Hostname: page-component-cd9895bd7-mkpzs Total loading time: 0 Render date: 2024-12-24T02:11:39.510Z Has data issue: false hasContentIssue false

A DOMAIN WITH NONPLURISUBHARMONIC d-BALANCED SQUEEZING FUNCTION

Published online by Cambridge University Press:  11 November 2022

NAVEEN GUPTA*
Affiliation:
Department of Mathematics, University of Delhi, Delhi 110 007, India
*
Rights & Permissions [Opens in a new window]

Abstract

In this note, we give an example of a domain whose d-balanced squeezing function is nonplurisubharmonic.

Type
Research Article
Creative Commons
Creative Common License - CCCreative Common License - BY
This is an Open Access article, distributed under the terms of the Creative Commons Attribution licence (https://creativecommons.org/licenses/by/4.0/), which permits unrestricted re-use, distribution, and reproduction in any medium, provided the original work is properly cited.
Copyright
© The Author(s), 2022. Published by Cambridge University Press on behalf of Australian Mathematical Publishing Association Inc.

1 Introduction

We present an example of a domain in $\mathbb {C}^2$ whose d-balanced squeezing function fails to be plurisubharmonic. Let us first recall some related notions.

For a bounded domain $D\subseteq \mathbb {C}^n$ and $z\in {D}$ , Deng et al. [Reference Deng, Guan and Zhang3] introduced the squeezing function $S_{D}$ on D, defined by

$$ \begin{align*}S_{D}(z):=\sup_f\{r:\mathbb{B}^n(0,r)\subseteq f(D), f\in{\mathcal{O}_u(D,\mathbb{B}^n), f(z)=0}\},\end{align*} $$

where $\mathbb {B}^n(0,r)$ denotes a ball of radius r centred at the origin and $\mathcal {O}_u(D,\mathbb {B}^n)$ denotes the collection of injective holomorphic maps from D to the unit ball $\mathbb {B}^n$ .

Rong and Yang [Reference Rong and Yang10] extended this idea by replacing the unit ball with a bounded, balanced, convex domain. Recall that a domain $\Omega \subseteq \mathbb {C}^n $ is called balanced if $\lambda z$ belongs to ${\Omega } $ for each z in ${\Omega }$ and $\lambda $ in the closed unit disc $\overline {\mathbb {D}}$ of the complex plane. Its Minkowski function $h_{\Omega }$ on $\mathbb {C}^n$ is defined by

$$ \begin{align*}h_{\Omega}(z):=\inf \{t>0:z/t\in{\Omega}\}\end{align*} $$

and $\Omega (r)=\{z\in \mathbb {C}^n:h_{\Omega }(z)<r\}$ for $0<r\leq 1$ .

For a bounded domain $D\subseteq \mathbb {C}^n$ , the generalised squeezing function $S_D^{\Omega }$ on D is defined by

$$ \begin{align*} S^{\Omega}_D(z):=\sup \{r:\Omega(r)\subseteq f(D), f\in{\mathcal{O}_u(D,\Omega)}, f(z)=0\}. \end{align*} $$

In [Reference Gupta and Pant5], we introduced the d-balanced squeezing function by replacing a balanced domain with a d-balanced domain.

Let $d=(d_1,d_2,\ldots ,d_n)\in {\mathbb {Z}_n^{+}},n\geq 2$ . Then a domain $\Omega \subseteq \mathbb {C}^n$ is said to be d-balanced if $(\lambda ^{d_1}z_1,\lambda ^{d_2}z_2,\ldots , \lambda ^{d_n}z_n) \in \Omega $ for each $z=(z_1,z_2,\ldots , z_n)\in \Omega $ and $\lambda \in {\overline {\mathbb {D}}}$ .

For a d-balanced domain $\Omega $ , the d-Minkowski function $h_{d,\Omega }$ on $\mathbb {C}^n$ is defined by

$$ \begin{align*}h_{d,\Omega}(z):=\inf \bigg\{t>0:\bigg(\frac{z_1}{t^{d_1}},\frac{z_2}{t^{d_2}},\ldots, \frac{z_n}{t^{d_n}}\bigg)\in{\Omega}\bigg\}.\end{align*} $$

Let $\Omega ^d(r)=\{z\in \mathbb {C}^n:h^d_{\Omega }(z)<r\}$ for $0<r\leq 1$ .

