Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JP2716068B2 - Semiconductor device - Google Patents
[go: Go Back, main page]

JP2716068B2 - Semiconductor device - Google Patents

Semiconductor device

Info

Publication number
JP2716068B2
JP2716068B2 JP29909888A JP29909888A JP2716068B2 JP 2716068 B2 JP2716068 B2 JP 2716068B2 JP 29909888 A JP29909888 A JP 29909888A JP 29909888 A JP29909888 A JP 29909888A JP 2716068 B2 JP2716068 B2 JP 2716068B2
Authority
JP
Japan
Prior art keywords
light
solar cell
semiconductor
semiconductor device
temperature
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 - Lifetime
Application number
JP29909888A
Other languages
Japanese (ja)
Other versions
JPH02144975A (en
Inventor
恵昭 友成
淳 阪井
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.)
Panasonic Electric Works Co Ltd
Original Assignee
Matsushita Electric Works Ltd
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 Matsushita Electric Works Ltd filed Critical Matsushita Electric Works Ltd
Priority to JP29909888A priority Critical patent/JP2716068B2/en
Publication of JPH02144975A publication Critical patent/JPH02144975A/en
Application granted granted Critical
Publication of JP2716068B2 publication Critical patent/JP2716068B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Landscapes

  • Photo Coupler, Interrupter, Optical-To-Optical Conversion Devices (AREA)
  • Led Device Packages (AREA)
  • Led Devices (AREA)

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は、半導体発光素子と、この発光素子の光を
受ける半導体受光素子とを備えた半導体装置に関する。
Description: BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a semiconductor device including a semiconductor light emitting element and a semiconductor light receiving element that receives light from the light emitting element.

〔従来の技術〕[Conventional technology]

従来、半導体発光素子と、この発光素子の光を受けて
電流を出力をする半導体受光素子とを備えるとともに、
この受光素子の出力により駆動される半導体素子をさら
に備えた半導体装置がある。この種の装置では、半導体
発光素子と半導体受光素子とが透明(光透過)性絶縁層
を介して光の授受を行っており、そのため、半導体発光
素子と半導体受光素子とを電気的に完全に分離すること
ができるという特徴がある。
Conventionally, a semiconductor light-emitting element, and a semiconductor light-receiving element that receives the light of this light-emitting element and outputs a current,
There is a semiconductor device further provided with a semiconductor element driven by the output of the light receiving element. In this type of device, the semiconductor light emitting element and the semiconductor light receiving element transmit and receive light via a transparent (light transmitting) insulating layer. Therefore, the semiconductor light emitting element and the semiconductor light receiving element are completely electrically connected. It has the characteristic that it can be separated.

前記のような半導体装置の一例として、赤外LED(発
光素子)、単結晶シリコン太陽電池(受光素子)、FET
(半導体素子)の組み合わせがある。
Examples of the semiconductor device as described above include an infrared LED (light emitting element), a single crystal silicon solar cell (light receiving element), and an FET.
(Semiconductor elements).

この半導体装置では、入力信号を受けてFETがスイッ
チング動作する。すなわち、入力信号が赤外LEDに印加
されると、赤外LEDが発光し、この光は太陽電池に入
る。光を受けた太陽電池では光起電力が発生する。太陽
電池はFETのゲート・ソース間に接続されていて、起電
力がゲート・ソース間に加わり、これによりFETのソー
ス・ドレイン間が導通してスイッチオンの状態となる。
In this semiconductor device, the FET performs a switching operation in response to an input signal. That is, when an input signal is applied to the infrared LED, the infrared LED emits light, which enters the solar cell. A photovoltaic power is generated in a solar cell that receives light. The solar cell is connected between the gate and the source of the FET, and an electromotive force is applied between the gate and the source, thereby conducting between the source and the drain of the FET to be turned on.

〔発明が解決しようとする課題〕[Problems to be solved by the invention]

従来の半導体装置は、入力信号を受けてからターン・
オフ状態となるまでの時間(応答速度)が温度変化に伴
って変動し、安定しない。
Conventional semiconductor devices turn on after receiving an input signal.
The time (response speed) until the device is turned off fluctuates with a change in temperature and is not stable.

