11The deep-water fold and thrust belt of the southern Niger Delta has prominent thrusts and folds 12 oriented perpendicular to the regional slope that formed as a result of the thin-skinned gravitational 13 collapse of the delta above overpressured shale. The thrust-related folds have grown in the last 12.8 14 Ma and many of the thrusts are still actively growing and influencing the pathways of modern 15 seabed channels. We use 3D seismic reflection data to constrain and analyze the spatial and 16 temporal variation in shortening of four thrusts and folds having seabed relief in a study area of 17 2600 km 2 size in 2200-3800 m water depth. Using these shortening measurements, we have 18 quantified the variation in strain rates through time for both fault-propagation and detachment folds 19 in the area, and we relate this to submarine channel response. The total amount of shortening on 20 the individual structures investigated ranges from 1 to 4 km, giving a time-averaged maximum 21shortening rate of between 90 10 and 350 50 m/Myr (0.1 and 0.4 mm/yr). Fold shortening varies 22 both spatially and temporally: The maximum interval shortening rate occurred between 9.5 Ma and 23 3.7 Ma, and has reduced significantly in the last 3.7 Ma. We suggest that the reduction in the 24Pliocene-Recent fold shortening rate is a response to the slow-down in extension observed in the up-25 dip extensional domain of the Niger Delta gravitational system in the same time interval. In the area 26 dominated by the fault-propagation folds, the channels are able to cross the structures, but the 27 detachment fold is a more significant barrier and has caused a channel to divert for 25 km parallel to 28 the fold axis. The two sets of structures have positive bathymetric expressions, with an associated 29 present day uphill slope of between 1.5 o and 2 o . However, the shorter uphill slopes of the fault-30 propagation folds and increased sediment blanketing allow channels to cross these structures. 31Channels that develop coevally with structural growth and that cross structures, do so in positions of 32 recent strain minima and at interval strain rates that are generally less than -0.02 Ma -1 (-1 x 10 -16 s -1 ). 33 However, the broad detachment fold has caused channel diversion at an even lower strain rate of c. 34 -0.002 Ma -1 (-7 x 10 -17 s -1 ). 35 36