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JP3535002B2 - Pass / fail judgment method of semiconductor laser - Google Patents
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JP3535002B2 - Pass / fail judgment method of semiconductor laser - Google Patents

Pass / fail judgment method of semiconductor laser

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Publication number
JP3535002B2
JP3535002B2 JP02767098A JP2767098A JP3535002B2 JP 3535002 B2 JP3535002 B2 JP 3535002B2 JP 02767098 A JP02767098 A JP 02767098A JP 2767098 A JP2767098 A JP 2767098A JP 3535002 B2 JP3535002 B2 JP 3535002B2
Authority
JP
Japan
Prior art keywords
semiconductor laser
current
temperature
resistance value
measurement result
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 - Fee Related
Application number
JP02767098A
Other languages
Japanese (ja)
Other versions
JPH11233872A (en
Inventor
弘美 大橋
光男 福田
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.)
NTT Inc
NTT Inc USA
Original Assignee
Nippon Telegraph and Telephone Corp
NTT Inc USA
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, NTT Inc USA filed Critical Nippon Telegraph and Telephone Corp
Priority to JP02767098A priority Critical patent/JP3535002B2/en
Publication of JPH11233872A publication Critical patent/JPH11233872A/en
Application granted granted Critical
Publication of JP3535002B2 publication Critical patent/JP3535002B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Semiconductor Lasers (AREA)

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【発明の属する技術分野】本発明は、半導体レ―ザの良
否を判別する半導体レ―ザの良否判別法に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a semiconductor laser pass / fail determination method for determining pass / fail of a semiconductor laser.

【0002】[0002]

【従来の技術】半導体レ―ザの良否は、その半導体レ―
ザに対し、駆動電流を、半導体レ―ザから光出力が一定
値で得られるように通電し、その駆動電流の経時変化が
予定値を超えるか否かという判別基準によつて、判別し
得る。このような観点から、従来、(1)半導体レ―ザ
に対し、室温に比し十分高い例えば70℃の温度から半
導体レ―ザがレーザ発振可能な最高温度(通常180℃
程度)までの範囲内の温度下において、駆動電流の通電
を行い、そして、その半導体レ―ザに対する駆動電流の
通電の前後で、半導体レ―ザの電流−光出力特性の測定
を各別に行い、その半導体レ―ザに対する駆動電流の通
電前での半導体レ―ザの電流−光出力特性の測定の結果
から半導体レ―ザの閾値電流の変化率を求めるととも
に、半導体レ―ザに対する駆動電流の通電後での電流−
光出力特性の測定の結果から半導体レ―ザの閾値電流の
変化率を求め、その半導体レ―ザに対する駆動電流の通
電前の電流−光出力特性の測定の結果から求められる半
導体レ―ザの閾値電流の変化率と半導体レ―ザに対する
駆動電流の通電後の電流−光出力特性の測定の結果から
求められる半導体レ―ザの閾値電流の変化率との差を閾
値電流変化率差とするとき、その閾値電流変化率差が例
えば10%というような予定値を超えていない場合半導
体レ―ザが上述した半導体レ―ザの良否の判別基準によ
る良であること、閾値電流変化率差が予定値を超えてい
る場合半導体レ―ザが上述した半導体レ―ザの良否の判
別基準による否(不良)であることから、(2)半導体
レ―ザに対し、室温に比し十分高い例えば70℃の温度
から半導体レ―ザがレーザ発振可能な最高温度(例えば
180℃程度)までの範囲内の温度下において、駆動電
流の通電を行い、そして、その半導体レ―ザに対する駆
動電流の通電の前後で、半導体レ―ザの電流−光出力特
性の測定を各別に行い、その半導体レ―ザに対する駆動
電流の通電前での半導体レ―ザの電流−光出力特性の測
定の結果から半導体レ―ザの閾値電流の変化率を求める
とともに、半導体レ―ザに対する駆動電流の通電後での
電流−光出力特性の測定の結果から半導体レ―ザの閾値
電流の変化率を求め、その半導体レ―ザに対する駆動電
流の通電前の電流−光出力特性の測定の結果から求めら
れる半導体レ―ザの閾値電流の変化率と半導体レ―ザに
対する駆動電流の通電後の電流−光出力特性の測定の結
果から求められる半導体レ―ザの閾値電流の変化率との
差を閾値電流変化率差とし、その閾値電流変化率差が例
えば10%というような予定値を超えるか否かによっ
て、超えない場合は半導体レ―ザが良、超える場合は半
導体レ―ザが不良であると判別する、という半導体レ―
ザの良否判別法が提案されている。
2. Description of the Related Art The quality of a semiconductor laser depends on its quality.
The drive current can be applied to the laser so that the optical output from the semiconductor laser can be obtained at a constant value, and the drive current can be discriminated based on a discrimination criterion as to whether or not the change over time of the drive current exceeds a predetermined value. . From this point of view, conventionally, (1) the maximum temperature (usually 180 ° C.) at which the semiconductor laser can oscillate from a temperature sufficiently higher than room temperature, for example, 70 ° C.
Drive current at a temperature within the range of up to about 1), and the current-optical output characteristics of the semiconductor laser are measured separately before and after the drive current is applied to the semiconductor laser. , The rate of change of the threshold current of the semiconductor laser is obtained from the measurement result of the current-optical output characteristics of the semiconductor laser before the drive current is applied to the semiconductor laser, and the drive current for the semiconductor laser is calculated. Current after energizing
The change rate of the threshold current of the semiconductor laser is obtained from the measurement result of the optical output characteristics, and the current-optical output characteristic of the semiconductor laser before the drive current is applied to the semiconductor laser is obtained from the measurement result of the semiconductor laser. The difference between the rate of change of the threshold current and the rate of change of the threshold current of the semiconductor laser obtained from the measurement result of the current-optical output characteristics after the drive current is applied to the semiconductor laser is defined as the difference of the threshold current change rate. At this time, when the difference in the threshold current change rate does not exceed a predetermined value such as 10%, it is determined that the semiconductor laser is good according to the above-mentioned criteria for determining whether the semiconductor laser is good or bad. When the value exceeds the predetermined value, the semiconductor laser is defective (defective) according to the above-mentioned criteria for judging whether the semiconductor laser is good or bad. (2) The semiconductor laser is sufficiently higher than room temperature, for example, Semiconductor laser from 70 ℃ The current of the semiconductor laser is supplied before and after the drive current is supplied to the semiconductor laser at a temperature within the range up to the maximum temperature at which laser oscillation is possible (for example, about 180 ° C.). -The optical output characteristics are measured separately and the current of the semiconductor laser before the drive current is applied to the semiconductor laser-The rate of change of the threshold current of the semiconductor laser is calculated from the results of the measurement of the optical output characteristics. In addition to obtaining the change rate of the threshold current of the semiconductor laser from the measurement result of the current-optical output characteristics after the drive current was applied to the semiconductor laser, the change rate before the drive current was applied to the semiconductor laser was calculated. Change rate of threshold current of semiconductor laser obtained from measurement result of current-optical output characteristics and semiconductor laser obtained from measurement result of current-optical output characteristic after drive current is applied to the semiconductor laser Threshold of The difference between the current change rate and the threshold current change rate is defined as the difference, and if the threshold current change rate difference exceeds a planned value such as 10%, the semiconductor laser is good if it does not exceed, and the semiconductor laser is good if it does. Is a semiconductor laser that determines that the semiconductor laser is defective.
The quality judgment method of The has been proposed.

