JPS62174623A - Polarized wave ratio measuring instrument for semiconductor laser - Google Patents
Polarized wave ratio measuring instrument for semiconductor laserInfo
- Publication number
- JPS62174623A JPS62174623A JP61017108A JP1710886A JPS62174623A JP S62174623 A JPS62174623 A JP S62174623A JP 61017108 A JP61017108 A JP 61017108A JP 1710886 A JP1710886 A JP 1710886A JP S62174623 A JPS62174623 A JP S62174623A
- Authority
- JP
- Japan
- Prior art keywords
- polarizer
- semiconductor laser
- photodetector
- light
- power source
- 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.)
- Pending
Links
- 239000004065 semiconductor Substances 0.000 title claims abstract description 11
- 230000010287 polarization Effects 0.000 claims description 8
- 238000001514 detection method Methods 0.000 abstract description 3
- 238000005259 measurement Methods 0.000 description 3
- 239000000835 fiber Substances 0.000 description 2
- 239000003795 chemical substances by application Substances 0.000 description 1
- 238000004891 communication Methods 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 230000003287 optical effect Effects 0.000 description 1
- 230000000644 propagated effect Effects 0.000 description 1
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は、半導体レーザの特性のうち、偏波比の測定装
置に関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a device for measuring polarization ratio among the characteristics of semiconductor lasers.
半導体レーザからの出力光は通常TE波とTM波に分か
れており、一般ではTE波に偏波して、TM波はほとん
どない。ところで元をファイバで伝搬させる場合、両偏
彼成分間で伝搬定数や群速度にわずかに差があり、元フ
ァイバー通信において問題となることかある。Output light from a semiconductor laser is usually divided into TE waves and TM waves, and is generally polarized into TE waves with almost no TM waves. By the way, when the source is propagated through a fiber, there is a slight difference in the propagation constant and group velocity between the two polarized components, which can cause problems in the source fiber communication.
したがってTE波成分とTM波成分の比、すなわち偏波
比を測定する必要がある。Therefore, it is necessary to measure the ratio of the TE wave component to the TM wave component, that is, the polarization ratio.
従来の偏波比の測定装置では、被測定用半導体レーザと
その光出力を検出するための受光器の間にポラライザー
をおきポラライザーの角度を調整しながらTE波成分と
TM波成分を検出し、測定していた。In conventional polarization ratio measuring equipment, a polarizer is placed between the semiconductor laser to be measured and a light receiver for detecting its optical output, and the TE wave component and TM wave component are detected while adjusting the angle of the polarizer. was measuring.
上述した従来の偏波比測定装置は、ポラライザーの角度
を調整してから両側波成分を測定する必要がある。よっ
て測定作業としてはポラライザーをそれぞれの偏波にな
るように調整しなければならないため、測定時間か長く
なるという欠点かある。The conventional polarization ratio measuring device described above needs to measure both side wave components after adjusting the angle of the polarizer. Therefore, the measurement process requires adjusting the polarizer to obtain each polarized wave, which has the disadvantage of lengthening the measurement time.
本発明は以上の欠点を鑑みて、測定操作が容易な装置を
提供することである。SUMMARY OF THE INVENTION In view of the above drawbacks, the present invention provides an apparatus that is easy to operate for measurement.
この目的を達成するために、本発明の測定装置は、連続
回転するポラライザーとこれにより変化する受光器の出
力信号を検出する装置を有している。To achieve this objective, the measuring device of the invention has a continuously rotating polarizer and a device for detecting the changing output signal of the receiver.
第1図は本発明の一実施例を示す。 FIG. 1 shows an embodiment of the invention.
