logging in or signing up Quantum Mechanics for Applied Physics ankush85 Download Post to : URL : Related Presentations : Share Add to Flag Embed Email Send to Blogs and Networks Add to Channel Uploaded from authorPOINT lite Insert YouTube videos in PowerPont slides with aS Desktop Copy embed code: Embed: Flash iPad Dynamic Copy Does not support media & animations Automatically changes to Flash or non-Flash embed WordPress Embed Customize Embed URL: Copy Thumbnail: Copy The presentation is successfully added In Your Favorites. Views: 414 Category: Education License: All Rights Reserved Like it (0) Dislike it (0) Added: September 04, 2009 This Presentation is Public Favorites: 1 Presentation Description No description available. Comments Posting comment... By: saydhameen (42 month(s) ago) please allow to download Saving..... Post Reply Close Saving..... Edit Comment Close By: saydhameen (42 month(s) ago) please allow to downlod Saving..... Post Reply Close Saving..... Edit Comment Close Premium member Presentation Transcript Quantum Mechanics for Applied Physics : Quantum Mechanics for Applied Physics Two levels system : 2 Two levels system | cb(t) | 2 = cos(ωt)2 where ω is the Rabi frequency Slide 3: 3 Slide 4: 4 Classical Electrodynamics : 5 micro/macroscopic electric field micro/macroscopic magnetic field charge/current density Constitutive equations Classical Electrodynamics Potentials Charge conservation polarization magnetization speed of light Energy & momentum : 6 Energy & momentum Point charge: , Lorentz force Energy balance in a space domain EM energy density Kinetic energy of charges Poynting’s energy flux vector using identity Electron in a Magnetic field : 7 Electron in a Magnetic field Quantization P change to Popand r to rop Wave function Lev_Davidovich_Landau Slide 8: 8 To actually solve Schrödinger’s equation for an electron confined to a plane in a uniform perpendicular magnetic field, it is convenient to use the Landau gauge. H commutes with px, so H and px have a common set of eigenstates, taking Landau Levels : 9 Landau Levels Example of quantization measurement Effects of Landau levels are only observed when the mean thermal energy is smaller than the energy level separation, , meaning low temperatures and strong magnetic fields Aharonov Bohm : 10 Aharonov Bohm The Aharonov-Bohm effect demonstrates that the electromagnetic potentials, rather than the electric and magnetic fields, are the fundamental quantities in quantum mechanics. The necessary conditions to observe the Aharonov-Bohm effect, i.e. a shift of the diffraction pattern that varies periodically with B, are: There must be at least two interfering alternatives for the particle to arrive at the detector, and At least two of these interfering alternatives must enclose a shielded magnetic field and must be topologically distinct. The animation shows the superposition of the waves for the case with (in blue) and without (in red) a magnetic field. Magnetic Aharonov Bohm effect : 11 Magnetic Aharonov Bohm effect Result of the requirement that quantum physics be invariant with respect to the gauge choice for the vector potential A. This implies that a particle with electric charge q traveling along some path P in a region with zero magnetic field must acquire a phase which is in si units: phase difference between any two paths with the same endpoints therefore determined by the magnetic flux Φ through the area between the paths is given by: Slide 12: 12 Dong-In Chang, Gyong Luck Khym, Kicheon Kang, Yunchul Chung, Hu-Jong Lee, Minky Seo, Moty Heiblum, Diana Mahalu, Vladimir Umansky Nature Physics 4, 205 (2008) Aharonov-Bohm Oscillations in Semiconductor Quantum Rings : 13 Aharonov-Bohm Oscillations in Semiconductor Quantum Rings Now an international research team from the Nijmegen High Field Magnet Laboratory (the Netherlands), the Eindhoven University of Technology (the Netherlands), the University of Antwerp (Belgium), the University of Moldova (Moldova) and the the Institute of Microelectronics in Madrid (Spain) has succeeded to detect oscillatory currents carried by single electron states in a semiconductor quantum ring. These findings were published in the journal Physical Review Letters. You do not have the permission to view this presentation. In order to view it, please contact the author of the presentation.
