In the present work, we study the interplay between relativistic effects and quantumness in the system of two relativistic fermions. In particular, we explore entropic measures of quantum correlations and quantum discord before and after application of a boost and subsequent Wigner rotation. We also study the positive operator-valued measurements (POVM) invasiveness before and after the boosts. While the relativistic principle is universal and requires Lorentz invariance of quantum correlations in the entire system, we have found specific partitions where quantum correlations stored in particular subsystems are not invariant. We calculate quantum discords corresponding of the states before and after applying a boost, and observe that the state gains extra discord after the boost. When analyzing the invasiveness of the POVMs, we have found that the POVM applied to the initial entangled state reduces the discord to zero. However, discord of the boosted state survives after the same POVM. Thus we conclude that the quantum discord generated by Lorentz boost is robust concerning the protective POVM, while the measurement exerts an invasive effect on the discord of the initial state. Finally, we discuss potential implementation of the ideas of this work using top quarks as a benchmark scenario.
CONTENTSI. Introduction 1 II. Entropic measures 2 III. Quantum formalism in particle-antiparticle production 3 IV. Spin-momentum density matrix 4 A. Spin-momentum system in the rest frame 4 B. Measurement 5 C. Conditional entropies 5 V. Relativistic transformations 6 A. Influence of the Wigner rotations on entanglement 6 B. Measurement 8 C. Conditional entropies 8 VI. Quantum discord 9 A. General expressions and definitions 9 B. Quantum discord for arbitrary boost 10 C. Quantum discord after the measurement 12 VII. Experimental remarks 13 A. Top-antitop quark production 13 B. Specific measurements with top-antitop quark pairs 15 VIII. Conclusions 15 Acknowledgments 15 A. Calculation of entropy for any density matrix 16 B. Simplest case: a system of two spins 16 C. Structure of the density matrix for the boosted system 17 D. Boosted density matrix after the measurement 18 References 18