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110   Principles and Methods



                   Ceria before thermal treatment
                          Ceria after thermal treatment





          PDR(r)












                 3      4      5      6     7      8
                               r(Å)
        Figure 4.3 PDF of ceria before and after thermal treatment
        (adapted from Mamontov and Egami, 2000).

        used for studying the nonperiodic structure of matter in noncrystalline
        materials (glasses) [Warren, 1990]. The local structure determined by the
        pair distribution function is the probability of finding an atom at a dis-
        tance r from a reference z atom. The PDF transforms the signal obtained
        in the reciprocal space (wave vector space Q 5 4p sin u/l  with  the scat-
                                                                u
                        l
        tering angle and  wavelength of the incident beam) to the real space
        (interatomic distance space). The spatial resolution is directly linked to
                                              1
        the Q range scanned (greater than 20 Å ). Therefore, to obtain a high
        interatomic size resolution it is necessary to measure data using high
        X-ray energy (> 100 KeV), that is to say, low wavelength (<0.12 Å). The
        high X-ray energy is a strong limitation of this technique, since it requires
        a synchrotron radiation source. The PDF analysis of ceria nanoparticles
        [Mamontov and Egami, 2000] illustrates the interest of such a tool.
          Using neutron diffraction, the authors have shown that the nanoscale
        ceria had Fenkel-type oxygen defects. The defects disappeared after a ther-
        mal treatment as shown in the post-thermal treatment PDF curve, which
        exhibits a higher intensity compared to the ceria before thermal treat-
        ment, for example, a higher number of interatomic distances (Figure 4.3).

          Raman spectroscopy
          Operating principles. Raman spectra result from the scattering of elec-
        tromagnetic radiation by the molecules in solid bulk materials. The
        energy of the incident light beam (usually in the visible region of the
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