JP2005136350A - Electrostatic chuck, plasma processing apparatus, and plasma processing method - Google Patents

Abstract

<P>PROBLEM TO BE SOLVED: To provide an electrostatic chuck for stably and surely chucking and supporting an insulator substrate without causing abnormal discharge and dielectric breakdown. <P>SOLUTION: In a placing stand 10 on which the insulator substrate G is placed; a rectangular block shaped susceptor 14 made of a conductor such as aluminum, and a rectangular frame shaped focus ring 16 made of an insulator such as quartz for surrounding around the susceptor 14, are provided on a base member 12. An electrostatic chucking part 24 comprises a three-layer structure of a lower dielectric layer 18, an electrode layer 20, and an upper dielectric layer 22 each formed on a principal face (upper face) of the susceptor 14 respectively by the thermal spraying method. The lower dielectric layer 18 and the upper dielectric layer 22 are made of ceramics of at least alumina (Al<SB>2</SB>O<SB>3</SB>) or zirconia (ZrO<SB>2</SB>) whose volume resistivity is 1×10<SP>14</SP>Ω cm or over. An output terminal of a DC power supply 34 is electrically connected to the electrode layer 20. <P>COPYRIGHT: (C)2005,JPO&NCIPI

Description

  The present invention relates to an electrostatic adsorption apparatus that electrostatically adsorbs and fixes a substrate to be processed made of an insulator, a plasma processing apparatus and a plasma processing method using the same.

  In the manufacture of flat panel display (FPD) panels, pixel devices or electrodes, wirings, and the like are generally formed on a substrate made of an insulator such as glass. Among various processes of panel manufacture, plasma is used in fine processing such as etching, CVD, ashing, and sputtering. In a manufacturing apparatus that performs such plasma processing, a substrate is mounted on a mounting table in a processing container that can be depressurized, and processing is performed by exposing the upper surface (surface to be processed) of the substrate to plasma of a processing gas. I have to. In this case, it is necessary to control the temperature of the substrate to be constant by suppressing the temperature rise due to heat generation during the plasma processing.For this reason, the coolant temperature-controlled from the chiller device is circulated and supplied to the coolant passage in the mounting table, A method of indirectly cooling the substrate by supplying a gas with good heat conductivity such as He gas to the back surface of the substrate through the mounting table is often used. This cooling method requires a mechanism for fixing and holding the substrate on the mounting table against the supply pressure of He gas.

  FIG. 13 shows a configuration of a conventional electrostatic chucking apparatus that holds an insulating substrate with an electrostatic chucking force in a plasma processing apparatus. In this electrostatic chuck, the mounting table 200 is provided with a susceptor 204 made of a conductor and a focus ring 206 made of an insulator on a base member 202. The insulating substrate G is placed on the upper surface of the susceptor 204 so that the peripheral edge of the substrate covers the upper surface of the focus ring 206. A refrigerant passage 208 is provided inside the susceptor 204, and refrigerant from a chiller device (not shown) flows through the refrigerant flow path 208. In addition, a large number of through holes 210 are provided on the upper surface of the susceptor 204, and He gas for heat transfer from a He gas supply unit (not shown) passes through these through holes 210 on the back surface of the substrate G. It is supplied at a predetermined pressure.

  A high frequency of several MHz to several tens of MHz is applied to the susceptor 204 from the high frequency power supply 212. A plasma PZ of a processing gas is generated on the substrate G during the plasma processing. The plasma PZ may be generated by a high frequency from a high frequency power supply 212 or may be generated by a high frequency from another high frequency power supply (not shown). In the latter case, the high frequency applied to the susceptor 204 from the high frequency power supply 212 is used as a bias for drawing ions in the plasma PZ into the surface to be processed of the substrate G.

  Further, a DC voltage of about several kV is applied to the susceptor 204 from a DC (direct current) power source 214. When this DC voltage is a positive voltage, negative charges (electrons and negative ions) in the plasma PZ are accumulated on the upper surface (surface to be processed) of the substrate G so as to be attracted. An electrostatic force (Coulomb force) attracting each other acts between the negative surface charge on the upper surface and the susceptor 204, and the substrate G is attracted and fixed on the susceptor 204 by this electrostatic attraction.

  FIG. 14 shows a conventional technique obtained by improving the electrostatic adsorption device (FIG. 13). In this electrostatic adsorption device, the upper surface of the susceptor 204 is covered with an insulator layer 216. The through hole 210 is formed so as to penetrate the upper surface of the susceptor 204 and the insulator layer 216 from the gas flow path inside the susceptor 204.

  In recent years, there has been an increasing demand for increasing the size of FPD insulating substrates. In the electrostatic attraction apparatus as described above, the larger the size of the insulating substrate, the more likely the substrate is warped by thermal stress. Therefore, the supply pressure of the heat transfer gas (He gas) used for controlling the substrate temperature must be increased. Accordingly, it is necessary to increase the electrostatic attraction force for fixing and holding the substrate. However, when the DC voltage applied to the susceptor is increased in order to increase the electrostatic attraction force, there is a problem that damage such as abnormal discharge (mostly arc discharge) or dielectric breakdown is likely to occur.

  In fact, in the conventional example of FIG. 13, when the DC voltage applied to the susceptor 204 from the DC power source 214 is increased in order to increase the electrostatic attraction force with the increase in the size of the insulating substrate G, the peripheral end portion on the upper surface of the susceptor 204 Abnormal discharge is likely to occur between the plasma PZ and the susceptor 204 is likely to be destroyed (electrode destruction). In this regard, in the conventional example of FIG. 14, the above-described abnormal discharge can be suppressed to some extent by the insulator layer 216. However, abnormal discharge may still occur from the gap between the susceptor 204 and the focus ring 206, the susceptor 204 exposed in the through hole 210, or the like. Further, when the temperature of the susceptor 204 is increased, a large thermal stress is applied to the insulator layer 216 due to a difference between the expansion coefficient of the susceptor 204 and the expansion coefficient of the insulator layer 216, and the insulator layer 216 is easily cracked. Such cracks are more likely to occur as the substrate size increases (generally when the substrate longest dimension is 500 mm or more).

  In addition, poor adhesion of the substrate G on the mounting table 200, end defects, mounting displacement (conveyance displacement), and the like cause abnormal discharge, but there is no effective solution for this problem in the prior art. It was. As described above, when the DC voltage is increased, abnormal discharge or dielectric breakdown is likely to occur. Therefore, it is difficult to increase the electrostatic adsorption force, and thus uniform temperature control is performed on a large substrate. It becomes difficult to perform the plasma processing, and finally, it becomes difficult to perform the in-plane uniform plasma processing.

