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JPS6234701B2 - - Google Patents
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JPS6234701B2 - - Google Patents

Info

Publication number
JPS6234701B2
JPS6234701B2 JP57099126A JP9912682A JPS6234701B2 JP S6234701 B2 JPS6234701 B2 JP S6234701B2 JP 57099126 A JP57099126 A JP 57099126A JP 9912682 A JP9912682 A JP 9912682A JP S6234701 B2 JPS6234701 B2 JP S6234701B2
Authority
JP
Japan
Prior art keywords
glass
core
sio
weight
geo
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
JP57099126A
Other languages
Japanese (ja)
Other versions
JPS58217450A (en
Inventor
Nobuo Inagaki
Minoru Watanabe
Gotaro Tanaka
Kunio Fujiwara
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
NTT Inc
Original Assignee
Nippon Telegraph and Telephone Corp
Sumitomo Electric Industries 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 Nippon Telegraph and Telephone Corp, Sumitomo Electric Industries Ltd filed Critical Nippon Telegraph and Telephone Corp
Priority to JP57099126A priority Critical patent/JPS58217450A/en
Publication of JPS58217450A publication Critical patent/JPS58217450A/en
Publication of JPS6234701B2 publication Critical patent/JPS6234701B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/02Optical fibres with cladding with or without a coating
    • G02B6/028Optical fibres with cladding with or without a coating with core or cladding having graded refractive index
    • CCHEMISTRY; METALLURGY
    • C03GLASS; MINERAL OR SLAG WOOL
    • C03CCHEMICAL COMPOSITION OF GLASSES, GLAZES OR VITREOUS ENAMELS; SURFACE TREATMENT OF GLASS; SURFACE TREATMENT OF FIBRES OR FILAMENTS MADE FROM GLASS, MINERALS OR SLAGS; JOINING GLASS TO GLASS OR OTHER MATERIALS
    • C03C13/00Fibre or filament compositions
    • C03C13/04Fibre optics, e.g. core and clad fibre compositions
    • C03C13/045Silica-containing oxide glass compositions
    • C03C13/046Multicomponent glass compositions
    • CCHEMISTRY; METALLURGY
    • C03GLASS; MINERAL OR SLAG WOOL
    • C03CCHEMICAL COMPOSITION OF GLASSES, GLAZES OR VITREOUS ENAMELS; SURFACE TREATMENT OF GLASS; SURFACE TREATMENT OF FIBRES OR FILAMENTS MADE FROM GLASS, MINERALS OR SLAGS; JOINING GLASS TO GLASS OR OTHER MATERIALS
    • C03C3/00Glass compositions
    • C03C3/04Glass compositions containing silica
    • C03C3/076Glass compositions containing silica with 40% to 90% silica, by weight
    • C03C3/11Glass compositions containing silica with 40% to 90% silica, by weight containing halogen or nitrogen
    • C03C3/112Glass compositions containing silica with 40% to 90% silica, by weight containing halogen or nitrogen containing fluorine

Landscapes

  • Chemical & Material Sciences (AREA)
  • Physics & Mathematics (AREA)
  • Materials Engineering (AREA)
  • Chemical Kinetics & Catalysis (AREA)
  • General Chemical & Material Sciences (AREA)
  • Geochemistry & Mineralogy (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Organic Chemistry (AREA)
  • Engineering & Computer Science (AREA)
  • Optics & Photonics (AREA)
  • General Physics & Mathematics (AREA)
  • Optical Fibers, Optical Fiber Cores, And Optical Fiber Bundles (AREA)
  • Glass Compositions (AREA)

Description

【発明の詳細な説明】 本発明は素材ガラスに特徴のある光伝送用ガラ
スフアイバおよびその製造方法に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a glass fiber for optical transmission characterized by a glass material and a method for manufacturing the same.

