JPH0447980Y2 - - Google Patents

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Publication number
JPH0447980Y2
JPH0447980Y2 JP10980286U JP10980286U JPH0447980Y2 JP H0447980 Y2 JPH0447980 Y2 JP H0447980Y2 JP 10980286 U JP10980286 U JP 10980286U JP 10980286 U JP10980286 U JP 10980286U JP H0447980 Y2 JPH0447980 Y2 JP H0447980Y2
Authority
JP
Japan
Prior art keywords
light
buffer layer
light receiving
waveguide
substrate
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
Application number
JP10980286U
Other languages
Japanese (ja)
Other versions
JPS6316475U (en
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 filed Critical
Priority to JP10980286U priority Critical patent/JPH0447980Y2/ja
Publication of JPS6316475U publication Critical patent/JPS6316475U/ja
Application granted granted Critical
Publication of JPH0447980Y2 publication Critical patent/JPH0447980Y2/ja
Expired legal-status Critical Current

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Description

【考案の詳細な説明】 (イ) 産業上の利用分野 本考案はレーザ光等をモニタするための光学モ
ニタに関する。
[Detailed description of the invention] (a) Industrial application field The present invention relates to an optical monitor for monitoring laser light, etc.

(ロ) 従来の技術 現在、光学デイスク読取用の装置としては、消
去用、読出用、書込用の各ビームを個々に出力で
きるように3つの独立した共振器を約100μm間隔
で並列させてなる3ビーム型の半導体レーザが提
案されている(実願昭61−40952号)。
(b) Prior art At present, optical disk reading devices use three independent resonators arranged in parallel at intervals of about 100 μm so that each beam for erasing, reading, and writing can be output individually. A three-beam type semiconductor laser has been proposed (Utility Application No. 61-40952).

このように近接した共振器から出射されるレー
ザ光を夫々独立にモニタするためには特開昭58−
102590号公報に開示されている如く共振器近傍に
共振器個々に対応してモニタ用の受光素子を配す
る方法が考えられる。
In order to independently monitor the laser beams emitted from adjacent resonators, Japanese Patent Laid-Open No. 58-
As disclosed in Japanese Patent No. 102590, a method of arranging a monitoring light receiving element for each resonator near the resonator can be considered.

第4図は斯る方法を模式的に示したもので、1
〜3は半導体レーザチツプであり、該チツプは各
チツプから出力されるレーザ光の光軸4間距離が
100μmとなるように整列配置されている。また、
上記各チツプ1〜3から出力されるレーザ光1a
〜3aのビーム広がり角θは10°である。5〜7
は受光素子であり、該受光素子は夫々上記チツプ
1〜3に対向して配される。
Figure 4 schematically shows such a method.
-3 are semiconductor laser chips, and the distance between the optical axes 4 of the laser beams output from each chip is
They are arranged so that the distance is 100 μm. Also,
Laser light 1a output from each of the above chips 1 to 3
The beam spread angle θ of ~3a is 10°. 5-7
are light-receiving elements, and the light-receiving elements are arranged to face the chips 1 to 3, respectively.

(ハ) 考案が解決しようとする問題点 然るに、斯る方法では第4図より明らかな如く
各チツプ1〜3と受光素子5〜7との距離が
500μm以上となると受光素子側において各レーザ
光が重畳することとなる。従つて各受光素子5〜
7は夫々対向するレーザチツプ以外のチツプから
出力されるレーザ光をも受光することとなり、
個々のレーザチツプ毎のモニタが不可能となる。
(c) Problems to be solved by the invention However, as is clear from FIG.
If it is 500 μm or more, each laser beam will be superimposed on the light receiving element side. Therefore, each light receiving element 5~
7 also receive laser light output from chips other than the laser chips facing each other,
It becomes impossible to monitor each individual laser chip.

尚、各チツプ1〜3と受光素子5〜7との距離
を500μm以下とすると上記問題は解決できるが、
このように近接させることはレーザチツプと受光
素子との光軸合せ及びワイヤボンドによる配線等
が複雑となり実用的ではない。
Note that the above problem can be solved by setting the distance between each chip 1 to 3 and the light receiving elements 5 to 7 to 500 μm or less, but
Providing the laser chip and the light receiving element in close proximity to each other in this manner complicates optical axis alignment between the laser chip and the light receiving element, wiring by wire bonding, etc., and is not practical.

更に上記問題点を解決する方法としては対応づ
けられた半導体レーザチツプと受光素子とを光フ
アイバで光学的に結合することによりレーザチツ
プと受光素子との間隔を必要な大きさとする方法
も考えられるが、斯る方法では光フアイバの取付
のために装置が大型化するという問題がある。
Furthermore, as a method to solve the above-mentioned problem, it is possible to optically couple the associated semiconductor laser chip and the light-receiving element with an optical fiber so that the distance between the laser chip and the light-receiving element is set to the required size. This method has a problem in that the device becomes larger due to the attachment of the optical fiber.

