JPS606298B2 - optical fiber - Google Patents
optical fiberInfo
- Publication number
- JPS606298B2 JPS606298B2 JP55090697A JP9069780A JPS606298B2 JP S606298 B2 JPS606298 B2 JP S606298B2 JP 55090697 A JP55090697 A JP 55090697A JP 9069780 A JP9069780 A JP 9069780A JP S606298 B2 JPS606298 B2 JP S606298B2
- Authority
- JP
- Japan
- Prior art keywords
- glass
- mol
- fiber
- optical
- optical fiber
- 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
Links
Classifications
-
- C—CHEMISTRY; METALLURGY
- C03—GLASS; MINERAL OR SLAG WOOL
- C03B—MANUFACTURE, SHAPING, OR SUPPLEMENTARY PROCESSES
- C03B37/00—Manufacture or treatment of flakes, fibres, or filaments from softened glass, minerals, or slags
- C03B37/01—Manufacture of glass fibres or filaments
- C03B37/02—Manufacture of glass fibres or filaments by drawing or extruding, e.g. direct drawing of molten glass from nozzles; Cooling fins therefor
- C03B37/025—Manufacture of glass fibres or filaments by drawing or extruding, e.g. direct drawing of molten glass from nozzles; Cooling fins therefor from reheated softened tubes, rods, fibres or filaments, e.g. drawing fibres from preforms
- C03B37/027—Fibres composed of different sorts of glass, e.g. glass optical fibres
-
- C—CHEMISTRY; METALLURGY
- C03—GLASS; MINERAL OR SLAG WOOL
- C03C—CHEMICAL 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
- C03C13/00—Fibre or filament compositions
- C03C13/04—Fibre optics, e.g. core and clad fibre compositions
- C03C13/041—Non-oxide glass compositions
- C03C13/043—Chalcogenide glass compositions
-
- C—CHEMISTRY; METALLURGY
- C03—GLASS; MINERAL OR SLAG WOOL
- C03B—MANUFACTURE, SHAPING, OR SUPPLEMENTARY PROCESSES
- C03B2201/00—Type of glass produced
- C03B2201/80—Non-oxide glasses or glass-type compositions
- C03B2201/86—Chalcogenide glasses, i.e. S, Se or Te glasses
Landscapes
- Chemical & Material Sciences (AREA)
- Engineering & Computer Science (AREA)
- Materials Engineering (AREA)
- Geochemistry & Mineralogy (AREA)
- Life Sciences & Earth Sciences (AREA)
- Organic Chemistry (AREA)
- Manufacturing & Machinery (AREA)
- General Life Sciences & Earth Sciences (AREA)
- Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Chemical Kinetics & Catalysis (AREA)
- General Chemical & Material Sciences (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LO.5〜10ぶれの広い波長城で透過性とを
有し、特に2〜7〆のにおいて光損失の値が小さい、透
過の窓を有する光フアイバに関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention provides LO. The present invention relates to an optical fiber having a transmission window that has a transmittance over a wide wavelength range of 5 to 10 wavelengths, and has a small optical loss value particularly in a range of 2 to 7 wavelengths.
従来の光フアィバはSi02を主成分としているため、
Si−○結合の振動に起因する赤外吸収が存在し、波長
領域0.6〜1.7仏肌にのみ限って光損失の低減化が
図られている。Since conventional optical fibers have Si02 as their main component,
There is infrared absorption due to the vibration of the Si-◯ bond, and optical loss is reduced only in the wavelength region of 0.6 to 1.7 degrees.
