JPH0826895A - Method for producing yttrium vanadate single crystal - Google Patents

Method for producing yttrium vanadate single crystal

Info

Publication number
JPH0826895A
JPH0826895A JP16365194A JP16365194A JPH0826895A JP H0826895 A JPH0826895 A JP H0826895A JP 16365194 A JP16365194 A JP 16365194A JP 16365194 A JP16365194 A JP 16365194A JP H0826895 A JPH0826895 A JP H0826895A
Authority
JP
Japan
Prior art keywords
crystal
single crystal
yttrium vanadate
laser
plane
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.)
Pending
Application number
JP16365194A
Other languages
Japanese (ja)
Inventor
Masahiro Kubo
正洋 久保
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 Metal Mining Co Ltd
Original Assignee
Sumitomo Metal Mining 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 Sumitomo Metal Mining Co Ltd filed Critical Sumitomo Metal Mining Co Ltd
Priority to JP16365194A priority Critical patent/JPH0826895A/en
Publication of JPH0826895A publication Critical patent/JPH0826895A/en
Pending legal-status Critical Current

Links

Landscapes

  • Crystals, And After-Treatments Of Crystals (AREA)

Abstract

PURPOSE:To obtain an yttrium vanadate single crystal in a higher yield and suppress the developing of crystal defects causing losses to laser beams while maintaining the simplicity of making a {100}-plane wafer. CONSTITUTION:This yttrium vanadate single crystal is obtained by pull method. In this case, the azimuth of the seed crystal is set at <110>.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は引き上げ法によるイット
リウムバナデイト単結晶の製造方法に関するもので、上
記単結晶は光学用途、主として小型の固体レーザ用材料
として用いられる。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method for producing a yttrium vanadate single crystal by a pulling method, which is used as a material for optical applications, mainly as a small solid-state laser.

【0002】[0002]

【従来の技術】イットリウムバナデイト単結晶は、YV
4の化学式で表すことのできる材料で、Nd等の希土
類元素を添加しレーザ結晶として用いられる。イットリ
ウムバナデイト単結晶には通常Ndを2〜3原子%ほど
添加するが、Ndを2原子%添加したイットリウムバナ
デイト単結晶は、最も一般的なレーザ結晶であるNdを
1原子%添加したイットリウムアルミニウムガーネット
に比べ、波長0.8μmの半導体レーザ光に対する吸収
係数が約6倍も大きい。そのため半導体レーザにより結
晶を端面から励起しレーザ発振を行う場合には、レーザ
結晶の光軸方向に対する長さは1mm程度で良く、特に
小型の固体レーザ用材料として用いられている。
2. Description of the Related Art Yttrium vanadate single crystals are YV
It is a material that can be represented by the chemical formula of O 4 , and is used as a laser crystal to which a rare earth element such as Nd is added. Yttrium vanadate single crystal is usually doped with 2 to 3 atomic% of Nd. Yttrium vanadate single crystal containing 2 atomic% of Nd is the most common laser crystal containing 1 atomic% of Nd. Compared with aluminum garnet, the absorption coefficient for semiconductor laser light with a wavelength of 0.8 μm is about 6 times larger. Therefore, when laser oscillation is performed by exciting a crystal from the end face with a semiconductor laser, the length of the laser crystal in the optical axis direction may be about 1 mm, and it is particularly used as a small-sized solid-state laser material.

【0003】また、この結晶は正方晶系に属し、光学的
に異方で、電界ベクトルの方向がc軸に平行な、いわゆ
るπ偏光の光に対する吸収係数が、c軸に垂直なσ偏光
の光と比較し大きい。そこで通常は結晶の光軸がc軸と
垂直となるよう、厚さ1mm程度の{100}面ウエハ
ーから数mm角の小片を切り出し、レーザ発振器中のレ
ーザ結晶として用いられている。
This crystal belongs to a tetragonal system and is optically anisotropic. The absorption coefficient for so-called π-polarized light whose electric field vector is parallel to the c-axis is σ-polarized light perpendicular to the c-axis. Larger than light. Therefore, a small piece of a few mm square is cut out from a {100} plane wafer having a thickness of about 1 mm and used as a laser crystal in a laser oscillator so that the optical axis of the crystal is perpendicular to the c-axis.

