JPH0115135B2 - - Google Patents
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- Publication number
- JPH0115135B2 JPH0115135B2 JP56072464A JP7246481A JPH0115135B2 JP H0115135 B2 JPH0115135 B2 JP H0115135B2 JP 56072464 A JP56072464 A JP 56072464A JP 7246481 A JP7246481 A JP 7246481A JP H0115135 B2 JPH0115135 B2 JP H0115135B2
- Authority
- JP
- Japan
- Prior art keywords
- nitrogen
- mobility
- substrate
- indium
- antimony
- 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
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Classifications
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10P—GENERIC PROCESSES OR APPARATUS FOR THE MANUFACTURE OR TREATMENT OF DEVICES COVERED BY CLASS H10
- H10P14/00—Formation of materials, e.g. in the shape of layers or pillars
- H10P14/20—Formation of materials, e.g. in the shape of layers or pillars of semiconductor materials
- H10P14/29—Formation of materials, e.g. in the shape of layers or pillars of semiconductor materials characterised by the substrates
- H10P14/2901—Materials
- H10P14/2921—Materials being crystalline insulating materials
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10P—GENERIC PROCESSES OR APPARATUS FOR THE MANUFACTURE OR TREATMENT OF DEVICES COVERED BY CLASS H10
- H10P14/00—Formation of materials, e.g. in the shape of layers or pillars
- H10P14/20—Formation of materials, e.g. in the shape of layers or pillars of semiconductor materials
- H10P14/24—Formation of materials, e.g. in the shape of layers or pillars of semiconductor materials using chemical vapour deposition [CVD]
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10P—GENERIC PROCESSES OR APPARATUS FOR THE MANUFACTURE OR TREATMENT OF DEVICES COVERED BY CLASS H10
- H10P14/00—Formation of materials, e.g. in the shape of layers or pillars
- H10P14/20—Formation of materials, e.g. in the shape of layers or pillars of semiconductor materials
- H10P14/34—Deposited materials, e.g. layers
- H10P14/3402—Deposited materials, e.g. layers characterised by the chemical composition
- H10P14/3414—Deposited materials, e.g. layers characterised by the chemical composition being group IIIA-VIA materials
- H10P14/3422—Antimonides
Landscapes
- Hall/Mr Elements (AREA)
- Physical Deposition Of Substances That Are Components Of Semiconductor Devices (AREA)
Description
本発明は、半導体として各種用途に供されるイ
ンジウム―アンチモン系混合結晶の製造方法、さ
らに詳しくいえば電気特性の向上したインジウム
―アンチモン系混合結晶の製造方法に関するもの
である。
