 
									
								
									The Wilsonian Revolution in Statistical Mechanics and Quantum
									
... fails near phase transitions, where fluctuations exist at all scales and the process of averaging proceeds ad infinitum; to treat these requires new insights and techniques embodied in Wilson’s renormalization group, as we will detail below. Let us return to the ferromagnets to illustrate Landau’s m ...
                        	... fails near phase transitions, where fluctuations exist at all scales and the process of averaging proceeds ad infinitum; to treat these requires new insights and techniques embodied in Wilson’s renormalization group, as we will detail below. Let us return to the ferromagnets to illustrate Landau’s m ...
									5 The Physics of Rotating Bodies
									
... for the precessional angular velocity of the gyroscope. Confirm the concept of gyroscopic precession in the following experiment. First, suspend a non-spinning gyroscope by its string and handle from one of the small cranes attached to the lab tables. Add a hanger and weights to the loop of string at ...
                        	... for the precessional angular velocity of the gyroscope. Confirm the concept of gyroscopic precession in the following experiment. First, suspend a non-spinning gyroscope by its string and handle from one of the small cranes attached to the lab tables. Add a hanger and weights to the loop of string at ...
									quantum computer - Caltech Particle Theory
									
... Spectacular quantum speedups seem to be possible only for problems with special structure, not for NP-complete problems like 3-SAT. (Quantum physics speeds up unstructured search quadratically, not exponentially.) ...
                        	... Spectacular quantum speedups seem to be possible only for problems with special structure, not for NP-complete problems like 3-SAT. (Quantum physics speeds up unstructured search quadratically, not exponentially.) ...
									Spontaneous persistent currents in a quantum spin Hall insulator D. Soriano
									
... Ordered electronic phases can emerge in condensed matter with properties fundamentally different from those of the constituent atoms. Two main different scenarios are known that result in the emergence of nontrivial electronic order. On one side, spontaneous symmetry breaking driven by manybody inte ...
                        	... Ordered electronic phases can emerge in condensed matter with properties fundamentally different from those of the constituent atoms. Two main different scenarios are known that result in the emergence of nontrivial electronic order. On one side, spontaneous symmetry breaking driven by manybody inte ...
									A quantum model for the stock market
									
... mass, length and currency, is different from the real mass, it does not affect the calculation of the wave function which is non-dimensional and we still call it mass in this paper. It should be an intrinsic property and represents the inertia of a stock. When the stock has a bigger mass, its price ...
                        	... mass, length and currency, is different from the real mass, it does not affect the calculation of the wave function which is non-dimensional and we still call it mass in this paper. It should be an intrinsic property and represents the inertia of a stock. When the stock has a bigger mass, its price ...
									Quantum-teleportation benchmarks for independent and identically
									
... is well approximated by a simpler Gaussian shift model, N := {N (u,I −1 (θ0 )) : u ∈ Rk }, where u ∈ Rk is the local unknown parameter of the distribution, and I −1 (θ0 ) is the inverse Fisher information matrix at θ0 . Note that this approximation holds only locally, reflecting the intrinsic uncert ...
                        	... is well approximated by a simpler Gaussian shift model, N := {N (u,I −1 (θ0 )) : u ∈ Rk }, where u ∈ Rk is the local unknown parameter of the distribution, and I −1 (θ0 ) is the inverse Fisher information matrix at θ0 . Note that this approximation holds only locally, reflecting the intrinsic uncert ...
									Chapter 5
									
... Figure 5.4-8 A point mass m and a distributed mass M are rotating at a uniform angular velocity . The linear momentum of a mass m moving in the x direction with a velocity Vx is mVx. The angular momentum (L) of a point mass m rotating with an angular velocity  rad/s in an arc having a radius of c ...
                        	... Figure 5.4-8 A point mass m and a distributed mass M are rotating at a uniform angular velocity . The linear momentum of a mass m moving in the x direction with a velocity Vx is mVx. The angular momentum (L) of a point mass m rotating with an angular velocity  rad/s in an arc having a radius of c ...
									Conservation of Momentum Notes
									
... • Elastic Collisions: Two or more objects collide, bounce (don’t stick together), and kinetic energy is conserved. • An ideal situation that is often never quite reached… billiard ball collisions are often used as an example of elastic collisions. • Kinetic (motion) energy is conserved: • KE1 + KE2 ...
                        	... • Elastic Collisions: Two or more objects collide, bounce (don’t stick together), and kinetic energy is conserved. • An ideal situation that is often never quite reached… billiard ball collisions are often used as an example of elastic collisions. • Kinetic (motion) energy is conserved: • KE1 + KE2 ...
									Topological quantum field theory
									
... of connections) and to study these by standard linear methods (homology, etc.). In other words we use quantum field theory as a refined tool to study low-dimensional manifolds. Now quantum field theories have, because of the difficulties involved in constructing them, often been described axiomatica ...
                        	... of connections) and to study these by standard linear methods (homology, etc.). In other words we use quantum field theory as a refined tool to study low-dimensional manifolds. Now quantum field theories have, because of the difficulties involved in constructing them, often been described axiomatica ...
									11-1 Angular Momentum—Objects Rotating About a Fixed Axis
									
... A simple clutch consists of two cylindrical plates that can be pressed together to connect two sections of an axle, as needed, in a piece of machinery. The two plates have masses MA = 6.0 kg and MB = 9.0 kg, with equal radii R0 = 0.60 m. They are initially separated. Plate MA is accelerated from res ...
                        	... A simple clutch consists of two cylindrical plates that can be pressed together to connect two sections of an axle, as needed, in a piece of machinery. The two plates have masses MA = 6.0 kg and MB = 9.0 kg, with equal radii R0 = 0.60 m. They are initially separated. Plate MA is accelerated from res ...
 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									 
									