alphaFeedback

WorksMathematics

Noncommutative Buzano-Dragomir Inequality and Applications

AI contributions
  • AI
View details

Abstract

Dragomir [Bull. Aust. Math. Soc., 2016] showed that the Buzano inequality holds for orthogonal projections on Hilbert spaces. Dragomir [Linear Multilinear Algebra, 2016] also derived the most general form of the Buzano inequality for bounded linear operators on Hilbert spaces. We show that Dragomir result extends to adjointable morphisms on Hilbert C*-modules. Using this generalization, we derive bounds for the roots of polynomials over commutative unital C*-algebras. We formulate the notion of noncommutative numerical range and derive numerical radius bounds for self-adjoint morphisms on Hilbert C*-modules over unital C*-algebras. We formulate several open problems, including the noncommutative Toeplitz-Hausdorff, von Neumann inequality, Ando inequality, Berger power dilation, Kittaneh inequality, Crouzeix problems.

Introduction

More than half-century ago, Buzano derived the following generalization of the Cauchy-Schwarz inequality [18].

Theorem 1.1. [18, 91] [36] (Buzano Inequality) Let H\mathcal{H} be a complex Hilbert space (with the inner product linear in the first variable and conjugate linear in the second variable). Then

∣⟨τ,h⟩⟨h,ω⟩∣≤∥h∥2(∣⟨τ,ω⟩∣+∥τ∥∥ω∥)2≤∥h∥2∥τ∥∥ω∥,∀h,τ,ω∈H.(1)|\langle\tau,h\rangle\langle h,\omega\rangle| \leq\frac{\|h\|^2\left(|\langle\tau,\omega\rangle|+\|\tau\|\|\omega\|\right)}{2} \leq\|h\|^2\|\tau\|\|\omega\|,\quad\forall h,\tau,\omega\in\mathcal{H}. \tag*{(1)}

In other words,

∣⟨τ,h∥h∥⟩⟨h∥h∥,ω⟩∣≤∣⟨τ,ω⟩∣+∥τ∥∥ω∥2≤∥τ∥∥ω∥,∀τ,ω∈H, ∀h∈H∖{0}.\left|\left\langle\tau,\frac{h}{\lVert h\rVert}\right\rangle\left\langle\frac{h}{\lVert h\rVert},\omega\right\rangle\right|\le\frac{|\langle\tau,\omega\rangle|+\lVert\tau\rVert\lVert\omega\rVert}{2}\le\lVert\tau\rVert\lVert\omega\rVert,\quad\forall\tau,\omega\in\mathcal{H},\ \forall h\in\mathcal{H}\setminus\{0\}.

Further, we have following.

(i) Let τ,ω∈H∖{0}\tau,\omega\in\mathcal{H}\setminus\{0\} be such that ⟨τ,ω⟩=0\langle\tau,\omega\rangle=0. Choose α,β∈C\alpha,\beta\in\mathbb{C} with ∣β∣=1|\beta|=1. Define

hα,β:=α(τ∥τ∥+βω∥ω∥).h_{\alpha,\beta}:=\alpha\left(\frac{\tau}{\lVert\tau\rVert}+\beta\frac{\omega}{\lVert\omega\rVert}\right).

Then

∣⟨τ,hα,β⟩⟨hα,β,ω⟩∣=∥hα,β∥2(∣⟨τ,ω⟩∣+∥τ∥∥ω∥)2.\left|\langle\tau,h_{\alpha,\beta}\rangle\langle h_{\alpha,\beta},\omega\rangle\right|=\frac{\lVert h_{\alpha,\beta}\rVert^2\left(|\langle\tau,\omega\rangle|+\lVert\tau\rVert\lVert\omega\rVert\right)}{2}.

(ii) Let τ,ω∈H∖{0}\tau,\omega\in\mathcal{H}\setminus\{0\} be such that ⟨τ,ω⟩≠0\langle\tau,\omega\rangle\ne0. For α∈C\alpha\in\mathbb{C}, define

hα:=α(τ∥τ∥+⟨τ,ω⟩∣⟨τ,ω⟩∣ω∥ω∥).h_\alpha:=\alpha\left(\frac{\tau}{\lVert\tau\rVert}+\frac{\langle\tau,\omega\rangle}{|\langle\tau,\omega\rangle|}\frac{\omega}{\lVert\omega\rVert}\right).

Then

∣⟨τ,hα⟩⟨hα,ω⟩∣=∥hα∥2(∣⟨τ,ω⟩∣+∥τ∥∥ω∥)2.\left|\langle\tau,h_\alpha\rangle\langle h_\alpha,\omega\rangle\right|=\frac{\lVert h_\alpha\rVert^2\left(|\langle\tau,\omega\rangle|+\lVert\tau\rVert\lVert\omega\rVert\right)}{2}.

Ten years ago, Dragomir made the following far reaching generalization of Theorem 1.1 [29].

Theorem 1.2. [29] (Buzano-Dragomir Inequality) Let H\mathcal{H} be a complex Hilbert space and P:H→HP:\mathcal{H}\to\mathcal{H} be an orthogonal projection. Then

∣⟨Pτ,ω⟩∣≤∣⟨τ,ω⟩∣+∥τ∥∥ω∥2,∀τ,ω∈H.(2)|\langle P\tau,\omega\rangle|\le\frac{|\langle\tau,\omega\rangle|+\lVert\tau\rVert\lVert\omega\rVert}{2},\quad\forall\tau,\omega\in\mathcal{H}. \tag*{(2)}

Now note that for any nonzero h∈Hh\in\mathcal{H}, the map

H∋τ↦⟨τ,h∥h∥⟩h∥h∥∈H\mathcal{H}\ni\tau\mapsto\left\langle\tau,\frac{h}{\lVert h\rVert}\right\rangle\frac{h}{\lVert h\rVert}\in\mathcal{H}

is a rank one orthogonal projection. Thus Inequality (2) recovers Inequality (1). Inequality (1) has various applications, we describe few. Recall that [93] [44, 46, 50, 56] the numerical range of a bounded linear operator T:H→HT:\mathcal{H}\to\mathcal{H} is defined as

WC(T):={⟨Th,h⟩:h∈H, ∥h∥=1}W_{\mathbb{C}}(T):=\{\langle Th,h\rangle:h\in\mathcal{H},\ \lVert h\rVert=1\}

and the numerical radius of TT is defined as

wC(T):=sup⁡h∈H,∥h∥=1∣⟨Th,h⟩∣.w_{\mathbb{C}}(T):=\sup_{h\in\mathcal{H},\lVert h\rVert=1}|\langle Th,h\rangle|.

For τ,ω∈H\tau,\omega\in\mathcal{H}, define the rank one operator

τ⊗ω:H∋h↦(τ⊗ω)h:=⟨h,ω⟩τ∈H.\tau\otimes\omega:\mathcal{H}\ni h\mapsto(\tau\otimes\omega)h:=\langle h,\omega\rangle\tau\in\mathcal{H}.

In 1993, Fujii and Kubo derived following result, using Inequality (1) [36].

Theorem 1.3. [36] Let H\mathcal{H} be a complex Hilbert space and τ,ω∈H\tau,\omega\in\mathcal{H}. Then

wC(τ⊗ω)=∣⟨τ,ω⟩∣+∥τ∥∥ω∥2.w_{\mathbb{C}}(\tau\otimes\omega)=\frac{|\langle\tau,\omega\rangle|+\lVert\tau\rVert\lVert\omega\rVert}{2}.

Let p(z):=a0+a1z+⋯+an−1zn−1+zn∈C[z]p(z):=a_0+a_1z+\cdots+a_{n-1}z^{n-1}+z^n\in\mathbb{C}[z]. A direct observation reveals that the zeros of pp are the eigenvalues of the Frobenius companion matrix

Cp:=(−an−1−an−2−an−3⋯−a2−a1−a0100⋯000010⋯000⋮⋮⋮⋱⋮⋮⋮000⋯000000⋯100000⋯010)∈Mn(C)C_p:=\begin{pmatrix} -a_{n-1} & -a_{n-2} & -a_{n-3} & \cdots& -a_2 & -a_1 & -a_0\\ 1 & 0 & 0 & \cdots& 0 & 0 & 0\\ 0 & 1 & 0 & \cdots& 0 & 0 & 0\\ \vdots& \vdots& \vdots& \ddots& \vdots& \vdots& \vdots\\ 0 & 0 & 0 & \cdots& 0 & 0 & 0\\ 0 & 0 & 0 & \cdots& 1 & 0 & 0\\ 0 & 0 & 0 & \cdots& 0 & 1 & 0 \end{pmatrix}\in\mathrm{M}_n(\mathbb{C})

and the eigenvalues of CpC_p are the same as the zeros of pp. Let RR be the right shift matrix defined by

R:=(000⋯000100⋯000010⋯000⋮⋮⋮⋱⋮⋮000⋯000000⋯100000⋯010)∈Mn(C).R:=\begin{pmatrix} 0 & 0 & 0 & \cdots& 0 & 0 & 0\\ 1 & 0 & 0 & \cdots& 0 & 0 & 0\\ 0 & 1 & 0 & \cdots& 0 & 0 & 0\\ \vdots& \vdots& \vdots& \ddots& \vdots& \vdots\\ 0 & 0 & 0 & \cdots& 0 & 0 & 0\\ 0 & 0 & 0 & \cdots& 1 & 0 & 0\\ 0 & 0 & 0 & \cdots& 0 & 1 & 0 \end{pmatrix}\in\mathrm{M}_n(\mathbb{C}).

Define

a:=(a‾n−1a‾n−2a‾n−3⋮a‾2a‾1a‾0),e1:=(100⋮000).\mathbf{a}:=\begin{pmatrix} \overline{a}_{n-1}\\ \overline{a}_{n-2}\\ \overline{a}_{n-3}\\ \vdots\\ \overline{a}_2\\ \overline{a}_1\\ \overline{a}_0 \end{pmatrix},\quad \mathbf{e}_1:=\begin{pmatrix} 1\\ 0\\ 0\\ \vdots\\ 0\\ 0\\ 0 \end{pmatrix}.

Then

Cp=R−e1⊗a.(3)C_p=R-\mathbf{e}_1\otimes\mathbf{a}. \tag*{(3)}

Fujii and Kubo derived following bound for the zeros of pp using Inequality 1 and the representation (3) [36].

Theorem 1.4. [36] (Fujii-Kubo polynomial root upper bound) Let p(z):=a0+a1z+⋯+an−1zn−1+zn∈C[z]p(z):=a_0+a_1z+\cdots+a_{n-1}z^{n-1}+z^n\in\mathbb{C}[z]. If λ\lambda is a zero of pp, then

∣λ∣≤wC(R)+∑j=0n−1∣aj∣2+∣an−1∣2=cos⁡(πn+1)+∑j=0n−1∣aj∣2+∣an−1∣2.(4)|\lambda|\leq w_{\mathbb{C}}(R)+\frac{\sqrt{\sum_{j=0}^{n-1}|a_j|^2+|a_{n-1}|}}{2}=\cos\left(\frac{\pi}{n+1}\right)+\frac{\sqrt{\sum_{j=0}^{n-1}|a_j|^2+|a_{n-1}|}}{2}. \tag*{(4)}

Let p(z):=a0+a1z+⋯+an−1zn−1+zn∈C[z]p(z):=a_0+a_1z+\cdots+a_{n-1}z^{n-1}+z^n\in\mathbb{C}[z] with a0≠0a_0\ne0. Define

q(z):=1a0znp(1z)=1a0+an−1a0z+⋯+a1a0zn−1+zn∈C[z].q(z):=\frac{1}{a_0}z^np\left(\frac{1}{z}\right)=\frac{1}{a_0}+\frac{a_{n-1}}{a_0}z+\cdots+\frac{a_1}{a_0}z^{n-1}+z^n\in\mathbb{C}[z].