Definition 1.1. For a bounded domain $D\subseteq \mathbb {C}^n$ and a bounded, convex, d-balanced domain $\Omega $ , where $d=(d_1,d_2,\ldots , d_n)$ , the d-balanced squeezing function $S_{d,D}^\Omega $ is

$$ \begin{align*} S_{d,D}^\Omega(z):=\sup \{r:\Omega^d(r)\subseteq f(D), f\in{\mathcal{O}_u(D,\Omega)}, f(z)=0\}. \end{align*} $$

We can easily see that if $\Omega $ is balanced, then $d=(1,1,\ldots , 1)$ and $S_{d,D}^{\Omega }$ reduces to  $S_D^{\Omega }.$

In [Reference Fornæss and Shcherbina4], Fornæss and Scherbina gave an example of a domain whose squeezing function is nonplurisubharmonic. Recently, Rong and Yang [Reference Rong and Yang11] gave examples of domains with nonplurisubharmonic generalised squeezing functions. Here we consider the same problem for d-balanced squeezing functions and present an example (see Theorem 3.5).

2 Background and an estimate for a d-balanced squeezing function

Let us first recall the definitions of the Carathéodory pseudodistance and the Carathéodory extremal maps. For a domain $D\subseteq \mathbb {C}^n$ and $z_1,z_2\in D$ , a Carathéodory pseudodistance $c_{D}$ on D is defined by

$$ \begin{align*}c_D(z_1,z_2)=\sup_f \{p(0,\mu):f\in{\mathcal{O}(\mathbb{D}, D), f(z_1)=0, f(z_2)=\mu}\},\end{align*} $$

where p denotes the Poincaré metric on the unit disc $\mathbb {D}$ and $\mathcal {O}(\mathbb {D}, D)$ denotes the set of holomorphic maps from $\mathbb {D}$ to D. A function $f\in {\mathcal {O}(\mathbb {D}, D)} $ at which this supremum is attained is called a Carathéodory extremal function.

We now recall results that will be used in this section. Lempert [Reference Lempert8, Theorem 1] and Kosi $\grave{\rm n}$ ski and Warszawski [Reference Kosiǹski and Warszawski7, Theorem 1.3 and Remark 1.6] yield the following result.

Result 2.1. For a convex domain $\Omega \subseteq \mathbb {C}^n,\, c_{\Omega } =\tilde {k}_{\Omega },$ where $\tilde {k}_{\Omega }$ denotes the Lempert function on $\Omega $ .

Combining Result 2.1 with [Reference Bharali2, Theorem 1.6], we get the following result.

Result 2.2. For a bounded, convex, d= $(d_1,d_2,\ldots ,d_n)$ -balanced domain $\Omega \subseteq \mathbb {C}^n$ ,

$$ \begin{align*}\tanh^{-1}h_{d,\Omega}(z)^L\leq c_{\Omega}(0,z)=\tilde{k}_{\Omega}(0,z)\leq \tanh^{-1}h_{d,\Omega}(z),\end{align*} $$

where $L=\max _{1\leq i\leq n}d_i.$

Result 2.3. Let $\Omega \subseteq \mathbb {C}^n$ be a domain and $K\subseteq \Omega $ be compact such that $\Omega \setminus K$ is connected. Then, each holomorphic function f on $\Omega \setminus K$ extends to a holomorphic function on $\Omega $ .

Result 2.4 (see [Reference Nikolov9, Proposition 1]).

Let $\Omega \subseteq \mathbb {C}^n$ be a balanced domain and let $h_{d,\Omega }$ be its d-Minkowski function. Then $\Omega $ is pseudoconvex if and only if $h_{d,\Omega }$ is plurisubharmonic.

Result 2.5 (see [Reference Jarnicki and Pflug6, Remark 2.2.14]).

If $\Omega \subseteq \mathbb {C}^n$ is a d-balanced domain, then:

  1. (1) $\Omega =\{z\in {\mathbb {C}^n}:h_{d,\Omega }(z)<1\}$ ;

  2. (2) $h_{d,\Omega }(\lambda ^{d_1}z_1,\lambda ^{d_2}z_2,\ldots , \lambda ^{d_n} z_n)=\lvert \lambda \rvert h_{d,\Omega }(z)$ for each $z=(z_1,z_2,\ldots , z_n)\in {\mathbb {C}^n}$ and ${\lambda \in {\mathbb {C}}}$ ;

  3. (3) $h_{d,\Omega }$ is upper semicontinuous.

