WO2012038926A1 - Method of depositing a layer of a material on a substrate - Google Patents
Method of depositing a layer of a material on a substrate Download PDFInfo
- Publication number
- WO2012038926A1 WO2012038926A1 PCT/IB2011/054182 IB2011054182W WO2012038926A1 WO 2012038926 A1 WO2012038926 A1 WO 2012038926A1 IB 2011054182 W IB2011054182 W IB 2011054182W WO 2012038926 A1 WO2012038926 A1 WO 2012038926A1
- Authority
- WO
- WIPO (PCT)
- Prior art keywords
- layer
- substrate
- platinum
- target
- deposition
- Prior art date
Links
- 239000000758 substrate Substances 0.000 title claims abstract description 69
- 238000000034 method Methods 0.000 title claims abstract description 46
- 238000000151 deposition Methods 0.000 title claims description 59
- 239000000463 material Substances 0.000 title claims description 46
- 230000008021 deposition Effects 0.000 claims abstract description 52
- 229910052594 sapphire Inorganic materials 0.000 claims abstract description 4
- 239000010980 sapphire Substances 0.000 claims abstract description 4
- 239000010410 layer Substances 0.000 claims description 122
- BASFCYQUMIYNBI-UHFFFAOYSA-N platinum Chemical compound [Pt] BASFCYQUMIYNBI-UHFFFAOYSA-N 0.000 claims description 48
- 229910052697 platinum Inorganic materials 0.000 claims description 24
- 230000004913 activation Effects 0.000 claims description 15
- 239000002178 crystalline material Substances 0.000 claims description 15
- 239000003990 capacitor Substances 0.000 claims description 8
- 239000000203 mixture Substances 0.000 claims description 7
- 238000001755 magnetron sputter deposition Methods 0.000 claims description 6
- 239000002245 particle Substances 0.000 claims description 5
- 238000004519 manufacturing process Methods 0.000 claims description 4
- 239000002344 surface layer Substances 0.000 claims description 3
- 238000004140 cleaning Methods 0.000 claims 2
- 238000010894 electron beam technology Methods 0.000 claims 1
- 230000005855 radiation Effects 0.000 claims 1
- 229910019351 (BaxSr1-x)TiO3 Inorganic materials 0.000 abstract 1
- 239000013078 crystal Substances 0.000 description 17
- 239000007789 gas Substances 0.000 description 17
- 238000010438 heat treatment Methods 0.000 description 8
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 description 5
- 239000004020 conductor Substances 0.000 description 5
- 239000010408 film Substances 0.000 description 5
- 230000003287 optical effect Effects 0.000 description 5
- 239000010409 thin film Substances 0.000 description 5
- XKRFYHLGVUSROY-UHFFFAOYSA-N Argon Chemical compound [Ar] XKRFYHLGVUSROY-UHFFFAOYSA-N 0.000 description 4
- 239000012777 electrically insulating material Substances 0.000 description 4
- 239000012535 impurity Substances 0.000 description 4
- OKKJLVBELUTLKV-UHFFFAOYSA-N Methanol Chemical compound OC OKKJLVBELUTLKV-UHFFFAOYSA-N 0.000 description 3
- 238000002679 ablation Methods 0.000 description 3
- 239000001301 oxygen Substances 0.000 description 3
- 229910052760 oxygen Inorganic materials 0.000 description 3
- 238000002360 preparation method Methods 0.000 description 3
- 238000001228 spectrum Methods 0.000 description 3
- CSCPPACGZOOCGX-UHFFFAOYSA-N Acetone Chemical compound CC(C)=O CSCPPACGZOOCGX-UHFFFAOYSA-N 0.000 description 2
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 2
- 229910052786 argon Inorganic materials 0.000 description 2
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 description 2
- 230000003750 conditioning effect Effects 0.000 description 2
- 239000011521 glass Substances 0.000 description 2
- 238000005259 measurement Methods 0.000 description 2
- 229910052751 metal Inorganic materials 0.000 description 2
- 239000002184 metal Substances 0.000 description 2
- 230000004048 modification Effects 0.000 description 2
- 238000012986 modification Methods 0.000 description 2
- 229910052757 nitrogen Inorganic materials 0.000 description 2
- 230000008569 process Effects 0.000 description 2
- 238000007741 pulsed electron deposition Methods 0.000 description 2
- 239000000126 substance Substances 0.000 description 2
- 238000009997 thermal pre-treatment Methods 0.000 description 2
- VYZAMTAEIAYCRO-UHFFFAOYSA-N Chromium Chemical compound [Cr] VYZAMTAEIAYCRO-UHFFFAOYSA-N 0.000 description 1
