Let {B t } t≥0 be a fractional Brownian motion with Hurst parameter 2 3 < H < 1. We prove that the approximation of the derivative of self-intersection local time, defined aswhere p ε (x) is the heat kernel, satisfies a central limit theorem when renormalized by ε 3 2 − 1 H . We prove as well that for q ≥ 2, the q-th chaotic component of α ε converges in L 2 when 2 3 < H < 3 4 , and satisfies a central limit theorem when renormalized by a multiplicative factor ε 1− 3 4H in the case 3 4 < H < 4q−3 4q−2 .Motivated by spatial integrals with respect to local time, developed by Rogers and Walsh in [10], Rosen introduced in [12] a formal derivative of I(y), in the one-dimensional Brownian case, denoted byThe random variable α := α(0) is called the derivative of the self-intersection local time at zero, and is equal to the limit in L 2 of