Fig. 3

Photon trajectories (solid curves) drawn from the perspective of an observer in patch C (see Fig. 2). The curve Rγe(t) is the null geodesic for light signals arriving at C at time te from any source at proper distance Rsrc(t) = Rγe(t) (for t < te), whereas Rγ0(t) is the corresponding null geodesic for photons arriving at C at time t0 (>te), though from sources at Rsrc(t) = Rγ0(t) (at any t < t0). The other curves and symbols are defined in the text.
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