JPH025720B2 - - Google Patents
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- Publication number
- JPH025720B2 JPH025720B2 JP22221384A JP22221384A JPH025720B2 JP H025720 B2 JPH025720 B2 JP H025720B2 JP 22221384 A JP22221384 A JP 22221384A JP 22221384 A JP22221384 A JP 22221384A JP H025720 B2 JPH025720 B2 JP H025720B2
- Authority
- JP
- Japan
- Prior art keywords
- partial pressure
- crystal
- oxygen partial
- oxygen
- single crystal
- 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.)
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- Crystals, And After-Treatments Of Crystals (AREA)
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明はルチル(TiO2)単結晶の製造方法に
関するものである。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a method for producing rutile (TiO 2 ) single crystal.
複屈折が大きく、偏光プリズムなど高精度光学
機器部品に利用されている方解石は、合成技術が
充分に確立されていないため、天然品が使用され
ている。しかし、良質天然方解石は近時品薄状態
になつて来ており、しかも硬度が低いため、取扱
いに不便である等の問題がある。
Calcite, which has a large birefringence and is used in high-precision optical equipment parts such as polarizing prisms, is a natural product because the synthesis technology has not been fully established. However, high-quality natural calcite has recently been in short supply, and its low hardness causes problems such as inconvenience in handling.
そこで、最近複屈折率が0.3と大きいルチル
(TiO2)が着目され、方解石の代替品として期待
されている。しかし現在市販されているルチル
は、ベルヌーイ法で育成した製品で、熱歪による
光学的歪が大きいこと、気泡入り製品が多いなど
の欠点があり、高精度の光学機械器具の部品とし
ては不適当なものである。 Therefore, rutile (TiO 2 ), which has a high birefringence index of 0.3, has recently attracted attention and is expected to be a substitute for calcite. However, the rutile currently on the market is a product grown using the Bernoulli method, and has drawbacks such as large optical distortion due to thermal distortion and many products containing bubbles, making it unsuitable as a component for high-precision optical equipment. It is something.
また引上法などで代表されるその他の融液成長
法による結晶育成も試みられているが、サブグレ
イン組織、即ち、結晶方位が比較的そろつた直径
数百ミクロンから数ミリ程度の結晶粒の集合体と
なつている組織が現われることが多く、ベルヌー
イ法結晶より劣る品質の結晶しか得られていな
い。 Attempts have also been made to grow crystals using other melt growth methods, such as the pulling method. Aggregated structures often appear, and only crystals of inferior quality to the Bernoulli method crystals are obtained.
そこで本発明は、高精度の光学機械器具の部品
としても使用できる光学的に無歪で気泡のないル
チル単結晶を製造する方法を提案しようとするも
のである。 Therefore, the present invention seeks to propose a method for producing an optically undistorted and bubble-free rutile single crystal that can also be used as a component of high-precision opto-mechanical equipment.
酸化チタンにおいては、Ti4+とTi3+の共存に
よりTinO2n-1(nは1以上の整数)で表わされ
る、一連の類似した結晶構造を持つ、それぞれ独
立した結晶相の存在が知られている。それぞれの
相は特定範囲の酸素分圧の下でのみ安定に存在す
る。従つて融液から結晶が固化する時、固化する
結晶の組成、即ち結晶構造は雰囲気中の酸素分圧
に左右される。即ち、酸素分圧が高い時はnの大
きな結晶が、酸素分圧が低い時はnの小さな結晶
相が得られる。酸素分圧の値によつては2種の隣
り合つた組成の結晶相が同時に晶出する。この様
な場合には、一般の融液からの結晶成長技術を適
用しても、単結晶が得られないことは自明であ
る。
In titanium oxide, the existence of a series of independent crystal phases with similar crystal structures, expressed as TinO 2 n -1 (n is an integer of 1 or more), is known to exist due to the coexistence of Ti 4+ and Ti 3+ . It is being Each phase exists stably only under a specific range of oxygen partial pressure. Therefore, when a crystal solidifies from a melt, the composition of the solidified crystal, that is, the crystal structure, depends on the oxygen partial pressure in the atmosphere. That is, when the oxygen partial pressure is high, a crystal with a large n is obtained, and when the oxygen partial pressure is low, a crystal phase with a small n is obtained. Depending on the value of the oxygen partial pressure, two types of crystal phases having adjacent compositions may crystallize simultaneously. In such a case, it is obvious that a single crystal cannot be obtained even if ordinary crystal growth techniques from melt are applied.
