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Bergman Metrics Overview

Updated 6 January 2026
  • Bergman metrics are canonical Kähler metrics defined via Bergman kernels in bounded domains, serving as biholomorphically invariant measures of complex structure.
  • They exhibit rigidity properties, exemplified by the unit ball case with constant negative curvature, confirming key conjectures in complex geometry.
  • Extensions include weighted and random variants that provide statistical interpretations and finite-dimensional approximations for quantum limit structures.

A Bergman metric is a canonical Kähler metric intrinsically associated with a domain or complex manifold via the Bergman kernel. The rich structure of Bergman metrics, their analytic and geometric properties, and their connections with information geometry and metric equivalence underpin substantial developments in complex analysis, several complex variables, complex differential geometry, and mathematical physics. This article provides a comprehensive view of Bergman metrics, their explicit realizations, rigidity phenomena, weighted and random variants, statistical interpretations, and recent advances.

1. Definition and Construction of the Bergman Metric

Let DCnD \subset \mathbb{C}^n be a bounded domain. The Hilbert space A2(D)A^2(D) consists of square-integrable holomorphic functions with respect to Lebesgue measure. Any orthonormal basis %%%%2%%%% defines the Bergman kernel: KD(z,w)=j=0sj(z)sj(w).K_D(z, w) = \sum_{j=0}^\infty s_j(z)\overline{s_j(w)}. The diagonal KD(z,z)>0K_D(z,z) > 0 is strictly positive. The Bergman metric is the Kähler metric whose potential is logKD(z,z)\log K_D(z, z): gijˉ(z)=2zizˉjlogKD(z,z),g_{i\bar j}(z) = \frac{\partial^2}{\partial z_i \partial \bar z_j} \log K_D(z,z), with associated (1,1)-form

ωB=ii,j=1ngijˉ(z)dzidzˉj.\omega_B = i\sum_{i,j=1}^n g_{i\bar j}(z)\,dz_i\wedge d\bar z_j.

This metric is biholomorphically invariant and is uniquely determined by the complex structure and the underlying measure on the domain (Yum, 2024).

Model Example: Unit Ball

For Bn={z<1}\mathbb{B}^n = \{|z|<1\},

KBn(z,w)=n!πn(1z,w)n1K_{\mathbb{B}^n}(z, w) = \frac{n!}{\pi^n} (1 - \langle z, w\rangle)^{-n-1}

and the Bergman metric has constant negative holomorphic sectional curvature 4-4 (Ganguly et al., 2022).

2. Canonical and Weighted Bergman Metrics

Weighted Bergman spaces generalize classical constructions by introducing a measurable weight w(z)>0w(z)>0, yielding a weighted kernel Kw(z,wˉ)K_w(z, \bar w) and associated metric. Crucially, under an invariant weight assignment M\mathcal{M}, weighted Bergman metrics remain biholomorphically invariant: ωμD=FωμD for F:DD\omega_{\mu_D} = F^*\omega_{\mu_{D'}} \quad \text{ for } F: D \to D' when the weights transform as μDF=hF2μD\mu_{D'}\circ F = |h_F|^2 \mu_D (Yoo, 2024).

Important examples include:

  • Tian's sequence: Assigning powers of the determinant of the Kähler-Einstein metric.
  • Tsuji's dynamical kernel: Inductive constructions where each weight is reciprocal to the preceding Bergman kernel.

On uniform squeezing domains, the Tian-Yau-Zelditch expansion ensures uniform convergence of weighted Bergman metrics to the Kähler-Einstein metric (Yoo, 2024).

3. Rigidity and Curvature Phenomena

Bergman metrics exhibit rigidity: if on a bounded domain the Bergman metric is Kähler-Einstein, then the domain is biholomorphic to the ball. This is a central result answering Yau's question and confirming Cheng's rigidity conjecture in all dimensions (Huang et al., 2016, Savale et al., 2023, Ganguly et al., 2022).

  • Cheng's Conjecture: The Bergman metric is Kähler-Einstein if and only if the domain is biholomorphic to the ball.
  • Ball Quotients: For finite Γ\Gamma and two-dimensional Stein spaces B2/ΓB^2/\Gamma, the Bergman metric is Kähler-Einstein if and only if Γ\Gamma is trivial (Ganguly et al., 2022).
  • Cartan-Hartogs Domains: For MΩ,μM_{\Omega,\mu}, the following are equivalent (Loi et al., 7 Oct 2025):
    • MΩ,μBn+1M_{\Omega,\mu} \simeq \mathbb{B}^{n+1},
    • The Bergman metric is a Kähler-Ricci soliton,
    • After rescaling, the Bergman dual is finitely projectively induced.