【0004】イットリウムバナデイト単結晶は引き上げ
法により単結晶を製造しているが、上記{100}面ウ
エハーを作製するには、種結晶の方位を〈100〉ある
いは〈001〉として製造した単結晶を用いるのが簡単
である。種結晶方位を〈100〉として製造した単結晶
の場合には、引き上げ軸方向に対し垂直な方向に切断す
るだけで上記{100}面ウエハーを作製することがで
きる。また種結晶方位を〈001〉とした場合には、製
造された結晶において、結晶径が一定になるよう制御し
成長させた部分の結晶表面、つまり直胴部表面に必ず
{100}面が現れるため、この{100}面に対し平
行に結晶を切断することで上記ウエハーを作製すること
ができる。
The yttrium vanadate single crystal is produced by the pulling method. To produce the above {100} plane wafer, the single crystal produced by setting the seed crystal orientation to <100> or <001>. Is easy to use. In the case of a single crystal manufactured with a seed crystal orientation of <100>, the {100} plane wafer can be manufactured simply by cutting in the direction perpendicular to the pulling axis direction. When the seed crystal orientation is <001>, in the manufactured crystal, the {100} plane always appears on the crystal surface of the grown portion where the crystal diameter is controlled to be constant, that is, on the surface of the straight body portion. Therefore, the wafer can be manufactured by cutting the crystal parallel to the {100} plane.

【0005】以上のように上記2つの種結晶方位を用い
た場合には、{100}面ウエハー切断の際に基準とな
る方向ないし面が存在するため、容易にかつ正確に{1
00}面ウエハーを作製することができる。そのためレ
ーザ材料として用いるイットリウムバナデイト単結晶を
作製する際の種結晶方位には、専ら〈100〉あるいは
〈001〉が用いられている。
As described above, when the above two seed crystal orientations are used, there is a reference direction or plane when the {100} plane wafer is cut, so that {1} can be easily and accurately obtained.
A 00} plane wafer can be manufactured. Therefore, <100> or <001> is exclusively used as the seed crystal orientation when producing the yttrium vanadate single crystal used as the laser material.

【0006】[0006]

【発明が解決しようとする課題】レーザ結晶の具備すべ
き条件の1つに、結晶欠陥を持っていないことがある。
それは結晶欠陥が存在するウエハーをレーザ結晶として
レーザ発振に用いると、結晶欠陥がレーザ光に対する散
乱体つまりレーザ共振器にとってレーザ光の損失要因と
して働くため、高強度のレーザ光出力が得られないから
である。
One of the conditions that the laser crystal should have is that it does not have a crystal defect.
This is because when a wafer with crystal defects is used as a laser crystal for laser oscillation, the crystal defects act as a loss factor of the laser light for the scatterer for the laser light, that is, the laser resonator, so that high-intensity laser light output cannot be obtained. Is.

