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... relevant to the work described here. In particular, one key constraint in quantum computation is the no cloning theorem [33], which states that a superposition state cannot be perfectly copied from one qubit to another qubit, without destroying the first one. Thus, in order to use the state of a qub ...
... relevant to the work described here. In particular, one key constraint in quantum computation is the no cloning theorem [33], which states that a superposition state cannot be perfectly copied from one qubit to another qubit, without destroying the first one. Thus, in order to use the state of a qub ...
Quantum gases in optical lattices
... the same and does not fluctuate. How- (a) Controlled interactions between atoms on the lab. The ETH team has compared ever, this means that the phase coherence different lattice sites are possible with the help of the oscillation frequencies of an axial lattice potentials. In such a between atoms on ...
... the same and does not fluctuate. How- (a) Controlled interactions between atoms on the lab. The ETH team has compared ever, this means that the phase coherence different lattice sites are possible with the help of the oscillation frequencies of an axial lattice potentials. In such a between atoms on ...
What Makes a Classical Concept Classical? Toward a
... -3it to be a vindication of Oxford ordinary language philosophy (Bergstein 1972); and still others see it as having an “affinity” with P. F. Strawson's argument for the indispensability of the common-sense conceptual scheme (Murdoch 1987). In the end, however, all of these interpretations are equal ...
... -3it to be a vindication of Oxford ordinary language philosophy (Bergstein 1972); and still others see it as having an “affinity” with P. F. Strawson's argument for the indispensability of the common-sense conceptual scheme (Murdoch 1987). In the end, however, all of these interpretations are equal ...
Quantum Mechanics - Home Page for Richard Fitzpatrick
... complete set of probabilities. This condition is equivalent to the self-evident statement that an observation of a system must definitely result in one of its possible outcomes. There is another way in which we can combine probabilities. Suppose that we make an observation on a system picked at rand ...
... complete set of probabilities. This condition is equivalent to the self-evident statement that an observation of a system must definitely result in one of its possible outcomes. There is another way in which we can combine probabilities. Suppose that we make an observation on a system picked at rand ...
Quantum random walks and their boundaries
... Random walks form an important part of classical probability theory [26, 28] and have remarkable applications to group theory, geometry and rigidity theory [16, 15, 7, 25]. Various results of the corresponding non-commutative theory can be traced back to the 70s. Notwithstanding the vast literature ...
... Random walks form an important part of classical probability theory [26, 28] and have remarkable applications to group theory, geometry and rigidity theory [16, 15, 7, 25]. Various results of the corresponding non-commutative theory can be traced back to the 70s. Notwithstanding the vast literature ...
Program and Booklet - Fakultät für Mathematik
... Quantum computation is standardly assumed to happen on a definite causal structure, where the order of the gates in a circuit is fixed in advance and is independent of the states. However, the interplay between general relativity and quantum mechanics might require to consider more general situation ...
... Quantum computation is standardly assumed to happen on a definite causal structure, where the order of the gates in a circuit is fixed in advance and is independent of the states. However, the interplay between general relativity and quantum mechanics might require to consider more general situation ...
Document
... Allowed values for K and J: both must, by conditions of quantum mechanics, be integral or zero. The total angular momentum can be as large as we like – i.e., (except that a real molecule will be disrupted at very high rotational speeds) Once we have chosen J, however, K is more limited. ...
... Allowed values for K and J: both must, by conditions of quantum mechanics, be integral or zero. The total angular momentum can be as large as we like – i.e., (except that a real molecule will be disrupted at very high rotational speeds) Once we have chosen J, however, K is more limited. ...
Tutorial 9 - UBC Physics
... f) lf the initial light has photons with a random assortment of polarizations, we can show that the average probability of passing though the first polarizer is t/2 (can you prove this?). ln parts c and e, you have calculated the probability for a photon that has passed through the first polarizer ...
... f) lf the initial light has photons with a random assortment of polarizations, we can show that the average probability of passing though the first polarizer is t/2 (can you prove this?). ln parts c and e, you have calculated the probability for a photon that has passed through the first polarizer ...