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As before, we note that problem (6) does not admit the trivial solution (u(t)equiv0_{mathbf{R}^{2}}).
As before, we note that L and J are user-defined parameters known at both ends of the communication and kept constant throughout the duration of the tests.
As before, we note that these results are suggestive only, with a stricter test requiring a BF hypothesis test that includes a point null hypothesis.
Before, we note that the considerable agreement observed between four of the six transformation functions and the morphological distances also confirms the use of latter as reference datasets.
Similar(55)
Before proceeding, we note that there is a small number of weak links where the pathloss falls below dB.
Before proceeding, we note that there exists t0 > 0 such that ∫ 0 t g ( s ) d s ≥ ∫ 0 t 0 g ( s ) d s = g * > 0, ∀ t ≥ t 0, (3.9).
Before proceeding we note that these equations can be extended to cover the situation introduced in Eq. (7) which incorporates spatial effects.
Before starting, we note that the OFDM implementation herein described has been created for the purpose of this proof-of-concept to increase the flexibility and transparency of the legacy GNU Radio implementation.
Before proceeding, we note that the noise σ P can be broken down into two independent components: laser intensity fluctuations σ PL and electronic measurement error σ PM; σ PL is common to both conventional TPEF and AIM, while σ PM is unique to AIM.
Before doing this we note that many papers on asymptotics of difference equations involve difference systems fitting this pattern under special choices of parameters.
Before proceeding, however, we note that CS can also be useful in settings where it is possible to acquire high-resolution signals, but is difficult or expensive to subsequently encode them.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com