JPS6229762B2 - - Google Patents
Info
- Publication number
- JPS6229762B2 JPS6229762B2 JP57219822A JP21982282A JPS6229762B2 JP S6229762 B2 JPS6229762 B2 JP S6229762B2 JP 57219822 A JP57219822 A JP 57219822A JP 21982282 A JP21982282 A JP 21982282A JP S6229762 B2 JPS6229762 B2 JP S6229762B2
- Authority
- JP
- Japan
- Prior art keywords
- optical fiber
- measurement
- transmission line
- optical
- loss
- 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
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01M—TESTING STATIC OR DYNAMIC BALANCE OF MACHINES OR STRUCTURES; TESTING OF STRUCTURES OR APPARATUS, NOT OTHERWISE PROVIDED FOR
- G01M11/00—Testing of optical apparatus; Testing structures by optical methods not otherwise provided for
- G01M11/30—Testing of optical devices, constituted by fibre optics or optical waveguides
- G01M11/33—Testing of optical devices, constituted by fibre optics or optical waveguides with a light emitter being disposed at one fibre or waveguide end-face, and a light receiver at the other end-face
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- Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- General Physics & Mathematics (AREA)
- Testing Of Optical Devices Or Fibers (AREA)
- Optical Integrated Circuits (AREA)
- Optical Fibers, Optical Fiber Cores, And Optical Fiber Bundles (AREA)
- Arrangements For Transmission Of Measured Signals (AREA)
Description
本発明は光フアイバの特性を測定する際に用い
られる入射光伝送路に関し、特に伝送損失の測定
と伝送帯域の測定とに兼用できる入射光伝送路に
関する。
光フアイバにつき、伝送損失、伝送帯域を測定
し、これを知得しておくことは光通信システムの
設計、その他に関した重要事項である。
従来、こうした測定法として被測定光フアイバ
の所定位置に断点をつくり、この断点と測定点と
の相対関係から伝送損失などを求めるカツトバツ
ク法(破壊測定法)と、上記断点の設定を必要と
しないインサーシヨン法(非破壊測定法)とがあ
り、インサーシヨン法は断点を必要としないので
カツトバツク法よりも都合よいとされている。
上記インサーシヨン法の1つとしてすでに実施
されている第1図のものはつぎのような仕組にな
つている。
同図において、1は発信器、2はレーザダイオ
ード、3は発光ダイオード、41,42は光スイ
ツチ、5は入射光伝送路、61,62はV溝型の
簡易接続器、7は被測定光フアイバ、8はAP
(アバランシエフオト)ダイオード、9は受信
器、10は光パワーメータ、111,112は光
コード、121,122,123は該光コード1
11,112のものよりもコア径が大きい光コー
ドであり、これらは図示のごとく光学的に接続さ
れている。
上記第1図の測定手段を介して被測定光フアイ
バ7の伝送損失、伝送帯域を測定するとき、入射
光伝送路5はその測定目的に応じて損失測定用の
ものと、帯域測定用のものとが使い分けられ、そ
の帯域測定時、損失測定時における光パルスの流
れを第1図の符号によりフローチヤートすると、
帯域測定のときは、1,2→111→41→5→
7→121→42→122→8,9のようにな
り、かつ、APダイオード8ならびに受信器9を
介して被測定光フアイバ7の伝送帯域が検出さ
れ、一方、損失測定のときは3→112→41→
5→7→121→42→123→10のようにな
り、そして光パワーメータ10により被測定光フ
アイバ7の伝送損失が検出される。
ところで前述した入射光伝送路5の場合、帯域
測定用のものにあつてはこれを利用した帯域測定
時、被測定光フアイバ7への入射条件(励振条
件)を適切にするための構成が要求され、同様に
損失測定用のものもそのための入射条件を適切な
らしめる構成が必要となる。
例えば帯域測定用の入射光伝送路5にあつて
は、時間的ないし空間的コヒーレンスを満足さ
せ、入射光が単一周波数の連続波であるとか、光
がランダムに重なり合つたり波面に歪みがないと
いつたことが要求され、一方、損失測定用の入射
光伝送路5の場合は、波長の位相が不揃いで多モ
ードの光を出すことが要求されている。
従来、帯域測定用、損失測定用など、個々に専
用の入射光伝送路はすでに提供されており、ステ
ツプインデツクス型(SI型)光フアイバとグレイ
デツドインデツクス型(GI型)光フアイバとの
組み合せからなる上記2種の従来例でも、それぞ
れ専用型としては満足のいく結果が得られてい
る。
以下これら従来例につき、第2図イ,ロを参照
して簡単に説明する。
第2図イは損失測定用の入射光伝送路5Aを示
し、同図ロは帯域測定用の入射光伝送路5Bを示
したもので、一方の入射光伝送路5AはGI型の
光フアイバ21、SI型の光フアイバ22、GI型
の光フアイバ23、同じくGI型の光フアイバ2
4が長手方向に融着接続されて構成されており、
他方の入射光伝送路5BはSI型の光フアイバ3
1、GI型の光フアイバ32、SI型の光フアイバ
33が長手方向に融着接続されて構成されてい
る。
ここで上記入射光伝送路5A,5Bのスペツク
を表1に示す。
The present invention relates to an incident optical transmission line used in measuring the characteristics of an optical fiber, and more particularly to an incident optical transmission line that can be used for both transmission loss measurement and transmission band measurement. Measuring and knowing the transmission loss and transmission band of an optical fiber is an important matter for designing optical communication systems and other matters. Conventionally, such measurement methods include the cutback method (destructive measurement method), in which a break