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JP3668005B2 - Semiconductor light emitting device - Google Patents
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JP3668005B2 - Semiconductor light emitting device - Google Patents

Semiconductor light emitting device Download PDF

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Publication number
JP3668005B2
JP3668005B2 JP20843698A JP20843698A JP3668005B2 JP 3668005 B2 JP3668005 B2 JP 3668005B2 JP 20843698 A JP20843698 A JP 20843698A JP 20843698 A JP20843698 A JP 20843698A JP 3668005 B2 JP3668005 B2 JP 3668005B2
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Prior art keywords
wavelength
light emitting
light
transmittance
film
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JP20843698A
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JP2000040855A (en
Inventor
晋 西村
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Sanyo Electric Co Ltd
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Tottori Sanyo Electric Co Ltd
Sanyo Electric Co Ltd
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Description

【0001】
【発明の属する技術分野】
本発明は、半導体発光素子とその出力を受光する受光素子からなる半導体発光装置に関する。
【0002】
【従来の技術】
単一の波長もしくはそれに近い波長で発光することが要求される場合の光源として、半導体レーザ素子や光通信用発光ダイオード等の発光素子が利用される。そして一般に、発光素子の出力を一定に保つ場合は、発光素子の出力を受光素子で検知して発光素子の動作を制御する自動出力制御が行われる。
【0003】
ところで、半導体発光素子は、それ自体が動作することによる内部温度の上昇や、動作環境温度の変化等により、出力波長が微妙に変動するが、このような変動が前記自動出力制御に悪影響を及ぼすことがある。すなわち、受光素子の受光面には、透明な被膜が設けられており、この被膜を透過する光の量は波長によって変動する。温度変化によって波長が変動し、それによって被膜を透過する量が変動すると、受光素子の検知出力も変動し、感度があたかも温度によって変化したかのようになる。
【0004】
図2は、被膜(酸化シリコン)の膜厚(t)に対する、波長λ0(790nm)の光の透過率(a)、波長λ1(800nm)の光の透過率(b)、並びに波長λ1の透過率から波長λ0の透過率を引いた両波長の透過率の差(c)を示している。この透過率差(c)特性において、透過率差が負の値を示す膜厚においては、標準的な波長λ0が温度上昇によって波長λ1に変化すると、透過率が低下することを示しているが、受光素子の被膜がこのような膜厚に設定されていると、温度上昇によって受光出力が減少したというフィードバックが生じ、発光素子の駆動電流が増加する。その結果、発光素子の出力が増大するとともに、発光素子自体の劣化が誘発されやすくなる。
【0005】
また、半導体レーザ素子においては、駆動電流の増加によって出力が増加し、これにより自励発振が非自励発振となりやすく、このレーザ素子を光ピックアップ等に実装した場合に、記録媒体からの戻り光によるノイズが発生し易くなるという問題も生じる。
【0006】
【発明が解決しようとする課題】
本発明は上述の点を考慮し、温度上昇による影響を受けにくい半導体発光装置を提供することを課題の1つとする。また、温度上昇によって発光素子の波長が変動しても受光素子の検知出力が低下することがない半導体発光装置を提供することを課題の1つとする。また、半導体発光素子の劣化を防止することを課題の1つとする。また、半導体発光素子として半導体レーザを用いる場合は、その発振状態の変動を防止することを課題の1つとする。
【0007】
【課題を解決するための手段】
