TW202223125A - Film-forming device - Google Patents
Film-forming device Download PDFInfo
- Publication number
- TW202223125A TW202223125A TW111107128A TW111107128A TW202223125A TW 202223125 A TW202223125 A TW 202223125A TW 111107128 A TW111107128 A TW 111107128A TW 111107128 A TW111107128 A TW 111107128A TW 202223125 A TW202223125 A TW 202223125A
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- Taiwan
- Prior art keywords
- film
- substrate
- piezoelectric
- conductive
- piezoelectric film
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- 239000000758 substrate Substances 0.000 claims abstract description 454
- 229910052451 lead zirconate titanate Inorganic materials 0.000 claims description 127
- BASFCYQUMIYNBI-UHFFFAOYSA-N platinum Chemical compound [Pt] BASFCYQUMIYNBI-UHFFFAOYSA-N 0.000 claims description 92
- 239000012528 membrane Substances 0.000 claims description 72
- HFGPZNIAWCZYJU-UHFFFAOYSA-N lead zirconate titanate Chemical compound [O-2].[O-2].[O-2].[O-2].[O-2].[Ti+4].[Zr+4].[Pb+2] HFGPZNIAWCZYJU-UHFFFAOYSA-N 0.000 claims description 70
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 claims description 51
- 229910052710 silicon Inorganic materials 0.000 claims description 51
- 239000010703 silicon Substances 0.000 claims description 51
- MCMNRKCIXSYSNV-UHFFFAOYSA-N Zirconium dioxide Chemical compound O=[Zr]=O MCMNRKCIXSYSNV-UHFFFAOYSA-N 0.000 claims description 46
- 229910052697 platinum Inorganic materials 0.000 claims description 29
- 239000000126 substance Substances 0.000 claims description 29
- 239000002131 composite material Substances 0.000 claims description 22
- 229910052751 metal Inorganic materials 0.000 claims description 11
- 239000002184 metal Substances 0.000 claims description 11
- 238000007667 floating Methods 0.000 abstract description 23
- 230000002093 peripheral effect Effects 0.000 abstract description 19
- 239000010408 film Substances 0.000 description 978
- 239000013078 crystal Substances 0.000 description 162
- 230000010287 polarization Effects 0.000 description 63
- 238000000034 method Methods 0.000 description 59
- RKTYLMNFRDHKIL-UHFFFAOYSA-N copper;5,10,15,20-tetraphenylporphyrin-22,24-diide Chemical compound [Cu+2].C1=CC(C(=C2C=CC([N-]2)=C(C=2C=CC=CC=2)C=2C=CC(N=2)=C(C=2C=CC=CC=2)C2=CC=C3[N-]2)C=2C=CC=CC=2)=NC1=C3C1=CC=CC=C1 RKTYLMNFRDHKIL-UHFFFAOYSA-N 0.000 description 49
- 230000000052 comparative effect Effects 0.000 description 35
- 238000004544 sputter deposition Methods 0.000 description 35
- 238000010586 diagram Methods 0.000 description 32
- 239000007789 gas Substances 0.000 description 31
- 239000010410 layer Substances 0.000 description 31
- 239000010936 titanium Substances 0.000 description 31
- 230000015572 biosynthetic process Effects 0.000 description 29
- 238000004519 manufacturing process Methods 0.000 description 28
- 238000010438 heat treatment Methods 0.000 description 20
- 238000001228 spectrum Methods 0.000 description 18
- 235000012431 wafers Nutrition 0.000 description 16
- 238000001514 detection method Methods 0.000 description 15
- 230000005684 electric field Effects 0.000 description 14
- RTAQQCXQSZGOHL-UHFFFAOYSA-N Titanium Chemical compound [Ti] RTAQQCXQSZGOHL-UHFFFAOYSA-N 0.000 description 12
- 238000002441 X-ray diffraction Methods 0.000 description 12
- 239000000463 material Substances 0.000 description 10
- 230000035945 sensitivity Effects 0.000 description 10
- 238000012986 modification Methods 0.000 description 9
- 230000004048 modification Effects 0.000 description 9
- 239000000243 solution Substances 0.000 description 9
- 230000002269 spontaneous effect Effects 0.000 description 9
- 230000007423 decrease Effects 0.000 description 8
- 239000000203 mixture Substances 0.000 description 8
- VEALVRVVWBQVSL-UHFFFAOYSA-N strontium titanate Chemical compound [Sr+2].[O-][Ti]([O-])=O VEALVRVVWBQVSL-UHFFFAOYSA-N 0.000 description 8
- 238000000576 coating method Methods 0.000 description 7
- 230000000694 effects Effects 0.000 description 7
- 239000002243 precursor Substances 0.000 description 7
- 239000002994 raw material Substances 0.000 description 7
- 239000003990 capacitor Substances 0.000 description 6
- 238000009826 distribution Methods 0.000 description 6
- 229910052719 titanium Inorganic materials 0.000 description 6
- 229910019606 La0.5Sr0.5CoO3 Inorganic materials 0.000 description 5
- PNEYBMLMFCGWSK-UHFFFAOYSA-N aluminium oxide Inorganic materials [O-2].[O-2].[O-2].[Al+3].[Al+3] PNEYBMLMFCGWSK-UHFFFAOYSA-N 0.000 description 5
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 description 5
- 230000008859 change Effects 0.000 description 5
- 239000001301 oxygen Substances 0.000 description 5
- 229910052760 oxygen Inorganic materials 0.000 description 5
- 238000003980 solgel method Methods 0.000 description 5
- 229910001220 stainless steel Inorganic materials 0.000 description 5
- 239000010935 stainless steel Substances 0.000 description 5
- XKRFYHLGVUSROY-UHFFFAOYSA-N Argon Chemical compound [Ar] XKRFYHLGVUSROY-UHFFFAOYSA-N 0.000 description 4
- 238000001704 evaporation Methods 0.000 description 4
- RVTZCBVAJQQJTK-UHFFFAOYSA-N oxygen(2-);zirconium(4+) Chemical compound [O-2].[O-2].[Zr+4] RVTZCBVAJQQJTK-UHFFFAOYSA-N 0.000 description 4
- 238000012545 processing Methods 0.000 description 4
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N silicon dioxide Inorganic materials O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 4
- 239000010409 thin film Substances 0.000 description 4
- 229910001928 zirconium oxide Inorganic materials 0.000 description 4
- 229910003781 PbTiO3 Inorganic materials 0.000 description 3
- 238000001816 cooling Methods 0.000 description 3
- 238000013461 design Methods 0.000 description 3
- 238000005516 engineering process Methods 0.000 description 3
- 230000008020 evaporation Effects 0.000 description 3
- 238000009413 insulation Methods 0.000 description 3
- 238000001755 magnetron sputter deposition Methods 0.000 description 3
- 238000005259 measurement Methods 0.000 description 3
- 238000000206 photolithography Methods 0.000 description 3
- 239000010453 quartz Substances 0.000 description 3
- 238000001552 radio frequency sputter deposition Methods 0.000 description 3
- 238000007789 sealing Methods 0.000 description 3
- 239000002356 single layer Substances 0.000 description 3
- 229910052712 strontium Inorganic materials 0.000 description 3
- CIOAGBVUUVVLOB-UHFFFAOYSA-N strontium atom Chemical compound [Sr] CIOAGBVUUVVLOB-UHFFFAOYSA-N 0.000 description 3
- 229910052726 zirconium Inorganic materials 0.000 description 3
- LFQSCWFLJHTTHZ-UHFFFAOYSA-N Ethanol Chemical compound CCO LFQSCWFLJHTTHZ-UHFFFAOYSA-N 0.000 description 2
- KJTLSVCANCCWHF-UHFFFAOYSA-N Ruthenium Chemical compound [Ru] KJTLSVCANCCWHF-UHFFFAOYSA-N 0.000 description 2
- 229910004121 SrRuO Inorganic materials 0.000 description 2
- QCWXUUIWCKQGHC-UHFFFAOYSA-N Zirconium Chemical compound [Zr] QCWXUUIWCKQGHC-UHFFFAOYSA-N 0.000 description 2
- 238000007792 addition Methods 0.000 description 2
- 229910052786 argon Inorganic materials 0.000 description 2
- 125000004429 atom Chemical group 0.000 description 2
- 238000012937 correction Methods 0.000 description 2
- 238000010292 electrical insulation Methods 0.000 description 2
- 238000005566 electron beam evaporation Methods 0.000 description 2
- 238000010894 electron beam technology Methods 0.000 description 2
- 230000010354 integration Effects 0.000 description 2
- 239000000395 magnesium oxide Substances 0.000 description 2
- CPLXHLVBOLITMK-UHFFFAOYSA-N magnesium oxide Inorganic materials [Mg]=O CPLXHLVBOLITMK-UHFFFAOYSA-N 0.000 description 2
- 230000010355 oscillation Effects 0.000 description 2
- 239000002245 particle Substances 0.000 description 2
- 229920002530 polyetherether ketone Polymers 0.000 description 2
- 239000011347 resin Substances 0.000 description 2
- 229920005989 resin Polymers 0.000 description 2
- 230000004044 response Effects 0.000 description 2
- 229910052707 ruthenium Inorganic materials 0.000 description 2
- 230000001568 sexual effect Effects 0.000 description 2
- 239000002904 solvent Substances 0.000 description 2
- 238000007740 vapor deposition Methods 0.000 description 2
- -1 2-n-butoxy alcohol Chemical compound 0.000 description 1
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 description 1
- 229910004298 SiO 2 Inorganic materials 0.000 description 1
- 229910002367 SrTiO Inorganic materials 0.000 description 1
- QAKZFDCCFWBSGH-UHFFFAOYSA-N [Ru].[Sr] Chemical compound [Ru].[Sr] QAKZFDCCFWBSGH-UHFFFAOYSA-N 0.000 description 1
- 230000002159 abnormal effect Effects 0.000 description 1
- 238000009825 accumulation Methods 0.000 description 1
- 239000002253 acid Substances 0.000 description 1
- 239000000919 ceramic Substances 0.000 description 1
- 238000012512 characterization method Methods 0.000 description 1
- 239000011248 coating agent Substances 0.000 description 1
- 230000006835 compression Effects 0.000 description 1
- 238000007906 compression Methods 0.000 description 1
- 239000000470 constituent Substances 0.000 description 1
- 238000011109 contamination Methods 0.000 description 1
- 239000000498 cooling water Substances 0.000 description 1
- 230000003247 decreasing effect Effects 0.000 description 1
- 238000012217 deletion Methods 0.000 description 1
- 230000037430 deletion Effects 0.000 description 1
- 238000000407 epitaxy Methods 0.000 description 1
- 238000011156 evaluation Methods 0.000 description 1
- 230000005621 ferroelectricity Effects 0.000 description 1
- 230000004907 flux Effects 0.000 description 1
- 238000007716 flux method Methods 0.000 description 1
- 239000005350 fused silica glass Substances 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 230000005484 gravity Effects 0.000 description 1
- 230000012447 hatching Effects 0.000 description 1
- 238000002347 injection Methods 0.000 description 1
- 239000007924 injection Substances 0.000 description 1
- 239000012212 insulator Substances 0.000 description 1
- 238000010884 ion-beam technique Methods 0.000 description 1
- 229910052741 iridium Inorganic materials 0.000 description 1
- GKOZUEZYRPOHIO-UHFFFAOYSA-N iridium atom Chemical compound [Ir] GKOZUEZYRPOHIO-UHFFFAOYSA-N 0.000 description 1
- 229910052745 lead Inorganic materials 0.000 description 1
- AXZKOIWUVFPNLO-UHFFFAOYSA-N magnesium;oxygen(2-) Chemical compound [O-2].[Mg+2] AXZKOIWUVFPNLO-UHFFFAOYSA-N 0.000 description 1
- 239000011553 magnetic fluid Substances 0.000 description 1
- 238000012423 maintenance Methods 0.000 description 1
- 239000012046 mixed solvent Substances 0.000 description 1
- 150000002902 organometallic compounds Chemical class 0.000 description 1
- 230000003647 oxidation Effects 0.000 description 1
- 238000007254 oxidation reaction Methods 0.000 description 1
- 125000004430 oxygen atom Chemical group O* 0.000 description 1
- 229910021420 polycrystalline silicon Inorganic materials 0.000 description 1
- 229920005591 polysilicon Polymers 0.000 description 1
- 239000000843 powder Substances 0.000 description 1
- 230000002265 prevention Effects 0.000 description 1
- 230000002035 prolonged effect Effects 0.000 description 1
- 230000005855 radiation Effects 0.000 description 1
- 229910052594 sapphire Inorganic materials 0.000 description 1
- 239000010980 sapphire Substances 0.000 description 1
- VSZWPYCFIRKVQL-UHFFFAOYSA-N selanylidenegallium;selenium Chemical compound [Se].[Se]=[Ga].[Se]=[Ga] VSZWPYCFIRKVQL-UHFFFAOYSA-N 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
- 238000005477 sputtering target Methods 0.000 description 1
- 239000013077 target material Substances 0.000 description 1
- LLZRNZOLAXHGLL-UHFFFAOYSA-J titanic acid Chemical compound O[Ti](O)(O)O LLZRNZOLAXHGLL-UHFFFAOYSA-J 0.000 description 1
- PMTRSEDNJGMXLN-UHFFFAOYSA-N titanium zirconium Chemical compound [Ti].[Zr] PMTRSEDNJGMXLN-UHFFFAOYSA-N 0.000 description 1
- 239000011800 void material Substances 0.000 description 1
Images
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N—ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N30/00—Piezoelectric or electrostrictive devices
- H10N30/80—Constructional details
- H10N30/85—Piezoelectric or electrostrictive active materials
- H10N30/853—Ceramic compositions
- H10N30/8548—Lead-based oxides
- H10N30/8554—Lead-zirconium titanate [PZT] based
-
- 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
- C23C14/00—Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
- C23C14/06—Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material characterised by the coating material
- C23C14/08—Oxides
- C23C14/088—Oxides of the type ABO3 with A representing alkali, alkaline earth metal or Pb and B representing a refractory or rare earth metal
-
- 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
- C23C14/00—Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
- C23C14/22—Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material characterised by the process of coating
- C23C14/34—Sputtering
- C23C14/3407—Cathode assembly for sputtering apparatus, e.g. Target
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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
- C23C14/00—Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
- C23C14/22—Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material characterised by the process of coating
- C23C14/34—Sputtering
- C23C14/3435—Applying energy to the substrate during sputtering
-
- 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
- C23C14/00—Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
- C23C14/22—Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material characterised by the process of coating
- C23C14/34—Sputtering
- C23C14/35—Sputtering by application of a magnetic field, e.g. magnetron sputtering
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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
- C23C14/00—Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
- C23C14/22—Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material characterised by the process of coating
- C23C14/50—Substrate holders
- C23C14/505—Substrate holders for rotation of the substrates
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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
- C23C14/00—Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
- C23C14/22—Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material characterised by the process of coating
- C23C14/56—Apparatus specially adapted for continuous coating; Arrangements for maintaining the vacuum, e.g. vacuum locks
- C23C14/564—Means for minimising impurities in the coating chamber such as dust, moisture, residual gases
-
- C—CHEMISTRY; METALLURGY
- C30—CRYSTAL GROWTH
- C30B—SINGLE-CRYSTAL GROWTH; UNIDIRECTIONAL SOLIDIFICATION OF EUTECTIC MATERIAL OR UNIDIRECTIONAL DEMIXING OF EUTECTOID MATERIAL; REFINING BY ZONE-MELTING OF MATERIAL; PRODUCTION OF A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; SINGLE CRYSTALS OR HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; AFTER-TREATMENT OF SINGLE CRYSTALS OR A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; APPARATUS THEREFOR
- C30B23/00—Single-crystal growth by condensing evaporated or sublimed materials
- C30B23/02—Epitaxial-layer growth
- C30B23/025—Epitaxial-layer growth characterised by the substrate
-
- C—CHEMISTRY; METALLURGY
- C30—CRYSTAL GROWTH
- C30B—SINGLE-CRYSTAL GROWTH; UNIDIRECTIONAL SOLIDIFICATION OF EUTECTIC MATERIAL OR UNIDIRECTIONAL DEMIXING OF EUTECTOID MATERIAL; REFINING BY ZONE-MELTING OF MATERIAL; PRODUCTION OF A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; SINGLE CRYSTALS OR HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; AFTER-TREATMENT OF SINGLE CRYSTALS OR A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; APPARATUS THEREFOR
- C30B23/00—Single-crystal growth by condensing evaporated or sublimed materials
- C30B23/02—Epitaxial-layer growth
- C30B23/06—Heating of the deposition chamber, the substrate or the materials to be evaporated
- C30B23/063—Heating of the substrate
-
- C—CHEMISTRY; METALLURGY
- C30—CRYSTAL GROWTH
- C30B—SINGLE-CRYSTAL GROWTH; UNIDIRECTIONAL SOLIDIFICATION OF EUTECTIC MATERIAL OR UNIDIRECTIONAL DEMIXING OF EUTECTOID MATERIAL; REFINING BY ZONE-MELTING OF MATERIAL; PRODUCTION OF A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; SINGLE CRYSTALS OR HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; AFTER-TREATMENT OF SINGLE CRYSTALS OR A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; APPARATUS THEREFOR
- C30B29/00—Single crystals or homogeneous polycrystalline material with defined structure characterised by the material or by their shape
- C30B29/10—Inorganic compounds or compositions
- C30B29/16—Oxides
- C30B29/22—Complex oxides
- C30B29/32—Titanates; Germanates; Molybdates; Tungstates
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- 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
- H01J37/32715—Workpiece holder
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- 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
- H01J37/32715—Workpiece holder
- H01J37/32724—Temperature
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- 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
- H01J37/34—Gas-filled discharge tubes operating with cathodic sputtering
- H01J37/3402—Gas-filled discharge tubes operating with cathodic sputtering using supplementary magnetic fields
- H01J37/3405—Magnetron sputtering
- H01J37/3408—Planar magnetron sputtering
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N—ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N30/00—Piezoelectric or electrostrictive devices
- H10N30/01—Manufacture or treatment
- H10N30/07—Forming of piezoelectric or electrostrictive parts or bodies on an electrical element or another base
- H10N30/074—Forming of piezoelectric or electrostrictive parts or bodies on an electrical element or another base by depositing piezoelectric or electrostrictive layers, e.g. aerosol or screen printing
- H10N30/076—Forming of piezoelectric or electrostrictive parts or bodies on an electrical element or another base by depositing piezoelectric or electrostrictive layers, e.g. aerosol or screen printing by vapour phase deposition
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N—ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N30/00—Piezoelectric or electrostrictive devices
- H10N30/30—Piezoelectric or electrostrictive devices with mechanical input and electrical output, e.g. functioning as generators or sensors
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- Chemical & Material Sciences (AREA)
- Engineering & Computer Science (AREA)
- Materials Engineering (AREA)
- Organic Chemistry (AREA)
- Metallurgy (AREA)
- Mechanical Engineering (AREA)
- Chemical Kinetics & Catalysis (AREA)
- Analytical Chemistry (AREA)
- Crystallography & Structural Chemistry (AREA)
- Physics & Mathematics (AREA)
- Plasma & Fusion (AREA)
- Ceramic Engineering (AREA)
- Inorganic Chemistry (AREA)
- Manufacturing & Machinery (AREA)
- Physical Vapour Deposition (AREA)
- Crystals, And After-Treatments Of Crystals (AREA)
- Physical Deposition Of Substances That Are Components Of Semiconductor Devices (AREA)
Abstract
Description
本發明係關於成膜裝置及成膜方法。 The present invention relates to a film forming apparatus and a film forming method.
作為具有基板、被形成於基板上的導電膜、被形成於導電膜上的壓電膜之膜構造體,已知有具有基板、被形成於基板上的含鉑之導電膜,及被形成於導電膜上的含鈦鋯酸鉛(PZT)的壓電膜之膜構造體。 As a film structure including a substrate, a conductive film formed on the substrate, and a piezoelectric film formed on the conductive film, there are known a conductive film including a substrate, a platinum-containing film formed on the substrate, and a conductive film formed on the substrate. A film structure of a piezoelectric film containing lead zirconate titanate (PZT) on a conductive film.
於國際公開第2016/009698號公報(專利文獻1),揭示著於強介電體陶瓷,具備Pb(Zr1-ATiA)O3膜、被形成於該Pb(Zr1-ATiA)O3膜上的Pb(Zr1-xTix)O3膜,A及x滿足0≦A≦0.1及0.1<x<1之技術。 In International Publication No. 2016/009698 (Patent Document 1), it is disclosed that a ferroelectric ceramic is provided with a Pb(Zr 1-A Ti A )O 3 film, which is formed on the Pb(Zr 1-A Ti A ) ) On the Pb(Zr 1-x Ti x )O 3 film on the O 3 film, A and x satisfy the technology of 0≦A≦0.1 and 0.1<x<1.
於日本特開2014-84494號公報(專利文獻2),揭示著於矽基板(Si)上預先依序層積YSZ(8%Y2O3+92%ZrO2)、CeO2、LaSrCoO3之膜而形成的緩衝層上形成PZT(鈦鋯酸鉛)薄膜的技術。特別是在專利文獻2,揭示了LaSrCoO3(LSCO)對其他膜旋轉45°晶格之技術。
In Japanese Patent Laid-Open No. 2014-84494 (Patent Document 2), it is disclosed that YSZ (8%Y 2 O 3 +92% ZrO 2 ), CeO 2 , and LaSrCoO 3 are sequentially laminated on a silicon substrate (Si) in advance. The technology of forming a PZT (lead zirconate titanate) thin film on the buffer layer formed by the film. In particular,
於非專利文獻1,揭示了再矽基板上,形成依序被層積YSZ、CeO2、La0.5Sr0.5CoO3(LSCO)、SrRuO3(SRO)的緩衝層,於該緩衝層上,被形成c軸配向之
0.06Pb(Mn1/3,Nb2/3)O3-0.94Pb(Zr0.5Ti0.5)O3(PMnN-PZT)磊晶(epitaxial)薄膜之技術。於非專利文獻1,揭示了PMnN-PZT之晶格在面內方向對矽旋轉45°之技術。
In
於非專利文獻2,揭示了使用氧化鎂單晶坩鍋藉由助熔劑(flux)法育成的PbTiO3之相對介電常數在室溫下為150,為純粹的PbTiO3單晶之相對介電常數的1.5倍之技術。 In Non-Patent Document 2 , it is disclosed that the relative permittivity of PbTiO3 grown by a flux method using a magnesium oxide single crystal crucible is 150 at room temperature, which is the relative permittivity of a pure PbTiO3 single crystal. 1.5 times the constant technique.
於含鈦鋯酸鉛的壓電膜,在壓電膜的結晶性等品質並非良好的場合,壓電膜的壓電特性會降低。另一方面,壓電膜的結晶性等品質良好的場合,壓電膜的壓電特性提升,而壓電膜的相對介電常數不會變小的話,例如在把該壓電膜作為壓力感測器使用的場合,會因為例如壓力感測器的容量變大等理由,而使壓力感測器的檢測感度降低,而有該壓力感測器的檢測電路的設計變得困難之虞。 In the piezoelectric film containing lead titanate zirconate, when the quality such as crystallinity of the piezoelectric film is not good, the piezoelectric properties of the piezoelectric film are degraded. On the other hand, when the crystallinity of the piezoelectric film is good, the piezoelectric properties of the piezoelectric film are improved, and the relative permittivity of the piezoelectric film does not decrease. For example, when the piezoelectric film is used as a pressure sensor When the pressure sensor is used, for example, the capacity of the pressure sensor increases, the detection sensitivity of the pressure sensor decreases, and the design of the detection circuit of the pressure sensor may become difficult.
然而,使用從前的成膜裝置,要形成這樣結晶性等品質良好的鈦鋯酸鉛之壓電膜是困難的。 However, it is difficult to form a piezoelectric film of lead zirconate titanate having such good quality such as crystallinity using the conventional film forming apparatus.
