2,618 research outputs found
Helical nuclear spin order in two-subband quantum wires
In quantum wires, the hyperfine coupling between conduction electrons and
nuclear spins can lead to a (partial) ordering of both of them at low
temperatures. By an interaction-enhanced mechanism, the nuclear spin order,
caused by RKKY exchange, acts back onto the electrons and gaps out part of
their spectrum. In wires with two subbands characterized by distinct Fermi
momenta kF1 and kF2, the nuclear spins form a superposition of two helices with
pitches {\pi}/kF1 and {\pi}/kF2, thus exhibiting a beating pattern. This order
results in a reduction of the electronic conductance in two steps upon lowering
the temperature.Comment: 20 pages, 9 figures. Version as published with minor modification as
compared to v1 (some short discussions in the introduction and summary, and
one figure, have been added
Strongly Interacting Holes in Ge/Si Nanowires
We consider holes confined to Ge/Si core/shell nanowires subject to strong
Rashba spin-orbit interaction and screened Coulomb interaction. Such wires can,
for instance, serve as host systems for Majorana bound states. Starting from a
microscopic model, we find that the Coulomb interaction strongly influences the
properties of experimentally realistic wires. To show this, a Luttinger liquid
description is derived based on a renormalization group analysis. This
description in turn allows to calculate the scaling exponents of various
correlation functions as a function of the microscopic system parameters. It
furthermore permits to investigate the effect of Coulomb interaction on a small
magnetic field, which opens a strongly anisotropic partial gap
Quantum criticality with multiple dynamics
Quantum critical systems with multiple dynamics possess not only one but
several time scales, tau_i ~ xi^(z_i), which diverge with the correlation
length xi. We investigate how scaling predictions are modified for the simplest
case of multiple dynamics characterized by two dynamical critical exponents,
z_> and z_<. We argue that one should distinguish the case of coupled and
decoupled multiple dynamic scaling depending on whether there exists a scaling
exponent which depends on both z_i or not. As an example, we study generalized
Phi^4-theories with multiple dynamics below their upper critical dimension,
d+z_<<4. We identify under which condition coupled scaling is generated. In
this case the interaction of quantum and classical fluctuations leads to an
emergent dynamical exponent, z_e=z_>/(nu (z_>-z_<)+1).Comment: 8 pages including supplementary material. Minor changes as compared
to the previous versio
Renormalization of anticrossings in interacting quantum wires with Rashba and Dresselhaus spin-orbit couplings
We discuss how electron-electron interactions renormalize the spin-orbit
induced anticrossings between different subbands in ballistic quantum wires.
Depending on the ratio of spin-orbit coupling and subband spacing,
electron-electron interactions can either increase or decrease anticrossing
gaps. When the anticrossings are closing due to a special combination of Rashba
and Dresselhaus spin-orbit couplings, their gap approaches zero as an
interaction dependent power law of the spin-orbit couplings, which is a
consequence of Luttinger liquid physics. Monitoring the closing of the
anticrossings allows to directly measure the related renormalization group
scaling dimension in an experiment. If a magnetic field is applied parallel to
the spin-orbit coupling direction, the anticrossings experience different
renormalizations. Since this difference is entirely rooted in electron-electron
interactions, unequally large anticrossings also serve as a direct signature of
Luttinger liquid physics. Electron-electron interactions furthermore increase
the sensitivity of conductance measurements to the presence of anticrossing.Comment: 12 Pages, 10 figures, final versio
Quantum Critical Matter: Quantum Phase Transitions with Multiple Dynamics and Weyl Superconductors
In this PhD thesis, the physics of quantum critical matter and exotic quantum state close to quantum phase transitions is investigated. We will focus on three different examples that highlight some of the interesting phenomena related to quantum phase transitions. Firstly, we discuss the physics of quantum phase transitions in quantum wires as a function of an external gate voltage when new subbands are activated. We find that at these transitions, strong correlations lead to the formation of an impenetrable gas of polarons, and identify criteria for possible instabilities in the spin- and charge sectors of the model. Our analysis is based on the combination of exact resummations, renormalization group techniques and Luttinger liquid approaches.
Secondly, we turn to the physics of multiple divergent time scales close to a quantum critical point. Using an appropriately generalized renormalization group approach, we identify that the presence of multiple dynamics at a quantum phase transition can lead to the emergence of new critical scaling exponents and thus to the breakdown of the ususal scaling schemes. We calculate the critical behavior of various thermodynamic properties and detail how unusual physics can arise. It is hoped that these results might be helpful for the interpretation of experimental scaling puzzles close to quantum critical points.
Thirdly, we turn to the physics of topological transitions, and more precisely the physics of Weyl superconductors. The latter are the superconducting variant of the topologically non-trivial Weyl semimetals, and emerge at the quantum phase transition between a topological superconductor and a normal insulator upon perturbing the transition with a time reversal symmetry breaking perturbation, such as magnetism. We characterize the topological properties of Weyl superconductors and establish a topological phase diagram for a particular realization in heterostructures. We discuss the physics of vortices in Weyl superconductors, and establish under which conditions they can trap zero energy Majorana modes. Our disucssion ends with some remarks on possible experimental signatures
Helical nuclear spin order in a strip of stripes in the Quantum Hall regime
We investigate nuclear spin effects in a two-dimensional electron gas in the
quantum Hall regime modeled by a weakly coupled array of interacting quantum
wires. We show that the presence of hyperfine interaction between electron and
nuclear spins in such wires can induce a phase transition, ordering electrons
and nuclear spins into a helix in each wire. Electron-electron interaction
effects, pronounced within the one-dimensional stripes, boost the transition
temperature up to tens to hundreds of millikelvins in GaAs. We predict specific
experimental signatures of the existence of nuclear spin order, for instance
for the resistivity of the system at transitions between different quantum Hall
plateaus.Comment: 16+ pages, 6 figures, updated reference
Low-energy properties of fractional helical Luttinger liquids
We investigate the low-energy properties of (quasi) helical and fractional
helical Luttinger liquids. In particular, we calculate the Drude peak of the
optical conductivity, the density of states, as well as charge transport
properties of the interacting system with and without attached Fermi liquid
leads at small and large (compared to the gap) frequencies. For fractional
wires, we find that the low energy tunneling density of states vanishes. The
conductance of a fractional helical Luttinger liquid is non-integer. It is
independent of the Luttinger parameters in the wire, despite the intricate
mixing of charge and spin degrees of freedom, and only depends on the relative
locking of charge and spin degrees of freedom.Comment: 9 pages, 4 figures. Final versio
Impurity Induced Quantum Phase Transitions and Magnetic Order in Conventional Superconductors: Competition between Bound and Quasiparticle states
We theoretically study bound states generated by magnetic impurities within
conventional -wave superconductors, both analytically and numerically. In
determining the effect of the hybridization of two such bound states on the
energy spectrum as a function of magnetic exchange coupling, relative angle of
magnetization, and distance between impurities, we find that quantum phase
transitions can be modulated by each of these parameters. Accompanying such
transitions, there is a change in the preferred spin configuration of the
impurities. Although the interaction between the impurity spins is
overwhelmingly dominated by the quasiparticle contribution, the ground state of
the system is determined by the bound state energies. Self-consistently
calculating the superconducting order parameter, we find a discontinuity when
the system undergoes a quantum phase transition as indicated by the bound state
energies.Comment: 8 pages, 7 figure
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