本発明の半導体発光装置は、標準波長がλ0に設定され、動作保障範囲の上限とされた温度における波長がλ1に変動する半導体発光素子と、該発光素子が出力する光を表面の被膜を介して受光する受光素子を備えた半導体発光装置において、前記発光素子の波長λ0の光と波長λ1の光が被膜を透過する透過率の差を被膜の厚さを変化させて求めて、その透過率差が正の範囲(正とは、波長がλ0からλ1に変動することによって被膜を通過する光の量が増加する場合)で、しかも、この透過率差が被膜の膜厚変動によって負の範囲に変動することを防止するように0と極大値の中間の値をとる膜厚の範囲内に、前記被膜の膜厚を設定したことを特徴とする。
【0008】
本発明の半導体発光装置は、標準波長がλ0に設定され、動作保障範囲の上限とされた温度における波長がλ1に変動する半導体発光素子と、該発光素子が出力する光を表面の被膜を介して受光する受光素子を備えた半導体発光装置において、前記発光素子の波長λ0の光と波長λ1の光が被膜を透過する透過率の差を被膜の厚さを変化させて求めて、その透過率差が正の範囲(正とは、波長がλ0からλ1に変動することによって被膜を通過する光の量が増加する場合)で、しかも、この透過率差が被膜の膜厚変動によって負の範囲に変動することを防止するように極大値を挟んで位置する0と極大値の中間の値をとる2つの領域のうち、前記発光素子の波長λ0の光の透過率が大きい側の領域の膜厚の範囲内に、前記被膜の膜厚を設定したことを特徴とする。
【0010】
【発明の実施の形態】
以下本発明の実施例を、半導体発光素子として半導体レーザ素子を用いる場合を例に取り、図面を参照して説明する。半導体発光装置1は、図1に概略的な構成を示すように、金属製ステム2に金属製のヘッダ3を一体的に設け、このヘッダ3の側面にシリコンなどのサブマウント4を介して半導体発光素子としての半導体レーザ素子5を配置している。ステム2の上には、半導体レーザ素子5の後方出力をモニターするための受光素子6を半導体レーザ素子5の直下に位置して配置している。
【0011】
この受光素子6は、例えばフォトダイオードによって構成され、図1中にその要部断面を拡大して示すように、その表面に保護膜並びに反射防止膜としての酸化シリコン、窒化シリコン等の透明な被膜7を備えている。受光素子6は、500Ωcm以上の抵抗値のN型シリコン基板8が用いられ、その表側には、受光領域に沿ってP型導電性高濃度不純物層9をボロン(B)等のP型不純物を拡散することによって、深さ1〜5μm、不純物濃度1×1020cm-3程度で形成し、基板裏側には、N型導電性高濃度不純物層10をリン(P)等のN型不純物を拡散することによって、深さ100μm前後、不純物濃度1×1020cm-3程度で形成し、この層10を介してN型オ−ミック電極11を形成している。被膜7の上には、この被膜7に形成したコンタクトホールを介して層9に至るP型電極12を形成している。
【0012】
次に前記被膜7の膜厚(t)設定について説明する。ここで、前記半導体レーザ素子5は、その標準の発振波長(λ0)が790nm(常温:25℃)に設定され、動作保障された温度範囲の上限とされた温度(70℃)における発振波長(λ1)が800nmであるものとする。また、受光素子6の表面の被膜7は、屈折率が1.46の酸化シリコンとし、レーザ素子5の後方出力は受光素子6の受光面に垂直に入射するものとする。
【0013】
被膜7の膜厚(t)を順次変化させると、図2に示すように、標準波長(λ0)の光の透過率(a)、及び変動後の波長(λ1)の光の透過率(b)は、極大値(約93%)と極小値(約68%)を周期的に繰り返す正弦波的な特性を描いて変動する。また、同図には、標準波長(λ0)における光透過率から変動後の波長(λ1)における光透過率を差引いた透過率差(c)を示している。この透過率差(c)もグラフの右軸に示す値をとって極大値と極小値(グラフの右軸参照)を周期的に繰り返す正弦波的な特性を描いて変動するが、膜厚(t)が厚くなるにしたがって、その振幅が大きくなっていく。
【0014】
この透過率差(c)の値が負の領域は、波長がλ0からλ1に変動することによって、被膜7を通過する光の量が減少すること、すなわち、受光素子6の検知出力が低下することを示している。受光素子6の出力を検知してレーザ素子5の出力を一定に保つ回路を備えている場合は、受光素子6の被膜7が、透過率差(c)が負の値を示す膜厚に設定されていると、上記のような受光素子6の検知出力低下に伴い、レーザ素子5の駆動電流が増加され、レーザ素子5に対する負荷が増加されて素子劣化を早めてしまう。また、レーザ素子5の出力増加に伴い、自励発振状態から非自励発振状態となって戻り光ノイズが増加し易くなる。
【0015】
そこで、受光素子6の被膜7の膜厚は、透過率差(c)が正の値をとる範囲に設定する。このように膜厚(t)を設定すれば、波長がλ0からλ1に変動すると、被膜7を通過する光の量が増加し、受光素子6の検知出力が増加する。そして、受光素子6の出力を検知してレーザ素子5の出力を一定に保つ回路を備えている場合は、上記のような受光素子6の出力上昇に伴い、レーザ素子5の駆動電流が減少され、レーザ素子5に対する負荷が軽減されて素子劣化を防止する。また、レーザ素子5は、自励発振状態を維持するので、戻り光ノイズの影響を受けにくくすることができる。
