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The E2g and A1g modes are at around 383 and 403 cm−1, respectively.
The two identified dominant modes are at about 0.5 Hz and 1.3 Hz respectively.
In particular the two modes are at X = 0 and X = 1 if ν β p = 1.
These curves show that the first (dipole), second (quadrupole), and third (sextupole) plasmon modes are at 1,870, 960, and 700 nm, respectively.
Figure 4a,b indicates that the first, second, third, and fourth modes are at 1,910, 970, 710, and 610 nm, respectively.
The peaks of these plasmon modes are little red-shifted from those induced by a plane wave, where the first and second modes are at the NIR regime.
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Understanding, and preventing, these failure modes is at the heart of developing new armour materials and systems.
The maxima and minima of ΔI occur when one of the two modes is at the central frequency.
The center of mass of the population of the mode 3 particles is found to be 51.3 km and that of all three modes is at 55.1 km.
Further, a plot of the GADA titer according to patient frequency revealed a possible bimodality, and the lowest value between the two modes was at a GADA titer of 200 WHO IU (data not shown).
The other significant changes in the fluctuation orientation in this mode are at residues 56′ and 78′.
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Since I tried Ludwig back in 2017, I have been constantly using it in both editing and translation. Ever since, I suggest it to my translators at ProSciEditing.

Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com