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Insulators, charging

Clearly additional layers may be used to accomplish other benefits, tailoring the energy profiles and mobilities across the entire organic stack. Splitting the transport layer(s) into two separate layers permits the optimization of injection into the layer nearest the electrode (sometimes called the injection layer), and transport in the farther layer [101]. Layers of insulator (charge confinement layers) have also been used in an attempt to control the motion of the charges and ensure recombination in the desired region [102]. [Pg.226]

The switching or memory phenomena induced by electric field application or photo irradiation have been studied on Mott insulators, charge ordered insulators, and N-I transition systems and were found to be fast phase transitions in general. For the former two systems, the phase transitions caused a pronounced change in reflectance and conductivity from insulating to metallic features. The third system also exhibited a change in conductivity and dielectric response connected with the transports of solitons and/or domain walls, dynamic dimerization, and... [Pg.86]

Ion Bombardment Conditions. A base pressure of 10 9 Torr is maintained in this chamber the noble gas pressure (He, Xe) rises to about 10"7 Torr during the ion bombardment. The ion beam is rastered on (1.5 x 1.5) mm2 areas at normal incidence 4He-2 keV ions are used for the ISS analysis when Xe-4 keV ions are used for SIMS. The incident ion current is measured with the aid of a moveable Faraday cup. Since the investigated samples are electrical insulators, charge neutralization is performed with low energy electrons ( 10 eV) emitted from a heated W filament. [Pg.211]

Fig. 7.2 Photographs of Lichtenberg figures produced by sparks to an insulator charged (a) positive and (b) negative. (Courtesy of Mile H. Bertein.)... Fig. 7.2 Photographs of Lichtenberg figures produced by sparks to an insulator charged (a) positive and (b) negative. (Courtesy of Mile H. Bertein.)...
The curves of Figure 5, taken from an experiment by Pollock [60] illustrate the two mechanisms of charging. RDX, an insulator, charges by contact, the graphite-coated propellant charges by induction, and lead azide charges by both mechanisms. At this point a word of caution may be in order. At sufficiently... [Pg.97]

Polymers being in general insulators, charging effect under electron bombardment is conoolled with the use of a flood gun alternatively, one can ny to cast a very thin polymer film (thickness of about 10 nm) on a conducting substrate to ciicumvent this problem. [Pg.160]

Other related electron-beam-readout imaging devices with semi-insulating charge-storage surfaces or diode-array retinas are operationally similar to scanned photoemissive sensors and compete with or outperform them in some applications, but these non photoemissive devices are not treated in this chapter [5.6].)... [Pg.149]

Figure 9. The effect of surface-state density and insulator charge on conversion efficiency (Ref 23)... Figure 9. The effect of surface-state density and insulator charge on conversion efficiency (Ref 23)...
Figure 10. Effect of fixed oxide/insulator charge on the effective junction space-charge region (a) flat-band condition (b) positive fixed charge causes inversion of the p side and formation of a n-type surface channel (c) negative fixed charge causes accumulation of the p side and a narrow field induced junction at the surface (d) larger amount of negative fixed charge causes inversion of the n side and formation of a p-type surface channel. (With permission of Academic Press.)... Figure 10. Effect of fixed oxide/insulator charge on the effective junction space-charge region (a) flat-band condition (b) positive fixed charge causes inversion of the p side and formation of a n-type surface channel (c) negative fixed charge causes accumulation of the p side and a narrow field induced junction at the surface (d) larger amount of negative fixed charge causes inversion of the n side and formation of a p-type surface channel. (With permission of Academic Press.)...
The electrical conductivity of the polymer pure and the nanocomposites was measured by four-point probe method [123]. The conductivity of the PAni/HCl was 83 S cm and for the nanocomposites was about 62 S cm. It has been noted the addition of clay directed to a Utde reduction in conductivity, unsurprisingly, owing to the presence of insulating charges between the polymer chains. However, the synthesized nanocomposite materials stiU present an excellent electrical conductivity. [Pg.159]

The method can be directly applied to metal and semiconductor subsfrates however, in the case of insulators charging problems can make measurements very difficult. Nevertheless, it has been possible to overcome this limitation in many cases and high-quality EEL-specfra have been obtained, e.g. for hydrogen adlayers on diamond C(lll) [94AND]. [Pg.39]


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See also in sourсe #XX -- [ Pg.62 , Pg.66 ]




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Charge transfer, insulating character

Charge-transfer insulators

Charging of Insulating Samples

Contact charging metal-insulator

Insulator-semiconductor interface charge trapping

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