JP3152249B2 - Method and apparatus for producing transparent conductive film - Google Patents
Method and apparatus for producing transparent conductive filmInfo
- Publication number
- JP3152249B2 JP3152249B2 JP34927691A JP34927691A JP3152249B2 JP 3152249 B2 JP3152249 B2 JP 3152249B2 JP 34927691 A JP34927691 A JP 34927691A JP 34927691 A JP34927691 A JP 34927691A JP 3152249 B2 JP3152249 B2 JP 3152249B2
- Authority
- JP
- Japan
- Prior art keywords
- film
- transparent conductive
- light
- conductive film
- surface resistance
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Fee Related
Links
- 238000000034 method Methods 0.000 title description 53
- 238000002834 transmittance Methods 0.000 claims description 20
- 238000004519 manufacturing process Methods 0.000 claims description 14
- 238000012545 processing Methods 0.000 claims description 7
- 239000004020 conductor Substances 0.000 claims description 2
- 230000003595 spectral effect Effects 0.000 claims description 2
- 239000010408 film Substances 0.000 description 128
- 239000000758 substrate Substances 0.000 description 14
- 238000004544 sputter deposition Methods 0.000 description 13
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 description 10
- 238000005259 measurement Methods 0.000 description 10
- 239000001301 oxygen Substances 0.000 description 10
- 229910052760 oxygen Inorganic materials 0.000 description 10
- 230000003647 oxidation Effects 0.000 description 9
- 238000007254 oxidation reaction Methods 0.000 description 9
- 230000015572 biosynthetic process Effects 0.000 description 8
- 238000010438 heat treatment Methods 0.000 description 8
- 239000000463 material Substances 0.000 description 8
- 239000013307 optical fiber Substances 0.000 description 8
- 238000001771 vacuum deposition Methods 0.000 description 8
- XOLBLPGZBRYERU-UHFFFAOYSA-N tin dioxide Chemical compound O=[Sn]=O XOLBLPGZBRYERU-UHFFFAOYSA-N 0.000 description 7
- 229910001887 tin oxide Inorganic materials 0.000 description 7
- 238000007740 vapor deposition Methods 0.000 description 7
- XLOMVQKBTHCTTD-UHFFFAOYSA-N Zinc monoxide Chemical compound [Zn]=O XLOMVQKBTHCTTD-UHFFFAOYSA-N 0.000 description 6
- 239000002585 base Substances 0.000 description 6
- 239000007789 gas Substances 0.000 description 6
- 229910052751 metal Inorganic materials 0.000 description 6
- 239000002184 metal Substances 0.000 description 6
- 238000005546 reactive sputtering Methods 0.000 description 6
- 239000000523 sample Substances 0.000 description 6
- 238000005229 chemical vapour deposition Methods 0.000 description 5
- 229910003437 indium oxide Inorganic materials 0.000 description 5
- PJXISJQVUVHSOJ-UHFFFAOYSA-N indium(iii) oxide Chemical compound [O-2].[O-2].[O-2].[In+3].[In+3] PJXISJQVUVHSOJ-UHFFFAOYSA-N 0.000 description 5
- 229910044991 metal oxide Inorganic materials 0.000 description 5
- 150000004706 metal oxides Chemical class 0.000 description 5
- 230000008569 process Effects 0.000 description 5
- -1 Generally Chemical compound 0.000 description 4
- 239000011248 coating agent Substances 0.000 description 4
- 238000000576 coating method Methods 0.000 description 4
- 238000000151 deposition Methods 0.000 description 4
- 230000008021 deposition Effects 0.000 description 4
- 239000010409 thin film Substances 0.000 description 4
- 239000011521 glass Substances 0.000 description 3
- 238000000691 measurement method Methods 0.000 description 3
- 238000012544 monitoring process Methods 0.000 description 3
- 229920006267 polyester film Polymers 0.000 description 3
- 229920006254 polymer film Polymers 0.000 description 3
- 239000002994 raw material Substances 0.000 description 3
- 230000035945 sensitivity Effects 0.000 description 3
- 239000011787 zinc oxide Substances 0.000 description 3
- XKRFYHLGVUSROY-UHFFFAOYSA-N Argon Chemical compound [Ar] XKRFYHLGVUSROY-UHFFFAOYSA-N 0.000 description 2
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 description 2
- MYMOFIZGZYHOMD-UHFFFAOYSA-N Dioxygen Chemical compound O=O MYMOFIZGZYHOMD-UHFFFAOYSA-N 0.000 description 2
- CBENFWSGALASAD-UHFFFAOYSA-N Ozone Chemical compound [O-][O+]=O CBENFWSGALASAD-UHFFFAOYSA-N 0.000 description 2
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 2
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 description 2
- ATJFFYVFTNAWJD-UHFFFAOYSA-N Tin Chemical compound [Sn] ATJFFYVFTNAWJD-UHFFFAOYSA-N 0.000 description 2
- 239000000956 alloy Substances 0.000 description 2
- 238000006243 chemical reaction Methods 0.000 description 2
- 230000000052 comparative effect Effects 0.000 description 2
- 150000001875 compounds Chemical class 0.000 description 2
- 229910001882 dioxygen Inorganic materials 0.000 description 2
- 238000009826 distribution Methods 0.000 description 2
- RHZWSUVWRRXEJF-UHFFFAOYSA-N indium tin Chemical compound [In].[Sn] RHZWSUVWRRXEJF-UHFFFAOYSA-N 0.000 description 2
- 150000002500 ions Chemical class 0.000 description 2
- 239000000203 mixture Substances 0.000 description 2
- 230000001590 oxidative effect Effects 0.000 description 2
- 238000005240 physical vapour deposition Methods 0.000 description 2
- 229910052710 silicon Inorganic materials 0.000 description 2
- 239000010703 silicon Substances 0.000 description 2
- 239000007787 solid Substances 0.000 description 2
- 229910052718 tin Inorganic materials 0.000 description 2
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 2
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 1
- 239000004698 Polyethylene Substances 0.000 description 1
- 239000004743 Polypropylene Substances 0.000 description 1
- 229910001128 Sn alloy Inorganic materials 0.000 description 1
- 229910006404 SnO 2 Inorganic materials 0.000 description 1
- 238000010521 absorption reaction Methods 0.000 description 1
- 239000003513 alkali Substances 0.000 description 1
- 229910045601 alloy Inorganic materials 0.000 description 1
- 229910052786 argon Inorganic materials 0.000 description 1
- 239000005388 borosilicate glass Substances 0.000 description 1
- CXKCTMHTOKXKQT-UHFFFAOYSA-N cadmium oxide Inorganic materials [Cd]=O CXKCTMHTOKXKQT-UHFFFAOYSA-N 0.000 description 1
- CFEAAQFZALKQPA-UHFFFAOYSA-N cadmium(2+);oxygen(2-) Chemical compound [O-2].[Cd+2] CFEAAQFZALKQPA-UHFFFAOYSA-N 0.000 description 1
- 239000000919 ceramic Substances 0.000 description 1
- 230000008859 change Effects 0.000 description 1
- 239000000470 constituent Substances 0.000 description 1
- 238000010924 continuous production Methods 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 238000001816 cooling Methods 0.000 description 1
- 229910052802 copper Inorganic materials 0.000 description 1
- 239000010949 copper Substances 0.000 description 1
- 230000003247 decreasing effect Effects 0.000 description 1
