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From the obtained decay heat, an accident analysis was performed.
Figure 6 shows the temperature dependence of the obtained decay lifetimes.
The obtained decay times are almost the same as the distribution peaks shown in Figure 3.
The obtained decay lifetimes at different photon energy were shown in Fig. 5, guided by the broad SSPL peak.
Moreover, it was proposed that the observed broadening of obtained decay rate distributions reflects the disorder in the samples.
The obtained decay times τ0 were equal to 16 and 5.2 μs for uncoated and Au-coated nc-Si-SiO x samples, respectively.
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The obtained decay-associated spectral components show clear differences of the peak energy of 20 to 30 meV between the slowest component (τ1) and the faster two components (τ2, τ3).
A typical analytical HPLC chromatogram is shown in Fig. 4. Method 2: In 35 runs, 0.76 ± 0.27 GBq of [11C]erlotinib were obtained (decay-corrected radiochemical yields are 7.3±2.8%8% and 16.1 ± 4.9% based on [11C]CH4 and trapped [11C]CH3I, respectively).
Let us describe briefly how the energy method can be applied to obtain decay estimates for local problems.
The method of proof was used by Schenck [232] to obtain decay estimates for damped wave equations and by Ingremeau [141] to describe distorted plane waves in quantum chaotic scattering.
We performed an additional 3x3 spatial pixel binning to obtain decay profiles with ~5000 photons.
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