この波長領域を越える長波長城、例えば2〜7仏のにお
いて低損失となる光フアィバを得るには、赤外吸収端が
Si02よりも長波長側に位置している素材を用いて光
フアィバを製造する必要がある。この種の赤外透過素材
として、これまでにハロゲン化物を主成分とするガラス
、KRS−5、KCI、A多1等のハラィド結晶、As
2S3に代表されるカルコゲナイドガラス等が知られて
いるが、各素材にはいずれも以下に述べるような欠点が
あるため、波長領域2〜7ぶれにおいて光損失の値が小
さい光フアィバは実現し得なかった。その理由は、ハロ
ゲン化物を主成分とするガラスについては、その含有成
分である茂F2、ZnC!2自身の潮解性、毒性のため
汎用の光フアィバ用素材としては不適当であり、またB
eF2、ZnC12を除くとガラス状態が得にくいので
ガラスフアィバを作製することは困難であるからである
。In order to obtain an optical fiber with low loss at long wavelengths exceeding this wavelength range, for example 2 to 7 wavelengths, the optical fiber is manufactured using a material whose infrared absorption edge is located on the longer wavelength side than Si02. There is a need to. As this type of infrared transmitting material, so far we have used glass mainly composed of halides, halide crystals such as KRS-5, KCI, and A-1, As
Chalcogenide glasses such as 2S3 are known, but each material has the following drawbacks, so it is impossible to create an optical fiber with small optical loss values in the wavelength range 2 to 7 deviations. There wasn't. The reason for this is that for glasses whose main components are halides, the contained components Shigeru F2, ZnC! B2 itself is unsuitable as a material for general-purpose optical fibers due to its deliquescent nature and toxicity;
This is because if eF2 and ZnC12 are excluded, it is difficult to obtain a glass state, making it difficult to produce a glass fiber.
また、AgCI等を用いた結晶フアィバは、結晶粒界で
の光散乱が避けられないため、光損失の低減化が困難で
あるのに加えて「加工性の点で問題があり、長尺化がむ
ずかしい。更に、カルコゲナィドガラスに関しては、A
sぶ3ガラスを用いた光フアィバが実現されているにす
ぎないが「 この偽2S3ガラスを用いた光フアィバの
光損失の値は、波長5.5山肌で2×1ぴdB/紋と大
きく、しかも毒性の強いAsを含むため「作業上の安全
性の点からも問題がある。−方ト蛇−P−S系ガラス等
船を含有しないカルコゲナイドガラスも知られているが
、この種ガラスを用いた光フアィバを実現するための研
究はほとんどなされておらず、単に赤外線透過用ガラス
(厚さは肋から節オーダー)としての性質が一部調べら
れているにすぎない。In addition, crystal fibers using AgCI etc. cannot avoid light scattering at crystal grain boundaries, making it difficult to reduce optical loss. Furthermore, regarding chalcogenide glass, A
Although only an optical fiber using SBU3 glass has been realized, the optical loss value of this optical fiber using fake 2S3 glass is as large as 2 × 1 pi dB/fri at a wavelength of 5.5 peaks. Furthermore, since it contains highly toxic As, there is also a problem from the point of view of work safety. Chalcogenide glasses that do not contain glass, such as P-S glass, are also known, but this type of glass Very little research has been done to realize optical fibers using this material, and only some research has been done on its properties as an infrared transmitting glass (thickness is on the order of ribs to nodes).
本発明はこのような現状に鑑みてなされたものであり、
Q−P−S系ガラスを用いて光フアイバを得るに最適な
ガラス組成を明らかにし、毒性が低く「 しかも0.5
〜10山肌の広い波長城で透過性を有し、特に2〜7仏
のの波長頃的こおいて透過の窓を有するカルコゲナィド
ガラス光フアィバを提供することを目的とする。The present invention was made in view of the current situation, and
We clarified the optimal glass composition for obtaining optical fibers using Q-P-S glass, and found that it has low toxicity and 0.5
The object of the present invention is to provide a chalcogenide glass optical fiber that has transparency over a wide range of wavelengths ranging from 10 to 10 cm, and in particular has a window of transmission over 2 to 7 wavelengths.
以下に示す実施例に従い本発明の詳細を説明する。The details of the present invention will be explained according to the examples shown below.
実施例 1
まず、2成分系CeSx(x=2〜6)ガラスファィバ
を以下の手順に従って各種作製した。Example 1 First, various two-component CeSx (x=2 to 6) glass fibers were produced according to the following procedure.
