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According to proponents of this view, the content of a mental representation consists of a proposition, where propositions are taken to be functions from possible worlds to truth values, or alternatively the set of possible worlds in which the proposition is true.
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Here, the traditional term "range" (alternatively, "image") is the set of values produced by the function.
Alternatively the smaller set of cycles could be tested first with the larger set only utilised if potentially aromatic atoms were remaining.
Groups (b) and (c) together form the set of alternatively targeted genes in which one or more target sites are located in alternative 3'UTR segments.
Specifically, we required that there be a non-empty intersection between the set of alternatively-expressed exon probes from at least two experiments at the timepoint.
Alternatively, probabilities of each phasing given the set of reads can be computed and uncertainty can be accounted for when extending phase to adjacent edges.
Alternatively, this set of traits may reflect an adaptation to high opportunities for extra-pair matings (Munshi-South 2007; Cohas & Allainé 2009).
Suppose, as Lewis does, that properties are sets of possible objects; alternatively, suppose that a property \(F\) is an intension, namely a function whose value at any world \(w\) is the set of objects that have \(F\) at \(w\).
Both consider the set of active fluxes, Z ¯ v = i : v i ≠ 0, 1 ≤ i ≤ R. For example, the rank test states that the flux vector v : Sv = 0, v ≥ 0 is elementary, if (1) nullity S *, Z ¯ v = Z ¯ v − rank S *, Z ¯ v = 1 Alternatively, we can consider the set of inactive fluxes Z v) = { i : v i = 0, 1 ≤ i ≤ R}.
Alternatively, the initial setting of r g could be determined to ensure that the frequency deviations shall not trigger any under-frequency load shedding (UFLS) incident.
Alternatively, another set of estimators can be obtained by minimizing the mean squared error between x(k) and x ̂ ′ ( k ) : J mse ′ = E v ( k ) − ∑ i = P ′ + 1 L β i ′ b i T v ( k ) − ∑ i = P ′ + 1 L β i ′ b i T x ( k ) 2 = σ v 2 − 2 ∑ i = P ′ + 1 L β i ′ i L T R v b i + ∑ i = P ′ + 1 L ( 1 + λ i ) β i ′ 2, (42).
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com