JPH0483874A - Method for forming conductive graphite film - Google Patents

Method for forming conductive graphite film

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Publication number
JPH0483874A
JPH0483874A JP2200682A JP20068290A JPH0483874A JP H0483874 A JPH0483874 A JP H0483874A JP 2200682 A JP2200682 A JP 2200682A JP 20068290 A JP20068290 A JP 20068290A JP H0483874 A JPH0483874 A JP H0483874A
Authority
JP
Japan
Prior art keywords
graphite film
people
graphite
temperature
raw material
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.)
Granted
Application number
JP2200682A
Other languages
Japanese (ja)
Other versions
JP2794913B2 (en
Inventor
Jun Shiotani
塩谷 準
Takayuki Mishima
隆之 三島
Hideki Ueno
秀樹 上野
Norihiko Yasuda
安田 則彦
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.)
Sumitomo Electric Industries Ltd
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Sumitomo Electric Industries Ltd
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Publication date
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Priority to JP2200682A priority Critical patent/JP2794913B2/en
Publication of JPH0483874A publication Critical patent/JPH0483874A/en
Application granted granted Critical
Publication of JP2794913B2 publication Critical patent/JP2794913B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Manufacturing Of Electric Cables (AREA)
  • Crystals, And After-Treatments Of Crystals (AREA)
  • Carbon And Carbon Compounds (AREA)
  • Chemical Vapour Deposition (AREA)
  • Conductive Materials (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は優れた導電性を有するグラファイト膜を比較的
低温において形成する方法に関するものである。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a method for forming graphite films with excellent electrical conductivity at relatively low temperatures.

従来の技術 高い導電性を与える炭素材料として、コークス等の選択
的配向性の良い、いわゆる“易グラファイト化性炭素″
が知られており、その−船釣な炭素の格子定数(Co)
及び常温における電導度は、処理温度が1000℃の場
合、約6.91人、約100S/am、2000℃の場
合、約6.81人、約300S/am、3000℃の場
合、約6.71人約200 OS/cmであることが[
炭素化工学の基礎J(大釜ら著、オーム社発行、198
0年)に示されている。
Conventional technology As a carbon material that provides high conductivity, so-called "graphitizable carbon", which has good selective orientation such as coke, is used.
is known, and the lattice constant of carbon (Co)
And the conductivity at room temperature is about 6.91 people, about 100 S/am when the processing temperature is 1000°C, about 6.81 people, about 300 S/am, about 6.8 people when the processing temperature is 2000°C, and about 6. Approximately 200 OS/cm for 71 people [
Fundamentals of Carbonization Engineering J (written by Ohkama et al., published by Ohmsha, 198
Year 0).

易グラファイト化性炭素の中でも、特に配向性に優れて
いるのが、メタン、プロパン等の炭化水素ガスの気相熱
分解により得られる“熱分解炭素”であり、2000〜
2200℃で沈積されたものは2500〜5000 S
/cmを発現することが「炭素材料入門J(長油ら、炭
素材料学会、1979年)に示されている。又、これを
300〜500 kg/C1n”の−軸性の圧力を加え
ながら3000℃以上で熱処理することによりCo<6
.72人(グラファイト単結晶:Co=6.708人)
を有する高配向熱分解グラファイト(HOPG)の得ら
れることが、「炭素材料工学」(稲垣ら2日刊工業新聞
社、1985年)に示されており、これはグラファイト
単結晶に匹敵するような電導度l〜2X10’S/am
を持つことが知られている。
Among easily graphitizable carbons, "pyrolytic carbon" obtained by gas-phase thermal decomposition of hydrocarbon gases such as methane and propane has particularly excellent orientation.
2500-5000 S for those deposited at 2200℃
/cm is shown in ``Introduction to Carbon Materials J (Nagayu et al., Carbon Materials Society of Japan, 1979). Co<6 by heat treatment at 3000℃ or higher
.. 72 people (graphite single crystal: Co=6.708 people)
It has been shown in "Carbon Materials Engineering" (Inagaki et al. 2, Nikkan Kogyo Shimbunsha, 1985) that highly oriented pyrolytic graphite (HOPG) can be obtained, which has electrical conductivity comparable to that of single crystal graphite. degree l~2X10'S/am
is known to have.

