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The coexistence of crystalline and liquid phases compels us to re-evaluate the GT equation's treatment of multicomponent compounds within a confined slit geometry. The extended Gibbs-Thomson equation, supplementing the interfacial energy term, further considers the extra free energies originating from compositional fluctuations experienced during the process of freezing or melting. In the initial application of the direct coexisting method (DCM), we determine the melting