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William Angerer - Department of Physics and Astronomy - University ...

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105<br />

current source<br />

carbon glllll8<br />

resl8lcr<br />

r---------I<br />

C2J 1<br />

o<br />

Amp<br />

meler<br />

1<br />

L ________ I<br />

CF77EZ<br />

cpamp<br />

1KC<br />

Figure -1.11: Device to measure temperature <strong>of</strong> GaN during low temperature photoluminescence.<br />

The thick wires represent the four leads (two current, two voltage) to<br />

the carbon-glass resistor.<br />

pIe. In the region near the b<strong>and</strong> gap, ,...., 400 nm, the doped samples exhibit a similar<br />

behavior as the undoped sample. Again this is attributed to donor-acceptor reCOffibination.<br />

C'nIike the spectra from the undoped sample, the doped sample spectra<br />

display a wide feature at ",2.2 eV. In contrast to the DA recombination feature. this<br />

feature is insensitive to temperature. This yellow b<strong>and</strong> luminescence is ubiquitous in<br />

GaN samples. The oscillations in the yellow b<strong>and</strong> are due to a micro cavity formed<br />

by the front <strong>and</strong> back surfaces <strong>of</strong> the GaN film [61].<br />

Reproduced with permission <strong>of</strong> the copyright owner. Further reproduction prohibited without permission.

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