English (United Kingdom)

https://curated-unify.zendy.io/wp-json/zendy-region/v1/featured_content/oa?rat=en

https://curated-unify.zendy.io/wp-json/zendy-region/v1/highlighted_journal/

Global: Zendy Plus annual

Presents the access of premium content as premium feature

Premium Content

Presents the keyphrase highlighting as premium feature

Keyphrase Highlighting

Presents the summarisation as premium feature

Summarisation

Insights

Presents the pdf analysis as premium feature

PDF Analysis

Presents the zaia usage as premium feature

ZAIA

Global: Zendy Tools annual

Global: Zendy Free Plan

Global: Zendy Tools monthly

Global: Zendy Plus monthly

The topological Anderson and Mott insulators are two phases that have so farbeen separately and widely explored beyond topological band insulators. Here wecombine the two seemingly different topological phases into a system ofspin-1/2 interacting fermionic atoms in a disordered optical lattice. We findthat the topological Anderson and Mott insulators in the noninteracting andclean limits can be adiabatically connected without gap closing in the phasediagram of our model. Lying between the two phases, we uncover a disorderedcorrelated topological insulator, which is induced from a trivial bandinsulator by the combination of disorder and interaction, as the generalizationof topological Anderson insulators to the many-body interacting regime. Thephase diagram is determined by computing various topological properties andconfirmed by unsupervised and automated machine learning. We develop anapproach to provide a unified and clear description of topological phasetransitions driven by interaction and disorder. The topological phases can bedetected from disorder/interaction induced edge excitations and charge pumpingin optical lattices.

Connecting Topological Anderson and Mott Insulators in Disordered Interacting Fermionic Systems