1は、被測定用半導体レーザで2はその駆動用@流電源
である。この出力光はポラライザー4を通り受光器5に
入る。ポラライザー4は光の進行方向に対し、垂直な面
で一定な回転数で回転し、ている。6は受光器5のバイ
アス電源である、抵抗7は信号検出用抵抗でその信号出
力は、オシロスコープ8により61す定される。ポララ
イザー4が回転しているため、これを通した光は偏光成
分比が時間とともに変わるため、受光器5への入射量も
変化する。したかってこれにつれて、検出力抵抗7の信
号出力も変化し、この様子はオシロスコープ8で観測さ
れる。第2図は信号出力の変化を示したもので周期的に
最大値P MAX と最小値P MINが見られる。1 is a semiconductor laser to be measured, and 2 is a @current power source for driving it. This output light passes through a polarizer 4 and enters a light receiver 5. The polarizer 4 rotates at a constant rotational speed in a plane perpendicular to the direction in which the light travels. Reference numeral 6 is a bias power source for the photoreceiver 5, and resistor 7 is a signal detection resistor, the signal output of which is determined by an oscilloscope 8. Since the polarizer 4 is rotating, the polarization component ratio of the light passing through it changes over time, and the amount of light incident on the light receiver 5 also changes. Accordingly, the signal output of the detection resistor 7 changes accordingly, and this situation is observed with the oscilloscope 8. FIG. 2 shows changes in the signal output, and a maximum value P MAX and a minimum value P MIN can be seen periodically.
この図で横軸は時間t、縦軸は抵抗7の信号出力すなわ
ち受光器5への入射量を示す。In this figure, the horizontal axis shows time t, and the vertical axis shows the signal output of the resistor 7, that is, the amount of light incident on the light receiver 5.
ここで最大値PMAXは被測定用半導体レーザのTE波
成分に比例したf+u1最小値PMINはTM波成分に
比例した値となる。Here, the maximum value PMAX is proportional to the TE wave component of the semiconductor laser to be measured f+u1, and the minimum value PMIN is a value proportional to the TM wave component.
したがって、PMAx とP MINをオシロスコー
プ8で4111定することにより(1)式で偏波比T
E / T Mが求められる
TE/TM=PvAx/Pm+* ++++++++
+++ (1)〔発明の効果〕
以上説明したように本発明は、ポラライザーの調整が必
要なく副足操作の簡略化が実現できる。Therefore, by setting PMAx and P MIN to 4111 on the oscilloscope 8, the polarization ratio T
E/TM is calculated TE/TM=PvAx/Pm+* +++++++++++
+++ (1) [Effects of the Invention] As explained above, according to the present invention, it is possible to simplify the operation of the secondary leg without having to adjust the polarizer.
なお第1図の゛一実施例で示したように抵抗7の検出は
オシロスコープである必要ではなく、PMAI及びPM
INが測定できるような測定器であれはよい。Note that as shown in the embodiment of FIG.
Any measuring device that can measure IN is fine.
第1図は本発明の一実施例を示すブロック図、第2図は
、受光器の出力信号を示すグラフである。
l・・・・・・被測定用半纏体レーザ、2,6・・・・
・・直流111X、3. 7・・・・・・抵抗、4・・
・・・・ポラライザ、5・・・・・・受光器、8・・・
・・・オシロスコープ。
/−N\
代理人 弁理士 内 原 8
・ノ
河1図FIG. 1 is a block diagram showing an embodiment of the present invention, and FIG. 2 is a graph showing an output signal of a light receiver. l...Semiconductor laser to be measured, 2, 6...
...DC 111X, 3. 7...Resistance, 4...
...Polarizer, 5...Receiver, 8...
···oscilloscope. /-N\ Agent Patent Attorney Uchihara 8 ・Nogawa 1
Claims (1)
イザーを位置し、前記半導体レーザの偏波比の測定する
ことを特徴とする半導体レーザの偏波比測定装置。A polarization ratio measuring device for a semiconductor laser, characterized in that a rotating polarizer is positioned between a semiconductor laser to be measured and a light receiver, and the polarization ratio of the semiconductor laser is measured.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61017108A JPS62174623A (en) | 1986-01-28 | 1986-01-28 | Polarized wave ratio measuring instrument for semiconductor laser |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61017108A JPS62174623A (en) | 1986-01-28 | 1986-01-28 | Polarized wave ratio measuring instrument for semiconductor laser |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS62174623A true JPS62174623A (en) | 1987-07-31 |
Family
ID=11934833
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP61017108A Pending JPS62174623A (en) | 1986-01-28 | 1986-01-28 | Polarized wave ratio measuring instrument for semiconductor laser |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS62174623A (en) |
-
1986
- 1986-01-28 JP JP61017108A patent/JPS62174623A/en active Pending
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