Isaac Scientific Publishing

Theoretical Physics

Effective Dark Energy from Decoherence

Download PDF (522.2 KB) PP. 22 - 29 Pub. Date: December 30, 2016

DOI: 10.22606/tp.2016.11006

Author(s)

  • Chris Fields*
    243 West Spain Street, Sonoma, United States

Abstract

Within the quantum Darwinist framework introduced by W. H. Zurek (Nat. Phys., 5:181-188, 2009), observers obtain effectively-classical pointer-state information about quantum systems by interacting with local samples of the surrounding environment, e.g. local samples of the ambient photon field. Quantum Darwinism requires the environment to encode such effectivelyclassical information uniformly and hence redundantly throughout its entire volume, making the information equally available to all possible observers regardless of their locations. This framework is applied to the observation of stellar center-of-mass positions, which are assumed to be encoded by the ambient photon field with sufficient redundancy to be uniformly accessible at all locations within our observable universe. Assuming Landauer’s Principle, constructing such an environmental encoding requires (ln2)kT per encoded classical bit. For the observed 1024 stars and a uniform binary encoding of center-of-mass positions into voxels with a linear dimension of 5 km, the free energy required at the current CMB temperature T = 2.7 K is  2.5 · 10−27 kg · m−3, strikingly close to the observed value of ΩΛρc. Decreasing the voxel size to (lP)3 results in a free energy requirement 10117 times larger.

Keywords

Classicality, critical density, dark sector, environment as witness, landauer’s principle, quantum Darwinism

References

[1] PLANCK Collaboration (P. A. R. Ade et al.), “Planck 2013 results. I. Overview of products and scientific results,” Astronomy and astrophysics, vol. 571, paper A1, 2013.

[2] M. Tegmark et al., “Cosmological parameters from SDSS and WMAP,” Physical review D, vol. 69, paper 103501, 2004.

[3] M. Tegmark et al., “Cosmological constraints from the SDSS luminous red galaxies,” Physical review D, vol. 74, paper 123507, 2006.

[4] J. Frieman, M. Turner and D. Huterer Dark energy and the accelerating universe,” Annual review of astronomy and astrophysics, vol. 46, pp. 385-432, 2008.

[5] C. Corda, “Interferometric detection of gravitational waves: The definitive test for General Relativity,” International journal of modern physics D, vol. 18, pp. 2275-2282, 1999.

[6] T. Clifton, P. G. Ferreira, A. Padilla and C. Skordis, “Modified gravity and cosmology,” Physics reports, vol. 513, pp. 1-189, 2012.

[7] PLANCK Collaboration (P. A. R. Ade et al.), “Planck 2015 results. XIV. Dark energy and modified gravity,” Astronomy and astrophysics, vol. 594, paper A14, 2016.

[8] N. Yunes, K. Yagi and F. Pretorius, “Theoretical physics implications of the binary black-hole mergers GW150914 and GW151226,” Physical review D, vol. 94, paper 084002, 2016.

[9] H. Ollivier, D. Poulin and W. H. Zurek, “Objective properties from subjective quantum states: Environment as a witness,” Physical review letters, vol. 93, paper 220401, 2004.

[10] H. Ollivier, D. Poulin and W. H Zurek, “Environment as a witness: Selective proliferation of information and emergence of objectivity in a quantum universe,” Physical review A, vol. 72, paper 042113, 2005.

[11] R. Blume-Kohout and W. H. Zurek, “Quantum Darwinism: Entanglement, branches, and the emergent classicality of redundantly stored quantum information,” Physical review A, vol. 73, paper 062310, 2006.

[12] W. H. Zurek, “Quantum Darwinism,” Nature physics, vol. 5, pp. 181-188, 2009.

[13] C. J. Riedel and W. H. Zurek, “Quantum Darwinism in an everyday environment: Huge redundancy in scattered photons,” Physical review letters, vol. 105, paper 020404, 2010.

[14] C. J. Riedel, W. H. Zurek and M. Zwolak, “The rise and fall of redundancy in decoherence and quantum Darwinism,” New Journal of physics, vol. 14, paper 083010, 2012.

[15] M. Zwolak, C. J. Riedel and W. H. Zurek, “Amplification, redundancy, and quantum Chernoff information,” Physical review letters, vol. 112, paper 140406, 2014.

[16] R. Horodecki, J. K. Korbicz and P. Horodecki, “Quantum origins of objectivity,” Physical review A, vol. 91, paper 032122, 2015.

[17] F. G. S. L. Brand?o, M. Piani and P. Horodecki, “Generic emergence of classical features in quantum Darwinism,” Nature communications, vol. 6, paper 7908, 2015.

[18] R. Landauer, “Irreversibility and heat generation in the computing process,” IBM Journal of research and development, vol. 5, pp. 183-195, 1961.

[19] R. Landauer, “Information is a physical entity,” Physica A, vol. 263, pp. 63-67, 1999.