For a bounded domain $\Omega \subseteq \mathbb {C}^n$ and a compact subset K of $\Omega $ , denote

$$ \begin{align*}d_{c_{\Omega}}^{K}(z)=\min_{w\in K}\tanh (c_{\Omega}(z,w)). \end{align*} $$

We begin with the following theorem for d-balanced domains, which is analogous to Theorem 2.1 in [Reference Rong and Yang11].

Theorem 2.6. Let $\Omega \subseteq \mathbb {C}^n$ be a bounded, d= $(d_1,d_2,\ldots , d_n)$ -balanced, convex, homogeneous domain. If K is a compact subset of $\Omega $ such that $D=\Omega \setminus K$ is connected, then

(2.1) $$ \begin{align} S^d(z)^L\leq d_{c_{\Omega}}^{\partial K}(z)=d_{c_{\Omega}}^{K}(z)\leq S^d(z), \end{align} $$

where $L=\max _{1\leq i \leq n}d_i.$

Proof. For $z\in D$ , let $g\in {\mathrm {Aut}(\Omega )}$ be such that $g(z)=0.$ Using the convexity of $\Omega $ , we have $\{tv+(1-t)w:0\leq t\leq 1,\, v\in {D}, w\in K^{\circ }\}\cap \partial K\neq \emptyset ;$ therefore, $d_{c_{\Omega }}^{\partial K}(v)=d_{c_{\Omega }}^{K}(v)$ for each $v\in {D}.$

Clearly, $h=g|_{D}:D\to \Omega $ is injective and holomorphic with $h(z)=0$ . For notational convenience, let us denote $d_{c_{\Omega }}^{K}(z)$ by $\alpha $ . We claim that $\Omega ^d(\alpha )\subseteq h(D)$ . Let $h_{d,\Omega }(v)<\alpha $ , which upon using Result 2.2 implies $\tanh (c_{\Omega }(0,v))<\alpha $ . Since g is an automorphism, we get $\tanh (c_{g(\Omega )}(g(z),g(v')))<\alpha $ for $v'\in \Omega $ . Therefore, $\tanh (c_{\Omega }(z,v'))<\alpha =\min _{w\in K}\tanh (c_{\Omega }(z,w))$ . Thus, we get $v'\notin K$ and therefore, $v=g(v')\in g(D)$ . This proves our claim and hence, we obtain

$$ \begin{align*}S^d(z)\geq \alpha =d_{c_{\Omega}}^{K}(z).\end{align*} $$

For the other inequality, consider an injective holomorphic map $f:D\to \Omega $ such that $f(z)=0$ . By Result 2.3, there exists a holomorphic function $F:\Omega \to \mathbb {C}^n$ such that $F|_{D}=f$ . Using Result 2.4 and following the argument as in [Reference Rong and Yang11, Theorem 2.1], we obtain $F(\Omega )\subseteq \Omega $ . Observe that $F(\partial K)\cap F(D)\neq \emptyset $ . Let $r>0$ be such that $\Omega ^d(r)\subseteq F(D)$ . If possible, let $\tanh (c_{\Omega }(0,F( \partial K)))^{1/L}<r$ , then upon using Result 2.2, we get $h_{d,\Omega }(F(\partial K))<r.$ This implies that $F(\partial K)\in \Omega ^d(r)\subseteq F(D)$ , which is a contradiction. Therefore, $r<\tanh (c_{\Omega }(0,F(\partial K)))^{1/L}$ which, upon using the decreasing property of $c_{\Omega }$ , implies that $r<\tanh (c_{\Omega }(z, \partial K))^{1/L}$ . Finally, we can conclude that $ S^d(z)^L\leq d_{c_{\Omega }}^{ K}(z).$

Remark 2.7. A careful look at the above proof makes it clear that the left-hand side of inequality (2.1) holds even if $\Omega $ is not homogeneous.

