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Anatomy                                                                     109






























                 FIGURE 2.72 Schematic drawing of two instants mechanism used by Euglena gracilis to orientate. The
                 asterisk indicates the extension of the flagellum and the tumbling of the cell.



                 rotates while swimming, the eyespot comes between the light source and the photoreceptor, thus
                 modulating the light that reaches it, and regulating the steering of the locomotory flagellum. Differ-
                 ent experimental data exist providing evidence that the photoreceptor of Euglena could use either
                 rhodopsin-like proteins or flavoproteins. In 2000 Barsanti et al. isolated the photoreceptors of
                 Euglena in very high yield and performed the purification of a rhodopsin-like protein from this
                 sample. Just recently Iseki et al. (2002) biochemically characterized a new type of blue-light recep-
                 tor flavoprotein, a photoactivated adenyl cyclase, in the photoreceptor organelle of Euglena.
                 Though is not yet certain which is the primary light detecting protein in the photoreceptor, still a
                 model of how Euglena orients itself in a luminous field can be provided.
                     The photoreceptor possesses optical bistability, that is, upon photoexcitation the ground state
                 generates a stable excited state, which can be photochemically driven back to the ground state.
                 Euglena photoreceptor undergoes a very simple photocycle: UV light (365 nm) of the non-fluor-
                 escent ground state leads to the photogeneration of the fluorescent excited state, which in turn is
                 driven back to the ground state by blue light (436 nm). Figure 2.73 shows the absorption spectrum
                 of the ground and excited states of the photoreceptor, together with the absorption spectrum of the
                 eyespot. The latter spectrum clearly overlaps the excited state spectrum of the photoreceptor. The
                 photocycle of the photoreceptor and shading effect of the eyespot are shown in the bottom part of
                 the figure.
                     As the cell rotates while swimming (rotation frequency: 2 Hz, that is, two complete revolutions
                 per second), the photoreceptor experiences periodic shading by the eyespot, which comes between
                 the light source and the organelle. As the absorption spectra of the eyespot and that of the excited
                 state of the photoreceptor are superimposable, the screening effect of the eyespot leads to the inter-
                 ruption of the photocycle, preventing the transition of the excited state of the photoreceptor to its
                 ground state, hence a signal can arise. Cell reorientation is brought about by a selective screening of
                 the absorption window of the excited state of the photoreceptor by the eyespot.
                     During the entire shading period, the photoreceptor is in the excited state, which could generate
                 a photoelectric signal due to the change in dipole orientations between the excited and parent con-
                 formers of the photoreceptive protein. Under the influence of this electric field, a displacement
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