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Electron thermal

This frequency is a measure of the vibration rate of the electrons relative to the ions which are considered stationary. Eor tme plasma behavior, plasma frequency, COp, must exceed the particle-coUision rate, This plays a central role in the interactions of electromagnetic waves with plasmas. The frequencies of electron plasma waves depend on the plasma frequency and the thermal electron velocity. They propagate in plasmas because the presence of the plasma oscillation at any one point is communicated to nearby regions by the thermal motion. The frequencies of ion plasma waves, also called ion acoustic or plasma sound waves, depend on the electron and ion temperatures as well as on the ion mass. Both electron and ion waves, ie, electrostatic waves, are longitudinal in nature that is, they consist of compressions and rarefactions (areas of lower density, eg, the area between two compression waves) along the direction of motion. [Pg.107]

The emission of thermal electrons is subject to statistical fluctuations (lead shot effect). It is influenced by the current strength, the number of electric charges hberated and the frequency of the radiation [55] (see [40] for further details). [Pg.28]

The first type of polycarbosilane synthesized by using ADMET methodology was a poly[carbo(dimethyl)silane].14c Linear poly(carbosilanes) are an important class of silicon-containing polymers due to their thermal, electronic, and optical properties.41 They are also ceramic precursors to silicon carbide after pyrolysis. ADMET opens up a new route to synthesize poly(carbosilanes), one that avoids many of the limitations found in earlier synthetic methods.41... [Pg.450]

Table 6.12 shows the main characteristics of thermal electron impact ionisation. Electron impact can be used for analysing a wide variety of volatile organic... [Pg.361]

Table 6.12 Main characteristics of thermal electron impact ionisation... Table 6.12 Main characteristics of thermal electron impact ionisation...
Cryoprobe Probe offering greatly enhanced sensitivity by the reduction of thermal electronic noise achieved by maintaining probe electronics at or near liquid helium temperature. [Pg.206]

In a nonattaching gas electron, thermalization occurs via vibrational, rotational, and elastic collisions. In attaching media, competitive scavenging occurs, sometimes accompanied by attachment-detachment equilibrium. In the gas phase, thermalization time is more significant than thermalization distance because of relatively large travel distances, thermalized electrons can be assumed to be homogeneously distributed. The experiments we review can be classified into four categories (1) microwave methods, (2) use of probes, (3) transient conductivity, and (4) recombination luminescence. Further microwave methods can be subdivided into four types (1) cross modulation, (2) resonance frequency shift, (3) absorption, and (4) cavity technique for collision frequency. [Pg.250]

Comments on the thermal nitration of enol silyl ethers with TNM. The strikingly similar color changes that accompany the photochemical and thermal nitration of various enol silyl ethers in Table 2 indicates that the preequilibrium [D, A] complex in equation (15) is common to both processes. Moreover, the formation of the same a-nitroketones from the thermal and photochemical nitrations suggests that intermediates leading to thermal nitration are similar to those derived from photochemical nitration. Accordingly, the differences in the qualitative rates of thermal nitrations are best reconciled on the basis of the donor strengths of various ESEs toward TNM as a weak oxidant in the rate-limiting dissociative thermal electron transfer (kET), as described in Scheme 4.40... [Pg.208]

Importantly, the purple color is completely restored upon recooling the solution. Thus, the thermal electron-transfer equilibrium depicted in equation (35) is completely reversible over multiple cooling/warming cycles. On the other hand, the isolation of the pure cation-radical salt in quantitative yield is readily achieved by in vacuo removal of the gaseous nitric oxide and precipitation of the MA+ BF4 salt with diethyl ether. This methodology has been employed for the isolation of a variety of organic cation radicals from aromatic, olefinic and heteroatom-centered donors.174 However, competitive donor/acceptor complexation complicates the isolation process in some cases.175... [Pg.243]

The D/A complexation in equation (41) is further substantiated by infrared and NMR studies. These observations suggest that an initial thermal electron transfer within the D/A charge-transfer complex generates an ion-radical pair, and a rapid methyl transfer subsequently completes the 1,4-addition (equation 42). [Pg.246]

In a similar vein, the cleavage of the photodimer of anthracene occurs in the dark in the presence of nitrosonium cation to afford the anthracene cation radical as its 7t-dimer via a thermal electron transfer196 (equation 66). [Pg.259]

The efficient formation of the cyclophane suggests that the [DDD, TCNQ] charge-transfer complex is converted to the ion-radical pair via a thermal electron transfer. Subsequent fragmentation of the resulting DDD+ and a homolytic coupling with TCNQ leads then to a zwitterionic intermediate which collapses to the cyclophane within the ion pair, as summarized in Scheme 20. [Pg.268]

Thermal electron transfer. The high degree of charge-transfer character in [ArH, NO+] complexes is consistent with the fact that a variety of electron-rich aromatic donors undergo reversible electron transfer (in the dark) to form the corresponding cation-radical pair239 (equation 86). [Pg.288]

The thermal electron-transfer (ET) via the charge-transfer (CT) equilibrium depicted in equation (86) is established by temperature dependent (UV-vis) spectral studies. For example, an equimolar mixture of hydroquinone ether MA and NO + salt at low temperatures (—78°C) immediately forms the purple [MA, NO+] charge-transfer complex (lmax = 360 nm). However, upon warming the solution an orange-red color of the MA+ cation radical (Amax = 518 nm) develops, and the intensity increases with increasing temperature. Moreover, the identity of liberated NO is confirmed by the quantitative analysis of the head gas with a diagnostic N—O stretching band at 1876 cm -1 in the infrared... [Pg.288]

We now return to the thermal electron transfer reaction in eq 20, in which the rate-limiting activation process has been shown to proceed from the electron donor acceptor complex (23), i.e.,... [Pg.139]


See other pages where Electron thermal is mentioned: [Pg.438]    [Pg.157]    [Pg.1218]    [Pg.53]    [Pg.890]    [Pg.892]    [Pg.893]    [Pg.34]    [Pg.357]    [Pg.147]    [Pg.890]    [Pg.892]    [Pg.893]    [Pg.656]    [Pg.656]    [Pg.657]    [Pg.989]    [Pg.992]    [Pg.357]    [Pg.53]    [Pg.70]    [Pg.251]    [Pg.253]    [Pg.272]    [Pg.274]    [Pg.303]    [Pg.327]    [Pg.167]    [Pg.28]    [Pg.64]    [Pg.398]    [Pg.326]    [Pg.176]    [Pg.101]   
See also in sourсe #XX -- [ Pg.321 ]




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Electrons thermalized

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