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Space, time and Riemann zeros (Madrid, 2013)

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... and 4. We use elements from the set up in the paper by Haven (2015). For a lot more detail, the paper by Nelson (1966) is the essential reference. The book by Paul and Baschnagel (1999) is also an excellent source (see also Haven and Khrennikov, 2013). We will follow, as in the paper by Haven (2015) ...
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... without requiring either assumption. The entanglement of particles with a rest mass shall be treated separately below (as it requires an additional premise). But the entanglement of all other particles (collectively identifiable on the current Standard Model as massless bosons, the most well known o ...
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The weak-coupling limit of large classical and quantum systems

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... frequency is greater than a threshold value. An airbag occurs between the surface and the drop, does not permitting it to mix with the liquid. However the droplet begins to move on the surface when the oscillating frequency of the bath exceeds a second threshold value. In this case an attenuating Fa ...
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... since in that approximation both H and h are equivalent to H, [neglecting terms The rigorous path-integral definition described in this paper enables variable transformations (e.g. , canoniSuch a poscal transformations) to be examined much more critically than in the usual formal formulation. sibili ...
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7 Commutators, Measurement and The Uncertainty Principle

... if the potential U (x) has some symmetry. For example, if U (x) = f (r) is spherically symmetric, then we know that the total angular momentum L is conserved. In Quantum Mechanics, conservation laws are expressed as the vanishing of the observable with the Hamiltonian, i.e. if Ô commutes with Ĥ [O ...
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Interference and Coulomb correlation effects in P. T
Interference and Coulomb correlation effects in P. T

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Propagator

In quantum mechanics and quantum field theory, the propagator gives the probability amplitude for a particle to travel from one place to another in a given time, or to travel with a certain energy and momentum. In Feynman diagrams, which calculate the rate of collisions in quantum field theory, virtual particles contribute their propagator to the rate of the scattering event described by the diagram. They also can be viewed as the inverse of the wave operator appropriate to the particle, and are therefore often called Green's functions.
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