JPS6073334A - Method and apparatus for measuring transmission characteristic of optical fiber - Google Patents
Method and apparatus for measuring transmission characteristic of optical fiberInfo
- Publication number
- JPS6073334A JPS6073334A JP18233283A JP18233283A JPS6073334A JP S6073334 A JPS6073334 A JP S6073334A JP 18233283 A JP18233283 A JP 18233283A JP 18233283 A JP18233283 A JP 18233283A JP S6073334 A JPS6073334 A JP S6073334A
- Authority
- JP
- Japan
- Prior art keywords
- optical fiber
- light source
- signal
- output
- separated
- 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.)
- Granted
Links
- 239000013307 optical fiber Substances 0.000 title claims description 46
- 230000005540 biological transmission Effects 0.000 title claims description 27
- 238000000034 method Methods 0.000 title claims description 12
- 230000005284 excitation Effects 0.000 claims description 21
- 238000005259 measurement Methods 0.000 claims description 16
- 230000003287 optical effect Effects 0.000 claims description 13
- 238000000926 separation method Methods 0.000 claims description 5
- 238000012545 processing Methods 0.000 claims description 4
- 238000012544 monitoring process Methods 0.000 claims description 2
- 239000000835 fiber Substances 0.000 description 7
- 238000010586 diagram Methods 0.000 description 2
- 239000004065 semiconductor Substances 0.000 description 2
- 238000012360 testing method Methods 0.000 description 2
- 206010028813 Nausea Diseases 0.000 description 1
- 238000004891 communication Methods 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 230000006866 deterioration Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000007526 fusion splicing Methods 0.000 description 1
- 230000008693 nausea Effects 0.000 description 1
- 230000002123 temporal effect Effects 0.000 description 1
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
- G01M11/333—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 using modulated input signals
-
- 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
- G01M11/335—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 using two or more input wavelengths
Landscapes
- Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- General Physics & Mathematics (AREA)
- Testing Of Optical Devices Or Fibers (AREA)
- Mechanical Coupling Of Light Guides (AREA)
- Light Guides In General And Applications Therefor (AREA)
Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】
(技術分野)
本発明は、光ファイバの伝送帯域を高精度に測定する方
法および装置に関する。DETAILED DESCRIPTION OF THE INVENTION (Technical Field) The present invention relates to a method and apparatus for measuring the transmission band of an optical fiber with high precision.
(従来技術とその問題点)
光ファイバの伝送帯域は、通信路としての性能を支配す
る重要な特性であり、これを精度良く測定することは極
めて重要である。(Prior Art and its Problems) The transmission band of an optical fiber is an important characteristic that governs its performance as a communication path, and it is extremely important to accurately measure this.
従来、光ファイバの伝送帯域測定は、第1図に示すよう
に、信号発生器2により適当な信号波形(パルスあるい
は正弦波)で変調された光源1からの出力光を励1辰用
ダミーファイバ3を介して、被測定光ファイバ5に入射
させ、被測定光ファイバの出射端で光検出器6により受
光される光信号を信号処理部7にて処理することにより
、伝送帯域を測定する。Conventionally, transmission band measurement of optical fibers has been carried out using a dummy fiber that excites the output light from a light source 1 that has been modulated by a signal generator 2 with an appropriate signal waveform (pulse or sine wave), as shown in Figure 1. 3 to the optical fiber to be measured 5 and received by the photodetector 6 at the output end of the optical fiber to be measured, the optical signal is processed by the signal processing unit 7 to measure the transmission band.
ここて、励振用ダミーファイバ3と被測定光ファイバ5
の接続は、V溝を用いたつき合わせ、あるいは融着接続
等で行なわれていた。ところが、光ファイバの伝送帯域
は、被測定光ファイバの入射端における励損条件に大き
く依存する性質をもっている。このため、励振用ダミー
ファイバと被測定光ファイバの接続状態によって伝送帯
域測定値は変化しやすいという欠点があった。これは、
被測定光ファイバのコア部が偏心している場合に特に著
しい。Here, the excitation dummy fiber 3 and the optical fiber to be measured 5
The connections were made by butting using V-grooves or by fusion splicing. However, the transmission band of an optical fiber has a property that it largely depends on the excitation conditions at the input end of the optical fiber to be measured. For this reason, there is a drawback that the measured value of the transmission band tends to change depending on the connection state between the excitation dummy fiber and the optical fiber to be measured. this is,
This is particularly noticeable when the core portion of the optical fiber to be measured is eccentric.
