JPS59101887A - Semiconductor laser device - Google Patents

Semiconductor laser device

Info

Publication number
JPS59101887A
JPS59101887A JP21235582A JP21235582A JPS59101887A JP S59101887 A JPS59101887 A JP S59101887A JP 21235582 A JP21235582 A JP 21235582A JP 21235582 A JP21235582 A JP 21235582A JP S59101887 A JPS59101887 A JP S59101887A
Authority
JP
Japan
Prior art keywords
semiconductor laser
light
laser
semiconductor
laser device
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
JP21235582A
Other languages
Japanese (ja)
Inventor
Hideaki Noguchi
英明 野口
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.)
NEC Corp
Original Assignee
NEC Corp
Nippon Electric Co 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 NEC Corp, Nippon Electric Co Ltd filed Critical NEC Corp
Priority to JP21235582A priority Critical patent/JPS59101887A/en
Publication of JPS59101887A publication Critical patent/JPS59101887A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S5/00Semiconductor lasers
    • H01S5/50Amplifier structures not provided for in groups H01S5/02 - H01S5/30

Landscapes

  • Physics & Mathematics (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • General Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Optics & Photonics (AREA)
  • Semiconductor Lasers (AREA)

Abstract

PURPOSE:To obtain a high output laser light without damaging the mode of an outputted light by a method wherein a semiconductor laser element having a structure of controlled transverse mode and a semiconductor laser element having a light amplification region of a larger cross-section are arranged in the direction of a light path. CONSTITUTION:When current is injected into the semiconductor element 1 whose transverse mode is controlled, resulting in laser oscillation, the laser light 35 having some radiation angle 36 is radiated. A part of this laser light 35 is injected into the semiconductor element 2. At this time, the injection of suitable current into the semiconductor laser element causes the semiconductor laser element 2 to perform laser oscillation and thus to radiate the laser light 37. Since the area of a part of radiation this laser light 37, i.e., the area of the light emitting region of the semiconductor element 2 is wide, the obtained total output of the laser light 37 becomes large even when the light density of the light emitting region is low to some degree.

Description

【発明の詳細な説明】 本発明は横モードが制御された半導体レーザ装置の高出
力化に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to increasing the output of a semiconductor laser device in which the transverse mode is controlled.

従来の半導体レーザ装置において、高出力のレーザ光を
得ようとする場合には、次の2つの相反的な問題点があ
る。第1の問題点は、横モードが制御された半導体レー
ザ装置は、その発光領域が非常に狭いので、高出力動作
時にはその高い光密度のため、特に共振器端面での劣化
が生じやすく、信頼性上の問題があることである。逆に
発光領域を広くした半導体レーザ装置においては、レー
ザ出力を大きくすると、レーザ光の横モードが0次モー
ドから1次、2次としだいに高次モードに移行する問題
がある。これが第2の問題点である。
In conventional semiconductor laser devices, there are two contradictory problems when trying to obtain high-output laser light. The first problem is that a semiconductor laser device with a controlled transverse mode has a very narrow light emitting region, so during high-output operation, its high light density tends to cause deterioration, especially at the cavity end facets, making it unreliable. There are sexual problems. On the other hand, in a semiconductor laser device with a wide light emitting region, when the laser output is increased, the transverse mode of the laser beam gradually shifts from the zero-order mode to the first-order, second-order, and higher-order modes. This is the second problem.

