US20120234491A1 - Plasma processing method and plasma processing apparatus - Google Patents
Plasma processing method and plasma processing apparatus Download PDFInfo
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- US20120234491A1 US20120234491A1 US13/469,851 US201213469851A US2012234491A1 US 20120234491 A1 US20120234491 A1 US 20120234491A1 US 201213469851 A US201213469851 A US 201213469851A US 2012234491 A1 US2012234491 A1 US 2012234491A1
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- 238000003672 processing method Methods 0.000 title description 18
- 239000007789 gas Substances 0.000 claims abstract description 131
- XKRFYHLGVUSROY-UHFFFAOYSA-N Argon Chemical compound [Ar] XKRFYHLGVUSROY-UHFFFAOYSA-N 0.000 claims abstract description 22
- 229910052743 krypton Inorganic materials 0.000 claims abstract description 19
- 229910052724 xenon Inorganic materials 0.000 claims abstract description 16
- 229910052786 argon Inorganic materials 0.000 claims abstract description 15
- DNNSSWSSYDEUBZ-UHFFFAOYSA-N krypton atom Chemical compound [Kr] DNNSSWSSYDEUBZ-UHFFFAOYSA-N 0.000 claims abstract description 8
- FHNFHKCVQCLJFQ-UHFFFAOYSA-N xenon atom Chemical compound [Xe] FHNFHKCVQCLJFQ-UHFFFAOYSA-N 0.000 claims abstract description 8
- 238000000034 method Methods 0.000 claims description 29
- 230000005284 excitation Effects 0.000 claims description 13
- 238000005121 nitriding Methods 0.000 claims description 10
- 230000015572 biosynthetic process Effects 0.000 claims description 9
- 238000005530 etching Methods 0.000 claims description 8
- 230000001590 oxidative effect Effects 0.000 claims description 7
- 239000000758 substrate Substances 0.000 abstract description 13
- 210000002381 plasma Anatomy 0.000 description 99
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 description 12
- 229910052710 silicon Inorganic materials 0.000 description 12
- 239000010703 silicon Substances 0.000 description 12
- 238000010586 diagram Methods 0.000 description 11
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 10
- 150000002500 ions Chemical class 0.000 description 8
- 239000000203 mixture Substances 0.000 description 7
- 238000004519 manufacturing process Methods 0.000 description 6
- 230000007423 decrease Effects 0.000 description 5
- 229910052581 Si3N4 Inorganic materials 0.000 description 4
- 229910052681 coesite Inorganic materials 0.000 description 4
- 229910052906 cristobalite Inorganic materials 0.000 description 4
- 239000004065 semiconductor Substances 0.000 description 4
- 239000000377 silicon dioxide Substances 0.000 description 4
- 229910052682 stishovite Inorganic materials 0.000 description 4
- 229910052905 tridymite Inorganic materials 0.000 description 4
- BLRPTPMANUNPDV-UHFFFAOYSA-N Silane Chemical compound [SiH4] BLRPTPMANUNPDV-UHFFFAOYSA-N 0.000 description 3
- 230000009977 dual effect Effects 0.000 description 3
- 229910052814 silicon oxide Inorganic materials 0.000 description 3
- KRHYYFGTRYWZRS-UHFFFAOYSA-N Fluorane Chemical compound F KRHYYFGTRYWZRS-UHFFFAOYSA-N 0.000 description 2
- 238000005229 chemical vapour deposition Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 239000012212 insulator Substances 0.000 description 2
- 150000004767 nitrides Chemical class 0.000 description 2
- 239000000523 sample Substances 0.000 description 2
- HQVNEWCFYHHQES-UHFFFAOYSA-N silicon nitride Chemical compound N12[Si]34N5[Si]62N3[Si]51N64 HQVNEWCFYHHQES-UHFFFAOYSA-N 0.000 description 2
- MYMOFIZGZYHOMD-UHFFFAOYSA-N Dioxygen Chemical compound O=O MYMOFIZGZYHOMD-UHFFFAOYSA-N 0.000 description 1
- UFHFLCQGNIYNRP-UHFFFAOYSA-N Hydrogen Chemical compound [H][H] UFHFLCQGNIYNRP-UHFFFAOYSA-N 0.000 description 1
- 238000004140 cleaning Methods 0.000 description 1
- 238000009792 diffusion process Methods 0.000 description 1
- 238000010790 dilution Methods 0.000 description 1
- 239000012895 dilution Substances 0.000 description 1
- 229910001882 dioxygen Inorganic materials 0.000 description 1
- NBVXSUQYWXRMNV-UHFFFAOYSA-N fluoromethane Chemical compound FC NBVXSUQYWXRMNV-UHFFFAOYSA-N 0.000 description 1
- 238000010438 heat treatment Methods 0.000 description 1
- 239000001257 hydrogen Substances 0.000 description 1
- 229910052739 hydrogen Inorganic materials 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 230000003647 oxidation Effects 0.000 description 1
- 238000007254 oxidation reaction Methods 0.000 description 1
- 239000001301 oxygen Substances 0.000 description 1
- 229910052760 oxygen Inorganic materials 0.000 description 1
- 229910021420 polycrystalline silicon Inorganic materials 0.000 description 1
- 229920005591 polysilicon Polymers 0.000 description 1
- 238000010926 purge Methods 0.000 description 1
- 238000011084 recovery Methods 0.000 description 1
Images
Classifications
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- C—CHEMISTRY; METALLURGY
- C23—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
- C23C—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
- C23C16/00—Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes
- C23C16/22—Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the deposition of inorganic material, other than metallic material
- C23C16/30—Deposition of compounds, mixtures or solid solutions, e.g. borides, carbides, nitrides
- C23C16/40—Oxides
- C23C16/401—Oxides containing silicon
- C23C16/402—Silicon dioxide
-
- C—CHEMISTRY; METALLURGY
- C23—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
- C23C—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
- C23C16/00—Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes
- C23C16/44—Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating
- C23C16/50—Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating using electric discharges
- C23C16/511—Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating using electric discharges using microwave discharges
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J37/00—Discharge tubes with provision for introducing objects or material to be exposed to the discharge, e.g. for the purpose of examination or processing thereof
- H01J37/32—Gas-filled discharge tubes
- H01J37/32009—Arrangements for generation of plasma specially adapted for examination or treatment of objects, e.g. plasma sources
- H01J37/32192—Microwave generated discharge
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J37/00—Discharge tubes with provision for introducing objects or material to be exposed to the discharge, e.g. for the purpose of examination or processing thereof
- H01J37/32—Gas-filled discharge tubes
- H01J37/32431—Constructional details of the reactor