応答速度の不安定は、太陽電池の出力電流が温度変化
に伴って大きく変動することに起因している。すなわ
ち、従来の半導体装置における赤外LEDと単結晶シリコ
ン太陽電池の組み合せでは、太陽電池の出力電流が温度
変化に伴って大幅に変動するのである。赤外LEDの波長
は単結晶シリコン太陽電池の感度がピークとなる波長に
合わせられているが、この場合、赤外LEDの光出力量の
変動がそのまま太陽電池の出力電流の変動となってあら
われる。赤外LEDの光出力の変動量は、室温(25℃)か
ら80℃に上昇した場合に40%低下し、これを受けて単結
晶シリコン太陽電池も出力電流が40%ほど低下する。
The instability of the response speed is due to the fact that the output current of the solar cell fluctuates greatly with a change in temperature. That is, in the combination of an infrared LED and a single-crystal silicon solar cell in a conventional semiconductor device, the output current of the solar cell fluctuates greatly with a change in temperature. The wavelength of the infrared LED is tuned to the wavelength at which the sensitivity of the single crystal silicon solar cell peaks, but in this case, the fluctuation of the light output of the infrared LED directly appears as the fluctuation of the output current of the solar cell . The variation of the light output of the infrared LED decreases by 40% when the temperature rises from room temperature (25 ° C.) to 80 ° C. In response, the output current of the single crystal silicon solar cell also drops by about 40%.

一方、入力信号を受けて起電力が発生した当初、FET
のゲート・ソース間には大きな電圧が直ちにかかるので
はなく、太陽電池からの出力電流がゲート・ソース間容
量(静電容量)を充電するにつれ徐々に太陽電池の起電
力の電圧へと近づいてゆく。もちろん、太陽電池の出力
電流が多い程、FETをターン・オン状態にすることので
きる電圧に短い時間で到達する。したがって、上記のよ
うに太陽電池の出力電流が減少すると、ゲート・ソース
間容量の充電に時間がかかり、その分、ターン・オン状
態になるのが遅れる。
On the other hand, when an electromotive force is generated in response to an input signal,
A large voltage is not immediately applied between the gate and the source of the solar cell, but the output current from the solar cell gradually approaches the voltage of the electromotive force of the solar cell as the capacity (capacitance) between the gate and the source is charged. go. Of course, the higher the output current of the solar cell, the sooner it will reach the voltage at which the FET can be turned on. Therefore, when the output current of the solar cell decreases as described above, it takes time to charge the gate-source capacitance, and the turn-on state is delayed accordingly.

以上のように、従来の半導体装置では、温度が上がる
と応答速度が遅くなるのである。
As described above, in the conventional semiconductor device, the response speed decreases as the temperature increases.

この発明の目的は、温度変化に伴う出力変動の少ない
特性を有する半導体装置を提供することにある。
SUMMARY OF THE INVENTION An object of the present invention is to provide a semiconductor device having a characteristic in which output fluctuation due to a temperature change is small.

〔課題を解決するための手段〕[Means for solving the problem]

本発明に係る半導体装置は、半導体受光素子と半導体
発光素子とを有している。半導体受光素子は、所定の波
長領域で、受光する光の波長が増大するに伴って受光感
度が減少し、かつその受光感度特性が温度上昇に伴って
長波長側にずれるような構成の素子である。半導体発光
素子は、所定の波長領域に発光のピークを有するととも
に、温度上昇に伴って光出力量が減少し、受光素子に対
して光を出力するものである。
A semiconductor device according to the present invention has a semiconductor light receiving element and a semiconductor light emitting element. A semiconductor light receiving element is an element having a configuration in which, in a predetermined wavelength region, the light receiving sensitivity decreases as the wavelength of the received light increases, and the light receiving sensitivity characteristic shifts to a longer wavelength side with an increase in temperature. is there. The semiconductor light emitting element has a light emission peak in a predetermined wavelength region, and the light output amount decreases with an increase in temperature, and outputs light to the light receiving element.

