Quantum Theory: a Pragmatist Approach
... account of probability! Of course, he would insist that different persons may, and often do, hold different beliefs, which makes probability personalist—varying from person to person—and to that extent subjective. On other “subjectivist” views, an agent’s degrees of belief count as probabilities onl ...
... account of probability! Of course, he would insist that different persons may, and often do, hold different beliefs, which makes probability personalist—varying from person to person—and to that extent subjective. On other “subjectivist” views, an agent’s degrees of belief count as probabilities onl ...
Seeing a single photon without destroying it
... In our set-up26±28, a thermal beam of rubidium atoms is velocityselected by laser-induced optical pumping. The atoms are then prepared in the Rydberg circular state with principal quantum number 50 (level g) or 51 (level e). The e ) g transition is resonant at 51.1 GHz. Circular Rydberg states29,30 ...
... In our set-up26±28, a thermal beam of rubidium atoms is velocityselected by laser-induced optical pumping. The atoms are then prepared in the Rydberg circular state with principal quantum number 50 (level g) or 51 (level e). The e ) g transition is resonant at 51.1 GHz. Circular Rydberg states29,30 ...
7 Quantum Computing Applications of Genetic Programming
... the classical bit. A classical system of n bits is at any time in one of 2n states. Quantum mechanics tells us, however, that we must think of a quantum system of n qubits as having a distinct probability of “being in” (that is, “being found in upon measurement”) each of the 2n classical states at a ...
... the classical bit. A classical system of n bits is at any time in one of 2n states. Quantum mechanics tells us, however, that we must think of a quantum system of n qubits as having a distinct probability of “being in” (that is, “being found in upon measurement”) each of the 2n classical states at a ...
Quantum heat engine with multilevel quantum systems
... changes between ⌬h and ⌬l. For such a QHE, the system couples to the bath for a sufficiently long time until they reach the thermal equilibrium state. Then positive work can be performed when and only when Th ⬎ Tl共⌬h / ⌬l兲 共condition I兲. This result implies a broad validity of the second law and sho ...
... changes between ⌬h and ⌬l. For such a QHE, the system couples to the bath for a sufficiently long time until they reach the thermal equilibrium state. Then positive work can be performed when and only when Th ⬎ Tl共⌬h / ⌬l兲 共condition I兲. This result implies a broad validity of the second law and sho ...
1 - Hal-SHS
... would be calculable theoretically only with quantum field theory, shortly after the quantum mechanics formulation was obtained 18). The evidence for attributing radiation (defined by its frequency and wave length) both an energy and a momentum (property of a particle), seemed to show that atomic pro ...
... would be calculable theoretically only with quantum field theory, shortly after the quantum mechanics formulation was obtained 18). The evidence for attributing radiation (defined by its frequency and wave length) both an energy and a momentum (property of a particle), seemed to show that atomic pro ...
The Emergence and Interpretation of Probability
... which global existence and uniqueness can be proved for almost all initial conditions. Relevant to us later, the theory is also time-reversal invariant and (for most states) Poincaré recurrent. That is, for every history there is also the time-reversed history given by the transformations t→-t and Ψ ...
... which global existence and uniqueness can be proved for almost all initial conditions. Relevant to us later, the theory is also time-reversal invariant and (for most states) Poincaré recurrent. That is, for every history there is also the time-reversed history given by the transformations t→-t and Ψ ...
![Probability in Bohmian Mechanics[1]](http://s1.studyres.com/store/data/001567507_1-29d8fd2fe0d2e1e754834ae0307e0c62-300x300.png)
Probability in Bohmian Mechanics[1]
... then advertised as simply the problem of finding some reason to think (q,t) = |(q,t)|2 at some time or other, for one is then guaranteed that it will always hold. However, despite being repeated many times, this way of putting matters is misleading.4 What we want explained is why a system of parti ...
... then advertised as simply the problem of finding some reason to think (q,t) = |(q,t)|2 at some time or other, for one is then guaranteed that it will always hold. However, despite being repeated many times, this way of putting matters is misleading.4 What we want explained is why a system of parti ...
Document
... In this talk, the basic toolbox of the Innsbruck quantum information processor based on a string of trapped Ca+ ions will be reviewed. For quantum information science, the toolbox operations are used to encode one logical qubit in entangled states distributed over seven trapped-ion qubits. We demons ...
... In this talk, the basic toolbox of the Innsbruck quantum information processor based on a string of trapped Ca+ ions will be reviewed. For quantum information science, the toolbox operations are used to encode one logical qubit in entangled states distributed over seven trapped-ion qubits. We demons ...