To explain the anomalous increase in the permittivity of monoclinic Rb2ZnI4 at low temperatures, the dielectric susceptibilities of modulated structures are calculated. A quantum Ising model is reduced from a lattice Hamiltonian by the mean field approximation and two-quantum-level approximation. The susceptibilities of modulated phases remain to be finite values at zero temperature as in the uniform ferroelectric phase, if the quantum effect works. Furthermore, the susceptibilities of the incommensurate and high-order commensurate phases increase at low temperatures. Since the ferroelectric phase can be realized with accompanying strong discontinuity, such an increase is different from the phenomenon during the lock-in transition. The phase diagram and the temperature dependence of susceptibility are calculated. With the selection of a proper set of parameters, the theoretical results agree qualitatively with experimental reports of (Rb1-xKx)2ZnI4.