- 238000011161 development Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000010894 electron beam technology Methods 0.000 description 1
- 238000001704 evaporation Methods 0.000 description 1
- 239000000835 fiber Substances 0.000 description 1
- 230000001771 impaired effect Effects 0.000 description 1
- 229910052738 indium Inorganic materials 0.000 description 1
- APFVFJFRJDLVQX-UHFFFAOYSA-N indium atom Chemical compound [In] APFVFJFRJDLVQX-UHFFFAOYSA-N 0.000 description 1
- 230000006698 induction Effects 0.000 description 1
- 238000007733 ion plating Methods 0.000 description 1
- 230000001678 irradiating effect Effects 0.000 description 1
- 230000031700 light absorption Effects 0.000 description 1
- 239000004973 liquid crystal related substance Substances 0.000 description 1
- 238000001755 magnetron sputter deposition Methods 0.000 description 1
- 238000002844 melting Methods 0.000 description 1
- 230000008018 melting Effects 0.000 description 1
- 150000002739 metals Chemical class 0.000 description 1
- 229910052757 nitrogen Inorganic materials 0.000 description 1
- 230000003287 optical effect Effects 0.000 description 1
- TWNQGVIAIRXVLR-UHFFFAOYSA-N oxo(oxoalumanyloxy)alumane Chemical compound O=[Al]O[Al]=O TWNQGVIAIRXVLR-UHFFFAOYSA-N 0.000 description 1
- 239000002245 particle Substances 0.000 description 1
- 230000035699 permeability Effects 0.000 description 1
- 229920000573 polyethylene Polymers 0.000 description 1
- 229920000139 polyethylene terephthalate Polymers 0.000 description 1
- 239000005020 polyethylene terephthalate Substances 0.000 description 1
- 229920001155 polypropylene Polymers 0.000 description 1
- 229920000915 polyvinyl chloride Polymers 0.000 description 1
- 239000004800 polyvinyl chloride Substances 0.000 description 1
- 238000003825 pressing Methods 0.000 description 1
- 239000010453 quartz Substances 0.000 description 1
- 230000009257 reactivity Effects 0.000 description 1
- 229910052594 sapphire Inorganic materials 0.000 description 1
- 239000010980 sapphire Substances 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
- 239000007921 spray Substances 0.000 description 1
- 239000012780 transparent material Substances 0.000 description 1
- 238000004804 winding 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
Landscapes
- Physical Vapour Deposition (AREA)
- Chemical Vapour Deposition (AREA)
Description
【0001】[0001]
【産業上の利用分野】本発明は、透明基盤上に金属酸化
物被膜を付着させた透明導電膜の製造方法、及び透明導
電膜の膜表面電気抵抗値の測定装置に関するものであ
る。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method for producing a transparent conductive film in which a metal oxide film is adhered on a transparent substrate, and to an apparatus for measuring the electric resistance of the film surface of the transparent conductive film.
【0002】[0002]
【従来の技術】ガラス又は高分子フイルム等の表面に、
透明であり、かつ膜表面の電気抵抗値の低い金属酸化物
被膜を付着させた透明導電膜は、その導電性を利用した
用途、例えば液晶ディスプレイ、ELディスプレイとい
ったフラットディスプレイや、太陽電池等の透明電極、
ブラウン管の窓の透明静電シールド板、又は透明電磁シ
ールド板、発熱体等の電気、電子分野の用途に広く使用
されている。又このような酸化物透明導電膜の中で、選
択透過性を有するものは、その赤外光反射特性を利用し
て、太陽エネルギー利用のための窓材や、建物、自動車
等の熱線反射用材料として利用されている。これらの透
明導電膜としては、通常、酸化すず、酸化インジウム、
酸化インジウム・酸化すず(ITO)、或は、酸化亜鉛
を被膜として透明基盤上に形成させたものが一般的であ
り、真空蒸着法、スパッター法、CVD法、スプレー法
等により作成できることが知られている。この中でも、
真空蒸着法、スパッター法は被膜の厚みが均一で、かつ
膜表面電気抵抗値(以下表面抵抗値という)の低い透明
導電膜が得られる方法である。この場合、酸化物を原料
とする場合と、金属を原料として、酸素と反応させなが
ら被膜を形成していく方法がある。例えばITOの薄膜
のスパッターによる被膜形成の場合には、ターゲットと
して、ITOの焼結ターゲットを使用する方法と、イン
ジウム・すず合金のターゲットを用い、酸素と反応させ
ながらおこなう反応性スパッターを行なう方法の両者が
知られているが、ターゲットの作成、再生が容易な点
や、製膜速度を早くとれることから、金属ターゲットを
用いる方法の方が有利であると考えられている。真空蒸
着法についても、同様な理由から、金属を原料として反
応性蒸着をおこなうことが有利である。製造される透明
導電膜は、透明度が高く、かつ表面抵抗値が低い膜が好
ましい。表面抵抗値は、二端子、或いは四端子等の接触
式表面抵抗測定法により測定されるが、精度を上げるた
めには四探針法が用いられる。この方法は、透明導電膜
の表面(被膜付着側)の4個所に接触探針を押しあて、
外側の2探針間に一定電圧をかけ、内側の2探針間の電
圧降下を測定することによって、電極間の抵抗値を求め
るもので、接触抵抗の影響をなくすことができる。2. Description of the Related Art On a surface of glass or a polymer film,
Transparent conductive films that are transparent and have a metal oxide film with a low electric resistance value attached to the film surface are used for applications utilizing the conductivity, for example, flat displays such as liquid crystal displays and EL displays, and transparent materials such as solar cells. electrode,
It is widely used for electric and electronic applications such as a transparent electrostatic shield plate or a transparent electromagnetic shield plate for a cathode ray tube window, a heating element, and the like. Among such transparent conductive oxide films, those having selective permeability are used for the window material for utilizing solar energy and for reflecting heat rays of buildings, automobiles, etc. by utilizing the infrared light reflection characteristics. Used as a material. As these transparent conductive films, usually, tin oxide, indium oxide,
Generally, indium oxide / tin oxide (ITO) or zinc oxide is formed on a transparent substrate as a coating film, and it is known that it can be formed by a vacuum deposition method, a sputtering method, a CVD method, a spray method, or the like. ing. Among them,
The vacuum vapor deposition method and the sputtering method are methods in which a transparent conductive film having a uniform film thickness and a low film surface electric resistance value (hereinafter referred to as surface resistance value) is obtained. In this case, there are a method using an oxide as a raw material and a method using a metal as a raw material to form a film while reacting with oxygen. For example, in the case of forming a film by sputtering of a thin film of ITO, a method of using a sintered target of ITO as a target and a method of performing reactive sputtering using an indium-tin alloy target while reacting with oxygen. Although both methods are known, it is considered that a method using a metal target is more advantageous in that the target can be easily formed and regenerated, and the film forming speed can be increased. Also for the vacuum deposition method, for the same reason, it is advantageous to perform reactive deposition using a metal as a raw material. The transparent conductive film to be manufactured is preferably a film having high transparency and low surface resistance. The surface resistance is measured by a contact type surface resistance measurement method such as a two-terminal or four-terminal method, and a four-probe method is used to increase the accuracy. In this method, contact probes are pressed at four positions on the surface of the transparent conductive film (coating side),
By applying a constant voltage between the two outer probes and measuring the voltage drop between the two inner probes, the resistance value between the electrodes is obtained, and the influence of the contact resistance can be eliminated.
