Heralded Single-Magnon Quantum Memory for Photon Polarization States
... pumping period of op ¼ 3L =2 ¼ 3 s, such that the ensembles are interchanged at every trial, which reduces population imbalance between jg i. The atomic-spin precession and the efficiency of the optical pumping are monitored via resonator transmission ^ polarized beam. In the frame of a weak, li ...
... pumping period of op ¼ 3L =2 ¼ 3 s, such that the ensembles are interchanged at every trial, which reduces population imbalance between jg i. The atomic-spin precession and the efficiency of the optical pumping are monitored via resonator transmission ^ polarized beam. In the frame of a weak, li ...
Algebraic approach to interacting quantum systems
... of complex phenomena exhibited by Nature exceeds our ability to explain them, in part, because the whole is not necessarily the sum of its parts [1] and thus typical perturbation-like-theory arguments or standard mathematical techniques are not appropriate to disentangle its mysteries. In this paper ...
... of complex phenomena exhibited by Nature exceeds our ability to explain them, in part, because the whole is not necessarily the sum of its parts [1] and thus typical perturbation-like-theory arguments or standard mathematical techniques are not appropriate to disentangle its mysteries. In this paper ...
URL - StealthSkater
... E. Generalization of thermodynamics allowing NE and a model for conscious information processing 1. Beauregard's model for computer 2. TGD-based variant of Beauregard's model and generalization of Thermodynamics 3. About biological implications of generalized Second Law abstract of this Chapter In t ...
... E. Generalization of thermodynamics allowing NE and a model for conscious information processing 1. Beauregard's model for computer 2. TGD-based variant of Beauregard's model and generalization of Thermodynamics 3. About biological implications of generalized Second Law abstract of this Chapter In t ...
Quantum Symmetric States - UCLA Department of Mathematics
... The tail σ-algebra is the intersection of the σ-algebras generated by {xN , xN +1 , . . .} as N goes to ∞. Thus, the expectation E can be seen as an integral (w.r.t. a probability measure on the tail algebra) — that is, as a sort of convex combination — of expectations with respect to which the rand ...
... The tail σ-algebra is the intersection of the σ-algebras generated by {xN , xN +1 , . . .} as N goes to ∞. Thus, the expectation E can be seen as an integral (w.r.t. a probability measure on the tail algebra) — that is, as a sort of convex combination — of expectations with respect to which the rand ...
Double-slit experiment From Wikipedia, the free encyclopedia Jump
... some of our most commonplace ideas. One of the most striking consequences of the new science is that it is not in agreement with the belief of Laplace that an omniscient entity, knowing the initial positions and velocities of all particles in the universe at one time, could predict their positions a ...
... some of our most commonplace ideas. One of the most striking consequences of the new science is that it is not in agreement with the belief of Laplace that an omniscient entity, knowing the initial positions and velocities of all particles in the universe at one time, could predict their positions a ...
