JPH02301166A - Structure of photodiode - Google Patents
Structure of photodiodeInfo
- Publication number
- JPH02301166A JPH02301166A JP1121914A JP12191489A JPH02301166A JP H02301166 A JPH02301166 A JP H02301166A JP 1121914 A JP1121914 A JP 1121914A JP 12191489 A JP12191489 A JP 12191489A JP H02301166 A JPH02301166 A JP H02301166A
- Authority
- JP
- Japan
- Prior art keywords
- mesa
- stripe
- semiconductor laser
- electrode
- face
- 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
Links
- 239000004065 semiconductor Substances 0.000 claims abstract description 18
- 239000000758 substrate Substances 0.000 claims abstract description 14
- 239000012535 impurity Substances 0.000 claims description 8
- 238000005530 etching Methods 0.000 abstract description 3
- 238000009792 diffusion process Methods 0.000 description 6
- 230000003287 optical effect Effects 0.000 description 4
- 229910000530 Gallium indium arsenide Inorganic materials 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 238000010586 diagram Methods 0.000 description 1
- 238000005468 ion implantation Methods 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 238000000034 method Methods 0.000 description 1
Landscapes
- Light Receiving Elements (AREA)
Abstract
Description
【発明の詳細な説明】 〔産業上の利用分野〕 この発説はホトダイオードに関するものである。[Detailed description of the invention] [Industrial application field] This statement is about photodiodes.
第3図は従来のポトスイオードの51を造を示す断面図
である。図において+Ilはn−工np基板、(2)は
n−工np バッファ層、(31は1−InGaAs層
。FIG. 3 is a sectional view showing the structure 51 of a conventional potosuiode. In the figure, +Il is an n-type np substrate, (2) is an n-type np buffer layer, and (31 is a 1-InGaAs layer).
+41 n n−InGaAs層、 151ij 81
N膜、161はp十拡散領域、(〕)はp電極、(8)
はn電極、(9)は入射光である。+41 n n-InGaAs layer, 151ij 81
N film, 161 is p diffusion region, (]) is p electrode, (8)
is the n-electrode, and (9) is the incident light.
次に動作について説明する。p十拡散領域16+上の受
光面に入射した入射光(9)は、1−1nGaAej台
131で電流に変換され、p電極+71 、 i電極(
8)より取り出される。Next, the operation will be explained. The incident light (9) that entered the light receiving surface on the p-10 diffusion region 16+ is converted into a current by the 1-1nGaAej stage 131, and the p-electrode +71, the i-electrode (
8) It is taken out from.
従来のホトダイオードは以上のような構造であるため、
ウェハの面に世直な方向からの入射光に対してのみ受光
が可能なことから、レーザウェハのエツチングによって
形成された端面溝内のような狭い空間内のレーザ元の受
光等には向かないという問題点かめつ之。Since the conventional photodiode has the above structure,
Since it can only receive light incident on the wafer surface from a normal direction, it is not suitable for receiving light from the laser source in a narrow space such as the end face groove formed by laser wafer etching. The problem is Kametsu.
この発明は上記のような問題点を解消するためになされ
たものであり、数μm〜数lOμm程度の狭い空間の入
射光を検出することができるホトダイオードのfla
e iることを目的とする。This invention was made to solve the above-mentioned problems, and is a photodiode fla that can detect incident light in a narrow space of several micrometers to several 10 micrometers.
The purpose is to
この発明に係るホトダイオードの構造は、半導体基板を
ストライプ状メサに形成し、その両側にpおよびn型の
不純物をそれぞれ拡散などによって注入し+p−1−n
の構造とし、ストライプの左右にp1L極およびn
電極をそれぞれ形成したものである。The structure of the photodiode according to the present invention is such that a semiconductor substrate is formed into a striped mesa, and p- and n-type impurities are implanted on both sides of the mesa by diffusion or the like.
structure, with p1L poles and n
Each electrode is formed separately.
この発明によるホトダイオードの構造は、半導体基板に
対して平行に形成されたストライプ状メサのp−1−、
n 構造により、半導体基板に対して平行な入射光に?
j しても受光が可能であり半導体レーザウェハのエツ
チング端面溝内のような狭い空間内の受光も可能になる
。The structure of the photodiode according to the present invention includes a striped mesa p-1- formed parallel to a semiconductor substrate,
n Due to the structure, does the incident light become parallel to the semiconductor substrate?
It is also possible to receive light even in a narrow space such as an etched end face groove of a semiconductor laser wafer.
以下この発明の一実蹴例について説明する。 A practical example of this invention will be described below.
第1図はホトダイオードの構造を示す断面図、第2図は
第1図のホトダイオードを半導体レーザウェハVC装着
した状況を示す断面図である。FIG. 1 is a sectional view showing the structure of a photodiode, and FIG. 2 is a sectional view showing the photodiode shown in FIG. 1 mounted on a semiconductor laser wafer VC.
図において、16)〜i91 ij 第3図の従来例に
示したものと同等であるので説明を省略する。In the figure, 16) to i91 ij are the same as those shown in the conventional example of FIG. 3, so their explanation will be omitted.
truけS、工(半絶縁性)工np基1&、[2)Hl
−InGaA11層、賭はn拡散領域、 Q41は1−
工npバッファ層、四は半導体レーザ(またはC)K工
C)次に、構造および動作について説明する。true S, engineering (semi-insulating) engineering np group 1&, [2) Hl
-InGaA11 layer, bet is n diffusion region, Q41 is 1-
(4) Semiconductor laser (or C) K (C) Next, the structure and operation will be explained.
