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We show the rigidity spectra of the first and the second harmonics of the 27-day variation of the galactic cosmic ray intensity have similar time profiles.
We show also, that the temporal changes of the power rigidity spectra of the first and the second harmonics of the 27-day variation of the galactic cosmic ray intensity are in a negative correlation with the changes of the rigidity spectrum of the corresponding 11-year variation.
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For example, the component corresponding to the second harmonic of the 'probe' component is 2F1, while the third harmonic of the 'mask' component would be 3F2.
In theory, the second, third and fourth harmonics of A2 should correspond exactly with the first, second and third harmonics of A3 (and so on).
The regions around 4,813, 4,285, and 5,208 cm-1 are combinations of the first harmonic of the CH stretching, and the region around 4,405 cm-1 is the combination of the first harmonic of CO stretching in polysaccharides [ 40, 41].
Apart from a small time lag, the second and fourth harmonics were in phase; on the contrary, the first harmonic of SP-D showed a phase near opposite that of cortisol.
Example: G4 is the third harmonic of C3, albeit 2 cents flatter than the true 3rd harmonic.
Supplementary Figure 3 shows the transmission through the third harmonic of the resonator.
The coupling of a single qubit to the third harmonic of the resonator follows as gi3/2π=(1.2±0.1) MHz.
If the first harmonic of is also overlapped, then all the harmonics of will be overlapped.
If the first harmonic of note is overlapped, we try to find some other note which has the first harmonic and harmonic reliable.
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