We propose a physical model based on disordered (a hole punched inside a
material) monolayer transition metal dichalcogenides (TMDs) to demonstrate a
large-gap quantum valley Hall insulator. We find an emergence of bound states
lying inside the bulk gap of the TMDs. They are strongly affected by
spin-valley coupling, rest- and kinetic- mass terms and the hole size. In
addition, in the whole range of the hole size, at least two in-gap bound states
with opposite angular momentum, circulating around the edge of the hole, exist.
Their topological insulator (TI) feature is analyzed by the Chern number,
characterized by spacial distribution of their probabilities and confirmed by
energy dispersion curves (Energy vs. angular momentum). It not only sheds light
on overcoming low-temperature operating limitation of existing narrow-gap TIs,
but also opens an opportunity to realize valley- and spin- qubits.Comment: 5 pages, 5 figures. Feedback is welcome