- ZOKXTWBITQBERF-UHFFFAOYSA-N Molybdenum Chemical compound [Mo] ZOKXTWBITQBERF-UHFFFAOYSA-N 0.000 description 1
- RTAQQCXQSZGOHL-UHFFFAOYSA-N Titanium Chemical compound [Ti] RTAQQCXQSZGOHL-UHFFFAOYSA-N 0.000 description 1
- 230000002411 adverse Effects 0.000 description 1
- 238000004220 aggregation Methods 0.000 description 1
- 230000002776 aggregation Effects 0.000 description 1
- PNEYBMLMFCGWSK-UHFFFAOYSA-N aluminium oxide Inorganic materials [O-2].[O-2].[O-2].[Al+3].[Al+3] PNEYBMLMFCGWSK-UHFFFAOYSA-N 0.000 description 1
- 239000003708 ampul Substances 0.000 description 1
- 238000000089 atomic force micrograph Methods 0.000 description 1
- 238000004630 atomic force microscopy Methods 0.000 description 1
- 239000000919 ceramic Substances 0.000 description 1
- 238000005229 chemical vapour deposition Methods 0.000 description 1
- 229910052804 chromium Inorganic materials 0.000 description 1
- 239000011651 chromium Substances 0.000 description 1
- 239000011248 coating agent Substances 0.000 description 1
- 238000000576 coating method Methods 0.000 description 1
- 238000010276 construction Methods 0.000 description 1
- 230000001419 dependent effect Effects 0.000 description 1
- 239000003989 dielectric material Substances 0.000 description 1
- 239000012153 distilled water Substances 0.000 description 1
- 238000009826 distribution Methods 0.000 description 1
- 230000005611 electricity Effects 0.000 description 1
- 238000000313 electron-beam-induced deposition Methods 0.000 description 1
- 230000004907 flux Effects 0.000 description 1
- 239000001307 helium Substances 0.000 description 1
- 229910052734 helium Inorganic materials 0.000 description 1
- SWQJXJOGLNCZEY-UHFFFAOYSA-N helium atom Chemical compound [He] SWQJXJOGLNCZEY-UHFFFAOYSA-N 0.000 description 1
- 229910052742 iron Inorganic materials 0.000 description 1
- 238000000608 laser ablation Methods 0.000 description 1
- 229910052750 molybdenum Inorganic materials 0.000 description 1
- 239000011733 molybdenum Substances 0.000 description 1
- 239000012811 non-conductive material Substances 0.000 description 1
- 238000000399 optical microscopy Methods 0.000 description 1
- 230000003647 oxidation Effects 0.000 description 1
- 238000007254 oxidation reaction Methods 0.000 description 1
- 239000013618 particulate matter Substances 0.000 description 1
- 238000009832 plasma treatment Methods 0.000 description 1
- 238000005086 pumping Methods 0.000 description 1
- 239000010453 quartz Substances 0.000 description 1
- 230000009467 reduction Effects 0.000 description 1
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N silicon dioxide Inorganic materials O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 1
- 230000002269 spontaneous effect Effects 0.000 description 1
- 230000006641 stabilisation Effects 0.000 description 1
- 238000011105 stabilization Methods 0.000 description 1
- 229910001220 stainless steel Inorganic materials 0.000 description 1
- 239000010935 stainless steel Substances 0.000 description 1
- 238000003860 storage Methods 0.000 description 1
- 229910052719 titanium Inorganic materials 0.000 description 1
- 239000010936 titanium Substances 0.000 description 1
- WFKWXMTUELFFGS-UHFFFAOYSA-N tungsten Chemical compound [W] WFKWXMTUELFFGS-UHFFFAOYSA-N 0.000 description 1
- 229910052721 tungsten Inorganic materials 0.000 description 1
- 239000010937 tungsten Substances 0.000 description 1
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Chemical compound O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 1
- 238000007704 wet chemistry method Methods 0.000 description 1
- 229910052724 xenon Inorganic materials 0.000 description 1
- FHNFHKCVQCLJFQ-UHFFFAOYSA-N xenon atom Chemical compound [Xe] FHNFHKCVQCLJFQ-UHFFFAOYSA-N 0.000 description 1
Classifications
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01G—CAPACITORS; CAPACITORS, RECTIFIERS, DETECTORS, SWITCHING DEVICES, LIGHT-SENSITIVE OR TEMPERATURE-SENSITIVE DEVICES OF THE ELECTROLYTIC TYPE
- H01G4/00—Fixed capacitors; Processes of their manufacture
- H01G4/002—Details
- H01G4/018—Dielectrics
- H01G4/06—Solid dielectrics
- H01G4/08—Inorganic dielectrics
- H01G4/12—Ceramic dielectrics
- H01G4/1209—Ceramic dielectrics characterised by the ceramic dielectric material