3 Nonplurisubharmonic d-balanced squeezing functions

Let $G_2\subseteq \mathbb {C}^2$ be the domain defined by

$$ \begin{align*}G_2=\{(z_1+z_2,z_1z_2):z_1,z_2\in \mathbb{D}\}.\end{align*} $$

The domain $G_2$ is called the symmetrised bidisc. Its genesis lies with the problem of ‘robust stabilisation’ in control engineering. Although it is closely related to the bidisc, its geometry is very different to that of the bidisc. It is polynomially convex, hyperconvex and starlike about the origin but not convex ( $(2,1),\, (2i, -1)\in G_2$ but $(1+i,0)\notin G_2$ ). Another point to note here is that it is not homogeneous (there is no automorphism of $G_2$ , which maps any $(a,0)$ with $0<a<1$ to $(0,0)$ ). For many equivalent characterisations of $G_2$ , see [Reference Agler and Young1].

The domain $G_2$ has several interesting properties. For example, Lempert’s theorem holds for $G_2$ even though it is neither convex nor can it be exhausted by domains biholomorphic to convex domains.

We will require Carathéodory extremal maps for $G_2$ to prove our result. Agler and Young [Reference Agler and Young1] proved that for each $z_1,z_2\in G_2$ , there exists $\lambda \in \mathbb {C}, \lvert \lambda \rvert =1$ such that $\phi _{\lambda }$ is a Carathéodory extremal function, where $\phi _{\lambda }$ is defined by

$$ \begin{align*}\phi_{\lambda}(z_1,z_2)=\frac{2\lambda z_2-z_1}{2-\lambda z_2}.\end{align*} $$

It is easy to check that $G_2$ is $(1,2)$ -balanced. Let us denote by $\Omega $ the set of all possible linear combinations of elements of $G_2$ , that is, $\Omega $ is the convex hull of $G_2$ . We begin with the following lemma.

Lemma 3.1. Let $\Omega $ be the convex hull of $G_2$ . Then:

  1. (1) $\Omega $ is $(1,2)$ -balanced;

  2. (2) $\lvert z_1\rvert <2$ and $\lvert z_2\rvert <1$ for each point $(z_1, z_2)\in \Omega $ .

Proof. (1) Let $\sum _{i=1}^k\alpha _i z_i\in \Omega $ , $\sum _{i=1}^k\alpha _i=1,\ \alpha _i\geq 0$ and $z_i=(z_i^{(1)},z_i^{(2)})\in G_2$ for each $i.$ Let $\lvert \lambda \rvert \leq 1$ . Each $z_i\in G_2$ so that $(\lambda z_i^{(1)},\lambda ^2 z_i^{(2)})\in G_2$ . Therefore, $\sum _{i=1}^k\alpha _i (\lambda z_i^{(1)},\lambda ^2 z_i^{(2)})=(\lambda \sum _{i=1}^k\alpha _i z_i^{(1)},\lambda ^2 \sum _{i=1}^k\alpha _i z_i^{(2)})\in \Omega $ and hence, $\Omega $ is $(1,2)$ -balanced.

(2) Follows from the structure of $G_2$ .

Choose r, with $0<r<1$ , such that $\overline {\mathbb {D}^2(0,r)}$ , the closure of the polydisk in $\mathbb {C}^2$ of radius r centred at the origin, is contained in $\Omega $ . Take the point ${Q=(0,r)\in \overline {\mathbb {D}^2(0,r)} \subseteq \Omega }$ and let $\epsilon>0$ be such that a ball $\mathbb {B}^2(Q,r)$ of radius $\epsilon <r$ centred at Q is contained in $\Omega $ . Let us take $K=\partial \mathbb {D}^2(0,r)\setminus \mathbb {B}^2(Q,\epsilon )$ and $H=\{z\in \mathbb {C}^2:z_2=0\}$ . It can be seen that K is compact and $D=\Omega \setminus K$ is connected. We will show that $S_{d,D}^{\Omega }$ (denoted by $S^d$ for notational convenience) is not plurisubharmonic. For this, we will show that $h=S^d|_{\mathbb {D}^n(0,r)\cap H}$ does not satisfy the maximum principle. In particular, such a restriction is not subharmonic; this, in turn, will imply that $S^d$ is not plurisubharmonic. This is proved via the following steps.

  • We begin by showing that $S^d(0)\geq \tfrac {1}{2}$ .

  • We use Theorem 2.6 to show that

    $$ \begin{align*}S^d(z)^2\leq \dfrac{r-\lvert{z}\rvert}{2-r\lvert{z}\rvert}\end{align*} $$
    for $z\in \mathbb {D}^n(0,r)\cap H,\ z\neq 0$ (observe Remark 2.7).
  • We then show that $S^d(z)\leq S^d(0)$ for $z=(z_1,0)\in \mathbb {D}^n(0,r)\cap H$ for $r>\lvert {z}\rvert >\beta $ , where $\beta ={r(4-r)}/{(4-r^3)}$ (note that $\beta <r$ ).

