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That overly simple relationship presupposes that quantum mechanics fully explains classical phenomena, or, alternatively, that quantum mechanics reduces the classical domain in an appropriate limit.
The obtained results indicate that the classical phenomena, such as the locking and peak amplitude, did not appear.
All of these limits involve singular asymptotic series; hence, the relationship between quantum phenomena and classical phenomena is not one involving anything like bridge laws relating the two domains as Nagelian and other forms of reduction would require.
If collapse happens faster than decoherence, then the superposition of components relevant to decoherence will not have time to arise, and insofar as the collapse theory is successful in recovering classical phenomena, decoherence plays no role in this recovery.
It is natural to extend this analysis from the case of measurements induced by an apparatus to that of 'spontaneous measurements' as performed by the environment in the theory of decoherence, thus applying the same strategy to recover both quantum and classical phenomena.
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Classical electromagnetically induced reflectance (Cl-EIR) is a classical phenomenon which is analogue to the EIR quantum phenomenon in atomic systems.
The classical phenomenon of droplet break up/coalescence is not applicable when an insoluble fraction is present.
A more detailed description of the classical phenomenon of canards in planar systems and analysis techniques can be found in [28 31].
In this section, we briefly review the classical phenomenon of canards as they arise in the FitzHugh-Nagumo oscillator, and the recently-identified phenomenon of torus canards as they arise in a Purkinje cell model.
The juxtaposition between large scale climate variability, for example, the combined effect of rainfall and high tides can generate the classical phenomenon called "tidal flooding" (Pezzoli et al. 2013b).
The classical phenomenon of progressive cracking of 90° plies in polymeric matrix cross-ply laminates, and potential or subsequent delamination along the 0°/90° ply interface, is critically revisited using a finite-volume homogenization theory with damage evolution capability.
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