Du,1,4 C.M. Quantum Hall trio. L. Wang3,b) 1National Lab of Solid State Microstructures, Department of Physics, Nanjing University, Nanjing 210093, People’s Republic of China Band, Yshai Avishai, in Quantum Mechanics with Applications to Nanotechnology and Information Science, 2013. Topological quantum numbers in the Hall effect J. E. Avron1, D. Osadchy1 and R. Seiler2 1 Department of Physics, Technion, 32000 Haifa, Israel 2 Department of Mathematics, TU Berlin, Berlin, Germany February 6, 2008 Abstract Topological quantum numbers account for the precise quantization that occurs in the integer Hall effect. Two prominent ones are • Prange and Girvin, “The Quantum Hall Effect” This is a collection 0038%1098/95 $9.50 + .OO 0038-1098(94)00828-O DISPERSIVE COLLECTIVE EXCITATION MODES IN THE QUANTUM HALL REGIME L.L. The quantum Hall e ect (QHE) is one of the most remark-able condensed-matter phenomena discovered in the second half of the 20th century, and our talk is mainly about the integer quantum hall e ect. PHYSICAL REVIEW B 87, 205429 (2013) Quantum Hall effect in graphene with twisted bilayer stripe defects Tomas L ofwander,¨ 1 Pablo San-Jose,2 and Elsa Prada3 1Department of Microtechnology and Nanoscience - MC2, Chalmers University of Technology, SE-412 96 G¨oteborg, Sweden 2Instituto de Estructura de la Materia (IEM-CSIC), Serrano 123, 28006 Madrid, Spain The basic experimen- Sohn, A. Pinczuk, B.S. 4. Dennis, L.N. It rivals superconductivity in its fundamental signi cance as a manifestation of quantum mechanics on macroscopic scales. Download PDF Abstract: Unconventional features of relativistic Dirac/Weyl quasi-particles in topological materials are most evidently manifested in the 2D quantum Hall effect (QHE), whose variety is further enriched by their spin and/or valley polarization. Pfeiffer and K.W. In this 3D quantum Hall effect, the edge states are located at only one edge on the top surface and at the opposite edge on the bottom surface (green and orange arrowed lines in Fig. We consider an infinite graphene sheet with weak disorder that leads to broadening of Landau levels. The set-up is as follows: Electrons are restricted to move in the 2D (x,y)-plane … The fundamental novelty of both those phenomena, which involve elec- In 1980 a quantized version of the Hall e ect was discovered by Klitzing, Dorda and Pepper, which later gave them the Nobel prize [1, p. 13]. The Half-Filled Landau level. ?integer quantum Hall effect: resolved Landau levels with localization between centers of Landau levels?low disorder 2D electron systems show fractional quantum Hall effect – correlations of electrons as described by the Laughlin wave function?what about many fractional quantum Hall states? 3. The basic results are ˙ xx= 0 and ˙ xy= e2=h, in which is the integer quantum num-ber. Si tenemos un campo magnético constante B en la dirección z y electrones restringidos a moverse en el plano (x,y), aparece una corriente I en la dirección x. El Efecto Hall nos dice que esto produce un voltaje V H en la dirección y. The original, classical Hall e↵ect was discovered in 1879 by Edwin Hall. 1d and e), which can be probed by scanning tunneling microscopy. Quasi-Holes and Quasi-Particles. We’ll start these lectures by reviewing the underlying physics of the Hall e↵ect. Although its extension to three dimensions has been long-sought and inspired theoretical proposals, material candidates have been lacking. Non-Abelian Quantum Hall States: PDF Higher Landau Levels. H is the external magnetic field, and M is the magnetization. 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