We note that λ∈C∖{0}\lambda\in\mathbb{C} \setminus\{0\} satisfies p(λ)=0p(\lambda)=0 if and only if q(1/λ)=0q(1/\lambda)=0 [56]. Frobenius companion matrix of qq is

Cq:=(−a1a0−a2a0−a3a0⋯−an−1a0−ana0−1a0100⋯000010⋯000⋮⋮⋮⋮⋮⋮000⋯000000⋯100000⋯010)∈Mn(C)C_q := \begin{pmatrix} -\frac{a_1}{a_0} & -\frac{a_2}{a_0} & -\frac{a_3}{a_0} & \cdots& -\frac{a_{n-1}}{a_0} & -\frac{a_n}{a_0} & -\frac{1}{a_0} \\ 1 & 0 & 0 & \cdots& 0 & 0 & 0 \\ 0 & 1 & 0 & \cdots& 0 & 0 & 0 \\ \vdots& \vdots& \vdots& & \vdots& \vdots& \vdots\\ 0 & 0 & 0 & \cdots& 0 & 0 & 0 \\ 0 & 0 & 0 & \cdots& 1 & 0 & 0 \\ 0 & 0 & 0 & \cdots& 0 & 1 & 0 \end{pmatrix} \in M_n(\mathbb{C})

By applying Theorem 1.4 to qq, we get following result.

Theorem 1.5. [36] (Fujii-Kubo polynomial root lower bound) Let p(z):=a0+a1z+⋯+an−1zn−1+anzn∈C[z]p(z):=a_0+a_1z+\cdots+a_{n-1}z^{n-1}+a_nz^n\in\mathbb{C}[z] with a0≠0a_0\ne0. If λ\lambda is a zero of pp, then

∣λ∣≥2∣a0∣2∣a0∣cos⁡(πn+1)+1+∑j=1n−1∣aj∣2+∣a1∣|\lambda| \ge\frac{2|a_0|}{2|a_0|\cos\left(\frac{\pi}{n+1}\right)+\sqrt{1+\sum_{j=1}^{n-1}|a_j|^2}+|a_1|}

For any bounded linear operator T:H→HT:\mathcal{H}\to\mathcal{H}, the Cauchy-Schwarz inequality gives

wC(T)≤∥T∥.(5)w_{\mathbb{C}}(T)\le\|T\|. \tag*{(5)}

In 2007, Dragomir strengthened Inequality (5) using Buzano inequality [30].

Theorem 1.6. [30] (Dragomir Numerical Radius Inequality) Let T:H→HT:\mathcal{H}\to\mathcal{H} be a bounded linear operator. Then

wC(T)≤12wC(T2)+∥T∥2≤∥T∥.w_{\mathbb{C}}(T)\le\frac{1}{\sqrt{2}}\sqrt{w_{\mathbb{C}}(T^2)+\|T\|^2}\le\|T\|.

Our fundamental motivation comes from the following question: What is the noncommutative analogue of Theorem 1.2? This is then naturally connected with the notion of Hilbert C*-modules which are first introduced by Kaplansky [58] for modules over commutative C*-algebras and later developed for modules over arbitrary C*-algebras by Paschke [81] and Rieffel [88].

Definition 1.7. [81, 88] [58] Let A\mathcal{A} be a unital C*-algebra. A right module E\mathcal{E} over A\mathcal{A} is said to be a semi-inner product C*-module if there exists a map ⟨⋅,⋅⟩:E×E→A\langle\cdot,\cdot\rangle:\mathcal{E}\times\mathcal{E}\to\mathcal{A} such that the following hold.

(i) ⟨x,x⟩≥0\langle x,x\rangle\ge0, ∀x∈E\forall x\in\mathcal{E}.

(ii) ⟨x+y,z⟩=⟨x,z⟩+⟨y,z⟩\langle x+y,z\rangle=\langle x,z\rangle+\langle y,z\rangle, ∀x,y,z∈E\forall x,y,z\in\mathcal{E}.

(iii) ⟨x,ya⟩=⟨x,y⟩a\langle x,ya\rangle=\langle x,y\rangle a, ∀x,y∈E\forall x,y\in\mathcal{E}, ∀a∈A\forall a\in\mathcal{A}.

(iv) ⟨x,y⟩=⟨y,x⟩∗\langle x,y\rangle=\langle y,x\rangle^*, ∀x,y∈E\forall x,y\in\mathcal{E}.

Semi-inner product C*-modules satisfy noncommutative Cauchy-Schwarz inequality.

Theorem 1.8. [68] (Kaplansky-Paschke-Rieffel Inequality) Let E\mathcal{E} be a semi-inner product C*-module. Then

⟨y,x⟩⟨x,y⟩≤∥⟨x,x⟩∥⟨y,y⟩,∀x,y∈E.\langle y,x\rangle\langle x,y\rangle\le\|\langle x,x\rangle\|\langle y,y\rangle,\quad\forall x,y\in\mathcal{E}.

In particular,

∥⟨y,x⟩∥2≤∥⟨x,x⟩∥∥⟨y,y⟩∥,∀x,y∈E.\|\langle y,x\rangle\|^2\le\|\langle x,x\rangle\|\|\langle y,y\rangle\|,\quad\forall x,y\in\mathcal{E}.

Definition 1.9. [68] A semi-inner product C∗C^*-module E\mathcal{E} is said to be an inner product C∗C^*-module if x∈Ex \in\mathcal{E} satisfies ⟨x,x⟩=0\langle x,x\rangle= 0, then x=0x = 0.

Definition 1.10. [68] A inner product C∗C^*-module E\mathcal{E} is said to be Hilbert C∗C^*-module if E\mathcal{E} is complete w.r.t. the norm ∥x∥:=∥⟨x,x⟩∥\|x\| := \sqrt{\|\langle x,x\rangle\|}, ∀x∈E\forall x \in\mathcal{E}.

In 2012, Khosravi, Drnovsek and Moslehian derived noncommutative version of Inequality (1) [61].

Theorem 1.11. [61] (Buzano-Khosravi-Drnovsek-Moslehian Inequality) Let E\mathcal{E} be a Hilbert C∗C^*-module. Then

∥⟨ω,x⟩⟨x,τ⟩∥≤∥⟨τ,ω⟩∥+∥τ∥∥ω∥2≤∥τ∥∥ω∥,∀τ,ω∈E, ∀x∈E with ⟨x,x⟩=1.(6)\|\langle\omega,x\rangle\langle x,\tau\rangle\| \le\frac{\|\langle\tau,\omega\rangle\|+\|\tau\|\|\omega\|}{2} \le\|\tau\|\|\omega\|,\qquad\forall\tau,\omega\in\mathcal{E},\ \forall x \in\mathcal{E}\text{ with }\langle x,x\rangle=1. \tag*{(6)}

In this article, we show that Theorem 1.2 extends to orthogonal projections on Hilbert C∗C^*-modules (which will also generalize Theorem 1.11). We also derive modular analogue of Theorems 1.4 and 1.6.

Noncommutative Buzano-Dragomir Inequality

We start by deriving noncommutative analogue of Theorem 1.2.

Theorem 2.1. (Noncommutative Buzano-Dragomir Inequality) Let E\mathcal{E} be a Hilbert C∗C^*-module over a unital C∗C^*-algebra A\mathcal{A} and P:E→EP:\mathcal{E}\to\mathcal{E} be an orthogonal projection. Then

∥⟨τ,Pω⟩∥≤∥⟨τ,ω⟩∥+∥τ∥∥ω∥2,∀τ,ω∈E.\|\langle\tau,P\omega\rangle\| \le\frac{\|\langle\tau,\omega\rangle\|+\|\tau\|\|\omega\|}{2},\qquad\forall\tau,\omega\in\mathcal{E}.

Proof. We find

∥2⟨τ,Pω⟩−⟨τ,ω⟩∥=∥⟨τ,2Pω−ω⟩∥≤∥τ∥∥2Pω−ω∥.\|2\langle\tau,P\omega\rangle-\langle\tau,\omega\rangle\|=\|\langle\tau,2P\omega-\omega\rangle\|\le\|\tau\|\|2P\omega-\omega\|.

We now find

∥2Pω−ω∥2=∥⟨2Pω−ω,2Pω−ω⟩∥=∥4⟨Pω,Pω⟩−2⟨Pω,ω⟩−2⟨ω,Pω⟩+⟨ω,ω⟩∥=∥⟨ω,ω⟩∥=∥ω∥2.\begin{aligned} \|2P\omega-\omega\|^2 &= \|\langle2P\omega-\omega,2P\omega-\omega\rangle\|\\ &=\|4\langle P\omega,P\omega\rangle-2\langle P\omega,\omega\rangle-2\langle\omega,P\omega\rangle+\langle\omega,\omega\rangle\|\\ &=\|\langle\omega,\omega\rangle\|\\ &=\|\omega\|^2. \end{aligned}

Therefore

2∥⟨τ,Pω⟩∥−∥⟨τ,ω⟩∥≤∥2⟨τ,Pω⟩−⟨τ,ω⟩∥≤∥τ∥∥ω∥.2\|\langle\tau,P\omega\rangle\|-\|\langle\tau,\omega\rangle\|\le\|2\langle\tau,P\omega\rangle-\langle\tau,\omega\rangle\|\le\|\tau\|\|\omega\|.

Corollary 2.2. Theorem 1.11 follows from Theorem 2.1.

Proof. Let E\mathcal{E} be a Hilbert C∗C^*-module and x∈Ex\in\mathcal{E} with ⟨x,x⟩=1\langle x,x\rangle=1. Define

P:E∋y↦Py:=x⟨x,y⟩∈E.P:\mathcal{E}\ni y\mapsto Py:=x\langle x,y\rangle\in\mathcal{E}.

Then PP is an orthogonal projection. Theorem 2.1 gives

∥⟨τ,x⟩⟨x,ω⟩∥=∥⟨τ,x⟨x,ω⟩⟩∥=∥⟨τ,Pω⟩∥≤∥⟨τ,ω⟩∥+∥τ∥∥ω∥2,∀τ,ω∈E.\|\langle\tau,x\rangle\langle x,\omega\rangle\|=\|\langle\tau,x\langle x,\omega\rangle\rangle\|=\|\langle\tau,P\omega\rangle\| \le\frac{\|\langle\tau,\omega\rangle\|+\|\tau\|\|\omega\|}{2},\qquad\forall\tau,\omega\in\mathcal{E}.

In 2016, Dragomir further improved Theorem 1.2 for bounded linear operators [28].

Theorem 2.3. [28] (Buzano-Dragomir Inequality) Let H\mathcal{H} be a complex Hilbert space and T:H→HT:\mathcal{H}\to\mathcal{H} be a bounded linear operator. Then

∣⟨Tτ,Tω⟩∣≤∥T∥2(∣⟨τ,ω⟩∣+∥τ∥∥ω∥)2,∀τ,ω∈H.|\langle T\tau,T\omega\rangle|\leq\frac{\lVert T\rVert^{2}(|\langle\tau,\omega\rangle|+\lVert\tau\rVert\lVert\omega\rVert)}{2},\qquad\forall\tau,\omega\in\mathcal{H}.

We now derive following noncommutative version of Theorem 2.3.

