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Quantum channels and their capacities: An introduction
Quantum channels and their capacities: An introduction

... Φ(aρ1 + aρ2 ) = aΦ(ρ1 ) + bΦ(ρ2 ) =⇒ ...
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... • So Bell’s inequality must hold if we are to have one of these “it’s all built in (like classical correlations) but we just can’t see it yet” type of models that Einstein wanted. • But (for n along some directions) the quantum calculation violates Bell’s inequality. • Therefore, they can’t both be ...
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An Expert`s Approach to Solving Physics Problems

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4.1 Symmetry Geometry and measures

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Von Neumann algebra automorphisms and time

... a smooth positive (normalized) function on the phase space, which defines a statistical distribution in the sense of Gibbs [10]. In a conventional non-generally covariant theory, a hamiltonian H is given and the equilibrium thermal states are Gibbs states ρ = exp{−βH}. Notice that the information on ...
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... are re-written in the usual way of thermodynamics for indistinguishable particles. For the system of distinguishable particles, the “reduced” entropy S red instead of the original entropy S defines the thermodynamical variables of the system. Our presentation is somehow a straightforward way to just ...
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On Quantum Nonseparability - Philsci

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Physics Notes for Class 12 Chapter 12 Atoms

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... We call (6) the “effective” energy because it is really the energy of the analogue problem, and not the real problem. The true potential energy V (r, t) of the test particle is defined to be the amount of work we must supply to move the particle to its present location from some fixed reference point, ...
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... the words of someone else as their own. Plagiarism can be the deliberate use of a whole piece of another person’s writing, but more frequently it occurs when students fail to acknowledge and document sources from which they have taken material. Whenever the words, research or ideas of others are dir ...
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QUANTUM DOTS - Electrical and Computer Engineering

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T-symmetry

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