【0003】[0003]

【発明が解決しようとする課題】上述した従来の半導体
レ―ザの良否判別法は、半導体レ―ザに対し駆動電流を
通電することを前提として、その通電の前後で各別の電
流−光出力特性の測定を行い、その結果から各別に求め
られる半導体レ―ザの閾値電流の変化率の差から、半導
体レ―ザの良否を判定する、というものであり、従っ
て、半導体レ―ザの電流−光出力特性の測定、その測定
結果を用いた半導体レ―ザの良否の判別という、測定及
び判別の外、半導体レ―ザに対する駆動電流の通電を必
要とし、しかも、その通電に長い時間を必要とする、と
いう欠点を有していた。
SUMMARY OF THE INVENTION The above-mentioned conventional method for determining the acceptability of a semiconductor laser is based on the premise that a drive current is applied to the semiconductor laser, and separate current-light before and after the application of the drive current. The output characteristics are measured, and the quality of the semiconductor laser is judged from the difference in the rate of change in the threshold current of the semiconductor laser, which is obtained from the results, respectively. Measurement of current-light output characteristics, determination of the quality of the semiconductor laser using the measurement result, other than measurement and determination, it is necessary to supply a drive current to the semiconductor laser, and it takes a long time to supply the drive current. It had the drawback that it required.

【0004】また、従来の半導体レ―ザの良否判別法の
場合、半導体レ―ザに対する駆動電流の通電の前後での
電流−光出力特性の測定に、光検出を伴うことから、そ
の測定を簡易、迅速に行うことができない、という欠点
を有していた。よって、本発明は、上述した欠点のな
い、新規な半導体レ―ザの良否判別法を提案せんとする
ものである。
Further, in the case of the conventional semiconductor laser quality determination method, the measurement of the current-optical output characteristics before and after the drive current is applied to the semiconductor laser involves optical detection. It had the drawback that it could not be done easily and quickly. Therefore, the present invention proposes a new semiconductor laser pass / fail determination method without the above-mentioned drawbacks.

【0005】[0005]