【0003】[0003]
【発明が解決しようとする課題】しかしながら、ITO
をはじめ酸化物系透明導電膜の表面電気抵抗値に関する
抵抗特性は、その酸化度に大きく依存し、表面抵抗値、
光透過率を共に満足する範囲は非常に狭い。そのため、
特に、反応性スパッター、あるいは、反応性蒸着法で
は、作製時の状態により、材料の酸化条件が変わり、そ
れが透明導電膜の特性、特に抵抗特性に敏感に影響す
る。例えば、真空槽中に残った水の量等が大きく影響
し、バッチ毎に条件が変化し、再現性が良くないという
現象が起こる。このようなことは、ターゲット、或は、
蒸着材料として、酸化物を用いた場合にも、反応性スパ
ッター法あるいは、反応性蒸着法の場合ほど大きくはな
いが、問題になっている。例えば、ITO焼結ターゲッ
トを用いて、スパッターをおこなった場合、ターゲット
表面が黒くなるという黒化現象が起こり、透明度、ある
いは膜表面抵抗値を大きくさせる。CVDにおいても同
様に、原料ガスの供給量、透明基盤温度等の変動による
特性のバラツキが問題になっている。従って、透明導電
膜の製造においては、表面抵抗値を膜の巾方向及び膜の
長さ方向、すなわち連続的な製造方法においては、酸化
物被膜の付着操作の経時的な変動を少なくすることは難
かしい。又接触式抵抗測定法で、求まる値は、端子間の
平均であり、幅方向の斑は判別できない。また、接触抵
抗値は接触端子の押し込み圧、表面形状でバラツキを生
じ、測定精度が良くない。更に、連続製造工程において
接触式測定法を用いる場合にはどうしてもフイルムにき
ずを付けることが多く、その部分を捨ててつかうことに
なり、歩留り率を大きく下げることになる。そこで、非
接触で表面抵抗値を測定し、その値が一定になる様に製
膜操作を制御し、膜の透明度が高く、かつ表面抵抗値の
低い膜の製造方法、及び表面抵抗値の非接触測定装置の
開発が期待されていた。SUMMARY OF THE INVENTION However, ITO
The resistance characteristics of the oxide-based transparent conductive film with respect to the surface electric resistance value greatly depend on the degree of oxidation, and the surface resistance value,
The range satisfying both the light transmittances is very narrow. for that reason,
In particular, in the reactive sputtering or the reactive evaporation method, the oxidizing condition of the material changes depending on the state at the time of manufacturing, which sensitively affects the characteristics of the transparent conductive film, particularly the resistance characteristics. For example, the amount of water remaining in the vacuum chamber or the like has a large effect, and the condition changes for each batch, and a phenomenon that reproducibility is not good occurs. This is the target or
When an oxide is used as the vapor deposition material, it is not as large as in the case of the reactive sputtering method or the reactive vapor deposition method, but it is a problem. For example, when sputtering is performed using an ITO sintered target, a blackening phenomenon occurs in which the target surface becomes black, and the transparency or the film surface resistance value is increased. Similarly, in CVD, variations in characteristics due to fluctuations in the supply amount of the source gas, the temperature of the transparent substrate, and the like have become a problem. Therefore, in the production of a transparent conductive film, the surface resistance value is reduced in the width direction of the film and in the length direction of the film, that is, in a continuous production method, it is possible to reduce the variation over time of the deposition operation of the oxide film. Difficult. The value obtained by the contact-type resistance measurement method is an average between terminals, and a spot in the width direction cannot be determined. In addition, the contact resistance value varies with the pressing pressure and surface shape of the contact terminal, and the measurement accuracy is not good. Further, when the contact measurement method is used in the continuous manufacturing process, the film is often scratched, and the film is discarded and used, which greatly reduces the yield. Therefore, the surface resistance is measured in a non-contact manner, the film forming operation is controlled so that the value is constant, a method of manufacturing a film having high transparency and a low surface resistance, and a method of manufacturing a film having a low surface resistance. The development of a contact measurement device was expected.
