Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JPS5812722B2 - Sankabutsu Handout Taihakumakuno Seizouhouhou - Google Patents
[go: Go Back, main page]

JPS5812722B2 - Sankabutsu Handout Taihakumakuno Seizouhouhou - Google Patents

Sankabutsu Handout Taihakumakuno Seizouhouhou

Info

Publication number
JPS5812722B2
JPS5812722B2 JP6682675A JP6682675A JPS5812722B2 JP S5812722 B2 JPS5812722 B2 JP S5812722B2 JP 6682675 A JP6682675 A JP 6682675A JP 6682675 A JP6682675 A JP 6682675A JP S5812722 B2 JPS5812722 B2 JP S5812722B2
Authority
JP
Japan
Prior art keywords
substrate
evaporation source
plasma
thin film
film
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
Application number
JP6682675A
Other languages
Japanese (ja)
Other versions
JPS51142697A (en
Inventor
篠原紘一
清水康博
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP6682675A priority Critical patent/JPS5812722B2/en
Publication of JPS51142697A publication Critical patent/JPS51142697A/en
Publication of JPS5812722B2 publication Critical patent/JPS5812722B2/en
Expired legal-status Critical Current

Links

Classifications

    • CCHEMISTRY; METALLURGY
    • C23COATING 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
    • C23CCOATING 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
    • C23C14/00Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
    • C23C14/0021Reactive sputtering or evaporation

Landscapes

  • Chemical & Material Sciences (AREA)
  • Chemical Kinetics & Catalysis (AREA)
  • Engineering & Computer Science (AREA)
  • Materials Engineering (AREA)
  • Mechanical Engineering (AREA)
  • Metallurgy (AREA)
  • Organic Chemistry (AREA)
  • Physical Vapour Deposition (AREA)
  • Apparatuses And Processes For Manufacturing Resistors (AREA)
  • Manufacturing Of Electric Cables (AREA)

Description

【発明の詳細な説明】 本発明は、酸化物半導体薄膜の製造方法に関する。[Detailed description of the invention] The present invention relates to a method for manufacturing an oxide semiconductor thin film.

一般にZn(LTt02pSn02等の酸化物半導体は
、透明電極、螢光材料、サーミスタ等、広範囲の用途を
有する材料であり、各種の薄膜化技術がこれまでに提供
され、実用に供されてきている。
In general, oxide semiconductors such as Zn (LTt02pSn02) are materials that have a wide range of uses, such as transparent electrodes, fluorescent materials, and thermistors, and various thin film techniques have been provided and put into practical use.

ZnO,TiO2等は、n形の半導体として知られ、一
般に化学量論的組成からはずれたイオン結晶において金
属あるいは金属イオンが過剰の場合につくられることが
知られている。
ZnO, TiO2, etc. are known as n-type semiconductors, and are generally known to be produced when metal or metal ions are in excess in an ionic crystal that deviates from the stoichiometric composition.

したがって真空蒸着法により薄膜化することにより、半
導体薄膜を作ることが原理的に可能である。
Therefore, it is theoretically possible to create a semiconductor thin film by thinning it using a vacuum evaporation method.

すなわち、ZnO,TiO2等の酸化物の粉末を電子ビ
ーム加熱、抵抗加熱等の公知の蒸発法により蒸発させる
時、熱解離を起こすことにより金属過剰状態を作ること
ができるからである。
That is, when powders of oxides such as ZnO and TiO2 are evaporated by known evaporation methods such as electron beam heating and resistance heating, a metal-excess state can be created by causing thermal dissociation.

しかし、実際、これを行い、かつ実用に供し得るだけの
制御性をもたせ得ることは困難であり、原子価制御の方
法がとられるのが普通である。
However, in reality, it is difficult to achieve this and to provide sufficient controllability for practical use, and a method of valence control is usually used.

最も良く知られているSnO2は2〜3%のSb203
を含むことにより、面積抵抗で数Ω/cILの低抵抗で
かつ透明な半導体となり、これを透明電極として用いて
いるのである。
The best known SnO2 is 2-3% Sb203
By including , it becomes a transparent semiconductor with a low sheet resistance of several Ω/cIL, and this is used as a transparent electrode.

