Abstract

Dynamic nuclear polarization (DNP) is well recognized as being important in spintronics and quantum-information processing. DNP gives rise to high nuclear spin polarization that not only can prolong electron-spin lifetime by generating an Overhauser field (OHF), but also has fertilized the idea to explore nuclear spin qubits. In strained quantum-dot structures (QDSs), a nuclear spin is coupled to a strain field via its quadrupole moment. It has been shown that such nuclear quadrupole interaction (NQI) can be used to achieve appreciable DNP and hence electron-spin polarization. Here, we uncover magneto-optical anomalies from a series of laterally arranged $(\mathrm{In},\mathrm{Ga})\mathrm{As}$ QDSs that arise from the NQI and DNP in these nanostructures. We find that the principal axis of NQI in symmetry-lowered QDSs significantly deviates from the growth direction, resulting in tilting of OHF with an angle exceeding 37\ifmmode^\circ\else\textdegree\fi{}. The resulting transverse component of OHF is probed with respect to the crystallographic orientations and its influence on the DNP and ensemble spin dephasing is analyzed. We show that a high-symmetry electronic confinement potential for excitons does not guarantee a high-symmetry NQI for nuclei within the same nano-object, thereby calling for correlated optimization in the symmetry of the electronic confinement potential and that of the nuclear spin bath. Our results underline the role of oblique NQI in electron-spin decoherence and depolarization, which has so far largely been overlooked. This work thus sheds light on design rules for engineering the electronic and spin landscape of QDSs for better performance of DNP desirable for applications in spintronics and quantum computation.

Highlights

  • Dynamic nuclear polarization (DNP) in semiconductor quantum-dot structures (QDSs) has been a subject of intense studies over recent decades [1,2,3,4,5]

  • We show that the field dependence of electronspin polarization significantly deviates from the commonly seen behavior of QDs in both Voigt and Faraday geometries

  • We find that the observed anomalies appear only under the condition when DNP is present and its behavior can be understood by assuming a transverse component of the Overhauser field that is fixed to a certain crystallographic orientation

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Summary

INTRODUCTION

Dynamic nuclear polarization (DNP) in semiconductor quantum-dot structures (QDSs) has been a subject of intense studies over recent decades [1,2,3,4,5]. Gradient at different atomic sites such that the principal axes of NQI for individual nuclei are not necessarily oriented along the growth direction [19,20] Such a spread of nuclear spin interactions is believed to be responsible for the observation of the broadened ODNMR signal and an intermediate stage of electron-nuclear spin relaxation [18]. Since most early studies only involve a single QD with symmetry of C2v or higher such that the anisotropy of NQI is averaged out, a direct probe of its effect on DNP is not accessible so far This is despite the fact that QD arrays, which are at the core of many ideas for solid-state implementations of scalable QIP using electron spins, are typically accompanied by a low-symmetry strain field due to the presence of surrounding interacting QDs where a better understanding and control of the anisotropic NQI and its effect on electron spins are required. Our results call for special attention to be given to the role of anisotropic NQI in asymmetric QDSs and its detrimental effect on spin coherence

EXPERIMENTAL DETAILS
Quantum-dot structures with low symmetries
Effect of a transverse magnetic field on dynamic nuclear polarization
Effect of a longitudinal magnetic field on dynamic nuclear polarization
Oblique nuclear quadrupole interaction and its physical origin
Influence from the lateral arrangement of the QDSs
Angular dependence of B0
Effect on the AEI
CONCLUSION

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