純度99.999%の硫黄(S)および99.9999
9999%のゲルマニウム(W)を所定の割合で秤量し
「 肉厚3柳も内径3物協、長さi50肋の石英ガラス
管に総重量約50夕のQとSを真空封入した。次いでト
ガラス管内のS、蛇を灘拝しながら、温度800〜10
0000で20〜20斑時間にわたって加熱した後に冷
却することによりガラスブロックを得た。具体的には「
Q=33.3モル%、S=66。7モル%の蛇S2を用
いてガラスを得るには〜 loooqoで20畑寿間の
加熱を要した。99.999% pure sulfur (S) and 99.9999
9999% germanium (W) was weighed at a predetermined ratio, and Q and S having a total weight of about 50 mm were vacuum-sealed into a quartz glass tube with a wall thickness of 3 willows and an inner diameter of 3 mm, and a length of 50 mm. S in the jurisdiction, worshiping the snake, temperature 800-10
A glass block was obtained by heating at 0,000 for 20-20 hours and then cooling. in particular"
To obtain glass using Snake S2 with Q = 33.3 mol% and S = 66.7 mol%, heating was required for ~ 20 days at loooqo.
Q;14.3モル%〜 S:85.7モル%の蛇S6用
いた場合にはも800ooト20時間の加熱で十分ガラ
ス化した。また「 Sの含有量が66.7モル%と85
.7モル%の間〜すなわちxが2と6との間の領域のW
SXを用いてガラスを得るには、加熱温度および加熱時
間はともにト前述した値800〜1000qCおよび2
0〜20脚時間の範囲内であった。このように、ガラス
化に必要とされる加熱温度および加熱時間は、Sの含有
量に依存」硫黄Sが多いほども低い加熱温度〜短い加熱
時間により均一で透明なガラスが得られることが判明し
た。また「 S<66.?モル%すなわちx<2の領域
のQSxを用いた場合には、1000o○で20期時間
加熱した後に空冷しても「均一で透明なガラス試料を得
ることができなかった。このようにして得られたガラス
を切断「研摩して直径5〜8職「長さ30〜5物肋のガ
ラスロッドを得、更に「第亀図に示す線引き装置を窮い
て、直径150ム肌のアンクラッドフアィバを得た。When Snake S6 containing Q: 14.3 mol % to S: 85.7 mol % was used, sufficient vitrification was achieved by heating at 800 mol % for 20 hours. Also, the S content is 66.7 mol% and 85
.. W in the region between 7 mol% ~ i.e. x between 2 and 6
To obtain glass using SX, the heating temperature and heating time are both 800 to 1000 qC and 2
It was within the range of 0 to 20 leg hours. In this way, the heating temperature and heating time required for vitrification depend on the S content.It has been found that the higher the sulfur S content, the lower the heating temperature and the shorter the heating time, the more uniform and transparent glass can be obtained. did. Furthermore, when using QSx in the region of S < 66.?mol%, that is, x < 2, "it is not possible to obtain a uniform and transparent glass sample even if it is heated at 1000o○ for 20 periods and then air cooled." The glass thus obtained was cut and polished to obtain a glass rod with a diameter of 5 to 8 mm and a length of 30 to 5 mm. I got an unclad fiber with thick skin.
驚喜図において、符号軍はカルコゲナイドガラスロッド
、2は発熱体〜 乳ま不活性ガス導入口「 Wまロッド
支持管、5音まガス排出口「 蚤さまシャツ夕、7は線
引き用駆動モータ、8はカバー用石英ガラス管をそれぞ
れ示す。フアィバ化にあたっては「不活性ガス導入口3
からロッド支持管亀内に不活性ガスを供給し、発熱体2
によりガラスロッド1を線引き温度400〜700qo
で加熱しながら6〜15のノ分の線引き速度で線引きし
た。ここで「 S=66.7モル%の技S2ガラスを用
いて直径150rmの光フアィバを得るためには「 約
700o0、S=85.7モル%のWS6ガラスの場合
には約400ooの温度で線引きが可能であった。すな
わち、適正な線引き温度は400〜700qoであり「
ここで硫黄Sの含有量が多いほど低い温度で線引きが
可能であった。一方、前述したようにフアィバ化は〜不
活性ガスを流しながら常圧下で行うため、フアイバ化の
工程中にガラス表面から硫黄Sの揮発が生じた。In the illustration, the code group is chalcogenide glass rod, 2 is heating element, inert gas inlet port, W rod support tube, 5 gas outlet port, flea shirt, 7 is drive motor for wire drawing, 8 1 shows the quartz glass tube for the cover.When converting to fiber, inert gas inlet 3
Inert gas is supplied into the rod support tube from the heating element 2.
