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(A ) Data as in Figure 2E, where the mode is plotted for several time points of the evolution experiment for bem1∆ (and10) and wild-type lines.
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Next, the measurement results of the directionality of the MSC for each gain mode are plotted in Fig. 12.
There is no degeneracy for modes in Figure 3a, but since the third and fifth modes are degenerate, in Figure 3b four modes are plotted.
The frequency and cumulative participating mass of the important modes are plotted as a function of the dimensionless total stiffness of the piers.
The coefficients for the first three cylinder and torus modes are plotted against frequency for the case of a plane wave incident upon a 90° bend.
The capacity gains of the four DF relaying modes are plotted in Fig. 8, and the maximum value of the four gains can be seen as the gain of the proposed DF relaying scheme.
An example of a predicted cell structure belonging to this dominant mode in the distribution is plotted in Fig. 4AB.
As an example, a computational cell structure from this mode of the orientational distribution is plotted in Fig. 4GH.
Figure 3 The optical properties of the SPP modes with m = 1, 2, and 3. (a) The resonant wavelengths and mode volumes are plotted as a function of L. An extremely small mode volume on the order of 10-5 μm3 results.
The corresponding two-dimensional mode shapes are plotted so that the wave vibrations can be identified.
Three-dimensional mode shapes are plotted for some typical square plates.
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