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JPS6367347B2 - - Google Patents
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JPS6367347B2 - - Google Patents

Info

Publication number
JPS6367347B2
JPS6367347B2 JP19832484A JP19832484A JPS6367347B2 JP S6367347 B2 JPS6367347 B2 JP S6367347B2 JP 19832484 A JP19832484 A JP 19832484A JP 19832484 A JP19832484 A JP 19832484A JP S6367347 B2 JPS6367347 B2 JP S6367347B2
Authority
JP
Japan
Prior art keywords
crystal
compositions
observed
wavelength tunable
introducing
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
JP19832484A
Other languages
Japanese (ja)
Other versions
JPS6177380A (en
Inventor
Shigeyuki Kimura
Shoken Sai
Yasuto Myazawa
Masami Sekida
Fujio Minami
Kenji Kitamura
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
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 KAGAKU GIJUTSUCHO MUKIZAISHITSU KENKYUSHOCHO filed Critical KAGAKU GIJUTSUCHO MUKIZAISHITSU KENKYUSHOCHO
Priority to JP19832484A priority Critical patent/JPS6177380A/en
Publication of JPS6177380A publication Critical patent/JPS6177380A/en
Publication of JPS6367347B2 publication Critical patent/JPS6367347B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/14Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range characterised by the material used as the active medium
    • H01S3/16Solid materials

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Engineering & Computer Science (AREA)
  • Plasma & Fusion (AREA)
  • Optics & Photonics (AREA)
  • Lasers (AREA)

Description

【発明の詳細な説明】 産業上の利用分野 本発明は波長可変レーザー用ガーネツト結晶に
関する。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to a garnet crystal for wavelength tunable lasers.

従来技術 従来、Cr3+を活性イオンとする波長可変レーザ
ー用のガーネツト結晶としては、数種のものが知
られているが、なかでもGd3Sc2Ga3O12は高いレ
ーザー性能を有するものとして期待されている。
Conventional technology Several types of garnet crystals for wavelength tunable lasers using Cr 3+ as the active ion have been known, but among them, Gd 3 Sc 2 Ga 3 O 12 has high laser performance. It is expected that

しかしながら、この結晶は構成成分として極め
て高価で、且つ資源的にも限られているスカンジ
ウム(Sc)を含んでいる。そのため、結晶が高
価になると言う欠点を有している。
However, this crystal contains scandium (Sc), which is an extremely expensive and limited resource. Therefore, it has the disadvantage that the crystal is expensive.

発明の目的 本発明はGd3Sc2Ga3O12の結晶における構成成
分であるScの1部を置換元素の導入によりScの
使用量を少くし、比較的低廉な波長可変レーザー
用ガーネツト結晶を提供せんとするにある。
Purpose of the Invention The present invention aims to reduce the amount of Sc used in a Gd 3 Sc 2 Ga 3 O 12 crystal by introducing a substituting element for a portion of Sc, thereby creating a relatively inexpensive garnet crystal for wavelength tunable lasers. It is not intended to be provided.

発明の構成 本発明者は前記目的を達成すべく研究の結果、
その結晶において、Scが占める結晶格子は、8
個の酸素イオンに囲まれた格子であり、イオン半
径の類似した金属イオンで、しかも安価な金属イ
オンにより置換できる可能性があることを知り得
た。そしてScは3価の陽イオンであるから、置
換金属イオンはScの価数を過不足なく補うもの
でなければならないとの考察から置換可能な陽イ
オンについて検討を加えた。
Structure of the Invention As a result of research to achieve the above object, the present inventor has
In that crystal, the crystal lattice occupied by Sc is 8
It was discovered that the lattice is surrounded by oxygen ions, and that it may be possible to replace it with a metal ion with a similar ionic radius, which is also inexpensive. Since Sc is a trivalent cation, we considered that the substituted metal ion must compensate for the valence of Sc in just the right amount, so we investigated cations that can be substituted.

実験的に調べた結果、Li+またはMg2+とTi4+
Zr4+、Hf4+の4価金属イオンまたはNb5+、Ta5+
の5価金属との組合せにより、Scイオンの格子
点を過不足なく埋め、かつ価数を過不足なく補う
とよいこと、また、完全にScが存在しない組成
まで置換できないことが分つた。この知見に基い
て本発明を完成した。
As a result of experimental investigation, Li + or Mg 2+ and Ti 4+ ,
Tetravalent metal ions of Zr 4+ , Hf 4+ or Nb 5+ , Ta 5+
It was found that by combining with a pentavalent metal, the lattice points of Sc ions can be filled in just the right amount, and the valence can be compensated for just the right amount, and that it is not possible to replace the composition to a composition where Sc is completely absent. The present invention was completed based on this knowledge.

