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Statistical Mechanics of Covariant Systems with Multi-fingered Time

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Abstract

In recent previous work, the authors proposed a new approach extending the framework of statistical mechanics to reparametrization-invariant systems with no additional gauges. In this paper, the approach is generalized to systems defined by more than one Hamiltonian constraint (multi-fingered time). We show how well-known features as the Ehrenfest–Tolman effect and the Jüttner distribution for the relativistic gas can be consistently recovered from a covariant approach in the multi-fingered framework. Eventually, the crucial role played by the interaction in the definition of a global notion of equilibrium is discussed.

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Notes

  1. The “problem of time” has played a central role for several distinct issues [6, 7], from the choice of an internal time variable in quantum gravity, to the emergence of a directional global time in cosmology.

  2. If \(C^b\) is not the only conserved quantity for \(\mathcal {S}^b\), the statistical state should include additional “\(\delta\)-functions”.

  3. The split \(C= C^a+C^b=0\) determines a foliation of the presymplectic surface

    $$\begin{aligned} \varSigma = \bigsqcup _{I^a+I^b=0} \varSigma ^a_{I^a} \times \varSigma ^b_{I^b}, \end{aligned}$$

    where \(X^\alpha = \bigsqcup _{I^\alpha } \varSigma ^\alpha _{I^\alpha }\) and \(I^\alpha\) is the value of \(C^\alpha\) on the leave. Each \(\left( \varSigma ^\alpha _{I^\alpha }, \omega _{X^\alpha }|_{\varSigma ^\alpha _{I^\alpha }} \right)\) is the presymplectic space that would describe the subsystem \(\mathcal {S}^\alpha\) if it was isolated. The existence of the split implies the existence of the conserved quantity \(I=I^b=-I^a\), defined up to clock reparametrization \(I \rightarrow f(I)\). See cf. [8] for full details.

  4. This fact was actually glimpsed by Einstein [12], even before General Relativity was completed!

  5. So that the local gravitational field is approximately uniform.

  6. V can be thought as an effective potential coming from a (Lorentz invariant) interaction with an (relativistic) ambient field.

  7. In the absence of an external potential, the total 4-momentum is conserved, insuring Lorentz covariance of the statistical state.

References

  1. Bardeen, J.M., Carter, B., Hawking, S.W.: The four laws of black hole mechanics. Commun. Math. Phys. 31(2), 161–170 (1973)

    Article  ADS  MathSciNet  Google Scholar 

  2. Hawking, S.W.: Black hole explosions? Nature 248(5443), 30–31 (1974)

    Article  ADS  Google Scholar 

  3. Bekenstein, J.D.: Black holes and entropy. Phys. Rev. D 7, 2333–2346 (1973)

    Article  ADS  MathSciNet  Google Scholar 

  4. Jacobson, T.: Thermodynamics of spacetime: the Einstein equation of state. Phys. Rev. Lett. 75, 1260–1263 (1995)

    Article  ADS  MathSciNet  Google Scholar 

  5. Verlinde, E.: On the origin of gravity and the laws of Newton. J. High Energy Phys. 2011(4), 1–27 (2011)

    Article  MathSciNet  Google Scholar 

  6. Kuchař, K.V.: Time and interpretations of quantum gravity. In: G. Kunstatter, D.E. Vincent, and J.G. Williams (eds.), Proceedings of the 4th Canadian Conference on General Relativity and Relativistic Astrophysics, p. 211 (1992)

  7. Rovelli, C.: Analysis of the distinct meanings of the notion of time, in different physical theories. Il Nuovo Cimento B Series 11 110(1), 81–93 (1995)

    Article  MathSciNet  Google Scholar 

  8. Chirco, G., Josset, T., Rovelli, C.: Statistical mechanics of reparametrization-invariant systems. It takes three to tango. Class. Quant. Gravity 33(4), 045005 (2016)

    Article  ADS  MathSciNet  Google Scholar 

  9. Dirac, P. A. M.: Generalized hamiltonian mechanics. Can. J. Maths. Phys. 2 (1950)

  10. Rovelli, C.: Quantum Gravity. Cambridge University Press, Cambridge (2004)

    Book  Google Scholar 

  11. Tolman, R.: On the weight of heat and thermal equilibrium in general relativity. Phys. Rev. 35, 904–924 (1930)

    Article  ADS  Google Scholar 

  12. Einstein, A.: Zur theorie des statischen gravitationsfeldes. Ann. Phys. 38, 443–458 (1912)

    Article  Google Scholar 

  13. Tolman, R., Ehrenfest, P.: Temperature equilibrium in a static gravitational field. Phys. Rev. 36, 1791–1798 (1930)

    Article  ADS  Google Scholar 

  14. Balazs, N., Dawson, J.: On thermodynamic equilibrium in a gravitational field. Physica 31(2), 222–232 (1965)

    Article  ADS  MathSciNet  Google Scholar 

  15. Ebert, R., Göbel, R.: Carnot cycles in general relativity. Gen. Relat. Gravit. 4(5), 375–386 (1973)

    Article  ADS  MathSciNet  Google Scholar 

  16. Rovelli, C., Smerlak, M.: Thermal time and the Tolman–Ehrenfest effect: temperature as the speed of time. Class. Quant. Gravit. 28, 075007 (2011)

    Article  ADS  MathSciNet  Google Scholar 

  17. Haggard, H.M., Rovelli, C.: Death and resurrection of the zeroth principle of thermodynamics. Phys. Rev. D 87, 084001 (2013)

    Article  ADS  Google Scholar 

  18. Jüttner, F.: Das maxwellsche gesetz der geschwindigkeitsverteilung in der relativtheorie. Ann. Phys. 339(5), 856–882 (1911)

    Article  Google Scholar 

  19. Cubero, D., Casado-Pascual, J., Dunkel, J., Talkner, P., Hänggi, P.: Thermal equilibrium and statistical thermometers in special relativity. Phys. Rev. Lett. 99, 170601 (2007)

    Article  ADS  Google Scholar 

  20. Rovelli, C.: Why Gauge? Found. Phys. 44, 91–104 (2014)

    Article  ADS  Google Scholar 

  21. Chirco, G., Haggard, H.M., Rovelli, C.: Coupling and thermal equilibrium in general-covariant systems. Phys. Rev. D 88, 084027 (2013)

    Article  ADS  Google Scholar 

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Acknowledgements

The authors are grateful to Carlo Rovelli for careful reading of the draft and useful comments, and to the Quantum Gravity Group at the Centre de Physique Théorique de Luminy, where this project was started. G.C. is grateful to Daniele Oriti and Hermann Nicolai for the support at the Max Planck Institute for Gravitational Physics in Potsdam, where the work was partially completed.

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Correspondence to Goffredo Chirco.

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Chirco, G., Josset, T. Statistical Mechanics of Covariant Systems with Multi-fingered Time. Found Phys 51, 3 (2021). https://doi.org/10.1007/s10701-021-00406-3

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