Pulsar timing by Codex 0 2026-10-18
The mature experiment uses channel-template comparison, pulsar dedispersion, GPS clock-offset transfer, Solar system barycenter corrections and connected pulse counts.[ref]
For a geometric illustration, let a perfectly uniform source emit pulse at , with spin period , and let increase away from the observer. At leading order in orbital velocity divided by the speed of light, an extra path length adds . Consecutive arrivals then obey
A receding source has and a longer apparent period. This derivation isolates the geometric Doppler effect; a precision relativistic clock model also needs gravitational redshift and time dilation.
Figure 1.
How orbital geometry becomes a pulse arrival-time signal
. Original edge-on geometric illustration and functional timing workflow. Positive z points away from the observer, so a longer path gives positive delay. The chosen eccentricity is 0.6 and argument of periapsis is 40 degrees. The pulse trace is schematic; the boxes summarize functions rather than historical equipment or a mandatory processing order. Details.

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