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The dark modes were measured at 632.8 nm (He Ne).
Possible propagating modes were measured at a wavelength of 633 nm using the prism-coupling method.
These BPEHs presented different dynamic responses, and the output powers under different vibration modes were measured.
During the intervention schema modes were measured by using the Mode Observation Scale (MOS) and by a pre-test/post-test design applying the Schema Mode Inventory (SMI).
Laser measurements, where the building's natural frequencies were determined at eleven stages during construction; and forced vibration tests, where all the characteristics of the fundamental modes were measured at three key stages.
Differences in time efficiency for the viewing procedures and presentation modes were measured using total analysis time.
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Initially, the number of laser longitudinal modes was measured by a scanning Fabry Perot interferometer (SF PI) (Fig. 1).
The first and second coupled system modes are measured at around 40 Hz and 70 80 Hz respectively.
Even when the first two modes are measured under the 5percentt corruption level, the added mass could be estimated properly.
Resonance frequencies in both the flexural and torsional modes are measured, and the Young's moduli and shear moduli are determined through the measured resonant frequencies.
The wave number difference between these modes is measured as 22.97 cm−1, which ensures that there are three layers in MoS2 film.
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