I disagree. Assuming that the first position is reached as some unspecified clock time ##\Delta t##, the other positions are reached at clock times ##t_n=n\Delta t## and are separated by equal time intervals. This brings to mind Galileo's experiment wherein he rolled a ball down an incline with small bumps separated so that the clicks heard when the ball went over bumps were at equal time intervals.
The spatial separation between events is easy to find. If the object starts from rest at the origin, the space intervals are at positions
##s_1=\frac{1}{2}a(\Delta t)^2##
##s_2=\frac{1}{2}a(2\Delta t)^2=4\frac{1}{2}a(\Delta t)^2=4s_1##
##\dots##
##s_n=\frac{1}{2}a(n\Delta t)^2=n^2 s_1.##
The spatial separation between adjacent events is an oddmultiple of ##s_1##:
##\Delta s_n=s_{n+1}-s_n=\left[(n+1)^2-n^2\right]s_1=(2n+1)s_1.##
Here we have
##\Delta s_1=(0.10-0.05)~\rm{m}=0.05~\rm{m}=1\times(0.05)~\rm{m}.##
##\Delta s_2=(0.25-0.10)~\rm{m}=0.15~\rm{m}=3\times(0.05)~\rm{m}.##
##\Delta s_3=(0.50-0.25)~\rm{m}=0.25~\rm{m}=5\times(0.05)~\rm{m}.##
##\Delta s_4=(0.85-0.50)~\rm{m}=0.35~\rm{m}=7\times(0.05)~\rm{m}.##
It follows that ##s_1=0.05~\rm{m}## which allows us to find the acceleration
$$s_1=\frac{1}{2}a(\Delta t)^2\implies a=\frac{2s_1}{(\Delta t)^2}=\frac{2\times 0.05~\rm{m}}{(0.1~\rm{s})^2}=10~\rm{m}/{s}^2.$$ This result is in agreement with polynomial fits reported above. It is not in agreement with any of the choices offered in the formulation of the question. I also note that this method of analysis does not rely on knowing the initial position but only on the condition that the object start from rest which is given. It was started by
@nasu in post #12, but not completed algebraically.