【0004】[0004]
【問題を解決するための手段】本発明者らは、上記の課
題を解決すべく、鋭意検討した結果、透明導電膜の表面
電気抵抗(R)と該膜の光透過率の間に、一定波長の範
囲において、具体的な関係を見出し、非接触法によって
膜の表面電気抵抗値を測定すると共に均質な透明導電膜
を製造する方法を発明するに至った。すなわち本発明は
透明導電膜の光透過率を測定し、得られる測定値から、
あらかじめ求められた表面抵抗値と光透過率の関係式を
用いて表面抵抗値を算出し、その算出された値により製
膜工程における操作を制御することによって、均一な表
面抵抗値を有する透明導電膜の製造方法、及び表面抵抗
値の測定装置に係るものである。Means for Solving the Problems The present inventors have conducted intensive studies in order to solve the above-mentioned problems, and as a result, a constant value has been established between the surface electric resistance (R) of the transparent conductive film and the light transmittance of the film. The inventors found a specific relationship in the wavelength range, and came to invent a method of measuring the surface electric resistance of the film by a non-contact method and manufacturing a homogeneous transparent conductive film. That is, the present invention measures the light transmittance of the transparent conductive film, and from the measured value obtained,
A transparent conductive material having a uniform surface resistance value is calculated by calculating the surface resistance value using a relational expression of the surface resistance value and the light transmittance obtained in advance, and controlling the operation in the film forming process based on the calculated value. The present invention relates to a method for manufacturing a film and a device for measuring a surface resistance value.
【0005】一般に酸化物系透明導電膜は、酸化が進む
につれて不透明で表面抵抗値の小さい金属質の膜から、
透明だが表面抵抗値の大きい半導体の膜へと変わる途中
に、光透過率が高く、かつ表面抵抗値の小さい領域があ
る。本発明者らは、この領域について詳細に調べたとこ
ろ、表面抵抗値と光透過率の間に一定の関係があること
を見出した。図1は被膜形成時における操作要因の一つ
である酸素供給量の変動に伴う光透過率と表面抵抗値の
関係を示す。さらに詳しくこの関係を調べていくと、図
2に示すように、表面抵抗値、光透過率及び測定波長の
間には、一定の関係があり、特に測定波長が300nm
乃至1000nmにおいて、この傾向が強いことが見出
された。例えば、340nm及び380nmの波長につ
いては、測定波長λ、光透過率T(λ)について、図3
に示す関係が見られ、これを数式化すると一般的に表面
抵抗値Rに関してR=A・EXP(−B・T(λ))の
関係式を得る。式中A・Bは定数であり、いつも一定の
値をとるとは限らない。すなわち、透明導電膜は金属酸
化物被膜を真空蒸着法、スパッタ法等によって透明基盤
上に付着させるため、測定される光透過率は、基盤の光
透過率及び該被膜の光透過率の重ね合わせたものになる
こと、又被膜においてもその光透過率はその酸化度、膜
の厚みにより影響を受けるためである。そのため、上記
の関係式を求めるためには、被膜の厚みや、酸化度の異
った試料についてあらかじめ光透過率と表面電気抵抗値
の関係を求めておくことが必要である。関係式を求める
ための表面抵抗値の測定は従来法による接触式の測定法
によって求めることができる。この場合、測定は関係式
を求めるための試料についてあらかじめ測定するもので
あって、生産工程における膜の損傷とは無関係である。
得られる関係式は上式を簡略化して、折線又は、多次曲
線等によって近似することができる。透過光の波長は、
300nm乃至1000nmが好ましいが、更に好まし
くは、330nm乃至は500nmの範囲である。In general, an oxide-based transparent conductive film is made of a metal film having an opaque and low surface resistance as oxidation proceeds.
In the course of changing to a semiconductor film which is transparent but has a large surface resistance, there is a region where the light transmittance is high and the surface resistance is small. The present inventors have examined this region in detail and found that there is a certain relationship between the surface resistance value and the light transmittance. FIG. 1 shows the relationship between the light transmittance and the surface resistance value accompanying a change in the oxygen supply amount, which is one of the operating factors during the film formation. When this relationship is examined in more detail, as shown in FIG. 2, there is a certain relationship between the surface resistance value, the light transmittance, and the measurement wavelength, and particularly, the measurement wavelength is 300 nm.
It was found that this tendency was strong at 1000 nm. For example, for the wavelengths of 340 nm and 380 nm, the measurement wavelength λ and the light transmittance T (λ) are shown in FIG.
The relationship shown in the following is seen, and when this is converted into a mathematical expression, a relational expression of R = A.EXP (-BT (.lamda.)) Is generally obtained with respect to the surface resistance value R. In the formula, A and B are constants, and do not always take constant values. That is, since the transparent conductive film attaches a metal oxide film on the transparent substrate by a vacuum deposition method, a sputtering method, or the like, the measured light transmittance is obtained by superimposing the light transmittance of the substrate and the light transmittance of the film. This is also because the light transmittance of the film is affected by the degree of oxidation and the thickness of the film. Therefore, in order to determine the above relational expression, it is necessary to determine in advance the relationship between the light transmittance and the surface electrical resistance value for samples having different coating thicknesses and oxidation degrees. The measurement of the surface resistance value for obtaining the relational expression can be obtained by a conventional contact-type measuring method. In this case, the measurement is performed in advance on the sample for obtaining the relational expression, and is not related to the damage of the film in the production process.
The obtained relational expression can be simplified from the above expression and approximated by a broken line or a polynomial curve. The wavelength of the transmitted light is
The range is preferably from 300 nm to 1000 nm, and more preferably from 330 nm to 500 nm.
【0006】透明導電膜の被膜を形成する金属酸化物と
しては、酸化インジウム、酸化インジウム・酸化すず
(ITO)、酸化すず、酸化亜鉛、酸化亜鉛・酸化アル
ミニウム、酸化カドミウム・酸化すず等があり、特にI
TO、酸化すず系が適している。膜の基板としては、石
英ガラス、ホウケイ酸ガラス、低アルカリガラス等のガ
ラス、サファイア等のセラミックス、ポリエチレン、ポ
リプロピレン、ポリエチレンテレフタレート、ポリ塩化
ビニル等の高分子膜に適用されるが、特に長尺の被膜形
成が可能な高分子膜が好ましい。As the metal oxide forming the transparent conductive film, there are indium oxide, indium oxide / tin oxide (ITO), tin oxide, zinc oxide, zinc oxide / aluminum oxide, cadmium oxide / tin oxide, and the like . Especially I
TO and tin oxide are suitable. As a substrate of the film, quartz glass, borosilicate glass, glass such as low alkali glass , ceramics such as sapphire , polyethylene, polypropylene, polyethylene terephthalate, applied to polymer films such as polyvinyl chloride, especially long A polymer film capable of forming a film is preferable.