インジウム―アンチモン(以下InSbと示す)
の薄膜は、常温における移動度78000cm2/V・sec
と、インジウム―ヒ素の30000cm2/V・secやガリ
ウム―ヒ素の7000cm2/V・secに比べ非常に高い
値を示し、ホール素子や磁気抵抗素子の素材とし
て優れたものであるため、最近、ダイレクトドラ
イブモーター用位置検出装置やVTR、音響機器
などの無接点ポテンシヨメーターとして注目され
るようになつた。
ところで、通常ホール効果を考えるときには、
ホール係数RHとホール移動度μHとが重要なパラ
メーターとなる。そして、添附図面に示す形状で
パターニング及び電極付けを行つたInSbのサン
プルについて、入力電極1,2を定電流電源Iに
接続したときの出力電極3,4間に生じる電圧を
VHiとし、入力電極1,2を定電圧電源Vに接続
したときの出力電極3,4間に生じる電圧をVHv
とした場合、VHiとVHvとはそれぞれ次の式によつ
て求められる。
VHi=I/t・RH・B・I・f …(1)
VHv=ω/l・μH・B・V・f …(2)
ただし、tはサンプルの膜厚、lはパターンの
長さ、ωはパターンの幅であり、Bは印加される
外部磁場の磁束密度、Iはサンプルに流される電
流、Vはサンプル印加される電圧、fはサンプル
の形状因子、RHはサンプルのホール係数、μHは
ホール移動度である。
この式(1)から明らかなように、出力電圧は、サ
ンプルの膜厚に反比例するので、高感度のホール
素子や磁気抵抗効果素子とするときは、薄膜にす
る方がよい。
またInSbは、その禁制帯の幅が狭いので、前
記式(1)のホール係数RHは温度により著しく変化
し、実用時には、定電流出力電圧VHiの温度依存
性が大きいという結果になつて現われる。
他方、式(2)により示されるホール移動度μHは、
温度による変化が比較的少ないので、実用上、
InSbのホール素子は、もつぱら定電圧下で用い
られ、したがつてホール係数を大きくすることよ
りも、移動度を高くすることが要望されている。
従来、高い移動度のInSb薄膜を製造する方法
として、バルク単結晶を切り出して研摩し、薄膜
化する方法が知られている。このようにして得ら
れる薄膜は、優れた特性を有するものであるが、
単結晶の切り出しや研摩には、多量のロスを生じ
高価なInSb単結晶を無駄に費消することになる
ので、工業的方法として必ずしも適当ではない。
また、InとSbとをいつたん基板上に10μm程度
の厚さに蒸着その他の手段で付着させておき、次
いでゾーンメルトした後、研摩し、薄膜化する方
法も提案されている(特開昭50―9373号公報)。
しかし、この方法は作業が複雑であり、工業的に
実施する場合にかなり制約されるのを免れない。
ところで、InSb薄膜を製造する最も簡便な方
法は、蒸着操作だけで基板上に付着させる方法で
あり、これまで数多くの蒸着方法が試みられてき
たが、膜厚1μm程度で、ホール移動度25000cm2/
V・sec以上の薄膜を得ることはできなかつた。
本発明らは先に基板におけるInとSbの原子到
達速度比(AIn/Asb)を1.1〜1.7に制御するこ
とによりInSb結晶と、単体のIn結晶からなる組
成及び特性のバラツキのないInSb複合結晶を得
る方法を提案したが、さらに研究を重ねた結果、
特定の条件下で処理することによりさらに移動度
を向上させうることを見出し、この知見に基づい
て本発明をなすに至つた。
すなわち、本発明は、基板上にインジウム及び
アンチモンを蒸着させてインジウム―アンチモン
系混合結晶を製造するに当り、窒素の存在下、基
板上でのインジウムとアンチモンとの原子到達速
度比AIn/ASbが1.1〜1.7となる条件のもので蒸
着処理することを特徴とする方法を提供するもの
である。この場合、窒素は少なくとも大気の成分
比よりも多い割合で存在させるのが好ましい。
本発明者らは、先に提案した製造方法に基づい
て、より高い移動度をめざして、Ar等の希ガス
を蒸着中に導入したが、かえつて移動度を低下さ
せる結果となつたが、窒素を蒸着中に導入した場
合は、移動度の大きな向上がみられた。この際重
要なことは、窒素が大気の成分比より多く入つて
いることである。窒素の他のガスに対する相対量
は、最初の到達真空度と導入後の真空度によつて
変化する。例えば最初の真空度が10-6Torrで5
×10-6Torrまで窒素導入によつて真空度を下げ
た時には、窒素量比は約90mol%になる。驚くべ
きことには、この程度の雰囲気の変化(空気中で
の80mol%から90mol%へ)によつてかなりの効
果がでる。すなわち、空気中の窒素含量の80mol
%よりも多い窒素の雰囲気下で蒸着することで、
これによりかなりの移動度の向上がみられた。他
方、窒素量比が80mol%未満では、なんら移動度
の向上効果はなく、他の成分ガスの質によつては
むしろ移動度が低下した。
本発明の方法は、種々の実施態様をとりうる。
例えば充分真空度を上げておいてから窒素導入を
行い、もう一度真空度をあげて蒸着する方式ある
いは、窒素用バルブを蒸着装置に設置し、微量窒
素を導入しつつ初期の真空度から全体の真空度を
下げて蒸着する方式等が考えられる。例えば好ま
しい実施態様としては、10-7Torrまで真空度を
上げてから10-5Torrまで窒素導入によつて真空
度を下げ、そのまま窒素導入を続けるような方式
である。
窒素以外の成分ガスは特定されるものではな
い。また最終の真空度の限界は、インジウムとア
ンチモンのmean free pathから設定されるが、
