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

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Chapter 6<br />

Critical Discussion and Future<br />

Perspective<br />

At first we address the topic <strong>of</strong> diffusive-ballistic crossover which was discussed <strong>in</strong><br />

Sec.4.5.1: The ansatz which was used to show a reduction <strong>of</strong> sp<strong>in</strong> relaxation rate appear<strong>in</strong>g<br />

due to cubic Dresselhaus SOC, was a discretization <strong>of</strong> angles when summ<strong>in</strong>g over momenta<br />

<strong>of</strong> the Cooperon. Although the constra<strong>in</strong>t for the angles reduces the Cooperon eigenvalues<br />

significantly, this ansatz is still based on l<strong>in</strong>ear response. One consequence is that contributions<br />

appear<strong>in</strong>g at low channel number and steam<strong>in</strong>g from edge to edge skipp<strong>in</strong>g orbits, as<br />

shown <strong>in</strong> Ref.[BvH88b], are not <strong>in</strong>cluded. Such orbits can lead to flux cancellation effects,<br />

which e.g. can weaken the magnetic field dependence <strong>of</strong> WL correction to the conductivity.<br />

However, <strong>in</strong> further work we will show the reduction <strong>of</strong> sp<strong>in</strong> relaxation rate dependence on<br />

the number <strong>of</strong> transverse channels <strong>in</strong> the framework <strong>of</strong> a nonperturbative theory based on<br />

the paper by S. Kettemann et al., Ref.[KM02]. In latter work the magnetic phase-shift<strong>in</strong>g<br />

rate 1/τ B has been identified with a correlation function <strong>of</strong> the magnetic vector potential.<br />

In turn this correlation function is related to a term <strong>in</strong> the nonl<strong>in</strong>ear σ-model which appears<br />

due to time-reversal symmetry break<strong>in</strong>g. Thus, <strong>in</strong> case <strong>of</strong> an effective magnetic field due to<br />

SOC, which brakes sp<strong>in</strong> rotation symmetry, the respective term <strong>in</strong> the nonl<strong>in</strong>ear σ-model<br />

has to be identified to yield a nonperturbative expression for the sp<strong>in</strong> relaxation rate 1/τ s .<br />

The last chapter <strong>of</strong> this work stands out from the rest by the fact that the focus is more<br />

on numerical calculations. The code was developed as general as possible by decompos<strong>in</strong>g<br />

all matrix operations <strong>in</strong> connectivity and hopp<strong>in</strong>g matrices <strong>in</strong>clud<strong>in</strong>g magnetic field and<br />

106

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