TinO2n-1の組成の結晶相は、nが大きい時、
即ち組成がTiO2に極めて近い時、徐冷又は焼鈍
により単結晶のまま容易にルチル構造に変化す
る。それは、TinO2n-1の構造が、ルチル構造に
酸素欠損型の格子欠陥を整然と導入した形になつ
ており、低温での酸素拡散によりこれらが除去さ
れ易いためである。しかも同じ酸素分圧下では低
温程Ti3+の許容含有量は少なくなる。従つて、
上記の2相共存状態で固化した結晶は、室温まで
徐冷すると、すべてルチル構造になつているにも
かかわらず、サブグレイン組織を含んだものにな
る。これが従来融液成長法により良質結晶の得ら
れなかつた理由である。 The crystal phase of the composition TinO 2 n -1 is, when n is large,
That is, when the composition is very close to TiO 2 , it easily changes to a rutile structure while remaining a single crystal by slow cooling or annealing. This is because the structure of TinO 2 n -1 has oxygen-deficient lattice defects introduced into the rutile structure in an orderly manner, and these are easily removed by oxygen diffusion at low temperatures. Furthermore, under the same oxygen partial pressure, the lower the temperature, the lower the allowable content of Ti 3+ . Therefore,
When the crystals solidified in the above-mentioned two-phase coexistence state are slowly cooled to room temperature, they contain a subgrain structure even though they all have a rutile structure. This is the reason why good quality crystals have not been obtained by conventional melt growth methods.
従つてサブグレイン組織のない、良質のルチル
結晶を得る手段は、固化に際して、一種類だけの
結晶相が晶出する様な酸素分圧を供給することで
ある。 Therefore, the means to obtain high-quality rutile crystals without subgrain structure is to supply oxygen partial pressure such that only one type of crystal phase is crystallized during solidification.
本発明は、上記の様な考え方に基づくもので雰
囲気中の酸素分圧を3×10-2気圧以下の範囲に保
つて、融液から酸化チタンの単結晶を成長させる
ようにしたものである。
The present invention is based on the above-mentioned concept, and is designed to grow a single crystal of titanium oxide from a melt while maintaining the oxygen partial pressure in the atmosphere within a range of 3 x 10 -2 atmospheres or less. .
本発明により初めて、晶出する酸化チタンが一
種類だけになる酸素分圧の範囲は、該範囲である
ことが明らかとなつた。 The present invention has revealed for the first time that the oxygen partial pressure range in which only one type of titanium oxide crystallizes falls within this range.
本発明において適用する融液からの結晶成長法
とは引上法、ベルヌーイ法、ブリジマン法、フロ
ーテイングゾーン法など何でも良いが、成長結晶
の高品質化が達成し易いので引上法やフローテイ
ングゾーン法が好ましく、特に容器からの不純物
汚染が無いフローテイングゾーン法が好ましい。 The method for growing crystals from a melt applied in the present invention may be any method such as the pulling method, Bernoulli method, Brigeman method, or floating zone method, but since it is easy to achieve high quality grown crystals, The zone method is preferred, and the floating zone method, which is free from impurity contamination from the container, is particularly preferred.
本発明に用いる出発原料としてのTiO2は市販
の特級試薬で良いが、光学結晶の原料としての純
度は高い程好ましい。尚、用途に応じて物理的、
化学的性質を制御するために、Fe、Ni、Co、
Mn、Cr、Li、Mg、Cu、Zn、Cd、Al、Ga、V、
Nb、Ta、Si、Ge、Zr、Hf、Mo、Wなどの元素
を少量添加することができる。 TiO 2 as a starting material used in the present invention may be a commercially available special grade reagent, but as a raw material for optical crystals, the higher the purity, the better. In addition, depending on the use, physical
Fe, Ni, Co,
Mn, Cr, Li, Mg, Cu, Zn, Cd, Al, Ga, V,
Small amounts of elements such as Nb, Ta, Si, Ge, Zr, Hf, Mo, and W can be added.
本発明における結晶の成長速度は0.1〜300mm/
時、好ましくは0.5〜15mm/時、特に好ましくは
3〜8mm/時である。 The crystal growth rate in the present invention is 0.1 to 300 mm/
time, preferably 0.5 to 15 mm/hour, particularly preferably 3 to 8 mm/hour.
本発明において結晶成長雰囲気中の酸素分圧範
囲3×10-2気圧以下を実現するためには結晶成長
近傍の高温で熱平衡反応や熱分解反応などによ
り、遊離の酸素を所定量放出するCO2やNOx等
のガスが利用される。酸素分圧範囲を正しく設定
するために、これらのガスの純度は高い程好まし
い。 In the present invention, in order to achieve an oxygen partial pressure range of 3×10 -2 atmospheres or less in the crystal growth atmosphere, a predetermined amount of free oxygen must be released by thermal equilibrium reaction or thermal decomposition reaction at a high temperature near the crystal growth region . Gases such as NOx and NOx are used. In order to correctly set the oxygen partial pressure range, the higher the purity of these gases, the better.