【0007】透明導電膜の作成方法としては、種々知ら
れているが、真空蒸着法、スパッター法、イオンプレー
ティング法などの物理蒸着法(PVD)、あるいは化学
蒸着法(CVD)などが適宜用いられる。真空蒸着法と
は、10-3Torr以下の高真空下で、薄膜材料を加熱
蒸発させ、これを基盤上に堆積させる。真空蒸着法は装
置が簡単であり、高い成膜速度が容易に得られる等の長
所をもつが、基盤と膜との付着速度が弱く、組成、膜厚
制御が難しい等の欠点ももつ。スパッター法とは、低圧
気体放電において、イオンや原子等の数+eV以上の高
運動エネルギー粒子が固体(ターゲット)に衝突し、タ
ーゲット表面から、固体構成原子或いは、分子が弾きと
ばされる現象を利用して、被膜を形成する。真空蒸着に
くらべ、被膜と基盤との付着力が大きく、高融点物質の
膜でも製膜可能であり、被膜の組成、膜厚の制御も容易
である。化学蒸着法とは、形成させようとする薄膜材料
を構成する元素からなる1種または2種類以上の化合物
又は、単体のガスを反応領域の基盤上に供給し、気相
中、又は基盤表面上での化学反応により、所望の薄膜を
形成させる方法である。このように透明導電膜の作成法
としては、種々知られているが、本発明においては、こ
れらの方法に適用することができる。例えば、スパッタ
ー法の場合、電源として、直流、高周波又ターゲットと
しては酸化物、金属を用いる等、様々な方法があるが、
どのような場合にも適用できる。スパッター法での制御
パラメーターとしては、スパッター時の真空圧、酸素分
圧、酸素流量、スパッター電流、電圧等があり、例え
ば、スパッター圧としては5×10-4〜8×10-2To
rr、酸素分圧5×10-6〜10-2Torrの範囲が好
ましい。又、スパッター電流は、0.2〜100Å、ス
パッター電力0.1〜100Kwの範囲が好ましい。Various methods for forming the transparent conductive film are known, and a physical vapor deposition method (PVD) such as a vacuum vapor deposition method, a sputtering method, an ion plating method, or a chemical vapor deposition method (CVD) is appropriately used. Can be In the vacuum deposition method, a thin film material is heated and evaporated under a high vacuum of 10 −3 Torr or less, and deposited on a substrate. The vacuum vapor deposition method has the advantages that the apparatus is simple and a high film-forming rate can be easily obtained, but it also has disadvantages such as low adhesion speed between the substrate and the film, and difficulty in controlling the composition and film thickness. The sputter method uses a phenomenon in which high kinetic energy particles, such as ions and atoms, of several + eV or more collide with a solid (target) in a low-pressure gas discharge, and solid constituent atoms or molecules are repelled from the target surface. To form a coating. Compared to vacuum deposition, the adhesion between the film and the substrate is large, and it is possible to form a film of a high melting point material, and it is easy to control the composition and thickness of the film. Chemical vapor deposition is a method in which one or two or more compounds composed of elements constituting a thin film material to be formed, or a single gas is supplied to a base of a reaction region, and in a gas phase or on a surface of the base. Is a method of forming a desired thin film by the chemical reaction in the above. As described above, various methods for forming the transparent conductive film are known, but the present invention can be applied to these methods. For example, in the case of the sputtering method, there are various methods such as using a direct current as a power supply, a high frequency or using an oxide or a metal as a target,
Applicable in any case. The control parameters in the sputter method include vacuum pressure during sputtering, oxygen partial pressure, oxygen flow rate, sputtering current, voltage and the like. For example, the sputtering pressure is 5 × 10 -4 to 8 × 10 -2 To
rr, the oxygen partial pressure is preferably in the range of 5 × 10 −6 to 10 −2 Torr. Further, sputtering current, 0.2 to 100 Å, preferably in the range of sputter power 0.1~100Kw.
【0008】又、真空蒸着法においては、蒸着源材料と
して、インジウム、すず等の金属、合金や酸化インジウ
ム、酸化すず等の化合物が用いられる。また、加熱方式
としては、抵抗加熱、高周波誘導加熱、電子ビーム加熱
等を用いることができる。また、反応性ガスとして、酸
素、窒素、水蒸気等を導入したり、オゾン添加、イオン
アシスト等の手段を用いた反応性蒸着を用いてもよい。
また、基盤にバイアス等を加えたり、基盤温度を上昇、
あるいは、冷却したり等、本発明の目的を損なわない限
りに於て、製膜時の操作条件を変更することができる。
スパッター法や真空蒸着法等のほかの作成法でも同様で
ある。真空蒸着法での制御パラメーターとしては、上記
の外に蒸着時の真空圧、酸素分圧等があり加熱電力等が
あり、例えば、蒸着時の真空圧としては、1×10-5〜
5×10-1Torr、加熱電力、0.1〜100Kwの
範囲が好ましい。又各種製膜法に共通する制御パラメー
ターとしては、基盤の送り速度、基盤温度等がある。表
面抵抗の制御方法としては、膜の酸化度の制御と膜厚の
制御の2つに分けられる。酸化度の制御方法としては、
酸化雰囲気を調整するための酸素分圧、酸素流量、アル
ゴンガス流量等と反応性を制御するための基盤温度、オ
ゾン添加、バイアス付加等がある。又、膜厚の制御のた
めには、基盤送り速度、製膜速度、膜厚制限板等の調節
等が有効である。例えば、表面抵抗値を下げたいときに
は、酸化度を上げるか、膜厚を上げるかの2つの方法が
あり、酸化度を上げるには、O2流量を、例えば100
cc/分から105cc/分と多くする。流量のコント
ロールとしては、真空槽の大きさ、製膜条件により多少
異なるものの0.5cc/分程度の感度での制御が好ま
しい。一方、膜厚を上げるためには、フイルムの送り速
度を下げるか、製膜速度を上げる方法があり、そのため
に、例えば、スパッター電力を上げる。スパッター電力
としては、例えば2Kwを2.2Kwに上げ、0.01
〜0.05Kw程度の感度での制御が好ましい。[0008] In the vacuum deposition method, metals such as indium and tin, alloys and compounds such as indium oxide and tin oxide are used as a vapor deposition source material. As a heating method, resistance heating, high-frequency induction heating, electron beam heating, or the like can be used. Further, oxygen, nitrogen, water vapor, or the like may be introduced as a reactive gas, or reactive vapor deposition using means such as ozone addition or ion assist may be used.
In addition, a bias is applied to the base, the base temperature rises,
Alternatively, as long as the object of the present invention is not impaired, such as cooling, the operating conditions at the time of film formation can be changed.
