Plasma processing apparatus and filter unit

A filter unit 54(IN) includes a housing 82 formed of a cylindrical conductor. Further, in the housing 82, the air-core solenoid coils AL1 and BL1; the first capacitors AC1 and BC1; the troidal coils AL2 and BL2; and the second capacitors AC2 and BC2 are arranged in this sequence from top to bottom. In the vicinity of the air-core solenoid coils AL1 and BL1, a multiple number of rod-shaped comb-teeth members 86, which are extended in parallel to a coil axis direction, are provided adjacent to outer peripheries of the air-core solenoid coils AL1 and BL1 at a regular interval in a circumferential direction thereof. A comb teeth M are formed on an inner surface of each comb-teeth member 86, and the comb teeth M are inserted into winding gaps of the air-core solenoid coils AL1 and BL1.

CROSS-REFERENCE TO RELATED APPLICATION

This Application is a U.S. national phase application under 35 U.S.C. §371 of PCT Application No. PCT/JP2014/002614 filed on May 19, 2014, which claims the benefit of Japanese Patent Application No. 2013-110201 filed on May 24, 2013, the entire disclosures of which are incorporated herein by reference.

TECHNICAL FIELD

The embodiments described herein pertain generally to a plasma processing apparatus configured to perform a plasma process on a processing target substrate by using a high frequency power; and, more particularly, to a plasma processing apparatus equipped with a filter for blocking a high frequency noise introduced into a line such as a power feed line or a signal line from an electrical member other than a high frequency electrode within a processing vessel.

BACKGROUND ART

In micro-processing for manufacturing a semiconductor device or a FPD (Flat Panel Display) using plasma, it is very important to control a temperature or a temperature distribution of a processing target substrate (a semiconductor wafer, a glass substrate, etc.) as well as to control a plasma density distribution on the processing target substrate. If the temperature control of the substrate is not properly performed, not only the uniformity of a surface reaction of the substrate but also the uniformity of process characteristics may not be achieved, so that a production yield of semiconductor devices or display devices is decreased.

In general, a mounting table or susceptor, which mounts thereon a processing target substrate within a chamber of a plasma processing apparatus (particularly, a capacitively coupled plasma processing apparatus), has a function as a high frequency electrode that applies a high frequency power into a plasma space, a function as a holder that holds thereon the substrate by electrostatic attraction or the like, and a function as a temperature controller that controls the temperature of the substrate to a preset temperature through heat transfer. As for the temperature control function, it is required to appropriately correct a heat input characteristic distribution of the substrate affected by non-uniform radiant heat from plasma or a wall of the chamber, or a heat distribution affected by a substrate supporting structure.

Conventionally, in order to control the temperature of the susceptor and, further, the temperature of the substrate, a heater structure is widely employed. In this heater structure, a heating element that generates heat by an electric current applied thereto is provided in the susceptor, and Joule heat generated by the heating element is controlled. When using this heater structure, however, a part of a high frequency power applied to the susceptor from a high frequency power supply may be easily introduced into a heater power feed line through the heating element as a noise. If this high frequency noise reaches a heater power supply through the heater power feed line, operation and performance of the heater power supply is degraded. Furthermore, if a high frequency current flows in the heater power feed line, the high frequency power may be wasted. Typically, to solve these problems, a filter that reduces or blocks the high frequency noise flowing from the heating element embedded in the susceptor is provided on the heater power feed line. Typically, this kind of filter is provided outside the chamber (processing vessel) to be located directly under the susceptor.

The present applicant describes, in Patent Document 1, a filter technique that provides improved filter performance for blocking a high frequency noise introduced to a line such as a power feed line or a signal line from an electrical member other than a high frequency electrode within a processing vessel of a plasma processing apparatus. This filter technique employs a regular multiple parallel resonance characteristic of a distributed constant line. Accordingly, only one air coil is provided within the filter.Patent Document 1: Japanese Patent Laid-open Publication No. 2011-135052

DISCLOSURE OF THE INVENTION

Problems to be Solved by the Invention

In the capacitively coupled plasma processing apparatus, in order to improve function and controllability of the high frequency power in the plasma process, multiple high frequency powers of different frequencies are often applied to the electrode within the processing vessel. By way of example, in an apparatus of applying dual high frequency powers to a lower electrode, a first high frequency power HF having a relatively high basic frequency (typically, 27 MHz or higher) suitable for plasma generation and a second high frequency power having a relatively low basic frequency (typically, 13 MHz or less) suitable for controlling energy of ions attracted to a processing target substrate from plasma are both applied to a susceptor (lower electrode) on which the processing target substrate is mounted. In this case, noises of the first and second high frequency powers HF and LF are introduced into a heater power feed line at the same time through a heating element which is embedded in the susceptor to control a temperature of the processing target substrate. A filter provided on the heater power feed line is required to block the high frequency noises of the two different high frequency powers at the same time.

In the filter described in Patent Document 1, inductance required for an air core coil, i.e., a size of the coil (particularly, a length of the coil in an axial direction) is determined based on the basic frequency of the second high frequency power LF, which is the lowest frequency among the frequencies to be blocked. The lower the basic frequency of the second high frequency power LF is, the longer the length of the coil needs to be. For example, when the basic frequency of the second high frequency power LF is 3.2 MHz, the length of the coil needs to be 200 mm or larger, whereas when the basic frequency of the second high frequency power LF is 400 kHz, the length of the coil needs to be 750 mm or larger. If the size of the air core coil increases, however, resistance of a conducting wire of the coil also increases, so that Joule heat generated when an electric current from a heater power supply flows is increased. As a consequence, a power loss within the filter is increased. Furthermore, if the size of the air core coil, i.e., the filter size is increased, it may be difficult to design a layout of various kinds of power supply systems provided under the susceptor or a chamber.

In addition, in the filter described in Patent Document 1, there is obtained a frequency-impedance characteristic in which multiple parallel resonance frequencies appear at a substantially constant frequency interval due to multiple parallel resonance of a distributed constant line formed by the air core coil and a cylindrical outer conductor surrounding the air core coil. Since, however, these parallel resonance frequencies are obtained at the regular frequency interval, it is very difficult to match the multiple parallel resonance with the frequencies of the two high frequency powers HF and LF at the same time, which are selected in consideration of various aspects such as the kind or specification of a process involved.

Particularly, if the filter of Patent Document 1 is designed to match the lowest parallel resonance frequency of the multiple parallel resonance with the basic frequency of the second high frequency power LF set to be of a low value, e.g., 3.2 MHz or 400 kHz, the air core coil is scaled up as described above, and there is obtained a frequency-impedance characteristic in which an interval between the resonance frequencies is very small and a gradient (change rate) is sharp. For this reason, if there is even a slight error or non-uniformity in the filter design, the basic frequency to be blocked is affected by a next serial resonance frequency rather than a parallel resonance frequency, so that remarkably low impedance may be obtained, and a filter function may not be properly exerted. Accordingly, design, manufacture and control of the filter may be difficult, and an apparatus difference on a plasma processing apparatus level may be easily generated.

In view of the foregoing problems, exemplary embodiments provide a plasma processing apparatus and a filter unit capable of improving reproducibility and reliability of a plasma process by applying sufficiently high impedance efficiently, stably and securely to undesired high frequency noises of multiple frequencies, which are introduced into a line such as a power feed line or a signal line from an electrical member other than a high frequency electrode within a processing vessel.

Means for Solving the Problems

In a first exemplary embodiment, a plasma processing apparatus includes an external circuit of a power meter or a signal meter electrically connected via a line to an electrical member within a processing vessel in which a plasma process is performed. In the plasma processing apparatus, noises of multiple high frequency powers of different frequencies introduced from the electrical member into the line toward the external circuit are reduced or blocked by a filter provided on the line. Further, the filter includes an air-core solenoid coil provided at an uppermost portion of the filter, when viewed from a side of the electrical member, and configured to block noises of a single or plural high frequency powers among the noises of the multiple high frequency powers except a high frequency power having a lowest frequency; insulating comb teeth inserted in winding gaps of the air-core solenoid coil locally at plural positions in a circumferential direction thereof; a coil having a core connected in series to the air-core solenoid coil, and configured to block a noise of the high frequency power having the lowest frequency; and a cylindrical conductor, accommodating or surrounding at least the air-core solenoid coil, configured to form, by being combined with the air-core solenoid coil, a distributed constant line in which parallel resonance occurs at multiple frequencies.

Within a plasma processing apparatus in which an electrical member within a processing vessel in which a plasma process is performed is electrically connected via a line to an external circuit provided outside the processing vessel, a filter provided on the line is configured to reduce or block noises of multiple high frequency powers of different frequencies introduced from the electrical member into the line toward the external circuit. The filter unit includes an air-core solenoid coil provided at an uppermost portion of the filter, when viewed from a side of the electrical member, and configured to block noises of a single or plural high frequency powers among the noises of the multiple high frequency powers except a high frequency power having a lowest frequency; insulating comb teeth inserted in winding gaps of the air-core solenoid coil locally at plural positions in a circumferential direction thereof; a coil having a core connected in series to the air-core solenoid coil, and configured to block a noise of the high frequency power having the lowest frequency; and a cylindrical conductor, accommodating or surrounding at least the air-core solenoid coil, configured to form, by being combined with the air-core solenoid coil, a distributed constant line in which parallel resonance occurs at multiple frequencies.

In the first exemplary embodiment, the air-core solenoid coil provided at the first stage of the filter blocks the high frequency noise having the higher frequency among the noises of the multiple high frequency powers introduced from the electrical member within the processing vessel into the line toward the external circuit outside the processing vessel, whereas the troidal coil provided at the next stage of the filter blocks the high frequency noise having the lowest frequency having passed through the air-core coil. That is, the air-core solenoid and the troidal coil are configured to perform the filter blocking functions against the high frequency noise having the higher frequency and the high frequency noise having the lower frequency, respectively.

