Formalism and Interpretation in Quantum Theory1 1 Two Views of
... the basic properties of entangled states are in no way specifically or characteristically quantum-mechanical phenomena. Most of the serious interpretational issues confronting quantum theory arise precisely in connection with entangled states; thus, the stage is set to rehearse familiar arguments co ...
... the basic properties of entangled states are in no way specifically or characteristically quantum-mechanical phenomena. Most of the serious interpretational issues confronting quantum theory arise precisely in connection with entangled states; thus, the stage is set to rehearse familiar arguments co ...
(Dynamical) quantum typicality: What is it and what are its
... no attractive fixed point (Schroedinger equation) Schroedinger equation is no rate equation ...
... no attractive fixed point (Schroedinger equation) Schroedinger equation is no rate equation ...
Elementary Particle Mixing for Maximum Channel Capacity in Measured Decays
... In recent years the physics of the implied ensemble has been worked out by quantum information theorists. Channel capacity has been defined as a measure of the number of accessibly distinguishable classical states, and shown to be computable using the Holevo bound [3, 4]. In this paper, we adopt the ...
... In recent years the physics of the implied ensemble has been worked out by quantum information theorists. Channel capacity has been defined as a measure of the number of accessibly distinguishable classical states, and shown to be computable using the Holevo bound [3, 4]. In this paper, we adopt the ...
Quantum linear Boltzmann equation with finite intercollision time
... perfect diagonal in P储. Gradually, after many collisions, the state ˆ becomes a mixture of plane waves, no off-diagonal mechanism will be left at all. This result contradicts to what we have so far learned as QLBE. The art of deriving a plausible QLBE has always been about the nontrivial treatment ...
... perfect diagonal in P储. Gradually, after many collisions, the state ˆ becomes a mixture of plane waves, no off-diagonal mechanism will be left at all. This result contradicts to what we have so far learned as QLBE. The art of deriving a plausible QLBE has always been about the nontrivial treatment ...
probability in quantum mechanics
... field can be found limitingly close in towards a vortex centre. ...
... field can be found limitingly close in towards a vortex centre. ...
Nonlocal “realistic” Leggett models can be considered refuted by the
... According to the postulate of “nonlocal realism” all measurements A and B are determined by the “preexisting” properties (hidden variables) the particles carry [1, 5]. However, the individual B outcomes cannot be considered to be predetermined by the polarization vectors v the photons B carry when t ...
... According to the postulate of “nonlocal realism” all measurements A and B are determined by the “preexisting” properties (hidden variables) the particles carry [1, 5]. However, the individual B outcomes cannot be considered to be predetermined by the polarization vectors v the photons B carry when t ...
Rapid readout of a register of qubits using open loop... Joshua Combes , Aaron Denney , and Howard M. Wiseman
... In this section we derive the rate at which a continuous measurement extracts information from a quantum system for a reasonably general measurement model. The starting point for our analysis is the quantum trajectory description of the measurement process. The physics behind the quantum trajectory ...
... In this section we derive the rate at which a continuous measurement extracts information from a quantum system for a reasonably general measurement model. The starting point for our analysis is the quantum trajectory description of the measurement process. The physics behind the quantum trajectory ...
Quantum Geometry: a reunion of Physics and Math
... formula for the probability of this process. ...
... formula for the probability of this process. ...