- H01J37/3244—Gas supply means
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J37/00—Discharge tubes with provision for introducing objects or material to be exposed to the discharge, e.g. for the purpose of examination or processing thereof
- H01J37/32—Gas-filled discharge tubes
- H01J37/32431—Constructional details of the reactor
- H01J37/3244—Gas supply means
- H01J37/32449—Gas control, e.g. control of the gas flow
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/04—Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer
- H01L21/18—Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer the devices having semiconductor bodies comprising elements of Group IV of the Periodic Table or AIIIBV compounds with or without impurities, e.g. doping materials
- H01L21/30—Treatment of semiconductor bodies using processes or apparatus not provided for in groups H01L21/20 - H01L21/26
- H01L21/302—Treatment of semiconductor bodies using processes or apparatus not provided for in groups H01L21/20 - H01L21/26 to change their surface-physical characteristics or shape, e.g. etching, polishing, cutting
- H01L21/306—Chemical or electrical treatment, e.g. electrolytic etching
- H01L21/3065—Plasma etching; Reactive-ion etching
Definitions
- This invention relates to a method of plasma-processing a substrate or workpiece of an electronic device, such as a semiconductor-element or semiconductor-chip mounting substrate, a wiring substrate, or a flat panel display substrate, a processing apparatus therefor, and a manufacturing method for manufacturing an electronic device by such plasma processing.
- an electronic device such as a semiconductor-element or semiconductor-chip mounting substrate, a wiring substrate, or a flat panel display substrate, a processing apparatus therefor, and a manufacturing method for manufacturing an electronic device by such plasma processing.
- a plasma is generated using a single rare gas in plasma processing for oxidizing, nitriding, or oxynitriding the surface of a workpiece such as a silicon semiconductor, forming an oxide film, a nitride film, an oxynitride film, a polysilicon film, an organic EL film, or the like on the surface of a workpiece, or etching the surface of a workpiece by the use of a plasma.
- the rare gas use is made of a krypton (Kr) gas or a xenon (Xe) gas with a large electron-collision cross-sectional area and a low plasma electron temperature for reducing plasma damage on the workpiece (see, e.g. Patent Document 1).
- Patent Document 1 discloses an apparatus using Kr as a plasma excitation gas for forming an oxide film and a nitride film.
- This apparatus has a structure in which a coaxial waveguide, a radial line slot antenna, and microwave introducing windows are provided at an upper portion of a vacuum container serving as a process chamber in the order named from the outer side, a shower plate is provided inside the vacuum container, and a stage with a heating mechanism for placing a workpiece thereon is disposed under the shower plate.
- a plasma processing method the inside of the vacuum container is evacuated, an Ar gas is introduced from the shower plate, then the Ar gas is switched to a Kr gas and the pressure is set to 133 Pa.
- a silicon substrate (workpiece) having been subjected to dilute hydrofluoric acid cleaning is introduced into the process chamber and placed on the stage and then the workpiece is heated so as to be maintained at 400° C.
- a microwave is supplied to the radial slot antenna from the coaxial waveguide, for example, for 1 minute, thereby introducing the microwave into the process chamber through the dielectric plates (the microwave introducing windows and the shower plate).
- the dielectric plates the microwave introducing windows and the shower plate.
- a Kr/O 2 mixed gas at a predetermined partial pressure ratio is introduced from the shower plate, thereby forming a silicon oxide film having a nano-order thickness on the surface of the silicon substrate.
- a K 2 /NH 3 mixed gas is introduced from the shower plate and, while setting the pressure in the process chamber at about 133 Pa, the microwave is again supplied to generate a high-density plasma in the process chamber, thereby forming a silicon nitride film having a nano-order thickness on the surface of the silicon oxide film.
- the introduction of the microwave power is stopped to finish the plasma excitation when the formation of the silicon nitride film is finished, and then the Ar gas is substituted for the Kr/NH 3 mixed gas, thereby finishing the oxidation-nitriding process.
- the Ar gas is substituted for the Kr/NH 3 mixed gas, thereby finishing the oxidation-nitriding process.
- a plasma processing method and a plasma processing apparatus of this invention are characterized in that the electron temperature in a plasma is defined by a rare gas having a large electron-collision cross-sectional area while dilution of the gas is performed with a less expensive rare gas, thereby forming a gas in the plasma by these two or more kinds of rare gases.
- a plasma-processing method which comprises genarating a plasma by the use of a rare gas; and processing a workpies by the use of said plasma.
- the rare gas includes two or more kinds of different rare gases.
- the above-mentioned plasma processing method in which the different rare gases have electron-collision cross-sectional areas different from each other.
- any one of the above-mentioned plasma processing methods in which one of said two or more kinds of different rare gases is an argon gas while other gas is a gas having an electron-collision cross-sectional area larger than that of said argon gas.
- any one of the above-mentioned plasma processing methods in which one of said two or more kinds of different rare gases is an argon gas while other gas is at lease one of krypton and xenon.
- any one of the above-mentioned plasma processing methods in which the plasma is generated by microwave excitation.
- any one of the above-mentioned plasma processing methods in which the processing includes one of: oxidizing, nitriding, or oxynitriding of at least a portion of a surface of the workpiece; film forming on at least a portion of a surface of the workpiece; and etching of at least a portion of a surface of the workpiece.
- any one of the above-mentioned plasma processing methods in which the oxidizing, nitriding, or oxynitrizing at least a portion of a surface of the workpiece by the use of the plasma includes introducing a nitriding gas or an oxidizing gas into the plasma.