本発明の要旨は、 Cr3+を活性イオンとする波長可変レーザー用媒
質結晶として用いるGd3Sc2Ga3O12の結晶におい
て、Scイオンの1部を、Li+またはMg2+とTi4+
Zr4+、Hf4+、Nb5+及びTa5+から選ばれた単独ま
たは2種以上の金属イオンとの組合せにより、結
晶内の電価が中和に保たれるように置換したこと
を特徴とする波長可変レーザー用ガーネツト結晶
にある。
The gist of the present invention is that in a Gd 3 Sc 2 Ga 3 O 12 crystal used as a medium crystal for a wavelength tunable laser with Cr 3+ as an active ion, a part of the Sc ions are replaced with Li + or Mg 2+ and Ti 4 + ,
Substituting metal ions selected from Zr 4+ , Hf 4+ , Nb 5+ and Ta 5+ or in combination with two or more metal ions to maintain a neutralized charge within the crystal. Garnet crystal for wavelength tunable lasers is characterized by:

本発明において言う、Cr3+を活性イオンとする
波長可変レーザー用媒質とは、フオノンを介在し
たレーザー発光過程が可能になり、広いスペクト
ル領域での蛍光が可能になるような電子構造が
Cr3+イオンに内部において実現されるために必要
となる結晶場を備えた固体媒質を言う。
Gd3Sc2Ga3O12はこのような固体媒質であり、結
晶構造はガーネツト型であることは知られてい
る。
In the present invention, a wavelength tunable laser medium containing Cr 3+ as an active ion is one that has an electronic structure that enables a phonon-mediated laser emission process and enables fluorescence in a wide spectral range.
A solid medium with the necessary crystal field for Cr 3+ ions to be realized inside.
Gd 3 Sc 2 Ga 3 O 12 is such a solid medium, and it is known that its crystal structure is garnet type.

本発明における置換後の組成は、 Gd3Sc2-xAxGa3O12(ただし、x<2である)で
示される。
The composition after substitution in the present invention is represented by Gd 3 Sc 2-x A x Ga 3 O 12 (x<2).

Aは1/2(B4++Mg2+)(ただし、BはZr4+
Ti4+またはHf4+を表わす)、これは1モルのSc+3
を1/2モルのB4+と1/2モルのMg2+で置換し、モ
ル数のバランスが置換前後で保たれることを示
す。また、1/2(C5++Li)(ただし、CはNb5+
たはTa5+を表わす)、1/3(B4++B′4++Li+)、ま
たは1/3(C′5++2Mg2+)、ただし、B′はBと同じ
陽イオン、C′はCと同じ5価陽イオンを表わす)
で表わすことができる。すなわち、価数を過不足
なく補うことが必要である。
A is 1/2 (B 4+ + Mg 2+ ) (B is Zr 4+ ,
Ti 4+ or Hf 4+ ), which represents 1 mole of Sc +3
is replaced with 1/2 mole of B 4+ and 1/2 mole of Mg 2+ to show that the balance of moles is maintained before and after the substitution. Also, 1/2 (C 5+ + Li) (where C represents Nb 5+ or Ta 5+ ), 1/3 (B 4+ + B' 4+ + Li + ), or 1/3 (C' 5 + +2Mg 2+ ), where B' represents the same cation as B, and C' represents the same pentavalent cation as C)
It can be expressed as In other words, it is necessary to compensate for the valence in just the right amount.

このような組成を有する単結晶を育成する方法
は、均質な結晶を育成する方法であればその方法
を問わない。好ましくは融液からの育成技術、例
えば引上げ法、フローテイングゾーン法である。
特に引上げ法は大型結晶の育成に好都合である
が、この方法の適用に際しては、置換組成のガー
ネツト結晶が一致溶融(結晶と融液とが同じ組成
になる)することが望ましい。
Any method can be used to grow a single crystal having such a composition as long as it grows a homogeneous crystal. Preferred is a growth technique from a melt, such as a pulling method or a floating zone method.
In particular, the pulling method is convenient for growing large crystals, but when applying this method, it is desirable that the garnet crystals with the substituted composition melt simultaneously (the crystal and the melt have the same composition).

