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Spin waves and the anomalous Hall effect in ferromagnetic (Ga,Mn)As

Spin waves and the anomalous Hall effect in ferromagnetic (Ga,Mn)As

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semiconductors. For this reason, dilute magnetic semiconductors are a majorfocus of sp<strong>in</strong>tronics research. In particular, manganese-doped galliumarsenide, (<strong>Ga</strong>,<strong>Mn</strong>)<strong>As</strong>, is based on gallium arsenide, a direct gap semiconductorthat hit <strong>the</strong> market back <strong>in</strong> <strong>the</strong> 1970s <strong>and</strong> nowadays is commonlyused <strong>in</strong> various electronic <strong>and</strong> optoelectronic devices. Enhanced with magneticproperties, <strong>the</strong> material can realise <strong>the</strong> full potential of sp<strong>in</strong>tronics asit offers <strong>the</strong> <strong>in</strong>tegration of magnetic <strong>and</strong> semiconductor properties, allow<strong>in</strong>g<strong>the</strong> comb<strong>in</strong>ation of data process<strong>in</strong>g <strong>and</strong> storage <strong>in</strong> one chip.However, <strong>the</strong>re is a serious obstacle on <strong>the</strong> way to <strong>the</strong> commercialisationof DMS-based sp<strong>in</strong>tronic devices—<strong>the</strong>ir operation temperature. The magneticorder <strong>in</strong> <strong>the</strong>se materials occurs below <strong>the</strong> Curie temperature, which—despite long years of research effort—does not exceed 200K <strong>in</strong> (<strong>Ga</strong>,<strong>Mn</strong>)<strong>As</strong><strong>and</strong>o<strong>the</strong>rIII–VDMS[28]. Theoretical<strong>and</strong>experimentalquesttowardroomtemperatureferromagnetism <strong>in</strong> <strong>the</strong>se systems is be<strong>in</strong>g pursued by manylaboratories, from different po<strong>in</strong>ts of view <strong>and</strong> often shap<strong>in</strong>g new researchdirections. For its purposes, (<strong>Ga</strong>,<strong>Mn</strong>)<strong>As</strong> is identified as a prototypical DMS<strong>and</strong> used as a test bed for various sp<strong>in</strong>tronic device concepts <strong>and</strong> functionalities.In this context, my dissertation work can be seen as a contributionto this application-oriented struggle. For example, <strong>the</strong> <strong>the</strong>ory of sp<strong>in</strong> <strong>waves</strong>it explores is a basis of <strong>the</strong> mechanism of current-<strong>in</strong>duced doma<strong>in</strong> wall motionemployed <strong>in</strong> racetrack memories, while <strong>the</strong> <strong>anomalous</strong> <strong>Hall</strong> <strong>effect</strong> is animportant tool for prob<strong>in</strong>g sp<strong>in</strong>tronic properties as well as sp<strong>in</strong> generation<strong>and</strong> manipulation <strong>in</strong> DMS. Sceptics have raised doubts whe<strong>the</strong>r we will eversucceed [29]. Even if <strong>the</strong>y are right, research <strong>in</strong> <strong>the</strong> solid-state physics hasvalue of its own as <strong>the</strong> obstacles we encounter are often catalysts for fundamental<strong>in</strong>vestigations. For example, <strong>the</strong> exclusion of magnetic flux froma superconductor was <strong>in</strong>terpreted by Anderson as generation of mass for agauge boson [30]—<strong>the</strong> <strong>effect</strong> popularised by Higgs himself plays a centralrole <strong>in</strong> <strong>the</strong> electroweak <strong>the</strong>ory [31]. Statistical Chern-Simons gauge fields <strong>in</strong>field <strong>the</strong>ory are now commonly used to describe <strong>the</strong> quantum <strong>Hall</strong> <strong>effect</strong> [32],which also started <strong>the</strong> experimental search for a related phenomenon of <strong>the</strong>parity anomaly <strong>in</strong> (2+1)-dimensional electrodynamics <strong>in</strong> solid bodies [33].The significant development of quantum physics over <strong>the</strong> 20th century haveresulted from efforts to <strong>the</strong>oretically describe ensembles of atoms <strong>and</strong> <strong>the</strong>ir<strong>in</strong>teraction, lead<strong>in</strong>g to fundamental <strong>the</strong>oretical <strong>and</strong> numerical methods, like<strong>the</strong> Metropolis algorithm for solv<strong>in</strong>g of <strong>the</strong> many-body Schröd<strong>in</strong>ger equation[34]. To <strong>the</strong>se I added two penn’orth predict<strong>in</strong>g <strong>the</strong> cycloidal sp<strong>in</strong>structure on <strong>the</strong> surface of <strong>the</strong> z<strong>in</strong>cblende DMS structures or formulat<strong>in</strong>gma<strong>the</strong>matical methods, like <strong>the</strong> Löwd<strong>in</strong> variation-perturbational calculusgeneralis<strong>in</strong>g <strong>the</strong> RKKY <strong>the</strong>ory to more complex, realistic energy b<strong>and</strong>s, anexact formula for <strong>the</strong> sum of states of classical sp<strong>in</strong>s, <strong>and</strong> a general methodused for modell<strong>in</strong>g sp<strong>in</strong>-wave excitations (enforc<strong>in</strong>g <strong>the</strong> correct constra<strong>in</strong>ton <strong>the</strong>ir number). The detailed outl<strong>in</strong>e of my work will be provided <strong>in</strong> <strong>the</strong>next chapter.17

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