- any one of the above-mentioned plasma processing methods in which the film forming on at least a portion of a surface of the workpiece includes introducing a gas necessary to film forming into the plasma.
- any one of the above-mentioned plasma processing methods in which the film forming includes forming an insulating film.
- any one of the above-mentioned plasma processing methods which includes introducing a gas necessary for etching into the plasma and etching a selected portion or the whole of a surface of the workpiece.
- any one of the above-mentioned plasma processing methods in which the gas having the larger electron-collision cross-sectional area, of the two or more kinds of different rare gases, is introduced into a plasma excitation region.
- the gas having the smaller electron-collision cross-sectional area is introduced to the outside of the plasma excitation region.
- any one of the above-mentioned plasma processing methods which further comprises recovering a part or the whole of the rare gas for reuse is recovered.
- a method of manufacturing an electronic device such as a semiconductor device, a flat panel display device, a computer, or a portable telephone terminal, the method comprising a step of processing a workpiece by any one of the above-mentioned plasma processing methods.
- a plasma processing apparatus in which two or more kinds of different rare gases are supplied into a plasma process chamber.
- the above-mentioned plasma processing apparatus in which the rare gases have electron-collision cross-sectional areas different from each other.
- any one of the above-mentioned plasma processing apparatuses in which one of the rare gases is an argon gas and other gas is a gas having an electron-collision cross-sectional area larger than that of the argon gas.
- any one of the above-mentioned plasma processing apparatuses in which one of the rare gases is an argon gas and other gas is one or both of krypton and xenon.
- any one of the above-mentioned plasma processing apparatuses in which the plasma is generated by microwave excitation.
- any one of the above-mentioned plasma processing apparatuses in which the plasma chamber is supplied with a nitriding gas or an oxidizing gas in addition to the rare gases.
- any one of the above-mentioned plasma processing apparatuses in which the plasma chamber is supplied with a desired gas in addition to the rare gases to perform film formation on a workpiece.
- any one of the above-mentioned plasma processing apparatuses in which the plasma chamber is supplied with etching at least a portion of a workpiece, in addition to the rare gases.
- any one of the above-mentioned plasma processing apparatuses which introduces the rare gas having the larger electron-collision cross-sectional area into a plasma excitation region; and also introduces the argon gas to the outside of the plasma excitation region.
- any one of the above-mentioned plasma processing apparatuses which further comprises a rare gas recovery apparatus.
- a plasma processing method that recovers, regenerates, and uses the used rare gases, thereby making it possible to more efficiently use the expensive rare gases.
- a gas in which an Ar gas is added to one or both of Xe and Kr wherein the required ratio of Xe or/and Kr in the mixed gas changes depending on various conditions. In many cases, at least 20 vol % is required. When the ratio is about 40% or more, substantially no difference in effect is observed as compared with the case of 100%, and there is no problem when the ratio is 50% or more. Naturally, the ratio is less than 100%.
- FIG. 1 is a sectional view of a microwave-excited plasma processing apparatus for use in an embodiment 1 of this invention.
- FIG. 2 includes an explanatory diagram showing electron temperatures and collision cross-sectional areas of respective rare gases and a diagram showing excitation energies, ionization energies, and electron temperatures of Ar, Kr, and Xe gases.
- FIG. 3 is a sectional view showing a plasma measuring method.
- FIG. 4 shows luminous intensities of Ar/Xe mixed plasmas, wherein (a) shows relative intensities in the case of Xe + (466.8 nm) at 20 mTorr (2.66 Pa), (b) shows relative intensities in the case of Xe + (466.8 nm) at 40 mTorr (5.33 Pa), (c) shows relative intensities in the case of Ar (750.4 nm) at 20 mTorr (2.66 Pa), and (d) shows relative intensities in the case of Ar (750.4 nm) at 40 mTorr (5.33 Pa).
- FIG. 6 includes diagrams (a), (b), (c), and (d) showing electron densities, VSWRs, ion currents, and electron temperatures of Ar/Xe mixed plasmas, respectively.
- FIG. 7 includes a diagram (a) showing ion current densities when the pressure of a mixed gas is changed, and a diagram (b) showing electron temperatures when the pressure of a mixed gas is changed.
- FIG. 8 is a sectional view of a dual shower plate microwave-excited plasma processing apparatus for use in embodiments 2 and 3 of this invention.
- FIG. 1 is a sectional view of a microwave-excited plasma processing apparatus.
- FIG. 2 is a diagram showing the relationship between the electron energy and the total ionization cross-sectional area.
- FIG. 3 is a sectional view showing a plasma measuring method.
- FIG. 4 are diagrams showing luminous intensities of Ar/Xe mixed plasmas, wherein (a) shows relative intensities in the case of Xe + (466.8 nm) at 2.66 Pa (20 mTorr), (b) shows relative intensities in the case of Xe + (466.8 nm) at 5.33 Pa (40 mTorr), (c) shows relative intensities in the case of Ar (750.4 nm) at 2.66 Pa (20 mTorr), and (d) shows relative intensities in the case of Ar (750.4 nm) at 5.33 Pa (40 mTorr).
- FIG. 6( a ), ( b ), (c), and (d) are diagrams showing electron densities, VSWRs, ion currents, and electron temperatures of Ar/Xe mixed plasmas, respectively.
- FIG. 7( a ) is a diagram showing ion current densities when the ratio of Xe in an Ar/Xe mixed gas is changed from 0 to 1
- FIG. 7( b ) is a diagram showing electron temperatures when the ratio of Xe in an Ar/Xe mixed gas (pressure) is changed in the same manner.
- a microwave is radiated into an apparatus 11 by an antenna 1 disposed at an upper portion of a plasma processing apparatus 101 through an insulator plate 2 .