  The present invention has been made in view of the above-described problems of the prior art, and is a highly reliable electrostatic adsorption device capable of increasing the holding force on an insulating substrate without causing abnormal discharge or dielectric breakdown. The purpose is to provide.

  Another object of the present invention is to provide an electrostatic attraction apparatus capable of stably and reliably holding a substrate in response to an increase in size of an insulating substrate.

  Another object of the present invention is to stably hold the substrate in response to the increase in size of the insulating substrate, and to uniformly control the temperature of each part of the substrate to perform in-plane uniform plasma processing on the substrate. The object is to provide a processing apparatus and a plasma processing method.

  Another object of the present invention is to provide a plasma processing apparatus and a plasma processing method capable of preventing abnormal discharge due to poor holding of the substrate to be processed on the mounting table, end defect, or mounting displacement. .

  In order to achieve the above object, an electrostatic adsorption device of the present invention is a substrate holding device for holding a substrate to be processed made of an insulator in a space where plasma is formed, and supports the substrate. A susceptor made of a conductive material, a first dielectric layer formed on the main surface of the susceptor by a thermal spraying method, an electrode layer formed on the first dielectric layer by a thermal spraying method, A second dielectric layer formed on the electrode layer by a thermal spraying method; and a DC voltage application unit that applies a DC (direct current) voltage to the electrode layer. A DC (direct current) voltage is applied to the electrode layer. By applying the charge, charges are accumulated on the surface to be processed of the substrate placed on the second dielectric layer, and the substrate is attracted by an electrostatic attractive force acting between the charges and the electrode layer. Hold.

In the above configuration, the DC voltage from the DC voltage application unit is applied to the electrode layer that is completely insulated and separated from the surroundings by the first and second dielectric layers, and is not directly applied to the susceptor. As a result, abnormal discharge is unlikely to occur between the susceptor and the plasma, and abnormal discharge can also be prevented between the electrode layer to which the DC voltage is applied and the plasma. The first and second dielectric layers preferably have a volume resistivity of 1 × 10 ¹⁴ Ω · cm or more in order to guarantee reliability as an insulator against a high-voltage DC voltage. As the material, ceramics mainly containing at least one of Al ₂ O ₃ and ZrO ₂ is preferable.

  According to a preferred aspect of the present invention, a through hole for heat transfer gas for controlling the temperature of the substrate is provided penetrating from the susceptor to the upper surface of the second dielectric layer, and the electrode layer is formed in the through hole. Use a structure that is not exposed on the wall. According to this through-hole inner wall insulator structure, even if a heat transfer gas leakage path is formed between the substrate and the second dielectric layer, the electrode layer is not electrically coupled with the plasma, There is no discharge. The susceptor may be provided with a cooling mechanism or a heating mechanism for controlling the temperature of the substrate by a cooling method or a heating method.

  According to one aspect of the present invention, a high frequency from a high frequency power supply is applied to the susceptor with a desired power. In this case, it is preferable that the DC voltage application unit includes a direct current power source that outputs a DC voltage, and a resistor or a low-pass filter that substantially blocks the high frequency from the high frequency power source and passes the DC voltage. The DC voltage application unit can be protected from the high frequency on the susceptor side by such a high frequency cutoff function of the resistor or the low pass filter.

  According to a preferred aspect, the susceptor is grounded via a resistor. When a DC voltage is applied to the electrode layer from the DC voltage application unit, the potential of the susceptor rises to the vicinity of the DC voltage due to capacitive coupling via the first dielectric layer, but the potential of the susceptor is increased via the resistor. It can be lowered to near the ground electric field to prevent abnormal discharge between the susceptor and the plasma.

According to a preferred aspect, a thermal stress buffer material having an expansion coefficient intermediate between the expansion coefficient of the first dielectric layer and the expansion coefficient of the susceptor is inserted between the first dielectric layer and the susceptor. Is done. As described above, when the first dielectric layer is made of ceramics mainly composed of Al ₂ O ₃ or ZrO ₂ and the susceptor is made of Al metal, a Ni-5Al alloy is preferably used as the thermal stress buffer. Can be used. By interposing such a thermal stress buffer material, the thermal stress resistance of the first dielectric layer is greatly improved, and cracks are less likely to occur.

  A first plasma processing apparatus of the present invention is a plasma processing apparatus for performing a desired plasma processing on a substrate to be processed made of an insulator, a processing container for providing a processing space for the plasma processing, and the processing An electrostatic adsorption device of the present invention for holding the substrate in a container, a processing gas supply unit for supplying a processing gas into the processing chamber, an exhaust unit for exhausting the processing chamber, and a processing chamber A plasma generation unit that generates plasma of the processing gas.

  In the first plasma processing apparatus, even if the insulating substrate is large, the electrostatic adsorption device of the present invention holds the substrate stably and reliably, so that the temperature of each part of the substrate can be uniformly controlled. An in-plane uniform plasma treatment can be performed on the top.

  A second plasma processing apparatus of the present invention is a plasma processing apparatus for performing a desired plasma processing on a substrate to be processed made of an insulator, a processing container providing a processing space for the plasma processing, and the processing An electrostatic adsorption apparatus of the present invention for holding the substrate in a container; a processing chamber in which a predetermined plasma process is performed on the substrate; a processing gas supply unit for supplying a processing gas into the processing chamber; An exhaust part for exhausting the interior of the processing chamber; a plasma generating part for generating plasma of a processing gas in the processing chamber; and the insulation placed on the second dielectric layer of the electrostatic adsorption device And a heat transfer gas supply unit that supplies heat transfer gas to the back surface of the substrate.

  In the second plasma processing apparatus, the electrostatic adsorption apparatus of the present invention is provided with a heat transfer gas passage for controlling the temperature of the substrate penetrating from the susceptor to the upper surface of the second dielectric layer, It has a structure in which the electrode layer is not exposed on the inner wall surface of the through hole, that is, the through hole inner wall insulating structure. Thereby, abnormal discharge from the inside of the through hole does not occur.

  In a preferred aspect of the second plasma processing apparatus, a gas flow rate monitoring unit that monitors the flow rate of the heat transfer gas supplied from the heat transfer gas supply unit to the back surface of the substrate, and a measured value of the gas supply flow rate A sequence control unit is provided for comparing with a predetermined reference value and determining whether or not to activate the plasma generation unit according to the comparison result. Preferably, the heat transfer gas is He gas, the gas pressure supplied to the back surface of the substrate is set in the range of 1 Torr to 10 Torr, and the DC voltage applied to the electrode layer of the electrostatic adsorption device is in the range of 2 kV to 5 kV. May be set.

  According to a preferred aspect, in the monitoring, the heat transfer gas is supplied to the back surface of the substrate at a first pressure, and when performing plasma processing on the substrate, the heat transfer is performed at a second pressure larger than the first pressure. Gas is supplied to the back side of the substrate.

