Thesis-PDF - IAP/TU Wien
Thesis-PDF - IAP/TU Wien
Thesis-PDF - IAP/TU Wien
Create successful ePaper yourself
Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.
Figure 4.7: Scheme of the photoreceptor photocycle (intermediate states<br />
omitted). Upon absorption of light with a wavelength of around 365 nm the<br />
rhodopsin-like protein changes into the excited state, then upon a second<br />
absorption at a wavelength of around 436 nm it falls back again into the<br />
ground state. This last step from the excited state to the ground state is<br />
almost exclusively triggered by light. It occurs only once in a thousand years<br />
through thermal deactivation at ambient temperature.<br />
Sensitivity<br />
For detecting the direction of the light of a specific range a photoreceptor demands<br />
a high packing density of chromophore molecules organized in a lattice<br />
structure, with high absorption cross section (high absorption probability) of the<br />
chromophore and very low dark noise 10 . For transmitting the detected signal a<br />
photoreceptor must generate an electrical potential difference, or an electrical current.<br />
This is exactly what Euglena’s photoreceptor is designed for.<br />
One of the most investigated photoreception systems is that of Chlamydomonas.<br />
It consist of a patch of rhodopsin-like proteins in the plasma membrane.<br />
The packing density of these molecules appears to be about 20 − 30, 000/µ 2 m of<br />
membrane, with a molar absorption coefficient of 40 − 60, 000 M −1 ∗ cm −1 and a<br />
dark noise of almost zero. The number of embedded molecules per µ 2 m of membrane,<br />
the absorption, the absorption cross section, and the dark noise are at the<br />
best of theoretical limits. Nevertheless, the fraction of photons absorbed from a<br />
single layer of these molecules is less than 0.05%.<br />
An estimate of how many photons this simplest but real photoreceptive system<br />
can absorb is effectuated here. On a sunny day about 10 18 photons ∗m −2 ∗ s −1 per<br />
nanometer wavelength are incident. On a cloudy day this lowers to 10 17 photons<br />
∗m −2 ∗ s −1 per nanometer wavelength. Through absorption of the water column<br />
this number is lowered to 10 17 and 10 16 respectively. Thus a photoreceptor of a<br />
cross section of about 1µm 2 can catch at most 10 5 photons, 10 7 in its 100 nm<br />
absorption band. Since only about 0.05% of these are effectively catched by the<br />
protein monolayer, the maximum number lowers to 5 ∗ 10 3 . Now during revolving<br />
motion of the algae it is illuminated for about 400 ms and shaded by the stigma<br />
10 Dark noise is inherent to such a receptor and independent of light level. It arises from the<br />
random thermal motion of the molecules.<br />
49