Abstract

The notion of gravitational radiation as a radiation of the same level as the electromagnetic radiation is based on the theoretically proven and experimentally confirmed facts of the existence of stationary states of an electron in its gravitational field, characterized by the gravitational constant K = 1042 G (G is Newtonian gravitational constant) and unrecoverable space-time curvature Λ. These experimental facts include, in particular, data on the broadening of the spectra of the characteristic radiation of multielectron atoms. This broadening of the spectra can be only due to the additional broadening mechanism, in particular the presence of excited states of electrons in their gravitational field. Another fact is the new line in the X-ray emission spectrum according to the results of observation with MOS-camera of the XMM-Newton observatory. This line unlike other identified lines of electromagnetic radiation cannot be assigned to any atomic transition.

Highlights

  • Numerous attempts to detect experimentally gravitational radiation brought no result

  • Studying the development of the relativistic theory of gravitation, the authors obtained a model of gravitational interaction at the quantum level, which has no analogues [1] [2]

  • This model detailed in these papers made it possible to calculate the spectrum of gravitational radiation and its subsequent interpretation based on the available experimental data

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Summary

Introduction

Numerous attempts to detect experimentally gravitational radiation (as based on the notions of the general relativity theory and alternative theories) brought no result. Studying the development of the relativistic theory of gravitation (which is the relativistic theory of gravitation, and not any of its particular case, such as general relativity theory), the authors obtained a model of gravitational interaction at the quantum level, which has no analogues [1] [2] This model detailed in these papers made it possible to calculate the spectrum of gravitational radiation and its subsequent interpretation based on the available experimental data. The consequence of such resonant interaction is appearance, including new lines, of electromagnetic transitions not associated with atomic transitions

Broadening Spectra of Characteristic Radiation
New Lines in the Spectra of X-Ray Radiation
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