また、該酸素分圧範囲を実現するためには酸素
と不活性ガスから成る混合ガスを用いてもよい。
前記不活性ガスとは、Arを初めとする希ガス元
素又は窒素である。これらの不活性ガスは酸素分
圧範囲を正しく設定するために純度が高い程好ま
しい。 Further, in order to realize the oxygen partial pressure range, a mixed gas consisting of oxygen and an inert gas may be used.
The inert gas is a rare gas element such as Ar or nitrogen. It is preferable that these inert gases have higher purity in order to correctly set the oxygen partial pressure range.
本発明により得られる結晶は、室温への冷却過
程でほゞTiO2.0の組成になるが、分析による検出
が困難な程度のTi3+を含んでおり、透明度が不
充分であることがある。この様な場合、結晶を
1000℃以下の空気又は酸素中で焼鈍することによ
り透明度を増すことができる。焼鈍温度は600〜
1000℃、好ましくは700〜900℃である。焼鈍温度
は長ければ長い程良いが、生産効率を上昇させ、
且つ充分な透明度を確保するために3〜100時間、
好ましくは5〜70時間である。 The crystals obtained by the present invention have a composition of approximately TiO 2.0 during the cooling process to room temperature, but they contain Ti 3+ to an extent that is difficult to detect by analysis, and their transparency may be insufficient. be. In such cases, the crystal
Transparency can be increased by annealing in air or oxygen at temperatures below 1000°C. Annealing temperature is 600~
The temperature is 1000°C, preferably 700-900°C. The longer the annealing temperature, the better, but it is important to increase production efficiency.
3 to 100 hours to ensure sufficient transparency.
Preferably it is 5 to 70 hours.
実施例 1
市販のTiO2(99.98%)粉末を1ton/cm2の静水
圧で棒状にラバープレス成形し、1400℃の空気中
で焼結した。これを回転楕円面鏡を用いた集光フ
ローテイングゾーン法単結晶製造装置に原料棒と
して装填し、別に準備したルチル単結晶を種結晶
として装填した。雰囲気中の酸素分圧を制御する
ためにCO2を結晶成長室に導入し、2/分の流
量で結晶成長終了まで流し続け、フローテイング
ゾーン法の常法に従つて結晶育成操作を行い青黒
色の結晶を得た。Example 1 Commercially available TiO 2 (99.98%) powder was rubber press molded into a rod shape under a hydrostatic pressure of 1 ton/cm 2 and sintered in air at 1400°C. This was loaded as a raw material rod into a condensing floating zone method single crystal manufacturing apparatus using a spheroidal mirror, and a separately prepared rutile single crystal was loaded as a seed crystal. In order to control the oxygen partial pressure in the atmosphere, CO 2 was introduced into the crystal growth chamber and continued to flow at a flow rate of 2/min until the crystal growth was completed. Black crystals were obtained.
育成条件は、原料棒及び種結晶の回転速度が逆
方向にそれぞれ25回/分、結晶成長速度は5mm/
時であつた。得られた結晶を800℃48時間空気中
で焼鈍してわずかに黄色を帯びた透明な結晶体を
得た。この結晶から成長方向及びそれに垂直な方
向に平行な面を持つ試料を切り出し、光学研磨の
上、偏光顕微鏡で調べた所、歪、気泡、サブグレ
イン組織などが検出されない良質ルチル単結晶で
あることが明らかになつた。 The growth conditions are that the rotation speed of the raw material rod and the seed crystal is 25 times/min in opposite directions, and the crystal growth rate is 5 mm/min.
It was hot at the time. The obtained crystal was annealed in air at 800°C for 48 hours to obtain a slightly yellowish transparent crystal. A sample with planes parallel to the growth direction and the direction perpendicular to it is cut out from this crystal, and after optical polishing and examination using a polarizing microscope, it is a high-quality rutile single crystal with no detectable distortion, bubbles, or subgrain structure. has become clear.
実施例 2
実施例1と全く同様の操作において、雰囲気中
の酸素分圧を制御するために超高純度ArとO2を
100対3の割合で混合した混合ガスを結晶成長室
に導入し、2/分の流量で育成終了まで流し続
けた。他の操作も実施例1と全く同様にして、
歪、気泡、サブグレイン組織等がほとんど検出さ
れない良質ルチル単結晶を得た。Example 2 In exactly the same operation as Example 1, ultra-high purity Ar and O 2 were used to control the oxygen partial pressure in the atmosphere.
