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Scanning gate microscopy of electron flow from a spin-orbit-coupled quantum point contact Michal P. Nowak, Krzysztof Kolasiński, Bartlomiej Szafran AGH University of Science and Technology, Faculty of Physics and Applied Computer Science, al. Mickiewicza 30, 30-059 Kraków, Poland Scanning gate microscopy (SGM) is a technique that allows for spatial mapping of current flow and charge densities in semiconductor nanostructures. This technique has been used to map electron flow from a constriction introduced in a quantum channel – quantum point contact (QPC). The experiments observed branching of electron flow [1] and angular dependence of the flow that corresponds to the number of conducting modes through the QPC [2]. Moreover the measured conductance maps exhibit fringes that are separated by the half of the Fermi wavelength due to the interference between the coherent waves propagating through the QPC and scattered back from the tip [3]. Currently there is a growing in2600 (a) (b) 2500 terest in spin phenomena in semi2400 conductor media that focuses the 2300 attention to materials that pro2200 vide strong coupling between or2100 bital and spin degrees of free2000 dom – spin-orbit (SO) interac1900 1800 tion – and allow for electrical con-400-300-200-100 0 100 200 300 400 -400-300-200-100 0 100 200 300 400 x [nm] x [nm] trol of the electron spin. In the present work we investigate the Figure 1: Maps of the conductance changes as a function of influence of strong SO coupling the scanning gate tip position obtained on the first (a) and that is present in InGaAs on the (b) second conductance step in the presence of SO interaction. maps of electron flow from QPC Distinct radial interference fringes are present in both maps obtained by the SGM [4]. We find and mode mixing in (b) is visible. that the angular dependence measured on the conductance plateaux [2e2 /h, 4e2 /h, ...] is lost as SO interaction mixes the orbital modes that enter the QPC. On the other hand on the maps gathered for the QPC tuned to the conductance steps the mode mixing is still visible but the distinct radial fringes are preserved despite the presence of the two different Fermi wavelengths that results from lifted by SO interaction spin degeneracy. We explain that the spatial separation of the fringes is determined by the mean value of the two Fermi wavevectors. 0.2 -0.2 -0.4 -0.6 -0.8 ∆G [e2/h] y [nm] -5.6E-017 0 -1 -1.2 [1] M. A. Topinka, B. J. LeRoy, R. M. Westervelt, S. E. J. Shaw, R. Fleischmann, E. J. Heller, K. D. Maranowski and A. C. Gossard, Nature 410, 183 (2001). [2] M. A. Topinka, B. J. LeRoy, S. E. J. Shaw, E. J. Heller, R. M. Westervelt, K. D. Maranowski, and A. C. Gossard, Science 289, 2323 (2000). [3] M. P. Jura, M. A. Topinka, M. Grobis, L. N. Pfeiffer, K. W. West, and D. GoldhaberGordon, Phys. Rev. B 80, 041303(R) (2009). [4] M. P. Nowak, K. Kolasiński, and B. Szafran, arXiv:1401.1707 (2014).