【0007】ところが種結晶方位を〈100〉あるいは
〈001〉として製造を行った単結晶には、結晶欠陥が
多いという欠点がある。引き上げ法による結晶成長で
は、結晶成長炉内の温度制御を行い結晶径が一定な直胴
部を形成しているが、イットリウムバナデイト単結晶の
製造では、結晶が直径方向に突起的かつ急激に成長する
急成長と呼ばれる現象が頻繁に発生していた。ここで、
結晶が突起的に成長する方向は決まっており、必ず〈1
00〉方向となっている。その理由は、{100}面の
成長速度が他の面に比較し速いためと考えられている。
一般に急激に成長した結晶には欠陥が多く入るが、イッ
トリウムバナデイト単結晶の場合も急成長が生じた部分
は他の部分に比べボイド等の結晶欠陥が多く、このこと
が種結晶方位を〈100〉あるいは〈001〉として製
造を行った単結晶の品質を低下させていた。
However, a single crystal manufactured with a seed crystal orientation of <100> or <001> has a drawback that it has many crystal defects. In the crystal growth by the pulling method, the temperature in the crystal growth furnace is controlled to form a straight body with a constant crystal diameter.However, in the production of yttrium vanadate single crystal, the crystal is projected and suddenly increases in the diameter direction. A phenomenon called rapid growth frequently occurred. here,
The direction in which the crystal grows in a protruding manner is fixed, and always <1
00> direction. It is considered that the reason is that the growth rate of the {100} plane is higher than that of other planes.
Generally, rapidly grown crystals have many defects, but in the case of yttrium vanadate single crystal, the parts where rapid growth occurs have more crystal defects such as voids than other parts, which causes seed crystal orientation The quality of the single crystal manufactured as 100> or <001> was deteriorated.

【0008】本発明の目的は、イットリウムバナデイト
単結晶製造において、{100}面ウエハー作製の簡便
性を維持しつつ、レーザ光に対し損失として働く結晶欠
陥の発生を抑制し、単結晶の歩留まりを向上させること
にある。
The object of the present invention is to suppress the occurrence of crystal defects that act as a loss for laser light and maintain the yield of single crystals in the production of yttrium vanadate single crystals while maintaining the simplicity of producing {100} plane wafers. To improve.

【0009】[0009]

【課題を解決するための手段】本発明は、上記目的を達
成するために、引き上げ法によるイットリウムバナデイ
ト単結晶の製造方法において種結晶の方位を〈110〉
として製造することを特徴とする。
In order to achieve the above-mentioned object, the present invention provides a seed crystal having an orientation of <110> in a method for producing a yttrium vanadate single crystal by a pulling method.
It is characterized by being manufactured as.

【0010】[0010]

【作用】種結晶の方位を〈110〉とすると、直胴部製
造中に{100}面の出現を防ぐことができるため、強
いては急成長を防止することができる。それは直胴部製
造中に{100}面が現れるとすれば、坩堝内の融液と
接している結晶底部の面と引き上げ軸のなす角度、いわ
ゆる結晶底部角度が45度の角度になったときのみ{1
00}面が出現するからである。結晶底部角度は、炉内
の温度環境を調節することにより容易に変更することが
できるため、{100}面の出現は容易に防止すること
ができる。
When the orientation of the seed crystal is <110>, it is possible to prevent the appearance of the {100} plane during the production of the straight body portion, so that it is possible to prevent sudden growth. If the {100} plane appears during the production of the straight body, the angle between the pulling axis and the plane of the crystal bottom that is in contact with the melt in the crucible, the so-called crystal bottom angle, becomes 45 degrees. Only {1
This is because the {00} plane appears. Since the crystal bottom angle can be easily changed by adjusting the temperature environment in the furnace, the appearance of the {100} plane can be easily prevented.

【0011】また直胴部製造中には防止したい{10
0}面の出現も、種結晶から所定の径にまで結晶径を太
くする結晶肩部製造中においては、徐々に太くなる結晶
外周が積算された面、いわゆる肩部表面と引き上げ軸の
なす角度を45度とし、むしろ積極的に結晶肩部表面に
{100}面が生じるようにすることにより、引き上げ
られた単結晶から{100}面ウエハーを切り出す際の
基準面を作製することができる。結晶肩部の{100}
面を基準として、この面に平行に結晶を切断すれば、容
易にかつ正確に{100}面ウエハーを作製することが
できる。
In addition, it is desired to prevent this during manufacturing of the straight body part {10
The appearance of the 0} plane also increases the crystal diameter from the seed crystal to a predetermined diameter during the production of the crystal shoulder portion. Is 45 degrees, and rather, the {100} plane is positively generated on the surface of the crystal shoulder portion, whereby the reference plane for cutting the {100} plane wafer from the pulled single crystal can be produced. Crystal shoulder {100}
If the crystal is cut parallel to this plane with the plane as the reference, a {100} plane wafer can be easily and accurately manufactured.