The glass rod 1 is drawn at a temperature of 400 to 700 qo.
The wire was drawn at a drawing speed of 6 to 15 minutes while heating at . Here, ``In order to obtain an optical fiber with a diameter of 150 rm using WS6 glass with S = 66.7 mol%, the temperature is approximately 700 o 0, and in the case of WS6 glass with S = 85.7 mol %, the temperature is approximately 400 oo. It was possible to draw the wire.In other words, the appropriate drawing temperature is 400 to 700 qo.
Here, the higher the sulfur S content, the lower the temperature for drawing. On the other hand, as mentioned above, since fiberization is carried out under normal pressure while flowing an inert gas, sulfur S volatilizes from the glass surface during the fiberization process.
これは、硫黄Sの含有量が増加するほど著しくなり、S
Z85。7モル%すなわちxZ6の組成のガラスでは、
線引き工程中に硫黄Sの揮発が激しくフアィバ表面が白
色化し、フアィバ化自体が困難であった。This becomes more remarkable as the sulfur S content increases, and S
Z85. In a glass with a composition of 7 mol% or xZ6,
During the drawing process, the sulfur S volatilized violently, causing the fiber surface to turn white, making it difficult to form the fiber itself.
更に加えて「 このような硫黄Sの揮発が生じると、得
られたフアィバの散乱損失が増加し「光損失の低いフア
ィバを得ることが難しかった。以上の各実施例に基づい
て「ゲルマニウムGeと硫黄Sから成る2成分系の素材
を用いて低損失の光ファィバを得るには、蛇=167〜
33.3モル%、S:66.7〜83。In addition, ``When such volatilization of sulfur S occurs, the scattering loss of the obtained fiber increases, making it difficult to obtain a fiber with low optical loss. In order to obtain a low-loss optical fiber using a two-component material consisting of sulfur S, snake = 167 ~
33.3 mol%, S: 66.7-83.
3モル%すなわち蛇Sx(2ミ又≦5)の領域の素材を
用いればよいことが分かった。It has been found that it is sufficient to use a material in the range of 3 mol %, that is, Sx (2 mm ≦5).
次に、技SX(2Sx≦5)系ガラスの光透過特性およ
び快S395ガラスを用いた光ファィバの光損失を測定
した。Next, the light transmission characteristics of the GSX (2Sx≦5) glass and the optical loss of the optical fiber using the S395 glass were measured.
(光損失の測定)
上述した実施例1のようにして作製した長さ1〜2仇の
WS3,5(S=77.8モル%)ガラスフアイバの光
損失を、1〜5#肌の波長領域において測定した。(Measurement of optical loss) The optical loss of the WS3,5 (S = 77.8 mol%) glass fiber with a length of 1 to 2 mm, prepared as in Example 1 above, was measured at the wavelength of 1 to 5 # skin. Measured in the area.
その結果を第鷲図に示す。光損失の測定にあたっては〜
検出器としてlnSbを、光源としてはタングステンラ
ンプもニクロム線を用い「30肌毎にフアィバを切断し
て各出力端における各波長の出力を測定し「その出力差
から光損失を求めた。第2図においても波長4。5仏肌
近傍での光損失値は2.5×1ぴdB′奴であったが「
2.5必m近傍の吸収ピークはOH不純物による吸収
も3〜4A肌の吸収ピークはSH不純物による吸収に帰
属しており〜これらの不純物を除去すことにより、WS
X系ガラスの光ファィバの光損失を、素材の固有損失(
5×10‐2dB′物程度と推定されている)まで低減
化できる可能性があることが分かった。The results are shown in Fig. When measuring optical loss
Using lnSb as a detector and a nichrome wire with a tungsten lamp as a light source, the fiber was cut every 30 skins and the output of each wavelength at each output end was measured, and the optical loss was determined from the output difference. In the figure, the optical loss value near wavelength 4.5 was 2.5×1 pidB'.