- H01G4/1218—Ceramic dielectrics characterised by the ceramic dielectric material based on titanium oxides or titanates
- H01G4/1227—Ceramic dielectrics characterised by the ceramic dielectric material based on titanium oxides or titanates based on alkaline earth titanates
-
- 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
- C23C14/24—Vacuum evaporation
- C23C14/28—Vacuum evaporation by wave energy or particle radiation
- C23C14/30—Vacuum evaporation by wave energy or particle radiation by electron bombardment
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01G—CAPACITORS; CAPACITORS, RECTIFIERS, DETECTORS, SWITCHING DEVICES, LIGHT-SENSITIVE OR TEMPERATURE-SENSITIVE DEVICES OF THE ELECTROLYTIC TYPE
- H01G4/00—Fixed capacitors; Processes of their manufacture
- H01G4/002—Details
- H01G4/018—Dielectrics
- H01G4/06—Solid dielectrics
- H01G4/08—Inorganic dielectrics
- H01G4/085—Vapour deposited
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01G—CAPACITORS; CAPACITORS, RECTIFIERS, DETECTORS, SWITCHING DEVICES, LIGHT-SENSITIVE OR TEMPERATURE-SENSITIVE DEVICES OF THE ELECTROLYTIC TYPE
- H01G4/00—Fixed capacitors; Processes of their manufacture
- H01G4/33—Thin- or thick-film capacitors
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J3/00—Details of electron-optical or ion-optical arrangements or of ion traps common to two or more basic types of discharge tubes or lamps
- H01J3/02—Electron guns
- H01J3/025—Electron guns using a discharge in a gas or a vapour as electron source
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/02104—Forming layers
- H01L21/02107—Forming insulating materials on a substrate
- H01L21/02109—Forming insulating materials on a substrate characterised by the type of layer, e.g. type of material, porous/non-porous, pre-cursors, mixtures or laminates
- H01L21/02112—Forming insulating materials on a substrate characterised by the type of layer, e.g. type of material, porous/non-porous, pre-cursors, mixtures or laminates characterised by the material of the layer
- H01L21/02172—Forming insulating materials on a substrate characterised by the type of layer, e.g. type of material, porous/non-porous, pre-cursors, mixtures or laminates characterised by the material of the layer the material containing at least one metal element, e.g. metal oxides, metal nitrides, metal oxynitrides or metal carbides
- H01L21/02197—Forming insulating materials on a substrate characterised by the type of layer, e.g. type of material, porous/non-porous, pre-cursors, mixtures or laminates characterised by the material of the layer the material containing at least one metal element, e.g. metal oxides, metal nitrides, metal oxynitrides or metal carbides the material having a perovskite structure, e.g. BaTiO3
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/02104—Forming layers
- H01L21/02107—Forming insulating materials on a substrate
- H01L21/02225—Forming insulating materials on a substrate characterised by the process for the formation of the insulating layer
- H01L21/0226—Forming insulating materials on a substrate characterised by the process for the formation of the insulating layer formation by a deposition process
- H01L21/02263—Forming insulating materials on a substrate characterised by the process for the formation of the insulating layer formation by a deposition process deposition from the gas or vapour phase
- H01L21/02266—Forming insulating materials on a substrate characterised by the process for the formation of the insulating layer formation by a deposition process deposition from the gas or vapour phase deposition by physical ablation of a target, e.g. sputtering, reactive sputtering, physical vapour deposition or pulsed laser deposition
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L28/00—Passive two-terminal components without a potential-jump or surface barrier for integrated circuits; Details thereof; Multistep manufacturing processes therefor
- H01L28/40—Capacitors
- H01L28/55—Capacitors with a dielectric comprising a perovskite structure material
Definitions
- the present invention relates to a method for the deposition of a material on a substrate, a method of manufacturing an electronic device and an electronic device.
