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Photochemistry and Photophysics of Coordination Compounds

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<strong>Photochemistry</strong> <strong>and</strong> <strong>Photophysics</strong> <strong>of</strong> <strong>Coordination</strong> <strong>Compounds</strong>: Ruthenium 189<br />

monolayer <strong>of</strong> dye molecules. The breakthrough in the field was brought about<br />

by the introduction <strong>of</strong> mesoscopic films made <strong>of</strong> sintered nanoparticles <strong>of</strong><br />

a semiconductor metal oxide with a large surface area, which allowed the<br />

adsorption, at monolayer coverage, <strong>of</strong> a much larger number <strong>of</strong> sensitizer<br />

molecules leading to absorbance values, <strong>of</strong> thin films <strong>of</strong> a few microns, well<br />

above unity [407].<br />

Wide-b<strong>and</strong>gap semiconductor materials such as TiO2 show a separation<br />

between the energy levels <strong>of</strong> the valence <strong>and</strong> conduction b<strong>and</strong>s <strong>of</strong> the order<br />

<strong>of</strong> 3 eV, which means that the electron–hole pair needs to be produced by irradiation<br />

with light having a wavelength shorter than 400 nm, i.e., UV light.<br />

In order to use sunlight, mainly visible <strong>and</strong> near-IR, two general approaches<br />

have been developed: doping <strong>and</strong> molecular sensitization. The doping approach<br />

is the preferred choice for conventional photovoltaic devices [405].<br />

Dye-sensitized photelectrochemical cells rely on photosensitization. In this<br />

process, a photoexcited species, the sensitizer (S), is capable <strong>of</strong> injecting an<br />

electron into the conduction b<strong>and</strong> (CB) or a hole into the valence b<strong>and</strong> (VB)<br />

<strong>of</strong> the semiconductor (Fig. 18).<br />

Fig. 18 Schemes for sensitized charge injection in the photoelectrochemical solar cells:<br />

a electron injection, b hole injection<br />

In fact, when the excited-state energy level <strong>of</strong> the sensitizer is higher with<br />

respect to the bottom <strong>of</strong> the conduction b<strong>and</strong>, an electron can be injected<br />

with no thermal activation barrier in the semiconductor, leaving the sensitizer<br />

in its one-electron oxidized form (Fig. 18a). When the excited state<br />

is lower in energy with respect to the top <strong>of</strong> the valence b<strong>and</strong>, an electron<br />

transfer (formally a hole transfer) between the semiconductor <strong>and</strong> the sensitizer<br />

can take place, leaving the molecule in its one-electron reduced form<br />

(Fig. 18b) [408].<br />

The operation <strong>of</strong> a dye-sensitized solar cell is schematized in Fig. 19 [403,<br />

405]. The system is comprised <strong>of</strong> two facing electrodes, a photoanode <strong>and</strong><br />

a counter electrode, with an electrolyte in between. The transparent conductive<br />

photoanode is covered with a thin film (7–10 µm) <strong>of</strong> a mesoporous

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