[專利文獻1]國際公開第2016/009698號公報 [Patent Document 1] International Publication No. 2016/009698
[專利文獻2]日本特開2014-84494號公報 [Patent Document 2] Japanese Patent Laid-Open No. 2014-84494
[非專利文獻1]S. Yoshida et al., “Fabrication and characterization of large figure-of-merit epitaxial PMnN-PZT/Si transducer for piezoelectric MEMS sensors”, Sensors and Actuators A 239 (2016) 201-208 [Non-Patent Document 1] S. Yoshida et al., “Fabrication and characterization of large figure-of-merit epitaxial PMnN-PZT/Si transducer for piezoelectric MEMS sensors”, Sensors and Actuators A 239 (2016) 201-208
[非專利文獻2]小舟正文、其他1人、「根據MgO單 晶製坩鍋之PbTiO3單晶之育成及評估」、窯業協會誌、1987年、第95巻、第11號、p.1053-1058 [Non-Patent Document 2] Xiaozhou Text, 1 other person, "Growing and Evaluation of PbTiO3 Single Crystal Based on MgO Single Crystal Crucible", Journal of the Kiln Industry Association, 1987, Vol. 95, No. 11, p.1053 -1058
本發明之一態樣,以提供形成結晶性良好的膜之成膜裝置或成膜方法為課題。 In one aspect of the present invention, an object of the present invention is to provide a film-forming apparatus or a film-forming method for forming a film with good crystallinity.
以下,說明本發明之各種態樣。 Hereinafter, various aspects of the present invention will be described.
一種成膜裝置,其特徵為具有:被導電連接於接地電位的真空室、被配置於前述真空室內的靶、對前述靶供給高頻電力的電力供給部、對前述真空室內供給氣體的氣體供給部、被配置於前述真空室內,使基板對向於前述靶而保持之絕緣性基板保持部、支撐前述絕緣性基板保持部之導電性支撐部、被配置於前述導電性支撐部與前述真空室之間的第1絕緣性構件;前述導電性支撐部藉由前述第1絕緣性構件對前述真空室為電氣浮動狀態,藉著前述基板的外周部與前述絕緣性基板保持部接觸,前述基板被保持於前述絕緣性基板保持部,前述基板對前述導電性支撐部為電氣浮動狀態,前述絕緣性基板保持部,平面俯視不與前述基板的中央部重疊。 A film forming apparatus comprising: a vacuum chamber electrically connected to a ground potential, a target disposed in the vacuum chamber, a power supply unit for supplying high-frequency power to the target, and a gas supply for supplying gas into the vacuum chamber part, an insulating substrate holding part arranged in the vacuum chamber to hold the substrate facing the target, a conductive support part supporting the insulating substrate holding part, arranged in the conductive support part and the vacuum chamber The first insulating member between the two; the conductive support portion is electrically floated to the vacuum chamber by the first insulating member, and the substrate is held by the outer peripheral portion of the substrate in contact with the insulating substrate holding portion. The insulating substrate holding portion is held by the insulating substrate holding portion, the substrate is electrically floating with respect to the conductive support portion, and the insulating substrate holding portion does not overlap with the central portion of the substrate in a plan view.
根據前述[1]之成膜裝置,藉由對真空室為電氣浮動狀態的導電性支撐部來支撐絕緣性基板保持部,使保持於 該絕緣性基板保持部的基板對導電性支撐部為電氣浮動狀態,可以使成膜時蓄積於基板的電荷不會逃逸至接地電位。藉此,可以於基板蓄積多量的電荷,結果,可以形成結晶性良好之膜。 According to the film forming apparatus of the aforementioned [1], the insulating substrate holding portion is supported by the conductive support portion in an electrically floating state with respect to the vacuum chamber, and the insulating substrate holding portion is held in the vacuum chamber. The substrate of the insulating substrate holding portion is in an electrically floating state with respect to the conductive support portion, so that charges accumulated on the substrate during film formation do not escape to the ground potential. Thereby, a large amount of electric charges can be accumulated on the substrate, and as a result, a film with good crystallinity can be formed.
如前述[1]之成膜裝置,其中具有被配置於前述靶與前述基板之間,位在前述基板起30mm以內的距離之導電性防附著板,前述導電性防附著板對前述真空室為電氣浮動狀態。 The film forming apparatus according to the aforementioned [1], further comprising a conductive anti-adhesion plate disposed between the target and the substrate at a distance of within 30 mm from the substrate, and the conductive anti-adhesion plate is oriented to the vacuum chamber. Electrically floating state.
根據前述[2]之成膜裝置,即使把導電性防附著板配置於基板其算30mm以內的距離,藉著使該導電性防附著板對真空室為電氣浮動狀態,可以使成膜時蓄積於基板的電荷不會逃逸至接地電位。 According to the film forming apparatus of the above [2], even if the conductive anti-adhesion plate is arranged on the substrate within a distance of 30 mm, by making the conductive anti-adhesion plate in an electrically floating state with respect to the vacuum chamber, accumulation during film formation can be made. The charge on the substrate does not escape to the ground potential.
如前述[2]之成膜裝置,其中前述導電性防附著板被水冷。 The film forming apparatus according to the above [2], wherein the conductive anti-adhesion plate is water-cooled.
如前述[2]或[3]之成膜裝置,其中具有被配置於前述真空室與前述導電性防附著板之間的第2絕緣性構件。 The film-forming apparatus of the said [2] or [3] which has the 2nd insulating member arrange|positioned between the said vacuum chamber and the said electroconductive adhesion prevention board.
如前述[1]至[4]之任一之成膜裝置,其中前述基板與前述絕緣性基板保持部之接觸面積縮小到20mm2以下。 The film forming apparatus according to any one of the above [1] to [4], wherein the contact area between the substrate and the insulating substrate holding portion is reduced to 20 mm 2 or less.
根據前述[4]之成膜裝置,藉由使基板與絕緣性基板保持部之接觸面積在20mm2以下,可以同時取得往基板之熱絕緣以及電絕緣。 According to the film forming apparatus of the aforementioned [4], by setting the contact area between the substrate and the insulating substrate holding portion to 20 mm 2 or less, thermal insulation and electrical insulation to the substrate can be simultaneously obtained.
如前述[1]至[5]之任一之成膜裝置,其中前述絕緣性基板保持部之角具有曲面。 The film forming apparatus according to any one of the above [1] to [5], wherein a corner of the insulating substrate holding portion has a curved surface.
如前述[1]至[6]之任一之成膜裝置,其中前述導電 性支撐部,包含支撐前述絕緣性基板保持部之第1導電性構件,前述第1導電性構件,以第1軸為中心而可與前述絕緣性基板保持部一體旋轉地設置,具有被配置在前述第1導電性構件與前述絕緣性基板保持部之間的第3絕緣性構件,前述成膜裝置,進而具有旋轉驅動前述第1導電性構件之旋轉驅動部。 The film forming apparatus according to any one of the aforementioned [1] to [6], wherein the aforementioned conductive The supporting portion includes a first conductive member supporting the insulating substrate holding portion, the first conductive member is rotatably provided with the insulating substrate holding portion around the first axis, and has a The third insulating member between the first electroconductive member and the insulating substrate holding portion, the film forming apparatus, further includes a rotational driving portion for rotationally driving the first electroconductive member.
如前述[1]至[6]之任一之成膜裝置,其中前述導電性支撐部,包含支撐前述絕緣性基板保持部之第2導電性構件,前述第2導電性構件,以第2軸為中心而可與前述絕緣性基板保持部一體旋轉地設置;前述第1絕緣性構件,中介在前述真空室與前述第2導電性構件之間,前述第2導電性構件為電氣浮動狀態,前述成膜裝置進而具有旋轉驅動前述第2導電性構件之旋轉驅動部。 The film forming apparatus according to any one of the above [1] to [6], wherein the conductive support portion includes a second conductive member for supporting the insulating substrate holding portion, and the second conductive member is connected to a second axis by a second axis. The first insulating member is interposed between the vacuum chamber and the second conductive member, the second conductive member is in an electrically floating state, and the The film-forming apparatus further includes a rotational driving unit that rotationally drives the second conductive member.
如前述[7]之成膜裝置,其中具有加熱前述基板之基板加熱部,前述第3絕緣性構件,平面俯視具有包圍前述基板的包圍部,前述絕緣性基板保持部,平面俯視具有由前述包圍部朝向前述基板的中心側分別突出的複數個突出部,前述絕緣性基板保持部,在前述基板的外周部與前述複數個突出部之各個接觸的狀態下保持前述基板。 The film forming apparatus according to the aforementioned [7], further comprising a substrate heating unit for heating the substrate, the third insulating member having an enclosing portion enclosing the substrate in a plan view, and the insulating substrate holding portion having an enclosing portion enclosing the substrate in a plan view A plurality of protruding portions each protruding toward the center side of the substrate, and the insulating substrate holding portion holds the substrate in a state in which the outer peripheral portion of the substrate is in contact with each of the plurality of protruding portions.
[10]如前述[1]至[9]之任一之成膜裝置,其中具有在前述真空室內保持前述靶之靶保持部,及對前述靶施加磁場的磁場施加部;被施加前述磁場的前述靶的表面之水平磁場為140~220G。 [10] The film forming apparatus according to any one of the above [1] to [9], comprising a target holding portion for holding the target in the vacuum chamber, and a magnetic field application portion for applying a magnetic field to the target; The horizontal magnetic field on the surface of the target is 140-220G.
[11]如前述[10]之成膜裝置,其中前述靶的表面之前 述磁場,係沿著前述靶的表面。 [11] The film forming apparatus according to the aforementioned [10], wherein the surface of the aforementioned target is before The magnetic field is along the surface of the target.
[12]如前述[1]至[11]之任一之成膜裝置,其中前述成膜裝置,藉由濺鍍含有鈦鋯酸鉛的前述靶的表面而於前述基板的表面形成含有鈦鋯酸鉛之膜。 [12] The film forming apparatus according to any one of the above [1] to [11], wherein the film forming apparatus forms a titanium zirconium-containing material on the surface of the substrate by sputtering the surface of the target containing lead titanic zirconate. Lead acid film.
[13]如前述[1]至[12]之任一之成膜裝置,其中前述成膜裝置,藉由在前述真空室內濺鍍與前述基板下面對向配置之前述靶上面而於前述基板下面形成膜。 [13] The film formation apparatus according to any one of the above [1] to [12], wherein the film formation apparatus is formed on the substrate by sputtering in the vacuum chamber the upper surface of the target disposed opposite to the lower surface of the substrate The film is formed below.
[14]一種成膜方法,其特徵係在被導電連接於接地電位的真空室內,藉著基板的外周部與絕緣性基板保持部接觸,藉由前述絕緣性基板保持部保持前述基板,藉由在前述真空室內濺鍍靶的表面而於前述基板的表面形成膜,前述絕緣性基板保持部,藉由對前述真空室為電氣浮動狀態的導電性支撐部被支撐,前述基板對前述導電性支撐部為電氣浮動狀態,前述絕緣性基板保持部平面俯視不與前述基板的中央部重疊。 [14] A film forming method, characterized in that in a vacuum chamber electrically connected to a ground potential, an outer peripheral portion of a substrate is in contact with an insulating substrate holding portion, the insulating substrate holding portion holds the substrate, and The surface of the target is sputtered in the vacuum chamber to form a film on the surface of the substrate, the insulating substrate holding portion is supported by a conductive support portion electrically floating with respect to the vacuum chamber, and the substrate is supported by the conductive support The portion is in an electrically floating state, and the insulating substrate holding portion does not overlap with the central portion of the substrate in plan view.
[15]如前述[14]之成膜方法,其中導電性防附著板被配置於前述靶與前述基板之間,前述導電性防附著板位在前述基板起30mm以內的距離,前述導電性防附著板對前述真空室為電氣浮動狀態。 [15] The film forming method according to the aforementioned [14], wherein a conductive anti-adhesion plate is disposed between the target and the substrate, the conductive anti-adhesion plate is positioned within a distance of 30 mm from the substrate, and the conductive anti-adhesion plate is positioned within a distance of 30 mm from the substrate. The attachment plate is electrically floating to the aforementioned vacuum chamber.
[16]如前述[14]之成膜方法,其中前述導電性防附著板被水冷。 [16] The film-forming method according to the aforementioned [14], wherein the conductive anti-adhesion plate is water-cooled.
[17]如前述[14]至[16]之任一之成膜方法,其中前述基板與前述絕緣性基板保持部之接觸面積在20mm2以下。 [17] The film forming method according to any one of the above [14] to [16], wherein the contact area between the substrate and the insulating substrate holding portion is 20 mm 2 or less.
[18]如前述[14]至[17]之任一之成膜方法,其中藉由 磁場施加部對前述靶施加磁場,且在藉由電力供給部對前述靶供給高頻電力的狀態下,藉由濺鍍前述靶的表面,於前述基板的表面形成前述膜,被施加前述磁場的前述靶的表面之水平磁場為140~220G。 [18] The film-forming method according to any one of the aforementioned [14] to [17], wherein the The magnetic field applying unit applies a magnetic field to the target, and in a state where high-frequency power is supplied to the target by the power supply unit, the film is formed on the surface of the substrate by sputtering the surface of the target, and the magnetic field is applied. The horizontal magnetic field on the surface of the target is 140-220G.
[19]如前述[18]之成膜方法,其中前述靶的表面之前述磁場,係沿著前述靶的表面。 [19] The film-forming method according to the aforementioned [18], wherein the magnetic field on the surface of the target is along the surface of the target.
[20]如前述[14]至[19]之任一之成膜方法,其中前述靶含有鈦鋯酸鉛,藉由濺鍍前述靶的表面而於前述基板的表面形成含有鈦鋯酸鉛之前述膜。 [20] The film forming method according to any one of the aforementioned [14] to [19], wherein the target contains lead zirconate titanate, and the surface of the target is sputtered to form a film containing lead zirconate titanate on the surface of the substrate. the aforementioned film.
[21]如前述[20]之成膜方法,其中前述基板,包含:包含由(100)面所構成的主面之矽基板、被形成於前述主面上,具有立方晶結晶構造,且包含(100)配向的氧化鋯膜之第1膜、以及被形成於前述第1膜上,具有立方晶結晶構造,且包含(100)配向的鉑膜之第1導電膜;前述氧化鋯膜,以沿著前述氧化鋯膜的前述主面之<100>方向,與沿著前述矽基板的前述主面之<100>方向平行的方式配向;前述鉑膜,以沿著前述鉑膜的前述主面之<100>方向,與沿著前述矽基板的前述主面之<100>方向平行的方式配向;藉由濺鍍前述靶的表面,於前述第1導電膜上,形成具有正方晶之結晶構造,且包含(001)配向的第1鈦鋯酸鉛膜之第1壓電膜,前述第1鈦鋯酸鉛膜,具有由下列一般式(化學式1)所表示的鈦鋯酸鉛所構成的第1複合氧化物,Pb(Zr1-xTix)O3‧‧‧(化學式1)前述第1鈦鋯酸鉛膜,以沿著前述第1鈦鋯酸鉛膜的前述主面之< 100>方向,與沿著前述矽基板的前述主面之<100>方向平行的方式配向;前述x滿足0.32≦x≦0.52。 [21] The film forming method according to the above [20], wherein the substrate includes a silicon substrate including a main surface formed by a (100) plane, is formed on the main surface, has a cubic crystal structure, and includes A first film of a (100) oriented zirconia film, and a first conductive film formed on the first film, having a cubic crystal structure, and including a (100) oriented platinum film; the zirconia film, with Aligning the <100> direction along the main surface of the zirconia film in parallel with the <100> direction along the main surface of the silicon substrate; and aligning the platinum film along the main surface of the platinum film The <100> direction is aligned parallel to the <100> direction along the main surface of the silicon substrate; by sputtering the surface of the target, a tetragonal crystal structure is formed on the first conductive film , and a first piezoelectric film including a (001)-aligned first lead zirconate titanate film, the first lead zirconate titanate film having a lead zirconate titanate film represented by the following general formula (chemical formula 1) The first composite oxide, Pb(Zr 1-x Ti x )O 3 ‧‧‧(Chemical formula 1), the first lead titan zirconate film is formed along the main surface of the first lead titan zirconate film. The 100> direction is aligned parallel to the <100> direction along the main surface of the silicon substrate; the x satisfies 0.32≦x≦0.52.
[22]如前述[14]至[21]之任一之成膜方法,其中藉由在前述真空室內濺鍍與前述基板下面對向配置之前述靶上面而於前述基板下面形成膜。 [22] The film-forming method according to any one of the above [14] to [21], wherein the film is formed on the underside of the substrate by sputtering the topside of the target disposed opposite to the underside of the substrate in the vacuum chamber.
藉著適用本發明之一態樣,可以提供形成結晶性良好的膜之成膜裝置或成膜方法。 By applying one aspect of the present invention, a film forming apparatus or a film forming method for forming a film with good crystallinity can be provided.
10:膜構造體 10: Membrane constructs
11:基板 11: Substrate
11a:上面 11a: Above
12:配向膜 12: Alignment film
12a:氧化鋯膜 12a: Zirconia film
13、18:導電膜 13, 18: Conductive film
13a:鉑膜 13a: Platinum film
14、17f:膜 14, 17f: Membrane
14a:SRO膜 14a: SRO membrane
15、16、17:壓電膜 15, 16, 17: Piezoelectric film
15a、16a、17a:鈦鋯酸鉛膜 15a, 16a, 17a: lead titanate zirconate film
16g、17g:晶粒 16g, 17g: grains
20:成膜裝置 20: Film forming device
21:真空室 21: Vacuum Chamber
21a:底板部 21a: Bottom plate
21b、21e:側板部 21b, 21e: side plate
21c、21f:頂板部 21c, 21f: top plate
21d:蓋部 21d: Cover
22:真空排氣部 22: Vacuum exhaust part
23、24:氣體供給部 23, 24: Gas supply part
23a、24a:流量控制器 23a, 24a: flow controller
23b、24b:氣體供給管 23b, 24b: Gas supply pipes
25:基板保持部 25: Substrate holding part
25a:絕緣性包圍部 25a: Insulating enclosure
25b:突出部 25b: Protrusion
25c:導電性包圍部 25c: Conductive enclosure
25d:階差部 25d: Step part
25b1:角 25b1: Corner
26:支撐部 26: Support Department
27:旋轉驅動部 27: Rotary drive part
27a:馬達 27a: Motor
27b:皮帶 27b: Belt
27c:帶輪 27c: Pulley
27d:旋轉軸 27d: Rotation axis
28:基板加熱部 28: Substrate heating section
29:防附著板 29: Anti-adhesion plate
29a:冷卻管 29a: Cooling pipe
31:靶保持部 31: Target holding part
32:電力供給部 32: Power Supply Department
32a:高頻電源 32a: High frequency power supply
32b:整合器 32b: Integrator
33:VDC控制部 33: V DC control part
34:磁石部 34: Magnet Department
35:磁石旋轉驅動部 35: Magnet rotating drive part
41、42、45、46、47:導電性構件 41, 42, 45, 46, 47: Conductive members
41a、42a、45a:基部 41a, 42a, 45a: base
41b、42b、45b:軸部 41b, 42b, 45b: Shaft
41c、42c、45c:接續部 41c, 42c, 45c: Connections
43、56:螺絲 43, 56: Screws
44:滑移環 44: Slip Ring
51、52、53、54、55:絕緣性構件 51, 52, 53, 54, 55: Insulating members
BP1:背板(backing plate) BP1: backing plate
CE1:密封部 CE1: Sealing part
CN1:中心 CN1: Center
CP1:強介電質電容器 CP1: ferroelectric capacitor
EP:終點 EP: End Point
OP1、OP2、OP3:開口 OP1, OP2, OP3: Opening
P1:分極成分 P1: Polarized composition
RA1:旋轉軸 RA1: Rotary axis
SB:基板 SB: Substrate
SP:起點 SP: starting point
TG:靶 TG: target
TM1:靶材 TM1: Target
圖1係實施型態之膜構造體之剖面圖。 FIG. 1 is a cross-sectional view of a membrane structure of an embodiment.
圖2係實施型態之膜構造體具有作為上部電極之導電膜的場合之膜構造體之剖面圖。 2 is a cross-sectional view of the film structure in the case where the film structure of the embodiment has a conductive film as the upper electrode.
圖3係由圖2所式的膜構造體除去基板及配向膜的場合膜構造體之剖面圖。 FIG. 3 is a cross-sectional view of the film structure when the substrate and the alignment film are removed from the film structure shown in FIG. 2 .
圖4係實施型態之膜構造體之其他例之剖面圖。 4 is a cross-sectional view of another example of the membrane structure of the embodiment.
圖5係模式顯示實施型態之膜構造體所包含的2個壓電膜的剖面構造之圖。 FIG. 5 is a diagram schematically showing a cross-sectional structure of two piezoelectric films included in the film structure of the embodiment.
圖6係模式顯示實施型態之膜構造體所包含的壓電膜的分極之電場依存性之圖。 FIG. 6 is a diagram schematically showing the electric field dependence of the polarization of the piezoelectric film included in the film structure of the embodiment.
圖7係說明包含於實施型態的膜構造體之各層的膜磊晶成長的狀態之圖。 7 is a diagram illustrating a state of film epitaxial growth of each layer included in the film structure of the embodiment.
圖8係模式顯示實施型態之成膜裝置之剖面圖。 FIG. 8 is a cross-sectional view schematically showing a film forming apparatus of an embodiment.
圖9係模式顯示實施型態之成膜裝置之剖面圖。 FIG. 9 is a cross-sectional view schematically showing the film forming apparatus of the embodiment.
圖10(A)係實施型態之成膜裝置具有的基板保持部
之平面圖,圖10(B)~(D)係顯示圖10(A)所示的突出部25b的形狀之圖。
FIG. 10(A) shows the substrate holding portion included in the film forming apparatus of the embodiment.
10(B) to (D) are plan views showing the shape of the protruding
圖11係實施型態之膜構造體的製造步驟中之剖面圖。 Fig. 11 is a cross-sectional view in a manufacturing step of the film structure of the embodiment.
圖12係實施型態之膜構造體的製造步驟中之剖面圖。 Fig. 12 is a cross-sectional view in a manufacturing step of the film structure of the embodiment.
圖13係實施型態之膜構造體的製造步驟中之剖面圖。 FIG. 13 is a cross-sectional view in a manufacturing step of the film structure of the embodiment.
圖14係實施型態之膜構造體的製造步驟中之剖面圖。 FIG. 14 is a cross-sectional view in a manufacturing step of the membrane structure of the embodiment.
圖15係實施型態的變形例之膜構造體之剖面圖。 15 is a cross-sectional view of a membrane structure according to a modification of the embodiment.
圖16係顯示實施例1之膜構造體之根據XRD法之θ-2θ頻譜之例之圖。 16 is a diagram showing an example of the θ-2θ spectrum of the film structure of Example 1 according to the XRD method.
圖17係顯示實施例1之膜構造體之根據XRD法之θ-2θ頻譜之例之圖。 FIG. 17 is a diagram showing an example of the θ-2θ spectrum by the XRD method of the film structure of Example 1. FIG.
圖18係顯示比較例1之膜構造體之根據XRD法之θ-2θ頻譜之例之圖。 18 is a diagram showing an example of the θ-2θ spectrum of the film structure of Comparative Example 1 according to the XRD method.
圖19係顯示比較例1之膜構造體之根據XRD法之θ-2θ頻譜之例之圖。 FIG. 19 is a diagram showing an example of the θ-2θ spectrum by the XRD method of the film structure of Comparative Example 1. FIG.
圖20係顯示實施例1之膜構造體之根據XRD法之極點圖之例之圖。 FIG. 20 is a diagram showing an example of a pole diagram according to the XRD method of the film structure of Example 1. FIG.
圖21係顯示實施例1之膜構造體之根據XRD法之極點圖之例之圖。 FIG. 21 is a diagram showing an example of a pole diagram according to the XRD method of the film structure of Example 1. FIG.