この種の素材ガラスとしては、従来、硅酸を主
成分とするガラスが多く用いられている。特に
SiO2にGeO2を添加したガラスは、可視〜近赤外
領域の波長の光を殆んど吸収することがなく、好
適である。またSiCl4、GeCl4など常温付近で蒸気
圧の高い原料が入手できるため、ガラス原料を気
相反応させることにより合成した微粒子状ガラス
の堆積体を焼結して透明ガラス体とする気相合成
法によれば、合成過程で汚染機会が少なく、純度
の極めて高いガラスを容易に得ることができ光伝
送損失上、好都合である。そしてSiO2は機械的
強度、耐候性などに秀れるため、一般にSiO2
クラツドとし、上記GeO2を添加したSiO2ガラス
をコアとしたフアイバが多く用いられているが、
現実には多くの問題がある。
As this type of raw glass, glass containing silicic acid as a main component has conventionally been widely used. especially
Glass in which GeO 2 is added to SiO 2 is suitable because it hardly absorbs light with wavelengths in the visible to near-infrared region. In addition, since raw materials with high vapor pressure near room temperature such as SiCl 4 and GeCl 4 are available, vapor phase synthesis is used to produce a transparent glass body by sintering a deposit of fine glass particles synthesized by vapor phase reaction of glass raw materials. According to this method, there is little chance of contamination during the synthesis process, and glass of extremely high purity can be easily obtained, which is advantageous in terms of optical transmission loss. Since SiO 2 has excellent mechanical strength and weather resistance, fibers with a cladding of SiO 2 and a core of SiO 2 glass doped with GeO 2 are often used.
In reality, there are many problems.

問題の1つは気相合成法(例えば特公昭56−
31291号、同56−33327号公報に示されるような
H2/O2火炎内反応を利用した気相軸付法)で
GeO2濃度を上げたSiO2−GeO2ガラスを合成する
場合、まず微粒子状ガラス堆積体(スート体と称
す)を合成し、これを焼結して透明ガラス体を得
るが、このスート体を合成する過程でGeO2の微
結晶の形成機会が多くなり、微粒子状ガラス(ス
ートと称す)の中に上記GeO2微結晶を含有する
ものが得られる。このGeO2微結晶は、通常、焼
結過程でも保存されており、コア材と石英管を組
合せてフアイバ化する際に約2000℃程度の高温下
にさらされるため、この微結晶の蒸気圧が高くな
り、低粘性体となるガラス中で発泡することが多
くなる。通常GeO2ドープSiO2ガラスの屈折率が
1%以上となると(このときGeO2濃度としては
約15重量%である)、この傾向は顕著になる。ま
たこの傾向はGeO2濃度以外の他の要因として、
スート体堆積時に堆積体表面温度の低くなつてい
る箇所(スート体の外周部分)で顕著である。こ
のため、コアとクラツドとの屈折率差が高く、か
つコアの屈折率分布がステツプ型に近い良好な光
フアイバは特に得ることが難かしい。また屈折率
差が1%程度で屈折率分布が2乗曲線のいわゆる
グレーデイツド型光フアイバの場合にも上記
GeO2の微結晶が形成される場合があり、これに
よりフアイバ中に不要な微小空間が形成された
り、フアイバの線径変動が生じる場合がある。
One of the problems is that gas-phase synthesis methods (e.g.
As shown in No. 31291 and No. 56-33327
(vapor phase axis method using H 2 / O 2 flame reaction)
When synthesizing SiO 2 −GeO 2 glass with an increased GeO 2 concentration, first a particulate glass deposit (referred to as a soot body) is synthesized, and this is sintered to obtain a transparent glass body. During the synthesis process, there are many opportunities for the formation of GeO 2 microcrystals, and a glass particulate (referred to as soot) containing the GeO 2 microcrystals is obtained. These GeO 2 microcrystals are usually preserved during the sintering process, and when the core material and quartz tube are combined to form a fiber, they are exposed to high temperatures of approximately 2000°C, so the vapor pressure of these microcrystals increases. foaming occurs in the glass, which becomes a low-viscosity substance. Usually, this tendency becomes noticeable when the refractive index of GeO 2 -doped SiO 2 glass becomes 1% or more (at this time, the GeO 2 concentration is about 15% by weight). This trend is also due to other factors other than GeO 2 concentration.
This is noticeable in areas where the surface temperature of the soot body is low during soot body deposition (the outer periphery of the soot body). For this reason, it is particularly difficult to obtain a good optical fiber in which the difference in refractive index between the core and the cladding is high and the refractive index distribution of the core is close to that of a step type. The above also applies to so-called graded optical fibers, where the refractive index difference is about 1% and the refractive index distribution is a square curve.
Microcrystals of GeO 2 may be formed, which may create unnecessary microscopic spaces in the fiber or cause fiber diameter variations.

