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JPH0232237B2 - CHITANTANCHITSUKABUTSUNOTANKETSUSHONOSEIZOHO - Google Patents
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JPH0232237B2 - CHITANTANCHITSUKABUTSUNOTANKETSUSHONOSEIZOHO - Google Patents

CHITANTANCHITSUKABUTSUNOTANKETSUSHONOSEIZOHO

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Publication number
JPH0232237B2
JPH0232237B2 JP23904885A JP23904885A JPH0232237B2 JP H0232237 B2 JPH0232237 B2 JP H0232237B2 JP 23904885 A JP23904885 A JP 23904885A JP 23904885 A JP23904885 A JP 23904885A JP H0232237 B2 JPH0232237 B2 JP H0232237B2
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JP
Japan
Prior art keywords
composition
crystal
titanium carbonitride
rod
sintered
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 - Lifetime
Application number
JP23904885A
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Japanese (ja)
Other versions
JPS62100500A (en
Inventor
Shigeki Ootani
Takao Tanaka
Yoshio Ishizawa
Tetsuo Yamada
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.)
KAGAKU GIJUTSUCHO MUKIZAISHITSU KENKYUSHOCHO
Original Assignee
KAGAKU GIJUTSUCHO MUKIZAISHITSU KENKYUSHOCHO
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Application filed by KAGAKU GIJUTSUCHO MUKIZAISHITSU KENKYUSHOCHO filed Critical KAGAKU GIJUTSUCHO MUKIZAISHITSU KENKYUSHOCHO
Priority to JP23904885A priority Critical patent/JPH0232237B2/en
Publication of JPS62100500A publication Critical patent/JPS62100500A/en
Publication of JPH0232237B2 publication Critical patent/JPH0232237B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【発明の詳細な説明】[Detailed description of the invention]

産業上の利用分野 本発明はチタン炭窒化物の単結晶の製造法に関
する。 チタン炭窒化物は、炭化チタンの高融点(3100
℃)、高硬度(ビツカース硬度3000Kg/mm2)とい
う特性と、窒化チタンの高融点(2950℃)と高靭
性という特性を兼ね備えた材料であり、サーメツ
トとして各種の切削工具、耐摩耗部品などに実用
に供せられている。 その仕事関数は、耐熱金属(W、Mo等)より
低い値であり、化学的にも安定であることなどか
ら、この単結晶は電子材料、特にフイールド・エ
ミツター材としても有望なものである。 従来技術 チタン炭窒化物(TiCXNY)の結晶の製造法と
しては、次の方法が知られている。 (1) TiCとTiNとの混合粉末を不活性雰囲気中で
高温に加熱させる固相反応法。 (2) TiCl4、炭化水素及び窒素ガスを、水素等を
キヤリアーガスとして輸送し、高温の基板上で
熱分解させてチタン炭窒化物を析出させる気相
反応法。 しかし、(1)の固相反応法は、粉末合成法であ
り、多結晶のものしか得られない欠点がある。(2)
の気相反応法では針状または柱状の結晶は得られ
るが、その結晶は非常に小さく、多結晶膜以外の
用途には利用できない欠点があつた。 このように、チタン炭窒化物の単結晶の製造
は、従来、実際上不可能であつた。 発明の目的 本発明は従来法では全く得られなかつた大型で
良質のチタン炭窒化物の単結晶を製造する方法を
提供するにある。また他の目的はフイールド・エ
ミツター材として利用し得るチタン炭窒化物の単
結晶を製造する方法を提供するにある。 発明の構成 本発明者らは前記目的を達成すべく、フローテ
イング・ゾーン法(以下FZ法と略記する)によ
るチタン炭窒化物の単結晶の育成を試みた。しか
しながら、単にチタン炭窒化物の焼結体ロツドを
使用してFZ法を実施しただけでは、窒素及びま
たは窒化チタンの蒸発が激しくて、目的とする
