JPH084160B2 - Magnetoresistive element and manufacturing method thereof - Google Patents
Magnetoresistive element and manufacturing method thereofInfo
- Publication number
- JPH084160B2 JPH084160B2 JP62203731A JP20373187A JPH084160B2 JP H084160 B2 JPH084160 B2 JP H084160B2 JP 62203731 A JP62203731 A JP 62203731A JP 20373187 A JP20373187 A JP 20373187A JP H084160 B2 JPH084160 B2 JP H084160B2
- Authority
- JP
- Japan
- Prior art keywords
- superconducting
- magnetoresistive element
- short
- magnetic flux
- semiconductor
- 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.)
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- Superconductor Devices And Manufacturing Methods Thereof (AREA)
- Hall/Mr Elements (AREA)
Description
【発明の詳細な説明】 (イ) 産業上の利用分野 本発明はインジウムアンチモナイドInSb等の高移動度
半導体結晶を用いた磁気抵抗素子及びその製造方法に関
する。The present invention relates to a magnetoresistive element using a high mobility semiconductor crystal such as indium antimonide InSb and a method for manufacturing the same.
(ロ) 従来の技術 高移動度半導体結晶を用いた磁気抵抗素子は、高感
度、低雑音であるため、高精度の磁気センサとして、実
用化が進んでいる。(B) Conventional Technology Since a magnetoresistive element using a high-mobility semiconductor crystal has high sensitivity and low noise, it has been put into practical use as a highly accurate magnetic sensor.
この種磁気抵抗素子の抵抗値Rは、抵抗率変化が小さ
いとき、次式で示される。The resistance value R of this kind of magnetoresistive element is expressed by the following equation when the change in resistivity is small.
但し、R0は磁場を加えないときの基準抵抗、lは長
さ、wは幅、μは電子移動度、Bは磁束密度である。 However, R 0 is a reference resistance when no magnetic field is applied, l is length, w is width, μ is electron mobility, and B is magnetic flux density.
この抵抗値変化を大きくするためには、(1)式にお
けるl/wを小さくすればよい。このため、従来装置にお
いては、第6図に示すように、磁気抵抗素子(21)の表
面に銀線などの短絡線(22)を張りつけたり、真空蒸着
したりして、ホール電圧を短絡する方法が取られている
(特公昭42−7984号公報参照)。In order to increase this resistance value change, it is sufficient to decrease l / w in the equation (1). Therefore, in the conventional device, as shown in FIG. 6, a short-circuit wire (22) such as a silver wire is attached to the surface of the magnetoresistive element (21) or vacuum evaporation is performed to short-circuit the Hall voltage. The method has been adopted (see Japanese Patent Publication No. 42-7984).
(ハ) 発明が解決しようとする問題点 前述の磁気抵抗素子はホール電圧を短絡する短絡線と
して銀線を用いているので、素子を通過する磁束が短絡
線の領域をも通過することにより、(1)式における磁
束密度Bを大きくすることができない。(C) Problems to be solved by the invention Since the above-described magnetoresistive element uses the silver wire as the short-circuit line for short-circuiting the Hall voltage, the magnetic flux passing through the element also passes through the area of the short-circuit line, The magnetic flux density B in the equation (1) cannot be increased.
本発明はかかる点に鑑み発明されたものにして、前記
磁束密度Bを大きくして磁束の有無による抵抗値Rの変
化を大きくすることができる磁気抵抗素子及びその製造
方法を提供しようとするものである。The present invention has been made in view of the above points, and an object of the present invention is to provide a magnetoresistive element capable of increasing the magnetic flux density B and increasing the change in the resistance value R depending on the presence or absence of magnetic flux, and a method for manufacturing the same. Is.
(ニ) 問題点を解決するための手段 かかる問題点を解決するため、本発明の磁気抵抗素子
は、ホール電圧を短絡する短絡線として、超伝導片を用
い、隣接する超伝導片間に磁束を集中せしめるものであ
る。(D) Means for Solving the Problems In order to solve the problems, the magnetoresistive element of the present invention uses a superconducting piece as a short-circuit line for short-circuiting a Hall voltage, and a magnetic flux is generated between adjacent superconducting pieces. It is a thing to concentrate.