普通は10-3Torr以上の真空度である。
本発明方法においては、インジウムとアンチモ
ンの原子到達速度比Aln/ASbを1.1〜1.7の範囲
に選ぶことが必要であり、これによつて特に高い
移動度を得ることができる。このときの蒸発源と
して単体のInとSbを用いるのが極めて好ましい
が、特に限定されない。InとSbの蒸発源として
InSbや適当な混合比のInSb+In(又はSb)を用い
ることもできる。またSbのみの蒸発源として
GaSb等も用いることができる。
本発明の基板には特に制限はなく、慣用されて
いるもの、例えばサフアイア、CaF2,NaCl、雲
母、ガラスCr―ドープのGaAs等が使用できる。
特に好ましいのは結晶性基板である。更に好まし
いのは、容易にへき開面の出せる雲母である。
基板温度は、特に限定されない。一定の温度や
蒸着中徐々にあるいは急速に上昇又は下降させた
基板温度が適用できる。しかし上限の温度は
InSbの融点である約530℃によつて制限される。
本発明を実施する手段としては、本発明の基本
概念をくずさないものであれば、なんでもよい。
すなわち、普通の蒸着(ヒーター加熱、EB加熱、
フラツシユ蒸着)、MBE、イオンビーム法等が適
用できる。薄膜形成速度はかなりの広範囲の0.1
〜1000Å/secを適用できるが、AIn/ASbの制
御の容易さから1〜100Å/secが特に好ましい。
以下に実施例を用いて本発明を更に説明する。
実施例 1
基板としては雲母を用いた。6枚のウエハーが
設置できる同心円周上に回転する基板ホルダーを
有する真空蒸着装置を使用した。基板温度はウエ
ハー上10mmの所に設けられたPt―Pdサーモカツ
プルで検知され、また、別のサーモカツプルを制
御用に設けた。
原料In,Sbは共にフルウチ化学社製6―Nの
ものを用いた。
まず、真空度を1×10-6Torrにし、基板温度
を400℃に設定した。次いで、ニードルバルブに
より窒素を導入し10-4Torrに真空度を下げ、ニ
ードルバルブをそのまま固定した。次にAIn/
ASb1.4になるようにInとSbを飛ばし、30分間で
厚み1.1μmになるまで蒸着させた。基板温度を
480℃まで上昇しつつ蒸着した。
6枚のウエハーを添附図面に示すようにパター
ニングして特性を測定したところ、移動度は
26000〜28000cm2/V・secであつた。
比較例 1
実施例1で窒素導入を行わず、10-6Torrの真
空度で行つたところ、得られた膜の移動度は
20000〜22000cm2/V・secであつた。
実施例 2
基板温度を440℃で一定にする以外は、実施例
1と同様に蒸着したところ、得られた膜の移動度
は、22000〜23000cm2/V・secであつた。
比較例 2
実施例2で窒素導入を行わず、10-6Torrの真
空度で蒸着を行つたところ、得られた膜の移動度
は15000〜17000cm2/V・secであつた。
実施例3〜5及び参考例
AIn/ASbを0.9,1.2,1.3,1.6について実施例
1と同様に窒素導入下で行つた結果を第1表に示
す。
The present invention relates to a method for manufacturing an indium-antimony mixed crystal that is used for various purposes as a semiconductor, and more specifically to a method for manufacturing an indium-antimony mixed crystal with improved electrical properties. Indium-antimony (hereinafter referred to as InSb)
The thin film has a mobility of 78000cm 2 /V・sec at room temperature.
This value is much higher than that of indium-arsenic (30,000 cm 2 /V・sec) and gallium-arsenide (7,000 cm 2 /V・sec), making it an excellent material for Hall elements and magnetoresistive elements. It has gained attention as a non-contact potentiometer for position detection devices for direct drive motors, VTRs, audio equipment, etc. By the way, when considering the Hall effect,
The Hall coefficient R H and the Hall mobility μ H are important parameters. For an InSb sample patterned and electroded in the shape shown in the attached drawing, the voltage generated between output electrodes 3 and 4 when input electrodes 1 and 2 are connected to constant current power supply I is calculated.