このような原因による再現性の劣化を改善する方法とし
て、従来から行なわれている方法は、第2図に示すよう
に、励損用ダミーファイバ3と被測定光ファイバ5の接
続点において、一方の光ファイバ端を微動可能な調心装
置8に固定し、受光部において受光される光出力が最大
となるよう出力レベルモニタ9により監視しながら接続
部において光ファイバの軸調心を行なう方法である。し
かし、半導体レーザ等の伝送帯域測定用光源自体が一般
に出力安定度が悪い上に、被測定光ファイバを透過した
光出力には不可避的にモード雑音と呼ばれる出力変動が
発生する。従って上記のように受光部において光出力が
最大となるよう高精度に軸調心を行なうことは極めて困
@+1であった。As a method to improve the deterioration of reproducibility due to such causes, the conventional method is to connect one side of the excitation dummy fiber 3 and the optical fiber under test 5 at the connection point, as shown in FIG. The optical fiber end is fixed to a finely movable alignment device 8, and the axis of the optical fiber is aligned at the connection point while being monitored by an output level monitor 9 so that the light output received at the light receiving section is maximized. be. However, the light source for transmission band measurement, such as a semiconductor laser, generally has poor output stability, and in addition, output fluctuations called mode noise inevitably occur in the optical output transmitted through the optical fiber to be measured. Therefore, as described above, it is extremely difficult to align the axis with high precision so that the light output is maximized in the light receiving section.
(発明の内容)
本発明は、かかる欠点を解消し、常に一定の励振条件全
実現して再現性良く光ファイバの伝送帯域を測定する方
法および装置を提供するものである。(Contents of the Invention) The present invention eliminates such drawbacks and provides a method and apparatus for measuring the transmission band of an optical fiber with good reproducibility by always realizing constant excitation conditions.
このため本発明による方法は、伝送帯域測定用光源と出
力が高安定な参照用光源の両光源からの出力光を励振用
光ファイバの一端に入射させ、該励振用光ファイバの他
端を調心装置を介して被測定ブCファイバに接続し、該
被測定光ファイバの出射端を受光部に結合し、該受光部
内で前記2つの光源からの光信号を分離し、該分離され
た参照用光源からの信号を励振用光ファイバと被測定光
ファイバの接続状態を最適とすべく調心装置全制御する
ための参照信号とし、該分離されたもう一方の光源から
の信号全伝送帯域測定用信号とすることを%漱とする。Therefore, in the method according to the present invention, output light from both light sources, a transmission band measurement light source and a highly stable reference light source, is incident on one end of an excitation optical fiber, and the other end of the excitation optical fiber is adjusted. The optical fiber to be measured is connected to the optical fiber to be measured via a core device, the output end of the optical fiber to be measured is coupled to a light receiving section, the optical signals from the two light sources are separated in the light receiving section, and the separated reference The signal from the optical source is used as a reference signal to fully control the alignment device in order to optimize the connection between the excitation optical fiber and the optical fiber under test, and the signal from the other separated light source is used to measure the entire transmission band. It is assumed that it is used as a signal for use.
また、本発明による装置は伝送帯域測定用光源と、出力
が高安定な参照用光源と、両光源からの出力光を一端に
入射される励振用光ファイバと、該励振用元ファイバの
他端に調心装置を介して接続された被iN、lI定光フ
ァイバと、該被測定光ノア゛イバの出射端に結合された
受光部とを含み、該受光部内に前記2つの光源からの光
j言置を分1tfIするイ装置分離手段を有し、該受光
部に該信号分離手段により分離された参照用光源からの
信号を受ける励振用光ファイバと被測定光ファイノ(の
接続状態を監視する出力レベルモニタともう一方の光源
からの信号金堂ける伝送帯域測定用信号処理部とを接続
したことを特徴とする。Further, the device according to the present invention includes a transmission band measurement light source, a reference light source with a highly stable output, an excitation optical fiber into which the output light from both light sources is input at one end, and the other end of the excitation source fiber. It includes an iN, lI constant optical fiber connected to the optical fiber through an alignment device, and a light receiving section coupled to the output end of the optical fiber to be measured; The device has a separation means for separating the signal from the reference light source, and monitors the connection state of the excitation optical fiber and the optical fiber to be measured, which receives a signal from the reference light source separated by the signal separation means in the light receiving section. It is characterized in that the output level monitor is connected to a signal processing section for measuring the transmission band of the signal from the other light source.