本発明人の出願による「導電性グラファイト膜の形成方
法J(特願昭60−261383号)では、ベンゼンを
原料としてl000℃のステンレス鋼基村上にプラズマ
放電により炭素膜形成後、3300℃て熱処理すること
により2.2X10’S/amの高導電性グラファイト
膜を得ている。
In the "Method for Forming Conductive Graphite Film J (Japanese Patent Application No. 60-261383) filed by the present inventor, a carbon film is formed by plasma discharge on a stainless steel substrate at 1000°C using benzene as a raw material, and then heat-treated at 3300°C. By doing so, a highly conductive graphite film of 2.2×10'S/am was obtained.

発明が解決しようとする課題 ]−クス等の一般的な易グラファイト化性炭素の場合、
高結晶性、高導電性のグラファイトを得るには3000
℃以上の高温処理が必要であるが、それで漸く、約20
00 S/cmの電導度が得られる程度である。
Problems to be Solved by the Invention] - In the case of general graphitizable carbon such as carbon,
3000 to obtain highly crystalline and highly conductive graphite
Although high-temperature treatment above ℃ is necessary, the temperature of about 20
This is the level at which an electrical conductivity of 0.00 S/cm can be obtained.

又、特に配向性が良く、グラファイト化性に優れた熱分
解炭素では、Co<6.72人、電導度l〜2xlO’
S/cmが得られているが、その作製には、かなりの高
温(>3000℃)、高圧(300〜500kg/cm
りを要するという問題があった。
In addition, for pyrolytic carbon which has particularly good orientation and excellent graphitization properties, Co<6.72 and conductivity 1~2xlO'
S/cm has been obtained, but its production requires considerable high temperature (>3000°C) and high pressure (300 to 500 kg/cm
The problem was that it required a lot of work.

従来のプラズマ放電法でも、Go<6.72人を得るに
は、2750℃以上の高温熱処理が必要であっいずれに
せよ、従来の炭素材料において、高電導性(高結晶性)
を得るには、形成後、更に2750〜3000°Cを越
える高温処理の実施が不可欠であり、このことは、これ
ら材料の応用範囲を著しく狭めるという欠点となってい
た。
Even with the conventional plasma discharge method, high-temperature heat treatment of 2750°C or higher is required to obtain Go < 6.72. In any case, conventional carbon materials have high conductivity (high crystallinity).
In order to obtain this, it is necessary to further perform a high-temperature treatment at temperatures exceeding 2750 to 3000° C. after formation, which has been a disadvantage of significantly narrowing the range of applications of these materials.

それ故、セラミックス等の各種素材と複合化して応用範
囲を広げるため、高結晶性・高導電性グラファイトを2
000℃以下の比較的低温で得fこいという要求がある
Therefore, in order to expand the range of applications by compounding with various materials such as ceramics, highly crystalline and highly conductive graphite is
There is a demand for high performance at a relatively low temperature of 000°C or less.

2000℃以下の比較的低温でグラファイトを得る方法
として、キッシュグラファイトの生成機構と同様、炭素
を金属に溶解させ、その溶融金属から、グラファイトを
析出させる方法が良く知られている。グラファイトを鉄
、鋼に1800〜1900℃で溶解し、溶融鉄、あるい
は鋼を1500℃以下に徐々に冷却する事により溶融鉄
表面にグラファイト膜が生成する事が野田らによって開
示されている(Carbon  6 813(1968
))。
A well-known method for obtaining graphite at a relatively low temperature of 2000° C. or lower is a method in which carbon is dissolved in metal and graphite is precipitated from the molten metal, similar to the production mechanism of Quiche graphite. Noda et al. have disclosed that a graphite film is formed on the surface of molten iron by melting graphite into iron or steel at 1800 to 1900°C and gradually cooling the molten iron or steel to 1500°C or less (Carbon et al. 6 813 (1968
)).

しかし、この方法では、−度、炭素を十分に溶解させ、
1800℃以上に加熱された溶融鉄か必要となり、生成
するクラファイト膜は溶融鉄表面形状により形状か限定
される。さらに1800°Cから鉄の融点である150
0℃まで冷却する必要があり、冷却速度も5℃/分以下
とおそく、精密な温度コントロールが要求される。
However, in this method, the carbon is sufficiently dissolved,
Molten iron heated to 1800° C. or higher is required, and the shape of the graphite film formed is limited by the surface shape of the molten iron. Furthermore, from 1800°C to 150, which is the melting point of iron.
It is necessary to cool down to 0°C, and the cooling rate is slow at 5°C/min or less, requiring precise temperature control.