【課題を解決するための手段】本発明による半導体レ―
ザの良否判別法は、(1)半導体レ―ザの電流−電圧特
性の測定を、第1の温度下と、その第1の温度に比し高
い第2の温度下とで各別に行い、その第1の温度下での
電流−電圧特性の測定結果から半導体レ―ザの閾値電流
またはその近傍における抵抗値を求めるとともに、第2
の温度下での電流−電圧特性の測定結果から半導体レ―
ザの閾値電流またはその近傍における抵抗値を求め、そ
の第1の温度下での電流−電圧特性の測定結果から求め
られる半導体レ―ザの閾値電流またはその近傍における
抵抗値と第2の温度下での電流−電圧特性の測定結果か
ら求められる半導体レ―ザの閾値電流またはその近傍に
おける抵抗値との差を抵抗値差とするとき、その抵抗値
差が予定値を超えていない場合、半導体レ―ザが上述し
た半導体レ―ザの良否の判別基準による良であること、
抵抗値差が予定値を超えている場合、半導体レ―ザが上
述した半導体レ―ザの良否の判別基準による否(不良)
であることを確認するに到ったことから、(2)半導体
レ―ザの電流−電圧特性の測定を、第1の温度下と、そ
の第1の温度に比し高い第2の温度下とで各別に行い、
その第1の温度下での電流−電圧特性の測定結果から半
導体レ―ザの閾値電流またはその近傍における抵抗値を
求めるとともに、第2の温度下での電流−電圧特性の測
定結果から半導体レ―ザの閾値電流またはその近傍にお
ける抵抗値を求め、その第1の温度下での電流−電圧特
性の測定結果から求められる半導体レ―ザの閾値電流ま
たはその近傍における抵抗値と第2の温度下での電流−
電圧特性の測定結果から求められる半導体レ―ザの閾値
電流またはその近傍における抵抗値との差を抵抗値差と
し、その抵抗値差が予定値を超えるか否かによって、半
導体レ―ザの良否を判別する。
A semiconductor laser according to the present invention.
The quality determination method of the laser is as follows: (1) The current-voltage characteristics of the semiconductor laser are measured separately under a first temperature and a second temperature higher than the first temperature, The resistance value at or near the threshold current of the semiconductor laser is obtained from the measurement result of the current-voltage characteristics under the first temperature, and the second value
From the measurement results of the current-voltage characteristics under the temperature of
Of the semiconductor laser threshold current or its vicinity and the resistance value at or near the threshold current of the semiconductor laser obtained from the measurement result of the current-voltage characteristics at the first temperature. When the difference between the threshold current of the semiconductor laser obtained from the measurement result of the current-voltage characteristics at or in the vicinity and the resistance value in the vicinity is taken as the resistance value difference, if the resistance value difference does not exceed the planned value, the semiconductor The laser is good according to the above-mentioned criteria for judging whether the semiconductor laser is good or bad,
If the resistance difference exceeds the expected value, the semiconductor laser is judged to be defective (defective) according to the above-mentioned criteria for judging whether the semiconductor laser is good or bad.
Since it has been confirmed that (2) the current-voltage characteristics of the semiconductor laser are measured under the first temperature and the second temperature higher than the first temperature. And each separately,
The resistance value at or near the threshold current of the semiconductor laser is obtained from the measurement result of the current-voltage characteristic under the first temperature, and the semiconductor laser is calculated from the measurement result of the current-voltage characteristic under the second temperature. -The resistance value at or near the threshold current of the semiconductor laser obtained by measuring the resistance value at or near the threshold current of the laser and from the measurement result of the current-voltage characteristics under the first temperature Current under −
The difference between the threshold current of the semiconductor laser obtained from the measurement result of the voltage characteristics or the resistance value in the vicinity of the semiconductor laser is taken as the resistance difference, and whether the semiconductor laser is good or bad depends on whether the difference exceeds the planned value. To determine.

【0006】この場合、半導体レ―ザの電流−電圧特性
の測定時の第1の温度は、室温(25℃)であるのを可
とし、また、第2の温度は、半導体レ―ザがレーザ発振
可能な最高温度以下であって、第1の温度との間に40
℃〜50℃以上の差を有する温度であるのを可とする。
In this case, the first temperature at the time of measuring the current-voltage characteristics of the semiconductor laser can be room temperature (25 ° C.), and the second temperature can be measured by the semiconductor laser. It is less than the maximum temperature at which laser oscillation is possible,
It is acceptable that the temperature has a difference of 50 ° C to 50 ° C or more.

【0007】[0007]

【発明の実施の形態】次に、図1〜図4を伴って、本発
明による半導体レ―ザの良否判別法の実施の形態を述べ
よう。
BEST MODE FOR CARRYING OUT THE INVENTION Next, an embodiment of a pass / fail judgment method for a semiconductor laser according to the present invention will be described with reference to FIGS.