Further, in the first exemplary embodiment, the winding pitch of the air-core solenoid coil is accurately adjusted to a set value by the comb-teeth pitch, so that a frequency-impedance characteristic having high reproducibility and little object difference can be obtained. Furthermore, since air gaps are formed between respective winding gaps of the air-core solenoid coil except where the comb teeth are inserted, heat generated from the coil is rapidly discharged out through the air gaps. Thus, the air-core solenoid coil can be cooled efficiently.

In a second exemplary embodiment, a plasma processing apparatus includes an external circuit of a power meter or a signal meter electrically connected via a line to an electrical member within a processing vessel in which a plasma process is performed. In the plasma processing apparatus, noises of multiple high frequency powers of different frequencies introduced from the electrical member into the line toward the external circuit are reduced or blocked by a filter provided on the line. The filter further includes an air-core solenoid coil provided at an uppermost portion of the filter, when viewed from a side of the electrical member, and configured to block noises of a single or plural high frequency powers among the multiple high frequency powers except a high frequency power having a lowest frequency; insulating comb teeth inserted in winding gaps of a first section of the air-core solenoid coil locally at plural positions in a circumferential direction thereof; a coil tube configured to block winding gaps of a second section of the air-core solenoid coil in the entire circumferential direction; a coil having a core connected in series to the air-core solenoid coil, and configured to block a noise of the high frequency power having the lowest frequency; and a cylindrical conductor, accommodating or surrounding at least the air-core solenoid coil, configured to form, by being combined with the air-core solenoid coil, a distributed constant line in which parallel resonance occurs at multiple frequencies.

Within a plasma processing apparatus in which a heating element provided in a first electrode within a processing vessel in which a plasma process is performed is electrically connected via a power feed line to a heater power supply provided outside the processing vessel, a filter unit provided on the power feed line is configured to reduce or block noises of multiple high frequency powers of different frequencies introduced from the heating element into the power feed line toward the heater power supply. The filter unit includes an air-core solenoid coil provided at an uppermost portion of the filter, when viewed from a side of the heating element, and configured to block noises of a single or plural high frequency powers among the multiple high frequency powers except a high frequency power having a lowest frequency; insulating comb teeth inserted in winding gaps of a first section of the air-core solenoid coil locally at plural positions in a circumferential direction thereof; a coil tube configured to block winding gaps of a second section of the air-core solenoid coil entirely in the circumferential direction; a coil having a core connected in series to the air-core solenoid coil, and configured to block a noise of the high frequency power having the lowest frequency; and a cylindrical conductor, accommodating or surrounding at least the air-core solenoid coil, configured to form, by being combined with the air-core solenoid coil, a distributed constant line in which parallel resonance occurs at multiple frequencies.

In the second exemplary embodiment, the air-core solenoid coil provided at the first stage of the filter blocks the high frequency noise having the higher frequency among the noises of the multiple high frequency powers introduced from the electrical member within the processing vessel into the line toward the external circuit outside the processing vessel, whereas the troidal coil at the next stage of the filter blocks the high frequency noise having the lowest frequency having passed through the air-core solenoid coil. That is, the air-core solenoid and the troidal coil are configured to perform the filter blocking functions against the high frequency noise having the higher frequency and the high frequency noise having the lower frequency, respectively.

Furthermore, in the second exemplary embodiment, first insulating comb teeth are inserted into the winding gaps of the air-core solenoid coil in the first section thereof locally at the plural positions in the circumferential direction thereof, and a second coil tube blocks the winding gaps of the air-core solenoid coil in the second section thereof entirely in the circumferential direction. Accordingly, it is possible to shift a part or all of resonance frequencies of multiple parallel resonance by changing the characteristic impedance in each section, while maintaining a distance interval of the distributed constant line or a coaxial line formed between the air-core solenoid coil and the cylindrical conductor to be uniform.

In a third exemplary embodiment, a plasma processing apparatus includes an external circuit of a power meter or a signal meter electrically connected via a line to an electrical member within a processing vessel in which a plasma process is performed. In the plasma processing apparatus, noises of multiple high frequency powers of different frequencies introduced from the electrical member into the line toward the external circuit are reduced or blocked by a filter provided on the line. Further, the filter includes an air-core solenoid coil provided at an uppermost portion of the filter, when viewed from a side of the electrical member, and configured to block noises of a single or plural high frequency powers among the noises of the multiple high frequency powers except a high frequency power having a lowest frequency; a first coil tube, having a first dielectric constant, configured to block winding gaps of a first section of the air-core solenoid coil entirely in a circumferential direction; a second coil tube, having a second dielectric constant, configured to block winding gaps of a second section of the air-core solenoid coil entirely in the circumferential direction; a coil having a core connected in series to the air-core solenoid coil, and configured to block a noise of the high frequency power having the lowest frequency; and a cylindrical conductor, accommodating or surrounding at least the air-core solenoid coil, configured to form, by being combined with the air-core solenoid coil, a distributed constant line in which parallel resonance occurs at multiple frequencies.

Within a plasma processing apparatus in which an electrical member within a processing vessel in which a plasma process is performed is electrically connected via a line to an external circuit provided outside the processing vessel, a filter unit provided on the line is configured to reduce or block noises of multiple high frequency powers of different frequencies introduced from the electrical member into the line toward the external circuit. Here, the filter unit includes an air-core solenoid coil provided at an uppermost portion of the filter, when viewed from a side of the electrical member, and configured to block noises of a single or plural high frequency powers among the multiple high frequency powers except a high frequency power having a lowest frequency; a first coil tube, having a first dielectric constant, configured to block winding gaps of a first section of the air-core solenoid coil entirely in a circumferential direction; a second coil tube, having a second dielectric constant, configured to block winding gaps of a second section of the air-core solenoid coil entirely in the circumferential direction; a coil having a core connected in series to the air-core solenoid coil, and configured to block a noise of the high frequency power having the lowest frequency; and a cylindrical conductor, accommodating or surrounding at least the air-core solenoid coil, configured to form, by being combined with the air-core solenoid coil, a distributed constant line in which parallel resonance occurs at multiple frequencies.

In the third exemplary embodiment, the air-core solenoid coil provided at the first stage of the filter blocks the high frequency noise having the higher frequency among the noises of the multiple high frequency powers introduced from the electrical member within the processing vessel into the line toward the external circuit outside the processing vessel, whereas the troidal coil provided at the next stage of the filter blocks the high frequency noise having the lowest frequency having passed through the air-core solenoid coil. That is, the air-core solenoid and the troidal coil are configured to perform the filter blocking functions against the high frequency noise having the higher frequency and the high frequency noise having the lower frequency, respectively.

In the third exemplary embodiment, the first coil tube having the first dielectric constant blocks the winding gaps of the air-core solenoid coil in the first section thereof entirely in the circumferential direction, and the second coil tube having the second dielectric constant blocks the winding gaps of the air-core solenoid coil in the second section thereof entirely in the circumferential direction. Accordingly, it is possible to shift a part or all of resonance frequencies of multiple parallel resonance by changing characteristic impedance in each section, while maintaining a distance interval of the distributed constant line or a coaxial line formed between the air-core solenoid coil and the cylindrical conductor to be uniform.

Effect of the Invention

According to the plasma processing apparatus and the filter unit of the exemplary embodiments, with the above-described configuration and operation, it is possible to improve reproducibility and reliability of the plasma process by applying sufficiently high impedance to the high frequency noises of multiple frequencies introduced into the line such as a power feed line or a signal line from the electrical member other than the high frequency electrode within the processing vessel.

DETAILED DESCRIPTION

In the following, exemplary embodiments will be described in detail, and reference is made to the accompanying drawings, which form a part of the description.

<Overall Configuration of Plasma Processing Apparatus>

FIG. 1illustrates a configuration of a plasma processing apparatus in accordance with a first exemplary embodiment. The plasma processing apparatus is configured as a capacitively coupled plasma etching apparatus in which dual frequency powers are applied to a lower electrode. The plasma etching apparatus includes a cylindrical chamber (processing vessel)10made of, e.g., a metal material such as aluminum or stainless steel. The chamber10is grounded.

A circular plate-shaped susceptor12configured to mount thereon a processing target substrate, e.g., a semiconductor wafer W is horizontally disposed as a lower electrode in the chamber10. The susceptor12is made of, but not limited to, aluminum and supported on an insulating cylindrical supporting member14without being grounded. The insulating cylindrical supporting member14is made of, but not limited to, a ceramic material and vertically extended upwards from a bottom of the chamber10. An annular exhaust path18is formed between an inner wall of the chamber10and a conductive cylindrical supporting member16that is vertically extended upwards from the bottom of the chamber10along a periphery of the insulating cylindrical supporting member14. An exhaust opening20is formed at a bottom of the exhaust path18, and an exhaust device24is connected to the exhaust opening20through an exhaust pipe22. The exhaust device24includes a vacuum pump such as a turbo molecular pump and is capable of depressurizing a processing space within the chamber10to a required vacuum level. A gate valve26configured to open and close a loading/unloading opening for the semiconductor wafer W is provided at a sidewall of the chamber10.

The susceptor12is electrically connected with a first high frequency power supply28and a second high frequency power supply30via a matching unit32and a power feed rod34. The first high frequency power supply28is configured to output a first high frequency power HF of a certain frequency (typically, equal to or higher than, e.g., about 27 MHz) that mainly contributes to plasma generation. Meanwhile, the second high frequency power supply30is configured to output a second high frequency power LF of a certain frequency (typically, equal to or lower than, e.g., about 13 MHz) that mainly contributes to ion attraction into the semiconductor wafer W mounted on the susceptor12. The matching unit32accommodates a first matching device and a second matching device (not shown) configured to match impedance between the first and second high frequency power supplies28and30and a plasma load, respectively.

