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Introduction to Nanotechnology

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212 OPTICAL AND VIBRATIONAL SPECTROSCOPY<br />

plotted below the experimental one. The peaks of the experimental spectrum are<br />

much broader due <strong>to</strong> the roughness and structural irregularities of the surface. The<br />

theoretical fit provided values for the shear modulus p E 4.0 GPa, the bulk modulus<br />

-3.7 GPa, and Poisson's ratio El .O, consistent with the known value of the graphite<br />

elastic constant C44.<br />

Acoustic phonons of nanoparticles exhibit Brillouin scattering that depends on<br />

particle size, and an example of this is the results shown in Fig. 8.22 for Ag<br />

nanoparticles. Figure 8.22a presents the spectra for particle diameters d = 2.7, 4.1,<br />

and 5.2 nm, and Fig. 8.22b gives the dependence of the wavenumber (cm-') on the<br />

reciprocal of the particle diameter, l/d. The latter figure also plots the theoretically<br />

expected results for <strong>to</strong>rsional and spheroidal vibrational modes with angular<br />

momenta 1= 1,2,3. A related work carried out with nucleated cordierite glass<br />

(Mg2AL&OI8) provided Brillouin scattering peaks with positions that were linear<br />

with the reciprocal of the diameter 1 /d (1 /D on the figure) in the range of particle<br />

diameters from 15 <strong>to</strong> 40nm, as shown in Fig. 8.23. Small-angle neutron scattering<br />

provided the nanoparticle diameters plotted in this figure.<br />

Thus we have seen from Brillouin scattering data that acoustic modes shift <strong>to</strong><br />

higher frequencies with reduced particle size, and we have seen from Raman data<br />

that optical modes shift <strong>to</strong> lower frequencies as the particle size is reduced.<br />

RAMAN SHIFT (cm-1)<br />

(4<br />

AVERAGE DIAMETER d (nm)<br />

0.0 0.1 0.2 0.3 0.4 0.5<br />

l/d (nm-1)<br />

Figure 8.22. Low-frequency Raman shifts in the Brillouin scattering of Ag nanoparticles<br />

embedded in Si02: spectra for particle sizes 2.7, 4.1, and 52nm and (b) peak position as a<br />

function of inverse particle diameter. Theoretical calculations for spheroidal (solid lines) and<br />

<strong>to</strong>rsional (dashed lines) modes with angular momenta I=O, 1 and 2 are indicated. [From<br />

E. Duval, A. Boukenter, and 6. Champagnon, Phys. Rev. Lett. 56, 2052 (1986).]<br />

(b)

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