JPS6353713B2 - - Google Patents
Info
- Publication number
- JPS6353713B2 JPS6353713B2 JP56002898A JP289881A JPS6353713B2 JP S6353713 B2 JPS6353713 B2 JP S6353713B2 JP 56002898 A JP56002898 A JP 56002898A JP 289881 A JP289881 A JP 289881A JP S6353713 B2 JPS6353713 B2 JP S6353713B2
- Authority
- JP
- Japan
- Prior art keywords
- electrodes
- thin film
- terminal
- semiconductor thin
- electrode
- 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
Links
- 239000010409 thin film Substances 0.000 claims description 28
- 239000004065 semiconductor Substances 0.000 claims description 24
- 230000000694 effects Effects 0.000 claims description 11
- 239000002184 metal Substances 0.000 description 8
- 229910052751 metal Inorganic materials 0.000 description 8
- WPYVAWXEWQSOGY-UHFFFAOYSA-N indium antimonide Chemical compound [Sb]#[In] WPYVAWXEWQSOGY-UHFFFAOYSA-N 0.000 description 6
- 239000000758 substrate Substances 0.000 description 6
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 4
- 229910052802 copper Inorganic materials 0.000 description 4
- 239000010949 copper Substances 0.000 description 4
- 238000010586 diagram Methods 0.000 description 4
- 238000007772 electroless plating Methods 0.000 description 4
- 229920002120 photoresistant polymer Polymers 0.000 description 4
- 229910000859 α-Fe Inorganic materials 0.000 description 4
- 239000003822 epoxy resin Substances 0.000 description 3
- 239000007788 liquid Substances 0.000 description 3
- 239000000463 material Substances 0.000 description 3
- 238000007747 plating Methods 0.000 description 3
- 229920000647 polyepoxide Polymers 0.000 description 3
- 229910000679 solder Inorganic materials 0.000 description 3
- 238000004519 manufacturing process Methods 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 239000010445 mica Substances 0.000 description 2
- 229910052618 mica group Inorganic materials 0.000 description 2
- 238000000465 moulding Methods 0.000 description 2
- 239000000243 solution Substances 0.000 description 2
- 238000007738 vacuum evaporation Methods 0.000 description 2
- 229910001218 Gallium arsenide Inorganic materials 0.000 description 1
- 229910000673 Indium arsenide Inorganic materials 0.000 description 1
- 229910021578 Iron(III) chloride Inorganic materials 0.000 description 1
- 229910018605 Ni—Zn Inorganic materials 0.000 description 1
- 229910004298 SiO 2 Inorganic materials 0.000 description 1
- 229910045601 alloy Inorganic materials 0.000 description 1
- 239000000956 alloy Substances 0.000 description 1
- 239000007864 aqueous solution Substances 0.000 description 1
- 239000000919 ceramic Substances 0.000 description 1
- 239000011248 coating agent Substances 0.000 description 1
- 238000000576 coating method Methods 0.000 description 1
- 150000001875 compounds Chemical class 0.000 description 1
- 238000005530 etching Methods 0.000 description 1
- 239000010408 film Substances 0.000 description 1
- RPQDHPTXJYYUPQ-UHFFFAOYSA-N indium arsenide Chemical compound [In]#[As] RPQDHPTXJYYUPQ-UHFFFAOYSA-N 0.000 description 1
- RBTARNINKXHZNM-UHFFFAOYSA-K iron trichloride Chemical compound Cl[Fe](Cl)Cl RBTARNINKXHZNM-UHFFFAOYSA-K 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 238000004806 packaging method and process Methods 0.000 description 1
- 238000000206 photolithography Methods 0.000 description 1
- 229920005989 resin Polymers 0.000 description 1
- 239000011347 resin Substances 0.000 description 1
- 238000004544 sputter deposition Methods 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N—ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N50/00—Galvanomagnetic devices
- H10N50/10—Magnetoresistive devices
Landscapes
- Hall/Mr Elements (AREA)
Description
【発明の詳細な説明】
この発明は、4つの端子を有する高感度型の磁
気抵抗素子に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a highly sensitive magnetoresistive element having four terminals.
従来、磁気抵抗素子は、二端子又は三端子の形
で形成されて使用されて来た。この従来の磁気抵
抗素子の形状を第1図、第2図、第3図に示す。 Conventionally, magnetoresistive elements have been formed and used in the form of two terminals or three terminals. The shape of this conventional magnetoresistive element is shown in FIGS. 1, 2, and 3.