  The plasma processing method of the present invention is a method of performing plasma processing using the second plasma processing apparatus, wherein the substrate is placed on a second dielectric layer of the electrostatic adsorption apparatus; The step of introducing a processing gas into the processing chamber of the processing apparatus, the step of applying a DC voltage to the electrode layer of the electrostatic adsorption apparatus, and after starting the application of the DC voltage, from the heat transfer gas supply unit Supplying heat transfer gas to the back surface of the substrate at a predetermined pressure and monitoring the supply flow rate, comparing the measured value of the heat transfer gas flow rate with a predetermined reference value, and performing the processing according to the comparison result Determining whether to generate plasma of the processing gas in the room.

  According to the plasma processing method of the present invention, a processing gas is introduced into a processing container, and before and after this, a DC voltage is applied to the electrode layer of the electrostatic adsorption device, and then a heat transfer gas pressure is applied to the insulating substrate. Part of the glass substrate is ionized by the introduction of the processing gas, so that the upper surface of the glass substrate is appropriately charged, and an appropriate electrostatic adsorption force is obtained. Under this electrostatic adsorption force, the heat transfer gas leakage flow rate is monitored. . As a preferred embodiment, when the measured value of the heat transfer gas flow rate is equal to or less than the reference value, plasma of the process gas may be generated in the processing chamber to perform plasma processing on the substrate, and the measured value of the heat transfer gas flow rate is When the reference value is exceeded, plasma processing on the substrate may be stopped without generating plasma of the processing gas in the processing chamber. This can prevent abnormal discharge caused by poor holding of the substrate, edge loss or mounting displacement on the mounting table.

  According to the electrostatic attraction apparatus of the present invention, with the above-described configuration and operation, the holding force to the insulating substrate is increased without causing abnormal discharge or dielectric breakdown, and even a large substrate is stably and reliably held. Can be improved.

  According to the plasma processing apparatus and the plasma processing method of the present invention, with the above-described configuration and operation, the substrate can be stably and reliably held in response to the increase in size of the insulating substrate, and the entire substrate can be cooled uniformly. In-plane uniform plasma treatment can be performed. It is also possible to prevent abnormal discharge due to poor holding of the substrate to be processed on the mounting table, edge loss, or mounting displacement.

  Hereinafter, preferred embodiments of the present invention will be described with reference to FIGS.

  FIG. 1 shows the configuration of an electrostatic chuck according to a first embodiment of the present invention. This electrostatic adsorption apparatus is for holding an FPD insulating substrate, for example, a glass substrate G, in a processing container of a plasma processing apparatus, and has a rectangular mounting table 10 corresponding to the rectangular glass substrate G. Yes. In the mounting table 10, a rectangular block-shaped susceptor 14 made of a conductor such as aluminum and a rectangular frame-shaped focus ring 16 made of an insulator such as ceramic or quartz are provided on a base member 12 and surrounding the susceptor 14. And an electrostatic attraction portion 24 having a three-layer structure of a lower dielectric layer 18, an electrode layer 20 and an upper dielectric layer 22 each formed by a thermal spraying method on the main surface (upper surface) of the susceptor 14. Yes.

Here, the lower dielectric layer 18 and the upper dielectric layer 22 are made of an insulator having a volume resistivity of 1 × 10 ¹⁴ Ω · cm or more, preferably alumina (Al ₂ O ₃ ) and zirconia (ZrO ₂ ). It consists of ceramics which have at least one as a main component. The electrode layer 20 may be any conductive material, and is made of, for example, tungsten. Three layers of the lower dielectric layer 18, the electrode layer 20, and the upper dielectric layer 22 can be sequentially stacked on the main surface of the susceptor 14 by a known plasma spraying method.

  A refrigerant flow path 26 is provided inside the susceptor 14, and a temperature-controlled refrigerant from a chiller device (not shown) flows through the refrigerant flow path 26. The upper surface of the susceptor 14 and the electrostatic adsorption portion 24 (18, 20, 22) are provided with a large number of through holes 28, and He gas from a He gas supply system (not shown) is used for heat transfer. Gas is supplied to the back surface of the glass substrate G at a predetermined pressure through the gas flow path inside the susceptor and the through holes 28.

  As shown in FIG. 2, a circular cutout (notch) 20 a having a larger diameter than the through-hole 28 is formed in the electrode layer 20 around the through-hole 28 (portion shown by oblique lines). The electrode layer 20 is not exposed in the through hole 28, and the middle or upper wall surface in the through hole 28 is constituted by the lower dielectric layer 18 and the upper dielectric layer 22. Further, the outer peripheral edge of the electrode layer 20 is also recessed inside the outer peripheral edges of the lower dielectric layer 18 and the upper dielectric layer 22, and has a structure that is not exposed to the outside. As described above, the entire electrode layer 20 is buried between the lower dielectric layer 18 and the upper dielectric layer 22.

  In FIG. 1, an output terminal of a high frequency power supply 32 is electrically connected to the susceptor 14 via a matching unit 30. The output frequency of the high frequency power supply 32 is selected within the range of several MHz to several tens of MHz, and the output power is selected to be about several kW. On the other hand, an output terminal of a direct current (DC) power supply 34 is electrically connected to the electrode layer 20 of the electrostatic adsorption unit 24 via a high frequency cutoff unit 36. The high-frequency cutoff unit 36 is for blocking high-frequency waves from the susceptor 14 side, and may be configured by a resistor having a high resistance value of preferably 1 MΩ or more or a low-pass filter that passes a direct current. The switch 38 is for switching the DC power supply 34 and the ground potential with respect to the electrode layer 20.

  During the plasma processing, a plasma PZ of processing gas is generated on the glass substrate G. The plasma PZ may be generated by a high frequency from a high frequency power source 32 or may be generated by a high frequency from another high frequency power source (not shown). In the latter case, the high frequency applied to the susceptor 14 from the high frequency power supply 32 is used as a bias for drawing ions in the plasma PZ into the upper surface (surface to be processed) of the glass substrate G.

  When the switch 38 is switched to the DC power supply 34 side, a DC voltage from the DC power supply 34 is applied to the electrode layer 20. When this DC voltage is a positive voltage, it accumulates on the upper surface of the glass substrate G so as to attract negative charges (electrons and negative ions). As a result, an electrostatic force that attracts the glass substrate G and the upper dielectric layer 22 between the negative surface charge on the upper surface of the glass substrate G and the electrode layer 20, that is, a Coulomb force, works. Is fixed to the mounting table 10 by suction. When the switch 38 is switched to the ground side, the electrode layer 20 is neutralized, and the glass substrate G is also neutralized accordingly, and the Coulomb force, that is, the electrostatic adsorption force is released.