  • Now we restrict h to $A=\overline {\mathbb {B}(0,\beta )}$ to obtain a maximum at some $a\in A $ .

  • We conclude by combining all these points along with the observation that $S^d(z)\to 0$ as $\lvert {z}\rvert \to r$ .

Lemma 3.2. $S^d(0)\geq \tfrac {1}{2}$ .

Proof. Consider the identity map . Clearly, is injective holomorphic with . We claim that . To see this, take z such that $h_{d,\Omega }(z)<r/2.$ Upon using Result 2.5, we first get $z\in \Omega $ and then $({2z_1}/{r}, {4z_2}/{r^2})\in ~\Omega .$ Now using Lemma 3.1(2), $\lvert {z_1}\rvert <r$ and $\lvert {z_2}\rvert <{r^2}/{4}<r$ . Thus, $z\notin \partial \mathbb {D}^2(0,r)$ and therefore, $z\notin K.$ This proves our claim and shows that $S^d(0)\geq 1/2$ .

We need the following elementary lemma to prove our next proposition.

Lemma 3.3. For each $z=(z_1,0)$ , $z_1=a+ib$ with $0<\lvert {z_1}\rvert <r$ and $w_0=(sz_1,0)$ , where $s={r}/{\sqrt {a^2+b^2}}$ , we have

$$ \begin{align*}\bigg\lvert\frac{\phi_{\tau}(z)-\phi_{\tau}(w_0)}{1-\phi_{\tau}(z)\phi_{\tau}(w_0)}\bigg\rvert \leq \dfrac{r-\lvert{z_1}\rvert}{1-r\lvert{z_1}\rvert},\end{align*} $$

where $\tau \in \mathbb {C}$ with $\lvert \tau \rvert =1$ .

Proof. First note that $\lvert {w_0}\rvert =r$ and $\lvert (2-\tau z_1)(2-\tau w_0)\rvert \geq (2-r)^2>1$ . Now consider

$$ \begin{align*} \left\lvert\dfrac{\phi_{\tau}(z)-\phi_{\tau}(w_0)}{1-\phi_{\tau}(z)\phi_{\tau}(w_0)}\right\rvert&=\left\lvert\dfrac{\dfrac{z_1}{2-\tau z_1}-\dfrac{w_0}{2-\tau w_0}}{1-\dfrac{z_1}{2-\tau z_1}\dfrac{w_0}{2-\tau w_0}}\right\rvert =\left\lvert\dfrac{\dfrac{2(z_1-w_0)}{(2-\tau z_1)(2-\tau w_0)}}{1-\dfrac{z_1}{2-\tau z_1}\dfrac{w_0}{2-\tau w_0}}\right\rvert\\ &\leq \dfrac{2\lvert{z_1-w_0}\rvert}{1-\lvert{z_1}\rvert\lvert{w_0}\rvert} =\dfrac{r-\lvert{z_1}\rvert}{1-\lvert{z_1}\rvert r}.\\[-3.6pc] \end{align*} $$

Proposition 3.4. For each $z=(z_1,0)\in \mathbb {D}^n(0,r)\cap H,\ z\neq 0$ , we have

$$ \begin{align*}S^d(z)^2\leq \dfrac{r-\lvert{z_1}\rvert}{1-r\lvert{z_1}\rvert}.\end{align*} $$

Proof. Let $z_1=a+ib$ . Take $w_0=(sz_1,0)$ , where $s={r}/{\sqrt {a^2+b^2}}$ so that $w\in K$ because $Q<r.$ Now, using Theorem 2.6 and Remark 2.7, we obtain

$$ \begin{align*} S^d(z)^2&\leq d_{c_{\Omega}}^K(z) =\min_{w\in K}\tanh (c_{\Omega}(z,w))\\ &\leq \tanh (c_{\Omega}(z,w_0))\\ &\leq \tanh (c_{G_2}(z,w_0)) \quad (\mbox{since }G_2\subseteq \Omega) \\ &=\bigg\lvert\frac{\phi_{\tau}(z)-\phi_{\tau}(w_0)}{1-\phi_{\tau}(z)\phi_{\tau}(w_0)}\bigg\rvert \quad (\mbox{for some } \lvert\tau\rvert\leq 1)\\ &\leq \dfrac{r-\lvert{z_1}\rvert}{1-r\lvert{z_1}\rvert} \quad (\mbox{using Lemma 3.3}).\\[-3.5pc] \end{align*} $$

This proposition, in particular, implies $S^d(z)\to 0$ as $\lvert {z_1}\rvert \to r$ . We summarise these results with the following theorem.

