Optoelectronics with Carbon Nanotubes
Optoelectronics with Carbon Nanotubes
Optoelectronics with Carbon Nanotubes
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Figure V-2. (a) Schematic illustration and (b) scanning electron microscope image of<br />
CNT film diodes <strong>with</strong> split top gates (TG1 and TG2). The white scale bar on lower<br />
left is 5 μm long.<br />
3. Transport characteristics of the CNT film diode<br />
As we saw in the case of the single-tube CNT diode, good transport behavior is critical<br />
for efficient light emission. This is not surprising since the radiative recombination rate of<br />
excitons in CNTs is much smaller than the non-radiative recombination rate. Here, we discuss<br />
electronic transport of CNT film devices <strong>with</strong> top-split gate to confirm that they do indeed<br />
behave as diodes.<br />
(a)<br />
(b)<br />
The electrical transfer characteristics of two devices <strong>with</strong> different channel lengths (4 μm<br />
and 6 μm) are shown in Figure V-3 (a) and (b). We see that the fundamental requirement for<br />
CNT diode construction, namely the ambipolar behavior upon gate-sweeping, is satisfied in these<br />
devices. The almost symmetric, ambipolar transfer characteristics of the devices indicate that<br />
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