1987
DOI: 10.1007/bf00668779
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Gravitational Yukawa potential from a Yang-Mills theory for gravity

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Cited by 5 publications
(3 citation statements)
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“…and F 1 (k, t) = g 1 n(k, t). At this point, it should be noticed that this new wave-kinetic equation is coupled with the radiation transport Equation (22) in two different ways: first, through the expression of the force function F 0 , which depends on the radiation intensity I(r, t) and, second, through the dependence of the diffusion coefficient D on the density of matter, or equivalently, on the quasi-probability W.…”
Section: Diffusive Radiationmentioning
confidence: 99%
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“…and F 1 (k, t) = g 1 n(k, t). At this point, it should be noticed that this new wave-kinetic equation is coupled with the radiation transport Equation (22) in two different ways: first, through the expression of the force function F 0 , which depends on the radiation intensity I(r, t) and, second, through the dependence of the diffusion coefficient D on the density of matter, or equivalently, on the quasi-probability W.…”
Section: Diffusive Radiationmentioning
confidence: 99%
“…We can study the evolution of the SN system, associated with matter coupled with a background, as described by the wave-kinetic Equation (26) and the radiation transport Equation (22). We start from a given equilibrium (I 0 , W 0 , n 0 ) and consider perturbations (Ĩ k ,W k ,ñ k ) evolving with frequency ω and wavevector k. Replacing this in Equation ( 26), we obtain, after linearization:…”
Section: Modified Jeans Instabilitymentioning
confidence: 99%
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