TiCXNY組成の単結晶の育成はできなかつた。 これを解決すべく、更に研究を重ねた結果、供
給焼結体のロツドの組成、溶融体の組成及び雰囲
気中の窒素ガスの分圧を適正に制御すると、チタ
ン炭窒化物の単結晶も育成し得られることを究明
し得た。この知見に基いて本発明を完成した。 発明の要旨 焼結体ロツドをホルダーで支持し、加圧不活性
ガス雰囲気下で、その一部を加熱溶融させながら
焼結体ロツドを移動させて、単結晶を育成する方
法において、供給焼結体ロツドの組成を、得よう
とするチタン炭窒化物結晶の固相成分に溶融時に
融帯から蒸発する窒素、炭素の成分を添加した組
成となして、溶融帯の組成を、得ようとするチタ
ン炭窒化物結晶の固相成分と共存する液相成分の
組成となし、かつ該チタン炭窒化物の平衡解離圧
の0.1〜10倍の窒素ガス分圧を有する全圧2〜100
気圧の不活性ガス加圧雰囲気下で溶融帯を形成さ
せて結晶を育生させることを特徴とするチタン炭
窒化物の単結晶の製造法にある。 本発明の方法に用いるFZ法を図面に基いて説
明する。 第1図はFZ法の装置の概念図である。装置と
しては例えばADL社製の高圧タイプの結晶育生
炉が用いられる。第1図において、1はシヤフ
ト、2はホルダー、3は焼結体ロツド、4は結晶
棒、5は融帯、6はRFコイルである。 例えば長さ10〜20cmの焼結体ロツド3の端を
RFコイル6から高周波を発生させて誘導加熱溶
融させて融帯5を形成し、ホルダー2に保持され
た焼結体ロツド3をゆつくり移動させて結晶を育
成させる。この時の融帯5の移動速度は0.5〜5
cm/hが適当である。移動方向は上下いずれの方
向でもよい。雰囲気は不活性ガスが使用され、通
常はアルゴン、ヘリウムまたはこれとの混合ガス
である。雰囲気ガスは主に試料の蒸発を抑制する
ためとRFコイル間およびコイルと試料間の放電
を抑制するために用いられる。ガス圧は通常2〜
100気圧、好ましくは5〜50気圧である。2気圧
より圧力が低いと蒸発と放電を抑制する効果が殆
んどなく、また、100気圧より高いと対流による
熱損失が大きくなるので好ましくない。 また、コイル間およびコイルと焼結体ロツド間
の放電抑制効果はアルゴンよりもヘリウムの方が
優れている。これはヘリウムのイオン化ポテンシ
ヤルがアルゴンのそれよりも高いためと考えられ
る。 しかし、単にチタン炭窒化物の焼結体ロツドを
使用してFZ法を行つても目的とするTiCXNY組成
の単結晶は得られなかつた。 そこで、固相線と液相線との対応、および液相
組成と気相組成との対応を求めるために、次の実
験を行つた。 先ず、所定の窒素ガス分圧を有する窒素、ヘリ
ウム混合ガス加圧下で、組成のはつきりした
TiCXNY焼結体ロツドを用いて、FZ法で長さ数cm
の結晶棒を作り、この結晶棒の始端部、終端部、
固化した融帯及び焼結体の炭素含有量、窒素含有
量を分析した。 この分析によりチタン炭窒化物の固相組成とこ
れと共存する液相組成とを求めた。 また、焼結体ロツドの組成を変えて同様な実験
を行いその固相組成とこれに共存する液相組成を
求めた。更に炉内の気相組成を分析した。次に、
窒素ガス分圧を変化させて同様の実験を行い液相
組成とこれに共存する固相組成及び気相組成との
対応関係をしらべた。 その結果、溶融時の融帯からの蒸発のため結晶
組成は供給焼結体ロツドの組成と異なつてくるの
で、供給焼結体ロツドの組成は、得ようとするチ
タン炭窒化物結晶の固相成分に、溶融時に融帯か
ら蒸発する窒素、炭素の成分を添加した組成とす
ることが必要であり、また、溶融帯の組成は、得
ようとするチタン炭窒化物結晶の固相成分と共存
する液相成分の組成とすることが必要であること
が分つた。 また、チタン炭窒化物の単結晶育成において
は、雰囲気中のガスの組成及び窒素ガス分圧の制
御が重要であることが分つた。即ち、窒素ガス分
圧がチタン炭窒化物の平衡解離圧(計算値)の
0.1〜10倍であり、且つ全圧が2〜100気圧、好ま
しくは5〜50気圧のときのみ単結晶が得られるこ
とが分つた。 チタン炭窒化物の平衡解離圧は、 TiCXNY+C(固体)+N2(ガス)系の相平衡に
基づき、次式により計算する。 RTln(X/Y・KN/KC・(PN21/2) = ΔG゜f,TiN−ΔG゜f,TiC 但し、 R:気体定数 T:絶対温度 KN:窒素の分配係数 KC:炭素の分配係数 PN2:窒素ガス分圧 ΔG゜f,TiN:TiN(液体)の標準生成自由エネルギー ΔG゜f,TiC:TiC(液体)の標準生成自由エネルギー。 窒素ガス分圧が、平衡解離圧の0.1倍未満の場
合には、融帯からの窒素の蒸発が激しくて、結晶
中への窒素の固溶量が僅かとなるばかりでなく、
(焼結ロツドの窒素含有量の10%程度)き裂が生
じ、実際上、単結晶の育成が困難となる。また平
衡解離圧の10倍を超えると、融帯表面に不溶不融
性の析出物が生じ、加熱溶融させながら焼結体ロ
ツドを移動させることが困難となり、単結晶が得
られなくなる。 本発明における得ようとする単結晶の組成と窒
素分圧との関係を示すと第2図の通りである。図
中の斜線部が必要とする窒素ガス分圧である。 また、全圧が2気圧より低いと、チタン炭窒化
物の蒸発が激しく、蒸発物がコイルに付着して放
電が起こり単結晶の育成が困難となる。また全圧
が100気圧を超えると、対流による熱損失が大き
くなる。 本発明における前記の融帯部に融帯組成ロツド
を存在させてFZ法を行う方法としては、 (1) 焼結体ロツドを2分し、下部に供給焼結体ロ
ツド、上部に融帯組成ロツドとし、先ず、上部
の融帯組成ロツドを溶かして融帯を形成させ、
焼結体ロツドを上方に向つて移動させる方法。
また上、下のロツドを逆に設け、下方向に向つ
