Although our experiments showed that A/H5N1 virus can acquire a capacity for airborne transmission, the efficiency of this mode remains unclear.
The antenna mode-scattered signal can be varied according to the antenna load, Z L, whereas the scattering of the structural mode remains the same.
An appropriate mode shape function is proposed for the postbuckling process, under the assumption that the buckling mode remains unchanged as the deflection increases.
We found that upon a 266 nm laser excitation, while the G mode remains pronounced, the G′ mode is not observed.
The presence of the porous layer reduces the frictional influence on the films, which significantly alters the length and time scales of the shear mode while the interfacial mode remains dormant to this effect.
These all consistently show that increasing the thickness of the oxidation layer blue-shifts the plasmonic resonance peak while the transverse mode remains constant, which is well matched by simulations.
These charged particles belong solely to the upper mode, whereas the lower mode remains charge neutral, suggesting that ions do not act as soot nuclei.
Since the phase velocity of the fast mode remains always positive, it is observed that this mode always propagates in the plasma.
It is, however, important to note that the LO mode is dependent on the intralayer hopping between two inequivalent carbon atoms, and the LO mode remains essentially unchanged when changing the IL interactions8,9,10,11,12,13,14,15.
Interestingly, for fibrils composed of laterally stacked antiparallel intermolecular β-sheets (i.e. not in-register sheets) all the low-frequency modes remain parallel to the fibril axis, while the high-frequency mode remains in the direction of the β-strands; normal-mode orientations similar as for isolated antiparallel (intermolecular) β-sheets (Fig. S8).