- the ferroelectric materials of perovskite family (Bai_ x Sr x )Ti0 3 (BST) have a very high dielectric constant, low dielectric loss, a very large "energy gap” and good structural stability. These substances prove to be the perfect materials for a wide range of applications including “dynamic random access memory (DRAM) , microwave phase shifters, integrated circuits for microwave and millimeter- range electro-optical devices. Other applications include switches and optical switches, planar waveguides, non-cooled infrared detectors and, above all, the super-capacitors for storage of electricity.
- DRAM dynamic random access memory
- Other applications include switches and optical switches, planar waveguides, non-cooled infrared detectors and, above all, the super-capacitors for storage of electricity.
- Thin films of BST for the various possible applications should be as homogeneous, uniform and of smooth surface (a small roughness at the nanoscale)as possible.
- PLD pulsed laser ablation
- the deposition temperature can be lower than in other methods because the arrangement of the material deposited on the substrate is helped by the high energy with which the ablated material is deposited.
- the PLD method suffers from the important disadvantage of producing large amounts of particulate matter (particle size between 0.1 and 10 pm) that is deposited on the substrate, significantly and adversely affecting the electrical and optical properties of thin film thus obtained.
- 165205 (lip) is proposed the use of a pulsed electron deposition (PED) for the application of BST materials on substrates .
- PED pulsed electron deposition
- this article does not provide sufficient information to allow effectively to obtain a layer of good quality BST (sufficiently smooth, homogeneous and free of impurities) .
- the aim of the present invention is to provide a method for the deposition of a layer of material, a method for the construction of an electronic device and an electronic device, which allow to overcome, at least partially, the problems of the prior art and possibly are at the same time cheap and easy implementation.
- the present invention provides a method of depositing a layer of a material, a method of manufacturing an electronic device and an electronic device in accordance with the following independent claims and preferably with any of the dependent claims directly or indirectly of the independent claims .
- FIG. 1 shows schematically and partly in section of an apparatus that can be used in a method in accordance with the present invention
- FIG. 2 schematically shows a different embodiment of the apparatus of Figure 1;
- - Figure 9 is a photograph SEM (scanning electron microscope) of a layer obtained by a method in accordance with the present invention
- - Figure 10 is an optical spectrum of a "plum" obtained during the application of a method in accordance with the present invention
- FIG. 11 shows an image AFM (atomic force microscope) three-dimensional (a) and two-dimensional (b) a layer obtained by a method in accordance with the present invention
- FIG. 12 is an XRD spectrum of a layer obtained by a method in accordance with the present invention.
- FIG. 1 With 1 as a whole is shown an apparatus for the deposition of a material having a specific composition (Bai- x Sr x) Ti0 3 , where x ⁇ 0 ⁇ 1 (BST) by pulsed plasma deposition (Pulsed Plasma Deposition - PPD) .
- the apparatus 1 comprises a device 2 for plasma generation (that is to say at least partial ionization of a rarefied gas) and to direct a flow (pulsed) of electrons at a target 3, which shows (in particular consists of) the given material, so that at least part of the given material separated from the target 3 deposits on a surface of a substrate 4.
- the target 3 and the substrate 4 are located inside a chamber 24 outside the apparatus 1, which also comprises a heating unit HU for heating the substrate 4.
- the heating of the substrate 4 is achieved by irradiation with infrared rays .
- the heating of the substrate by heating a back portion of 4 (in particular heating surface 4 opposite to the surface of the substrate) .
- the substrate 4 is located between the heating unit and the target 3.
- the substrate 4 is maintained at a temperature of deposition from 400°C to 800°C.
- the substrate 4 is maintained at a temperature of deposition greater than 525 °C (more precisely, more than 600°C) .
- the substrate 4 is maintained at a temperature of deposition from about 650°C to about 750°C.
- the given material (BST) is able to acquire a crystalline conformation during the deposition on the substrate 4.
- the substrate 4 comprises a layer 4a ( Figures 3 and 4) of a crystalline material with its 0001 hexagonal crystal plane substantially parallel to the surface 4' of the substrate.
- the substrate 4 is formed by the aforementioned crystalline material .
- the crystal plane 0001 of the hexagonal crystalline material has a length of 0.45 nm to 0.49 nm (in particular, from 0.46 nm to 0.48 nm) .
- the crystal plane 0001 of the crystalline material has a hexagonal symmetry, whose side has the dimensions specified above .
- the crystalline material is sapphire.
- the length of the faces (crystals) of the crystalline material are measured by means of X rays .
- the crystalline material is located in the area of the surface 4' . In other words, the crystalline material defines the surface 4' .
