Figure 3 ODMR transition frequencies as a function of magnetic field.
By plotting these center frequencies as a function of time a graph called spectrogram can be produced.
Plate frequencies as a function of the piezoelectric layer thickness and the plate aspect ratio are presented and discussed.
Contour plots of fundamental linear and nonlinear frequencies as a function of fiber orientation angles are presented.
The predicted −3/2 power law dependence of the quadrupolar and octupolar mode frequencies as a function of the bubble radius is found.
Therefore, the real lattice angle should observe the following rules: Fig. 4 a Spatial frequencies as a function of the lattice angles of graphene.
Note that these results are further validated by inelastic neutron scattering measurements to probe phonon frequencies as a function of the crystal volume.
Using the assignment of RBMs to the measured positions (1) to (7), we plot the observed G- frequencies as a function of tube diameters in Figure 5. Figure 5 Calculated (from ref. [16]) and experimental TERS and confocal Raman G - -mode frequencies as a function of the calculated tube diameter.
