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Light-emission processes

Certain features of light emission processes have been alluded to in Sect. 4.4.1. Fluorescence is light emission between states of the same multiplicity, whereas phosphorescence refers to emission between states of different multiplicities. The Franck-Condon principle governs the emission processes, as it does the absorption process. Vibrational overlap determines the relative intensities of different subbands. In the upper electronic state, one expects a quick relaxation and, therefore, a thermal population distribution, in the liquid phase and in gases at not too low a pressure. Because of the combination of the Franck-Condon principle and fast vibrational relaxation, the emission spectrum is always red-shifted. Therefore, oscillator strengths obtained from absorption are not too useful in determining the emission intensity. The theoretical radiative lifetime in terms of the Einstein coefficient, r = A-1, or (EA,)-1 if several lower states are involved,... [Pg.91]

George [8] suggests that there may be several light emission processes occurring in the polymer and Lacey and Dudler [17] suggest that the identity of the CL emitting species changes with oxidation time. [Pg.154]

PL observed in the red optical region for Si-NC immersed in a SiC>2 matrix can then be found in the properties of this interface. Our result, concerning the role of both Si-NC and the interface Si-O region with respect to the absorption process, is in close agreement with X-ray absorption fine structure measurements [98] that indicate the presence of an intermediate region between the Si-NC and the SiC>2 matrix, about 1 nm thick, that participates in the light emission process. [Pg.235]

Fluorescence is the light emission process in which a fluorophore, a molecule able to adsorb light, after reaching an excited state releases light (photons) with... [Pg.549]

The probability of direct electron-hole recombination even in direct semiconductors is low and various defects facilitate the light emission processes. In particular... [Pg.89]

The various light-emission process are best described with reference to the Jablonski diagram. The diagram for a simple carbonyl compound is given in Fig. 5. The absorption process leads to the formation of excited singlet states (Sj, 2, etc.). A very rapid depopulation of the upper excited states occurs by internal conversion through vibrational relaxation processes. After deactivation to the first excited singlet state (Si), several procrases are possible for the molecule to reduce... [Pg.201]

This may or may not be a collision process and it may be light emission. Process (16) may indeed be some method of determining the instantaneous concentration of A , such as absorption spectrum, nuclear magnetic resonance, electron spin resonance, or magnetic susceptibility. [Pg.54]

Total energy calculations have been performed to understand the role of oxidation on the structural, electronic and optical properties of Si nanoclusters. Our aim is to explain the peculiar properties of aged porous Si samples, heavily oxidized Si nanoparticles and embedded Si nanocrystals. We have studied two types of structures isolated H-covered clusters, replacing Si-H bonds with various Si-0 bonds and Si nanoclusters embedded in a SiOz matrix. Regarding the isolated clusters we find that the optoelectronic properties depend on the type and the number of Si-O bonds at the cluster surface. For the embedded systems our results show that a close interplay between chemical and structural effects plays a key role in the light emission processes. [Pg.235]

These results agree with x-ray absorption fine structure measurements on Si nanocrystals dispersed in Si02, that indicate an active role in the light emission process of both nanocrystals and interface region [11]. [Pg.238]

State (Es, which can be obtained spectroscopically), the light emission process follows the singlet route S-route (Eqn (3a)) and the system is called the energy-sufficient system. AH can be calculated based on Eqn (5), where TAS is estimated to be about 0.1 eV at 25 °C, E is reversible standard potentials of the redox couples. Most ECL systems based on aromatic compounds are in accordance with this mechanism,such as the ECL of rubrene (AH obtained from the electron-transfer reaction is 2.32 eV, and Eg is 2.30 eV). Another example of an energy sufficient system is the inorganic species Ru(bpy)3 + (AH is ca. 2.6 eV, and Es lies at 2.10eV with = 620 nm). ... [Pg.3]

Forster, E.G., and Wong, P.P., 1980, The dynamics of electrical breakdown in liquid hydrocarbons. V light emission processes, Conf. Rec. of the IEEE Intern. Symp. on Elec. Insul., Boston 222. [Pg.500]

Thus, within half a century after the discovery of quantum electronics, it has become possible to control, both in principle and in practice, both of the fundamental light emission processes, namely, stimulated and spontaneous emission of radiation. [Pg.7]

The requirement for a s-ms spectroscopic "clock implies that suitable photophysical processes must be used. Furthermore, in the case of inherently dilute systems such as suspensions of living cells, sensitivity of detection is a major consideration. In this respect, light emission processes offer significant advantages compared to measurements based upon light absorption. They include delayed luminescence (phosphorescence, fluorescence) involving the long-lived triplet state (7-12) and other two-laser techniques to be described below. [Pg.352]

The radial motion of the bubble was illustrated in Fig. 2. During the main collapse of the bubble, the interior heats up and at the final stages of coUapse, light is emitted. With SBSL, the light emission process may occur each and every acoustic cycle, with a synchronicity better than 1 part per billion for instance, in a 20-kHz sound field (with a period of 50 fis), the light emission can have a jitter of less than 50 ps. [Pg.484]

The STL technique has also been applied to multilayers of CdSe quantum dots. Interestingly, the opposite behavior is found in results on single dots on Au surfaces in that the presence of the quantum dots leads to an increase in the plasmon emission because of a more conducive dielectric environment in the multilayer geometry. It was also observed that the onset of STL in these cases occurred at the band gap of the quantum dots divided by a factor of two, indicating that tunneling to the dots is an important step in the light emission process. It also indicates that better modeling of the potential distribution inside the quantum dot layers is necessary. ... [Pg.291]


See other pages where Light-emission processes is mentioned: [Pg.400]    [Pg.219]    [Pg.13]    [Pg.12]    [Pg.538]    [Pg.192]    [Pg.1190]    [Pg.1190]    [Pg.288]    [Pg.295]    [Pg.94]    [Pg.144]    [Pg.297]    [Pg.655]    [Pg.412]    [Pg.52]    [Pg.703]    [Pg.108]    [Pg.7]    [Pg.83]    [Pg.784]    [Pg.342]    [Pg.655]    [Pg.483]   
See also in sourсe #XX -- [ Pg.400 ]




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