【0012】以上に示したように種結晶方位として〈1
10〉を用い、単結晶の製造を行うことにより結晶径の
急成長の発生を抑えることができ、結晶欠陥の無いイッ
トリウムバナデイト単結晶が製造できる。
As shown above, the seed crystal orientation <1
10> to produce a single crystal, it is possible to suppress the rapid growth of the crystal diameter, and an yttrium vanadate single crystal having no crystal defects can be produced.

【0013】[0013]

【実施例】【Example】

(実施例1) 実施例について説明する。まず、酸化イ
ットリウムに対する酸化ネオジウムの混合比率が2原子
%となるような混合物を作製した。ここで酸化イットリ
ウムの純度は99.999重量%、酸化ネオジウムの純
度は99.995重量%であった。次に直径100m
m、深さ100mmのイリジウム製坩堝に純度99.9
9重量%の五酸化バナジウムと上記混合物のモル比が
1:1となるように混入し、2体積%の酸素を含有した
窒素雰囲気中で高周波加熱炉により原料の溶融を行っ
た。次に種結晶方位を本発明の[110]とし、イット
リウムバナデイト種結晶を10rpmで回転させ、融液
に充分浸した後、毎時1mmの引き上げ速度で結晶成長
炉内の温度を制御しながら結晶成長を行い、直径40m
m、全長60mmのイットリウムバナデイト単結晶を製
造した。このとき、急成長は発生しなかった。このイッ
トリウムバナデイト単結晶から厚さ5mmの(100)
面ウエハーを切り出し、光学顕微鏡により観察したが、
光学顕微鏡で見る限りウエハー内には結晶欠陥は認めら
れなかった。
Example 1 An example will be described. First, a mixture was prepared such that the mixing ratio of neodymium oxide to yttrium oxide was 2 atom%. The yttrium oxide had a purity of 99.999% by weight and the neodymium oxide had a purity of 99.995% by weight. Next, diameter 100m
m, depth 100 mm, iridium crucible, purity 99.9
9% by weight of vanadium pentoxide and the above mixture were mixed at a molar ratio of 1: 1 and the raw material was melted in a nitrogen atmosphere containing 2% by volume of oxygen in a high frequency heating furnace. Next, the seed crystal orientation is set to [110] of the present invention, and the yttrium vanadate seed crystal is rotated at 10 rpm and sufficiently immersed in the melt. Grows, diameter 40m
A yttrium vanadate single crystal having a length of 60 mm and a total length of 60 mm was produced. At this time, no rapid growth occurred. From this yttrium vanadate single crystal, a 5 mm thick (100)
The surface wafer was cut out and observed with an optical microscope.
No crystal defects were found in the wafer as viewed with an optical microscope.

【0014】(比較例) 従来例による種結晶方位を
[100]とした製造も行った。種結晶方位以外の条件
を同一にして製造を行ったところ、結晶長が20mmと
なったところで急成長が発生してしまった。急成長が発
生し、結晶径が太くなった部分から前述同様厚さ5mm
の(100)ウエハーを切り出し、光学顕微鏡により同
様に観察を行ったところ、急成長部にのみ多数の散乱体
が観察された。
(Comparative Example) A conventional example was also manufactured in which the seed crystal orientation was [100]. When manufacturing was performed under the same conditions except for the seed crystal orientation, rapid growth occurred at a crystal length of 20 mm. From the part where the crystal diameter became large due to the rapid growth, the thickness was 5 mm as above.
When a (100) wafer was cut out and observed with an optical microscope in the same manner, a large number of scatterers were observed only in the rapidly growing portion.

