Spin-Mode-Switching at the nu=3 edge

Slides:



Advertisements
Similar presentations
Protected edge modes without symmetry Michael Levin University of Maryland.
Advertisements

Quasiparticle Scattering in 2-D Helical Liquid arXiv: X. Zhou, C. Fang, W.-F. Tsai, J. P. Hu.
Spintronics with topological insulator Takehito Yokoyama, Yukio Tanaka *, and Naoto Nagaosa Department of Applied Physics, University of Tokyo, Japan *
Exploring Topological Phases With Quantum Walks $$ NSF, AFOSR MURI, DARPA, ARO Harvard-MIT Takuya Kitagawa, Erez Berg, Mark Rudner Eugene Demler Harvard.
D-wave superconductivity induced by short-range antiferromagnetic correlations in the Kondo lattice systems Guang-Ming Zhang Dept. of Physics, Tsinghua.
Funded by NSF, Harvard-MIT CUA, AFOSR, DARPA, MURI Takuya Kitagawa Harvard University Mark Rudner Harvard University Erez Berg Harvard University Yutaka.
Quantum anomalous Hall effect (QAHE) and the quantum spin Hall effect (QSHE) Shoucheng Zhang, Stanford University Les Houches, June 2006.
Quantum Spin Hall Effect - A New State of Matter ? - Naoto Nagaosa Dept. Applied Phys. Univ. Tokyo Collaborators: M. Onoda (AIST), Y. Avishai (Ben-Grion)
Robustness of Majorana induced Fractional Josephson Effect
David Gershoni The Physics Department, Technion-Israel Institute of Technology, Haifa, 32000, Israel and Joint Quantum Institute, NIST and University of.
Activation energies and dissipation in biased quantum Hall bilayer systems at. B. Roostaei [1], H. A. Fertig [2,3], K. J. Mullen [1], S. Simon [4] [1]
Fractional topological insulators
14. April 2003 Quantum Mechanics on the Large Scale Banff, Alberta 1 Relaxation and Decoherence in Quantum Impurity Models: From Weak to Strong Tunneling.
Revealing anyonic statistics by multiphoton entanglement Jiannis K. Pachos Witlef Wieczorek Christian Schmid Nikolai Kiesel Reinhold Pohlner Harald Weinfurter.
Glassy dynamics of electrons near the metal-insulator transition in two dimensions Acknowledgments: NSF DMR , DMR , NHMFL; IBM-samples; V.
Experimental observation of the Spin-Hall Effect in InGaN/GaN superlattices Student : Hsiu-Ju, Chang Advisor : Yang Fang, Chen.
Quantum Hall Effect Jesse Noffsinger Group Meeting Talk (As required by the Governor of the State of California) April 17, 2007.
Correlated tunneling and the instability of the fractional quantum Hall edge Dror Orgad Oded Agam July 21, 2009 PRL 100, (2008)
Activation energies and dissipation in biased quantum Hall bilayer systems at. B. Roostaei [1,2], H. A. Fertig [3,4], K. J. Mullen [2], S. Simon [5] [1]
Measuring quantum geometry From superconducting qubits to spin chains Michael Kolodrubetz, Physics Department, Boston University Theory collaborators:
Quantum conductance I.A. Shelykh St. Petersburg State Polytechnical University, St. Petersburg, Russia International Center for Condensed Matter Physics,
Topological Insulators and Beyond
Observation of neutral modes in the fractional quantum hall effect regime Aveek Bid Nature (2010) Department of Physics, Indian Institute of Science,
The world of 2d electrons is exciting: enabling ‘ballistic high mobility transport’ modulation doping enabling ‘ballistic high mobility transport’ modulation.
Quantum Spin Hall Effect and Topological Insulator Weisong Tu Department of Physics and Astronomy University of Tennessee Instructor: Dr. George Siopsis.
© Copyright National University of Singapore. All Rights Reserved. ENHANCING THERMOELECTRIC EFFICIENCY FOR NANOSTRUCTURES AND QUANTUM DOTS Jian-Sheng Wang.
Technion – Israel Institute of Technology Physics Department and Solid State Institute Eilon Poem, Stanislav Khatsevich, Yael Benny, Illia Marderfeld and.
Berry Phase Effects on Electronic Properties
Infrared Hall effect in conventional and unconventional materials John Cerne, SUNY at Buffalo, DMR In metals, magnetic fields (H) deflect moving.
2003/8/18ISSP Int. Summer School Interaction effects in a transport through a point contact Collaborators A. Khaetskii (Univ. Basel) Y. Hirayama (NTT)
Two Level Systems and Kondo-like traps as possible sources of decoherence in superconducting qubits Lara Faoro and Lev Ioffe Rutgers University (USA)
Molecular dynamics simulation of strongly coupled QCD plasmas Peter Hartmann 1 Molecular dynamics simulation of strongly coupled QCD plasmas Péter Hartmann.
Photonic Topological Insulators
Ady Stern (Weizmann) Papers: Stern & Halperin , PRL
Topology induced emergent dynamic gauge theory in an extended Kane-Mele-Hubbard model Xi Luo January 5, 2015 arXiv:
Progress Report: Tools for Quantum Information Processing in Microelectronics ARO MURI (Rochester-Stanford-Harvard-Rutgers) Third Year Review, Harvard.
Topological Insulators Effects of spin on transport of electrons in solids.
The Puzzling Boundaries of Topological Quantum Matter Michael Levin Collaborators: Chien-Hung Lin (University of Chicago) Chenjie Wang (University of Chicago)
Basics of edge channels in IQHE doing physics with integer edge channels studies of transport in FQHE regime deviations from the ‘accepted’ picture Moty.
University of Washington
Topological physics with a BEC: geometric pumping and edge states Hsin-I Lu with Max Schemmer, Benjamin K. Stuhl, Lauren M. Aycock, Dina Genkina, and Ian.
Introduction to Chalker- Coddington Network Model Jun Ho Son.
Flat Band Nanostructures Vito Scarola
Thermal and electrical quantum Hall effects in ferromagnet — topological insulator — ferromagnet junction V. Kagalovsky 1 and A. L. Chudnovskiy 2 1 Shamoon.
Quantum spin Hall effect Shoucheng Zhang (Stanford University) Collaborators: Andrei Bernevig, Congjun Wu (Stanford) Xiaoliang Qi (Tsinghua), Yongshi Wu.
1 The 5/2 Edge IPAM meeting on Topological Quantum Computing February 26- March 2, 2007 MPA Fisher, with Paul Fendley and Chetan Nayak Motivation: FQHE:
Arnau Riera, Grup QIC, Dept. ECM, UB 16 de maig de 2009 Intoduction to topological order and topologial quantum computation.
New Materials and topological phases
From fractionalized topological insulators to fractionalized Majoranas
Fractional Berry phase effect and composite particle hole liquid in partial filled LL Yizhi You KITS, 2017.
Topological Insulators
Quantum Hall Fluids By Andrew York 12/5/2008.
Peter Samuelsson, Sara Kheradsoud, Björn Sothmann
QHE discovered by Von Klitzing in 1980
Primordial BHs.
Tunneling between helical edge states through extended contacts
Zhejiang Normal University
Novel quantum states in spin-orbit coupled quantum gases
D. Ferraro N. Magnoli M. Merlo
Charging and noise as probes of non-abelian quantum Hall states
Non- Abelian Quantum Hall States:
Correlations of Electrons in Magnetic Fields
SOC Fermi Gas in 1D Optical Lattice —Exotic pairing states and Topological properties 中科院物理研究所 胡海平 Collaborators : Chen Cheng, Yucheng Wang, Hong-Gang.
Michael Fuhrer Director, FLEET Monash University
Sep. 23, 2008 Correlated tunneling and the instability of the fractional quantum Hall edge Dror Orgad Oded Agam PRL 100, (2008)
Y. Baum, T. Posske, I. C. Fulga, B. Trauzettel, A. Stern
FSU Physics Department
Evidence for a fractional fractal quantum Hall effect in graphene superlattices by Lei Wang, Yuanda Gao, Bo Wen, Zheng Han, Takashi Taniguchi, Kenji Watanabe,
Simple Stretch “Flips” the Sign of Charge Carriers
Department of Physics, Sichuan University
Presentation transcript:

