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Yiu-Tung Poon

Publications and source records attributed to Yiu-Tung Poon.

At least 19 recordsLinked to original sources

Characterizing Quantum Codes via the Coefficients in Knill-Laflamme Conditions

Quantum error correction (QEC) is essential for protecting quantum information against noise, yet understanding the structure of the Knill-Laflamme (KL) coefficients $λ_{ij}$ from the condition $PE_i^\dagger E_j P = λ_{ij} P$ remains challenging, particularly for nonadditive codes. In this work, we introduce the signature vector $\vecλ(P)$, composed of the off-diagonal KL coefficients $λ_{ij}$, where each coefficient corresponds to equivalence classes of errors counted only once. We define its Euclidean norm $λ^*(P)$ as a scalar measure representing the total strength of error correlations within the code subspace defined by the projector $P$. We parameterize $P$ on a Stiefel manifold and formulate an optimization problem based on the KL conditions to systematically explore possible values of $λ^*$. Moreover, we show that, for $((n,K,d))$ codes, $λ^*$ is invariant under local unitary transformations. Applying our approach to the $((6, 2, 3))$ quantum code, we find that $λ^*_{\text{min}} = \sqrt{0.6}$ and $λ^*_{\text{max}} = 1$, with $λ^* = 1$ corresponding to a known degenerate stabilizer code. We construct continuous families of new nonadditive codes parameterized by vectors in $\mathbb{R}^5$, with $λ^*$ varying over the interval $[\sqrt{0.6}, 1]$. For the $((7, 2, 3))$ code, we identify $λ^*_{\text{min}} = 0$ (corresponding to the non-degenerate Steane code) and $λ^*_{\text{max}} = \sqrt{7}$ (corresponding to the permutation-invariant code by Pollatsek and Ruskai), and we demonstrate continuous paths connecting these extremes via cyclic codes characterized solely by $λ^*$. Our findings provide new insights into the structure of quantum codes, advance the theoretical foundations of QEC, and open new avenues for investigating intricate relationships between code subspaces and error correlations.

quant-ph

NISQ: Error Correction, Mitigation, and Noise Simulation

Error-correcting codes were invented to correct errors on noisy communication channels. Quantum error correction (QEC), however, may have a wider range of uses, including information transmission, quantum simulation/computation, and fault-tolerance. These invite us to rethink QEC, in particular, about the role that quantum physics plays in terms of encoding and decoding. The fact that many quantum algorithms, especially near-term hybrid quantum-classical algorithms, only use limited types of local measurements on quantum states, leads to various new techniques called Quantum Error Mitigation (QEM). This work examines the task of QEM from several perspectives. Using some intuitions built upon classical and quantum communication scenarios, we clarify some fundamental distinctions between QEC and QEM. We then discuss the implications of noise invertibility for QEM, and give an explicit construction called Drazin-inverse for non-invertible noise, which is trace preserving while the commonly-used Moore-Penrose pseudoinverse may not be. Finally, we study the consequences of having an imperfect knowledge about the noise, and derive conditions when noise can be reduced using QEM.