【0016】
被膜7の膜厚(t)は、透過率差(c)が正の範囲に設定することが第1の条件であるが、第2の条件としては、透過率(a)(若しくは(b))の値が極大値に近い数値をとるような膜厚に設定することである。透過率(a)(若しくは(b))の値が小さいと、素子5の出力が小さい場合は、受光素子6による十分な検知出力が得られない場合が生じるので、これを防ぐために上記のように設定するのが好ましい。この条件に従えば、例えば、1350〜2000Å、4150〜4700Å、6800〜7400Åから選択した膜厚(t)に設定することが好ましい。
【0017】
ここで、透過率(a)(若しくは(b))の値が極大値をとる膜厚においては、透過率差(c)が0付近の値となり、製造誤差等による被膜7の膜厚変動によって、透過率差(c)が負の範囲に変動する恐れがあるので、これを防ぐための条件が必要となる。そのための第3の条件としては、透過率差(c)が極大値と0の中間の値を取るような膜厚(t)に設定することである。このように設定すれば、被膜7の膜厚変動によって、透過率差(c)が負の範囲に変動することを有効に防止することができる。この条件に従えば、例えば、1500〜1800Å、4250〜4600Å、6900〜7300Åから選択した膜厚に設定することが最も好ましい。
【0018】
上記のように、第1の条件を満足した上で、第2、第3の条件のいずれかを満足することが望ましく、上記3つの条件を同時に満足するのが最も好ましい。
【0019】
上記実施例は、素子5の出力が受光素子6に垂直に入射する(入射角θ=0度)場合を例にとって説明したが、素子5の出力が受光素子6に所定範囲の入射角(θMAX〜θMIN)をもって斜めに入射する場合にも本発明を適用することができる。図3に示す特性は、上述したものと同じ特性を備えるレーザ素子5と受光素子6の配置を、受光素子6の受光面への入射が斜めで、その入射角θが82.5度(θMAX)〜73.5度(θMIN)の範囲となるように配置した場合において、波長λ0,λ1のそれぞれについて、入射角θをθMAX〜θMINまで0.5度刻みに変化させた場合の、波長λ0の合計透過率(a)、波長λ1の合計透過率(b)、並びに、合計透過率(a)から合計透過率(b)を差し引いた透過率差(c)を、被膜7の膜厚(t)を順次変化させて求めたものである。この場合においても、被膜7の膜厚(t)を上述と同様の条件によって設定することができ、透過率差(c)が正の値であることを前提条件とし、波長λ0の合計透過率(a)が極大付近である2000〜2300Å,もしくは5850〜6250Åを好ましい範囲とし、透過率差(c)が極大値と0の中間値付近に位置する2100〜2200Å、もしくは5950〜6150Åを最も好ましい範囲として被膜7の膜厚(t)が設定される。
【0020】
尚、図4は、図1に示す素子5のみを以下のように変更、すなわち、標準発光波長λ0が670nmに設定され、動作保障範囲の上限温度における波長λ1が680nmに変動する赤色レーザ、に変更した場合の特性図(図2の特性図と同様の特性図)である。この場合は、被膜7の膜厚(t)を、2800〜3400Å、5200〜5800Å、7400〜8000Åの中から選択するのが好ましく、3000〜3300Å、5300〜5700Å、7500〜7900Åの中から選択するのが最も好ましい。
【0021】
尚、上記実施例は、半導体発光素子として半導体レーザ素子を用いる場合を示したが、本発明は、発光波長がほぼ単一の波長に設定された発光ダイオードを発光素子として用いる場合にも適用することができる。
【0022】
【発明の効果】
以上のように本発明によれば、発光素子と受光素子を備えた半導体発光装置を温度上昇による影響を受けにくい構成とすることができる。また、温度上昇によって発光素子の波長が変動しても受光素子の感度が低下することがない半導体発光装置を提供することができる。また、半導体発光素子の劣化を防止することができる。また、半導体発光素子として半導体レーザを用いる場合は、その発振状態の変動を防止することができる。
【図面の簡単な説明】
【図1】本発明の一実施例を示す正面図である。
【図2】本発明に係わる被膜の膜厚と透過率ないし透過率差の関係の1つの例を示す特性図である。
【図3】本発明に係わる被膜の膜厚と透過率ないし透過率差の関係の別の例を示す特性図である。
【図4】本発明に係わる被膜の膜厚と透過率ないし透過率差の関係の別の例を示す特性図である。
【符号の説明】
1 半導体発光装置
5 半導体レーザ素子(半導体発光素子)
6 受光素子
7 被膜
[0001]
BACKGROUND OF THE INVENTION
The present invention relates to a semiconductor light emitting device including a semiconductor light emitting element and a light receiving element that receives an output thereof.