課題を解決するための手段 この発明は、上記従来技術の問題点に鑑み、高導電性、
高結晶性のグラファイト膜を従来よりも低い温度で、し
かも後の熱処理過程を経ずに、1段で形成させる方法を
提供するものである。
Means for Solving the Problems In view of the problems of the above-mentioned prior art, the present invention provides high conductivity,
The present invention provides a method for forming a highly crystalline graphite film in one step at a lower temperature than conventional methods and without a subsequent heat treatment process.

その要旨とするところは、分離されたプラズマ放電室と
形成室とを有するプラズマCVD装置において、炭化水
素を原料とし、1200℃以上に加熱した遷移金属を含
む基材上にプラズマ放電によって格子定数Co<6.7
2人、電導度2000S/cm以上の導電性グラファイ
ト膜を形成させる方法にある。
The gist of this is that in a plasma CVD apparatus having a separate plasma discharge chamber and formation chamber, a hydrocarbon is used as a raw material, and a lattice constant Co <6.7
Two people are involved in a method for forming a conductive graphite film with an electrical conductivity of 2000 S/cm or more.

この発明において、原料となる炭化水素としてガスとな
り得る物質、例えば、メタン、エタン、プロパン等の脂
肪族化合物CnH2n+z;アルケン、アルキノ等の不
飽和誘導体、即ち1つまたはそれ以上の二重結合或いは
三重結合を有するもの;ヘンセン、ナフタレン、アント
ラセン、ピレン等の芳香族化合物か用いられる。
In this invention, the raw material hydrocarbons include substances that can become gases, such as aliphatic compounds CnH2n+z such as methane, ethane, and propane; unsaturated derivatives such as alkenes and alkinos, that is, one or more double bonds or triple bonds; Those having a bond; aromatic compounds such as Hensen, naphthalene, anthracene, and pyrene are used.

プラズマ放電により基材上にグラファイト膜を形成させ
る方法は、真空チャンバー及び反応管内を真空引きし、
基材を加熱して定温に保った後、原料である炭化水素蒸
気を所定の圧力で流しながら高周波電界を印加し、その
蒸気を基材上に供給することによって、基材上にグラフ
ァイト膜を形成するもので、例えば第1図に示すような
装置が用いられる。
The method of forming a graphite film on a substrate by plasma discharge involves evacuating the inside of a vacuum chamber and reaction tube,
After heating the base material and keeping it at a constant temperature, a high-frequency electric field is applied while flowing hydrocarbon vapor as a raw material at a predetermined pressure, and the vapor is supplied onto the base material to form a graphite film on the base material. For example, an apparatus as shown in FIG. 1 is used.

第1図において、真空チャンバー1内にヒーター2が設
けられており、ヒーター2の中間に基材3が設置されて
、ヒーター2により加熱される。
In FIG. 1, a heater 2 is provided in a vacuum chamber 1, and a base material 3 is placed between the heaters 2 and heated by the heater 2.

真空チャンバー1はバルブ5を介して、油回転ポンプ4
により真空引される。又、真空チャンバー1には反応管
6が接続され、反応管6の回りにはスパイラル状の電極
8が設置されている。電極8には整合器9と高周波発振
器lOが接続され、電気エネルギーが加えられて、反応
管6内にプラズマが発生する。
The vacuum chamber 1 is connected to an oil rotary pump 4 via a valve 5.
is evacuated by. Further, a reaction tube 6 is connected to the vacuum chamber 1, and a spiral electrode 8 is installed around the reaction tube 6. A matching device 9 and a high frequency oscillator IO are connected to the electrode 8, and electric energy is applied to generate plasma in the reaction tube 6.

原料容器12内の原料13は、恒11t14により一定
温度に保持されて気化し、バルブ11を介して反応管6
に導入され、プラズマ放電により活性化された後、ノズ
ル7より真空チャン)<−1内の基材3上に導びかれグ
ラファイト膜の形成に供される。
The raw material 13 in the raw material container 12 is kept at a constant temperature by the constant temperature controller 11t14 and vaporized, and is passed through the valve 11 to the reaction tube 6.
After being activated by plasma discharge, it is guided from a nozzle 7 onto a substrate 3 in a vacuum chamber (<-1) to form a graphite film.

