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The biochemical transducer cascade that leads to the electrical signal has an ability to regulate its own gain, thereby reducing the size of the electrical signal at high photon capture rates.
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These are the photon capture, the bleaching at high light intensities, and a decay reaction which prevents that unused excitons "pile up" in the LHCs.
This suggests that the incident light is not effectively converted into electricity at a higher photon density, which may be attributed to a lower rate of photon capture due to the insufficient QDs loading on TiO2 nanorods.
It was concluded that such structural adaptation ensures efficient photon capture under low-light conditions and prevents photodamage under high-light conditions.
Rods respond to single photons of light with large electrical signals, which means that the electrical responses saturate at low rates of photon capture by the rhodopsin molecules.
Limiting values are τ ≈ 3.5 for low photon fluxes and τ ≈ 6.5 for high photon fluxes.
On the other hand, photosynthetic efficiencies are affected by the efficiency of solar photon capture and the conversion of captured photon to chemically stored energy [ 33].
A large number of light sensitive molecules are needed to increase the probability of photon capture.
Thus, the spectral maxima of cVA photopigments are ideally suited to maximize photon capture within the bird hypothalamus.
Further experiment demonstrates that the optimized pyramid structure enables the integrated luminescent intensity to reach ∼3× increase in a smaller distance of optical transport, which means the advantages in photon capturing efficiency for cells with higher aspect ratio.
For most of their range the rods are signaling single photon captures.
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