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Nanostructure Science and Technology - World Technology ...

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Appendix D. Site Reports—Japan 287<br />

for Exotic Nano Materials (Knoll). The emphasis is on basic research, rather<br />

than on applications (this was explicitly stated).<br />

RESEARCH AND DEVELOPMENT HIGHLIGHTS<br />

Dr. Aoyagi gave the WTEC team an introduction to some of his team’s<br />

research activities.<br />

Quantum wire growth: they used a technique similar to that developed by<br />

Kapon for the growth of (primarily) GaAs/AlGaAs <strong>and</strong> GaP/AlGaP quantum<br />

wires. The attempt was to improve that process <strong>and</strong> gain better control of the<br />

growth process, with a higher selectivity of incorporation, using the fact that<br />

the growth rates on the (111)A plane is minimal to zero. Measurements<br />

were done in a 40 T magnetic field; the researchers expected to observe a<br />

diamagnetic shift in the luminescence peak under the high field conditions,<br />

<strong>and</strong> obtained 123 µeV/T 2 for the LH transition <strong>and</strong> 210 µeV/T 2 for the HH<br />

transition. These are far larger shifts than expected (110 µeV/T 2 for bulk<br />

<strong>and</strong> 20 µeV/T 2 for 2-D systems). Aoyagi attributes the discrepancy to the<br />

influence of the interaction of the electrons in the wire with the adjacent<br />

impurities.<br />

Si nanostructure formation: these studies began with amorphous silicon<br />

deposited onto Si substrates <strong>and</strong> annealed in a hydrogen or nitrogen ambient.<br />

The result was the formation of Si nanocrystals, ~ 7 nm in size, embedded<br />

within an amorphous matrix. Emission in the blue was observed, with about<br />

10 -5 stated efficiency. Emission at 420 nm <strong>and</strong> 380 nm was observed.<br />

Simulations have been carried out to look at the effects of confinement on<br />

the relative regions of the amorphous <strong>and</strong> crystalline areas (Figure D.8).<br />

amorphous<br />

2.17 nm<br />

crystalline<br />

2.72 nm<br />

Figure D.8. Effects of confinement on the relative regions of the amorphous <strong>and</strong> crystalline<br />

areas.

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