なお、前記発光素子が、LED、半導体レーザ及びエレ
クトロルミネッセンス素子からなる群のうちのひとつで
あって約550nm〜800nmの波長範囲に発光のピークを有
し、前記受光素子が、アモルファスシリコンからなる太
陽電池であるのが好ましい。
The light-emitting element is one of a group consisting of an LED, a semiconductor laser, and an electroluminescence element, has a light emission peak in a wavelength range of about 550 nm to 800 nm, and the light-receiving element is a solar cell made of amorphous silicon. Preferably, it is a battery.

また、前記発光素子が、600nm付近に発光のピークを
有する赤色LEDであり、前記受光素子が、約600nm〜約70
0nmの波長範囲において波長の増加に伴い受光感度が減
少する感度特性を示すアモルファスシリコンからなる太
陽電池であることが好ましい。
Further, the light emitting element is a red LED having a light emission peak near 600 nm, and the light receiving element is about 600 nm to about 70 nm.
It is preferable that the solar cell is made of amorphous silicon and has a sensitivity characteristic in which the light receiving sensitivity decreases as the wavelength increases in the wavelength range of 0 nm.

さらに、前記受光素子の出力により駆動される半導体
素子をさらに備えていてもよい。
Further, the semiconductor device may further include a semiconductor element driven by an output of the light receiving element.

〔作用〕[Action]

本発明に係る半導体装置では、半導体発光素子(以
下、単に発光素子と記す)の温度変化に伴う光出力変動
と、半導体受光素子(以下、単に受光素子と記す)の温
度変化に伴う受光感度変動が、逆であるような素子を用
いて、結果として、受光素子の出力が温度変化に対して
あまり変動しなくなるようにしている。このため、半導
体装置の出力の温度特性が向上する。
In the semiconductor device according to the present invention, the light output fluctuation due to the temperature change of the semiconductor light emitting element (hereinafter simply referred to as light emitting element) and the light receiving sensitivity fluctuation due to the temperature change of the semiconductor light receiving element (hereinafter simply referred to as light receiving element). However, by using an element that is the opposite, as a result, the output of the light receiving element does not fluctuate much with a change in temperature. Therefore, the temperature characteristics of the output of the semiconductor device are improved.

受光素子は、発光素子の光の波長を含む領域におい
て、波長の増大に伴って受光感度が減少する感度特性を
有し、かつこの温度特性が温度上昇に伴って長波長側に
ずれる(温度変化によって光学的禁制帯Egoptが変化す
る)ような構成となっているので、温度上昇に伴って受
光感度が増大する。この受光感度の増大で、発光素子の
方の温度上昇に伴う光出力量の減少分が補われることと
なり、全体としての変動が抑えられる。
The light receiving element has a sensitivity characteristic in which the light receiving sensitivity decreases with an increase in the wavelength in a region including the wavelength of the light of the light emitting element, and the temperature characteristic shifts to a longer wavelength side with an increase in temperature (temperature change). The optical forbidden band Egopt changes), so that the light receiving sensitivity increases as the temperature rises. The increase in the light receiving sensitivity compensates for the decrease in the light output amount due to the temperature rise in the light emitting element, and suppresses the fluctuation as a whole.

発光素子としては、LED、半導体レーザ及びエレクト
ロルミネッセンス素子等が用いられ、受光素子としては
太陽電池等が用いられるが、LEDが赤色LEDであり、太陽
電池がアモルファスシリコンからなる太陽電子である場
合は、温度特性の改善の度合いが大きい。
As the light emitting element, an LED, a semiconductor laser, an electroluminescence element, or the like is used.As the light receiving element, a solar cell or the like is used.If the LED is a red LED and the solar cell is a solar electron made of amorphous silicon, The degree of improvement in temperature characteristics is large.

特に、発光素子が、LED、半導体レーザ及びエレクト
ロルミネッセンス素子からなる群のうちのひとつであっ
て約550nm〜800nmの波長範囲に発光のピークを有し、受
光素子が、アモルファスシリコンからなる太陽電池であ
れば、受光素子の出力変動をより抑えられる。
In particular, the light emitting element is one of a group consisting of an LED, a semiconductor laser, and an electroluminescent element, has a light emission peak in a wavelength range of about 550 nm to 800 nm, and the light receiving element is a solar cell made of amorphous silicon. If it is, the output fluctuation of the light receiving element can be further suppressed.

