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Mass discharge measurement error was investigated using a Monte Carlo modeling analysis as a function of the contaminant plume position and width, and as a function of the pumping conditions used in the different pumping tests.
In Fig. 4(b), we plot the emission intensity as a function of the pumping power.
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Figure 6 shows the laser wavelengths behaviour as a function of the pump power.
Fig. 5 Dual-wavelength laser lines output power as a function of the pump power.
Fig. 6 Dual-wavelength laser emission as a function of the pump power, a Output laser spectrum for different pump powers, b Laser lines wavelength displacement versus pump power.
Figure 5 shows the output power of the generated laser lines as a function of the pump power.
The count rate measured on the detectors is presented in Fig. 4c, as a function of the pump power.
The transient reflectivity change ΔR/R of the probe beam was measured as a function of the pump-probe delay time.
With a pump power of 40 mW the separation between the laser wavelengths is ~13.4 nm whereas a separation of ~14.2 nm is observed with a pump power of 120 mW. Figure 6b shows the wavelength displacement Δλ as a function of the pump power where λ 1 is the shorter wavelength and λ 2 the longer wavelength.
Fig. 5 a shows the measured laser power as a function of the diode pump current.
In both cases, the output laser power at 1530 nm was measured as a function of the injected pump power.
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