  In this electrostatic adsorption device, a DC voltage from a DC power source 34 is applied to the electrode layer 20 that is completely insulated and separated from the surroundings by the lower dielectric layer 18 and the upper dielectric layer 22 and directly applied to the susceptor 14. There is nothing. As a result, abnormal discharge hardly occurs between the susceptor 14 and the plasma PZ, and no abnormal discharge occurs between the electrode layer 20 to which the DC voltage is applied and the plasma PZ. In particular, since the inner wall of the through hole 28 is also composed of the dielectric layers 18 and 22, even if the He gas leakage path is formed on the contact surface between the substrate G and the upper dielectric layer 22, no abnormal discharge occurs. . Accordingly, the electrostatic attraction force can be increased by increasing the DC voltage. For this reason, it becomes possible to increase the supply amount of He gas, and good and uniform substrate temperature control can be performed even if the size of the glass substrate G is large.

  Further, in this electrostatic adsorption device, the high frequency cutoff unit 36 connected between the susceptor 14 and the DC power source 34 prevents the high frequency on the susceptor 14 side from leaking to the DC power source 34 side, and the DC power source 34. Can be protected from high frequency.

  In FIG. 3, the structure of the electrostatic attraction apparatus by the 2nd Example of this invention is shown. In the figure, parts having the same configuration or function as those of the first embodiment (FIG. 1) are denoted by the same reference numerals. In the second embodiment, a film-like (for example, 50 μm thick) thermal stress buffer 40 is provided between the susceptor 14 and the lower dielectric layer 18. This thermal stress buffer 40 can also be formed by plasma spraying.

  For example, in plasma etching, depending on the plasma processing conditions, the susceptor temperature may be set around 80 ° C. In this case, a thermal crack may occur in the dielectric layers 18 and 22 due to a difference in expansion coefficient between the dielectric layers 18 and 22 and the susceptor 14 in the electrostatic attraction portion 24, which may cause dielectric breakdown. In particular, when a high voltage is applied to the electrode layer 20, slight fatigue due to thermal stress of the dielectric layers 18 and 22 may lead to dielectric breakdown.

  The inventor examined the insulator material that constitutes the dielectric layers 18 and 22 and the conductor material that constitutes the susceptor 14 for dielectric breakdown caused by thermal stress of the dielectric layers 18 and 22. As a result, it was found that the difference in the expansion coefficient of the material between room temperature and 100 ° C. is the most important, but the toughness (particularly the shear stress resistance) of the dielectric layer or the insulator is also very important. The material of the susceptor 14 is preferably a material having high thermal conductivity, low metal contamination, and high workability. The material of the dielectric layers 18 and 22 is high insulation, high dielectric constant, and further, the top surface of the susceptor. It was confirmed that those having high adhesiveness with these are preferable.

Then, as shown in FIG. 3, it has been found that it is most effective from all points of view to interpose a thermal stress buffer material 40 as a conductor material in the interface region between the susceptor 14 and the lower dielectric layer 18. In this embodiment, the material of the susceptor 14 is Al metal, and the material of the lower dielectric layer 18 and the upper dielectric layer 22 is alumina (Al ₂ O ₃ ) having high voltage resistance or zirconia (ZrO ₂ ) having high toughness. The thermal stress buffer 40 is made of a Ni-5Al alloy. Here, the Ni-5Al alloy is an alloy having a (atomic) hybrid ratio of nickel and aluminum of 1: 5, and its linear expansion coefficient is larger than that of alumina or zirconia as shown in Table 1. It is smaller than the linear expansion coefficient of aluminum metal. Thus, as a material of the thermal stress buffer material 40, the linear expansion coefficient (expansion coefficient) is an intermediate value between the dielectric layers 18 and 22 and the susceptor 14, and the adhesion between the dielectric layers 18 and 22 is high. A high one is preferred.

  Thus, by providing the thermal stress buffer material 40 having an expansion coefficient intermediate between the susceptor 14 and the lower dielectric layer 18, the thermal stress resistance of the electrostatic adsorption unit 24 is greatly improved, The dielectric breakdown of the dielectric layers 18 and 22 due to stress can be reduced. Accordingly, it is possible to apply a high voltage DC to the electrode layer 20 with high reliability, and the glass substrate G can be stably and securely held on the mounting table 10 with high reliability.

  FIG. 4 shows the configuration of an electrostatic adsorption device according to a third embodiment of the present invention. In the figure, parts having the same configuration or function as those of the first and second embodiments (FIGS. 1 and 3) described above are denoted by the same reference numerals.

In the electrostatic adsorption device of the present invention, the electrode layer 20 and the susceptor 14 are capacitively coupled via the lower dielectric layer 18. Therefore, as shown in FIG. 5, the application of a DC voltage of from DC power source 34 [Phi _P (e.g. 5 kV) to the electrode layer 20, [Phi _s0 closer to be [Phi _P potential susceptor 14 by capacitive coupling (e.g. around 4kV ). If the plasma is ignited in this state (or if DC application is started during the generation of the plasma), an arc discharge may occur between the high potential susceptor 14 and the plasma PZ.

Therefore, in the third embodiment, the susceptor 14 is grounded via the resistor 42. Even if the potential of the susceptor 14 rises to several kV immediately after the start of the DC voltage application due to the capacitive coupling as described above, the potential of the susceptor 14 is exponentially expressed as Φ _s1 in FIG. Can be quickly lowered to the ground potential. Thereby, arc discharge between the susceptor 14 and the plasma PZ can be prevented. On the other hand, the resistor 42 needs to have a high resistance value R ₄₂ that can substantially cut off the high frequency applied to the susceptor 14 from the high frequency power supply 32. In this resistor 42, the optimum range of the resistance value R ₄₂ for achieving both high-frequency cutoff function and a dc potential clamping function as above is 1Emuomega～10emuomega.

  Next, an embodiment of a plasma processing apparatus provided with the electrostatic adsorption apparatus of the present invention will be described. FIG. 6 shows the configuration of an inductively coupled plasma (ICP) etching apparatus according to one embodiment. This plasma etching apparatus makes it possible to generate a high-density plasma at a low pressure. For example, when a thin film transistor (TFT) is formed on a glass substrate in manufacturing an LCD, a metal film, an ITO film, an oxide film, etc. are etched at a high speed. Used for. In the figure, parts having the same configuration or function as those of the first to third embodiments (FIGS. 1 to 4) described above are denoted by the same reference numerals.

