If we can construct a narrow band-stop filter in the SFrFT domain whose center frequency around at the center of the narrowband spectrum of a strong moving target, then the signal component of this moving target can be extracted from the initial signal.
In the emission spectrum of 1⋅Eu, strong sensitised Eu-based emission with the characteristic sharp lines from the D0→Dn manifold superimposed on the Ir-based emission profile can be also seen.
However, it is surprising that C60 electronic transitions are not detected in the high-quality optical spectrum of the strongest C60 source without AIB emission, Tc 1 (García-Hernández and Díaz-Luis, 2013).
For more than one solar cycle, spectra of some strong TR lines have been acquired in many CDS observations.
In the SFrFT domain with a proper α, the spectra of any strong moving target will concentrate to a narrow impulse, and that of the clutter will be spread.
Their spectra were composed of strong red emission (4F9/2→4I15/2) and green emission (2H11/2, 4S3/2→4I15/2) with the excitation of a 980 nm near-infrared (NIR) laser diode (less than 90 mW/cm2).
In their IR spectra, the presence of strong absorption bands at 1288 1296 and 3275 3380 cm−1 attributed to the C=S, NH and NH2 functional groups confirmed the formation of the 1,2,4-triazole ring.
Based on reconceptualisations of multifunctional agriculture as a normative spectrum of decision-making (strong to weak multifunctionality) bounded by productivist and non-productivist action and thought [Hollander, G.M., 2004.
In the Raman spectrum of PEDOT, one strong peak at 1,424 cm−1 and a few weaker bands are observed.
The absorption spectrum of DNA shows strong absorption for UVB-radiation and much lower absorption for UVA-radiation (Fig. 1).