この発明において、基材としては、遷移金属、例えば鉄
、コバルト、ニッケル等の金属、或はステンレス等の合
金からなる板、シート、フィルム、その他の成形品を使
用することりかでき、ファイバ状のもの及びその織布、
或いは、パウダー、及びその成形品も使用することがで
きる。
In this invention, the substrate may be a plate, sheet, film, or other molded product made of a transition metal such as iron, cobalt, or nickel, or an alloy such as stainless steel. things and their woven fabrics,
Alternatively, powders and molded products thereof can also be used.

得られたグラファイト膜に適当なドーパントをドープす
ることによって、更に導電性を増すことができる。
The electrical conductivity can be further increased by doping the obtained graphite film with a suitable dopant.

適当なドーパントとしては、電子受容性試薬の例として
、ハロゲン(例えば、C1,、Brt、I tsICL
ICI3、rBr)、ルイス酸、プロトン酸(例えば、
PF5、A s F s、SbF5、AgCl0.、A
gBF、、BF2、BCl3、BBr3、FSo、00
S02F、(NO,)(S bF e)、(No)Sb
C1,、(N O2XB F 、)、SO3、TiF4
、NbF3、TaF5、NbC11、TaCl5、Mn
C1,、MoC1,、M。
Suitable dopants include, as examples of electron-accepting reagents, halogens (e.g. C1, Brt, ItsICL).
ICI3, rBr), Lewis acids, protic acids (e.g.
PF5, AsFs, SbF5, AgCl0. ,A
gBF, BF2, BCl3, BBr3, FSo, 00
S02F, (NO,) (S bF e), (No) Sb
C1, (N O2XB F ,), SO3, TiF4
, NbF3, TaF5, NbC11, TaCl5, Mn
C1,,MoC1,,M.

C1s、Mo0C1,、NiC1,、ZnCl、、Cr
0zCL、F eC13、CdCl2、AuCl3、C
rCl3、AlCl3、AlBr3、G aB r3、
PtC1,、S bC15、UCl3.5OC12、X
eFe、H,SO,、HClO4、HN O3、FSO
3H,CF35○3H)及び電子供与性試薬Li5Na
、に、Rb、Cs等が使用される。
C1s, Mo0C1,, NiC1,, ZnCl,, Cr
0zCL, FeC13, CdCl2, AuCl3, C
rCl3, AlCl3, AlBr3, GaB r3,
PtC1,,S bC15, UCl3.5OC12,X
eFe, H, SO,, HClO4, HN O3, FSO
3H, CF35○3H) and electron donating reagent Li5Na
, Rb, Cs, etc. are used.

作用 第1図に示した装置を用いた場合に導電性グラファイト
膜の形成は以下のように行われる。
Operation When the apparatus shown in FIG. 1 is used, a conductive graphite film is formed as follows.

遷移金属を含む基材3を真空チャンバー1内のヒーター
2間に設置する。又、原料容器12内に炭化水素原料1
3を充填し、原料13が液相の場合は、凍結脱気を行っ
た後、所定の蒸気圧を得るため、恒温槽14により一定
温度に保持する。その後、真空チャンバー1、反応管6
を含む系全体を油回転ポンプ4によりI O−2mmH
g程度に真空引きし、ヒーター2により基材3を120
0°C以上に加熱する。バルブ11を開いて、原料13
の蒸気を反応管6→ノズル7−真空チャンバー1−バル
ブ5−油回転ポンプ4のルートを経由して、系内を所定
の圧力に保ちながら流す。
A base material 3 containing a transition metal is placed between heaters 2 in a vacuum chamber 1. In addition, the hydrocarbon raw material 1 is contained in the raw material container 12.
3 and when the raw material 13 is in a liquid phase, the temperature is maintained at a constant temperature in a constant temperature bath 14 in order to obtain a predetermined vapor pressure after freezing and deaeration. After that, vacuum chamber 1, reaction tube 6
The entire system including
Vacuum the base material 3 to about 120g using the heater 2.
Heat above 0°C. Open the valve 11 and release the raw material 13.
The vapor flows through the reaction tube 6 -> nozzle 7 - vacuum chamber 1 - valve 5 - oil rotary pump 4 route while maintaining the system at a predetermined pressure.

