The present invention concerns a method and a device for forming a plasma beam.
It is known that certain techniques, such as the etching of semiconductor devices, space propulsion, magnetically confined fusion, biotechnology, etc., use electrically neutral plasma beams, which can be obtained by different methods.
The best-known method, cited as prior art in documents WO 2004/002201, WO 2007/065315 and WO 2010/060887, consists of extracting and accelerating positive ions from a plasma via negatively-biased grids, and then using an auxiliary electron beam to neutralise the flow of ions thus obtained in order to form an electrically neutral plasma beam. Of course, this first method has the disadvantage of requiring an auxiliary source of electrons.
Another method is that which is the subject of documents WO 2007/065915 and WO 2010/060887 and which consists of extracting and accelerating positive ions and negative ions from a plasma via at least two grids biased negatively and positively respectively and of combining the flow of said positive ions and the flow of said negative ions to form an electrically neutral plasma beam. This method has the advantage of combining the positive ions and the negative ions extremely rapidly (approximately 5×10−8 cm3/s), particularly if they originate from a single source, but it can be difficult to implement due to the simultaneous presence of grids with an opposite bias.
Yet another method (see, for example, documents EP 1 220 272 A1 and U.S. Pat. No. 5,156,703) consists of extracting and accelerating the positive ions and the negatively-charged particles from the plasma by subjecting an extraction and acceleration grid to bias potentials that are alternately positive and negative. In this method, said grid extracts and accelerates positive particles (in other words, positive ions) and negative particles (which can be negative ions or electrons) alternately from the plasma, said positive and negative particles then combining to neutralise their charges. However, experience has shown that, in practice, the quality of the electrical neutrality of a plasma beam obtained in this way is not the best.
The object of the present invention is to improve this last known method, in order to obtain greater electrical neutrality of the plasma beam.
To that end, according to the invention, the method for forming a plasma beam by extracting and accelerating electrically-charged particles from a plasma and using at least one extraction and acceleration grid subjected to bias potentials that are alternately positive and negative is notable in that:
The present invention makes use of the fact that the number of positive and negative particles extracted and accelerated depends on the duration and the amplitude of the positive and negative potentials applied to said extraction and acceleration grid.
The result is that adjusting the duration and/or the amplitude of the positive and/or the negative bias potentials acts, in accordance with the invention, on the qualify of the electrical neutrality of the plasma beam. An adjustment of this kind can be performed in real time, via, for example, analysis of the grid currents or by an external sensor monitoring said plasma beam.
In order to further improve the quality of the electrical neutrality of the plasma beam. It is advantageous for the frequency of alternation of the positive and negative bias potentials to be a radio-frequency included in the range between a few kHz and a few MHz, in other words, for the duration for which a positive or negative potential is applied to said extraction and acceleration grid to be included in the range between a few ms and a few μs. Experience has shown that such a frequency promotes the combination of positive and negative particles.
In the case where said plasma is pulsed, it is also advantageous for this alternating sequence of positive and negative bias potentials to be synchronised with the pulsing of the plasma and for the positive ions to be extracted from the plasma during the pulsing thereof, while the negative particles are extracted in the intervals between said pulsings.
The alternating sequence of positive and negative bias potentials may have any appropriate continuous form, for example sinusoidal. However, it preferably takes the form of a sequence of rectangular waves with steep edges, in which the rise time is approximately the transit time of the ions, or faster.
Preferably, the positive and negative potentials used to bias said extraction and acceleration grid amount to several hundred volts, for example 400 volts.
The present invention also relates to a device for implementing the method described above. Such a device according to the invention, which has a plasma generator provided with at least one grid to extract and accelerate electrically charged particles from said plasma, and also means for the electrical biasing of said grid, producing bias potentials that are alternately positive and negative, is notable in that it has a detector delivering a signal representing the quality of the electrical neutrality of said plasma beam and in that said means for electrical biasing is controlled by said detector so that said plasma beam is at least approximately electrically neutral.
A detector of this kind can he a sensor, for example an induction sensor, monitoring said plasma beam, or a current sensor in a grid of said device. To that end, it is advantageous that:
Preferably, said electrical biasing means has a MOSFET rapid switch, switching alternately between the two opposed polarities.
The plasma generator device according to the present invention can also have means for synchronising the electrical biasing means with the pulsing of the plasma.
The accompanying drawings will give a clear understanding as to how the invention may be embodied. In these drawings, identical reference numerals refer to similar elements.