しかし、この製法は、スプレイ法と呼ばれるもので、高
温(400〜500℃)に保持した基板上にSn,sb
の塩化物の溶液を吹き付ける方法であり、基板にプラス
チック等の低融点材料を用いることは不可能である。
However, this manufacturing method is called a spray method, in which Sn, sb, and
This method involves spraying a chloride solution, and it is impossible to use a low melting point material such as plastic for the substrate.

条件によりプラスチックを基板とすることもできる。Depending on the conditions, plastic can also be used as the substrate.

比較的低温で、半導体薄膜を作る方法に、酸素中蒸着法
■熱処理法がある。
Oxygen evaporation method and heat treatment method are methods for producing semiconductor thin films at relatively low temperatures.

すなわち、10−’mmug程度の酸素中で、ゆっくり
とSn,In等の金属を蒸発させて、酸素雰囲気で15
0℃〜200℃程度の熱処理をすることにより、比較的
低抵抗の半導体薄膜を作る方法である。
That is, metals such as Sn and In are slowly evaporated in about 10 mm of oxygen, and then 15 mm is heated in an oxygen atmosphere.
This is a method of making a semiconductor thin film with relatively low resistance by performing heat treatment at about 0°C to 200°C.

この方法で原子価制御をするのは、二元蒸着であり、す
薔わち、例えばSn*Sbを別々のボートにのせ、別電
源により加熱制御するのであるが、極めて制御がやっか
いで再現性に乏しい。
This method of controlling valence is binary vapor deposition, in which, for example, Sn*Sb is placed on separate boats and heated by a separate power source, but control is extremely difficult and reproducibility is difficult. Poor.

本発明は、再現性良く、かつ低抵抗から高抵抗まで広範
囲の望む抵抗値を有する半導体薄膜を得る方法を提供す
ることを目的とする。
An object of the present invention is to provide a method for obtaining a semiconductor thin film with good reproducibility and having a desired resistance value over a wide range from low resistance to high resistance.

具体的には、原子価制御にN原子を用いることにより、
導電率の制御を行う方法に関する。
Specifically, by using N atoms for valence control,
This invention relates to a method for controlling conductivity.

酸化物半導体としてSnO2を例にとーて、以下説明す
る。
A description will be given below using SnO2 as an example of an oxide semiconductor.

図面は本発明を実施するための装置の一例であり、真空
容器1内に基板2と蒸発源3を対向配設する。
The drawing shows an example of an apparatus for carrying out the present invention, in which a substrate 2 and an evaporation source 3 are disposed facing each other in a vacuum container 1.

蒸発源3は公知の電子ビーム蒸発源、抵抗加熱蒸発源、
誘導加熱蒸発源等いずれで構成しても良いが、説明は抵
抗加熱で行った。
The evaporation source 3 is a known electron beam evaporation source, a resistance heating evaporation source,
Although it may be configured with any type of induction heating evaporation source, the explanation was given using resistance heating.

すなわち、Ta,MotW等の高融点金属で出来たボー
ト3′にのせた蒸発物質、Sn02の場合Sn金属粒3
の蒸気化は、絶縁導入端子14を介して、加熱電源4の
制御により、ボート3′を通電加熱することにより行う
方式の蒸発源を配設した。
That is, an evaporated substance placed on a boat 3' made of a high-melting point metal such as Ta or MotW, or Sn metal particles 3 in the case of Sn02.
An evaporation source was provided in which the boat 3' was evaporated by heating the boat 3' under the control of the heating power source 4 via the insulated introduction terminal 14.

蒸発源の一端は直流的に接地してあるが、必ずしもそれ
にこだわらず、コンデンサを介して接地してもよい。
Although one end of the evaporation source is DC grounded, this is not necessarily the case, and it may be grounded via a capacitor.