Theorem 2.4. (Noncommutative Buzano-Dragomir Inequality) Let E\mathcal{E} be a Hilbert C∗C^*-module over a unital C∗C^*-algebra A\mathcal{A} and T:E→ET:\mathcal{E}\to\mathcal{E} be an adjointable morphism. Then

∥⟨Tτ,Tω⟩∥≤∥T∥2∥⟨τ,ω⟩∥+∥⟨τ,τ⟩∥T∥2−⟨Tτ,Tτ⟩∥12∥⟨ω,ω⟩∥T∥2−⟨Tω,Tω⟩∥12,∀τ,ω∈E.\lVert\langle T\tau,T\omega\rangle\rVert\leq\lVert T\rVert^{2}\lVert\langle\tau,\omega\rangle\rVert+\left\lVert\langle\tau,\tau\rangle\lVert T\rVert^{2}-\langle T\tau,T\tau\rangle\right\rVert^{\frac{1}{2}}\left\lVert\langle\omega,\omega\rangle\lVert T\rVert^{2}-\langle T\omega,T\omega\rangle\right\rVert^{\frac{1}{2}},\qquad\forall\tau,\omega\in\mathcal{E}.

Proof. Our proof is motivated by the Hilbert space argument due to Dragomir [28]. Let T:E→ET:\mathcal{E}\to\mathcal{E} be an adjointable morphism and τ,ω∈E\tau,\omega\in\mathcal{E}. Define

[⋅,⋅]:E×E∋(x,y)↦[x,y]:=⟨x,y⟩∥T∥2−⟨Tx,Ty⟩∈A.[\cdot,\cdot]:\mathcal{E}\times\mathcal{E}\ni(x,y)\mapsto[x,y]:=\langle x,y\rangle\lVert T\rVert^{2}-\langle Tx,Ty\rangle\in\mathcal{A}.

Then [⋅,⋅][\cdot,\cdot] is a semi-inner product. By applying Theorem 1.8 to this semi-inner product, we get

∥[x,y]∥2≤∥[x,x]∥∥[y,y]∥,∀x,y∈E.\lVert[x,y]\rVert^{2}\leq\lVert[x,x]\rVert\lVert[y,y]\rVert,\qquad\forall x,y\in\mathcal{E}.

In particular,

∥[τ,ω]∥2≤∥[τ,τ]∥∥[ω,ω]∥.\lVert[\tau,\omega]\rVert^{2}\leq\lVert[\tau,\tau]\rVert\lVert[\omega,\omega]\rVert.

Previous inequality gives

∥⟨τ,ω⟩∥T∥2−⟨Tτ,Tω⟩∥2≤∥⟨τ,τ⟩∥T∥2−⟨Tτ,Tτ⟩∥∥⟨ω,ω⟩∥T∥2−⟨Tω,Tω⟩∥.\left\lVert\langle\tau,\omega\rangle\lVert T\rVert^{2}-\langle T\tau,T\omega\rangle\right\rVert^{2}\leq\left\lVert\langle\tau,\tau\rangle\lVert T\rVert^{2}-\langle T\tau,T\tau\rangle\right\rVert\left\lVert\langle\omega,\omega\rangle\lVert T\rVert^{2}-\langle T\omega,T\omega\rangle\right\rVert.

Therefore

∥⟨Tτ,Tω⟩∥−∥T∥2∥⟨τ,ω⟩∥≤∥⟨τ,ω⟩∥T∥2−⟨Tτ,Tω⟩∥≤∥⟨τ,τ⟩∥T∥2−⟨Tτ,Tτ⟩∥12∥⟨ω,ω⟩∥T∥2−⟨Tω,Tω⟩∥12.\begin{aligned} \lVert\langle T\tau,T\omega\rangle\rVert-\lVert T\rVert^{2}\lVert\langle\tau,\omega\rangle\rVert\leq\left\lVert\langle\tau,\omega\rangle\lVert T\rVert^{2}-\langle T\tau,T\omega\rangle\right\rVert\\ &\leq\left\lVert\langle\tau,\tau\rangle\lVert T\rVert^{2}-\langle T\tau,T\tau\rangle\right\rVert^{\frac{1}{2}}\left\lVert\langle\omega,\omega\rangle\lVert T\rVert^{2}-\langle T\omega,T\omega\rangle\right\rVert^{\frac{1}{2}}. \end{aligned}

We are unable to simplify Theorem 2.4. We therefore ask following problem.

Problem 2.5. Let E\mathcal{E} be a Hilbert C∗C^*-module over a unital C∗C^*-algebra A\mathcal{A} and T:E→ET:\mathcal{E}\to\mathcal{E} be an adjointable morphism. Whether

∥⟨Tτ,Tω⟩∥≤∥T∥2(∥⟨τ,ω⟩∥+∥τ∥∥ω∥)2,∀τ,ω∈E?\lVert\langle T\tau,T\omega\rangle\rVert\leq\frac{\lVert T\rVert^{2}(\lVert\langle\tau,\omega\rangle\rVert+\lVert\tau\rVert\lVert\omega\rVert)}{2},\qquad\forall\tau,\omega\in\mathcal{E}?

Let E\mathcal{E} be a Hilbert C∗C^*-module over a unital C∗C^*-algebra A\mathcal{A}. Similar to Hilbert space case, we define the noncommutative numerical range of an adjointable morphism T:E→ET:\mathcal{E}\to\mathcal{E} is defined as

WA(T):={⟨x,Tx⟩:x∈E,⟨x,x⟩=1}⊆AW_{\mathcal{A}}(T):=\{\langle x,Tx\rangle:x\in\mathcal{E},\langle x,x\rangle=1\}\subseteq\mathcal{A}

and the noncommutative numerical radius TT is defined as

wA(T):=sup⁡x∈E,⟨x,x⟩=1∥⟨x,Tx⟩∥≥0.w_{\mathcal{A}}(T):=\sup_{x\in\mathcal{E},\langle x,x\rangle=1}\lVert\langle x,Tx\rangle\rVert\geq0.

Note that our definition of numerical range and radius on Hilbert C*-modules differ from the existing same notion on Hilbert C*-modules [76, 86, 105] We give various examples. In all following examples, A\mathcal{A} is a unital C*-algebra.

Example 2.6. Let b∈Ab \in\mathcal{A}. Then

WA(b)={a∗ba:a∈A,a∗a=1}W_{\mathcal{A}}(b)=\{a^{*}ba:a\in\mathcal{A},a^{*}a=1\}

and

wA(b)=sup⁡{∥a∗ba∥:a∈A,a∗a=1}w_{\mathcal{A}}(b)=\sup\{\lVert a^{*}ba\rVert:a\in\mathcal{A},a^{*}a=1\}
=∥b∥.=\lVert b\rVert.

If A\mathcal{A} is commutative, then WA(b)={b}W_{\mathcal{A}}(b)=\{b\}.

Example 2.7. Let d∈Nd\in\mathbb{N} and IdI_d be the identity matrix of size dd by dd. Then we have

WA(Id)={⟨x,x⟩:x∈Ad,⟨x,x⟩=1}={1}W_{\mathcal{A}}(I_d)=\{\langle x,x\rangle:x\in\mathcal{A}^{d},\langle x,x\rangle=1\}=\{1\}

and

wA(Id)=1.w_{\mathcal{A}}(I_d)=1.

Example 2.8. Define

M:=(0100).M:=\begin{pmatrix}0&1\\0&0\end{pmatrix}.

Then

WA(M)={⟨x,Mx⟩:x∈A2,⟨x,x⟩=1}W_{\mathcal{A}}(M)=\{\langle x,Mx\rangle:x\in\mathcal{A}^{2},\langle x,x\rangle=1\}
={a∗b:a,b∈A,a∗a+b∗b=1}=\{a^{*}b:a,b\in\mathcal{A},a^{*}a+b^{*}b=1\}

and

wA(M)=sup⁡{∥a∗b∥:a,b∈A,a∗a+b∗b=1}.w_{\mathcal{A}}(M)=\sup\{\lVert a^{*}b\rVert:a,b\in\mathcal{A},a^{*}a+b^{*}b=1\}.

We note that

a∗bb∗a≤a∗a+b∗b2,∀a,b∈A.a^{*}bb^{*}a\leq\frac{a^{*}a+b^{*}b}{2},\qquad\forall a,b\in\mathcal{A}.

Therefore

wA(M)=sup⁡{∥a∗b∥:a,b∈A,a∗a+b∗b=1}w_{\mathcal{A}}(M)=\sup\{\lVert a^{*}b\rVert:a,b\in\mathcal{A},a^{*}a+b^{*}b=1\}
≤12sup⁡{∥a∗a+b∗b∥:a,b∈A,a∗a+b∗b=1}\leq\frac{1}{\sqrt{2}}\sup\{\sqrt{\lVert a^{*}a+b^{*}b\rVert}:a,b\in\mathcal{A},a^{*}a+b^{*}b=1\}
=12.=\frac{1}{\sqrt{2}}.

Example 2.9. Let d∈Nd\in\mathbb{N} and b1,…,bd∈Ab_1,\ldots,b_d\in\mathcal{A}. Define diag⁡((bj)j=1d)\operatorname{diag}((b_j)_{j=1}^{d}) as the diagonal matrix with diagonal entries b1,…,bdb_1,\ldots,b_d. Then

WA(diag⁡((bj)j=1d))={∑j=1daj∗bjaj:(aj)j=1d∈Ad,∑j=1daj∗aj=1}W_{\mathcal{A}}\left(\operatorname{diag}\left((b_j)_{j=1}^{d}\right)\right) = \left\{ \sum_{j=1}^{d}a_j^{*}b_ja_j:(a_j)_{j=1}^{d}\in\mathcal{A}^{d},\sum_{j=1}^{d}a_j^{*}a_j=1 \right\}

and

wA(diag⁡((bj)j=1d))=sup⁡{∥∑j=1daj∗bjaj∥:(aj)j=1d∈Ad, ∑j=1daj∗aj=1}≤∑j=1d∥bj∥.\begin{aligned} w_{\mathcal{A}}(\operatorname{diag}((b_j)_{j=1}^{d}))=\sup\left\{\left\|\sum_{j=1}^{d}a_j^{*}b_ja_j\right\|:(a_j)_{j=1}^{d}\in\mathcal{A}^{d},\ \sum_{j=1}^{d}a_j^{*}a_j=1\right\} \\ &\leq\sum_{j=1}^{d}\lVert b_j\rVert. \end{aligned}

The set WA(diag⁡((bj)j=1d))W_{\mathcal{A}}(\operatorname{diag}((b_j)_{j=1}^{d})) is the C∗C^{*}-convex hull of {bj}j=1d\{b_j\}_{j=1}^{d} [71].

Example 2.10. Let R∈Md(A)R\in\mathbb{M}_{d}(\mathcal{A}) be the right shift matrix defined by

R:=(000⋯000100⋯000010⋯000⋮⋮⋮⋱⋮⋮⋮000⋯000000⋯100000⋯010).R:=\begin{pmatrix} 0 & 0 & 0 & \cdots& 0 & 0 & 0\\ 1 & 0 & 0 & \cdots& 0 & 0 & 0\\ 0 & 1 & 0 & \cdots& 0 & 0 & 0\\ \vdots& \vdots& \vdots& \ddots& \vdots& \vdots& \vdots\\ 0 & 0 & 0 & \cdots& 0 & 0 & 0\\ 0 & 0 & 0 & \cdots& 1 & 0 & 0\\ 0 & 0 & 0 & \cdots& 0 & 1 & 0 \end{pmatrix}.

Thus the action of RR is

R((aj)j=1d)=(0,a1,a2,…,ad−1),∀(aj)j=1d∈Ad.R((a_j)_{j=1}^{d})=(0,a_1,a_2,\ldots,a_{d-1}),\quad\forall(a_j)_{j=1}^{d}\in\mathcal{A}^{d}.

We then have

⟨(aj)j=1d,R(aj)j=1d⟩=a2∗a1+⋯+ad∗ad−1,∀(aj)j=1d∈Ad.\left\langle(a_j)_{j=1}^{d},R(a_j)_{j=1}^{d}\right\rangle=a_2^{*}a_1+\cdots+a_d^{*}a_{d-1},\quad\forall(a_j)_{j=1}^{d}\in\mathcal{A}^{d}.