圖22係顯示實施例1之膜構造體之根據XRD法之極點圖之例之圖。 FIG. 22 is a diagram showing an example of a pole diagram according to the XRD method of the film structure of Example 1. FIG.
圖23係顯示實施例1之膜構造體之根據XRD法之極點圖之例之圖。 23 is a diagram showing an example of a pole diagram according to the XRD method of the film structure of Example 1. FIG.
圖24係顯示被形成於實施例1之17枚晶圓之各個的膜 構造體之分別的X線繞射圖案之繞射角度2θ004之圖。 24 is a diagram showing the diffraction angle 2θ 004 of each X-ray diffraction pattern of the film structures formed on each of the 17 wafers of Example 1. FIG.
圖25係顯示被形成於實施例1之12枚晶圓之各個的膜構造體之分別的X線繞射圖案之繞射角度2θ004之圖。 FIG. 25 is a diagram showing the diffraction angle 2θ 004 of each X-ray diffraction pattern of the film structures formed on each of the 12 wafers of Example 1. FIG.
圖26係顯示實施例1之膜構造體之分極的電壓依存性之圖。 FIG. 26 is a graph showing the voltage dependence of polarization of the membrane structure of Example 1. FIG.
圖27係顯示比較例1之膜構造體之分極的電壓依存性之圖。 FIG. 27 is a graph showing the voltage dependence of polarization of the membrane structure of Comparative Example 1. FIG.
圖28係顯示實施例2之膜構造體之分極的電壓依存性之圖。 FIG. 28 is a graph showing the voltage dependence of polarization of the membrane structure of Example 2. FIG.
圖29係顯示實施例3之膜構造體之分極的電壓依存性之圖。 FIG. 29 is a graph showing the voltage dependence of polarization of the membrane structure of Example 3. FIG.
圖30係顯示實施例4之膜構造體之分極的電壓依存性之圖。 FIG. 30 is a graph showing the voltage dependence of polarization of the membrane structure of Example 4. FIG.
圖31係顯示實施例5之膜構造體之分極的電壓依存性之圖。 FIG. 31 is a graph showing the voltage dependence of polarization of the membrane structure of Example 5. FIG.
圖32係顯示匯集實施例1、實施例6至實施例8、比較例1及比較例2之成膜條件以及PZT的繞射角度2θ004及相對介電常數εr等之測定結果之表。 32 is a table showing the measurement results of the film formation conditions of Example 1, Example 6 to Example 8, Comparative Example 1 and Comparative Example 2, and the diffraction angle 2θ 004 and relative permittivity ε r of PZT.
圖33係顯示實施例6之膜構造體之根據XRD法之θ-2θ頻譜之例之圖。 FIG. 33 is a diagram showing an example of the θ-2θ spectrum according to the XRD method of the film structure of Example 6. FIG.
圖34係顯示實施例7之膜構造體之根據XRD法之θ-2θ頻譜之例之圖。 34 is a diagram showing an example of the θ-2θ spectrum of the film structure of Example 7 according to the XRD method.
圖35係顯示實施例8之膜構造體之根據XRD法之θ-2θ頻譜之例之圖。 35 is a diagram showing an example of the θ-2θ spectrum according to the XRD method of the film structure of Example 8. FIG.
圖36係顯示比較例2之膜構造體之分極的電壓依存性之圖。 FIG. 36 is a graph showing the voltage dependence of polarization of the membrane structure of Comparative Example 2. FIG.
圖37係顯示實施例6之膜構造體之分極的電壓依存性之圖。 FIG. 37 is a graph showing the voltage dependence of polarization of the membrane structure of Example 6. FIG.
圖38係顯示實施例7之膜構造體之分極的電壓依存性之圖。 FIG. 38 is a graph showing the voltage dependence of polarization of the membrane structure of Example 7. FIG.
圖39係顯示實施例8之膜構造體之分極的電壓依存性之圖。 FIG. 39 is a graph showing the voltage dependence of polarization of the membrane structure of Example 8. FIG.
圖40係顯示實施例9之膜構造體之分極的電壓依存性之圖。 FIG. 40 is a graph showing the voltage dependence of polarization of the membrane structure of Example 9. FIG.
圖41係顯示實施例10之膜構造體之分極的電壓依存性之圖。 FIG. 41 is a graph showing the voltage dependence of polarization of the membrane structure of Example 10. FIG.
以下,使用圖式詳細說明本發明之實施型態及實施例。但本發明並不以下列說明為限,在不逸脫本發明的要旨及其範圍的情況下,可將其形態或者詳細內容加以種種變更,這對熟悉該項技藝者而言應屬容易理解的範圍。從而,本發明並不被限定解釋為以下所示的實施型態的記載內容及實施例。 Hereinafter, embodiments and examples of the present invention will be described in detail using the drawings. However, the present invention is not limited to the following description, and various changes can be made to its form or detailed content without departing from the gist and scope of the present invention, which should be easily understood by those skilled in the art range. Therefore, the present invention is not to be construed as being limited to the descriptions and examples of the embodiments shown below.
此外,圖式可使說明更為明確,與實施的態樣相比,各部分的寬幅、厚度、形狀等亦有模式表示的場合,其終究只是一例示而已,並非用於限定本發明之解釋。 In addition, the drawings can make the description more clear, and when the width, thickness, shape, etc. of each part are schematically shown compared with the embodiment, it is only an example after all, and is not intended to limit the present invention. explain.
此外,於本說明書與各圖式,關於已經圖示而與先前 所述相同的要素會被賦予同一符號而適當省略詳細說明。 In addition, in this specification and each drawing, with respect to what has been shown and the previous The same elements are given the same symbols, and detailed descriptions are appropriately omitted.
進而,於實施型態使用的圖式,亦有因應於圖式而省略供區別構造物之用而賦予的影線(網線)的情形。 Furthermore, depending on the drawings used in the embodiments, hatching (network lines) provided for distinguishing structures may be omitted in accordance with the drawings.
又,於以下的實施型態,以A~B來顯示範圍的場合,在沒有特別說明的情況下,係指A以上B以下。 In addition, in the following embodiment, when the range is shown by A to B, it means A or more and B or less unless otherwise specified.
首先,說明本發明之一實施型態之實施的型態之膜構造體。圖1係實施型態之膜構造體之剖面圖。圖2係實施型態之膜構造體具有作為上部電極之導電膜的場合之膜構造體之剖面圖。圖3係由圖2所式的膜構造體除去基板及配向膜的場合膜構造體之剖面圖。圖4係實施型態之膜構造體之其他例之剖面圖。 First, the membrane structure of the embodiment of one embodiment of the present invention will be described. FIG. 1 is a cross-sectional view of a membrane structure of an embodiment. 2 is a cross-sectional view of the film structure in the case where the film structure of the embodiment has a conductive film as the upper electrode. FIG. 3 is a cross-sectional view of the film structure when the substrate and the alignment film are removed from the film structure shown in FIG. 2 . 4 is a cross-sectional view of another example of the membrane structure of the embodiment.
如圖1所示,本實施型態之膜構造體10,具有基板11、配向膜12、導電膜13、膜14、壓電膜15。配向膜12,被形成於基板11上。導電膜13,被形成於配向膜12上。膜14,被形成於導電膜13上。壓電膜15,被形成於膜14上。
As shown in FIG. 1 , the
又,如圖2所示,本實施型態之膜構造體10,亦可具有導電膜18。導電膜18,被形成於壓電膜15上。此時,導電膜13,係作為下部電極之導電膜,導電膜18,係作為上部電極之導電膜。此外,如圖3所示,本實施型態之膜構造體10,亦可不具有基板11(參照圖2)及配向膜12(參照圖2),而僅具有作為下部電極之導電膜13、膜14、壓
電膜15、與作為上部電極之導電膜18。
Moreover, as shown in FIG. 2, the
此外,如圖4所示,本實施型態之膜構造體10,亦可僅具有基板11、配向膜12、導電膜13。這樣的場合,可以把膜構造體10作為供形成壓電膜15之用的電極基板來使用,可以在導電膜13上磊晶成長,且可容易形成具有良好壓電特性的壓電膜15。
In addition, as shown in FIG. 4 , the
基板11,係由矽(Si)單晶所構成的矽基板。作為矽基板之基板11,包含由(100)面構成的主面之上面11a。配向膜12,被形成於上面11a,具有立方晶之結晶構造,且包含(100)配向之氧化鋯。導電膜13,具有立方晶之結晶構造,且包含(100)配向之鉑。藉此,壓電膜15,在包含具有鈣鈦礦(perovskite)型構造的複合氧化物的場合,可以使壓電膜15,在基板11上,成為以正方晶表示之(001)配向或以擬立方晶表示之(100)配向。
The
在此,所謂配向膜12為(100)配向,是指具有立方晶的結晶構造之配向膜12的(100)面,係沿著矽基板之基板11的作為由(100)面構成的主面之上面11a,較佳為平行於矽基板之基板11的(100)面所構成的上面11a。此外,配向膜12之(100)面平行於基板11之(100)面所構成的上面11a,是指不僅是配向膜12的(100)面完全平行於基板11的上面11a的場合,也包含完全平行於基板11的上面11a的面與配向膜12的(100)面之夾角在20°以下的場合。此外,不僅配向膜12,其他層之膜的配向也是相同的。
Here, that the
或者是,作為配向膜12,替代由單層膜所構成的配向膜12,改為由層積膜構成的配向膜12被形成於基板11上亦可。
Alternatively, instead of the
較佳為配向膜12,磊晶成長於基板11的上面11a上,導電膜13,磊晶成長於配向膜12上。藉此,壓電膜15,在包含具有鈣鈦礦(perovskite)型構造的複合氧化物的場合,可以使壓電膜15磊晶成長於導電膜13上。
Preferably, the
此處,把在基板11之作為主面的上面11a內相互正交的2個方向作為X軸方向及Y軸方向,把垂直於上面11a的方向作為Z軸方向時,某個膜磊晶成長,是指該膜在X軸方向、Y軸方向及Z軸方向之任一方向均為配向的。又,針對適切的上面11a內之配向方向,使用後述的圖7來進行說明。
Here, when two directions orthogonal to each other in the
膜14,以下列一般式(化學式4)表示,且包含以擬立方晶表示為(100)配向之複合氧化物。
The
Sr(Ti1-zRuz)O3‧‧‧(化學式4) Sr(Ti 1-z Ru z )O 3 ‧‧‧(Chemical formula 4)
在此,z為滿足0≦z≦1。此外,在以下,亦有把z滿足z=0時之Sr(Ti1-zRuz)O3亦即SrTiO3稱為STO,z滿足0<z<1時之Sr(Ti1-zRuz)O3稱為STRO,z滿足z=1時之Sr(Ti1-zRuz)O3亦即SrRuO3稱為SRO之情形。 Here, z satisfies 0≦z≦1. In addition, in the following, Sr(Ti 1-z Ru z )O 3 or SrTiO 3 when z satisfies z=0 is also called STO, and Sr(Ti 1-z Ru 3 when z satisfies 0<z<1 z )O 3 is called STRO, and Sr(Ti 1-z Ru z )O 3 when z satisfies z=1, that is, SrRuO 3 is called SRO.
SRO具有金屬導電性,STO具有半導性或絕緣性。因此,z越接近1,越提高膜14的導電性,可以把膜14作為包含導電膜13的下部電極的一部分使用。
SRO has metallic conductivity and STO has semiconducting or insulating properties. Therefore, as z is closer to 1, the conductivity of the
此處,膜14是藉由濺鍍法形成的場合,z以滿足
0≦z≦0.4為佳,以滿足0.05≦z≦0.2為更佳。z超過0.4的場合,前述一般式(化學式4)表示的複合氧化物變成粉,有無法充分固化之虞,要製造濺鍍靶會變得困難。
Here, when the
另一方面,膜14,例如藉由溶膠凝膠法等塗布法來形成的場合,即使z>0.4也可以容易形成。
On the other hand, when the
以前述一般式(化學式4)表示,具有鈣鈦礦(perovskite)型構造的複合氧化物以擬立方晶表示為(100)配向,意味著如以下所述的場合。 The composite oxide having a perovskite (perovskite) type structure represented by the aforementioned general formula (Chemical formula 4) is represented by a pseudo-cubic crystal as (100) orientation, which means the following cases.
首先,包含被排列為3次元的單位晶格,以一般式ABO3表示的鈣鈦礦(perovskite)型構造的晶格,考慮單位晶格含有1個原子A,1個原子B及3個氧原子的場合。 First, a perovskite (perovskite) structure lattice represented by the general formula ABO 3 , including a unit lattice arranged in a 3-dimensional dimension, considers that the unit lattice contains one atom A, one atom B and three oxygen atoms atomic case.
這樣的場合,以擬立方晶表示之(100)配向,意味著該單位晶格具有立方晶的結晶構造,而且為(100)配向的場合。此時,把該單位晶格的1邊的長度作為晶格常數ac。 In such a case, the (100) orientation represented by the pseudo-cubic crystal means that the unit cell has a cubic crystal structure and the (100) orientation. In this case, the length of one side of the unit lattice is taken as the lattice constant a c .
另一方面,考慮以前述一般式(化學式4)表示,具有鈣鈦礦(perovskite)型構造的複合氧化物,具有斜方晶的結晶構造的場合。接著,考慮斜方晶的3個晶格常數之中的第1個晶格常數ao約略等於擬立方晶的晶格常數ac的21/2倍,斜方晶的3個晶格常數之中的第2個晶格常數bo約略等於擬立方晶的晶格常數ac的2倍,斜方晶的3個晶格常數之中的第3個晶格常數co約略等於擬立方晶的晶格常數ac的21/2倍的場合。又,在本案說明書,數值V1與數值V2約略相等,是指數值V1與數值V2之差的比,相對於數值V1 與數值V2的平均而言在5%程度以下。 On the other hand, consider the case where the composite oxide having a perovskite (perovskite) type structure represented by the aforementioned general formula (Chemical formula 4) has an orthorhombic crystal structure. Next, consider that the first lattice constant a o among the three lattice constants of the orthorhombic crystal is approximately equal to 2 1/2 times the lattice constant a c of the quasi-cubic crystal, and the three lattice constants of the orthorhombic crystal are The second lattice constant b o is approximately equal to twice the lattice constant a c of the quasi-cubic crystal, and the third lattice constant c o of the three lattice constants of the orthorhombic crystal is approximately equal to the quasi-cubic crystal When the lattice constant a c of the crystal is 2 1/2 times. In addition, in this specification, the numerical value V1 and the numerical value V2 are approximately equal, and the ratio of the difference between the index value V1 and the numerical value V2 is about 5% or less with respect to the average of the numerical value V1 and the numerical value V2.
此時,以擬立方晶表示為(100)配向,意味著以斜方晶表示為(101)配向或(020)配向。 In this case, the pseudo-cubic crystal is expressed as (100) orientation, which means that the orthorhombic crystal is expressed as (101) orientation or (020) orientation.
膜14,由於以前述一般式(化學式4)表示,滿足0≦z≦1,所以擬立方晶之晶格常數ac滿足0.390nm≦ac≦0.393nm,如使用後述之圖7所說明的,可以使膜14在導電膜13上以擬立方晶表示被(100)配向。
Since the
壓電膜15,中介著膜14被形成於導電膜13上,具有正方晶之結晶構造,而且包含作為(001)配向的複合氧化物之鈦鋯酸鉛(PZT)。或者是,包含於壓電膜15的鈦鋯酸鉛(PZT),包含具有正方晶的結晶構造的部分,與具有菱面體晶的結晶構造的部分的場合,壓電膜15中介著膜14被形成於導電膜13上,而且包含作為以擬立方晶表示為(100)配向的複合氧化物之鈦鋯酸鉛(PZT)亦可。
The
壓電膜15包含鈦鋯酸鉛(PZT),意味著壓電膜15包含以下列一般式(化學式5)表示的複合氧化物。
The
Pb(Zr1-uTiu)O3‧‧‧(化學式5) Pb(Zr 1-u Ti u )O 3 ‧‧‧(Chemical formula 5)
u滿足0<u<1。 u satisfies 0<u<1.
此外,壓電膜15,具有正方晶之結晶構造,而且在包含(001)配向的鈦鋯酸鉛的場合,在本實施型態,於根據使用CuKα線的θ-2θ法之壓電膜15的X線繞射圖案,鈦鋯酸鉛的正方晶表示之(004)面的繞射峰的繞射角度為2θ004時,2θ004滿足下列式(數式1)。
In addition, the
2θ004≦96.5°‧‧‧(數式1) 2θ 004 ≦96.5°‧‧‧(Formula 1)
藉此,鈦鋯酸鉛之正方晶表示之(004)面的間隔變長。或者是壓電膜15中之具有正方晶結晶構造,且(001)配向(c軸配向)之鈦鋯酸鉛的含有率,可以比壓電膜15中之具有正方晶之結晶構造,且(100)配向(a軸配向)之鈦鋯酸鉛的含有率還要大。亦即,包含於壓電膜15的複數晶粒之各個之分極方向可以排整齊,所以可提高壓電膜15的壓電特性。
Thereby, the space|interval of the (004) plane represented by the tetragonal crystal of lead titanate zirconate becomes long. Alternatively, the
另一方面,壓電膜15,包含擬立方晶表示(100)配向之鈦鋯酸鉛(PZT)的場合,可以考慮如下。
On the other hand, the case where the
包含於壓電膜15的鈦鋯酸鉛,具有正方晶之結晶構造,正方晶的2個晶格常數為at及ct,at及ct滿足ct>at,單位晶格考慮相互正交的3個邊的長度為at、at及ct之直方體的場合。接著,考慮正方晶的晶格常數at約略等於擬立方晶的晶格常數ac,正方晶的晶格常數ct約略等於擬立方晶的晶格常數ac的場合。這樣的場合,鈦鋯酸鉛以擬立方晶表示成(100)配向,是指鈦鋯酸鉛在正方晶表示成(100)配向(a軸配向),或者(001)配向(c軸配向)。
The lead titanate zirconate contained in the
另一方面,考慮包含於壓電膜15的PZT,具有菱面體晶的結晶構造,菱面體晶的晶格常數為ar的場合。接著,考慮菱面體晶的晶格常數ar約略等於擬立方晶的晶格常數ac的場合。這樣的場合,PZT以擬立方晶表示成(100)配向,是指PZT在菱面體晶表示成(100)配向。
On the other hand, consider the case where the PZT included in the
這樣的場合,在本實施型態,於根據使用CuKα線的
θ-2θ法之壓電膜15的X線繞射圖案,鈦鋯酸鉛的擬立方晶表示之(400)面的繞射峰的繞射角度為2θ400時,2θ400滿足前述式(數式1),成為滿足替代2θ004而置換為2θ400之式(2θ400≦96.5°)。接著,藉此,鈦鋯酸鉛之擬立方晶表示之(400)面的間隔變長。因此,壓電膜15中之具有正方晶結晶構造,且(001)配向之鈦鋯酸鉛的含有率,可以比壓電膜15中之具有正方晶之結晶構造,且(100)配向之鈦鋯酸鉛的含有率還要大。亦即,包含於壓電膜15的複數晶粒之各個之分極方向可以排整齊,所以可提高壓電膜15的壓電特性。
In this case, in this embodiment, the diffraction peak of the (400) plane represented by the quasi-cubic crystal of lead zirconate titanate is shown in the X-ray diffraction pattern of the
此外,在本實施型態,壓電膜15的相對介電常數為εr時,εr滿足下列式(數式2)。
In addition, in this embodiment, when the relative permittivity of the
εr≦450‧‧‧(數式2)。 ε r ≦450‧‧‧ (Equation 2).
藉此,把膜構造體10,例如作為使用壓電效果的壓力感測器使用的場合,可以提高檢測感度,可以容易設計該壓力感測器之檢測電路。或者是,把膜構造體10,例如作為使用逆壓電效果的超音波振動件使用的場合,可以容易設計振盪電路。
Thereby, when the
於具有含鈦鋯酸鉛的壓電膜的膜構造體,由於例如膜密度小,或者鈦鋯酸鉛的含量少等理由,在壓電膜的結晶性等品質並非良好的場合,壓電膜的壓電特性會降低。另一方面於具有含鈦鋯酸鉛的壓電膜的膜構造體,由於例如膜密度大,或者鈦鋯酸鉛的含量多等理由,而使壓電膜的結晶性等品質良好的場合,壓電膜的壓電特性會提高,而 壓電膜的相對介電常數不會小。 For a film structure having a piezoelectric film containing lead zirconate titanate, for example, due to a low film density or a small content of lead zirconate titanate, when the quality of the piezoelectric film such as crystallinity is not good, the piezoelectric film piezoelectric properties will be reduced. On the other hand, in the case of a film structure having a piezoelectric film containing lead zirconate titanate, for example, for reasons such as high film density or high content of lead zirconate titanate, the quality of the piezoelectric film such as crystallinity is good. The piezoelectric properties of the piezoelectric film will be improved, while The relative permittivity of the piezoelectric film is not small.
如此,於具有含鈦鋯酸鉛的壓電膜的膜構造體,使壓電膜的壓電特性提高時,會有壓電膜的相對介電常數不小的情形。接著,壓電膜的相對介電常數不會變小的話,例如在把該壓電膜作為壓力感測器使用的場合,會因為例如壓力感測器的容量變大等理由,而使壓力感測器的檢測感度降低,而有該壓力感測器的檢測電路的設計變得困難之虞。 In this way, when the piezoelectric properties of the piezoelectric film are improved in the film structure having the piezoelectric film containing lead titanate zirconate, the relative permittivity of the piezoelectric film may not be small. Next, if the relative permittivity of the piezoelectric film does not decrease, for example, when the piezoelectric film is used as a pressure sensor, for example, the capacity of the pressure sensor increases, and the pressure sensor The detection sensitivity of the pressure sensor decreases, and the design of the detection circuit of the pressure sensor may become difficult.
