JPH03195076A - External resonator type variable wavelength semiconductor laser - Google Patents

External resonator type variable wavelength semiconductor laser

Info

Publication number
JPH03195076A
JPH03195076A JP33583789A JP33583789A JPH03195076A JP H03195076 A JPH03195076 A JP H03195076A JP 33583789 A JP33583789 A JP 33583789A JP 33583789 A JP33583789 A JP 33583789A JP H03195076 A JPH03195076 A JP H03195076A
Authority
JP
Japan
Prior art keywords
active layer
end surface
window end
wavelength
reflection
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP33583789A
Other languages
Japanese (ja)
Inventor
Tetsuya Suzuki
徹也 鈴木
Haruo Nagai
治男 永井
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.)
Anritsu Corp
Original Assignee
Anritsu Corp
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 Anritsu Corp filed Critical Anritsu Corp
Priority to JP33583789A priority Critical patent/JPH03195076A/en
Publication of JPH03195076A publication Critical patent/JPH03195076A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To obtain an end surface having a low reflectivity in a wide band by a method wherein a reflection-proof film is provided outside the window end surface structure of a semiconductor element and only lights having required wavelengths are selected from among lights emitted through the window end surface structure and the reflection-proof film and are made to return. CONSTITUTION:Photons created in an active layer 3 by applying a current between an electrode 1 and an electrode 2 are guided along the active layer 3. The photons guided to one direction are reflected by a cleavage plane 4 and return to the active layer 3. The photons guided to the other direction are transmitted through a window end surface structure 5 and a reflection-proof film 6. The transmitted photons are condensed by a convex lens 7 which is a light condensing means and reflected by a diffraction grating 8 selectively and return to the active layer 3 again. An oscillation is created by multireflection between the cleavage plane 4 and the deffraction grating 8. The oscillated lights are emitted from the cleavage plane 4. In order to emit only lights having required wavelengths selectively, the diffraction grating 8 is controlled by a deffraction grating scanning means 9. With this constitution, the reflectivity of a semiconductor end surface of the window end surface side can be returned and, further, the end surface having a low reflectivity in a wide band can be obtained.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、コヒーレント光通信、干渉型光ファイバセン
サ、光応用測定器等の光源として使用される、外部共振
器型波長可変半導体レーザに関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to an external cavity type wavelength tunable semiconductor laser used as a light source for coherent optical communications, interference type optical fiber sensors, optical application measuring instruments, etc.

〔従来の技術〕[Conventional technology]

活性層端面の片側に反射防止膜を形成した半導体レーザ
と回折格子より構成される外部共振器型波長可変半導体
レーザは、反射防止膜での反射率が反射防止膜厚に依存
するため、特に低反射を実現しようとする場合、製作上
膜厚の制御が難しい。
External cavity type wavelength tunable semiconductor lasers, which are composed of a semiconductor laser with an anti-reflection film formed on one side of the active layer end face and a diffraction grating, have particularly low reflectance because the reflectance of the anti-reflection film depends on the thickness of the anti-reflection film. When trying to achieve reflection, it is difficult to control the film thickness during manufacturing.

例えば1.3μm帯では、反射率を0.1%以下にする
ために反射防止膜厚の誤差を±60人(約3%)以内に
しなければならず、また波長帯域幅は最適膜厚条件に於
いても40nm程度であった。そのため反射防止膜の反
射率がばらつき、外部共振器型波長可変半導体レーザは
安定した緒特性を得ることができなかった。
For example, in the 1.3 μm band, in order to keep the reflectance below 0.1%, the error in the anti-reflection film thickness must be within ±60 (approximately 3%), and the wavelength bandwidth is set to the optimum film thickness. It was also about 40 nm. As a result, the reflectance of the antireflection film varies, making it impossible for external cavity type wavelength tunable semiconductor lasers to obtain stable performance characteristics.