て移動させる方法。 (2) 上下に供給焼結体ロツドを設け、その間に融
帯組成ロツドまたは融帯組成になる量の炭化チ
タン、窒化チタン、炭素板及び金属チタン板を
はさみ、先ず融帯部分を溶かした後、供給焼結
体ロツドを上下いずれかの方向に移動させる方
法。 (3) 通常のFZ法を行なうと、融帯移動を行うに
つれ、融帯組成が、その共存液相組成に近づい
て行く。そのため十分融帯移動を行い、融帯組
成が共存液相組成に一致した時、融帯部分を固
化させて、これを用いて(1)の方法により対応す
る組成の結晶を育成する方法。 が挙げられる。 結晶育成の際には上下のシヤフトに回転を与え
ることにより融帯の撹拌を促進し、ゾーンパスを
容易にする。 本発明において使用する供給焼結体ロツドは、
市販の炭化チタン、窒化チタン粉末に、チタン金
属及びカーボンを混合して作ることができる。 原料の純度は高い方が好ましく、通常98重量%
以上、好ましくは99重量%以上のものがよい。そ
の平均粒径は10μm以下であることが好ましい。 焼結体ロツドの形状は、角柱(例えば10×10×
200mm3、15×15×100mm3、円柱(例えば、10φ×
150mm3等を通常用いるが、任意の形状でよい。成
形方法としては均一な密度の成形体を得るため、
ラバープレスを用いるのが好ましい。成形圧は通
常1t/cm2である。次に成形体を焼結する。焼結は
通常1500〜2400℃で0.3から6時間行う。焼結雰
囲気としては真空、不活性ガス下で行い、使用す
る焼結炉はどのようなものでもよいが、高周波誘
導加熱炉が便利である。このような条件下で得ら
れる焼結体ロツドの密度は55〜75%である。 実施例 1 市販のTiC粉末(全炭素19.45重量%、遊離炭
素0.05重量%)及びTiN粉末(窒素21.1重量%)
を所定割合に混合した後、直径10mmφ、長さ150
mmと50mmの2本の円柱をラバープレス成形した。
これを真空中2000℃で30分間焼結した。得られた
焼結体の組成は、TiC0.08N0.09であつた。 次に、予備実験の結果に基づき、前記TiC粉
末、TiN粉末に発光分析用カーボンを混合し、
前記と同じ方法で焼結し、TiC1.10N0.01組成の融
帯形成用の焼結体ロツドを作つた。 前記TiC0.88N0.09組成の2本の焼結体ロツドを
ホルダーで支持し、その間にTiC1.10N0.01組成の
ものをはさんだ。 平衡解離圧は0.18気圧と算出されたので、全圧
10気圧、PN20.55気圧の窒素ヘリウム混合ガス加
圧下で、融帯形成用焼結体ロツドを溶かして融帯
を生成させ、上方及び下方のロツドをゆつくり下
方に移動させた。 その回転数は5rpmとし、移動速度をそれぞれ
33mm/hr、及び25mm/hrとした。その結果、上方
ロツドは融帯中に溶け込み、一方下部にはチタン
炭窒化物単結晶が育成された。 得られた単結晶の始端部、中央部及び終端部の
組成分析を行つたところ、表−1の通りであつ
た。
INDUSTRIAL APPLICATION FIELD The present invention relates to a method for producing a single crystal of titanium carbonitride. Titanium carbonitride has a high melting point of titanium carbide (3100
It is a material that combines the characteristics of high hardness (Vickers hardness: 3000Kg/mm 2 ) with the high melting point (2950℃) and high toughness of titanium nitride, and is used as a cermet for various cutting tools, wear-resistant parts, etc. It is put into practical use. Since its work function is lower than that of heat-resistant metals (W, Mo, etc.) and it is chemically stable, this single crystal is promising as an electronic material, especially as a field emitter material. Prior Art The following method is known as a method for producing crystals of titanium carbonitride (TiC X N Y ). (1) A solid phase reaction method in which a mixed powder of TiC and TiN is heated to high temperature in an inert atmosphere. (2) A gas phase reaction method in which TiCl 4 , hydrocarbons, and nitrogen gas are transported using hydrogen or other carrier gas, and thermally decomposed on a high-temperature substrate to precipitate titanium carbonitride. However, the solid phase reaction method (1) is a powder synthesis method, and has the drawback that only polycrystalline products can be obtained. (2)
