Natura semina nobis scientiae dedit, scientiam non dedit. Lucius Annaeus Seneca,Epistulaea, CXX, 4.
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Notes
- 1.
Curves for the intensities of rising and falling signals are approximated by exponential functions \(\exp \left( {t/{\tau _r}} \right) \) and \(\exp \left( { - t/{\tau _f}} \right) \), respectively. Their time constants \({\tau _r}\) and \({\tau _f}\) are defined as the rise and fall times, respectively.
- 2.
If all of the logical functions expressing the relations between \(M\) inputs and \(N\) outputs \(\left( {M,N = 1,2,3,\ldots } \right) \) can be given by the combination of a few basic logical functions, the set of these basic logical functions is called a complete set. All digital operations become possible with a complete set.
- 3.
When the value of the cross-correlation coefficient is smaller than unity at zero time difference between the detections, the quantum state of the photon is called an anti-bunching state.
- 4.
The magnitude of the transferred energy was evaluated by measuring the photocurrent from a photodiode on which these QDs were dispersed [38]. As can be understood from Fig. 5.34a, this optical-to-electrical energy conversion corresponds to the optical frequency down-conversion because the photon energy emitted from the lower energy level\(L_l\) in QD\(_\mathrm{L}\) is lower than that of the incident light, which is resonant with the energy level\(S\) in QDs. In the case of the presently used CdSe QDs, it corresponds to conversion from ultraviolet light to visible light. Thus, as an example, dispersing these QDs on the surface of a solar cell is expected to increase its optical-to-electrical energy conversion efficiency, and additionally, the surface of the solar cell can be protected from ultraviolet radiation exposure [38].
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Ohtsu, M. (2014). Devices Using Dressed Photons. In: Dressed Photons. Nano-Optics and Nanophotonics. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-39569-7_5
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