The power feed rod34is made of a cylindrical or columnar conductor having a certain outer diameter. An upper end of the power feed rod34is connected to a central portion of a bottom surface of the susceptor12, and a lower end of the power feed rod34is connected to high frequency output terminals of the first and second matching devices within the matching unit32. Further, a cylindrical conductive cover35surrounding the power feed rod34is provided between a bottom surface of the chamber10and the matching unit32. To elaborate, a circular opening having a certain diameter larger than the outer diameter of the power feed rod34is formed at the bottom surface of the chamber10. An upper end of the conductive cover35is connected to this opening of the chamber while a lower end thereof is connected to ground (returning wire) terminals of the matching devices.

The susceptor12has a diameter larger than that of the semiconductor wafer W. A top surface of the susceptor12is divided into a central region having the substantially same shape (circular shape) and the substantially same size as those of the wafer W, i.e., a wafer mounting portion; and an annular peripheral region extended outwards from the wafer mounting portion. The semiconductor wafer W as a processing target object is mounted on the wafer mounting portion. A ring-shaped plate member, i.e., a so-called focus ring36is mounted on the annular peripheral region. The focus ring36has an inner diameter larger than the diameter of the semiconductor wafer W and may be made of, by way of example, but not limitation, one of Si, SiC, C and SiO2depending on a material of the semiconductor wafer W to be etched.

An electrostatic chuck38configured to attract and hold the wafer and a heating element40are provided on the wafer mounting portion of the top surface of the susceptor12. In the electrostatic chuck38, a DC electrode44is embedded within a film-shaped or plate-shaped dielectric member42that is formed or fastened on the top surface of the susceptor12as one body therewith. The DC electrode44is electrically connected with a DC power supply45provided at the outside of the chamber10via a switch46, a resistor48having a high resistance value and a DC high voltage line50. If a high DC voltage is applied to the DC electrode44from the DC power supply45, the semiconductor wafer W can be attracted to and held on the electrostatic chuck38by a Coulomb force. The DC high voltage line50is a coated line and is connected to the DC electrode44of the electrostatic chuck38while penetrating the susceptor12from below after passing through the inside of the cylindrical power feed rod34.

The heating element40is implemented by, for example, a resistance heating wire having a spiral shape, which is embedded in the dielectric member42of the electrostatic chuck38along with the DC electrode44. In this exemplary embodiment, this heating element40is divided in two parts in a radial direction of the susceptor12: an inner heating wire40(IN) and an outer heating wire40(OUT), as depicted inFIG. 2. Among these components, the inner heating wire40(IN) is electrically connected to a dedicated heater power supply58(IN) provided at the outside of the chamber10via power feed conductors52(IN) covered with an insulating coating, a filter unit54(IN) and electric cables56(IN). The outer heating wire40(OUT) is electrically connected to a dedicated heater power supply58(OUT) provided at the outside of the chamber10via power feed conductors52(OUT) covered with an insulating coating, a filter unit54(OUT) and electric cables56(OUT). Among these components, the filter units54(IN) and54(OUT) are primary features of the present exemplary embodiment, and an internal configuration and an operation of these filter units will be described in detail later.

An annular coolant room or coolant path60extended along, e.g., a circumferential direction is formed within the susceptor12. A coolant of a preset temperature, e.g., cooling water cw from a chiller unit (not shown) is supplied into and circulated through the coolant path60via a coolant supply line. A temperature of the susceptor12can be reduced by adjusting the temperature of the coolant. Further, a heat transfer gas such as a He gas from a heat transfer gas supply unit (not shown) is supplied to an interface between the electrostatic chuck38and the semiconductor wafer W through a gas supply line and a gas passage62within the susceptor12in order to thermally connect the semiconductor wafer W to the susceptor12.

A shower head64serving as an upper electrode is provided at a ceiling of the chamber10, facing the susceptor12in parallel. The shower head64includes an electrode plate66directly facing the susceptor12; and an electrode supporting body68configured to support the electrode plate66from a backside thereof (from above it) in a detachable manner. A gas room70is formed within the electrode supporting body68, and a multiple number of gas discharge holes72extended from the gas room70toward the susceptor12are formed through the electrode supporting body68and the electrode plate66. A space SP between the electrode plate66and the susceptor12serves as a plasma generation space or a processing space. A gas supply line76led from a processing gas supply unit74is connected to a gas inlet opening70aformed at a top portion of the gas room70. The electrode plate66may be made of, by way of non-limiting example, but not limitation, Si, SiC or C, and the electrode supporting body68may be made of, by way of example, but not limitation, alumite-treated aluminum.

Operations of individual components of the plasma etching apparatus, e.g., the exhaust device24, the high frequency power supplies28and30, the switch46of the DC power supply45, the heater power supplies58(IN) and58(OUT), the chiller unit (not shown), the heat transfer gas supply unit (not shown), the processing gas supply unit74, and so forth and the overall operation (sequence) of the plasma etching apparatus are controlled by a controller75having a microcomputer.

A basic single-substrate dry-etching operation in this plasma etching apparatus is performed as follows. First, the gate valve26is first opened, and the semiconductor wafer W to be processed is loaded into the chamber10and mounted on the electrostatic chuck38. Then, an etching gas (generally, a mixture gas) is introduced into the chamber10from the processing gas supply unit74at a certain flow rate, and an internal pressure of the chamber10is controlled to a preset value by the exhaust device24. Further, the first and second high frequency power supplies28and30are powered on, and the first and second high frequency power supplies28and30output the first high frequency power HF and the second high frequency power LF at required power levels, respectively, and apply the high frequency powers HF and LF to the susceptor (lower electrode)12via the matching unit32and the power feed rod34. Further, the heat transfer gas (e.g., a He gas) is supplied to the interface between the electrostatic chuck38and the semiconductor wafer W from the heat transfer gas supply unit. Further, by turning on the switch46for the electrostatic chuck, the heat transfer gas is confined into the interface between the electrostatic chuck38and the semiconductor wafer W by an electrostatic attracting force. Meanwhile, by turning on the heater power supplies58(IN) and58(OUT), Joule heats are generated by the inner heating wire40(IN) and the outer heating wire40(OUT), respectively, so that the temperature or a temperature distribution of the top surface of the susceptor12can be controlled to a preset value. The etching gas discharged from the shower head64is excited into plasma by a high frequency discharge between the susceptor12and the shower head64(i.e., between the two facing electrodes). A processing target film on the surface of the semiconductor wafer W is etched to have a required pattern by radicals or ions in the plasma.

This plasma etching apparatus is of a cathode-coupled type, and by applying the first high frequency power HF having a relatively high frequency (desirably, equal to or higher than 27 MHz) suitable for plasma generation to the susceptor12, plasma can be highly densified in a desirably dissociated state. Accordingly, high-density plasma can be generated under a lower pressure condition. Further, by applying the second high frequency power LF having a relatively lower frequency (equal to or lower than 13 MHz) suitable for ion attraction to the susceptor12, an anisotropic etching process having high selectivity can be performed on the semiconductor wafer W mounted on the susceptor12.

Especially, in this exemplary embodiment, as will be described later, the first high frequency power HF and the second high frequency power LF have a high frequency range (typically, 40 MHz or higher) suitable for generating high-density plasma and a low frequency range (typically, 3.2 MHz or lower) suitable for controlling ion energy, respectively.

Moreover, in this capacitively coupled plasma etching apparatus, the susceptor12is cooled by the chiller unit and heated by the heater, and the heating by the heater is controlled independently at the central region and the peripheral region of the susceptor12in the radial direction thereof. Thus, the temperature can be changed and increased or decreased rapidly at a high speed, and profile of the temperature distribution can be controlled as required or in various ways.

Further, in this capacitively coupled plasma etching apparatus, during a plasma etching process, a part of the first high frequency power HF and a part of the second high frequency power LF applied to the susceptor12from the high frequency power supplies28and30, respectively, may be introduced as high frequency noises into the power feed conductors52(IN) and52(OUT) through the inner heating wire40(IN) and the outer heating wire40(OUT) embedded in the susceptor12, respectively. If any of these high frequency noises of the two different frequencies reaches the heater power supplies58(IN) and58(OUT), operation and performance of the heater power supplies58(IN) and58(OUT) may be degraded.

In this regard, as described above, the filter units54(IN) and54(OUT) are provided on heater power feed lines which electrically connect the heater power supplies58(IN) and58(OUT) and the inner heating wire40(IN) and the outer heating wire40(OUT), respectively. These filter units54(IN) and54(OUT) are configured to stably and securely perform a filter blocking function with sufficiently high impedance against any of the noises of the first and second high frequency powers HF and LF, which are introduced into the heater power feed lines from the inner and outer heating wires40(IN) and40(OUT), at low power consumption efficiently, as will be described in detail later. Accordingly, in this plasma etching apparatus of the exemplary embodiment, a wafer temperature control function using a heater is improved, and a leakage of the first and second high frequency powers HF and LF from the chamber10into the heater power feed lines through the heating element40within the susceptor12can be effectively suppressed or reduced. Thus, reproducibility and reliability of the plasma process can be improved.

<Circuit Configuration within Filter Unit>

Now, a circuit configuration within the filter units54(IN) and54(OUT), which is a major feature in this plasma processing apparatus, will be explained. Since the filter units54(IN) and54(OUT) have the same configuration and operation, only one filter unit54(IN) will be explained.