point is created at a predetermined position on the optical fiber to be measured, and the transmission loss is determined from the relative relationship between this break point and the measurement point, and the cutback method (destructive measurement method), which involves setting the above break point. There is an insertion method (non-destructive measurement method) that does not require a breaking point, and the insertion method is said to be more convenient than the cutback method because it does not require a breaking point. One of the above-mentioned insertion methods, the one shown in FIG. 1, which has already been implemented, has the following structure. In the figure, 1 is a transmitter, 2 is a laser diode, 3 is a light emitting diode, 4 1 and 4 2 are optical switches, 5 is an incident optical transmission line, 6 1 and 6 2 are V-groove type simple connectors, and 7 is the optical fiber to be measured, 8 is the AP
(avalanche photo) diode, 9 is a receiver, 10 is an optical power meter, 11 1 , 11 2 is an optical code, 12 1 , 12 2 , 12 3 is the optical code 1
This optical cord has a larger core diameter than those of No. 1 1 and No. 11 2 , and these are optically connected as shown. When measuring the transmission loss and transmission band of the optical fiber 7 to be measured using the measuring means shown in FIG. The flowchart of the flow of optical pulses during band measurement and loss measurement using the symbols in Figure 1 is as follows:
For band measurement, 1, 2 → 11 1 → 4 1 → 5 →
7 → 12 1 → 4 2 → 12 2 → 8, 9, and the transmission band of the optical fiber 7 to be measured is detected via the AP diode 8 and the receiver 9. On the other hand, when measuring the loss, 3 → 11 2 → 4 1 →
5 → 7 → 12 1 → 4 2 → 12 3 → 10, and the transmission loss of the optical fiber 7 to be measured is detected by the optical power meter 10. By the way, in the case of the above-mentioned incident optical transmission line 5, if it is used for band measurement, a configuration is required to make the incident conditions (excitation conditions) to the optical fiber 7 to be measured appropriate when using this for band measurement. Similarly, a configuration for adjusting the incident conditions for loss measurement is also required. For example, the incident light transmission line 5 for band measurement must satisfy temporal or spatial coherence, such that the incident light is a continuous wave with a single frequency, the lights are randomly overlapped, or the wavefront is distorted. On the other hand, in the case of the incident optical transmission line 5 for loss measurement, it is required to emit multimode light with uneven wavelength phases. Traditionally, dedicated input optical transmission lines have already been provided for bandwidth measurement, loss measurement, etc., and include step index type (SI type) optical fiber and graded index type (GI type) optical fiber. The above two types of conventional examples consisting of a combination of the above have also obtained satisfactory results as dedicated types. These conventional examples will be briefly explained below with reference to FIGS. 2A and 2B. Figure 2A shows the incident optical transmission line 5A for loss measurement, and Figure 2B shows the incident optical transmission line 5B for band measurement. , SI type optical fiber 22, GI type optical fiber 23, and also GI type optical fiber 2
4 are fused and spliced in the longitudinal direction,
The other incident optical transmission line 5B is an SI type optical fiber 3.
