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We represent these functions in Fig. 4b.
We also show the functions in Fig. 8.
The results are shown with the black functions in Fig. 6 for d′ = 1.5.
The functions in Fig. 6b reflect only direct tephra fall impact at a water treatment plant.
The fits are a good, but not perfect, match to the real aberration functions in Fig. 2a.
b Temperature dependence of the A exciton peaks in imaginary part of dielectric functions in Fig. 3d f.
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We show the map view of its inverted slip distribution in Fig. 2(b), and depict its moment rate function in Fig. 2(d).
We show the map view of its inverted slip distribution in Fig. 2(a), and depict its moment rate function in Fig. 2(d).
We show the map view of its inverted slip distribution in Fig. 2(c), and depict its moment rate function in Fig. 2(d).
If the edges of the triangular function in Fig. 4 are blurred, Fig. 5 can be produced.
This duration coincides with the peak pulse duration in the moment-rate function in Fig. 3(b) (orange bar).
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com