JPS59129483A - Hall element - Google Patents
Hall elementInfo
- Publication number
- JPS59129483A JPS59129483A JP58004507A JP450783A JPS59129483A JP S59129483 A JPS59129483 A JP S59129483A JP 58004507 A JP58004507 A JP 58004507A JP 450783 A JP450783 A JP 450783A JP S59129483 A JPS59129483 A JP S59129483A
- Authority
- JP
- Japan
- Prior art keywords
- hall element
- square
- film
- substrate
- resist film
- 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
Abstract
Description
【発明の詳細な説明】 産業上の利用分野 本発明はホール効果を利用したホール素子に関する。[Detailed description of the invention] Industrial applications The present invention relates to a Hall element that utilizes the Hall effect.
従来例の構成とその問題点
現在化合初手導体を用いたホール素子としてはI n
S bの蒸着膜を用いたものと半絶縁性のC1riLA
s基板上にn形の薄層を設けたものが多い。GaAsを
用いたものは第1図aの側断面図、bの平面図に示すよ
うに半絶縁性基板1上にエピタキシャル法またはイオン
注入法により薄いn形層2を設け、このR42tメサエ
ッチにエフ十字形のホール素子として形成する。尚、3
は電極である。The structure of the conventional example and its problems Currently, as a Hall element using a compound initial conductor, I n
One using a vapor-deposited film of Sb and the other using semi-insulating C1riLA.
Many have an n-type thin layer provided on an s-substrate. In the case of using GaAs, as shown in the side cross-sectional view in Fig. 1a and the plan view in Fig. 1b, a thin n-type layer 2 is formed on a semi-insulating substrate 1 by epitaxial method or ion implantation method, and etching is performed on this R42t mesa etch. It is formed as a cross-shaped Hall element. In addition, 3
is an electrode.
22,2・
磁界のない時はホール素子の出力(ホール電圧)は理想
的には零でなければならない。しかし現実には結晶欠陥
による電流の流れの不均一性や、ホール素子のパターン
ユング時の形状の非対称性などにより、無磁界でも出力
端に僅な電位差を生じる。これを不平衡電圧と呼び;こ
の値は小さいほどよい。ところが、従来のようにメサエ
ッチでパターンユングを行うと、エツチングのムラなど
によりホール素子の形状の対称性が崩れ易くなり、また
メサエッチで露出したパターンの端面が汚染されるなど
の原因によりかなりの量の不平衡電圧の発生は、実際上
、避けられなかった。22, 2. Ideally, the output of the Hall element (Hall voltage) should be zero when there is no magnetic field. However, in reality, a slight potential difference occurs at the output end even in the absence of a magnetic field due to non-uniformity in current flow due to crystal defects and asymmetry in the shape of the Hall element during pattern Jung. This is called unbalanced voltage; the smaller this value is, the better. However, when pattern etching is performed using mesa etch as in the past, the symmetry of the Hall element shape tends to be lost due to uneven etching, and the end face of the pattern exposed by mesa etch is contaminated, resulting in a considerable amount of etching. The occurrence of unbalanced voltages was practically unavoidable.
1だポール素子のブレーナ化は、半絶縁性基板の表面の
熱変成により1だ成功していない。Converting a single pole element into a brainer has not been successful due to thermal transformation of the surface of the semi-insulating substrate.
発明の目的
この発明は従来避けることのできなかった不平衡電圧を
大幅低減し、かつ製造プロセスも簡略化可能なホール素
子を提供するものである。OBJECTS OF THE INVENTION The present invention provides a Hall element that can significantly reduce the unbalanced voltage that could not be avoided in the past, and that can also simplify the manufacturing process.
発明の構成
本発明は、半絶縁性牛導体基板の表面に正方形3ページ
の導電領域を形成し、前記正方形導電領域の四隅にオー
ミック電極を設けた構造のホール素子であυ、これによ
り、上述の目的全達成し得ろ。Structure of the Invention The present invention is a Hall element having a structure in which three square conductive regions are formed on the surface of a semi-insulating conductive substrate, and ohmic electrodes are provided at the four corners of the square conductive regions. Achieve all of your goals.