以下、本発明の内容を添ト1」図に示した実施例に沿っ
て説明する。Hereinafter, the content of the present invention will be explained with reference to the embodiment shown in the attached figure 1.
第3図は本発明方法を実施するだめの装置構成例を示し
、同図において第1.2図と同−参ff@番号は同一構
成要素を示す。FIG. 3 shows an example of the configuration of an apparatus for carrying out the method of the present invention, and in this figure, the same reference numerals as in FIG. 1.2 indicate the same components.
本装置においては、伝送帯域測定用光源1の他に、参照
用光源10として高度に安定化さ4tた光源(例えばL
ED光源)をもち、その出力光が光合波alit−介し
て励振用ファイノく3に導入されている。受光部におい
て、これら2つの光源からの光信号を分離し、参照用光
のみの出力を参照しつつ、該出力が最大となるよう出力
レベルモニタ9により監視しながら接続部の軸調心を行
なえば、高1青度な軸合せができる。In this device, in addition to the transmission band measurement light source 1, a highly stabilized 4t light source (for example, L
ED light source), and its output light is introduced into the excitation fin 3 via an optical multiplexer. In the light receiving section, the optical signals from these two light sources are separated, and while referring to the output of only the reference light, the axis alignment of the connection part is performed while monitoring with the output level monitor 9 so that the output becomes maximum. For example, high-quality alignment can be achieved.
受光部において参照用光出力のみを分離する方法として
は、第3図(、z)に示すように、伝送帯域測定用光源
と参照用光源の波長を離して設定しくこの場合0.05
μm以上離せば十分である)、受光部において波長選択
性のある分波器12で両党出力を分離するか、或は第3
図(1))に示すように、参照用光源に伝送帯域(aす
定角信号の周波数と異なる一定周波数の連続波形で変調
音かけ、受光部において、光検出器6の電気信号出力か
ら該周波数の1吉号成分のみを嘔気回路13にて分離す
る等の方、去があるが、いずれも有効である。As a method of separating only the reference light output in the light receiving section, as shown in Fig. 3 (,z), the wavelengths of the transmission band measurement light source and the reference light source should be set apart by 0.05 in this case.
(It is sufficient if the separation is at least μm), the outputs of both parties must be separated by a wavelength-selective demultiplexer 12 in the light receiving section, or a third
As shown in Figure (1)), a modulated sound is applied to the reference light source with a continuous waveform of a constant frequency different from the frequency of the constant-angle signal (a), and the signal is detected from the electrical signal output of the photodetector 6 at the light receiving section. There are alternatives, such as separating only the 1 auspicious frequency component in the nausea circuit 13, but both are effective.
このように、高麓に安定化された参照用光を利用して励
振用ファイバ3と被測定光ファイバ5との高2蒲度な軸
合わせを行うことにょシ、被測定光ファイバの励振条件
が一定となるよう高度に制御卸されて安定かつ精度の高
い伝送帯域測定が可能となる。In this way, it is necessary to align the excitation fiber 3 and the optical fiber to be measured 5 with a high degree of coherence using the reference light stabilized at the foot of the mountain. is highly controlled so that it remains constant, making stable and highly accurate transmission band measurement possible.
(発明の効果)
本発明における接続部の軸調心能力音調べるため、第3
図(α)の構成で接続点(でおける軸ずれ量と参’It
(を出光出力の間係を測定した。1llll定結果全第
4図に示す。使用した光ファイバのコア径は50μmで
ある。また、参照用光出力の時間変動を測定したところ
1分間内の最大変動幅は0.01 dB以下であった。(Effect of the invention) In order to investigate the axis alignment ability sound of the connection part in the present invention, the third
In the configuration shown in figure (α), the amount of axis misalignment at the connection point (
(The relationship between the light output and output power was measured. The constant results are shown in Figure 4. The core diameter of the optical fiber used was 50 μm. Also, the time fluctuation of the reference light output was measured, and the results were shown in Figure 4. The maximum variation width was less than 0.01 dB.