[0002]
[Prior art]
A light emitting element such as a semiconductor laser element or a light emitting diode for optical communication is used as a light source when light emission is required at a single wavelength or a wavelength close thereto. In general, when the output of the light emitting element is kept constant, automatic output control is performed in which the output of the light emitting element is detected by the light receiving element to control the operation of the light emitting element.
[0003]
By the way, the output wavelength of the semiconductor light emitting element slightly changes due to an increase in internal temperature due to its operation or a change in operating environment temperature. However, such a change adversely affects the automatic output control. Sometimes. That is, a transparent film is provided on the light receiving surface of the light receiving element, and the amount of light transmitted through the film varies depending on the wavelength. When the wavelength changes due to the temperature change, and the amount of light passing through the film changes accordingly, the detection output of the light receiving element also changes, and the sensitivity looks as if it changes with temperature.
[0004]
FIG. 2 shows the transmittance (a) of light of wavelength λ0 (790 nm), the transmittance (b) of light of wavelength λ1 (800 nm), and the transmission of wavelength λ1 with respect to the film thickness (t) of the coating (silicon oxide). The difference (c) between the transmittances of both wavelengths obtained by subtracting the transmittance of the wavelength λ0 from the rate is shown. In the transmittance difference (c) characteristic, in the film thickness where the transmittance difference is a negative value, the transmittance decreases when the standard wavelength λ0 changes to the wavelength λ1 due to the temperature rise. When the film of the light receiving element is set to such a film thickness, feedback that the light receiving output is reduced due to the temperature rise occurs, and the driving current of the light emitting element increases. As a result, the output of the light emitting element increases, and deterioration of the light emitting element itself tends to be induced.
[0005]
Also, in a semiconductor laser element, the output increases due to an increase in drive current, which tends to cause self-excited oscillation to become non-self-excited oscillation. When this laser element is mounted on an optical pickup or the like, the return light from the recording medium There is also a problem that noise due to the above becomes easy to occur.
[0006]
[Problems to be solved by the invention]
An object of the present invention is to provide a semiconductor light-emitting device that is not easily affected by a temperature rise in consideration of the above-described points. Another object is to provide a semiconductor light emitting device in which the detection output of the light receiving element does not decrease even if the wavelength of the light emitting element fluctuates due to temperature rise. Another object is to prevent deterioration of a semiconductor light emitting element. In addition, when a semiconductor laser is used as the semiconductor light emitting element, it is an object to prevent fluctuations in the oscillation state.
[0007]
[Means for Solving the Problems]
The semiconductor light emitting device of the present invention includes a semiconductor light emitting element in which the standard wavelength is set to λ0 and the wavelength at a temperature set as the upper limit of the operation guarantee range varies to λ1, and the light output from the light emitting element through the surface coating. In a semiconductor light emitting device including a light receiving element for receiving light, a difference in transmittance at which light of wavelength λ0 and light of wavelength λ1 of the light emitting element transmits through the film is obtained by changing the thickness of the film, and the transmittance The difference is in the positive range (when the wavelength increases from λ0 to λ1 and the amount of light passing through the film increases), the transmittance difference is in the negative range due to the film thickness variation of the film. The film thickness of the coating film is set within the range of the film thickness that takes an intermediate value between 0 and the maximum value so as to prevent the fluctuation.
[0008]
The semiconductor light emitting device of the present invention includes a semiconductor light emitting element in which the standard wavelength is set to λ0 and the wavelength at a temperature set as the upper limit of the operation guarantee range varies to λ1, and the light output from the light emitting element through the surface coating. In a semiconductor light emitting device including a light receiving element for receiving light, a difference in transmittance at which light of wavelength λ0 and light of wavelength λ1 of the light emitting element transmits through the film is obtained by changing the thickness of the film, and the transmittance The difference is in the positive range (when the wavelength increases from λ0 to λ1 and the amount of light passing through the film increases), the transmittance difference is in the negative range due to the film thickness variation of the film. Among the two regions that take an intermediate value between 0 and the maximum value that are located across the maximum value so as to prevent fluctuations, the film in the region on the side where the light transmittance of the wavelength λ0 of the light emitting element is large The film thickness is set within the thickness range. The features.