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

従来の、端面に反射防止膜を施しただけの半導体レーザ
を用いた場合、反射防止膜のみで低反射率を実現しなけ
ればならなかった。しかしながら、低反射率を実現でき
る反射防止膜の膜厚の一許容範囲が狭く、実用が可能な
波長範囲が狭く、また反耐重のばらつきが生じやすい等
の問題があり、そのため、半導体素子の広帯域の利得を
十分に活用することが出来ず、また波長範囲がばらつ(
事が多かった。
When using a conventional semiconductor laser that only has an anti-reflection film applied to its end facets, it is necessary to achieve low reflectance with just the anti-reflection film. However, there are problems such as the permissible range of the film thickness of the antireflection film that can achieve low reflectance is narrow, the practical wavelength range is narrow, and the anti-load resistance is likely to vary. The gain cannot be fully utilized, and the wavelength range varies (
A lot of things happened.

本発明は、このような事情に鑑みてなされたものであり
、広帯域で低反射な窓端面構造半導体レーザを用いた外
部共振器型波巻可変半導体レーザを提供することを課題
とする。
The present invention has been made in view of the above circumstances, and an object of the present invention is to provide an external cavity type wave-wound variable semiconductor laser using a window edge structure semiconductor laser having a wide band and low reflection.

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

上記課題を解決するために本発明の外部共振器型波長可
変半導体レーザに於いては、 ■出射端面から延びる活性層と、活性層に続く領域を窓
端面構造とした半導体素子とし、■その半導体素子の窓
端面構造の外側に反射防止膜を備え、 ■窓端面構造と反射防止膜を通過して放出された光のう
ち所定の波長のみを選択して帰還させる構造をとった。
In order to solve the above problems, in the external cavity type wavelength tunable semiconductor laser of the present invention, (1) an active layer extending from the emission end face and a semiconductor element having a window end face structure in a region following the active layer, and (2) the semiconductor An antireflection film is provided on the outside of the window end face structure of the element, and a structure is adopted in which only a predetermined wavelength of light is selected and returned from the light emitted after passing through the window end face structure and the antireflection film.

なお、波長選択の手段は、所定の波長のみを選択するよ
うに制御することとした。
Note that the wavelength selection means is controlled to select only a predetermined wavelength.

C作用〕 このように三つの構成要件を備えた外部共振器型波長可
変半導体レーザによれば、窓端面構造の領域で相対反射
率を0.3%に低減できるので、反射防止膜の反射率へ
の性能要求を低減できる。すなわち、反射防止膜厚の許
容範囲が広がり、例えば反射防止膜の反射率が30%以
下であれば窓端面構造と合わせた端面反射率を0.1%
以下にすることが出来るので、反射率のばらつきを抑え
ることができる。また窓端面構造の精度、反射防止膜の
反射率の精度を製造上緩和できるようになる。具体的に
は、窓端面構造によれば広帯域で反射率が低減でき、反
射防止膜との組合せによってo、oos%以下の反射率
が100n m程度の波長範囲で得られる。
C effect] According to the external cavity type wavelength tunable semiconductor laser having the three structural requirements as described above, the relative reflectance can be reduced to 0.3% in the region of the window end face structure, so that the reflectance of the antireflection film can be reduced to 0.3%. performance requirements can be reduced. In other words, the tolerance range for the thickness of the anti-reflection film is widened; for example, if the reflectance of the anti-reflection film is 30% or less, the end face reflectance combined with the window end face structure can be reduced to 0.1%.
Since it is possible to do the following, variations in reflectance can be suppressed. In addition, it becomes possible to reduce the precision of the window end surface structure and the reflectance precision of the antireflection film during manufacturing. Specifically, the window end face structure can reduce the reflectance in a wide band, and in combination with an antireflection film, a reflectance of less than 0.000% can be obtained in a wavelength range of about 100 nm.

〔実施例〕〔Example〕

以下本発明の一実施例を図面を用いて説明する。 An embodiment of the present invention will be described below with reference to the drawings.

(第一の実施例) 第1図は本発明の外部共振器型波長可変半導体レーザの
第一の実施例を示す構造図である。第一の実施例では、
波長選択手段として回折格子、制御手段として回折格子
を回転する回折格子走査手段を用いたものである。
(First Embodiment) FIG. 1 is a structural diagram showing a first embodiment of an external cavity type wavelength tunable semiconductor laser of the present invention. In the first embodiment,
A diffraction grating is used as the wavelength selection means, and a diffraction grating scanning means for rotating the diffraction grating is used as the control means.