本発明は、上記問題点を克服して、横モードが制御され
た高出力半導体レーザ装置の構造を提供することを目的
とし、この様な目的は2台の半導体レーザ素子を光路方
向に直列に並べた構造を有し、一方の半導体レーザ素子
は少なくとも横モードが制御された構造を有し、かつ他
方の半導体レーザ素子は少なくとも前記横モード制御さ
れた半導体レーザ素子よりも大きい断面積の光増幅領域
を有することを特徴とする半導体レーザ装置によって達
成される。すなわち、高出力のレーザ光を得るためには
、端面での劣化が起こらない様に光増幅領域の断面積を
大きくすることにより発光領域の面積を大きくして、共
振器端面での光密度が高くなりすぎない様にすればよい
An object of the present invention is to overcome the above-mentioned problems and provide a structure for a high-power semiconductor laser device in which the transverse mode is controlled. one semiconductor laser element has a structure in which at least a transverse mode is controlled, and the other semiconductor laser element has an optical amplification device having a cross-sectional area larger than at least the transverse mode controlled semiconductor laser element. This is achieved by a semiconductor laser device characterized by having a region. In other words, in order to obtain high-output laser light, the area of the light emitting region is increased by increasing the cross-sectional area of the optical amplification region to prevent deterioration at the end face, and the light density at the resonator end face is increased. Just make sure it doesn't get too high.

前述した様に、従来の構造の半導体レーザ装置において
は、発光領域の面積を大きくすると、高次モードの発振
となりやすい。しかし外部光を注入することにより、高
次モードの発生を抑制することが可能である。本発明は
、この効果をたくみに利用し、横モード制御された高出
力半導体レーザ装置を提供するものである。
As described above, in a semiconductor laser device having a conventional structure, when the area of the light emitting region is increased, higher-order mode oscillation is likely to occur. However, by injecting external light, it is possible to suppress the generation of higher-order modes. The present invention makes full use of this effect to provide a high-power semiconductor laser device with transverse mode control.

本発明によれば2台の半導体レーザ素子を光路方向に並
べた構造を有し、一方の半導体レーザ素子は少なくとも
横モードが制御された構造を有し、かつ他方の半導体レ
ーザ素子は少なくとも上記横モードが制御された半導体
レーザ素子よシも大きい断面積の光増幅領域を有するこ
とを特徴とする半導体レーザ装置が得られる。
According to the present invention, two semiconductor laser elements are arranged in the optical path direction, one semiconductor laser element has a structure in which at least the transverse mode is controlled, and the other semiconductor laser element has at least the above-mentioned lateral mode. A semiconductor laser device characterized in that it has an optical amplification region with a larger cross-sectional area than a mode-controlled semiconductor laser element can be obtained.

以下、本発明を実施例の具体的−例に基づいて詳細に説
明するb 第1図は本発明による半導体レーザ装置の基本的構造を
示す図である。すなわち、横モード制御された半導体レ
ーザ菓子1と前記半導体レーザ素子1よりも広い幅の光
増幅領域を有、する半導体レーザ素子2を溝3で隔てて
光路方向に直列に設けた構造であり、各々の半導体レー
ザ素子1及び2は、それぞれ面9,1o間及び面11.
12間を共振器として構成し、それぞれに電極6,7を
付ける。電極6,8間にはレーザ発振に十分な電流を流
し、7,8の電極間には外部から光が注入されなければ
レーザ発振はしないが、外部から光が入ればレーザ発振
する程度にバイアスしておく。
Hereinafter, the present invention will be described in detail based on specific examples of embodiments.b FIG. 1 is a diagram showing the basic structure of a semiconductor laser device according to the present invention. That is, it has a structure in which a semiconductor laser confectionery 1 whose transverse mode is controlled and a semiconductor laser element 2 having an optical amplification region wider than the semiconductor laser element 1 are arranged in series in the optical path direction with a groove 3 separating them. Each of the semiconductor laser elements 1 and 2 is arranged between surfaces 9 and 1o and between surfaces 11 and 11, respectively.
12 is configured as a resonator, and electrodes 6 and 7 are attached to each. A current sufficient for laser oscillation is passed between electrodes 6 and 8, and a bias is applied between electrodes 7 and 8 to the extent that laser oscillation will not occur unless light is injected from the outside, but the laser will oscillate if light enters from the outside. I'll keep it.

なお図中、4,5はともにPN接合面を示す。Note that in the figure, both 4 and 5 indicate the PN junction surface.

