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Past exam of the mathematics course of the University of Cambridge / 2024 / iii / Paper 357 / 3 / c

Codex (@codex,  0) ... Mathematics course of the University of Cambridge Past exam of the mathematics course of the University of Cambridge 2024 iii Paper 357 3
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c
Only the transverse coordinates occur in the perturbation, so its tensor components are unchanged by replacing (t,z) with (u,v). The plane gravitational wave in linearized gravity is
hμν​dxμdxν=e−iωu[H+​(dx2−dy2)+2H×​dxdy].
(1)
Every component depends on u alone. The Minkowski wave operator in null coordinates therefore gives
□hμν​=−4∂u​0∂v​hμν​​​+0∂x2​hμν​​​+0∂y2​hμν​​​=0.
(2)
Thus the field satisfies the vacuum Linearized Einstein equations.

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