第1図は単純な二端子素子の場合で磁気抵抗効
果を生ずる半導体薄膜の両端にオーミツク電極1
2,13が形成され、これら電極12,13間に
おいて半導体薄膜11上にその幅方向に延長した
オーミツク電極よりなるシヨートバー14が配列
され、シヨートバー14は半導体薄膜11の磁気
抵抗効果を高める作用をする。電極12,13は
外部接続用である。 Figure 1 shows a simple two-terminal device with ohmic electrodes at both ends of the semiconductor thin film that produces the magnetoresistive effect.
2 and 13 are formed, and between these electrodes 12 and 13, short bars 14 made of ohmic electrodes extending in the width direction are arranged on the semiconductor thin film 11, and the short bars 14 serve to enhance the magnetoresistive effect of the semiconductor thin film 11. . Electrodes 12 and 13 are for external connection.
第2図は、第1図に示した磁気抵抗素子の端子
電極12,13の中間にオーミツク電極よりなる
外部接続用の端子電極15が形成される。この素
子は三端子素子であり、電極12,15間と、電
極13,15間とに異つた値の磁界を加えること
により、電極15より、差動出力をとり出せる。 In FIG. 2, a terminal electrode 15 for external connection made of an ohmic electrode is formed between the terminal electrodes 12 and 13 of the magnetoresistive element shown in FIG. This element is a three-terminal element, and by applying magnetic fields of different values between electrodes 12 and 15 and between electrodes 13 and 15, a differential output can be obtained from electrodes 15.
第3図は第2図における端子電極13,15間
のシヨートバー14を省略した素子である。この
場合、電極12,15間の磁気抵抗効果は大きく
これに対し、電極13,15間の磁気抵抗効果は
小さい。このため、素子全体に一様な磁界を加え
ると、電極15より差動出力をとり出すことがで
きる。 FIG. 3 shows an element in which the short bar 14 between the terminal electrodes 13 and 15 in FIG. 2 is omitted. In this case, the magnetoresistive effect between the electrodes 12 and 15 is large, whereas the magnetoresistive effect between the electrodes 13 and 15 is small. Therefore, if a uniform magnetic field is applied to the entire element, a differential output can be obtained from the electrodes 15.
これら従来用いられた形式の磁気抵抗素子の問
題点は強力な磁界を加えないと、大きな抵抗値変
化が得られず、従つて、実際に使用する場合の出
力が小さいということと、また第2図、第3図に
示したものでは磁界がゼロで出力がゼロとなら
ず、いわゆるオフセツト電圧が本質的に存在し、
差動出力のみを素子から直接とり出せないことで
ある。 The problem with these conventionally used types of magnetoresistive elements is that a large change in resistance value cannot be obtained unless a strong magnetic field is applied, and therefore the output when actually used is small. In the case shown in Fig. 3, the output is not zero even when the magnetic field is zero, and a so-called offset voltage essentially exists.
The problem is that only the differential output cannot be directly extracted from the elements.
この発明の目的は、このような従来素子の欠点
を除き、出力が従来素子の2倍となり、かつオフ
セツト電圧ゼロで使える差動出力が得られる磁気
抵抗素子を提供することにある。 It is an object of the present invention to provide a magnetoresistive element which eliminates the drawbacks of the conventional element, has an output twice that of the conventional element, and provides a differential output that can be used with zero offset voltage.
この発明の磁気抵抗素子は磁気抵抗効果を有す
る半導体薄膜をループ状に形成し、その半導体薄
膜上に、間隔をおいて4つのオーミツクの電極か
ら成る外部接続用の第1、第2、第3、第4端子
電極が配置され、その第1、第2端子電極間及び
第3、第4端子電極間の各半導体薄膜上にオーミ
ツク電極より成るシヨートバーがそれぞれ形成さ
れ、第2、第3端子電極間及び第4、第1端子電
極間にはシヨートバーを形成しない構造とされ
る。 The magnetoresistive element of the present invention has a semiconductor thin film having a magnetoresistive effect formed in a loop shape, and first, second, and third electrodes for external connection consisting of four ohmic electrodes spaced apart on the semiconductor thin film. , a fourth terminal electrode is arranged, shot bars made of ohmic electrodes are formed on each of the semiconductor thin films between the first and second terminal electrodes and between the third and fourth terminal electrodes, and the second and third terminal electrodes The structure is such that no short bar is formed between the fourth terminal electrode and between the fourth and first terminal electrodes.