FIG. 3illustrates circuit configurations of heater power supply unit configured to apply a power to the heating element40which is provided in the susceptor12to control the temperature of the wafer. In this exemplary embodiment, the heater power supply units having the substantially same circuit configuration are connected to the inner heating wire40(IN) and the outer heating wire40(OUT) of the heating element40, respectively. With this configuration, heating amounts or heating temperatures of the inner heating wire40(IN) and the outer heating wire40(OUT) can be controlled individually. In the following description, a configuration and an operation of the heater power supply unit for the inner heating wire40(IN) will be elaborated. The heater power supply unit for the outer heating wire40(OUT) has the completely same configuration and operation.

The heater power supply58(IN) is an AC output power supply that performs a switching (ON/OFF) operation for a commercial frequency by using, e.g., SSR (Solid State Relay). The heater power supply58(IN) is connected with the inner heating wire40(IN) in a closed-loop circuit. To elaborate, a first output terminal of a pair of output terminals of the heater power supply58(IN) is electrically connected to a first terminal hAof the inner heating wire40(IN) via a first power feed line (power cable)80A and a second output terminal thereof is electrically connected to a second terminal hBof the inner heating wire40(IN) via a second power feed line (power cable)80B.

The filter unit54(IN) includes a first filter84A and a second filter84B configured to block high frequency noises introduced into the first and second power feed lines80A and80B, respectively, in a housing82. Here, the housing82is made of a cylindrical conductor and grounded. The filters84A and84B have substantially the same circuit configuration, and characteristic values of corresponding reactance elements between the two filters are also substantially same.

More specifically, in the filter84A (84B), a first-stage coil AL1(BL1) and a next-stage coil AL2(BL2) are connected in series on the power feed line80A (80B) in this sequence when viewed from the side of the heating element40. Further, a first capacitor AC1(BC1) is electrically connected between the housing82and a connection point NA(NB) between the first-stage coil AL1(BL1) and the next-stage coil AL2(BL2). Moreover, a second capacitor AC2(BC2) is electrically connected between a terminal of the next-stage coil AL2(BL2) at the side of the heater power supply58(IN) and the housing82.

In the heater power supply unit having the above-described configuration, during a positive cycle, an electric current outputted from the heater power supply58(IN) may flow from a first terminal hAto the inner heating wire40(IN) through the first power feed line80A, i.e., through the electric cable56(IN), the next-stage coil AL2, the first-stage coil AL1, and the power feed conductor52(IN), so that each part of the inner heating wire40(IN) generates Joule heat. Then, after flowing from a second terminal hB, the electric current is returned back through the second power feed line80(B), i.e., through the power feed conductor52(IN), the first-stage coil BL1, the next-stage coil BL2and the electric cable56(IN). During a negative cycle, the electric current flows through the same circuit in the reverse direction to that stated above. Since the electric current of this AC output from the heater is typically in a range from 50 Hz to several hundreds of hertz (Hz), voltage drops of the coils AL1, BL1, AL2and BL2may be negligibly small, and the amount of a leakage current flowing to the earth through the capacitors AC1, BC1, AC2and BC2may also be negligibly small. In this exemplary embodiment, as will be described later, the first-stage coils AL1and BL1are implemented by cylindrical air-core solenoid coils, i.e., air-core solenoid coils, and the next-stage coils AL2and BL2are implemented by troidal coils.

<Physical Configuration within Filter Unit>

FIG. 4illustrates a physical structure within the filter unit54(IN) according to the present exemplary embodiment.FIG. 5AtoFIG. 9illustrate a configuration of major parts within the filter unit54(IN).

As depicted inFIG. 4, the filter unit54(IN) includes the housing82or a grounded cylindrical conductor made of, but not limited to, aluminum, and the air-core solenoid coils AL1and BL1, the first capacitors AC1and BC1, the troidal coils AL2and BL2, and the second capacitors AC2and BC2are arranged in this sequence from top to bottom therein.

Each of the air-core solenoid coils AL1and BL1has a thicker coil conductor and a larger coil size than those of a general solenoid coil. With this configuration, each of the air-core solenoid AL1and BL1may serve as a power feed line through which a sufficiently large electric current (e.g., about 30 A) flows into the inner heating wire40(IN) from the heater power supply58(IN), and further, may obtain very large inductance and a large line length with the air core without having a magnetic core such as ferrite for the purpose of suppressing heat generation (power loss).

In this exemplary embodiment, however, since the frequency of the high frequency noise to be blocked by the air-core solenoid coils AL1and BL1is set to be in a high frequency range (40 MHz or higher), the size of the air-core solenoid coils AL1and BL1does not need to be so large. For example, the air-core solenoid coils AL1and BL2may have a diameter D of 25 mm or less and a length S of 150 mm or less.

Within the housing82, the two air-core solenoid coils AL1and BL1are provided coaxially with respect to the housing82by being supported by a coil supporting shaft (not shown) which is made of an insulator, e.g., a resin. The coil conductor of each of the air-core solenoid coils AL1and BL1is spirally wound at a variable winding pitch p in multiple stages in a substantially bare wire state without being covered with a coil sleeve, and has the same coil length S.

In the vicinity of the air-core solenoid coils AL1and BL1, a multiple number of, e.g., four rod-shaped comb-teeth members86, which are extended in parallel to a coil axis direction, are provided adjacent to the outer periphery of the air-core solenoid coils AL1and BL1at a regular interval in a circumferential direction thereof. Each comb-teeth member86is made of a resin having high hardness, processibility and heat resistance, such as, but not limited to, an insulator, e.g., PEEK or PCTFE, and is fixed in the filter unit54(IN) independently from the air-core solenoid coils AL1and BL1.

As depicted inFIG. 5AandFIG. 5B, comb teeth M are formed on an inner surface of each comb-teeth member86, and the comb teeth M are inserted (fitted) into respective winding gaps of the air-core solenoid coils AL1and BL1. From another viewpoint, the coil conductor of each of the air-core solenoid coils AL1and BL1is inserted into each of slits between every two adjacent comb teeth M. Accordingly, a winding pitch p of each of the air-core solenoid coils AL1and BL1is determined according to a pitch m of the comb teeth M. In this exemplary embodiment, since the two the air-core solenoid coils AL1and BL1are spirally wound while being overlapped, the winding pitch p of each of the air-core solenoid coils AL1and BL1is twice the pitch m of the comb teeth M. That is, a relationship of p=2m is established. In this exemplary embodiment, the winding pitch p of each of the two air-core solenoid coils AL1and BL1is constant (P5) from one end of the coil to the other end thereof.

An annular cover body88and an upper connector90made of a resin are provided at an upper opening of the housing82. Upper ends of the aforementioned non-illustrated coil supporting shaft and the comb-teeth members86are coupled to the upper connector90. Further, upper ends of the air-core solenoid coils AL1and BL1are electrically connected to the filter terminals TA and TB, respectively, within or in the vicinity of the upper connector90.

FIG. 6AandFIG. 6Bdepict a configuration of a sub-assembly the vicinity of the air-core solenoid coils AL1and BL1in the present exemplary embodiment. As illustrated, the multiple (four) rod-shaped comb-teeth members86are coupled by bolts94to a ring-shaped supporting body92, which is made of, for example, a resin and surrounds the comb-teeth members86at multiple positions (three positions at both end portions and at an intermediate portion) in an axial direction. The comb teeth M formed on the inner surface of each comb-teeth member86are inserted (fitted) into the winding gaps of the air-core solenoid coils AL1and BL1. Accordingly, the winding pitch p of the air-core solenoid coils AL1and BL1corresponds to the pitch m of the comb teeth M in a relationship of p=2m, and air gaps G corresponding to the thickness of the comb teeth M are formed in winding gaps of the coils except where the comb teeth M are inserted (FIG. 6B,FIG. 5B).

A coil supporting shaft96having, for example, a cross-shaped cross section is inserted into the air-core solenoid coils AL1and BL1. This coil supporting shaft96is formed of a multiple number of plate-shaped members98which are made of an insulator, e.g., a resin and are radially extended in a coil radial direction to come into contact with inner peripheral surfaces of the air-core solenoid coils AL1and BL1and, also, extended in parallel to the air-core solenoid coils AL1and BL1in the coil axis direction. Further, inFIG. 6AandFIG. 6B, a block100that holds the coil supporting shaft96, the comb-teeth members86, and so froth at one end side of the air-core solenoid coils AL1and BL1is a jig configured to assemble this sub-assembly.

FIG. 7illustrates a structure of a sub-assembly in the vicinity of the air-core solenoid coils AL1and BL1according to a modification example. In this modification example, comb teeth M are formed at outer end surfaces of the plate-shaped members98forming the coil supporting shaft96. The comb teeth M of the plate-shaped members98are inserted (fitted) into the winding gaps of the air-core solenoid coils AL1and BL1from the inside thereof in the coil radial direction, and define the winding pitch p with a relationship of p=2m. In this structure, since the plate-shaped members98forming the coil supporting shaft96also serve as the comb-teeth members, the aforementioned rod-shaped comb-teeth members86need not be provided in the vicinity of the air-core solenoid coils AL1and BL1.

As another modification example, the comb teeth M are formed with a preset pitch m at the outer end surfaces of the plate-shaped members98provided within the air-core solenoid coils AL1and BL1as shown inFIG. 7, and the rod-shaped comb-teeth members86having, on the inner surfaces thereof, the comb teeth M formed with the same pitch m as shown inFIG. 6Aare arranged in the vicinity of the air-core solenoid coils AL1and BL1. That is, it is possible to adopt a configuration in which the comb teeth M are inserted (fitted) into the winding gaps of the air-core solenoid coils AL1and BL1at different positions in the circumferential direction from both the inner side and the outer side in the coil radial direction. Furthermore, as still another modification example, it may be also possible to adopt a configuration in which a multiple number of rod-shaped comb-teeth members86are provided within the air-core solenoid coils AL1and BL1, and the comb teeth M formed at the outer surfaces of the respective comb-teeth members86are inserted into the winding gaps of the coils AL1and BL1.

