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The strain of the small ring makes photoexcitation easy.
The semiconductor material, such as silicon, is controlled by photoexcitation.
Effect of photoexcitation of the two retinas on pupil size.
It is produced by the photoexcitation of material, resulting in the production of thermal energy (heat).
A complication that arises from this approach is the reaction of the precursors through alternative, more favorable photoexcitation routes.
But, it differs in that the electrons used for reduction are generated from the photoexcitation of another molecule, called a photosensitizer.
Photoexcitation plays role in photoisomerization.
Photoexcitation leads to the activation of phosphodiesterase and a decrease in cGMP levels.
When an electron is ejected through photoexcitation, the atom it was formerly bound to is left with a net positive charge.
Closely related to the atomic recoil is the electron recoil, (see photoexcitation and photoionization).
The photochromism is due to electrocyclic cleavage of the C-spiro-O bond with photoexcitation.
Exposed to UV, ecamsule undergoes reversible photoisomerization, followed by photoexcitation.
Due to this decay which is called dephasing, coherent effects are observable only for a certain temporal duration after pulsed photoexcitation.
Photoexcitation of the adsorbate which then reacts with the catalyst substrate is classified as a catalyzed photoreaction.
In chemistry, photoisomerization is molecular behavior in which structural change between isomers is caused by photoexcitation.
When placed in the sun, photons of the sunlight can excite electrons on the p-type side of the semiconductor, a process known as photoexcitation.
When the glass is heated to temperatures in the range 550-560 C for several hours the latent image is converted to a visible image through photoexcitation.
During construction, the sponge is filled with an organic dye, typically ruthenium-polypyridine, which injects electrons into the titanium dioxide upon photoexcitation.
Luminescence arises from electronic transitions from an excited state, caused by photoexcitation, to the ground state, resulting in the emission of light.
Monitoring of the absorbance at individual wavelengths after photoexcitation is used to determine the relative concentrations and decay times of each of these photointermediates.
The Ca 2+ -calmodulin effect on the cGMP-gated channel can be incorporated into the current model for photoexcitation and photorecovery.
The mechanism of [2+2] photocyclization is proposed to begin with photoexcitation of the enone to a singlet excited state.
A plasma begins with a rare natural 'background' ionization event of a neutral air molecule, perhaps as the result of photoexcitation or background radiation.
Any photon with more energy than the bandgap can cause photoexcitation, but in this case any energy above and beyond the bandgap energy is lost.
Photoexcitation of the catalyst followed by interaction of the catalyst with a ground state reactant is classified as a sensitized photoreaction.