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Plausibly assuming constant γC throughout the resonance we can analogously to Ref. 16 extrapolate the γE to the resonance (shaded) region in Fig. 1d (solid lines) from the expression for the current.
We can analogously prove the following lemma as in Menger PM-spaces.
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And if the time to complete the job is t, we can define, analogously, its earliest finish time (EF) to be ES + t. (1) Mark the value of S to the left and to the right of Start.
We can proceed analogously to the proof of Lemma 2.6 in order to show that (2.36).
We can proceed analogously to the proof of Lemma 3.2 by induction as in Lemma 3.1.
Step 1.2.: In equality (33) we have (lambda<0) and (v(t)<0) a.e. in I, so it remains true and we can proceed analogously.
Second, if the point t 0 is left-scattered and right-dense, i.e., ρ ( t 0 ) < t 0 = σ ( t 0 ), we can proceed analogously as in the case before.
We will apply this approach for model comparison accordingly, and can analogously apply this method using BIC.
From (2.18), one can analogously obtain (2.32).
One can analogously show that the integral along the lower side tends to the same number.
These quantities can analogously be defined for DSP, this time following Ref. [9].
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