The absorption peak near 2.5 m is attributed to absorption by OH impurities, and the absorption peak of 3 to 4 A skin is attributed to absorption by SH impurities ~ By removing these impurities, WS
The optical loss of an optical fiber made of X-based glass can be calculated from the inherent loss of the material (
It was found that it is possible to reduce the noise level to 5 × 10-2 dB'.
(光透過特性の測定)
実施例1の方法で作製した厚さ0.5肋のWS2(S=
66.7モル%)ガラス板の光透過特性を0.25〃の
〜30仏のの波長城にわたって測定した。(Measurement of light transmission characteristics) WS2 (S=
(66.7 mol%) The light transmission properties of the glass plate were measured over a wavelength range of 0.25 to 30 French.
その結果を第3図に示す。第3図において、このガラス
の吸収端は、紫外において約0.4仏の、赤外において
約12仏のにあるが、これら吸収端の外そう値は第4図
から分かるように、5〜7〃の波長城で5×10‐2d
B′物の低損失値を示している。この低損失値は、現在
ガラスフアィバとして広く知られている石英ガラス系フ
アィバの最低損失値の約うに相当するものである。また
、本発明光ファィバに用いるWSX((2≦x≦5)系
のガラスは、上記○eS2(S=66.7モル%)ガラ
スとほぼ同様の光透過特性を示しており、2〜7rの波
長城において1船′物程度以下の低損失値を実現できる
可能性のあることが分かった。実施例 2
次に実施例1と同機の手順で3成分Q−P−S系ガラス
において、各種組成のガラスおよびガラスフアィバを作
製し、ガラスフアィバ作製に最適なガラス組成範囲を明
らかにした。The results are shown in FIG. In Fig. 3, the absorption edges of this glass are at about 0.4 F in the ultraviolet and about 12 F in the infrared, but as can be seen from Fig. 5×10-2d at wavelength castle of 7〃
It shows the low loss value of B' product. This low loss value corresponds to about the lowest loss value of silica glass fiber, which is currently widely known as glass fiber. Furthermore, the WSX ((2≦x≦5) glass used in the optical fiber of the present invention exhibits almost the same light transmission characteristics as the above-mentioned ○eS2 (S=66.7 mol%) glass, and has a 2 to 7 r It was found that there is a possibility of achieving a low loss value of less than that of a single ship at a wavelength castle of Glasses and glass fibers of various compositions were produced, and the optimal glass composition range for glass fiber production was clarified.
WS2に燐Pを少量添加した蛇S2P,/3(Q=30
モル%、S=60モル%、P=10モル%)においては
、ガラス化は950qo、80時間の加熱で十分であっ
た。Snake S2P, /3 (Q = 30
mol%, S=60 mol%, P=10 mol%), heating at 950 qo for 80 hours was sufficient for vitrification.
10モル%以下の燐Pを添加した場合、ガラス化が容易
に行われることがわかった。It was found that when 10 mol% or less of phosphorus P was added, vitrification was easily performed.
ところが、燐Pの含有量を、QS2Pにおける燐Pの割
合以上、すなわち>25モル%にすると「均一で透明な
ガラスが得られなくなった。一方、Q一P−S系のフア
ィバ化に際してはt隣Pを11モル%以上に増加させる
と、表面からの硫黄S、燐Pの揮発が増大し、低損失な
フアィバが得られなくなることがわかった。However, when the phosphorus P content exceeds the proportion of phosphorus P in QS2P, that is, >25 mol%, it becomes impossible to obtain a uniform and transparent glass.On the other hand, when forming a fiber from the Q1P-S system, It has been found that when the neighboring P content is increased to 11 mol% or more, the volatilization of sulfur S and phosphorus P from the surface increases, making it impossible to obtain a fiber with low loss.
