This work presents a fully theoretical and self consistent framework for calculating the third-order nonlinear susceptibility 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(including Lorentzian/Voigt broadening) follow from the response expansion. Homogenization yields macroscopic scaling laws that link microscopic descriptors (core radius, shell thickness, dielectric mismatch) to bulk coefficients and. 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.

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