Referring back toFIG. 4, the first capacitors AC1and BC1are implemented by two-terminal capacitors available on the market, respectively, and are horizontally arranged in a pair within a space between the air-core solenoid coils AL1and BL1and the troidal coils AL2and BL2. One terminal of the first capacitor AC1of the first filter84A is connected to a lower terminal of the air-core solenoid coil AL1via a connection conductor102A, and the other terminal of this first capacitor AC1is connected to a sidewall of the housing82via a connection conductor104A. One terminal of the first capacitor BC1of the second filter84B is connected to a lower terminal of the air-core solenoid coil BL1via a connection conductor102B, and the other terminal of this first capacitor BC1is connected to the sidewall of the housing82via a connection conductor104B.

Desirably, a coil conductor of each of the troidal coils AL2and BL2is spirally wounded halfway around a common troidal core106which is provided coaxially with respect to the air-core solenoid coils AL1and BL1, as illustrated inFIG. 4andFIG. 8. Here, the coil conductors of the two troidal coils AL2and BL2are wounded in the reverse directions so that magnetic fluxes φAand φBgenerated within the troidal core106when high frequency electric currents IAand IBof the same phase are flown into the two troidal coils AL2and BL2, respectively, have the same direction (are overlapped in the same direction) in the circumference direction thereof. The troidal core106is made of a core material having high relative permeability, such as Ni—Zn-based ferrite, and forms an annular closed magnetic path.

One terminal (upper terminal) of the troidal coil AL2of the first filter84A is connected to the lower terminal of the air-core solenoid coil AL1via the connection conductor102A, and the other terminal (lower terminal) of the troidal coil AL2is connected to one terminal of the second capacitor AC2via a connection conductor107A. One terminal (upper terminal) of the troidal coil BL2of the second filter84B is connected to the lower terminal of the air-core solenoid coil BL1via the connection conductor102B, and the other terminal (lower terminal) of the troidal coil BL2is connected to one terminal of the second capacitor BC2via a connection conductor107B.

In the present exemplary embodiment, to increase stray capacitance per a single turn of the coil winding between the troidal coils AL2and BL2and the housing82, a thickness t of the troidal core106is set to be at least twice (desirably, four or more times) as large as a typical thickness thereof. For this reason, multiple single-body troidal cores TC, which are available on the market, are stacked on top of each other in an axial direction (vertical direction) in plural levels (e.g., four levels), as illustrated inFIG. 9.

Assume that each single-body troidal core TC has an inner radius a, an outer radius b and a thickness (height) c. Generally, a horizontal width (b−a) of a body portion of the core and the thickness c are substantially same, and there is established a relationship of c≈(b−a). Accordingly, if two troidal cores TC are stacked in two levels, the thickness (height) t of the troidal core106is t=2c, and there is established a relationship of t≈2(b−a). Further, if four troidal cores TC are stacked in four levels, as in the illustrated configuration example, the thickness (height) t of the troidal core106is t=4c, and a relationship of t≈4(b−a) is established. In this exemplary embodiment, to establish a relationship of t≧2(b−a), desirably, a relationship of t≧4(b−a), the thickness t of the troidal core106is set to be much larger than a thickness of a typical troidal.

Further, the typical troidal core always serves as a lumped constant element in a high frequency range. In this exemplary embodiment, the troidal coils AL2and BL2also serve as lumped constant elements in the high frequency range, particularly, for the basic frequencies of the first and second high frequency powers HF and LF.

Further, if a core is inserted in a coil, a loss of a high frequency power, i.e., a core loss occurs in a core material. Such a core loss of the core material, particularly, a hysteresis loss or an eddy current loss increases as a frequency increases. In the filter unit54(IN) of the present exemplary embodiment, the noise of the first high frequency power HF having the high frequency is blocked by the first-stage air-core solenoid coils AL1and BL1, and does not reach the next-stage troidal coils AL2and BL2. Accordingly, a core loss of the troidal core106is small. As such, since the loss caused by the troidal core106is small, the troidal coils AL2and BL2can be scaled down by using a core material (e.g., ferrite) having high relative permeability as the troidal core106.

Each of the second capacitors AC2and BC2is also implemented by a two-terminal capacitor available on the market. As depicted inFIG. 4, the second capacitors AC2and BC2are horizontally arranged in a pair within a space between the troidal coils AL2and BL2and a bottom plate110of the housing82. One terminal of the second capacitor AC2of the first filter84A is connected to the lower terminal of the troidal coil AL2and one of the electric cables56(IN) via a connection conductor107A, and the other terminal of the second capacitor AC2is connected to a sidewall of the housing82via a connection conductor109A. One terminal of the second capacitor BC2of the second filter84B is connected to a lower terminal of the troidal coil BL2and the other of the electric cables56(IN) via a connection conductor107B, and the other terminal of this second capacitor BC2is connected to the sidewall of the housing82via a connection conductor109B.

A lower end opening of the housing82is closed by the bottom plate110made of, but not limited to, a resin. Further, either one or both of the cover body88and the bottom plate110of the housing82may be made of a conductive plate.

Further, a multiple number of vent holes (not shown) for air-cooling the air-core solenoid coils AL1and BL1and the troidal coils AL2and BL2accommodated in the housing82are formed at the housing82by, for example, a punching process.

As stated above, the filter unit54(IN) includes, in the housing82which is made of the cylindrical conductor and is grounded, the air-core solenoid coils AL1and BL1arranged at the uppermost portion thereof, i.e., at the first stage, coaxially with respect to the housing82; the troidal coils AL2and BL2arranged via the first capacitors AC1and BC1at the next stage coaxially with respect to the housing82; and the second capacitors AC2and BC2arranged at the lowermost portion thereof.

In the above-described layout within the filter unit54(IN), the air-core solenoid coils AL1and BL1are spirally wound at a uniform winding pitch interval while being overlapped in the axial direction (vertical direction). Further, the coil length S of the air-core solenoid coils AL1and BL1is not very large, and the air-core solenoid coils AL1and BL1is configured as a comparatively compact assembly. Meanwhile, the troidal coils AL2and BL2are wound halfway around the common troidal core106, respectively, and they form a compact dual-coil assembly. Further, although the troidal coils AL2and BL2have the height (thickness) twice as large as the typical troidal coil, as mentioned above, their height dimension is smaller than that in a case where a rod-shaped solenoid coil having the same inductance is disposed vertically.

Further, since the troidal core106of the troidal coils AL2and BL2forms the annular closed magnetic path and is coaxially placed with respect to the air-core solenoid coils AL1and BL1which are located above the troidal core106(accordingly, magnetic fluxes of the air-core solenoid coils AL1and BL1and the troidal coils AL2and BL2are orthogonally intersected with each other), electrical interference between the air-core solenoid coils AL1and BL1and the troidal coils AL2and BL2can be avoided. Thus, a distance or a space between the two kinds of coils AL1, BL1and AL2, BL2in the axial or vertical direction can be reduced.

In the filter unit54(IN), as will be described later, the air-core solenoid coils AL1and BL1are configured to perform the function of blocking the noise of the first high frequency power HF having the higher frequency. Meanwhile, the troidal coils AL2and BL2are configured to perform the function of blocking the noise of the second high frequency power LF having the lower frequency. That is, by allowing the air-core solenoid coils AL1and BL1and the troidal coils AL2and BL2to perform the individual filter functions of blocking the noise of the first high frequency power HF and the noise of the second high frequency power LF, respectively, design, manufacture and control of the entire filter unit54(IN) are eased, and an apparatus difference may hardly occur. Further, since the filter unit54(IN) can be sized down, the design layout of various kinds of power supply systems provided under the susceptor12or the chamber10can also be eased.

Furthermore, in the filter unit54(IN), a layout in which the air-core solenoid coils AL1and BL1and the troidal coils AL2and BL2are exchanged, i.e., a layout in which the troidal coils AL2and BL2are arranged at the uppermost portion and the air-core solenoid coils AL1and BL1are arranged at the next stage is not desirable. That is, if the troidal coils AL2and BL2are arranged at the uppermost portion, the troidal coils AL2and BL2just allow, among the noises of the first and second high frequency powers HF and LF introduced into the high frequency power feed lines80A and80B from the heating element40(IN), the noise of the first high frequency power HF having the higher frequency to pass therethrough, though they block the noise of the second high frequency power LF having the lower frequency. Further, since the capacitance of the first capacitors AC1and BC1is set to have a very small value as will be described later, not only the noise of the second high frequency power LF but also the noise of the first high frequency power HF are not flown to the earth. Accordingly, the noise of the first high frequency power HF is introduced into the troidal coils AL2and BL2, and the electric current of the first high frequency power HF flows in the troidal coils AL2and BL2. As a result, a great amount of core loss may occur within the troidal core106, so that the troidal core106generates heat and reaches a high temperature. If the temperature of the troidal core106increases up to the Curie temperature or higher, magnetic permeability may decline sharply, so that the blocking function against the noise of the second high frequency power LF may not be performed.

On the other hand, in the layout where the air-core solenoid coils AL1and BL1are arranged at the uppermost portion and the troidal coils AL2and BL2are arranged at the next stage, as in the present exemplary embodiment, since the air-core solenoid coils AL1and BL1block the noise of the first high frequency power HF having the higher frequency, noise of the first high frequency power HF hardly reaches the troidal coils AL2and BL2. Accordingly, the electric current of the first high frequency power HF having the higher frequency hardly flows in the troidal coils AL2and BL2, so that the troidal core106neither generates heat nor reaches a high temperature.

