a-3c show top views of the different planes of the directional coupler of
The second coupling line 15 for decoupling the forward power is disposed at a larger vertical separation from the transmission line 11. The second coupling line 15 is also disposed on an electrical insulator 16 that is designed as a printed circuit board. Due to the larger separation between the second coupling line 15 and the transmission line 11, power is decoupled at a smaller coupling factor by way of the second coupling line 15. The separation between the second coupling line 15 and the transmission line 11 can be predetermined. The coupling line 15 is offset from the transmission line 11 by the vertical separation, and the coupling line 15 does not overlap the first coupling line 13. This ensures electrical decoupling of the two coupling lines 13, 15.
Each coupling line 13, 15 has a predetermined and adjusted characteristic impedance, and the impedance can be adjusted with precision by selecting or by determining the separations between, the coupling line 13, 15 and the ground surface 10. Because the reference potential of the ground surface 10 is fixed, a fixed characteristic impedance can be predetermined with, precision, reliability, and high repetition accuracy. In some implementations, the characteristic impedance of each coupling line 13, 15 can be set as that commonly used in industry. For example, the characteristic impedance can be 50 ohms or 75 ohms. In some implementations, the characteristic impedance can be adjusted by adjusting the length and/or width of the coupling lines 13, 15.
A second reference member that is at ground potential (in this implementation, the second reference member is a second ground surface 17) is provided in a further plane adjacent the insulator 16. The ground surfaces 10, 17 can be connected to several through-contacts (not shown) formed in the printed circuit boards of the insulators 12, 14, 16 to electrically connect the ground surfaces 10, 17 in order to ensure that the current in the ground surfaces 10, 17 is homogeneous. The coupling lines 13, 15 are disposed at a defined vertical separation from the ground surface 17, thereby precisely determining the characteristic impedance of the coupling lines 13, 15. Additionally, there is no coupling line (either 13 or 15) between the transmission line (11) and a ground potential such as the ground surface 10. The characteristic impedance is determined by the length and the width of the coupling lines 13, 15. The length and width of the coupling lines 13, 15 and the vertical separation of the coupling lines 13, 15 from the ground surface 17 are thereby matched in order to obtain a defined, predetermined characteristic impedance for each coupling line 13, 15.
The separation between the coupling lines 13, 15 and one or more of the ground surfaces 10, 17 can be predetermined. Moreover, the characteristic impedance of each coupling line 13, 15 can be adjusted with some precision based on one ground reference potential and the electrical coupling between the transmission line 11 and the coupling lines 13, 15 can be adjusted using the second ground reference member.
The coupling lines 13, 15 can be embedded between the respective electrical insulators 12, 14 and 14, 16. The transmission line 11 can be insulated from the ground surface 10.
Coupling between the coupling lines 13, 15 and the transmission line 11 can be effected through electrical and magnetic fields. If done in this manner, the electric and magnetic couplings need to be balanced. Magnetic coupling can be done through the progression of the lines of magnetic flux in the area of the section where the coupling lines 13, 15 are guided in the direct vicinity of the transmission line 11. Electric coupling can be produced through the progression of the lines of electric flux between the transmission line 11 and the respective coupling line 13 or 15, and the area of the respective coupling line. Short coupling lines 13, 15 imply little magnetic coupling, and to provide balance, little electric coupling would be required in this case.
The progression of the lines of flux can be deflected by the ground surface 10, which, in the implementation shown in
In some implementations, the forward power and the reflected power (or values describing them) can be decoupled from the transmission line 11 with different coupling factors (that is, that portion of power that is coupled out of the transmission line 11 by ground surface 10). Usually, the reflected power is smaller than the forward power. If the reflected power is decoupled with a larger coupling factor than the forward power, the signal-to-noise ratio at the input of the evaluation device 7 increases because the temporal behavior of the evaluation device 7 in reaction to an input signal is advantageously utilized. In this way, the reflected power can be measured more precisely. Different coupling factors can be realized by positioning the coupling lines 13, 15 at different separations from the transmission line 11. The coupling factors are also influenced by the length and width of the coupling lines 13, 15, and the width and the length of the transmission line 11. The coupling factors can be adjusted by disposing the transmission line 11, the coupling line 13, and the coupling line 15 in different planes. Moreover, the coupling lines 13, 15 can be offset from each other to reduce or prevent coupling between the coupling lines and therefore to reduce or prevent errors in the measurement results.