例えば第4図に示すように磁気抵抗効果を有す
る半導体薄膜11が方形のループ状に形成され、
その方形の各角において半導体薄膜11上に端子
電極16,17,18,19がそれぞれ形成され
る。電極16,17間、また電極18,19間の
各半導体薄膜11上にシヨートバー14がそれぞ
れ形成される。電極17,18間、19,16間
にはシヨートバーは形成されない。 For example, as shown in FIG. 4, a semiconductor thin film 11 having a magnetoresistive effect is formed in a rectangular loop shape,
Terminal electrodes 16, 17, 18, and 19 are formed on the semiconductor thin film 11 at each corner of the rectangle. Short bars 14 are formed on each semiconductor thin film 11 between electrodes 16 and 17 and between electrodes 18 and 19, respectively. No short bars are formed between the electrodes 17 and 18 and between the electrodes 19 and 16.
この第4図に示した磁気抵抗素子において端子
電極17,19間に、一定電圧を入力し、素子全
体に一様な磁界を加えると、電極17,18間及
び電極18,19間の各抵抗値変化にもとずく電
極18の電位変化と、同様に電極16の電位変化
との差が16,18間に取出される。しかも、磁
界ゼロのときの電極16,18間の電位差がゼロ
となるように、各電極間の抵抗値を与えておくこ
とにより、電極16,18間から磁気抵抗効果に
よる差動電圧出力のみをとり出すことが出来る。
又、この素子はブリツジ構造となつているため電
極17,18,19間における変化と、電極1
7,16,19間における変化とが差動的にとり
出させるため、従来の磁気抵抗素子、例えば第3
図に示したものに比して2倍の差動出力を得るこ
とができる。しかも、第2図に示したものと異な
り、素子全体に一様磁界を加えれば、差動出力が
得られるため、素子を小さく形成しても効果を失
なわない。 In the magnetoresistive element shown in FIG. 4, when a constant voltage is input between terminal electrodes 17 and 19 and a uniform magnetic field is applied to the entire element, each resistance between electrodes 17 and 18 and between electrodes 18 and 19 is The difference between the potential change of the electrode 18 due to the value change and the potential change of the electrode 16 is also taken out between 16 and 18. Moreover, by giving a resistance value between each electrode so that the potential difference between the electrodes 16 and 18 is zero when the magnetic field is zero, only the differential voltage output due to the magnetoresistive effect is generated between the electrodes 16 and 18. It can be taken out.
Also, since this element has a bridge structure, changes between electrodes 17, 18, and 19 and changes in electrode 1
In order to extract the changes between 7, 16, and 19 differentially, a conventional magnetoresistive element, for example, the third
A differential output twice as large as that shown in the figure can be obtained. Moreover, unlike the device shown in FIG. 2, differential output can be obtained by applying a uniform magnetic field to the entire device, so the effect is not lost even if the device is made small.
この発明の磁気抵抗素子の好ましい場合とし
て、磁界が印加されていない状態で、電極16,
17間と電極17,18間との各抵抗値を同一に
し、かつ、電極18,19間と、電極19,16
間との各抵抗値を同一にした素子がある。この場
合、磁界を加えないときの電極16,18の各電
位は等しく磁界を加えたときは、磁気抵抗効果に
よる差動出力のみが電極16,18間に生ずる。 In a preferred case of the magnetoresistive element of the present invention, when no magnetic field is applied, the electrodes 16,
17 and between electrodes 17 and 18, and between electrodes 18 and 19 and between electrodes 19 and 16.
There is an element that has the same resistance value between the two. In this case, when no magnetic field is applied, the potentials of the electrodes 16 and 18 are equal, and when a magnetic field is applied, only a differential output is generated between the electrodes 16 and 18 due to the magnetoresistive effect.
又、更に好ましい場合として、各隣接電極間の
すべての抵抗値を同一にした素子がある。この場
合は、どの電極も全く対称的な関係になり、電極
17,19を入力とし、電極16,18を出力電
極としても、又、電極16,18を入力とし電極
17,19を出力電極としてよい。 Moreover, as a more preferable case, there is an element in which all the resistance values between adjacent electrodes are the same. In this case, all the electrodes have a completely symmetrical relationship, with electrodes 17 and 19 serving as input and electrodes 16 and 18 serving as output electrodes, and electrodes 16 and 18 serving as input and electrodes 17 and 19 serving as output electrodes. good.