The same applies to other forming methods such as a sputter method and a vacuum evaporation method. The control parameters in the vacuum deposition method, a vacuum pressure during deposition outside the above there is an oxygen partial pressure has heating power and the like, for example, the vacuum pressure during the deposition, 1 × 10 -5 ~
5 × 10 −1 Torr, heating power, and a range of 0.1 to 100 Kw are preferable. In addition, control parameters common to various film forming methods include a feed speed of a substrate, a substrate temperature, and the like. table
The method of controlling the sheet resistance is divided into two methods , control of the degree of oxidation of the film and control of the film thickness. As a method for controlling the degree of oxidation,
There are an oxygen partial pressure for adjusting an oxidizing atmosphere, an oxygen flow rate, an argon gas flow rate, and the like, and a substrate temperature for controlling reactivity, ozone addition, bias addition, and the like. In order to control the film thickness, it is effective to adjust the substrate feeding speed, the film forming speed, the film thickness limiting plate, and the like. For example, if you want to lower the surface resistance, increase the degree of oxidation, there are of two ways increasing the film thickness, the increase of oxidation, the O 2 flow rate, for example 100
Increase from cc / min to 105 cc / min. The flow rate is preferably controlled at a sensitivity of about 0.5 cc / min, although it may vary somewhat depending on the size of the vacuum chamber and the film forming conditions. On the other hand, in order to increase the film thickness, there are methods of decreasing the film feeding speed or increasing the film forming speed. For this purpose, for example, the sputtering power is increased. As the sputter power, for example, 2 Kw is increased to 2.2 Kw, and
Control with a sensitivity of about 0.05 Kw is preferred.
【0009】図4は本発明の方法を実施する透明導電膜
の製造装置及び本発明の膜の表面抵抗値を測定する測定
装置の概略図の例示である。図において、巻出しロール
5から送り出される透明基盤膜8は、チルロール4に導
かれ、その下方部においてスパッターターゲット7によ
り金属酸化物被膜が該透明基盤膜面に形成され、巻取り
ロール6によって巻取られる。一方、光源部1の光源か
らの光は光ファイバーによって真空槽11に導かれ、膜
を透過した光は、再び光ファイバーによって、槽外に導
かれ、分光部9のフイルターにより分光され、受光部1
0のフォトメーターによって電気信号に変換され、コン
ピューターを有する演算処理部12により、前述の関係
式により表面抵抗値を表示する値に変換され出力され
る。該出力は出力制御装置22に入力され、膜の表面抵
抗値が一定となる様に製膜工程の操作要因であるターゲ
ットの加熱電流、膜供給速度、酸素ガスの供給速度等の
製膜操作が制御される。制御はPID制御によっておこ
なうことができる。膜面における投光、受光は膜面近く
でおこなうのが好ましく、光ファイバーを用いて膜面近
くの任意の位置においておこなうのが便利である。製膜
工程においてはこの投光端、受光端を一点に固定するの
でなく膜の巾方向に膜を傷つけることなくトラバースさ
せ巾方向の表面抵抗値の平均値や、分布を知ることがで
きる。膜の巾方向における表面抵抗値の分布が許容範囲
をはずれる場合には、膜の巾を減少させたり、ターゲッ
トを膜の巾方向に複数個用いたり、スパッターターゲッ
トと膜面との間に遮蔽板を用いることができる。FIG. 4 is an example of a schematic view of an apparatus for producing a transparent conductive film for performing the method of the present invention and a measuring apparatus for measuring the surface resistance of the film of the present invention. In the drawing, a transparent base film 8 sent out from an unwinding roll 5 is guided to a chill roll 4, a metal oxide film is formed on the surface of the transparent base film by a sputter target 7 below the chill roll 4, and is wound by a winding roll 6. Taken. On the other hand, light from the light source of the light source unit 1 is guided to the vacuum chamber 11 by an optical fiber, and light transmitted through the film is again guided to the outside of the chamber by the optical fiber, separated by the filter of the light splitting unit 9, and separated by the filter of the light splitting unit 9.
The signal is converted into an electric signal by a photometer of 0, and converted into a value indicating the surface resistance value by the above-described relational expression by the arithmetic processing unit 12 having a computer, and output. The output is input to the output control device 22, and a film forming operation such as a target heating current, a film supply speed, and an oxygen gas supply speed, which are operation factors of the film formation process, is performed so that the surface resistance value of the film becomes constant. Controlled. The control can be performed by PID control. Light emission and light reception on the film surface are preferably performed near the film surface, and it is convenient to use an optical fiber at an arbitrary position near the film surface. In the film forming process, the light emitting end and the light receiving end are not fixed to one point, but are traversed without damaging the film in the width direction of the film, and the average value and distribution of the surface resistance values in the width direction can be known. If the distribution of the surface resistance in the width direction of the film is out of the allowable range, reduce the width of the film, use multiple targets in the width direction of the film, or use a shielding plate between the sputter target and the film surface. Can be used.
【0010】光源部1は、真空槽内の透明導電膜に測定
範囲に該当する300nm乃至1000nmの波長の光
を照射する機能が必要であるが、連続投光でも断続投光
でもよく、また、光を絞ったり、平行光にして投光して
もよい。分光部9は、少なくとも透明導電膜の吸収特性
を示す波長に分光する機能があればよい。フィルターに
おいて分光される光は、あらかじめ定めた一つの波長で
も良いが、光源光量の変動等の影響を除くために基準と
なる波長を併せて測定し、その比によって表面抵抗値を
算出し、測定精度の向上をはかることもできる。受光部
10は、透明導電膜の光吸収波長帯の受光感度特性のよ
い光電子増倍管、シリコンフォトダイオード等がある。
演算処理部12は、透明導電膜を透過分光された光を、
その強度に応じた電気信号に変換する受光素子と、得ら
れた電気信号を演算できるレベルまで増幅する増幅回路
と、バックグランドノイズを除去するフィルタ回路と、
演算により、表面抵抗値をもとめる演算回路と結果をモ
ニタする表示回路で構成され、演算は、アナログ演算で
も、デジタル演算でもよい。The light source unit 1 needs to have a function of irradiating the transparent conductive film in the vacuum chamber with light having a wavelength of 300 nm to 1000 nm corresponding to the measurement range, and it may be continuous light emission or intermittent light emission. The light may be narrowed, or the light may be projected as parallel light. The light splitting unit 9 only needs to have a function of splitting light into at least a wavelength indicating the absorption characteristics of the transparent conductive film. The light to be spectrally separated by the filter may have a predetermined wavelength.However, in order to eliminate influences such as fluctuations in the light source light amount, the reference wavelength is also measured, and the surface resistance value is calculated based on the ratio. Accuracy can also be improved. The light receiving unit 10 includes a photomultiplier tube, a silicon photodiode, and the like having good light receiving sensitivity characteristics in a light absorption wavelength band of the transparent conductive film.
