Temperature-dependent dynamical nuclear polarization bistabilities in double quantum dots in the spin-blockade regime

TL;DR

This paper investigates how temperature influences dynamical nuclear polarization bistabilities in double quantum dots under spin-blockade, revealing a transition temperature below which hysteretic current behavior emerges due to nuclear-electron spin interactions.

Contribution

It introduces a detailed analysis of temperature-dependent DNP bistabilities, identifying transition temperatures and developing simplified models for different energy level crossings.

Findings

Bistability in DNP occurs below a specific transition temperature.

Transition temperatures depend on hyperfine couplings and other parameters.

Hysteretic leakage current appears near certain magnetic field crossings.

Abstract

The interplay of dynamical nuclear polarization (DNP) and leakage current through a double quantum dot in the spin-blockade regime is analyzed. A finite DNP is built up due to a competition between hyperfine (HF) spin-flip transitions and another inelastic escape mechanism from the triplets, which block transport. We focus on the temperature dependence of the DNP for zero energy-detuning (i.e. equal electrostatic energy of one electron in each dot and a singlet in the right dot). Our main result is the existence of a transition temperature, below which the DNP is bistable, so a hysteretic leakage current versus external magnetic field B appears. This is studied in two cases: (i) Close to the crossing of the three triplet energy levels near B=0, where spin-blockade is lifted due to the inhomogeneity of the effective magnetic field from the nuclei. (ii) At higher B-fields, where the two spin-polarized triplets simultaneously cross two different singlet energy levels. We develop simplified models leading to different transition temperatures T_TT and T_ST for the crossing of the triplet levels and the singlet-triplet level crossings, respectively. We find T_TT analytically to be given solely by the HF couplings, whereas T_ST depends on various parameters and T_ST>T_TT. The key idea behind the existence of the transition temperatures at zero energy-detuning is the suppression of energy absorption compared to emission in the inelastic HF transitions. Finally, by comparing the rate equation results with Monte Carlo simulations, we discuss the importance of having both HF interaction and another escape mechanism from the triplets to induce a finite DNP.