Introduction to integer quantum Hall effect by Ganpathy Murthy

Ғылым және технология

DISCUSSION MEETING : EDGE DYNAMICS IN TOPOLOGICAL PHASES
ORGANIZERS : Subhro Bhattacharjee, Yuval Gefen, Ganpathy Murthy and Sumathi Rao
DATE & TIME : 10 June 2019 to 14 June 2019
VENUE : Madhava Lecture Hall, ICTS Bangalore
Topological phases of matter have been at the forefront of research in condensed matter physics for the last 15-20 years. The low energy dynamics of these phases is governed by non-trivial topology, manifest in measurable observables, and having major consequences on the field of quantum Hall effect. The common feature of these systems is that the bulk has a charge gap and transport is mainly through edge or surface states. In recent times, besides the excitement about the new topological phases such as time-reversal invariant topological insulators and topological superconductors, there are many new and unexplained phenomena pertaining to quantum Hall phases (integer and fractional), graphene phases and more, and a workshop focussing on these phenomena will be very useful and timely.
In particular, this workshop will focus on recent work (mainly theoretical, but with some input from experimentalists) in the area of transport and edge dynamics at the boundaries of two dimensional systems including quantum Hall edges, graphene, and topological insulator edges. More specifically, the range of topics include edge reconstruction in quantum Hall syste ms, helical edges in topological insulators, transport through graphene edges and possible reconstructions artificially engineered edges including Floquet edges and parafermions at the edge.
The principal aim of this workshop is to foster interaction and collaborations between the researchers. An important secondary goal is to provide a learning experience for faculty, post-doctoral fellows and relatively experienced students with related expertise wishing to enter the field. In this spirit, we expect to have at least one longer pedagogical lecture each day, followed by 1/2 hour talks on recent results by experts in the field.
Eligibility criteria: We invite applications from senior PhD students, postdocs and faculty who are working in related areas, and have some interest in the field.
Accommodation for outstation/non-local participants will be provided at our on campus ICTS guest house.
APPLICATION DEADLINE : 25 February 2019
CONTACT US : edytop2019 ictsresin
PROGRAM LINK : www.icts.res.in/discussion-me...
Table of Contents (powered by videoken.com)
0:00:00 Introduction to integer quantum Hall
0:01:28 Agenda
0:03:25 1. Classical Hall Effect
0:08:54 Graph
0:19:22 Clean non interacting Hamiltonian
0:21:54 Landan gauge
0:30:44 Solution
0:34:55 Degeneracy
0:38:23 Gauge argument (Laughlin + Halperin)
0:49:15 Charge passing a particular x = e
0:49:50 Faraday emf
0:51:05 Equation for Conductivity
0:56:06 Summary

Пікірлер: 18

  • @brendawilliams8062
    @brendawilliams80623 ай бұрын

    The one to the next one will not change

  • @payalwadhwa7993
    @payalwadhwa79934 жыл бұрын

    Awesome lecture! Thank you, Sir!

  • @jeremiah6928
    @jeremiah69282 жыл бұрын

    Professor speaking FACTS!!!

  • @atomicdmt8763
    @atomicdmt8763 Жыл бұрын

    very good one. knowledge drop!

  • @polarkerr
    @polarkerr3 жыл бұрын

    Awesome indeed!

  • @felixmende2693
    @felixmende26933 жыл бұрын

    excellent talk!

  • @byronwatkins2565
    @byronwatkins25652 жыл бұрын

    When the sample is curled into a cylinder, the flux that did go off to infinity now collects along the axis and comes out the end as shown. The flux loops back outside the cylinder, penetrates the cylinder at right angle, and comes out along the axis to close the loop.

  • @boudouindillmann7080
    @boudouindillmann70802 жыл бұрын

    Nice introductory lecture, however putting the density of charges too close to the integer that is also at the denominator of the Hall resistance is not pedagogical at all.

  • @timwatz2948
    @timwatz29483 жыл бұрын

    I was out, when he started talking about Hamiltonians.

  • @zainuddin4564
    @zainuddin45643 жыл бұрын

    sir where is the other part?

  • @andrealiu8650
    @andrealiu865011 ай бұрын

    Perfect

  • @polarkerr
    @polarkerr3 жыл бұрын

    you lost me right after classical hall effect, nothing wrong with the lecture, just me, I need to learn more, I was hoping for more physics and less math

  • @anastasiawalrave5715
    @anastasiawalrave57153 ай бұрын

    23:00 how do we see that py commutes with the hamiltonian? How do we see that px doesn't?

  • @Physics20byabhinav

    @Physics20byabhinav

    Ай бұрын

    I think it's simple remember basic commutation relation [x,px] = h [y,py] = h But [px,py] = 0 [y,px] =0 [x,py] = 0 Prof. used these simple commutators to say that [py,H] = 0 . I hope you get it.

  • @ankitlabh
    @ankitlabh3 жыл бұрын

    Question on classical hall effect part: The Magnetic field (B) you mentioned is corrected for demagnetization effect or just the external field? Second question, whether q (charge carrier) is elementary or can it be an effective charge carrier (q_eqv) which could be quasiparticles? Thanks

  • @edwardmacnab354
    @edwardmacnab3542 жыл бұрын

    What is the tiny solenoid in the gauge argument exactly ? At around time 44:36 or less ! That was not sufficiently explained POV:

  • @brendawilliams8062

    @brendawilliams8062

    3 ай бұрын

    What’s a length. Planck scale. Phi diameter can’t be Planck length So you have a crucial point. I guess

  • @bestowicprimer8835
    @bestowicprimer88354 жыл бұрын

    Seeing geometry in ancient architecture and glyph

Келесі