This plasma etching apparatus has an airtight main body container 50 made of a conductive material such as aluminum whose inner wall surface is anodized (anodized). The main body container 50 is grounded. The interior of the main body container 50 is partitioned into an upper antenna chamber 54 and a lower processing chamber 56 by a horizontally extending dielectric wall 52. The dielectric wall 52 is made of ceramics such as Al ₂ O ₃ or quartz, and constitutes a ceiling wall on the processing chamber 56 side. A support shelf 58 projecting inward is provided between the side wall 54a of the antenna chamber 54 and the side wall 56a of the processing chamber 56, and the dielectric wall 52 is a seal member (not shown) on the support shelf 58. And are fixed by screws (not shown).

  The dielectric wall 52 has an assembled structure, and substantially the entire lower surface thereof is covered with a cover member 60 made of a dielectric material such as ceramics or quartz, and a shower head 62 for supplying a processing gas is contained therein. Is provided. The shower head 62 is made of aluminum whose inner surface is anodized, for example. A gas flow path or buffer chamber 64 that extends horizontally extends in the shower head 62. The buffer chamber 64 communicates with a plurality of gas discharge holes 64 a extending downward and opening through the cover member 60. On the other hand, a gas supply pipe 66 communicating with the buffer chamber 64 is attached to the center of the upper surface of the dielectric wall 52. The gas supply pipe 66 penetrates from the ceiling of the main body container 50 to the outside thereof and is connected to a processing gas supply system 68 including a processing gas supply source and a valve system. During plasma etching, the processing gas from the processing gas supply system 68 is introduced into the shower head 64 through the gas supply pipe 66 and discharged into the processing chamber 56 from the gas supply hole 64a on the lower surface thereof. Yes.

  In the antenna chamber 54, a high-frequency antenna 70 made of a planar coil antenna wound in a substantially square spiral shape is disposed on the dielectric wall 52. The spiral central end of the high-frequency antenna 70 is led out from the ceiling of the main body container 50, and is electrically connected to the output terminal of the high-frequency power source 74 via the matching unit 72. On the other hand, the outer end of the spiral is electrically connected to the main body container 52 and grounded via the main body container 52.

  During plasma etching, a high frequency power of a predetermined frequency, for example, 13.56 MHz, is supplied from the high frequency power source 74 to the high frequency antenna 70 via the matching unit 72, so that an alternating electric field parallel to the high frequency antenna 30 is generated in the processing chamber 56. The processing gas formed and supplied from the shower head 64 into the processing chamber 56 is turned into plasma by this alternating electric field. The output power of the high-frequency power source 74 may be set as appropriate so as to have a value sufficient to generate plasma.

  Below the processing chamber 56, the mounting table 10 of the electrostatic chuck according to the present invention is installed so as to face the high-frequency antenna 70 with the dielectric wall 52 interposed therebetween. In this plasma etching apparatus, the mounting table 10 is accommodated in a tray 76 made of an insulator, and further supported by a hollow column 78. The support 78 penetrates the bottom of the main body container 50 while maintaining an airtight state, and is supported by an elevating mechanism (not shown) disposed outside the main body container 50. When the substrate G is loaded and unloaded, the mounting table 10 is moved in the vertical direction by driving the lifting mechanism. A bellows 80 that hermetically surrounds the support column 78 is provided between the tray 76 and the bottom plate portion of the main body container 50 so that the airtightness in the processing chamber 56 can be maintained even when the mounting table 10 moves up and down. It has become. A gate valve 82 for opening and closing the substrate loading / unloading port is provided on the side wall 56a of the processing chamber 56.

  The base member 12 of the mounting table 10 is made of a conductive material such as aluminum or stainless steel, and a high frequency power supply 32 is electrically connected to the base member 12 via a matching unit 30 and a power feeding rod. During plasma etching, a high frequency for bias of 3.2 MHz, for example, is applied to the susceptor 14 from the high frequency power supply 32 via the base member 12, and ions in the plasma generated in the processing chamber 56 are effectively on the mounting table 10. Drawn into the glass substrate G. Here, the high frequency power supplied from the high frequency power supply 32 is normally set to a value lower than the high frequency power for plasma generation supplied from the upper high frequency power supply 74.

  Pipes and wires for each part of the mounting table 10 are drawn out of the main body container 50 through the hollow column 78 and connected to various power sources or various power / control devices. The He gas delivered from the He gas supply system 84 is pressure-adjusted by a PCV (Pressure Control Valve) 86 and then sent to the through hole 28 of the mounting table 10. The flow rate measuring device 88 attached to the PCV 86 detects the flow rate of He gas supplied to the through hole 28 side, and is used to monitor the leakage flow rate of He gas during electrostatic adsorption described later. The gas flow rate measurement value obtained by the flow rate measuring device 88 is given to the control unit 90.

  An exhaust mechanism 94 including an exhaust pipe 92 and a vacuum pump (not shown) is connected to an exhaust port provided at the bottom of the processing chamber 56. The inside of the processing chamber 56 is exhausted by the exhaust mechanism 94, and the inside of the processing chamber 56 is maintained in a predetermined vacuum atmosphere (for example, 10 mTorr = about 1.33 Pa) during the plasma processing. The control unit 90 may be constituted by a microcomputer and individually controls each part of the plasma etching apparatus, that is, the high frequency power sources 32 and 74, the switch 38, the processing gas supply system 68, the He gas supply system 84, the exhaust mechanism 94, and the like. At the same time, the operation sequence of the entire apparatus is controlled.

  In this plasma etching apparatus, even if the glass substrate G is large, the electrostatic adsorption device of the present invention holds the substrate G stably and reliably. In-plane uniform plasma etching can be performed.

  Next, the preferable form of the electrostatic attraction apparatus incorporated in this plasma etching apparatus is demonstrated.

FIG. 7 shows the results of an experiment in which the substrate cooling effect of the heat transfer He gas on the glass substrate G on the mounting table 10 was examined. In this experiment, the temperature of measurement points set at different positions on the substrate was measured using a thermocouple by changing the supply pressure of He gas. As a representative measurement point, the “center” is the center of the substrate, and the “edge” is the edge of the substrate. The main conditions are as follows.
Substrate size (diagonal dimension) = 500 mm
Board thickness = 0.7mm
Pressure in chamber = 30mTorr
Process gas = O ₂
High frequency power (13.56MHz / 3.2MHz) = 5000W / 3000W
DC voltage = 2500V
Time = 180 seconds

  During plasma etching, the temperature of the glass substrate G rises due to heat input from the plasma, but by applying He gas from the susceptor 14 side to the back surface of the substrate, the substrate temperature is lowered to a constant value and the temperature in the substrate surface is made uniform. Can be maintained. As can be seen from FIG. 7, when the He gas pressure is 0 to 2 Torr, the cooling effect increases as the pressure increases, and the substrate temperature decreases. However, when the He gas pressure is 2 Torr or more (particularly 3 Torr or more), the cooling effect is saturated. . Therefore, it is preferable that the heat transfer He gas pressure used in this plasma etching apparatus is 2 Torr or more. On the other hand, since the He gas pressure acts on the back surface of the insulating substrate and works in a direction that causes the insulating substrate to be detached from the mounting table or cause mounting displacement, an excessive He gas pressure is not preferable. For this reason, it is preferable that the He gas pressure has an upper limit of about 10 Torr.

