- Letter
- Open Access
Alternative interpretation of relativistic time-reversal and the time arrow
Phys. Rev. Research 4, L022052 – Published 1 June, 2022
DOI: https://doi.org/10.1103/PhysRevResearch.4.L022052
Abstract
It is well known that the 4-rotation in four-dimensional space-time is equivalent to the transformation ( is the charge conjugation, is the space inversion, and is the time reversal). The standard definition of the reversal includes the change of the sign of the time variable and replacement of the initial state of the particle (system of particles) by the final state and vice versa. Since the time-reversal operation changes the state of a particle, the particle's wave function cannot be the eigenfunction of the corresponding operator with a certain eigenvalue, as in the case of space parity. Unlike the transformation, the separate , , or transformations cannot be reduced to any 4-rotation. The extended Lorentz group incorporates all the separate , , or transformations which do not bring the time axis out of the corresponding light cone. The latter restriction is included in the standard definition of the time reversal. In the present Letter, we ignore this restriction. This allows us to introduce the “time arrow” operator and characterize every particle by the new quantum number—the “time arrow” value. The wave functions of all particles are eigenfunctions of this operator with eigenvalues equal to time arrow values. The particles with the time arrow values opposite to the time arrow value in our universe form another universe (antiuniverse). The existence of an antiuniverse can be confirmed, in principle, by laboratory (atomic) experiments. The antiuniverse may be also considered as a candidate for the role of dark matter.
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References (30)
- J. H. Christenson, J. W. Cronin, V. L. Fitch, and R. Turlay, Evidence for the Decay of the Meson, Phys. Rev. Lett. 13, 138 (1964).
- E. M. Purcell and N. F. Ramsey, On the possibility of electric dipole moments for elementary particles and nuclei, Phys. Rev. 78, 807 (1950).
- P. Sandars, The electric dipole moment of an atom, Phys. Lett. 14, 194 (1965).
- P. Sandars, in Atomic Physics 4, edited by G. zu Putlitz, E. W. Weber, and A. Winnacker (Springer, Boston, 1975), pp. 71–92.
- O. Sushkov and V. Flambaum, Parity breaking effects in diatomic molecules, J. Exp. Theor. Phys. 48, 608 (1978).
- V. G. Gorshkov, L. N. Labzovskii, and A. N. Moskalev, Effects of nonconservation of spatial and temporal parities in spectra of diatomic molecules, J. Exp. Theor. Phys. 49, 209 (1979).
- V. Andreev, D. G. Ang, D. DeMille, J. M. Doyle, G. Gabrielse, J. Haefner, N. R. Hutzler, Z. Lasner, C. Meisenhelder, B. R. O'Leary, C. D. Panda, A. D. West, E. P. West, X. Wu et al. (ACME Collaboration), Improved limit on the electric dipole moment of the electron, Nature (London) 562, 355 (2018).
- Y. Yamaguchi and N. Yamanaka, Quark level and hadronic contributions to the electric dipole moment of charged leptons in the standard model, Phys. Rev. D 103, 013001 (2021).
- M. Pospelov and A. Ritz, CKM benchmarks for electron electric dipole moment experiments, Phys. Rev. D 89, 056006 (2014).
- D. V. Chubukov and L. N. Labzowsky, Pt-odd electron-nucleus interaction in atomic systems as an exchange by Higgs bosons, Phys. Rev. A 93, 062503 (2016).
- J. P. Lees et al. (The BABAR Collaboration), Observation of Time-Reversal Violation in the Meson System, Phys. Rev. Lett. 109, 211801 (2012).
- V. Berestetskii, E. Lifshits, and L. Pitaevskii, Quantum Electrodynamics (Oxford Butterworth-Heinemann, Oxford, U.K., 1982).
- S. Weinberg, The Quantum Theory of Fields (Cambridge University Press, Cambridge, U.K., 1995), Vol. 1.
- E. Wigner, On the quantum correction for thermodynamic equilibrium, Phys. Rev. 40, 749 (1932).
- L. Maccone, Quantum Solution to the Arrow-of-Time Dilemma, Phys. Rev. Lett. 103, 080401 (2009).
- D. Jennings and T. Rudolph, Comment on “Quantum Solution to the Arrow-of-Time Dilemma”, Phys. Rev. Lett. 104, 148901 (2010).
- T. B. Batalhão, A. M. Souza, R. S. Sarthour, I. S. Oliveira, M. Paternostro, E. Lutz, and R. M. Serra, Irreversibility and the Arrow of Time in a Quenched Quantum System, Phys. Rev. Lett. 115, 190601 (2015).
- G. Rubino, G. Manzano, and Č. Brukner, Quantum superposition of thermodynamic evolutions with opposing time's arrows, Commun. Phys. 4, 251 (2021).
- S. Goldstein, R. Tumulka, and N. Zanghì, Is the hypothesis about a low entropy initial state of the universe necessary for explaining the arrow of time? Phys. Rev. D 94, 023520 (2016).
- L. Boyle, K. Finn, and N. Turok, -Symmetric Universe, Phys. Rev. Lett. 121, 251301 (2018).
- L. Boyle and N. Turok, Quantum causality and the arrows of time and thermodynamics, arXiv:2109.06204.
- E. Alvarez, Exercise: Dark Matter as fields that evolve backward in time, arXiv:1803.08531.
- J. F. Donoghue and G. Menezes, Quantum causality and the arrows of time and thermodynamics, Prog. Part. Nucl. Phys. 115, 103812 (2020).
- T. D. Lee and C. N. Yang, Question of parity conservation in weak interactions, Phys. Rev. 104, 254 (1956).
- I. Y. Kobzarev, L. B. Okun, and I. Y. Pomeranchuk, On the possibility of experimental observation of mirror particles, Sov. J. Nucl. Phys. 3, 837 (1966).
- L. Landau, On the conservation laws for weak interactions, Nucl. Phys. 3, 127 (1957).
- S. I. Blinnikov, Mirror matter and other dark matter models, Phys. Usp. 57, 183 (2014).
- L. D. Landau and E. M. Lifshitz, Field Theory (Pergamon Press, Oxford, U.K., 1965).
- I. B. Khriplovich, Parity Nonconservation in Atomic Phenomena (Gordon and Breach, Philadelphia, 1991).
- S. Weinberg, The decay of the proton, Sci. Am. 244, 64 (1981).