore, y=(y1β,β¦,ynβ1β,q)βGnββ=Ξnβ.
Conversely, suppose y=(y1β,β¦,ynβ1β,q)βΞnβ. Also suppose (2) does not hold, that is, for some j=1,β¦,[2nβ]
[TABLE]
Since yβΞnβ, we have β£ynβjββ£β€(jnβ) and hence ynβjβwβ(jnβ)ξ =0 for all wβD. Therefore,
[TABLE]
and consequently β£Ξ¦jβ(w,y)β£>1 for some wβD. Again by Theorem 2.2 we have that, β£Ξ¦jβ(w,ΞΆ)β£<1 whenever wβD and ΞΆβGnβ. Since yβΞnβ, we must have β£Ξ¦jβ(w,y)β£β€1 for any wβD, a contradiction. Hence (2) must holds, if yβΞnβ.
Now we prove the equivalence of (2)β(6) and (8),(9).
The proof of this part is similar to the proof of the corresponding part of Theorem 2.2. For the case yyβynβjβ=(jnβ)2q, each condition is equivalent to the pair of statements β£yjββ£β€(jnβ) and β£ynβjββ£β€(jnβ). The explanations for each case are similar to the proof (for the corresponding case) of Theorem 2.2. In this case, we explain the reason for the parts (4) and (4β²) as they are slightly different form the similar parts in Theorem 2.2.
: Since yjβynβjβ=(jnβ)2q, we have the following:
[TABLE]
Since β£ynβjββ£>(jnβ) provides a contradiction, as the left hand side of the inequality \eqref11 becomes positive while the right hand side becomes negative. Hence statement (3) implies β£yjββ£β€(jnβ) and β£ynβjββ£β€(jnβ). On the other hand
[TABLE]
That is, β£yjββ£β€(jnβ) and β£ynβjββ£β€(jnβ) together imply statement (4) for the case yyβynβjβ=(jnβ)2q.
: Similarly, statement (4β²) is equivalent to the inequality
[TABLE]
which implies β£yjββ£<(jnβ). Hence statement (4β²) implies β£yjββ£β€(jnβ) and β£ynβjββ£β€(jnβ). Also, β£yjββ£β€(jnβ) and β£ynβjββ£β€(jnβ) together imply statement (4β²) for this case.
For the case yyβynβjβξ =(jnβ)2q, the proof is similar to the corresponding parts of Theorem 2.2.
(2)β(7): we can have similar proof as in the corresponding part of Theorem 2.2.
(7)β(10):
Suppose condition (7) holds, then β£qβ£β€1. For β£qβ£<1, the part (7)β(1) of the proof of Theorem 2.2 works here, that is, take
[TABLE]
to obtain statement (10). If β£qβ£=1, then condition (3) implies yjβ=yΛβnβjβq and ynβjβ=yΛβjβq, for all j=1,β¦,[2nβ]. Hence β£ynβjββ£=β£yjββ£β€(jnβ). Choose r1β,β¦,r[2nβ]ββ[0,1]. Consider
[TABLE]
Then for all j=1,β¦,[2nβ] we have the following
[TABLE]
Thus for either cases, there exists (Ξ²1β,β¦,Ξ²nβ1β)βCn such that yjβ=Ξ²jβ+Ξ²Λβnβjβq, ynβjβ=Ξ²nβjβ+Ξ²Λβjβq and β£Ξ²jββ£+β£Ξ²nβjββ£β€(jnβ) for all j=1,β¦,[2nβ]. Hence (10) holds.
(10)β(2):
Suppose (10) holds. Then β£qβ£β€1, and there is (Ξ²1β,β¦,Ξ²nβ1β)βCn such that for any jβ{1,β¦,[2nβ]}
[TABLE]
Hence
[TABLE]
Let jβ{1,β¦,[2nβ]} be arbitrary. Then
[TABLE]
and ynβjββyΛβjβq=Ξ²nβjβ+Ξ²Λβjβqβ(Ξ²Λβjβ+Ξ²nβjβqΛβ)q=Ξ²nβjβ(1ββ£qβ£2).
