Symmetry Principles toward Solutions of $\mu$ Problem

We stress that a natural solution of the $\mu$ problem requires two ingredients: a symmetry that would enforce $\mu =0$ as well as the occurence of a small breaking parameter that generates a nonzero $\mu$. It is suggested that both the Peccei-Quinn symmetry and the spontaneously broken $R$ symmetry may be the sources of the needed $\mu$ term in the minimal supersymmetric standard model provided that they are spontaneously broken at a scale ${10}^{10}-{10}^{12}$ GeV. To solve the strong CP problem with a hidden sector confining group, both of these symmetries are needed in superstring models with an anomalous $U(1{)}_A$.