Although acicular or columnar crystals can be obtained using the gas phase reaction method, the crystals are very small and have the disadvantage that they cannot be used for purposes other than polycrystalline films. As described above, production of a single crystal of titanium carbonitride has heretofore been practically impossible. OBJECTS OF THE INVENTION The object of the present invention is to provide a method for producing large-sized, high-quality titanium carbonitride single crystals that could not be obtained using conventional methods. Another object of the present invention is to provide a method for producing a titanium carbonitride single crystal that can be used as a field emitter material. Structure of the Invention In order to achieve the above object, the present inventors attempted to grow a single crystal of titanium carbonitride by a floating zone method (hereinafter abbreviated as FZ method). However, if the FZ method is simply carried out using a sintered body rod of titanium carbonitride, the evaporation of nitrogen and/or titanium nitride will be intense, and the target
It was not possible to grow a single crystal of TiC X N Y composition. In order to solve this problem, we conducted further research and found that by appropriately controlling the composition of the rod of the supplied sintered body, the composition of the melt, and the partial pressure of nitrogen gas in the atmosphere, single crystals of titanium carbonitride can also be grown. I was able to find out what could be done. The present invention was completed based on this knowledge. Summary of the Invention A method for growing a single crystal by supporting a sintered rod with a holder and moving the sintered rod while heating and melting a part of the rod in a pressurized inert gas atmosphere. The composition of the melting zone is obtained by changing the composition of the body rod to a composition in which nitrogen and carbon components that evaporate from the melting zone are added to the solid phase components of the titanium carbonitride crystal to be obtained. The composition of the liquid phase component coexisting with the solid phase component of the titanium carbonitride crystal, and a total pressure of 2 to 100, having a nitrogen gas partial pressure of 0.1 to 10 times the equilibrium dissociation pressure of the titanium carbonitride.