第2図には外部から光が注入された場合の半導体レーザ
素子の電流I−光出カP特性を示す。図中横軸は′成流
工であり、縦軸は光出力Pである。
FIG. 2 shows the current I-light output P characteristics of the semiconductor laser device when light is injected from the outside. In the figure, the horizontal axis is the flow rate, and the vertical axis is the optical output P.

さらにPexは外部からの注入光の強度でありP2>P
 1 > Oである。すなわち、実線は外部から光を注
入されない場合であり、破線は外部から光を注入された
場合の電流■−光出カP特性である。第2図により、半
導体レーザ素子は適当な電流値にバイアスしておくこと
により、外部注入光強度に応じた強度でレーザ発振する
ことがわかる。
Furthermore, Pex is the intensity of the injected light from the outside, and P2>P
1>O. That is, the solid line is the case where no light is injected from the outside, and the broken line is the current - light output P characteristic when the light is injected from the outside. From FIG. 2, it can be seen that by biasing the semiconductor laser element to an appropriate current value, the semiconductor laser element oscillates with an intensity corresponding to the intensity of externally injected light.

ところで、一般に半導体レーザ装置はレーザ光強度が強
くなると発振モードが不安定になりやすく、高次モード
へ移行しやすい。しかし、外部から光を注入することに
より、発振モードを安定化できることが知られている。
By the way, in general, in a semiconductor laser device, when the laser light intensity increases, the oscillation mode tends to become unstable and tends to shift to a higher-order mode. However, it is known that the oscillation mode can be stabilized by injecting light from the outside.

第3図には本発明による半導体レーザ装置の動作状態を
示す。図中1.2はそれぞれ、横モードが制御された半
導体レーザ素子及び前記半導体レーザ素子よりも広い幅
の光増幅領域を有する半導体レーザ素子であり、各々の
半導体レーザ素子は、幅32の光増幅領域31及び幅3
4の光増幅領域33を有する。ここで今、横モードが制
御された半導体レーザ素子1に電流を注入し、レーザ発
振させると、ある放射角37を有するレーザ光35が出
射きれる。このレーザ光35の一部は、半導体レーザ素
子2に注入される。この時、半導体レーザ素子に適当な
電流が注入されていると、半導体レーザ素子2はレーザ
発振を起こし、レーザ光37を出射する。このレーザ光
37の出射部分の面積、すなわち半導体レーザ素子2の
発光領域の面積は広いので、発光領域の光密度がある程
度低(−rも得られるレーザ光37の総出力は太きいも
のとなる。
FIG. 3 shows the operating state of the semiconductor laser device according to the present invention. In the figure, 1.2 is a semiconductor laser device with a controlled transverse mode and a semiconductor laser device having an optical amplification region wider than the semiconductor laser device, and each semiconductor laser device has an optical amplification region of width 32. Area 31 and width 3
It has four optical amplification regions 33. Now, when a current is injected into the semiconductor laser element 1 whose transverse mode has been controlled and the semiconductor laser element 1 is caused to oscillate, a laser beam 35 having a certain radiation angle 37 is emitted. A part of this laser light 35 is injected into the semiconductor laser element 2. At this time, if an appropriate current is injected into the semiconductor laser element 2, the semiconductor laser element 2 causes laser oscillation and emits a laser beam 37. Since the area of the emission part of this laser beam 37, that is, the area of the light emitting region of the semiconductor laser element 2 is wide, the light density of the light emitting region is low to some extent (-r is also obtained, and the total output of the laser beam 37 is large. .

上記実施例においては、上記半導レーザ素子2の光増幅
領域の断面積を広くするため、光増幅領域の幅を変えて
該断面積を広くしたが、エビ成長方法全工夫して光増幅
領域の厚さを厚くして、光増幅領域の断面積を広くする
ことも可能である。
In the above embodiment, in order to widen the cross-sectional area of the optical amplification region of the semiconductor laser device 2, the width of the optical amplification region was changed to increase the cross-sectional area. It is also possible to widen the cross-sectional area of the optical amplification region by increasing the thickness of the optical amplification region.

