On the positive axis, and . Taking this limit in the spatial components giveswith evaluated at retarded time . A wave propagating toward the observer along the direction has polarization matrixConsequently the observed gravitational wave polarization amplitudes areThe mode and the orthogonal combination of do not contribute on this symmetry axis. The observer therefore sees a purely plus-polarized wave; a rotation of the transverse axes would represent the same physical polarization as the corresponding spin-two mixture of plus and cross.
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