- An Ar gas, a Kr gas (or a Xe gas), and an oxygen gas (a N 2 /H 2 or NH 3 gas in the case of a nitriding process or a mixed gas of an oxidizing gas and a nitriding gas, such as an O 2 /NH 3 , O 2 /N 2 O, or O 2 /NO gas, in the case of an oxynitriding process) are introduced into the apparatus inside 11 from a gas introducing pipe 13 through a shower plate 3 , so that a plasma is excited above a workpiece 4 in the apparatus inside 11 by the microwave irradiated there as described above.
- the silicon wafer 4 being a workpiece substrate is placed in the process chamber 11 at a place where the plasma is directly irradiated, and is oxidized by oxygen radicals etc. excited by the plasma. In this event, it is preferable that the workpiece 4 be placed in the process chamber 11 not in a space where the plasma is excited, but in a space where the plasma is diffused.
- An exhaust gas in the process chamber 11 passes through exhaust ducts 6 via exhaust ports 5 so as to be conducted to non-illustrated small pumps through inlet ports 7 a and 7 b for the respective small pumps as indicated by broken-line arrows 19 .
- a probe 9 For measuring the excited plasma, a probe 9 is provided so that its tip end is projected into the process chamber 11 as shown in FIG. 3 .
- the probe 9 is fixed by an attaching member 15 .
- Luminous measurement is carried out through a different window as indicated by an arrow 14 .
- the luminous intensity (relative intensity) of Xe + is greater at 40 mTorr (5.33 Pa) than at 20 mTorr (2.66 Pa), while, the luminous intensity of Ar does not depend on the pressure when the partial pressure (molar fraction) of Xe is 0.2 or more.
- the electron density increases from a Xe composition ratio of 20% and, thereafter, monotonously increases as the composition ratio increases, and VSWR monotonously slightly decreases as the Xe composition ratio increases. It is seen that the ion current abruptly increases at a Xe composition ratio of 20% and the electron temperature abruptly decreases until a Xe composition ratio of 20% and, thereafter, monotonously decreases as the composition ratio increases.
- FIG. 7( a ) it is seen that when a pressure of a mixed gas, which corresponds to the total flow rate, is 20 mTorr (2.66 Pa), the ion current density abruptly increases near a Xe flow rate ratio of 0.75. Further, it is seen that when the total flow rate is 40 mTorr (5.33 Pa), the ion current density abruptly increases when the Xe flow rate ratio exceeds 0.2. Further, it is seen that when the total flow rate is 100 mTorr (13.33 Pa), the ion current density tends to almost monotonously increase.
- FIG. 8 is a schematic sectional view of a dual shower plate microwave-excited plasma processing apparatus for use in the second embodiment of this invention.
- the apparatus of FIG. 8 has a structure in which a lower shower plate 22 is disposed in the plasma diffusion region of the microwave-excited plasma processing apparatus shown in FIG. 1 .
- Kr (or Xe) and Ar for plasma excitation and an O 2 gas are introduced from an upper shower plate 21 .
- a SiH 4 gas being a reactive gas for film formation is introduced from the lower shower plate 22 .
- a high-density plasma is excited in a space between the upper shower plate 21 and the lower shower plate 22 and the plasma diffuses onto the surface of a silicon wafer 4 through gaps of a lattice-shaped pipe (having many holes for ejecting the reactive gas) of the lower shower plate 22 , so that a SiO 2 film is formed on the surface of the workpiece 4 by the reactive gas supplied thereto.
- FIG. 8 Kr (or Xe) and Ar gases for plasma excitation are introduced from the upper shower plate 21 .
- a CxHy gas being a reactive gas is introduced from the lower shower plate 22 .
- RF bias
- An outline arrow indicated by symbol 17 denotes a microwave for plasma excitation and symbol 26 denotes a high-density plasma region.
- a plasma processing apparatus and a plasma processing method according to this invention are, of course, applicable to semiconductor manufacturing processes and are also applicable to the manufacture of electronic/electrical devices and the manufacture of various machine components.
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Abstract
A plasma processing apparatus in which consumption of expensive krypton and xenon gases is suppressed as much as possible while reducing damage on a workpiece during plasma processing. In plasma processing of a substrate using a rare gas, two or more kinds of different rare gases are employed, and an inexpensive argon gas is used as one rare gas and any one or both of krypton and xenon gases having a larger collision cross-sectional area against electron than that of the argon gas is used as the other gas. Consequently, consumption of expensive krypton and xenon gases is suppressed as much as possible and damage on a workpiece is reduced during plasma processing.
Description
- This application is a Divisional of U.S. application Ser. No. 11/992,540 (National Stage of PCT/JP2005/017600), filed Mar. 25, 2008, incorporated herein by reference in its entirety.
- 1. Technical Field
- This invention relates to a method of plasma-processing a substrate or workpiece of an electronic device, such as a semiconductor-element or semiconductor-chip mounting substrate, a wiring substrate, or a flat panel display substrate, a processing apparatus therefor, and a manufacturing method for manufacturing an electronic device by such plasma processing.
- 2. Background Art
- Conventionally, a plasma is generated using a single rare gas in plasma processing for oxidizing, nitriding, or oxynitriding the surface of a workpiece such as a silicon semiconductor, forming an oxide film, a nitride film, an oxynitride film, a polysilicon film, an organic EL film, or the like on the surface of a workpiece, or etching the surface of a workpiece by the use of a plasma. As the rare gas, use is made of a krypton (Kr) gas or a xenon (Xe) gas with a large electron-collision cross-sectional area and a low plasma electron temperature for reducing plasma damage on the workpiece (see, e.g. Patent Document 1).