A mixed gas mixed at a ratio of 100:3 was introduced into the crystal growth chamber and continued to flow at a flow rate of 2/min until the end of growth. Other operations were performed in exactly the same manner as in Example 1,
A high-quality rutile single crystal with almost no detectable distortion, bubbles, subgrain structure, etc. was obtained.
以上の実施例から明らかなように、本発明の特
長は、融液からルチル単結晶を成長させる際に、
雰囲気中の酸素分圧を3×10-2気圧以下の範囲に
保つことにより、一種類だけの結晶相を晶出さ
せ、サブグレイン組織のない、良質のルチル単結
晶を得ることにある。
As is clear from the above examples, the feature of the present invention is that when growing a rutile single crystal from a melt,
The purpose is to crystallize only one type of crystal phase by maintaining the oxygen partial pressure in the atmosphere within a range of 3 x 10 -2 atmospheres or less, and to obtain a high-quality rutile single crystal without subgrain structure.
これに対して、酸素、空気等を供給して本発明
において限定した範囲より高い酸素分圧とする
か、あるいは超高純度Arを供給してほとんど零
の酸素分圧とすると、晶出する結晶は多くのサブ
グレイン組織を含み、良質の結晶は得られない。
なお、酸素分圧の下限値を決定することは困難で
あるが、超高純度ArとO2を100ppm含むArを
100:1の割合で混合して酸素分圧10-6気圧の雰
囲気をつくり、実施例1と全く同様にして結晶を
育成したところ、局部的にサブグレインが検出さ
れたが、ほぼ良質なルチル単結晶を得た。 On the other hand, if oxygen, air, etc. are supplied to make the oxygen partial pressure higher than the range limited in the present invention, or if ultra-high purity Ar is supplied to make the oxygen partial pressure almost zero, crystals will crystallize. contains many subgrain structures, and high quality crystals cannot be obtained.
Although it is difficult to determine the lower limit of oxygen partial pressure, ultra-high purity Ar and Ar containing 100ppm O2 are used.
When an atmosphere with an oxygen partial pressure of 10 -6 atmospheres was created by mixing at a ratio of 100:1 and crystals were grown in exactly the same manner as in Example 1, subgrains were locally detected, but mostly good quality rutile was grown. A single crystal was obtained.
Claims (1)
長させる方法において、雰囲気中の酸素分圧を3
×10-2気圧以下の範囲に保つことを特徴とするル
チル単結晶の製造方法。 2 融液及び成長結晶の近傍に少量酸素を放出す
るCO2又はNOxを導入して雰囲気中の酸素分圧
を3×10-2気圧以下の範囲に制御することを特徴
とする特許請求の範囲第1項記載のルチル単結晶
の製造方法。 3 融液及び成長結晶の近傍に酸素と不活性ガス
の混合ガスを導入して雰囲気中の酸素分圧を3×
10-2気圧以下の範囲に制御することを特徴とする
特許請求の範囲第1項記載のルチル単結晶の製造
方法。[Claims] 1. In a method of growing crystals from a melt obtained by melting TiO 2 at high temperature, the oxygen partial pressure in the atmosphere is
A method for producing a rutile single crystal characterized by maintaining the temperature within a range of ×10 -2 atmospheres or less. 2. Claims characterized in that the oxygen partial pressure in the atmosphere is controlled to a range of 3×10 -2 atmospheres or less by introducing CO 2 or NOx that releases a small amount of oxygen into the vicinity of the melt and the growing crystal. 2. The method for producing a rutile single crystal according to item 1. 3 Introducing a mixed gas of oxygen and inert gas near the melt and growing crystal to increase the oxygen partial pressure in the atmosphere by 3
The method for producing a rutile single crystal according to claim 1, characterized in that the pressure is controlled to a range of 10 -2 atmospheres or less.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP22221384A JPS61101495A (en) | 1984-10-24 | 1984-10-24 | Method for producing rutile single crystal |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP22221384A JPS61101495A (en) | 1984-10-24 | 1984-10-24 | Method for producing rutile single crystal |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS61101495A JPS61101495A (en) | 1986-05-20 |
| JPH025720B2 true JPH025720B2 (en) | 1990-02-05 |
Family
ID=16778901
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP22221384A Granted JPS61101495A (en) | 1984-10-24 | 1984-10-24 | Method for producing rutile single crystal |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS61101495A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH042683A (en) * | 1990-04-16 | 1992-01-07 | Chichibu Cement Co Ltd | Production of rutile single crystal |
| KR100414519B1 (en) * | 2001-10-26 | 2004-01-13 | 학교법인 한양학원 | method of growing rutile single crystal under high oxygen pressure |
-
1984
- 1984-10-24 JP JP22221384A patent/JPS61101495A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS61101495A (en) | 1986-05-20 |
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