また、発光素子が、600nm付近に発光のピークを有す
る赤色LEDであり、受光素子が、約600nm〜約700nmの波
長範囲において波長の増加に伴い受光感度が減少する感
度特性を示すアモルファスシリコンからなる太陽電池で
ある場合は、前記同様に、受光素子の出力変動をより抑
えられる。
The light-emitting element is a red LED having an emission peak near 600 nm, and the light-receiving element is made of amorphous silicon exhibiting sensitivity characteristics in which the light-receiving sensitivity decreases with an increase in wavelength in a wavelength range of about 600 nm to about 700 nm. In the case of a solar cell, the output fluctuation of the light receiving element can be further suppressed as described above.

さらに、受光素子の出力により駆動される半導体素子
をさらに備えていれば、改めて半導体素子を用意したり
接続したりする必要がなく、利用しやすい。
Furthermore, if a semiconductor element driven by the output of the light receiving element is further provided, there is no need to prepare or connect a semiconductor element again, and it is easy to use.

〔実施例〕〔Example〕

以下、この発明の半導体装置を、その一例をあらわす
図面を参照しながら詳しく説明する。
Hereinafter, a semiconductor device of the present invention will be described in detail with reference to the drawings showing an example thereof.

第1図(a)は本発明の一実施例に係る半導体装置の
回路図であり、同図(b)は概略断面図である。
FIG. 1A is a circuit diagram of a semiconductor device according to one embodiment of the present invention, and FIG. 1B is a schematic sectional view.

半導体装置1は、LED(発光ダイオード)L1、このLED
L1の光を受ける太陽電池DA1及び太陽電池DA1の出力でス
イッチング駆動されるように接続された電界効果トラン
ジスタTR1からなる。
The semiconductor device 1 includes an LED (light emitting diode) L 1 ,
Consisting field effect transistors connected TR 1 as switched driven by the output of the solar cell DA 1 and the solar cell DA 1 receives light L 1.

トランジスタTR1は半導体基板2に形成されていて、
太陽電池DA1(3)は絶縁層5を介して基板2の上に積
層形成されている。太陽電池DA1(3)とLEDL1(4)と
は、透明絶縁層6を間にしてLEDL1の光が太陽電池DA1
入るように向かい合っている。太陽電池DA1は出力電圧
を高くするために複数個が直列に接続されたアレイ構成
をとっている。
The transistor TR 1 is formed on the semiconductor substrate 2,
The solar cell DA 1 (3) is formed on the substrate 2 with the insulating layer 5 interposed therebetween. The solar cell DA 1 (3) and the LED L 1 (4) face each other with the transparent insulating layer 6 interposed therebetween so that light of the LED L 1 enters the solar cell DA 1 . Solar DA 1 has taken an array configuration in which a plurality are connected in series to increase output voltage.

この半導体装置1は、例えば次のようにして製造され
る。
The semiconductor device 1 is manufactured, for example, as follows.

トランジスタTR1が形成された半導体基板2の上に太
陽電池DA1(3)を積層形成したものと、別途に製造し
たLEDL1(4)とを、金型内に所定の間隔をあけた状態
で配置しておき、その間隙に透明樹脂等の透明絶縁材を
充填し一体化する。
A state in which a solar cell DA 1 (3) is laminated and formed on a semiconductor substrate 2 on which a transistor TR 1 is formed, and an LEDL 1 (4) manufactured separately are spaced apart in a mold by a predetermined distance. And the gap is filled with a transparent insulating material such as a transparent resin to be integrated.

入力端子T1、T2に電気入力信号が入力されると、LEDL
1が発光し、この光は太陽電池DA1に入る。光を受けた太
陽電池DA1では起電力が発生し、トランジスタTR1のゲー
ト・ソース間に電圧が印加され、これによりトランジス
タTR1がターン・オン状態となる。トランジスタTR1は太
陽電池DA1の出力によりスイッチング駆動される。
When an electric input signal is input to input terminals T 1 and T 2 , LEDL
1 emits light, the light enters the solar cell DA 1. In the solar cell DA 1 receives the light electromotive force is generated, the voltage between the gate and source of the transistor TR 1 is applied, thereby the transistor TR 1 is turned on state. Transistor TR 1 is switched driven by the output of the solar cell DA 1.

