The technique is based on a new class of intravascular microbubble agent, consisting of perfluoro-gases combined with multipulse scanning modes sensitive to non-linear (harmonic) responses of the microbubbles and enabling tissue signal suppression[ 6, 7 ].
Raman spectroscopy was used to rule out strain and electrostatic doping as primary causes of the variations in emission intensity; the frequency of E2g vibrational mode is sensitive to strain, whereas the frequency of A1g vibrational mode is sensitive to electrostatic doping.
In our studies, we find that the behavior of the recycle mode is sensitive to the parameter, D. Hence, the dispersion coefficient is obtained using the recycle mode data.
Due to the dispersion in the dielectric function of ITO, it is found that the defect mode is sensitive to the ITO thickness.
It is shown that both the strength and the deformation mode are sensitive to the notch depth, and in particular to the inter-void ligament distance.
Obviously, it might be expected that dimers would give a single and more pronounced reflex in the spectra compared to disordered aggregated objects since longitudinal plasmon coupling mode is sensitive to the interparticle distance [24].
We also find the asymmetric G∗ double resonant mode is sensitive to the high incident laser energy, and I(G /I 2D) of monolayer graphene is most sensitive to UV laser energy due to near off resonant behavior of 2D modes at high excitation energy.
Moreover, when the mixed investment is optimal, we found that the absolute and relative investments in each adaptation mode are sensitive to the spatial configuration of hosts (Fig. 2).
However, conventional methods lose effectiveness for expanding mode shapes of cable domes whose modes are sensitive to the pretension deviations.
The coupling strengths of the fundamental hybrid modes between the two categories of modes are sensitive to variations in the NW radii, rGaN and rAg, and the width of the air gap d.