quant-ph

The joint $k$-numerical range of operators

Let ${\mathcal B}({\mathcal H})$ be the algebra of all bounded linear operators on the Hilbert space ${\mathcal H}$. For a positive integer $k$ less than the dimension of ${\mathcal H}$ and ${\mathbf A} = (A_1, \dots, A_m)\in {\mathcal B}({\mathcal H})^m$, the joint $k$-numerical range $W_k({\mathbf A})$ is the set of vector $(α_1, \dots, α_m) \in{\mathbb C}^m$ such that $α_i = \sum_{j = 1}^k \langle A_ix_j, x_j\rangle$ for an orthonormal set $\{x_1, \ldots, x_k\}$ in ${\mathcal H}$. Geometrical properties of $W_k({\mathbf A})$ and their relations with the algebraic properties of $\{A_1, \dots, A_m\}$ are investigated in this paper. For example, conditions for $W_k({\mathbf A})$ to be convex are studied. Descriptions are given for the closure of $W_k({\mathbf A})$ and the closure of ${\rm conv}\, W_k({\mathbf A})$ in terms of the joint essential numerical range of ${\mathbf A}$ for infinite dimensional operators $A_1, \dots, A_m$. Characterizations are obtained for $W_k({\mathbf A})$ or ${\rm conv}\, W_k({\mathbf A})$ to be closed. It is shown that $W_k({\mathbf A})$ is a polyhedral set if and only if $A_1, \dots, A_k$ have a common reducing subspace ${\mathbf V}$ of finite dimension such that the compression of $A_1, \dots, A_m$ on the subspace ${\mathbf V}$ are diagonal operators $D_1, \dots, D_m$ and $W_k({\mathbf A}) = W_k(D_1, \dots, D_m)$. Similar results are obtained for ${\bf A}$ such that the closure of $W_k({\mathbf A})$ is polyhedral. Classifications are given for operators satisfying (1) $\{A_1, \dots, A_m\}$ is a commuting family of normal operators, or (2) $W_k(A_1, \dots, A_m)$ is polyhedral for every positive integer $k$ less than $\dim {\mathcal H}$.

math.FA

Commuting normal operators and joint numerical range

Let ${\mathcal H}$ be a complex Hilbert space and let ${\mathcal B}({\mathcal H})$ be the algebra of all bounded linear operators on ${\mathcal H}$. For a positive integer $k$ less than the dimension of ${\mathcal H}$ and ${\mathbf A} = (A_1, \dots, A_m)\in {\mathcal B}({\mathcal H})^m$, the joint $k$-numerical range $W_k({\mathbf A})$ is the set of $(α_1, \dots, α_m) \in{\mathbb C}^m$ such that $α_i = \sum_{j = 1}^k \langle A_ix_j, x_j\rangle$ for an orthonormal set $\{x_1, \ldots, x_k\}$ in ${\mathcal H}$. Relations between the geometric properties of $W_k({\mathbf A})$ and the algebraic and analytic properties of $A_1, \dots, A_m$ are studied. It is shown that there is $k\in {\mathbb N}$ such that $W_k({\mathbf A})$ is a polyhedral set, i.e., the convex hull of a finite set, if and only if $A_1, \dots, A_k$ have a common reducing subspace ${\mathbf V}$ of finite dimension such that the compression of $A_1, \dots, A_m$ on the subspace ${\mathbf V}$ are diagonal operators $D_1, \dots, D_m$ and $W_k({\mathbf A}) = W_k(D_1, \dots, D_m)$. Characterization is also given to ${\bf A}$ such that the closure of $W_k({\mathbf A})$ is polyhedral. The conditions are related to the joint essential numerical range of ${\mathbf A}$. These results are used to study ${\bf A}$ such that (a) $\{A_1, \dots, A_m\}$ is a commuting family of normal operators, or (b) $W_k(A_1, \dots, A_m)$ is polyhedral for every positive integer $k$. It is shown that conditions (a) and (b) are equivalent for finite rank operators but it is no longer true for compact operators. Characterizations are given for compact operators $A_1, \dots, A_m$ satisfying (a) and (b), respectively. Results are also obtained for general non-compact operators.

math.FA

Observing geometry of quantum states in a three-level system

In quantum mechanics, geometry has been demonstrated as a useful tool for inferring non-classical behaviors and exotic properties of quantum systems. One standard approach to illustrate the geometry of quantum systems is to project the quantum state space to the Euclidean space via measurements of observables on the system. Despite the great success of this method in studying two-level quantum systems (qubits) with the celebrated Bloch sphere representation, there is always the difficulty to reveal the geometry of multi-dimensional quantum systems. Here we report the first experiment measuring the geometry of such projections beyond the qubit. Specifically, we observe the joint numerical ranges (JNRs) of a triple of observables in a three-level photonic system, providing complete classification of the JNRs. We further show that the geometry of different classes reveal ground-state degeneracies of a Hamiltonian as a linear combination of the observables, which is related to quantum phases in the thermodynamic limit. Our results offer a versatile geometric approach for exploring the properties of higher-dimensional quantum systems.

quant-ph

Determining system Hamiltonian from eigenstate measurements without correlation functions