Hence

∥⟨(aj)j=1d,R(aj)j=1d⟩∥=∥a2∗a1+⋯+ad∗ad−1∥≤∥∑j=2daj∗aj∥12∥∑k=1d−1ak∗ak∥12≤∥∑j=1daj∗aj∥12∥∑k=1dak∗ak∥12=∥∑j=1daj∗aj∥,∀(aj)j=1d∈Ad.\begin{aligned} \left\|\left\langle(a_j)_{j=1}^{d},R(a_j)_{j=1}^{d}\right\rangle\right\|=\left\|a_2^{*}a_1+\cdots+a_d^{*}a_{d-1}\right\| \\ &\leq\left\|\sum_{j=2}^{d}a_j^{*}a_j\right\|^{\frac{1}{2}}\left\|\sum_{k=1}^{d-1}a_k^{*}a_k\right\|^{\frac{1}{2}} \\ &\leq\left\|\sum_{j=1}^{d}a_j^{*}a_j\right\|^{\frac{1}{2}}\left\|\sum_{k=1}^{d}a_k^{*}a_k\right\|^{\frac{1}{2}} \\ &=\left\|\sum_{j=1}^{d}a_j^{*}a_j\right\|,\quad\forall(a_j)_{j=1}^{d}\in\mathcal{A}^{d}. \end{aligned}

Therefore

WA(R)={a2∗a1+⋯+ad∗ad−1:(aj)j=1d∈Ad, ∑j=1daj∗aj=1}W_{\mathcal{A}}(R)=\left\{a_2^{*}a_1+\cdots+a_d^{*}a_{d-1}:(a_j)_{j=1}^{d}\in\mathcal{A}^{d},\ \sum_{j=1}^{d}a_j^{*}a_j=1\right\}

and

wA(R)=sup⁡{∥a2∗a1+⋯+ad∗ad−1∥:(aj)j=1d∈Ad, ∑j=1daj∗aj=1}w_{\mathcal{A}}(R)=\sup\left\{\left\|a_2^{*}a_1+\cdots+a_d^{*}a_{d-1}\right\|:(a_j)_{j=1}^{d}\in\mathcal{A}^{d},\ \sum_{j=1}^{d}a_j^{*}a_j=1\right\}
≤1.\leq1.

Example 2.11. Let AA be a unital C∗C^*-algebra and ℓ2(A)\ell^2(A) be the standard Hilbert C∗C^*-module defined by

ℓ2(A):={{an}n=1∞:an∈A, ∀n∈N, ∑n=1∞an∗an∈A}.\ell^2(A):=\left\{\{a_n\}_{n=1}^{\infty}:a_n\in A,\ \forall n\in\mathbb{N},\ \sum_{n=1}^{\infty}a_n^*a_n\in A\right\}.

equipped with inner product

⟨{an}n=1∞,{bn}n=1∞⟩:=∑n=1∞an∗bn,∀{an}n=1∞,{bn}n=1∞∈ℓ2(A).\left\langle\{a_n\}_{n=1}^{\infty},\{b_n\}_{n=1}^{\infty}\right\rangle:=\sum_{n=1}^{\infty}a_n^*b_n,\quad\forall\{a_n\}_{n=1}^{\infty},\{b_n\}_{n=1}^{\infty}\in\ell^2(A).

and norm

∥{an}n=1∞∥=∥∑n=1∞an∗an∥12,∀{an}n=1∞∈ℓ2(A).\left\|\{a_n\}_{n=1}^{\infty}\right\|=\left\|\sum_{n=1}^{\infty}a_n^*a_n\right\|^{\frac{1}{2}},\quad\forall\{a_n\}_{n=1}^{\infty}\in\ell^2(A).

Let LL be the left shift morphism defined by

L:ℓ2(A)∋{an}n=1∞↦L{an}n=1∞:={an+1}n=1∞∈ℓ2(A).L:\ell^2(A)\ni\{a_n\}_{n=1}^{\infty}\mapsto L\{a_n\}_{n=1}^{\infty}:=\{a_{n+1}\}_{n=1}^{\infty}\in\ell^2(A).

Then

WA(L)={∑n=1∞an∗an+1:{an}n=1∞∈ℓ2(A), ∑n=1∞an∗an=1}.W_A(L)=\left\{\sum_{n=1}^{\infty}a_n^*a_{n+1}:\{a_n\}_{n=1}^{\infty}\in\ell^2(A),\ \sum_{n=1}^{\infty}a_n^*a_n=1\right\}.

and

wA(L)=sup⁡{∥∑n=1∞an∗an+1∥:{an}n=1∞∈ℓ2(A), ∑n=1∞an∗an=1}≤1.w_A(L)=\sup\left\{\left\|\sum_{n=1}^{\infty}a_n^*a_{n+1}\right\|:\{a_n\}_{n=1}^{\infty}\in\ell^2(A),\ \sum_{n=1}^{\infty}a_n^*a_n=1\right\}\leq1.

Example 2.12. Define

A:=(abcd).A:=\begin{pmatrix}a&b\\c&d\end{pmatrix}.

Then

WA(A)={x∗ax+x∗by+y∗cx+y∗dy:x,y∈A, x∗x+y∗y=1}.W_A(A)=\{x^*ax+x^*by+y^*cx+y^*dy:x,y\in A,\ x^*x+y^*y=1\}.

and

wA(A)=sup⁡{∥x∗ax+x∗by+y∗cx+y∗dy∥:x,y∈A, x∗x+y∗y=1}≤∥a∥+∥b∥+∥c∥+∥d∥.w_A(A)=\sup\{\|x^*ax+x^*by+y^*cx+y^*dy\|:x,y\in A,\ x^*x+y^*y=1\} \leq\|a\|+\|b\|+\|c\|+\|d\|.

Given r>0r>0 and v∈Av\in A, the closed disc centered at v∈Av\in A of radius rr is defined as

DA[v,r]:={z∈A:∥z−v∥≤r}.D_A[v,r]:=\{z\in A:\|z-v\|\leq r\}.

Following are basic properties of noncommutative numerical range and radius.

Proposition 2.13. Let E\mathcal{E} be a Hilbert C∗C^*-module over a unital C∗C^*-algebra AA. Let A+A^+ be the set of all positive elements in AA. Let T,S:E→ET,S:\mathcal{E}\to\mathcal{E} be adjointable morphisms and a,b∈Aa,b\in A. Let II be the identity morphism on E\mathcal{E}.

(i) WA(T)⊆DA[0,∥T∥]W_A(T)\subseteq D_A[0,\|T\|].

(ii) 0≤wA(T)≤∥T∥0\leq w_A(T)\leq\|T\|.

(iii) WA(T+S)⊆WA(T)+WA(S)W_A(T+S)\subseteq W_A(T)+W_A(S).

(iv) wA(S+T)≤wA(S)+wA(T)w_A(S+T)\leq w_A(S)+w_A(T).

  • (v) WA(Ta)=WA(T)aW_A(Ta)=W_A(T)a.

  • (vi) wA(Ta)≤∥a∥wA(T)w_A(Ta)\le\lVert a\rVert w_A(T).

  • (vii) WA(T∗)=(WA(T))∗W_A(T^*)=(W_A(T))^*.

  • (viii) wA(T∗)=wA(T)w_A(T^*)=w_A(T).

  • (ix) WA(Ta+bI)=WA(T)a+bW_A(Ta+bI)=W_A(T)a+b.

  • (x) WA(Re⁡(T))=Re⁡(WA(T))W_A(\operatorname{Re}(T))=\operatorname{Re}(W_A(T)) and WA(Im⁡(T))=Im⁡(WA(T))W_A(\operatorname{Im}(T))=\operatorname{Im}(W_A(T)).

  • (xi) If T≥0T\ge0, then WA(T)⊆A+W_A(T)\subseteq A^+.

  • (xii) Let E0\mathcal{E}_0 be a Hilbert C∗C^*-module over a unital C∗C^*-algebra AA such that E\mathcal{E} is orthogonally complementable in E0\mathcal{E}_0. If an adjointable morphism V:E0→E0V:\mathcal{E}_0\to\mathcal{E}_0 is a dilation of TT, then WA(T)⊆WA(V)W_A(T)\subseteq W_A(V).

  • (xiii) Let E1\mathcal{E}_1 be an orthogonally complementable closed submodule in E\mathcal{E}. Let P:E→E1P:\mathcal{E}\to\mathcal{E}_1 be an onto orthogonal projection. Then WA(PT∣E1)⊆WA(T)W_A(P T|_{\mathcal{E}_1})\subseteq W_A(T).

  • (xiv) WA(U∗TU)=WA(T)W_A(U^*TU)=W_A(T) for every unitary morphism U:E→EU:\mathcal{E}\to\mathcal{E}.

  • (xv) Let a∈Aa\in A be such that there exists a x∈Ex\in\mathcal{E} with Tx=xaTx=xa and ⟨x,x⟩=1\langle x,x\rangle=1. Then a∈WA(T)a\in W_A(T). In other words,

σ1(T):={a∈A:∃x∈E,Tx=xa,⟨x,x⟩=1}⊆WA(T)\sigma_1(T):=\{a\in A:\exists x\in\mathcal{E},Tx=xa,\langle x,x\rangle=1\}\subseteq W_A(T)

and

∥a∥≤wA(T),∀a∈σ1(T).\lVert a\rVert\le w_A(T),\qquad\forall a\in\sigma_1(T).
  • (xvi)

wA(ST+TS)≤wA((S+T)2)+wA((S−T)2)2.w_A(ST+TS)\le\frac{w_A((S+T)^2)+w_A((S-T)^2)}{2}.

In particular, if ST=TSST=TS, then

wA(ST)≤wA((S+T)2)+wA((S−T)2)4.w_A(ST)\le\frac{w_A((S+T)^2)+w_A((S-T)^2)}{4}.
  • (xvii) If a sequence {Tn}n=1∞\{T_n\}_{n=1}^{\infty} of adjointable morphisms on E\mathcal{E} converges to an adjointable morphism TT on E\mathcal{E} in the morphism norm, then the sequence {wA(Tn)}n=1∞\{w_A(T_n)\}_{n=1}^{\infty} converges to wA(T)w_A(T) in the norm.

Using generalized polarization identity, it is known that wC(T)≥∥T∥/2w_C(T)\ge\lVert T\rVert/2 [46]. We are unable to derive noncommutative version of this result. For τ,ω∈E\tau,\omega\in\mathcal{E}, define the morphism

τ⊗ω:E∋x↦(τ⊗ω)x:=τ⟨ω,x⟩∈E.\tau\otimes\omega:\mathcal{E}\ni x\mapsto(\tau\otimes\omega)x:=\tau\langle\omega,x\rangle\in\mathcal{E}.

Following is modular version of Theorem 1.3.

Theorem 2.14. Let E\mathcal{E} be a Hilbert C∗C^*-module over a commutative unital C∗C^*-algebra AA and τ,ω∈E\tau,\omega\in\mathcal{E}. Then

wA(τ⊗ω)≤∥⟨τ,ω⟩∥+∥τ∥∥ω∥2≤∥τ∥∥ω∥.(7)w_A(\tau\otimes\omega)\le\frac{\lVert\langle\tau,\omega\rangle\rVert+\lVert\tau\rVert\lVert\omega\rVert}{2}\le\lVert\tau\rVert\lVert\omega\rVert. \tag*{(7)}

In particular,

wA(τ⊗τ)≤∥τ∥2.w_A(\tau\otimes\tau)\le\lVert\tau\rVert^2.