【0008】本発明者等は、(1)一般に、半導体レ―
ザの電流−電圧特性はダイオード特性を呈し、また、半
導体レ―ザの電流−抵抗特性は半導体レ―ザの電流−電
圧特性の一次微分特性で得られるが、従来の技術の項で
上述した半導体レ―ザの良否の判別基準によって良であ
る半導体レ―ザについて、その半導体レ―ザの電流−電
圧特性及び電流−抵抗特性が、図1中実線図示のように
得られるとき、その半導体レ―ザと同様の構成を有する
が上述した半導体レ―ザの良否の判別基準によって不良
である半導体レ―ザについては、その半導体レ―ザの電
流−電圧特性が、良である半導体レ―ザの電流−電圧特
性を基準として、図1中点線図示のように、電流の増加
につれて電圧が低下しているものとして得られ、また電
流−抵抗特性が、図1中点線図示のように、閾値電流以
上の電流において、その電流の増加につれて抵抗値が、
良である半導体レ―ザの電流−抵抗特性の場合に比し、
低下しているものとして得られること、(2)上述した
半導体レ―ザの良否の判別基準によって良であるとする
半導体レ―ザについて、その半導体レ―ザの例えば室温
である25℃でなる第1の温度で測定された電流−電圧
特性が、図2中実線図示のように得られるとき、その半
導体レ―ザの例えば85℃でなる第1の温度に比し高い
第2の温度で測定された電流−電圧特性が、第1の温度
で測定された電流−電圧特性を基準として、図2中点線
図示のように、電流の低下につれて電圧が低下している
ものとして得られ、また、電流−抵抗特性が、図2中点
線図示のように、閾値電流またはその近傍の電流におけ
る抵抗値が、第1の温度で測定された電流−抵抗特性の
場合の閾値電流またはその近傍における抵抗値からほと
んど変化していないものとして得られること、(3)上
述した半導体レ―ザの良否の判別基準によって良である
とする上述した(2)の半導体レ―ザと同様の構成を有
するが、上述した半導体レ―ザの良否の判別基準によっ
て不良である半導体レ―ザについて、(a)その半導体
レ―ザの上述した第1の温度で測定された電流−電圧特
性が、上述した半導体レ―ザの良否の判別基準によって
良であるとする上述した(2)の半導体レ―ザの第1の
温度で測定された電流−電圧特性を基準として、図3中
実線図示のように電流の増加につれて電圧が増加してい
るものとして得られ、また、電流−抵抗特性が、図3中
実線図示のように、上述した半導体レ―ザの良否の判別
基準によって良であるとする上述した(2)の半導体レ
―ザの第1の温度で測定された電流−抵抗特性とほぼ同
様に得られ、また、(b)半導体レ―ザの上述した第1
の温度に比し十分高い第2の温度で測定された電流−電
圧特性が、第1の温度で測定された電流−電圧特性を基
準として、図3中点線図示のように、電流の増加につれ
て電圧が増加し、次で、電流の増加につれて電圧が低下
しているものとして得られ、また、電流−抵抗特性が、
図3中点線図示のように、閾値電流またはその近傍にお
ける抵抗値が、第1の温度で測定された電流−抵抗特性
の場合の閾値電流またはその近傍における抵抗値に比し
大きく低下しているものとして得られること、を確認す
るに到った。
The present inventors (1) generally
The current-voltage characteristic of the laser exhibits a diode characteristic, and the current-resistance characteristic of the semiconductor laser is obtained by the first-order differential characteristic of the current-voltage characteristic of the semiconductor laser. When the current-voltage characteristics and the current-resistance characteristics of the semiconductor laser are obtained as shown by the solid line in FIG. 1, the semiconductor laser is good according to the criteria for judging the quality of the semiconductor laser. A semiconductor laser having the same configuration as that of the laser but having a defect according to the above-mentioned criteria for determining the quality of the semiconductor laser is a semiconductor laser having good current-voltage characteristics of the semiconductor laser. Based on the current-voltage characteristics of the Z, the voltage is reduced as the current increases as shown by the dotted line in FIG. 1, and the current-resistance characteristic is as shown by the dotted line in FIG. At a current above the threshold current Resistance with increasing the current,
Compared to the current-resistance characteristics of a good semiconductor laser,
(2) For a semiconductor laser that is judged to be good according to the criteria for judging whether the semiconductor laser is good or bad, the temperature of the semiconductor laser is, for example, 25 ° C. which is room temperature. When the current-voltage characteristic measured at the first temperature is obtained as shown by the solid line in FIG. 2, at the second temperature higher than the first temperature of 85 ° C. of the semiconductor laser, for example. The measured current-voltage characteristics are obtained on the basis of the current-voltage characteristics measured at the first temperature, as the voltage decreases as the current decreases, as shown by the dotted line in FIG. As for the current-resistance characteristic, as shown by the dotted line in FIG. 2, the resistance value at the threshold current or a current in the vicinity thereof is the resistance at the threshold current or its vicinity in the case of the current-resistance characteristic measured at the first temperature. Almost no change from the value (3) The semiconductor laser has the same configuration as that of the semiconductor laser of (2) described above, which is judged to be good according to the criteria for judging the quality of the semiconductor laser described above. Regarding a semiconductor laser that is defective according to the quality determination criteria of (a), the current-voltage characteristics measured at the above-mentioned first temperature of the semiconductor laser are (a) the above-mentioned determination of the quality of the semiconductor laser. Based on the current-voltage characteristic measured at the first temperature of the semiconductor laser of (2) which is considered good according to the reference, the voltage increases as the current increases as shown by the solid line in FIG. In addition, the current-resistance characteristics are determined to be good according to the criteria for determining the quality of the semiconductor laser, as shown by the solid line in FIG. The current measured at the first temperature of the Substantially the same obtained with resistive properties and, (b) semiconductor laser - first mentioned above for The
The current-voltage characteristic measured at the second temperature, which is sufficiently higher than the temperature of, is based on the current-voltage characteristic measured at the first temperature, as shown by the dotted line in FIG. It is obtained as the voltage increases, and then the voltage decreases as the current increases.
As shown by the dotted line in FIG. 3, the resistance value at or near the threshold current is significantly lower than the resistance value at or near the threshold current in the case of the current-resistance characteristic measured at the first temperature. It came to confirm that it can be obtained as a thing.