第1図において、S、エーエnp基板qv上に形成され
た1−InGaAa層a21ハスドライブ状のメサに形
成され、左右の側面にpおよびn型の不純物を拡散され
、S、エーエnp基板upて対して平行にp−1−nの
構造となっている。また、pおよびn型不純物はストラ
イプ状メサの左右のウェハ面上にも拡散され、その上V
Cp 1!極;7)およびn電極(8)がそれぞれ形成
されている。In FIG. 1, a 1-InGaAa layer a21 formed in a hash drive-shaped mesa is formed on the S, AEN np substrate qv, and p- and n-type impurities are diffused on the left and right side surfaces, and the S, AEN np substrate up It has a p-1-n structure parallel to the . In addition, the p- and n-type impurities are also diffused onto the wafer surfaces on the left and right sides of the striped mesa, and the V
Cp 1! A pole; 7) and an n-electrode (8) are respectively formed.
S、I−工np基板dυに平行に入射して来た入射光(
9)はストライプ状メサの側面の受光面より取り入れら
れ、電流VC変換されて、p電極171.n電極(8)
より外部に取り出される。S, I - Incident light incident parallel to the np substrate dυ (
9) is taken in from the light-receiving surface on the side surface of the striped mesa, converted into a current VC, and sent to the p-electrode 171. n-electrode (8)
taken out to the outside.
このストライプ状メサの幅は例えば数μm % I O
数μmで高さは10〜数1011mであるため、第8図
に示すように半導体レーザウェハ園内に形成されたエツ
チング端面溝−内にストライプ状の受光面を押入して、
発光領域211からの光出力8を受光することが可能で
あり、ウェハ状態で半導体レーザまたは01!i工Cの
光出力特性が測定できる。The width of this striped mesa is, for example, several μm% IO
Since the height is several μm and the height is 10 to several 1011 m, a striped light-receiving surface is pushed into the etched end face groove formed in the semiconductor laser wafer garden as shown in FIG.
It is possible to receive the optical output 8 from the light emitting region 211, and the semiconductor laser or 01! The optical output characteristics of i-C can be measured.
なお、上記実施例では’S、I−工np基板α1Jを用
いたが他の材料1例えば81などの材料を用いたホトダ
イオードにも適用できる。また、nおよびp型不純物を
拡散によって注入したがイオン注入などの方法によって
もよい。In the above embodiment, the 'S, I-Engineering np substrate α1J is used, but the present invention can also be applied to photodiodes using other materials such as 1, 81, and the like. Further, although the n- and p-type impurities are implanted by diffusion, methods such as ion implantation may also be used.
以上のようにこの発明によれば、ストライプ状のメサ型
受光面を持つホトダイオードの構造としたことにより、
半導体レーザウェハのエツチング端面溝のような狭い部
分の光出力が検出でき、半導体レーザまたは01[i工
Cの光出力特性をウェハ状態で測定できる効果がある。As described above, according to the present invention, by adopting a photodiode structure having a striped mesa-type light-receiving surface,
The optical output of a narrow portion such as an etched end face groove of a semiconductor laser wafer can be detected, and the optical output characteristics of a semiconductor laser or 01[i-C can be measured in the wafer state.
第1図はこの発明の一実施gAJを示すホトダイオード
の断面図、第2図は第1図のホトダイオードを半導体レ
ーザウェハに装着し、た状況を示す断面図、第8図は従
来のホトダイオードを示す断面図である。
図において(6)はp十拡赦領域、(71はp電極、(
8)はn電極、(9)は入射光、几はS、エーエnp基
板、(121rii−InGjAs層、(13Hjn拡
散領域、0モはなお、図中、同一符号は同一、または相
当部分を示す。Fig. 1 is a sectional view of a photodiode showing an embodiment of the present invention gAJ, Fig. 2 is a sectional view showing the photodiode of Fig. 1 mounted on a semiconductor laser wafer, and Fig. 8 is a sectional view of a conventional photodiode. It is a diagram. In the figure, (6) is the p ten-extension region, (71 is the p electrode, (
8) is an n-electrode, (9) is an incident light, 几 is S, AEN Np substrate, (121rii-InGjAs layer, (13Hjn diffusion region), 0mo is the same reference numeral indicates the same or equivalent part in the figure. .
Claims (1)
サの一方の側面を含む上記メサの一方の側の半導体基板
にp型不純物を混入し、上記メサのもう一方の側面を含
む、上記メサのもう一方の側の半導体基板にn型不純物
を上記メサに混入されたp型不純物に達しない程度の深
さに混入し、上記メサを除く半導体基板上にp電極およ
びn電極をそれぞれ形成したことを特徴とするホトダイ
オードの構造。The surface of the semiconductor substrate is formed into a striped mesa, a p-type impurity is mixed into the semiconductor substrate on one side of the mesa including one side of the mesa, and the mesa including the other side of the mesa is mixed with a p-type impurity. An n-type impurity is mixed into the semiconductor substrate on the other side to a depth that does not reach the p-type impurity mixed into the mesa, and a p-electrode and an n-electrode are respectively formed on the semiconductor substrate excluding the mesa. A photodiode structure characterized by:
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1121914A JPH02301166A (en) | 1989-05-15 | 1989-05-15 | Structure of photodiode |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1121914A JPH02301166A (en) | 1989-05-15 | 1989-05-15 | Structure of photodiode |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH02301166A true JPH02301166A (en) | 1990-12-13 |
Family
ID=14823038
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP1121914A Pending JPH02301166A (en) | 1989-05-15 | 1989-05-15 | Structure of photodiode |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH02301166A (en) |
-
1989
- 1989-05-15 JP JP1121914A patent/JPH02301166A/en active Pending
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