[0010]
DETAILED DESCRIPTION OF THE INVENTION
Embodiments of the present invention will be described below with reference to the drawings, taking as an example the case where a semiconductor laser element is used as the semiconductor light emitting element. As shown in FIG. 1, the semiconductor light emitting device 1 is provided with a metal header 3 integrally on a metal stem 2, and a semiconductor is mounted on a side surface of the header 3 via a submount 4 such as silicon. A semiconductor laser element 5 as a light emitting element is arranged. On the stem 2, a light receiving element 6 for monitoring the rear output of the semiconductor laser element 5 is disposed directly below the semiconductor laser element 5.
[0011]
The light receiving element 6 is composed of, for example, a photodiode, and as shown in an enlarged cross-sectional view of the main part in FIG. 1, a transparent film such as a protective film and a silicon oxide or silicon nitride film as an antireflection film is formed on the surface thereof. 7 is provided. The light-receiving element 6 uses an N-type silicon substrate 8 having a resistance value of 500 Ωcm or more, and a P-type conductive high-concentration impurity layer 9 is formed on the front side with a P-type impurity such as boron (B) along the light-receiving region. By diffusion, it is formed with a depth of 1 to 5 μm and an impurity concentration of about 1 × 10 20 cm −3 , and an N-type conductive high-concentration impurity layer 10 is formed on the back side of the substrate with an N-type impurity such as phosphorus (P). By diffusing, it is formed with a depth of about 100 μm and an impurity concentration of about 1 × 10 20 cm −3 , and an N-type ohmic electrode 11 is formed through this layer 10. On the coating 7, a P-type electrode 12 that reaches the layer 9 through a contact hole formed in the coating 7 is formed.
[0012]
Next, the film thickness (t) setting of the film 7 will be described. Here, the semiconductor laser element 5 has its standard oscillation wavelength (λ0) set to 790 nm (normal temperature: 25 ° C.), and the oscillation wavelength (70 ° C.) at the upper limit of the guaranteed temperature range (70 ° C.). Let λ1) be 800 nm. The film 7 on the surface of the light receiving element 6 is made of silicon oxide having a refractive index of 1.46, and the rear output of the laser element 5 is incident on the light receiving surface of the light receiving element 6 perpendicularly.
[0013]
When the film thickness (t) of the coating 7 is sequentially changed, as shown in FIG. 2, the transmittance (a) of the light having the standard wavelength (λ0) and the transmittance (b) of the light having the changed wavelength (λ1) are obtained. ) Varies with a sinusoidal characteristic that periodically repeats a maximum value (about 93%) and a minimum value (about 68%). The figure also shows a transmittance difference (c) obtained by subtracting the light transmittance at the wavelength (λ1) after the change from the light transmittance at the standard wavelength (λ0). This transmittance difference (c) also takes a value shown on the right axis of the graph and fluctuates in a sinusoidal characteristic that periodically repeats a maximum value and a minimum value (see the right axis of the graph). As t) becomes thicker, its amplitude increases.
[0014]
In the region where the value of the transmittance difference (c) is negative, the wavelength varies from λ0 to λ1, so that the amount of light passing through the coating 7 decreases, that is, the detection output of the light receiving element 6 decreases. It is shown that. When a circuit for detecting the output of the light receiving element 6 and keeping the output of the laser element 5 constant is provided, the coating 7 of the light receiving element 6 is set to a film thickness at which the transmittance difference (c) shows a negative value. If so, the drive current of the laser element 5 is increased with the decrease in the detection output of the light receiving element 6 as described above, the load on the laser element 5 is increased, and the element deterioration is accelerated. Further, as the output of the laser element 5 increases, the return light noise tends to increase from the self-excited oscillation state to the non-self-excited oscillation state.
[0015]
Therefore, the film thickness of the coating 7 of the light receiving element 6 is set in a range where the transmittance difference (c) takes a positive value. If the film thickness (t) is set in this way, when the wavelength varies from λ0 to λ1, the amount of light passing through the coating 7 increases and the detection output of the light receiving element 6 increases. When a circuit that detects the output of the light receiving element 6 and keeps the output of the laser element 5 constant is provided, the drive current of the laser element 5 is reduced as the output of the light receiving element 6 increases. The load on the laser element 5 is reduced to prevent element deterioration. Further, since the laser element 5 maintains the self-excited oscillation state, it can be made less susceptible to the influence of return light noise.