Local Hamiltonians arise naturally in physical systems. Despite its seemingly `simple' local structure, exotic features such as nonlocal correlations and topological orders exhibit in eigenstates of these systems. Previous studies for recovering local Hamiltonians from measurements on an eigenstate $|ψ\rangle$ require information of nonlocal correlation functions. In this work, we develop an algorithm to determine local Hamiltonians from only local measurements on $|ψ\rangle$, by reformulating the task as an unconstrained optimization problem of certain target function of Hamiltonian parameters, with only polynomial number of parameters in terms of system size. We also develop a machine learning-based-method to solve the first-order gradient used in the algorithm. Our method is tested numerically for randomly generated local Hamiltonians and returns promising reconstruction in the desired accuracy. Our result shed light on the fundamental question on how a single eigenstate can encode the full system Hamiltonian, indicating a somewhat surprising answer that only local measurements are enough without additional assumptions, for generic cases.

quant-ph

Error correction schemes for fully correlated quantum channels protecting both quantum and classical information

We study efficient quantum error correction schemes for the fully correlated channel on an $n$-qubit system with error operators that assume the form $σ_x^{\otimes n}$, $σ_y^{\otimes n}$, $σ_z^{\otimes n}$. Previous schemes are improved to facilitate implementation. In particular, when $n$ is odd and equals $2k+1$, we describe a quantum error correction scheme using one arbitrary qubit $σ$ to protect the data state $ρ$ in a $2k$-qubit system. The encoding operation $σ\otimes ρ\mapsto Φ(σ\otimes ρ)$ only requires $3k$ CNOT gates (each with one control bit and one target bit). After the encoded state $Φ(σ\otimes ρ)$ goes through the channel, we can apply the inverse operation $Φ^{-1}$ to produce $\tilde σ\otimes ρ$ so that a partial trace operation can recover $ρ$. When $n$ is even and equals $2k+2$, we describe a hybrid quantum error correction scheme using any one of the two classical bits $σ\in \{|ij\rangle \langle ij|: i, j \in \{0,1\}\}$ to protect a $2k$-qubit state $ρ$ and 2 classical bits. The encoding operation $σ\otimes ρ\mapsto Φ(σ\otimes ρ)$ can be done by $3k+2$ CNOT gates and a single quibt Hadamard gate. After the encoded state $Φ(σ\otimes ρ)$ goes through the channel, we can apply the inverse operation $Φ^{-1}$ to produce $σ\otimes ρ$ so that a perfect protection of the two classical bits $σ$ and the $2k$-qubit state is achieved. If one uses an arbitrary $2$-qubit state $σ$, the same scheme will protect $2k$-qubit states. The scheme was implemented using Matlab, Mathematica, Python, and the IBM's quantum computing framework qiskit.

quant-ph

Joint numerical ranges and communtativity of matrices

The connection between the commutativity of a family of $n\times n$ matrices and the generalized joint numerical ranges is studied. For instance, it is shown that ${\cal F}$ is a family of mutually commuting normal matrices if and only if the joint numerical range $W_k(A_1, \dots, A_m)$ is a polyhedral set for some $k$ satisfying $|n/2-k|\le 1$, where $\{A_1, \dots, A_m\}$ is a basis for the linear span of the family; equivalently, $W_k(X,Y)$ is polyhedral for any two $X, Y \in {\cal F}$. More generally, characterization is given for the $c$-numerical range $W_c(A_1, \dots, A_m)$ to be polyhedral for any $n\times n$ matrices $A_1, \dots, A_m$. Other results connecting the geometrical properties of the joint numerical ranges and the algebraic properties of the matrices are obtained. Implications of the results to representation theory, and quantum information science are discussed.

math.FA

Experimental self-characterization of quantum measurements

The accurate and reliable description of measurement devices is a central problem in both observing uniquely non-classical behaviors and realizing quantum technologies from powerful computing to precision metrology. To date quantum tomography is the prevalent tool to characterize quantum detectors. However, such a characterization relies on accurately characterized probe states, rendering reliability of the characterization lost in circular argument. Here we report a self-characterization method of quantum measurements based on reconstructing the response range, the entirety of attainable measurement outcomes, eliminating the reliance on known states. We characterize two representative measurements implemented with photonic setups and obtain fidelities above 99.99% with the conventional tomographic reconstructions. This initiates range-based techniques in characterizing quantum systems and foreshadows novel device-independent protocols of quantum information applications.

