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Green's Function Comparison Method

Updated 5 January 2026
  • Green's Function Comparison Method is a technique for comparing pluricomplex Green functions on matrix domains using holomorphic symmetrization.
  • It establishes equality for cyclic matrices and strict inequality for derogatory ones through a rigorous analysis of nilpotence and Jordan decomposition.
  • The method integrates pluripotential theory with spectral analysis to differentiate classical invariants like the Carathéodory distance and Green function in higher dimensions.

The Green's function comparison method is a technique for relating the pluricomplex Green functions on two distinct domains linked via a holomorphic mapping, with a particular focus on the spectral ball Ωspec\Omega_{\rm spec} and the symmetrized polydisk GnG_n in several complex variables. Core results establish precise inequalities and characterizations for the Green functions on these domains, especially highlighting the distinction between cyclic (non-derogatory) and derogatory matrices and the role of nilpotence in the behavior of these functions. The method is rigorously developed in Thomas–Trao–Zwonek, "Green functions of the spectral ball and symmetrized polydisk" (Thomas et al., 2010).

1. Spectral Ball, Symmetrized Polydisk, and Symmetrization Map

Let MnM_n denote the space of n×nn \times n complex matrices. The spectral ball is defined as

Ωspec={AMn:ρ(A)<1},\Omega_{\rm spec} = \{ A \in M_n : \rho(A) < 1 \},

where ρ(A)=max{λ:λsp(A)}\rho(A)=\max\{|\lambda|: \lambda \in\operatorname{sp}(A)\} is the spectral radius of AA.

Given the characteristic polynomial PA(t)=det(tIA)=tns1(A)tn1++(1)nsn(A)P_A(t)=\det(tI-A)=t^n - s_1(A) t^{n-1} + \cdots + (-1)^n s_n(A), the symmetrization map

π:ΩspecCn,π(A)=(s1(A),...,sn(A))\pi: \Omega_{\rm spec}\to\mathbb{C}^n, \qquad \pi(A) = (s_1(A),...,s_n(A))

maps AA to the vector of its elementary symmetric functions. The image GnG_n0 is called the symmetrized polydisk, which is a bounded, complete hyperbolic, and hyperconvex domain.

The pluricomplex Green function with pole at GnG_n1 is

GnG_n2

with GnG_n3 for GnG_n4 and GnG_n5 for GnG_n6 (Thomas et al., 2010).

2. Main Comparison Theorem and Inequality

For any GnG_n7, the Green's function on the spectral ball dominates the pullback via symmetrization: GnG_n8 If GnG_n9 is cyclic (non-derogatory), i.e. it has a single Jordan block per eigenvalue, then equality holds for every MnM_n0: MnM_n1 If MnM_n2 is derogatory (it has a repeated eigenvalue and more than one Jordan block per eigenvalue), the inequality is always strict. The difference

MnM_n3

is strictly positive and estimates for this gap depend on the orders of nilpotence in the Jordan decomposition of MnM_n4 (Thomas et al., 2010).

3. Role of Derogatory Poles and Nilpotence

To formalize strictness, conjugate MnM_n5 into Jordan form. For eigenvalue MnM_n6,

MnM_n7

MnM_n8 is derogatory iff for some MnM_n9 one has n×nn \times n0.

For a nilpotent matrix n×nn \times n1, n×nn \times n2, n×nn \times n3, n×nn \times n4. For small perturbation n×nn \times n5,

n×nn \times n6

Homogeneity of the elementary symmetric polynomials yields

n×nn \times n7

Therefore,

n×nn \times n8

is strictly positive for small n×nn \times n9 when Ωspec={AMn:ρ(A)<1},\Omega_{\rm spec} = \{ A \in M_n : \rho(A) < 1 \},0.

For general derogatory Ωspec={AMn:ρ(A)<1},\Omega_{\rm spec} = \{ A \in M_n : \rho(A) < 1 \},1 with repeated eigenvalue Ωspec={AMn:ρ(A)<1},\Omega_{\rm spec} = \{ A \in M_n : \rho(A) < 1 \},2 and Ωspec={AMn:ρ(A)<1},\Omega_{\rm spec} = \{ A \in M_n : \rho(A) < 1 \},3, one applies a Möbius-type automorphism moving Ωspec={AMn:ρ(A)<1},\Omega_{\rm spec} = \{ A \in M_n : \rho(A) < 1 \},4 to Ωspec={AMn:ρ(A)<1},\Omega_{\rm spec} = \{ A \in M_n : \rho(A) < 1 \},5 and repeats the estimation with the same order distinction, confirming strict inequality (Thomas et al., 2010).

