Program: DYNQUA - Toulon University - February
... distances. In the case of 1-dimensional operators, these correlations depend on the structure of the energy shell of the unperturbed operator (a finite set of points), and of the type of perburbation (random matrix vs. random potential), but otherwise enjoy a form of universality, where the central ...
... distances. In the case of 1-dimensional operators, these correlations depend on the structure of the energy shell of the unperturbed operator (a finite set of points), and of the type of perburbation (random matrix vs. random potential), but otherwise enjoy a form of universality, where the central ...
Quine`s Holism and Quantum Holism
... Quine’s holism and holism in quantum physics are usually considered to be two different issues which merely have the name “holism” in common. My aim, by contrast, is to build a bridge between these two sorts of holism. This paper is an argument for three theses: 1) The discussion on holism and other ...
... Quine’s holism and holism in quantum physics are usually considered to be two different issues which merely have the name “holism” in common. My aim, by contrast, is to build a bridge between these two sorts of holism. This paper is an argument for three theses: 1) The discussion on holism and other ...
A limit relation for quantum entropy, and channel capacity per unit cost
... The quantum formulation includes the case where both and are diagonal matrices. This will be referred to as the classical case. If and commute, then in an appropriate basis both of them will be diagonal. Apparently no exact proof of (1) has been published even for the classical case, althoug ...
... The quantum formulation includes the case where both and are diagonal matrices. This will be referred to as the classical case. If and commute, then in an appropriate basis both of them will be diagonal. Apparently no exact proof of (1) has been published even for the classical case, althoug ...
The principle of a finite density of information
... understand what entanglement is, one must apply the superposition principle again, but this time to pairs of systems. For instance if systems A and B may be in state uu, meaning that both are in state u, or in state vv, meaning that both are in state v, then the state λ(uu) + µ(vv) is also allowed. ...
... understand what entanglement is, one must apply the superposition principle again, but this time to pairs of systems. For instance if systems A and B may be in state uu, meaning that both are in state u, or in state vv, meaning that both are in state v, then the state λ(uu) + µ(vv) is also allowed. ...
powerpoint
... which is quantized. However, the effect of quantization will become smaller as L → ∞. In a macroscopic scale (L very large) or for a free space (L = ∞), energy and energy differences become continuous (quantum classical correspondence). ...
... which is quantized. However, the effect of quantization will become smaller as L → ∞. In a macroscopic scale (L very large) or for a free space (L = ∞), energy and energy differences become continuous (quantum classical correspondence). ...