- the particular structure of the substrate 4 permits growth of the given material surprisingly epitaxial with respect to the crystalline material, in particular, with the crystal plane of Ill-type substantially parallel to the crystal plane 0001 of the layer 4a.
- the substrate 4 comprises a layer 4b ( Figures 3 and 4), which is placed at the surface 4' .
- the layer 4b comprises (in particular consists of) platinum. More precisely, the layer 4b define the surface 4' .
- the substrate 4 is maintained at a temperature above the deposition temperature (up to 50°C higher than the temperature of deposition) for a period of at least 1 hour 30 minutes.
- the platinum layer 4b has the Ill-type crystal plane substantially parallel to the surface 4' (thus parallel to the face 0001 of crystalline material) .
- the layer 4b has a typical thickness of less than 200 nm (in particular from about 40 nm to about 200 nm, more precisely, from about 80 nm to about 140 nm) . According to specific embodiments, the layer 4b has a thickness from about 90 nm to about 110 nm. According to the embodiment shown in Figure 3, the layer 4b is deposited in contact with the layer 4a.
- the substrate 4 comprises (below and in contact with layer 4b) layer 4c ( Figure 4), which is located on the layer 4a (in contact) .
- the layer 4c comprises (in particular consists of) a further material with composition (Bai-y Sr y )Ti0 3 wherein y ⁇ 0 ⁇ 1 (BST) .
- the given material and the further material are identical to each other.
- the layer 4c typically has a thickness less than
- the layer 4c has a thickness from about 30 nm to about 40 nm.
- the layer 4c thermally and mechanically stabilizes the layer 4b.
- the layers 4b and/or 4c are deposited by magnetron sputtering on the layer 4a. According to alternative embodiments, 4b and 4c are the layers deposited by other techniques such as pulsed plasma deposition (PPD) or wet chemical methods .
- PPD pulsed plasma deposition
- the layer 4b (and/or layer 4c) is surprisingly deposited in a substantially ordered way with the Ill-type crystal plane substantially parallel to the 0001 crystal plane crystal of the layer 4a.
- the product Pi shown in Figure 5 is obtained by pulsed plasma deposition (PPD) of a layer 4d of a given material
- the product P2 shown in Figure 6 is obtained by pulsed plasma deposition (PPD) of a layer 4d of the given material (BST) .
- the layer 4d is surprisingly deposited in a substantially ordered way with the 111-type crystal plane substantially parallel to the surface 4" (in particular, to the 0001 crystal plane of the layer 4a and/or to the crystal plane 111 of the layer 4b) .
- the layer 4d has a thickness less than 0.3 ⁇ . Note that it is possible to get a layer 4d with a thickness up to about 0.05 ⁇ .
- the layer 4d is crystalline and very homogeneous and substantially free of pin holes.
- the apparatus 1 also comprises a cover element C movable between an operating position (shown dashed) and a rest position (shown in solid line) .
- the target 3 is cleaned.
- a beam (pulsed) of electrons (generated by the device 2) is directed against the target 3 so that the surface layer (on which the impurities can be deposited potentially) of the target 3 itself is removed and its particles are intercepted by cover element C (placed in its operational position) .
- the target 3 has been cleaned it is possible to proceed with the deposition of the given material (BST) on the substrate 4 so as to obtain a higher quality layer 4d.
- the cover element C is maintained in its rest position to allow the particles of the given material to deposit freely on the surface 4'.
- the target 3 is connected to ground. In this way, the target 3 does not reject (and indeed attracts) the flow of electrons even in the case that the electrons have already hit the target 3 itself.
- the device 2 includes a hollow element 5, which acts as a cathode and has (externally delimits) internal cavity 6; and an activation electrode 7, which includes (in particular, consists of) an electrically conductive material (especially metal) .
- the activation electrode 7 is located within the cavity 6 (defined by the hollow element 5) .
- the hollow element 5 comprises (more specifically, it consists of) an electrically conductive material (more specifically a metal) .
- electrically conductive material eg. Stainless Steel, Tungsten, Molybdenum, Chromium, Iron, Titanium
- electrically conductive material means a material that has an electrical resistivity (measured at 20 °C) lower than 10 "1 ⁇ -m.
- the electrically conductive material has an electrical resistivity (measured at 20 °C) less than 10 ⁇ 3 ⁇ -m.
- the activation electrode 7 extends through a wall 8 of the hollow element 5. Between the activation electrode 7 and the wall 8 is interposed a ring 9 of substantially electrically insulating material (especially ceramics) .