A method for producing a single crystal of titanium carbonitride, which is characterized by growing a crystal by forming a molten zone in a pressurized atmosphere of an inert gas at atmospheric pressure. The FZ method used in the method of the present invention will be explained based on the drawings. Figure 1 is a conceptual diagram of the FZ method equipment. As the device, for example, a high-pressure type crystal growth furnace manufactured by ADL is used. In FIG. 1, 1 is a shaft, 2 is a holder, 3 is a sintered rod, 4 is a crystal rod, 5 is a melt zone, and 6 is an RF coil. For example, the end of sintered rod 3 with a length of 10 to 20 cm
A high frequency is generated from the RF coil 6 to cause induction heating and melting to form a melt zone 5, and the sintered rod 3 held in the holder 2 is slowly moved to grow the crystal. At this time, the moving speed of fusion zone 5 is 0.5 to 5
cm/h is appropriate. The direction of movement may be either up or down. The atmosphere is an inert gas, usually argon, helium, or a mixture thereof. The atmospheric gas is mainly used to suppress evaporation of the sample and to suppress electrical discharge between the RF coil and between the coil and the sample. Gas pressure is usually 2~
The pressure is 100 atmospheres, preferably 5 to 50 atmospheres. If the pressure is lower than 2 atm, there is almost no effect of suppressing evaporation and discharge, and if it is higher than 100 atm, heat loss due to convection increases, which is not preferable. Furthermore, helium is more effective than argon in suppressing discharge between the coils and between the coil and the sintered body rod. This is thought to be because the ionization potential of helium is higher than that of argon. However, even if the FZ method was simply performed using a sintered rod of titanium carbonitride, the desired single crystal of TiC X N Y composition could not be obtained. Therefore, the following experiment was conducted to find the correspondence between the solidus line and the liquidus line, and the correspondence between the liquid phase composition and the gas phase composition. First, under pressure of a nitrogen and helium mixed gas having a predetermined nitrogen gas partial pressure, the composition was determined.
Using a TiC
Make a crystal rod, and define the starting and ending parts of this crystal rod,
The carbon content and nitrogen content of the solidified melt zone and sintered body were analyzed. Through this analysis, the solid phase composition of titanium carbonitride and the liquid phase composition coexisting therewith were determined. In addition, similar experiments were carried out by changing the composition of the sintered rod, and the solid phase composition and liquid phase composition coexisting therewith were determined. Furthermore, the gas phase composition inside the furnace was analyzed. next,
Similar experiments were carried out by varying the partial pressure of nitrogen gas, and the correspondence between the liquid phase composition and the coexisting solid phase composition and gas phase composition was investigated. As a result, the crystal composition differs from that of the supplied sintered rod due to evaporation from the melt zone during melting, so the composition of the supplied sintered rod is determined by the solid phase of the titanium carbonitride crystal to be obtained. It is necessary to add nitrogen and carbon components that evaporate from the melting zone during melting, and the composition of the melting zone must be such that it coexists with the solid phase components of the titanium carbonitride crystal to be obtained. It has been found that it is necessary to have a composition of liquid phase components that Furthermore, it has been found that controlling the gas composition and nitrogen gas partial pressure in the atmosphere is important in growing single crystals of titanium carbonitride. In other words, the nitrogen gas partial pressure is equal to the equilibrium dissociation pressure (calculated value) of titanium carbonitride.
It has been found that single crystals can be obtained only when the total pressure is 0.1 to 10 times higher and the total pressure is 2 to 100 atm, preferably 5 to 50 atm. The equilibrium dissociation pressure of titanium carbonitride is calculated by the following formula based on the phase equilibrium of the TiC X N Y +C (solid) + N2 (gas) system. RTln (X/Y・K N /K C・(P N2 ) 1/2 ) = ΔG゜f,TiN −ΔG゜f,TiC However, R: Gas constant T: Absolute temperature K N : Nitrogen partition coefficient K C : Carbon partition coefficient P N2 : Nitrogen gas partial pressure ΔG゜f, TiN : Standard free energy of formation of TiN (liquid) ΔG゜f, TiC : Standard free energy of formation of TiC (liquid). When the nitrogen gas partial pressure is less than 0.1 times the equilibrium dissociation pressure, the evaporation of nitrogen from the melt zone is intense, and not only is the amount of nitrogen dissolved in solid solution in the crystal small;
(Approximately 10% of the nitrogen content of the sintered rod) Cracks occur, making it difficult to grow single crystals. If the pressure exceeds 10 times the equilibrium dissociation pressure, insoluble precipitates will form on the surface of the melting zone, making it difficult to move the sintered rod while heating and melting it, making it impossible to obtain a single crystal. FIG. 2 shows the relationship between the composition of the single crystal to be obtained in the present invention and the nitrogen partial pressure. The shaded area in the figure is the required nitrogen gas partial pressure. Furthermore, if the total pressure is lower than 2 atmospheres, titanium carbonitride evaporates rapidly, and the evaporated material adheres to the coil, causing discharge and making it difficult to grow a single crystal. Furthermore, when the total pressure exceeds 100 atmospheres, heat loss due to convection increases. In the present invention, the method of performing the FZ method with a melt zone composition rod present in the melt zone is as follows: (1) The sintered rod is divided into two parts, the sintered rod to be supplied is in the lower part, and the melt zone composition is in the upper part. First, the upper melt zone composition rod is melted to form a melt zone,
A method of moving the sintered rod upward.
