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Maximum optical power in this case is also limited by the threshold of the next Stokes order generation.
The maximum optical power was approximately 2.2 μW at 40 mA.
In our proposed design, the active layer position in waveguide region was optimized for obtaining maximum optical power and minimum threshold current.
At 35 °C, the maximum optical power is about 1.9 mW.
At high temperature of 65 °C, the maximum optical power is still more than 5 mW.
Its maximum optical power was 2.4 mW, and the corresponding power dissipation was 0.76 W.
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This provides the difference between the maximum and minimum optical power values from all of the calculation points.
We proceed to test the ionization state of our laser performance using a typical gas mixture of CO2-N2-He with proportion of 1 1.2 3.7 correspondingly and at a final pressure of 70 Torr a maximum optical output power better than 20 W was obtained at a maximum RF feed power of 173 W.
The current value corresponding to the maximum optical output power was 60 and 40 mA, respectively, with and without AgNW film, which indicated the better thermal performance.
The lasers linewidth should be in the order of tens of Hz, with a maximum relative intensity noise (RIN) of -107 dB/Hz and a minimum optical power of 0.94 mW.
Particularly, in Figure 2a, at each current point, local maxima of the output optical power time trace over the last 20 round trips are gathered and plotted, showing the pulse peak power stability/fluctuation in such time interval.
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