また、その素子の製造方法は、基板上にストライプ状
に超伝導片を形成した後、その上に移動度の高い半導体
をコーティングすることを特徴とする。Further, the device manufacturing method is characterized in that after forming a superconducting piece in a stripe shape on a substrate, a semiconductor having high mobility is coated thereon.
(ホ) 作 用 磁気抵抗素子におけるホール電圧を短絡する短絡線を
超伝導片にて構成するため、素子に入る磁束が超伝導片
を通過せず隣接する超伝導片間に集中することになり、
前述の短絡辺に銀線を用いるものに比し、磁束密度Bを
大きくする。従って抵抗値Rが大きくなる。(E) Operation Since the short-circuit line that short-circuits the Hall voltage in the magnetoresistive element is composed of superconducting pieces, the magnetic flux entering the element will not pass through the superconducting pieces but will be concentrated between adjacent superconducting pieces. ,
The magnetic flux density B is increased as compared with the above-mentioned one using a silver wire for the short-circuited side. Therefore, the resistance value R becomes large.
また、超伝導片を用いるため、この素子は低温下で使
用されることから電子移動度μも大きく、抵抗値Rがよ
り一層大きくなる。Further, since the superconducting piece is used, this element is used at a low temperature, so that the electron mobility μ is also large and the resistance value R is further increased.
さらに、短絡線としての超伝導片の本数が多いと、
(1)式におけるl/wが小さくなり、低磁界領域におけ
る抵抗値変化の直線性が向上する。Furthermore, if the number of superconducting pieces as short-circuit wires is large,
The l / w in the equation (1) becomes small, and the linearity of the resistance change in the low magnetic field region is improved.
一方、本発明による製造方法によれば、磁気抵抗素子
におけるホール電圧を短絡する短絡線として超伝導線を
用いることができ、抵抗値変化の大きい磁気抵抗素子を
製造することができる。On the other hand, according to the manufacturing method of the present invention, a superconducting wire can be used as a short-circuit wire for short-circuiting the Hall voltage in the magnetoresistive element, and a magnetoresistive element with a large change in resistance value can be manufactured.
(ヘ) 実施例 本発明の一実施例を図面に基づいて説明する。(F) Example An example of the present invention will be described with reference to the drawings.
第1図は磁気抵抗素子の斜視図である。この図面にお
いて、電子移動度の高い半導体(1)の両端電極
(2),(3)間にはホール電圧を短絡する短絡線とし
ての超伝導片(4)が複数設けられている。半導体
(1)として実施例ではインジウムアンチモナイドInSb
を用いたが、インジウムヒ素InSb、ガリウムヒ素GaAsを
使用してもよい。また、超伝導片(4)としては、酸化
物系超伝導材を使用した。具体的にはA−Ba−Cu−O系
のAとしてYを使用したが、Aとしてはその他にYb、E
r、Gd、Dy、Ho、Eu、Sm、Ndから選択されるものを用い
てもよい。FIG. 1 is a perspective view of a magnetoresistive element. In this figure, a plurality of superconducting pieces (4) as short-circuiting lines for short-circuiting the Hall voltage are provided between the electrodes (2) and (3) of the semiconductor (1) having a high electron mobility. As the semiconductor (1), indium antimonide InSb is used in the embodiment.
However, indium arsenide InSb and gallium arsenide GaAs may be used. Further, as the superconducting piece (4), an oxide superconducting material was used. Specifically, Y was used as A of the A-Ba-Cu-O system, but as A, Yb, E
Those selected from r, Gd, Dy, Ho, Eu, Sm, and Nd may be used.
尚、第1図において、両端電極(2),(3)には、
夫々リード線(5)が接続されている。In FIG. 1, the electrodes (2) and (3) on both ends are
Lead wires (5) are connected to each.
磁気抵抗素子(6)は次のようにして製造される。 The magnetoresistive element (6) is manufactured as follows.
まず、第2図(a)に示すように基板(7)を用意す
る。この基板はAl2O3,MgOあるいはガラスよりなるもの
である。この基板(7)上に複数の超伝導片(4)をス
トライプ状に形成する。First, a substrate (7) is prepared as shown in FIG. This substrate is made of Al 2 O 3 , MgO or glass. A plurality of superconducting pieces (4) are formed in stripes on this substrate (7).