この半導体装置では、温度変化に伴う太陽電池DA1
出力電流変動が、従来のものに比べ著しく減少してい
る。
In this semiconductor device, the output current fluctuation of the solar cell DA 1 due to temperature changes, are significantly reduced compared with the conventional.

第3図の直線Cは実施例の半導体装置の太陽電池DA1
の出力電流と温度の関係をあらわし、同図の直線Dは従
来の半導体装置の太陽電池の出力電流と温度の関係をあ
らわしている。
The straight line C in FIG. 3 is the solar cell DA 1 of the semiconductor device of the embodiment.
Represents the relationship between the output current and the temperature, and the straight line D in the figure represents the relationship between the output current and the temperature of the solar cell of the conventional semiconductor device.

実施例の太陽電池では、出力電流変動が−0.44%/℃
であって、80℃での減少率は室温の場合に比べ約25%で
ある。一方、従来例の太陽電池では、出力電流変動が−
0.8%/℃であって、80℃での減少率は約40%を越え
る。このように実施例の太陽電池では、変動が従来のそ
れの約半分になっている。
In the solar cell of the embodiment, the output current fluctuation is −0.44% / ° C.
The reduction rate at 80 ° C. is about 25% compared to that at room temperature. On the other hand, in the conventional solar cell, the output current fluctuation is −
0.8% / ° C., the rate of reduction at 80 ° C. exceeds about 40%. As described above, in the solar cell of the embodiment, the fluctuation is about half that of the conventional solar cell.

実施例の太陽電池DA1の出力電流の温度変化に伴う変
動が減少する点について、さらに詳しく説明する。
For that variation due to the temperature change of the output current of the solar cell DA 1 in the embodiment is reduced will be described in more detail.

上記LEDL1は約660nmの波長に鋭い発光ピークのある赤
色LEDである。このLEDL1の発光量と温度の関係みると、
第4図の直線Eに示されるように、20℃を基準として、
−20℃〜80℃の温度変化に対し、光量が150%から60%
へと急激に減少していく。すなわち、LEDL1の光出力量
は温度上昇に伴って急激に減少する(負の変化をす
る)。
It said LEDL 1 is a red LED with a sharp emission peak at a wavelength of approximately 660 nm. Looking at the relationship between the light emission amount and temperature of this LEDL 1 ,
As shown by the straight line E in FIG.
Light intensity from 150% to 60% for temperature changes from -20 ° C to 80 ° C
It rapidly decreases to. That is, the light output of LEDL 1 is (a negative change) that decreases rapidly with increasing temperature.

一方、太陽電池DA1はアモルファスシリコンからなる
太陽電池である。この太陽電池DA1は、第2図の曲線
A、Bに示されるように、LEDL1の光の波長(660nm)の
ある約600nm〜約700nmの波長では、波長の増加に伴い受
光感度が急激に減少する。第2図では、曲線Aが温度T1
での分光感度特性をあらわし、第2図の曲線Bが温度T2
(T1<T2)での分光感度特性をあらわしており、この太
陽電池DA1の場合、温度上昇につれ光学的禁制帯巾Egopt
の巾が減少して分光感度特性が長波長側にずれるような
構成となっている。そのため、LEDL1の光の波長でみる
と、温度T1では感度A1であるのに対し、温度T2では感度
B1と温度上昇に伴い感度が向上する。もちろん、温度が
下がると分光感度特性は逆に短波長側にずれる。
Meanwhile, solar cell DA 1 is a solar cell made of amorphous silicon. As shown by curves A and B in FIG. 2, this solar cell DA 1 has a light receiving sensitivity that increases sharply with an increase in wavelength at a wavelength of about 600 nm to about 700 nm, which is the light wavelength (660 nm) of LED L 1. To decrease. In FIG. 2, curve A represents temperature T 1.
The curve B in FIG. 2 shows the spectral sensitivity characteristic at the temperature T 2
(T 1 <T 2 ). In the case of this solar cell DA 1 , the optical bandgap Egopt increases as the temperature rises.
Is reduced so that the spectral sensitivity characteristic shifts to the longer wavelength side. Therefore, when viewed at a wavelength of light LEDL 1, whereas the sensitivity A 1 in the temperature T 1, the temperature T 2 sensitivity
Sensitivity is enhanced with the B 1 and the temperature rise. Of course, as the temperature decreases, the spectral sensitivity characteristic shifts to the shorter wavelength side.