Hence
[TABLE]
that is,
[TABLE]
Thus, condition (5) holds.
Since j was chosen arbitrarily and condition (2) is equivalent to (5),
thus condition (2) of this theorem holds. Consequently, the proof is complete.
Remark 2.5**.**
The set Ξnβ can be described as follows :
[TABLE]
Remark 2.6**.**
Let y=(y1β,β¦,ynβ1β,q)βCn. For any jβ{1,β¦,[2nβ]}, if y~βj=(y~β1β,β¦,y~βnβ1β,q~β) where
y~βkβ=ykβ for kξ =j,nβj;y~βjβ=ynβjβ,y~βnβjβ=yjβ and q~β=q,
then yβGnβ(or Ξnβ) if and only if y~βjβGnβ(or Ξnβ).
Remark 2.7**.**
It was proved in [8] (see Theorem 1.1 in [8]) that the closed symmetrized bidisc Ξ2β has the following representation:
[TABLE]
Thus it is evident from Theorem 2.4 (and also from Remark 2.5) that Ξ2ββ=Ξ2β. We shall see in Section 4 that ΞnββΞnβ for all nβ₯3.
3. Characterizations of the points in Gnβ and Ξnβ
In this section, we find a variety of characterizations for the symmetrized polydisc Gnβ via the characterizations of Gnβ as in Theorem 2.2. In [17], Costara found the following interesting characterization of a point in Gnβ and Ξnβ.
For a point (s1β,β¦,snβ1β,p)βCn, the following are equivalent:
(1)
*The point *(s1β,β¦,snβ1β,p)βGnβ(respectively βΞnβ).
2. (2)
β£pβ£<1(*respectively β€1) and there exists *(S1β,β¦,Snβ1β)βGnβ1β(respectively βΞnβ1β) such that
[TABLE]
We have mentioned before (see Remark 2.7) that Ξ2β=Ξ2β. Indeed, it is true that Gnβ=Gnβ for n=2 but Gnββ«Gnβ for nβ₯3. The first part of this claim follows straight from the above result of Costara (Theorem 3.1). We show below that Gnββ«Gnβ for nβ₯3. By Theorem 3.1, siβ=Siβ+SΛnβiβp for every point (s1β,β¦,snβ1β,p)βGnβ, where (S1β,β¦,Snβ1β)βGnβ1β. Needless to mention that β£Siββ£+β£Snβiββ£<(inβ) and this implies that (s1β,β¦,snβ1β,p)βGnβ. Now consider the point (25β,45β,21β)βC3. We can write (25β,45β,21β)=(Ξ²1β+Ξ²β2βp,Ξ²2β+Ξ²β1βp,p), where Ξ²1β=25β,Ξ²2β=0,p=21β. Also Ξ²1β,Ξ²2β are unique because if we write (y1β,y2β,p)=(25β,45β,21β), then
[TABLE]
Since β£Ξ²1ββ£+β£Ξ²2ββ£<3, (25β,45β,21β)βG3ββ. Clearly (Ξ²1β,Ξ²2β)β/G2β, as β£Ξ²1ββ£>2. By Theorem 3.1, (25β,45β,21β)β/G3β. So, G3ββ«G3ββ. Similarly for any n>3, we may choose (Ξ²1β,β¦,Ξ²nβ1β)=(22nβ1β,0,β¦,0) and p=21β to obtain a point (y1β,β¦,ynβ1β,p), where yiβ=Ξ²iβ+Ξ²Λβnβiβp, for i=1,β¦,nβ1, which is in Gnββ but not in Gnβ.
3.1. Characterizations of a point in Gnβ
Theorem 3.2**.**
Let (s1β,β¦,snβ1β,p)βCn with β£pβ£ξ =1. Consider the point
[TABLE]
Then (s1β,β¦,snβ1β,p)βGnβ if and only if (s1β,β¦,snβ1β,p)βGnβ and QβGnβ1β.
Proof.