Proof. Let τ,ω∈E\tau,\omega\in\mathcal{E}. Let x∈Ex\in\mathcal{E} with ⟨x,x⟩=1\langle x,x\rangle=1. Then using commutativity of C∗C^*-algebra,

∥⟨x,(τ⊗ω)x⟩∥=∥⟨x,τ⟨ω,x⟩⟩∥=∥⟨x,τ⟩⟨ω,x⟩∥\lVert\langle x,(\tau\otimes\omega)x\rangle\rVert=\lVert\langle x,\tau\langle\omega,x\rangle\rangle\rVert=\lVert\langle x,\tau\rangle\langle\omega,x\rangle\rVert
=∥⟨ω,x⟩⟨x,ω⟩∥≤∥⟨τ,ω⟩∥+∥τ∥∥ω∥2.=\lVert\langle\omega,x\rangle\langle x,\omega\rangle\rVert\le\frac{\lVert\langle\tau,\omega\rangle\rVert+\lVert\tau\rVert\lVert\omega\rVert}{2}.

Therefore

wA(τ⊗ω)≤∥⟨τ,ω⟩∥+∥τ∥∥ω∥2.w_A(\tau\otimes\omega) \le\frac{\left\|\langle\tau,\omega\rangle\right\|+\|\tau\|\|\omega\|}{2}.

Unlike the Hilbert space case, we are unable to derive equality in Inequality (7). Let A\mathcal{A} be a unital C*-algebra and p(z):=a0+a1z+⋯+an−1zn−1+zn∈A[z]p(z):=a_0+a_1z+\cdots+a_{n-1}z^{n-1}+z^n\in\mathcal{A}[z]. Define the modular Frobenius companion matrix

Cp:=(−an−1−an−2−an−3⋯−a2−a1−a0100⋯000010⋯000⋮⋮⋮⋱⋮⋮⋮000⋯000000⋯100000⋯010)∈Mn(A).C_p:=\begin{pmatrix} -a_{n-1} & -a_{n-2} & -a_{n-3} & \cdots& -a_2 & -a_1 & -a_0\\ 1 & 0 & 0 & \cdots& 0 & 0 & 0\\ 0 & 1 & 0 & \cdots& 0 & 0 & 0\\ \vdots& \vdots& \vdots& \ddots& \vdots& \vdots& \vdots\\ 0 & 0 & 0 & \cdots& 0 & 0 & 0\\ 0 & 0 & 0 & \cdots& 1 & 0 & 0\\ 0 & 0 & 0 & \cdots& 0 & 1 & 0 \end{pmatrix}\in M_n(\mathcal{A}).

Given n∈Nn\in\mathbb{N}, we consider An\mathcal{A}^n with the standard inner product

⟨(aj)j=1n,(bj)j=1n⟩:=∑j=1naj∗bj,∀(aj)j=1n,(bj)j=1n∈An.\left\langle(a_j)_{j=1}^n,(b_j)_{j=1}^n\right\rangle:=\sum_{j=1}^n a_j^*b_j,\quad\forall(a_j)_{j=1}^n,(b_j)_{j=1}^n\in\mathcal{A}^n.

Hence the norm on An\mathcal{A}^n is

∥(aj)j=1n∥=∥∑j=1naj∗aj∥12,∀(aj)j=1n∈An.\left\|(a_j)_{j=1}^n\right\|=\left\|\sum_{j=1}^n a_j^*a_j\right\|^{\frac{1}{2}},\quad\forall(a_j)_{j=1}^n\in\mathcal{A}^n.

We then have the following result.

Theorem 2.15. Let A\mathcal{A} be a commutative unital C*-algebra and p(z):=a0+a1z+⋯+an−1zn−1+zn∈A[z]p(z):=a_0+a_1z+\cdots+a_{n-1}z^{n-1}+z^n\in\mathcal{A}[z]. If b∈Ab\in\mathcal{A} satisfies p(b)=0p(b)=0, then b∈WA(Cp)b\in W_{\mathcal{A}}(C_p).

Proof. Define

x:=(bn−1bn−2bn−3⋮b2b1)(∑j=0n−1(b∗)jbj)−12.x:=\begin{pmatrix} b^{n-1}\\ b^{n-2}\\ b^{n-3}\\ \vdots\\ b^2\\ b\\ 1 \end{pmatrix}\left(\sum_{j=0}^{n-1}(b^*)^jb^j\right)^{-\frac{1}{2}}.

Then ⟨x,x⟩=1\langle x,x\rangle=1. Using commutativity of C*-algebra, we have

⟨x,Cpx⟩=⟨(bn−1bn−2bn−3⋮b2b1)(∑j=0n−1(b∗)jbj)−12,(−an−1−an−2−an−3⋯−a2−a1−a0100⋯000010⋯000⋮⋮⋮⋱⋮⋮⋮000⋯000000⋯100000⋯010)(bn−1bn−2bn−3⋮b2b1)(∑j=0n−1(b∗)jbj)−12⟩=(∑j=0n−1(b∗)jbj)−12⟨(bn−1bn−2bn−3⋮b2b1),(−an−1−an−2−an−3⋯−a2−a1−a0100⋯000010⋯000⋮⋮⋮⋱⋮⋮⋮000⋯000000⋯100000⋯010)(bn−1bn−2bn−3⋮b2b1)⟩(∑j=0n−1(b∗)jbj)−12=(∑j=0n−1(b∗)jbj)−12⟨(bn−1bn−2bn−3⋮b2b1),(−∑j=0n−1ajbjbn−1bn−2⋮b3b2b)⟩(∑j=0n−1(b∗)jbj)−12=(∑j=0n−1(b∗)jbj)−12⟨(bn−1bn−2bn−3⋮b2b1),(bnbn−1bn−2⋮b3b2b)⟩(∑j=0n−1(b∗)jbj)−12=(∑j=0n−1(b∗)jbj)−12⟨(bn−1bn−2bn−3⋮b2b1),(bn−1bn−2bn−3⋮b2b1)⟩b(∑j=0n−1(b∗)jbj)−12=(∑j=0n−1(b∗)jbj)−12(∑j=0n−1(b∗)jbj)b(∑j=0n−1(b∗)jbj)−12=(∑j=0n−1(b∗)jbj)−12(∑j=0n−1(b∗)jbj)(∑j=0n−1(b∗)jbj)−12b=b.(8)\begin{aligned} \langle x,C_p x\rangle &= \left\langle \begin{pmatrix} b^{n-1}\\ b^{n-2}\\ b^{n-3}\\ \vdots\\ b^2\\ b\\ 1 \end{pmatrix} \left(\sum_{j=0}^{n-1}(b^*)^j b^j\right)^{-\frac{1}{2}}, \begin{pmatrix} -a_{n-1} & -a_{n-2} & -a_{n-3} & \cdots& -a_2 & -a_1 & -a_0\\ 1 & 0 & 0 & \cdots& 0 & 0 & 0\\ 0 & 1 & 0 & \cdots& 0 & 0 & 0\\ \vdots& \vdots& \vdots& \ddots& \vdots& \vdots& \vdots\\ 0 & 0 & 0 & \cdots& 0 & 0 & 0\\ 0 & 0 & 0 & \cdots& 1 & 0 & 0\\ 0 & 0 & 0 & \cdots& 0 & 1 & 0 \end{pmatrix} \begin{pmatrix} b^{n-1}\\ b^{n-2}\\ b^{n-3}\\ \vdots\\ b^2\\ b\\ 1 \end{pmatrix} \left(\sum_{j=0}^{n-1}(b^*)^j b^j\right)^{-\frac{1}{2}} \right\rangle\\ &= \left(\sum_{j=0}^{n-1}(b^*)^j b^j\right)^{-\frac{1}{2}} \left\langle \begin{pmatrix} b^{n-1}\\ b^{n-2}\\ b^{n-3}\\ \vdots\\ b^2\\ b\\ 1 \end{pmatrix}, \begin{pmatrix} -a_{n-1} & -a_{n-2} & -a_{n-3} & \cdots& -a_2 & -a_1 & -a_0\\ 1 & 0 & 0 & \cdots& 0 & 0 & 0\\ 0 & 1 & 0 & \cdots& 0 & 0 & 0\\ \vdots& \vdots& \vdots& \ddots& \vdots& \vdots& \vdots\\ 0 & 0 & 0 & \cdots& 0 & 0 & 0\\ 0 & 0 & 0 & \cdots& 1 & 0 & 0\\ 0 & 0 & 0 & \cdots& 0 & 1 & 0 \end{pmatrix} \begin{pmatrix} b^{n-1}\\ b^{n-2}\\ b^{n-3}\\ \vdots\\ b^2\\ b\\ 1 \end{pmatrix} \right\rangle \left(\sum_{j=0}^{n-1}(b^*)^j b^j\right)^{-\frac{1}{2}}\\ &= \left(\sum_{j=0}^{n-1}(b^*)^j b^j\right)^{-\frac{1}{2}} \left\langle \begin{pmatrix} b^{n-1}\\ b^{n-2}\\ b^{n-3}\\ \vdots\\ b^2\\ b\\ 1 \end{pmatrix}, \begin{pmatrix} -\sum_{j=0}^{n-1}a_jb^j\\ b^{n-1}\\ b^{n-2}\\ \vdots\\ b^3\\ b^2\\ b \end{pmatrix} \right\rangle \left(\sum_{j=0}^{n-1}(b^*)^j b^j\right)^{-\frac{1}{2}}\\ &= \left(\sum_{j=0}^{n-1}(b^*)^j b^j\right)^{-\frac{1}{2}} \left\langle \begin{pmatrix} b^{n-1}\\ b^{n-2}\\ b^{n-3}\\ \vdots\\ b^2\\ b\\ 1 \end{pmatrix}, \begin{pmatrix} b^n\\ b^{n-1}\\ b^{n-2}\\ \vdots\\ b^3\\ b^2\\ b \end{pmatrix} \right\rangle \left(\sum_{j=0}^{n-1}(b^*)^j b^j\right)^{-\frac{1}{2}}\\ &= \left(\sum_{j=0}^{n-1}(b^*)^j b^j\right)^{-\frac{1}{2}} \left\langle \begin{pmatrix} b^{n-1}\\ b^{n-2}\\ b^{n-3}\\ \vdots\\ b^2\\ b\\ 1 \end{pmatrix}, \begin{pmatrix} b^{n-1}\\ b^{n-2}\\ b^{n-3}\\ \vdots\\ b^2\\ b\\ 1 \end{pmatrix} \right\rangle b\left(\sum_{j=0}^{n-1}(b^*)^j b^j\right)^{-\frac{1}{2}}\\ &= \left(\sum_{j=0}^{n-1}(b^*)^j b^j\right)^{-\frac{1}{2}} \left(\sum_{j=0}^{n-1}(b^*)^j b^j\right)b \left(\sum_{j=0}^{n-1}(b^*)^j b^j\right)^{-\frac{1}{2}}\\ &= \left(\sum_{j=0}^{n-1}(b^*)^j b^j\right)^{-\frac{1}{2}} \left(\sum_{j=0}^{n-1}(b^*)^j b^j\right) \left(\sum_{j=0}^{n-1}(b^*)^j b^j\right)^{-\frac{1}{2}}b\\ &=b. \tag*{(8)} \end{aligned}

Therefore b=⟨x,Cpx⟩∈WA(Cp)b=\langle x,C_p x\rangle\in W_A(C_p).

We now derive modular analogue of Theorem 1.4.