- substantially electrically insulating material means a material that has an electrical resistivity (measured at 20 °C) higher than 10 3 ⁇ -m.
- the electrically non-conductive material has an electrical resistivity (measured at 20 °C) higher than 10 7 ⁇ -m (more advantageously, more than 10 9 ⁇ -m) .
- substantially electrically insulating material is a dielectric material.
- the device 2 also includes a resistor 10, which connects the activation electrode 7 to ground and has a resistance of at least 100 ohms, advantageously at least 1 kOhm.
- the resistor 10 has a resistance of about 20 kOhm.
- the cavity contains the rare gas at a pressure less than or equal to 10 "2 mbar (in particular, less than 10 "3 mbar) .
- the rarefied gas contained within the cavity 6 has a pressure less than or equal to 10 "4 mbar.
- the rarefied gas contained within the cavity 6 has a pressure greater than or equal to 10 "6 mbar (more specifically, greater than or equal to 10 ⁇ 5 mbar) .
- the apparatus 2 comprises a group of gas supply (which in itself is known and not shown) to feed an anhydrous gas, (non-exhaustive examples - oxygen, nitrogen, argon, helium, xenon, etc.) inside the cavity 6 via a conduit 23.
- anhydrous gas non-exhaustive examples - oxygen, nitrogen, argon, helium, xenon, etc.
- the hollow element 5 is electrically connected to an activation assembly 11 which is adapted to decrease the electrical potential of the hollow element 5 of at least 4 kV (in particular, from an electrical potential substantially equal to zero) in less than 20 ns directing a pulse of electrical charge of at least 0.16 mC to the hollow element 5 itself.
- the activation assembly 11 is chosen in such a way to impose a reduction of potential to the hollow element 5 from 8 kV to 35 kV (more precisely, to 25 kV) in less than 15 ns, in particular in about 10 ns .
- the hollow element 5 is connected to ground. In this way, when the flux of electrons is not carried out, the hollow element 5 is maintained at substantially zero potential and the risk of spontaneous activation of the discharges between the hollow element 5 and the electrode 7 is substantially canceled.
- a resistor 12 is connected between the hollow element 5 and ground.
- the resistor 12 has a resistance of 50 kOhm.
- the resistor 12 has a resistance of at least 100 kOhm, particulary about of at least 0.5 MOhm. According to some embodiments, the resistance is less than 1 MOhm.
- the activation assembly 11 includes a thyratron 13, a capacitor 14 which has one armature connected to an anode 15 of the thyratron 13 and the other armature connected to the hollow element 5, and a power supply 16, which has a positive electrode 17 electrically connected to anode 15 and a negative electrode 18 connected to ground.
- the thyratron 13 also has a cathode 19, which is connected to ground.
- capacitor 14 is electrically connected to ground (in particular, through the resistor 12) .
- the activation assembly 11 also includes a control unit 20 of the thyratron 13 , which is capable of operating the thyratron 13 and is connected to ground.
- the device 2 also comprises an operator interface assembly (known per se and not shown here) , which allows an operator to adjust the operation (for example switching on and/or modification of operating parameters) of device 2 itself.
- an operator interface assembly known per se and not shown here
- the device 2 also comprises a tubular element 21, which includes (in particular, is) a substantially electrically insulating material (in particular glass, quartz or alumina) and is connected to the hollow element 5.
- the tubular element 21 has two open ends 21a and 21b and an inner opening which connects the cavity 6 with the outside space (in particular, with the outer chamber 24) .
- the hollow element 5 (except of the conduit 23 and the tubular element 21) is vacuum-tight to the outside.
- the tubular element 21 extends at least partially within the outer chamber 24 ( Figure 1), where the target element 3 and the substrate element 4 are arranged in.
- the tubular element 21 and its inner opening have, respectively, substantially circular cross sections.
- the cavity contains the diluted gas at a pressure less than or equal to 10 "2 mbar (in particular, less than 10 "3 mbar) .
- the diluted gas contained within the outer chamber 24 is maintained at a pressure less than or equal to 10 "4 mbar using a pumping device (of a known type and not shown) .
- the diluted gas contained within the outer chamber 24 has a pressure greater than or equal to 10 ⁇ 6 mbar (more specifically, greater than or equal to lC 5 mbar) .
- the gas is oxygen.
- the pressure (from about 5xl0 "4 mbar to about 1CT 2 mbar) inside the cavity 6 is maintained (slightly) higher than that present in the outer chamber 24 (in particular, feeding small amounts of gas through a duct 23) .
