on incompatibility of gravitational radiation with the 1915 einstein equation 法律论文

possible to turn (6) to become an equation for a first-order approximation for weak gravity.
from the viewpoint of physics, since it has been proven that (3) necessarily gives a first-order approximation [11], a failure of such a coordinate transformation means only that such a solution is not valid in physics. moreover, for the dynamic of massive matter, experiment [16] supports the fact that maxwell-newton approximation (3) is related to a dynamic solution of weak gravity [13]. otherwise, not only is einstein's radiation formula not valid, but the theoretical framework of general relativity, including the notion of the plane-wave as an idealization, should be re-examined (see section 3). in other words, theoretical considerations in physics as well as experiments eliminate other unverified speculations thought to be possible since 1957.
as shown, the difficulty comes from the assumption of boundedness (section 3), which allows the existence of a bounded first-order approximation, which in turn implies that a time-average of the radiative part of g(2)(( is non-zero (7(. the present method has an advantage over fock's approach to obtaining logarithmic divergence [13,14( for being simple and clear.
in short, according to einstein's radiation formula, a time average of g(2)(t is non-zero and of o(k2/r2) [13(. although (3) implies

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