この発明の素子における半導体薄膜11の基本
のパターンは、第4図に示したものであるが、こ
のパターンの基本的な構成をかえないどのような
変形もこの発明に属することはもちろんであり、
これは素子を構成する材質、その他の要件によつ
てかわるものではない。従つて、実用的な素子を
製作するため、各隣接電極間の通路の長さ、シヨ
ートバー14の幅、シヨートバー14の間隔、半
導体薄膜11の幅、外部接続用の端子電極16〜
19の大きさ等は自由にかえてよく、又、各電極
間の抵抗値も設計で自由にえらべることはもちろ
んである。半導体薄膜11の各種パターンの例を
第5図A〜Fに示す。更に、この発明は素子が載
置される基板にも限定されるものでなく、かつ下
地の絶縁基板と感磁部の半導体薄膜とが一体で形
成されていてもよく、又別のものであつてもよ
い。 The basic pattern of the semiconductor thin film 11 in the device of this invention is shown in FIG. 4, but it goes without saying that any modification that does not change the basic structure of this pattern also belongs to this invention.
This does not change depending on the material constituting the element or other requirements. Therefore, in order to manufacture a practical device, the length of the path between adjacent electrodes, the width of the shoot bars 14, the spacing between the shoot bars 14, the width of the semiconductor thin film 11, and the terminal electrodes 16 for external connection are determined.
It goes without saying that the size of 19 can be changed freely, and the resistance value between each electrode can also be freely selected in the design. Examples of various patterns of the semiconductor thin film 11 are shown in FIGS. 5A to 5F. Furthermore, the present invention is not limited to the substrate on which the element is mounted, and the underlying insulating substrate and the semiconductor thin film of the magnetically sensitive part may be formed integrally or may be formed separately. You can.
次に、この発明の磁気抵抗素子の半導体薄膜1
1、即ち感磁部を構成する材料としては、化合物
半導体が用いられ、特にInSb,InxGaySbz(x+
y+z=2),GaAs,InAs,InP等が好ましく、
更にこれらの材料で移動度が高いほど好ましい。
シヨートバー14は上記の感磁部半導体薄膜11
をオーミツク接触をする金属より構成される。シ
ヨートバー14は、一種類の金属、合金又は二
層、三層の金属より構成されてもよく、これらの
適当な組合せも用いられる。 Next, the semiconductor thin film 1 of the magnetoresistive element of this invention
1. In other words, compound semiconductors are used as the material constituting the magnetically sensitive part, especially InSb, In x Ga y Sb z (x+
y+z=2), GaAs, InAs, InP, etc. are preferable,
Furthermore, the higher the mobility of these materials, the more preferable.
The shot bar 14 is the magnetically sensitive part semiconductor thin film 11.
It is made of metal that makes ohmic contact. The short bar 14 may be constructed of one type of metal, an alloy, or two or three layers of metal, or any suitable combination thereof may be used.
外部接続用の端子電極16〜19は、感磁部半
導体薄膜11とオーミツク接触をする金属より構
成され、シヨートバー14と同一の構成のもので
ももちろんよい。しかし、端子電極は通常素子の
リード付けのとき行なわれているリード線を接続
するための工夫が更に加えられる場合もある。そ
のためには通常は、ハンダが表面に付き易い金属
層とハンダが付けられたり、又、ワイヤポンデイ
ング金属層が表面に形成される。図に示してない
が、リード線等の外部引き出し線が47の端子電
極に付けられたあと、保護のために半導体素子で
通常行なわれるパツケージとして樹脂によるモー
ルドが行なわれたり、金属によるメタルパツケー
ジが行なわれる。 The terminal electrodes 16 to 19 for external connection are made of metal that makes ohmic contact with the magnetically sensitive semiconductor thin film 11, and may of course have the same structure as the shot bar 14. However, the terminal electrodes may be further modified to connect lead wires that are normally used when attaching leads to devices. For this purpose, a metal layer to which solder easily adheres is usually attached to the surface, or a wire bonded metal layer is formed on the surface. Although not shown in the figure, after external lead wires such as lead wires are attached to the terminal electrodes of 47, resin molding is performed as a package normally used for semiconductor devices for protection, or metal packaging is used. It is done.