The plasma generation device I, according to the present invention and shown diagrammatically in
The plasma generation device I has a grid 4 in contact with the plasma in order to be able to extract and accelerate the positive ions A+ and the negative ions A− from the plasma situated in the adjacent area 5, after eliminating the electrons e−, for example via a magnetic filter 6. A grid 7 connected to the earth or to a slightly negative potential (for example approximately −10V) is disposed upstream from the extraction and acceleration grid 4. An intermediate grid 8, which is negatively biased, could be disposed between the grids 4 and 7. The grid 4 could be replaced by an internal electrode in the plasma core 1, the bias potentials then being applied to this internal electrode and the grids 8 and 7 being used as before.
The extraction and acceleration grid 4 is biased alternately positively and negatively via an electrical biasing device 9, comprising for example a MOSFET rapid switch able to switch two opposite electrical polarities rapidly, without the potential being exceeded significantly, “rapidly” meaning approximately the transit time of the ions.
A known example of a bias signal B at high voltage +HT, −HT (for example approximately 400V), capable of being applied to the grid 4, is shown in
The bias signal B consists of an alternating sequence of positive rectangular waveforms with steep edges b+ (between 0 and +HT) and negative rectangular waveforms with steep edges b− (between 0 and −HT). In this bias signal B, all the positive bias waveforms b+ are of equal amplitude a and duration d and the same applies to the negative waveforms b− which, in addition, are identical to said positive waveforms, except in polarity.
If, in an ideal case where the filter 6 was perfect, so that no electron was to be found in the area 5 adjacent to the acceleration and extraction grid 4, and where the bias signal B was applied to said grid:
Thus, in this ideal case, at the output from the generator I there would then appear, alternately but almost simultaneously, as many positive ions A+ as negative ions A−, which would combine and form the electrically neutral plasma beam PB.
However, in reality, for various reasons (for example, because the magnetic filter 6 is not perfect) some electrons e− are to be found in the area 5 adjacent to the extraction and acceleration grid 4, and therefore at the outlet from the plasma [beam] generation device, so that the plasma beam PB, which results from the grid 4 being biased by the biasing signal B, cannot be electrically neutral.
In order to remedy this disadvantage, according to the present invention, the electrical biasing device 9 is controllable and is able to produce a biasing signal B′ consisting of a sequence of positive rectangular waveforms b′+ and negative rectangular waveforms b′− whose amplitude a′ and duration d′ can be varied.
In addition, the device I has a sensor 12, for example an induction sensor, capable of detecting a lack of electrical neutrality in the beam PB and of acting on the controllable electrical biasing device 9 so that said device varies the amplitude a′ and/or the duration d′ of the positive waveforms b′+ and/or the negative waveforms b′−, in order to make this lack of neutrality disappear. Thus, the plasma beam PB can be made electrically neutral in real time.
As a variant, the sensor 12 can be replaced by an electrical current sensor 13, monitoring, for example, for the presence of any current in the grid 7.
In addition, in order to further improve the electrical neutrality of the plasma beam PB, in the plasma generator I of
The plasma generation device II, according to the present invention and shown diagrammatically in
This extraction and acceleration grid 24 is biased by an electrical biasing device 26, of the same type as the device 9 described above, capable of issuing a signal B″ consisting of a series of positive waveforms b″+ and negative waveforms b″− whose amplitude a″ and duration d″ can be varied.
In a similar manner to that described above as regards the device I, the positive ions X+ are extracted and accelerated during the positive waveforms b″+ and the electrons e− are extracted and accelerated during the negative waveforms b″−. Given the differences in mass and mobility between the positive ions X+ and the electrons e−, the duration and the amplitude of the negative waveforms b″− are very much less than those of the positive waveforms b″−, as can be seen in
In addition, the device II has a sensor 27, for example an induction sensor (or a sensor 28 monitoring for the presence of electrical current in the grid 25), capable of detecting a lack of electrical neutrality in the beam PB and of acting on the controllable electric biasing device 26 so that said device varies the amplitude a″ and/or the duration d″ of the positive waveforms b″+ and/or the negative waveforms b″−, in order to cause any lack of electrical neutrality in the plasma beam PB to disappear.
Thus, at the outlet of the plasma generator device II, ions X+ and electrons e− appear which, by combining, form an electrically-neutral plasma beam PB, without the aid of an auxiliary source of electrons.
As described previously in relation to the plasma generation device I, a line 10 can ensure that the signal B″ is synchronised with the pulsed ionising electric field RF.
Number | Date | Country | Kind |
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1057890 | Sep 2010 | FR | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/FR11/52090 | 9/14/2011 | WO | 00 | 6/26/2013 |