同様にして、Q、P、Sの各種配合比についてガラスお
よびフアィバを作製した結果、Q=15〜33.3モル
%、Pニ0〜10モル%、S:60〜83.3モル%の
配合比、すなわち、第5図の斜線を施した領域内の配合
比においてのみ、2×1ぴdB′物程度以下の低損失な
光フアイバを作製できることが分かった。Similarly, glasses and fibers were prepared with various blending ratios of Q, P, and S. It has been found that it is possible to produce an optical fiber with a low loss of about 2×1 dB' or less only at the compounding ratio, that is, the compounding ratio within the shaded area in FIG.
次いで、この種Pe一P−S系のガラスフアイバの光損
失を測定した。Next, the optical loss of this kind of Pe-P-S glass fiber was measured.
(光損失の測定) QS2.5P,/3(Qニ26。(Measurement of optical loss) QS2.5P, /3 (Q226.
1モル%、Sニ65.2モル%、P=8.7モル%)ガ
ラスフアィバの光損失を約1〜5ムの波長城において測
定した例を第6図に示す。1 mol %, S 65.2 mol %, P = 8.7 mol %) An example in which the optical loss of a glass fiber was measured at a wavelength range of approximately 1 to 5 μm is shown in FIG.
第6図において、波長2仏の近傍で、4×lぴ船′鰍、
4.5山肌近傍で4×lぴdB′舷の低損失値が得られ
た。この様にQ−P一S系ガラスフアィバでは、適正な
組成域内のガラスを用いることにより、2〜7山肌帯で
比較的低額失な値を得ることができることが分かった。
実施例 3
次いで、第5図に示した光ファィバ作製に適するガラス
組成領域内のガラスの屈折率を測定したところ、硫黄S
および燐Pの含有量が増加するにつれて増大していた。In Figure 6, in the vicinity of wavelength 2 Buddha, 4
A low loss value of 4×l pi dB′ was obtained near the 4.5 mountain surface. In this manner, it has been found that with the Q-P-S glass fiber, by using glass within an appropriate composition range, a relatively low cost value can be obtained in the 2-7 slope zone.
Example 3 Next, the refractive index of the glass in the glass composition region suitable for producing the optical fiber shown in FIG. 5 was measured, and it was found that sulfur S
and increased as the phosphorus P content increased.
そこで、戊S3P,/3ガラスおよびこのガラスより屈
折率の低いWS3ガラスのブロックをそれぞれ円柱状お
よび円筒状のロッド‘こ加工し、それぞれをコアおよび
クラッドとするいわゆるロッドインチューブ法により、
ステップ状の屈折率分布を有する光フアィバを線引きし
た。コア、クラッドーこそれぞれ用いる2種類のガラス
の熱膨張係数は共に20〜25×10‐6であり、熱的
なマッチングは良好で、外径160山肌、コア蓬約50
仏肌の光フアィバを、約low/分の速度で数十机線引
く二とができた。しかして、比較的取扱い易い太径の屈
折率階段形光ファィバを、戊−P−S系ガラスをコアと
し、Q−S系ガラスをクラッドとして作製できることも
分かった。以上説明したように、本発明による蛇‐S系
または蛇−P−S系力ルコゲナィドガラスは毒性が低く
、しかもそのガラス組成を戊申15〜33.3モル%、
Pニ0〜10モル%、Sニ60〜83.3モル%とする
ことにより、カルコゲナイドガラスのガラス化およびフ
アィバ化が容易となり、2〜7r机の波長城における光
伝送損失を低減させた光フアイバを実現することができ
る。Therefore, by using the so-called rod-in-tube method, blocks of S3P, /3 glass and WS3 glass, which has a lower refractive index than this glass, are processed into cylindrical and cylindrical rods, respectively, and these are used as the core and cladding.