SiO2とGeO2系ガラスの他の問題としては、
GeO2濃度が増すと、上記の結晶化と更にGeO2
度ゆらぎなどが増大し、光フアイバのコアをこれ
で構成すると、レイレイ散乱と称する光散乱損失
が増し、光伝送特性が劣化するという問題もあ
る。
Other problems with SiO 2 and GeO 2 glasses include:
As the GeO 2 concentration increases, the above-mentioned crystallization and GeO 2 concentration fluctuations increase, and if the core of an optical fiber is made of this, light scattering loss called Ray-Ray scattering increases and optical transmission characteristics deteriorate. There is also.

SiO2−GeO2系ガラスをコアとし、SiO2ガラス
をクラツドとする光フアイバの更に他の問題点の
1つとして、GeO2をドープしたSiO2ガラスは、
SiO2濃度が高くなる程、クラツドのSiO2ガラス
との粘性差が大きくなり、このために線引時コア
形状の変動が発生するという問題がある。例えば
GeO2濃度の平均値として約20重量%(径方向の
濃度分布が2乗の場合は、中心のピーク値濃度は
40%となつている)のSiO2コアガラスは、SiO2
チユーブと組合せて線引する過程において、加熱
部ではコアがクラツド層から引きしぼられるよう
な外からの力を受け、設定のコア径−クラツド径
比が得難い。コアが真円形状からずれたいびつな
形状となる場合も多い。そこでコア−クラツドの
屈折率差の平均値が1.5%(分布形状が2乗曲線
の場合には中心のピーク値は3.0%である)以上
を有する良好な光フアイバを得ることは難かしい
などの問題点があつた。
Another problem with optical fibers with SiO 2 -GeO 2 glass as the core and SiO 2 glass as the cladding is that SiO 2 glass doped with GeO 2
As the SiO 2 concentration increases, the difference in viscosity between the cladding and the SiO 2 glass increases, which causes a problem in that the core shape changes during drawing. for example
The average GeO 2 concentration is approximately 20% by weight (if the radial concentration distribution is squared, the central peak concentration is
SiO 2 core glass (40%) is SiO 2
In the process of drawing in combination with a tube, the heating section receives an external force that causes the core to be squeezed away from the cladding layer, making it difficult to obtain a predetermined core diameter-to-cladding diameter ratio. In many cases, the core is distorted and deviates from a perfect circle. Therefore, it is difficult to obtain a good optical fiber with an average core-clad refractive index difference of 1.5% or more (if the distribution shape is a square curve, the central peak value is 3.0%). There was a problem.

本発明は上記の問題点に鑑み為されたもので、
その目的は光フアイバ断面部で泡を持たず、コア
径が真円で、かつ寸法精度および耐候性、機械的
強度に秀れ、かつ伝送特性の秀れた光フアイバ用
ガラスを提供することにある。
The present invention has been made in view of the above problems.
The purpose is to provide glass for optical fibers that has no bubbles in the cross section of the optical fiber, has a perfectly circular core diameter, has excellent dimensional accuracy, weather resistance, mechanical strength, and has excellent transmission characteristics. be.

本発明の別の目的は、特にコア−クラツドの屈
折率差の大きな、いわゆる高NAフアイバで特性
の秀れた良好なフアイバを容易に構成しうるガラ
スを提供することである。
Another object of the present invention is to provide a glass that can be easily formed into a so-called high-NA fiber with excellent characteristics, especially a fiber having a large core-cladding refractive index difference.