V Hi , and the voltage generated between output electrodes 3 and 4 when input electrodes 1 and 2 are connected to constant voltage power supply V is V Hv
In this case, V Hi and V Hv are calculated by the following formulas. V Hi = I/t・R H・B・I・f …(1) V Hv =ω/l・μ H・B・V・f …(2) However, t is the sample film thickness, and l is the pattern , ω is the width of the pattern, B is the magnetic flux density of the applied external magnetic field, I is the current passed through the sample, V is the voltage applied to the sample, f is the sample form factor, R The Hall coefficient of , μ H is the Hall mobility. As is clear from equation (1), the output voltage is inversely proportional to the film thickness of the sample, so it is better to use a thin film when making a highly sensitive Hall element or magnetoresistive element. Furthermore, since the forbidden band width of InSb is narrow, the Hall coefficient R H in equation (1) above changes significantly depending on the temperature, resulting in a large temperature dependence of the constant current output voltage V Hi in practical use. appear. On the other hand, the Hall mobility μ H given by equation (2) is
Since there are relatively few changes due to temperature, for practical purposes,
InSb Hall elements are mainly used under constant voltage, and therefore it is desired to increase the mobility rather than increase the Hall coefficient. Conventionally, a method known for producing a high-mobility InSb thin film is to cut out a bulk single crystal and polish it to make it thin. The thin film obtained in this way has excellent properties, but
Cutting out and polishing a single crystal is not necessarily suitable as an industrial method because it involves a large amount of loss and wastes expensive InSb single crystals. Another method has also been proposed in which In and Sb are deposited on a substrate to a thickness of about 10 μm by vapor deposition or other means, and then zone melted and polished to form a thin film (Japanese Patent Application Laid-Open No. 50-9373).
However, this method is complicated and has considerable limitations when implemented industrially. By the way, the simplest method for producing an InSb thin film is to deposit it on a substrate simply by vapor deposition.Many vapor deposition methods have been tried so far, but only a film with a thickness of about 1 μm and a hole mobility of 25,000 cm 2 /
It was not possible to obtain a thin film of Vsec or higher. By controlling the atomic arrival velocity ratio (AIn/Asb) of In and Sb in the substrate to 1.1 to 1.7, the present inventors first created an InSb composite crystal with uniform composition and properties consisting of an InSb crystal and a single In crystal. However, as a result of further research,
It was discovered that the mobility could be further improved by treatment under specific conditions, and the present invention was completed based on this finding. That is, in the present invention, when indium and antimony are vapor-deposited on a substrate to produce an indium-antimony mixed crystal, the atomic arrival velocity ratio AIn/ASb of indium and antimony on the substrate is determined in the presence of nitrogen. The present invention provides a method characterized in that vapor deposition is performed under conditions of 1.1 to 1.7. In this case, it is preferable that nitrogen be present at least in a higher proportion than the atmospheric component ratio. The present inventors introduced a rare gas such as Ar during evaporation with the aim of achieving higher mobility based on the previously proposed manufacturing method, but this resulted in a decrease in mobility. A significant improvement in mobility was observed when nitrogen was introduced during deposition. What is important in this case is that the nitrogen content is greater than the atmospheric component ratio. The relative amount of nitrogen to other gases varies depending on the initial vacuum level and the vacuum level after introduction. For example, if the initial vacuum level is 10 -6 Torr,
When the degree of vacuum is lowered to ×10 -6 Torr by introducing nitrogen, the nitrogen content ratio becomes approximately 90 mol%. Surprisingly, a change in atmosphere of this magnitude (from 80 mol% in air to 90 mol%) has a significant effect. i.e. 80mol of nitrogen content in air
By depositing in an atmosphere of nitrogen more than %,
This resulted in a considerable improvement in mobility. On the other hand, when the nitrogen ratio is less than 80 mol %, there is no effect of improving the mobility, and depending on the quality of other component gases, the mobility may actually decrease. The method of the invention can take various embodiments.
