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In the B1s spectrum (Fig. 5b), the peak can be fitted using two components: B N bond (190.4 eV) and B O bond (191.2 eV).
For further reference, based on the monthly emission of radioCs until the end of 2011 estimated by TEPCO 2012, the primary emission decrease can be fitted using two exponential laws with half-time constants of 2.3 days (±2 %) and 48 days (±23 %).
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Figure 1a shows the PL spectrum measured under an excitation power of 100 mW at 15 K. Obviously, it can be fitted using three Gaussian-shaped peaks with a nearly equal energy difference of approximately 60 meV.
Figure 2 shows results of the deconvolution of the PL spectra of the samples H, M, and L. It is found that PL spectra of all samples in the whole spectral range can be fitted using four components: B, G, and two PL bands in the red and near infrared ranges that are labeled as R1 and R2.
Equation (4) was fitted using two different approaches.
The experimental Raman spectrum is fitted using two Gaussian functions centered at 501 and 460 cm−1.
The same data is fitted using two forms of the TOS decay function.
Moreover, the O 1s core-level spectra of the cross-linked CCIONPs were fitted using two peaks at 532.3 and 534 eV.
If the time-activity curve did not converge at the last PET scan (e.g. intestines and gallbladder), time-activity curves were fitted using two exponential functions, and then the area under the curve after the acquisition of the last image was calculated by assuming only physical decay of 18F and no additional biologic clearance to be conservative [10].
In accordance with previous research done by Pajchel et al. [34], 31P BD NMR signals were fitted using two lines: a narrow one, which corresponds to the nuclei of phosphorus-31 originating from inside the crystal, and a broad one, which may be attributed to the nuclei of phosphorus-31 located in the hydrated surface layer.
The event-related data were fitted using two variations of the general linear model (GLM).
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