この超伝導片は溶融した超伝導材料を塗布させてもよ
いが、実施例では第3図に示すスパタリング装置により
形成した。同図において、スパタリング装置のベルジャ
ー(8)には、排気系(9)が連なると共にベルジャー
内に放電ガスであるアルゴンガスを供給するアルゴンガ
スボンベ(10)がバリアブルリークバルブ(11)及びス
トップバルブ(12)を介して連なっている。ベルジャー
(8)内には対抗電極(13),(14)がシャッター(1
7)を介して対抗配置されている。陽極(13)は接地さ
れると共にその表面上に超伝導薄膜を堆積させる基板
(7),(7)が置かれている。また陰極(14)は超伝
導材料であるY−Ba−Cu−O系焼結体からなるターゲッ
ト材にて構成されており、この陰極(14)には負の高い
電圧が印加される。(15),(16)は高真空計、低真空
計である。This superconducting piece may be formed by applying a molten superconducting material, but in the embodiment, it was formed by the sputtering device shown in FIG. In the figure, an exhaust system (9) is connected to a bell jar (8) of a spattering device, and an argon gas cylinder (10) for supplying an argon gas as a discharge gas into the bell jar is provided with a variable leak valve (11) and a stop valve (10). 12) is connected through. In the bell jar (8), the counter electrodes (13) and (14) have shutters (1
7) are counter-placed through. The anode (13) is grounded and the substrates (7), (7) on which the superconducting thin film is deposited are placed on the surface thereof. The cathode (14) is made of a target material made of a Y-Ba-Cu-O-based sintered body which is a superconducting material, and a high negative voltage is applied to the cathode (14). (15) and (16) are high and low vacuum gauges.
而して、アルゴンガスボンベ(10)からベルジャー
(8)内にアルゴンガスを1〜10-4Torrの圧力で供給す
ると同時に、対抗電極(13),(14)間に15Kvの電圧を
印加して、対抗電極(13),(14)間でグロー放電させ
る。この時、基板(7)を置いた陽極(13)の温度が室
温もしくはせいぜい100℃までの温度に保たれている。
その状態でシャッター(17)を開くと、陰極(14)を構
成するY−Ba−Cu−O系焼結体がスパタリングされて基
板(7),(7)に飛散する。基板(7),(7)に到
達した焼結体の材料は、基板(7)上のストライプ状の
マスクされていない領域において、基板が低温状態にあ
るので、基板表面上で結晶化することなくアモルファス
状態で堆積する。従って基板上には、ストライプ状に複
数の超伝導片(4),(4)が形成される。この状態で
マスクを取り除くと第2図(b)のものとなる。Then, argon gas is supplied from the argon gas cylinder (10) into the bell jar (8) at a pressure of 1 to 10 -4 Torr, and at the same time, a voltage of 15 Kv is applied between the counter electrodes (13) and (14). A glow discharge is generated between the counter electrodes (13) and (14). At this time, the temperature of the anode (13) on which the substrate (7) is placed is kept at room temperature or at most 100 ° C.
When the shutter (17) is opened in this state, the Y-Ba-Cu-O-based sintered body forming the cathode (14) is sputtered and scattered on the substrates (7) and (7). The material of the sintered body that has reached the substrates (7) and (7) is crystallized on the substrate surface because the substrate is in a low temperature state in the striped unmasked region on the substrate (7). Instead, it deposits in an amorphous state. Therefore, a plurality of stripe-shaped superconducting pieces (4), (4) are formed on the substrate. When the mask is removed in this state, the result is as shown in FIG.
ついで基板(7)及び超伝導片(4),(4)上に電
子移動度の高い半導体(1)をスパタまたは蒸着により
コーティングする(第2図(c))。基板(7)を除く
ことにより、第1図に示す磁気抵抗素子(6)を得る。Then, the semiconductor (1) having high electron mobility is coated on the substrate (7) and the superconducting pieces (4) and (4) by sputtering or vapor deposition (FIG. 2 (c)). By removing the substrate (7), the magnetoresistive element (6) shown in FIG. 1 is obtained.