本発明はコアとクラツドからなる光フアイバに
おいて、平均組成(重量%)として、 65≦SiO2≦85 5≦GeO2≦20 5≦Al2O3≦15 0≦F≦3 からなるコアと、 SiO2またはF含有のSiO2からなるクラツドを
有することを特徴とする光フアイバに関するもの
である。
The present invention provides an optical fiber consisting of a core and a cladding, in which the average composition (weight %) is 65≦SiO 2 ≦85 5≦GeO 2 ≦20 5≦Al 2 O 3 ≦15 0≦F≦3; The present invention relates to an optical fiber characterized by having a cladding made of SiO 2 or F-containing SiO 2 .

上記のコアガラス組成において、GeO2含有量
が20%より大きく、かつAl2O3含有量が5%より
小さいとガラスの結晶化が生じ易くなり、光フア
イバの断面に泡をもち、また線引時にコア径の寸
法精度が悪く真円となり難い。
In the above core glass composition, if the GeO 2 content is greater than 20% and the Al 2 O 3 content is less than 5%, the glass tends to crystallize, resulting in bubbles on the cross section of the optical fiber and wires. When pulled, the dimensional accuracy of the core diameter is poor and it is difficult to form a perfect circle.

Al2O3が15%より大きいとガラス中にAl2O3
十分な固溶が起らず、通常の焼結により透明ガラ
スが得られない。
If Al 2 O 3 is greater than 15%, sufficient solid solution of Al 2 O 3 will not occur in the glass, and transparent glass will not be obtained by normal sintering.

GeO2含有量が5%より小さいとコアとクラツ
ドの屈折率差が十分にとれず、安定した光フアイ
バを構成できない。
If the GeO 2 content is less than 5%, a sufficient difference in refractive index between the core and the cladding cannot be obtained, and a stable optical fiber cannot be constructed.

Fの含有量がなくとも上記の長所を有する光フ
アイバを構成できるが、Fを含有させると光伝送
特性上、良好な光フアイバを得ることができる。
特に、本発明で集束型(GRINと称する)光フア
イバをつくる場合、コア領域の外周部における屈
折率値をクラツドの屈折率値と一致させるように
フツ素を含有させることで、帯域特性の良好な光
フアイバを得ることができ、この場合、コアまた
はクラツドに弗素を含有させることができる。
Although it is possible to construct an optical fiber having the above-mentioned advantages without the content of F, an optical fiber with good optical transmission characteristics can be obtained by containing F.
In particular, when producing a focusing type (referred to as GRIN) optical fiber according to the present invention, good band characteristics can be achieved by incorporating fluorine so that the refractive index value at the outer periphery of the core region matches the refractive index value of the cladding. Optical fibers can be obtained in which the core or cladding can contain fluorine.

本発明の場合、弗素を上記の如く含有させるこ
とで帯域特性の良好な光フアイバを得ることがで
き、更に長波長帯での伝送損失も低下させること
ができる。ただしコアでの含有量としては、3%
より多くなると、本ガラス組成の場合、屈折率値
及びガラスの硬さに悪影響を及ぼし好ましくな
い。クラツドの外層部としては、弗素を含有させ
ないSiO2ガラスが機械的強度、耐候性などの面
で好都合である。
In the case of the present invention, by containing fluorine as described above, an optical fiber with good band characteristics can be obtained, and transmission loss in a long wavelength band can also be reduced. However, the content in the core is 3%
If the amount is larger than this, in the case of the present glass composition, it is not preferable because it adversely affects the refractive index value and the hardness of the glass. For the outer layer of the cladding, SiO 2 glass that does not contain fluorine is advantageous in terms of mechanical strength, weather resistance, etc.

第1図イ及びロに本発明における集束型光フア
イバの屈折率分布およびドーパント濃度(重量
%)分布の例を示す。
FIGS. 1A and 1B show examples of the refractive index distribution and dopant concentration (wt%) distribution of the focusing optical fiber according to the present invention.

