Quantum orders in an exact soluble model
... (FQH) states discovered in 1982[3, 4] opened a new chapter in condensed matter physics. The theory of phases and phase transitions entered into a new era. This is because all different FQH states have the same symmetry and hence cannot be described by the Landau’s theory. In 1989, it was realized th ...
... (FQH) states discovered in 1982[3, 4] opened a new chapter in condensed matter physics. The theory of phases and phase transitions entered into a new era. This is because all different FQH states have the same symmetry and hence cannot be described by the Landau’s theory. In 1989, it was realized th ...
Chapter04
... A and B are different operators that represent different observables, e. g., energy and angular momentum. If S are simultaneous eigenvectors of two or more linear operators representing observables, then these observables can be ...
... A and B are different operators that represent different observables, e. g., energy and angular momentum. If S are simultaneous eigenvectors of two or more linear operators representing observables, then these observables can be ...
Lecture 8: The fractional quantum Hall effect The fractional quantum
... The fractional quantum Hall effect: Laughlin wave function The fractional QHE is evidently prima facie impossible to obtain within an independentelectron picture, since it would appear to require that the extended states be only partially occupied and this would immediately lead to a nonzero value o ...
... The fractional quantum Hall effect: Laughlin wave function The fractional QHE is evidently prima facie impossible to obtain within an independentelectron picture, since it would appear to require that the extended states be only partially occupied and this would immediately lead to a nonzero value o ...
Classical analogy of Fano resonances
... The location of the resonant peaks corresponds to the real parts of the complex eigen-frequencies, ω̃1 and ω̃2 , which are determined from the vanishing condition of the denominator of equations (13) and (14). The imaginary part of the eigenfrequency specifies the width of the resonance, so as the s ...
... The location of the resonant peaks corresponds to the real parts of the complex eigen-frequencies, ω̃1 and ω̃2 , which are determined from the vanishing condition of the denominator of equations (13) and (14). The imaginary part of the eigenfrequency specifies the width of the resonance, so as the s ...
Experimental quantum teleportation articles
... can be fully characterized by its properties, which in classical physics can be determined by measurement. To make a copy of that object at a distant location one does not need the original parts and pieces— all that is needed is to send the scanned information so that it can be used for reconstruct ...
... can be fully characterized by its properties, which in classical physics can be determined by measurement. To make a copy of that object at a distant location one does not need the original parts and pieces— all that is needed is to send the scanned information so that it can be used for reconstruct ...
Gravitational Radiation:
... The lengthscale for significant conversion of EM wave energy into GW energy is equal to the radius of curvature of spacetime produced by the catalyzing DC magnetic field. ...
... The lengthscale for significant conversion of EM wave energy into GW energy is equal to the radius of curvature of spacetime produced by the catalyzing DC magnetic field. ...
MATH 32A: MIDTERM 1 REVIEW 1. Vectors 1. Let v = . a
... t = 0 or t = −1 (the line y = −x is an asymptote to the curve). So this is why setting y = tx allows us to parametrize the curve. When you parametrize a curve, it can be helpful to work out how an imaginary object travels along the curve as a function of the “time” t. This parametrization is a littl ...
... t = 0 or t = −1 (the line y = −x is an asymptote to the curve). So this is why setting y = tx allows us to parametrize the curve. When you parametrize a curve, it can be helpful to work out how an imaginary object travels along the curve as a function of the “time” t. This parametrization is a littl ...
Chapter 6 - MrCrabtreesScience
... to a dock. The boater steps out of the canoe at a velocity of 2.5m/s to the right. What velocity will the boat move to the left at? ...
... to a dock. The boater steps out of the canoe at a velocity of 2.5m/s to the right. What velocity will the boat move to the left at? ...
Chapter 21 The Electric Field 1: Discrete Charge Distributions
... equilateral triangle that has sides of length L as shown in Figure 21-38. A third point particle that has a charge equal to 2q sits at the apex of the triangle. Where must a fourth point particle that has a charge equal to q be placed in order that the electric field at the center of the triangle be ...
... equilateral triangle that has sides of length L as shown in Figure 21-38. A third point particle that has a charge equal to 2q sits at the apex of the triangle. Where must a fourth point particle that has a charge equal to q be placed in order that the electric field at the center of the triangle be ...
