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on its closure which is a special time scale with fascinating symmetry properties.
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It should be noticed that the proof of Lemma 2.5 is independent of special time scale features, except for the notion of rd-continuity at the end.
In Theorem 2.1, if we take T 1, T 2 for some special time scales, then we immediately obtain the following three corollaries.
In this sense, Corollary 5.2 shows that Definition 3.1 is consistent for special time scales T L with the approach utilized in [16].
In this section, we assume that (y^{Delta^{sigma}}(t)=y^{sigma ^{Delta}}(t)) for all (tin[rho(0),+infty capmathbb{T}) in order to establish several criteria for equation (1.1) to be in the case I on the special time scales.
In Theorems 2.4 2.7, if we take (mathbb{T}) for some special time scales, such as (mathbb{T}=mathbb{R}), (mathbb {T}=mathbb{Z}), (mathbb{T}=q^{mathbb{Z}}), we can obtain corresponding oscillation criteria for fractional differential equations, fractional difference equations, fractional q-difference equations and so on.
That was a special time.
It's such a special time.
This is a special time.
This is a special time for Lewis.
"It's a special time in New York.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com