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Thesis-PDF - IAP/TU Wien

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Figure 4.6: A photoreceptor cross section as imaged by TEM. Note the<br />

horizontal striations attributed to the regular layered structure of the photoreceptor<br />

- it consists of about one hundred layers stacked on top of each<br />

other. Image adapted from [87]. Scale bar is 0.1 µm.<br />

triggered almost exclusively by light. In the dark it occurs only about once in a<br />

thousand years.<br />

The isomerization and possible conformational changes of the protein follow a<br />

photocycle and are therefore repeatable. The photocycle leads through a series of<br />

conformational changes from the initial state to an excited state and back again.<br />

Usually also a number of intermediates can be identified. The photocycle of the<br />

chromophore in the photoreceptor of Euglena shows such a cycle including a ground<br />

and an excited state, (the so-called optical bistability is visualized in Fig. 4.7).<br />

As different conformational states possess different fluorescence characteristics, a<br />

photoreceptor whose chromophore proteins are mostly excited differs in emission<br />

from a photoreceptor containing chromophore protein mostly in the ground state<br />

(see Fig. 4.8).<br />

When the excited state is reached, the signal transmission is triggered and the<br />

cellular signal transduction pathway is responsible for amplification of the signal,<br />

signal processing and delivery.<br />

The time it takes for the whole photocycle to complete is only in the order<br />

of microseconds or less. The isomerization alone is one of the fastest processes<br />

ocurring in nature, completing in only about 200 femtoseconds. ([96])<br />

48

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