1. A GI type optical fiber 32 and an SI type optical fiber 33 are fused and spliced in the longitudinal direction. Table 1 shows the specifications of the incident light transmission lines 5A and 5B.
【表】
なお、第2図イ,ロの入射光伝送路5A,5B
において、出射NA(50%)は0.1±0.03であり、
スポツトサイズ(50%)は30±3μmである。
上記において、一方の入射光伝送路5Aは既知
のカツトバツク法で使用し、他方の入射光伝送路
5Bはこれを第1図(インサーシヨン法)の光ス
イツチ41〜簡易接続器61間にセツトして用
い、それぞれ被測定光フアイバを測定した。
その結果を表2に示す。[Table] In addition, the incident light transmission lines 5A and 5B in Figure 2 A and B
, the exit NA (50%) is 0.1±0.03,
Spot size (50%) is 30±3 μm. In the above, one input optical transmission line 5A is used by the known cutback method, and the other input optical transmission line 5B is connected between the optical switch 41 and the simple connector 61 in FIG. 1 (insertion method). The optical fibers to be measured were each measured. The results are shown in Table 2.
【表】
なお、No.1〜5の被測定光フアイバは長さ1Km
の光フアイバ心線であり、コア径/クラツド径は
50μm/125±3μm、比屈折率差(△)は1.0±
0.15%である。
また、入射光伝送路5Aを用いた損失測定、入
射光伝送路5Bを用いた帯域測定のとき、発光ダ
イオード(LED)、レーザダイオード(LD)によ
る使用波長は、それぞれ0.85μmである。
上記表2に示した測定結果はきわめて信頼ので
きる値であり、それ故、従来では入射光伝送路5
A,5Bを用いて個々に損失測定、帯域測定を実
施している。
しかし、損失測定と帯域測定とを各別的に行な
わねばならないので、手数がかかる。
もちろん損失測定用のものを帯域測定に用いて
も、逆に帯域測定用のものを損失測定に用いても
後述する本発明との比較で明らかなように、信頼
性のある値は得られない。
本発明は上記に鑑み、損失測定と帯域測定とで
入射の条件が異なつていても、両測定に適合した
入射条件が得られるように入射光伝送路を改良し
たもので、以下その構成、効果を図面と実験結果
とに基づいて説明する。
第3図は本発明に係る入射光伝送路5Cを示し
たものであり、同図において41はSI型の光フア
イバ、42はGI型の光フアイバ、43はSI型の
光フアイバである。
上記における各光フアイバ41,42,43
は、図示の通りSI型−GI型−SI型の配列状態で
長手方向に融着接続されており、これらのスペツ
クは表3のようになつている。[Table] The length of the optical fibers No. 1 to 5 to be measured is 1 km.