The arithmetic processing unit 12 converts the light transmitted through the transparent conductive film into
A light-receiving element that converts the electric signal into an electric signal corresponding to the intensity, an amplifier circuit that amplifies the obtained electric signal to a level that can be calculated, a filter circuit that removes background noise,
It is composed of an operation circuit for obtaining the surface resistance value by operation and a display circuit for monitoring the result. The operation may be analog operation or digital operation.
【0011】[0011]
【実施例1】 図4に示す装置において光源にキセノンラ
ンプを用い、紫外線透過型石英光ファイバーで槽内に光
を導き、透明導電膜表面から5mm離した位置にファイ
バー先端部を固定し、その先端部から透明導電膜表面に
対して垂直に連続光を投光し、透過した光を膜の裏面か
ら5mm離した位置に固定された上記光ファイバーと同
種の光ファイバーで受けて真空槽の外に導き、該光ファ
イバーからの光バンドパスフィルタで380nmの透過
光を通過させ、その光をシリコンフォトダイオードで電
気信号に変換し、その信号をロックインアンプで増幅さ
せた後12ビットアナログ/デジタル変換器でデジタル
値に変換し、マイクロコンピュータ回路で演算し、表面
抵抗値を連続的に測定した。測定波長λと表面抵抗値R
の関係式はあらかじめ測定された関係式R=1.45×
105EXP(−10.4T(λ))を使用した。被膜
を形成させるための合金材料としてインジウム・すず
(すず:5重量%含有)をターゲットとして用い、反応
性スパッターによって膜厚みが75μmのポリエステル
フイルムに透明被膜(被膜の厚み300オングストロー
ム)を形成した。製膜条件は真空圧3×10 -3 Tor
r、スパッター電流5A、スパッター電圧300Vと
し、フイルムの送り速度は10m/分で成膜した。酸素
ガスの供給量の制御は、マスフロー流量計の入力電圧を
表面抵抗値の検出装置より得られる出力値により制御す
ることにより、10cc/分乃至100cc/分の間で
制御した。結果を表1に示す。本発明に係る非接触式の
表面抵抗測定装置を使うため、得られた膜には全く損傷
は見られず、生産歩留りが大幅に向上した。又表面抵抗
のバラツキは±3%以内となり、従来の市販品のレベル
である±20%に比べて著しく改善された。 Example 1 In the apparatus shown in FIG . 4, a xenon lamp was used as a light source, light was guided into the tank with an ultraviolet transmitting quartz optical fiber, and the fiber tip was fixed at a position 5 mm away from the surface of the transparent conductive film. A continuous light is projected perpendicularly to the surface of the transparent conductive film from the portion, and the transmitted light is received by an optical fiber of the same type as the optical fiber fixed at a position separated from the back surface of the film by 5 mm, and guided out of the vacuum chamber. The transmitted light of 380 nm is passed through the optical band pass filter from the optical fiber, the light is converted into an electric signal by a silicon photodiode, the signal is amplified by a lock-in amplifier, and then the signal is digitalized by a 12-bit analog / digital converter. The values were converted into values, calculated by a microcomputer circuit, and the surface resistance was continuously measured. Measurement wavelength λ and surface resistance R
Is a previously measured relational expression R = 1.45 ×
10 5 EXP (-10.4T (λ)) was used. A transparent film (thickness of 300 Å) was formed on a 75 μm-thick polyester film by reactive sputtering using indium tin (containing 5% by weight of tin ) as an alloy material for forming the film. The film forming condition is a vacuum pressure of 3 × 10 −3 Torr.
r, a sputter current of 5 A, and a sputter voltage of 300 V, and the film was formed at a feed speed of 10 m / min. The supply rate of the oxygen gas was controlled between 10 cc / min and 100 cc / min by controlling the input voltage of the mass flow meter with the output value obtained from the surface resistance detector. Table 1 shows the results. Since the non-contact type surface resistance measuring device according to the present invention was used, no damage was observed on the obtained film, and the production yield was greatly improved. Further, the variation in the surface resistance was within ± 3%, which was remarkably improved as compared with the level of a conventional commercially available product of ± 20%.
【0012】[0012]
【実施例2】実施例1において、使用する装置におい
て、ITO(SnO 2 :10wt%含有)の焼結ターゲ
ットを用い、マグネトロンスパッターによって膜厚みが
75μmであるポリエステルフィルムに膜厚み200オ
ングストロームの被膜を成形した。製膜条件は真空圧3
×10 -3 Torr、スパッター電流3A、スパッター電
圧250Vとし、膜の送り速度は3m/分で成膜した。
製膜における制御は膜抵抗測定装置から得られた出力値
により、スパッター電流値を3.5A乃至5.0Aの間
でフィードバックしながら5回成膜をおこなった。表面
抵抗値の測定結果を表2に示す。一つの膜についての長
さ方向のばらつき、及び膜間のばらつきは従来法に比べ
非常に小さく、目標値の200Ω/口に比べ最大のずれ
で3%であった。Example 2 In Example 1, a 200 Å-thick polyester film having a thickness of 75 μm was applied to a polyester film having a thickness of 75 μm by magnetron sputtering using a sintered target of ITO ( containing SnO 2 : 10 wt%). Molded. Film formation conditions are vacuum pressure 3
The film was formed at a feed rate of 3 m / min, with × 10 −3 Torr, a sputter current of 3 A, and a sputter voltage of 250 V.
In the control of the film formation, the film formation was performed five times while feeding back the sputtering current value between 3.5 A and 5.0 A based on the output value obtained from the film resistance measuring device. Table 2 shows the measurement results of the surface resistance values. The variation in the length direction of one film and the variation between the films were very small as compared with the conventional method, and the maximum deviation was 3% compared with the target value of 200Ω / port.
