The measurement of red-shift and flat time.

Details The measurement of red-shift and flat time. The measurement of red-shift and flat time.

Jul 1992

adsabs.harvard.edu/cgi-bin/nph-data_query?bibcode=1992acppb..23..745c&link_type=abstract

Acta Phys. Pol., B, Vol. 23, No. 7, p. 745 - 757

Physics

Quantum Physics

Scientific paper

The measurement of the red-shift (R-S) effect of the general theory of relativity (GTR) resorts to the existence of two essentially different kinds of metrical objects: a) the macro-corpuscules of rigid bodies and the clocks which constitute reference bodies S¯ and b) the light signals never at rest with regard to any reference body, which interconnect different regions of the metrical spacetime found by S¯'s. The aim is to show that the comparison of frequencies of the photons emitted by atomic clocks at different spacetime regions must call for flat time continuum. Thus quantum physics which integrates the wave and the corpuscular aspects of mircoobjects would distinguish flat spacetime.

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