電極1と電極2間に電流を注入することにより、活性層
3で発生した光子は活性N3に沿って導波し、一方の光
子はへき開面4で反射して活性層3に戻り、他方の光子
は窓端面構造5と反射防止膜6を透過し、その透過した
光子は集光手段としての凸レンズ7で集光され、回折格
子8で選択的に反射して再び活性層3に戻り、へき開面
4と回折格子8とで多重反射をして発振する。その発振
した光がへき開面4から出射される。なお、所望の波長
のみを選択的に反射しうるように回折格子8は、回折格
子走査手段9により制御される。具体的には、回折格子
8を回転し回折格子8の法線に対する光の入射角を制御
する。
By injecting a current between the electrodes 1 and 2, photons generated in the active layer 3 are guided along the active N3, one photon is reflected by the cleavage plane 4 and returns to the active layer 3, and the other photon is guided along the active layer 3. The photons pass through the window end surface structure 5 and the anti-reflection film 6, and the transmitted photons are focused by a convex lens 7 as a focusing means, selectively reflected by the diffraction grating 8, returned to the active layer 3, and cleaved. Multiple reflections occur between the surface 4 and the diffraction grating 8, resulting in oscillation. The oscillated light is emitted from the cleavage plane 4. Note that the diffraction grating 8 is controlled by a diffraction grating scanning means 9 so that only desired wavelengths can be selectively reflected. Specifically, the diffraction grating 8 is rotated to control the incident angle of light with respect to the normal line of the diffraction grating 8.

第2図は本発明の外部共振器型波長可変半導体レーザの
半導体素子の製造工程を示す図である。
FIG. 2 is a diagram showing the manufacturing process of the semiconductor element of the external cavity type wavelength tunable semiconductor laser of the present invention.

1回目の成長として液相成長(LPE)法、気相成長(
VPE、MO−CVD)法、または分子線エピタキシー
(MBE)法等により、p形1nP基板10上にp形I
nPバッファ層11、ノンドープI nGaAsP活性
層(λ:  1.3μm組成)3、その上にn形InP
クラッド層12を薄(成長させる(第2図(a))、基
板表面全体に5iNxllを蒸着し、窓端面構造を形成
する部分の5iNxliを除去することにより、5jN
xllのマスク13をバターニングする。マスク13に
より覆われていない部分のn型InPクラッド層12、
ノンドープInGaAsP活性層3をエツチングにより
除去する(第2図(b))、マスク13を除去した後(
第2図(c))、2回目の成長としてn型1nPを成長
し、窓端面構造5および厚クラッド層12を成長させる
(第2図(d))。
For the first growth, liquid phase epitaxy (LPE) method, vapor phase epitaxy (
P-type I is deposited on p-type 1nP substrate 10 by VPE, MO-CVD) method, or molecular beam epitaxy (MBE) method.
nP buffer layer 11, non-doped InGaAsP active layer (λ: 1.3 μm composition) 3, and n-type InP layer thereon.
The cladding layer 12 is grown thinly (FIG. 2(a)), 5iNxll is deposited on the entire substrate surface, and 5iNxli is removed from the portion where the window end surface structure is formed.
Buttering the xll mask 13. n-type InP cladding layer 12 in a portion not covered by mask 13;
The non-doped InGaAsP active layer 3 is removed by etching (FIG. 2(b)), and after removing the mask 13 (
FIG. 2(c)), n-type 1nP is grown as a second growth, and the window end face structure 5 and thick cladding layer 12 are grown (FIG. 2(d)).

次に、導波路、埋め込み層を形成するために、SiNx
膜のパターニング、メサエッチング、3回目の成長とし
て、電流障壁層の埋め込み成長を行う(第2図(e))
、成長の終わった基板の両面には電極1および電極2を
蒸着しく第2図(f))、チップ状にスクライプし、反
射防止膜6を形成する(第2図(g))、このような工
程で製造された半導体素子を外部共振器に組み込み外部
共振器型波長可変半導体レーザを形成する。
Next, in order to form a waveguide and a buried layer, SiNx
Film patterning, mesa etching, and third growth of buried current barrier layer (Figure 2 (e))
After the growth, electrodes 1 and 2 are deposited on both sides of the substrate (Fig. 2(f)), and an antireflection film 6 is formed by scribing into chips (Fig. 2(g)). The semiconductor element manufactured through the process is assembled into an external resonator to form an external resonator type wavelength tunable semiconductor laser.