在本實施型態之膜構造體10,2θ004滿足前述式(數式1),且εr滿足前述式(數式2)。藉由使2θ004滿足前述式(數式1),於壓電膜15中,可以使其具有正方晶的結晶構造,且(001)配向的鈦鋯酸鉛的含有率變大,所以可提高壓電特性。。此外,藉由εr滿足前述式(數式2),使得相對介電常數變小,所以可增大壓力感測器的檢測感度。亦即,根據本實施型態之膜構造體10的話,可以提高壓電特性,而且可以提高使用了壓電效果的感測器的檢測感度。亦即,於具有含鈦鋯酸鉛的壓電膜的膜構造體,可以使壓電膜的壓電特性提高,而且可以提高使用了該壓電膜的壓力感測器的檢測感度。
In the
如前述非專利文獻2所記載的,在PbTiO3,為單晶狀,包含配向性等的結晶性提高的話,相對介電常數變低。亦即,PZT也與PbTiO3同樣,由於使包含薄膜的配向性的結晶性提高,而使得相對介電常數變低。亦即,膜構造體10之相對介電常數εr低到450以下,顯示包含鈦鋯酸
鉛的壓電膜之壓電膜15變成單晶狀。
As described in the aforementioned
適切者為,膜構造體10具有導電膜18的場合,導電膜13與導電膜18之間施加具有1kHz的頻率的交流電壓而測定的壓電膜15的相對介電常數為εr時,壓電膜15的εr滿足前述式(數式2)。藉由使在具有這樣的頻率的交流電壓下之相對介電常數變小,例如可以使檢測電路的時脈頻率提高,可以提高使用了膜構造體10的壓力感測器之回應速度。
Suitably, when the
膜構造體10具有導電膜18的場合,藉由導電膜13、導電膜15及導電膜18形成強介電質電容器CP1。接著,壓電膜15之εr,根據對導電膜13與導電膜18之間施加具有1kHz的頻率的交流電壓時之強介電質電容器CP1的靜電電容而算出。
When the
適切者為,壓電膜15的殘留分極值為Pr時,Pr滿足下列式(數式3)。
Suitably, when the residual extreme value of the
Pr≧28μC/cm2‧‧‧(數式3) P r ≧28μC/cm 2 ‧‧‧(Equation 3)
殘留分極值,是成為也是強介電質之壓電體的強介電特性的指標之值,但一般而言,強介電特性優異的壓電膜,壓電特性也優異。亦即,藉由壓電膜15的Pr滿足前述式(數式3),可以提高壓電膜15的強介電特性,所以壓電膜15的壓電特性也可以提高。
The residual extreme value is a value that serves as an index of the ferroelectric properties of a piezoelectric body that is also a ferroelectric material. Generally, a piezoelectric film having excellent ferroelectric properties also has excellent piezoelectric properties. That is, since P r of the
又,Pr滿足Pr≧40μC/cm2較佳,滿足Pr≧50μC/cm2更佳,滿足Pr≧55μC/cm2又更佳。Pr越大,越能提高壓電膜15的強介電特性,所以壓電膜15的壓電特性也可以更為提
高。
In addition, it is preferable that Pr satisfies Pr ≧ 40 μC/cm 2 , more preferably Pr ≧ 50 μC/cm 2 , and even more preferably Pr ≧ 55 μC/cm 2 . The larger the Pr , the more the ferroelectric properties of the
膜構造體10具有導電膜18的場合,測定顯示使施加於導電膜13與導電膜18之間的電壓改變時之壓電膜15的分極變化之分極電壓遲滯曲線(參照後述的圖6)時,使被施加於導電膜13與導電膜18之間的電壓由0往正側增加再度回到0時的分極值,為壓電膜15的殘留分極值Pr。此外,施加於導電膜13與導電膜18之間的電壓由0往負側減少再度回到0時之分極值,為壓電膜15的殘留分極值-Pr。
When the
亦即,測定顯示使施加於壓電膜15的電場改變時之壓電膜15的分極變化之分極電場遲滯曲線時,使被施加於壓電膜15的電壓由0往正側增加再度回到0時的分極,為壓電膜15的殘留分極值Pr。此外,施加於壓電膜15的電場由0往負側減少再度回到0時之分極,為壓電膜15的殘留分極值-Pr。
That is, when measuring the polarization electric field hysteresis curve showing the polarization change of the
如圖2所示,膜構造體10具有導電膜18的場合,藉由導電膜13、導電膜15及導電膜18形成強介電質電容器CP1。這樣的場合,壓電膜15之Pr,為強介電質電容器CP1的殘留分極值。
As shown in FIG. 2 , when the
適切者為壓電膜15包含壓電膜16及壓電膜17。壓電膜16,包含由被形成於膜14上的鈦鋯酸鉛所構成的複合氧化物。壓電膜17,包含由被形成於壓電膜16上的鈦鋯酸鉛所構成的複合氧化物。壓電膜16具有壓縮應力,壓電膜17具有拉伸應力。
Suitably, the
考慮壓電膜16具有拉伸應力,壓電膜17具有拉伸應力
的場合。這樣的場合,膜構造體10,在以基板11的上面11a為主面時,容易以具有往下凸出的形狀的方式變成翹曲。因此,例如使用光蝕刻技術加工膜構造體10的場合之形狀精度會降低,使得加工膜構造體10而形成的壓電元件的特性也降低。
Considering that the
此外,考慮壓電膜16具有壓縮應力,壓電膜17具有壓縮應力的場合。這樣的場合,膜構造體10,在以基板11的上面11a為主面時,容易以具有往上凸出的形狀的方式變成翹曲。因此,例如使用光蝕刻技術加工膜構造體10的場合之形狀精度會降低,使得加工膜構造體10而形成的壓電元件的特性也降低。
Also, consider a case where the
另一方面,在本實施型態,壓電膜16具有壓縮應力,壓電膜17具有拉伸應力。藉此,與壓電膜16及壓電膜17之任一都具有拉伸應力的場合相比,可以減低膜構造體10翹曲之翹曲量,與壓電膜16及壓電膜17之任一都具有壓縮應力的場合相比,可以減低膜構造體10翹曲之翹曲量。因此,例如可以提高使用光蝕刻技術加工膜構造體10的場合之形狀精度,可以提高加工膜構造體10而形成的壓電元件的特性。
On the other hand, in this embodiment, the
又,所謂壓電膜16具有壓縮應力,壓電膜17具有拉伸應力,是指例如在由膜構造體10依序除去壓電膜17及壓電膜16時,可以藉由在壓電膜17之除去前後,基板11從下為凸側變形為上為凸側,在壓電膜16之除去前後,基板11從上為凸側變形為下為凸側,而確認。
Further, that the
適切者為,壓電膜16包含以下列一般式(化學式6)表示的由鈦鋯酸鉛(PZT)構成的複合氧化物。
Suitably, the
Pb(Zr1-xTix)O3‧‧‧(化學式6) Pb(Zr 1-x Ti x )O 3 ‧‧‧(Chemical formula 6)
在此,x滿足0.32≦x≦0.52。 Here, x satisfies 0.32≦x≦0.52.
其中,x滿足0.32≦x≦0.48的場合,包含於壓電膜16的PZT,原本該具有菱面體結晶的結晶構造之組成,主要藉由來自基板11的拘束力等,具有正方晶的結晶構造,而且容易成(001)配向。接著,含PZT的壓電膜16,磊晶成長於膜14上。又,x滿足0.48<x≦0.52的場合,包含於壓電膜16的PZT,原本就是具有正方晶的結晶構造之組成的緣故,具有正方晶的結晶構造,而且成(001)配向。接著,含PZT的壓電膜16,磊晶成長於膜14上。藉此,包含於壓電膜16的鈦鋯酸鉛之分極軸的方向可以約略垂直地配向於上面11a,所以可提高壓電膜16的壓電特性。
Among them, when x satisfies 0.32≦x≦0.48, the PZT included in the
此外,適切者為,壓電膜17包含以下列一般式(化學式7)表示的由鈦鋯酸鉛(PZT)構成的複合氧化物。
Further, it is appropriate that the
Pb(Zr1-yTiy)O3‧‧‧(化學式7) Pb(Zr 1-y Ti y )O 3 ‧‧‧(Chemical formula 7)
在此,y滿足0.32≦y≦0.52。 Here, y satisfies 0.32≦y≦0.52.
其中,y滿足0.32≦y≦0.48的場合,包含於壓電膜17的PZT,原本該具有菱面體結晶的結晶構造之組成,主要藉由來自基板11的拘束力等,具有正方晶的結晶構造,而且容易成(001)配向。接著,含PZT的壓電膜17,磊晶成長於壓電膜16上。又,y滿足0.48<y≦0.52的場合,包含於壓電膜17的PZT,原本就是具有正方晶的結晶構造之
組成的緣故,具有正方晶的結晶構造,而且成(001)配向。接著,含PZT的壓電膜17,磊晶成長於壓電膜16上。藉此,包含於壓電膜17的鈦鋯酸鉛之分極軸的方向可以約略垂直地配向於上面11a,所以可提高壓電膜17的壓電特性。
Among them, when y satisfies 0.32≦y≦0.48, the PZT included in the
如使用後述的圖14所說明的,具有壓縮應力的壓電膜16,例如可以藉由濺鍍法形成。此外,說明膜構造體的製造步驟時,如使用後述的圖1所說明的,具有拉伸應力的壓電膜17,例如可以藉由溶膠凝膠法等塗布法來形成。
The
圖5係模式顯示實施型態之膜構造體所包含的2個壓電膜的剖面構造之圖。圖5係藉由掃描型電子顯微鏡(Scanning Electron Microscope:SEM)觀察藉由劈開包含於圖1所示的實施型態之膜構造體10的基板11所形成的剖面,亦即破斷面之觀察影像之中,模式顯示壓電膜16及壓電膜17。
FIG. 5 is a diagram schematically showing a cross-sectional structure of two piezoelectric films included in the film structure of the embodiment. FIG. 5 is an observation of a cross section formed by cleaving the
圖6係模式顯示實施型態之膜構造體所包含的壓電膜的分極之電場依存性之圖。圖6係模式顯示使包含於圖2所示的實施型態的膜構造體10的下部電極(導電膜13)與上部電極(導電膜18)之間的電場時的壓電膜15的分極的變化之分極電場遲滯(hysteresis)曲線之圖。
FIG. 6 is a diagram schematically showing the electric field dependence of the polarization of the piezoelectric film included in the film structure of the embodiment. FIG. 6 schematically shows polarization of the
如圖5所示,藉由濺鍍法形成壓電膜16的場合,壓電膜16,包含從壓電膜16的下面至上面為止分別被一體地形成之複數晶粒16g。此外,在基板11的主面(圖1的上面11a)內互為相鄰的2個晶粒16g之間,不容易殘留空孔或
空隙。因此,藉由集束離子束(Focused Ion Beam:FIB)法來加工而在壓電膜16形成供在SEM觀察之用的剖面的場合,該剖面容易看成是單一的剖面,晶粒16g難以被觀察到。
As shown in FIG. 5 , when the
另一方面,藉由塗布法形成壓電膜17的場合,壓電膜17包含複數層在壓電膜17的厚度方向上相互層積之層的膜17f。作為各個複數之層的膜17f,包含由1層之膜17f的下面至上面為止分別一體地形成的複數晶粒17g。此外,在壓電膜17的厚度方向上互為相鄰的2層膜17f之間,會有空孔或空隙殘留。
On the other hand, when the
如圖5所示,適切者為複數晶粒之各個具有自發分極。此自發分極,包含平行於壓電膜16的厚度方向的分極成分P1,包含於複數晶粒之各個所具有的自發分極之分極成分P1,彼此朝向相同方向。
As shown in FIG. 5, it is appropriate that each of the plurality of grains has spontaneous polarization. This spontaneous polarization includes the polarization component P1 parallel to the thickness direction of the
這樣的場合,如圖6所示,於初期狀態,壓電膜15具有大的自發分極。因此,由電場為0的起點SP起使電場往正側增加再度回到0以後,使電場往負側減少再度回到0的終點EP的場合之顯示壓電膜15的分極的電場依存性之遲滯曲線,顯示由離開原點的點為起點SP之曲線。亦即,把本實施型態的膜構造體10作為壓電元件使用的場合,在使用前,沒有必要對壓電膜15實施分極處理。
In such a case, as shown in FIG. 6 , in the initial state, the
這應該是如此般的壓電膜15於初期狀態具有大的自發分極,例如,在使用後述的圖8至圖10說明的作為RF濺鍍裝置之成膜裝置來形成壓電膜16時,電漿或者電子,不容
易受到接地電位(零電位)的影響,藉著在靶與基板之間安定封入,可以在基板蓄積大量的電荷的緣故。
This should be so that the
圖7係說明包含於實施型態的膜構造體之各層的膜磊晶成長的狀態之圖。又,在圖7模式顯示基板11、配向膜12、導電膜13、膜14及壓電膜15之各層。
7 is a diagram illustrating a state of film epitaxial growth of each layer included in the film structure of the embodiment. 7, the layers of the
包含於基板11的矽的晶格常數、包含於配向膜12的ZrO2的晶格常數、包含於導電膜13的Pt的晶格常數、包含於膜14的SRO的晶格常數、及包含於壓電膜15的PZT的晶格常數顯示於表1。
The lattice constant of silicon included in the
如表1所示,Si的晶格常數為0.543nm、ZrO2的晶格常數為0.511nm、相對於Si的晶格常數之ZrO2的晶格常數的不整合為6.1%相對較小,所以相對於Si的晶格常數之ZrO2的晶格常數的整合性是好的。因此,如圖7所示,可以使包含ZrO2的配向膜12,在包含矽單晶的基板11之(100)面構成的作為主面之上面11a上磊晶成長。亦即,可以使包含ZrO2的配向膜12,在包含矽單晶的基板11之(100)面上,以立方晶的結晶構造成(100)配向,可以提高配
向膜12的結晶性。
As shown in Table 1, the lattice constant of Si is 0.543 nm, the lattice constant of ZrO 2 is 0.511 nm, and the unconformity of the lattice constant of ZrO 2 with respect to the lattice constant of Si is relatively small at 6.1%. The conformity of the lattice constant of ZrO 2 with respect to the lattice constant of Si is good. Therefore, as shown in FIG. 7 , the
配向膜12,具有立方晶之結晶構造,且包含(100)配向之氧化鋯膜12a。這樣的場合,氧化鋯膜12a,係以沿著氧化鋯膜12a之由矽基板構成的基板11的作為主面之上面11a的<100>方向,與基板11自身的上面11a的<100>方向成為平行的方式進行配向。
The
又,氧化鋯膜12a之沿著基板11的上面11a之<100>方向,與矽基板構成的基板11自身的上面11a之<100>方向為平行,是不只包含了氧化鋯膜12a之<100>方向與沿著基板11自身的上面11a之<100>方向完全平行的場合,還包含氧化鋯膜12a的<100>方向與沿著基板11自身的上面11a之<100>方向之夾角在20°以下的場合。此外,不僅氧化鋯膜12a,其他層之膜的面內的配向也是相同的。
In addition, the <100> direction of the zirconia film 12a along the
另一方面,如表1所示,也可能是ZrO2的晶格常數為0.511nm、Pt的晶格常數為0.392nm、Pt在平面內旋轉45°的話,對角線的長度成為0.554nm,相對於ZrO2的晶格常數之該對角線長度的不整合為8.1%相對較小的緣故,而可以使包含Pt的導電膜13,在包含ZrO2的配向膜12的(100)面上磊晶成長。例如,在前述專利文獻2及前述非專利文獻1,報告了不是Pt膜而由具有與Pt的晶格常數相同程度的晶格常數(0.381nm)的LSCO所構成的LSCO膜之面內之<100>方向,與矽基板的主面內之<110>方向成平行的方式配向著。
On the other hand, as shown in Table 1, the lattice constant of ZrO 2 is 0.511 nm, the lattice constant of Pt is 0.392 nm, and when Pt is rotated by 45° in the plane, the length of the diagonal becomes 0.554 nm, Since the unconformity of the diagonal length with respect to the lattice constant of ZrO 2 is relatively small at 8.1%, the
但是,本案發明人等,首先發現了對Pt的晶格常數對
ZrO2的晶格常數之不整合高達26%,但Pt不在平面內旋轉45°,就可以使包含Pt的導電膜13在矽基板上磊晶成長。亦即,導電膜13,為具有立方晶之結晶構造,且包含(100)配向之鉑膜13a者。這樣的場合,鉑膜13a,係以沿著鉑膜13a之由矽基板構成的基板11的上面11a的<100>方向,與基板11自身的上面11a的<100>方向成為平行的方式進行配向。可知如此進行,可使包含Pt的導電膜13,在包含ZrO2的配向膜12之(100)面上,以立方晶的結晶構造成(100)配向,可以提高導電膜13的結晶性。
However, the inventors of the present application first discovered that the unconformity between the lattice constant of Pt and the lattice constant of ZrO 2 is as high as 26%, but if the Pt is not rotated by 45° in the plane, the
又,藉由調整形成ZrO2時的條件,或者形成Pt時的條件,可以在Pt在平面內旋轉45°的狀態下,亦即於基板11的主面內,Pt的<100>方向沿著Si的<110>方向的狀態下,於在包含ZrO2的配向膜12的(100)面上使包含Pt的導電膜13磊晶成長。
In addition, by adjusting the conditions for forming ZrO 2 or the conditions for forming Pt, the <100> direction of Pt can be aligned in the state where Pt is rotated by 45° in the plane, that is, in the main surface of the
此外,如表1所示,Pt的晶格常數為0.392nm、SRO的晶格常數為0.390~0.393nm、相對於Pt的晶格常數之PZT的晶格常數的不整合為0.5%以下相對較小,所以相對於Pt的晶格常數之SRO的晶格常數的整合性是好的。因此,如圖7所示,可以使包含SRO的膜14,在包含Pt的導電膜13之(100)面上磊晶成長。也就是說,可以使包含SRO的膜14,在包含Pt的導電膜13之(100)面上,以立方晶的結晶構造成(100)配向,可以提高膜14的結晶性。
In addition, as shown in Table 1, the lattice constant of Pt is 0.392 nm, the lattice constant of SRO is 0.390 to 0.393 nm, and the unconformity of the lattice constant of PZT with respect to the lattice constant of Pt is 0.5% or less. Since it is small, the integration of the lattice constant of SRO with the lattice constant of Pt is good. Therefore, as shown in FIG. 7, the
膜14,具有擬立方晶之結晶構造,且為包含(100)配向之SRO膜14a者。這樣的場合,SRO膜14a,係以沿著
SRO膜14a之由矽基板構成的基板11的上面11a的<100>方向,與基板11自身的上面11a的<100>方向成為平行的方式進行配向。
The
此外,如表1所示,SRO的晶格常數為0.390~0.393nm、PZT的晶格常數為0.411nm、相對於SRO的晶格常數之PZT的晶格常數的不整合為4.5~5.2%相對較小,所以相對於SRO的晶格常數之PZT的晶格常數的整合性是好的。因此,如圖7所示,可以使包含PZT的壓電膜15,在包含SRO的膜14之(100)面上磊晶成長。也就是說,可以使包含PZT的壓電膜15,在包含SRO的膜14之(100)面上,以正方晶顯示成(001)配向或擬立方晶的結晶構造成(100)配向,可以提高壓電膜15的結晶性。
In addition, as shown in Table 1, the lattice constant of SRO is 0.390 to 0.393 nm, the lattice constant of PZT is 0.411 nm, and the unconformity of the lattice constant of PZT with respect to the lattice constant of SRO is 4.5 to 5.2% relative to Since it is smaller, the integration of the lattice constant of PZT with respect to the lattice constant of SRO is good. Therefore, as shown in FIG. 7, the
壓電膜15,具有正方晶之結晶構造,而且為包含(001)配向的鈦鋯酸鉛膜15a者。這樣的場合,鈦鋯酸鉛膜15a,係以沿著鈦鋯酸鉛膜15a之由矽基板構成的基板11的上面11a的<100>方向,與基板11自身的上面11a的<100>方向成為平行的方式進行配向。
The
如此,本案發明人等,首先發現了鈦鋯酸鉛不在平面內旋轉45°,就可以使包含鈦鋯酸鉛的壓電膜15在矽基板上磊晶成長。這是與例如在前述專利文獻2及前述非專利文獻1所記載的面內配向的關係完全不同之關係。
In this way, the inventors of the present application first discovered that the
又,在膜14與壓電膜15之間,被形成包含鈦鋯酸鉛之膜亦可。該膜,以下列一般式(化學式8)表示,且包含以擬立方晶表示為(100)配向之複合氧化物亦可。
In addition, a film containing lead titanate zirconate may be formed between the
Pb(Zr1-vTiv)O3‧‧‧(化學式8) Pb(Zr 1-v Ti v )O 3 ‧‧‧(Chemical formula 8)
此處,v滿足0≦v≦0.1。 Here, v satisfies 0≦v≦0.1.