  FIG. 8 shows the relationship between the DC voltage applied to the electrode layer 20 and the adsorption pressure (electrostatic adsorption force) to the glass substrate G. As illustrated, the adsorption pressure increases in proportion to the square of the DC applied voltage. As described with reference to FIG. 7, it is considered that a He gas pressure of about 5 Torr is sufficient from the viewpoint of the substrate cooling effect. This means that 5 Torr is sufficient as the adsorption pressure for fixing and holding the substrate against the He gas pressure. In FIG. 9, the relationship between the insulating film thickness and the applied voltage necessary for obtaining the adsorption pressure of 5 Torr is shown by a characteristic curve (straight line) A, and the dielectric breakdown voltage of the insulating film itself is shown by a characteristic curve (straight line) B. The shaded area in the figure (area surrounded by A and B) is a combination of an insulating film thickness and an applied voltage that can be realized. Thereby, it can be said that it is preferable that the insulating film thickness is 400 μm and the applied voltage is about 5 kV.

In FIG. 9, an alumina film is described as the material of the dielectric layers 18 and 22, but a zirconia film formed by a thermal spraying method is also examined and confirmed that it can be used sufficiently. As described above, since zirconia has high toughness and is particularly resistant to thermal stress, it is suitable for increasing the reliability of the electrostatic adsorption portion. Zirconia is excellent in plasma resistance like alumina, and its relative dielectric constant is 20-30, which is more than twice that of the alumina film (10). Usually, the adsorption force (adsorption pressure) increases in proportion to the square of the dielectric constant of the dielectric layer, so it can be said that it is a more promising ceramic than alumina in the future. However, zirconia has a higher leakage current (hopping current) in the film than the alumina film, and in order to suppress the leakage current and ensure the reliability in FIG. is there. The adsorption pressure decreases in inverse proportion to the square of the film thickness. In short, the alumina film is excellent in terms of voltage resistance and thinning, and the zirconia film is excellent in toughness or crack resistance, and both can be suitably used as the material of the dielectric layers 18 and 22. When alumina (Al ₂ O ₃ ) and zirconia (ZrO ₂ ) are mixed in the ceramic material constituting the dielectric layers 18 and 22, the component ratio is preferably about 50%: 50%.

  Thus, the dielectric layer formed by the thermal spraying method as in the present invention is superior in insulation properties to the insulator layer of a normal ceramic sintered body. Further, the thermal spraying method has an advantage that a dielectric film can be easily formed even on the surface of a member having a large area, and can be advantageously applied to a mounting table for a large substrate.

  Next, a characteristic operation in the plasma etching apparatus of this embodiment will be described with reference to FIGS.

FIG. 10 shows an equivalent circuit of a main part around the mounting table 10 in this plasma etching apparatus. In this equivalent circuit, SW ₁ is a changeover switch 38, SW ₂ is an on / off switch of a high-frequency power supply 32, R ₃₆ and R ₄₂ are resistances of a high-frequency cutoff unit 36 and a resistor 42, respectively, and C ₁₈ is a lower dielectric layer. 18 is a capacitance (capacitance), C _{G, 22} is a series capacitance of the glass substrate G and the upper dielectric layer 22, and Z _P is the impedance of the plasma. Nodes N ₂₀ and N ₁₄ correspond to the electrode layer 20 and the susceptor 14, respectively. FIG. 11 shows an operation sequence immediately after the start of the plasma etching process in this plasma etching apparatus. This operation sequence is executed under the control of the control unit 90.

First, the processing gas supply system 68 is operated, and the processing gas is introduced into the processing chamber 56 through the shower head 94. Before and after this, the switch SW ₁ (38) is switched to the DC power source 34. Thus, DC voltage from the DC power source 34 is applied to the node N ₂₀ via the resistor R ₃₆ (electrode layer 20). The potential of the node ₂₀ rises as Φ _P in FIG. 5 with a time constant C ₁₈ × (R ₃₆ + R ₄₂ ). Charge is accumulated on the upper surface of the glass substrate G by the application of the DC voltage, and the glass substrate G is placed on the mounting table 10 (by the electrostatic attraction (Coulomb force) acting between the surface charge and the electrode layer 20 on the mounting table 10 side. More precisely, it is held fixed on the upper dielectric layer 22). On the other hand, when the potential of the node ₂₀ rises as described above, the potential of the node N ₁₄ (susceptor 14) also rises due to the coupling via the capacitor _C18 . However, since the node N ₁₄ is grounded via the resistor R ₄₂ , the potential of the node N ₁₄ is approximately a time constant C ₁₈ × (R ₃₆ + R ₄₂ ) and is exponential as shown by Φ _s1 in FIG. Immediately drops to near ground potential.

As described above, a predetermined time after switching the switch SW ₁ (38) to the DC power source 34, the He gas supply system 84 is operated to supply He gas to the substrate G on the mounting table 10. In addition, the cooling medium is supplied to the refrigerant flow path 26 of the susceptor 14 before the plasma processing is started. When starting the supply of the He gas, a supply pressure (for example, 1.5 Torr) lower than a set value (for example, 4 Torr) at the time of processing is selected. Then, the He gas flow rate at that time is monitored by the flow rate measuring device 88 and the control unit 90. When the monitor value (He flow rate measurement value) is below the reference value, it is determined that the amount of He gas leaking from the mounting table 10 is within the allowable range, and the switch SW ₂ is turned on and high-frequency power is turned on. Then, the plasma is ignited (SW ₃ on). Then, the He gas flow rate is increased to the original set value (steady value), and the intended plasma etching is performed. However, when the monitor value (He gas flow rate measurement value) exceeds the reference value as shown by the dotted line in FIG. 11, it is determined that the amount of He gas leaking from the mounting table 10 exceeds the allowable range, At this time, that is, without generating plasma, the process is interrupted or stopped without turning on the switches SW ₂ and SW ₃ .

  The reason why considerable gas leakage occurs from the beginning of the supply of He gas in this way is that when a sufficient electrostatic adsorption force as set on the glass substrate G is not acting on the mounting table 10 or glass The case where the edge part of the board | substrate G is missing, the case where the mounting position of the glass substrate G has shifted | deviated, etc. can be considered. In any case, if plasma is generated with such troubles, abnormal discharge may occur at that time and the electrode may be damaged. In this embodiment, such trouble can be detected at an early stage by monitoring the He gas leakage flow rate before the generation of plasma, so that abnormal discharge can be prevented in advance.