本発明における結晶組成を利用して単結晶を育
成するにあたり、必要に応じてCa、Sr、Ba、
Na、K、Al、Fe、V、Mn、Co、Ni、Cu、Zn、
SiまたはGeの微量成分を配合することによつて、
単結晶の特性を向上させることができる。
When growing a single crystal using the crystal composition of the present invention, Ca, Sr, Ba,
Na, K, Al, Fe, V, Mn, Co, Ni, Cu, Zn,
By incorporating trace components of Si or Ge,
Characteristics of single crystals can be improved.

発明の効果 本発明のガーネツト結晶は従来波長可変レーザ
ー結晶として利用が進められている
Gd3Sc2Ga3O12結晶と比べて、格段に安価で、且
つ性能的に劣らぬ結晶であり、その結晶の用途で
あるCr3の波長可変レーザーの媒質結晶としての
機能を代替し得られる優れた効果を有する。
Effects of the invention The garnet crystal of the present invention has been used as a wavelength tunable laser crystal.
Compared to Gd 3 Sc 2 Ga 3 O 12 crystal, it is much cheaper and has comparable performance, and can replace the function as a medium crystal for Cr 3 wavelength tunable laser, which is the crystal's intended use. It has excellent effects.

実施例 実施例 1 Gd3Sc2-xZr1/2xMg1/2xGa3O12において、x値が
最大1.90までの組成の試料を用いて、集光式フロ
ーテイングゾーン法により、不純物相の混入のな
い無色透明の単結晶を得た。結晶構造はX線によ
りガーネツト型であることが確認された。
Examples Example 1 In Gd 3 Sc 2-x Zr 1/2x Mg 1/2x Ga 3 O 12 , using a sample with a composition with an A colorless and transparent single crystal without contamination was obtained. The crystal structure was confirmed to be garnet type by X-rays.

この組成の試料に0.1原子%のCr3+を導入し、
集光式フローテイングゾーン法により淡緑色透明
の単結晶を得た。得られた結晶に水銀ランプの光
を照射したところ、波長700〜900nmの範囲にわ
たる強い蛍光が見られた。これにより
Gd3Sc2Ga3O12と同様に、波長可変レーザー用結
晶として利用されることが明らかとなつた。
Introducing 0.1 at% Cr 3+ into a sample with this composition,
A pale green transparent single crystal was obtained using the condensing floating zone method. When the resulting crystals were irradiated with light from a mercury lamp, strong fluorescence over a wavelength range of 700 to 900 nm was observed. This results in
It has become clear that, like Gd 3 Sc 2 Ga 3 O 12 , it can be used as a crystal for wavelength tunable lasers.

実施例 2 Gd3Sc2-xTi1/2xMg1/2xGa3O12において、x値が
最大1.90までの組成について、以下実施例1と同
様に単結晶を作り、これらの組成の試料に0.1原
子%のCr3+を導入し、単結晶を作つた。その結
果、実施例1と同様に強い蛍光が見られた。
Example 2 For Gd 3 Sc 2-x Ti 1/2x Mg 1/2x Ga 3 O 12 , single crystals were produced in the same manner as in Example 1 for compositions with x values up to 1.90, and samples with these compositions were prepared. By introducing 0.1 atomic percent Cr 3+ into the material, a single crystal was created. As a result, similar to Example 1, strong fluorescence was observed.

実施例 3 Gd3Sc2-xHf1/2xMg1/2xGa3O12において、x値が
最大1.85までの組成について、以下実施例1と同
様に単結晶を作り、これらの組成の試料に0.1原
子%のCr3+を導入し、単結晶を作つた。その結
果、実施例1と同様に強い蛍光が見られた。
Example 3 For Gd 3 Sc 2-x Hf 1/2x Mg 1/2x Ga 3 O 12 , single crystals were produced in the same manner as in Example 1 for compositions with x values up to 1.85, and samples with these compositions were prepared. By introducing 0.1 atomic percent Cr 3+ into the material, a single crystal was created. As a result, similar to Example 1, strong fluorescence was observed.