そこで、電極8に高周波電場(例えば13.56MHz
)を印加することにより原料蒸気はプラズマ放電し、ノ
ズル7より引き出されて基材3上に達し、グラファイト
膜が形成される。
Therefore, a high frequency electric field (for example, 13.56 MHz) is applied to the electrode 8.
), the raw material vapor is plasma-discharged, is drawn out from the nozzle 7, reaches the base material 3, and forms a graphite film.

同方法では、熱エネルギーの代替えとしてプラズマ放電
を利用したことにより、従来の熱分解法に比ベグラファ
イト化温度の低温化を図ることが出来る。また、従来の
プラズマ法によるグラファイト形成では放電室にヒータ
ー及び基材があったため、加熱は1000℃前後が限界
であった。(第1図のように外部電極を用いる場合、反
応管はパイレックスか石英ガラス製である。)本発明に
おいては、第1図に示す如く、形成室(基材設置、加熱
域)を放電室から分離した装置を用いたことにより、基
材を1200°C以上に加熱することか可能となり、又
、基材や生成膜かプラズマ損傷を受けないという効果ら
期待てきる。
In this method, by using plasma discharge as an alternative to thermal energy, it is possible to lower the graphitization temperature compared to the conventional thermal decomposition method. Furthermore, in the conventional plasma method for graphite formation, since a heater and a base material were provided in the discharge chamber, heating was limited to around 1000°C. (When external electrodes are used as shown in Figure 1, the reaction tube is made of Pyrex or quartz glass.) In the present invention, as shown in Figure 1, the formation chamber (substrate installation, heating area) is connected to the discharge chamber. By using a separate device, it is possible to heat the substrate to 1200° C. or higher, and it is also expected that the substrate and the produced film will not be damaged by the plasma.

このため、従来法(1000°Cでの合成)では、Co
=6.81−6.9人、Lc=30〜70人程戻しか得
られず、Co<6.72人、Lc>1000.Aを得る
には更に2750°C以上の高温熱処理が必要であった
が、本発明では1200℃以上の温度での1段法で得る
ことができる。
Therefore, in the conventional method (synthesis at 1000°C), Co
= 6.81-6.9 people, Lc = only about 30-70 people returned, Co < 6.72 people, Lc > 1000. In order to obtain A, a further high-temperature heat treatment at 2750°C or higher was required, but in the present invention it can be obtained by a one-step process at a temperature of 1200°C or higher.

実施例 実施例1 グラファイト製ボートに鉄パウダー(100メツシユ)
を充填して平らに成形したものを基材とし、第1図3の
位置に静置した。真空チャンバー内を10−”mmHg
まで減圧し、基材を1320℃に加熱した後、原料のベ
ンゼン蒸気を反応管から真空チャンバーに、系内圧力を
1amHgに保ちながら流した。然る後、高周波電界(
13,56MHz、出力500W)を印加してプラズマ
放電を起こし、ベンゼン蒸気を加熱された碁打上に送り
、碁打上に膜厚的30μmのグラファイト膜を形成させ
た。
Examples Example 1 Iron powder (100 mesh) on graphite boat
A base material that was filled with and molded flat was placed at the position shown in FIG. 1, 3. 10-”mmHg inside the vacuum chamber
After reducing the pressure to 1,320° C. and heating the base material to 1,320° C., benzene vapor as a raw material was flowed from the reaction tube into the vacuum chamber while maintaining the system internal pressure at 1 amHg. After that, a high frequency electric field (
13.56 MHz, output 500 W) was applied to generate plasma discharge, and benzene vapor was sent onto the heated Go board to form a graphite film with a thickness of 30 μm on the Go board.

得られたグラファイト膜の電導塵は9000〜l川X 
I O’S 7cmであった。又、X線回折の結果第2
図に示す如く、ンヤープなC(002)、C(004)
等の各回折線が測定され、極めて結晶性の高いことがわ
かった。格子定数Co=6.708人、C軸方向の人品
C軸方向さLc> I 000人であった。
The conductive dust of the obtained graphite film is 9000 to 1 river
I O'S was 7 cm. In addition, the second result of X-ray diffraction
As shown in the figure, Nyaap C (002), C (004)
The following diffraction lines were measured, and it was found that the crystallinity was extremely high. The lattice constant Co = 6.708 people, and the length of the human body in the C-axis direction was Lc > I 000 people.