実施例の説明
第2図は本発明実施例装置の側断面図aおよび平面図す
である。DESCRIPTION OF EMBODIMENTS FIG. 2 is a side sectional view a and a plan view of an apparatus according to an embodiment of the present invention.
この発明においては半絶縁性基板11として例えば厚さ
3oOμmでCrドープの比抵抗108.QlのGaA
s単結晶を用い、これを所定表面層部のみ化学エツチン
グした後にイオン注入1呆護膜として1000人のS
io 2膜を形成する。In the present invention, the semi-insulating substrate 11 is, for example, 300 μm thick and Cr-doped with a specific resistance of 108. GaA of Ql
Using S single crystal, chemically etching only a predetermined surface layer, and then applying 1,000 S as a protective film for ion implantation.
io2 film is formed.
n形ドーパントとして28Si”e加速エネルギー13
0KaVでドーズKl: 6 X 10 CTL
で選択注入する。選択注入のマスクとしてはポジ型レジ
スト膜177 m k用い、注入後ポジ型レジスト膜と
SiO2保護膜を除去する。この後に水素雰囲気中で8
50℃16分間のキャップレスアニールを行い正方形の
深さ0.3μmの埋込みn形層12を形成した。28Si”e acceleration energy 13 as n-type dopant
Dose Kl at 0KaV: 6 x 10 CTL
Inject selectively. A positive resist film 177mk is used as a mask for selective implantation, and after the implantation, the positive resist film and the SiO2 protective film are removed. After this, 8
Capless annealing was performed at 50° C. for 16 minutes to form a square buried n-type layer 12 with a depth of 0.3 μm.
n形層12へのオーミック性電極は、捷ず5i02膜全
5000人形成しポジ型ホトレジストマスクを用いて、
電極部の土にあろ5iOz膜のみを化学エツチングで除
去した後にAuGe、Niを蒸着し。The ohmic electrode to the n-type layer 12 was formed by forming a total of 5,000 5i02 films and using a positive photoresist mask.
After removing only the Aro5iOz film on the soil of the electrode part by chemical etching, AuGe and Ni were deposited.
ポジ型ホトレジストを除去して電極を形成するいわゆる
リフトオフ法を用いろ。これを440°Cで熱処理し、
更にこの電極の上にリフトオフ法でn。Use the so-called lift-off method, which removes the positive photoresist and forms the electrodes. This was heat treated at 440°C,
Furthermore, n was applied on top of this electrode using the lift-off method.
Pt、Aui形成して電極13とした。An electrode 13 was formed by forming Pt and Au.
n形層12の一辺は0.36m1lでこの周辺にダイシ
ング幅0.025uをとり、チップとしてはq4肌の正
方形である。One side of the n-type layer 12 is 0.36 ml, a dicing width of 0.025 u is taken around this, and the chip is a square with q4 skin.
この構造においても正方形のn形導電領域12の外側は
アニール時の熱変成によって絶縁性が低下しているが、
導電領域が十字形のパターンに比べて内部抵抗が低いの
で領域外のインピーダンスの低下に工ろ影響を小ζくお
さえろことができた。Even in this structure, the insulation properties of the outside of the square n-type conductive region 12 are reduced due to thermal transformation during annealing.
Since the conductive region has a lower internal resistance than a cross-shaped pattern, it was possible to suppress the influence of the machining process on the decrease in impedance outside the region.
さて、前述の不平衡電圧ヲvHoとし、 I KGの磁
場内でホール素子の入力端子に6v印加したときに生じ
るホール電圧から不平衡電圧を差し引いた値を無負荷ホ
ール電圧vHとすると、不平衡率この不平衡率で従来の
十字形パターンホール素子と本発明実施例のホール素子
を比較すると、±6%に対して±3%と小さくすること
ができた。Now, if the aforementioned unbalanced voltage is vHo, and the unloaded Hall voltage vH is the value obtained by subtracting the unbalanced voltage from the Hall voltage that occurs when 6V is applied to the input terminal of the Hall element in the magnetic field of I KG, then the unbalanced Hall voltage is When comparing the conventional cross-shaped pattern Hall element and the Hall element of the embodiment of the present invention with respect to this unbalance ratio, it was possible to reduce the unbalance ratio to ±3% compared to ±6%.