-
Patent Document 1 discloses an apparatus using Kr as a plasma excitation gas for forming an oxide film and a nitride film. This apparatus has a structure in which a coaxial waveguide, a radial line slot antenna, and microwave introducing windows are provided at an upper portion of a vacuum container serving as a process chamber in the order named from the outer side, a shower plate is provided inside the vacuum container, and a stage with a heating mechanism for placing a workpiece thereon is disposed under the shower plate. In a plasma processing method, the inside of the vacuum container is evacuated, an Ar gas is introduced from the shower plate, then the Ar gas is switched to a Kr gas and the pressure is set to 133 Pa. Then, a silicon substrate (workpiece) having been subjected to dilute hydrofluoric acid cleaning is introduced into the process chamber and placed on the stage and then the workpiece is heated so as to be maintained at 400° C. A microwave is supplied to the radial slot antenna from the coaxial waveguide, for example, for 1 minute, thereby introducing the microwave into the process chamber through the dielectric plates (the microwave introducing windows and the shower plate). In this manner, by exposing the surface of the silicon substrate to a high-density Kr plasma generated in the process chamber, surface-terminating hydrogen is removed. Then, while maintaining the pressure in the process chamber at about 133 Pa, a Kr/O2 mixed gas at a predetermined partial pressure ratio is introduced from the shower plate, thereby forming a silicon oxide film having a nano-order thickness on the surface of the silicon substrate. Then, after once stopping the supply of the microwave, stopping the introduction of the O2 gas, and purging the inside of the process chamber with Kr, a K2/NH3 mixed gas is introduced from the shower plate and, while setting the pressure in the process chamber at about 133 Pa, the microwave is again supplied to generate a high-density plasma in the process chamber, thereby forming a silicon nitride film having a nano-order thickness on the surface of the silicon oxide film. Further, the introduction of the microwave power is stopped to finish the plasma excitation when the formation of the silicon nitride film is finished, and then the Ar gas is substituted for the Kr/NH3 mixed gas, thereby finishing the oxidation-nitriding process. In this manner, a semiconductor integrated circuit device is manufactured using the above apparatus. - However, the existing amount of a Kr gas and a Xe gas in the natural world is small and thus they are expensive as compared with an Ar gas used in normal plasma processing, and therefore, it has been difficult to use them in the industry.
- Patent Document 1: Japanese Unexamined Patent Application Publication (JP-A) No. 2002-261091
- It is an object of this invention to suppress the consumption of expensive krypton and xenon gases as much as possible and to reduce damage on a workpiece during plasma processing.
- For accomplishing the above object, a plasma processing method and a plasma processing apparatus of this invention are characterized in that the electron temperature in a plasma is defined by a rare gas having a large electron-collision cross-sectional area while dilution of the gas is performed with a less expensive rare gas, thereby forming a gas in the plasma by these two or more kinds of rare gases.
- That is, according to this invention, there is provided a plasma-processing method which comprises genarating a plasma by the use of a rare gas; and processing a workpies by the use of said plasma. In the method, the rare gas includes two or more kinds of different rare gases.
- According to this invention, there is provided the above-mentioned plasma processing method, in which the different rare gases have electron-collision cross-sectional areas different from each other.
- According to this invention, there is provided any one of the above-mentioned plasma processing methods, in which one of said two or more kinds of different rare gases is an argon gas while other gas is a gas having an electron-collision cross-sectional area larger than that of said argon gas.
- According to this invention, there is provided any one of the above-mentioned plasma processing methods, in which one of said two or more kinds of different rare gases is an argon gas while other gas is at lease one of krypton and xenon.
- According to this invention, there is provided any one of the above-mentioned plasma processing methods, in which the plasma is generated by microwave excitation.
- According to this invention, there is provided any one of the above-mentioned plasma processing methods, in which the processing includes one of: oxidizing, nitriding, or oxynitriding of at least a portion of a surface of the workpiece; film forming on at least a portion of a surface of the workpiece; and etching of at least a portion of a surface of the workpiece.
- According to this invention, there is provided any one of the above-mentioned plasma processing methods, in which the oxidizing, nitriding, or oxynitrizing at least a portion of a surface of the workpiece by the use of the plasma includes introducing a nitriding gas or an oxidizing gas into the plasma.
- According to this invention, there is provided any one of the above-mentioned plasma processing methods, in which the film forming on at least a portion of a surface of the workpiece includes introducing a gas necessary to film forming into the plasma.
- According to this invention, there is provided any one of the above-mentioned plasma processing methods, in which the film forming includes forming an insulating film.
- According to this invention, there is provided any one of the above-mentioned plasma processing methods, which includes introducing a gas necessary for etching into the plasma and etching a selected portion or the whole of a surface of the workpiece.
- According to this invention, there is provided any one of the above-mentioned plasma processing methods, in which the gas having the larger electron-collision cross-sectional area, of the two or more kinds of different rare gases, is introduced into a plasma excitation region. The gas having the smaller electron-collision cross-sectional area is introduced to the outside of the plasma excitation region.
- According to this invention, there is provided any one of the above-mentioned plasma processing methods, which further comprises recovering a part or the whole of the rare gas for reuse is recovered.
- Further, according to this invention, there is provided a method of manufacturing an electronic device such as a semiconductor device, a flat panel display device, a computer, or a portable telephone terminal, the method comprising a step of processing a workpiece by any one of the above-mentioned plasma processing methods.
- According to this invention, there is provided a plasma processing apparatus in which two or more kinds of different rare gases are supplied into a plasma process chamber.
- According to this invention, there is provided the above-mentioned plasma processing apparatus in which the rare gases have electron-collision cross-sectional areas different from each other.
- According to this invention, there is provided any one of the above-mentioned plasma processing apparatuses, in which one of the rare gases is an argon gas and other gas is a gas having an electron-collision cross-sectional area larger than that of the argon gas.
- According to this invention, there is provided any one of the above-mentioned plasma processing apparatuses, in which one of the rare gases is an argon gas and other gas is one or both of krypton and xenon.
- According to this invention, there is provided any one of the above-mentioned plasma processing apparatuses, in which the plasma is generated by microwave excitation.
- According to this invention, there is provided any one of the above-mentioned plasma processing apparatuses, in which the plasma chamber is supplied with a nitriding gas or an oxidizing gas in addition to the rare gases.
- According to this invention, there is provided any one of the above-mentioned plasma processing apparatuses, in which the plasma chamber is supplied with a desired gas in addition to the rare gases to perform film formation on a workpiece.