第1図イはFを含有させたSiO2をクラツド領
域のコア周辺部に配し、その外側をSiO2とした
フアイバ構造のものに関する。このフアイバは上
記のように帯域特性、伝送損失特性とも極めて良
好であり、かつ機械的強度、耐候性などの点でも
秀れたフアイバとなる。クラツド領域での弗素含
有濃度としては、本発明の場合、コアガラス・最
外層SiO2クラツドガラスとの物性面におけるマ
ツチング上、3重量%以下が望ましい。第1図ロ
はクラツドがSiO2であり、コアがSiO2−GeO2
Al2O3−Fからなるガラスより構成したフアイバ
構造のものに関する。
FIG. 1A relates to a fiber structure in which F-containing SiO 2 is arranged around the core of the cladding region, and the outside thereof is made of SiO 2 . As mentioned above, this fiber has extremely good band characteristics and transmission loss characteristics, and is also excellent in terms of mechanical strength, weather resistance, etc. In the case of the present invention, the fluorine content concentration in the cladding region is desirably 3% by weight or less in view of physical property matching between the core glass and the outermost SiO 2 cladding glass. In Figure 1B, the cladding is SiO 2 and the core is SiO 2 −GeO 2
The present invention relates to a fiber structure made of glass made of Al 2 O 3 -F.

上記の説明において、Al2O3の代りにその一部
をGa2O3に置換えて用いても本発明の効果は基本
的に発揮できる。これは、ガラスの物性特性に与
える影響がAlとGaとでは類似しており、置換可
能のためである。Al2O3に対してGa2O3含有量を
増すと屈折率差は大きくとれるが、結晶化し易く
なる。Ga2O3濃度条件としては10重量%以下の範
囲が好ましい。
In the above description, the effects of the present invention can basically be achieved even if a part of Al 2 O 3 is replaced with Ga 2 O 3 . This is because Al and Ga have similar effects on the physical properties of glass and can be substituted. If the content of Ga 2 O 3 is increased relative to Al 2 O 3 , the difference in refractive index can be increased, but crystallization becomes easier. The Ga 2 O 3 concentration condition is preferably in a range of 10% by weight or less.

本発明の酸化物成分はいずれも気相反応と生じ
させて生成物を得るために必要な高純度原料を容
易に入手することができ、これにより遷移金属不
純物などを含まない、超高純度で可視から近赤外
領域まで光吸収の極めて少ないガラスを得ること
ができる。
All of the oxide components of the present invention can be produced in a gas phase reaction to obtain the high purity raw materials necessary to obtain the products. It is possible to obtain glass with extremely low light absorption in the visible to near-infrared region.

実施例 1 SiCl4、GeCl4、Al(CH33、SiF4をガラス合成
用原料とし、これらの原料を気相状で火炎内に導
入して、微粒子状ガラスの堆積体を合成し、これ
を焼結すること、すなわち気相軸付法を用いるこ
とにより円柱状ガラス母材の平均組成として、
SiO2=84% GeO2=7.5% Al2O3=6.8% F=
1.7%を有する(但し、GeO2については、母材径
方向の濃度分布が2乗の曲線をもつている。)コ
ア用ガラスを合成した。これを外径10mmの棒状ガ
ラスに引伸した。一方、外径が25.5mm、内径が11
mmの石英管を準備し、石英管の中にコアガラス棒
を挿入しヒータ温度が約2000℃の炉体により線引
し、外径125μmのフアイバを作つたこのフアイ
バの外径変動は125μm±0.5μmにおさまつてお
り、局部的な線径変動が全長約20Kmにわたつてみ
られなかつた。またフアイバ断面のコア形状が真
円であつた。また光伝送損失の波長特性として
1.50〜1.65μmの波長において0.5dB/Km以下の
特性を有し、また6dB低下帯域特性としては1.3
μm波長帯にて500MHz・Km以上を有するものが
得られた。
Example 1 Using SiCl 4 , GeCl 4 , Al(CH 3 ) 3 , and SiF 4 as raw materials for glass synthesis, these raw materials were introduced into a flame in a vapor phase to synthesize a deposit of fine glass particles, By sintering this, that is, using the vapor phase axial method, the average composition of the cylindrical glass base material is
SiO 2 = 84% GeO 2 = 7.5% Al 2 O 3 = 6.8% F =
1.7% (however, for GeO 2 , the concentration distribution in the radial direction of the base material has a square curve) was synthesized. This was enlarged into a glass rod with an outer diameter of 10 mm. On the other hand, the outer diameter is 25.5mm and the inner diameter is 11mm.
A core glass rod was inserted into the quartz tube and drawn in a furnace with a heater temperature of approximately 2000°C to produce a fiber with an outer diameter of 125 μm. The outer diameter variation of this fiber was 125 μm ± The wire diameter remained at 0.5 μm, and no local variations in wire diameter were observed over the entire length of approximately 20 km. Moreover, the core shape of the fiber cross section was a perfect circle. Also, as a wavelength characteristic of optical transmission loss,
It has a characteristic of 0.5dB/Km or less at wavelengths of 1.50 to 1.65μm, and a 6dB reduction band characteristic of 1.3
A product with a wavelength of 500MHz/Km or more in the μm wavelength band was obtained.