基地2は基板ホルダ5に保持される形を示したが、これ
も例えばプラスチックフイルム上にSn02薄膜を形成
する場合は、フイルムの巻取り機構示これに代るであろ
うし、一般に絶縁物が基板の場合は基板の蒸発源対向側
前面に、メッシュ等の開孔部を有する電極を配設する等
の工夫は、基板の種類形状により当熱行われるものであ
るが、本発明の説明は最も簡単な場合について行った。
Although the base 2 is shown to be held by the substrate holder 5, for example, when forming a Sn02 thin film on a plastic film, the film winding mechanism may be used instead. In this case, measures such as arranging an electrode with openings such as a mesh on the front surface of the substrate facing the evaporation source are carried out depending on the type and shape of the substrate, but the explanation of the present invention is most I went to a simple case.

蒸発源3と基板2の間の空間に、プラズマ形成のための
電極6を配設する。
An electrode 6 for plasma formation is provided in the space between the evaporation source 3 and the substrate 2.

プラズマの発生方法は、高周波グロー、直流グローに大
別さわるが、直流グローには、熱陰!プラズマも含む。
Plasma generation methods can be broadly divided into high-frequency glow and DC glow, but DC glow uses hot shade! Including plasma.

最も簡単で、比較的高真空域でプラズマ発生、維持が可
能な高周波グローを用いる場合を図面には示したが、高
周波電源7と、西周波電極6で構成する。
The drawing shows the simplest case of using high frequency glow, which is capable of generating and maintaining plasma in a relatively high vacuum region, and is composed of a high frequency power source 7 and a west frequency electrode 6.

高周波電極6はアルミまたは銅パイプ等のスバイラル構
造が良く用いられるが、形状は筒状、その他適宜設計さ
れるものである。
The high frequency electrode 6 often has a spiral structure such as an aluminum or copper pipe, but the shape may be cylindrical or otherwise designed as appropriate.

真空容器1は、ガラスまたはステンレススチール等で構
成され、例えば油拡散ポンプ、水冷トラップ、油廻転ポ
ンプで構成される真空排気系8に連結している。
The vacuum container 1 is made of glass, stainless steel, or the like, and is connected to a vacuum exhaust system 8 that includes, for example, an oil diffusion pump, a water-cooled trap, and an oil rotary pump.

また真空容器1には、リークバ省グ9,10が連結され
、ガス11.12の源に埠結されている。
Further, leak bars 9 and 10 are connected to the vacuum vessel 1 and connected to a source of gas 11 and 12.

なお基板2は、直流電源13により、接地電位または負
電位にバイアスされる。
Note that the substrate 2 is biased to a ground potential or a negative potential by a DC power supply 13.

勢縁物を!板とする時は前記したメッシュ等の電極に、
基板電位を与える訳である。
A relative! When making it into a plate, use the mesh electrode as described above,
This gives the substrate potential.

本装置を用いて、ガラス基板上にSn02を作成する場
合を例にとり、説明する。
An example of creating Sn02 on a glass substrate using this apparatus will be explained.

真空容器1内は、あらかじめ真空排気系8によりl×l
Q−5mmHg〜1×10−6wlHgに排気される。
The inside of the vacuum container 1 is made up of l×l by the vacuum evacuation system 8 in advance.
Exhausted to Q-5 mmHg to 1 x 10-6 wlHg.

ζの真空度は一義的に決定されるものではないが、高真
空程好ましいが、実用上の差異が認められるのは10−
4maHg程度までしか排気されない場合であり、IX
IO−51mHg以下の値になれば、特に問題はない。
Although the degree of vacuum of ζ is not uniquely determined, the higher the vacuum, the better, but the practical difference is recognized at 10-
This is a case where the exhaust is only about 4maHg, and IX
There is no particular problem if the value is IO-51 mHg or less.

その後、バリアプルリークバルブ9,10のi節により
、02を例えば8X10−4’mHgの分圧になるよう
導入する。
Thereafter, 02 is introduced through the i nodes of the barrier pull leak valves 9 and 10 to a partial pressure of, for example, 8×10 −4′ mHg.

