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A photochemical logic gate is based on the photochemical intersystem crossing and molecular electronic transition between photochemically active molecules, leading to logic gates that can be produced.[1]
[edit] The OR gate electron–photon transfer chain
_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. Input Input [edit] The ‘AND’ gate
_C** Second excited state of molecule C 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 [edit] 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. [edit] See also
[edit] References |
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