For example, you can raise the vacuum level sufficiently, then introduce nitrogen, and then increase the vacuum level again for evaporation. Alternatively, you can install a nitrogen valve in the evaporation equipment and introduce a small amount of nitrogen while increasing the initial vacuum level to the overall vacuum level. Possible methods include vapor deposition at a lower temperature. For example, a preferred embodiment is a method in which the degree of vacuum is raised to 10 -7 Torr, the degree of vacuum is lowered to 10 -5 Torr by introducing nitrogen, and then the degree of vacuum is continued to be introduced. Component gases other than nitrogen are not specified. Also, the final vacuum degree limit is set from the mean free path of indium and antimony,
Usually the vacuum level is 10 -3 Torr or higher. In the method of the present invention, it is necessary to select the atomic arrival velocity ratio Aln/ASb of indium and antimony in the range of 1.1 to 1.7, thereby making it possible to obtain particularly high mobility. Although it is extremely preferable to use single In and Sb as the evaporation source at this time, there is no particular limitation. As an evaporation source for In and Sb
InSb or InSb+In (or Sb) at an appropriate mixing ratio can also be used. Also, as an evaporation source of Sb only
GaSb etc. can also be used. The substrate of the present invention is not particularly limited, and commonly used materials such as sapphire, CaF 2 , NaCl, mica, glass Cr-doped GaAs, etc. can be used.
Particularly preferred is a crystalline substrate. More preferred is mica, which can be easily cleaved. The substrate temperature is not particularly limited. A constant temperature or a substrate temperature that is gradually or rapidly increased or decreased during the deposition can be applied. However, the upper temperature limit is
It is limited by the melting point of InSb, about 530°C. Any means for carrying out the present invention may be used as long as it does not destroy the basic concept of the present invention.
That is, ordinary vapor deposition (heater heating, EB heating,
Flash evaporation), MBE, ion beam method, etc. can be applied. Thin film formation rate has a fairly wide range of 0.1
~1000 Å/sec can be applied, but 1~100 Å/sec is particularly preferable from the viewpoint of ease of control of AIn/ASb. The present invention will be further explained below using Examples. Example 1 Mica was used as the substrate. A vacuum evaporation apparatus having a concentrically rotating substrate holder capable of holding six wafers was used. The substrate temperature was detected by a Pt-Pd thermocouple placed 10 mm above the wafer, and another thermocouple was provided for control. Both In and Sb used as raw materials were 6-N manufactured by Furuuchi Chemical Co., Ltd. First, the degree of vacuum was set to 1×10 -6 Torr, and the substrate temperature was set to 400°C. Next, nitrogen was introduced through a needle valve to lower the degree of vacuum to 10 -4 Torr, and the needle valve was fixed as it was. Next, AIn/
In and Sb were evaporated to give an ASb of 1.4, and evaporated to a thickness of 1.1 μm in 30 minutes. Substrate temperature
Vapor deposition was performed while increasing the temperature to 480℃. When we patterned six wafers as shown in the attached drawing and measured their characteristics, we found that the mobility was
It was 26,000 to 28,000 cm 2 /V·sec. Comparative Example 1 In Example 1, nitrogen was not introduced and the process was carried out at a vacuum level of 10 -6 Torr, and the mobility of the obtained film was
It was 20,000 to 22,000 cm 2 /V·sec. Example 2 Vapor deposition was carried out in the same manner as in Example 1 except that the substrate temperature was kept constant at 440° C. The mobility of the obtained film was 22,000 to 23,000 cm 2 /V·sec. Comparative Example 2 In Example 2, vapor deposition was performed at a vacuum level of 10 −6 Torr without introducing nitrogen, and the mobility of the obtained film was 15,000 to 17,000 cm 2 /V·sec. Examples 3 to 5 and Reference Examples Table 1 shows the results of AIn/ASb of 0.9, 1.2, 1.3, and 1.6 under nitrogen introduction in the same manner as in Example 1.
【表】
比較例 3〜6
窒素を導入しない場合の実施例3〜5及び参考
例に対する比較例を第2表に示す。[Table] Comparative Examples 3 to 6 Table 2 shows comparative examples for Examples 3 to 5 and Reference Examples in which nitrogen was not introduced.