It is an optical fiber core wire, and the core diameter/cladding diameter is
50μm/125±3μm, relative refractive index difference (△) is 1.0±
It is 0.15%. Further, when measuring loss using the incident optical transmission line 5A and measuring bandwidth using the incident optical transmission line 5B, the wavelengths used by the light emitting diode (LED) and the laser diode (LD) are each 0.85 μm. The measurement results shown in Table 2 above are extremely reliable values, and therefore, conventionally, the incident optical transmission line 5
A and 5B are used to perform loss measurements and band measurements individually. However, loss measurement and band measurement must be performed separately, which is time-consuming. Of course, even if a device for loss measurement is used for band measurement, or conversely, a device for band measurement is used for loss measurement, as will be clear from the comparison with the present invention described later, reliable values cannot be obtained. . In view of the above, the present invention improves the input optical transmission path so that even if the input conditions are different for loss measurement and band measurement, the input optical transmission path can obtain input conditions suitable for both measurements. The effects will be explained based on drawings and experimental results. FIG. 3 shows an incident light transmission line 5C according to the present invention, in which 41 is an SI type optical fiber, 42 is a GI type optical fiber, and 43 is an SI type optical fiber. Each optical fiber 41, 42, 43 in the above
As shown in the figure, they are fused and spliced in the longitudinal direction in an SI type-GI type-SI type arrangement, and their specifications are as shown in Table 3.
【表】
なお、本発明における入射光伝送路5Cの場
合、出射NA(50%)は0.1±0.03であり、スポツ
トサイズ(50%)は26±3μmである。
つぎに本発明の入射光伝送路5Cを第1図の光
スイツチ41、簡易接続器61間にセツトして前
記と同じく被測定光フアイバの伝送損失、伝送帯
域を測定した。
その結果を表4、表5により説明する。
なお、この際の入射光伝送路5Cは1〜2mの
光フアイバ41と1mの光フアイバ42と1〜2
mの光フアイバ43からなるものを用い、一方、
被測定光フアイバ(No.1〜5)は前記表2のもの
を用いた。
また、伝送損失の測定結果を示した表4では、
表2の電送損失測定値を基準とし、さらに伝送帯
域の測定結果を示した表5では、表2の伝送帯域
測定値を基準とした。[Table] In the case of the incident light transmission line 5C in the present invention, the output NA (50%) is 0.1±0.03 and the spot size (50%) is 26±3 μm. Next, the incident optical transmission line 5C of the present invention was set between the optical switch 41 and the simple connector 61 shown in FIG. 1 , and the transmission loss and transmission band of the optical fiber under test were measured in the same manner as above. The results will be explained using Tables 4 and 5. Incidentally, the incident light transmission line 5C at this time includes a 1-2 m optical fiber 41, a 1-m optical fiber 42, and 1-2 m optical fibers.
m optical fiber 43 is used, and on the other hand,
The optical fibers (No. 1 to 5) to be measured were those shown in Table 2 above. In addition, in Table 4 showing the measurement results of transmission loss,
The transmission loss measurement values in Table 2 were used as a standard, and Table 5, which shows the transmission band measurement results, was based on the transmission band measurement values in Table 2.
【表】【table】
【表】
表4で明らかなように本発明の入射光伝送路5
Cを用いた損失測定の結果は基準値とほぼ近似
し、信頼性のある値を示したが、帯域測定専用
(第2図ロ)の入射光伝送路5Bでは満足な値を
示しておらず、一方、表5の帯域測定結果にして
も本発明のものは基準値と殆ど差がないのに対
し、損失測定用(第2図イ)の入射光伝送路5A
では、基準値をかなり上回つたり下回つたりして
おり、バラツキが大きい。
つぎに上記伝送帯域測定時の再現性につき、表
6を参照して説明する。
なお、表6では前記No.1の被測定光フアイバを
測定対象とし、各入射光伝送路5A,5B,5C
をそれぞれ第1図の装置にセツトして5回あて帯
域測定した。[Table] As is clear from Table 4, the incident light transmission line 5 of the present invention
The loss measurement results using C were almost close to the reference values and showed reliable values, but the incident optical transmission line 5B, which is dedicated to band measurement (Figure 2 B), did not show satisfactory values. On the other hand, even in the band measurement results shown in Table 5, there is almost no difference between the band measurement results of the present invention and the reference values, whereas the incident optical transmission line 5A for loss measurement (Fig. 2 A)
However, the values fluctuate considerably above and below the standard value, with large variations. Next, the reproducibility during the above transmission band measurement will be explained with reference to Table 6. In Table 6, the No. 1 optical fiber to be measured is the measurement target, and each incident optical transmission line 5A, 5B, 5C
Each was set in the apparatus shown in FIG. 1, and the applied band was measured five times.