ここで参照用光源としてはLEDt用いている。第4図
の結果から本発明方法によれば容属に1μm以内の精度
て軸合わせ可能であることがわかる。一方、帯域測定用
光出力(光源として半導体レーザを用いた)の時間変動
は、1分間内の最大変動1層が0.8 dBにも達した
。第4図から、従来の装置では5Am程夏の精度でしか
調心できないことがわかる。Here, an LEDt is used as a reference light source. From the results shown in FIG. 4, it can be seen that according to the method of the present invention, it is possible to align the axis to the container with an accuracy of within 1 μm. On the other hand, the temporal variation of the optical output for band measurement (a semiconductor laser was used as the light source) reached a maximum variation of 1 layer within 1 minute of 0.8 dB. From FIG. 4, it can be seen that the conventional device can only align with an accuracy of about 5 Am.
以上の結果から、本発明によれば、被ホ1j定光ファイ
バの励振条件を高度に1tlli即でき、これによって
安定かつ精度の高い伝送帯域測定が可能となることが明
白である。また、本発明においては、極めて簀定な参照
用信号が得られることから、この参照用信号を用いて接
続部を自動的に調心する装置全付加することも極めて容
易に実現し得る。From the above results, it is clear that according to the present invention, the excitation conditions for the optical fiber to be 1j can be set to a high degree of uniformity, thereby making it possible to perform stable and highly accurate transmission band measurements. Further, in the present invention, since a very specific reference signal can be obtained, it is extremely easy to add a complete device that automatically aligns the connecting portion using this reference signal.
第1図、第2図は、従来法による装置の構成図である。
第3図(cLl(blは本発明に基づく装置の構成図で
ある。
第4図は、本発明方法による接続点における軸ずれ量と
参照用光出力の関係を測定した結果を示すグラフである
。
図面において1は伝送帯域測定用光源、2(は信号発生
器、3は励振用ファイバ、4は接続点、5は′e1.測
定光ファイバ、6.6′は光検出器、7は信号処理部、
8(は接り先部調心機構、9は出力レベルモニタ、10
は参照用光源、11は光合波器、12は光分波器、13
は旧号分離回路全それぞれ示す。
(外4名)FIGS. 1 and 2 are configuration diagrams of a conventional apparatus. Figure 3 (cLl (bl) is a configuration diagram of the device based on the present invention. Figure 4 is a graph showing the results of measuring the relationship between the amount of axis deviation at the connection point and the reference light output using the method of the present invention. In the drawing, 1 is a light source for transmission band measurement, 2 (is a signal generator, 3 is an excitation fiber, 4 is a connection point, 5 is an 'e1. measurement optical fiber, 6.6' is a photodetector, and 7 is a signal processing section,
8 (is the tip alignment mechanism, 9 is the output level monitor, 10 is the
is a reference light source, 11 is an optical multiplexer, 12 is an optical demultiplexer, 13
shows all the old separation circuits. (4 other people)
Claims (4)
の両光源からの出力光を励振用光ファイバの一端に入射
させ、該励振用光ファイバの他端を調心装置を介して被
測定光ファイバに接続し、該被1till定光フアイバ
の出射端を受光部に結合し、該受光部内で前記2つの光
源からの光信号を分離し、該分離された参照用光源から
の信号全励振用光ファイバと被tt1+定光ファイバの
接続状態を最適とすべく調心装置tf flllilす
るだめの参照信号とし、該分離されたもう一方の光源か
らの信号を云送帯域両定用信号とすることを特徴とする
光ファイバの伝送特性測定方法。(1) The output light from both the transmission band measurement light source and the reference light source with highly stable output is input into one end of an excitation optical fiber, and the other end of the excitation optical fiber is connected via an alignment device. Connect it to the optical fiber to be measured, couple the output end of the constant optical fiber to the light receiving part, separate the optical signals from the two light sources in the light receiving part, and collect all the signals from the separated reference light source. In order to optimize the connection state between the excitation optical fiber and the target tt1+ constant optical fiber, the alignment device tf is used as a reference signal for fullil, and the signal from the other separated light source is used as a signal for both transmission and transmission bands. A method for measuring transmission characteristics of an optical fiber.
波長とを0.05μm以上離し、受光部にて波長選択性
のある光分波器Qτより両光源からの光信号を分離する
ことを特徴とする特許請求の範囲第1項記載の方法。(2) Transmission band z11] The wavelength of the regular light source and the wavelength of the reference light source are separated by 0.05 μm or more, and the optical signals from both light sources are separated by an optical demultiplexer Qτ with wavelength selectivity in the light receiving section. A method according to claim 1, characterized in that:
る一定の周波数の変調をかけ、受光部にて該周波数の信
号成分を電気回路により分離することを特徴とする特許
請求の範囲第1項記載の方法。(3) The reference light source is modulated with a constant frequency different from the frequency of the transmission band measurement signal, and the signal component of the frequency is separated by an electric circuit in the light receiving section. The method described in section.