【表】
実施例 6
最初の真空度を10-6Torr、窒素導入後の真空
度を10-5TOrrにする以外は実施例1と同様に行
つて、移動度25000〜27000cm2/V・secの薄膜を
得た。
実施例 7
基板をガラスとして実施例1と同様に行つて、
6000〜8000cm2/V・secの薄膜を得た。
比較例 7
実施例8の比較として、窒素導入なしで行つた
ところ、4000〜6000cm2/V・secの薄膜を得た。[Table] Example 6 The same procedure as in Example 1 was carried out except that the initial degree of vacuum was 10 -6 Torr and the degree of vacuum after nitrogen introduction was 10 -5 TOrr, and the mobility was 25,000 to 27,000 cm 2 /V・sec. A thin film was obtained. Example 7 The same procedure as in Example 1 was carried out using glass as the substrate.
A thin film of 6000 to 8000 cm 2 /V·sec was obtained. Comparative Example 7 As a comparison with Example 8, a thin film of 4000 to 6000 cm 2 /V·sec was obtained when nitrogen was not introduced.
図面は本発明におけるサンプルのパターニング
及び電極取付けを説明するための平面図である。
図中1,2は入力電極、3,4は出力電極であ
る。
The drawing is a plan view for explaining sample patterning and electrode attachment in the present invention. In the figure, 1 and 2 are input electrodes, and 3 and 4 are output electrodes.
Claims (1)
せてインジウム―アンチモン系混合結晶を製造す
るに当り、窒素の存在下、基板上でのインジウム
とアンチモンとの原子到達速度比AIn/ASbが
1.1〜1.7となる条件のもとで蒸着処理することを
特徴とする方法。1. When producing an indium-antimony mixed crystal by vapor depositing indium and antimony on a substrate, the atomic arrival velocity ratio AIn/ASb of indium and antimony on the substrate in the presence of nitrogen is
A method characterized by performing vapor deposition under conditions of 1.1 to 1.7.
Priority Applications (7)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56072464A JPS57187934A (en) | 1981-05-14 | 1981-05-14 | Manufacture of indium-antimony system mixing crystal |
| US06/361,939 US4468415A (en) | 1981-03-30 | 1982-03-25 | Indium-antimony complex crystal semiconductor and process for production thereof |
| AT82102605T ATE20629T1 (en) | 1981-03-30 | 1982-03-27 | INDIUM-ANTIMONY SEMICONDUCTOR WITH COMPLEX CRYSTALLINE STRUCTURE AND PROCESS FOR ITS PRODUCTION. |
| EP82102605A EP0062818B2 (en) | 1981-03-30 | 1982-03-27 | Process of producing a hall element or magnetoresistive element comprising an indium-antimony complex crystal semiconductor |
| DE8282102605T DE3271874D1 (en) | 1981-03-30 | 1982-03-27 | Indium-antimony complex crystal semiconductor and process for production thereof |
| KR8201347A KR860000161B1 (en) | 1981-03-30 | 1982-03-29 | Indium antimony composite crystal semiconductor and its manufacturing method |
| US06/620,645 US4539178A (en) | 1981-03-30 | 1984-06-14 | Indium-antimony complex crystal semiconductor and process for production thereof |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56072464A JPS57187934A (en) | 1981-05-14 | 1981-05-14 | Manufacture of indium-antimony system mixing crystal |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS57187934A JPS57187934A (en) | 1982-11-18 |
| JPH0115135B2 true JPH0115135B2 (en) | 1989-03-15 |
Family
ID=13490047
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP56072464A Granted JPS57187934A (en) | 1981-03-30 | 1981-05-14 | Manufacture of indium-antimony system mixing crystal |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS57187934A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US7567078B2 (en) | 2004-12-28 | 2009-07-28 | Asahi Kasei Emd Corporation | Magnetic rotation-angle sensor and angle-information processing device |
-
1981
- 1981-05-14 JP JP56072464A patent/JPS57187934A/en active Granted
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US7567078B2 (en) | 2004-12-28 | 2009-07-28 | Asahi Kasei Emd Corporation | Magnetic rotation-angle sensor and angle-information processing device |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS57187934A (en) | 1982-11-18 |
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