4. Isospectral Fibres, Cyclicity, and the Proof Strategy

The Green function Ωspec={AMn:ρ(A)<1},\Omega_{\rm spec} = \{ A \in M_n : \rho(A) < 1 \},6 is constant along fibers of the symmetrization map: Ωspec={AMn:ρ(A)<1},\Omega_{\rm spec} = \{ A \in M_n : \rho(A) < 1 \},7 This invariance under the isospectral equivalence is central. The composition Ωspec={AMn:ρ(A)<1},\Omega_{\rm spec} = \{ A \in M_n : \rho(A) < 1 \},8 is plurisubharmonic on Ωspec={AMn:ρ(A)<1},\Omega_{\rm spec} = \{ A \in M_n : \rho(A) < 1 \},9, ensuring by the maximum property that it is always bounded above by ρ(A)=max{λ:λsp(A)}\rho(A)=\max\{|\lambda|: \lambda \in\operatorname{sp}(A)\}0, yielding the main inequality.

For ρ(A)=max{λ:λsp(A)}\rho(A)=\max\{|\lambda|: \lambda \in\operatorname{sp}(A)\}1 cyclic, the differential ρ(A)=max{λ:λsp(A)}\rho(A)=\max\{|\lambda|: \lambda \in\operatorname{sp}(A)\}2 has maximal rank and ρ(A)=max{λ:λsp(A)}\rho(A)=\max\{|\lambda|: \lambda \in\operatorname{sp}(A)\}3 is a submersion locally. A theorem of Jarnicki–Pflug shows that the pullback of the Green function along a submersion coincides with the Green function of the source, establishing equality for cyclic poles (Thomas et al., 2010).

In the derogatory case, one examines one-parameter families ρ(A)=max{λ:λsp(A)}\rho(A)=\max\{|\lambda|: \lambda \in\operatorname{sp}(A)\}4 tangent to the isospectral fiber. The spectral radius of ρ(A)=max{λ:λsp(A)}\rho(A)=\max\{|\lambda|: \lambda \in\operatorname{sp}(A)\}5 grows as ρ(A)=max{λ:λsp(A)}\rho(A)=\max\{|\lambda|: \lambda \in\operatorname{sp}(A)\}6, but under ρ(A)=max{λ:λsp(A)}\rho(A)=\max\{|\lambda|: \lambda \in\operatorname{sp}(A)\}7, the coordinate growth is ρ(A)=max{λ:λsp(A)}\rho(A)=\max\{|\lambda|: \lambda \in\operatorname{sp}(A)\}8, so the difference in exponents after taking logarithms underscores the strict gap between ρ(A)=max{λ:λsp(A)}\rho(A)=\max\{|\lambda|: \lambda \in\operatorname{sp}(A)\}9 and AA0.

5. Infinitesimal Estimates and Metric Separation in AA1

For domains AA2, the following inequalities relate the (pseudo-)Carathéodory distance AA3, the Green function AA4, and the Lempert function AA5: AA6 On the symmetrized polydisk, novel phenomena appear for AA7. At the origin AA8 and in the “last coordinate” direction AA9,

PA(t)=det(tIA)=tns1(A)tn1++(1)nsn(A)P_A(t)=\det(tI-A)=t^n - s_1(A) t^{n-1} + \cdots + (-1)^n s_n(A)0

where PA(t)=det(tIA)=tns1(A)tn1++(1)nsn(A)P_A(t)=\det(tI-A)=t^n - s_1(A) t^{n-1} + \cdots + (-1)^n s_n(A)1 is the infinitesimal Azukawa metric and PA(t)=det(tIA)=tns1(A)tn1++(1)nsn(A)P_A(t)=\det(tI-A)=t^n - s_1(A) t^{n-1} + \cdots + (-1)^n s_n(A)2 the Carathéodory–Reiffen metric.

For PA(t)=det(tIA)=tns1(A)tn1++(1)nsn(A)P_A(t)=\det(tI-A)=t^n - s_1(A) t^{n-1} + \cdots + (-1)^n s_n(A)3,

PA(t)=det(tIA)=tns1(A)tn1++(1)nsn(A)P_A(t)=\det(tI-A)=t^n - s_1(A) t^{n-1} + \cdots + (-1)^n s_n(A)4

Consequently, for small PA(t)=det(tIA)=tns1(A)tn1++(1)nsn(A)P_A(t)=\det(tI-A)=t^n - s_1(A) t^{n-1} + \cdots + (-1)^n s_n(A)5,

PA(t)=det(tIA)=tns1(A)tn1++(1)nsn(A)P_A(t)=\det(tI-A)=t^n - s_1(A) t^{n-1} + \cdots + (-1)^n s_n(A)6

Thus, the Green function and Carathéodory distance exhibit marked differences for the symmetrized polydisk in dimensions above two. This contrasts with the classical equivalence in the bidisk or the unit ball (Thomas et al., 2010).

6. Significance and Mathematical Context

The Green's function comparison method rigorously quantifies the distinction between the spectral ball and its symmetrized image, particularly through pluripotential-theoretic invariants and their extremal properties on matrix domains. The method demonstrates the central role of cyclicity, nilpotence, and isospectral geometry in the pluricomplex Green function's behavior and exposes deeper structure in fundamental complex-analytic metrics, revealing, for higher dimensions, non-trivial separations between classical objects such as the Carathéodory distance and the pluricomplex Green function (Thomas et al., 2010).

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