The exceptional status of the unit ball is reinforced in settings such as Cartan-Hartogs, Hartogs domains over homogeneous bases, and egg domains over irreducible symmetric bases (Palmieri, 20 Oct 2025).

4. Statistical and Information-Geometric Aspects

An embedding Φ:DP(D)\Phi: D \to \mathcal{P}(D), where P(D)\mathcal{P}(D) is the space of probability measures, allows interpreting the Bergman metric as the pullback of the Fisher information metric: ΦgF=gB,\Phi^* g_F = g_B, with

P(z,ξ)=K(z,ξ)2K(z,z)P(z,\xi) = \frac{|K(z, \xi)|^2}{K(z,z)}

the Poisson–Bergman kernel, yielding a statistical model structure on DD (Cho et al., 2023).

A statistical curvature formula relates holomorphic sectional curvature to the covariance of 2P/P\partial^2 P / P (Cho et al., 2023): Rααˉααˉ(z0)=2Ez0[zαzαP(z0,ξ)2P(z0,ξ)2].R_{\alpha\bar\alpha\alpha\bar\alpha}(z_0) = 2 - \mathbb{E}_{z_0}\left[ \frac{|\partial_{z_\alpha}\partial_{z_\alpha}P(z_0,\xi)|^2}{P(z_0,\xi)^2} \right]. Calabi's diastasis becomes a Bregman-type divergence, enabling analysis of Fréchet means and associated central limit behavior (Cho et al., 2023).

Rigidities utilizing sufficient statistics imply that, under mild regularity, Bergman local isometries must be biholomorphisms (Yum, 2024), and the Schwarz lemma for Bergman metrics can be deduced from Cauchy-Schwarz inequalities in this probabilistic context (Seo et al., 30 Dec 2025).

5. Bergman Metrics as Approximations and Quantum Limit Structures

Bergman metrics also serve as finite-dimensional approximations to infinite-dimensional spaces of Kähler metrics. On polarized Kähler manifolds (M,L,g,x)(M, L, g, x), the Kodaira embedding yields: ωk=ikˉlogKk(z,z)\omega_k = \frac{i}{k} \partial\bar\partial \log K_k(z, z) where KkK_k is the Bergman kernel for LkL^k. Uniform C1,αC^{1,\alpha} convergence holds as kk\to\infty at optimal rates up to O(k2logkα)\mathcal{O}(k^{-2}|\log k|^\alpha) (Zhou, 2021). For symplectic and almost-Kähler manifolds, analogous convergence results hold for Bergman metrics constructed from low-energy eigensections of the Bochner Laplacian, with speed 1/p21/p^2 (Lu et al., 2017).

6. Random Bergman Metrics and Stability

Randomization of Bergman metrics by integrating over finite-dimensional symmetric spaces (SL(Nk,C)/SU(Nk)SL(N_k,\mathbb{C})/SU(N_k)) with Haar measure leads to a family of random metrics, with important physical and geometric interpretations (Ferrari et al., 2011, Klevtsov et al., 2014). Partition functions for random Bergman metrics reveal stability invariants: the critical coupling constant γkcrit\gamma_k^{\rm crit} governs integrability and connects to geodesic stability and large deviations, with explicit expressions in genus-one cases γkcrit=kh\gamma_k^{\rm crit} = k-h (Klevtsov et al., 2014).

Expectation values of random Bergman metrics converge to the background Kähler metric, and higher-point functions display universality and contact phenomena related to the structure of the underlying space of sections.

7. Relationships to Other Invariant Metrics and Open Problems

On bounded convex domains, the Bergman metric, Carathéodory-Reiffen metric, and complete Kähler-Einstein metric of negative scalar curvature are uniformly equivalent but not proportional except on the unit ball Bn\mathbb{B}^n (Cho, 2018). For irreducible bounded symmetric domains in their Harish-Chandra realization, explicit comparison with the generalized Hilbert metric and Finsler norm quantifies distinctions (Falbel et al., 2024):

Metric Type Infinitesimal norm at 0
Carathéodory–Kobayashi maxiσi\max_i \sigma_i
Hilbert (FGW) 2iσi2\sum_i \sigma_i
Bergman γiσi2\sqrt{\gamma \sum_i \sigma_i^2}

Open questions concern the maximal domains where the Bergman dual metric is defined, conjectures on positivity of holomorphic sectional curvature for Stein manifolds, and the explicit metric classification in the presence of singularities (Loi et al., 7 Oct 2025, Huang et al., 2023).


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