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041 | _ | _ | |a eng |
082 | _ | _ | |a 530 |
084 | _ | _ | |2 WoS |a Physics, Condensed Matter |
100 | 1 | _ | |0 P:(DE-Juel1)VDB86485 |a Estévez Hernández, S. |b 0 |u FZJ |
245 | _ | _ | |a Spin-orbit coupling and phase coherence in InAs nanowires |
260 | _ | _ | |a College Park, Md. |b APS |c 2010 |
300 | _ | _ | |a 235303 |
336 | 7 | _ | |a Journal Article |0 PUB:(DE-HGF)16 |2 PUB:(DE-HGF) |
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440 | _ | 0 | |0 4919 |a Physical Review B |v 82 |x 1098-0121 |y 23 |
500 | _ | _ | |a We gratefully acknowledge M. Governale (Victoria University of Wellington, New Zealand) and A. Bringer (Institute of Solid State Research, Forschungszentrum Julich) for fruitful discussions. This work was financial support by the French ANR (Quantamonde project) and by DFG through FOR 912. |
520 | _ | _ | |a We investigated the magnetotransport of InAs nanowires grown by selective-area metal-organic vapor phase epitaxy. In the temperature range between 0.5 and 30 K reproducible fluctuations in the conductance upon variation in the magnetic field or the backgate voltage are observed, which are attributed to electron interference effects in small disordered conductors. From the correlation field of the magnetoconductance fluctuations the phase-coherence length l(phi) is determined. At the lowest temperatures l(phi) is found to be at least 300 nm while for temperatures exceeding 2 K a monotonous decrease in l(phi) with temperature is observed. A direct observation of the weak antilocalization effect indicating the presence of spin-orbit coupling is masked by the strong magnetoconductance fluctuations. However, by averaging the magnetoconductance over a range of gate voltages a clear peak in the magnetoconductance due to the weak antilocalization effect was resolved. By comparison of the experimental data to simulations based on a recursive two-dimensional Green's-function approach a spin-orbit scattering length of approximately 70 nm was extracted, indicating the presence of strong spin-orbit coupling. |
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