Yes, but he asked for a "non-circular" proof! The point is that the standard proof of the derivative of ex requires taking that limit. Thus, using the derivative to get that limit is "circular".
However, it is not necessary to use the "standard proof" of the derivative. One thing commonly done in modern Calculus books is to define the logarithm first:
Define
ln(x)= \int_1^x \frac{1}{t} dt
All of the usual properties of the natural logarithm can be derived from that including the fact that it is a one-to-one function from the postive real numbers to the real numbers and so has an inverse function from the real numbers to the positive real numbers. Call that inverse function "exp(x)". Since it is clear from the definition above that the derivative of ln(x) is 1/x, knowing that ln(exp(x))= x tells us that (1/exp(x))(exp(x))'= 1 so the derivative of exp(x) is exp(x) itself. Once we have that, then we can use the L'Hospital as Matthollyw00d says.
(Also, if y= exp(x), then x= ln(y) and, if x\ne 0 1= (1/x)ln(y)= ln(y1/x. Going back to the exp form, exp(1)= y1/x so y= (exp(1))x. That is, the "exp" function, defined as the inverse to ln(x), really is ex where e is defined as exp(1), the number whose natural logarithm is 1.)
But if you want a more direct proof, you have to go back to the definition of "e". e can be defined by e= \lim_{h\to 0}(1+ h)^{1/h}. So we can say that, for h close to 0, we have e= (1+h)^{1/h}, approximately. Then e^h= 1+h so e^h-1 = h and then (e^{h}-1)/h= 1. That is, as I said, approximate. taking the limit, as h goes to 0, makes it exact.