而して、磁気抵抗素子(21)のホール電圧を短絡する
短絡線(22)を銀線により構成する従来装置において
は、第4図(b)に示すように、磁気抵抗素子(21)に
入る磁束は短絡線領域にも均等分散して通過するため、
隣接する短絡線(22),(22)間の磁束密度を特に高め
ることがない。Thus, in the conventional device in which the short-circuit line (22) for short-circuiting the Hall voltage of the magnetoresistive element (21) is made of a silver wire, as shown in FIG. Since the incoming magnetic flux passes evenly in the short-circuit line area,
The magnetic flux density between the adjacent short-circuit wires (22) and (22) is not particularly increased.
また、短絡線(22)によりホール電圧を短絡する従来
装置においては、短絡線(22)として銀線、銅線あるい
はインジウム線を用いるため、ホール電圧を生ずる両側
端間の電界を弱くすることができるが、その程度がイン
ジウム線では約60%、銀線あるいは銅線では約80%であ
り、電界の影響を受け、抵抗値変化をより一層大きくす
ることができない。Further, in the conventional device that short-circuits the Hall voltage with the short-circuit wire (22), a silver wire, a copper wire, or an indium wire is used as the short-circuit wire (22), so that the electric field between both ends that generates the Hall voltage can be weakened. However, the degree of indium wire is about 60% and that of silver wire or copper wire is about 80%, and the change in resistance value cannot be further increased due to the influence of the electric field.
これに対し、本発明による磁気抵抗素子(6)におい
ては、短絡線である超伝導片(4)の領域に入ろうとす
る磁束は、超伝導片(4)のマイスナー効果により、超
伝導片への進入が阻止されて、同図(a)に示すよう
に、隣接する超伝導片(4),(4)間に集中して流れ
る。このため、超伝導片(4),(4)間の磁束密度が
同図(a)のものに比し大きくなる。On the other hand, in the magnetoresistive element (6) according to the present invention, the magnetic flux that tries to enter the region of the superconducting piece (4) which is a short-circuit line is transferred to the superconducting piece due to the Meissner effect of the superconducting piece (4). Of the superconducting pieces (4), (4) are concentrated and flow, as shown in FIG. Therefore, the magnetic flux density between the superconducting pieces (4) and (4) is larger than that in FIG.
また、短絡線を超伝導片(4)にて構成するため、ホ
ール電圧を生ずる両側端間は内部抵抗零の超伝導片
(4)にて接続されることから、等電位となり、その両
側端間に電界が生じなくなる。従って、電界の影響を受
けなくなり、磁束の有無による抵抗値変化が従来のもの
に比しより一層大きくなる。Further, since the short-circuit wire is composed of the superconducting piece (4), the both ends that generate the Hall voltage are connected by the superconducting piece (4) with zero internal resistance, so that the both ends have the same potential. No electric field is generated between them. Therefore, the influence of the electric field is eliminated, and the change in resistance value due to the presence or absence of magnetic flux becomes larger than that of the conventional one.
また、実施例においては、超伝導片(4)をY−Ba−
Cu−O系のもので構成したから、液体窒素の沸点(77
K)より高い雰囲気温度で超伝導状態になる。このた
め、本発明による磁気抵抗素子(6)は低温で使用され
ることになる。従って半導体(1)における電子移動度
を室温で使用する従来のものに比し高めることができ
る。実施例においては、半導体としてインジウムアンチ
モナイドInSbを使用しており、その電子移動度μは室温
では80,000cm2/(v・s)であるのに対し、77Kでは40
0,000cm2/(v・s)に大きくなる。このため、磁場の
有無による抵抗値変化が大きくなる。In addition, in the examples, the superconducting piece (4) is replaced with Y-Ba-
Since it is composed of Cu-O type, the boiling point of liquid nitrogen (77
K) becomes superconducting at higher ambient temperature. Therefore, the magnetoresistive element (6) according to the present invention is used at a low temperature. Therefore, the electron mobility in the semiconductor (1) can be increased as compared with the conventional one that is used at room temperature. In the example, indium antimonide InSb is used as a semiconductor, and its electron mobility μ is 80,000 cm 2 / (v · s) at room temperature, whereas it is 40 at 77K.
It becomes as large as 0,000 cm 2 / (v · s). Therefore, the resistance value changes greatly depending on the presence or absence of a magnetic field.