【表】
表6で明らかなように、損失測定専用(第2図
イ)の入射光伝送路5Aは基準となる帯域測定用
(第2図ロ)の入射光伝送路5Bと比べ、その測
定値が大きく上回つてずれているとともに偏差値
も大きくなつているが、本発明の入射光伝送路5
Cはその測定値が第2図ロのものと近似してお
り、かつ、偏差値も小さく、再現性のよいことが
うかがえる。
つぎに伝送損失につき、インサーシヨン法とカ
ツトバツク法との対比、接続損失との関係からま
とめた結果を表7に示す。
この場合、本発明の入射光伝送路5Cは第1図
のインサーシヨン法によりデータを採取し、第2
図イの入射光伝送路5Aは既述のカツトバツク法
によるデータを示した。
被測定光フアイバ(No.1〜5)は前述したもの
と同じである。[Table] As is clear from Table 6, the input optical transmission line 5A used exclusively for loss measurement (Figure 2 A) is compared with the reference input optical transmission line 5B for band measurement (Figure 2 B). Although the deviation value is greatly exceeded and the deviation value is also large, the incident light transmission line 5 of the present invention
The measured value of C is similar to that of FIG. 2B, and the deviation value is small, indicating good reproducibility. Next, regarding transmission loss, Table 7 shows the results summarized from the comparison between the insertion method and the cutback method and the relationship with connection loss. In this case, the incident optical transmission line 5C of the present invention collects data by the insertion method shown in FIG.
The incident light transmission line 5A in Figure A shows data obtained by the cutback method described above. The optical fibers to be measured (Nos. 1 to 5) are the same as those described above.
【表】
表7で明らかなように、第2図イの入射光伝送
路5Aは伝送損失の測定値が±0.1dBを越えてば
らついており、接続損失も最大値と最小値で
0.12dBの差があるが、本発明の入射光伝送路5
Cの場合では、伝送損失の測定値が0.1dB以内で
一致しており、接続損失の差も0.05dB以内にお
さまつている。
なお、本発明に係る入射光伝送路5Cの場合、
各光フアイバ41,42,43の長さが0.1〜10
mの範囲内にあれば、前述したとほぼ同じ結果が
得られることになるが、実用的には光フアイバ4
1が1〜2m、光フアイバ42が1m、光フアイ
バ43が1〜2m程度であるのがよい。
以上説明した通り、本発明の入射光伝送路は両
端にステツプインデツクス型(SI)の光フアイ
バ、その中間にグレイデツドインデツクス型
(GI型)の光フアイバを配してこれら3本の光フ
アイバが長手方向に接続されており、該各光フア
イバは長さが0.1〜10m、コア径が30±5μm、
比屈折率差が0.8±0.1%となつていることを特徴
としており、1つの当該入射光伝送路により伝送
損失と伝送帯域との両測定に供することができる
ので、従来のようにそれぞれ専用の伝送路を2種
用意するとか、これを用いて各別的に特性を調べ
るといつた面倒が解消され、もちろんその測定値
も信頼性の高いものが得られるとともに再現性も
充分にあり、しかも断点を要するカツトバツク法
でなく、これよりも簡易なインサーシヨン法にお
いて信頼性のある測定値が得られるから、総じて
都合のよい測定条件が確保できる。[Table] As is clear from Table 7, the measured transmission loss of the incident optical transmission line 5A in Figure 2A varies by more than ±0.1 dB, and the connection loss also varies between the maximum and minimum values.
