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Itinerant Spin Dynamics in Structures of ... - Jacobs University

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Chapter 5<br />

<strong>Sp<strong>in</strong></strong> Hall Effect<br />

5.1 Introduction<br />

In order to realize sp<strong>in</strong>tronic devices like the sp<strong>in</strong> field effect transistor, one needs<br />

to <strong>in</strong>duce sp<strong>in</strong> polarized electrons <strong>in</strong> low dimensional electron systems (LDES)[icvacFDS04,<br />

DD90]. <strong>Sp<strong>in</strong></strong> polarized electrons can be generated by <strong>in</strong>ject<strong>in</strong>g a current with ferromagnetic<br />

metallic leads <strong>in</strong>to the LDES. However, it has been found that <strong>in</strong> practice the efficiency<br />

<strong>of</strong> such sp<strong>in</strong> <strong>in</strong>jection is poor because <strong>of</strong> the conductivity mismatch. Therefore, recently<br />

there has been a strong effort to f<strong>in</strong>d new ways for generat<strong>in</strong>g polarized sp<strong>in</strong> currents. One<br />

possibility is to use a T-shaped conductor with SOC as proposed by Yamamoto[YDKO06],<br />

whose efficiency is restricted however strongly by impurity scatter<strong>in</strong>g and is therefore only<br />

applicable to narrow wires with few channels. Another approach is to dope the semiconductor<br />

with magnetic impurities: When doped with several percent one speaks <strong>of</strong> dilute<br />

magnetic semiconductors. With transition metal atoms, like Mn, these materials become<br />

ferromagnetic, such as In 1−x Mn x As which has been discovered by Ohno to have a ferromagnetic<br />

phase with a relatively high critical temperature[OMP + 92]. Due to the still relatively<br />

small concentration <strong>of</strong> impurities this system can still be manipulated <strong>in</strong> a wide range <strong>of</strong><br />

carrier density, impurity concentration and acceptor level energy: As these impurities not<br />

only provide sp<strong>in</strong>, but also dope the system with holes, the density <strong>of</strong> charge carriers, and<br />

the Fermi energy can be changed, by chang<strong>in</strong>g their concentration. By choos<strong>in</strong>g different<br />

elements, also the acceptor level energy can be changed. This together with the disorder<br />

provided by these magnetic impurities does change the magnetic properties substantially,<br />

s<strong>in</strong>ce the effective magnetic coupl<strong>in</strong>g between the magnetic ions does depend itself on the<br />

83

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