- According to this invention, there is provided any one of the above-mentioned plasma processing apparatuses, in which the plasma chamber is supplied with etching at least a portion of a workpiece, in addition to the rare gases.
- According to this invention, there is provided any one of the above-mentioned plasma processing apparatuses, which introduces the rare gas having the larger electron-collision cross-sectional area into a plasma excitation region; and also introduces the argon gas to the outside of the plasma excitation region.
- According to this invention, there is provided any one of the above-mentioned plasma processing apparatuses, which further comprises a rare gas recovery apparatus.
- Further, in this invention, there is provided a plasma processing method that recovers, regenerates, and uses the used rare gases, thereby making it possible to more efficiently use the expensive rare gases.
- According to this invention, use is made of a gas in which an Ar gas is added to one or both of Xe and Kr, wherein the required ratio of Xe or/and Kr in the mixed gas changes depending on various conditions. In many cases, at least 20 vol % is required. When the ratio is about 40% or more, substantially no difference in effect is observed as compared with the case of 100%, and there is no problem when the ratio is 50% or more. Naturally, the ratio is less than 100%.
- According to this invention, since plasma generation is carried out using a gas in which an Ar gas is added to one or both of Kr and Xe, it is possible to reduce damage during plasma processing and to achieve a reduction in amount of use of expensive Kr and Xe gases.
-
FIG. 1 is a sectional view of a microwave-excited plasma processing apparatus for use in anembodiment 1 of this invention. -
FIG. 2 includes an explanatory diagram showing electron temperatures and collision cross-sectional areas of respective rare gases and a diagram showing excitation energies, ionization energies, and electron temperatures of Ar, Kr, and Xe gases. -
FIG. 3 is a sectional view showing a plasma measuring method. -
FIG. 4 shows luminous intensities of Ar/Xe mixed plasmas, wherein (a) shows relative intensities in the case of Xe+ (466.8 nm) at 20 mTorr (2.66 Pa), (b) shows relative intensities in the case of Xe+ (466.8 nm) at 40 mTorr (5.33 Pa), (c) shows relative intensities in the case of Ar (750.4 nm) at 20 mTorr (2.66 Pa), and (d) shows relative intensities in the case of Ar (750.4 nm) at 40 mTorr (5.33 Pa). -
FIG. 5 shows plasma electron densities, wherein (a) shows the relationship between the operating pressure (mTorr=x 0.133 Pa) and the number of electrons (1012 cm−3) of Ar and (b) shows the relationship between the operating pressure (mTorr=x 0.133 Pa) and the number of electrons (1012 cm−3) of Xe. -
FIG. 6 includes diagrams (a), (b), (c), and (d) showing electron densities, VSWRs, ion currents, and electron temperatures of Ar/Xe mixed plasmas, respectively. -
FIG. 7 includes a diagram (a) showing ion current densities when the pressure of a mixed gas is changed, and a diagram (b) showing electron temperatures when the pressure of a mixed gas is changed. -
FIG. 8 is a sectional view of a dual shower plate microwave-excited plasma processing apparatus for use in 2 and 3 of this invention.embodiments -
-
- 1 antenna for microwave irradiation
- 2 insulator
- 3 shower plate
- 4 wafer
- 5 exhaust port
- 6 exhaust duct
- 7 a, 7 b small pump inlet pipe (exhaust pipe)
- 10 chamber
- 13 gas introducing pipe
- 15 attaching member
- 19 gas flow
- 21 upper shower plate
- 22 lower shower plate
- 25 RF bias power supply
- 101 microwave-excited plasma processing apparatus
- 102 dual shower plate microwave-excited plasma processing apparatus
- Hereinbelow, embodiments of this invention will be described with reference to the drawings.
- In the first embodiment of this invention, a description will be given of a mode in which plasma processing is a silicon direct oxidation/nitriding process.
-
FIG. 1 is a sectional view of a microwave-excited plasma processing apparatus. -
FIG. 2 is a diagram showing the relationship between the electron energy and the total ionization cross-sectional area.FIG. 3 is a sectional view showing a plasma measuring method.FIG. 4 are diagrams showing luminous intensities of Ar/Xe mixed plasmas, wherein (a) shows relative intensities in the case of Xe+ (466.8 nm) at 2.66 Pa (20 mTorr), (b) shows relative intensities in the case of Xe+ (466.8 nm) at 5.33 Pa (40 mTorr), (c) shows relative intensities in the case of Ar (750.4 nm) at 2.66 Pa (20 mTorr), and (d) shows relative intensities in the case of Ar (750.4 nm) at 5.33 Pa (40 mTorr).FIG. 5 are diagrams showing plasma electron densities, wherein (a) shows the relationship between the operating pressure (mTorr=x 0.133 Pa) and the number of electrons (1012 cm−3) of Ar and (b) shows the relationship between the operating pressure (mTorr=x 0.133 Pa) and the number of electrons (1012 cm−3) of Xe.FIG. 6( a), (b), (c), and (d) are diagrams showing electron densities, VSWRs, ion currents, and electron temperatures of Ar/Xe mixed plasmas, respectively.FIG. 7( a) is a diagram showing ion current densities when the ratio of Xe in an Ar/Xe mixed gas is changed from 0 to 1, andFIG. 7( b) is a diagram showing electron temperatures when the ratio of Xe in an Ar/Xe mixed gas (pressure) is changed in the same manner. - Referring to
FIG. 1 , a microwave is radiated into anapparatus 11 by anantenna 1 disposed at an upper portion of aplasma processing apparatus 101 through aninsulator plate 2. An Ar gas, a Kr gas (or a Xe gas), and an oxygen gas (a N2/H2 or NH3 gas in the case of a nitriding process or a mixed gas of an oxidizing gas and a nitriding gas, such as an O2/NH3, O2/N2O, or O2/NO gas, in the case of an oxynitriding process) are introduced into the apparatus inside 11 from agas introducing pipe 13 through ashower plate 3, so that a plasma is excited above a workpiece 4 in the apparatus inside 11 by the microwave irradiated there as described above. - Referring back to
FIG. 1 , the silicon wafer 4 being a workpiece substrate is placed in theprocess chamber 11 at a place where the plasma is directly irradiated, and is oxidized by oxygen radicals etc. excited by the plasma. In this event, it is preferable that the workpiece 4 be placed in theprocess chamber 11 not in a space where the plasma is excited, but in a space where the plasma is diffused. - An exhaust gas in the
process chamber 11 passes throughexhaust ducts 6 viaexhaust ports 5 so as to be conducted to non-illustrated small pumps through 7 a and 7 b for the respective small pumps as indicated by broken-inlet ports line arrows 19. - For measuring the excited plasma, a
probe 9 is provided so that its tip end is projected into theprocess chamber 11 as shown inFIG. 3 . Theprobe 9 is fixed by an attachingmember 15. Luminous measurement is carried out through a different window as indicated by anarrow 14. - Herein, as shown in
