If the position operator is $\mathbf R = (\tilde X,\tilde Y,\tilde Z)$ and the momentum operator is $\mathbf P = (\tilde P_x,\tilde P_y,\tilde P_z)$ with components $$ \tilde X = X\otimes\mathbb I \otimes\mathbb I,\qquad \tilde Y = \mathbb I \otimes Y \otimes\mathbb I,\qquad \tilde Z = \mathbb I \otimes \mathbb I \otimes Z \\ \tilde P_x = P_x\otimes\mathbb I \otimes\mathbb I,\qquad \tilde P_y = \mathbb I \otimes P_y \otimes\mathbb I,\qquad \tilde P_z = \mathbb I \otimes \mathbb I \otimes P_z $$ These operators (with a twidle) are called the extended from the untwidled operators (as in Tannoudji) and they act on the tensor product of the Hilbert spaces $\scr E_x,\ \scr E_y$ and $\scr E_z$, i.e., on $\scr E = \scr E_x \otimes \scr E_y \otimes \scr E_z$
then does that the angular momentum operator $\mathbf L = (L_x,L_y,L_z)$ have components like $$ L_x = \tilde Y\tilde P_z - \tilde Z\tilde P_y = \mathbb I \otimes Y \otimes P_z - \mathbb I \otimes P_y \otimes Z \\ L_y = \tilde Z\tilde P_x - \tilde X \tilde P_z = P_x \otimes \mathbb I \otimes Z - X \otimes \mathbb I \otimes P_z \\ L_Z = \tilde X\tilde P_y - \tilde Y\tilde P_x = X \otimes P_y \otimes \mathbb I - P_x \otimes Y \otimes \mathbb I \\ $$