実施例 4 Gd3Sc2-xNb1/2xLi1/2xGa3O12において、x値が
最大1.70までの組成について、以下実施例1と同
様に単結晶を作り、これらの組成の試料に0.1原
子%のCr3+を導入し、単結晶を作つた。その結
果、実施例1と同様に強い蛍光が見られた。
Example 4 For Gd 3 Sc 2-x Nb 1/2x Li 1/2x Ga 3 O 12 , single crystals were made in the same manner as in Example 1 for compositions with x values up to 1.70, and samples with these compositions were prepared. By introducing 0.1 atomic percent Cr 3+ into the material, a single crystal was created. As a result, similar to Example 1, strong fluorescence was observed.

実施例 5 Gd3Sc2-xTa1/2xLi1/2xGa3O12において、x値が
最大1.70までの組成について、以下実施例1と同
様に単結晶を作り、これらの組成の試料に0.1原
子%のCr3+を導入し、単結晶を作つた。その結
果、実施例1と同様に強い蛍光が見られた。
Example 5 In Gd 3 Sc 2-x Ta 1/2x Li 1/2x Ga 3 O 12 , single crystals were made in the same manner as in Example 1 for compositions with x values up to 1.70, and samples with these compositions were prepared. By introducing 0.1 atomic percent Cr 3+ into the material, a single crystal was created. As a result, similar to Example 1, strong fluorescence was observed.

実施例 6 Gd3Sc2-xZr2/3xLi1/3xGa3O12において、x値が
最大1.60までの組成について、以下実施例1と同
様に単結晶を作り、これらの組成の試料に0.1原
子%のCr3+を導入し、単結晶を作つた。その結
果、実施例1と同様に強い蛍光が見られた。
Example 6 For Gd 3 Sc 2-x Zr 2/3x Li 1/3x Ga 3 O 12 , single crystals were made in the same manner as in Example 1 for compositions with x values up to 1.60, and samples with these compositions were prepared. By introducing 0.1 atomic percent Cr 3+ into the material, a single crystal was created. As a result, similar to Example 1, strong fluorescence was observed.

実施例 7 Gd3Sc2-xTi2/3xLi1/3xGa3O12において、x値が
最大1.65までの組成について、以下実施例1と同
様に単結晶を作り、これらの組成の試料に0.1原
子%のCr3 +を導入し、単結晶を作つた。その結
果、実施例1と同様に強い蛍光が見られた。
Example 7 For Gd 3 Sc 2-x Ti 2/3x Li 1/3x Ga 3 O 12 , single crystals were made in the same manner as in Example 1 for compositions with x values up to 1.65, and samples with these compositions were prepared. By introducing 0.1 atomic percent Cr 3 + into the material, a single crystal was created. As a result, similar to Example 1, strong fluorescence was observed.

実施例 8 Gd3Sc2-xHf2/3xLi1/3xGa3O12において、x値が
最大1.55までの組成について、以下実施例1と同
様に単結晶を作り、これらの組成の試料に0.1原
子%のCr3+を導入し、単結晶を作つた。その結
果、実施例1と同様に強い蛍光が見られた。
Example 8 In Gd 3 Sc 2-x Hf 2/3x Li 1/3x Ga 3 O 12 , single crystals were produced in the same manner as in Example 1 for compositions with x values up to 1.55, and samples with these compositions were prepared. By introducing 0.1 atomic percent Cr 3+ into the material, a single crystal was created. As a result, similar to Example 1, strong fluorescence was observed.

実施例 9 Gd3Sc2-xNb1/3xMg2/3xGa3O12において、x値
が最大1.50までの組成について、以下実施例1と
同様に単結晶を作り、これらの組成の試料に0.1
原子%のCr3+を導入し、単結晶を作つた。その結
果、実施例1と同様に強い蛍光が見られた。
Example 9 For Gd 3 Sc 2-x Nb 1/3x Mg 2/3x Ga 3 O 12 , single crystals were produced in the same manner as in Example 1 for compositions with x values up to 1.50, and samples with these compositions were prepared. 0.1 to
A single crystal was created by introducing atomic percent Cr 3+ . As a result, similar to Example 1, strong fluorescence was observed.

