Skip to main content

Quantum geometry from coordinate transformations relating quantum observers

Abstract

The relativity principle that the law of propagation for light has the same form for all macroscopic observers is extended to include quantum observers; i.e., observers who may be large, but not infinitely large, by comparison with quantum mechanical systems. This leads to the extension of the covariance group from the diffeomorphisms to the conservation group (which is the largest group of coordinate transformations under which conservation laws are covariant statements) and, thus, to the quantum geometry and quantum unified field theory considered in a previous paper.

This is a preview of subscription content, access via your institution.

References

  • Einstein, A. (1949). InAlbert Einstein: Philosopher-Scientist, Vol. I, P. A. Schilpp, ed., p. 89. Harper, New York.

    Google Scholar 

  • Everett, H., III, (1957).Rev. Mod. Phys.,29, 454.

    Google Scholar 

  • Pandres, D., Jr., (1981).Phys. Rev. D,24, 1499.

    Google Scholar 

Download references

Author information

Authors and Affiliations

Authors

Rights and permissions

Reprints and Permissions

About this article

Cite this article

Pandres, D. Quantum geometry from coordinate transformations relating quantum observers. Int J Theor Phys 23, 839–842 (1984). https://doi.org/10.1007/BF02214069

Download citation

  • Received:

  • Issue Date:

  • DOI: https://doi.org/10.1007/BF02214069

Keywords

  • Covariance
  • Field Theory
  • Elementary Particle
  • Quantum Field Theory
  • Mechanical System