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Bose-Einstein condensation in relativistic plasma (1908.04402v1)

Published 12 Aug 2019 in physics.plasm-ph, astro-ph.HE, and cond-mat.stat-mech

Abstract: The phenomenon of Bose-Einstein condensation is traditionally associated with and experimentally verified for low temperatures: either of nano-Kelvin scale for alkali atoms [1-3] or room temperatures for quasi-particles [4,5] or photons in two dimensions [6]. Here we demonstrate out of first principles that for certain initial conditions non-equilibrium plasma at relativistic temperatures of billions of Kelvin undergoes condensation, predicted by Zeldovich and Levich in their seminal work [7]. We determine the necessary conditions for the onset of condensation and discuss the possibilities to observe such a phenomenon in laboratory and astrophysical conditions.

Citations (2)

Summary

  • The paper reveals that Bose-Einstein condensation emerges in relativistic electron-positron plasma under specific initial photon conditions.
  • It employs kinetic theory and solves relativistic Boltzmann equations with Uehling-Uhlenbeck collision integrals to model both transient and sustained condensation phases.
  • The study quantifies characteristic timescales and spectral adjustments, providing insights for astrophysical contexts and experimental validations.

Bose-Einstein Condensation in Relativistic Plasma: An Analytical Approach

The paper, "Bose-Einstein condensation in relativistic plasma," addresses a unique aspect of quantum statistical mechanics by exploring the conditions under which Bose-Einstein Condensation (BEC) can occur in relativistic, high-temperature plasma. The researchers M. A. Prakapenia and G. V. Vereshchagin provide a comprehensive analysis, backing up the theoretical predictions made by Zeldovich and Levich regarding photon condensation at high relativistic temperatures.

Bose-Einstein condensation is a quantum mechanical phenomenon typically observed in systems at ultra-cold temperatures, where particles gather into the lowest quantum state, leading to macroscopic quantum phenomena. Traditionally, this phenomenon has been associated with low temperatures, as seen in experiments with alkali atoms and photons in confined conditions. However, this paper challenges the conventional understanding by showing that BEC can also emerge in a non-equilibrium plasma at relativistic temperatures, opening new theoretical and practical perspectives in plasma physics.

Main Findings

  1. Analytical and Numerical Evidence: The paper leverages kinetic theory and solves relativistic Boltzmann equations with Uehling-Uhlenbeck collision integrals to show that under specific initial conditions, BEC is achievable in optically thick electron-positron plasma. The results are presented for both nonrelativistic and relativistic temperature regimes and exhibit that BEC can manifest as a transient state during the relaxation of the plasma.
  2. Initial Conditions and Stability: It is shown that for BEC to occur, the initial distribution of photons should not exceed Wien distribution in width, with the peak energy above the critical level where triple interactions dominate. The characteristic transitional nature of the condensation is maintained for both low and relativistic temperature scenarios, albeit with variations in spectral characteristics.
  3. Condensate Dynamics: The paper meticulously calculates the timescales of kinetic and thermal equilibria, highlighting the stages at which photon condensation emerges and eventually dissipates. In the nonrelativistic field, BEC is observed to sustain longer than in relativistic scenarios due to slower thermalization processes.
  4. Photon Distribution Adjustments: In contrast to previous assumptions, the paper demonstrates that initial states with broader spectral distributions, including the Planck distribution, do not favor condensation unless specific conditions regarding photon energy and density are met.

Theoretical and Practical Implications

The implications of this research are multifaceted. Theoretically, it redefines the landscape of BEC applicability beyond low-temperature regimes into realms of extreme energy conditions, thereby expanding the boundaries of quantum statistical mechanics. It also aligns photon condensates in plasma with concepts akin to those within microcavity settings, elucidating the transient nature of these phenomena.

Practically, this research proposes scenarios that might allow for the observation of BEC at relativistic energies, pushing forward the capabilities of current experimental setups like X-ray lasers and dense plasma targets. The identification of BEC in astrophysical contexts, such as gamma-ray bursts, offers another intriguing application by suggesting that such phenomena might offer critical insight into particle distributions in high-energy environments in the universe.

Future Directions

The paper paves the way for future exploration into condensate dynamics under astrophysical and laboratory conditions. Experimental validation remains a critical next step, particularly in verifying the predicted transient behaviors and interaction-specific signatures that define photon condensation. Investigating the adaptation of these principles in the context of other fundamental particles would also serve to enrich the foundational knowledge of quantum anomalies in high-energy physics.

In conclusion, Prakapenia and Vereshchagin's research effectively bridges a gap in understanding BEC, demonstrating its presence at temperatures previously thought to inhibit such phenomena. This work not only invites experimental confirmation but also enriches the theoretical landscape by introducing the potential for broader applicability and understanding of BEC in plasma physics.

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