Although there is a difference of 0.12 dB, the incident optical transmission line 5 of the present invention
In case C, the measured values of transmission loss match within 0.1 dB, and the difference in connection loss also falls within 0.05 dB. In addition, in the case of the incident light transmission line 5C according to the present invention,
The length of each optical fiber 41, 42, 43 is 0.1 to 10
If it is within the range of m, almost the same results as described above can be obtained, but in practice
1 is preferably about 1 to 2 m, the optical fiber 42 is about 1 m, and the optical fiber 43 is about 1 to 2 m. As explained above, the input optical transmission line of the present invention has step index type (SI) optical fibers at both ends and a graded index type (GI type) optical fiber in the middle. Optical fibers are connected in the longitudinal direction, and each optical fiber has a length of 0.1 to 10 m, a core diameter of 30 ± 5 μm,
It is characterized by a relative refractive index difference of 0.8 ± 0.1%, and can be used to measure both transmission loss and transmission band using one incident optical transmission path, so unlike conventional methods, it is possible to measure both transmission loss and transmission band. This eliminates the trouble of preparing two types of transmission lines or using them to investigate the characteristics of each separately.Of course, the measured values are also highly reliable and have sufficient reproducibility. Since reliable measurement values can be obtained not by the cutback method, which requires cut-off points, but by the insertion method, which is simpler than this method, convenient measurement conditions can be ensured overall.
第1図はインサーシヨン法による測定手段を略
示した説明図、第2図イ,ロは従来の入射光伝送
路を略示した正面図、第3図は本発明に係る入射
光伝送路を略示した正面図である。
5C……入射光伝送路、41……ステツプイン
デツクス型光フアイバ、42……グレイデツドイ
ンデツクス型光フアイバ、43……ステツプイン
デツクス型光フアイバ。
FIG. 1 is an explanatory diagram schematically showing a measurement means using the insertion method, FIGS. 2A and 2B are front views schematically showing a conventional incident light transmission path, and FIG. 3 is a schematic diagram of an incident light transmission path according to the present invention. FIG. 3 is a schematic front view. 5C...Incoming light transmission line, 41...Step index type optical fiber, 42...Graded index type optical fiber, 43...Step index type optical fiber.
Claims (1)
バ、その中間にグレイデツドインデツクス型の光
フアイバを配してこれら3本の光フアイバが長手
方向に接続されており、該各光フアイバは、長さ
が0.1〜10m、コア径が30±5μm、比屈折率差
が0.8±0.1%となつている光フアイバの伝送損
失、伝送帯域測定用入射光伝送路。 2 各光フアイバの長さが1〜2mである特許請
求の範囲第1項記載の光フアイバの伝送損失、伝
送帯域測定用入射光伝送路。[Claims] 1. A step index type optical fiber is arranged at both ends and a graded index type optical fiber is arranged in the middle, and these three optical fibers are connected in the longitudinal direction. The optical fiber has a length of 0.1 to 10 m, a core diameter of 30 ± 5 μm, and a relative refractive index difference of 0.8 ± 0.1%. It is an incident light transmission line for measuring transmission loss and transmission band. 2. An incident light transmission line for measuring transmission loss and transmission band of an optical fiber according to claim 1, wherein each optical fiber has a length of 1 to 2 m.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57219822A JPS59111103A (en) | 1982-12-15 | 1982-12-15 | Incident light transmission line for measuring transmission loss and transmission band of optical fiber |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57219822A JPS59111103A (en) | 1982-12-15 | 1982-12-15 | Incident light transmission line for measuring transmission loss and transmission band of optical fiber |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS59111103A JPS59111103A (en) | 1984-06-27 |
| JPS6229762B2 true JPS6229762B2 (en) | 1987-06-29 |
Family
ID=16741577
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP57219822A Granted JPS59111103A (en) | 1982-12-15 | 1982-12-15 | Incident light transmission line for measuring transmission loss and transmission band of optical fiber |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS59111103A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2737158B2 (en) * | 1988-06-21 | 1998-04-08 | 三菱瓦斯化学株式会社 | Optical merger |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4229067A (en) * | 1978-11-17 | 1980-10-21 | Corning Glass Works | Optical waveguide mode scrambler |
-
1982
- 1982-12-15 JP JP57219822A patent/JPS59111103A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS59111103A (en) | 1984-06-27 |
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