次に、この発明素子の製作方法を実施例によつ
て説明するが、この発明はこれら実施例の場合の
みに限定されるものではない。 Next, a method of manufacturing the device of the present invention will be explained using Examples, but the present invention is not limited to these Examples.
実施例 1
表面が平滑なマイカ基板上に、厚さ1μm、電
子移動度25000cm2/vsecの1nSb薄膜を真空蒸着に
より形成した。次に、このInSb薄膜の表面に、
日本ペルノツクス社製エポキシ樹脂、ME―264
を塗布し、厚さ0.3mm、一辺が37mmの正方形をし
たNi―Zn系のフエライト基板上に接着した。つ
いで、マイカを除去した。Example 1 A 1 nSb thin film having a thickness of 1 μm and an electron mobility of 25000 cm 2 /vsec was formed by vacuum evaporation on a mica substrate with a smooth surface. Next, on the surface of this InSb thin film,
Epoxy resin manufactured by Nippon Pernox Co., Ltd., ME-264
was applied onto a square Ni-Zn ferrite substrate with a thickness of 0.3 mm and a side of 37 mm. Then, mica was removed.
次に、コダツク社製マイクロフオトレジスト
752を使用し、通常行なわれている方法で、InSb
薄膜の表面にフオトレジスト被膜を形成した。次
に、室町化学製の無電解メツキ液MK―400を使
用し、液温28℃、30分間無電解メツキを行い銅を
厚さ1.0μ所要の部分のみに付着させオーミツク接
触電極用の金属層を形成した。 Next, Kodatsu Microphotoresist
752 in the usual way, InSb
A photoresist coating was formed on the surface of the thin film. Next, using Muromachi Kagaku's electroless plating liquid MK-400, electroless plating was performed for 30 minutes at a liquid temperature of 28℃ to deposit copper only on the required part with a thickness of 1.0μ, forming the metal layer for the ohmic contact electrode. was formed.
次に、無電解メツキ液をかえて、更に銅の厚付
けを行うため、シツプし一社の無電解メツキ液
CP―802を用い、液温50℃で30分間メツキを行
い、更に2.0μの銅を付着せしめた。こうして、二
段のパターンメツキ法の工程を終えたあと、上記
のメツキ用のフオトレジストをトリクレンで除去
した。 Next, in order to change the electroless plating solution and further thicken the copper, we used an electroless plating solution from one company.
Using CP-802, plating was performed for 30 minutes at a liquid temperature of 50°C, and an additional 2.0μ of copper was deposited. After completing the two-stage pattern plating process in this manner, the photoresist for plating was removed using trichloride.
次に、上記のフオトレジストを再度用い、フオ
トリソグラフイーの手法により不要なInSb及び、
一部の不要な銅を塩化第2鉄の塩酸々性水溶液
で、エツチング除去し、第4図に示したこの発明
素子の感磁部半導体薄膜11及び4つの端子電極
16〜19を形成した。その後上記のフオトレジ
ストを使用し、フオトリソグラフイの手法によ
り、この発明素子の電極16〜19のみを残し
て、その他の部分にレジストの被膜を形成したの
ち、溶融ハンダ槽につけることにより、電極16
〜19のみにハンダをつけた。ついで、上記レジ
ストを除去し、素子を一辺が34mm角のフエライト
ウエーハー上に約300個形成した。 Next, using the above photoresist again, unnecessary InSb and
A part of the unnecessary copper was removed by etching with a hydrochloric-acidic aqueous solution of ferric chloride to form the magnetically sensitive semiconductor thin film 11 and four terminal electrodes 16 to 19 of the device of the invention shown in FIG. Thereafter, using the photoresist described above, a resist film was formed on the other parts by photolithography, leaving only the electrodes 16 to 19 of the device of the present invention, and then the electrodes were placed in a molten solder bath. 16
I soldered only ~19. Then, the resist was removed, and about 300 elements were formed on a ferrite wafer having a side of 34 mm.
次に、このウエハーをダイシングカツターにか
け、1.8mm×1.7mmの方形素子チツプに切断した。
そのおのおのに4本のリード線をハンダ付けし、
大きさが2.4mm×2.8mmで高さ1.5mmのエポキシ樹脂
の箱に入れ、日本ベルノツクス社製のモールド用
エポキシ樹脂、ME―264でモールドし、第4図
に示したこの発明の磁気抵抗素子を製作した。 Next, this wafer was cut into square element chips measuring 1.8 mm x 1.7 mm using a dicing cutter.
