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(a) Photoconductive gain as a function of applied bias.
Fig. 6 The gain as a function of laser dyes concentration.
Inset shows the inverter threshold voltage and gain as a function of curvature radius.
Figure 7 Integrated PL, EL and EPL intensities and gain as a function of applied voltage.
The calculated gain as a function of intensity is shown in Fig. 3c.
Figure 5 illustrates the variation of gain as a function of frequency for different values of plasma density.
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