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

Duo-Duo Chen, Xue-Ke Song, Liu Ye, Dong Wang

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.

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

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.

Paper Structure

This paper contains 7 sections, 19 equations, 9 figures.

Figures (9)

  • Figure 1: QMI as a function of invariant mass $M_{t\bar{t} }$ and production angle $\Theta$ for $t\bar{t}$ pairs production processes. (a): $gg \to t\bar{t}$; (b): $q\bar{q} \to t\bar{t}$.
  • Figure 2: QMI in $t\bar{t}$ production with mixed gluons $(gg)$ and quarks $(q\bar{q})$ initial state, where the gluons probability $\mathcal{W} _{gg}$ varies: (a): $\mathcal{W} _{gg}=0.2$; (b): $\mathcal{W} _{gg}=0.4$; (c): $\mathcal{W} _{gg}=0.6$; (d): $\mathcal{W} _{gg}=0.8$.
  • Figure 3: REC as a function of the invariant mass $M_{t\bar{t} }$ and the production angle $\Theta$ in a $t\bar{t}$ pairs. (a): $gg \to t\bar{t}$. (b): $q\bar{q} \to t\bar{t}$.
  • Figure 4: REC $C_{\text{re}}(\hat{\rho}_{AB})$ in $t\bar{t}$ production for mixed gluons $(gg)$ and quarks $(q\bar{q})$ initial state with varying gluon probability $\mathcal{W} _{gg}$: (a): $\mathcal{W} _{gg}=0.2$; (b): $\mathcal{W} _{gg}=0.4$; (c): $\mathcal{W} _{gg}=0.6$; (d): $\mathcal{W} _{gg}=0.8$.
  • Figure 5: CCR in $t\bar{t}$ production from mixed initial states of gluons $(gg)$ and quarks $(q\bar{q})$. Blue circles represent the QMI $I_{A:B}(\hat{\rho} _{AB} )$, orange triangles show conditional entropy $S_{A|B}(\hat{\rho} _{AB} )$, and green diamonds indicate the CCR. The gluons probability $\mathcal{W} _{gg}$ varies: (a): $\mathcal{W} _{gg}=0.2$; (b): $\mathcal{W} _{gg}=0.4$; (c): $\mathcal{W} _{gg}=0.6$; (d): $\mathcal{W} _{gg}=0.8$. The invariant mass is fixed to $M_{t\bar{t} }=500$ GeV.
  • ...and 4 more figures