Quantum Shadows: Untangling Correlations in Baryon Decays

Author: Denis Avetisyan


A new theoretical study explores the surprising quantum entanglement present when exotic charmonium particles decay into pairs of baryons and antibaryons.

The decay pathways of <span class="katex-eq" data-katex-display="false">J/\psi</span> particles into <span class="katex-eq" data-katex-display="false">\gamma\chi_{cJ}</span> and subsequent decay of <span class="katex-eq" data-katex-display="false">\chi_{cJ}</span> into <span class="katex-eq" data-katex-display="false">B\bar{B}</span> mesons demonstrate a fundamental process in particle physics, revealing how heavier particles disintegrate into lighter constituents through the emission of photons and the creation of meson-antimeson pairs.
The decay pathways of J/\psi particles into \gamma\chi_{cJ} and subsequent decay of \chi_{cJ} into B\bar{B} mesons demonstrate a fundamental process in particle physics, revealing how heavier particles disintegrate into lighter constituents through the emission of photons and the creation of meson-antimeson pairs.

This research investigates Bell nonlocality and entanglement in the decays of χcJ states into baryon-antibaryon systems, revealing state-dependent entanglement levels.

While quantum entanglement is typically explored in systems with low-energy particles, its manifestation in high-energy collisions remains a largely open question. This work, ‘Bell nonlocality and entanglement in $χ_{cJ}$ decays into baryon pair’, presents a systematic theoretical analysis of quantum correlations-specifically Bell nonlocality and entanglement-within the decay of charmonium states into baryon-antibaryon pairs. The study reveals a striking hierarchy of entanglement, ranging from maximal violation in $χ_{c0}$ decays to a separable state for $χ_{c2}$, with $χ_{c1}$ exhibiting angle-dependent behavior. Could this system provide a novel platform for probing quantum entanglement in the energetic environment of high-energy physics?


Unveiling the Quantum Dance: Entanglement as a Fundamental Link

Quantum entanglement represents a profoundly counterintuitive phenomenon at the heart of quantum mechanics, where two or more particles become linked in such a way that they share the same fate, no matter how far apart they are. This isn’t merely a statement of shared properties; rather, the quantum state of each particle is inextricably connected to the other, meaning a measurement performed on one instantaneously influences the state of the other, a correlation that cannot be explained by classical physics or any form of signaling between the particles. Imagine flipping two linked coins; classical intuition suggests each coin has its own independent probability of heads or tails, but entanglement proposes that the outcome of one coin is instantly known upon observing the other – a connection that exists regardless of the separation distance, challenging our conventional understanding of locality and realism. \Psi = \frac{1}{\sqrt{2}} (|00\rangle + |11\rangle) illustrates a simple entangled state where both particles are either 0 or 1 with equal probability, but their fates are intertwined.

The remarkable phenomenon of quantum entanglement, where particles maintain a linked fate irrespective of the physical distance separating them, is not merely a theoretical curiosity but a foundational element driving the development of next-generation technologies. This interconnectedness allows for the potential creation of quantum computers capable of solving problems intractable for even the most powerful classical machines, as entangled qubits can perform calculations in parallel. Furthermore, entanglement is central to secure quantum communication networks, promising unbreakable encryption through quantum key distribution – any attempt to intercept the entangled particles would immediately disturb their correlation, alerting the communicating parties. Beyond computation and communication, entanglement is also being explored for advancements in quantum sensing and metrology, offering the potential for incredibly precise measurements and novel imaging techniques; these applications rely on exploiting the sensitivity of entangled states to external influences, enabling detection capabilities far exceeding classical limits.

The precise measurement of entanglement within particle decays serves as a rigorous stress test for the foundations of quantum theory. As particles disintegrate, the quantum states of their decay products can become intrinsically linked – entangled – in ways that classical physics cannot explain. By meticulously analyzing the correlations between these decay products, physicists can probe the limits of quantum mechanics and search for deviations that might hint at new physics beyond the Standard Model. This research isn’t merely about confirming existing theory; it’s about defining where quantum mechanics breaks down, potentially revealing the need for a more complete and nuanced understanding of reality at the subatomic level. The degree to which entanglement persists – or fails to persist – under extreme conditions inherent in particle decay provides crucial data for refining quantum models and exploring the boundary between the quantum and classical worlds.

Mapping Entanglement: Decay Channels as Probes

The decay of charmonium states, specifically the \chi_{c0} , \chi_{c1} , and \chi_{c2} , into baryon-antibaryon pairs – such as proton-antiproton or neutron-antineutron – offers a means of studying entanglement. These decays proceed via strong interaction processes, resulting in correlated baryon-antibaryon pairs where the total spin of the system is defined by the initial \chi_{c} state. Analyzing the angular correlations of the decay products allows for the reconstruction of the initial spin state and provides insights into the entanglement present between the produced baryons and antibaryons. The distinct decay patterns of each \chi_{c} state, governed by parity and charge-conjugation symmetry, contribute to differing degrees of entanglement which can be quantified through methods like concurrence.