Suppose (s1β,β¦,snβ1β,p)βGnβ. Then β£pβ£<1 and (s1β,β¦,snβ1β,p)βGnβ as GnββGnβ. By Theorem 3.1, there exists (Ξ²1β,β¦,Ξ²nβ1β)βGnβ1β so that
[TABLE]
Then for each j=1,β¦,nβ1, we have
Ξ²jβ=1ββ£pβ£2sjββsΛnβjβpβ.
Also these Ξ²jβ²βs are unique. So,
by Theorem 3.1,
[TABLE]
Conversely, suppose (s1β,β¦,snβ1β,p)βGnβ and QβGnβ1β. Then β£pβ£<1.
For each j=1,β¦,nβ1, consider
[TABLE]
Then, we have Ξ²jβ+Ξ²Λβnβjβp=sjβ for each j=1,β¦,nβ1. Since (Ξ²1β,β¦,Ξ²nβ1β)=QβGnβ1β, it follows from Theorem 3.1 that (s1β,β¦,snβ1β,p)βGnβ.
We finally arrive at the main result of this paper, which characterizes a point in Gnβ in several different ways.
Theorem 3.3**.**
Let x=(s1β,β¦,snβ1β,p)βCn and let
[TABLE]
Then the following are equivalent:
(1)
xβGnβ;
2. (2)
QβGnβ1β* and
(jnβ)βsjβzβsnβjβw+(jnβ)pzwξ =0, for all z,wβD and for all j=1,β¦,[2nβ] ;*
3. (3)
QβGnβ1β* and for all j=1,β¦,[2nβ] either*
[TABLE]
or
[TABLE]
4. (4)
QβGnβ1β* and for all j=1,β¦,[2nβ] either*
[TABLE]
or
[TABLE]
5. (5)
QβGnβ1β* and for all j=1,β¦,[2nβ] either*
[TABLE]
or
[TABLE]
6. (6)
QβGnβ1β, β£pβ£<1 and
β£sjββ£2+β£snβjββ£2β(jnβ)2β£pβ£2+2βsjβsnβjββ(jnβ)2pβ<(jnβ)2 for all j=1,β¦,[2nβ];
7. (7)
QβGnβ1β* and β£snβjββsΛjβpβ£+β£sjββsΛnβjβpβ£<(jnβ)(1ββ£pβ£2) for all j=1,β¦,[2nβ];*
8. (8)
QβGnβ1β* and there exist [2nβ] number of 2Γ2 matrices B1β,β¦,B[2nβ]β such that β₯Bjββ₯<1, sjβ=(jnβ)[Bjβ]11β, snβjβ=(jnβ)[Bjβ]22β for all j=1,β¦,[2nβ] and*
[TABLE]
9. (9)
QβGnβ1β* and there exist [2nβ] number of 2Γ2 symmetric matrices B1β,β¦,B[2nβ]β such that β₯Bjββ₯<1, sjβ=(jnβ)[Bjβ]11β, snβjβ=(jnβ)[Bjβ]22β for all j=1,β¦,[2nβ] and*
[TABLE]
Proof.
The proof follows from Theorem 2.2 and Theorem 3.2.
3.2. Characterizations of a point in Ξnβ
Recall from the literature (see [18]) that the distinguished boundary of Ξnβ is the smallest closed subset bΞnβ of βΞnβ such that every complex-valued function on Ξnβ, that is analytic in the interior Gnβ and continuous on Ξnβ, attains its maximum modulus on bΞnβ. Evidently, bΞnβ is a subset of the topological boundary βΞnβ of Ξnβ. In [15], the points in the distinguished boundary bΞnβ of Ξnβ are characterized in the following way:
For (s1β,β¦,snβ1β,p)βCn the following are equivalent:
(1)
(s1β,β¦,snβ1β,p)βbΞnβ*β;*
2. (2)
(s1β,β¦,snβ1β,p)βΞnβ*
and β£pβ£=1β;*
3. (3)
β£pβ£=1, sjβ=sΛnβjβp and
(nnβ1βs1β,nnβ2βs2β,β¦,n1βsnβ1β)βΞnβ1ββ;
4. (4)
β£pβ£=1*
and there exists (Ξ²1β,β¦,Ξ²nβ1β)βbΞnβ1β such that*
sjβ=Ξ²jβ+Ξ²Λβnβjβp* , for j=1,β¦,nβ1.*
Theorem 3.4 provides several independent descriptions of the points in bΞnβ. Thus, in order to characterize the points in Ξnβ it suffices if we find characterizations for the points in ΞnββbΞnβ.