【0009】また、このようなことから、(1)(i)
半導体レ―ザの電流−電圧特性の測定を、上述した例え
ば室温である25℃でなる第1の温度下と、上述した例
えば85℃でなる第1の温度に比し高い第2の温度下と
で各別に行い、(ii)その第1の温度下での電流−電
圧特性の測定結果から半導体レ―ザの閾値電流またはそ
の近傍における抵抗値を求めるとともに、第2の温度下
での電流−電圧特性の測定結果から半導体レ―ザの閾値
電流またはその近傍における抵抗値を求め、(iii)
その第1の温度下での電流−電圧特性の測定結果から求
められる半導体レ―ザの閾値電流またはその近傍におけ
る抵抗値と第2の温度下での電流−電圧特性の測定結果
から求められる半導体レ―ザの閾値電流またはその近傍
における抵抗値との差を抵抗値差とするとき、(2)そ
の抵抗値差が予定値を超えていない場合、半導体レ―ザ
が上述した半導体レ―ザの良否の判別基準による良であ
ること、抵抗値差が予定値を超えている場合、半導体レ
―ザが上述した半導体レ―ザの良否の判別基準による否
(不良)であること、を確認するに到った。
Further, from the above, (1) (i)
The current-voltage characteristics of the semiconductor laser are measured under the first temperature of 25 ° C., which is room temperature, and under the second temperature higher than the first temperature of 85 ° C., for example. And (ii) obtaining the resistance value at or near the threshold current of the semiconductor laser from the measurement result of the current-voltage characteristics at the first temperature, and (ii) the current at the second temperature. -The resistance value at or near the threshold current of the semiconductor laser is obtained from the measurement result of the voltage characteristics, and (iii)
A semiconductor obtained from the measurement result of the current-voltage characteristic at the first temperature and the resistance value at or near the threshold current of the semiconductor laser obtained from the measurement result of the current-voltage characteristic at the second temperature. When the difference between the threshold current of the laser and the resistance value in the vicinity thereof is taken as the resistance value difference, (2) if the resistance value difference does not exceed the predetermined value, the semiconductor laser is the semiconductor laser described above. If the resistance difference exceeds the expected value, it is confirmed that the semiconductor laser is a failure (defective) according to the above-mentioned semiconductor laser quality determination criteria. Came to do.

【0010】以上に基づき、本発明による半導体レ―ザ
の良否判別法の実施の形態は、(i)半導体レ―ザの電
流−電圧特性の測定を、上述した例えば25℃でなる第
1の温度下と、上述した例えば85℃でなる第1の温度
に比し高い第2の温度下とで、それ自体は公知の種々の
方法によって各別に行い、(ii)第1の温度下での電
流−電圧特性の測定結果から半導体レ―ザの閾値電流ま
たはその近傍における抵抗値を、それ自体は公知の種々
の方法によって求めるとともに、第2の温度下での電流
−電圧特性の測定結果から半導体レ―ザの閾値電流また
はその近傍における抵抗値を、第1の温度下での電流−
電圧特性の測定結果から半導体レ―ザの閾値電流または
その近傍における抵抗値を求めた方法と同じ方法で求
め、そして、第1の温度下での電流−電圧特性の測定結
果から求められる半導体レ―ザの閾値電流またはその近
傍における抵抗値と第2の温度下での電流−電圧特性の
測定結果から求められる半導体レ―ザの閾値電流または
その近傍における抵抗値との差を抵抗値差とし、典型的
には、そのような抵抗値差を求め、その抵抗値差が予定
値を超えるか否かによって、超えない場合半導体レ―ザ
が上述した半導体レ―ザの良否の判別基準による良、超
える場合半導体レ―ザが上述した半導体レ―ザの良否の
判別基準による不良であるとして、半導体レ―ザの良否
を判別する。
Based on the above, the embodiment of the method for determining the quality of the semiconductor laser according to the present invention is: (i) The measurement of the current-voltage characteristics of the semiconductor laser is performed at the above-mentioned first temperature of 25 ° C., for example. Under a temperature and a second temperature higher than the first temperature, which is, for example, 85 ° C. described above, each is performed separately by various methods known per se, and (ii) under the first temperature From the measurement result of the current-voltage characteristics, the resistance value at or near the threshold current of the semiconductor laser is obtained by various methods known per se, and from the measurement result of the current-voltage characteristics at the second temperature. The resistance value at or near the threshold current of the semiconductor laser is the current at the first temperature
The semiconductor laser is obtained by the same method as the method for obtaining the resistance value at or near the threshold current of the semiconductor laser from the measurement result of the voltage characteristic, and is obtained from the measurement result of the current-voltage characteristic at the first temperature. -The difference between the resistance value at or near the threshold current of the laser and the resistance value at or near the threshold current of the semiconductor laser obtained from the measurement results of the current-voltage characteristics under the second temperature is defined as the resistance value difference. Typically, such a resistance difference is obtained, and if the resistance difference does not exceed a predetermined value, if it does not exceed the predetermined value, the semiconductor laser is judged to be good according to the above-mentioned criteria for judging whether the semiconductor laser is good or bad. If it exceeds, it is determined that the semiconductor laser is defective according to the above-mentioned criterion for determining the quality of the semiconductor laser, and the quality of the semiconductor laser is determined.

