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Initially, the number of laser longitudinal modes was measured by a scanning Fabry Perot interferometer (SF PI) (Fig. 1).
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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.
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.
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).
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.
The transient variations in flow and electrochemical characteristics of the dead-end and recirculation modes are measured and discussed in detail.
The attenuation of the T 0,1) and L 0,2) guided wave modes is measured using a full-scale experimental apparatus in a fusion-bonded epoxy (FBE -coated 8 in.
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