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At the flat band-edge, the group velocity tends to zero, so that the density of surface plasmon modes is high.
Modes close to cut-off, therefore, do not contribute significantly to the radiated acoustic power in the downstream direction, even though the modal pressure amplitude for these modes is high since they are excited close to resonance.
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Due to larger distances between the lobes in the transverse electric field profile for m = 3 compared to m = 1 and higher similarity of spatial fields for higher-order modes, for m = 3, the possibility of mode coupling into adjacent modes is higher than the possibility of mode coupling into adjacent modes for m = 1.
As noted by Wiback et al. [ 27], the reconstruction of a particular flux vector according to Eq. (1) is not unique if the number of elementary modes is higher than the number of fluxes, which is generally the case.
The default mode is high medieval, but alongside all the tournaments and castles there are echoes as well of earlier periods.
The agreement between the readings with the prototype 2 and the readings with the Nikon microscope completed by the same technician was 96.61% (Kappa statistic = 0.9322, P<0.0001, 49% MODS culture-positive by Nikon reading); the level of agreement between the Nikon microscope and the prototype 2 system in standard mode is high and within the range of the between-technician variability.
As we are interested in the exact onset localisation of the seizure, the spatial mode of BTD is chosen to be rank-1, while the frequency and temporal modes are higher rank.
In addition, the ultimate load reduction for columns bent in single curvature modes were higher than those of the columns had the same end eccentricities but bent in double curvature modes.
At low temperature, the Q factors of the SPP modes are higher than that of the optical mode (dipole mode) due to low metallic absorption loss and relatively low optical radiation loss, however, they seriously deteriorate with increasing temperature and absorption loss [2 4].
First, the peak locations of the probability density function (i.e., the modes) are higher for the active nuclei (22, 15 and 12 for bins at x/L = 0.2∼0.22, 0.3∼0.32 and 0.4∼0.42, respectively) than their inactive counterparts (20, 13 and 11 for same respective bins).
Derived force constants of both stretching and bending modes are higher in the oxidized form than in the reduced form.
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