[0016]
The first condition for the film thickness (t) of the coating 7 is that the transmittance difference (c) is set in a positive range. The second condition is that the transmittance (a) (or (b) ) Is set to such a film thickness that takes a value close to the maximum value. If the value of the transmittance (a) (or (b)) is small, if the output of the element 5 is small, a sufficient detection output by the light receiving element 6 may not be obtained. It is preferable to set to. According to this condition, for example, it is preferable to set the film thickness (t) selected from 1350 to 2000 mm, 4150 to 4700 mm, and 6800 to 7400 mm.
[0017]
Here, in the film thickness at which the value of the transmittance (a) (or (b)) is a maximum value, the transmittance difference (c) is a value near 0, and due to the film thickness variation of the coating film 7 due to manufacturing error or the like. Since the transmittance difference (c) may fluctuate in the negative range, a condition for preventing this is necessary. The third condition for this is to set the film thickness (t) such that the transmittance difference (c) takes an intermediate value between the maximum value and zero. By setting in this way, it is possible to effectively prevent the transmittance difference (c) from fluctuating in the negative range due to the film thickness fluctuation of the coating 7. According to this condition, for example, it is most preferable to set the film thickness to a thickness selected from 1500 to 1800 mm, 4250 to 4600 mm, and 6900 to 7300 mm.
[0018]
As described above, it is desirable to satisfy either the second or third condition after satisfying the first condition, and it is most preferable to satisfy the three conditions at the same time.
[0019]
In the above embodiment, the case where the output of the element 5 is perpendicularly incident on the light receiving element 6 (incident angle θ = 0 °) has been described as an example. However, the output of the element 5 is incident on the light receiving element 6 within a predetermined range of incident angles (θ The present invention can also be applied to the case of oblique incidence with MAX to θ MIN ). The characteristic shown in FIG. 3 is that the arrangement of the laser element 5 and the light receiving element 6 having the same characteristics as those described above is such that the incidence on the light receiving surface of the light receiving element 6 is oblique and the incident angle θ is 82.5 degrees (θ MAX ) to 73.5 degrees (θ MIN ), when the incident angle θ is changed in increments of 0.5 degrees from θ MAX to θ MIN for each of the wavelengths λ0 and λ1. The total transmittance (a) of wavelength λ0, the total transmittance (b) of wavelength λ1, and the transmittance difference (c) obtained by subtracting the total transmittance (b) from the total transmittance (a) The film thickness (t) is obtained by sequentially changing. Also in this case, the film thickness (t) of the film 7 can be set under the same conditions as described above, and the total transmittance of the wavelength λ0 is assumed on the precondition that the transmittance difference (c) is a positive value. (A) is in the range of 2000 to 2300 mm or 5850 to 6250 mm in which the maximum is near, and the transmittance difference (c) is most preferably in the range of 2100 to 2200 mm or 5950 to 6150 mm in the vicinity of the intermediate value between the maximum value and 0. The film thickness (t) of the film 7 is set as the range.
[0020]
In FIG. 4, only the element 5 shown in FIG. 1 is changed as follows, that is, a red laser in which the standard emission wavelength λ0 is set to 670 nm and the wavelength λ1 at the upper limit temperature of the operation guarantee range varies to 680 nm. FIG. 3 is a characteristic diagram in the case of a change (characteristic diagram similar to the characteristic diagram of FIG. 2). In this case, the film thickness (t) of the film 7 is preferably selected from 2800 to 3400 mm, 5200 to 5800 mm, and 7400 to 8000 mm, and is selected from 3000 to 3300 mm, 5300 to 5700 mm, and 7500 to 7900 mm. Is most preferred.
[0021]
In the above embodiment, the semiconductor laser element is used as the semiconductor light emitting element. However, the present invention is also applied to the case where a light emitting diode whose emission wavelength is set to a substantially single wavelength is used as the light emitting element. be able to.