このグラフフィト膜に室温でA s P sドーピング
を行った(AsFs圧8X10’Pa)結果、電導塵は
1.4X105S/Cmとなった。
This graphite film was doped with AsPs at room temperature (AsFs pressure 8×10'Pa), and as a result, the conductive dust was 1.4×105S/Cm.

実施例2 基材を1240℃に加熱する他は実施例1と同様の条件
で膜厚的20μmのグラファイト膜を形成した。
Example 2 A graphite film having a thickness of 20 μm was formed under the same conditions as in Example 1 except that the substrate was heated to 1240° C.

得られたグラファイト膜の電導塵は2800〜4100
S/amであった。又、Go=6.718人。
The conductive dust of the obtained graphite film is 2800 to 4100
It was S/am. Also, Go = 6.718 people.

Lc>1000人であった。Lc>1000 people.

実施例3 基材を1430℃に加熱する他は実施例1と同様の条件
で膜厚的15μmのグラファイト膜を形成した。
Example 3 A graphite film having a thickness of 15 μm was formed under the same conditions as in Example 1 except that the substrate was heated to 1430° C.

得られfこグラファイト膜の電導塵は5900〜630
0 S/amであった。又、Co=6.715人Lc>
 l OO0人であった。
The conductive dust of the obtained graphite film is 5900 to 630
It was 0 S/am. Also, Co=6.715 people Lc>
l OO There were 0 people.

実施例4 基材を1690℃に加熱する他は実施例1と同様の条件
で膜厚的35μmのグラファイト膜を形成した。
Example 4 A graphite film having a thickness of 35 μm was formed under the same conditions as in Example 1 except that the substrate was heated to 1690° C.

得られたグラファイト膜の電導塵は7500〜l X 
10’ 97cmであった。又、Co=6.71人。
The conductive dust of the obtained graphite film is 7500~l
It was 10' 97cm. Also, Co=6.71 people.

Lc>1000人であった。Lc>1000 people.

比較例1 基材を1340℃に加熱し、プラズマを印加しない他は
実施例1と同様の条件で、膜厚的40μmのグラファイ
ト膜を形成した。得られたグラファイト膜の電導塵は4
400〜5800 S/amでありプラズマ印加した場
合の1/2の値であった。又、Co=6.725人、L
c> l OO0人であつ比較例2 基材を1100℃に加熱する他は実施例1と同様の条件
で膜厚的45μmの炭素膜を形成した。
Comparative Example 1 A graphite film having a thickness of 40 μm was formed under the same conditions as in Example 1 except that the substrate was heated to 1340° C. and no plasma was applied. The conductive dust of the obtained graphite film was 4
It was 400 to 5800 S/am, which was 1/2 the value when plasma was applied. Also, Co=6.725 people, L
c> l OO 0 persons Comparative Example 2 A carbon film having a thickness of 45 μm was formed under the same conditions as in Example 1 except that the substrate was heated to 1100° C.

得られた炭素膜の電導塵は650〜800S/cmであ
った。又、Co=6.885人、Lc=40人であった
The conductive dust of the obtained carbon film was 650 to 800 S/cm. Moreover, Co=6.885 people and Lc=40 people.

比較例3 基材を1690℃に加熱し、プラズマを印加しない他は
実施例1と同様の条件で、膜厚的25μmのグラファイ
ト膜を形成した。
Comparative Example 3 A graphite film having a thickness of 25 μm was formed under the same conditions as in Example 1 except that the substrate was heated to 1690° C. and no plasma was applied.

得られたグラファイト膜の電導塵は2600〜4100
 S/amであり、プラズマを印加した場合の215〜
1/3の値であった。又、Co=6.742人、Lc>
1000人であった。
The conductive dust of the obtained graphite film is 2600 to 4100
S/am, 215~ when plasma is applied
The value was 1/3. Also, Co=6.742 people, Lc>
There were 1000 people.