<Operation of Filter Unit>

In the filter unit54(IN) in accordance with the present exemplary embodiment, a distributed constant line is formed between the air-core solenoid coil AL1(BL1) of the filter84A (84B) and the housing82as the outer conductor.

In general, characteristic impedance Zoof a transmission line is expressed as Zo=√(L/C) by using electrostatic capacitance C per a unit length and inductance L per a unit length when no loss is assumed. Further, a wavelength λ is calculated by the following equation (1).
λ=2π/(ω√(LC))  (1)

Unlike in a general distributed constant line (especially, in a coaxial line) where a rod-shaped cylindrical conductor serves as the central portion of the transmission line, the cylindrical air-core solenoid coils serve as a central conductor in the filter unit54(IN). It is assumed that the inductance L per a unit length is mainly caused by the cylindrical coil. Meanwhile, the electrostatic capacitance per a unit length is defined as electrostatic capacitance C of a capacitor formed by a coil surface and the outer conductor. In this filter unit54(IN), when the inductance per a unit length and the electrostatic capacitance per a unit length are L and C, respectively, it is assumed that a distributed constant line of which characteristic impedance Zois expressed as Zo=√(L/C) is formed.

When the filter unit having this distributed constant line is viewed from the side of the terminal T, since an opposite side thereof is nearly short-circuited by the capacitor having large capacitance (e.g., about 5000 pF), there may be obtained a frequency-impedance characteristic in which large impedance is repeated at a constant frequency interval. This impedance characteristic may be obtained when the wavelength and the length of the distributed line are same.

In this filter unit54(IN), not a winding length of the air-core solenoid coils AL1and BL1but a coil length S in the axial direction (FIG. 4) becomes the length of the distributed line. By using the air-core solenoid coils AL1and BL1as the central conductor, L can be increased to be much larger than that in case of using a rod-shaped cylindrical conductor as the central conductor, so that λ can be reduced. Thus, it is possible to realize an effective length that is a comparatively short line length (coil length S) and is equal to or larger than the wavelength. Therefore, in the first-stage filter circuit composed of the first capacitor AC1(BC1) and the air-core solenoid coil AL1(BL1) having the constant winding pitch psas shown inFIG. 10, it is possible to obtain a frequency-impedance characteristic in which high impedances are repeated at a regular frequency interval as illustrated inFIG. 11, for example.

In the present exemplary embodiment, the air-core solenoid coil AL1(BL1) only needs to block a high frequency noise in a high frequency range (equal to or higher than 40 MHz). It may be allowable that the air-core solenoid coil AL1(BL1) has low impedance against a high frequency noise in a low frequency range (equal to or lower than 3.2 MHz) by being reduced in its coil size.

By way of example, when the frequency of the first high frequency power HF is 40 MHz, impedance equal to or higher than several hundreds of angstroms (Ω) is obtained according to the frequency-impedance characteristic ofFIG. 11. Thus, the noise of the first high frequency power HF introduced into the power feed line80A (80B) can be completely blocked in the first-stage filter circuit composed of the air-core solenoid coil AL1(BL1) and the first capacitor AC1(BC1).

FIG. 12depicts an equivalent circuit of the troidal coil AL2(BL2) and the second capacitor AC2(BC2). The troidal coil AL2(BL2) not only provides an inductor L2or an inductive element having self-inductance, but also has an inter-coil-wire capacitor C2Kgenerated in the vicinity of the inductor L2and a ground stray capacitor C2Fgenerated between the coil and the housing82. In the equivalent circuit, the capacitors C2Kand C2Fare connected to the inductor L2in parallel.

Here, inductance of the inductor L2of the troidal coil AL2(BL2) is represented by the following equation (1).
L2=N2×μ×t×ln(b/a)/2π  (1)

In the present exemplary embodiment, as stated above, a core material (e.g., ferrite) having high permeability is used as the troidal core106. Further, by setting the thickness (height) t of the troidal core106to be at least twice (desirably, four or more times) as large as the typical thickness and selecting the winding number N to be large enough, the inductance of the inductor L2can be set to be a considerably high value (e.g., 100 μH or higher).

The capacitance of the inter-coil-wire capacitor C2Kdepends on the winding interval (pitch) of the coil AL2(BL2), not on the winding number N. Meanwhile, the capacitance of the ground stray capacitor C2Fdepends on a distance from the housing82and a total area of a coil surface facing the housing82. Accordingly, in the troidal coil AL2(BL2), as long as the diameter of the housing82and the size of the troidal core106are constant, the inductance of the inductor L2and the capacitance of the ground stray capacitor C2Fincrease as the coil winding number increases.

Particularly, since the troidal core106, which is formed by stacking the individual troidal cores TC in the multiple levels and thus has the large thickness (height) t, has a large coil surface area per a single turn, the capacitance of the ground stray capacitor C2Fis considerably large, and may be equal to or larger than four times or five times the inter-coil-wire capacitor C2K(e.g., equal to or larger than 20 pF).

As stated above, in the troidal coil AL2(BL2), the low inductance of the inductor L2and the larger capacitance of the ground stray capacitor C2Fthan the capacitance of the inter-coil-wire capacitor C2Kare advantageous (appropriate) to set a self-resonance frequency of the troidal coil AL2(BL2), i.e., a second parallel resonance frequency fPLapplied from a second parallel resonance circuit112to be described below to a sufficiently low frequency range.

In the equivalent circuit (FIG. 12) as described above, the parallel resonance circuit112having the parallel resonance frequency fPLwithin a very low frequency range is formed by the inductor L2of the troidal coil AL2(BL2), the inter-coil-wire capacitor C2Kand the ground stray capacitor C2F. Here, the parallel resonance frequency fPLis the self-resonance frequency of the troidal coil AL2(BL2) and is expressed by the following equation (2).
fPL=1/2π√L2(C2K+C2F)  (2)

FIG. 13illustrates an example of the frequency-impedance characteristic obtained by the next-stage filter circuit composed of the troidal coil AL2(BL2) and the second capacitor AC2(BC2) when the basic frequency of the second high frequency power LF is 3.2 MHz.

In the shown frequency-impedance characteristic, the parallel resonance frequency fPLis substantially equal to the basic frequency (3.2 MHz) of the second high frequency power LF, which can be easily achieved. That is, as mentioned above, if the winding number N of the troidal coil AL2(BL2) is changed, the inductance of the inductor L2and the capacitance of the ground stray capacitor C2Fare changed in the same tendency according to the changing amount of the winding number N, though there is no change in the capacitance of the inter-coil-wire capacitor C2K. Thus, the second parallel resonance frequency fPLchanges smoothly according to the above equation (2). Further, if the stacking number of the troidal cores TC forming the troidal core106is changed, the inductance of the inductor L2and the capacitance of the ground stray capacitor C2Fare changed sharply in the same direction, so that the parallel resonance frequency fPLis changed in the step shape according to the above equation (2). Therefore, by changing the stacking number of the troidal cores TC forming the troidal core106in case of adjusting the parallel resonance frequency roughly and, also, by changing the winding number N of the troidal coil AL2(BL2) in case of adjusting the parallel resonance frequency precisely, the parallel resonance frequency fPLcan be made approximately equal to the basic frequency (3.2 MHz) of the second high frequency power LF.

Since the characteristic near the parallel resonance frequency fPLhas a margin (i.e., is broad), it is still possible to apply sufficiently high impedance to the noise of the second high frequency power LF even if the parallel resonance frequency fPLis slightly deviated from the basic frequency (3.2 MHz) of the second high frequency power LF.

As discussed above, in the filter84A (84B) according to the present exemplary embodiment, the first-stage air-core solenoid coil AL1(BL1) is configured to form, by being combined with the housing82as the outer conductor, the distributed constant line in which parallel resonance occurs at multiple frequencies. These first-stage air-core solenoid coil AL1(BL1) performs the filter blocking function, with sufficiently high impedance, the noise of the first high frequency power HF having the higher frequency introduced into the heater power feed line80A (80B) from the heating element40within the susceptor12, while allowing the noise of the second high frequency power LF having the lower frequency, which is introduced along with the noise of the first high frequency power HF, to pass therethrough. The next-stage troidal coil AL2(BL2) having the self (parallel)-resonance frequency fPLequal to or approximate to the basic frequency of the second high frequency power LF has also the filter blocking function of blocking, with sufficiently high impedance, the noise of the second high frequency power LF having passed through the first-stage air-core solenoid coil AL1(BL1). Since the parallel resonance frequency of the air-core solenoid coil AL1(BL1) and the self-resonance frequency fPLof the troidal coil AL2(BL2) are independent from each other, it is possible to adjust these frequencies independently in the respective coils, as stated above.

Moreover, in this exemplary embodiment, the comb-teeth members86or98extended in parallel to the coil axis direction are provided in the vicinity of or within the air-core solenoid coils AL1and BL1. Further, comb teeth M which are formed at the inner surfaces or the outer surfaces of the comb-teeth members86or98and have a pitch m corresponding to the winding pitch p are inserted into winding gaps of the air-core solenoid coils AL1and BL1.

With this configuration, since the winding pitch p of the air-core solenoid coils AL1and BL1is accurately set to a preset value by the comb-teeth pitch m, the frequency-impedance characteristic or filter characteristic having high reproducibility and no object difference can be obtained. Furthermore, since the air gaps G are formed in winding gaps of the air-core solenoid coils AL1and BL1except where the comb teeth M are inserted, heat generated from the coil is rapidly discharged out through the air gaps G. Therefore, the air-core solenoid coils AL1and BL1can be cooled efficiently.

