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Berezin Sectorial Operators Overview

Updated 13 January 2026
  • Berezin sectorial operators are bounded linear operators on reproducing kernel Hilbert spaces defined via the Berezin transform, emphasizing a refined Berezin range.
  • They generalize classical sectorial operators by replacing the numerical range with a tighter geometric support, which leads to sharper operator inequalities.
  • The framework yields new comparison results and improved spectral estimates, with applications in spaces such as Hardy-Hilbert and Dirichlet.

Berezin sectorial operators constitute a novel class of bounded linear operators on reproducing kernel Hilbert spaces, generalizing classical sectorial operators by means of the Berezin transform. Rather than controlling the numerical range, Berezin sectorial operators are characterized via the geometry of their Berezin range—a typically smaller and subtler region in the complex plane—which leads to distinct operator-theoretic and geometric phenomena. This approach yields new comparison results, sharp inequalities for the Berezin number, and offers novel perspectives on structure and index reduction, particularly in contexts such as the Hardy-Hilbert and Dirichlet spaces (Mahapatra et al., 6 Jan 2026).

1. Formal Definition and Foundational Framework

Let K\mathcal{K} be a reproducing-kernel Hilbert space over a set Ω\Omega, with normalized kernels {k^λ:λΩ}\{\hat{k}_\lambda: \lambda \in \Omega\}. For any TB(K)T \in \mathscr{B}(\mathcal{K}) the Berezin transform of TT is

T~(λ)=Tk^λ,k^λ,Ber(T)={T~(λ):λΩ},ber(T)=supλΩT~(λ).\widetilde{T}(\lambda) = \langle T \hat{k}_\lambda, \hat{k}_\lambda \rangle, \qquad Ber(T) = \{\widetilde{T}(\lambda): \lambda \in \Omega\}, \qquad ber(T) = \sup_{\lambda \in \Omega} |\widetilde{T}(\lambda)|.

Fix an angle θ[0,π2)\theta \in [0, \tfrac{\pi}{2}) and the sector Sθ={zC:argzθ}S_\theta = \{z \in \mathbb{C}: |\arg z| \leq \theta\}. TT is Berezin sectorial of semi-angle θ\theta, denoted TΠθBerT \in \Pi^{Ber}_{\theta}, if

Ber(T)Sθ.Ber(T) \subseteq S_\theta.

Equivalently, for all ϕ<θ|\phi|<\theta, eiϕT~(λ)\widetilde{e^{-i\phi} T}(\lambda) lies in the right half-plane for all λ\lambda.

2. Relationship with Classical Sectorial Operators

Classically, an operator TT on a Hilbert space is sectorial of angle θ\theta if its numerical range

W(T)={Tx,x:x=1}W(T) = \{\langle T x, x \rangle : \|x\|=1\}

satisfies W(T)SθW(T) \subseteq S_\theta. Berezin sectoriality is strictly weaker:

  • In H2(D)H^2(\mathbb{D}), for Dϕ(f)=fϕD_\phi(f)=f'\circ\phi with ϕ(z)=ρz\phi(z)=\rho z, 0<ρ<10<\rho<1, one finds

Ber(Dϕ)=B(0,r1(ρ)),W(Dϕ)=B(0,w(Dϕ))Ber(D_\phi) = \overline{B(0, r_1(\rho))}, \qquad W(D_\phi) = \overline{B(0, w(D_\phi))}

where r1(ρ)r_1(\rho) and w(Dϕ)w(D_\phi) are given by semiexplicit formulas and inequalities. Numerically, r1(ρ)<12Dϕw(Dϕ)r_1(\rho)<\tfrac{1}{2}\|D_\phi\| \leq w(D_\phi), resulting in Ber(Dϕ)W(Dϕ)Ber(D_\phi) \subsetneq W(D_\phi).

  • By adding a real shift αI\alpha I, one constructs operators that are Berezin sectorial but not sectorial in the classical sense. Even when classical sectoriality holds, the Berezin sectorial index (the minimal θ\theta) can be strictly smaller due to the smaller geometric support: the Berezin range may fit inside a cone strictly contained in the one containing the numerical range.

A plausible implication is that operator inequalities or spectral inclusions based on sectoriality can be sharpened when the Berezin transform is considered instead of the numerical range.

3. Berezin Number Inequalities: Angle and Product Bounds

The Berezin number ber(T)ber(T), central to analysis, admits a variety of inequalities for Berezin sectorial operators TΠθBerT\in\Pi^{Ber}_\theta, 0<θ<π20<\theta<\frac{\pi}{2}.

  • Angle lemma: sinθber(T)ber(T)\sin\theta \cdot ber(T) \geq ber(\Im T) This provides a lower bound for the imaginary part in terms of the Berezin number and the sectorial angle.
  • Lower bound for ber(T)ber(T): ber(T)cscθ2ber(T±T)+cscθ2(ber(T)ber(T))ber(T) \geq \frac{\csc\theta}{2} \, ber(\Re T \pm \Im T) + \frac{\csc\theta}{2} \left(ber(\Im T)-ber(\Re T)\right)
  • Product estimate: If TSΠθBerT^* S \in \Pi^{Ber}_\theta, for any α>0\alpha>0,

ber(TS)max{β1,β2}ber(T^* S) \geq \max\{\beta_1, \beta_2\}

with

β1=cscθ2α(S+iαT2berSS+α2TTber)\beta_1 = \frac{\csc\theta}{2\alpha} \left(\||S+i\alpha T|^2\|_{ber} - \|S^* S + \alpha^2 T^* T\|_{ber}\right)