(ニ) 問題点を解決するための手段 本考案は斯る点に鑑みてなされたもので、その
構成的特徴は一導電型の半導体基板、該基板の1
主面に選択的に形成された受光領域、少なくとも
上記受光領域表面を除く上記基板の1主面上に積
層されたバツフア層、該バツフア層上に積層さ
れ、一端が上記受光領域に光学的に結合すると共
に上記バツフア層より大なる光屈折率を有する材
料からなる導波路を備えたことにある。
(d) Means for solving the problems The present invention has been made in view of the above points, and its structural features include a semiconductor substrate of one conductivity type, and one conductivity type of the substrate.
a light-receiving region selectively formed on the main surface; a buffer layer laminated on one main surface of the substrate excluding at least the surface of the light-receiving region; A waveguide made of a material having a larger optical refractive index than the buffer layer is provided.

(ホ) 作用 斯る構成では光を伝播するための導波路と受光
素子とを小型集積化できる。
(E) Effect With such a configuration, the waveguide for propagating light and the light receiving element can be integrated in a small size.

(ヘ) 実施例 第1図、第2図は本考案の実施例を示し、11
はn+型シリコン基板、12はn-型シリコン層で
あり、該層は上記基板11上にエピタキシヤル成
長させたものである。13〜15は第1〜第3受
光領域であり、該領域は上記シリコン層12表面
よりボロン等のP型不純物を選択的に拡散して形
成できる。16は二酸化シリコンからなるバツフ
ア層であり、該バツフア層は上記受光領域13〜
15表面を除くシリコン層12上に例えばスパツ
タ法により積層される。尚、上記バツフア層16
の各受光素子13〜15との境界部分はテーパ状
となつている。
(F) Embodiment Figures 1 and 2 show embodiments of the present invention.
12 is an n + type silicon substrate, and 12 is an n - type silicon layer, which is epitaxially grown on the substrate 11 described above. 13 to 15 are first to third light receiving regions, which can be formed by selectively diffusing P-type impurities such as boron from the surface of the silicon layer 12. Reference numeral 16 denotes a buffer layer made of silicon dioxide, and the buffer layer is connected to the light-receiving areas 13 to 16.
It is laminated on the silicon layer 12 except for the surface 15 by, for example, a sputtering method. Note that the buffer layer 16
The boundary portion between each of the light receiving elements 13 to 15 is tapered.

17〜19はアルミニウムからなる第1〜第3
電極であり、該電極はバツフア層16の右辺側に
整列されると共に夫々第1〜第3受光領域13〜
15に電気的に接続される。20は基板裏面に形
成された裏面電極である。
17 to 19 are the first to third parts made of aluminum.
The electrodes are arranged on the right side of the buffer layer 16 and are arranged in the first to third light receiving regions 13 to 13, respectively.
15. 20 is a back electrode formed on the back surface of the substrate.

21〜23は例えば米国コーニング社製ガラス
材料#7059からなるリツジ形の第1〜第3導波路
であり、該導波路はその一端がバツフア層16の
左辺端に100μmピツチで整列され、他端が夫々第
1〜第3受光素子13〜15表面に重畳されるよ
うにバツフア16層上にスパツタリング及びエツ
チング法を用いて積層される。
Reference numerals 21 to 23 are the first to third waveguides in the shape of a ridge made of glass material #7059 manufactured by Corning, Inc., for example. One end of the waveguide is aligned with the left end of the buffer layer 16 at a pitch of 100 μm, and the other end is aligned with the left end of the buffer layer 16 at a pitch of 100 μm. are laminated on the buffer layer 16 using sputtering and etching methods so as to be superimposed on the surfaces of the first to third light receiving elements 13 to 15, respectively.

斯る構成では、導波路21〜23の光屈折率は
約1.54、バツフア層16の光屈折率は約1.46、空
気の光屈折率は約1.0と導波路21〜23周囲の
屈折率が導波路21〜23のそれより小となつて
いる。従つて例えば導波路22左端より入射した
光は第2図中矢印で示す如く導波路22を通過し
て受光領域側に進むと共に受光領域14近傍のテ
ーパ部22aで反射されて光屈折率が約3.45と大
なる受光領域14に入射することとなる。尚、上
記テーパ部22aはバツフア層16表面のテーパ
部に沿つてできるものであり、従つてバツフア層
16にテーパが形成されていないときには導波路
22のテーパ部22aも形成されない。また、こ
のようなテーパ部22aが形成されないときに
は、導波路22を伝播してくる光の受光領域14
側への反射率は低下するため、受光領域14への
光入射量が低下する。
In such a configuration, the optical refractive index of the waveguides 21 to 23 is approximately 1.54, the optical refractive index of the buffer layer 16 is approximately 1.46, the optical refractive index of air is approximately 1.0, and the refractive index around the waveguides 21 to 23 is approximately the same as that of the waveguide. It is smaller than that of 21-23. Therefore, for example, light incident from the left end of the waveguide 22 passes through the waveguide 22 as shown by the arrow in FIG. The light will be incident on the light receiving area 14 which is as large as 3.45. The tapered portion 22a is formed along the tapered portion of the surface of the buffer layer 16, and therefore, when the buffer layer 16 is not tapered, the tapered portion 22a of the waveguide 22 is not formed either. Moreover, when such a taper part 22a is not formed, the light receiving area 14 of the light propagating through the waveguide 22
Since the reflectance to the side decreases, the amount of light incident on the light receiving area 14 decreases.