Theorem 2.16. Let A\mathcal{A} be a commutative unital C∗C^*-algebra and p(z):=a0+a1z+⋯+an−1zn−1+zn∈A[z]p(z):=a_0+a_1z+\cdots+a_{n-1}z^{n-1}+z^n\in\mathcal{A}[z]. If b∈Ab\in\mathcal{A} satisfies p(b)=0p(b)=0, then

∥b∥≤wA(R)+∥∑j=0n−1aj∗aj∥+∥an−1∥2\lVert b\rVert\le w_{\mathcal{A}}(R)+\frac{\sqrt{\left\lVert\sum_{j=0}^{n-1}a_j^*a_j\right\rVert}+\lVert a_{n-1}\rVert}{2}
≤wA(R)+∑j=0n−1∥aj∥2+∥an−1∥2,\le w_{\mathcal{A}}(R)+\frac{\sqrt{\sum_{j=0}^{n-1}\lVert a_j\rVert^2}+\lVert a_{n-1}\rVert}{2},

where RR is the right shift matrix defined by

R:=(000⋯000100⋯000010⋯000⋮⋮⋮⋱⋮⋮⋮000⋯000000⋯100000⋯010)∈Mn(A).R:=\begin{pmatrix} 0&0&0&\cdots&0&0&0\\ 1&0&0&\cdots&0&0&0\\ 0&1&0&\cdots&0&0&0\\ \vdots&\vdots&\vdots&\ddots&\vdots&\vdots&\vdots\\ 0&0&0&\cdots&0&0&0\\ 0&0&0&\cdots&1&0&0\\ 0&0&0&\cdots&0&1&0 \end{pmatrix}\in\mathbb{M}_n(\mathcal{A}).

Proof. Define

a:=((an−1)∗(an−2)∗(an−3)∗⋮(a2)∗(a1)∗(a0)∗)∈An,e1:=(100⋮000)∈An.\mathbf{a}:=\begin{pmatrix} (a_{n-1})^*\\ (a_{n-2})^*\\ (a_{n-3})^*\\ \vdots\\ (a_2)^*\\ (a_1)^*\\ (a_0)^* \end{pmatrix}\in\mathcal{A}^n,\quad \mathbf{e}_1:=\begin{pmatrix} 1\\ 0\\ 0\\ \vdots\\ 0\\ 0\\ 0 \end{pmatrix}\in\mathcal{A}^n.

Then

Cp=R−e1⊗a.(9)C_p=R-\mathbf{e}_1\otimes\mathbf{a}. \tag*{(9)}

Using (8) and Inequality (7), we get

∥b∥≤wA(Cp)=wA(R−e1⊗a)≤wA(R)+wA(e1⊗a)≤wA(R)+∥∑j=0n−1aj∗aj∥+∥an−1∥2≤wA(R)+∑j=0n−1∥aj∥2+∥an−1∥2.\begin{aligned} \lVert b\rVert\le w_{\mathcal{A}}(C_p) =w_{\mathcal{A}}(R-\mathbf{e}_1\otimes\mathbf{a}) \le w_{\mathcal{A}}(R)+w_{\mathcal{A}}(\mathbf{e}_1\otimes\mathbf{a}) \\ &\le w_{\mathcal{A}}(R)+\frac{\sqrt{\left\lVert\sum_{j=0}^{n-1}a_j^*a_j\right\rVert}+\lVert a_{n-1}\rVert}{2} \le w_{\mathcal{A}}(R)+\frac{\sqrt{\sum_{j=0}^{n-1}\lVert a_j\rVert^2}+\lVert a_{n-1}\rVert}{2}. \end{aligned}

Let A\mathcal{A} be a commutative unital C∗^*-algebra. Let p(z):=a0+a1z+⋯+an−1zn−1+zn∈A[z]p(z):=a_0+a_1z+\cdots+a_{n-1}z^{n-1}+z^n\in\mathcal{A}[z] with a0a_0 invertible. Define

q(z):=1a0znp(1z)=1a0+an−1a0z+⋯+a1a0zn−1+zn∈A[z].q(z):=\frac{1}{a_0}z^np\left(\frac{1}{z}\right)=\frac{1}{a_0}+\frac{a_{n-1}}{a_0}z+\cdots+\frac{a_1}{a_0}z^{n-1}+z^n\in\mathcal{A}[z].

We note that an invertible element b∈Ab\in\mathcal{A} satisfies p(b)=0p(b)=0 if and only if q(1/b)=0q(1/b)=0. Frobenius companion matrix of qq is

Cq:=(−a1a0−a2a0−a3a0⋯−an−1a0−an−1a0−1a0100⋯000010⋯000⋮⋮⋮⋱⋮⋮⋮000⋯000000⋯100000⋯010)∈Mn(A).C_q:= \begin{pmatrix} -\frac{a_1}{a_0} & -\frac{a_2}{a_0} & -\frac{a_3}{a_0} & \cdots& -\frac{a_{n-1}}{a_0} & -\frac{a_{n-1}}{a_0} & -\frac{1}{a_0}\\ 1 & 0 & 0 & \cdots& 0 & 0 & 0\\ 0 & 1 & 0 & \cdots& 0 & 0 & 0\\ \vdots& \vdots& \vdots& \ddots& \vdots& \vdots& \vdots\\ 0 & 0 & 0 & \cdots& 0 & 0 & 0\\ 0 & 0 & 0 & \cdots& 1 & 0 & 0\\ 0 & 0 & 0 & \cdots& 0 & 1 & 0 \end{pmatrix}\in M_n(\mathcal{A}).

By applying Theorem 4 to qq, we get following result.

Theorem 2.17. Let A\mathcal{A} be a commutative unital C∗^*-algebra and p(z):=a0+a1z+⋯+an−1zn−1+zn∈A[z]p(z):=a_0+a_1z+\cdots+a_{n-1}z^{n-1}+z^n\in\mathcal{A}[z] with a0a_0 invertible. If an invertible element b∈Ab\in\mathcal{A} satisfies p(b)=0p(b)=0, then

1∥b−1∥≥22wA(R)+∥(a0−1)∗a0−1+∑j=1n−1(aja0−1)∗aja0−1∥2+∥a1a0−1∥2.\frac{1}{\lVert b^{-1}\rVert}\geq\frac{2}{2w_{\mathcal{A}}(R)+\sqrt{\left\lVert(a_0^{-1})^*a_0^{-1}+\sum_{j=1}^{n-1}(a_ja_0^{-1})^*a_ja_0^{-1}\right\rVert^2+\lVert a_1a_0^{-1}\rVert^2}}.

Equality term in (4) comes from the numerical radius of right shift matrix obtained by Davidson and Holbrook [25] (also see [48,59]). We are unable to do this for the right shift matrix over C∗^*-algebras. We now derive Theorem 1.6 for Hilbert C∗^*-modules.

Theorem 2.18. (Modular Dragomir Numerical Radius Inequality) Let E\mathcal{E} be a Hilbert C∗^*-module over a unital C∗^*-algebra A\mathcal{A} and T:E→ET:\mathcal{E}\to\mathcal{E} be a self-adjoint morphism. Then

wA(T)≤12wA(T2)+∥T∥2≤12∥T2∥+∥T∥2≤∥T∥.w_{\mathcal{A}}(T)\leq\frac{1}{\sqrt{2}}\sqrt{w_{\mathcal{A}}(T^2)+\lVert T\rVert^2}\leq\frac{1}{\sqrt{2}}\sqrt{\lVert T^2\rVert+\lVert T\rVert^2}\leq\lVert T\rVert.

Proof. Let x∈Ex\in\mathcal{E} with ⟨x,x⟩=1\langle x,x\rangle=1. Then using Inequality (6) and the self-adjointness of TT, we get

∥⟨x,Tx⟩∥2=∥⟨x,Tx⟩⟨x,Tx⟩∗∥=∥⟨x,Tx⟩⟨Tx,x⟩∥=∥⟨Tx,x⟩⟨x,Tx⟩∥≤∥⟨Tx,x⟩∥+∥Tx∥∥Tx∥2=∥⟨x,T2x⟩∥+∥Tx∥∥T∗x∥2≤∥⟨x,T2x⟩∥+∥T∥∥x∥∥T∥∥x∥2=∥⟨x,T2x⟩∥+∥T∥22≤sup⁡y∈E,⟨y,y⟩=1∥⟨y,T2y⟩∥+∥T∥22=wA(T2)+∥T∥22.\begin{aligned} \lVert\langle x,Tx\rangle\rVert^2=\lVert\langle x,Tx\rangle\langle x,Tx\rangle^*\rVert=\lVert\langle x,Tx\rangle\langle Tx,x\rangle\rVert\\ &=\lVert\langle Tx,x\rangle\langle x,Tx\rangle\rVert\leq\frac{\lVert\langle Tx,x\rangle\rVert+\lVert Tx\rVert\lVert Tx\rVert}{2} \\ &=\frac{\lVert\langle x,T^2x\rangle\rVert+\lVert Tx\rVert\lVert T^*x\rVert}{2}\leq\frac{\lVert\langle x,T^2x\rangle\rVert+\lVert T\rVert\lVert x\rVert\lVert T\rVert\lVert x\rVert}{2} \\ &=\frac{\lVert\langle x,T^2x\rangle\rVert+\lVert T\rVert^2}{2}\leq\frac{\sup_{y\in\mathcal{E},\langle y,y\rangle=1}\lVert\langle y,T^2y\rangle\rVert+\lVert T\rVert^2}{2} \\ &=\frac{w_{\mathcal{A}}(T^2)+\lVert T\rVert^2}{2}. \end{aligned}

Therefore

wA(T)=sup⁡x∈E,⟨x,x⟩=1∥⟨x,Tx⟩∥≤12wA(T2)+∥T∥2≤12∥T2∥+∥T∥2≤∥T∥.w_{\mathcal{A}}(T)=\sup_{x\in\mathcal{E},\langle x,x\rangle=1}\lVert\langle x,Tx\rangle\rVert\leq\frac{1}{\sqrt{2}}\sqrt{w_{\mathcal{A}}(T^2)+\lVert T\rVert^2}\leq\frac{1}{\sqrt{2}}\sqrt{\lVert T^2\rVert+\lVert T\rVert^2}\leq\lVert T\rVert.

Note that we derived Theorem 2.18 only for self-adjoint morphisms. We are unable to derive Theorem 2.18 for arbitrary adjointable morphisms. We also note that in the case of self-adjoint operator TT on Hilbert spaces, we have wC(T)=∥T∥w_{\mathrm{C}}(T)=\lVert T\rVert [46] which we can’t say for self-adjoint morphisms on Hilbert C*-modules.

Noncommutative Toeplitz-Hausdorff Problem

Motivated from several breakthrough results in numerical range and radius, we formulate following problems. What is noncommutative

  1. Toeplitz-Hausdorff Theorem (fundamental theorem of the numerical range) [26, 74, 78, 85, 92, 97] [34, 45, 46, 47, 50, 51]?

  2. Wintner spectral inclusion theorem for numerical range [8, 102] [46]?

  3. Halmos-Bernau-Smithies-Berger power inequality [11, 82]?

  4. Alpin-Chien-Yeh inequality [6]?

  5. Kittaneh inequalities [63, 64]?

  6. Yamazaki inequality [104]?

  7. Kittaneh-Moslehian-Yamazaki inequality [66]?

  8. Abu-Omar-Kittaneh inequality [3]?

  9. Bhunia-Bag-Paul inequality [12]?

  10. elliptical range theorem [17, 70]?

  11. Berger power dilation for numerical contraction [9, 10, 95] [46]?

  12. Ando theorem for numerical contraction [7]?

  13. Furuta-Nakamoto theorem for numerical contractions [37]?

  14. El-Haddad-Kittaneh numerical radius inequality [33]?

  15. description of numerical range of 3×33 \times3 matrices [60]?

  16. description of numerical range of 4×44 \times4 matrices [39]?

