“…[1][2][3][4][5][6][7] For example, ͑1͒ the physical confinement, the interfacial interaction between guest and host, and the reduction of the physical size of the confined particles can lead to ͑a͒ hardness change of materials; 1 ͑b͒ depression of the melting and freezing phase transition temperatures; 2 and ͑c͒ alteration of crystal nucleation and growth characteristics; 3 ͑2͒ the quantum confinement of free electrons in metals and excitons in semiconductors can result in the observation of the surface plasmon resonance ͑SPR͒ and the shifts of the band gap, respectively; 4,5 ͑3͒ dielectric confinement gives rise to surface phonon observation in a wide range of nanophase materials. [1][2][3][4][5][6][7] For example, ͑1͒ the physical confinement, the interfacial interaction between guest and host, and the reduction of the physical size of the confined particles can lead to ͑a͒ hardness change of materials; 1 ͑b͒ depression of the melting and freezing phase transition temperatures; 2 and ͑c͒ alteration of crystal nucleation and growth characteristics; 3 ͑2͒ the quantum confinement of free electrons in metals and excitons in semiconductors can result in the observation of the surface plasmon resonance ͑SPR͒ and the shifts of the band gap, respectively; 4,5 ͑3͒ dielectric confinement gives rise to surface phonon observation in a wide range of nanophase materials.…”