Excitation cascade

G4 Gaussian Cascade Excitation only, Pure-phase 7.8 25.4 [43]... 

FIGURE 17.1 Number of species contributing to the effect of radiation on matter. PI, Primary interaction occurs in very short time CE, the cascade excitation P, the electron cloud plasma, electron relaxation LR, lattice relaxation TD, thermodynamic equilibrium PD, point-defect and DL, dislocations loops. 

Cascadely excited state transition (QE > 10-100) Spatial patterns... 

Fig.9.1. Different schemes for excitation of an alkali atom including (a) single-step, (b) two-step, (c) two-photon, and (d,e) cascade excitation...

If the temperature were raised, more molecules would attain the excited state, but even at 50,000°C there would be only one excited-state atom for every two ground-state atoms, and stimulated emission would not produce a large cascade effect. To reach the excess of stimulated emissions needed to build a large cascade (lasing), the population of excited-state molecules must exceed that of the ground state, preferably at normal ambient temperatures. This situation of an excess of excited-state over ground-state molecules is called a population inversion in order to contrast it with normal ground-state conditions. 

Interaction of an excited-state atom (A ) with a photon stimulates the emission of another photon so that two coherent photons leave the interaction site. Each of these two photons interacts with two other excited-state molecules and stimulates emission of two more photons, giving four photons in ail. A cascade builds, amplifying the first event. Within a few nanoseconds, a laser beam develops. Note that the cascade is unusual in that all of the photons travel coherently in the same direction consequently, very small divergence from parallelism is found in laser beams. 

Though theories have been proposed (32-35) to explain this phenomenon, the mechanism of fluorescence is still not yet fully understood. Jankow and Willis (36) proposed a mechanism which involves a direct excitation of the molecule or an impurity to an excited state, followed by internal conversion and then reversion back to the original state with emission of light. This mechanism can be explained as follows A molecule in the lowest vibrational level of the ground state A is transferred to a certain vibrational level in the excited state D. The molecule tends to cascade into the lowest vibrational level of state D by collisions with other excited molecules. It passes from state D to state C and then to state B by radiationless transi-... 

FIGURE 7.4 Modified Jablonski diagram showing transitions between excited states and the ground state. Radiative processes are shown by straight lines, radiationless processes by wavy lines. IC = internal conversion ISC = intersystem crossing, vc = vibrational cascade hvf = fluorescence hVp = phosphorescence. 

Ionized calcium is an important regulator of a variety of cellular processes, including muscle contraction, stimulus-secretion coupling, the blood clotting cascade, enzyme activity, and membrane excitability. It is also an intracellular messenger of hormone action. 

The exact process(es) by which a2-adrenoceptors blunt release of transmitter from the terminals is still controversial but a reduction in the synthesis of the second messenger, cAMP, contributes to this process. a2-Adrenoceptors are negatively coupled to adenylyl cyclase, through a Pertussis toxin-sensitive Gi-like protein, and so their activation will reduce the cAMP production which is vital for several stages of the chemical cascade that culminates in vesicular exocytosis (see Chapter 4). The reduction in cAMP also indirectly reduces Ca + influx into the terminal and increases K+ conductance, thereby reducing neuronal excitability (reviewed by Starke 1987). Whichever of these releasecontrolling processes predominates is uncertain but it is likely that their relative importance depends on the type (or location) of the neuron. 

Impulse-evoked release of 5-HT, like that of noradrenaline, is subject to fine control by a system of autoreceptors, in particular 5-HTia receptors on the cell bodies of neurons in the Raphe nuclei and 5-HTib/id receptors on their terminals. Because these are all G /o protein-coupled receptors, their activation reduces the synthesis of cAMP so that 5-HTia agonists (or 5-HT itself) decrease neuronal excitability and the firing of Raphe neurons whereas activation of 5-HTib/id receptors seems to disrupt the molecular cascade that links the receptor with transmitter release (see Chapter 4). 

A lifetimes comparison for each excited state (Table 8) shows that they are smaller for the A n state except for v =0. The vibrational decays occur by means of cascade processes. Rotational effects (v =l - 2 i =l - 2) appear to be even more intense than for the corresponding transition bands and in either case these effects disappear for j =4. For... 

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