arXiv:1601.06197v1 [cond-mat.quant
... significantR many-body corrections once the interaction energy g k.p dk nk of particles with momenta below a given scale p exceeds the kinetic energy at that scale, and these are indeed the prevailing conditions when phase coherence emerges and the condensate begins to grow [19]. In a series of pape ...
... significantR many-body corrections once the interaction energy g k.p dk nk of particles with momenta below a given scale p exceeds the kinetic energy at that scale, and these are indeed the prevailing conditions when phase coherence emerges and the condensate begins to grow [19]. In a series of pape ...
Non-Abelian Anyons and Topological Quantum Computation
... is anti-symmetric. One cannot overemphasize, of course, the importance of the symmetry of the wavefunction, which is the root of the Pauli principle, superfluidity, the metallic state, Bose-Einstein condensation, and a long list of other phenomena. The limitation to one of two possible types of quan ...
... is anti-symmetric. One cannot overemphasize, of course, the importance of the symmetry of the wavefunction, which is the root of the Pauli principle, superfluidity, the metallic state, Bose-Einstein condensation, and a long list of other phenomena. The limitation to one of two possible types of quan ...
Paper - College of the Redwoods
... down both sides of the hoop. The second example is the same but the velocity of the bead has died down. When we increase the value of γ, the bead is restricted to one side of the hoop, but the area in which it moves gets much smaller as the angular velocity increases. It gets to a point where we can ...
... down both sides of the hoop. The second example is the same but the velocity of the bead has died down. When we increase the value of γ, the bead is restricted to one side of the hoop, but the area in which it moves gets much smaller as the angular velocity increases. It gets to a point where we can ...
draft
... Finally, an operator concave function f is a function such that −f is operator convex. In all three cases it is assumed that the inequalities hold for all matrix sizes (so that an operator monotone function is always monotone in the ordinary sense, but the converse may fail). 1 The definitions are s ...
... Finally, an operator concave function f is a function such that −f is operator convex. In all three cases it is assumed that the inequalities hold for all matrix sizes (so that an operator monotone function is always monotone in the ordinary sense, but the converse may fail). 1 The definitions are s ...
Simple Nature
... concept, they began looking for a way to define mass in terms of a definite measuring procedure. If they tried such a procedure, and the result was that it led to nonconservation of mass, then they would throw it out and try a different procedure. For instance, we might be tempted to define mass usi ...
... concept, they began looking for a way to define mass in terms of a definite measuring procedure. If they tried such a procedure, and the result was that it led to nonconservation of mass, then they would throw it out and try a different procedure. For instance, we might be tempted to define mass usi ...
Markov property in non-commutative probability
... often called density matrix. From the quantum theoretical point of view the selfadjoint elements of B(H) are identified with physical observables, while state φ represents the state of a physical system. It is a natural question, that how can we generalize the concept of Markovianity in the non-comm ...
... often called density matrix. From the quantum theoretical point of view the selfadjoint elements of B(H) are identified with physical observables, while state φ represents the state of a physical system. It is a natural question, that how can we generalize the concept of Markovianity in the non-comm ...
