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Protected Helical Transport in Topological Insulators and Magnetically Doped Quantum Wires

Subject Area Theoretical Condensed Matter Physics
Term from 2016 to 2023
Project identifier Deutsche Forschungsgemeinschaft (DFG) - Project number 285941391
 
Final Report Year 2024

Final Report Abstract

Quantum technologies promise tremendous progress in electronics, computation, and communication. Their fundamental building blocks are protected quantum states which are able to provide error-free operation of quantum devices and their nanoelements. A famous representative of this family is helical states. They were discovered experimentally on edges of so-called topological insulators (TI) – insulators, whose bulk is in a topologically nontrivial state (1). The time-reversal symmetry (TRS) and the non-trivial topology of the TI bulk guarantee helicity (lock-in relation between spin and direction of propagation) of the gapless one-dimensional (1D) edge modes. Helicity prohibits elastic singleparticle backscattering by a spinless potential. Thus, at least in the absence of interactions, the helical modes are not liable to the effects of material imperfections, such as localization. In reality, the protection of the helical states in TI-based samples is not perfectly robust. Understanding possible mechanisms, which can lead to suppression of ballistic helical edge transport in TIs, attracted huge attention. Despite enormous efforts of researchers, a fully consistent theory explaining the suppression of helical transport in TIs in all experimental setups is still absent and remains a hot topic. This calls for a search for alternative platforms where the protected states, including helical ones, can be realized. Emergent helicity can originate in 1D wires with various interactions (2). A challenge is to find a flexible possibility for developing platforms which would allow one to maintain ballistic transport in rather long samples. The project addressed both the above-mentioned aspects of the theory of the helical low-dimensional systems, namely: 1) robustness of the helical protection on the TI edges, and 2) emergent helicity and related protection in magnetically doped wires. The latter systems are described by the seminal model of the Kondo- or Kondo-Heisenberg lattice (3). It includes itinerant electrons interacting with localized magnetic moments, named also Kondo spins. Apart from these main directions, several highly nontrivial phases and phase transitions were found in the magnetically doped TI edges and 1D wires. They encompassed a chiral lattice supersolid, a chiral spin liquid and an unusual transition between Kondo- and indirect exchange-dominated phases

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