この電子移動度μ及び磁束密度Bが大きくなることか
ら、抵抗値変化は磁束密度Bの変化に対し、直線性を向
上することになる。第5図は実施例によるものXと前述
の従来のものYとの特性図である。Since the electron mobility μ and the magnetic flux density B increase, the change in the resistance value improves the linearity with respect to the change in the magnetic flux density B. FIG. 5 is a characteristic diagram of X according to the embodiment and the above-mentioned conventional Y.
(ト) 発明の効果 本発明は、電子移動度の高い半導体の両端電極間に、
ホール電圧を短絡する超伝導片を複数設け、隣接する超
伝導片間に磁束を集中せしめることを特徴とするもので
あるから、磁束の有無による抵抗値変化の大きい磁気抵
抗素子を提供することができる。(G) Effect of the Invention The present invention is directed to between both electrodes of a semiconductor having high electron mobility,
Since it is characterized by providing a plurality of superconducting pieces for short-circuiting the Hall voltage and concentrating magnetic flux between adjacent superconducting pieces, it is possible to provide a magnetoresistive element having a large resistance value change depending on the presence or absence of magnetic flux. it can.
また、基板上にストライプ状の超伝導片を形成した
後、その上に電子移動度の高い半導体をコーティングす
ることにより磁気抵抗素子を製造するため、磁束の有無
による抵抗値変化の大きい磁気抵抗素子を製造すること
ができる。In addition, since a magnetoresistive element is manufactured by forming a stripe-shaped superconducting piece on a substrate and then coating a semiconductor with high electron mobility on it, a magnetoresistive element with a large resistance value change depending on the presence or absence of magnetic flux. Can be manufactured.
第1図乃至第5図は本発明の一実施例を示し、第1図は
磁気抵抗素子の斜視図、第2図(a)(b)(c)は製
造工程を説明する図、第3図はスパタリング装置の概念
図、第4図(a)(b)は実施例のものと従来のものに
おける磁束の通過説明図、第5図は磁気抵抗素子の磁束
密度−抵抗値特性図である。第6図は従来の磁気抵抗素
子の斜視図である。 (1)……半導体、(2),(3)……電極、(4)…
…超伝導片、(7)……基板。1 to 5 show an embodiment of the present invention, FIG. 1 is a perspective view of a magnetoresistive element, and FIGS. 2 (a), (b) and (c) are views for explaining the manufacturing process, and FIG. FIG. 4 is a conceptual diagram of the sputtering device, FIGS. 4 (a) and 4 (b) are explanatory views of passage of magnetic flux in the embodiment and the conventional one, and FIG. 5 is a magnetic flux density-resistance value characteristic diagram of the magnetoresistive element. . FIG. 6 is a perspective view of a conventional magnetoresistive element. (1) ... Semiconductor, (2), (3) ... Electrode, (4) ...
… Superconducting piece, (7) …… Substrate.
Claims (2)
ホール電圧を短絡する超伝導片を複数設け、隣接する超
伝導片間に磁束を集中せしめたことを特徴とする磁気抵
抗素子。1. A semiconductor having high electron mobility between electrodes at both ends,
A magnetoresistive element characterized in that a plurality of superconducting pieces for short-circuiting a Hall voltage are provided, and magnetic flux is concentrated between adjacent superconducting pieces.
た後、その上に電子移動度の高い半導体をコーティング
することを特徴とする磁気抵抗素子の製造方法。2. A method of manufacturing a magnetoresistive element, which comprises forming a stripe-shaped superconducting piece on a substrate and then coating a semiconductor having a high electron mobility thereon.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62203731A JPH084160B2 (en) | 1987-08-17 | 1987-08-17 | Magnetoresistive element and manufacturing method thereof |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62203731A JPH084160B2 (en) | 1987-08-17 | 1987-08-17 | Magnetoresistive element and manufacturing method thereof |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6446992A JPS6446992A (en) | 1989-02-21 |
| JPH084160B2 true JPH084160B2 (en) | 1996-01-17 |
Family
ID=16478922
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP62203731A Expired - Fee Related JPH084160B2 (en) | 1987-08-17 | 1987-08-17 | Magnetoresistive element and manufacturing method thereof |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH084160B2 (en) |
-
1987
- 1987-08-17 JP JP62203731A patent/JPH084160B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6446992A (en) | 1989-02-21 |
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