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Introduction to Nanotechnology

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216 OPTICAL AND VIBRATIONAL SPECTROSCOPY<br />

600 500<br />

Wavelength (nrn)<br />

400 300<br />

'A'<br />

I 1<br />

2.0 2.4 2.8 3.2 3.6 4.0 4.4<br />

Energy (eV)<br />

Figure 8.26. Normalized pho<strong>to</strong>luminescence excitation spectra for seven CdSe quantum dots<br />

ranging in size from -1.5 nm (<strong>to</strong>p spectrum) <strong>to</strong> -4.3 nm (bot<strong>to</strong>m spectrum). [From D. J. Norris<br />

and M. G. Bawendi, Phys. Rev. B53, 16338 (1996).]<br />

the surface, and a smaller (2.1-nm) nanoparticle (shell 4) has 63% of its 147 a<strong>to</strong>ms<br />

on the surface. Irregularities of the surface <strong>to</strong>pology can provide electron and hole<br />

traps during optical excitation. The presence of trapped electron-hole pairs bleaches<br />

the exci<strong>to</strong>n absorption, but this absorption recovers when the trapped electron-hole<br />

pairs decay away. We will describe how this complex process has been studied by<br />

time-resolved laser spectroscopy, which furnishes us with details about how the<br />

initial excitation energy passes through various intermediate states before finally<br />

being dissipated.<br />

The surface states of two nanoparticles of CdS with dimensions of 3.4 and<br />

4.3 nm, respectively, were studied by fluorescence spectroscopy. We see from the<br />

resulting spectra presented in Fig. 8.28 that they each exhibit a sharp fluorescence at<br />

435 and 480nm, respectively, arising from exci<strong>to</strong>ns, and a broad fluorescence

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