2011
DOI: 10.1134/s1064229311070076
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Reflections on the new monograph by M.A. Glazovskaya

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Cited by 4 publications
(12 citation statements)
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“…In such the model, the Newton constant may be computed. The attractive force F 1 due to pressure of single gravitons in this model is equal to: 4 • G, that is of three order greater than the Newton constant, G. If single gravitons are elastically scattered, they create a repulsive force F ′ 1 which is equal to F 1 . But for black holes which absorb any particles and do not re-emit them, we will have F ′ 1 = 0.…”
Section: A Quantum Mechanism Of Classical Gravitymentioning
confidence: 90%
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“…In such the model, the Newton constant may be computed. The attractive force F 1 due to pressure of single gravitons in this model is equal to: 4 • G, that is of three order greater than the Newton constant, G. If single gravitons are elastically scattered, they create a repulsive force F ′ 1 which is equal to F 1 . But for black holes which absorb any particles and do not re-emit them, we will have F ′ 1 = 0.…”
Section: A Quantum Mechanism Of Classical Gravitymentioning
confidence: 90%
“…It was shown by the author [4,5] that screening the background of superstrong interacting gravitons creates for any pair of bodies both attractive and repulsive forces due to pressure of gravitons. For single gravitons, these forces are approximately equal.…”
Section: A Quantum Mechanism Of Classical Gravitymentioning
confidence: 99%
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