2012/11/30 by Anders Mathias Lunde, Carlos López-Monís, Ioanna A. Vasiliadou +3
Chemistry · Physics and Astronomy · #Atomic physics #Chemistry #Condensed matter physics #Electron #Excited state #Hyperfine structure #Magnetic field #Physics #Physics of Superconductivity and Magnetism #Polarization (electrochemistry) #Quantum and electron transport phenomena #Quantum dot #Quantum mechanics #Semiconductor Quantum Structures and Devices #Singlet state #Spin (aerodynamics) #Spin polarization #Spin-flip #cond-mat.mes-hall #nlin.CD
paper · pdf · doi:10.1103/physrevb.88.035317
published as Phys. Rev. B 88, 035317 (2013) · 26 pages, 17 figures
arxiv created 2013/07/29 · openalex publication_date 2013/07/29 · arxiv updated 2013/07/30 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
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 Tc,TT and Tc,ST for the crossing of the triplet levels and the singlet-triplet level crossings, respectively. We find Tc,TT analytically to be given solely by the HF couplings, whereas Tc,ST depends on various parameters and Tc,ST>Tc,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.