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The modes are shifted and the polaritonic gap decreases with temperature.
As is evident from Fig. 5, both and modes are shifted to the higher wavenumbers after Berkovich nanoindentation.
The Raman active modes are shifted from 458 to 461 cm−1 for the CeO2 samples heated at 160°C to 200°C.
It was found out that the bands at ≈250 cm−1 and ≈700 cm−1 in the spectrum of the film, corresponding to FeO vibrational modes, are shifted by about 20 cm−1 to higher frequencies as compared to the bulk samples.
The vibrational infrared and Raman spectra of B3N3C54 and C60 have been compared and it was noticed that the strongest peak in vibrational spectrum of B3N3C54 is due to BN stretching and CC stretching modes are shifted to higher wavenumber region.
Thus, the strong triple bond stretch modes, which are present in the linearly conjugated molecules, are strongly repressed in the CC molecules due to the small overlap between the in- and the out-channels, but since the vibrational modes are shifted slightly away from the interference feature, the stretches are not completely suppressed.
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These modes exhibited well-defined thickness dependence, thus the frequencies of these two modes are shifting away from each other with increasing thickness.
In order to collect balanced data of the two participants behaviour, the modes were shifted regularly (every 10 turns), but they were always complementary ACTIVE on one side and PASSIVE on the other.
The bending stretch mode was shifted to the higher frequency.
The primary failure mode is shifted whenever the weakest link is removed through design improvement.
Using this table we observe that the TE210 mode is shifted twice as much compared to the TE110 mode.
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