実施例 2 実施例1と同様な気相軸付法を用いて、円柱状
ガラス母材の平均組成としてSiO2=66%、GeO2
=20%(但し断面のGeO2濃度分布としてはほぼ
4乗曲線に近い形状とした)Al2O3=14%を有す
るコア用ガラスを合成した。これを外径10mmの棒
状ガラスに引伸した一方外径が15mm内径が11.5mm
の石英管を準備し、実施例1と同様な斗法により
外径140μmのフアイバを作つた。コアとクラツ
ドとの屈折率差はフアイバ断面中央部で約3.0%
あるものが得られた。このフアイバの外径変動は
140μmに対し±3μm以上の局部的な線径変動
箇所が全長5Kmにわたり2ケであつた。またコア
は真円であつた。
Example 2 Using the same vapor phase axial method as in Example 1, the average composition of the cylindrical glass base material was SiO 2 = 66%, GeO 2
A core glass having Al 2 O 3 = 20% (however, the GeO 2 concentration distribution in the cross section was shaped almost like a fourth power curve) was synthesized. This was enlarged into a rod-shaped glass with an outer diameter of 10 mm, and the outer diameter was 15 mm and the inner diameter was 11.5 mm.
A quartz tube was prepared, and a fiber with an outer diameter of 140 μm was made using the same method as in Example 1. The refractive index difference between the core and cladding is approximately 3.0% at the center of the fiber cross section.
I got something. The outer diameter variation of this fiber is
There were two locations over a total length of 5 km where the wire diameter varied by ±3 μm or more compared to 140 μm. Moreover, the core was perfectly round.

比較例 1 実施例2と同様な手法により、コアの平均組成
としてSiO2=70%、GeO2=30%(但し、断面の
屈折率分布としては実施例2とほぼ同一の分布を
もつ形状をした)を有する外径140μmのフアイ
バを作つた。このフアイバの外径変動としては、
±3μm以上の局所的な線径変動箇所が全長5Km
にわたり15ケあつた。この線径変動箇所のフアイ
バ断面を顕微鏡で観察するとコアとクラツドの界
面に外径10μm程度の空間の存在が観察された。
またコアの形状に関しては長軸対短軸が1:0.8
の楕円形状であつた。
Comparative Example 1 Using the same method as in Example 2, the average composition of the core was SiO 2 = 70%, GeO 2 = 30% (however, the refractive index distribution in the cross section was shaped to have almost the same distribution as in Example 2). A fiber with an outer diameter of 140 μm was fabricated. As for the variation in the outer diameter of this fiber,
Local wire diameter fluctuations of ±3μm or more are 5Km in total length.
There were 15 cases total. When the cross section of the fiber at the point where the wire diameter fluctuated was observed under a microscope, a space with an outer diameter of approximately 10 μm was observed at the interface between the core and the cladding.
Also, regarding the shape of the core, the long axis to short axis is 1:0.8
It had an elliptical shape.