藉此,可以使包含PZT的壓電膜15,在包含SRO的膜14之(100)面上,進而更容易地以正方晶顯示成(001)配向或擬立方晶的結晶構造成(100)配向,可以更容易提高壓電膜15的結晶性。
In this way, the
其次,說明前述之可以使壓電膜的壓電特性提高,而且可以提高使用了該壓電膜的壓練感測器的檢測感度的膜構造體所包含的壓電膜15之中,供形成壓電膜16之成膜裝置。該成膜裝置,係藉由在真空室內濺鍍含有鈦鋯酸鉛的靶的表面而於基板的表面形成含有鈦鋯酸鉛之膜的濺鍍裝置。
Next, the
又,在以下,說明適用於作為供形成壓電膜16的成膜裝置,藉由濺鍍在真空室內與基板的下面對向配置的靶的上面而在基板的下面形成膜之所謂的面朝下(face down)型濺鍍裝置之例。但是,供形成壓電膜16的成膜裝置,藉由濺鍍在真空室內與基板的上面對向配置的靶的下面而在基板的上面形成膜之所謂的面朝上(face up)型濺鍍裝置也可以適用。
In the following, a description will be given of a so-called surface applied to a film-forming apparatus for forming the
圖8及圖9係模式顯示實施型態之成膜裝置之剖面圖。圖9係圖8的剖面圖之中擴大顯示基板保持部25及支撐部26附近。圖10係模式顯示實施型態之成膜裝置具有的基板保
持部之平面圖。
8 and 9 are cross-sectional views schematically showing the film forming apparatus of the embodiment. FIG. 9 is an enlarged cross-sectional view of FIG. 8 showing the vicinity of the
如圖8所示,成膜裝置20,具有真空室21、真空排氣部22、氣體供給部23及24、基板保持部25、支撐部26、旋轉驅動部27、基板加熱部28、防附著板29、靶保持部31、電力供給部32。基板保持部25,保持基板SB。作為基板SB,例如可以使用在前述基板11上被形成配向膜12、導電膜13及膜14的膜構造體。
As shown in FIG. 8 , the
真空室21,被設置為可真空排氣。真空排氣部22,把真空室21真空排氣。氣體供給部23,對真空室21內供給例如氬(Ar)氣體等稀有氣體。氣體供給部24,對真空室21內供給例如氧(O2)氣體或氮(N2)氣體等原料氣體。
The
真空室21,例如包含底板部21a、側板部21b、頂板部21c。於側板部21b,被形成開口OP1,於開口OP1,被連接著把真空室21進行真空排氣的真空排氣部22。作為真空排氣部22,例如可以使用冷凍泵(cryo pump)。
The
在圖8所示之例,於頂板部21c,被設有開口OP2,真空室21,包含氣密地塞住開口OP2的蓋部21d。蓋部21d,例如包含側板部21e,與頂板部21f。被形成於真空室21內的空間,與藉由側板部21e與頂板部21f包圍的空間連通。於頂板部21f,設有開口OP3。又,雖省略圖示,於側板部21b,被形成供把基板SB搬入真空室21內之用的搬入口。
In the example shown in FIG. 8, the opening OP2 is provided in the
氣體供給部23,中介著流量控制器23a被連接於氣體供給管23b,由氣體供給部23供給的稀有氣體,以流量控制器23a調整流量,由氣體供給管23b往真空室21內供給。
此外,氣體供給部24,中介著流量控制器24a被連接於氣體供給管24b,由氣體供給部24供給的原料氣體,以流量控制器24a調整流量,由氣體供給管24b往真空室21內供給。又,在圖8所示之例,圖示著氣體供給管23b與氣體供給管24b為同一的場合,但氣體供給管23b與氣體供給管24b亦可分別設置。
The
基板保持部25,在真空室21內保持基板SB。如圖8至圖10所示,基板保持部25,係在基板SB的外周部與基板保持部25接觸,而且在基板SB的中央部與基板保持部25隔離的狀態下,保持基板SB。
The
考慮基板保持部25例如於平面俯視與基板SB的下面全面重疊的場合,而且是基板保持部25例如與基板SB的下面全面接觸的場合。在這樣的場合,基板SB的中央部,不容易與基板保持部25為熱絕緣,容易受到來自基板保持部25的熱的影響。此外,基板SB的中央部容易受到基板保持部25的熱容量的影響,所以難以控制基板SB的中央部的溫度。因此,藉由基板加熱部28加熱基板SB時,基板SB的中央部之實際的溫度由目標溫度偏移掉等等理由,使得被成膜在基板SB表面的膜的結晶性等品質發生離散。
Consider, for example, a case where the
另一方面,在本實施型態,基板SB的外周部與基板保持部25接觸,但是基板SB的中央部與基板保持部25隔離。在這樣的場合,基板SB的中央部,容易與基板保持部25為熱絕緣,不容易受到來自基板保持部25的熱的影響。此外,基板SB的中央部不容易受到基板保持部25的熱容量的
影響,所以容易控制基板SB的中央部的溫度。因此,藉由基板加熱部28加熱基板SB時,可以防止或者抑制基板SB的中央部之實際的溫度由目標溫度偏移掉,可以防止或者抑制被成膜在基板SB表面的膜的結晶性等品質發生離散。
On the other hand, in the present embodiment, the outer peripheral portion of the substrate SB is in contact with the
如前所述,本實施型態之成膜裝置20,是藉由濺鍍在真空室21內與基板SB的下面對向配置的靶TG的上面而在基板SB的下面形成膜之所謂的面朝下(face down)型濺鍍裝置。這樣的場合,藉由基板保持部25例如於平面俯視不與基板SB的下面重疊,而可以在基板SB的下面的中央部形成膜。
As described above, the
基板保持部25的形狀沒有特別限定,基板保持部25,最好是包含:由絕緣性構件所構成,而且於平面俯視包圍基板SB的絕緣性包圍部25a,以及由絕緣性構件所構成,且平面俯視由絕緣包圍部25a朝向基板SB的中心側分別突出之複數突出部25b為較佳。亦即,基板保持部25,以具有所謂的五德形狀為較佳(參照圖10(A))。此外,基板保持部25,以在基板SB的下面的外周部(外緣部)與複數突出部25b之各個的上面接觸的狀態下,保持基板SB為較佳。複數之突出部25b,藉由複數突出部25b保持的基板SB的重心,於平面俯視,以被配置在依序連結的複數突出部25b而形成的多角形的內部的方式,來進行配置為較佳。
The shape of the
一個突出部25b與基板SB接觸的面積越小,越可減少成膜時之往基板SB的熱影響及電氣影響,其接觸面積以
20mm2以下為佳。總之,藉著使基板SB與突出部25b之接觸面積儘量減少,可以同時取得熱絕緣與電氣絕緣,可以使電漿的電子對基板充電,同時不使蓄積於基板的熱逃逸掉。
The smaller the contact area of one protruding
突出部25b,具有圖10(B)~(D)所示的形狀。圖10(B)為突出部25b的正面圖,圖10(C)為突出部25b的上面圖,圖10(D)為突出側25b的側面圖。突出部25b之角25b1,不尖銳,具有曲面。相對於角若尖銳,被成膜於該角的膜容易剝落,角若具有曲面的話,被成膜於該角的膜變得不容易剝離,可以減少微粒。
The protruding
又,突出部25b亦可被稱為絕緣性基板保持部,絕緣性包圍部25a與突出部25b合稱絕緣性基板保持部亦可。絕緣性包圍部25a亦可稱為第3絕緣性構件。
In addition, the protruding
在這樣的場合,在基板SB的中央部下,基板保持部25之任一部分都未被配置,所以基板SB的中央部,更容易與基板保持部25為熱絕緣,更不容易受到來自基板保持部25的熱的影響。此外,基板SB的中央部更不容易受到基板保持部25的熱容量的影響,所以更容易控制基板SB的中央部的溫度。因此,藉由基板加熱部28加熱基板SB時,可以更為防止或者抑制基板SB的中央部之實際的溫度由目標溫度偏移掉,可以更為防止或者抑制被成膜在基板SB表面的膜的結晶性等品質發生離散。
In such a case, no part of the
針對絕緣性包圍部25a的絕緣性構件,及複數突出部25b之各個絕緣性構件,雖沒有特別限定,但例如以使用
溶融石英或合成石英等石英,或者氧化鋁(alumina)為較佳。其中,基板SB由矽基板構成的場合,從與基板SB接觸也不使基板SB汙染的觀點來看,複數突出部25b之各個絕緣性構件,由石英所構成為更佳。
The insulating member of the insulating surrounding
此外,基板保持部25,進而由導電性構件所構成,包含包圍絕緣性包圍部25a的導電性包圍部25c亦可。於導電性包圍部25c的內緣部被形成階差部25d,藉由絕緣性包圍部25a的外緣部被保持於階差部25d,而形成基板保持部25亦可。
Moreover, the board|
作為基板保持部25保持的基板SB,可以使用平面俯視具有圓形形狀的晶圓所構成的基板SB。此時,基板保持部25,在旋轉軸RA1通過基板SB的表面的中心CN1(參照圖10)的狀態下,可旋轉地保持基板SB。
As the substrate SB held by the
又,可以使旋轉軸RA1延伸的方向,為與鉛直方向平行的方向。此時,被保持於基板保持部25的基板SB的表面,平行於水平面。
In addition, the direction in which the rotation axis RA1 extends may be a direction parallel to the vertical direction. At this time, the surface of the substrate SB held by the
支撐部26,被安裝於真空室21,而且在真空室21內支撐基板保持部25。支撐部26,包含被安裝於真空室21,而且在真空室21內支撐基板保持部25之導電性構件(後述之導電性構件41及42)。支撐部26,以垂直於基板SB表面的旋轉軸RA1為中心,可與基板保持部25一體旋轉地設置。旋轉驅動部27,旋轉驅動支撐部26。
The
在圖8及圖9所示之例,支撐部26,作為導電性構件,包含被安裝於真空室21的導電性構件41、及被安裝於導電
性構件41的導電性構件42。導電性構件41及42,以旋轉軸RA1為中心可與基板保持部25一體旋轉地設置。旋轉驅動部27,旋轉驅動導電性構件41及42。
In the example shown in FIGS. 8 and 9 , the
又,導電性構件42亦可稱為導電性支撐部,導電性構件42與導電性包圍部25c亦可合稱導電性支撐部。此外,導電性包圍構件25c亦可稱為第1導電性構件。此外,導電性構件42亦可稱為第2導電性構件。
In addition, the
導電性構件41,包含:具有圓筒形狀的基部41a、具有圓筒形狀,可與基部41a一體旋轉地設置,且具有比基部41a的直徑更小的直徑之軸部41b。此外,導電性構件41,具有環狀形狀,包含連接基部41a與軸部41b的接續部41c。基部41a、軸部41b及接續部41c被一體形成,基部41a、軸部41b及接續部41c例如由不銹鋼等金屬構成。
The
導電性構件41,以軸部41b由蓋部21d的開口OP3往上方突出的方式設置,由開口OP3往上方突出的軸部41b,例如藉由磁性流體密封件所構成的密封部CE1,氣密地安裝於開口OP3。此外,軸部41b,藉由密封部CE1,以能夠以垂直於基板SB表面的旋轉軸RA1為中心而旋轉地設置。因此,軸部41b,被安裝於蓋部21d亦即真空室21。此時,軸部41b,與真空室21導電連接。如前所述,真空室21例如由不銹鋼等金屬所構成,被接地。因此,導電性構件41也被接地。
The
旋轉驅動部27,例如包含馬達27a、皮帶27b與帶輪27c。軸部41b,透過帶輪27c及皮帶27b被連接於馬達27a
的旋轉軸27d。藉著馬達27a的旋轉驅動力,透過皮帶27b及帶輪27c,被傳達到軸部41b,旋轉驅動部27以旋轉軸RA1為中心,旋轉驅動導電性構件41。
The
導電性構件42,包含:具有圓筒形狀的基部42a、具有圓筒形狀,可與基部42a一體旋轉地設置,且具有比基部42a的直徑更小的直徑之軸部42b。此外,導電性構件42,具有環狀形狀,包含連接基部42a與軸部42b的接續部42c。基部42a、軸部42b及接續部42c被一體形成,基部42a、軸部42b及接續部42c例如由不銹鋼等金屬構成。
The
基部42a,以基部42a的外周面與基部41a的內周面對向的方式,設為與基部41a同心。軸部42b,以軸部42b的外周面與軸部41b的內周面對向的方式,設為與軸部41b同心。接續部42c,藉由絕緣性構件51固定於接續部41c,藉此,導電性構件42,被設為可與導電性構件41一體旋轉。作為絕緣性構件51,例如可以使用由氧化鋁(alumina)構成的絕緣性構件。
The
基部42a,使用例如由導電性構建構成的螺絲43固定於基板保持部25。因此,基板保持部25具有導電性包圍部25c的場合,亦即具有導電性的場合,導電性包圍部25c亦即基板保持部25的電位,等於基部42a亦即導電性構件42的電位。或者是,基板保持部25不具有導電性包圍部25c的場合,亦即不具有導電性的場合,基板保持部25之與螺絲43接觸的部分的電位,等於基部42a亦即導電性構件42的電位。
The
此外,如前所述,導電性構件42,藉由使用例如由導電性構件構成的螺絲43固定於基板保持部25,被安裝於真空室21的導電性構件41,成為中介著絕緣性構件51、導電性構件42以及螺絲43,支撐基板保持部25。此時,成為絕緣性構件51中介在導電性構件41與基板保持部25之間。
In addition, as described above, the
此外,導電性構件42,成為透過螺絲43支撐基板保持部25。此時,成為絕緣性構件53中介在真空室21與導電性構件42之間,導電性構件42對真空室21為電氣浮動狀態。
In addition, the
又,於導電性構件構成的螺絲43的周圍,設有絕緣性構件52。作為絕緣性構件52,可以使用例如由氧化鋁構成的絕緣性構件。此時,絕緣性構件52,被配置在導電性構件41與基板保持部25之間,所以也可以說是絕緣性構件52中介於導電性構件41與基板保持部25之間。
Moreover, the insulating
考慮絕緣性構件51未中介在導電性構件41與基板保持部25之間,導電性構件41與基板保持部25為電氣接觸的場合。這樣的場合,且基板保持部25具有導電性包圍部25c的場合,亦即具有導電性的場合,導電性包圍部25c亦即基板保持部25成為被接地的狀態,導電性包圍部25c,亦即基板保持部25的電位成為零電位。因此,在真空室21內使電漿產生而將靶TG予以濺鍍時,電漿或電子,容易受到接地電位(零電位)的影響,不容易安定地封入靶TG與基板SB之間。亦即,在形成例如鈦鋯酸鉛那樣的壓電膜的場合,成膜中之壓電膜的電荷分布難成一定,結晶性等膜的品質不易提高。
Consider the case where the insulating
此外,基板保持部25不具有導電性包圍部25c的場合,亦即不具有導電性的場合,電漿或電子,也依然容易受到接地電位(零電位)的影響,依然不容易安定地封入靶TG與基板SB之間。
In addition, when the
另一方面,在本實施型態,絕緣性構件52中介在導電性構件41與基板保持部25之間。這樣的場合,且基板保持部25具有導電性包圍部25c的場合,亦即具有導電性的場合,導電性包圍部25c,亦即基板保持部25成為電氣浮動狀態。因此,在真空室21內使電漿產生而將靶TG予以濺鍍時,電漿或電子,不容易受到接地電位(零電位)的影響,容易安定地封入靶TG與基板SB之間。亦即,在形成例如鈦鋯酸鉛那樣的壓電膜的場合,成膜中之壓電膜的電荷分布容易成一定,結晶性等膜的品質容易提高。
On the other hand, in the present embodiment, the insulating
又,絕緣性構件53亦可稱為第1絕緣性構件,絕緣性構件52亦可稱為第1絕緣性構件,絕緣性構件53與絕緣性構件52亦可合稱第1絕緣性構件。
In addition, the insulating
此外,即使基板保持部25不具有導電性包圍部25c的場合,亦即不具有導電性的場合,與導電性構件41與基板保持部25之間未中介著絕緣性構件52的場合相比,電漿或電子,不容易受到接地電位(零電位)的影響,容易安定地封入靶TG與基板SB之間。
Further, even when the
又,某個構件具有導電性,意味著該構件的電阻率例如為10-6Ωm以下的場合。另一方面,某個構件具有絕緣性,意味著該構件的電阻率例如為108Ωm以上的場合。 In addition, when a certain member has conductivity, it means that the resistivity of the member is, for example, 10 -6 Ωm or less. On the other hand, when a certain member has insulating properties, it means that the resistivity of the member is, for example, 10 8 Ωm or more.
如前所述,在真空室21與導電性構件42之間,中介著絕緣性構件52,53,導電性構件42為電氣浮動狀態。
As described above, the insulating
考慮在真空室21與導電性構件42之間未中介著絕緣性構件53,真空室21與導電性構件42為電氣接觸的狀態。這樣的場合,且基板保持部25具有導電性包圍部25c的場合,亦即具有導電性的場合,導電性包圍部25c亦即基板保持部25成為被接地的狀態,導電性包圍部25c,亦即基板保持部25的電位成為零電位。因此,在真空室21內使電漿產生而將靶予以濺鍍時,電漿或電子,容易受到接地電位(零電位)的影響,不容易安定地封入靶TG與基板SB之間。
Considering that the insulating
此外,基板保持部25不具有導電性包圍部25c的場合,亦即不具有導電性的場合,電漿或電子,也依然容易受到零電位的影響,依然不容易安定地封入靶TG與基板SB之間。
In addition, when the
另一方面,在本實施型態,在真空室21與導電性構件42之間,中介著絕緣性構件53,導電性構件42為電氣浮動狀態。這樣的場合,且基板保持部25具有導電性包圍部25c的場合,亦即具有導電性的場合,導電性包圍部25c,亦即基板保持部25成為電氣浮動狀態。因此,在真空室21內使電漿產生而將靶TG予以濺鍍時,電漿或電子,不容易受到接地電位(零電位)的影響,容易安定地封入靶TG與基板SB之間。亦即,在形成例如鈦鋯酸鉛那樣的壓電膜的場合,成膜中之壓電膜的電荷分布容易成一定,結
晶性等膜的品質容易提高。
On the other hand, in the present embodiment, the insulating
此外,即使基板保持部25不具有導電性包圍部25c的場合,亦即不具有導電性的場合,真空室21與導電性構件42之間未中介著絕緣性構件53的場合相比,電漿或電子,不容易受到接地電位(零電位)的影響,容易安定地封入靶TG與基板SB之間。
In addition, even when the
又,絕緣性構件53,亦可分別配置在例如軸部41b的上端部與軸部42b之間、軸部41b的下端部與軸部42b的下端部之間,以及接續部41c的下面與接續部42c的上面之間。作為絕緣性構件53,可以使用例如由PEEK(Poly Ether Ether Keton,聚醚醚酮)樹脂或氧化鋁構成的絕緣性構件。
In addition, the insulating
此外,設置包圍導電性構件42的軸部42b之滑移環44亦可。滑移環44的內周面,接觸於軸部42b的外周面。這樣的場合,中介著滑移環44可以自在地控制軸部42b的電位,所以能夠以使導電性構件42的電位等於一定電位的方式來進行控制。
In addition, the
如圖8及圖9所示,支撐部26,亦可包含支撐基板保持部25的導電性構件45。導電性構件45,包含:具有圓筒形狀的基部45a、具有圓筒形狀,可與基部45a一體旋轉地設置,且具有比基部45a的直徑更小的直徑之軸部45b。此外,導電性構件45,具有環狀形狀,包含連接基部45a與軸部45b的接續部45c。基部45a、軸部45b及接續部45c被一體形成,基部45a、軸部45b及接續部45c例如由不銹鋼
等金屬構成。
As shown in FIGS. 8 and 9 , the
在圖8及圖9所示之例,基部45a,以基部45a的外周面與基部42a的內周面對向的方式,設為與基部42a及基部41a同心。軸部45b,以軸部45b的外周面與軸部42b的內周面對向的方式,設為與軸部42b及軸部41b同心。接續部45c,藉由絕緣性構件54固定於接續部42c及接續部41c,藉此,導電性構件45,被設為可與導電性構件42及導電性構件41一體旋轉。
In the example shown in FIGS. 8 and 9, the
此外,如前所述,導電性構件42,藉由使用例如由導電性構件構成的螺絲43固定於基板保持部25,導電性構件45,成為中介著絕緣性構件51、導電性構件42以及螺絲43,支撐基板保持部25。此時,成為絕緣性構件52中介在導電性構件45與基板保持部25之間。
In addition, as described above, the
此外,如前所述,於導電性構件構成的螺絲43的周圍,設有絕緣性構件52。此時,絕緣性構件52,被配置在導電性構件45與基板保持部25之間,所以也可以說是絕緣性構件52中介於導電性構件45與基板保持部25之間。
Moreover, as mentioned above, the insulating
又,亦可分別在軸部42b的上端部與軸部45b之間、軸部42b的下端部與軸部45b的下端部之間,以及接續部42c的下面與接續部45c的上面之間,中介著絕緣性構件54。作為絕緣性構件54,可以使用例如由PEEK樹脂或氧化鋁構成的絕緣性構件。
In addition, between the upper end portion of the
基板加熱部28加熱基板SB。基板加熱部28,與被保持於基板保持部25的基板SB的上面對向配置,且可與支撐部
26一體旋轉地設置。作為基板加熱部28,可以使用具備例如紅外線燈的燈單元。
The
防附著板29,由被安裝在真空室21的導電性構件所構成。防附著板29,係成膜裝置20,在藉由將靶TG的表面與以濺鍍而使成膜材料附著於基板SB的表面形成膜的場合,防止成膜材料附著在真空室21內之不想要使成膜材料附著的部分者。在本實施型態,防附著板29,平面俯視係防止成膜材料附著在被配置於保持在基板保持部25的基板SB的周圍之部分。在圖8所示之例,防附著板29,係防止成膜材料附著在基板保持部25。作為構成防附著板29的導電性構件,可以使用由不銹鋼構成的導電性構件。藉此,可以藉由例如被通以冷卻水的冷卻管29a而容易地調整防附著板29的溫度,可以減低防附著板29對於被保持於基板保持部25的基板SB的溫度造成的影響。
The
此外,防附著板29被配置距離基板SB在30mm以內(較佳為25mm以內,更佳為20mm以內)的距離。
In addition, the
此外,將防附著板29進行水冷為較佳的理由如下。不把防附著板予以水冷的話,附著於防附著板的膜的硬度會變高,容易剝離,相對於此,水冷防附著板29的話,膜在防附著板29的表面成長時之熱能會下降,膜應力也變小,所以附著之膜變成不易剝離。結果,可以延長成膜裝置之維修周期。
In addition, the reason why it is preferable to water-cool the
又,防附著板29亦可稱為導電性防附著板。
In addition, the
此外,在真空室21與防附著板29之間,中介著絕緣性
構件55,防附著板29為電氣浮動狀態。又,在真空室21與絕緣性構件55之間,中介著導電性構件46,在絕緣性構件55與防附著板29之間,中介著導電性構件47,導電性構件46與導電性構件47,在絕緣性構件55中介的狀態下,使用由絕緣性構件構成的螺絲56來締結亦可。
In addition, insulating properties are interposed between the
考慮在真空室21與防附著板29之間未中介著絕緣性構件55,真空室21與防附著板29為電氣接觸的場合。這樣的場合,防附著板29成為被接地的狀態,防附著板29的電位成為零電位。因此,在真空室21內使電漿產生而將靶TG予以濺鍍時,電漿或電子,容易受到接地電位(零電位)的影響,不容易安定地封入靶TG與基板SB之間。亦即,在形成例如鈦鋯酸鉛那樣的壓電膜的場合,成膜中之壓電膜的電荷分布難成一定,結晶性等膜的品質不易提高。
Consider the case where the
此外,使配置在由基板SB起30mm以內的距離之防附著板29成為接地電位而在基板SB形成壓電膜的話,位在基板SB之端的壓電膜會白濁。使防附著板29距離比30mm更遠的話,即使防附著板為接地電位,壓電膜雖不會白濁,但在那樣遠離的位置的防附著板,無法充分發揮作為防附著板之機能。
In addition, if the
又,絕緣性構件55亦可稱為第2絕緣性構件。
In addition, the insulating
另一方面,在本實施型態,絕緣性構件55中介在真空室21與防附著板29之間。這樣的場合,防附著板29成為電氣浮動狀態。因此,在真空室21內使電漿產生而將靶TG予以濺鍍時,電漿或電子,不容易受到接地電位(零電
位)的影響,容易安定地封入靶TG與基板SB之間。亦即,在形成例如鈦鋯酸鉛那樣的壓電膜的場合,成膜中之壓電膜的電荷分布容易成一定,結晶性等膜的品質容易提高。
On the other hand, in the present embodiment, the insulating
如此,本實施型態之成膜裝置20,藉著不在基板SB的附近(具體而言由基板SB起算的距離在30mm以下,較佳為25mm以下,更佳為20mm以下的範圍內)配置導電性構件,或者即使把導電性構件配置在基板SB的附近也使成電氣浮動狀態,而可以在靶TG與基板SB之間使電漿或電子安定地封入。藉此,本案發明人等,首次發現,在形成例如鈦鋯酸鉛那樣的壓電膜的場合,成膜中之壓電膜的電荷分布容易成一定,結晶性等膜的品質提高,形成的壓電膜的強介電性及壓電性優異。藉此,於形成包含鈦鋯酸鉛的壓電膜之成膜裝置,可以形成結晶性等品質為良好的壓電膜。
In this way, in the
此外,根據本實施型態的話,藉由對真空室21為電氣浮動狀態的支撐部26來支撐基板保持部25,可以使保持於該基板保持部25的基板SB對支撐部26成電氣浮動狀態。藉著如此雙重浮動,可以使成膜時蓄積於基板SB的電荷不會逃逸至接地電位。藉此,可以於基板蓄積多量的電荷,結果,可以形成結晶性良好之膜。
Furthermore, according to the present embodiment, the
換句話說,藉著使基板SB由支撐部26浮動,可以防止電漿的電子所導致的從基板之電子洩漏。在基板蓄積多量電荷時,電漿會使來自基板的電荷逃逸至接地電位,或是
具有使其異常放電的性質,所以藉著儘可能抑制而可以形成結晶性良好之膜。
In other words, by floating the substrate SB by the
此外,藉著使被連接於接地電位的導電性構件遠離基板SB,可以使成膜於基板的壓電膜的白濁消除。 In addition, by keeping the conductive member connected to the ground potential away from the substrate SB, cloudiness of the piezoelectric film formed on the substrate can be eliminated.
靶保持部31,在真空室21內保持靶TG。此外,靶TG,包含背板(backing plate)BP1、及被固定於背板BP1的一方之側的靶材TM1。被保持於靶保持部31的靶TG的表面,與基板SB的表面對向。在圖8所示之例,靶保持部31,被設於比基板保持部25更為下方,被保持於靶保持部31的靶TG的上面與被保持於基板保持部25的基板SB的下面對向。
The
電力供給部32,對靶TG供給高頻電力。藉著藉由電力供給部32對靶TG供給高頻電力,靶TG被濺鍍。亦即,本實施型態的成膜裝置20,為RF(Radio Frequency,射頻)濺鍍裝置。
The
電力供給部32,具有高頻電源32a與整合器32b。適切者為,高頻電源32a,是把高頻電力調變為脈衝狀的附有脈衝調變機能的高頻電源。高頻電源32a,被連接於整合器32b,整合器32b,被連接於靶TG的背板BP1。又,在本實施型態,電力供給部32將高頻電力中介著靶保持部31對靶TG供給,但也可以是電力供給部32將高頻電力直接供給至靶TG。
The
此外,成膜裝置,亦可具有把藉由電力供給部32供給高頻電力時把在靶TG所產生的直流成分的電壓VDC控制在
-200V以上-80V以下之VDC控制部33。VDC控制部33,具有VDC感測器、導電連接於電力供給部32。
In addition, the film forming apparatus may include a V DC control unit 33 that controls the voltage V DC of the DC component generated at the target TG to be -200V or more and -80V or less when the high-frequency power is supplied by the
適切者為成膜裝置20,具有磁石部34與磁石旋轉驅動部35。磁石部34,例如以旋轉軸RA1為中心可旋轉地設置。磁石旋轉驅動部35,以旋轉軸RA1為中心而旋轉驅動磁石部34,藉由被旋轉驅動的磁石部34,對靶TG施加磁場。亦即,本實施型態的成膜裝置為,RF磁控管濺鍍裝置。此外,磁石部34或磁石旋轉驅動部35,是對靶TG施加磁場的磁場施加部。
A suitable one is the
適切者為,被施加磁場的靶TG的表面(在圖8所示之例為上面)的水平磁場為140~220G。這是因為靶TG的表面的水平磁場比220G更大的話,靶TG表面的能量變得太高,基板上之膜全體變白濁,比140G更小的話,靶TG的表面能變得太小,成膜速度降低而變得不實用,結晶性也降低的緣故。靶TG的表面的水平磁場為140G以上的場合,與靶TG表面之磁束密度未滿140G的場合相比,電漿或電子安定地被封入靶TG的表面附近。另一方面,靶TG的表面的水平磁場為220G以下的場合,與靶TG表面之水平磁場超過220G的場合相比,電漿或電子不會太過於集中在靶TG的表面,而以適切的密度被封入。又,靶TG的表面之磁場,以沿著靶TG的表面為佳。 Suitably, the horizontal magnetic field of the surface of the target TG to which the magnetic field is applied (the upper surface in the example shown in FIG. 8 ) is 140 to 220 G. This is because if the horizontal magnetic field on the surface of the target TG is larger than 220G, the energy on the surface of the target TG becomes too high, and the entire film on the substrate becomes cloudy. If it is smaller than 140G, the surface energy of the target TG becomes too small. The reason is that the film formation rate is lowered and it is not practical, and the crystallinity is also lowered. When the horizontal magnetic field on the surface of the target TG is 140 G or more, plasma or electrons are more stably enclosed in the vicinity of the surface of the target TG than when the magnetic flux density on the surface of the target TG is less than 140 G. On the other hand, when the horizontal magnetic field on the surface of the target TG is 220 G or less, compared with the case where the horizontal magnetic field on the surface of the target TG exceeds 220 G, the plasma or electrons are not concentrated too much on the surface of the target TG, and the Density is enclosed. In addition, the magnetic field on the surface of the target TG is preferably along the surface of the target TG.
