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arXiv:2610.36391

Consensus And Information Redistribution In Quantum Networks

J. Novotný, D. Štěrba, I. Jex, H. -H. Kowalski, A. Abedi

quant-phSubmitted Oct 26, 2026• Announced Oct 28, 2026• 0 citations
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Abstract

Consensus algorithms are mechanisms driving nodes of a network to agreement. In quantum networks they also redistribute information encoded in the global quantum state, allowing global properties to be inferred from local measurements without reconstructing the global state. Motivated by this, we investigate decentralized quantum consensus in qudit networks governed by discrete random unitary dynamics. We characterize the analytic asymptotic dynamics, identify global information preserved by the evolution, and derive conditions for which different notions of quantum consensus emerge. A general theorem is derived that establishes a unified framework for extracting globally encoded information from local measurements beyond consensus states. First, we analyze CNOT networks and determine which global information can be recovered by individual nodes and which requires joint measurements on cooperating nodes. The CNOT model is well understood and presents a case with entanglement creation - a characteristic quantum feature of networks worth analyzing in detail. Second, we identify the complete class of two-qubit interactions that asymptotically achieve consensus on the average number of excitations, thereby establishing a quantum analogue of classical average consensus. We further show that joint measurements on k cooperating nodes recover exactly the first k moments of the excitation-number distribution.

AI Summary

The paper asks which global properties of a quantum-network state survive decentralized dynamics and become accessible through measurements on individual nodes or cooperating subsets. It considers discrete random-unitary channels $\mathcal P(\rho)=\sum_e p_eU_e\rho U_e^\dagger$, with pairwise interactions assigned to network edges. Using the peripheral eigenspaces of these channels, it derives necessary and sufficient algebraic conditions for expectation-value, reduced-state, and permutation-symmetric consensus. A second theorem characterizes stationary global information accessible through a chosen local observable: its projection onto the stationary attractor space identifies the corresponding conserved global observable, provided its overlaps with nonstationary attractors vanish. The construction extends to multi-node measurements and, as stated in the paper, discrete unital Markov channels. Two applications illustrate the framework. Strongly connected CNOT networks with $n>2$ have a five-dimensional stationary attractor space and reach permutation-symmetric consensus. Individual nodes can recover ground-state and uniform-superposition probabilities and an imaginary coherence component, whereas other preserved quantities require two-node measurements. For excitation-number consensus, the paper classifies two-qubit interactions by analyzing the two-node attractor equations, then gives an $n+3$-dimensional attractor structure for the selected mechanisms at $n>2$. Proper subsets of $m$ nodes access exactly the first $m$ moments of the conserved excitation-number distribution; explicit moment observables are constructed recursively. The analysis concerns asymptotic accessibility. Observable reconstruction becomes harder for large attractor spaces. Non-unital dynamics and a fuller characterization of recoverable properties, particularly in entangled consensus states, are left for future work.

Little sign of AI-generated textIncrementalOverclaimsPossible error

Central claim may not hold: The claimed complete interaction classification labels some interactions as achieving average consensus even though they admit stationary states with unequal local excitation expectations. The local-observable theorem incorrectly tests |lambda|!=1 instead of lambda!=1, making its printed nonstationary-overlap condition vacuous and its statement false. The claim that the m-node reduced state is completely determined by the first m excitation-number moments fails at m=n because the dynamics also retains all-zero/all-one coherence. The displayed CNOT consensus state is generally not normalized because the coefficient multiplying the Hilbert–Schmidt-normalized attractor Y_5 lacks a factor of 1/sqrt(2^n-2).

Written by gpt-6.1-sol from the paper's full text. Automated: it can be wrong.