一方N2をIX10−4mmHg導入する。Meanwhile, N2 is introduced at IX10-4 mmHg.

系内の圧力はその時、9X10−4mmHgとなる。The pressure in the system is then 9×10 −4 mmHg.

導入されるガス0211とN212の純度は、市販され
ている圧力ボンベより減圧弁、タンクリザーバを介して
、直接導入して充分で、特に精製装置を付加する必要は
ない。
The purity of the introduced gases 0211 and N212 is sufficient when they are directly introduced from a commercially available pressure cylinder via a pressure reducing valve and a tank reservoir, and there is no need to add any particular purification equipment.

その状態で高周波電源7を動作させて、高周波グロー放
電を発生させる。
In this state, the high frequency power supply 7 is operated to generate high frequency glow discharge.

グローは02/N2の混合比によるが、ピンク色の励起
発光を観察できる。
Although the glow depends on the mixing ratio of 02/N2, pink excited light emission can be observed.

高周波電極6の近傍はイオンシースにより発光は観察さ
れない輝度の暗い部分ができる。
In the vicinity of the high-frequency electrode 6, a dark area where no light emission is observed is formed due to the ion sheath.

ピンク色の部盆はプラズマ状態で、この領域に後述の金
属蒸気を露呈するのが要点であり、そのためのジオメト
リー、スリット等は工夫されるのは当然である。
The pink tray is in a plasma state, and the key point is to expose the metal vapor described below in this region, so it is natural that the geometry, slits, etc. for this purpose must be devised.

タングステン製のボート3lの上にのせたSn3の粒は
外部の加熱電源4の調節により、蒸気化される。
The Sn3 grains placed on the tungsten boat 3l are vaporized by adjusting the external heating power source 4.

この蒸気流は前記プラズマと相互作用の結果、基板2上
に、SnO2膜を形成し、かつN原子が02/N2比の
調節により適当量含まれ、それがドナーとなり、導電率
を向上させる結果となり、望む酸化物半導体薄膜かえら
れることになる。
As a result of interaction with the plasma, this vapor flow forms a SnO2 film on the substrate 2, and N atoms are included in an appropriate amount by adjusting the O2/N2 ratio, which become donors and improve the conductivity. Therefore, the desired oxide semiconductor thin film can be changed.

Sn02の他、Pb02tSin2tTi02pZrO
2,HiO。
In addition to Sn02, Pb02tSin2tTi02pZrO
2.HiO.

についても同様に導電率の制いのではなく、一般的傾向
として、基板と膜の密着力を高めるためにはIKV程度
以上高い方がよい(勿論、物質により異なるが3〜4K
Vを越すと、逆に密着力の低下をきたす現象がみられる
Similarly, in order to increase the adhesion between the substrate and the film, it is better to have it as high as IKV or higher, rather than limiting the conductivity (of course, it varies depending on the material, but 3 to 4K
If V is exceeded, a phenomenon in which the adhesion force decreases is observed.

)が、膜の損傷が逆に増加し、半導体物性に悪影響を及
ぼすので、200v〜500V(蒸発源に対して負の値
)の電圧を印加するのが適当である。
), the damage to the film increases and adversely affects the physical properties of the semiconductor, so it is appropriate to apply a voltage of 200 V to 500 V (a negative value with respect to the evaporation source).

なおN2と02の分圧比は、02の分圧が高い程(高々
5X10−3Torrである。
Note that the higher the partial pressure of N2 and 02 is, the higher the partial pressure of N2 and 02 (at most 5×10 −3 Torr).

)、N2分圧を高くする必要があり(その時が実験的に
およそ1/5である。
), it is necessary to increase the N2 partial pressure (experimentally, this is approximately 1/5 of the time).

)それより02分圧の低い時は、N2は1/5以下に保
持する必要がある。
) When the 02 partial pressure is lower than that, N2 needs to be maintained at 1/5 or less.

次に従来法と本発明法の比較をすると次のようである。Next, a comparison between the conventional method and the method of the present invention is as follows.