  In the operation sequence of this embodiment, the procedure of first introducing the processing gas into the processing chamber 56 and then applying the He gas pressure to the glass substrate G is important. That is, a part of the glass substrate G is ionized by introducing the processing gas, whereby the upper surface of the glass substrate G is appropriately charged, and an appropriate electrostatic attraction force is obtained. On the other hand, in the procedure in which He gas pressure is applied while the processing chamber 56 is kept in a high vacuum without introducing the processing gas, the electrostatic adsorption force applied to the glass substrate G is very weak, and even at a low He gas pressure. There is a possibility that the glass substrate G is detached from the mounting table 10 or misaligned. Note that the electrostatic attraction force at the time of introducing the processing gas may vary depending on the type and flow rate of the processing gas. If a sufficiently large (for example, 2 Torr or more) electrostatic adsorption force can be obtained only by introducing the processing gas, the He gas may be supplied from the beginning at the original set flow rate.

As for the order of the timing for introducing the processing gas and the timing for turning on the switch SW ₁ , the same effect as described above can be obtained even if the processing gas is introduced after turning on the SW _{1 first} .

  FIG. 12 shows a configuration of a capacitively coupled plasma (CCP) etching apparatus as another example of the plasma processing apparatus provided with the electrostatic adsorption apparatus of the present invention. In the figure, parts having the same configuration or function as those of the plasma etching apparatus (FIG. 6) in the fourth embodiment are given the same reference numerals.

  This plasma etching apparatus has a chamber (processing vessel) 100 formed into a rectangular tube shape made of aluminum whose surface is anodized, for example. At the bottom of the chamber 100, a mounting table 10 for an electrostatic chuck according to the present invention is installed. Here, the base member 12 of the mounting table 10 is made of an insulating material, and the susceptor 14 constituting the lower electrode is insulated and separated from the chamber 100.

  Above the mounting table 10, a shower head 102 that functions as an upper electrode is provided so as to face the susceptor 14 in parallel. The shower head 102 is supported on the upper part of the chamber 100, has a buffer chamber 104 inside, and has a plurality of discharge holes 106 for discharging a processing gas on the lower surface facing the susceptor 14. The shower head 102 is grounded and forms a pair of parallel plate electrodes together with the susceptor 14.

A gas inlet 108 is provided on the upper surface of the shower head 102, and the processing gas from the processing gas supply system 68 is introduced into the buffer chamber 104 of the shower head 102 through the gas inlet 108. As the processing gas (etching gas), a gas usually used in this field, such as a halogen-based gas, an O ₂ gas, or an Ar gas, can be used. The high frequency applied to the susceptor 14 from the high frequency power supply 32 is selected to be a relatively high frequency, for example, 13.56 MHz, and is used for both plasma generation and bias. Also in this CCP etching apparatus, the effect of the present invention can be obtained in the same manner as in the above-described ICP etching apparatus.

  Although the plasma processing apparatus of the above-described embodiment is related to an etching apparatus, it is also used in applications such as plasma CVD of an insulator film, a conductor film, or a semiconductor film, plasma cleaning of an insulating substrate surface, and plasma cleaning of a chamber inner wall. The same applies. In this case, the present invention can be similarly applied to a system in which the susceptor side of the electrostatic adsorption device is grounded. The present invention can also be applied to a plasma processing apparatus using helicon wave plasma generation or ECR (Electron Cyclotron Resonance) plasma generation as plasma generation. The monitoring function of the heat transfer gas leakage flow rate in the present invention and the abnormality detection function or operation sequence function based on this monitoring function can be suitably applied to the plasma processing apparatus provided with the electrostatic adsorption device of the present invention as described above. The present invention can be applied to a plasma processing apparatus including any electrostatic adsorption device that uses a heat transfer gas.

  In addition, various modifications can be made within the scope of the technical idea of the present invention. For example, a system in which a negative DC voltage is applied to the electrode layer (22) in the electrostatic adsorption device of the present invention, a configuration in which a heating mechanism is provided in the susceptor 14, and the like are possible. It is also possible to use different insulating materials for the lower dielectric layer 18 and the upper dielectric layer 22. The substrate to be processed of the insulator in the present invention is not limited to the LCD glass substrate, but can be applied to an arbitrary insulating substrate for FPD and an insulating substrate for other purposes.

It is a schematic sectional drawing which shows the structure of the electrostatic attraction apparatus in 1st Example of this invention. It is a schematic plan view which shows the structure of the principal part of the mounting base in the electrostatic attraction apparatus of an Example. It is a schematic sectional drawing of the electrostatic attraction apparatus in a 2nd Example. It is a schematic sectional drawing of the electrostatic attraction apparatus in a 3rd Example. It is a figure which shows typically the change of a susceptor electric potential at the time of DC voltage application in the electrostatic attraction apparatus of this invention. It is a schematic sectional drawing which shows the structure of the plasma processing apparatus in a 4th Example. It is a graph of one experimental example which shows the board | substrate cooling effect of He gas in the electrostatic attraction apparatus of this invention. It is a graph which shows the relationship between the attractive_force | adsorptive_power and applied voltage in the electrostatic attraction apparatus of this invention. It is a graph for showing the preferable film thickness of the dielectric material layer used for the electrostatic attraction apparatus of this invention. It is a circuit diagram which shows the equivalent circuit of the principal part of the plasma processing apparatus of an Example. It is a time sequence which shows the operation | movement sequence in the plasma processing apparatus of an Example. It is a schematic sectional drawing which shows the structure of the plasma processing apparatus in 2nd Embodiment. It is a schematic sectional drawing which shows the structure of the electrostatic attraction apparatus of one prior art example. It is a schematic sectional drawing which shows the structure of the electrostatic adsorption apparatus of another prior art example.