Solder the four lead wires to each one,
The magnetoresistive element of the present invention was placed in an epoxy resin box with a size of 2.4 mm x 2.8 mm and a height of 1.5 mm, and molded with ME-264, an epoxy resin for molding made by Nippon Vernox Co., Ltd., as shown in Fig. 4. was produced.
こうして製作したこの発明素子の特性は次の如
くであつた。 The characteristics of the inventive device thus manufactured were as follows.
各隣接電極相互間の抵抗値は500±5Ωであり、
電極17,19間に1Vの電圧を印加したとき、
電極16,18間に発生するオフセツト電位差は
0.5±4.1mVであり、実質的にゼロに近い値であ
つた。素子全体に3K.Gの磁界を印加したとき、
電極16,18間の電位差(出力電圧)は±
6mVとなつた。又、電極16及び電極18の各
中点電位500mVからのずれは上記電極16,1
8間の電位差の半分であつた。このように、この
発明素子では磁界印加時の出力は、従来素子(例
えば第3図のもの)の2倍となり、又、実質的な
オフセツト電圧、即ち磁界を印加しないときの電
極16,18間の電位差は著しく小さい。従つ
て、実用上極めて有用性大なる磁気抵抗素子であ
る。 The resistance value between each adjacent electrode is 500±5Ω,
When a voltage of 1V is applied between electrodes 17 and 19,
The offset potential difference generated between electrodes 16 and 18 is
The value was 0.5±4.1 mV, which was substantially close to zero. When a 3K.G magnetic field is applied to the entire element,
The potential difference (output voltage) between electrodes 16 and 18 is ±
It became 6mV. Moreover, the deviation from the midpoint potential of each electrode 16 and electrode 18 is 500 mV.
It was half of the potential difference between 8 and 8. As described above, in the device of this invention, the output when a magnetic field is applied is twice that of the conventional device (for example, the one in FIG. 3), and the substantial offset voltage, that is, the output between the electrodes 16 and 18 when no magnetic field is applied, The potential difference between is extremely small. Therefore, it is a magnetoresistive element that is extremely useful in practice.
実施例 2
表面が平滑な2インチ角のセラミツク基板上
に、厚さ1μmのSiO2薄膜層をスパツターにより
形成した。次に、厚さ1.0μm、電子移動度22000
cm2/vsecのInSb薄膜を真空蒸着により形成した。
次に実施例1におけるフエライト基板上に接着し
たInSb薄膜に対して行なつたと同様の手法によ
りこの発明の磁気抵抗素子を作つた。ただしこの
場合は一辺が37mm角のフエライトウエーハー上に
約400個の素子を形成した。こうして製作したこ
の発明の素子の特性は、次の如くであつた。Example 2 A 1 μm thick SiO 2 thin film layer was formed by sputtering on a 2 inch square ceramic substrate with a smooth surface. Next, the thickness is 1.0μm, the electron mobility is 22000
An InSb thin film of cm 2 /vsec was formed by vacuum evaporation.
Next, a magnetoresistive element of the present invention was fabricated using the same method as that applied to the InSb thin film adhered to the ferrite substrate in Example 1. However, in this case, approximately 400 elements were formed on a 37 mm square ferrite wafer. The characteristics of the device of the present invention thus manufactured were as follows.
各電極間相互の抵抗値は560±5Ωであり、電
極17,19間に1Vの電圧を印加したとき、電
極16,18間に生ずるオフセツト電位差は0.8
±3.5mVでほとんどゼロに近い値であつた。 The mutual resistance value between each electrode is 560±5Ω, and when a voltage of 1V is applied between electrodes 17 and 19, the offset potential difference generated between electrodes 16 and 18 is 0.8
The value was ±3.5mV, which was almost zero.
素子全体に、3K.Gの磁界を印加したとき電極
16,18間に生ずる電位差(出力電圧)は±
6.5mVであつた。又、電極16及び電極18の各
中点電位500mVよりのずれは、上記電極16,
18の電位差の正しく半分であつた。このよう
に、この発明素子では磁界印加時の出力電圧即
ち、電極16,18間の電位差は、従来素子、第
3図に示したものと比較して2倍となる。又、実
質的なオフセツト電圧は上記の如く小さい。従つ
て、実用上極めて有用性の高い磁気抵抗素子であ
る。 When a 3K.G magnetic field is applied to the entire element, the potential difference (output voltage) generated between electrodes 16 and 18 is ±
It was 6.5mV. Moreover, the deviation from the midpoint potential of each electrode 16 and electrode 18 from 500 mV is determined by the difference between the electrodes 16 and 18.
