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Raman Spectroscopy of nanomaterials - institut de chimie et des ...

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ARTICLE IN PRESS+ MODEL14 G. Goua<strong>de</strong>c, Ph. Colomban / Progress in Crystal Growth and Characterization <strong>of</strong> Materialsxx (2007) 1e564035Γ(cm -1 ) = 10.1 + 124.7/d g (nm)30Half Width / cm -125201510single crystal50.0 0.1 0.21/d g (nm -1 )Fig. 6. The half-width at half height <strong>of</strong> the CeO 2 <strong>Raman</strong> band at 466 cm 1 plotted as the inverse <strong>of</strong> the grain size obtainedby X-ray diffraction. Reprinted from Ref. [196, pp. 99e105] with permission from Elsevier.acknowledge the choice <strong>of</strong> a Gaussian form but chose the more confining param<strong>et</strong>er a ¼ 8p 2first proposed by Tiong <strong>et</strong> al. [198], which corresponds to a rigid confinement hypothesisðjCð~k 0 ;~kÞj 2 ¼ 0 for r ¼ L=2Þ [180,183,185,197,200]. A bond polarisability mo<strong>de</strong>lling<strong>of</strong> vibrations in silicon nanocrystals also r<strong>et</strong>urned a value <strong>of</strong> 9.67 for a [201]. As a matter <strong>of</strong>fact, a may be consi<strong>de</strong>red, with L, as an adjustment variable <strong>of</strong> the mo<strong>de</strong>l [184]. Besi<strong>de</strong>s, Lshould not systematically i<strong>de</strong>ntify with the grain size. Phonons can in<strong>de</strong>ed be confined byany ‘‘spatially limiting’’ feature in the grain (twins, stacking faults, inclusions, vacancies,boundaries, pores, <strong>et</strong>c.). L is therefore equal to 2p/Dk, where Dk is the extension <strong>of</strong> BZ domain<strong>of</strong> which the mo<strong>de</strong>s are activated. It is nothing but a coherence length which may correspond toan actual grain size [179,191,202e205] but also to <strong>de</strong>fects/impurities interspacing[185,196,200,206,207] or the size <strong>of</strong> cation-or<strong>de</strong>red domains in incommensurate phases[91], undamaged crystalline domains in ion-implanted GaAs [198], polytypic domains (seeFig. 16 and associated comments) [181,208,209] or clusters in semiconducting alloys[182,183,210] and ferroelectrics [12]. The physical interpr<strong>et</strong>ation <strong>of</strong> L therefore is a key element.For instance, Weber thought it was the grain size in CeO 2 but found an or<strong>de</strong>r <strong>of</strong> magnitu<strong>de</strong>discrepancy with results from electronic microscopy [197]. In fact, Kosacki <strong>et</strong> al. [196]showed L was the distance b<strong>et</strong>ween <strong>de</strong>fects in the oxygen lattice <strong>of</strong> ceria (see Fig. 18b and attachedcomments). Carles <strong>et</strong> al. [180] showed that the meaning <strong>of</strong> L could even change for germaniumparticles <strong>de</strong>pending on their size: L corresponds to the actual size for the bigger grains,but represents the domain size in smaller grains where alloying has taken place.Although Richter <strong>et</strong> al. took ~k 0 at the BZc, their mo<strong>de</strong>l did not preclu<strong>de</strong> it from standingsomewhere else (which many authors have forgotten). Adding this <strong>de</strong>gree <strong>of</strong> freedom to thePlease cite this article in press as: G. Goua<strong>de</strong>c, Ph. Colomban, Prog. Cryst. Growth Charact. Mater. (2007),doi:10.1016/j.pcrysgrow.2007.01.001

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