Theorem 3.5**.**
Let (s1β,β¦,snβ1β,p)βCn. Then the following are equivalent:
Suppose (s1β,β¦,snβ1β,p)βΞnββbΞnβ. Then (s1β,β¦,snβ1β,p)βΞnβ and β£pβ£β€1. By Theorem 3.4, we have β£pβ£<1. By Theorem 3.1, there exists (Ξ²1β,β¦,Ξ²nβ1β)βΞnβ1β such that
[TABLE]
Since β£pβ£<1, we have that
[TABLE]
Thus, (1ββ£pβ£2s1ββsΛnβ1βpβ,1ββ£pβ£2s2ββsΛnβ2βpβ,β¦,1ββ£pβ£2snβ1ββsΛ1βpβ)βΞnβ1β.
Since (s1β,β¦,snβ1β,p)β/bΞnβ, by Theorem 3.4,
(1ββ£pβ£2s1ββsΛnβ1βpβ,1ββ£pβ£2s2ββsΛnβ2βpβ,β¦,1ββ£pβ£2snβ1ββsΛ1βpβ)βΞnβ1ββbΞnβ1β. Thus (1)β(2).
Conversely, suppose (2) holds. Then β£pβ£β€1. First suppose β£pβ£<1 and consider
Ξ²jβ=1ββ£pβ£2sjββsΛnβjβpβ.
Then, we have Ξ²jβ+Ξ²Λβnβjβp=sjβ for each j=1,β¦,nβ1. By hypothesis (Ξ²1β,β¦,Ξ²nβ1β)βΞnβ1β. Hence by Theorem 3.7 in [17], we have (s1β,β¦,snβ1β,p)βΞnβ. Now suppose β£pβ£=1. Since
(1ββ£pβ£2s1ββsΛnβ1βpβ,1ββ£pβ£2s2ββsΛnβ2βpβ,β¦,1ββ£pβ£2snβ1ββsΛ1βpβ)β/bΞnβ1β, by Theorem 3.4 we can conclude that (s1β,β¦,snβ1β,p)β/bΞnβ. Hence (1) holds.
The following theorem, which is another main result of this article, is a consequence of Theorems 2.4 and 3.5 and it provides several independent characterizations of a point in ΞnββbΞnβ.
Theorem 3.6**.**
Let x=(s1β,β¦,snβ1β,p)βCn and let
[TABLE]
Then the following are equivalent:
(1)
xβΞnββbΞnβ;
2. (2)
QβGnβ1β* and
(jnβ)βsjβzβsnβjβw+(jnβ)pzwξ =0, for all z,wβD and 1β€jβ€[2nβ] ;*
3. (3)
QβGnβ1β* and for all j=1,β¦,[2nβ] either*
[TABLE]
or
[TABLE]
4. (4)
QβGnβ1β* and for all j=1,β¦,[2nβ] either*
[TABLE]
or
[TABLE]
5. (5)
QβGnβ1β* and for all j=1,β¦,[2nβ] either*
[TABLE]
or
[TABLE]
6. (6)
QβGnβ1β, β£pβ£<1 and
β£sjββ£2+β£snβjββ£2β(jnβ)2β£pβ£2+2βsjβsnβjββ(jnβ)2pββ€(jnβ)2 for j=1,β¦,[2nβ];
7. (7)
QβGnβ1β* and
β£snβjββsΛjβpβ£+β£sjββsΛnβjβpβ£β€(jnβ)(1ββ£pβ£2) for j=1,β¦,[2nβ] ;*
8. (8)
QβGnβ1β* and there exist [2nβ] number of 2Γ2 matrices B1β,β¦,B[2nβ]β such that β₯Bjββ₯β€1, sjβ=(jnβ)[Bjβ]11β, snβjβ=(jnβ)[Bjβ]22β for all j=1,β¦,[2nβ] and
detB1β=detB2β=detB[2nβ]β=p ;*
9. (9)
QβGnβ1β* and there exist [2nβ] number of 2Γ2 symmetric matrices B1β,β¦,B[2nβ]β such that β₯Bjββ₯β€1, sjβ=(jnβ)[Bjβ]11β, snβjβ=(jnβ)[Bjβ]22β for all j=1,β¦,[2nβ] and detB1β=detB2β=detB[2nβ]β=p.*
4. Some more geometric properties of Gnβ and Ξnβ
