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Electronic states more than three electrons

A dye molecule has one or more absorption bands in the visible region of the electromagnetic spectrum (approximately 350-700 nm). After absorbing photons, the electronically excited molecules transfer to a more stable (triplet) state, which eventually emits photons (fluoresces) at a longer wavelength (composing three-level system.) The delay allows an inverted population to build up. Sometimes there are more than three levels. For example, the europium complex (Figure 18.15) has a four-level system. [Pg.132]

After the first theoretical work of Tamm (1932), a series of theoretical papers on surface states were published (for example, Shockley, 1939 Goodwin, 1939 Heine, 1963). However, there has been no experimental evidence of the surface states for more than three decades. In 1966, Swanson and Grouser (1966, 1967) found a substantial deviation of the observed fie Id-emission spectroscopy on W(IOO) and Mo(lOO) from the theoretical prediction based on the Sommerfeld theory of metals. This experimental discovery has motivated a large amount of theoretical and subsequent experimental work in an attempt to explain its nature. After a few years, it became clear that the observed deviation from free-electron behavior of the W and Mo surfaces is an unambiguous exhibition of the surface states, which were predicted some three decades earlier. [Pg.101]

This is the simplest case. It is usually sufficient to have the valence orbitals active, perhaps with added Rydberg type orbitals for studies of excited states. One can normally leave the ns orbital inactive for main group atoms with more than three np electrons. First row transition metals are, however, more demanding. It has been shown that in order to be able to accurately describe the relative correlation effects in atomic states, which differ in the number of 3d electrons, one needs to use two sets of d-orbitals, 3d and 3d where the second set describes the strong radial correlation effects in the 3d shell [29]. Adding the 4s and 4p orbital one is faced with an active space of 14 orbitals. The importance of the second 3d orbital decreases for second and, in particular, for third row transition metals. [Pg.741]

For molecules with more than two vibrational degrees of freedom recourse must be had to a geometrical representation in a space with more than three dimensions. The reasoning is the same as before, but one may expect that the differences with the case of diatomic molecules become still more accentuated. Hence, it is quite comprehensible why discrete electronic band spectra should occur only as an exception for polyatomic molecules (see sections 31 and 46), the excited electronic states being apt to suffer from predissociation over the whole or almost the whole range of their vibration-rotation levels. [Pg.225]

By alloying Pt with transition metals M (M = V, Cr, Co, Ni, Fe, Ti, etc.), the ORR activity can be enhanced remarkably in both phosphoric acid fuel cell (PAFC) and PEMFC [20-22]. The activity enhancement mechanisms have been an open question for more than three decades and ascribed to decreased Pt-ft bond distance [23], enhanced surface roughness [24], increased Pt d-band vacancy [25-27], weakened OH adsorption [28, 29], and downshifted d-band center [30-35]. Nprskov and Mavrikakis et al. combined the stmctural and electronic effects by introducing a d-band model that correlates changes in the energy center of the valence d-band density of states at the surface sites with their ability to form chemisorption bonds. [Pg.516]

For more than three decades, continued improvements in silicon (Si) transistor density, integration, switching speed and energy, and cost per electronic function have driven the 160-billion semiconductor industry, one of the most dynamic industries in the world. These faster and cheaper technologies have led to fundamental changes in the economies of the United States and other countries around the world. The exponential inaease in transistor count that has occurred over the past few decades was accurately predicted by Gordon Moore in 1965. To continue to power the information technology economy, however, the Si industry must remain on the Moore s Law trajectory. [Pg.27]


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See also in sourсe #XX -- [ Pg.784 ]




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More Than

Three-electron

Three-state

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