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16 pages, 6 figures

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Consensus algorithms are mechanisms driving nodes of a network to agreement. In quantum networks they also redistribute information encoded in the global quantum state, allowing global properties to be inferred from local measurements without reconstructing the global state. Motivated by this, we investigate decentralized quantum consensus in qudit networks governed by discrete random unitary dynamics. We characterize the analytic asymptotic dynamics, identify global information preserved by the evolution, and derive conditions for which different notions of quantum consensus emerge. A general theorem is derived that establishes a unified framework for extracting globally encoded information from local measurements beyond consensus states. First, we analyze CNOT networks and determine which global information can be recovered by individual nodes and which requires joint measurements on cooperating nodes. The CNOT model is well understood and presents a case with entanglement creation - a characteristic quantum feature of networks worth analyzing in detail. Second, we identify the complete class of two-qubit interactions that asymptotically achieve consensus on the average number of excitations, thereby establishing a quantum analogue of classical average consensus. We further show that joint measurements on k cooperating nodes recover exactly the first k moments of the excitation-number distribution.
The paper asks which global properties of a quantum-network state survive decentralized dynamics and become accessible through measurements on individual nodes or cooperating subsets. It considers discrete random-unitary channels P(ρ)=∑epeUeρUe†\mathcal P(\rho)=\sum_e p_eU_e\rho U_e^\daggerP(ρ)=∑e​pe​Ue​ρUe†​, with pairwise interactions assigned to network edges.
Using the peripheral eigenspaces of these channels, it derives necessary and sufficient algebraic conditions for expectation-value, reduced-state, and permutation-symmetric consensus. A second theorem characterizes stationary global information accessible through a chosen local observable: its projection onto the stationary attractor space identifies the corresponding conserved global observable, provided its overlaps with nonstationary attractors vanish. The construction extends to multi-node measurements and, as stated in the paper, discrete unital Markov channels.
Two applications illustrate the framework. Strongly connected CNOT networks with n>2n>2n>2 have a five-dimensional stationary attractor space and reach permutation-symmetric consensus. Individual nodes can recover ground-state and uniform-superposition probabilities and an imaginary coherence component, whereas other preserved quantities require two-node measurements. For excitation-number consensus, the paper classifies two-qubit interactions by analyzing the two-node attractor equations, then gives an n+3n+3n+3-dimensional attractor structure for the selected mechanisms at n>2n>2n>2. Proper subsets of mmm nodes access exactly the first mmm moments of the conserved excitation-number distribution; explicit moment observables are constructed recursively.
The analysis concerns asymptotic accessibility. Observable reconstruction becomes harder for large attractor spaces. Non-unital dynamics and a fuller characterization of recoverable properties, particularly in entangled consensus states, are left for future work.
We consider a basic quantum hybrid network model consisting of a number of nodes each holding a qubit, for which the aim is to drive the network to a consensus in the sense that all qubits reach a common state. Projective measurements are applied serving as control means, and the measurement results are exchanged among the nodes via classical communication channels. In this way the quantum-opeartion/classical-communication nature of hybrid quantum networks is captured, although coherent states and joint operations are not taken into consideration in order to facilitate a clear and explicit analysis. We show how to carry out centralized optimal path planning for this network with all-to-all classical communications, in which case the problem becomes a stochastic optimal control problem with a continuous action space. To overcome the computation and communication obstacles facing the centralized solutions, we also develop a distributed Pairwise Qubit Projection (PQP) algorithm, where pairs of nodes meet at a given time and respectively perform measurements at their geometric average. We show that the qubit states are driven to a consensus almost surely along the proposed PQP algorithm, and that the expected qubit density operators converge to the average of the network's initial values.
Abstract—This paper extends the consensus framework, widely studied in the literature on distributed computing and control algorithms, to networks of quantum systems. We define consensus situations on the basis of invariance and symmetry properties, finding four different generalizations of classical consensus states. This new viewpoint can be directly used to study consensus for probability distributions, as these can be seen as a particular case of quantum statistical states: in this light, our analysis is also relevant for classical problems. We then extend the gossip consen-sus algorithm to the quantum setting and prove it converges to symmetric states while preserving the expectation of permutation-invariant global observables. Applications of the framework and the algorithms to estimation and control problems on quantum networks are discussed. Index Terms—Consensus, distributed algorithms, Markov pro-cesses, quantum information and control. I.
This paper extends the consensus framework, widely studied in the literature on distributed computing and control algorithms, to networks of quantum systems. We define consensus situations on the basis of invariance and symmetry properties, finding four different generalizations of classical consensus states. This new viewpoint can be directly used to study consensus for probability distributions, as these can be seen as a particular case of quantum statistical states: in this light, our analysis is also relevant for classical problems. We then extend the gossip consensus algorithm to the quantum setting and prove it converges to symmetric states while preserving the expectation of permutation-invariant global observables. Applications of the framework and the algorithms to estimation and control problems on quantum networks are discussed.
In this article, we consider the partial quantum consensus problem of a qubit network in a distributed view. The local quantum operation is designed based on the Hamiltonian by using the local information of each quantum system in a network of qubits. We construct the unitary transformation for each quantum system to achieve the partial quantum consensus, that is, the directions of the quantum states in the Bloch ball will reach an agreement. A simple case of two-qubit quantum systems is considered first, and a minimum completing time of reaching partial consensus is obtained based on the geometric configuration of each qubit. Furthermore, we extend the approaches to deal with the more general N -qubit networks. Two partial quantum consensus protocols, based on the Lyapunov method for chain graphs and the geometry method for connected graphs, are proposed. The geometry method can be utilized to deal with more general connected graphs, while for the Lyapunov method, the global consensus can be obtained. The numerical simulation over a qubit network is demonstrated to verify the validity and the effectiveness of the theoretical results.
In this paper, we develop a blended dynamics framework for open quantum networks with diffusive couplings. The network consists of qubits interconnected through Hamiltonian couplings, environmental dissipation, and consensus-like diffusive interactions. Such networks commonly arise in spontaneous emission processes and non-Hermitian quantum computing, and their evolution follows a Lindblad master equation. Blended dynamics theory is well established in the classical setting as a tool for analyzing emergent behaviors in heterogeneous networks with diffusive couplings. Its key insight is to blend the local dynamics rather than the trajectories of individual nodes. Perturbation analysis then shows that, under sufficiently strong coupling, all node trajectories tend to stay close to those of the blended system over time. We first show that this theory extends naturally to the reduced-state dynamics of quantum networks, revealing classical-like clustering phenomena in which qubits converge to a shared equilibrium or a common trajectory determined by the quantum blended reduced-state dynamics. We then extend the analysis to qubit coherent states using quantum Laplacians and induced graphs, proving orbit attraction of the network density operator toward the quantum blended coherent dynamics, establishing the emergence of intrinsically quantum and dynamically clustering behaviors. Finally, numerical examples validate the theoretical results.
This paper proposes a novel approach to decentralized computation utilizing a network of quantum computers connected via entangled states. The core concept centers around achieving consensus among the nodes through iterative measurement protocols, capitalizing on the fundamental properties of quantum entanglement for secure and efficient communication. Unlike traditional distributed computing methods, this system leverages quantum superposition and entanglement to simultaneously process information from multiple nodes, offering potential advantages in computational speed and fault tolerance. The system's architecture consists of quantum nodes engaging in measurement campaigns, sharing measurement results via entangled links, and iteratively refining estimates until a consensus is reached. This iterative refinement process is formalized using a mathematical framework, detailing the measurement protocols and convergence criteria. The theoretical analysis demonstrates the feasibility of achieving consensus with a reasonable number of iterations, and highlights the security implications of employing quantum entanglement for data transmission. This work represents a radical departure from conventional distributed computing paradigms, presenting a new paradigm for computation through quantum networks.