【0011】以上が、本発明による半導体レ―ザの良否
判別法の実施の形態である。このような本発明による半
導体レ―ザの良否判別法の実施の形態によれば、それに
よって、上述した半導体レ―ザの判別基準による良であ
るとして判別された半導体レ―ザの5個及び上述した半
導体レ―ザの判別基準による否(不良)であるとして判
別された半導体レ―ザの5個のそれぞれについて、室温
に比し十分高い70℃の温度から半導体レ―ザがレーザ
発振可能な最高温度(通常180℃程度)までの範囲内
の85℃の温度下において、駆動電流を、1万時間とい
うような長時間に亘り、各半導体レ―ザから光出力が1
0mWの一定値で得られるように通電し、その駆動電流
の経時変化を測定したところ、上述した半導体レ―ザの
判別基準による良であるとして判別された半導体レ―ザ
については、駆動電流の経時変化が、図4中実線図示の
ように、5000時間以上経過してもほとんど生じず、
よって寿命時間が10万時間以上であると推定され、上
述した半導体レ―ザの判別基準による否(不良)である
として判別された半導体レ―ザについては、駆動電流の
経時変化が、図4中点線図示のように、5000時間に
到るまでにも大きく生じ、寿命時間がたかだか2万時間
程度であると推定される、という結果が得られた。
The above is the embodiment of the pass / fail judgment method of the semiconductor laser according to the present invention. According to the embodiment of the method for determining the acceptability of the semiconductor laser according to the present invention, the five semiconductor lasers determined to be good according to the above-described criteria for determining the semiconductor laser and For each of the five semiconductor lasers judged to be defective (defective) according to the above-mentioned semiconductor laser discrimination criteria, the semiconductor laser can oscillate from a temperature of 70 ° C. which is sufficiently higher than room temperature. At a temperature of 85 ° C, which is within the maximum temperature (usually about 180 ° C), the optical output from each semiconductor laser is 1 for a long time such as 10,000 hours.
When current was applied so that a constant value of 0 mW was obtained and the change over time of the drive current was measured, for the semiconductor laser that was determined to be good by the above-mentioned semiconductor laser determination criteria, the drive current of As shown by the solid line in FIG. 4, the change with time hardly occurs after 5000 hours or more,
Therefore, with respect to the semiconductor laser which is estimated to have a life time of 100,000 hours or more and is judged to be non-defective (defective) according to the above-mentioned semiconductor laser judgment criteria, the change over time of the driving current is shown in FIG. As shown by the middle dotted line, the result is that the large occurrence occurs up to 5000 hours and the life time is estimated to be about 20,000 hours at most.

【0012】このことからも、本発明による半導体レ―
ザの良否判別法の実施の形態によれば、半導体レ―ザの
良否を、[従来の技術]の項で上述した半導体レ―ザの
判別基準によって、判別することができることは明らか
である。
Also from this, the semiconductor laser according to the present invention is
According to the embodiment of the quality judgment method for the laser, it is clear that the quality of the semiconductor laser can be judged by the judgment standard of the semiconductor laser described in the section [Prior Art].

【0013】また、本発明による半導体レ―ザの良否判
別法の実施の形態において、第1の温度下及び第2の温
度下の半導体レ―ザの電流−電圧特性の各別の測定は、
第1の温度下であれ、第2の温度下であれ、それ自体公
知の方法によって、容易に行うことができるとともに、
その測定に長い時間を要さず、また、第1の温度下での
電流−電圧特性の測定結果から半導体レ―ザの閾値電流
またはその近傍における抵抗値を求めるのも、また、第
2の温度下での電流−電圧特性の測定結果から半導体レ
―ザの閾値電流またはその近傍における抵抗値を求める
のも、それ自体公知の方法によって、容易であるととも
に長い時間を要さず、さらに、第1の温度下での電流−
電圧特性の測定結果から求められる半導体レ―ザの閾値
電流またはその近傍における抵抗値と第2の温度下での
電流−電圧特性の測定結果から求められる半導体レ―ザ
の閾値電流またはその近傍における抵抗値との差として
の抵抗値差を求めることも長い時間を要さずに容易であ
り、さらに、抵抗値差を、図2及び図3に示す電流−抵
抗値特性からも明らかなように、大きな値で得ることが
できるので、その抵抗値差からの半導体レ―ザの良否の
判別を、容易、迅速に行うことができる。
Further, in the embodiment of the method for determining the quality of the semiconductor laser according to the present invention, the respective measurements of the current-voltage characteristics of the semiconductor laser under the first temperature and the second temperature are
Whether under the first temperature or the second temperature, it can be easily carried out by a method known per se, and
It does not require a long time for the measurement, and the resistance value at or near the threshold current of the semiconductor laser can be obtained from the measurement result of the current-voltage characteristics under the first temperature. It is easy and long time is not required to obtain the resistance value at or near the threshold current of the semiconductor laser from the measurement result of the current-voltage characteristic under temperature, and it is easy and does not require a long time. Current under the first temperature −
The resistance value at or near the threshold current of the semiconductor laser obtained from the measurement result of the voltage characteristic and the threshold current at or near the threshold current of the semiconductor laser obtained from the measurement result of the current-voltage characteristic at the second temperature It is easy to obtain a resistance value difference as a difference from the resistance value without requiring a long time, and further, the resistance value difference can be seen from the current-resistance value characteristics shown in FIGS. 2 and 3. Since it can be obtained with a large value, the quality of the semiconductor laser can be easily and quickly determined from the difference in resistance value.