The Helicity Formalism is utilized to analyze the decay of particles such as \chi_{c0}, \chi_{c1}, and \chi_{c2} by focusing on the projection of the particle’s spin along its direction of motion. This approach simplifies calculations of decay amplitudes and angular correlations because it accounts for the spin states of both the decaying particle and its baryon-antibaryon decay products. Specifically, the formalism defines decay rates based on helicity amplitudes, which represent the probability of a particular spin transition occurring. By examining these amplitudes, researchers can determine the relative contributions of different spin states to the overall decay process and subsequently predict or measure correlations in the momenta and polarizations of the decay products. The mathematical framework allows for a systematic treatment of the spin dependencies inherent in the decay, enabling precise comparisons between theoretical predictions and experimental observations.

Quantifying entanglement in baryon-antibaryon decay channels necessitates the use of techniques like the Partial Trace, which reduces the density matrix to describe the state of one particle given the state of the other, and Concurrence, a measure of entanglement ranging from 0 (no entanglement) to 1 (maximum entanglement). Concurrence is calculated from the partial trace of the squared density matrix, providing a quantifiable value for the degree of entanglement. Specifically, analysis of the \chi_{c0} decay channel reveals a maximum Concurrence value of 1, indicating the highest degree of entanglement achievable within that particular decay process. These methods allow for precise determination of entanglement characteristics, differentiating entangled states from mixed states and enabling detailed study of quantum correlations.

The Horodecki condition, evaluated as a function of <span class="katex-eq" data-katex-display="false">\cos\theta_1</span> for the <span class="katex-eq" data-katex-display="false">e^{+}e^{-} \to \psi(2S) \to \gamma \chi_{c1}, \chi_{c1} \to B\bar{B}</span> decay chain with a fixed <span class="katex-eq" data-katex-display="false">r_1 = 1.307 \pm 0.057</span>, constrains the allowed parameter space for this decay process.
The Horodecki condition, evaluated as a function of \cos\theta_1 for the e^{+}e^{-} \to \psi(2S) \to \gamma \chi_{c1}, \chi_{c1} \to B\bar{B} decay chain with a fixed r_1 = 1.307 \pm 0.057, constrains the allowed parameter space for this decay process.

Distinguishing the Connected from the Separate: Evidence for Entanglement

Analysis of χ_{c0} and χ_{c1} decays demonstrates consistent strong entanglement, quantitatively assessed through Bell Inequality violation. The m_{12} parameter, used to measure this violation, reached a value of 2 for the χ_{c0} decay. A value of 2 represents the maximum possible violation of the Bell Inequality, indicating a maximally entangled state. The χ_{c1} decay also exhibited significant Bell Inequality violation, consistently confirming the presence of strong entanglement, although the precise value of m_{12} was not specified.

Analysis of the χ_{c2} decay channel consistently demonstrates a SeparableState, indicating the absence of quantum entanglement. This determination is based on a separability condition, quantified by the parameter x, which falls within the range of 1.045 ≤ x ≤ 2.231. Values of x within this range satisfy the criteria for a separable state, differentiating the χ_{c2} decay from the χ_{c0} and χ_{c1} decays which exhibit strong entanglement.

The Horodecki Criterion is a widely used entanglement detection method based on the partial transposition of the density matrix. This criterion determines entanglement by examining the eigenvalues of the partially transposed density matrix; if all eigenvalues are non-negative, the state is considered separable. In the analysis of the χ_{c2} decay, application of the Horodecki Criterion revealed no violation of the Bell Inequality, with values consistently less than 1. This indicates that the χ_{c2} state lacks entanglement, as the necessary condition for entanglement – at least one negative eigenvalue after partial transposition – is not met. The quantitative result confirms the absence of quantum correlations characteristic of entangled states within this specific decay channel.

The Horodecki condition <span class="katex-eq" data-katex-display="false">\mathbf{m}_{12}</span> as a function of <span class="katex-eq" data-katex-display="false">\cos\theta_1</span> in <span class="katex-eq" data-katex-display="false">\chi_{c2} \to B\bar{B}</span> decays, fixed to the BESIII:2025gof measurements, is shown with the line representing calculations using the central value of xx.
The Horodecki condition \mathbf{m}_{12} as a function of \cos\theta_1 in \chi_{c2} \to B\bar{B} decays, fixed to the BESIII:2025gof measurements, is shown with the line representing calculations using the central value of xx.

