ito’s lemma is just the chain rule for stochastic integrals.
If X : dXt = μtdt + σtdWt, X0 = x0. With μt = μ(t, Xt) and σt = σ(t, Xt).
And Y : Yt = f(t, Xt) where f is smooth and f : [0, T] × ℝ → ℝ.
Further easy way to remember: $dY_t = \partial_t f dt + \partial_x f d X_t + \frac{1}{2} \frac{\partial ^2f}{\partial x^2} (dX_t)^2$ where (dt)2 = 0 dtdWt = 0 and (dWt)2 = dt
Suppose dXt = μdt + σt(1)dWt(1) + σt(2)dWt(2) and dYt = αdt + βt(1)dWt(1) + βt(2)dWt(2), Where W(1) and W(2) are independant Brownian motions.
Let Zt = f(t, Xt, Yt) for some smooth f.
Then $dZ_t= \partial_t f dt + \partial_x f d X_t + \partial_y f dY_t + \frac{1}{2} \partial_{xx} f(dX_t) ^2 + \frac{1}{2} \partial_{y y } f(d Y_t)^2 + \partial_{xy} f dX_t dY_t$.
Where (dt)2 = dtdWt(i) = dWt(1)dWt(2) = 0 and (dWt(i))2 = dt (think of this as a second order taylor expansion, especially dWt(2).