Solid state excitation

Figure 5.10 Normalized solid-state excitation (left) and emission (right) spectra of orange [Au2(dpim)2] " (solid line) and blue [Au2(dpim)2] " (dashed line), at room temperature. Reproduced with permission from [37]. Copyright (2003) American Chemical Society.

Figure 5.13 Solid-state excitation and emission spectra oftriphos...

Consider now a one-dimensional lattice of parameter /. The distance of each atomic jump depends on the rate of de-excitation once the adatom is excited and is translating along the lattice. This de-excitation process can be described by a characteristic life time r in the symmetric random walk, as in many other solid state excitation phenomena. The initial position of the adatom is taken to be the origin, denoted by an index 0. The adatom accomplishes a jump of distance il if it is de-excited within (i — i)l and (i + i)l, where / is the lattice parameter, or the nearest neighbor distance of the one-dimensional lattice, and i is an integer. The probability of reaching a distance il in one jump is given by... 

FIGURE 48. Solid-state excitation (dashed line) and emission spectra (solid line) of 35, recorded at ambient temperature. (Modified from Ref. 155.)... 

FIGURE 56. (a) Normalized solid-state excitation solid line) and emission dotted line) spectra of L49 recorded at 298 K. (b) Normalized excitation solid line) and emission dotted line) spectra of Ge(CH2SPh)4 L49 recorded in CH2C12 at 298 K. 

Figure I. a, emission spectrum of UOa(CH)COO)t 2 HtO in aqueous 10 M soiution and b, emission spectrum of UOt(CH)COO)i 2 HiO in the solid state. Excitation was carried out at 366 nm.

Solid state excitation of electron donor-acceptor complexes of various diaryl-acetylenes and dichlorobenzoquinone in either the acceptor or the 1 2 complex absorption bands induces [2+2] cycloaddition and produces identical mixtures of the quinone methides. Evidence is presented for the participation of an ion-radical pair as the reactive intermediate in both cases. Irradiation of an appropriately substituted o-hydroxybenzyl alcohol precursor generates the corresponding o-quinone methide which is reported to undergo an efficient [4+2] cycloaddition to form the hexahydrocannabinol system. Time-resolved studies confirm the intermediacy of the o-quinone methide and show its lifetime to be > 2 ms. Laser photolysis of 1,2-bis(phenoxymethyl)benzene, l,2-bis[(phenylthio)-methyl]benzene, and l,2-bis[(phenylseleno)methyl]benzene occurs by a two-photon process to produce o-quinodimethane which will cycloadd to various dienophiles including maleic anhydride, dimethyl maleate, dimethyl fumarate, fumaronitrile and dimethyl acetylenedicarboxylate. ... 

Raether, H., 1 5, Solid State Excitations by Electrons, in Springer Tracts in Modem Physics, Vol. 38, ed. G. Hohler (Springer, Berlin). 

Connally R, Dekker P, Piper J (2006) A novel luminescence analyser for europium chelates using solid-state excitation and a gated photomultiplier. Proc SPIE 6371 11133-11142... 

Fig. 2.8 Left Diffiise-reflectance absorption spectra of [Eu(hfa)3(dpb)] line 1), [Eu (hfa)3(dpbp)] line 2), [Eu(hfa)3(dppcz)] line 3), and [Eu(hfa)3(H20)2] dot line 4) in the solid state. The absorption bands at 310 nm are attributed to a k-k transition of the hfa lilgands. The small bands at 465 nm are assigned to the Fo 5D2 transition in the Eu(III) ion. Right Emission spectra of [Eu(hfa)3(dpbp)] , [Eu(hfa)3(dppcz)] , and [Eu(hfa)3(dpb)] in the solid state. Excitation wavelength is 465 nm. The spectra were normalized with respect to the magnetic dipole transition ( Do- Fj)...

Figure 21 Potential energy diagram of the ground and the first excited electronic states of [Ag(CN)32 (eclipsed configuration) as plotted from extended Huckel calculations. The excimer [Ag(CN)32 corresponds to the potential minimum of the excited state. The optical transitions shown are (a) excimer emission, (b) solid state excitation and (c) dilute solution absorption. (Reproduced with permission from Omary MA and Patterson HH (1998) Luminescent homoatomic exciplexes in dicyanoargentate 0) ions doped in alkali halide crystals 1. Exciplex tuning by site-selective excitation. Journal of the American Chemical Society 120 7606-7706.

Both instrument design and capabilities of fluorescence spectroscopy have greatly advanced over the last several decades. Advancements include solid-state excitation sources, integration of fiber optic technology, highly sensitive multichannel detectors, rapid-scan monochromators, sensitive spectral correction techniques, and improved data manipulation software (Christian et al., 1981 Lochmuller and Saavedra, 1986 Cabaniss and Shuman, 1987 Lakowicz, 2006 Hudson et al., 2(X)7). The cumulative effect of these improvements have pushed the limits and expanded the application of fluorescence techniques to numerous scientific research fields. One of the more powerful advancements is the ability to obtain in situ fluorescence measurements of natural waters (Moore, 1994). 

Wokosin D L, Centonze V, White J G, Armstrong D, Robertson G and Ferguson A I 1996 All-solid-state ultrafast lasers facilitate multiphoton excitation fluorescence imaging IEEE J. Sel. Top. Quantum Electron. 21051-65... 

The development of tunable, narrow-bandwidtli dye laser sources in tire early 1970s gave spectroscopists a new tool for selectively exciting small subsets of molecules witliin inhomogeneously broadened ensembles in tire solid state. The teclmique of fluorescence line-narrowing [1, 2 and 3] takes advantage of tire fact tliat relatively rigid chromophoric... 

The reaction path shows how Xe and Clj react with electrons initially to form Xe cations. These react with Clj or Cl- to give electronically excited-state molecules XeCl, which emit light to return to ground-state XeCI. The latter are not stable and immediately dissociate to give xenon and chlorine. In such gas lasers, translational motion of the excited-state XeCl gives rise to some Doppler shifting in the laser light, so the emission line is not as sharp as it is in solid-state lasers. 

The term solid-state laser refers to lasers that use solids as their active medium. However, two kinds of materials are required a host crystal and an impurity dopant. The dopant is selected for its ability to form a population inversion. The Nd YAG laser, for example, uses a small number of neodymium ions as a dopant in the solid YAG (yttrium-aluminum-gar-net) crystal. Solid-state lasers are pumped with an outside source such as a flash lamp, arc lamp, or another laser. This energy is then absorbed by the dopant, raising the atoms to an excited state. Solid-state lasers are sought after because the active medium is relatively easy to handle and store. Also, because the wavelength they produce is within the transmission range of glass, they can be used with fiber optics. 

The proposed model for the so-called sodium-potassium pump should be regarded as a first tentative attempt to stimulate the well-informed specialists in that field to investigate the details, i.e., the exact form of the sodium and potassium current-voltage curves at the inner and outer membrane surfaces to demonstrate the excitability (e.g. N, S or Z shaped) connected with changes in the conductance and ion fluxes with this model. To date, the latter is explained by the theory of Hodgkin and Huxley U1) which does not take into account the possibility of solid-state conduction and the fact that a fraction of Na+ in nerves is complexed as indicated by NMR-studies 124). As shown by Iljuschenko and Mirkin 106), the stationary-state approach also considers electron transfer reactions at semiconductors like those of ionselective membranes. It is hoped that this article may facilitate the translation of concepts from the domain of electrodes in corrosion research to membrane research. 

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