In the above-described exemplary embodiment, in the filter unit54(IN), the winding pitch p of the air-core solenoid coils AL1and BL1is uniform (constant value ps) from one ends to the other ends of the coils (FIG. 4andFIG. 10), and a frequency-impedance characteristic of multiple parallel resonance in which impedance increases in a conical shape at a regular frequency interval is obtained, as shown inFIG. 11, for example. Accordingly, if the frequency of the noise of each of the high frequency powers (particularly, the first high frequency power HF) among the high frequency powers except the second high frequency power LF having the lowest frequency, which are introduced to the power feed lines80A and80B through the susceptor12and the heating element40, is designed to be equal to or approximate to any one parallel resonance frequency of the multiple parallel resonance, such a high frequency noise in the high frequency range can be effectively blocked by the filter unit54(IN).

However, in the aforementioned filter configuration where the winding pitch of the air-core solenoid coils AL1and BL1is uniform (constant value ps) over the entire length S, since the parallel resonance frequencies are obtained at a regular frequency interval, it is very difficult to match any one of the parallel resonance frequency of the multiple parallel resonance with the frequency of the first high frequency power HF, which is selected or changed in consideration of various aspects such as the kind or specification of a process involved.

For example, when the frequency of the first high frequency power HF is 40 MHz, impedance against the noise of the first high frequency power HF is just several hundreds of angstroms (Ω) and does not reach 1000 Ω or higher in the frequency-impedance characteristic ofFIG. 11. Furthermore, when there is a need or request to change the frequency of the first high frequency power HF from 40 MHz to 60 MHz, the impedance would be greatly lowered because a third serial resonance frequency fS3is about 60 MHz. Thus, it is difficult to efficiently respond to the need or request to change the frequency of the first high frequency power HF.

To solve this problem, in the prior art described in Patent Document 1, by providing a ring-shaped member between the air-core solenoid coils AL1and BL1and the housing (outer conductor)82in the filter unit54(IN), the gap of the coaxial line is narrowed locally. Accordingly, C (electrostatic capacitance per a unit length) is changed, and, also, the characteristic impedance Zo=√(L/C) is changed locally. Thus, a part or all of resonance frequencies of the multiple parallel resonance may be shifted.

In contrast, in the filter unit54(IN) according to the present exemplary embodiment, instead of providing such the ring-shaped member, the air-core solenoid coils AL1and BL1are divided to multiple sections K1, K2, . . . in the coil axis direction. By setting or adjusting the winding pitch p of the air-core solenoid coils AL1and BL1for each section Ki(i=1, 2, . . . ) independently, the characteristic impedance Zo=√(L/C) is changed in each section without changing the gap of the coaxial line, so that a part or all of resonance frequencies of the multiple parallel resonance can be shifted. In this case, in each section Ki, as the winding pitch p of the air-core solenoid coils AL1and BL1is decreased, C and L per a unit length are increased, so that the characteristic impedance Zo=√(L/C) is increased. On the contrary, as the winding pitch p of the air-core solenoid coils AL1and BL1is increased, C and L per a unit length are decreased, so that the characteristic impedance Zo=√(L/C) is decreased.

In this exemplary embodiment, as a division form (pattern) for dividing the air-core solenoid coils AL1and BL1to the multiple sections K1, K2, . . . regarding the winding pitch as stated above, a division pattern as depicted inFIG. 14andFIG. 15, for example, may be employed.

In this division pattern, as shown inFIG. 15, the air-core solenoid coils AL1and BL1are divided to three sections K1, K2and K3at a length ratio of 2:1:2 from an inlet (IN) of the filter unit54(IN) toward an outlet (OUT) thereof when viewed from the side of the coil terminals TA and TB, and a ratio between winding pitches p1, p2and p3of these three sections K1, K2and K3is set to be 2:1:2. In this case, with respect to the winding pitch psin the case (FIG. 10) where the air-core solenoid coils are not divided to the multiple sections, by setting p1=1.12ps, p2=0.56ps, p3=1.12ps, the entire length S of the coil can be maintained same.

Moreover, as depicted inFIG. 14, the comb-teeth members86(98) extended in parallel to the coil axis direction are provided in the vicinity of or within the air-core solenoid coils AL1and BL1in order to divide the air-core solenoid coils AL1and BL1to the three sections K1, K2and K3regarding the winding pitch p. Further, comb teeth Miwhich are formed at the inner surfaces or the outer surfaces of the comb-teeth members86(98) and have a pitch micorresponding to the winding pitch piin each section Kiare inserted into winding gaps of the air-core solenoid coils AL1and BL1.

FIG. 16depicts a frequency-impedance characteristic of the first-stage filter circuit obtained by the electromagnetic field computation when using the above-described division pattern (FIG. 15), in comparison with a frequency-impedance characteristic (FIG. 11) obtained when the winding pitch is uniform. As shown therein, second serial/parallel resonance frequencies and fourth serial/parallel resonance frequencies are shifted to higher frequency ranges (fs2<f′s2), (fp2<f′p2), (fs4<f′s4), (fp4<f′p4), respectively, and third serial/parallel resonance frequencies and fifth serial/parallel resonance frequencies are shifted to lower frequency ranges (fs3>f′s3), (fp3>f′p3), (fs5>f′s5), (fp5>f′p5), respectively.

By the shifts of the resonance frequencies, high impedance equal to or higher than 1000Ω can be obtained at the frequency of 40 MHz, and high impedance equal to or higher than several hundreds of angstroms (Ω) can also be obtained even at the frequency of 60 MHz. Accordingly, in the plasma processing apparatus according to the above-described exemplary embodiment, when the frequency of the first high frequency power HF is 40 MHz, the blocking function of the filter84A (84B) against the noise of the first high frequency power HF can be further improved, and can also be applied in the case where the frequency of the first high frequency power HF is switched into the two frequencies of 40 MHz and 60 MHz.

Further, the above-stated division pattern (FIG. 15) is nothing more than an example, and various selections or modifications may be made regarding the number of the division sections, the distributed forms of winding pitches, and so forth.

Furthermore, in order to shift a part of the resonance frequencies among the multiple parallel resonance characteristics of the filter84A (84B) selectively as stated above, a ratio between the lengths of the multiple sections K1, K2, . . . set on the air-core solenoid coils AL1and BL1and a ratio of winding pitches p1, p2, . . . need to be selected to appropriate values. By way of example, as for the division pattern ofFIG. 15, if the first section K1is extremely short, e.g., S/100 or less, it may be difficult to achieve the effect of shifting a part of the resonance frequencies as shown inFIG. 16. Likewise, when the winding pitch p1in the first section K1is different only several % from the winding pitch p2in the second section K2, such a shifting effect for a part of the resonance frequencies may not be achieved, either.

According to the electromagnetic field computation conducted by the present inventor, it is desirable that the length of the first section K1is equal to or larger than ⅕ of the length of the second section K2, and equal to or smaller than 5 times the length of the second section K2. Further, it is also desirable that the winding pitch p1of the first section K1is equal to or larger than twice the winding pitch p2of the second section K2, or equal to or less than ½ the winding pitch p2of the second section K2.

<Other Exemplary Embodiments Regarding Plasma Processing Apparatus>

FIG. 17illustrates a configuration of a plasma processing apparatus according to a modification example. In the drawing, parts having the same configuration or function in the plasma processing apparatus (FIG. 1) of the above-described exemplary embodiment will be assigned same reference numerals.

This plasma processing apparatus is configured as a capacitively coupled plasma etching apparatus of applying dual high frequency powers to the lower electrode and a single high frequency power to the upper electrode. This plasma processing apparatus is mainly different from the plasma processing apparatus (FIG. 1) of the above-described exemplary embodiment in that the first high frequency power HF for plasma generation is applied to the upper electrode64, and the second and a third high frequency power LF and MF having different frequencies are applied to the susceptor12in an overlapped manner to control energy (bias) of ions attracted to the semiconductor wafer W in various ways with higher degree of freedom. Here, the frequency of the third high frequency power MF is set to be a value (e.g., 12.88 MHz) higher than the frequency (e.g., 3.2 MHz) of the second high frequency power LF.

In this plasma processing apparatus, the upper electrode64is provided to a top surface of the chamber10via the ring-shaped insulator130. The first high frequency power supply28configured to output the first high frequency power HF for plasma generation is electrically connected to the upper electrode64via the matching unit132and an upper power feed rod134. Further, the second high frequency power supply30configured to output the second high frequency power LF and a third high frequency power supply136configured to output the third high frequency power MF are electrically connected to the susceptor12via matching devices (not shown) within the matching unit32and the lower power feed rod34. The controller75is configured to control a total power of the second and third high frequency powers LF and MF outputted from the high frequency power supplies30and136, respectively, and a power ratio therebetween based on specifications and conditions of the etching process or according to a recipe.

In this plasma processing apparatus, the filter units54(IN) and54(OUT) having the same configuration and function as those in the plasma processing apparatus (FIG. 1) may also be provided on the heater power feed line. Particularly, if a frequency-impedance characteristic shown inFIG. 16is obtained by dividing, regarding the winding pitch p, the air-core solenoid coil AL1(BL1) to three sections K1, K2and K3according to the division pattern as shown inFIG. 15, it is possible to block any noises of the first to third high frequency powers HF, LF and MF, which are introduced into the heater power feed lines80A and80B from the heater element40of the susceptor12, with sufficiently high impedance by using a filter configuration including the single air-core solenoid coil AL1(BL1) and the single troidal coil AL2(BL2) as in the above-described exemplary embodiment.