発明の効果
以上のようにこの発明はホール素子1GaAs基板でプ
レーナ化することにより、従来避けることのできなかっ
た不平衡電圧を低減させた。また製造プロセスも簡略化
することができ、実用的価値は犬なるものである。Effects of the Invention As described above, the present invention reduces the unbalanced voltage that could not be avoided in the past by making the Hall element planar with a 1GaAs substrate. The manufacturing process can also be simplified, and the practical value is significant.
第1図1!L、bはメサエッチによるホール素子の側断
面図、平面図、第2図a、bはこの発明の実施例による
ホール素子の側断面図、平面図を示す。
11・・・・・・半絶縁性基板、12・・・・・・n型
導電領域。
13・・・・・・電極。
代理人の氏名 弁理士 中 屋敷 男 ほか1名第1図
第2図Figure 1 1! L and b show a side sectional view and a plan view of a Hall element formed by mesa etching, and FIGS. 2a and 2b show a side sectional view and a plan view of a Hall element according to an embodiment of the present invention. 11... Semi-insulating substrate, 12... N-type conductive region. 13... Electrode. Name of agent: Patent attorney Naka Yashiki, and one other person Figure 1 Figure 2
Claims (1)
、前記正方形導電層の四隅にオーミック電極金有するホ
ール素子。A Hall element having a square thin layer of a predetermined conductivity type on the surface of a highly durable substrate, and having ohmic electrodes at the four corners of the square conductive layer.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP58004507A JPS59129483A (en) | 1983-01-14 | 1983-01-14 | Hall element |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP58004507A JPS59129483A (en) | 1983-01-14 | 1983-01-14 | Hall element |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS59129483A true JPS59129483A (en) | 1984-07-25 |
Family
ID=11585961
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP58004507A Pending JPS59129483A (en) | 1983-01-14 | 1983-01-14 | Hall element |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS59129483A (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4883773A (en) * | 1986-12-16 | 1989-11-28 | Sharp Kabushiki Kaisha | Method of producing magnetosensitive semiconductor devices |
WO2000052424A1 (en) * | 1999-02-26 | 2000-09-08 | Fraunhofer-Gesellschaft zur Förderung der angewandten Forschung e.V. | Hall sensor with a reduced offset signal |
JP2013157393A (en) * | 2012-01-27 | 2013-08-15 | Asahi Kasei Electronics Co Ltd | Magnetoelectric transducer |
US10333057B2 (en) | 2017-03-23 | 2019-06-25 | Asahi Kasei Microdevices Corporation | Hall element |
-
1983
- 1983-01-14 JP JP58004507A patent/JPS59129483A/en active Pending
Cited By (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4883773A (en) * | 1986-12-16 | 1989-11-28 | Sharp Kabushiki Kaisha | Method of producing magnetosensitive semiconductor devices |
WO2000052424A1 (en) * | 1999-02-26 | 2000-09-08 | Fraunhofer-Gesellschaft zur Förderung der angewandten Forschung e.V. | Hall sensor with a reduced offset signal |
US6639290B1 (en) * | 1999-02-26 | 2003-10-28 | Fraunhofer-Gesellschaft Zur Foerderung, Der Angewandten Forschung E.V. | Hall sensor with a reduced offset signal |
CZ301988B6 (en) * | 1999-02-26 | 2010-08-25 | Fraunhofer-Gesellschaft Zur Foerderung Der Angewandten Forschung E. V. | Hall sensor with reduced offset signal |
JP2013157393A (en) * | 2012-01-27 | 2013-08-15 | Asahi Kasei Electronics Co Ltd | Magnetoelectric transducer |
US10333057B2 (en) | 2017-03-23 | 2019-06-25 | Asahi Kasei Microdevices Corporation | Hall element |
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