従来法:2mmのガラス基板にSn蒸着後、空気中で5
50c、2Hr熱処理したとこ ろ、膜厚は2000A,透明度は可視 域において75%〜80%、抵抗値は IKΩlcA2であった。
Conventional method: After Sn vapor deposition on a 2 mm glass substrate, 5
When heat treated at 50C for 2 hours, the film thickness was 2000A, the transparency was 75% to 80% in the visible range, and the resistance value was IKΩlcA2.

本発明法二同じガラス基板に高周波電力=350W(2
.5KVp陽極電圧)、基板印加 電圧:DC−300V、02:8× 10−4TorrpN2:IXlO−4 Torrにて膜を形成させたところ膜厚 は2000X,透明度は80%〜85 %、抵抗値は50Ω/cA2〜300 Ω/cm2であった。
Method 2 of the present invention High frequency power = 350W (2
.. When a film was formed at 5KVp anode voltage), substrate applied voltage: DC-300V, 02:8×10-4 TorrpN2:IXlO-4 Torr, the film thickness was 2000X, transparency was 80% to 85%, and resistance was 50Ω. /cA2 to 300 Ω/cm2.

次に半導性制御の再現性の比較をすると次のようである
Next, a comparison of the reproducibility of semiconductor control is as follows.

従来法:Snをタングステンボートな用い抵抗加熱蒸発
し、sbを傍熱フィラメント により加熱蒸発したところ、SnO2 (sb)膜の抵抗値は、ioΩ/cft〜500KΩ/
cA2であった。
Conventional method: Sn was evaporated by resistance heating using a tungsten boat, and sb was evaporated by heating using an indirect heating filament. The resistance value of the SnO2 (sb) film was ioΩ/cft to 500KΩ/
It was cA2.

同一条件設定の条件下で製作した場合の抵抗値の バラツキは低抵抗もできるが、大きか った。Resistance value when manufactured under the same condition settings Variations can be made with low resistance, but are they large? It was.

本発明法:高周波電力:400W(2KVp陽極電圧)
で次のガス圧の場合の抵抗値は それぞれ下記のようであった。
Invention method: High frequency power: 400W (2KVp anode voltage)
The resistance values for the following gas pressures were as follows.

(i)02:5X10−4Torr+N2:7X10−
5Torr SnO2N膜の抵抗値:200Ω/cf2〜700Ω/
cm2 (2)02:6X10−4TorrtN2:6X10−
5Torr SnO2N膜の抵抗値:800Ω/cyR〜1.2KΩ
/ctA (3)02:8X10−”forrtN2:IX10−
’Torr Sn02N膜の抵抗値=70Ω/cIt〜18oΩ/d
m2 抵抗値のバラツキは小さかった。
(i) 02:5X10-4Torr+N2:7X10-
5 Torr Resistance value of SnO2N film: 200Ω/cf2~700Ω/
cm2 (2) 02:6X10-4 TorrtN2:6X10-
5Torr SnO2N film resistance value: 800Ω/cyR ~ 1.2KΩ
/ctA (3)02:8X10-”forrtN2:IX10-
'Torr Resistance value of Sn02N film = 70Ω/cIt ~ 18oΩ/d
m2 The variation in resistance value was small.

以上のように本発明によれば、再現性よく、薄膜化でき
、実用価値は大きいものであり、また全て特に基板の加
熱を必要としない点は特筆すべき点で、大形ディスプレ
イ用の透明電極や、EL等への適用、実用化に貢献でき
るものであり、その産業性は大きいものである。
As described above, according to the present invention, it is possible to form a thin film with good reproducibility, and it has great practical value.It is noteworthy that no heating of the substrate is required in any case. It can contribute to the application and practical use of electrodes, EL, etc., and its industrial potential is great.