In another implementation, the first ground surface 10 can be disposed in a plane that is distinct from the plane in which the transmission line 11 is disposed. For example, the first ground surface 10 can be disposed in a plane that is above and is parallel with a plane of the transmission line 11. The ground surface 10 influences the electric field in the surroundings of the transmission line 11. With this measure, the electric coupling between the transmission line 11 and the coupling lines 13, 15 can be influenced and adjusted.
a shows a top view of the ground surface 10 and the transmission line 11. The transmission line 11 is completely embedded in the ground surface 10 and is thereby also shielded by it. The directional coupler 3 can include an input terminal 21 for connecting to the HF generator 2 and an output terminal 20 for connecting to the plasma load 4.
b shows a top view of the electrical insulator 14 on which the first coupling line 13 is disposed. The coupling line 13 is bent outside of a coupling area 22, and in the coupling area 22, the first coupling line 13 extends parallel to the transmission line 11 such that connections 23, 24 of the first coupling line 13 are remote from the transmission line 11. A resistance 35 is exclusively connected to the connection 23, and the resistance 25 has resistance value that corresponds within a suitable tolerance to the characteristic impedance of the first coupling line 13. The connection 23 electrically couples to the transmission line 11. The connection 24 can be connected to the measuring device 6 to supply a quantity that describes the reflected power Pr.
c shows a top view of the insulator 16 on which the second coupling line 15 is disposed. The coupling line 15 is bent outside of the coupling area 22, and in the coupling area 22, the second coupling line 15 extends parallel to the transmission line 11 such that connections 26, 27 of the second coupling line 15 are remote from the transmission line 11 and from the connections 23, 24 of the first coupling line 13. A resistance 28 is exclusively connected to the connection 26, and the resistance 28 has a resistance value that corresponds within a suitable tolerance to the characteristic impedance of the second coupling line 15. The connection 26 electrically couples to the transmission line 11. The connection 27 can be connected to the measuring device 5 to supply a quantity that describes the forward power Pi.
In some implementations, the length of the coupling lines 13, 15 in the coupling areas 22 can be less than λ/4. In other implementations, the length of the coupling lines 13, 15 in the coupling areas 22 can be less than λ/8. In other implementations, the length of the coupling lines 13, 15 in the coupling areas 22 can be less than λ/10. In this way, the dimensions of the directional coupler 3 can be kept relatively small. If the coupling lines 13, 15 are relatively short, for example, shorter than λ/4, then coupling between the coupling lines 13, 15 and the transmission line 11 in accordance with line theory can be neglected.
For example, the resistance values of the resistances 25, 38 can match or equal the characteristic impedance of the directional coupler 3. That is, the resistance values of the resistances 25, 28 can correspond (within a tolerance of less than ±10%) to the characteristic impedance of the respective coupling line 13, 15. As another example, the resistance values of the resistances 25, 28 can correspond within a tolerance of less than ±5% to the characteristic impedance of the respective coupling line 13, 15. As a further example, the resistance values of the resistances 25, 28 can correspond within a tolerance of less than ±1% to the characteristic impedance of the respective coupling line 13, 15. Moreover, reflections produced by the measurement can be absorbed at the resistances 25, 28 and therefore no new reflections are produced that can potentially contribute to measurement errors at the other coupling line. Reflections due to mismatch can be reduced or prevented through adjustment of the resistances 25, 28 relative to the characteristic impedances of the coupling lines 13, 15 and the tolerances in the directional coupler 3 can be compensated for by such adjustment.
If the directional coupler 3 is designed for operation at frequencies of less than 200 MHz or at frequencies of less than 40 MHz, it can be well suited for operation in HF plasma process excitation configurations such as the configuration 1.
In
The connecting fines 37, 38 can be produced from any electrically conductive material such as copper or silver, which have a high electric conductivity. The length of the connecting lines 37, 38 can be ≦10 mm and the width can be ≧5 mm, in particular ≧10 mm. The flat short design of the connecting lines 37, 38 realizes a low-inductance connection between the outer conductor 35 and the ground of the HF generator 2 through the ground surface 17.
The housing 30 can be modified in order to increase the resistance for the returned HF current to thereby ensure that the return current flows substantially through the ground surface 17. For example, the housing 30 can be modified such that connecting elements (that is, elements that connect the HF generator 2 to the housing 30, for example, the lines 37, 38) between the housing 30 and the ground of the HF generator 2 can be ferrite rings. As another example, the connecting elements can be made of materials with a high relative permeability μr, since a high μr increases the skin effect, thereby impairing the HF current conduction. With this measure, the electric and magnetic fields are formed, which are required for good coupling between the coupling lines 13, 15 and the transmission line 11.
In this way, the entire return current from the plasma load 4 to the HF generator 2 flows through the ground surface 17. The DC resistance of the housing 30 can be increased by introducing inductances into the current path. Alternatively or additionally, the current path can be built up with little inductance through the ground potential of the directional coupler 3 to the ground of the HF generator 2.
It is to be understood that while the invention has been described in conjunction with the detailed description thereof, the foregoing description is intended to illustrate and not limit the scope of the invention, which is defined by the scope of the appended claims. Other aspects, advantages, and modifications are within the scope of the following claims.
Number | Date | Country | Kind |
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EP 06 006 202.3 | Mar 2006 | EP | regional |
This application claims priority under 35 U.S.C. §119(a) to European Application No. 06 006 202.3, filed on Mar. 25, 2006, and under 35 U.S.C. §119(e) from U.S. Provisional Application No. 60/745,791, filed Apr. 27, 2006. Both of these priority applications are hereby incorporated by reference in their entirety.
Number | Date | Country | |
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60745791 | Apr 2006 | US |