It was exactly half of the potential difference of 18. As described above, in the device of the present invention, the output voltage when a magnetic field is applied, that is, the potential difference between the electrodes 16 and 18, is twice that of the conventional device shown in FIG. Also, the actual offset voltage is small as described above. Therefore, it is a highly useful magnetoresistive element in practice.
第1図は従来の2端子の磁気抵抗素子のパター
ン例を示す図、第2図及び第3図はそれぞれ従来
の3端子の磁気抵抗素子のパターン例を示す図、
第4図はこの発明による磁気抵抗素子のパターン
例を示す図、第5図はこの発明素子の各種変形パ
ターン例を示す図である。
11:磁気抵抗効果を有する半導体薄膜、1
4:シヨートバー、16〜19:端子電極。
FIG. 1 is a diagram showing an example of a pattern of a conventional two-terminal magnetoresistive element, FIGS. 2 and 3 are diagrams each showing an example of a pattern of a conventional three-terminal magnetoresistive element,
FIG. 4 is a diagram showing an example of a pattern of a magnetoresistive element according to the present invention, and FIG. 5 is a diagram showing examples of various modified patterns of the element of this invention. 11: Semiconductor thin film with magnetoresistive effect, 1
4: shot bar, 16-19: terminal electrode.
Claims (1)
半導体薄膜と、その半導体薄膜上に間隔をおいて
形成され、オーミツク電極から成る外部接続用の
第1、第2、第3及び第4端子電極と、上記第
1、第2端子電極間及び第3、第4端子電極間の
上記半導体薄膜上に形成され、オーミツク電極よ
り成るシヨートバーとを具備し、上記第2、第3
端子電極間、上記第1、第4端子電極間の上記半
導体薄膜上にはシヨートバーが形成されていない
4端子磁気抵抗素子。 2 第1、第2端子電極間と、上記第1、第4端
子電極間との各抵抗値が等しく、かつ上記第3、
第4端子電極間と、上記第3、第2端子電極間の
各抵抗値が等しくされている特許請求の範囲第1
項記載の磁気抵抗素子。 3 互いに、相となりあう端子電極間の各抵抗値
がすべて等しい特許請求の範囲第1項又は第2項
記載の磁気抵抗素子。[Scope of Claims] 1. A semiconductor thin film having a magnetoresistive effect formed in a loop shape, and first, second, and third electrodes for external connection formed at intervals on the semiconductor thin film and consisting of ohmic electrodes. and a fourth terminal electrode, and a shot bar formed on the semiconductor thin film between the first and second terminal electrodes and between the third and fourth terminal electrodes and consisting of an ohmic electrode;
A four-terminal magnetoresistive element in which no shot bar is formed on the semiconductor thin film between the terminal electrodes and between the first and fourth terminal electrodes. 2. Each resistance value between the first and second terminal electrodes is equal to that between the first and fourth terminal electrodes, and the third,
Claim 1, wherein the resistance values between the fourth terminal electrode and between the third and second terminal electrodes are equal.
Magnetoresistive element as described in section. 3. The magnetoresistive element according to claim 1 or 2, wherein the resistance values between the terminal electrodes that are in phase with each other are all equal.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56002898A JPS57115889A (en) | 1981-01-12 | 1981-01-12 | Four-terminal magnetic resistance element |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56002898A JPS57115889A (en) | 1981-01-12 | 1981-01-12 | Four-terminal magnetic resistance element |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS57115889A JPS57115889A (en) | 1982-07-19 |
| JPS6353713B2 true JPS6353713B2 (en) | 1988-10-25 |
Family
ID=11542166
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP56002898A Granted JPS57115889A (en) | 1981-01-12 | 1981-01-12 | Four-terminal magnetic resistance element |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS57115889A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS63226084A (en) * | 1987-03-13 | 1988-09-20 | Matsushita Electric Ind Co Ltd | magnetoresistive element |
-
1981
- 1981-01-12 JP JP56002898A patent/JPS57115889A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS57115889A (en) | 1982-07-19 |
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