β2=cscθ2α(SS+α2TTberSiαT2ber)\beta_2 = \frac{\csc\theta}{2\alpha} \left(\|S^* S + \alpha^2 T^* T\|_{ber} - \||S-i\alpha T|^2\|_{ber}\right)

  • Norm-type bounds: For invertible SS with STΠθBerS^* T \in \Pi^{Ber}_\theta,

T2ber1/2S1(sinθber(ST)+12TiS2ber)\||T|^2\|_{ber}^{1/2} \leq \|S^{-1}\| \left(\sin \theta\, ber(S^* T) + \frac{1}{2} \||T-iS|^2\|_{ber}\right)

T2ber14(1+sinθ)2ber2(T)+12inftR(TtIber2+TitIber2)\||T|^2\|_{ber} \leq \frac{1}{4}(1+\sin\theta)^2\, ber^2(T) + \frac{1}{2} \inf_{t\in\mathbb{R}}\left(\|T-tI\|_{ber}^2 + \|T-itI\|_{ber}^2 \right)

  • Weak power-type inequalities: For TT in the subclass

ΠθBer,P={TΠθBer:ber(Tn)bern(T),ber(Tn)bern(T)  nN}\Pi^{Ber,P}_\theta = \{ T\in\Pi^{Ber}_\theta : ber(\Re T^n) \leq ber^n(\Re T),\, ber(\Im T^n)\leq ber^n(\Im T)\; \forall n\in\mathbb{N} \}

ber(Tn)(1+sin2θ)n1bern(T),n=1,2,ber(T^n) \leq (1+\sin^2\theta)^{n-1} \, ber^n(T), \qquad n=1, 2, \ldots

Notably, for Toeplitz operators TφT_\varphi on weighted Bergman spaces with harmonic symbol, the power-inequality ber(Tφn)bern(Tφ)ber(T_\varphi^n) \leq ber^n(T_\varphi) is exact.

4. Geometry of the Berezin Range

The structure of Ber(T)Ber(T) strongly influences both sectoriality and inequality sharpness.

  • Finite-rank operators on the Dirichlet space D\mathcal{D}: For T(f)=j=1nf,gjgjT(f) = \sum_{j=1}^n \langle f, g_j \rangle g_j, gjDg_j \in \mathcal{D},

T~(λ)=λ21ln(11λ2)j=1ngj(λ)2R\widetilde{T}(\lambda) = |\lambda|^2\, \frac{1}{\ln\left(\tfrac{1}{1-|\lambda|^2}\right)} \sum_{j=1}^n |g_j(\lambda)|^2 \in \mathbb{R}

Thus Ber(T)RBer(T)\subset \mathbb{R}, an interval, and hence convex in C\mathbb{C}.

  • General symmetry: For T(f)=f,gjhjT(f)=\sum \langle f, g_j \rangle h_j where gj,hjg_j, h_j have real Taylor coefficients, Ber(T)Ber(T) is symmetric about the real axis.
  • Weighted shifts on D\mathcal{D}: For T(anzn)=anβn+1zn+1T(\sum a_n z^n) = \sum a_n \beta_{n+1} z^{n+1}

T~(λ)=λ2λln(1/(1λ2))n=1λ2nβn+1\widetilde{T}(\lambda) = |\lambda|^2\, \frac{\lambda}{\ln(1/(1-|\lambda|^2))} \sum_{n=1}^\infty |\lambda|^{2n} \beta_{n+1}

Symmetry properties vary with the coefficients: real βn\beta_n yield symmetry about the real axis, purely imaginary βn\beta_n about the imaginary axis. For βn=c/n\beta_n = c/n (cDc\in\mathbb{D}), Ber(T)Ber(T) is a disk of radius c|c|.

This suggests that Berezin sectoriality is sensitive to symmetry conditions and spatial supports of the transform.

5. Applications and Operator Examples

Concrete construction of Berezin sectorial operators is illustrated on the Hardy-Hilbert space H2(D)H^2(\mathbb{D}) via composition-differentiation operators

Dϕ(f)=fϕ,ϕ(z)=ρz,  0<ρ<1D_\phi(f) = f' \circ \phi, \qquad \phi(z) = \rho z, \; 0<\rho<1

with explicit calculations of Berezin and numerical ranges showing the existence of operators that are Berezin sectorial but not classical sectorial.

A plausible implication is that Berezin sectoriality permits sharp control for operator families where traditional sectorial tools may fail, especially for operator inequalities and spectral localization.

6. Open Problems and Future Research

The systematic construction of Berezin sectorial composition-differentiation operators on the Dirichlet space remains unresolved. Critical open questions include:

  • For an analytic self-map ϕ\phi of D\mathbb{D}, finding conditions ensuring DϕD_\phi is Berezin sectorial of angle θ\theta but not classically sectorial.
  • Geometric criteria on the Berezin transform that guarantee a strictly smaller Berezin index than the numerical range index for composition-differentiation operators.

These open questions underscore the intricate relationships between Berezin transform geometry, sectoriality indices, and associated operator inequalities, signaling directions for deeper study of functional calculus, spectral theory, and operator geometry (Mahapatra et al., 6 Jan 2026).

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