An optical fiber with a step-like refractive index distribution was drawn. The coefficients of thermal expansion of the two types of glasses used for the core and cladding are both 20 to 25 x 10-6, and the thermal matching is good.
It was possible to draw dozens of lines through the optical fiber of Buddha's skin at a speed of about low per minute. It has also been found that a relatively easy-to-handle large-diameter stepped-index optical fiber can be produced with a core made of Bo-P-S glass and a cladding made of Q-S glass. As explained above, the Snake-S type or Snake-P-S type lucogenide glass according to the present invention has low toxicity and has a glass composition of 15 to 33.3 mol%.
By setting the P content to 0 to 10 mol% and the S content to 60 to 83.3 mol%, chalcogenide glass can be easily vitrified and made into a fiber, and light with reduced optical transmission loss at a wavelength range of 2 to 7 r. fiber can be realized.
第1図は本発明光フアィバを作製するための線引き装置
の構成図、第2図は波長1〜5ムの領域におけるWS3
.5ガラスファィバの光損失特性曲線図、第3図はWS
2ガラス板(0.5側厚)の各波長に対する光透過特性
曲線図「第4図は紫外および赤外吸収端の外そう直線を
示す特性曲線図、第5図は光ファイバ作製に最適なガラ
ス組成領域を示す線図L第6図は波長1〜5#の領域に
おけるWS2.5P,′3ガラスファィバの光損失特性
曲線図である。
亀……カルコゲナィドガラスロッド「 2……発熱体、
3……不活性ガス導入口、4・…・心ッド支持管も5…
…ガス排出口「 6……シャツ夕、7・・・…線引き用
駆動モー夕、8……カバー用石英ガラス管。
簾も図
第Z図
第3図
第4図
第5図
第6図Fig. 1 is a block diagram of a drawing apparatus for producing the optical fiber of the present invention, and Fig. 2 shows a WS3 in the wavelength range of 1 to 5 μm.
.. 5 Optical loss characteristic curve diagram of glass fiber, Figure 3 is WS
2 A diagram of the light transmission characteristic curve for each wavelength of the glass plate (0.5 side thickness) "Figure 4 is a characteristic curve diagram showing the straight lines of the ultraviolet and infrared absorption edges, and Figure 5 is the characteristic curve diagram that is optimal for making optical fibers. Diagram L showing the glass composition range Figure 6 is an optical loss characteristic curve diagram of the WS2.5P,'3 glass fiber in the wavelength range 1 to 5#. body,
3...Inert gas inlet, 4... Core support pipe 5...
...Gas exhaust port 6...Shirt cover, 7...Driving motor for wire drawing, 8...Quartz glass tube for cover.
Claims (1)
0モル%、硫黄を60〜83.3モル%含むガラスによ
りコアまたはクラツドを形成したことを特徴とする光フ
アイバ。1 Germanium 15-33.3 mol%, phosphorus 0-1
An optical fiber characterized in that its core or cladding is formed of glass containing 0 mol% and 60 to 83.3 mol% of sulfur.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP55090697A JPS606298B2 (en) | 1980-07-04 | 1980-07-04 | optical fiber |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP55090697A JPS606298B2 (en) | 1980-07-04 | 1980-07-04 | optical fiber |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5717445A JPS5717445A (en) | 1982-01-29 |
| JPS606298B2 true JPS606298B2 (en) | 1985-02-16 |
Family
ID=14005715
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP55090697A Expired JPS606298B2 (en) | 1980-07-04 | 1980-07-04 | optical fiber |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS606298B2 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6350166U (en) * | 1986-09-19 | 1988-04-05 |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH045491Y2 (en) * | 1985-10-16 | 1992-02-17 | ||
| JPH0695141B2 (en) * | 1987-10-14 | 1994-11-24 | 松下電器産業株式会社 | Laser radar image forming device |
-
1980
- 1980-07-04 JP JP55090697A patent/JPS606298B2/en not_active Expired
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6350166U (en) * | 1986-09-19 | 1988-04-05 |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5717445A (en) | 1982-01-29 |
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