- the tubular element 21 extends through a wall 22 of the hollow element 5 (opposite to the wall 8), partly inside and partly outside of the cavity 6 (in particular, inside of the outer chamber 24) .
- the tubular element 21 has a length of 90 mm to 220 mm.
- the tubular element 21 has a diameter of about 4 mm to 10 mm.
- the inner lumen 21c has a diameter from about 1.5 to about 8 mm.
- the outer chamber 24 is constructed to be vacuum-tight relation to its surroundings .
- the target 3 and substrate 4 are arranged at a distance of 35 mm to 65 mm (more precisely, from 40 mm to 60 mm) .
- the distance between the target 3 end an edge 21b is between 1 and 20 mm (more precisely, between 3 and 8 mm) .
- the device 2 also includes an external element 25 which is located outside of the hollow element 5 (in particular, in the outer chamber 24) along the tubular element 21 (i.e., not at one end of the element tube 21) and acts as an anode.
- the outer element 25 is placed in contact with an outer tubular element 21.
- the outer element 25 is shaped so as to be arranged around tubular element 21, in particular, the outer element 25 has a hole through which extends the tubular element 21. According to specific embodiments, the outer element 25 has a n annular shape.
- the device 2 also comprises a group 26 which maintains the electrical potential and which is electrically connected to the external element 25 to maintain the electrical potential of the external element 25 substantially grounded.
- the activation assembly 11 imposes a potential difference between the hollow element 5 and the activation electrode 7 according to the above parameters.
- the plasma is generated (that is to say at least partial ionization of the diluted gas) inside the cavity 6.
- the potential difference which was established with the external element 25, allows electrons to be accelerated along the same tubular element 21 to the target 3.
- the device 1 and device 2 (except for what concerns the outer chamber 24 and its contents) of Figure 1 show a similar structure and operation of the apparatus and the device described in the application of PCTIB2010000644 patent.
- Figure 2 shows an alternative embodiment of the device 2 and the apparatus 1. Components shown in Figure 2 which are similar to those shown in Figure 1 are denoted by the same reference number.
- the device 2 of Figure 2 shows an ampoule 28 (usually glass) , outside of which the activation electrode 7 is placed; and a stabilization group 27 as described above.
- the capacitance of the capacitor 14 is also in this case as indicated according to the embodiment of Figure 1.
- the hollow element 5 is maintained at a relatively high negative electric potential (i.e., negatively charged - about 13-16 kV) and when an electrical pulse is produced on the activation electrode 7 it creates a glow discharge which, in turn, generates a positive electrical charge inside the hollow element 5.
- the positive charge is compensated by the emission of electrons, which in turn are accelerated towards the first element 25 inside the outer tube 21.
- the electrons moving outward ionize more molecules producing more electrons (called secondary electrons), which, in turn, are accelerated toward the target 3.
- the device 1 and device 2 (except for what concerns the outer chamber 24, its contents and the tubular element 21) of Figure 2 show a similar structure and operation of the apparatus and the device described PCTEP2006003107 in the patent application of the applicant.
- the device 1 and device 2 (except for what concerns the outer chamber 24 and its contents) have a similar structure and function (with an appropriate adjustment of operating parameters) to equipment and devices described in Italian patent application BO2010A000525 of the same applicant.
- a method for the creation of an electronic device 30.
- the device 30 is an electronic capacitor (two embodiments are shown in Figures 7 and 8) .
- a layer 4d as described above and further layer 4e comprising (in particular, consisting of) platinum are deposited on the layer 4d.
- the deposition is carried out with PPD.
- the deposition of the fourth layer is made by magnetron sputtering.
- the layer 4e has typically a thickness less than 200 nm (in particular from about 40 nm to about 200 nm, more specifically, from about 80 nm to about 140 nm) . According to specific embodiments, layer 4e has a thickness from about 90 nm to about 110 nm.
- a device 30 ( Figure 8) comprising a layer 4a, a layer 4b, a layer 4e, a layer 4c interposed in contact between the layer 4a and layer 4b , and a layer 4d interposed in contact between the layer 4b and layer 4e.
- a device 30 ( Figure 7) comprising a layer 4a, a layer 4b, a layer 4e and a layer 4d interposed in contact between the layer 4b layer and 4e.
- the device 30 includes an electric contact
- the contact layer 31 is deposited substantially simultaneously with the deposition of the layer 4b.
- the contact 32 is deposited on the layer 4d substantially simultaneously with the deposition of the layer 4e.
