16 October 2018
Disorder induces topological Anderson insulator

Artist's depiction of a disorder-induced transition to the topological Anderson insulator phase. Image Credit: Lachina Creative, copyright Bryce Gadway, University of Illinois at Urbana-Champaign

In experiments with ultracold atoms trapped and driven by lasers, researchers have created a new disorder-induced topological state previously predicted to occur in electronic materials.
Topological insulators (TIs) host exotic physics that could shed new light on the fundamental laws of nature. What’s more, the unusual properties of TIs hold tremendous promise for technological applications, including in quantum computing, next-generation miniaturized data storage, and spintronics. Scientists around the globe are working to understand the microscopic properties of these materials that freely conduct electricity along their edges even though their bulk is an insulator.

Now a team of experimental physicists at the University of Illinois at Urbana-Champaign have made the first observation of a specific type of TI that’s induced by disorder. Professor Bryce Gadway and his graduate students Eric Meier and Alex An used atomic quantum simulation, an experimental technique employing finely tuned lasers and ultracold atoms about a billion times colder than room temperature, to mimic the physical properties of one-dimensional electronic wires with precisely tunable disorder. The system starts with trivial topology just outside the regime of a topological insulator; adding disorder nudges the system into the nontrivial topological phase. This type of topological insulator induced by disorder is called the topological Anderson insulator, named after the noted theoretical physicist and Nobel laureate Philip Anderson, an alumnus of University Laboratory High School on the U of I campus. Surprisingly, while disorder typically inhibits transport and destroys nontrivial topology, in this system it helps to stabilize a topological phase.

The observation was made possible through close collaboration with an international team of theoretical physicists at the U of I, at ICFO –the Institute of Photonic Sciences, and at the Universitat Politècnica de Catalunya (UPC) in Spain, who elucidated the quantum physics at work and identified the key signature the experimentalists should look for in the system.

Theoretical physicists included ICFO researchers Dr. Pietro Massignan, Alexandre Dauphin, and Dr. Maria Maffei. Massignan of UPC and ICFO comments,

Meier is lead author on the paper.

The group’s experimental observation validates the concept of topological Anderson insulators that was worked out roughly a decade ago. The topological Anderson insulator phase was first discovered theoretically by J. Li et al. in 2009, and its origin was further explained by C. W. Groth, et al. that same year. Five years later, a pair of works, one by A. Altland et al. and one by the group of Taylor Hughes at the U of I working with the group of Emil Prodan at Yeshiva University, predicted the occurrence of the topological Anderson insulator in one-dimensional wires, as realized in the new experiments from the Gadway group.

Gadway emphasizes,

This research was supported by the National Science Foundation and by the Office of Naval Research, and by the Spanish MINECO, the Generalitat de Catalunya, the EU, and the Fundació Privada Cellex. The results are those of the researchers and not necessarily those of the funding agencies.

Now a team of experimental physicists at the University of Illinois at Urbana-Champaign have made the first observation of a specific type of TI that’s induced by disorder. Professor Bryce Gadway and his graduate students Eric Meier and Alex An used atomic quantum simulation, an experimental technique employing finely tuned lasers and ultracold atoms about a billion times colder than room temperature, to mimic the physical properties of one-dimensional electronic wires with precisely tunable disorder. The system starts with trivial topology just outside the regime of a topological insulator; adding disorder nudges the system into the nontrivial topological phase. This type of topological insulator induced by disorder is called the topological Anderson insulator, named after the noted theoretical physicist and Nobel laureate Philip Anderson, an alumnus of University Laboratory High School on the U of I campus. Surprisingly, while disorder typically inhibits transport and destroys nontrivial topology, in this system it helps to stabilize a topological phase.

The observation was made possible through close collaboration with an international team of theoretical physicists at the U of I, at ICFO –the Institute of Photonic Sciences, and at the Universitat Politècnica de Catalunya (UPC) in Spain, who elucidated the quantum physics at work and identified the key signature the experimentalists should look for in the system.

Theoretical physicists included ICFO researchers Dr. Pietro Massignan, Alexandre Dauphin, and Dr. Maria Maffei. Massignan of UPC and ICFO comments,

**“Intuitively, one would think that disorder should play against conductance. For example, running is easy in an open field, but gets harder and harder as one moves through an increasingly denser forest. But here we show that suitably tailored disorder can actually trigger some peculiar conducting excitations, called topologically protected edge modes.“**Meier is lead author on the paper.

**“Interestingly,”**he adds,**“in a 3D or 2D topological system, those edge states would be characterized by freely flowing electrons. But in a 1D system like ours, the edge states simply sit there, at either end of the wire. In any TI, the boundary states have the dimensionality of your system minus one. In our 1D topological Anderson insulator, the boundary states are basically just points at either end of the wire. While the boundary physics is actually a bit boring in this system, there is rich dynamics going on in the bulk of the system that is directly related to the same topology–this is what we studied.”**The group’s experimental observation validates the concept of topological Anderson insulators that was worked out roughly a decade ago. The topological Anderson insulator phase was first discovered theoretically by J. Li et al. in 2009, and its origin was further explained by C. W. Groth, et al. that same year. Five years later, a pair of works, one by A. Altland et al. and one by the group of Taylor Hughes at the U of I working with the group of Emil Prodan at Yeshiva University, predicted the occurrence of the topological Anderson insulator in one-dimensional wires, as realized in the new experiments from the Gadway group.

Gadway emphasizes,

**“Our taking on this research was really inspired by the 2014 prediction of Taylor Hughes and his graduate student Ian Mondragon-Shem at the U. of I. Taylor was a key collaborator. Likewise, our colleagues in Spain made a tremendous contribution in introducing the concept of mean chiral displacement, which allows to measure the topology directly in the bulk of the material.”**“Working with Taylor,” Gadway adds, “our Spanish colleagues found that the mean chiral displacement is essentially equivalent to the topological invariant of such a one-dimensional system, something called the winding number. This was critical to our being able to take the data on the system and relate what we saw in experiment to the system’s topology. This was one project where having a bevy of theorists around was a big help, both for performing the right measurements and for understanding what it all meant.”**“This is an exciting result in terms of potential applications,**” Gadway affirms.**“This suggests we may be able to find real materials that are almost topological that we could manipulate through doping to imbue them with these topological properties. This is where quantum simulation offers a tremendous advantage over real materials—it’s good for seeing physical effects that are very subtle. Our ‘designer disorder’ is precisely controllable, where in real materials, disorder is as messy as it sounds—it’s uncontrollable.”****“Gadway’s experimental setup is a theorist’s dream**,” Massignan adds. “**It was like playing with LEGO: the model we envisaged could be built step-by-step, in a real laboratory. Every single element of the Hamiltonian we had in mind could be implemented in a very careful way, and changed in real time.” Alexandre Dauphin adds “This platform is also very promising for studying the effects of both interaction and disorder in topological systems, which could lead to exciting new physics.”**This research was supported by the National Science Foundation and by the Office of Naval Research, and by the Spanish MINECO, the Generalitat de Catalunya, the EU, and the Fundació Privada Cellex. The results are those of the researchers and not necessarily those of the funding agencies.