Phase-controlled localization and directed
... both have also been adopted to produce the exact solutions for a phase controllable lattice system [26] or for an analytically solvable two-level system [27, 45]. The adjustments of driving parameters can be performed in a nonadiabatic [23, 37] or adiabatic manner [46, 47]. On the other hand, the di ...
... both have also been adopted to produce the exact solutions for a phase controllable lattice system [26] or for an analytically solvable two-level system [27, 45]. The adjustments of driving parameters can be performed in a nonadiabatic [23, 37] or adiabatic manner [46, 47]. On the other hand, the di ...
CHARGE TO MAGNETIC FLUX RATIOS
... references, half levels may be filled separately and observed experimentally. The number ν is an integer if the highest full level is a complete level, a half integer if the highest full level is a half level and zero if the only full level is the non degenerate first level. Since there is the same ...
... references, half levels may be filled separately and observed experimentally. The number ν is an integer if the highest full level is a complete level, a half integer if the highest full level is a half level and zero if the only full level is the non degenerate first level. Since there is the same ...
The Helmholtz Function
... G = -W(other), so W(other) (Gi Gf ) Gf - Gi = -W (other) or The change in the Gibbs function gives the maximum energy that can be freed in an isothermal, isobaric process and made available for non-mechanical work. For this reason one often speaks of the Gibbs free energy. This can be confusing ...
... G = -W(other), so W(other) (Gi Gf ) Gf - Gi = -W (other) or The change in the Gibbs function gives the maximum energy that can be freed in an isothermal, isobaric process and made available for non-mechanical work. For this reason one often speaks of the Gibbs free energy. This can be confusing ...
5. Chern-Simons Theories
... again, if we identify k = e2 ⌫/~ then this is precisely the result we get had we kept ⌫ Landau levels filled while varying B(x). We see that the Chern-Simons term captures the basic physics of the integer quantum Hall e↵ect, but only if we identify the level k = e2 ⌫/~. But this is very restrictive ...
... again, if we identify k = e2 ⌫/~ then this is precisely the result we get had we kept ⌫ Landau levels filled while varying B(x). We see that the Chern-Simons term captures the basic physics of the integer quantum Hall e↵ect, but only if we identify the level k = e2 ⌫/~. But this is very restrictive ...
Essentials of Modern Physics
... (a) change the subject of an equation. Most relevant equations involve only the simpler operations but may include positive and negative indices and square roots (b) solve simple algebraic equations. Most relevant equations are linear but some may involve inverse and inverse square relationships. Li ...
... (a) change the subject of an equation. Most relevant equations involve only the simpler operations but may include positive and negative indices and square roots (b) solve simple algebraic equations. Most relevant equations are linear but some may involve inverse and inverse square relationships. Li ...
Effective Field Theories for Topological states of Matter
... but do carry information about topology, and also about excitations at the boundaries of the system. Typical examples are the Wen-Zee Chern-Simons theories for quantum Hall liquids[13, 14] and the BF-theories for superconductors and topological insulators[15, 16]. The third type, the effective actio ...
... but do carry information about topology, and also about excitations at the boundaries of the system. Typical examples are the Wen-Zee Chern-Simons theories for quantum Hall liquids[13, 14] and the BF-theories for superconductors and topological insulators[15, 16]. The third type, the effective actio ...
The space group classification of topological band insulators arXiv
... Topological phases of free fermionic matter are in general characterized by an insulating gap in the bulk and protected gapless modes on the boundary of the system[1, 2]. Integer quantum Hall states represent first examples of topologically protected phases in absence of any symmetries with the top ...
... Topological phases of free fermionic matter are in general characterized by an insulating gap in the bulk and protected gapless modes on the boundary of the system[1, 2]. Integer quantum Hall states represent first examples of topologically protected phases in absence of any symmetries with the top ...
electric potential
... function of r The electric field is a function of r2 The effect of a charge on the space surrounding it: The charge sets up a vector electric field which is related to the force The charge sets up a scalar potential which is related to the energy ...
... function of r The electric field is a function of r2 The effect of a charge on the space surrounding it: The charge sets up a vector electric field which is related to the force The charge sets up a scalar potential which is related to the energy ...
How to realize a universal quantum gate with trapped ions
... quantum games. As in a classical computer, errors will necessarily occur. Although the nature of errors is different in quantum mechanical and in classical computers, algorithms have been developed which can correct qubit errors [5, 6]. World-wide efforts aim at a scalable realization of a QC [7]. A ...
... quantum games. As in a classical computer, errors will necessarily occur. Although the nature of errors is different in quantum mechanical and in classical computers, algorithms have been developed which can correct qubit errors [5, 6]. World-wide efforts aim at a scalable realization of a QC [7]. A ...
Chapter 15
... particles in a solid, we say that the entropy is low. At any given temperature, a solid will have a lower entropy than a gas, because individual molecules in the gaseous state are moving randomly, while individual molecules in a solid are constrained in place. Entropy is important because it determi ...
... particles in a solid, we say that the entropy is low. At any given temperature, a solid will have a lower entropy than a gas, because individual molecules in the gaseous state are moving randomly, while individual molecules in a solid are constrained in place. Entropy is important because it determi ...
Zeeman Effect - Lab exercises 24
... The splitting can be observed by electronic transitions. The detection of the splitting requires the dispersion of the emitted light by usage of e.g. a prism. Thus the components can be found separately. The Zeeman splitting is rather small that’s why a high resolution is needed which is realized in ...
... The splitting can be observed by electronic transitions. The detection of the splitting requires the dispersion of the emitted light by usage of e.g. a prism. Thus the components can be found separately. The Zeeman splitting is rather small that’s why a high resolution is needed which is realized in ...