(第二の実施例) 第3図は本発明の外部共振器型波長可変半導体レーザの
第二の実施例を示す構造図である。第一の実施例は、回
折格子の入射角による波長選択性を利用したものである
が、第二の実施例では、回折格子および回折格子走査手
段の代わりに帯域フィルタ14と反射装置15を用いて
、所定の波長のみを選択し、その波長で発振させるよう
にしたものである。
(Second Embodiment) FIG. 3 is a structural diagram showing a second embodiment of the external cavity type wavelength tunable semiconductor laser of the present invention. The first embodiment utilizes wavelength selectivity depending on the incident angle of the diffraction grating, but the second embodiment uses a bandpass filter 14 and a reflection device 15 instead of the diffraction grating and the diffraction grating scanning means. Therefore, only a predetermined wavelength is selected and oscillation is performed at that wavelength.

電極1と電極2間に電流を注入することにより、活性層
3で発生した光子は活性層3に沿って導波し、一方の光
子はへき開面4で反射して活性層3に戻り、他方の光子
は窓端面構造5と反射防止膜6を透過し、その透過した
光子は集光手段としての凸レンズ7で集光され、帯域フ
ィルタ14により透過波長が選択され、反射装置15で
反射して再び活性層3に戻り、へき開面4と反射装置1
5とで多重反射をして発振する。その発振した光がへき
開面4から出射される。なお、所望の波長のみを選択的
に透過し、反射装置15で反射しうるように帯域フィル
タ14は、手動または自動により交換するように制御さ
れる。帯域フィルタ14の例として、具体的には多層膜
干渉フィルタがある。また、分光特性としてはバンドパ
スフィルタ、ロングウェーブフィルタ、ショートウェー
ブフィルタ等がある。また、帯域フィルタI4として連
続波長可変フィルタを使用し、その連続波長可変フィル
タの透過中心波長を所定の値にするよう制御することも
できる。さらに、反射袋215の例として、全反射器等
がある。
By injecting a current between the electrodes 1 and 2, photons generated in the active layer 3 are guided along the active layer 3, one photon is reflected by the cleavage plane 4 and returns to the active layer 3, and the other photon is guided along the active layer 3. The photons pass through the window end surface structure 5 and the anti-reflection film 6, and the transmitted photons are focused by a convex lens 7 as a focusing means, a transmission wavelength is selected by a bandpass filter 14, and reflected by a reflection device 15. Returning to the active layer 3 again, the cleavage plane 4 and the reflection device 1
5 and undergoes multiple reflections and oscillates. The oscillated light is emitted from the cleavage plane 4. Note that the bandpass filter 14 is controlled to be replaced manually or automatically so that only a desired wavelength can be selectively transmitted and reflected by the reflection device 15. A specific example of the bandpass filter 14 is a multilayer interference filter. Further, as the spectral characteristics, there are a band pass filter, a long wave filter, a short wave filter, etc. It is also possible to use a continuously variable wavelength filter as the bandpass filter I4 and control the transmission center wavelength of the continuously variable wavelength filter to a predetermined value. Furthermore, an example of the reflective bag 215 is a total reflector.