quant-ph

Higher Rank Matricial Ranges and Hybrid Quantum Error Correction

We introduce and initiate the study of a family of higher rank matricial ranges, taking motivation from hybrid classical and quantum error correction coding theory and its operator algebra framework. In particular, for a noisy quantum channel, a hybrid quantum error correcting code exists if and only if a distinguished special case of the joint higher rank matricial range of the error operators of the channel is non-empty. We establish bounds on Hilbert space dimension in terms of properties of a tuple of operators that guarantee a matricial range is non-empty, and hence additionally guarantee the existence of hybrid codes for a given quantum channel. We also discuss when hybrid codes can have advantages over quantum codes and present a number of examples.

quant-ph

Numerical Range Inclusion, Dilation, and Operator Systems

Researchers have identified complex matrices $A$ such that a bounded linear operator $B$ acting on a Hilbert space will admit a dilation of the form $A \otimes I$ whenever the numerical range inclusion relation $W(B) \subseteq W(A)$ holds. Such an operator $A$ and the identity matrix will span a maximal operator system, i.e., every unital positive map from ${\rm span} \{I, A, A^*\}$ to ${\cal B}({\cal H})$, the algebra of bounded linear operators acting on a Hilbert space ${\cal H}$, is completely positive. In this paper, we identify $m$-tuple of matrices ${\bf A} = (A_1, \dots, A_m)$ such that any $m$-tuple of operators ${\bf B} = (B_1, \dots, B_m)$ satisfying the joint numerical range inclusion $W({\bf B}) \subseteq {\rm conv} W({\bf A})$ will have a joint dilation of the form $(A_1\otimes I, \dots, A_m\otimes I)$. Consequently, every unital positive map from ${\rm span} \{I, A_1, A_1^*, \dots, A_m, A_m^*\}$ to ${\cal B}({\cal H})$ is completely positive. New results and techniques are obtained relating to the study of numerical range inclusion, dilation, and maximal operator systems.

math.FA

Preservation of the joint essential matricial range

Let $A = (A_1, \dots, A_m)$ be an $m$-tuple of elements of a unital $C$*-algebra ${\cal A}$ and let $M_q$ denote the set of $q \times q$ complex matrices. The joint $q$-matricial range $W^q(A)$ is the set of $(B_1, \dots, B_m) \in M_q^m$ such that $B_j = Φ(A_j)$ for some unital completely positive linear map $Φ: {\cal A} \rightarrow M_q$. When ${\cal A}= B(H)$, where $B(H)$ is the algebra of bounded linear operators on the Hilbert space $H$, the {\bf joint spatial $q$-matricial range} $W^q_s(A)$ of $A$ is the set of $(B_1, \dots, B_m) \in M_q^m$ for which there is a $q$-dimensional $V$ of $H$ such that $B_j$ is a compression of $A_j$ to $V$ for $j=1,\dots, m$. Suppose $K(H)$ is the set of compact operators in $B(H)$. The joint essential spatial $q$-matricial range is defined as $$W_{ess}^q(A) = \cap \{ {\bf cl}(W_s^q(A_1+K_1, \dots, A_m+K_m)): K_1, \dots, K_m \in K(H) \},$$ where ${\bf cl}$ denotes the closure. Let $π$ be the canonical surjection from $B(H)$ to the Calkin algebra $B(H)/K(H)$. We prove that $W_{ess}^q(A) =W^q(π(A) $, where $π(A) = (π(A_1), \dots, π(A_m))$. Furthermore, for any positive integer $N$, we prove that there are self-adjoint compact operators $K_1, \dots, K_m$ such that $${\bf cl}(W^q_s(A_1+K_1, \dots, A_m+K_m)) = W^q_{ess}(A) \quad \hbox{ for all } q \in \{1, \dots, N\}.$$ These results generalize those of Narcowich-Ward and Smith-Ward, obtained in the $m=1$ case, and also generalize a result of Müller obtained in case $m \ge 1$ and $q=1$. Furthermore, if $W_{ess}^1({\bf A}) $ is a simplex in ${\mathbb R}^m$, then we prove that there are self-adjoint $K_1, \dots, K_m \in K(H)$ such that ${\bf cl}(W^q_s(A_1+K_1, \dots, A_m+K_m)) = W^q_{ess}(A)$ for all positive integers $q$.