其次,說明本實施型態之膜構造體之製造方法。圖11 至圖14係實施型態之膜構造體的製造步驟中之剖面圖。 Next, the manufacturing method of the membrane structure of this embodiment is demonstrated. Figure 11 14 is a cross-sectional view in the manufacturing process of the membrane structure of the embodiment.
首先,如圖11所示,準備基板11(步驟S1)。在步驟S1,例如準備由矽(Si)單晶所構成的矽基板之基板11。由矽單晶構成的基板11,具有立方晶的結晶構造,且具有由(100)面構成的作為主面之上面11a。基板11為矽基板的場合,於基板11之上面11a上,亦可被形成SiO2膜等氧化膜。
First, as shown in FIG. 11, the
又,作為基板11,可以使用矽基板以外的各種基板,例如SOI(Silicon on Insulator)基板、矽以外之各種半導體單晶所構成的基板、藍寶石等各種氧化物單晶所構成的基板,或者表面被形成多晶矽膜的玻璃基板構成的基板等。
In addition, as the
如圖11所示,把矽單晶構成的基板11之(100)面構成的上面11a內相互正交的2個方向作為X軸方向及Y軸方向,垂直於上面11a的方向作為Z軸方向。
As shown in FIG. 11 , two directions orthogonal to each other in the
其次,如圖12所示,於基板11上形成配向膜12(步驟S2)。在以下,於步驟S2,以使用電子束蒸鍍法形成配向膜12的場合為例進行說明,但也可以使用例如濺鍍法等各種方法來形成。
Next, as shown in FIG. 12, an
在步驟S2,首先,在把基板11配置在一定的真空氛圍中的狀態,把基板11加熱到例如700℃。
In step S2, first, the
在步驟S2,接著,藉由使用了鋯(Zr)單晶的蒸鍍材料之電子束蒸鍍法使Zr蒸發。此時,藉由蒸發的Zr在例如被加熱至700℃的基板11上與氧反應,成膜成氧化鋯
(ZrO2)膜。接著,形成作為單層膜之ZrO2膜所構成的配向膜12。
In step S2, next, Zr is evaporated by the electron beam evaporation method using the evaporation material of zirconium (Zr) single crystal. At this time, the evaporated Zr reacts with oxygen on the
配向膜12,在矽單晶構成的基板11之由(100)面構成的作為主面之上面11a上,進行磊晶成長。配向膜12,具有立方晶之結晶構造,且包含(100)配向之氧化鋯(ZrO2)。亦即,在由矽單晶構成的基板11之(100)面所構成的上面11a上,被形成由包含(100)配向的氧化鋯(ZrO2)的單層膜構成的配向膜12。
The
如使用前述之圖11所說明的,把矽單晶構成的基板11之(100)面構成的上面11a內相互正交的2個方向作為X軸方向及Y軸方向,垂直於上面11a的方向作為Z軸方向。此時,某個膜進行磊晶成長,是指該膜在X軸方向、Y軸方向及Z軸方向之任一方向均進行配向。
As described using the aforementioned FIG. 11 , two directions orthogonal to each other in the
配向膜12,具有立方晶之結晶構造,且包含(100)配向之氧化鋯膜12a(參照圖7)。這樣的場合,氧化鋯膜12a,係以沿著氧化鋯膜12a之由矽基板構成的基板11的作為主面之上面11a的<100>方向,與基板11自身的上面11a的<100>方向成為平行的方式進行配向。
The
配向膜12的膜厚,以2~100nm為佳,10~50nm為更佳。藉由具有這樣的膜厚,可以磊晶成長,形成極接近單晶的配向膜12。
The thickness of the
其次,如圖4所示,形成導電膜13(步驟S3)。
Next, as shown in FIG. 4, the
在此步驟S3,首先,形成作為磊晶成長於配向膜12上之作為下部電極的一部分之導電膜13。導電膜13由金屬構
成。作為由金屬構成的導電膜13,使用例如含鉑(Pt)的導電膜。
In this step S3, first, the
作為導電膜13,形成含Pt的導電膜的場合,於配向膜12上,以450~600℃之溫度,藉由濺鍍法,把磊晶成長之導電膜13,形成作為下部電極的一部分。含Pt的導電膜13,磊晶成長於配向膜12上。此外,包含於導電膜13的Pt,具有立方晶之結晶構造,且(100)配向。
When a conductive film containing Pt is formed as the
導電膜13,為具有立方晶之結晶構造,且包含(100)配向之鉑膜13a(參照圖7)者。這樣的場合,鉑膜13a,係以沿著鉑膜13a之由矽基板構成的基板11的上面11a的<100>方向,與基板11自身的上面11a的<100>方向成為平行的方式進行配向。
The
又,作為由金屬構成的導電膜13,替代使用含鉑(Pt)的導電膜,而改用例如含銥(Ir)的導電膜亦可。
In addition, instead of using a conductive film containing platinum (Pt), for example, a conductive film containing iridium (Ir) may be used instead as the
在此步驟S3,接著使導電膜13在450~600℃之溫度進行熱處理。具體而言,在450~600℃之溫度藉由濺鍍法形成導電膜13之後,接著在450~600℃之溫度保持10~30分鐘進行熱處理為較佳。
In this step S3, the
熱處理導電膜13的溫度未滿450℃的場合,溫度太低的緣故,無法提高包含於導電膜13的鉑的結晶性,無法提高在導電膜13上中介著膜14形成的壓電膜15的結晶性。熱處理導電膜13的溫度超過600℃的場合,溫度太高,包含於導電膜13的鉑的晶粒會成長,反而無法提高鉑的結晶性,無法提高在導電膜13上中介著膜14形成的壓電膜15的
結晶性。另一方面,在450~600℃之溫度下熱處理導電膜13的場合,可以提高包含於導電膜13的鉑的結晶性,可以提高在導電膜13上中介著膜14形成的壓電膜15的結晶性。
When the temperature for heat-treating the
此外,在450~600℃之溫度熱處理導電膜13的場合,以保持10~30分鐘進行熱處理為較佳。熱處理導電膜13的時間未滿10分鐘的場合,時間太短,無法提高包含於導電膜13的鉑的結晶性,無法提高在導電膜13上中介著膜14形成的壓電膜15的結晶性。熱處理導電膜13的溫度超過30分鐘的場合,時間太長,包含於導電膜13的鉑的晶粒會成長,反而無法提高鉑的結晶性,無法提高在導電膜13上中介著膜14形成的壓電膜15的結晶性。
In addition, when the
其次,如圖13所示,形成膜14(步驟S4)。在此步驟S4,把包含以前述一般式(化學式4)表示的複合氧化物之膜14,在導電膜13上形成。作為以前述一般式(化學式4)表示的複合氧化物,例如可以形成包含鈦酸鍶(STO)、鈦酸釕酸鍶(STRO)、或者釕鍶(SRO)的導電膜。作為以前述一般式(化學式4)表示的複合氧化物形成含SRO的導電膜的場合,在步驟S4,變成在導電膜13上形成作為下部電極的一部分之作為導電膜的膜14。又,於前述一般式(化學式4),z滿足0≦z≦1。
Next, as shown in FIG. 13, the
作為膜14,形成含STO、STRO或SRO的導電膜的場合,於導電膜13上,以600℃程度之溫度,藉由濺鍍法,把磊晶成長之膜14,形成作為下部電極的一部分。含STO、STRO或SRO的膜14,磊晶成長於導電膜13上。此
外,包含於膜14的STO、STRO或SRO,以擬立方晶表示或立方晶表示為(100)配向。
When a conductive film containing STO, STRO, or SRO is formed as the
膜14,具有擬立方晶之結晶構造,且為包含(100)配向之SRO膜14a(參照圖7)者。這樣的場合,SRO膜14a,係以沿著SRO膜14a之由矽基板構成的基板11的上面11a的<100>方向,與基板11自身的上面11a的<100>方向成為平行的方式進行配向。
The
此外,替代濺鍍法,例如可藉由溶膠凝膠法等塗布法來形成膜14。這樣的場合,在步驟S4,首先,於膜14上,藉由塗布含有鍶及釕、鍶、鈦及釕,或者鍶及鈦的溶液,形成包含以前述一般式(化學式4)表示的複合氧化物之前驅體的膜。此外,藉由塗布法形成膜14的場合,在步驟S4,接著,藉由將膜熱處理使前驅體氧化進行結晶化,而形成包含以前述一般式(化學式4)表示的複合氧化物之膜14。
In addition, instead of the sputtering method, the
其次,如圖14所示,形成壓電膜16(步驟S5)。在此步驟S5,把包含以前述一般式(化學式6)表示的由鈦鋯酸鉛(PZT)構成的複合氧化物之壓電膜16,在膜14上例如藉由濺鍍法來形成。在此,於前述一般式(化學式6),x滿足0.32≦x≦0.52。
Next, as shown in FIG. 14, the
其中,x滿足0.32≦x≦0.48的場合,包含於壓電膜16的PZT,原本該具有菱面體結晶的結晶構造之組成,主要藉由來自基板11的拘束力等,具有正方晶的結晶構造,而且容易成(001)配向。接著,含PZT的壓電膜16,磊晶
成長於膜14上。又,x滿足0.48<x≦0.52的場合,包含於壓電膜16的PZT,原本就是具有正方晶的結晶構造之組成的緣故,具有正方晶的結晶構造,而且成(001)配向。接著,含PZT的壓電膜16,磊晶成長於膜14上。藉此,包含於壓電膜16的鈦鋯酸鉛之分極軸的方向可以約略垂直地配向於上面11a,所以可提高壓電膜16的壓電特性。
Among them, when x satisfies 0.32≦x≦0.48, the PZT included in the
壓電膜16,具有正方晶之結晶構造,而且為包含(001)配向的鈦鋯酸鉛膜16a(參照圖7)者。這樣的場合,鈦鋯酸鉛膜16a,係以沿著鈦鋯酸鉛膜16a之由矽基板構成的基板11的上面11a的<100>方向,與基板11自身的上面11a的<100>方向成為平行的方式進行配向。
The
例如,藉由濺鍍法形成壓電膜16時,可以藉由電漿使包含於壓電膜16的複數晶粒16g(參照圖5)之各個被分極。亦即,包含於被成膜的壓電膜16的複數晶粒16g之各個,具有自發分極。此外,複數晶粒16g之各個具有的自發分極,包含平行於壓電膜16的厚度方向的分極成分P1(參照圖5)。接著,複數晶粒16g之各個所具有的自發分極所包含的分極成分P1,彼此朝向相同方向。結果,被形成的壓電膜16,由進行分極處理之前,作為壓電膜16全體,具有自發分極。
For example, when the
亦即,在步驟S5,藉由濺鍍法形成壓電膜16時,可以藉由電漿使壓電膜16被分極。結果,如使用圖6說明的,把本實施型態的膜構造體10作為壓電元件使用的場合,在使用前,沒有必要對壓電膜16實施分極處理。
That is, in step S5, when the
此外,在步驟S5,藉由濺鍍法形成壓電膜16時,例如,由於壓電膜16內有濺鍍粒子及氬(Ar)氣體射入而使壓電膜16膨脹,壓電膜16具有壓縮應力。
In addition, in step S5, when the
適切者為,在步驟S5,以425~475℃之溫度,且以0.29nm/s以下之成膜速度,形成包含作為複合氧化物之PZT的膜,形成由被成膜之膜所構成的壓電膜16。藉由這樣的條件,可以容易得到滿足前述式(數式1)及式(數式2)的膜構造體。
Suitably, in step S5, at a temperature of 425 to 475° C. and a film-forming speed of 0.29 nm/s or less, a film containing PZT as a composite oxide is formed, and a pressure-sensitive film composed of the film to be formed is formed.
或者,適切者為,在步驟S5,以425~475℃之溫度,且以0.29nm/s以下之第1成膜速度,形成包含作為複合氧化物之PZT的下層膜。接著,在該下層膜之上,以425~475℃之溫度,且以比第1成膜速度更小的第2成膜速度,形成包含作為複合氧化物之PZT的上層膜,形成由被成膜之下層膜及上層膜所構成的壓電膜16。藉由這樣的條件,可以容易得到滿足前述式(數式1)及式(數式2)的膜構造體。
Alternatively, it is appropriate to form an underlayer film containing PZT as a complex oxide at a temperature of 425 to 475° C. and a first film-forming rate of 0.29 nm/s or less in step S5 . Next, on the lower layer film, at a temperature of 425 to 475° C., and at a second film formation rate that is lower than the first film formation rate, an upper layer film containing PZT as a composite oxide is formed to form an upper layer film composed of a composite oxide. The
此處,說明用使用前述之圖8至圖10說明的成膜裝置20形成壓電膜16的成膜方法。
Here, a film forming method for forming the
首先,藉由靶保持部31,在真空室21內保持靶TG。
First, the target TG is held in the
其次,藉由基板保持部25,在真空室21內保持基板SB。作為基板SB,例如可以使用在前述基板11上被形成配向膜12、導電膜13及膜14的膜構造體。基板保持部25,藉由被安裝於真空室21的支撐部26支撐,在支撐部26與基板保持部25之間,或者真空室21與支撐部26之間,有絕緣
性構件51中介著。此外,基板保持部25,係在基板SB的外周部與基板保持部25接觸,而且在基板SB的中央部與基板保持部25隔離的狀態下,保持基板SB。支撐部26,包含導電性構件41及42。導電性構件41及42,以旋轉軸RA1為中心可與基板保持部25一體旋轉地設置。導電性構件42為電氣浮動狀態。藉此,電漿或電子,不容易受到接地電位(零電位)的影響,容易安定地封入靶TG與基板SB之間。
Next, the substrate SB is held in the
基板保持部25,包含:由絕緣性構件所構成,而且於平面俯視包圍基板SB的絕緣性包圍部25a,以及由絕緣性構件所構成,且平面俯視由絕緣包圍部25a朝向基板SB的中心側分別突出之複數突出部25b。基板保持部25,以在基板SB的下面的外周部(外緣部)與複數突出部25b之各個的上面接觸的狀態下,保持基板SB。藉此,藉由基板加熱部28加熱基板SB時,可以防止或者抑制基板SB的中央部之實際的溫度由目標溫度偏移掉。
The
其次,藉由基板加熱部28加熱基板SB,藉由旋轉驅動部27旋轉驅動導電性構件41及42,藉由磁石部34對靶TG施加磁場,而且對靶TG藉由電力供給部32供給高頻電力的狀態下,在真空室21內藉由濺鍍靶TG的表面而在基板SB的表面形成壓電膜16。
Next, the substrate SB is heated by the
又,成膜裝置20,在藉由將靶TG的表面與以濺鍍而使成膜材料附著於基板SB的表面形成壓電膜16者,此時,藉由被安裝於真空室21的導電性構件所構成的防附著板
29,防止成膜材料附著在基板保持部25。此防附著板29與真空室21之間,中介著絕緣性構件55,防附著板29為電氣浮動狀態。藉此,電漿或電子,不容易受到接地電位(零電位)的影響,容易安定地封入靶TG與基板SB之間。
In addition, the
其次,如圖1所示,形成壓電膜17(步驟S6)。在此步驟S6,把包含以前述一般式(化學式7)表示的由鈦鋯酸鉛(PZT)構成的複合氧化物之壓電膜17,在壓電膜16上藉由例如溶膠凝膠法等塗布法來形成。以下,說明藉由溶膠凝膠法形成壓電膜17之方法。
Next, as shown in FIG. 1, the
在步驟S6,首先,於壓電膜16上,藉由塗布含有鉛、鋯及鈦的溶液,形成包含PZT之前驅體的膜。又,塗布含有鉛、鋯及鈦的溶液的步驟,反覆複數次亦可,藉此形成包含相互層積的複數膜之膜。
In step S6, first, a film containing a PZT precursor is formed on the
在步驟S6,接著,藉由將膜熱處理使前驅體氧化進行結晶化,而形成包含PZT之壓電膜17。在此,於前述一般式(化學式7),y滿足0.32≦y≦0.48。
In step S6, next, the precursor is oxidized and crystallized by heat-treating the film to form the
其中,y滿足0.32≦y≦0.48的場合,包含於壓電膜17的PZT,原本該具有菱面體結晶的結晶構造之組成,主要藉由來自基板11的拘束力等,具有正方晶的結晶構造,而且容易成(001)配向。接著,含PZT的壓電膜17,磊晶成長於壓電膜16上。又,y滿足0.48<y≦0.52的場合,包含於壓電膜17的PZT,原本就是具有正方晶的結晶構造之組成的緣故,具有正方晶的結晶構造,而且成(001)配向。接著,含PZT的壓電膜17,磊晶成長於壓電膜16上。
藉此,包含於壓電膜17的鈦鋯酸鉛之分極軸的方向可以約略垂直地配向於上面11a,所以可提高壓電膜17的壓電特性。
Among them, when y satisfies 0.32≦y≦0.48, the PZT included in the
壓電膜17,具有正方晶之結晶構造,而且為包含(001)配向的鈦鋯酸鉛膜17a(參照圖7)者。這樣的場合,鈦鋯酸鉛膜17a,係以沿著鈦鋯酸鉛膜17a之由矽基板構成的基板11的上面11a的<100>方向,與基板11自身的上面11a的<100>方向成為平行的方式進行配向。
The
具有正方晶的結晶構造之PZT為(001)配向的場合,平行於[001]方向的分極方向,與平行於壓電膜15的厚度方向的電場方向相互平行,所以提高壓電特性。亦即,在具有正方晶的結晶構造的PZT,被施加沿著[001]方向的電場的場合,可得大的絕對值的壓電常數d33及d31。因此,可以使壓電膜15的壓電常數更為增大。又,在本說明書,針對壓電常數d31,亦有其符號原本為負,但是省略負號而以絕對值來表示的場合。
When PZT having a tetragonal crystal structure is (001) oriented, the polarization direction parallel to the [001] direction and the electric field direction parallel to the thickness direction of the
在步驟S6,例如,在熱處理時藉由使溶液中的溶媒蒸發,或者在前驅體被氧化被結晶化時藉由膜收窄,而使壓電膜17具有拉伸應力。
In step S6, for example, the
如此進行,形成包含壓電膜16及壓電膜17的壓電膜15,形成圖1所示的膜構造體10。亦即,步驟S5及步驟S6,被包含於在導電膜13上中介著膜14,形成含正方晶表示為(001)配向或擬立方晶表示為(100)配向,磊晶成長的鈦鋯酸鉛之壓電膜15的步驟。
In this way, the
其次,藉由使用θ-2θ法之X線繞射測定,測定壓電膜15的繞射圖案(步驟S7)。
Next, the diffraction pattern of the
壓電膜15,具有正方晶之結晶構造,而且在包含(001)配向的鈦鋯酸鉛的場合,在本實施型態,於根據使用CuKα線的θ-2θ法之壓電膜15的X線繞射圖案,鈦鋯酸鉛的正方晶表示之(004)面的繞射峰的繞射角度為2θ004時,2θ004滿足下列式(數式1)。
The
2θ004≦96.5°‧‧‧(數式1) 2θ 004 ≦96.5°‧‧‧(Formula 1)
藉此,鈦鋯酸鉛之正方晶表示之(004)面的間隔變長。或者是,壓電膜15中之具有正方晶結晶構造,且(001)配向之鈦鋯酸鉛的含有率,可以比壓電膜15中之具有正方晶之結晶構造,且(100)配向之鈦鋯酸鉛的含有率還要大。亦即,包含於壓電膜15的複數晶粒之各個之分極方向可以排整齊,所以可提高壓電膜15的壓電特性。
Thereby, the space|interval of the (004) plane represented by the tetragonal crystal of lead titanate zirconate becomes long. Alternatively, the content of lead titanate zirconate in the
另一方面,壓電膜15,包含以擬立方晶表示(100)配向之PZT的場合,在本實施型態,於根據使用CuKα線的θ-2θ法之壓電膜15的X線繞射圖案,鈦鋯酸鉛的擬立方晶表示之(400)面的繞射峰的繞射角度為2θ400時,2θ400滿足前述式(數式1),成為滿足替代2θ004而置換為2θ400之式(2θ400≦96.5°)。
On the other hand, when the
此外,在本實施型態,壓電膜15的相對介電常數為εr時,εr滿足下列式(數式2)。
In addition, in this embodiment, when the relative permittivity of the
εr≦450‧‧‧(數式2)。 ε r ≦450‧‧‧ (Equation 2).
藉此,把膜構造體10,例如作為使用壓電效果的壓力
感測器使用的場合,可以提高檢測感度,可以容易設計該壓力感測器之檢測電路。或者是,把膜構造體10,例如作為使用逆壓電效果的超音波振動件使用的場合,可以容易設計振盪電路。
Thereby, the
又,形成壓電膜17後,於壓電膜17上,形成作為上部電極之導電膜18(參照圖2)亦可(步驟S8)。藉此,可以對壓電膜17在厚度方向施加電場。
Further, after the
此外,形成導電膜18後,對導電膜13與導電膜18之間施加具有1kHz的頻率的交流電壓測定相對介電常數亦可(步驟S9)。
In addition, after forming the
適切者為,膜構造體10具有導電膜18的場合,導電膜13與導電膜18之間施加具有1kHz的頻率的交流電壓而測定的壓電膜15的相對介電常數為εr時,壓電膜15的εr滿足前述式(數式2)。
Suitably, when the
藉由使在具有這樣的頻率的交流電壓下之相對介電常數變小,例如可以使檢測電路的時脈頻率提高,可以提高使用了膜構造體10的壓力感測器之回應速度。
By reducing the relative permittivity under an AC voltage having such a frequency, for example, the clock frequency of the detection circuit can be increased, and the response speed of the pressure sensor using the
適切者為,壓電膜15的殘留分極值為Pr時,Pr滿足下列式(數式3)。
Suitably, when the residual extreme value of the
Pr≧28μC/cm2‧‧‧(數式3) P r ≧28μC/cm 2 ‧‧‧(Equation 3)
藉此,能提高壓電膜15的強介電特性,所以壓電膜15的壓電特性也可以提高。
Thereby, since the ferroelectric property of the
又,在膜14與壓電膜15之間,形成包含鈦鋯酸鉛之膜亦可。該膜,以前述一般式(化學式8)表示,且包含以
擬立方晶表示為(100)配向之複合氧化物亦可。
In addition, a film containing lead titanate zirconate may be formed between the
在實施型態,如圖1所示,被形成包含壓電膜16及壓電膜17之壓電膜15。但是,壓電膜15,亦可為僅包含壓電膜16。將這樣的例,作為實施型態之變形例來說明。
In the embodiment, as shown in FIG. 1 , a
圖15係實施型態的變形例之膜構造體之剖面圖。 15 is a cross-sectional view of a membrane structure according to a modification of the embodiment.