ここで、LEDL1の光源の光量を一定に保っておき、太
陽電池DA1の温度だけを−40℃〜80℃まで変化させた場
合の出力電流の変化を第5図の直線Fに示す。この第5
図の直線Fから明らかなように、温度変化に対して出力
電流は、20℃を基準にして60%から150%(基準は20
℃)へと急激に増加している(正の変化をする)。
Here, previously kept constant the light quantity of the light source LEDL1, shows the change in the output current in the case of changing only the temperature of the solar cell DA 1 to -40 ° C. to 80 ° C. in a straight line F of FIG. 5. This fifth
As is clear from the straight line F in the figure, the output current with respect to the temperature change is 60% to 150% based on 20 ° C (the standard is 20%).
° C) (with a positive change).

正の変化をするこの太陽電池DA1と負の変化をする先
のLEDL1を組み合わせれば、温度変化に伴う互いの変動
が相殺され、温度変化があっても太陽電池DA1の出力電
流の変動は抑えられる。
By combining this solar cell DA 1 that makes a positive change and the LEDL 1 that makes a negative change, the mutual fluctuation due to the temperature change is canceled out, and even if there is a temperature change, the output current of the solar cell DA 1 Fluctuations are suppressed.

したがって、起電力発生当初のゲート・ソース間容量
(第1図(a)にコンデンサC1で示す)の充電の様子
は、温度が変化しても変化が少ない。そのため、入力信
号を受けた後、ターン・オン状態となるまでの時間が略
一定となり、温度変化にかかわらず応答速度が安定す
る。
Thus, state of charge of the electromotive force generated initial gate-source capacitance (indicated by the capacitor C 1 in FIG. 1 (a)) is less changed even if the temperature changes. Therefore, the time from when the input signal is received to when the turn-on state is attained becomes substantially constant, and the response speed becomes stable regardless of the temperature change.

〔他の実施例〕[Other embodiments]

発光素子や受光素子は上記例示のものに限らない。 The light emitting element and the light receiving element are not limited to those described above.

但し、発光素子は発光ピークが急峻な単色性の強い光
源が利用し易い。例えば、上記実施例では、LEDが660nm
付近に発光ピークをもつものであったが、アモルファス
シリコンからなる太陽電池の場合、約550nm〜800nmの波
長範囲に発光ピークをもつものであれば、例示の赤色LE
Dに近い特性の半導体装置となる。もちろん、太陽電池
がアモルファスシリコン以外の材料からなるものであっ
てもよい。
However, it is easy to use a light source having a strong monochromaticity with a sharp emission peak. For example, in the above embodiment, the LED is 660 nm
Although it had an emission peak in the vicinity, in the case of a solar cell made of amorphous silicon, if it has an emission peak in a wavelength range of about 550 nm to 800 nm, the exemplary red LE
The semiconductor device has characteristics close to D. Of course, the solar cell may be made of a material other than amorphous silicon.

また、上記実施例では、表面に受光素子が積層され半
導体素子の形成された半導体基板と、別途に製造された
発光素子とを金型内で透明樹脂を用いて結合するように
して製造したが、これに限らず半導体素子の形成された
半導体基板上に絶縁層、受光素子、透明絶縁層、発光素
子と順次積層形成していくようにして製造してもよい。
Further, in the above embodiment, the light receiving element is laminated on the surface, and the semiconductor substrate on which the semiconductor element is formed, and the separately manufactured light emitting element are manufactured in such a manner that the light emitting element is bonded using a transparent resin in a mold. However, the present invention is not limited to this, and an insulating layer, a light receiving element, a transparent insulating layer, and a light emitting element may be sequentially laminated and formed on a semiconductor substrate on which a semiconductor element is formed.

