Topological Superconductors and Majorana platforms based on TIs New Topological States of Matter: Platform for emergent Dirac, Majorana & Weyl fermions (Colloquium at CalTech) KITP talk on topological superconductivity and Majorana platform New Topological States of Matter (Inst. for Adv. Study Distinguished Lecture at HKUST) Pedagogical Lecture Series Spin-orbital ground states of superconducting doped topological insulators: A Majorana platform L. A. Wray, S. Xu, Y. Xia, D. Qian, A. V. Fedorov, H. Lin, A. Bansil, L. Fu, Y. S. Hor, R. J. Cava, and M. Z. Hasan Phys. Rev. B 83, 224516 (2011) Chiral Majorana Fermion Modes on the Surface of Superconducting Topological Insulators Ching-Kai Chiu, Guang Bian, Hao Zheng, Jiaxin Yin, Songtian S. Zhang, Su-Yang Xu, M. Zahid Hasan arXiv:1612.09276 (2016) Topological Dirac surface states and superconducting pairing correlations in PbTaSe2 (Topological Superconductor Candidate) T.-R. Chang, P.-J. Chen, G. Bian, S.-M. Huang, H. Zheng, T. Neupert, R. Sankar, S.-Y. Xu, I. Belopolski, G. Chang, B. Wang, F. Chou, A. Bansil, H.-T. Jeng, H. Lin, and M. Z. Hasan Phys. Rev. B 93, 245130 (2016) Momentum-space imaging of Cooper pairing in a half-Dirac-gas topological superconductor Su-Yang Xu, Nasser Alidoust, Ilya Belopolski, Anthony Richardella, Chang Liu, Madhab Neupane, Guang Bian, Song-Hsun Huang, Raman Sankar, Chen Fang, Brian Dellabetta, Wenqing Dai, Qi Li, Matthew J. Gilbert, Fangcheng Chou, Nitin Samarth & M. Zahid Hasan Nature Physics 10, 943 (2014) Observation of topological order in a superconducting doped topological insulator L. Andrew Wray, Su-Yang Xu, Yuqi Xia, Yew San Hor, Dong Qian, Alexei V. Fedorov, Hsin Lin, Arun Bansil, Robert J. Cava & M. Zahid Hasan Nature Physics 6, 855 (2010) |
||
Recently, there has been great interest in finding topologically nontrivial states in materials that are not insulators. A particularly exciting proposal is to realize a topological superconductor. Superconductivity is a collective phenomenon where electrons at the Fermi level cannot exist as single particles but are attracted to each other, forming Cooper pairs. This causes an energy gap, the superconducting gap, in the electronic single-particle spectrum. In a topological insulator, the bulk electronic structure has an insulating band gap whereas the surface shows protected Dirac electron states due to the nontrivial topology. It has been proposed that one can use a similar picture to qualitatively understand a topological superconductor. A topolological superconductor has a superconducting gap in the bulk but show protected metallic states on its boundaries or surfaces. However, unlike a topological insulator where the surface states consist of electrons, the surface states in a topological superconductor are made up of Majorana fermions. A Majorana fermion is a fermionic particle that is its own antiparticle. It was originally proposed in high energy physics as a way to understand neutrinos but has not been conclusively observed as any fundamental particle. On the other hand, it is believed that Majorana fermions arising in condensed matter systems can play a pivital role in building a fault-tolerant quantum computer. Moreover, it has been predicted that certain quantum phase transition associated with a topological superconductor can realize condensed matter supersymmetry. Supersymmetry is a fascinating theory in particle physics under which bosons and fermions can be converted into each other. However, observing supersymmetry in particle physics requires accelerating elementary particles to very high energies, which are probably beyond the capability of the most powerful accelerators currently available such as the large hadron collider, and therefore supersymmetry remains elusive to date. Topological superconductors provide a rare and exciting platform to realize Majorana fermions and supersymmetry physics in similar condensed matter settings. Recently, we have realized a 2D helical topological superconductor in a heterostructure sample constituting of a topological insulator Bi2Se3 film and a s-wave superconductor NbSe2. |
||
Spin and angle resolved photoemission (spin-ARPES) measurements on Bi_{2}Se_{3}/NbSe_{2} heterostructure demonstrate topological superconductivity and helical Cooper pairing via proximity effect. Published in S.-Y. Xu, N. Alidoust, I. Belopolski et al., Nature Physics 10, 943 (2014). |
||
Possible topological superconductivity in CuxBi2Se3
Back in 2010, we were already trying to search for topologically nontrivial states in superconductors. We systematically studied copper-doped bismuth selenide, CuxBi2Se3, which was found to be a superconductor with a transition temperature, Tc ~ 3.8 K. Our critical surface and bulk electronic structure results suggested two possible distinct types of topological superconductivity that can arise in CuxBi2Se3. One scenario (panel c) is that the surface of CuxBi2Se3 realizes a 2D helical topological superconductor via the natural proximity effect between the surface and the bulk of the sample. In this scenario, Majorana fermions are bounded within the magnetic vortices at the surface of the sample under an external magnetic field. The other scenario (panel d) is that the bulk of CuxBi2Se3 is a 3D topological superconductor, where Majorana fermions can flow along the surfaces of the sample in the form of a 2D Majorana surface state, or a 2D Majorana gas. Very recently, we have realized a 2D helical topological superconductor (the scenario one, panel c) in heterostructure samples constituting a topological insulator thin film and an s-wave superconductor NbSe2 substrate. |
||
Observation of topological order in a superconducting doped topological insulator. Published in L. A. Wray, S.-Y. Xu, Y. Xia, et al., Nature Physics 6, 855 (2010). |
||