如圖15所示,本變形例之膜構造體10,具有基板11、配向膜12、導電膜13、膜14、壓電膜15。配向膜12,被形成於基板11上。導電膜13,被形成於配向膜12上。膜14,被形成於導電膜13上。壓電膜15,被形成於膜14上。壓電膜15包含壓電膜16。
As shown in FIG. 15 , the
亦即,本變形例之膜構造體10,壓電膜15不含壓電膜17(參照圖1),僅包含壓電膜16這一點以外,與實施型態的膜構造體10是相同的。
That is, the
壓電膜15,包含具有壓縮應力的壓電膜16,但不包含具有拉伸應力的壓電膜17(參照圖1)的場合,壓電膜15,與具有壓縮應力的壓電膜16以及具有拉伸應力的壓電膜17(參照圖1)都包含的場合相比,膜構造體10翹曲的翹曲量增加。但是,例如在壓電膜15的厚度很薄的場合,可以減低膜構造體10翹曲的翹曲量。因此,即使壓電膜15僅含有壓電膜16的場合,也可以提高例如使用光蝕刻技術加工膜構造體10的場合之形狀精度,可以提高加工膜構造體10而形成的壓電元件的特性。
When the
又,本變形例的膜構造體10,也與實施型態的膜構造體10同樣,具有導電膜18(參照圖2)亦可。
In addition, the
以下,根據實施例進而詳細說明本實施型態。又,本發明並不受到以下實施例的限定。 Hereinafter, the present embodiment will be further described in detail based on examples. In addition, this invention is not limited by the following Examples.
在以下,把在實施型態使用圖1說明的膜構造體10,形成為實施例1之膜構造體。實施例1之膜構造體,於根據使用CuKα線的θ-2θ法之壓電膜15的X線繞射圖案,鈦鋯酸鉛的正方晶表示之(004)面的繞射峰的繞射角度為2θ004時,2θ004滿足前述式(數式1)。此外,在實施例1之膜構造體,壓電膜15的相對介電常數為εr時,εr滿足前述式(數式2)。另一方面,2θ004為滿足前述式(數式1)的膜構造體為比較例1之膜構造體。
Hereinafter, the
以下,針對實施例1之膜構造體之形成方法進行說明。又,比較例1之膜構造體之形成方法,在使用RF濺鍍裝置形成壓電膜16時,被供給的高頻電力(功率)為2750W這一點,與被供給的高頻電力(功率)為2250W之實施例1的條件是不同的。
Hereinafter, the formation method of the membrane structure of Example 1 is demonstrated. In addition, in the method for forming the film structure of Comparative Example 1, when the
首先,如圖11所示,作為基板11,具有由(100)面構成的作為主面之上面11a,準備由6吋矽單晶構成的晶圓。
First, as shown in FIG. 11 , as the
其次,如圖12所示,於基板11上,作為配向膜12,藉由電子束蒸鍍法形成氧化鋯(ZrO2)膜。此時的條件顯示如下。
Next, as shown in FIG. 12 , a zirconium oxide (ZrO 2 ) film was formed on the
裝置:電子束蒸鍍裝置 Device: Electron beam evaporation device
壓力:7.00×10-3Pa Pressure: 7.00×10 -3 Pa
蒸鍍源:Zr+O2 Evaporation source: Zr+O 2
加速電壓/放射電流:7.5kV/1.80mA Accelerating voltage/radiation current: 7.5kV/1.80mA
厚度:24nm Thickness: 24nm
成膜速度:0.005nm/s Film forming speed: 0.005nm/s
氧氣流量:7sccm Oxygen flow: 7sccm
基板溫度:500℃ Substrate temperature: 500℃
其次,如圖4所示,於配向膜12上,作為導電膜13藉由濺鍍法形成了鉑(Pt)膜。此時的條件顯示如下。
Next, as shown in FIG. 4, on the
裝置:DC濺鍍裝置 Device: DC sputtering device
壓力:1.20×10-1Pa Pressure: 1.20×10 -1 Pa
蒸鍍源:Pt Evaporation source: Pt
電力:100W Power: 100W
厚度:150nm Thickness: 150nm
成膜速度:0.14nm/s Film forming speed: 0.14nm/s
Ar流量:16sccm Ar flow: 16sccm
基板溫度:450~600℃ Substrate temperature: 450~600℃
其次,熱處理Pt膜。此時的條件顯示如下。 Next, the Pt film is heat-treated. The conditions at this time are shown below.
裝置:DC濺鍍裝置 Device: DC sputtering device
基板溫度(熱處理溫度):450~600℃ Substrate temperature (heat treatment temperature): 450~600℃
熱處理時間:10~30分鐘 Heat treatment time: 10~30 minutes
其次,如圖13所示,於導電膜13上,作為膜14藉由濺鍍法形成了SRO膜。此時的條件顯示如下。
Next, as shown in FIG. 13 , on the
裝置:RF磁控管濺鍍裝置 Device: RF magnetron sputtering device
功率:300W Power: 300W
氣體:Ar Gas: Ar
壓力:1.8Pa Pressure: 1.8Pa
基板溫度:600℃ Substrate temperature: 600℃
成膜速度:0.11nm/s Film forming speed: 0.11nm/s
厚度:20nm Thickness: 20nm
其次,如圖14所示,於膜14上,作為壓電膜16,藉由濺鍍法形成了具有1μm的膜厚之Pb(Zr0.58Ti0.42)O3膜(PZT膜)。此時的條件顯示如下。
Next, as shown in FIG. 14, on the
裝置:RF磁控管濺鍍裝置 Device: RF magnetron sputtering device
功率:2250W Power: 2250W
氣體:Ar/O2 Gas: Ar/O 2
壓力:0.6Pa Pressure: 0.6Pa
基板溫度:425℃ Substrate temperature: 425℃
成膜速度:0.29nm/s Film forming speed: 0.29nm/s
Ar流量:66sccm Ar flow: 66sccm
氧氣流量:6sccm Oxygen flow: 6sccm
成膜時間:4200s Film forming time: 4200s
其次,如圖1所示,於壓電膜16上,作為壓電膜17,藉由塗布法形成了Pb(Zr0.58Ti0.42)O3膜(PZT膜)。此
時的條件顯示如下。
Next, as shown in FIG. 1 , a Pb(Zr 0.58 Ti 0.42 )O 3 film (PZT film) was formed on the
使Pb、Zr及Ti之有機金屬化合物以成為Pb:Zr:Ti=100+δ:58:42之組成比的方式混合,對乙醇與2-正丁氧醇之混合溶媒,以使作為Pb(Zr0.58Ti0.42)O3之濃度成為0.35mol/l的方式調整使溶解之原料溶液。針對δ,為δ=20。接著,於原料溶液,進而溶解20g的重量之K值為27~33的聚咯烷酮。 The organometallic compounds of Pb, Zr and Ti were mixed so as to have a composition ratio of Pb:Zr:Ti=100+δ:58:42, and a mixed solvent of ethanol and 2-n-butoxy alcohol was used as Pb( The raw material solution to be dissolved was adjusted so that the concentration of Zr 0.58 Ti 0.42 )O 3 was 0.35 mol/l. For δ, δ=20. Next, 20 g of polyrolidone having a K value of 27 to 33 was dissolved in the raw material solution.
其次,把調製的原料溶液之中的3ml的原料溶液,滴下至6吋晶圓構成的基板11上,以3000rpm旋轉10秒鐘,藉由把原料溶液塗布於基板11上,形成了包含前驅體的膜。接著,藉由在200℃的溫度之熱板上,將基板11載置30秒鐘,進而在450℃的溫度之熱板上,將基板11載置30秒鐘,使溶媒蒸發而使膜乾燥。其後,藉由在0.2MPa的氧(O2)氛圍中,以600~700℃熱處理60秒鐘氧化前驅體使結晶化,形成作為具有30nm膜厚之壓電膜17。
Next, 3 ml of the raw material solution in the prepared raw material solution was dropped onto the
針對實施例1及比較例1之各個,測定了被形成製作為壓電膜17之PZT膜為止的膜構造體之根據XRD法之θ-2θ頻譜。亦即,針對實施例1及比較例1之各個,進行了根據θ-2θ法之X線繞射測定。
For each of Example 1 and Comparative Example 1, the θ-2θ spectrum by the XRD method of the film structure until the PZT film formed as the
圖16至圖19之各個,係顯示被形成至PZT膜為止的膜構造體之根據XRD法之θ-2θ頻譜之例之圖。圖16至圖19之各個的圖的橫軸顯示角度2θ,圖16至圖19之各個的圖的縱軸顯示X線的強度。圖16及圖17顯示針對實施例1之結果,圖18及圖19顯示針對比較例1的結果。圖16及圖18顯示20° ≦2θ≦50°之範圍,圖17及圖19顯示90°≦2θ≦110°之範圍。 Each of FIGS. 16 to 19 is a diagram showing an example of the θ-2θ spectrum by the XRD method of the film structure formed up to the PZT film. The horizontal axis of each of the graphs of FIGS. 16 to 19 shows the angle 2θ, and the vertical axis of each of the graphs of FIGS. 16 to 19 shows the intensity of the X-ray. 16 and 17 show the results for Example 1, and FIGS. 18 and 19 show the results for Comparative Example 1. FIG. Figures 16 and 18 show 20° The range of ≦2θ≦50°, Fig. 17 and Fig. 19 show the range of 90°≦2θ≦110°.
在圖16及圖17所示之例(實施例1),於θ-2θ頻譜,相當於具有立方晶的結晶構造的Pt的(200)面及(400)面的峰,以及相當於具有正方晶顯示之PZT的(001)面、(002)面及(004)面的峰被觀測到。因此,可知在圖16及圖17所示之例(實施例1),導電膜13包含具有正方晶的結晶構造,且(100)配向之Pt,壓電膜15包含立方晶顯示為(001)配向的PZT。
In the example (Example 1) shown in FIGS. 16 and 17 , in the θ-2θ spectrum, peaks corresponding to the (200) plane and (400) plane of Pt having a cubic crystal structure, and peaks corresponding to the (200) plane and (400) plane of Pt having a cubic crystal structure The peaks of the (001) plane, (002) plane and (004) plane of PZT were observed. Therefore, in the example shown in FIGS. 16 and 17 (Example 1), the
此外,在圖17所示之例(實施例1),PZT之正方晶表示之(004)面的繞射峰之繞射角度為2θ004時,為2θ004=96.5°。因此,在圖16及圖17所示之例(實施例1),2θ004滿足2θ004≦96.5°,可知滿足前述式(數式1)。 In addition, in the example shown in FIG. 17 (Example 1), when the diffraction angle of the diffraction peak of the (004) plane represented by the tetragonal crystal of PZT is 2θ 004 , it is 2θ 004 =96.5°. Therefore, in the example (Example 1) shown in FIGS. 16 and 17 , 2θ 004 satisfies 2θ 004 ≦96.5°, and it can be seen that the aforementioned formula (Equation 1) is satisfied.
即使圖18及圖19所示之例(比較例1),也與在圖16及圖17所示之例(實施例1)同樣,於θ-2θ頻譜,相當於具有立方晶的結晶構造的Pt的(200)面及(400)面的峰,以及相當於具有正方晶顯示之PZT的(001)面、(002)面及(004)面的峰被觀測到。因此,即使在圖18及圖19所示之例(比較例1),也與在圖16及圖17所示之例(實施例1)同樣,導電膜13包含具有正方晶的結晶構造,且(100)配向之Pt,壓電膜15包含立方晶顯示為(001)配向的PZT。
Even in the example (Comparative Example 1) shown in FIGS. 18 and 19 , as in the example (Example 1) shown in FIGS. 16 and 17 , the θ-2θ spectrum corresponds to a crystal structure having a cubic crystal structure. Peaks on the (200) plane and (400) plane of Pt, and peaks corresponding to the (001) plane, (002) plane, and (004) plane of PZT having a tetragonal crystal display were observed. Therefore, even in the example shown in FIGS. 18 and 19 (Comparative Example 1), as in the example shown in FIGS. 16 and 17 (Example 1), the
但是,在圖19所示之例(比較例),與圖17所示之例 (實施例1)不同,PZT之正方晶表示之(004)面的繞射峰之繞射角度為2θ004時,為2θ004=96.7°。因此,在圖18及圖19所示之例(比較例1),可知2θ004未滿足2θ004≦96.5°,未滿足前述式(數式1)。 However, in the example shown in FIG. 19 (comparative example), unlike the example shown in FIG. 17 (Example 1), when the diffraction angle of the diffraction peak of the (004) plane represented by the tetragonal crystal of PZT is 2θ 004 , is 2θ 004 =96.7°. Therefore, in the example (Comparative Example 1) shown in FIGS. 18 and 19 , it can be seen that 2θ 004 does not satisfy 2θ 004 ≦96.5°, and the aforementioned formula (Equation 1) is not satisfied.
針對實施例1,進行根據XRD法之極點圖的測定,調查各層的膜的面內的配向之關係。圖20至圖23之各個,係顯示實施例1之膜構造體之根據XRD法之極點圖之例之圖。圖20係Si(220)面之極點圖,圖21係ZrO2(220)面之極點圖,圖22係Pt(220)面之極點圖,圖23係PZT(202)面之極點圖。 In Example 1, the measurement of the pole diagram by the XRD method was performed, and the relationship between the in-plane orientations of the films of each layer was investigated. Each of FIGS. 20-23 is a figure which shows the example of the pole figure by the XRD method of the film structure of Example 1. Fig. 20 is a pole diagram of Si(220) plane, Fig. 21 is a pole diagram of ZrO 2 (220) plane, Fig. 22 is a pole diagram of Pt(220) plane, and Fig. 23 is a pole diagram of PZT(202) plane.
如前所述,配向膜12,具有立方晶之結晶構造,且包含(100)配向之氧化鋯膜12a(參照圖7)。這樣的場合,如圖20及圖21所示,可以明白氧化鋯膜12a係以沿著氧化鋯膜12a之由矽基板構成的基板11的作為主面之上面11a的<100>方向,與基板11自身的上面11a的<100>方向成為平行的方式配向著。換句話說,可以明白氧化鋯膜12a係以沿著氧化鋯膜12a之由矽基板構成的基板11的作為主面之上面11a的<110>方向,與基板11自身的上面11a的<110>方向成為平行的方式配向著。
As described above, the
此外,導電膜13,為具有立方晶之結晶構造,且包含(100)配向之鉑膜13a者(參照圖7)。這樣的場合,如圖20及圖22所示,可以明白鉑膜13a係以沿著鉑膜13a之由矽基板構成的基板11的上面11a的<100>方向,與基板11自身的上面11a的<100>方向成為平行的方式配向著。換
句話說,可以明白鉑膜13a係以沿著鉑膜13a之由矽基板構成的基板11的上面11a的<110>方向,與基板11自身的上面11a的<110>方向成為平行的方式配向著。
In addition, the
此外,壓電膜15,具有正方晶之結晶構造,而且為包含(001)配向的鈦鋯酸鉛膜15a者。這樣的場合,如圖20及圖23所示,可以明白鈦鋯酸鉛膜15a係以沿著鈦鋯酸鉛膜15a之由矽基板構成的基板11的上面11a的<100>方向,與基板11自身的上面11a的<100>方向成為平行的方式配向著。換句話說,可以明白鈦鋯酸鉛膜15a係以沿著鈦鋯酸鉛膜15a之由矽基板構成的基板11的上面11a的<110>方向,與基板11自身的上面11a的<110>方向成為平行的方式配向著。
In addition, the
針對實施例1,在No.1至No.17之17枚晶圓之各個之上以相同條件形成至作為壓電膜17的PZT膜為止的膜構造體,測定了被形成的膜構造體之根據XRD法之θ-2θ頻譜。亦即,針對作為實施例1之17枚膜構造體,進行了根據θ-2θ法之X線繞射測定。
For Example 1, film structures up to the PZT film as the
圖24係顯示被形成於作為實施例1之No.1至No.17之17枚晶圓之各個的膜構造體之分別的X線繞射圖案之繞射角度2θ004之圖。在圖24,針對某個膜構造體之繞射角度2θ004,把晶圓中心部之繞射角度2θ004顯示於左側,晶圓外周部之繞射角度2θ004顯示於右側。 24 is a diagram showing the diffraction angle 2θ 004 of the respective X-ray diffraction patterns formed on the film structures formed on each of the 17 wafers of No. 1 to No. 17 of Example 1. FIG. In FIG. 24 , the diffraction angle 2θ 004 of a certain film structure is shown on the left side, and the diffraction angle 2θ 004 at the outer periphery of the wafer is shown on the right side.
如圖24所示,被形成於作為實施例1之17枚晶圓之各個的膜構造體,繞射角度2θ004,都比95.9°還大,而未滿 96.4°。亦即,可知作為實施例1的17枚晶圓,繞射角度2θ004,滿足前述式(數式1)。 As shown in FIG. 24 , in each of the film structures formed on the 17 wafers of Example 1, the diffraction angle 2θ 004 was larger than 95.9° and smaller than 96.4°. That is, it can be seen that the 17 wafers of Example 1 have the diffraction angle 2θ 004 , which satisfies the aforementioned formula (Equation 1).
此外,針對實施例1,進而在No.21至No.32之12枚晶圓之各個之上以相同條件形成至作為壓電膜17的PZT膜為止的膜構造體,測定了被形成的膜構造體之根據XRD法之θ-2θ頻譜。亦即,針對作為實施例1之12枚膜構造體,進行了根據θ-2θ法之X線繞射測定。
In addition, with respect to Example 1, the film structure up to the PZT film as the
圖25係顯示被形成於作為實施例1之No.21至No.32之12枚晶圓之各個的膜構造體之分別的X線繞射圖案之繞射角度2θ004之圖。在圖25,也與圖24同樣,針對某個膜構造體之繞射角度2θ004,把晶圓中心部之繞射角度2θ004顯示於左側,晶圓外周部之繞射角度2θ004顯示於右側。 25 is a diagram showing the diffraction angle 2θ 004 of the respective X-ray diffraction patterns formed on the film structures formed on each of the 12 wafers of No. 21 to No. 32 of Example 1. FIG. In FIG. 25 , similarly to FIG. 24 , the diffraction angle 2θ 004 at the center of the wafer is shown on the left, and the diffraction angle 2θ 004 at the outer periphery of the wafer is shown at the diffraction angle 2θ 004 of a certain film structure. Right.
如圖25所示,被形成於作為實施例1之12枚晶圓之各個的膜構造體,繞射角度2θ004,都比96.0°還大,而未滿96.25°。亦即,可知作為實施例1的17枚晶圓,繞射角度2θ004,滿足前述式(數式1)。 As shown in FIG. 25 , in each of the film structures formed on the 12 wafers of Example 1, the diffraction angle 2θ 004 was larger than 96.0° and smaller than 96.25°. That is, it can be seen that the 17 wafers of Example 1 have the diffraction angle 2θ 004 , which satisfies the aforementioned formula (Equation 1).
又,於圖18及圖19之θ-2θ頻譜,PZT之正方晶表示為(00n)面(n為自然數)之高角側,被觀察到峰。這應該是例如具有正方晶的結晶構造的PZT之(100)配向的部分存在著微量的含有率,該部分作為應力緩和層發揮機能的緣故。 In addition, in the θ-2θ spectrum of FIGS. 18 and 19 , the tetragonal crystal of PZT is represented by the high-angle side of the (00n) plane (n is a natural number), and a peak is observed. This is probably because, for example, a portion of PZT having a tetragonal crystal structure with a (100) orientation has a small content rate, and this portion functions as a stress relaxation layer.
其次,如圖2所示,於壓電膜15上,作為導電膜18藉由濺鍍法形成了鉑(Pt)膜。其後,對導電膜13與導電膜18之間施加電壓測定了分極的電壓依存性。
Next, as shown in FIG. 2 , a platinum (Pt) film was formed on the
圖26係顯示實施例1之膜構造體之分極的電壓依存性之圖。圖27係顯示比較例1之膜構造體之分極的電壓依存性之圖。圖26及圖27之各個的圖的橫軸顯示電壓,圖26及圖27之各個的圖的縱軸顯示分極(於以下之顯示分極的電壓依存性之圖也同樣)。 FIG. 26 is a graph showing the voltage dependence of polarization of the membrane structure of Example 1. FIG. FIG. 27 is a graph showing the voltage dependence of polarization of the membrane structure of Comparative Example 1. FIG. The horizontal axis of each of the graphs of FIGS. 26 and 27 shows voltage, and the vertical axis of each of the graphs of FIGS. 26 and 27 shows polarization (the same applies to the following graphs showing the voltage dependence of polarization).