FIG. 2 , since the electron-collision cross-sectional area and the ionization energy of a Kr or Xe gas are both small where the electron temperature is low as compared with Ar, when a microwave is irradiated to a mixed gas of Ar and Kr (or Xe), Kr (or Xe) is selectively ionized to form a plasma so that the electron temperature of the plasma is defined by Kr (or Xe). Therefore, it is possible to suppress damage to a SiO2 film (Si3N4 film, SiON film) during formation thereof or having been formed and to suppress the use of the expensive Kr (or Xe) gas. - Further, referring to
FIG. 4( a), (b) and (c), (d), it is seen that the luminous intensity (relative intensity) of Xe+ is greater at 40 mTorr (5.33 Pa) than at 20 mTorr (2.66 Pa), while, the luminous intensity of Ar does not depend on the pressure when the partial pressure (molar fraction) of Xe is 0.2 or more. - Further, referring to
FIG. 5 , it is seen that the electron density of Ar increases as the flow rate ratio (i.e. partial pressure) of Xe increases, while, the electron density of Xe decreases as the flow rate ratio increases. - Further, referring to
FIG. 6 , the electron density increases from a Xe composition ratio of 20% and, thereafter, monotonously increases as the composition ratio increases, and VSWR monotonously slightly decreases as the Xe composition ratio increases. It is seen that the ion current abruptly increases at a Xe composition ratio of 20% and the electron temperature abruptly decreases until a Xe composition ratio of 20% and, thereafter, monotonously decreases as the composition ratio increases. - Further, referring to
FIG. 7( a), it is seen that when a pressure of a mixed gas, which corresponds to the total flow rate, is 20 mTorr (2.66 Pa), the ion current density abruptly increases near a Xe flow rate ratio of 0.75. Further, it is seen that when the total flow rate is 40 mTorr (5.33 Pa), the ion current density abruptly increases when the Xe flow rate ratio exceeds 0.2. Further, it is seen that when the total flow rate is 100 mTorr (13.33 Pa), the ion current density tends to almost monotonously increase. - Further, referring to
FIG. 7( b), it is seen that as the Xe flow rate ratio increases, the electron temperature becomes smaller in the order of pressures of the mixed gases, which correspond to the total flow rates, of 20 mTorr (2.66 Pa), 40 mTorr (5.33 Pa), and 100 mTorr (13.33 Pa) and, as the Xe flow rate ratio increases from 0.2, the electron temperature for each flow rate monotonously decreases. - All the above data show that substantially the same results as those in the case of 100% are obtained when the Xe composition ratio is 20% or more, preferably 50% or more, even if it is not 100%. That is, it is seen that damage during the plasma processing can be reduced even by using inexpensive Ar at about 80%, preferably about 50%. As a result, according to this invention, it is possible to achieve a reduction in amount of use of expensive Kr and Xe gases.
- Next, there is shown an example in which plasma processing according to this invention is applied to film formation. In the second embodiment, formation of a SiO2 film by a CVD (Chemical Vapor Deposition) process is carried out as the film formation.
-
FIG. 8 is a schematic sectional view of a dual shower plate microwave-excited plasma processing apparatus for use in the second embodiment of this invention. The apparatus ofFIG. 8 has a structure in which alower shower plate 22 is disposed in the plasma diffusion region of the microwave-excited plasma processing apparatus shown inFIG. 1 . Kr (or Xe) and Ar for plasma excitation and an O2 gas are introduced from anupper shower plate 21. A SiH4 gas being a reactive gas for film formation is introduced from thelower shower plate 22. A high-density plasma is excited in a space between theupper shower plate 21 and thelower shower plate 22 and the plasma diffuses onto the surface of a silicon wafer 4 through gaps of a lattice-shaped pipe (having many holes for ejecting the reactive gas) of thelower shower plate 22, so that a SiO2 film is formed on the surface of the workpiece 4 by the reactive gas supplied thereto. - In this event, if a Kr (or Xe), Ar, and NH3 (or N2/H2) mixed gas is supplied from the
upper shower plate 21 and a SiH4 gas is supplied from thelower shower plate 22, a Si3N4 film can be formed. - On the other hand, if Kr (or Xe) and Ar are supplied from the
upper shower plate 21 and a CxFy (C5F8, C4F8, or the like) gas is supplied from thelower shower plate 22, a fluorocarbon film can be formed. - On the other hand, if Kr (or Xe) and Ar are supplied from the
upper shower plate 21 and a SiH4 gas is supplied from thelower shower plate 22, a silicon film can be formed. - In any of the above cases, as is clear from
FIGS. 2 , 6, and 7, since the electron-collision cross-sectional area and the ionization energy of a Kr or Xe gas are both small where the electron temperature is low as compared with Ar, when a microwave is irradiated to a mixed gas of Ar and Kr (or Xe), Kr (Xe) is selectively ionized to form a plasma so that the electron temperature of the plasma is defined by Kr (Xe). Therefore, it is possible to suppress damage to various films during formation thereof or having been formed and to suppress the use of the expensive Kr (Xe) gas. - Next, there is shown an example in which plasma processing of this invention is applied to an etching process. Referring to
FIG. 8 , Kr (or Xe) and Ar gases for plasma excitation are introduced from theupper shower plate 21. A CxHy gas being a reactive gas is introduced from thelower shower plate 22. Herein, by applying a bias (RF) 25 to a substrate 4, a negative DC bias is applied to the side of the silicon wafer 4 so that SiO2 present on the silicon substrate 4 is etched. An outline arrow indicated bysymbol 17 denotes a microwave for plasma excitation andsymbol 26 denotes a high-density plasma region. - Also in this event, as is clear from
FIGS. 2 , 6, and 7, since the electron-collision cross-sectional area and the ionization energy of a Kr or Xe gas are both small where the electron temperature is low as compared with Ar, when a microwave is irradiated to a mixed gas of Ar and Kr (or Xe), Kr (Xe) is selectively ionized to form a plasma so that the electron temperature of the plasma is defined by Kr (Xe). Therefore, it is possible to suppress damage to the surface of the silicon substrate 4 or a film formed on the silicon substrate during etching and to suppress the use of the expensive Kr (Xe) gas. - As described above, a plasma processing apparatus and a plasma processing method according to this invention are, of course, applicable to semiconductor manufacturing processes and are also applicable to the manufacture of electronic/electrical devices and the manufacture of various machine components.