【0014】従って、本発明による半導体レ―ザの良否
判別法の実施の形態によれば、半導体レ―ザの電流−電
圧特性の測定、その測定結果を用いた半導体レ―ザの良
否の判別という、測定及び判別の外、従来の半導体レ―
ザの良否判別法の場合のように半導体レ―ザに対する駆
動電流の通電を行う、という必要なしに、半導体レ―ザ
の良否の判別を、短い時間で、簡易に行うことができ
る。
Therefore, according to the embodiment of the semiconductor laser pass / fail judgment method according to the present invention, the current-voltage characteristic of the semiconductor laser is measured, and the pass / fail judgment of the semiconductor laser is made by using the measurement result. In addition to measurement and discrimination, the conventional semiconductor laser
It is possible to easily determine the quality of the semiconductor laser in a short time without the need of supplying the drive current to the semiconductor laser as in the case of the quality determination method of the laser.

【0015】なお、上述においては、半導体レ―ザの電
流−電圧特性の測定時の第1及び第2の温度を室温(2
5℃)及び85℃とした場合について述べたが、第1の
温度については、室温(25℃)であるのが温度制御を
伴うことなしに容易に得られるので望ましいが、第2の
温度については、半導体レ―ザがレーザ発振可能な最高
温度(通常180℃)以下であって第1の温度との間に
40℃〜50℃以上の差を有する温度であれば、上述し
た抵抗値差を比較的大きな値で得ることができるので、
85℃に限る必要はなく、第1及び第2の温度がこのよ
うな温度であっても、上述した本発明による半導体レ―
ザの良否判別法の実施の形態の特徴が得られることは明
らかであろう。その他、本発明の精神を脱することなし
に種々の変型、変更をなし得るであろう。
In the above description, the first and second temperatures at the time of measuring the current-voltage characteristics of the semiconductor laser are set to room temperature (2
5 ° C.) and 85 ° C., the first temperature is preferably room temperature (25 ° C.) because it can be easily obtained without any temperature control. Is the maximum temperature (usually 180 ° C.) at which the semiconductor laser can oscillate and is a temperature having a difference of 40 ° C. to 50 ° C. or more from the first temperature, the above-mentioned resistance difference. Can be obtained with a relatively large value,
It is not necessary to limit the temperature to 85 ° C., and even if the first and second temperatures are such temperatures, the semiconductor laser according to the present invention described above is used.
It will be apparent that the characteristics of the embodiment of the quality determination method of Z can be obtained. Besides, various modifications and changes may be made without departing from the spirit of the present invention.

【0016】[0016]

【発明の効果】本発明による半導体レ―ザの良否判別法
によれば、半導体レ―ザの電流−電圧特性の測定、その
測定結果を用いた半導体レ―ザの良否の判別という、測
定及び判別の外、従来の半導体レ―ザの良否判別法の場
合のように半導体レ―ザに対する駆動電流の通電を行
う、という必要なしに、半導体レ―ザの良否の判別を、
簡易、迅速に行うことができる。
According to the method for determining the quality of a semiconductor laser according to the present invention, the current-voltage characteristics of the semiconductor laser are measured, and the quality of the semiconductor laser is determined using the measurement results. In addition to the determination, it is possible to determine whether the semiconductor laser is good or bad without the need to energize the semiconductor laser with a drive current as in the case of the conventional semiconductor laser quality determination method.
It can be done simply and quickly.

【図面の簡単な説明】[Brief description of drawings]

【図1】本発明による半導体レ―ザの良否判別法の実施
の形態の説明に供する、良であると判別される半導体レ
―ザ及び不良であると判別される半導体レ―ザの電流−
電圧特性、及び電流−抵抗特性を一般に示す図である。
FIG. 1 is a view for explaining an embodiment of a method for determining pass / fail of a semiconductor laser according to the present invention, and a current of a semiconductor laser determined to be good and a current of a semiconductor laser determined to be defective.
It is a figure which generally shows a voltage characteristic and a current-resistance characteristic.

【図2】本発明による半導体レ―ザの良否判別法の実施
の形態の説明に供する、良であると判別される半導体レ
―ザの25℃及び85℃の温度下での電流−電圧特性及
び電流−抵抗特性を示す図である。
FIG. 2 is a current-voltage characteristic at 25 ° C. and 85 ° C. of a semiconductor laser that is determined to be good, which is used for explaining an embodiment of a method for determining whether the semiconductor laser is good or bad according to the present invention. It is a figure which shows and a current-resistance characteristic.