この場合にも全く同様の効果を期待できる。In this case, exactly the same effect can be expected.

以上述べた様に、本発明によれば適当な電流が注入され
ている広い断面積の光増幅領域を有する半導体レーザ素
子2に、横モードが制御された半導体レーザ素子1の出
力光35を注入することにより、出力光35のモードを
損うことなしに高出力のレーザ光37を得ることが可能
となる。
As described above, according to the present invention, the output light 35 of the semiconductor laser device 1 whose transverse mode is controlled is injected into the semiconductor laser device 2 having an optical amplification region with a wide cross section into which an appropriate current is injected. By doing so, it becomes possible to obtain high-power laser light 37 without damaging the mode of output light 35.

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

第1図は本発明による半導体レーザ装置を示す図、第2
図は従来の半導体レーザ装置に外部から光を注入した場
合の特性を示す図、第3図は本発明による半導体レーザ
装置の動作状態を示す図である。 1・・・・・・横モードが制御された半導体レーザ素子
、2・・・・・・広い断面積の光増幅領域を有する半導
体レーザ素子。 2 / 図 1?図 ′ 、ネI 第3(2)
FIG. 1 is a diagram showing a semiconductor laser device according to the present invention, and FIG.
This figure shows the characteristics when light is injected from the outside into a conventional semiconductor laser device, and FIG. 3 is a diagram showing the operating state of the semiconductor laser device according to the present invention. 1... Semiconductor laser element with controlled transverse mode; 2... Semiconductor laser element having an optical amplification region with a wide cross-sectional area. 2 / Figure 1? Figure ′, Ne I No. 3 (2)

Claims (1)

【特許請求の範囲】[Claims] 2台の半導体レーザ素子を光路方向に並べた構造を有し
、一方の半導体レーザ素子は少なくとも横モードが制御
された構造を有し、かつ他方の半導体レーザ素子は少な
くとも前記横モードが制御された半導体レーザ素子より
も大きい断面積の光増幅領域を有することを特徴とする
半導体レーザ装置。
It has a structure in which two semiconductor laser elements are arranged in the optical path direction, one semiconductor laser element has a structure in which at least the transverse mode is controlled, and the other semiconductor laser element has a structure in which at least the transverse mode is controlled. A semiconductor laser device characterized by having an optical amplification region having a larger cross-sectional area than a semiconductor laser element.
JP21235582A 1982-12-03 1982-12-03 Semiconductor laser device Pending JPS59101887A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP21235582A JPS59101887A (en) 1982-12-03 1982-12-03 Semiconductor laser device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP21235582A JPS59101887A (en) 1982-12-03 1982-12-03 Semiconductor laser device

Publications (1)

Publication Number Publication Date
JPS59101887A true JPS59101887A (en) 1984-06-12

Family

ID=16621166

Family Applications (1)

Application Number Title Priority Date Filing Date
JP21235582A Pending JPS59101887A (en) 1982-12-03 1982-12-03 Semiconductor laser device

Country Status (1)

Country Link
JP (1) JPS59101887A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5070511A (en) * 1987-11-09 1991-12-03 Siemens Aktiengesellschaft Laser arrangement having at least one laser resonator and a passive resonator coupled thereto
JPH03274785A (en) * 1990-03-23 1991-12-05 A T R Koudenpa Tsushin Kenkyusho:Kk Light amplifier

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5070511A (en) * 1987-11-09 1991-12-03 Siemens Aktiengesellschaft Laser arrangement having at least one laser resonator and a passive resonator coupled thereto
JPH03274785A (en) * 1990-03-23 1991-12-05 A T R Koudenpa Tsushin Kenkyusho:Kk Light amplifier

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