circles and probability
... the one you're used to, y = ax2 + bx + c — unless the quadratic is "sideways", in which case the equation will look something like x = ay2 + by + c. The important difference in the two equations is in which variable is squared: for regular (vertical) parabolas, the x part is squared; for sideways (h ...
... the one you're used to, y = ax2 + bx + c — unless the quadratic is "sideways", in which case the equation will look something like x = ay2 + by + c. The important difference in the two equations is in which variable is squared: for regular (vertical) parabolas, the x part is squared; for sideways (h ...
lecture notes on statistical mechanics - MSU Physics
... to understand why all states are equally populated from the perspective of dynamics. The Ergodic theorem is built on the symmetry of time-reversal, i.e., the rate at which one changes from state i to state j is the same as the rate at which one changes from state j to state i. Here, we can consider ...
... to understand why all states are equally populated from the perspective of dynamics. The Ergodic theorem is built on the symmetry of time-reversal, i.e., the rate at which one changes from state i to state j is the same as the rate at which one changes from state j to state i. Here, we can consider ...
m2_MJC
... car travelling at 100 km.h-1 to being hit by a cricket ball also travelling at 100 km.h-1. The description of events like the impacts illustrated in figure (1) are made more precise by defining a quantity called the linear momentum and velocity ...
... car travelling at 100 km.h-1 to being hit by a cricket ball also travelling at 100 km.h-1. The description of events like the impacts illustrated in figure (1) are made more precise by defining a quantity called the linear momentum and velocity ...
Linear Momentum, Impulse, Conservation of Momentum
... car travelling at 100 km.h-1 to being hit by a cricket ball also travelling at 100 km.h-1. The description of events like the impacts illustrated in figure (1) are made more precise by defining a quantity called the linear momentum and velocity ...
... car travelling at 100 km.h-1 to being hit by a cricket ball also travelling at 100 km.h-1. The description of events like the impacts illustrated in figure (1) are made more precise by defining a quantity called the linear momentum and velocity ...
Another version - Scott Aaronson
... To me, it seems tied to the idea that a quantum computer could just “try every possible answer in parallel” But that’s not how quantum computing works! You need to choreograph an interference pattern, where the unwanted paths cancel The miracle, I’d say, is that this trick yields a speedup for any c ...
... To me, it seems tied to the idea that a quantum computer could just “try every possible answer in parallel” But that’s not how quantum computing works! You need to choreograph an interference pattern, where the unwanted paths cancel The miracle, I’d say, is that this trick yields a speedup for any c ...
Full text
... the so called superradiant phase. Later Emary and Brandes demonstrated the quantum phase transition (QPT) for DM without RWA using the Holstein-Primakoff (HP) series expansion of the Dicke Hamiltonian truncated to second order in terms of the ratio between the number of excited atoms to the total nu ...
... the so called superradiant phase. Later Emary and Brandes demonstrated the quantum phase transition (QPT) for DM without RWA using the Holstein-Primakoff (HP) series expansion of the Dicke Hamiltonian truncated to second order in terms of the ratio between the number of excited atoms to the total nu ...
( ) New Faculty Bruce Knuteson
... of particle physics as the correct theory of fundamental interactions down to a distance scale of 10 −18 meters. Despite this remarkable success, inadequacies inherent in the theory suggest that a qualitatively new description is required at energies soon to be probed by our accelerators. Lacking st ...
... of particle physics as the correct theory of fundamental interactions down to a distance scale of 10 −18 meters. Despite this remarkable success, inadequacies inherent in the theory suggest that a qualitatively new description is required at energies soon to be probed by our accelerators. Lacking st ...
relativistic field theory
... in general. The reason for this state of affairs is not far to find: it was clearly articulated more than ninety years ago by Hermann Minkowski, who in had occasion to speak as follows:1 “The views of space and time which I wish to lay before you have sprung from the soil of experimental physics, ...
... in general. The reason for this state of affairs is not far to find: it was clearly articulated more than ninety years ago by Hermann Minkowski, who in had occasion to speak as follows:1 “The views of space and time which I wish to lay before you have sprung from the soil of experimental physics, ...
Particle creation by black holes | SpringerLink
... classical General Relativity one has a classical metric which obeys the Einstein equations, the right hand side of which is supposed to be the energy momentum tensor of the classical matter fields. However, although it may be reasonable to ignore quantum gravitational effects on the grounds that the ...
... classical General Relativity one has a classical metric which obeys the Einstein equations, the right hand side of which is supposed to be the energy momentum tensor of the classical matter fields. However, although it may be reasonable to ignore quantum gravitational effects on the grounds that the ...
Definition of the spin current: The angular spin current and its
... charge current density ជj e共r , t兲 = Re关⌿†共r , t兲evជ ⌿共r , t兲兴 and its continuity equation 共d / dt兲e共r , t兲 + · ជj e共r , t兲 = 0 is well known in physics. Here ⌿共r , t兲 is the electronic wave function, vជ = ṙ is the velocity operator, and e共r , t兲 = e⌿†⌿ is the charge density. This continuity eq ...
... charge current density ជj e共r , t兲 = Re关⌿†共r , t兲evជ ⌿共r , t兲兴 and its continuity equation 共d / dt兲e共r , t兲 + · ជj e共r , t兲 = 0 is well known in physics. Here ⌿共r , t兲 is the electronic wave function, vជ = ṙ is the velocity operator, and e共r , t兲 = e⌿†⌿ is the charge density. This continuity eq ...