Quantum Mechanics for Applied Physics ankush85 Download Post to : URL : Related Presentations : Share Add to Flag Embed Email Send to Blogs and Networks Add to Channel Uploaded from authorPOINT lite Insert YouTube videos in PowerPont slides with aS Desktop Copy embed code: Embed: Flash iPad Dynamic Copy Does not support media & animations Automatically changes to Flash or non-Flash embed WordPress Embed Customize Embed URL: Copy Thumbnail: Copy The presentation is successfully added In Your Favorites. Views: 414 Category: Education License: All Rights Reserved Like it (0) Dislike it (0) Added: September 04, 2009 This Presentation is Public Favorites: 1 Presentation Description No description available. Comments Posting comment... By: saydhameen (42 month(s) ago) please allow to download Saving..... Post Reply Close Saving..... Edit Comment Close By: saydhameen (42 month(s) ago) please allow to downlod Saving..... Post Reply Close Saving..... Edit Comment Close Premium member Presentation Transcript Quantum Mechanics for Applied Physics : Quantum Mechanics for Applied Physics Two levels system : 2 Two levels system | cb(t) | 2 = cos(ωt)2 where ω is the Rabi frequency Slide 3: 3 Slide 4: 4 Classical Electrodynamics : 5 micro/macroscopic electric field micro/macroscopic magnetic field charge/current density Constitutive equations Classical Electrodynamics Potentials Charge conservation polarization magnetization speed of light Energy & momentum : 6 Energy & momentum Point charge: , Lorentz force Energy balance in a space domain EM energy density Kinetic energy of charges Poynting’s energy flux vector using identity Electron in a Magnetic field : 7 Electron in a Magnetic field Quantization P change to Popand r to rop Wave function Lev_Davidovich_Landau Slide 8: 8 To actually solve Schrödinger’s equation for an electron confined to a plane in a uniform perpendicular magnetic field, it is convenient to use the Landau gauge. H commutes with px, so H and px have a common set of eigenstates, taking Landau Levels : 9 Landau Levels Example of quantization measurement Effects of Landau levels are only observed when the mean thermal energy is smaller than the energy level separation, , meaning low temperatures and strong magnetic fields Aharonov Bohm : 10 Aharonov Bohm The Aharonov-Bohm effect demonstrates that the electromagnetic potentials, rather than the electric and magnetic fields, are the fundamental quantities in quantum mechanics. The necessary conditions to observe the Aharonov-Bohm effect, i.e. a shift of the diffraction pattern that varies periodically with B, are: There must be at least two interfering alternatives for the particle to arrive at the detector, and At least two of these interfering alternatives must enclose a shielded magnetic field and must be topologically distinct. The animation shows the superposition of the waves for the case with (in blue) and without (in red) a magnetic field. Magnetic Aharonov Bohm effect : 11 Magnetic Aharonov Bohm effect Result of the requirement that quantum physics be invariant with respect to the gauge choice for the vector potential A. This implies that a particle with electric charge q traveling along some path P in a region with zero magnetic field must acquire a phase which is in si units: phase difference between any two paths with the same endpoints therefore determined by the magnetic flux Φ through the area between the paths is given by: Slide 12: 12 Dong-In Chang, Gyong Luck Khym, Kicheon Kang, Yunchul Chung, Hu-Jong Lee, Minky Seo, Moty Heiblum, Diana Mahalu, Vladimir Umansky Nature Physics 4, 205 (2008) Aharonov-Bohm Oscillations in Semiconductor Quantum Rings : 13 Aharonov-Bohm Oscillations in Semiconductor Quantum Rings Now an international research team from the Nijmegen High Field Magnet Laboratory (the Netherlands), the Eindhoven University of Technology (the Netherlands), the University of Antwerp (Belgium), the University of Moldova (Moldova) and the the Institute of Microelectronics in Madrid (Spain) has succeeded to detect oscillatory currents carried by single electron states in a semiconductor quantum ring. These findings were published in the journal Physical Review Letters.