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Diffusion of electrons

The diffusion of electrons plays a major role in the surface treatment of polymers in a gas plasma apparatus. The adhesion of PE tapes increases to a maximum by this treatment at 0.20 to 0.30 A for 20 to 30 s [40]. IR absorption at 1600-1750 cm increases 1.5-fold on discharge treatment owing to the formation of polar >C==0 and —COOH groups, which increase tape adhesion. [Pg.527]

An external magnetic field has also been used to confine the plasma [143]. An arrangement where electromagnets are located under the cathode is known as the controlled plasma magnetron method [144]. The diffusion of electrons to the walls is prevented by the magnetic field between cathode and anode. This results in an increase in electron density, and consequently in a faster decomposition of silane and a higher deposition rate. At a deposition rate of 1 nm/s, device quality material is obtained [144]. In addition, a mesh is located near the anode, and the anode can by biased externally, both in order to confine the plasma and in order to control ion bombardment. [Pg.18]

Figure 18. Schematic illustration of slow charge recombination via lateral diffusion of electrons and holes in the A and the D layers, respectively, in the A-S-D triad monolayer. Radical anions and cations on A and S moieties were created by photoexcitation of the S moieties followed by the charge separation. Figure 18. Schematic illustration of slow charge recombination via lateral diffusion of electrons and holes in the A and the D layers, respectively, in the A-S-D triad monolayer. Radical anions and cations on A and S moieties were created by photoexcitation of the S moieties followed by the charge separation.
For an understanding of photocurrent density and photovoltage (Fig. 3) it is necessary to take into account that in the dark there is diffusion of electrons from the n side to the p side and that this depends among other things on an external voltage V,... [Pg.97]

Within the polymer layer we assume Fickian diffusion of electrons which results in an apparent diffusion of immobile P and Q centers with the same diffusivi-ty De. [Pg.251]

Peisert, A. and Sauli, F. (1984). Drift and diffusion of electrons in gases a compilation. CERN Report 84-08. [Pg.435]

Expansion of the blob. Because of attraction between ions and electrons, expansion of the blob is governed by the law of ambipolar diffusion. As a result out-diffusion of electrons is almost completely suppressed, but the diffusion coefficient of ions is increased by a factor of two. Thus, blob expansion proceeds very slowly and may usually be neglected in the problem of Ps formation. [Pg.131]

This analogy between the motion of electronic carriers and of hydrogen cannot be taken very far because the hydrogen diffusion has some added complications. Dispersive diffusion of electrons or holes occurs with a low density of carriers in a large density of traps and the trapping events are largely independent. Hydrogen diffusion takes... [Pg.206]

Momentum-transfer cross sections are normally determined by the electron swarm technique. A detailed discussion of the drift and diffusion of electrons in gases under the influence of electric and magnetic fields is beyond the scope of this book and only a brief summary will be given. The book by Huxley and Crompton (1974) should be consulted for a full description of the experimental methods and analysis procedures. [Pg.12]

S. Dou, C.R. Masson and P.D. Pacey, Diffusion of electronic defects in calcia-stabilized zirconia from a deorption rate study.. Electrochem. Soc., 137(11) (1990) 3455-3458. [Pg.520]

FIGURE 1.19 Scheme of the anodic process at the TPB for oxygen sensor without consideration of surface diffusion of electrons and holes. DR discharge reaction with an electron transfer Dj, Dj, D3 diffusion of oxygen by TPB interfaces and Ad, Adj reactions of oxygen desorption. [Pg.32]


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See also in sourсe #XX -- [ Pg.16 ]

See also in sourсe #XX -- [ Pg.18 ]




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Electron diffusion

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