実施例 10 Gd3Sc2-xTa1/3xMg2/3xGa3O12において、x値が
最大1.50までの組成について、以下実施例1と同
様に単結晶を作り、これらの組成の試料に0.1原
子%のCr3+を導入し、単結晶を作つた。その結
果、実施例1と同様に強い蛍光が見られた。
Example 10 In Gd 3 Sc 2-x Ta 1/3x Mg 2/3x Ga 3 O 12 , single crystals were made in the same manner as in Example 1 for compositions with x values up to 1.50, and samples with these compositions were prepared. By introducing 0.1 atomic percent Cr 3+ into the material, a single crystal was created. As a result, similar to Example 1, strong fluorescence was observed.

実施例 11 Gd3Sc2-xNb1/2xLi1/2xZr1/2yMg1/2yGa3O12におい
て、x+y値が最大1.50まで組成について、以下
実施例1と同様に単結晶を作り、これらの組成の
試料に0.1原子%のCr3+を導入し、単結晶を作つ
た。その結晶、実施例1と同様に強い蛍光が見ら
れた。
Example 11 In Gd 3 Sc 2-x Nb 1/2x Li 1/2x Zr 1/2y Mg 1/2y Ga 3 O 12 , single crystals were prepared in the same manner as in Example 1 for the composition up to the x+y value of 1.50. 0.1 atomic percent of Cr 3+ was introduced into samples with these compositions to produce single crystals. As in Example 1, strong fluorescence was observed in the crystal.

実施例 12 Gd3Sc2-x-yTa1/3xTi1/2yMg2/3x+1/2yGa3O12にお
いて、x+y値が最大1.50までの組成について、
以下実施例1と同様に単結晶を作り、これらの組
成の試料に0.1原子%のCr3+を導入し、単結晶を
作つた。その結果、実施例1と同様に強い蛍光が
見られた。
Example 12 Regarding the composition of Gd 3 Sc 2-xy Ta 1/3x Ti 1/2y Mg 2/3x+1/2y Ga 3 O 12 with x+y value up to 1.50,
Thereafter, single crystals were produced in the same manner as in Example 1, and 0.1 atomic % of Cr 3+ was introduced into samples having these compositions to produce single crystals. As a result, similar to Example 1, strong fluorescence was observed.

Claims (1)

【特許請求の範囲】[Claims] 1 Cr3+を活性イオンとする波長可変レーザー用
媒質結晶として用いるGd3Sc2Ga3O12の結晶にお
いて、Scイオンの1部を、Li+またはMg2+
Ti4+、Zr4+、Hf4+、Nb5+及びTa5+から選ばれた
単独または2種以上の金属イオンとの組合せによ
り、結晶内の電価が中和に保たれるように置換し
たことを特徴とする波長可変レーザー用ガーネツ
ト結晶。
1. In a Gd 3 Sc 2 Ga 3 O 12 crystal used as a medium crystal for a wavelength tunable laser with Cr 3+ as the active ion, part of the Sc ions are replaced with Li + or Mg 2+ .
The electric charge within the crystal is maintained at a neutral level by using it alone or in combination with two or more metal ions selected from Ti 4+ , Zr 4+ , Hf 4+ , Nb 5+ and Ta 5+ . A garnet crystal for wavelength tunable lasers characterized by substitution.
JP19832484A 1984-09-21 1984-09-21 Garnet crystal for wavelength tunable laser 1 Granted JPS6177380A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP19832484A JPS6177380A (en) 1984-09-21 1984-09-21 Garnet crystal for wavelength tunable laser 1

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP19832484A JPS6177380A (en) 1984-09-21 1984-09-21 Garnet crystal for wavelength tunable laser 1

Publications (2)

Publication Number Publication Date
JPS6177380A JPS6177380A (en) 1986-04-19
JPS6367347B2 true JPS6367347B2 (en) 1988-12-26

Family

ID=16389212

Family Applications (1)

Application Number Title Priority Date Filing Date
JP19832484A Granted JPS6177380A (en) 1984-09-21 1984-09-21 Garnet crystal for wavelength tunable laser 1

Country Status (1)

Country Link
JP (1) JPS6177380A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63501854A (en) * 1985-12-24 1988-07-28 トレスト“ユジボドプロボド” Batch type filtration equipment for fluids
IL82361A (en) * 1986-04-30 1990-11-05 American Telephone & Telegraph Device comprising congruently melting complex oxides

Also Published As

Publication number Publication date
JPS6177380A (en) 1986-04-19

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