[0022]
【The invention's effect】
As described above, according to the present invention, a semiconductor light-emitting device including a light-emitting element and a light-receiving element can be configured to be hardly affected by temperature rise. In addition, it is possible to provide a semiconductor light emitting device in which the sensitivity of the light receiving element does not decrease even when the wavelength of the light emitting element varies due to temperature rise. In addition, deterioration of the semiconductor light emitting element can be prevented. In addition, when a semiconductor laser is used as the semiconductor light emitting element, fluctuations in the oscillation state can be prevented.
[Brief description of the drawings]
FIG. 1 is a front view showing an embodiment of the present invention.
FIG. 2 is a characteristic diagram showing one example of the relationship between the film thickness and the transmittance or transmittance difference according to the present invention.
FIG. 3 is a characteristic diagram showing another example of the relationship between the film thickness and the transmittance or transmittance difference according to the present invention.
FIG. 4 is a characteristic diagram showing another example of the relationship between the film thickness and the transmittance or transmittance difference according to the present invention.
[Explanation of symbols]
DESCRIPTION OF SYMBOLS 1 Semiconductor light-emitting device 5 Semiconductor laser element (semiconductor light-emitting device)
6 Light receiving element 7 Coating

Claims (2)

標準波長がλ0に設定され、動作保障範囲の上限とされた温度における波長がλ1に変動する半導体発光素子と、該発光素子が出力する光を表面の被膜を介して受光する受光素子を備えた半導体発光装置において、前記発光素子の波長λ0の光と波長λ1の光が被膜を透過する透過率の差を被膜の厚さを変化させて求めて、その透過率差が正の範囲(正とは、波長がλ0からλ1に変動することによって被膜を通過する光の量が増加する場合)で、しかも、この透過率差が被膜の膜厚変動によって負の範囲に変動することを防止するように0と極大値の中間の値をとる膜厚の範囲内に、前記被膜の膜厚を設定したことを特徴とする半導体発光装置。A semiconductor light emitting element in which the wavelength at a temperature at which the standard wavelength is set to λ0 and the upper limit of the operation guarantee range is changed to λ1 and a light receiving element that receives light output from the light emitting element through a surface coating are provided. In the semiconductor light emitting device, the difference in transmittance between the light of the light emitting element having the wavelength λ0 and the light having the wavelength λ1 transmitted through the coating is obtained by changing the thickness of the coating, and the transmittance difference is in a positive range (positive and negative). (In the case where the amount of light passing through the film increases as the wavelength varies from λ0 to λ1) , and this transmittance difference is prevented from varying in the negative range due to the film thickness variation of the film. A film thickness of the coating film is set within a range of film thickness that takes an intermediate value between 0 and a maximum value. 標準波長がλ0に設定され、動作保障範囲の上限とされた温度における波長がλ1に変動する半導体発光素子と、該発光素子が出力する光を表面の被膜を介して受光する受光素子を備えた半導体発光装置において、前記発光素子の波長λ0の光と波長λ1の光が被膜を透過する透過率の差を被膜の厚さを変化させて求めて、その透過率差が正の範囲(正とは、波長がλ0からλ1に変動することによって被膜を通過する光の量が増加する場合)で、しかも、この透過率差が被膜の膜厚変動によって負の範囲に変動することを防止するように極大値を挟んで位置する0と極大値の中間の値をとる2つの領域のうち、前記発光素子の波長λ0の光の透過率が大きい側の領域の膜厚の範囲内に、前記被膜の膜厚を設定したことを特徴とする半導体発光装置。A semiconductor light emitting element in which the wavelength at a temperature at which the standard wavelength is set to λ0 and the upper limit of the operation guarantee range is changed to λ1 and a light receiving element that receives light output from the light emitting element through a surface coating are provided. In the semiconductor light emitting device, the difference in transmittance between the light of the light emitting element having the wavelength λ0 and the light having the wavelength λ1 transmitted through the coating is obtained by changing the thickness of the coating, and the transmittance difference is in a positive range (positive and negative). (In the case where the amount of light passing through the film increases as the wavelength varies from λ0 to λ1) , and this transmittance difference is prevented from varying in the negative range due to the film thickness variation of the film. The film is within the range of the film thickness of the region on the side where the transmittance of light of the wavelength λ0 of the light emitting element is large, out of the two regions having a maximum value between 0 and the maximum value located between the maximum value and A semiconductor light emitting device characterized by setting a film thickness of .
JP20843698A 1998-07-23 1998-07-23 Semiconductor light emitting device Expired - Fee Related JP3668005B2 (en)

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