The first known implementation of quantum spin Hall effect is the Kane-Mele model, introduced in this paper. It is a doubled copy of the Haldane model (get that one from the previous week's notebooks), with spin up and spin down having next-nearest neighbor hoppings complex conjugate of each other due to spin-orbit coupling.

Implement the Kane-Mele model and add a staggered onsite potential to also be able to create a trivial gap. Calculate the scattering matrix topological invariant of that model.

How would you add disorder and calculate the topological invariant? (Hint: you need to add disorder to the scattering region, and make leads on both sides conducting)

The helical edge states of quantum spin Hall effect survive for some time when a magnetic field is added. Make a Hall bar out of the BHZ model. Can you reproduce the experimental results? What do you see? Are the inversion symmetry breaking terms important?

What about conductance in a two terminal geometry: can you see the crossover from quantum spin Hall regime to quantum Hall regime?

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Discussion entitled 'Quantum spin Hall effect' is available in the online version of the course.

Lingjie Du, Ivan Knez, Gerard Sullivan, Rui-Rui Du

Topological insulators (TIs) are a novel class of materials with nontrivial
surface or edge states. Time-reversal symmetry (TRS) protected TIs are
characterized by the Z2 topological invariant and their helical property
becomes lost in an applied magnetic field. Currently there exist extensive
efforts searching for TIs that are protected by symmetries other than TRS. Here
we show, a topological phase characterized by a spin Chern topological
invariant is realized in an inverted electron-hole bilayer engineered from
indium arsenide-gallium antimonide (InAs/GaSb) semiconductors which retains
robust helical edges under a strong magnetic field. Wide conductance plateaus
of 2e2/h value are observed; they persist to 12T applied in-plane magnetic
field without evidence for transition to a trivial insulator. In a
perpendicular magnetic field up to 8T, there exists no signature to the bulk
gap closing. While the Fermi energy remains inside the bulk gap, the
longitudinal conductance increases from 2e2/h in strong magnetic fields
suggesting a trend towards chiral edge transport. Our findings are first
evidences for a quantum spin Hall (QSH) insulator protected by a spin Chern
invariant. These results demonstrate that InAs/GaSb bilayers are a novel system
for engineering the robust helical edge channels much needed for spintronics
and for creating and manipulating Majorana particles in solid state.

We propose and analyze inter-edge tunneling in a quantum spin Hall corner
junction as a means to probe the helical nature of the edge states. We show
that electron-electron interactions in the one-dimensional helical edge states
result in Luttinger parameters for spin and charge that are intertwined, and
thus rather different than those for a quantum wire with spin rotation
invariance. Consequently, we find that the four-terminal conductance in a
corner junction has a distinctive form that could be used as evidence for the
helical nature of the edge states.

Hint: What happens when edge states meet

Engineering a robust quantum spin Hall state in graphene via adatom
deposition

Conan Weeks, Jun Hu, Jason Alicea, Marcel Franz, Ruqian Wu

The 2007 discovery of quantized conductance in HgTe quantum wells delivered
the field of topological insulators (TIs) its first experimental confirmation.
While many three-dimensional TIs have since been identified, HgTe remains the
only known two-dimensional system in this class. Difficulty fabricating HgTe
quantum wells has, moreover, hampered their widespread use. With the goal of
breaking this logjam we provide a blueprint for stabilizing a robust TI state
in a more readily available two-dimensional material---graphene. Using symmetry
arguments, density functional theory, and tight-binding simulations, we predict
that graphene endowed with certain heavy adatoms realizes a TI with substantial
band gap. For indium and thallium, our most promising adatom candidates, a
modest 6% coverage produces an estimated gap near 80K and 240K, respectively,
which should be detectable in transport or spectroscopic measurements.
Engineering such a robust topological phase in graphene could pave the way for
a new generation of devices for spintronics, ultra-low-dissipation electronics
and quantum information processing.

Hint: A completely different approach

Induced Superconductivity in the Quantum Spin Hall Edge

Sean Hart, Hechen Ren, Timo Wagner, Philipp Leubner, Mathias Mühlbauer, Christoph Brüne, Hartmut Buhmann, Laurens W. Molenkamp, Amir Yacoby

Topological insulators are a newly discovered phase of matter characterized
by a gapped bulk surrounded by novel conducting boundary states. Since their
theoretical discovery, these materials have encouraged intense efforts to study
their properties and capabilities. Among the most striking results of this
activity are proposals to engineer a new variety of superconductor at the
surfaces of topological insulators. These topological superconductors would be
capable of supporting localized Majorana fermions, particles whose braiding
properties have been proposed as the basis of a fault-tolerant quantum
computer. Despite the clear theoretical motivation, a conclusive realization of
topological superconductivity remains an outstanding experimental goal. Here we
present measurements of superconductivity induced in two-dimensional
HgTe/HgCdTe quantum wells, a material which becomes a quantum spin Hall
insulator when the well width exceeds d_{C}=6.3 nm. In wells that are 7.5 nm
wide, we find that supercurrents are confined to the one-dimensional sample
edges as the bulk density is depleted. However, when the well width is
decreased to 4.5 nm the edge supercurrents cannot be distinguished from those
in the bulk. These results provide evidence for superconductivity induced in
the helical edges of the quantum spin Hall effect, a promising step toward the
demonstration of one-dimensional topological superconductivity. Our results
also provide a direct measurement of the widths of these edge channels, which
range from 180 nm to 408 nm.

Hint: Adding superconductors

Helical edge resistance introduced by charge puddles

Jukka I. Väyrynen, Moshe Goldstein, Leonid I. Glazman

We study the influence of electron puddles created by doping of a 2D
topological insulator on its helical edge conductance. A single puddle is
modeled by a quantum dot tunnel-coupled to the helical edge. It may lead to
significant inelastic backscattering within the edge because of the long
electron dwelling time in the dot. We find the resulting correction to the
perfect edge conductance. Generalizing to multiple puddles, we assess the
dependence of the helical edge resistance on temperature and doping level, and
compare it with recent experimental data.

Do you know of another paper that fits into the topics of this week, and you think is good?
Then you can get bonus points by reviewing that paper instead!

Read one of the above papers and see how it is
related to the current topic.

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Discussion entitled 'Quantum spin Hall effect' is available in the online version of the course.