Аннотация:This work presents a fully theoretical and self-consistent framework for calculating the third-order nonlinear susceptibility $\chi ^{(3)}$ of CdSe/ZnS?MOF composite quantum dots. The approach unifies finite-potential quantum confinement, the Liouville-von Neumann density matrix expansion to third order, and effective-medium electrodynamics (Maxwell?Garnett and Bruggeman) within a single Hamiltonian-based model, requiring no empirical fitting. Electron-hole quantized states and dipole matrix elements are obtained under the effective-mass approximation with BenDaniel?Duke boundary conditions; closed analytic forms for $\chi ^{(3)}(\omega)$ (including Lorentzian/Voigt broadening) follow from the response expansion. Homogenization yields macroscopic scaling laws $\chi _{\mathrm{eff}}^{(3)}(\omega)\sim \phi \,|L(\omega)|^{4}\chi ^{(3)}(\omega)$ that link microscopic descriptors (core radius, shell thickness, dielectric mismatch) to bulk coefficients $n_{2}$ and $\beta$. A Kramers?Kronig consistency check confirms causality and analyticity of the computed spectra with small residuals. The formalism provides a predictive, parameter-transparent route to engineer third-order nonlinearity in hybrid quantum materials, clarifying how size and environment govern the magnitude and dispersion of $\chi ^{(3)}$.