【図3】本発明による半導体レ―ザの良否判別法の実施
の形態の説明に供する、不良であると判別される半導体
レ―ザの25℃及び85℃の温度下での電流−電圧特性
及び電流−抵抗特性を示す図である。
FIG. 3 is a current-voltage characteristic at temperatures of 25 ° C. and 85 ° C. of a semiconductor laser that is determined to be defective, which is used for explaining an embodiment of a method for determining pass / fail of a semiconductor laser according to the present invention. It is a figure which shows and current-resistance characteristic.

【図4】本発明による半導体レ―ザの良否判別法の実施
の形態の説明に供する、半導体レ―ザに対する通電時間
に対する駆動電流の関係で示す駆動電流の、経時変化を
示す図である。
FIG. 4 is a diagram for explaining an embodiment of a method for determining pass / fail of a semiconductor laser according to the present invention, which is a diagram showing a change with time of a drive current represented by a relationship between a drive current and an energization time with respect to the semiconductor laser.

───────────────────────────────────────────────────── フロントページの続き (56)参考文献 特開 平9−113359(JP,A) 特開 昭61−84888(JP,A) 特開 昭64−9682(JP,A) 特開 平3−131737(JP,A) 特開 昭50−128978(JP,A) 特開 昭52−156589(JP,A) 特開 昭62−8583(JP,A) 特開 昭60−186078(JP,A) 特開 昭61−290372(JP,A) 特開 平9−186402(JP,A) 特開 昭57−48665(JP,A) 特開 平10−160785(JP,A) 特開 平7−115251(JP,A) 特開 平4−184175(JP,A) 実開 昭61−203575(JP,U) 特表 昭63−500279(JP,A) (58)調査した分野(Int.Cl.7,DB名) H01S 5/00 ─────────────────────────────────────────────────── ─── Continuation of the front page (56) Reference JP-A-9-113359 (JP, A) JP-A-61-84888 (JP, A) JP-A-64-9682 (JP, A) JP-A-3- 131737 (JP, A) JP 50-128978 (JP, A) JP 52-156589 (JP, A) JP 62-8583 (JP, A) JP 60-186078 (JP, A) JP-A 61-290372 (JP, A) JP-A 9-186402 (JP, A) JP-A 57-48665 (JP, A) JP-A 10-160785 (JP, A) JP-A 7-115251 (JP, A) JP-A-4-184175 (JP, A) Actual development Sho 61-203575 (JP, U) Special table Sho 63-500279 (JP, A) (58) Fields investigated (Int. Cl. 7) , DB name) H01S 5/00

Claims (2)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】半導体レ―ザの電流−電圧特性の測定を、
第1の温度下と、上記第1の温度に比し高い第2の温度
下とで各別に行い、 上記第1の温度下での電流−電圧特性の測定結果から、
上記半導体レ―ザの閾値電流またはその近傍における抵
抗値を求めるとともに、上記第2の温度下での電流−電
圧特性の測定結果から、上記半導体レ―ザの閾値電流ま
たはその近傍における抵抗値を求め、 上記第1の温度下での電流−電圧特性の測定結果から求
められる上記閾値電流またはその近傍における抵抗値と
上記第2の温度下での電流−電圧特性の測定結果から求
められる上記閾値電流またはその近傍における抵抗値と
の差を抵抗値差とし、その抵抗値差が、予定値を超える
か否かによって、上記半導体レ―ザの良否を判別するこ
とを特徴とする半導体レ―ザの良否判別法。
1. A method for measuring current-voltage characteristics of a semiconductor laser,
The measurement is performed separately under the first temperature and the second temperature higher than the first temperature, and from the measurement result of the current-voltage characteristics under the first temperature,
The resistance value at or near the threshold current of the semiconductor laser is obtained, and the resistance value at or near the threshold current of the semiconductor laser is calculated from the measurement result of the current-voltage characteristics under the second temperature. The threshold value obtained from the measurement result of the current-voltage characteristic under the first temperature and the threshold value obtained from the measurement result of the current-voltage characteristic under the second temperature and the resistance value at or near the threshold current. A semiconductor laser, characterized in that a difference between a current and a resistance value in the vicinity thereof is defined as a resistance value difference, and whether the semiconductor laser is good or bad is determined by whether or not the resistance value difference exceeds a predetermined value. How to judge pass / fail.
【請求項2】請求項1記載の半導体レ―ザの良否判別法
において、 上記第1の温度を室温(25℃)とし、 上記第2の温度を、半導体レ―ザのレーザ発振可能最高
温度以下であって、上記第1の温度との間で40℃〜5
0℃以上の差を有する温度であることを特徴とする半導
体レ―ザの良否判別法。
2. The method for determining the acceptability of a semiconductor laser according to claim 1, wherein the first temperature is room temperature (25 ° C.), and the second temperature is the maximum laser oscillation temperature of the semiconductor laser. 40 ° C to 5 ° C between the first temperature and the following.
A method for determining the quality of a semiconductor laser, which is characterized in that the temperatures have a difference of 0 ° C. or more.
JP02767098A 1998-02-09 1998-02-09 Pass / fail judgment method of semiconductor laser Expired - Fee Related JP3535002B2 (en)

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