Theorem 3.5. For D and $\Omega $ as considered above, $S^d$ is not plurisubharmonic.

Proof. It is easy to see that

$$ \begin{align*}\dfrac{r-\lvert{z_1}\rvert}{1-r\lvert{z_1}\rvert}<\dfrac{r^2}{4}\end{align*} $$

if and only if $\lvert {z_1}\rvert>\beta $ . Using Proposition 3.4 and Lemma 3.2, we get $h(z)=S^d(z)<{r}/{2}\leq S^d(0)=h(0)$ for $z=(z_1,0)$ with $\lvert {z_1}\rvert>\beta $ . Consider the restriction $h|_{\overline {\mathbb {B}(0,\beta )}}$ and let $h(a)$ be its maximum for some $a\in {\overline {\mathbb {B}(0,\beta )}}.$ Then, we have $h(z)\leq \max (h(a),h(0))$ on $\mathbb {D}^n(0,r)\cap H$ proving that $S^d|_{\mathbb {D}^n(0,r)\cap H}$ does not satisfy the maximum principle and $S^d$ is not plurisubharmonic.

Acknowledgement

I thank my thesis advisor Sanjay Kumar for reading the manuscript and suggesting changes.

References

Agler, J. and Young, N. J., ‘The hyperbolic geometry of the symmetrized bidisc’, J. Geom. Anal. 14 (2004), 375403.10.1007/BF02922097CrossRefGoogle Scholar
Bharali, G., ‘Non-isotropically balanced domains, Lempert function estimates, and the spectral Nevanlinna–Pick theorem’, Preprint, 2006, arXiv:0601107.Google Scholar
Deng, F., Guan, Q. and Zhang, L., ‘Some properties of squeezing functions on bounded domains’, Pac. J. Appl. Math. 57(2) (2012), 319342.10.2140/pjm.2012.257.319CrossRefGoogle Scholar
Fornæss, J. E. and Shcherbina, N., ‘A domain with non-plurisubharmonic squeezing function’, J. Geom. Anal. 28 (2018), 1321.10.1007/s12220-017-9782-7CrossRefGoogle Scholar
Gupta, N. and Pant, S. K., ‘ $d$ -balanced squeezing function’, Complex Var. Elliptic Equ., to appear. Published online (9 December 2021), DOI:10.1080/17476933.2021.2007380.10.1080/17476933.2021.2007380CrossRefGoogle Scholar
Jarnicki, M. and Pflug, P., Invariant Distances and Metrics in Complex Analysis, 2nd edn (extended), De Gruyter Expositions in Mathematics (De Gruyter, Berlin, 2013).10.1515/9783110253863CrossRefGoogle Scholar
Kosiǹski, L. and Warszawski, T., ‘Lempert theorem for strongly linearly convex domains’, Ann. Polon. Math. 107(2) (2013), 167216.10.4064/ap107-2-5CrossRefGoogle Scholar
Lempert, L., ‘Holomorphic retracts and intrinsic metrics in convex domains’, Anal. Math. 8 (1982), 257261.10.1007/BF02201775CrossRefGoogle Scholar
Nikolov, N., ‘The symmetrized polydisc cannot be exhausted by domains biholomorphic to convex domains’, Ann. Polon. Math. 88 (2006), 279283.10.4064/ap88-3-7CrossRefGoogle Scholar
Rong, F. and Yang, S., ‘On Fridman invariants and generalized squeezing functions’, Chin. Ann. Math. Ser. B 43 (2022), 161174.10.1007/s11401-022-0320-yCrossRefGoogle Scholar
Rong, F. and Yang, S., ‘On the generalized squeezing function and Fridman invariants of special domains’, Ann. Mat. Pura Appl. (4) 201 (2022), 115.10.1007/s10231-021-01179-2CrossRefGoogle Scholar