【0015】(実施例2) 次に本発明による種結晶方
位を[110]とした単結晶より切り出したウエハーと
従来例の種結晶方位を[100]とした単結晶より切り
出したウエハーを用い、波長0.8μmの半導体レーザ
で励起し、波長1.06μmでレーザ発振実験を行っ
た。本発明、従来例共にそれぞれ8枚のウエハーを準備
し、ウエハー面内を縦横7mmおきに25箇所励起し、
そのときのレーザ出力を記録した。従って測定点の数は
全部で400点になる。
Example 2 Next, a wafer cut from a single crystal having a seed crystal orientation of [110] according to the present invention and a wafer cut from a single crystal of a conventional example having a seed crystal orientation of [100] were used. Excitation was performed with a semiconductor laser having a wavelength of 0.8 μm, and a laser oscillation experiment was performed at a wavelength of 1.06 μm. In each of the present invention and the conventional example, eight wafers were prepared, and the wafer surface was excited at 25 locations every 7 mm in length and width,
The laser output at that time was recorded. Therefore, the total number of measurement points is 400 points.

【0016】前記400点の測定点の中、最高のレーザ
出力強度を1としたときの各測定点におけるレーザ出力
の相対強度の度数分布を図1および2に示す。図1は種
結晶方位が[110]のもの、図2は[100]のもの
の測定結果である。種結晶方位を[110]としたイッ
トリウムバナデイト単結晶ウエハーは、レーザ発振出力
が高いものの頻度が高く、その平均値は種結晶方位を
[100]としたものより約30%高かった。またウエ
ハー面位置によるレーザ発振出力のバラツキも、従来例
が0.1〜1.0であったのに対し、0.7〜1.0と
小さくなっていた。尚、レーザ出力が低いものは、結晶
欠陥の多い急成長部にのみ存在していた。
1 and 2 show the frequency distribution of the relative intensity of the laser output at each measurement point when the highest laser output intensity among the 400 measurement points is 1. FIG. 1 shows the measurement results for the seed crystal orientation of [110], and FIG. 2 for the measurement results of [100]. The yttrium vanadate single crystal wafer having a seed crystal orientation of [110] had a high laser oscillation output but a high frequency, and the average value thereof was about 30% higher than that of the seed crystal orientation of [100]. Further, the variation of the laser oscillation output depending on the position of the wafer surface was as small as 0.7 to 1.0, compared with 0.1 to 1.0 in the conventional example. The low laser output existed only in the rapid growth portion having many crystal defects.

【0017】図1および2の測定点の内、相対強度が
0.9以上のものを良品とすると、本発明の歩留まりは
80%、従来例では27%であった。
1 and 2, the yield of the present invention was 80% and the yield of the conventional example was 27% when the product having a relative strength of 0.9 or more was regarded as a good product.

【0018】[0018]

【発明の効果】本発明により、急成長に伴う結晶欠陥の
無いイットリウムバナデイト単結晶の製造方法を提供す
ることができる。本発明により製造された単結晶から切
り出されたウエハーを用いてレーザ発振を行ったとこ
ろ、ウエハー面位置の違いによるレーザ出力のバラツキ
が少なく、かつ得られるレーザ出力の平均値が高いとい
う結果が得られた。また歩留まりも27%から80%に
まで向上した。
Industrial Applicability According to the present invention, it is possible to provide a method for producing a yttrium vanadate single crystal free from crystal defects associated with rapid growth. When laser oscillation was performed using a wafer cut from a single crystal manufactured according to the present invention, there was little variation in laser output due to difference in wafer surface position, and the result was that the average value of the obtained laser output was high. Was given. The yield also improved from 27% to 80%.

