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Quantum mutual information, coherence and unified relations of top quarks in QCD processes

Published 3 Apr 2026 in quant-ph and hep-ph | (2604.03005v1)

Abstract: As the most massive particle in the Standard Model, the top quark's exceptionally short lifetime preserves its spin polarization information through direct decay, making it an ideal system for probing quantum correlations in high-energy physics. In this letter, we presents a comprehensive investigation of quantum correlations in top quark-antiquark pairs produced through QCD. We employ multiple quantum information theoretic measures including quantum mutual information, relative entropy of coherence, complete complementarity relations, and the intrinsic relationship, establishing their dependence on kinematic variables. Furthermore, we find that for quarks and gluons initial mixing, as the probability of gluons Wgg increases, the maximum of the left-hand side of the intrinsic relation also increases. We thus believe the current findings are beneficial to insight into the systemic quantumness in QCD.

Summary

  • The paper introduces a comprehensive framework linking quantum mutual information to correlations in top quark pair production.
  • It applies analytical and systematic parameter scans to reveal kinematic dependencies in QCD processes for both gluon and quark initiated channels.
  • It demonstrates how unified complementarity and intrinsic relations quantitatively benchmark quantum coherence and correlations in collider events.

Quantum Mutual Information, Coherence, and Unified Quantum Information Relations in Top Quark Pair Production

Introduction

This work provides a comprehensive analysis of quantum correlations in top quark-antiquark (ttˉt\bar{t}) production in QCD, leveraging contemporary quantum information theoretic tools including quantum mutual information (QMI), relative entropy of coherence (REC), complete complementarity relations (CCR), and a recently established intrinsic relation among these observables. The theoretical framework employed extends the utility of these quantum information measures beyond conventional collider observables (e.g., spin correlation) by probing both quantum and classical correlation structure, quantumness, and resource-related quantities in high-energy physics systems. Through analytical calculations and systematic parameter scans, the paper elucidates the scaling behavior and interplay of quantum observables over a broad kinematic range and for varying admixtures of initial-state QCD partonic channels.

Theoretical Framework and QCD Production Mechanisms

The study considers ttˉt\bar{t} production initiated by both qqˉq\bar{q} annihilation and gggg fusion at leading order in QCD, formalized in terms of invariant mass MttˉM_{t\bar{t}} and the production angle Θ\Theta in the center-of-mass frame. The spin density matrix formalism is utilized to capture the complete polarization and spin correlation content of the final state. The explicit forms for the production spin density matrices ρ^qqˉ\hat{\rho}^{q\bar{q}} and ρ^gg\hat{\rho}^{gg} are derived, parameterized by Lorentz-invariant coefficients with analytic dependence on β=14mt2/Mttˉ2\beta = \sqrt{1 - 4 m_t^2/M_{t\bar{t}}^2} and Θ\Theta. The admixture of partonic initial states is governed by the gluon weight parameter ttˉt\bar{t}0, thereby interpolating between Tevatron-like (ttˉt\bar{t}1 dominance) and LHC-like (ttˉt\bar{t}2 dominance) conditions.

Quantum Mutual Information and Kinematic Dependence

QMI quantifies the total correlation—classical plus quantum—between the top and anti-top quark spins: Figure 1

Figure 1: QMI as a function of invariant mass ttˉt\bar{t}3 and scattering angle ttˉt\bar{t}4 for pure ttˉt\bar{t}5 and pure ttˉt\bar{t}6 initiated ttˉt\bar{t}7 production.

Analysis demonstrates pronounced model and kinematic dependence. In ttˉt\bar{t}8 fusion, QMI exhibits a strong maximum near production threshold at ttˉt\bar{t}9 GeV and decays with increasing qqˉq\bar{q}0. For qqˉq\bar{q}1 annihilation, the inverse trend is observed with QMI increasing as both qqˉq\bar{q}2 and qqˉq\bar{q}3 increase, supporting high-energy, large-angle preference for stronger correlations.

Systematic studies for mixed initial states underscore the continuity of QMI as a function of qqˉq\bar{q}4, with the observable converging to the qqˉq\bar{q}5-dominated regime at high qqˉq\bar{q}6. Figure 2

Figure 2: QMI in qqˉq\bar{q}7 pairs for varying gluon admixture qqˉq\bar{q}8 shows a shift in maximum correlation structure toward the low-mass/large-angle region.