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

第1図は本発明における集束型光フアイバの屈
折率分布およびドーパント濃度分布の例を示すグ
ラフであり、第1図イはクラツドの一部にFを含
有させた層を有するフアイバ、ロはSiO2をクラ
ツドとするフアイバである。
FIG. 1 is a graph showing an example of the refractive index distribution and dopant concentration distribution of a focusing optical fiber according to the present invention. FIG. It is a fiber with a cladding of 2 .

Claims (1)

【特許請求の範囲】 1 コアおよびクラツドからなる光フアイバ用ガ
ラスにおいて、そのコア領域の平均組成が、
SiO2に換算して65〜85重量%のシリカと、GeO2
に換算して5〜20重量%の酸化ゲルマニウムと、
Al2O3を5〜15重量%と、Fを0〜3重量%含む
ガラスであり、クラツドがSiO2またはF含有
SiO2ガラスであることを特徴とする光フアイバ
用ガラス。 2 ガラス原料を気相反応させることにより合成
した微粒子状ガラスの堆積体を焼結して透明ガラ
ス体とする気相合成法を用いてコアガラスを合成
することを特徴とする、コア領域の平均組成が、
SiO2に換算して65〜85重量%のシリカと、GeO2
に換算して5〜20重量%の酸化ゲルマニウムと、
Al2O3を5〜15重量%と、Fを0〜3重量%含む
ガラスであり、クラツドがSiO2またはF含有
SiO2ガラスである、コアおよびクラツドからな
る光フアイバ用ガラスの製造方法。
[Claims] 1. In an optical fiber glass consisting of a core and a cladding, the average composition of the core region is
65-85% by weight of silica calculated as SiO 2 and GeO 2
5 to 20% by weight of germanium oxide in terms of
It is a glass containing 5 to 15% by weight of Al 2 O 3 and 0 to 3% by weight of F, and the cladding contains SiO 2 or F.
Glass for optical fibers characterized by being SiO 2 glass. 2. The average of the core area, which is characterized in that the core glass is synthesized using a vapor phase synthesis method in which a deposited body of particulate glass synthesized by subjecting glass raw materials to a vapor phase reaction is sintered to form a transparent glass body. The composition is
65-85% by weight of silica calculated as SiO 2 and GeO 2
5 to 20% by weight of germanium oxide in terms of
It is a glass containing 5 to 15% by weight of Al 2 O 3 and 0 to 3% by weight of F, and the cladding contains SiO 2 or F.
A method for manufacturing optical fiber glass consisting of a core and a cladding, which is SiO 2 glass.
JP57099126A 1982-06-11 1982-06-11 Glass for optical fiber and its production Granted JPS58217450A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57099126A JPS58217450A (en) 1982-06-11 1982-06-11 Glass for optical fiber and its production

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57099126A JPS58217450A (en) 1982-06-11 1982-06-11 Glass for optical fiber and its production

Publications (2)

Publication Number Publication Date
JPS58217450A JPS58217450A (en) 1983-12-17
JPS6234701B2 true JPS6234701B2 (en) 1987-07-28

Family

ID=14239060

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57099126A Granted JPS58217450A (en) 1982-06-11 1982-06-11 Glass for optical fiber and its production

Country Status (1)

Country Link
JP (1) JPS58217450A (en)

Families Citing this family (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6051635A (en) * 1983-08-31 1985-03-23 Furukawa Electric Co Ltd:The Quartz optical fiber
US4669821A (en) * 1984-09-19 1987-06-02 Hughes Aircraft Company Radiation resistant optical fiber waveguide
WO2007114105A1 (en) * 2006-03-30 2007-10-11 The Furukawa Electric Co., Ltd. Optical fiber
JP5315601B2 (en) * 2006-09-12 2013-10-16 住友電気工業株式会社 Optical fiber and optical fiber type device
CN110346866B (en) * 2019-06-12 2020-08-25 烽火通信科技股份有限公司 Panda type polarization maintaining optical fiber

Also Published As

Publication number Publication date
JPS58217450A (en) 1983-12-17

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