Claims (6)
1. A plasma processing apparatus comprising:
an upper shower plate which introduces a mixed rare gas including an argon gas and either one of xenon gas and krypton gas to generate plasma within a plasma process chamber; and
a lower shower member which is placed in a space between the upper shower plate and a workpiece to be treated; and
wherein the lower shower member has a plurality of holes for ejecting the reactive gas; and
wherein the mixed gas is controlled so that an amount of the argon gas becomes less than 80%.
2. The apparatus according to claim 1 , further comprising microwave excitation means for generating a plasma in said plasma process chamber.
3. The apparatus according to claim 1 , further comprising means for supplying a nitriding gas or an oxidizing gas into said plasma process chamber.
4. The apparatus according to claim 1 , further comprising means for supplying a gas, for use in performing film formation on the workpiece, into said plasma process chamber.
5. The apparatus according to claim 1 , further comprising means for supplying a gas, for use in etching at least a portion of the workpiece, into said plasma process chamber.
6. The apparatus according to claim 1 , wherein said lower shower member is structured by a lattice-shaped pipe with gaps left among the lattice-shaped pipe.
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| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US13/469,851 US20120234491A1 (en) | 2005-09-26 | 2012-05-11 | Plasma processing method and plasma processing apparatus |
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| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| PCT/JP2005/017600 WO2007034559A1 (en) | 2005-09-26 | 2005-09-26 | Plasma processing method and plasma processing apparatus |
| US99254008A | 2008-03-25 | 2008-03-25 | |
| US13/469,851 US20120234491A1 (en) | 2005-09-26 | 2012-05-11 | Plasma processing method and plasma processing apparatus |
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| Application Number | Title | Priority Date | Filing Date |
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| PCT/JP2005/017600 Division WO2007034559A1 (en) | 2005-09-26 | 2005-09-26 | Plasma processing method and plasma processing apparatus |
| US99254008A Division | 2005-09-26 | 2008-03-25 |
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| WO2008008098A2 (en) * | 2006-07-07 | 2008-01-17 | Silica Tech, Llc | Plasma deposition apparatus and method for making polycrystalline silicon |
| JP6587514B2 (en) * | 2015-11-11 | 2019-10-09 | 東京エレクトロン株式会社 | Plasma processing method and plasma processing apparatus |
| US20230023456A1 (en) | 2020-01-07 | 2023-01-26 | Cochlear Limited | Recovery of deeply discharged implantable battery |
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| US20060016781A1 (en) * | 2004-07-26 | 2006-01-26 | Kenichi Kuwabara | Dry etching method |
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| JPH1074600A (en) * | 1996-05-02 | 1998-03-17 | Tokyo Electron Ltd | Plasma processing equipment |
| US6357385B1 (en) | 1997-01-29 | 2002-03-19 | Tadahiro Ohmi | Plasma device |
| US6090722A (en) | 1999-01-06 | 2000-07-18 | International Business Machines Corporation | Process for fabricating a semiconductor structure having a self-aligned spacer |
| KR100319894B1 (en) | 1999-07-13 | 2002-01-10 | 윤종용 | Etching method of material fim formed on semiconductor wafer using surface wave coupled plasma etching apparatus |
| JP4713752B2 (en) | 2000-12-28 | 2011-06-29 | 財団法人国際科学振興財団 | Semiconductor device and manufacturing method thereof |
| JP2003073835A (en) | 2001-08-28 | 2003-03-12 | Tdk Corp | Plasma cvd apparatus and method for forming plasma cvd film |
| JP2003282565A (en) | 2002-01-18 | 2003-10-03 | Arieesu Gijutsu Kenkyu Kk | Film deposition method, film deposition apparatus, and semiconductor device |
| JP2004047580A (en) | 2002-07-09 | 2004-02-12 | Arieesu Gijutsu Kenkyu Kk | Film-forming equipment |
| SG124265A1 (en) * | 2002-12-02 | 2006-08-30 | Tadahiro Ohmi | Semiconductor device and method of manufacturing the same |
| US6942816B2 (en) | 2003-02-12 | 2005-09-13 | Lam Research Corporation | Methods of reducing photoresist distortion while etching in a plasma processing system |
| JP2005123389A (en) | 2003-10-16 | 2005-05-12 | Advanced Lcd Technologies Development Center Co Ltd | Plasma treatment method, plasma film forming method, plasma etching method and plasma treatment device |
| JP2006135161A (en) * | 2004-11-08 | 2006-05-25 | Canon Inc | Method and apparatus for forming insulating film |
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| US20060016781A1 (en) * | 2004-07-26 | 2006-01-26 | Kenichi Kuwabara | Dry etching method |
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| KR20080048514A (en) | 2008-06-02 |
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| WO2007034559A1 (en) | 2007-03-29 |
| KR101192613B1 (en) | 2012-10-18 |
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