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Two examples from Old English (OE) and from Old High German (OHG) with deontic modals selecting perfective infinitives demonstrate this relation (from Leiss 2008: 26).
The robustness function for the performance requirement in eq. (25) is: (26) α ^ (q, C m ) = max α : max u ∈ U C (t m, u ) ≤ C m We can "read" this relation from left to right as follows.
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This paper discusses the relation from a probabilistic mechanics point of view.
The validity of this relation follows from the fact that if is a solution of the inequality (3.2), then is a solution of the inequality (3.3) and vice versa.
But where does this relation come from?
For this, the scattered intensity I t) can be written as: This relation follows from Eq. [5], with a 0 equal to I eq and a 1 equal to I eq - I 0).
This relation results from the fact that the observed lifetime of the nascent branch intermediate is limited by the combination of the dissociation of diVCA from the filament-bound Arp2/3 complex (proceeds with rate kV−*) and the dissociation of diVCA-Arp2/3 complex from the filament (proceeds with rate kA−), such that τV* = 1/ kA− + kV−*).
One could find this interesting relation from [3, 4] and [5].
Let us look at this new relation from another point of view.
This relation is derived from the requirement that acoustic waves arriving from the object at normal incidence on the detector should be separated in time from any waves that reach the end of the detector.
This relation is derived from the following procedure.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com