【0013】[0013]
【比較例1】実施例1と同様に、反応性スパッターでI
TO膜を製膜し、その時、製膜した透明導電膜に銅電極
を接触させて、抵抗値のモニターをおこないながら製膜
条件を変えながら製膜をおこなった。このサンプルを取
り出し、表面抵抗値を測定したが、フイルム上に電極の
接触により生ずる傷が入っており、作成した透明導電膜
の良品率は60%であった。表面抵抗値は目標値の20
0Ω/口に対し、±20%であった。Comparative Example 1 In the same manner as in Example 1 , the reactive sputtering
A TO film was formed. At this time, a copper electrode was brought into contact with the formed transparent conductive film, and the film formation was performed while changing the film forming conditions while monitoring the resistance value. The sample was taken out and its surface resistance was measured. The film was found to have scratches caused by the contact of the electrodes, and the yield of the transparent conductive film thus produced was 60%. The surface resistance value is the target value of 20
It was ± 20% with respect to 0Ω / mouth.
【0014】[0014]
【比較例2】実施例1と同様に反応性スパッターでIT
O膜を成膜したが、特にモニターはおこなわなかった。
この膜の表面抵抗を測定した。その結果製膜の初期にお
いては表面抵抗値は良好であったが、徐々に酸化度が増
し、表面抵抗値が増大し、最後には導電性も失なってし
まった。Comparative Example 2 In the same manner as in Example 1 , the reactive sputtering
An O film was formed, but no particular monitoring was performed.
The surface resistance of this film was measured. As a result, the surface resistance was good at the beginning of the film formation, but the degree of oxidation gradually increased, the surface resistance increased, and finally the conductivity was lost.
【0015】[0015]
【表1】 [Table 1]
【表2】 [Table 2]
【0016】[0016]
【発明の効果】透明導電膜の光透過率と膜の表面抵抗値
の関係をあらかじめ測定し、得られる関係式を入力した
演算処理部を有する表面抵抗測定装置を製膜工程にオン
ラインで使用し、製膜工程における生産条件を制御する
ことにより、均一な表面抵抗値を有する透明導電膜を膜
の損傷を伴うことなく製造できる。According to the present invention, the relationship between the light transmittance of the transparent conductive film and the surface resistance value of the film is measured in advance, and a surface resistance measuring device having an arithmetic processing unit into which the obtained relational expression is input is used online in the film forming process. By controlling the production conditions in the film forming process, a transparent conductive film having a uniform surface resistance can be manufactured without damaging the film.
【図1】透明導電膜における光透過率と表面抵抗値の一
般的な関係を示す。FIG. 1 shows a general relationship between light transmittance and surface resistance of a transparent conductive film.
【図2】透明導電膜における光の波長、光透過率及び膜
の表面抵抗値を示す。FIG. 2 shows light wavelength, light transmittance, and surface resistance of a transparent conductive film.
【図3】図2における特定の関係を示す。FIG. 3 shows a specific relationship in FIG.
【図4】本発明の方法を実施するための製膜装置の概略
図を本発明の測定装置の概略図と共に例示する。FIG. 4 illustrates a schematic view of a film forming apparatus for carrying out the method of the present invention, together with a schematic view of a measuring apparatus of the present invention.
【符号の説明】 1 光源部 2 真空排気系 3 光ファイバー 4 チルロール 5 巻出しロール 6 巻取りロール 7 ターゲット 8 透明基板膜 9 分光部 10 受光部 11 真空槽 12 演算処理部 13 変換器 14 質量分析計 15 真空度計 16 温度センサー 17 速度センサー 18 スパッター電源 19 イオン化電源 20 流量計 21 モーター 22 出力制御装置 23 信号入力装置[Description of Signs] 1 light source unit 2 evacuation system 3 optical fiber 4 chill roll 5 unwind roll 6 take-up roll 7 target 8 transparent substrate film 9 spectral unit 10 light receiving unit 11 vacuum chamber 12 arithmetic processing unit 13 converter 14 mass spectrometer 15 Vacuum gauge 16 Temperature sensor 17 Speed sensor 18 Sputter power supply 19 Ionization power supply 20 Flow meter 21 Motor 22 Output control device 23 Signal input device
───────────────────────────────────────────────────── フロントページの続き (58)調査した分野(Int.Cl.7,DB名) C23C 14/00 - 14/58 ──────────────────────────────────────────────────続 き Continued on the front page (58) Field surveyed (Int.Cl. 7 , DB name) C23C 14/00-14/58
Claims (2)
導電膜の光透過率を測定し、該測定値を演算処理して得
られる膜表面電気抵抗値により上記製造工程における製
膜操作を制御することを特徴とする透明導電膜の製造方
法。In a manufacturing process of a transparent conductive film, a light transmittance of the transparent conductive film is measured, and a film forming operation in the manufacturing process is controlled by a film surface electric resistance value obtained by processing the measured value. A method for producing a transparent conductive film.
を有し、あらかじめ該演算処理部に入力された透明導電
膜の光透過率と膜表面電気抵抗値の関係式と、分光部よ
り得られる透明導電膜の光透過率により、膜表面電気抵
抗値を演算し、出力する膜表面電気抵抗値の測定装置。2. A transparent conductive material having a light source unit, a spectral unit, a light receiving unit, and an arithmetic processing unit, which is input to the arithmetic processing unit in advance.
An apparatus for calculating and outputting a film surface electric resistance value based on a relational expression between a film light transmittance and a film surface electric resistance value and a light transmittance of a transparent conductive film obtained from a spectroscopic unit.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP34927691A JP3152249B2 (en) | 1991-12-05 | 1991-12-05 | Method and apparatus for producing transparent conductive film |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP34927691A JP3152249B2 (en) | 1991-12-05 | 1991-12-05 | Method and apparatus for producing transparent conductive film |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH05156439A JPH05156439A (en) | 1993-06-22 |
| JP3152249B2 true JP3152249B2 (en) | 2001-04-03 |
Family
ID=18402673
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP34927691A Expired - Fee Related JP3152249B2 (en) | 1991-12-05 | 1991-12-05 | Method and apparatus for producing transparent conductive film |
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| Country | Link |
|---|---|
| JP (1) | JP3152249B2 (en) |
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| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2012237599A (en) * | 2011-05-10 | 2012-12-06 | Ulvac Japan Ltd | Processed body inspection device |
| WO2014112481A1 (en) * | 2013-01-16 | 2014-07-24 | 日東電工株式会社 | Transparent conductive film and production method therefor |
| KR101525767B1 (en) * | 2013-08-13 | 2015-06-04 | 포톤데이즈(주) | Apparatus for Measuring Electrical Property of Film Element with Light Scan and Method for the Same |
| JP6200729B2 (en) * | 2013-08-27 | 2017-09-20 | 日立造船株式会社 | Sputtering apparatus and thin film forming method |
-
1991
- 1991-12-05 JP JP34927691A patent/JP3152249B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPH05156439A (en) | 1993-06-22 |
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