Most spaceborne lidar applications use cross-track or conical scanning
to ensure a global coverage of the investigated areas: the return sig
nal of laser pulses shot at an angle with the nadir is biased by a sla
nting effect that induces a temporal spreading of the received signal
as compared with the return signal of a nadir shot. This paper gives t
he basic formulas of the return signal for both a topographic target (
laser range finders) and a diffuse target (atmospheric lidars).