That is, the first-stage air-core solenoid coil AL1(BL1) configured to form, by being combined with the housing82as the outer conductor, a distributed constant line in which parallel resonance occurs at multiple frequencies is capable of exerting a stable and secure filter blocking function against a noise of the third high frequency power MF (12.88 MHz) with sufficiently high impedance near the first parallel resonance frequency f′p1, and, also, capable of exerting a stable and secure filter blocking function against the noise of the first high frequency power HF (40 MHz or 60 MHz) with sufficiently high impedance near the second parallel resonance frequency f′p2or the third parallel resonance frequency f′p3. Further, the next-stage troidal coil AL2(BL2) is capable of providing a stable and secure filter blocking function against the noise of the second high frequency power LF (3.2 MHz), which is introduced through the first-stage air-core solenoid coil AL1(BL1), with sufficiently high impedance near the self-resonance frequency fPL.

Other Exemplary Embodiments or Modification Examples

FIG. 18illustrates a physical structure within the filter unit54(IN) according to another exemplary embodiment. In this exemplary embodiment, the air-core solenoid coils AL1and BL1are divided to multiple sections K1, K2, . . . in the coil axis direction, and winding gaps in a single section, e.g., K2, are blocked by a coil tube J in the entire circumferential direction. In the other sections, e.g., K1and K3, the comb teeth M of the comb-teeth members86(98) are inserted into the winding gaps locally in the circumferential direction, as in the above-described exemplary embodiment. The other configuration is mostly the same as that of the above-described exemplary embodiment.

In this case, in the section K2where the coil tube J is used, typically, a coil conductor of only one air-core solenoid coil BL1is put through the coil tube J, as shown inFIG. 19. Without putting a coil conductor of the other air-core solenoid coil AL1through the coil tube J, a constant winding pitch p and electrical insulation between both coils AL1and BL1can be obtained. However, it may be also possible to adopt a configuration in which coil conductors of both coils AL1and BL1are put through the respective coil tube J.

In this exemplary embodiment, as in the above-described exemplary embodiment, instead of providing the ring member between the air-core solenoid coils AL1and BL1and the housing82of the outer conductor within the filter unit54(IN), a physical characteristic of the solenoid coils AL1and BL1, which determines C and/or L of the coaxial line, is set or adjusted independently for each of the multiple sections. Thus, a characteristic impedance Zo=√(L/C) is changed in each section without changing the gap of the coaxial line, so that a part or all of resonance frequencies of multiple parallel resonance are shifted.

More specifically, in the inter-winding structure, the air-core solenoid coils AL1and BL1are divided to the multiple sections K1, K2, . . . as stated above, and in one of the sections, the comb teeth M are inserted into the winding gaps, whereas in the other sections, the winding gaps are blocked by the coil tube J. Accordingly, C and L of the coaxial line are changed in each section, and, thus, the characteristic impedance Zo=√(L/C) is changed in each section, so that a part or all of the resonance frequencies of the multiple parallel resonance can be shifted.

For example, in a division pattern ofFIG. 18, in the sections K1and K3where the comb teeth M are inserted into the winding gaps, as the winding pitch p decreases, C and L per a unit length are increased, so that the characteristic impedance Zo=√(LC) is also increased. On the contrary, as the winding pitch p increases, C and L per a unit length are decreased, so that the characteristic impedance Zo=√(LC) is also decreased. Furthermore, in the section K2where the winding gaps are blocked by the coil tube J, if the winding pitch p therein is constant, C per a unit length increases as a dielectric constant £ of the coil tube J increases, so that the characteristic impedance Zo=√(LC) is also increased. On the contrary, as the dielectric constant £ of the coil tube J decreases, C per a unit length is also decreased, so that the characteristic impedance Zo=√(LC) is decreased.

The present inventor has acquired, by the electromagnetic field computation, the frequency-impedance characteristics of the first filter84(A) having the division pattern of the air-core solenoid coil AL1as shown inFIG. 18andFIG. 20. Then, the frequency-impedance characteristic acquired for this division pattern is compared with a frequency-impedance characteristic obtained by the electromagnetic field computation for a configuration (FIG. 10) where the coils are not divided to multiple sections, the winding pitch is set to be uniform (constant value ps), and the comb teeth M are inserted into the winding gaps from one end to the other end of the coil. In this electromagnetic filed computation, the dielectric constant of the coil tube J is set to have a value of 4. By way of non-limiting example, if the coil tube J is made of PEEK, the dielectric constant value of 4 can be obtained. As depicted inFIG. 21, all of the serial resonance frequencies and the parallel resonance frequencies after the third ones are shifted to lower frequency ranges (fs3>f′s3), (fp3>f′p3)≈(fs6>f′s6), (fp6>f′p6), respectively.

In this exemplary embodiment, various selections and modifications may be made regarding the number of division sections, patterns in which a section in which the comb teeth M are inserted into the winding gaps, and a section, in which the winding gaps are blocked by the coil tube J, are mixed, and so forth.

Further, as another exemplary embodiment shown inFIG. 22, it may be possible to adopt a configuration in which the air-core solenoid coils AL1and BL1are divided to multiple sections K1, K2, . . . in the inter-winding structure, and the winding gaps in some sections (e.g., the section K1) are blocked in the entire circumferential direction by a first coil tube J1having a first dielectric constant, and the winding gaps in other sections (e.g., the section K2) are blocked in the entire circumferential direction by a second coil tube J2having a second dielectric constant. As an example, the first coil tube J1may be made of Teflon (registered trademark) having a dielectric constant of 1, and the second coil tube J2may be made of PEEK having a dielectric constant of 4.

In the above-described exemplary embodiments, within the single outer conductor (housing)82, the coil conductor forming the solenoid coil AL1of the first filter84A and the coil conductor forming the solenoid coil BL1of the second filter84B are spirally wound while being overlapped. In this coil winding structure, self-inductance between both air-core solenoid coils AL1and BL1are same each other, and maximum mutual inductance can be obtained. As a result, a RF power loss in the filter unit54(IN) is reduced, and an apparatus difference in the RF power loss is reduced. Further, though not illustrated, it is also possible to adopt a configuration in which the air-core solenoid coil AL1of the first filter84A and the air-core solenoid coil BL1of the second filter84B are accommodated in outer conductors (housings)82, respectively. In such a case, when the aforementioned comb-teeth members86or98are provided, a winding pitch p and a comb-teeth pitch m are same, and a relationship of p=m is established.

Further, in the above-described exemplary embodiment, the coil conductor of the troidal coil AL2(BL2) is wound around the single troidal core106which is composed of the multiple troidal cores TC stacked on top of each other. An assembly of a plurality of this type of troidal coil connected in series without capacitors provided therebetween may be used as a single troidal coil or a single set of troidal coils.

Furthermore, as depicted inFIG. 23, there may be used a complex type troidal coil AL which is prepared by connecting in series a plurality of (three in the shown example) troidal coils TR, each of which is composed of the coil conductor wound around the single-body troidal core TC. InFIG. 23, only the troidal coil AL on the first power feed line80A is shown, while a troidal coil BL on the second power feed line80B is not illustrated.

In the above-described exemplary embodiment, the capacitors AC1(BC1) and AC2(BC2) respectively included in the filter84A (84B) are accommodated within the housing82. However, a part or all of these capacitors may be provided at the outside of the housing82. Moreover, a ground potential member other than the housing82may be used for these capacitors. In addition, the troidal coils AL2and BL2and the air-core solenoid coils AL1and BL1may be accommodated in separate housings82. Further, the troidal coils AL2and BL2may be substituted with other types of coils having a core, for example, a solenoid coil having a core.

The above-described exemplary embodiments are directed to a filter configured to, in a capacitively coupled plasma etching apparatus of a lower electrode dual frequency application type in which the first high frequency power HF for plasma generation and the second high frequency power LF for ion attraction are applied to the susceptor12in the overlapped manner within the chamber10, reduce noises of both high frequency powers on a pair of the heater power feed lines80A and80B electrically connecting the heating element40mounted in the susceptor12and the heater power supplies58(IN) and58(OUT) provided outside the chamber10. However, the filter or the filter unit of the above-described exemplary embodiments may be properly applied to a capacitively coupled plasma etching apparatus of an upper-and-lower electrode dual frequency application type configured to apply the first high frequency power HF for plasma generation to an upper electrode64while applying the second high frequency power LF for ion attraction to the susceptor12, or a capacitively coupled plasma etching apparatus of a lower electrode single frequency application type configured to apply a single high frequency power to the susceptor12.

Further, by using multiple parallel resonance of the distributed constant line formed by the air-core solenoid coil AL1(BL1) and the housing82as the outer conductor, it is also possible to block a noise of a harmonic generated from the high frequency powers HF and LF applied for a plasma process (especially, a second harmonic of the first high frequency power HF).

Furthermore, the exemplary embodiments are not limited to the filter for a power cable such as the heater power feed line, but may also be applicable to any filter or filter unit provided on a pair of lines or a single line configured to electrically connect an electrical member within a chamber and an external circuit of a power meter or a signal meter provided outside the chamber.

The present exemplary embodiment may not be limited to the capacitively coupled plasma etching apparatus but can be applied to various types of plasma etching apparatuses such as a microwave plasma etching apparatus, an inductively coupled plasma etching apparatus, a helicon wave plasma etching apparatus, etc. and, also, can be applied to other plasma processing apparatuses such as a plasma CVD apparatus, a plasma oxidizing apparatus, a plasma nitriding apparatus, a sputtering apparatus, etc. Further, the processing target substrate may not be limited to the semiconductor wafer but may be a photomask, a CD substrate, a print substrate, or one of various types of substrates for a flat panel display, an organic EL and a solar cell.

EXPLANATION OF REFERENCE NUMERALS