(第三の実施例) 第4図は本発明の外部共振器型波長可変半導体レーザの
第三の実施例を示す構造図である。第三の実施例は、波
長選択手段として光学的圧電結晶16および反射装置1
7、制御手段として電圧供給装置18を用いたものであ
る。つまり、光学的圧電結晶16の表面に格子状の電極
を設置して電圧を加え、電界効果により電極直下の結晶
内に生じた格子状の屈折率変化部分の中に光を通過させ
、回折効果を利用して光路を波長選択的に偏向させ、反
射装置17で反射し、その選択された波長で発振させる
ようにしたものである。
(Third Embodiment) FIG. 4 is a structural diagram showing a third embodiment of the external cavity type wavelength tunable semiconductor laser of the present invention. A third embodiment uses an optical piezoelectric crystal 16 and a reflection device 1 as wavelength selection means.
7. A voltage supply device 18 is used as a control means. In other words, a lattice-shaped electrode is installed on the surface of the optical piezoelectric crystal 16, a voltage is applied, and light is passed through the lattice-shaped refractive index changing portion that occurs in the crystal directly under the electrode due to the electric field effect, resulting in a diffraction effect. The optical path is wavelength-selectively deflected by using the wavelength, and reflected by the reflection device 17 to cause oscillation at the selected wavelength.

電極1と電極2間に電流を注入することにより、活性層
3で発生した光子は活性層3に沿って導波し、一方の光
子はへき開面4で反射して活性層3に戻り、他方の光子
は窓端面構造5と反射防止膜6を透過し、その透過した
光子は集光手段としての凸レンズ7で集光され、光学的
圧電結晶16により回折波長が選択され、反射装置17
で反射して再び活性層3に戻り、へき開面4と反射装置
17とで多重反射をして発振する。その発振した光がへ
き開面4から出射される。なお、所望の波長のみを選択
的に反射装置17の方向に偏向するように、電極入力端
子間の電圧を電圧供給装置18を制御することにより、
電極直下の結晶内に生した格子状の部分の屈折率が変化
する。
By injecting a current between the electrodes 1 and 2, photons generated in the active layer 3 are guided along the active layer 3, one photon is reflected by the cleavage plane 4 and returns to the active layer 3, and the other photon is guided along the active layer 3. The photons pass through the window end surface structure 5 and the anti-reflection film 6, and the transmitted photons are focused by a convex lens 7 as a focusing means, a diffraction wavelength is selected by an optical piezoelectric crystal 16, and a reflection device 17
The light is reflected back to the active layer 3, undergoes multiple reflections at the cleavage plane 4 and the reflection device 17, and oscillates. The oscillated light is emitted from the cleavage plane 4. Note that by controlling the voltage between the electrode input terminals by the voltage supply device 18 so as to selectively deflect only the desired wavelength toward the reflection device 17,
The refractive index of the lattice-shaped portion formed within the crystal directly under the electrode changes.

〔発明の効果〕〔Effect of the invention〕

以上説明したように本発明の外部共振器型波長可変半導
体レーザは出射端面から延びる活性層と、活性層に続く
窓端面構造を備えた半導体素子と、窓端面構造の外側に
備えられた反射防止膜と、窓端面構造と反射防止膜を通
過して放出された光を集光する集光手段と、集光手段に
よって集光された光を入射し所定の波長のみを選択し入
射光とは逆向きに送出する波長選択手段と、波長選択手
段を所定の波長ρみを選択するように制御する制御手段
とを備えたものである。そのため、窓端面側の半導体レ
ーザ端面の反射率を0.003χ程度に低減することが
でき、しかも、広帯域で低反射な端面を安定して実現で
きる。このような窓端面構造半導体レーザを用いること
により、狭スペクトル線幅、低ノイズ、広帯域で波長可
変な外部共振器型波長可変半導体レーザを安定に生産す
ることができる。
As explained above, the external cavity type wavelength tunable semiconductor laser of the present invention includes an active layer extending from the emission end facet, a semiconductor element having a window end face structure following the active layer, and an anti-reflection device provided outside the window end face structure. A light collecting means that collects the light emitted after passing through the film, the window end surface structure and the anti-reflection film, and a light collecting means that enters the light collected by the light collecting means and selects only a predetermined wavelength. It is equipped with wavelength selection means for transmitting in the opposite direction, and control means for controlling the wavelength selection means to select a predetermined wavelength ρ. Therefore, the reflectance of the semiconductor laser end face on the window end face side can be reduced to about 0.003χ, and moreover, a wide band and low reflection end face can be stably realized. By using such a semiconductor laser with a window end facet structure, it is possible to stably produce an external cavity type wavelength tunable semiconductor laser having a narrow spectral linewidth, low noise, and a wavelength tunable over a wide band.

