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Photochemical Logic Gates
Additional recommended knowledge
_A* A* = excited state of molecule A _A _B _C
The OR Gate is based on the activation of molecule A, and thus pass Electron / Photon to molecule C’s excited state orbitals ( C*). The Electron from molecule A inter system crosses to C* via the excited state orbitals of B, eventually utilised as a signal in the C* hυc emission. The ‘OR’ gate uses two inputs of light (Photons) to molecule A in two separate Electron transfer chains, both of which are capable of transferring to C* and thus producing the output of an OR gate. Therefore, if either Electron transfer chain is activated, molecule C’s excitation produces a valid/ output emission. The ‘AND’ gate Excitation A _* * Second excited state of molecule C
_C Above, the energy level diagram illustrating the principle of pump probe spectroscopy –the excitation of an excited state.
The AND gate is produced by the necessity of both A Creating The NOT gate To stop the Electron transfer chain completing, producing output signals, the input of a Photon, hυc2, is used to produce a ‘pump probe spectroscopy’ effect by promoting an Electron in an Electron transfer chain. The fall of the pump probe promoted Electron produces an output that is quenched down an Electron transfer chain. An alternative is similar to the AND gate alternative; an input causes a change in molecule structure breaking the Electron transfer chain by not allowing the smooth energy transfer of Electrons. See also
Categories: Photochemistry | Molecular electronics |
This article is licensed under the GNU Free Documentation License. It uses material from the Wikipedia article "Photochemical_Logic_Gates". A list of authors is available in Wikipedia. |