We assume that the vectors x contains discrete observations from a diffusion
 process $x$ following the Ito stochastic differential equation 
 $$dx(t)= \sigma(t) \ dW(t) + b(t) \ dt,$$ 
 $$d\sigma^2(t)= \gamma(t) \ dZ(t) + a(t) \ dt,$$ 
 where  $W$ and $Z$ are two Brownian motions defined on the filtered probability space 
 $(\Omega, (\mathcal{F}_t)_{t \in [0,T]}, P)$, with correlation $\rho$, while 
 $\sigma, \gamma, b$ and $a$ are random processes, adapted to  $\mathcal{F}_t$.
 
 See the References for further  mathematical details.
 
 The integrated leverage on $[0,T]$ is defined as 
 $$IL_{[0,T]}:=  \langle  x,\sigma^2 \rangle_T =\rho\int_0^T\sigma(s)\gamma(s)ds.$$
 
 
For any positive integer $n$, let $\mathcal{S}_{n}:=\{ 0=t_{0}\leq \cdots
 \leq t_{n}=T  \}$ be the observation times. Moreover, let $\delta_l(x):=
 x(t_{l+1})-x(t_l)$ be the increments of $x$.
 
 The Fourier estimator of the integrated leverage on $[0,T]$ is
 given by 
 $$T c_0(B_{{n},N})={T^2\over {2M+1}} \sum_{|k|\leq M} c_{k}(d\sigma_{n,N})c_{-k}(dx_{n}),$$
 
 where:
 $$c_k(d\sigma_{n,N})= i k \frac{2\pi}{T} c_k(\sigma_{n,N}), \quad   c_k(\sigma_{{n},N})={T\over {2N+1}} \sum_{|s|\leq N} c_{s}(dx_{n})c_{k-s}(dx_{n}),$$
 $$c_k(dx_{n})= {1\over {T}} \sum_{l=0}^{n-1} e^{-{\rm i}\frac{2\pi}{T}kt_l}\delta_{l}(x).$$