people.ysu.edu
... you will always measure a discrete value that is an eigenvalue of the observable. You can have one Barium atom. Or one Yterbium atom. Your state can be an admixture of the two, but it is not real to find for a single measurement an atom that is some combination of the two. ...So if it was a mixed st ...
... you will always measure a discrete value that is an eigenvalue of the observable. You can have one Barium atom. Or one Yterbium atom. Your state can be an admixture of the two, but it is not real to find for a single measurement an atom that is some combination of the two. ...So if it was a mixed st ...
Posterior distributions on certain parameter spaces obtained by using group theoretic methods adopted from quantum physics
... orthogonal real 3 × 3 matrices SO(3). The set of left cosets SO(3)/SO(2) can be put into one-to-one correspondence with the unit two-sphere. ...
... orthogonal real 3 × 3 matrices SO(3). The set of left cosets SO(3)/SO(2) can be put into one-to-one correspondence with the unit two-sphere. ...
Why Quantum Theory? Lucien Hardy November 13, 2001 Centre for Quantum Computation,
... of quantum theory. It is rather striking that the difference between classical probability theory and quantum theory is just one word. A few comments on these axioms are appropriate here. We can think of any probability theory as a structure. This structure, however, has no physical meaning unless ...
... of quantum theory. It is rather striking that the difference between classical probability theory and quantum theory is just one word. A few comments on these axioms are appropriate here. We can think of any probability theory as a structure. This structure, however, has no physical meaning unless ...
Diverging equilibration times in long
... Generalizations.—To keep the presentation simple, the above exposition had been restricted to a onedimensional lattice and power law interactions ǫ(j) = j −α , but several generalizations are straightforward. In fact, only the large-j asymptotic behavior of ǫ(j) is relevant for the proof of Proposit ...
... Generalizations.—To keep the presentation simple, the above exposition had been restricted to a onedimensional lattice and power law interactions ǫ(j) = j −α , but several generalizations are straightforward. In fact, only the large-j asymptotic behavior of ǫ(j) is relevant for the proof of Proposit ...