さらに、半導体装置が、受光素子の出力で駆動される
半導体素子を備えておらず、発光素子と受光素子とから
なる構成であっても、OEIC(Opt Electric Integrated
Circuit)等、広い分野に応用が可能である。
Furthermore, even if the semiconductor device does not include a semiconductor element driven by the output of the light receiving element and is configured by a light emitting element and a light receiving element, the OEIC (Opt Electric Integrated
Circuit).

〔発明の効果〕〔The invention's effect〕

以上のように本発明に係る半導体装置では、発光素子
の温度変化に伴う光出力の変動と、受光素子の温度変化
に伴う出力変動とが互いに相殺されるため、出力温度特
性が優れる。
As described above, in the semiconductor device according to the present invention, the change in the optical output due to the temperature change of the light emitting element and the change in the output due to the temperature change of the light receiving element cancel each other, so that the output temperature characteristics are excellent.

また、発光素子あるいは受光素子として特定の構造及
び特定の波長範囲において特定の感度特性を有するもの
を用いることにより、発光素子と受光素子の温度特性と
が適切に対応して、受光素子の出力変動を抑えることが
できる。
In addition, by using a light-emitting element or a light-receiving element having a specific structure and a specific sensitivity characteristic in a specific wavelength range, the temperature characteristics of the light-emitting element and the light-receiving element appropriately correspond, and the output fluctuation of the light-receiving element is Can be suppressed.

さらに、受光素子の出力で駆動される半導体素子をさ
らに備えた場合には、利用しやすい。
Further, when a semiconductor element driven by the output of the light receiving element is further provided, it is easy to use.

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

第1図(a)は本発明の一実施例に係る半導体装置の電
気回路図、第1図(b)はその概略断面図、第2図は前
記半導体装置の太陽電池の分光感度特性をあらわす図、
第3図は前記半導体装置及び従来の半導体装置のそれぞ
れの太陽電池の出力電流と温度の関係をあらわす図、第
4図は前記半導体装置のLEDの光出力量と温度の関係を
あらわす図、第5図は前記実施例の太陽電池におけるLE
Dの発光する光の波長での温度と感度の関係をあらわす
図である。 1……半導体装置、L1……LED(発光素子)、DA1……太
陽電池(受光素子)、TR1……トランジスタ(半導体素
子)
FIG. 1A is an electric circuit diagram of a semiconductor device according to an embodiment of the present invention, FIG. 1B is a schematic sectional view thereof, and FIG. 2 shows a spectral sensitivity characteristic of a solar cell of the semiconductor device. Figure,
FIG. 3 is a diagram showing the relationship between the output current and the temperature of each solar cell of the semiconductor device and the conventional semiconductor device. FIG. 4 is a diagram showing the relationship between the light output amount of the LED of the semiconductor device and the temperature. FIG. 5 shows the LE in the solar cell of the above embodiment.
FIG. 6 is a diagram illustrating a relationship between temperature and sensitivity at a wavelength of light emitted by D. 1 ...... semiconductor device, L 1 ...... LED (light emitting element), DA 1 ...... solar cell (light receiving element), TR 1 ...... transistor (semiconductor device)

───────────────────────────────────────────────────── フロントページの続き (56)参考文献 特開 昭58−106878(JP,A) 特開 昭58−225322(JP,A) 特開 昭54−114192(JP,A) 特開 昭60−250718(JP,A) 特開 昭58−100469(JP,A) 特開 昭58−101476(JP,A) ──────────────────────────────────────────────────続 き Continuation of the front page (56) References JP-A-58-1006878 (JP, A) JP-A-58-225322 (JP, A) JP-A-54-114192 (JP, A) JP-A Sho 60- 250718 (JP, A) JP-A-58-100469 (JP, A) JP-A-58-101476 (JP, A)