- Sapphire substrates were prepared from single-crystal plates of dimensions 10 x 5 x 0.5 mm with the crystal plane 0001 oriented in parallel with the largest surface.
- plasma power P 100 W
- gas pressure in the chamber p 6 * 10 "1 mbar
- time treatment t 5 min.
- gas pressure in the chamber p 6 * 10 "1 mbar
- time treatment t 5 min.
- argon plasma plasma treatment substrates were transported in a deposition chamber (outer chamber) . Here were mounted on a rotating sample holder heated by the infrared system. The distance between the substrate and the target of BST ; from which is then ablated the deposited material, was set to 48 mm. All the deposition system was closed and taken to the base
- the substrates prepared according to the example above were heated in the range between 650 - 700 °C.
- the heater was set to rotate with the frequency ca. 0.1 Hz, gas pressure inside the deposition chamber was increased to 2.6 * 10 ⁇ 3 mbar and kept at this value throughout the period of deposition.
- the device 2 as shown in Figure 2 ie as described in the patent application PCTEP2006003107 of the applicant has been used.
- the voltage of the gun has been selected in the range between 14 kv and 25 kV.
- the voltage of 25 kv was judged the most suitable.
- the rotating target (rotated with a frequency of approximately 0.3 Hz) was subjected to an ablation under the same conditions of deposition as described below for a period of about 30 minutes, but the ablated material was intercepted with a cover element and did not arrive to the substrate.
- This process the conditioning of the target - ensures the same properties of the target deposition for each event and for any previous history of the target.
- the cover element After conditioning of the target, the cover element is removed and the ablated material begins to deposit on the substrate .
- the ablation rate (the rate of discharge of the gun) was varied between 1 Hz and 50 Hz, the frequency was selected between approx. 35 and 45 Hz (in particular, 40 Hz) .
- the quality of the "plum" (which is defined by the trajectories of particles that are separated from the target) generated by the PPD ablation of BST was checked by measurements of the optical spectrum ( Figure 10, the abscissa shows the wavelength in nm, the ordinate exhibits an intensity in arbitrary units) .
- the characteristic time of the deposition was chosen in the range between 15 and 120 min. The optimal duration of deposition was approximately 30 min.
- the layers of BST of about 0.1 (0.2) ⁇ m thick were obtained in this way.
- the thermal pretreatment consists of a heating of the substrate held in a vacuum at the temperatures higher from 0 to 50 °C than deposition temperatures about 2 hours. This process stabilizes the layer of platinum and the "pin-holes" in the deposited film does not open any more later.
- the morphology of the deposited BST films is shown in Figure 9.
- the layer is composed of a dense aggregation of grains of BST.
- the average size of grains is approx. 150 nm. Note the particulate on the surface layer of the characteristic size approx. 10 to 20 nm.
- the average lateral grains size of 150 nm is substantially larger than the roughness of the film (about 15 to 25 nm rms) , as shown in Figure 11 which shows the AFM images (Atomic Force Microscopy) of the surface - Figure 11a - and the single scan - Figure lib. This fact shows that the BST layer grows with a preferred orientation parallel to the substrate surface in an almost-epitaxial way.
- the same conclusion can be drawn also from the X-ray difractogram shown in Figure 12 [x-axis shows the fraction of 2theta angle (deg) , the ordinate shows the X-ray intensity in arbitrary units] .
- the X-ray difractogram ( Figure 12) shown in Figure 12 shows how the structure matches that of the crystalline structure of BST material (the maximum intensity at diffraction angles 2 ⁇ around 39.7 and 67.5 degrees correspond to the reflections of the substrate) .
- the relative intensities of maximum diffraction corresponding to the crystalline structure of BST suggest that the BST layer grows preferentially oriented with the 111 crystal plane parallel to the substrate surface.
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ITBO20110669A1 (it) * | 2011-11-23 | 2013-05-24 | Organic Spintronics S R L | Metodo per la deposizione di uno strato di un materiale su un substrato |
CN114059022A (zh) * | 2021-11-09 | 2022-02-18 | 西安交通大学 | 一种设置空心阴极等离子体的pld系统及薄膜的制备方法 |
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Cited By (2)
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ITBO20110669A1 (it) * | 2011-11-23 | 2013-05-24 | Organic Spintronics S R L | Metodo per la deposizione di uno strato di un materiale su un substrato |
CN114059022A (zh) * | 2021-11-09 | 2022-02-18 | 西安交通大学 | 一种设置空心阴极等离子体的pld系统及薄膜的制备方法 |
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