[20] S. E. Rugh and H. Zinkernagel, “The quantum vacuum and the cosmological constant problem,” Studies in the history and philosophy of modern physics, vol. 33, pp. 663-705, 2002.

[21] D. Zeh, “On the interpretation of measurement in quantum theory,” Foundations of physics, vol. 1, pp. 69-76, 1970.

[22] D. Zeh, “Toward a quantum theory of observation,” Foundations of physics, vol. 3, pp. 109-116, 1973.

[23] W. H. Zurek, “Pointer basis of the quantum apparatus: Into what mixture does the wave packet collapse?” Physical review D, vol. 24, pp. 1516-1525, 1981.

[24] W. H. Zurek, “Environment-induced superselection rules,” Physical review D, vol. 26, pp. 1862-1880, 1982.

[25] E. Joos and D. Zeh, “The emergence of classical properties through interaction with the environment,” Zeitschrift für physik B: Condensed matter, vol. 59, pp. 223-243, 1985.

[26] W. H. Zurek, “Decoherence, einselection and the existential interpretation (the rough guide),” Philosophical transactions of the Royal Society A, vol. 356, pp. 1793-1821, 1998.

[27] W. H. Zurek, “Decoherence, einselection, and the quantum origins of the classical,” Reviews of modern physics, vol. 75, pp. 715-775, 2003.

[28] M. Schlosshauer, Decoherence and the Quantum to Classical Transition, Springer, 2007.

[29] P. Martineau, “On the decoherence of primordial fluctuations during inflation,” Classical and quantum gravity, vol. 24, pp. 5817-5834, 2006.

[30] C. Kiefer and D. Polarski, “Why do cosmological perturbations look classical to us?” Advanced science letters, vol. 2, pp. 164-173, 2009.

[31] J. B. Hartle, “The quasiclassical realms of this quantum universe,” Foundations of physics, vol. 41, pp. 982-1006, 2011.

[32] E. Calzetta, “Chaos, decoherence and quantum cosmology,” Classical and quantum gravity, vol. 29, paper 143001, 2012.

[33] M. Tegmark, “How unitary cosmology generalizes thermodynamics and solves the inflationary entropy problem,” Physical review D, vol. 85, paper 123517, 2012.

[34] J. Martin, V. Vennin and P. Peter, “Cosmological inflation and the quantum measurement problem,” Physical review D, vol. 86, paper 103524, 2012.

[35] P. Ca?ate, P. Pearle and D. Sudarsky, “Continuous spontaneous localization wave function collapse model as a mechanism for the emergence of cosmological asymmetries in inflation,” Physical review D, vol. 87, paper 104024, 2013.

[36] P. van Dokkum and C. A. Conroy, “A substantial population of low-mass stars in luminous elliptical galaxies,” Nature, vol. 468, pp. 940-942, 2010.

[37] C. Conroy and P. van Dokkum, “Counting low-mass stars in integrated light,” Astrophysical journal, vol. 747, paper 69, 2012.

[38] C. Tortora, A. J. Romanowsky and N. R. Napolitano, “An inventory of the stellar initial mass function in early-type galaxies,” Astrophysical journal, vol. 765, paper 8, 2013.

[39] P. Zanardi, “Virtual quantum subsystems,” Physical review letters, vol. 87, paper 077901, 2001.

[40] P. Zanardi, D. A. Lidar and S. Lloyd, “Quantum tensor product structures are observable-induced,” Physical review letters, vol. 92, paper 060402, 2004.

[41] M. Dugic and J. Jeknic, “What is “system”: Some decoherence-theory arguments,” International journal of theoretical physics, vol. 45, pp. 2249-2259, 2006.

[42] M. Dugic and J. Jeknic - Dugic, “What is “system”: The information-theoretic arguments,” International journal of theoretical physics, vol. 47, pp. 805-813, 2008.

[43] A. C. de la Torre, D. Goyeneche and L. Leitao, “Entanglement for all quantum states,” European journal of physics, vol. 31, pp. 325-332, 2010.

[44] N. L. Harshman, N. L.; Ranade, K. S. Observables can be tailored to change the entanglement of any pure state,” Physical review A, vol. 84, paper 012303, 2011.

[45] W. Thirring, R. A. Bertlmann, P. K?hler and H. Narnhofer, “Entanglement or separability: The choice of how to factorize the algebra of a density matrix,” European physical journal D, vol. 64, pp. 181-196, 2011.

[46] M. Dugic and J. Jeknic - Dugic, “Parallel decoherence in composite quantum systems,” Pramana, vol. 79, pp. 199-209, 2012.

[47] C. Fields, “On the Ollivier-Poulin-Zurek definition of objectivity,” Axiomathes, vol. 24, pp. 137-156, 2014.

[48] R. Kastner, “‘Einselection’ of pointer observables: The new H-theorem?” Studies in the history and philosophy of modern physics, vol. 48, Part A, pp. 56-58, 2014.