Martin Claassen, PhD
Flatiron Research Fellow

Center for Computational Quantum Physics (CCQ), Flatiron Institute, 162 Fifth Avenue, New York, United States

Simons Foundation / Flatiron Institute / Center for Computational Physics

Dr. Michael Sentef
Michael Sentef
Research Group Leader
Phone: +49 (0)40 8998-88350
Room: 99/O2.023

Emmy-Noether Group leader

Prof. Dr. Angel Rubio
Angel Rubio
Managing Director
Phone: +49 (0)40 8998-88301
Room: 99/O2.021
Jenny Witt
Jenny Witt
Public Relations and Communications
Phone: +49 (0)40 8998-6593
Room: 99/O1.081


M. Claassen, D.M. Kennes, M. Zingl, M.A. Sentef, A. Rubio
Universal optical control of chiral superconductors and Majorana modes


Laser-controlled novel superconductors could pave the way to future quantum computers

May 29, 2019

Controlling the quantum properties of materials is a central challenge in physics as well as an essential step towards using quantum physics for applications or building scalable quantum computers.
Switching of a two-component chiral order parameter represented on the Bloch sphere (click on image to view video). Zoom Image
Switching of a two-component chiral order parameter represented on the Bloch sphere (click on image to view video).

The use of strong electromagnetic radiation to push materials out of their normal equilibrium is a new frontier in this field. Such manipulation leads to the emergence of new phases with novel, useful and controllable properties.

Now, a team of scientists in the USA and Germany has shown that tailored laser pulses can be used to control the properties of chiral topological superconductors. Their work has just been published in Nature Physics.

Superconductors are materials which can conduct electricity without resistance. Currently, this only happens in specific circumstances, for example at very low temperatures. Chiral topological superconductors are a particular class which hosts an elusive particle called a Majorana fermion. This can be used to encode quantum bits and perform error-resilient computation. However, controlling and manipulating these emergent properties poses a significant challenge.

Fundamentally, the chiral topological nature of these materials relies on the rotation and reflection symmetries of the crystal lattice to maintain a subtle balance between competing superconducting states. The researchers from the Flatiron Institute’s Center for Computational Quantum Physics (CCQ) in New York City (USA), Freie Universität Berlin and the Max Planck Institute for the Structure and Dynamics of Matter (both in Germany) found that a weak pulse can disrupt this balance and induce a dramatic change in the underlying electronic order. This occurs because the pulse  selectively breaks these symmetries via choice of polarization. 

In particular, the team showed numerically that an appropriately-tuned pulse sequence can selectively reverse the “handedness” of a chirally-superconducting region on a very fast time scale (on the order of picoseconds – a trillionth of a second). This handedness is an intrinsic topological property of such materials and sets the propagation direction (clockwise or counter-clockwise) of Majorana fermions that are induced along its boundary. 

An intriguing consequence of their work is the possibility to optically “program” topologically-protected quantum circuits, to perform computation on the charging states of single electrons injected into the Majorana boundary modes. Furthermore, the underlying mechanism is robust and relies solely on symmetry, not on the materials’ details. It could be applied to any material with multi-component order parameters. 

The scientists predict that topological superconductivity can be detected in time-resolved pump-probe experiments where an initial laser pulse alters the superconducting state in the material and a second ‘reads’ these changes after a short delay. This establishes pump-probe experiments as a new experimental tool to reveal the putative chiral topological nature of superconductivity in a wide array of candidate materials such as Sr2RuO4, twisted bilayer graphene, SrPtAs, or UPt3.

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