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These concepts, and also Dirac's idea of vacuum polarization (1934), helped a new generation of theorists after World War II invent ways of subtracting infinities from one another in their calculations so that predictions for physically observable results in quantum electrodynamics would always be finite quantities.
Geometrical constraints, termed "multipath preservers" were derived to ensure that multipath was physically observable in the radar returns.
Correlating compensation with any physically observable quantity is ill-advised, for a variety of reasons discussed here.
Multiple theoretical solutions are shown to exist and the criterion for selecting the physically observable solution is indicated.
Because Gaussian beams have favorable propagation characteristics and represent physically observable entities, these have played a vital role in many modeling schemes; see, for instance, [10].
For a wide class of radar-target geometries, functions termed multipath preservers are derived which indicate when multipath is physically observable in the radar returns; these functions assist in evaluating the potential of multipath exploitation in urban sensing.
Similar(51)
In this regime, the equation propagates oscillations with a wavelength of O, and finite difference approximations require the spatial mesh size h=o and the time step k=o in order to obtain physically correct observables.
This proportionality links an observable, physically real concentration, to the abstract but meaningful thermodynamic activity function.
Note that the amplitude of the oscillations is physically feasible and observable for all the genes, including CBF1.
Here, oscillations have period equal to 120 minutes, thus close to the the yeast cell cycle period in galactose; the amplitude is physically feasible and observable for all the mRNAs, but CBF1.
Note that the amplitude of the oscillations is physically feasible and observable for all the genes; in particular, it is significantly higher than in Scenario 2 for the genes SWI5 and ASH1.
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