Remember you have to worry about the temporal inversion by θ now. I think it is easiest to see this by explicitly writing it out as seen on page 87.
(θf)n(x1,...,xn)=fn(θx1,...,θxn)
where θx=(−x0,→x)
now remember by definition we have f(a,R)(x1,...,xn)=f(Rx1+a,...,Rxn+a) and (E1) states that the Euclidean Green function is invariant under SO(4) rotations and translations (as stated in your previous question).
Using your notation we have
(f,ˆTtg)=∑σn+m(Θf∗)n×(ˆTtg)m)=∑σn+m(Θf∗n×(g(−t,1))m)
Notice the minus sign on the t, for that is how they define the map, (ˆTtf)n(x1,...,xn)=fn(x1−t,...,xn−t) where t=(t,→0)
Now explicitly writing out your expression above we have
=∑σn+m(f∗n(θx1,...,θxn)×gm(x1−t,...,xn−t))
We then shift the whole thing by a factor of t, giving us
=∑σn+m(f∗n(θx1+t,...,θxn+t)×gm(x1,...,xn))
=∑σn+m(f∗n(θx1−θt,...,θxn−θt)×gm(x1,...,xn))
=∑σn+m(θf∗n(x1−t,...,xn−t)×gm(x1,...,xn))
=∑σn+m(θ(ˆTtf)∗n(x1,...,xn)×gm(x1,...,xn))
Where in the second line we used the fact that t is a purely temporal vector. This gives the result you are looking for in equation (4.7)