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Optoelectronics with Carbon Nanotubes

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Polarized measurements were taken <strong>with</strong> a linear polarizer, i.e. a Glan-Taylor prism in<br />

the infrared, in the parallel section of the beam bath as indicated in figure 3. The polarizer was<br />

rotated normal to the beam path to specific angles <strong>with</strong> respect to the tube orientation. The CNT<br />

orientation was determined by an optical microscope (not shown in figure) using the metal<br />

contacts as reference and comparing them to an SEM image of the device.<br />

In low-temperature experiments, the sample stage was first cooled down as much as<br />

possible (~20 K). For physical stability, the liquid helium transfer line was subsequently<br />

disconnected from the stage in order to mechanically decouple the measurement system from the<br />

environment. The probe needles were then lowered onto the contact pads, allowing the<br />

temperature to rise and then stabilize around 90 K for the first set of measurements. Since in this<br />

set-up, the temperature returns slowly to room temperature over several hours, it was possible to<br />

contact probe needles to the contact pads periodically to take a measurement at a given<br />

temperature. A resistor heater attached to the cold pad of the sample stage was used to raise the<br />

temperature when necessary. Only the sample stage was cooled, while the rest of the optical<br />

path remained at room temperature.<br />

37

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