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CHEM01200604009 Sreejith Kaniyankandy - Homi Bhabha ...

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91<br />

which is also neutral; therefore, we do not expect much change due to surface modifier.<br />

Therefore the changes observed in the absorption are due to the interaction between the TiO 2<br />

and alizarin molecule only.<br />

3.3.3. Femtosecond Transient Absorption Studies<br />

A (m O.D.)<br />

5<br />

4<br />

3<br />

2<br />

1<br />

0<br />

A<br />

500 600 700 800<br />

Wavelength (nm)<br />

0.1ps<br />

0.2 ps<br />

0.4 ps<br />

A (m O.D.)<br />

3<br />

2<br />

1<br />

0<br />

B<br />

500 600 700 800<br />

Wavelength (nm)<br />

1 ps<br />

2 ps<br />

4 ps<br />

A (m O.D.)<br />

5<br />

4<br />

3<br />

2<br />

1<br />

0<br />

C<br />

500 600 700 800<br />

Wavelength (nm)<br />

10 ps<br />

50 ps<br />

100 ps<br />

Figure 3.4: Transient absorption spectra of B- TiO 2 -Alizarin in toluene after 400nm excitation.<br />

To gain information of the interfacial electron transfer dynamics between alizarin and<br />

TiO 2 we have carried out femtosecond transient absorption study by exciting the samples at<br />

400 nm and following the dynamics using probe light in the wavelength range 470-900 nm.<br />

We have shown the time resolved transient absorption spectra in Figure 3.4. The spectrum<br />

shows a prominent peak in the region 500-600nm, which can be assigned to the cation radical<br />

of alizarin [3.3]. Also the spectrum shows a broad featureless band in the wavelength range<br />

700-900nm which can be attributed to injected electron into the conduction band of TiO 2 .

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