עוד בפרק זה:
Plasma Physics Laboratory
3-5026619 (972) |
:Fax |
:Email |
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building 8, room 202 |
:Location |
3-5026617 (972) |
:Tel |
building 8, room 108 |
:Location |
:Email |
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3-5026525 (972) |
:Tel |
Plasma accelerator |
Silicon etching |
Sintering |
Helicon |
The RF plasma source is composed of a vacuum chamber, a gas flow controller, solenoids that generate a DC magnetic field, a radio frequency generator with matching units, and an antenna. The plasma is generated inside a Pyrex tube, 52cm in length and 10cm in diameter. The radio-frequency generator radiates at 13.56 MHz with a power of up to 1 kW. The magnetic field intensity is up to 900G. The working pressure is between 0.5 mTorr and 10Torr. Argon and nitrogen are used, both separately and as a mixture. The antenna is a helix of six turns of a 350mm total length and a 100mm diameter.
Employing a Langmuir probe system we have measured the plasma density for various wave power levels, magnetic field intensities and gas mass flow rates. The plasma source operates as a helicon plasma source. The magnetic field intensity is made uniform along the tube. The gas mass flow rate is 7.1 sccm and the gas pressure is 2mTorr. The I-V characteristics of the probe are used to infer the electron temperatures and the ion saturation currents, from which we calculate the ion densities. The electron temperature was found to be about 5eV. As seen in the figure there is an abrupt density increase above 400 G, as the source enters the helicon mode, the experimental curves (except for the 200W curve) move above the theoretical resonant line. The density regime above the resonant line is the stable regime for the helicon mode operation.
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