Light-shift imbalance induced blockade of collective excitations beyond the lowest order
... use atomic ensembles as quantum bits. However, when an atomic ensemble is excited, by a laser beam matched to a two-level transition (or a Raman transition) for example, it leads to a cascade of many states as more and more photons are absorbed [R.H. Dicke, Phys. Rev. 93 (1954) 99]. In order to make ...
... use atomic ensembles as quantum bits. However, when an atomic ensemble is excited, by a laser beam matched to a two-level transition (or a Raman transition) for example, it leads to a cascade of many states as more and more photons are absorbed [R.H. Dicke, Phys. Rev. 93 (1954) 99]. In order to make ...
Titles and Abstracts
... arbitrary Gaussian states in the number basis are strictly decreasing functions of excitation number, and therefore no convex combination thereof can be proportional to a projection operator. We connect this observation with the construction of t-designs, important ensembles of states that reproduce ...
... arbitrary Gaussian states in the number basis are strictly decreasing functions of excitation number, and therefore no convex combination thereof can be proportional to a projection operator. We connect this observation with the construction of t-designs, important ensembles of states that reproduce ...
The Born rule and its interpretation
... simply a consequence of the fact that we describe the experiment in terms of classical physics; they do not depend in detail on the observer. One may call them subjective, in that they reflect our incomplete knowledge of the world.” (Heisenberg [4], pp. 53–54) In other words, one cannot say that the ...
... simply a consequence of the fact that we describe the experiment in terms of classical physics; they do not depend in detail on the observer. One may call them subjective, in that they reflect our incomplete knowledge of the world.” (Heisenberg [4], pp. 53–54) In other words, one cannot say that the ...
chapter 7 part 1
... high (and thick) potential walls – impenetrable – just a model that does not really correspond to reality at wave function (evanescent wave) always leaks into barrier – chapter 6 tunneling- and may be picked up at the other side, become a traveling wave again, i.e. a particle that can move so U(x,y, ...
... high (and thick) potential walls – impenetrable – just a model that does not really correspond to reality at wave function (evanescent wave) always leaks into barrier – chapter 6 tunneling- and may be picked up at the other side, become a traveling wave again, i.e. a particle that can move so U(x,y, ...