光源と、両光源からの出力光を一端に入射される励振用
光ファイバと、該励振用光ファイバの他端に調心装置を
介して接続された被測定光ファイバと、該被測定光ファ
イバの出射端に結合された受光部とを含み、該受光部内
に前記2つの光源からの光信号を分離する信号分離手段
を有し、該受光部に該信号分離手段により分離された参
照用光源からの信号を受ける励振用光ファイバと被測定
光ファイバの接続状態を監視する出力レベルモニタとも
う一方の光源からの信号を受ける伝送帯域測定用信号処
理部とを接続してなる光ファイバの伝送特性測定装置。(4) A transmission band measurement light source, a reference light source with highly stable output, an excitation optical fiber into which the output light from both light sources is input at one end, and an alignment device at the other end of the excitation optical fiber. and a light receiving section coupled to the output end of the optical fiber to be measured, the light receiving section having a signal separating means for separating the optical signals from the two light sources. and an output level monitor for monitoring the connection state between the excitation optical fiber and the optical fiber to be measured, which receives a signal from the reference light source separated by the signal separation means, and receives a signal from the other light source. An optical fiber transmission characteristic measurement device connected to a signal processing section for transmission band measurement.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP18233283A JPS6073334A (en) | 1983-09-30 | 1983-09-30 | Method and apparatus for measuring transmission characteristic of optical fiber |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP18233283A JPS6073334A (en) | 1983-09-30 | 1983-09-30 | Method and apparatus for measuring transmission characteristic of optical fiber |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6073334A true JPS6073334A (en) | 1985-04-25 |
| JPH037253B2 JPH037253B2 (en) | 1991-02-01 |
Family
ID=16116451
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP18233283A Granted JPS6073334A (en) | 1983-09-30 | 1983-09-30 | Method and apparatus for measuring transmission characteristic of optical fiber |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6073334A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| EP0212804A3 (en) * | 1985-08-19 | 1989-04-05 | Tektronix, Inc. | Multiple wavelength optical fiber measurement system |
-
1983
- 1983-09-30 JP JP18233283A patent/JPS6073334A/en active Granted
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| EP0212804A3 (en) * | 1985-08-19 | 1989-04-05 | Tektronix, Inc. | Multiple wavelength optical fiber measurement system |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH037253B2 (en) | 1991-02-01 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| WO2017016141A1 (en) | Performance testing device for multi-channel tunable laser | |
| US4378490A (en) | Optical attenuator providing controlled attenuation | |
| WO2001061303A1 (en) | Polarization mode dispersion measuring device and polarization mode dispersion measuring method | |
| CN112525486A (en) | Polarizer straight waveguide tail fiber polarization crosstalk test system | |
| CN109524874A (en) | A kind of method of gain fibre measuring device and the stability for measuring gain fibre output power | |
| JPS6073334A (en) | Method and apparatus for measuring transmission characteristic of optical fiber | |
| US20020044273A1 (en) | Apparatus and method for measuring optical characteristics and recording medium | |
| JPS6324138A (en) | Transmission-loss measuring device for optical fiber | |
| JP3237624B2 (en) | Laser oscillation wavelength monitor | |
| JPS6235627B2 (en) | ||
| JPH0363008B2 (en) | ||
| JP2507790B2 (en) | Semiconductor laser FM modulation characteristic measuring device | |
| CN117060996B (en) | Phase error evaluation system of coherent receiving chip | |
| JPS59669A (en) | Optical fiber magnetic field sensor | |
| JPH0620987Y2 (en) | Optical spectrum measuring device | |
| JPS60142228A (en) | Measuring method of optical fiber characteristics | |
| JP2511265B2 (en) | Optical transmission equipment test circuit | |
| JPH0117614B2 (en) | ||
| JPS60173429A (en) | Method and device for measuring dispersion of polarized wave | |
| JPH01153924A (en) | Coherent light measuring instrument | |
| JPS61118633A (en) | fiber optic sensor | |
| JPS6150037A (en) | Light splitting circuit | |
| JP2004317341A (en) | Optical electric field measuring apparatus and optical electric field measuring method | |
| JPS5862799A (en) | Light-applied measuring apparatus | |
| JPH05296831A (en) | Snr measuring apparatus |