I am looking to take the partial derivative of an integral with respect to brownian motion. For Simplicity I will make it the same integral as in this post (don't have enough reputation to comment): Partial Derivative of an Integral
My integral is:
$X(t)=\int^t_0 f(s)dB(s)$
My question is about how the the answerers arrived at their answer exactly. I already know that by definition,
$d(X(t))=d(\int^t_0 f(s)dB(s))=f(t)dB(t)$
However I would like to understand how to arrive at this through Leibniz rule. Leibniz' Rule is defined for when the integrator, which is in this case dBs, is the same variable as the secondary variable in f, i.e. f would have to be a function f(t,Bs). But we are given a function f(t,s) (well, actually it is just a function of s), so I don't understand how to apply the rule in this case. Of course if we ignore the dBt, we end up with d(X(t))=f(t)dt, but this is of course wrong. I think this is just a simple change of variables but could someone please help me out?
Thanks, Paul