math.FA

Numerical Range Inclusion, Dilation, and completely positive maps

A proof using the theory of completely positive maps is given to the fact that if $A \in M_2$, or $A \in M_3$ has a reducing eigenvalue, then every bounded linear operator $B$ with $W(B) \subseteq W(A)$ has a dilation of the form $I \otimes A$. This gives a unified treatment for the different cases of the result obtained by researchers using different techniques.

math.FA

Some notes on the robustness of k-coherence and k-entanglement

We show that two related measures of k-coherence, called the standard and generalized robustness of k-coherence, are equal to each other when restricted to pure states. As a direct application of the result, we establish an equivalence between two analogous measures of Schmidt rank k-entanglement for all pure states. This answers conjectures raised in the literature regarding the evaluation of the quantifiers, and facilitates an efficient quantification of pure-state resources by introducing computable closed-form expressions for the two measures.

quant-ph

Ranks of quantum states with prescribed reduced states

Let $M_n$ be the set of $n\times n$ complex matrices. In this note we determine all the possible ranks of a bipartite state in $M_m\otimes M_n$ with prescribed reduced states in the two subsystems. The results are used to determine the Choi rank of quantum channels $Φ: M_m \rightarrow M_n$ sending $I/m$ to a specific state $σ_2 \in M_n$.

quant-ph

The generalized numerical range of a set of matrices

For a given set of $n\times n$ matrices $\mathcal F$, we study the union of the $C$-numerical ranges of the matrices in the set $\mathcal F$, denoted by $W_C({\mathcal F})$. We obtain basic algebraic and topological properties of $W_C({\mathcal F})$, and show that there are connections between the geometric properties of $W_C({\mathcal F})$ and the algebraic properties of $C$ and the matrices in ${\mathcal F}$. Furthermore, we consider the starshapedness and convexity of the set $W_C({\mathcal F})$. In particular, we show that if ${\mathcal F}$ is the convex hull of two matrices such that $W_C(A)$ and $W_C(B)$ are convex, then the set $W_C({\mathcal F})$ is star-shaped. We also investigate the extensions of the results to the joint $C$-numerical range of an $m$-tuple of matrices.

math.FA

Convexity and Star-shapedness of Matricial Range

Let ${\bf A} = (A_1, \dots, A_m)$ be an $m$-tuple of bounded linear operators acting on a Hilbert space ${\cal H}$. Their joint $(p,q)$-matricial range $Λ_{p,q}({\bf A})$ is the collection of $(B_1, \dots, B_m) \in {\bf M}_q^m$, where $I_p\otimes B_j$ is a compression of $A_j$ on a $pq$-dimensional subspace. This definition covers various kinds of generalized numerical ranges for different values of $p,q,m$. In this paper, it is shown that $Λ_{p,q}({\bf A})$ is star-shaped if the dimension of $\cal H$ is sufficiently large. If $\dim {\cal H}$ is infinite, we extend the definition of $Λ_{p,q}({\bf A})$ to $Λ_{\infty,q}({\bf A})$ consisting of $(B_1, \dots, B_m) \in {\bf M}_q^m$ such that $I_\infty \otimes B_j$ is a compression of $A_j$ on a closed subspace of ${\cal H}$, and consider the joint essential $(p,q)$-matricial range $$Λ^{ess}_{p,q}({\bf A}) = \bigcap \{ {\bf cl}(Λ_{p,q}(A_1+F_1, \dots, A_m+F_m)): F_1, \dots, F_m \hbox{ are compact operators}\}.$$ Both sets are shown to be convex, and the latter one is always non-empty and compact.

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