Topological Effects. PH671 - Transport
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1 Topological Effects PH671 - Transport
2 Speakers include Yakir Aharonov Boris Altshuler Yshai Avishai Michael Berry Markus Buttiker Georgi Dvali Francois Englert Klaus Ensslin Yuval Gefen David Gross* Moty Heiblum Yoseph Imry Tony Klein * Charles M. Marcus Yoichiro Nambu* Murray Peshkin Sandu Popescu Moti Segev Jurgen Smet David Thouless Akira Tonomura Chang C Tsuei Sam Werner Chen Ning Yang *to be confirmed 50 years of the Aharonov-Bohm Effect Concepts and Applications Aharonov-Bohm Effect in: Gauge Theories Scalar form Mesoscopic Systems Quantum Hall Effect Quantum Dots Carbon Nanotubes High-TC Superconductivity Aharonov-Casher Effect Quantum Geometrical Phases Nonlocal Aspects of the Aharonov-Bohm effect The Organizing committee Lev Vaidman (Chairman) Eshel Ben Jacob Guy Deutscher Yaron Oz The Program committee Shmuel Nussinov (Chairman) Yshai Avishai Joseph Avron Aharon Casher Yuval Gefen Benni Reznik The Advisory committee Jacob Bekenstein Michael Berry Moty Heiblum Anthony Leggett Akira Tonomura Frank Wilczek Joshua Yortner
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4 Observation of h/e Aharonov-Bohm Oscillations in Normal-Metal Rings R. A. Webb, S. Washburn, C. P. Umbach, and R. B. Laibowitz Phys. Rev. Lett. 54, 2696 Published 24 June 1985
5 Electromagnetic Aharonov-Bohm effect in a two-dimensional electron gas ring W. G. van der Wiel, Yu. V. Nazarov, S. De Franceschi, T. Fujisawa, J. M. Elzerman, E. W. G. M. Huizeling, S. Tarucha, and L. P. Kouwenhoven Phys. Rev. B 67, Published 29 January 2003
6 Aharonov-Bohm effect in charge-density wave loops with inherent temporal current switching M. Tsubota, K. Inagaki, T. Matsuura and S. Tanda EPL, 97 (2012) doi: / /97/57011
7 Aharonov-Bohm effect in charge-density wave loops with inherent temporal current switching M. Tsubota, K. Inagaki, T. Matsuura and S. Tanda EPL, 97 (2012) doi: / /97/57011
8 Interferometer-Based Studies of Quantum Hall Phenomena, Douglas T. McClure III (PhD thesis, Harvard, 2012)
9 Interferometer-Based Studies of Quantum Hall Phenomena, Douglas T. McClure III (PhD thesis, Harvard, 2012)
10 The Composite Fermion: A Quantum Particle and Its Quantum Fluids Jainendra K. Jain Citation: Physics Today 53(4), 39 (2000); doi: / Integer QHE Fractional QHE
11 The Composite Fermion: A Quantum Particle and Its Quantum Fluids Jainendra K. Jain Citation: Physics Today 53(4), 39 (2000); doi: / Integer QHE Fractional QHE
12 Interferometer-Based Studies of Quantum Hall Phenomena, Douglas T. McClure III (PhD thesis, Harvard, 2012)
13 Interferometer-Based Studies of Quantum Hall Phenomena, Douglas T. McClure III (PhD thesis, Harvard, 2012) Chapter 2: Distinct signatures for Coulomb blockade and Aharonov-Bohm interference in electronic Fabry-Perot interferometers
14 Experimental observation of the quantum Hall effect and Berry's phase in graphene Yuanbo Zhang, Yan-Wen Tan, Horst L. Stormer and Philip Kim Nature 438, (10 November 2005) doi: /nature04235 a, Hall resistance (black) and magnetoresistance (red) measured in the device in Fig. 1 at T = 30 mk and Vg = 15 V. The verical arrows and the numbers on them indicate the values of B and the corresponding filling factor nu of the quantum Hall states. The horizontal lines correspond to h/e2nu values. The QHE in the electron gas is shown by at least two quanized plateaux in Rxy, with vanishing Rxx in the corresponding magneic field regime. The inset shows the QHE for a hole gas at Vg = - 4 V, measured at 1.6 K. The quanized plateau for filling factor nu = 2 is well defined, and the second and third plateaux with nu = 6 and nu = 10 are also resolved. b, Hall resistance (black) and magnetoresistance (orange) as a funcion of gate voltage at fixed magneic field B = 9 T, measured at 1.6 K. The same convenion as in a is used here. The upper inset shows a detailed view of high- filling- factor plateaux measured at 30 mk. c, A schemaic diagram of the Landau level density of states (DOS) and corresponding quantum Hall conductance (sigmaxy) as a funcion of energy. Note that, in the quantum Hall states, Unfortunately we are unable to provide accessible alternaive text for this. If you require assistance to access this image, or to obtain a text descripion, please contact npg@nature.com. The LL index n is shown next to the DOS peak. In our experiment the Fermi energy EF can be adjusted by the gate voltage, and Rxy- 1 changes by an amount gse2/h as EF crosses a LL.
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