  17. Holbrook numerical radius inequalities for the product of commuting matrices [54]?

  18. Okubo-Ando numerical radius inequalities for the product of commuting matrices [77, 80] [55]?

  19. Bouldin numerical radius inequalities for the product of commuting matrices [14, 15]?

  20. Poncelet property for numerical ranges [4, 103] [41]?

  21. Anderson theorem [31, 96] [44]?

  22. Kippenhahn boundary generating curve theorem [35, 62]?

  23. Kippenhahn corner-point theorem [35, 62]?

  24. Hildebrandt normal eigenvalue theorem [16] [53]?

  25. Hildebrandt intersection theorem [101] [38]?

  26. Marcus-Shure description for the numerical range of zero-one matrices [72] and Davidson-Holbrook estimate for the numerical radius of zero-one matrices [25]?

  27. Johnson numerical range inclusion theorem [57]?

  28. Choi-Li constrained numerical range theorem [20]?

  29. Wang-Wu-Gau result for Crawford number [100]?

  30. Abu-Omar-Kittaneh inequality (involving generalized Aluthge transform) [1]?

  31. Gau-Wu numerical radius equality characterizations [43]?

  32. Gau-Wu theorem for compact operators [42]?

  33. Perron-Frobenius type results on the numerical range [73]?

(34) Helton-Spitkovsky characterization of shapes of numerical ranges [52]?

(35) Radjabalipour-Radjavi result on numerical ranges [84]?

(36) Pollack theorem on numerical ranges [83]?

(37) Anderson result on numerical ranges [5]?

(38) Abu-Omar-Kittaneh numerical radius inequalities for the product of matrices [2]?

(39) Kittaneh-Moradi inequality [65]?

(40) Lancaster characterization for the closedness of numerical range [67]?

(41) Gau-Wu characterization for numerical ranges of completely non-unitary contractions [40]?

(42) Mees-Atherton domains containing numerical ranges [75]?

(43) Chien-Tam characterizations of circularity of numerical ranges [19]?

(44) Shiu theorem on the growth of numerical range of powers of operator [90]?

Noncommutative Crouzeix Inequality, von Neumann inequality and Ando inequality Problems

Breakthrough Crouzeix theorem says following.

Theorem 4.1. [13, 22, 23, 24, 87] (Crouzeix Theorem) For every d∈Nd \in\mathbb{N} and for every matrix M∈Md(C)M \in\mathrm{M}_{d}(\mathbb{C}), we have

(Crouzeix-Palencia Inequality)

∥p(M)∥≤(1+2)sup⁡{∣p(z)∣:z∈WC(M)},∀p∈C[z].\lVert p(M)\rVert\le(1+\sqrt{2})\sup\{\lvert p(z)\rvert: z \in W_{\mathbb{C}}(M)\}, \quad\forall p \in\mathbb{C}[z].

We formulate following problem.

Problem 4.2. (Noncommutative Crouzeix Problem) Let AA be a unital C∗C^{*}-algebra. Whether there is a universal constant RAR_{A} (which may depend upon AA) satisfying following: For every d∈Nd \in\mathbb{N} and for every matrix M∈Md(A)M \in\mathrm{M}_{d}(A), we have

∥p(M)∥≤RAsup⁡{∥p(z)∥:z∈WA(M)},∀p∈A[z].\lVert p(M)\rVert\le R_{A}\sup\{\lVert p(z)\rVert: z \in W_{A}(M)\}, \quad\forall p \in A[z].

An inequality which is very close to Crouzeix inequality is the von Neumann inequality.

Theorem 4.3. [27, 79, 94, 95, 99] (von Neumann Theorem) For every d∈Nd \in\mathbb{N} and for every matrix M∈Md(C)M \in\mathrm{M}_{d}(\mathbb{C}) with ∥M∥≤1\lVert M\rVert\le1, we have

(von Neumann Inequality)

∥p(M)∥≤sup⁡{∣p(z)∣:z∈C,∣z∣≤1},∀p∈C[z].\lVert p(M)\rVert\le\sup\{\lvert p(z)\rvert: z \in\mathbb{C}, \lvert z\rvert\le1\}, \quad\forall p \in\mathbb{C}[z].

Based on Theorem 4.3 we formulate following problems.

Problem 4.4. (Noncommutative von Neumann Inequality Problem) Let AA be a unital C∗C^{*}-algebra. Whether there is a universal constant RAR_{A} (which may depend upon AA) satisfying following: For every d∈Nd \in\mathbb{N} and for every A∈Md(A)A \in\mathrm{M}_{d}(A) with ∥A∥≤1\lVert A\rVert\le1, we have

∥p(A)∥≤RAsup⁡{∥p(z)∥:z∈A,∥z∥≤1},∀p∈A[z].\lVert p(A)\rVert\le R_{A}\sup\{\lVert p(z)\rVert: z \in A, \lVert z\rVert\le1\}, \quad\forall p \in A[z].

Theorem 4.3 has been extended by Ando for two variables.

Theorem 4.5. [7, 95] (Ando Theorem) For every d∈Nd \in\mathbb{N} and for all matrices M,N∈Md(C)M,N \in\mathrm{M}_{d}(\mathbb{C}) with ∥M∥≤1\lVert M\rVert\le1, ∥N∥≤1\lVert N\rVert\le1 and MN=NMMN=NM, we have

(Ando Inequality)

∥p(M,N)∥≤sup⁡{∣p(z,w)∣:z,w∈C,∣z∣≤1,∣w∣≤1},∀p∈C[z,w].\lVert p(M,N)\rVert\le\sup\{\lvert p(z,w)\rvert: z,w \in\mathbb{C}, \lvert z\rvert\le1, \lvert w\rvert\le1\}, \quad\forall p \in\mathbb{C}[z,w].

Based on Theorem 4.5, we formulate following problem.

Problem 4.6. (Noncommutative Ando Inequality Problem) Let A\mathcal{A} be a unital C∗C^*-algebra. Whether there is a universal constant RAR_{\mathcal{A}} (which may depend upon A\mathcal{A}) satisfying following: For every d∈Nd \in\mathbb{N} and for all A,B∈Md(A)A,B \in M_d(\mathcal{A}) with ∥A∥≤1\lVert A\rVert\le1, ∥B∥≤1\lVert B\rVert\le1 and AB=BAAB=BA, we have

∥p(A,B)∥≤sup⁡{∥p(z,w)∥:z,w∈A,∥z∥≤1,∥w∥≤1},∀p∈A[z,w].\lVert p(A,B)\rVert\le\sup\{\lVert p(z,w)\rVert: z,w \in\mathcal{A},\lVert z\rVert\le1,\lVert w\rVert\le1\},\qquad\forall p \in\mathcal{A}[z,w].

Note that Ando theorem cannot be extended to more than two commuting matrices [21, 98]. We observe that the Halmos dilation [49], Egervary dilation [32, 69] and Sz.-Nagy dilation (Schaffer construction) [89] carry over to adjointable morphisms on Hilbert C∗C^*-modules. This observation will give following result.

Theorem 4.7. (Noncommutative Sz.-Nagy Dilation) Let E\mathcal{E} be a Hilbert C∗C^*-module over a unital C∗C^*-algebra A\mathcal{A}. Let T:E→ET:\mathcal{E}\to\mathcal{E} be an adjointable morphism such that ∥T∥≤1\lVert T\rVert\le1. Then there exist a Hilbert C∗C^*-module E0\mathcal{E}_0 which contains E\mathcal{E} isometrically, E\mathcal{E} is orthogonally complementable in E0\mathcal{E}_0, PE:E0→EP_{\mathcal{E}}:\mathcal{E}_0\to\mathcal{E} is an onto orthogonal projection and unitary morphism U:E0→E0U:\mathcal{E}_0\to\mathcal{E}_0 such that

Tnx=PEUnx,∀n∈N,∀x∈E.T^n x=P_{\mathcal{E}}U^n x,\qquad\forall n\in\mathbb{N},\forall x\in\mathcal{E}.

Corollary 4.8. Let E\mathcal{E} be a Hilbert C∗C^*-module over a unital C∗C^*-algebra A\mathcal{A}. Let T:E→ET:\mathcal{E}\to\mathcal{E} be an adjointable morphism such that ∥T∥≤1\lVert T\rVert\le1. Let E0\mathcal{E}_0, PEP_{\mathcal{E}} and UU be as in Theorem 4.7. Then

∥p(T)∥≤∥p(U)∥,∀p(z)=a0+za1+⋯+znan∈A[z].\lVert p(T)\rVert\le\lVert p(U)\rVert,\qquad\forall p(z)=a_0+za_1+\cdots+z^n a_n\in\mathcal{A}[z].

Corollary 4.9. Let E\mathcal{E} be a Hilbert C∗C^*-module over a unital C∗C^*-algebra A\mathcal{A}. Let T:E→ET:\mathcal{E}\to\mathcal{E} be an adjointable morphism such that ∥T∥≤1\lVert T\rVert\le1. Let x∈Ex\in\mathcal{E} be such that Tx=xTx=x. Then T∗x=xT^*x=x.

Proof. Let x∈Ex\in\mathcal{E} be such that Tx=xTx=x. Let E0\mathcal{E}_0, PEP_{\mathcal{E}} and UU be as in Theorem 4.7. We then have

x=Tx=PEUx,⟨Ux,Ux⟩=⟨x,x⟩,PEx=x.x=Tx=P_{\mathcal{E}}Ux,\qquad\langle Ux,Ux\rangle=\langle x,x\rangle,\qquad P_{\mathcal{E}}x=x.

We see that

⟨Ux−x,Ux−x⟩=2⟨x,x⟩−⟨Ux,x⟩−⟨x,Ux⟩=2⟨x,x⟩−⟨Ux,PEx⟩−⟨PEx,Ux⟩=2⟨x,x⟩−⟨PEUx,x⟩−⟨x,PEUx⟩=2⟨x,x⟩−⟨Tx,x⟩−⟨x,Tx⟩=2⟨x,x⟩−⟨x,x⟩−⟨x,x⟩=0.\begin{aligned} \langle Ux-x,Ux-x\rangle&=2\langle x,x\rangle-\langle Ux,x\rangle-\langle x,Ux\rangle\\ &=2\langle x,x\rangle-\langle Ux,P_{\mathcal{E}}x\rangle-\langle P_{\mathcal{E}}x,Ux\rangle\\ &=2\langle x,x\rangle-\langle P_{\mathcal{E}}Ux,x\rangle-\langle x,P_{\mathcal{E}}Ux\rangle\\ &=2\langle x,x\rangle-\langle Tx,x\rangle-\langle x,Tx\rangle\\ &=2\langle x,x\rangle-\langle x,x\rangle-\langle x,x\rangle=0. \end{aligned}

Therefore

Ux=x⟹x=U∗x.Ux=x\Longrightarrow x=U^*x.

Hence

x=U∗x=PEU∗x=T∗x.x=U^*x=P_{\mathcal{E}}U^*x=T^*x.

We also observe that the proof of Ando dilation [7] for commuting operators on Hilbert space will not carry over to commuting adjointable morphisms on Hilbert C∗C^*-modules (mainly because submodules need not be orthogonally complementable and C∗C^*-algebras need not have invariant basis number property).

Acknowledgments

AI is used for the literature survey and grammar improvement.