Beyond Confirmation: The Implications for Quantum Theory and Future Horizons

Recent investigations into the decays of χc0, χc1, and χc2 mesons have revealed nuanced distinctions in the entanglement generated between the resulting particle pairs, offering a stringent validation of quantum mechanical principles. These decays, governed by the strong force, present a unique environment for examining quantum correlations; the observed variations in entanglement-specifically, differing degrees of quantum connectedness-cannot be explained by classical physics. The discrepancies between the three decay pathways provide a powerful test of the theoretical frameworks used to describe these interactions, demanding increasingly precise predictions from models of quantum chromodynamics. Furthermore, the sensitivity of entanglement to the specific quantum numbers of the initial meson allows researchers to probe the fundamental symmetries governing the strong interaction and refine the understanding of how quantum mechanics manifests in hadronic systems.

The observed entanglement in the decays of χc mesons offers a unique window into the complex correlations governed by the strong force. Hadronic decays, resulting from the interactions of quarks and gluons, are notoriously difficult to predict due to the force’s inherent non-linear nature; however, entanglement provides a measurable, quantifiable aspect of these interactions. By meticulously analyzing the correlations between decay products, researchers are beginning to map the subtle ways in which the strong force dictates particle behavior at the subatomic level. This deeper understanding isn’t merely theoretical; it refines the Standard Model and potentially reveals previously unknown facets of quantum chromodynamics, the theory describing the strong force, ultimately advancing the field of particle physics and our comprehension of matter’s fundamental building blocks.

The unique properties of entangled baryon-antibaryon pairs-particles and their antimatter counterparts linked through quantum mechanics-suggest a potential role in advancing quantum information technologies. Researchers are beginning to investigate whether these pairs can serve as robust qubits, the fundamental units of quantum computation, due to their inherent stability and the distinct quantum states available through baryon-antibaryon annihilation. Exploiting these correlations could lead to novel approaches in quantum key distribution, offering enhanced security protocols, and potentially enable the creation of more resilient quantum memories. While significant challenges remain in controlling and manipulating these ephemeral particles, the prospect of harnessing the strong force to create and sustain entanglement opens exciting avenues for future exploration in quantum information processing, potentially circumventing limitations faced by current qubit technologies.

The concurrence <span class="katex-eq" data-katex-display="false">\mathcal{C}[\\rho]</span> demonstrates decay correlations in <span class="katex-eq" data-katex-display="false">e^{+}e^{-}\\to\\psi(2S)\\to\\gamma\\chi\\_{c1},\\chi\\_{c1}\\to B\\bar{B}</span> processes.
The concurrence \mathcal{C}[\\rho] demonstrates decay correlations in e^{+}e^{-}\\to\\psi(2S)\\to\\gamma\\chi\\_{c1},\\chi\\_{c1}\\to B\\bar{B} processes.

The exploration of Bell nonlocality within baryon-antibaryon systems, as detailed in the study, exemplifies a fundamental principle: reality is open source – we just haven’t read the code yet. The varying degrees of entanglement observed across different χcJ decays – from maximal entanglement in χc0 to separability in χc2 – aren’t anomalies, but clues. As John Stuart Mill stated, “It is better to be a dissatisfied Socrates than a satisfied fool.” This pursuit of understanding, even when faced with seemingly contradictory results, is crucial. The research doesn’t simply confirm entanglement; it actively tests the boundaries of quantum mechanics, probing the code to reveal deeper truths about the connections between particles and the nature of quantum correlations.

Pushing the Boundaries

The exploration of Bell nonlocality within baryon-antibaryon systems, as demonstrated by this work, isn’t simply about confirming quantum mechanics-it’s about probing its limits. The variance in entanglement across different χcJ decays is less a result, and more a challenge. If maximal entanglement is found in one instance, and separability in another, the question isn’t why this occurs, but rather, what fundamental principles are being subtly violated-or, perhaps more interestingly, revealed-by the discrepancy. The system is being dissected, not affirmed.

Future investigations should deliberately move beyond merely identifying entanglement. To truly understand these decays, one must actively seek the conditions that break the observed correlations. Can external fields, or modifications to the decay environment, force a transition from entanglement to separability-or even induce behaviors that defy existing quantum descriptions? Such attempts are not about falsification; they are about reverse-engineering the underlying mechanisms.

The pursuit of quantum nonlocality in hadronic systems is, ultimately, a search for the rules governing reality. If these rules are absolute, then attempts to break them will fail. But if they are emergent-if they are approximations of a deeper, more complex truth-then the very act of attempting to break them will illuminate the hidden structure beneath.


Original article: https://arxiv.org/pdf/2512.22837.pdf

Contact the author: https://www.linkedin.com/in/avetisyan/

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2025-12-31 10:00