We further study the geometry of the domain Gnβ and its closure Ξnβ and obtain a few important features. We prove that Ξnβ is not convex but is polynomially convex. Since the closed symmetrized bidisc Ξ2β is not convex (see Section 2 of [5] and [18]), it follows that Ξ2ββ is not convex because Ξ2β=Ξ2ββ (see Remark 2.7). Below we show that Ξnβ is not convex for any nβ₯2. Also, we show that both Gnβ and Ξnβ are starlike about the origin but not circled. It follows from here that Gnβ is simply connected. For the convenience of a reader, we begin with a few definitions from the literature.
Definition 4.1**.**
A compact set KβCn is called polynomially convex if for any yβCnβK, there exists a polynomial in n variables, say P, such that
[TABLE]
Definition 4.2**.**
A set SβCn is said to be starlike if there exists a z0ββS such that for all zβS the line segment joining z and z0β, lies in S.
Definition 4.3**.**
A set SβCn is said to be circular if zβS implies that (eΞΉΞΈz1β,eΞΉΞΈz2β,...,eΞΉΞΈznβ)βS for all 0β€ΞΈ<2Ο.
Consider the points a=(n,0,β¦,0,ni,i)βCn and b=(βni,0β¦,0,n,βi)βCn. Then a,bβΞnβ, because, both the points a and b satisfy condition (7) of Theorem 2.4. The mid point of the line joining a and b is
[TABLE]
The point cβ/Ξnβ. This is because the inequality in condition (7) of Theorem 2.4, corresponding to the point c and j=1, does not hold. Indeed, after substituting the values in that particular inequality we get the following
[TABLE]
Hence, the line segment joining a and b does not entirely lie within Ξnβ and consequently Ξnβ is not convex.
We now show that Ξnβ is polynomially convex. The techniques that we use to prove this are similar to that in [2], where the authors established that the tetrablock is polynomially convex.
Theorem 4.4**.**
Ξnβ* is polynomially convex.*
Proof.
Consider a point y=(y1β,β¦,ynβ1β,q)βCnβΞnβ. To show Ξnβ is polynomially convex, it is enough to find a polynomial f in n variables, such that β£fβ£β€1 on Ξnβ and β£f(y)β£>1. Let β£yjββ£>(jnβ) for some j=1,β¦,[2nβ]. Then f((x1β,β¦,xnβ))=(jnβ)xjββ has the required property, since for any xβΞnβ, β£xjββ£β€(jnβ) for all j=1,β¦,[2nβ]. If β£qβ£>1 then take f((x1β,β¦,xnβ))=xnβ. Thus assume y to be such that β£yjββ£β€(jnβ) for all j=1,β¦,nβ1; and β£qβ£<1. Since yβ/Ξnβ, by condition (3) of Theorem 2.2 there exist some jβ{1,β¦,[2nβ]} such that β₯Ξ¦jβ(.,y)β₯>1. That is, there exist zβD and some jβ{1,β¦,[2nβ]} such that β£Ξ¦jβ(z,y)β£>1. Fix that j and z. Note the following cases :
: If yjβynβjβ=(jnβ)2q, then β£Ξ¦jβ(z,y)β£=(jnβ)β£yjββ£β. Hence β£yjββ£>(jnβ) and then the function f((x1β,β¦,xnβ))=(jnβ)xjββ is the required function.