従つて、第1〜第3導波路21〜23の左端近
傍の夫々に半導体レーザチツプを配し、斯るチツ
プから出力されるレーザ光を上記対応する導波路
21〜23に入射せしめると、斯る入射レーザ光
は各導波路21〜23を伝播して第1〜第3受光
領域13〜15に導かれることとなる。
Therefore, if a semiconductor laser chip is placed near the left end of each of the first to third waveguides 21 to 23, and the laser light output from the chip is made to enter the corresponding waveguide 21 to 23, the The incident laser light propagates through each of the waveguides 21 to 23 and is guided to the first to third light receiving regions 13 to 15.

尚、本実施例では、導波路をリツジ型とした
が、第3図に示す如く導波路材料24を少なくと
も第1〜第3電極17〜19を除くバツフア層1
6全面に積層すると共に第1〜第3導波路21〜
23となる部分を除く材料層24上に金属25を
積層してなる金属装荷型としても良い。
In this embodiment, the waveguide is of a rigid type, but as shown in FIG.
6 are laminated on the entire surface and the first to third waveguides 21 to
A metal-loaded type may be used in which the metal 25 is laminated on the material layer 24 except for the portion 23.

(ト) 考案の効果 本考案の光学モニタは導波路と受光素子とを集
積化してあるので、導波路と半導体レーザチツプ
とを光学的に位置合せするだけでレーザチツプと
受光素子とが光学的に結合でき、かつ斯る結合の
ための構造は大型化しない。
(g) Effects of the invention Since the optical monitor of the invention integrates a waveguide and a light receiving element, the laser chip and the light receiving element can be optically coupled by simply aligning the waveguide and the semiconductor laser chip optically. and the structure for such coupling does not become large.

また、集積化技術により、導波路と受光領域と
は高い精度で位置合せ可能であるので、受光領域
の面積をかなり小さくすることができる。更に受
光領域の面積が小となるとその接合容量が小とな
るので、その応答速度は速くなり、レーザ出力の
速い変動に対応したモニタが可能となる。
Moreover, since the waveguide and the light receiving region can be aligned with high precision using integration technology, the area of the light receiving region can be considerably reduced. Furthermore, as the area of the light-receiving region becomes smaller, its junction capacitance becomes smaller, so its response speed becomes faster, making it possible to monitor rapid fluctuations in laser output.

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

第1図及び第2図は本考案の第1実施例を示す
斜視図及び断面図、第3図は本考案の第2の実施
例を示す斜視図、第4図は従来構造を示す模式図
である。 11……n+型シリコン基板、12……n-型シ
リコン層、13〜15……第1〜第3受光領域、
16……バツフア層、21〜23……第1〜第3
導波路。
1 and 2 are perspective views and sectional views showing the first embodiment of the present invention, FIG. 3 is a perspective view showing the second embodiment of the invention, and FIG. 4 is a schematic diagram showing the conventional structure. It is. 11...n + type silicon substrate, 12... n - type silicon layer, 13-15... first to third light receiving regions,
16... Batsuhua layer, 21-23... 1st to 3rd
waveguide.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 一導電型の半導体基板、該基板の1主面に選択
的に形成された受光領域、少なくとも上記受光領
域表面を除く上記基板の1主面上に積層されたバ
ツフア層、該バツフア層上に積層され、一端が上
記受光領域に光学的に結合すると共に上記バツフ
ア層より大なる光屈折率を有する材料からなる導
波路を備えたことを特徴とする光学モニタ装置。
a semiconductor substrate of one conductivity type; a light-receiving region selectively formed on one main surface of the substrate; a buffer layer laminated on one main surface of the substrate excluding at least the surface of the light-receiving region; a buffer layer laminated on the buffer layer; An optical monitor device comprising: a waveguide made of a material having a larger optical refractive index than the buffer layer and having one end optically coupled to the light receiving region.
JP10980286U 1986-07-17 1986-07-17 Expired JPH0447980Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP10980286U JPH0447980Y2 (en) 1986-07-17 1986-07-17

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10980286U JPH0447980Y2 (en) 1986-07-17 1986-07-17

Publications (2)

Publication Number Publication Date
JPS6316475U JPS6316475U (en) 1988-02-03
JPH0447980Y2 true JPH0447980Y2 (en) 1992-11-12

Family

ID=30988232

Family Applications (1)

Application Number Title Priority Date Filing Date
JP10980286U Expired JPH0447980Y2 (en) 1986-07-17 1986-07-17

Country Status (1)

Country Link
JP (1) JPH0447980Y2 (en)

Also Published As

Publication number Publication date
JPS6316475U (en) 1988-02-03

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