Explanation of symbols

G Glass insulating substrate 10 Mounting table 12 Base member 14 Susceptor 16 Focus ring 18 Lower dielectric layer 20 Electrode layer 22 Upper dielectric layer 24 Electrostatic adsorption part 26 Refrigerant flow path 28 Through hole 30 Matching device 32 High frequency power supply 34 DC (direct current) ) Power supply 36 High frequency cutoff unit 38 Switch 40 Thermal stress buffer member 42 Resistor 50 Main body container 52 Dielectric wall 56 Processing chamber 64 Shower head 70 High frequency antenna 74 High frequency power supply 84 He gas supply system 86 PCV
88 Flow meter 90 Control unit 94 Exhaust mechanism 100 Chamber 102 Shower head

Claims (20)

An electrostatic adsorption apparatus for electrostatically adsorbing and holding a substrate to be processed made of an insulator in a space where plasma is generated,
A susceptor made of a conductor for supporting the substrate;
A first dielectric layer formed on the main surface of the susceptor by a thermal spraying method;
An electrode layer formed on the first dielectric layer by a thermal spraying method;
A second dielectric layer formed on the electrode layer by a thermal spraying method;
A surface to be processed of the substrate placed on the second dielectric layer by applying the DC voltage to the electrode layer. An electrostatic attraction apparatus for accumulating electric charges and holding the substrate by electrostatic attraction acting between the electric charges and the electrode layer. The electrostatic attraction apparatus according to claim 1, wherein the first and second dielectric layers have a volume resistivity of 1 × 10 ¹⁴ Ω · cm or more.   A through hole for heat transfer gas for controlling the temperature of the substrate is provided to penetrate from the susceptor to the upper surface of the second dielectric layer, and the electrode layer is not exposed on the inner wall surface of the through hole. The electrostatic attraction apparatus according to claim 1 or 2.   The electrostatic attraction apparatus according to claim 1, wherein a high-frequency power source that outputs a high frequency with a desired power is electrically connected to the susceptor.   5. The DC voltage application unit according to claim 4, comprising: a DC power supply that outputs the DC voltage; and a resistor or a low-pass filter that substantially cuts off a high frequency from the high-frequency power supply and passes the DC voltage. Electrostatic adsorption device.   The electrostatic adsorption device according to any one of claims 1 to 5, wherein the susceptor is grounded to a ground via a resistor.   The electrostatic attraction apparatus according to claim 6, wherein the resistor has a resistance value of 1 MΩ to 10 MΩ.   A thermal stress buffer material having an expansion coefficient intermediate between the expansion coefficient of the first dielectric layer and the expansion coefficient of the susceptor is inserted between the first dielectric layer and the susceptor. The electrostatic attraction apparatus as described in any one of 1-7. It said first and second dielectric layers, electrostatic chuck according to any one of claims 1 to 8 made of a ceramic composed mainly of at least one of Al ₂ O ₃ and ZrO _2.   The electrostatic attraction apparatus according to claim 9, wherein the susceptor is made of Al metal, and the thermal stress buffer is made of a Ni-5Al alloy.   The electrostatic attraction apparatus according to claim 1, wherein the susceptor is provided with a cooling mechanism for cooling the substrate.   The electrostatic attraction apparatus according to claim 1, wherein the susceptor is provided with a heating mechanism for heating the substrate. A plasma processing apparatus for performing a desired plasma processing on a substrate to be processed made of an insulator,
A processing vessel providing a processing space for the plasma processing;
The electrostatic adsorption device according to any one of claims 1 to 12, for holding the substrate in the processing container,
A processing gas supply unit for supplying a processing gas into the processing chamber;
An exhaust section for exhausting the interior of the processing chamber;
A plasma processing apparatus, comprising: a plasma generation unit configured to generate plasma of processing gas in the processing chamber. A plasma processing apparatus for performing a desired plasma processing on a substrate to be processed made of an insulator,
A processing vessel providing a processing space for the plasma processing;
The electrostatic attraction apparatus according to any one of claims 3 to 12 for holding the substrate in the processing container;
A processing chamber in which a predetermined plasma processing is performed on the substrate;
A processing gas supply unit for supplying a processing gas into the processing chamber;
An exhaust section for exhausting the interior of the processing chamber;
A plasma generator for generating plasma of a processing gas in the processing chamber;
A plasma processing apparatus, comprising: a heat transfer gas supply unit configured to supply a heat transfer gas to the back surface of the insulating substrate placed on the second dielectric layer of the electrostatic adsorption device. A gas flow rate monitoring unit for monitoring the supply flow rate of the heat transfer gas supplied from the heat transfer gas supply unit to the back surface of the substrate;
The plasma processing apparatus according to claim 14, further comprising: a sequence control unit that compares the measured value of the supply flow rate with a predetermined reference value and determines whether to operate the plasma generation unit according to the comparison result. The heat transfer gas is He gas, the gas pressure supplied to the back surface of the substrate is set in the range of 1 Torr to 10 Torr , and the DC voltage applied to the electrode layer of the electrostatic adsorption device is in the range of 2 kV to 5 kV. The plasma processing apparatus of Claim 14 or Claim 15 set to these. A method for performing plasma processing using the plasma processing apparatus according to claim 15 or 16, comprising:
Placing the substrate on the second dielectric layer of the electrostatic chuck;
Introducing a processing gas into the processing chamber of the processing apparatus;
Applying a DC voltage to the electrode layer of the electrostatic adsorption device;
After starting application of the DC voltage, supplying a heat transfer gas to the back surface of the substrate at a predetermined pressure from the heat transfer gas supply unit and monitoring the supply flow rate;
Comparing the measured value of the heat transfer gas flow rate with a predetermined reference value and determining whether or not to generate plasma of the processing gas in the processing chamber according to the comparison result. When the measured value of the heat transfer gas flow rate is less than or equal to the reference value, the plasma of the processing gas is generated in the processing chamber to perform plasma processing on the substrate,
The plasma processing method according to claim 17, wherein when the measured value of the heat transfer gas flow rate exceeds the reference value, the plasma processing for the substrate is stopped without generating plasma of the processing gas in the processing chamber.  In the monitoring, the heat transfer gas is supplied to the back surface of the insulating substrate at a first pressure, and when performing plasma processing on the substrate, the heat transfer gas is supplied at a second pressure higher than the first pressure. The plasma processing method according to claim 18, wherein the plasma processing method is supplied to a back surface of the insulating substrate. A plasma processing apparatus for performing a desired plasma processing on a substrate to be processed made of an insulator,
A processing vessel providing a processing space for the plasma processing;
A mounting table for mounting the substrate in the processing container;
An electrostatic chuck for fixing and holding the substrate with an electrostatic chucking force on the mounting table;
A temperature control mechanism for cooling or heating the substrate on the mounting table from the back side of the substrate;
A processing gas supply unit for supplying a processing gas to the processing chamber;
A plasma generator for generating plasma of a processing gas in the processing chamber;
A heat transfer gas supply unit for supplying a heat transfer gas to the back surface of the insulating substrate placed on the second dielectric layer of the electrostatic adsorption device;
A gas flow rate monitoring unit for monitoring the supply flow rate of the heat transfer gas supplied from the heat transfer gas supply unit to the back surface of the substrate;
A plasma processing apparatus, comprising: a sequence control unit that compares a measured value of the gas supply flow rate with a predetermined reference value and determines whether to operate the plasma generation unit according to a comparison result.

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