References

  1. [1]Amer Abu-Omar and Fuad Kittaneh. A numerical radius inequality involving the generalized Aluthge transform. Stud. Math., 216(1):69–75, 2013.DOI
  2. [2]Amer Abu-Omar and Fuad Kittaneh. Numerical radius inequalities for products of Hilbert space operators. J. Oper. Theory, 72(2):521–527, 2014.
  3. [3]Amer Abu-Omar and Fuad Kittaneh. Upper and lower bounds for the numerical radius with an application to involution operators. Rocky Mt. J. Math., 45(4):1055–1064, 2015.
  4. [4]Gregory Adams, Georgia Corbett, and Pamela Gorkin. Circular numerical ranges, Blaschke products, and Poncelet curves: why n circles are better than one. J. Math. Anal. Appl., 547(1):17, 2025. Id/No 129268.DOI
  5. [5]Jim Agler. Geometric and topological properties of the numerical range. Indiana Univ. Math. J., 31:767–777, 1982.
  6. [6]Yuri A. Alpin, Mao-Ting Chien, and Lina Yeh. The numerical radius and bounds for zeros of a polynomial. Proc. Am. Math. Soc., 131(3):725–730, 2003.DOI
  7. [7]T. Ando. Structure of operators with numerical radius one. Acta Sci. Math., 34:11–15, 1973.
  8. [8]S. K. Berberian. The numerical range of a normal operator. Duke Math. J., 31:479–483, 1964.DOI
  9. [9]C. A. Berger and J. G. Stampfli. Norm relations and skew dilations. Acta Sci. Math., 28:191–195, 1967.
  10. [10]G. A. Berger and J. G. Stampfli. Mapping theorems for the numerical range. Am. J. Math., 89:1047–1055, 1967.
  11. [11]S. J. Bernau and F. Smithies. A note on normal operators. Proc. Camb. Philos. Soc., 59:727–729, 1963.DOI
  12. [12]Pintu Bhunia, Santanu Bag, and Kallol Paul. Numerical radius inequalities and its applications in estimation of zeros of polynomials. Linear Algebra Appl., 573:166–177, 2019.
  13. [13]Kelly Bickel, Pamela Gorkin, Anne Greenbaum, Thomas Ransford, Felix L. Schwenninger, and Elias Crouzeix. Crouzeix’s conjecture and related problems. Comput. Methods Funct. Theory, 20(3-4):701–728, 2020.DOI
  14. [14]Richard Bouldin. The numerical range of a product. J. Math. Anal. Appl., 32:459–467, 1970.DOI
  15. [15]Richard Bouldin. The numerical range of a product. II. J. Math. Anal. Appl., 33:212–219, 1971.DOI
  16. [16]Paul S. Bourdon and Joel H. Shapiro. When is zero in the numerical range of a composition operator? Integral Equations Oper. Theory, 44(4):410–441, 2002.DOI
  17. [17]Ethan S. Brown and Ilya M. Spitkovsky. On matrices with elliptical numerical ranges. Linear Multilinear Algebra, 52(3-4):177–193, 2004.DOI
  18. [18]Maria Luisa Buzano. Generalizzazione della diseguaglianza di cauchy-schwarz. Rend. Sem. Mat. Univ. e Politec. Torino, 31:405–409, 1974.
  19. [19]Mao-Ting Chien and Bit-Shun Tam. Circularity of the numerical range. Linear Algebra Appl., 201:113–133, 1994.DOI
  20. [20]Man-Duen Choi and Chi-Kwong Li. Constrained unitary dilations and numerical ranges. J. Oper. Theory, 46(2):435–447, 2001.
  21. [21]M. J. Crabb and A. M. Davie. Von Neumann’s inequality for Hilbert space operators. Bull. Lond. Math. Soc., 7:49–50, 1975.DOI
  22. [22]M. Crouzeix and C. Palencia. The numerical range is a (1+√2)-spectral set. SIAM J. Matrix Anal. Appl., 38(2):649–655, 2017.DOI
  23. [23]Michel Crouzeix. Bounds for analytical functions of matrices. Integral Equations Oper. Theory, 48(4):461–477, 2004.DOI
  24. [24]Michel Crouzeix. Numerical range and functional calculus in Hilbert space. J. Funct. Anal., 244(2):668–690, 2007.DOI
  25. [25]Kenneth R. Davidson and John A. R. Holbrook. Numerical radii of zero-one matrices. Mich. Math. J., 35(2):261–267, 1988.DOI
  26. [26]Chandler Davis. The Toeplitz-Hausdorff theorem explained. Can. Math. Bull., 14:245–246, 1971.DOI
  27. [27]Bernard Delyon and Francois Delyon. Generalization of von Neumann’s spectral sets and integral representation of operators. Bull. Soc. Math. Fr., 127(1):25–41, 1999.DOI
  28. [28]S. S. Dragomir. A Buzano type inequality for two Hermitian forms and applications. Linear Multilinear Algebra, 65(3):514–525, 2016.DOI
  29. [29]S. S. Dragomir. Buzano’s inequality holds for any projection. Bull. Aust. Math. Soc., 93(3):504–510, 2016.DOI
  30. [30]Sever S. Dragomir. Inequalities for the norm and the numerical radius of linear operators in Hilbert spaces. Demonstr. Math., 40(2):411–417, 2007.
  31. [31]Michael A. Dritschel and Hugo J. Woerdeman. Model theory and linear extreme points in the numerical radius unit ball, volume 615 of Mem. Am. Math. Soc. Providence, RI: American Mathematical Society (AMS), 1997.
  32. [32]E. Egerváry. On the contractive linear transformations of n-dimensional vector space. Acta Sci. Math., 15:178–182, 1954.
  33. [66]Fuad Kittaneh, Mohammad Sal Moslehian, and Takeaki Yamazaki. Cartesian decomposition and numerical radius inequalities. Linear Algebra Appl., 471:46–53, 2015.DOI
  34. [67]John S. Lancaster. The boundary of the numerical range. Proc. Am. Math. Soc., 49:393–398, 1975.
  35. [68]E. Christopher Lance. Hilbert C*-modules. A toolkit for operator algebraists, volume 210 of Lond. Math. Soc. Lect. Note Ser. Cambridge University Press, 1995.
  36. [69]Elijah Levy and Orr Moshe Shalit. Dilation theory in finite dimensions: the possible, the impossible and the unknown. Rocky Mt. J. Math., 44(1):203–221, 2014.
  37. [70]Chi-Kwong Li. A simple proof of the elliptical range theorem. Proc. Am. Math. Soc., 124(7):1985–1986, 1996.DOI
  38. [71]Richard I. Loebl and Vern I. Paulsen. Some remarks on C*-convexity. Linear Algebra Appl., 35:63–78, 1981.DOI
  39. [72]Marvin Marcus and B. N. Shure. The numerical range of certain 0,1-matrices. Linear Multilinear Algebra, 7:111–120, 1979.DOI
  40. [73]J. Maroulas, P. J. Psarrakos, and M. J. Tsatsomeros. Perron-Frobenius type results on the numerical range. Linear Algebra Appl., 348(1-3):49–62, 2002.DOI
  41. [74]Alan McIntosh. The Toeplitz-Hausdorff theorem and ellipticity conditions. Am. Math. Mon., 85:475–477, 1978.
  42. [75]A. I. Mees and D. P. Atherton. Domains containing the field of values of a matrix. Linear Algebra Appl., 26:289–296, 1979.DOI
  43. [76]Marzieh Mehrazin, Maryam Amyari, and Mohsen Erfanian Omidvar. A new type of numerical radius of operators on Hilbert C*-module. Rend. Circ. Mat. Palermo (2), 69(1):29–37, 2020.
  44. [77]Vladimír Müller. The numerical radius of a commuting product. Mich. Math. J., 35(2):255–260, 1988.DOI
  45. [78]Francis J. Narcowich and Joseph D. Ward. A Toeplitz-Hausdorff theorem for matrix ranges. J. Oper. Theory, 6:87–101, 1981.
  46. [79]Edward Nelson. The distinguished boundary of the unit operator ball. Proc. Am. Math. Soc., 12:994–995, 1961.DOI
  47. [80]K. Oukobo and T. Ando. Operator radii of commuting products. Proc. Am. Math. Soc., 56:203–210, 1976.
  48. [81]William L. Paschke. Inner product modules over B*-algebras. Trans. Amer. Math. Soc., 182:443–468, 1973.
  49. [82]C. Pearcy. An elementary proof of the power inequality for the numerical radius. Mich. Math. J., 13:289–291, 1966.DOI
  50. [83]Fredric M. Pollack. Numerical range and convex sets. Can. Math. Bull., 17:295–296, 1974.DOI
  51. [84]Mehdi Radjabalipour and Heydar Radjavi. On the geometry of numerical ranges. Pac. J. Math., 61:507–511, 1975.DOI
  52. [85]R. Raghavendran. Toeplitz-Hausdorff theorem on numerical ranges. Proc. Am. Math. Soc., 20:284–285, 1969.DOI
  53. [86]Rajna Rajic. On the algebra range of an operator on a Hilbert C*-module over compact operators. Proc. Am. Math. Soc., 131(10):3043–3051, 2003.DOI
  54. [87]Thomas Ransford and Felix L. Schwenninger. Remarks on the Crouzeix-Palencia proof that the numerical range is a (1 + √2)-spectral set. SIAM J. Matrix Anal. Appl., 39(1):342–345, 2018.DOI
  55. [88]Marc A. Rieffel. Induced representations of C*-algebras. Advances in Math., 13:176–257, 1974.DOI
  56. [89]J. J. Schäffer. On unitary dilations of contractions. Proc. Am. Math. Soc., 6:322, 1955.
  57. [90]Elias S. W. Shiu. Growth of numerical ranges of powers of Hilbert space operators. Mich. Math. J., 23:155–160, 1976.DOI
  58. [91]J. Michael Steele. The Cauchy-Schwarz master class. An introduction to the art of mathematical inequalities. The Mathematical Association of America, 2004.
  59. [92]M. H. Stone. Hausdorff’s theorem concerning Hermitian forms. Bull. Am. Math. Soc., 36:259–261, 1930.DOI
  60. [93]Marshall Harvey Stone. Linear transformations in Hilbert space and their applications to analysis, volume 15. American Mathematical Society (AMS), Providence, RI, 1932.
  61. [94]Béla Sz.-Nagy. Sur les contractions de l’espace de Hilbert. Acta Sci. Math., 15:87–92, 1953.
  62. [95]Béla Sz.-Nagy, Ciprian Foias, Hari Bercovici, and László Kérchy. Harmonic analysis of operators on Hilbert space. Universitext. New York, NY: Springer, 2 edition, 2010.
  63. [96]Bit-Shun Tam and Shangjun Yang. On matrices whose numerical ranges have circular or weak circular symmetry. Linear Algebra Appl., 302-303:193–221, 1999.DOI
  64. [97]O. Toeplitz. Das algebraische Analogon zu einem Satze von Fejér. Math. Z., 2:187–197, 1918.DOI
  65. [98]N. Th. Varopoulos. On an inequality of von Neumann and an application of the metric theory of tensor products to operators theory. J. Funct. Anal., 16:83–100, 1974.DOI
  66. [99]Johann von Neumann. Eine Spektraltheorie für allgemeine Operatoren eines unitären Raumes. Math. Nachr., 4:258–281, 1951.
  67. [100]Kuo-Zhong Wang, Pei Yuan Wu, and Hwa-Long Gau. Crawford numbers of powers of a matrix. Linear Algebra Appl., 433(11-12):2243–2254, 2010.DOI
  68. [101]James P. Williams. Similarity and the numerical range. J. Math. Anal. Appl., 26:307–314, 1969.DOI
  69. [102]A. Wintner. Zur Theorie der beschränkten Bilinearformen. Math. Z., 30:228–282, 1929.
  70. [103]Pei Yuan Wu. Polygons and numerical ranges. Am. Math. Mon., 107(6):528–540, 2000.
  71. [104]Takeaki Yamazaki. On upper and lower bounds of the numerical radius and an equality condition. Stud. Math., 178(1):83–89, 2007.DOI
  72. [105]Ali Zamani. Numerical radius in Hilbert C*-modules. Math. Inequal. Appl., 24(4):1017–1030, 2021.arxiv.org/abs/2101.04396

Paper details

vlnc:W_9yep4fwk
v1 · latestHistory (1)

published · Fresh — added to the Hub within the last 30 days

added ·

Usage

views · 0

downloads · 0

A view counts once per browser per day, a download each time the PDF is requested.

CC BY 4.0

Original source

  • Mathematics

AI · View statement →

Looking for related papers…
Contents