【図面の簡単な説明】[Brief explanation of the drawing]

図面は本発明の製造方法を実施するために使用する装置
の概略断面正面図である。 1・・・・・・真空容器、2・・・・・・基板、3.3
’・・・・・蒸発源(蒸発物質とボート)、4・・・・
・・加熱電源、6・・・・・・高周波電極、7・・・・
・・高周波電源、11・・・・・・酸素ガス、12・・
・・・・窒素ガス。
The drawing is a schematic cross-sectional front view of an apparatus used to carry out the manufacturing method of the present invention. 1... Vacuum container, 2... Substrate, 3.3
'・・・Evaporation sources (evaporation substances and boats), 4...
... Heating power supply, 6 ... High frequency electrode, 7 ...
...High frequency power supply, 11...Oxygen gas, 12...
...Nitrogen gas.

Claims (1)

【特許請求の範囲】[Claims] 1 真空容器内に基板と蒸発源を対向配設し、両者間の
空間に、酸素・窒素の混合気体プラズマを形成し、蒸発
源より発生させた蒸気流を該プラズマに露呈し、蒸発源
と同電裕または負の電位におかれた基板上に、窒素によ
り原子価制御された酸化物半導体薄膜を形成することを
特徴とする酸化物半導体薄膜の製造方法。
1 A substrate and an evaporation source are arranged facing each other in a vacuum container, a mixed gas plasma of oxygen and nitrogen is formed in the space between them, and a vapor flow generated from the evaporation source is exposed to the plasma, and the vaporization source and the evaporation source are exposed to the plasma. 1. A method for producing an oxide semiconductor thin film, which comprises forming an oxide semiconductor thin film whose valence is controlled by nitrogen on a substrate placed at a high potential or a negative potential.
JP6682675A 1975-06-02 1975-06-02 Sankabutsu Handout Taihakumakuno Seizouhouhou Expired JPS5812722B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6682675A JPS5812722B2 (en) 1975-06-02 1975-06-02 Sankabutsu Handout Taihakumakuno Seizouhouhou

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6682675A JPS5812722B2 (en) 1975-06-02 1975-06-02 Sankabutsu Handout Taihakumakuno Seizouhouhou

Publications (2)

Publication Number Publication Date
JPS51142697A JPS51142697A (en) 1976-12-08
JPS5812722B2 true JPS5812722B2 (en) 1983-03-10

Family

ID=13327018

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6682675A Expired JPS5812722B2 (en) 1975-06-02 1975-06-02 Sankabutsu Handout Taihakumakuno Seizouhouhou

Country Status (1)

Country Link
JP (1) JPS5812722B2 (en)

Also Published As

Publication number Publication date
JPS51142697A (en) 1976-12-08

Similar Documents

Publication Publication Date Title
US4336277A (en) Transparent electrical conducting films by activated reactive evaporation
CN1826423B (en) Transparent conductive oxides
US4224897A (en) Methods of depositing materials on substrates
US4428810A (en) Method and apparatus for depositing conducting oxide on a substrate
US3418229A (en) Method of forming films of compounds having at least two anions by cathode sputtering
US3239368A (en) Method of preparing thin films on substrates by an electrical discharge
JP3779317B2 (en) Thin film formation method
JP4170507B2 (en) Method for producing transparent conductive film
JPS5812722B2 (en) Sankabutsu Handout Taihakumakuno Seizouhouhou
JPS5813006B2 (en) Sankabutsuhandoutaihakumakuno Seizouhouhou
JPS6389656A (en) Electrically conductive transparent film and its formation
JPH03101033A (en) Manufacture of thin film
CN115142033A (en) Non-stoichiometric alumina material and preparation method thereof
JP2018193580A (en) Method for forming carbon electrode film
US1273628A (en) Film conductor and the method of making the same.
KR100377376B1 (en) Ion Beam Assisted Evaporator and evaporating process thereof
US3575833A (en) Hafnium nitride film resistor
JPH03232959A (en) Production of thin film
JPH08337435A (en) Method for producing quartz glass film
JP5008211B2 (en) Deposition method
JP2002069616A (en) Method for producing anatase-type titanium oxide thin film
JPS61190066A (en) Formation of thin in2o3 film
JPS628409A (en) Formation of transparent conducting metal oxide film
JP2955667B2 (en) Method and apparatus for preparing a mixture thin film
JPS6158967B2 (en)