Another method is to reverse the upper and lower rods and move them downward. (2) Supply sintered body rods are provided on the upper and lower sides, and a melt zone composition rod or titanium carbide, titanium nitride, carbon plate, and metal titanium plate in an amount that will give a melt zone composition are sandwiched between them, and the melt zone portion is first melted. , a method in which the supplied sintered body rod is moved either up or down. (3) When the normal FZ method is performed, as the melt zone moves, the composition of the melt zone approaches the composition of the coexisting liquid phase. Therefore, when the melting zone is moved sufficiently and the melting zone composition matches the coexisting liquid phase composition, the melting zone is solidified, and this is used to grow crystals of the corresponding composition by method (1). can be mentioned. During crystal growth, rotation is applied to the upper and lower shafts to promote agitation of the melt zone and facilitate zone passing. The supply sintered body rod used in the present invention is
It can be made by mixing titanium metal and carbon with commercially available titanium carbide and titanium nitride powders. The higher the purity of the raw material, the better, usually 98% by weight.
Above, preferably 99% by weight or more. The average particle size is preferably 10 μm or less. The shape of the sintered rod is a prism (for example, 10×10×
200mm 3 , 15×15×100mm 3 , cylinder (for example, 10φ×
150 mm 3 or the like is usually used, but any shape may be used. As a molding method, in order to obtain a molded product with uniform density,
Preferably, a rubber press is used. The molding pressure is usually 1 t/cm 2 . Next, the molded body is sintered. Sintering is usually carried out at 1500 to 2400°C for 0.3 to 6 hours. The sintering is performed in a vacuum or inert gas atmosphere, and any type of sintering furnace may be used, but a high-frequency induction heating furnace is convenient. The density of the sintered rod obtained under these conditions is 55-75%. Example 1 Commercially available TiC powder (total carbon 19.45% by weight, free carbon 0.05% by weight) and TiN powder (nitrogen 21.1% by weight)
After mixing in the specified ratio, the diameter is 10mmφ and the length is 150mm.
Two cylinders of mm and 50 mm were rubber press molded.
This was sintered in vacuum at 2000°C for 30 minutes. The composition of the obtained sintered body was TiC 0.08 N 0.09 . Next, based on the results of preliminary experiments, carbon for emission analysis was mixed with the TiC powder and TiN powder,
A sintered body rod for forming a melt zone having a TiC 1.10 N 0.01 composition was produced by sintering in the same manner as described above. Two sintered rods having the TiC 0.88 N 0.09 composition were supported by a holder, and a TiC 1.10 N 0.01 composition was sandwiched between them. The equilibrium dissociation pressure was calculated to be 0.18 atm, so the total pressure
Under pressure of a nitrogen-helium mixed gas of 10 atmospheres and P N 2 0.55 atmospheres, the sintered body rod for forming a melt zone was melted to form a melt zone, and the upper and lower rods were slowly moved downward. The rotation speed is 5 rpm, and the movement speed is
33 mm/hr and 25 mm/hr. As a result, the upper rod melted into the melt zone, while a titanium carbonitride single crystal was grown in the lower part. The composition analysis of the starting end, center, and end of the single crystal obtained was as shown in Table 1.

