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The results suggest that pulse modulation where the power-off period is approximately 10 μs enables reduction of the mean electron temperature while keeping a high electron density.
With the increase of radio-frequency input power, the former temperature Tce, the latter temperature The, and mean electron temperature Te decrease, while their densities nce, nhe, ne increase.
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Through the application of a DC bias potential to the mesh the electron temperature Te and mean ion bombarding energy Ei to an electrically isolating substrate can be well controlled in the secondary discharge.
Fig. 7. (a) Daytime electron temperature from our data base (mean plus standard deviation) versus solar activity for different seasons (columns) and different altitudes (1st row: 550 ± 50 km, 2nd row: 850 ± 90 km; 3rd row: 2000 ± 300 km).
This carrier temperature corresponds to the mean electron energy of about 1.6 eV.
In the case when the carrier mean energy can be described by the electron temperature, the model in question is called the hydrodynamic (HD) model.
It is found that the electron temperature is about a half of the mean temperature at radii ∼ 1 Mpc.
The polytropic indices of the electron temperature profiles are ⋍ 1.5 whereas those of mean temperature ⋍ 1.3 for r≥ 1Mpc.
In order to characterize the plasma jet, its electron temperature and its composition have been determined by means of optical emissions spectroscopy.
This result is consistent both with the X-ray observations on electron temperature profiles and with some theoretical and numerical predictions about mean temperature profiles.
We present measurements of the electron temperature Te in the RF barrier-torch discharge by means of the planar RF-compensated Langmuir probe.
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