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

第1図は本発明の第一の実施例を示す構造図、第2図は
本発明の製造工程を示す図、 第3図は本発明の第二の実施例を示す構造図、第4図(
a)、第4図(b)は本発明の第三の実施例を示す構造
図の側面図および平面図。 活性層、4・ 窓端面構造、6 集光手段、8・ 制御手段。 ・へき開面、 ・・・反射防止膜、 ・波長選択手段、
Fig. 1 is a structural diagram showing the first embodiment of the present invention, Fig. 2 is a diagram showing the manufacturing process of the invention, Fig. 3 is a structural diagram showing the second embodiment of the invention, Fig. 4 (
a) and FIG. 4(b) are a side view and a plan view of a structural diagram showing a third embodiment of the present invention. Active layer, 4. Window end surface structure, 6. Light condensing means, 8. Control means.・cleavage plane, ... antireflection film, ・wavelength selection means,

Claims (1)

【特許請求の範囲】[Claims] 出射端面から延びる活性層と、該活性層に続く窓端面構
造を備えた半導体素子と、前記窓端面構造の外側に備え
られた反射防止膜と、前記窓端面構造と前記反射防止膜
を通過して放出された光を集光する集光手段と、該集光
手段によって集光された光を入射し所定の波長のみを選
択し入射光とは逆向きに送出する波長選択手段と、該波
長選択手段を所定の波長のみを選択するように制御する
制御手段とを備えたことを特徴とする外部共振器型波長
可変半導体レーザ。
A semiconductor element including an active layer extending from an output end face, a window end face structure following the active layer, an antireflection film provided on the outside of the window end face structure, and a semiconductor device that passes through the window end face structure and the antireflection film. a condensing means for condensing the light emitted by the condensing means, a wavelength selection means for inputting the light condensed by the condensing means, selecting only a predetermined wavelength, and transmitting it in the opposite direction to the incident light; 1. An external cavity type wavelength tunable semiconductor laser comprising: control means for controlling the selection means to select only a predetermined wavelength.
JP33583789A 1989-12-25 1989-12-25 External resonator type variable wavelength semiconductor laser Pending JPH03195076A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP33583789A JPH03195076A (en) 1989-12-25 1989-12-25 External resonator type variable wavelength semiconductor laser

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP33583789A JPH03195076A (en) 1989-12-25 1989-12-25 External resonator type variable wavelength semiconductor laser

Publications (1)

Publication Number Publication Date
JPH03195076A true JPH03195076A (en) 1991-08-26

Family

ID=18292959

Family Applications (1)

Application Number Title Priority Date Filing Date
JP33583789A Pending JPH03195076A (en) 1989-12-25 1989-12-25 External resonator type variable wavelength semiconductor laser

Country Status (1)

Country Link
JP (1) JPH03195076A (en)

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Publication number Priority date Publication date Assignee Title
EP0717302A3 (en) * 1994-12-15 1997-08-13 Anritsu Corp External stabilization of the output power of a tunable wavelength light source
US5754571A (en) * 1994-12-15 1998-05-19 Anritsu Corporation Tunable wavelength light source apparatus for stabilizing power intensity by using external auto-power control
EP0776075A1 (en) * 1995-11-21 1997-05-28 Alcatel Optronics Laser device, in particular for optical pumping, and method of fabrication
US5717711A (en) * 1995-11-21 1998-02-10 Alcatel Optronics Laser device, notably for optical pumping, and method of fabricating it
EP1128507A3 (en) * 1999-12-22 2003-10-15 Anritsu Corporation Tunable laser source apparatus
JP2012089776A (en) * 2010-10-22 2012-05-10 Sony Corp Semiconductor laser device assembly
US9048619B2 (en) 2010-10-22 2015-06-02 Sony Corporation Laser diode assembly
US9219346B2 (en) 2010-10-22 2015-12-22 Sony Corporation Laser diode assembly
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WO2024180728A1 (en) * 2023-03-01 2024-09-06 三菱電機株式会社 Laser light source device, and apparatus having laser light source device applied thereto
JP7555530B1 (en) * 2023-03-01 2024-09-24 三菱電機株式会社 Laser light source device and laser light source device application equipment

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