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Figure 2 PL time profiles and fitting results.
(b, c, d) Typical fitting results of the PL time profile using a triple exponential function, where the PL time profile is deconvoluted with an instrumental response function.
The PL time profile indicates three decaying components with different decay times.
(a) PL time profiles of the Si-ND array at different energy regions.
b PL time decay measured at peaks B and C shown in a. Next, we examined the PL time evolution at the higher energies spanning 1.30 1.35 and 1.35 1.42 eV.
Typical fitting result of the PL time profile at 250 K using a triple exponential function, where the PL time profile is deconvoluted with an instrumental response function (c).
Similar(49)
(b) PL time-decay curves measured at 1,220 nm and at temperatures in the 11- to 80-K range.
We also analyzed the behaviour of the PL time-decay curves at 11 K as a function of the photon flux, as reported in Figure 7b.
By comparing the PL time-courses of the two powders with those of a commercial rutile TiO2 powder, it was concluded that the photodesorption of O2 in air with ethanol occurs on the SnO2 powder, not on the KGSO powder.
From (13), (14), (19) and (20), it can be concluded that the computational cost of DCS-SOMP is pL times the cost of OMP.
From (15) to (18), it can be concluded that the computational cost of OMP-PKS+RS is approximately pL times the cost of OMP-PKS.
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