Quantum Coherence as Quantified by REC

The relative entropy of coherence (REC) captures basis-dependent quantum coherence inherent to the total qqˉq\bar{q}9 state: Figure 3

Figure 3: REC as a function of gggg0 and gggg1 for pure gggg2 and gggg3 production.

The REC exhibits clear qualitative distinction between initial channels. In gluon fusion, coherence is maximized at threshold and for small angles, subsequently decaying with gggg4. In contrast, the gggg5 channel yields monotonic enhancement with gggg6 at fixed mass. The admixture of gggg7 and gggg8 allows detailed interpolation, highlighting the nontrivial interplay between kinematic and initial-state effects. Figure 4

Figure 4: REC for varying gggg9, demonstrating the expansion of high-coherence regimes with increasing gluon fusion contribution.

Complete Complementarity and Mutual Constraints

The CCR combine QMI, conditional entropy, REC, and predictability measures, enforcing the constraint

MttˉM_{t\bar{t}}0

For the case at hand, with vanishing predictability and coherence for single subsystems, the relation reduces to a conservation law: Figure 5

Figure 5: QMI, conditional entropy, and their sum (CCR) as functions of MttˉM_{t\bar{t}}1 for fixed MttˉM_{t\bar{t}}2 and various MttˉM_{t\bar{t}}3. The sum remains unity across parameters.

This conservation directly reflects total decoherence of subsystems in the reduced description—a property enforced by environmental tracing inherent to collider measurement and quantum state reduction in QCD.

Intrinsic Relations Among Quantum Information Measures

A central result is the derivation and validation of an intrinsic relation involving conditional entropies, REC, and predictability, offering a nontrivial lower bound (e.g., MttˉM_{t\bar{t}}4 for two-qubit systems): Figure 6

Figure 6: Left-hand side of the intrinsic relation as a function of MttˉM_{t\bar{t}}5 and MttˉM_{t\bar{t}}6 for pure channel production.

Figure 7

Figure 7: Left-hand side of the intrinsic relation for varied MttˉM_{t\bar{t}}7. Higher gluon admixture enhances the lower-bound saturation near threshold at large MttˉM_{t\bar{t}}8.

Figure 8

Figure 8: Intrinsic relation as a function of MttˉM_{t\bar{t}}9 for fixed Θ\Theta0; larger masses reduce the observable’s magnitude at all angles.

Decomposition of the intrinsic relation into conditional entropy, predictability, and REC contributions reveals distinct angle and mass dependence, with coherence predominantly enhanced at large Θ\Theta1 and low Θ\Theta2. Figure 9

Figure 9

Figure 9

Figure 9: Decomposition of the intrinsic relation: (a) conditional entropy sum, (b) predictability, (c) REC, as functions of Θ\Theta3 for representative invariant masses.

Implications and Outlook

The analytic mapping of quantum information observables onto QCD Θ\Theta4 production delivers refined, basis-independent probes of the quantum correlation structure in high-energy processes. The independence of CCR and the universal scaling of the intrinsic relation with initial-state mixing provide tools for distinguishing quantum versus classical sources of correlation and coherence at colliders, with immediate relevance for experimental analyses seeking to characterize entanglement, decoherence, and new physics signals at reconstructed events.

Practically, these results set the stage for systematically benchmarking quantum resource theory observables across hadron collider datasets, extending to differential measurements and systematic scans over BSM-sensitive kinematic regions. Theoretically, the framework invites generalization to other multipartite systems and facilitates the cross-fertilization of quantum resource quantification and particle phenomenology, including in the presence of beyond-the-Standard Model couplings or decohering environments.

Conclusion

This work achieves a rigorous connection between quantum information measures and high-energy collider observables in Θ\Theta5 production. By embedding QMI, REC, and unified CCR/intrinsic relations into a systematic QCD calculation, it both elucidates the quantum structure of top quark events and provides analytic and numerical tools for future experimental and theoretical explorations of quantumness in the Standard Model and beyond.

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