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Light source, control

In the field of optoelectronics, the development of pure-blue-to-deep-blue-emitting ionic phosphors is an ultimate challenge for full-color displays and white-light sources. Control of the frontier orbital energy level (HOMO-LUMO) is the sole method to achieve better blue phosphorescent iridium complexes by appropriate ligand selection and the introduction of adequate substituents. [Pg.158]

The view of this author is that knowledge of the internal molecular motions, perhaps as outlined in this chapter, is likely to be important in achieving successfiil control, in approaches that make use of coherent light sources and quantum mechanical coherence. However, at this point, opinions on these issues may not be much more than speculation. [Pg.78]

C2.15.2 a right circularly polarized wave is illustrated. As tire wave propagates, Eq sweeps out a circle in tire x-y plane. It is clear tliat, given a well characterized light source, tliere are many attributes we can attempt to control (wavelengtli, polarization, etc.) tire question is how to generate well-characterized light ... [Pg.2857]

Given tire general description of tire electromagnetic field, let us explore the sources available for optoelectronics. The one primary light source for optoelectronic device and system architectures is tire laser. The laser [10] is tire source of choice simply because if we want to control light fields tliey need to be well defined at tire start and tire laser is tire most... [Pg.2857]

Chemiluminescence has been studied extensively (2) for several reasons (/) chemiexcitation relates to fundamental molecular interactions and transformations and its study provides access to basic elements of reaction mechanisms and molecular properties (2) efficient chemiluminescence can provide an emergency or portable light source (J) chemiluminescence provides means to detect and measure trace elements and pollutants for environmental control, or clinically important substances (eg, metaboHtes, specific proteins, cancer markers, hormones, DNA) and (4) classification of the hioluminescent relationship between different organisms defines their biological relationship and pattern of evolution. [Pg.262]

Commercially, the irradiation of the 5,7-diene provitamin to make vitamin D must be performed under conditions that optimize the production of the previtamin while avoiding the development of the unwated isomers. The optimization is achieved by controlling the extent of irradiation, as well as the wavelength of the light source. The best frequency for the irradiation to form previtamin is 295 nm (64—66). The unwanted conversion of previtamin to tachysterol is favored when 254 nm light is used. Sensitized irradiation, eg, with fluorenone, has been used to favor the reverse, triplet-state conversion of tachysterol to previtamin D (73,74). [Pg.131]

The advantages of microreactors, for example, well-defined control of the gas-liquid distributions, also hold for photocatalytic conversions. Furthermore, the distance between the light source and the catalyst is small, with the catalyst immobilized on the walls of the microchannels. It was demonstrated for the photodegradation of 4-chlorophenol in a microreactor that the reaction was truly kinetically controlled, and performed with high efficiency [32]. The latter was explained by the illuminated area, which exceeds conventional reactor types by a factor of 4-400, depending on the reactor type. Even further reduction of the distance between the light source and the catalytically active site might be possible by the use of electroluminescent materials [19]. The benefits of this concept have still to be proven. [Pg.294]

Also, photochemical approach can be used for hydrosilylation on hydrogen-terminated silicon. Light sources with a wavelength at ca. 350 nm can be employed for radical formation under degassed condition [28]. The monolayer packing density can be controlled by the wavelength of the irradiation. The shorter wavelength makes shorter irradiation time and forms more densely packed monolayers. [Pg.456]

Figure 5.15 shows a ray diagram for a light-optical projection microscope. The light source is placed behind a condenser system which collects the light which is diverging from the source and illuminates the specimen. The presence of the variable aperture near to the condenser lens permits control of the area of the specimen which is... [Pg.149]

As CO absorbs radiation in a similar way to C02, a control system could be developed, based on the use of light sources with suitable wavelengths or appropriate filters to measure CO. [Pg.42]


See other pages where Light source, control is mentioned: [Pg.186]    [Pg.186]    [Pg.77]    [Pg.1210]    [Pg.1968]    [Pg.374]    [Pg.37]    [Pg.368]    [Pg.134]    [Pg.418]    [Pg.129]    [Pg.81]    [Pg.743]    [Pg.713]    [Pg.718]    [Pg.718]    [Pg.182]    [Pg.428]    [Pg.727]    [Pg.166]    [Pg.292]    [Pg.241]    [Pg.216]    [Pg.26]    [Pg.36]    [Pg.362]    [Pg.280]    [Pg.416]    [Pg.8]    [Pg.187]    [Pg.195]    [Pg.156]    [Pg.146]    [Pg.82]    [Pg.49]    [Pg.22]    [Pg.132]    [Pg.265]    [Pg.449]    [Pg.260]    [Pg.255]   
See also in sourсe #XX -- [ Pg.274 , Pg.275 ]




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