【表】 この結果が示すように、TiC0.86NN0.05組成の均
質な単結晶となつた。 実施例 2 供給焼結体ロツドの組成、TiC0.87N0.10 融帯形成用焼結体ロツドの組成、TiC1.13N0.005 窒素分圧PN2 0.20気圧 全 圧 10気圧 の条件下で実施例1と同様にして単結晶を育成し
た。表−1に示したようなTiC0.88N0.02組成の均
質かつ良質な単結晶が得られた。 実施例 3 供給焼結体ロツドの組成、TiC0.69N0.27 融帯形成用焼結体ロツドの組成、TiC0.66N0.06 窒素分圧PN2 5気圧 全 圧 30気圧 の条件下で、実施例1と同様にして単結晶を育成
した。表−1に示すようなTiC0.71N0.18組成の単
結晶が得られた。 発明の効果 本発明の方法によると従来法では得られなかつ
た均一組成の大型良質な単結晶が得られる優れた
効果を奏し得られる。また、フイールド・エミツ
ター材として利用し得られる単結晶を提供し得ら
れる。
[Table] As shown by this result, a homogeneous single crystal with a composition of TiC 0.86 N N 0.05 was obtained. Example 2 Composition of supplied sintered rod, TiC 0.87 N 0.10 Composition of sintered rod for forming melting zone, TiC 1.13 N 0.005 Nitrogen partial pressure P N2 0.20 atm Total pressure 10 atm Same as Example 1 Single crystals were grown. A homogeneous and high-quality single crystal with a TiC 0.88 N 0.02 composition as shown in Table 1 was obtained. Example 3 Composition of sintered rod to be supplied, TiC 0.69 N 0.27 Composition of sintered rod for forming melt zone, TiC 0.66 N 0.06 Nitrogen partial pressure P N2 5 atm Total pressure 30 atm under the conditions of Example 1 and Single crystals were grown in the same manner. A single crystal with a composition of TiC 0.71 N 0.18 as shown in Table 1 was obtained. Effects of the Invention According to the method of the present invention, an excellent effect of obtaining a large, high-quality single crystal with a uniform composition, which could not be obtained by conventional methods, can be achieved. In addition, a single crystal that can be used as a field emitter material can be provided.

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

第1図はフローテイング・ゾーン法(FZ法)
の概念図、第2図は所望とするチタン炭窒化物の
単結晶の組成と結晶育成に必要な窒素分圧との関
係図を示す。 1:シヤフト、2:ホルダー、3:焼結体ロツ
ド、4:TiCXNY結晶ロツド、5:融帯、6:高
周波誘導加熱用コイル。
Figure 1 shows the floating zone method (FZ method)
FIG. 2 shows a relationship diagram between the composition of a desired single crystal of titanium carbonitride and the nitrogen partial pressure required for crystal growth. 1: Shaft, 2: Holder, 3: Sintered rod, 4: TiC X N Y crystal rod, 5: Melting zone, 6: High frequency induction heating coil.

Claims (1)

【特許請求の範囲】[Claims] 1 焼結体ロツドをホルダーで支持し、加圧不活
性ガス雰囲気下で、その一部を加熱溶融させなが
ら焼結体ロツドを移動させて、単結晶を育成する
方法において、供給焼結体ロツドの組成を、得よ
うとするチタン炭窒化物結晶の固相成分に、溶融
時に融帯から蒸発する窒素、炭素の成分を添加し
た組成となして、溶融帯の組成を、得ようとする
チタン炭窒化物結晶の固相成分と共存する液相成
分の組成となし、かつ該チタン炭窒化物の平衡解
離圧の0.1〜10倍の窒素ガス分圧を有する全圧2
〜100気圧の不活性ガス加圧雰囲気下で溶融帯を
形成させて結晶を育成することを特徴とするチタ
ン炭窒化物の単結晶の製造法。
1. A method of growing a single crystal by supporting a sintered rod with a holder and moving the sintered rod while heating and melting a part of the sintered rod under a pressurized inert gas atmosphere. The composition of the titanium carbonitride crystal to be obtained is determined by adding nitrogen and carbon components that evaporate from the melting zone during melting to the solid phase components of the titanium carbonitride crystal to be obtained. A total pressure 2 having a composition of a liquid phase component coexisting with a solid phase component of the carbonitride crystal, and having a nitrogen gas partial pressure of 0.1 to 10 times the equilibrium dissociation pressure of the titanium carbonitride.
A method for producing a single crystal of titanium carbonitride, which is characterized by growing a crystal by forming a molten zone in an inert gas pressurized atmosphere of ~100 atmospheres.
JP23904885A 1985-10-25 1985-10-25 CHITANTANCHITSUKABUTSUNOTANKETSUSHONOSEIZOHO Expired - Lifetime JPH0232237B2 (en)

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Publications (2)

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JPS62100500A JPS62100500A (en) 1987-05-09
JPH0232237B2 true JPH0232237B2 (en) 1990-07-19

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