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Optoelectronics with Carbon Nanotubes

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3. Experimental set-up<br />

The optical path for detecting emitted light is schematically described in Figure 3. The<br />

sample was mounted on a sample stage <strong>with</strong> silver paint in an MRR vacuum chamber equipped<br />

<strong>with</strong> four probes. The stage and the probes were electrically connected to an Agilent 4145C<br />

parameter analyzer for applying voltages and measuring currents. The vacuum level in the<br />

chamber was typically 3 to 5 × 10 -6 Torr.<br />

Emitted light from samples was collected by a 10x, 20x or 50x Mitutoyo near-infrared<br />

(NIR) objective lens mounted directly above the sapphire view port on top of the chamber. Light<br />

then goes through a grating prism (GRISM) for spectroscopy, and/or through a linear polarizer<br />

for polarized measurements. The field lens mounted before the camera is used to keep the light<br />

path parallel through the GRISM and the polarizer. All the optical components are at ambient<br />

temperature before the light enters the detector through the outer window. The short-pass filters<br />

and the mercury-cadmium-telluride (MCT) chip inside the detector are cooled by liquid nitrogen.<br />

For low-temperature measurements, a sample stage cooled directly by a small<br />

continuous-flow liquid helium cryostat by MMR Technologies was used in conjunction <strong>with</strong> an<br />

MMR K-20A Programmable Temperature Controller. The cold pad on the stage is equipped<br />

<strong>with</strong> a resistor heater and a temperature sensor. Liquid helium is pushed by the pressure in the<br />

dewar through a specially designed transfer line and into the cryostat. The sample stage can be<br />

cooled to about 20 K, but when the probe needles (connected thermally to ambient temperature<br />

through cables) are touching the sample, the temperature increases quickly and the practical low<br />

temperature measurement limit is close to 90 K.<br />

34

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