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

【図1】図1は本発明の種結晶方位を[110]とした
ウエハーのレーザ発振出力度数分布を示す図である。
FIG. 1 is a diagram showing a laser oscillation power frequency distribution of a wafer having a seed crystal orientation of [110] according to the present invention.

【図2】図2は従来の種結晶方位を[100]としたウ
エハーのレーザ発振出力度数分布を示す図である。
FIG. 2 is a diagram showing a laser oscillation output frequency distribution of a wafer having a conventional seed crystal orientation of [100].

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 引き上げ法によるイットリウムバナデイ
ト単結晶の製造方法において、種結晶の方位を〈11
0〉として製造することを特徴とするイットリウムバナ
デイト単結晶の製造方法。
1. A method for producing a yttrium vanadate single crystal by the pulling method, wherein the orientation of a seed crystal is <11.
0> as the yttrium vanadate single crystal.
JP16365194A 1994-07-15 1994-07-15 Method for producing yttrium vanadate single crystal Pending JPH0826895A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP16365194A JPH0826895A (en) 1994-07-15 1994-07-15 Method for producing yttrium vanadate single crystal

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP16365194A JPH0826895A (en) 1994-07-15 1994-07-15 Method for producing yttrium vanadate single crystal

Publications (1)

Publication Number Publication Date
JPH0826895A true JPH0826895A (en) 1996-01-30

Family

ID=15777996

Family Applications (1)

Application Number Title Priority Date Filing Date
JP16365194A Pending JPH0826895A (en) 1994-07-15 1994-07-15 Method for producing yttrium vanadate single crystal

Country Status (1)

Country Link
JP (1) JPH0826895A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008201618A (en) * 2007-02-20 2008-09-04 Covalent Materials Corp Method for producing rare earth vanadate single crystal

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008201618A (en) * 2007-02-20 2008-09-04 Covalent Materials Corp Method for producing rare earth vanadate single crystal

Similar Documents

Publication Publication Date Title
Lu et al. 110 W ceramic Nd3+: Y3Al5O12 laser
US4824598A (en) Synthetic laser medium
US4802180A (en) Growth of congruently melting gadolinium scandium gallium garnet
EP0535738B1 (en) Method of manufacturing potassium-lithium-niobate crystals
SU1609462A3 (en) Laser substance
EP0238142B1 (en) Solid state laser hosts
Ehrentraut et al. Epitaxial growth and spectroscopic investigation of BaSO4: Mn6+ layers
Yamaga et al. Superlattice structure of Ce3+-doped BaMgF4 fluoride crystals-x-ray diffraction, electron spin-resonance, and optical investigations
JPH11243247A (en) Lanthanum magnesium aluminate(lma) single-crystal layer, growth process based on liquid phase epitaxial growth thereof, and optical part containing the single-crystal layer
US5541764A (en) Cerium doped barium titanate single crystal, the process therefor and photorefractive device thereby
US11437773B2 (en) Wavelength conversion device
Fukuda et al. Crystal growth of oxide and fluoride materials for optical, piezoelectric and other applications
JP2003267799A (en) Magnesium lithium niobate single crystal and method for producing the same
JPH0618949A (en) Cerium-doped optical device
JPH09202699A (en) Method for producing garnet structure single crystal
US5311532A (en) Calcium-yttrium silicate oxyapatite lasers
JP3183192B2 (en) Method for producing oxide single crystal and oxide single crystal
JPH08283093A (en) Laser material manufacturing method
Kokta Crystal growth and characterization of oxides host crystals for tunable lasers
JP3286680B2 (en) Laser crystal and manufacturing method thereof
CN113948957B (en) Broadband tunable cerium-dysprosium-doped yellow laser crystal and preparation method and application thereof
JPH05335678A (en) Yag single crystal for laser
JP2004231423A (en) Gadolinium vanadate single crystal and its manufacturing method
JPH0891999A (en) Yttrium vanadate single crystal for laser and method for producing the same
JP2008201618A (en) Method for producing rare earth vanadate single crystal