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Space-Charge-Limited Discharge

From Child s law (Hclfrich. 1967 . the steady-state trap-free space-charge-limited current is [Pg.93]

Equation (37) is based on a mobility that is field independent. For a mobility with a field dependence given by Eq. (23), Eq. (37) becomes [Pg.93]

In the presence of traps. Eq. (38) must be modified to include the parameter 0, which represents the ratio of the free carrier density to the sum of the free and trapped carrier densities (Zmeskal et al., 1985 Nespurek and Sworakowski, 1990). The currents Je and Js in Eqs. (36) and (38) define two series resistances, Re = V/Je and/i = VUS. The total current. [Pg.93]


The experimental results are usually analyzed from plots of the logarithm of the rate of potential discharge versus the logarithm of time under space-charge-limited conditions (pQ = 1). For these conditions, Eqs. (47) and (49) can be simplified to the following. For / < tt... [Pg.99]

Figure 8 The rate of potential discharge for flash exposures under space-charge-limited conditions for different values of the initial potential VQ. Figure 8 The rate of potential discharge for flash exposures under space-charge-limited conditions for different values of the initial potential VQ.
If the discharge cell has windows of optical quality, it can be placed inside the laser resonator to take advantage of the -fold laser intensity (Sect. 6.2.2). With such an intracavity arrangement. Doppler-free saturation spectroscopy can also be performed with the optogalvanic technique (Sect. 7.2 and [6.101]). An increased sensitivity can be achieved by optogalvanic spectroscopy in thermionic diodes under space-charge-limited conditions (Sect. 6.4.5). Here... [Pg.415]

Figure 6 The photoinduced discharge under emission-limited (dashed line) and space-charge-perturbed conditions (solid lines). Figure 6 The photoinduced discharge under emission-limited (dashed line) and space-charge-perturbed conditions (solid lines).
Note that thermally stimulated current spectroscopy cannot be applied to conductive materials with a resistance smaller than lO Q/m thickness. In addition, the presence of space charges in the sample can produce artefacts. For solid samples the upper temperature limit of measurement is the onset of flow, which presents itself as a large current discharge. This discharge is due to the sample behaving like a battery and draining the charges accumulated at the surfaces. [Pg.150]

Energy is expensive in space It must either be gathered from sunlight from solar panels of limited area or generated from onboard fuel supplies, the exhaustion of which will end the mission. Batteries wear out through repeated charging and discharging... [Pg.1692]


See other pages where Space-Charge-Limited Discharge is mentioned: [Pg.87]    [Pg.92]    [Pg.96]    [Pg.101]    [Pg.104]    [Pg.652]    [Pg.87]    [Pg.92]    [Pg.96]    [Pg.101]    [Pg.104]    [Pg.652]    [Pg.7]    [Pg.94]    [Pg.120]    [Pg.128]    [Pg.7]    [Pg.487]    [Pg.43]    [Pg.292]    [Pg.28]    [Pg.127]    [Pg.58]    [Pg.407]    [Pg.1218]    [Pg.334]    [Pg.56]    [Pg.36]    [Pg.332]    [Pg.41]    [Pg.3564]    [Pg.1924]    [Pg.265]    [Pg.400]    [Pg.1914]    [Pg.234]    [Pg.343]    [Pg.395]    [Pg.175]    [Pg.405]    [Pg.188]    [Pg.43]    [Pg.80]    [Pg.7]   


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Limiting charge

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