根據圖26,於實施例1之膜構造體,相對介電常數εr為450以下(實測值450),殘留分極值Pr為28μC/cm2以上(實測值28μC/cm2)。此外,形成懸臂,使用形成的懸臂測定壓電常數d31時,壓電常數d31為200pm/V。
According to FIG. 26 , in the film structure of Example 1, the relative permittivity ε r was 450 or less (measured value 450), and the residual extreme value Pr was 28 μC/cm 2 or more (measured
另一方面,根據圖27,於比較例1之膜構造體,相對介電常數εr超過450(實測值800),殘留分極值Pr為未滿28μC/cm2(實測值10μC/cm2)。此外,與實施例1同樣測定壓電常數d31時,壓電常數d31為140pm/V。如前所述,比較例1之膜構造體之形成方法,在使用RF濺鍍裝置形成壓電膜16時,被供給的高頻電力(功率)為2750W這一點,與被供給的高頻電力為2250W之實施例1的條件是不同的。
On the other hand, according to FIG. 27 , in the film structure of Comparative Example 1, the relative permittivity ε r exceeded 450 (measured value 800), and the residual extreme value Pr was less than 28 μC/cm 2 (measured
亦即,根據實施例1及比較例1的話,可明白於本實施型態之膜構造體,形成壓電膜16時供給的高頻電力在一定範圍內時,相對介電常數εr滿足前述式(數式2),殘留分極值Pr滿足前述式(數式3)。此處,在以下,形成實施例2至實施例9以及比較例2之膜構造體,詳細調查相對介電常數εr滿足前述式(數式2),殘留分極值Pr滿足前述式(數式3)的條件。
That is, according to Example 1 and Comparative Example 1, it can be understood that in the film structure of the present embodiment, when the high-frequency power supplied when the
於實施例1之膜構造體之製造方法,除了把形成壓電膜16時的基板溫度由425℃變更為450℃以外,與實施例1之膜構造體之製造方法同樣進行,形成了實施例2之膜構造體。此外,於實施例1之膜構造體之製造方法,除了把形成壓電膜16時的基板溫度由425℃變更為475℃以外,與實施例1之膜構造體之製造方法同樣進行,形成了實施例3之膜構造體。
The production method of the film structure of Example 1 was carried out in the same manner as the production method of the film structure of Example 1, except that the substrate temperature at the time of forming the
針對實施例2及實施例3之膜構造體,對導電膜13與導電膜18之間施加電壓測定了分極的電壓依存性。圖28係顯示實施例2之膜構造體之分極的電壓依存性之圖。圖29係顯示實施例3之膜構造體之分極的電壓依存性之圖。
With respect to the film structures of Example 2 and Example 3, the voltage dependence of polarization was measured by applying a voltage between the
根據圖28,於實施例2之膜構造體,相對介電常數εr為450以下,殘留分極值Pr為28μC/cm2以上(實測值41μC/cm2)。此外,根據圖29,於實施例3之膜構造體,相對介電常數εr為450以下,殘留分極值Pr為28μC/cm2以上(實測值45μC/cm2)。
According to FIG. 28 , in the film structure of Example 2, the relative permittivity ε r was 450 or less, and the residual extreme value Pr was 28 μC/cm 2 or more (actually measured
亦即,根據實施例1至實施例3,可知被供給的高頻電力為2250W的場合,形成壓電膜16時的基板溫度在425~475℃之範圍,可得450以下之相對介電常數εr,可得28μC/cm2以上的殘留分極值Pr。又,雖省略詳細說明,但在形成壓電膜16時的基板溫度未滿425℃的場合,或者形成壓電膜16時的基板溫度超過475℃的場合,要得到450以
下的相對介電常數εr是困難的。
That is, according to Examples 1 to 3, it can be seen that when the supplied high-frequency power is 2250W, the substrate temperature when the
於實施例1之膜構造體之製造方法,除了把形成壓電膜16時被供給的高頻電力(功率)由2250W變更為2000W以外,與實施例1之膜構造體之製造方法同樣進行,形成了實施例4之膜構造體。此時,成膜速度為0.20nm/s,比實施例1之0.29nm/s還要小。
The method of manufacturing the film structure of Example 1 was performed in the same manner as the method of manufacturing the film structure of Example 1, except that the high-frequency power (power) supplied when the
此外,於實施例1之膜構造體之製造方法,除了把形成壓電膜16時被供給的高頻電力(功率)由2250W變更為1750W以外,與實施例1之膜構造體之製造方法同樣進行,形成了實施例5之膜構造體。此時,成膜速度為0.17nm/s,比實施例1之0.29nm/s還要小。
In addition, the manufacturing method of the membrane structure of Example 1 is the same as the manufacturing method of the membrane structure of Example 1, except that the high-frequency electric power (power) supplied when the
針對實施例4及實施例5之膜構造體,對導電膜13與導電膜18之間施加電壓測定了分極的電壓依存性。圖30係顯示實施例4之膜構造體之分極的電壓依存性之圖。圖31係顯示實施例5之膜構造體之分極的電壓依存性之圖。
For the film structures of Examples 4 and 5, the voltage dependence of polarization was measured by applying a voltage between the
根據圖30,於實施例4之膜構造體,相對介電常數εr為450以下,殘留分極值Pr為28μC/cm2以上(實測值45μC/cm2)。此外,根據圖31,於實施例5之膜構造體,相對介電常數εr為450以下,殘留分極值Pr為28μC/cm2以上(實測值50μC/cm2)。
According to FIG. 30 , in the film structure of Example 4, the relative permittivity ε r was 450 or less, and the residual extreme value Pr was 28 μC/cm 2 or more (actually measured
亦即,根據實施例1、實施例4及實施例5,可知基板溫度為425℃的場合,形成壓電膜16時的被供給的高頻電
力在1750~2250W之範圍,可得450以下之相對介電常數εr,可得28μC/cm2以上的殘留分極值Pr。這應該是高頻電力在1750~2250W之範圍,是高頻電力之值越小,成膜速度越慢,壓電膜16慢慢結晶成長的緣故,提高壓電膜16的單晶性,提高殘留分極值Pr的緣故。
That is, according to Example 1, Example 4 and Example 5, it can be seen that when the substrate temperature is 425° C., the high-frequency power supplied when the
於實施例1之膜構造體之製造方法,除了把形成壓電膜16時被供給的高頻電力(功率)之值由2250W變更為2500W以外,與實施例1之膜構造體之製造方法同樣進行,形成了比較例2之膜構造體。這些的條件顯示於圖32。又,圖32係針對實施例1、實施例6至實施例8、比較例1及比較例2之成膜條件以及PZT的繞射角度2θ004及相對介電常數εr等之測定結果之表。
The method of manufacturing the film structure of Example 1 is the same as the method of manufacturing the film structure of Example 1, except that the value of the high-frequency electric power (power) supplied when the
此外,於實施例1之膜構造體之製造方法,除了針對形成壓電膜16時被供給的高頻電力(功率),以使在後的步驟所供給的高頻電力比在前的步驟所供給的高頻電力之值還要小的方式,分為複數步驟變更其值而供給以外,與實施例1之膜構造體之製造方法同樣進行,形成了實施例6至實施例8之膜構造體。
In addition, in the method of manufacturing the film structure of Example 1, except for the high-frequency power (power) supplied at the time of forming the
如此,針對高頻電力,分為複數步驟變更其值而供給的理由,是因為形成壓電膜16的步驟,減少最初供給的高頻電力之值而使成膜速度變小的話,量產性會降低的緣故。另一方面,藉由僅使壓電膜16的上層部緩慢地成長,
作為全體能夠以比較快的成膜速度得到良好的單晶狀的壓電膜16,可得到良好的強介電性。
As described above, the reason why the high-frequency power is divided into a plurality of steps to change its value and supply it is because in the step of forming the
具體而言,在實施例6之膜構造體之製造方法,形成壓電膜16的步驟之中,在第1道步驟,使供給的高頻電力之值為2250W,使基板溫度為450℃,成膜時間為2100s,形成了具有500nm膜厚的Pb(Zr0.58Ti0.42)O3膜(下層PZT膜)。其次,形成壓電膜16的步驟之中,在第2道步驟,使供給的高頻電力之值為2000W,使基板溫度為450℃,成膜時間為2300s,形成了具有500nm膜厚的Pb(Zr0.58Ti0.42)O3膜(上層PZT膜)。藉此,形成由下層PZT膜及上層PZT膜所構成的壓電膜16。這些的條件顯示於圖32。又,於圖32,作為高頻電力,僅顯示形成上層PZT膜的步驟之值(2000W)。
Specifically, in the manufacturing method of the film structure of Example 6, in the step of forming the
此外,在實施例7之膜構造體之製造方法,形成壓電膜16的步驟之中,在第1道步驟,使供給的高頻電力之值為2250W,使基板溫度為450℃,成膜時間為4200s,形成了具有1μm膜厚的Pb(Zr0.58Ti0.42)O3膜(下層PZT膜)。其次,形成壓電膜16的步驟之中,在第2道步驟,使供給的高頻電力之值為1750W,使基板溫度為450℃,成膜時間為2300s,形成了具有500nm膜厚的Pb(Zr0.58Ti0.42)O3膜(中層PZT膜)。進而,形成壓電膜16的步驟之中,在第3道步驟,使供給的高頻電力之值為1750W,使基板溫度為425℃,成膜時間為2300s,形成了具有500nm膜厚的Pb(Zr0.58Ti0.42)O3膜(上層PZT膜)。藉此,形成由下
層PZT膜、中層PZT膜及上層PZT膜所構成的壓電膜16。成膜時間的合計為8800s。這些的條件顯示於圖32。又,於圖32,作為高頻電力,僅顯示形成上層PZT膜的步驟之值(1750W)。
In addition, in the method for producing the film structure of Example 7, among the steps of forming the
此外,在實施例8之膜構造體之製造方法,形成壓電膜16的步驟之中,在第1道步驟,使供給的高頻電力之值為1750W,使基板溫度為450℃,成膜時間為2300s,形成了具有500nm膜厚的Pb(Zr0.58Ti0.42)O3膜(下層PZT膜)。其次,形成壓電膜16的步驟之中,在第2道步驟,使供給的高頻電力之值為1750W,使基板溫度為425℃,成膜時間為2100s,形成了具有400nm膜厚的Pb(Zr0.58Ti0.42)O3膜(中層PZT膜)。進而,形成壓電膜16的步驟之中,在第3道步驟,使供給的高頻電力之值為1500W,使基板溫度為475℃,成膜時間為900s,形成了具有100nm膜厚的Pb(Zr0.58Ti0.42)O3膜(上層PZT膜)。藉此,形成由下層PZT膜、中層PZT膜及上層PZT膜所構成的壓電膜16。成膜時間的合計為5300s。這些的條件顯示於圖32。又,於圖32,作為高頻電力,僅顯示形成上層PZT膜的步驟之值(1500W)。
In addition, in the method for producing the film structure of Example 8, among the steps of forming the
針對實施例6至實施例8之各個,測定了被形成製作為壓電膜17之PZT膜為止的膜構造體之根據XRD法之θ-2θ頻譜。亦即,針對實施例6至實施例8之各個,進行了根據θ-2θ法之X線繞射測定。
For each of Examples 6 to 8, the θ-2θ spectrum by the XRD method of the film structure up to the PZT film formed as the
圖33至圖35之各個,係顯示被形成至PZT膜為止的膜 構造體之根據XRD法之θ-2θ頻譜之例之圖。圖33至圖35之各個的圖的橫軸顯示角度2θ,圖16至圖19之各個的圖的縱軸顯示X線的強度。圖33顯示針對實施例6之結果,圖34顯示針對實施例7之結果,圖35顯示針對實施例8的結果。此外,圖33至圖35顯示90°≦2θ≦110°之範圍。 Each of FIGS. 33 to 35 shows the film formed up to the PZT film A graph showing an example of the θ-2θ spectrum of the structure according to the XRD method. The horizontal axis of each of the graphs of FIGS. 33 to 35 shows the angle 2θ, and the vertical axis of each of the graphs of FIGS. 16 to 19 shows the intensity of X-rays. Figure 33 shows the results for Example 6, Figure 34 shows the results for Example 7, and Figure 35 shows the results for Example 8. 33 to 35 show the range of 90°≦2θ≦110°.
進而,圖17、圖19及圖33至圖35所得到的2θ004顯示於圖32。又,θ-2θ頻譜的圖示雖然省略,但是比較例2之膜構造體,也是把進行根據XRD法測定θ-2θ頻譜而得到的2θ004顯示於圖32。 Furthermore, 2θ 004 obtained in FIGS. 17 , 19 , and 33 to 35 is shown in FIG. 32 . In addition, although the illustration of the θ-2θ spectrum is omitted, in the film structure of Comparative Example 2, 2θ 004 obtained by measuring the θ-2θ spectrum by the XRD method is also shown in FIG. 32 .
如圖33至圖35及圖32所示,於實施例6之膜構造體,2θ004=96.4°,實施例7之膜構造體2θ004=96.1°,實施例8之膜構造體,2θ004=95.9°。此外,如前所述,於實施例1之膜構造體,2θ004=96.5°,雖省略詳細說明,但於實施例2至實施例5之膜構造體,2θ004滿足2θ004≦96.5°。因此,在實施例1至實施例8之膜構造體,2θ004滿足2θ004≦96.5°,可知滿足前述式(數式1)。 As shown in FIGS. 33 to 35 and 32 , in the membrane structure of Example 6, 2θ 004 =96.4°, the membrane structure of Example 7, 2θ 004 =96.1°, and the membrane structure of Example 8, 2θ 004 =95.9°. In addition, as described above, in the film structure of Example 1, 2θ 004 = 96.5°, and the detailed description is omitted, but in the film structure of Examples 2 to 5, 2θ 004 satisfies 2θ 004 ≦96.5°. Therefore, in the film structures of Examples 1 to 8, 2θ 004 satisfies 2θ 004 ≦96.5°, and it can be seen that the aforementioned formula (Equation 1) is satisfied.
此外,針對比較例2及實施例6至實施例8之膜構造體,對導電膜13與導電膜18之間施加電壓測定了分極的電壓依存性。圖36係顯示比較例2之膜構造體之分極的電壓依存性之圖。圖37係顯示實施例6之膜構造體之分極的電壓依存性之圖。圖38係顯示實施例7之膜構造體之分極的電壓依存性之圖。圖39係顯示實施例8之膜構造體之分極的電壓依存性之圖。
In addition, with respect to the film structures of Comparative Example 2 and Examples 6 to 8, the voltage dependence of polarization was measured by applying a voltage between the
根據圖36及圖32的話,於比較例2之膜構造體,相對
介電常數εr超過450(實測值580),殘留分極值Pr為未滿28μC/cm2(實測值18μC/cm2)。此外,形成懸臂,使用形成的懸臂測定壓電常數d31時,壓電常數d31為178pm/V。
According to FIGS. 36 and 32 , in the film structure of Comparative Example 2, the relative permittivity εr exceeds 450 (measured value 580), and the residual extreme value Pr is less than 28 μC/cm 2 (measured
根據圖37及圖32的話,於實施例6之膜構造體,相對介電常數εr為450以下(實測值330),殘留分極值Pr為28μC/cm2以上(實測值39μC/cm2)。此外,與比較例2同樣測定壓電常數d31時,壓電常數d31為210pm/V。
According to FIGS. 37 and 32 , in the film structure of Example 6, the relative permittivity ε r is 450 or less (measured value 330), and the residual extreme value Pr is 28 μC/cm 2 or more (measured
此外,根據圖38及圖32的話,於實施例7之膜構造體,相對介電常數εr為450以下(實測值263),殘留分極值Pr為28μC/cm2以上(實測值48μC/cm2)。此外,與比較例2同樣測定壓電常數d31時,壓電常數d31為220pm/V。
In addition, according to FIGS. 38 and 32 , in the film structure of Example 7, the relative permittivity ε r is 450 or less (actually measured value 263), and the residual extreme value P r is 28 μC/cm 2 or more (actually measured
此外,根據圖39及圖32的話,於實施例8之膜構造體,相對介電常數εr為450以下(實測值216),殘留分極值Pr為28μC/cm2以上(實測值57μC/cm2)。此外,與比較例2同樣測定壓電常數d31時,壓電常數d31為230pm/V。
In addition, according to FIGS. 39 and 32 , in the film structure of Example 8, the relative permittivity ε r was 450 or less (measured value 216), and the residual extreme value P r was 28 μC/cm 2 or more (measured
亦即,根據實施例1至實施例8的話,相對介電常數εr滿足εr≦450,殘留分極值Pr滿足Pr≧28μC/cm2,壓電常數d31滿足d31≧200pm/V,可知滿足前述式(數式1)及式(數式2)。 That is, according to Examples 1 to 8, the relative permittivity ε r satisfies ε r ≦450, the residual extreme value Pr satisfies Pr ≧ 28 μC/cm 2 , and the piezoelectric constant d 31 satisfies d 31 ≧ 200pm /V, it can be seen that the aforementioned formula (Formula 1) and formula (Formula 2) are satisfied.
如前所述,PZT也與PbTiO3同樣,由於使包含薄膜的配向性的結晶性提高,而使得相對介電常數變低。亦即,於實施例1至實施例8,相對介電常數εr低到450以下,顯示壓電膜15變成單晶狀。
As described above, PZT also lowers the relative permittivity by improving the crystallinity including the orientation of the thin film, similarly to PbTiO 3 . That is, in Examples 1 to 8, the relative permittivity ε r was as low as 450 or less, indicating that the
所謂壓電現象,是對壓電體施加應力時,藉由壓電體 的晶格形變,而於壓電體產生因應於該形變的電荷的現象。亦即,壓電形變,係把產生於壓電體的電荷密度,除以施加在壓電體的應力之值,在壓電體為強介電質的場合,比例於殘留分極值。 The so-called piezoelectric phenomenon is that when stress is applied to the piezoelectric body, the The crystal lattice is deformed, and the piezoelectric body generates charges corresponding to the deformation. That is, the piezoelectric deformation is a value obtained by dividing the charge density generated in the piezoelectric body by the stress applied to the piezoelectric body, and in the case of the piezoelectric body being a ferroelectric, it is proportional to the residual extreme value.
此外,由介電體,與被形成在介電體上下的2個電極所構成的電容器的容量,比例於介電體的相對介電常數與2個電極之各個的面積,但與介電體的厚度,亦即2個電極間的距離成反比。藉由此情形,與前述之對壓電體施加應力時產生電荷的情形,使得壓電形變比例於壓電體構成的介電體之相對介電常數。 In addition, the capacitance of a capacitor composed of a dielectric body and two electrodes formed above and below the dielectric body is proportional to the relative permittivity of the dielectric body and the area of each of the two electrodes, but is proportional to the dielectric body's relative permittivity and the area of each of the two electrodes. The thickness of , that is, the distance between the two electrodes is inversely proportional. In this case, and the above-mentioned case where electric charges are generated when stress is applied to the piezoelectric body, the piezoelectric deformation ratio is proportional to the relative permittivity of the dielectric body composed of the piezoelectric body.
比較例1及比較例2以及實施例1及實施例6至實施例8,在求取殘留分極值Pr與相對介電常數εr之積(Pr‧εr)時,如圖32所示,Pr‧εr之值與壓電常數d31成良好的比例關係。亦即,如前所述,確認了壓電形變,比例於殘留分極值,而且比例於相對介電常數。 In Comparative Example 1 and Comparative Example 2, and Example 1 and Example 6 to Example 8, when the product of the residual extreme value Pr and the relative permittivity ε r (P r ·ε r ) was obtained, as shown in Fig. 32 It can be seen that the value of P r ·ε r has a good proportional relationship with the piezoelectric constant d 31 . That is, as described above, it was confirmed that the piezoelectric strain is proportional to the residual extreme value and also proportional to the relative permittivity.
又,破斷面藉由SEM進行了觀察。其結果,省略詳細說明,相對於在實施例1及實施例6至實施例8,壓電膜16具有良好的單晶性,在比較例1及比較例2,於壓電膜16,於沿著主面的方向相鄰的2個晶粒之間,被觀察到延伸於壓電膜16的厚度方向的龜裂(開裂),可知壓電膜15的單晶性降低。在圖32,被觀察到龜裂的場合以×表示,未被觀察到龜裂的場合以○表示。
In addition, the fractured surface was observed by SEM. As a result, detailed descriptions are omitted, but the
由以上結果,可知膜構造體具有的壓電膜,藉由滿足前述式(數式1)及式(數式2),可得由高品質的單晶膜 構成的壓電膜,減低壓電膜的相對介電常數,而且可提高壓電膜的壓電特性,所以可使壓電膜的壓電特性提高,而且提高使用了該壓電膜之壓力感測器的檢測感度。 From the above results, it can be seen that the piezoelectric film included in the film structure can obtain a high-quality single crystal film by satisfying the above-mentioned equations (Equation 1) and Equation (Equation 2). The piezoelectric film formed can reduce the relative permittivity of the piezoelectric film and improve the piezoelectric characteristics of the piezoelectric film, so the piezoelectric characteristics of the piezoelectric film can be improved, and the pressure sensitivity of the piezoelectric film can be improved. The detection sensitivity of the detector.
與實施例1之膜構造體之製造方法同樣進行,形成了實施例9之膜構造體。此外,於實施例1之膜構造體之製造方法,除了把PZT的組成由x=0.42變更為x=0.48以外,與實施例1之膜構造體之製造方法同樣進行,形成了實施例10之膜構造體。針對實施例9及實施例10之膜構造體,對導電膜13與導電膜18之間施加電壓測定了分極的電壓依存性。圖40係顯示實施例9之膜構造體之分極的電壓依存性之圖。圖41係顯示實施例10之膜構造體之分極的電壓依存性之圖。
The membrane structure of Example 9 was formed in the same manner as in the method for producing the membrane structure of Example 1. In addition, the method for producing the film structure of Example 1 was performed in the same manner as the method for producing the film structure of Example 1, except that the composition of PZT was changed from x=0.42 to x=0.48, to form the film structure of Example 10. Membrane constructs. For the film structures of Examples 9 and 10, the voltage dependence of polarization was measured by applying a voltage between the
此外,針對實施例9及實施例10之測定強介電特性及壓電特性等的結果,顯示於表2。於表2,顯示殘留分極值Pr、相對介電常數εr、介電正切tanδ、壓電常數d31、壓電常數g31、壓電常數e31及膜厚。又,在表2,針對壓電常數d31、壓電常數g31及壓電常數e31,不是絕對值而是標以正負號表示。 In addition, Table 2 shows the results of measuring the ferroelectric properties, piezoelectric properties, and the like of Examples 9 and 10. In Table 2, the residual extreme value P r , the relative dielectric constant ε r , the dielectric tangent tanδ, the piezoelectric constant d 31 , the piezoelectric constant g 31 , the piezoelectric constant e 31 , and the film thickness are shown. In addition, in Table 2, the piezoelectric constant d 31 , the piezoelectric constant g 31 , and the piezoelectric constant e 31 are not absolute values, but are represented by signs.
如圖40及表2所示,在x=0.42(實施例9)的場合,殘留分極值Pr為50μC/cm2,相對介電常數εr為200,tanδ為0.01%,壓電常數d31為-200pm/V,壓電常數g31為-100×103Vm/N,壓電常數e31為-25C/m2,得到良好的特性。此外,如圖41及表2所示,即使在x=0.48的場合,殘留分極值Pr為60μC/cm2,相對介電常數εr為300,tanδ為0.01%,壓電常數d31為-250pm/V,壓電常數g31為-80×103Vm/N,壓電常數e31為-27C/m2,得到良好的特性。此外,雖省略詳細的說明,但在0.32≦x≦0.52之範圍變更x之值的場合,也可得到良好的特性。由以上結果,可清楚得知包含x=0.42、0.48的場合,在0.32≦x≦0.52之範圍可得良好的特性。
As shown in Fig. 40 and Table 2, when x=0.42 (Example 9 ) , the residual fractional extreme value Pr is 50 μC/cm 2 , the relative permittivity ε r is 200, the tanδ is 0.01%, and the piezoelectric constant d 31 was -200 pm/V, the piezoelectric constant g 31 was -100×10 3 Vm/N, and the piezoelectric constant e 31 was -25 C/m 2 , and good characteristics were obtained. In addition, as shown in Fig. 41 and Table 2, even in the case of x=0.48, the residual extreme value P r is 60 μC/cm 2 , the relative permittivity ε r is 300, the tanδ is 0.01%, and the piezoelectric constant d 31 The piezoelectric
以上根據其實施型態具體說明由本案發明人所完成的發明,但本發明並不以前述實施型態為限,在不逸脫於其要旨的範圍當然可以進行種種的變更。 As mentioned above, the invention made by the present inventors has been specifically described based on its embodiments, but the present invention is not limited to the above-mentioned embodiments, and various modifications can of course be made without departing from the gist of the invention.
在本發明的思想的範圍,只要是熟悉該項技藝者(業者),就可能會想到各種變更例及修正例,針對這些變更例及修正例也應該理解為屬於本發明的範圍。 Within the scope of the idea of the present invention, those skilled in the art (manufacturers) can think of various modifications and corrections, and these modifications and corrections should be understood as belonging to the scope of the present invention.
例如,對於前述各實施型態,熟悉該項技藝者進行適當的、構成要素的追加、削減或者設計變更者,或者進行了步驟的追加、省略或者條件變更者,只要具備本發明之要旨,都包含於本發明的範圍。 For example, for each of the above-mentioned embodiments, those skilled in the art make appropriate additions, deletions, or design changes of constituent elements, or additions, omissions, or conditions change of steps, as long as the gist of the present invention is satisfied. included in the scope of the present invention.
20:成膜裝置 20: Film forming device
21:真空室 21: Vacuum Chamber
21a:底板部 21a: Bottom plate
21b、21e:側板部 21b, 21e: side plate
21c、21f:頂板部 21c, 21f: top plate
21d:蓋部 21d: Cover
22:真空排氣部 22: Vacuum exhaust part
23、24:氣體供給部 23, 24: Gas supply part
23a、24a:流量控制器 23a, 24a: flow controller
23b、24b:氣體供給管 23b, 24b: Gas supply pipes
25:基板保持部 25: Substrate holding part
26:支撐部 26: Support Department
27:旋轉驅動部 27: Rotary drive part
28:基板加熱部 28: Substrate heating section
29:防附著板 29: Anti-adhesion plate
29a:冷卻管 29a: Cooling pipe
31:靶保持部 31: Target holding part
32:電力供給部 32: Power Supply Department
32a:高頻電源 32a: High frequency power supply
32b:整合器 32b: Integrator
33:VDC控制部 33: V DC control part
34:磁石部 34: Magnet Department
35:磁石旋轉驅動部 35: Magnet rotating drive part
41、42、45、46、47:導電性構件 41, 42, 45, 46, 47: Conductive members
43、56:螺絲 43, 56: Screws
44:滑移環 44: Slip Ring
51、52、53、54、55:絕緣性構件 51, 52, 53, 54, 55: Insulating members
BP1:背板(backing:plate) BP1: backing plate (backing: plate)
CE1:密封部 CE1: Sealing part
OP1、OP2、OP3:開口 OP1, OP2, OP3: Opening
RA1:旋轉軸 RA1: Rotary axis
SB:基板 SB: Substrate
TG:靶 TG: target
TM1:靶材 TM1: Target
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