: If yjβynβjβξ =(jnβ)2q, then Ξ¦jβ(z,y)=ynβjβzβ(jnβ)(jnβ)qzβyjββ. For mβN, define a polynomial fmβ in n variables as follows
[TABLE]
Let
[TABLE]
Then ΞnββW and also yβW. For xβW, we have β(jnβ)xnβjβzβββ€β£zβ£<1 and hence Ξ¦jβ(z,x) can be written in the following form
[TABLE]
For xβW, we also have
[TABLE]
Then for any xβW and for any mβN, we have
[TABLE]
Let 0<Ο΅<31β(β£Ξ¦jβ(z,y)β£β1). Note that zβD implies β£zβ£m+1β0 as mββ. Hence there exists kβN, large enough, such that 1ββ£zβ£2β£zβ£k+1β<Ο΅. Since
[TABLE]
we have
[TABLE]
Again since ΞnββW and β£Ξ¦jβ(z,x)β£β€1 for all xβΞnβ, we have
[TABLE]
Note that, β£Ξ¦jβ(z,y)β£>1+3Ο΅. Since yβW, we have β£Ξ¦jβ(z,y)βfkβ(y)β£<Ο΅, that is
[TABLE]
Therefore,
[TABLE]
Now take f=(1+Ο΅)β1fkβ. Then β£f(x)β£β€1 for all xβΞnβ, and
[TABLE]
Hence f is the required polynomial.
Theorem 4.5**.**
Gnβ* and Ξnβ are both starlike about (0,β¦,0) but not circular. Hence Gnβ is simply connected.*
Proof.
Let y=(y1β,β¦,ynβ1β,q)βΞnβ and let 0β€r<1. To prove that Gnβ and Ξnβ are starlike about (0,0,0), it is enough to show that ryβGnβ for all such y and r.
First note that, for r>0, zβC and j=1,β¦,nβ1 we have
[TABLE]
Since yβΞnβ, by condition (3) of Theorem 2.4, we have β₯Ξ¦jβ(.,y)β₯β€1 for all j=1,β¦,[2nβ]. Hence, for each j=1,β¦,[2nβ]
[TABLE]
Again for any zβD and for all j=1,β¦,[2nβ], we have
[TABLE]
This is because rβ£zynβjββ£2<β£zynβjββ£2β€β£ynβjββ£2β€(jnβ)2 (as yβΞnβ). Hence from equation \eqrefstarlike, we have
[TABLE]
for any rβ[0,1), zβD and for all j=1,β¦,[2nβ].
Therefore,
[TABLE]
whenever yβΞnβ, zβD and
0β€r<1. Thus, β₯Ξ¦jβ(.,ry)β₯<1 for all j=1,β¦,[2nβ], whenever yβΞnβ and 0β€r<1.
Therefore, by Theorem 2.2, ryβGnβ whenever yβΞnβ and 0β€r<1.
Hence Gnβ and Ξnβ are starlike about (0,β¦,0).
Next we show that Ξnβ is not a circular, which implies that Gnβ is not a circular domain either. Let y=(y1β,β¦,ynβ1β,q)βCn be such that yjβ=(jnβ) for j=1,β¦,[2nβ]. and q=1, that is,
[TABLE]
To prove Ξnβ is not a circular, we show that yβΞnβ but iyβ/Ξnβ. Note that, for the above mentioned point y, we have yjβynβjβ=(jnβ)2q, and
[TABLE]
and
[TABLE]
Therefore, by condition (4) of Theorem 2.2, yβΞnβ. Now consider the point
[TABLE]
Then for each j=1,β¦,[2nβ], we have
(jnβ)2ββ£y~βnβjββ£2=0. Again for each j=1,β¦,[2nβ],
[TABLE]
Thus y~β does not satisfy condition (4) of Theorem 2.2 and hence y~β=iyβ/Ξnβ. Thus Ξnβ is not circular. Thus it follows from here that Gnβ is simply connected.
Acknowledgement. We are thankful to the referee for making fruitful suggestions which help in improving the exposition of the article.
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