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It is seen that all the diffraction peaks for the bare SrTiO3 particles and the composites can be index to the cubic structure of SrTiO3, and no traces of impurity phases are detected.
All the peaks pattern for pure and SrF2 3Dy can be index with the Joint Committee on Powder Diffraction Standards (JCPDS) card number 06-0262 having cubical structure with space group Fm3m (225).
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The d-spacing of 0.321 nm observed in Fig. 4c can be indexed to the (020) planes of Zn5 NO3 2(OH)8·2H2O, but cannot be indexed to ZnO.
The floor can be indexed to inflation.
The cosets of in, that is, the sets, can be indexed in this way (7).
b SAD pattern can be indexed by Ag and some AgCl phases.
All the peaks can be indexed to the orthorhombic Nb2O5 (JCPDS no. 30-0873).
All the samples can be indexed to the tetragonal structure BiOI (JCPDS 10-0445).
All the diffraction peaks can be indexed to the wurtzite structure of ZnO (36 1451).
All diffraction lines can be indexed to the tetragonal rutile phase.
All the peaks can be indexed to a cubic In2O3 (JCPDS 06-0416) with a Space group La3.
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