Metric fluctuations and decoherence
... The decoherence time depends strongly on the scale of the energy difference E. For example, E = 1eV gives a decoherence time of the order of 1013 s, while E = 1MeV leads to a decoherence time of the order of 10 s. 5. Summary and discussion In [7] we showed that a fluctuating spacetime metric woul ...
... The decoherence time depends strongly on the scale of the energy difference E. For example, E = 1eV gives a decoherence time of the order of 1013 s, while E = 1MeV leads to a decoherence time of the order of 10 s. 5. Summary and discussion In [7] we showed that a fluctuating spacetime metric woul ...
Full Text - University of Arizona
... a sufficient barrier to ignore tunneling between different double wells [16–19]. In this case, the control problem is substantially simplified, as the relevant Hilbert space in a given time interval is restricted to a small discrete set of energy levels, as opposed to the infinite chain of levels in ...
... a sufficient barrier to ignore tunneling between different double wells [16–19]. In this case, the control problem is substantially simplified, as the relevant Hilbert space in a given time interval is restricted to a small discrete set of energy levels, as opposed to the infinite chain of levels in ...
Lecture Notes on Statistical Mechanics and Thermodynamics
... “phlogistons” (ϕλoγιστ óς: “burned”)1 . His proposal was ultimately refuted by other scientists such as A.L. de Lavoisier2 , who showed that the existence of such a particle did not explain, and was in fact inconsistent with, the phenomenon of burning, which he instead correctly associated also wit ...
... “phlogistons” (ϕλoγιστ óς: “burned”)1 . His proposal was ultimately refuted by other scientists such as A.L. de Lavoisier2 , who showed that the existence of such a particle did not explain, and was in fact inconsistent with, the phenomenon of burning, which he instead correctly associated also wit ...