発明の効果 本発明は、プラズマCVD法を採用することにより、熱
分解法に比べ、高結晶性、高導電性のグラファイト膜を
形成することが出来る。さらに、基材遷移金属の触媒作
用によりグラファイト形成温度の低温化を図ることが出
来、金属の溶融に至らない低温下でグラファイト膜の形
成が可能となりfこ。
Effects of the Invention By employing the plasma CVD method, the present invention can form a graphite film with higher crystallinity and higher conductivity than the thermal decomposition method. Furthermore, the graphite formation temperature can be lowered due to the catalytic action of the base transition metal, making it possible to form a graphite film at a low temperature that does not lead to melting of the metal.

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

第1図は本発明において使用されるプラズマCVD法の
装置の概略図、第2図は1320℃で形成したグラファ
イト膜のX線回折図である。 1は真空チャンバー、2はヒーター、3は基材、4は油
回転ポンプ、5はバルブ、6は反応管、7はノズル、8
は電極、9は整合器、IOは高周波発振器、11はバル
ブ、12は原料容器、I3は原料、14は恒温槽を示す
。 特許出願人住友電気工業株式会社 代理人弁理士 青 山 葆 ほか1名 第 図
FIG. 1 is a schematic diagram of an apparatus for the plasma CVD method used in the present invention, and FIG. 2 is an X-ray diffraction diagram of a graphite film formed at 1320°C. 1 is a vacuum chamber, 2 is a heater, 3 is a base material, 4 is an oil rotary pump, 5 is a valve, 6 is a reaction tube, 7 is a nozzle, 8
9 is an electrode, 9 is a matching box, IO is a high frequency oscillator, 11 is a valve, 12 is a raw material container, I3 is a raw material, and 14 is a constant temperature bath. Patent applicant Sumitomo Electric Industries, Ltd. Patent attorney Aoyama Ao and one other person Figure

Claims (1)

【特許請求の範囲】[Claims] (1)分離されたプラズマ放電室と形成室とを有するプ
ラズマCVD装置において、炭化水素を原料とし、12
00℃以上に加熱した遷移金属を含む基材上にプラズマ
放電により格子定数Coが6.72Å以下、電導度が2
000S/cm以上の特性を有する導電性グラファイト
膜を形成する方法。
(1) In a plasma CVD apparatus having a separate plasma discharge chamber and a forming chamber, a hydrocarbon is used as a raw material, and 12
The lattice constant Co is 6.72 Å or less and the electrical conductivity is 2 by plasma discharge on a substrate containing a transition metal heated to 00°C or higher.
A method of forming a conductive graphite film having characteristics of 000 S/cm or more.
JP2200682A 1990-07-25 1990-07-25 Method of forming conductive graphite film Expired - Fee Related JP2794913B2 (en)

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Application Number Priority Date Filing Date Title
JP2200682A JP2794913B2 (en) 1990-07-25 1990-07-25 Method of forming conductive graphite film

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JPH0483874A true JPH0483874A (en) 1992-03-17
JP2794913B2 JP2794913B2 (en) 1998-09-10

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Family Applications (1)

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Country Status (1)

Country Link
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* Cited by examiner, † Cited by third party
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GB2527209A (en) * 2014-06-13 2015-12-16 Fgv Cambridge Nanosystems Ltd Apparatus and method for plasma synthesis of graphitic products including graphene

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US9235468B2 (en) 2013-04-12 2016-01-12 Qualcomm Incorporated Systems and methods to improve the reliability and lifespan of flash memory
JP6248754B2 (en) 2014-03-28 2017-12-20 三浦工業株式会社 Boiler system

Cited By (5)

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Publication number Priority date Publication date Assignee Title
CN101858879A (en) * 2010-05-24 2010-10-13 清华大学 A method and device for measuring electrical conductivity of graphite
GB2527209A (en) * 2014-06-13 2015-12-16 Fgv Cambridge Nanosystems Ltd Apparatus and method for plasma synthesis of graphitic products including graphene
GB2527209B (en) * 2014-06-13 2019-08-28 Fgv Cambridge Nanosystems Ltd Apparatus and method for plasma synthesis of graphitic products including graphene
US11802052B2 (en) 2014-06-13 2023-10-31 Levidian Nanosystems Limited Apparatus and method for plasma synthesis of graphitic products including graphene
US12252402B2 (en) 2014-06-13 2025-03-18 Levidian Nanosystems Limited Apparatus and method for plasma synthesis of graphitic products including graphene

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