Spin-Mode-Switching at the nu=3 edge Ganpathy Murthy Mizpe Ramon, May 31, 2018 University of Kentucky, and the Technion

Acknowledgements NSF, US-Israel BSF, Aspen Center for Physics Lady Davis Fellowship from the Technion Udit Khanna, GM, Sumathi Rao, and Yuval Gefen, PRL 119, 186804 (2017).

A somewhat lesser known collaborator

Outline Mode-Switching at nu=3 The QHE Why study Quantum Hall Edges? Edge Reconstruction: Review Mode-Switching at nu=3 Experimental Signatures Conclusions

The Quantum Hall Effects

Quantum Hall Edges

Properties of Quantum Hall Edges Each edge mode is chiral. In the noninteracting integer QHE each mode carries a charge of e. The sum of the charge times chirality is the Hall conductance, which is a quantized, topologically protected, property of the bulk. In Abelian quantum Hall states, the sum of the chiralities of the modes is the thermal Hall conductance, another quantized and topologically protected property. Subject to these constraints, anything can happen depending on the details of interactions, disorder, and the confining edge potential.

Some recent puzzling/exciting phenomena at the edge A nu=2/3 edge mode in a bulk nu=1 sample (Venkatachalam et al 2012). “Pairing” of electrons near nu=3 (Choi et al 2014). 1/3 edge modes seen in a nu=2/3 bulk sample (Sabo et al, 2017). Observation of fractional thermal Hall conductance at nu=5/2 (Banerjee et al, arXiv:1710).

Edge Reconstruction Review Wang, Meir, Gefen, 2017

Chamon and Wen, 1994

An even more complicated case

The nu=3 bulk

An Argument for a reconstruction

Two New Edge Phases!

Hartree Fock Results

Some Obvious Questions Level crossings or avoided crossings? What is the order of the transition? What is the order parameter, if any? What is the “driving force” behind the transition?

All crossings are avoided in unrestricted HF

The transitions are first-order in the order parameter

The electronic density doesn’t change through the transition

Experimental Signatures in setups with QPCs Spin Transport

Charge Transport: Strong Plateau

Charge Transport: Weak Plateau

Conclusions and Open Questions We have discovered a new kind of edge reconstruction driven purely by exchange. Spin-Mode-Switching has very striking signatures in spin transport, and more subtle ones in charge transport. Should occur for other integer and even fractional states which have partial polarization. Is there a neutral spin mode? If so, there would be an upstream chiral and decoherence.

Thanks and Happy Birthday, Yigal!

The spin rotations of the two occupied states in Phase B