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Additionally, as shown in Figure 16, there is a significant shift in magnitude of FWHM E2 (high) phonon vibration modes of approximately 8.6 and approximately 25.8 for the as-grown ultrathin and thin ZnO NWs compared to the ultrahigh vacuum annealing treatment at 873 K.
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The other plasmon mode, of approximately 575 nm, corresponds to in-phase symmetric quadrupole-quadrupole plasmon mode.
The other Plasmon mode, of approximately 620 nm, corresponds to two in-phase quadrupole-quadrupole modes oscillating in the out-of-phase way.
The plasmon mode, of approximately 800 nm, corresponds to the two in-phase symmetric dipole-dipole modes oscillating in the out-of-phase way.
From Figure 3, it can be known that except for this plasmon mode of approximately 1050 nm, other plasmon modes consist of the essential plasmon modes of the core-shell nanocylinder pair.
The plasmon mode of approximately 690 nm is produced from the interaction between in-phase dipole-dipole mode of the first nanocylinder pair and the in-phase quadrupole-quadrupole mode of the second nanocylinder pair.
In this experiment, it is found that such a cavity mode of three solid nanocylinder pairs is essentially the same as the lightning-rod mode of approximately 979 nm.
In humans, COP values have been found to follow a Gaussian distribution with a mode of approximately 25 cm H2O [7] or a bimodal distribution with a second mode close to 40 cm H2O [5].
Figure 4b shows that as pair-distance decreases between the core-shell cylinder pairs, the intensity of the plasmon mode, of approximately 1100 nm, decreases and is red-shifted.
The plasmon mode, of approximately 700 nm, corresponds to in-phase symmetric dipole-dipole interaction mode, and the symmetric dipole mode is a result of the electrons at the inner surface of the core-shell nanocylinder aligned symmetrically with the electrons at the outer surface [21].
The CV of ISIs in the majority of units ranged in the baseline across all pattern types between 0.4 and 1 with a mode of approximately 0.6.
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