Claims (4)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】所定の波長領域で、受光する光の波長が増
大するに伴って受光感度が減少し、かつその受光感度特
性が温度上昇に伴って長波長側にずれる半導体受光素子
と、 前記所定の波長領域に発光のピークを有するとともに、
温度上昇に伴って光出力量が減少し、前記受光素子に対
して光を出力する半導体発光素子と、 を備えた半導体装置。
A semiconductor light-receiving element in which light-receiving sensitivity decreases as the wavelength of light to be received increases in a predetermined wavelength region, and whose light-receiving sensitivity characteristic shifts to a longer wavelength side with an increase in temperature; While having an emission peak in a predetermined wavelength region,
A semiconductor device comprising: a semiconductor light emitting element that outputs light to the light receiving element, the amount of light output decreasing with an increase in temperature.
【請求項2】前記発光素子が、LED、半導体レーザ及び
エレクトロルミネッセンス素子からなる群のうちのひと
つであって約550nm〜800nmの波長範囲に発光のピークを
有し、 前記受光素子が、アモルファスシリコンからなる太陽電
池である、請求項1記載の半導体装置。
2. The light-emitting device according to claim 1, wherein the light-emitting device is one of a group consisting of an LED, a semiconductor laser, and an electroluminescence device, and has a light emission peak in a wavelength range of about 550 nm to 800 nm. The semiconductor device according to claim 1, wherein the semiconductor device is a solar cell.
【請求項3】前記発光素子が、600nm付近に発光のピー
クを有する赤色LEDであり、 前記受光素子が、約600nm〜約700nmの波長範囲において
波長の増加に伴い受光感度が減少する感度特性を示すア
モルファスシリコンからなる太陽電池である、請求項1
記載の半導体装置。
3. The light emitting device according to claim 1, wherein the light emitting device is a red LED having a light emission peak near 600 nm, and the light receiving device has a sensitivity characteristic in which the light receiving sensitivity decreases as the wavelength increases in a wavelength range of about 600 nm to about 700 nm. 2. A solar cell comprising the amorphous silicon shown in claim 1.
13. The semiconductor device according to claim 1.
【請求項4】前記受光素子の出力により駆動される半導
体素子をさらに備えている、請求項1から3のいずれか
に記載の半導体装置。
4. The semiconductor device according to claim 1, further comprising a semiconductor element driven by an output of said light receiving element.
JP29909888A 1988-11-25 1988-11-25 Semiconductor device Expired - Lifetime JP2716068B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP29909888A JP2716068B2 (en) 1988-11-25 1988-11-25 Semiconductor device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP29909888A JP2716068B2 (en) 1988-11-25 1988-11-25 Semiconductor device

Publications (2)

Publication Number Publication Date
JPH02144975A JPH02144975A (en) 1990-06-04
JP2716068B2 true JP2716068B2 (en) 1998-02-18

Family

ID=17868129

Family Applications (1)

Application Number Title Priority Date Filing Date
JP29909888A Expired - Lifetime JP2716068B2 (en) 1988-11-25 1988-11-25 Semiconductor device

Country Status (1)

Country Link
JP (1) JP2716068B2 (en)

Also Published As

Publication number Publication date
JPH02144975A (en) 1990-06-04

Similar Documents

Publication Publication Date Title
US3304431A (en) Photosensitive transistor chopper using light emissive diode
EP0048146B1 (en) Solid state optically coupled electrical switch
US4329625A (en) Light-responsive light-emitting diode display
US4847846A (en) Semiconductor laser chip
US4675518A (en) Optical bistable device
JP2716068B2 (en) Semiconductor device
CN111682399A (en) Laser transmitter drive circuit, system and high-speed optical communication device
KR100187388B1 (en) Phase-controllable optical coupling element
JPS58102576A (en) High voltage output optical coupling isolator
JP2015177204A (en) Semiconductor device, driver and semiconductor relay
JPS59171181A (en) Photo coupling device
JPS63283082A (en) Light-coupling semiconductor device
JPS6246290Y2 (en)
JPS6215925A (en) Semiconductor relay circuit
JPS5929471A (en) Substrate for thin film optical waveguide
Litovski 8 Optoelectronic Components
US3263085A (en) Radiation powered semiconductor devices
JP2000106523A (en) Semiconductor relay and method of manufacturing the same
JPH06151844A (en) Field effect transistor
JPH0758803B2 (en) Optical switching device
JPS6461966A (en) Photocoupler
JPH05335616A (en) High-speed photocoupler
JPS5821182Y2 (en) Photocoupler
JPS606112B2 (en) Semiconductor photosensitive light emitting device
JP3533921B2 (en) Electronic automatic flasher