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Resonances of both modes are shown to be nonlinear due to partial and total contact loss.
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These results are summarized in Table 2 and typical direct flow injection (DFI) spectra in both positive and negative modes are shown in Figure 3.
The EPR spectra of 1Co- and 2Co-VIM-2, obtained in both parallel and perpendicular modes, are shown in Figure 6.
The NP film T-LSPR data from the calibration study done in water is shown in Figure 4. Similar data from both hydrated and dry PE layers in reflectivity and transmission modes are shown in the Supporting Information.
Quantum experiments also require coherent superposition states; a few examples of specific modes are shown in the lower row.
Finally, modes are shown to play a role particularly when their frequencies coincide with other contributions.
Zero-energy modes are shown to be completely damped in all cases.
The different modes are shown on a Weber number the viscosity ratio map.
The stationary oscillation modes are shown to be selectively excited by an electric field with suitable symmetry.
Surface modes are shown to preferentially develop for a bubble radius near the resonance of radial oscillations.
The position and the number of defect modes are shown to exhibit relationships with the structural parameters.
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