JPH0210882A - Semiconductor thin film magnetoresistance element and manufacture thereof - Google Patents

Semiconductor thin film magnetoresistance element and manufacture thereof

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Publication number
JPH0210882A
JPH0210882A JP63161718A JP16171888A JPH0210882A JP H0210882 A JPH0210882 A JP H0210882A JP 63161718 A JP63161718 A JP 63161718A JP 16171888 A JP16171888 A JP 16171888A JP H0210882 A JPH0210882 A JP H0210882A
Authority
JP
Japan
Prior art keywords
thin film
insb
semiconductor
material layer
alkaline earth
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
Application number
JP63161718A
Other languages
Japanese (ja)
Inventor
Hiroshi Ishihara
宏 石原
Akihiro Korechika
哲広 是近
Keizaburo Kuramasu
敬三郎 倉増
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP63161718A priority Critical patent/JPH0210882A/en
Publication of JPH0210882A publication Critical patent/JPH0210882A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To obtain sufficient reliability even in high temperature use such as a gear sensor for a vehicle by forming a material layer made of alkaline earth metal fluoride on a board, and forming a high mobility semiconductor material thin film on the layer. CONSTITUTION:After alkaline earth fluoride and particularly a material layer 2 made of any selected from CaF2, SrF2, BaF2 is formed on a board made of insulator or semiconductor or a surface insulated board 1, a high mobility semiconductor material thin film and particularly a thin film 3 made of InSb is formed. The layer 2 made of the alkaline earth metal fluoride and particularly BaF2 is similar to the lattice constant of InSb, a mixed crystal suitably mixed with CaF2, SrF2, etc. is employed in response to the adaptability of lattice constant with a base board material. Thus, the BaF2, CaF2, SrF2, etc., are oriented in a specific direction on the board, becoming a nucleus forming material of the InSb thin film, and its adhesive properties are satisfactory. Thus, stability at high temperature and high mobility can be imparted thereto.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は、回転センサ等に用いられる半導体薄膜磁電抵
抗素子の半導体薄膜の製造方法に関する。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a method for manufacturing a semiconductor thin film of a semiconductor thin film magnetoresistive element used in a rotation sensor or the like.

従来の技術 一般に、回転センサとしては、光方式、磁気方式を初め
、種々の方式がある。この中で、特に汚れ、塵埃等、雰
囲気の影響を受ける用途においては、そうした影響を受
けにくい磁気方式が最も有利である。一方、この磁気方
式においても、電磁ピックアップ、ホール素子、磁気抵
抗素子等、種種の方式がある。
2. Description of the Related Art In general, there are various types of rotation sensors including optical type and magnetic type. Among these, the magnetic method, which is less susceptible to such influences, is the most advantageous, particularly in applications that are affected by the atmosphere, such as dirt and dust. On the other hand, in this magnetic method, there are various methods such as an electromagnetic pickup, a Hall element, and a magnetoresistive element.

近年、自動車の電子化に伴ない、この為に各種センサ素
子が装着される中で、回転センサ、特にギヤセンサとし
ては、これまで、簡易で温度特性が良い点から、電磁ピ
ックアップ(インダクタンス型)が用いられてきた。し
かしながら、最近自動車用回転センサに要求される性質
として、非常に低速(Okm/h〜)から検出可能であ
ることが挙げられる。この点から、前述した電磁ピック
アップは、元来、低速度(0〜50RPM)の検出が不
可能であること及び、小型化が困難な点から、実用化さ
れているものの、必ずしも、現在の要求と合致してはい
ない。
In recent years, with the electronicization of automobiles, various sensor elements have been installed for this purpose. Until now, electromagnetic pickups (inductance type) have been used as rotation sensors, especially gear sensors, due to their simplicity and good temperature characteristics. has been used. However, one of the properties recently required of automotive rotation sensors is that they can be detected at very low speeds (0 km/h and up). From this point of view, although the electromagnetic pickup described above has been put into practical use because it is originally impossible to detect low speeds (0 to 50 RPM) and is difficult to miniaturize, it does not necessarily meet current requirements. It does not match.

一方、ホール素子(ホールIC)、強磁性薄膜磁気抵抗
素子、半導体磁気抵抗素子は、いずれも、前述した低速
からの検出が可能である。これらの素子には、各々、一
長一短があるが、自動車用回転センサとして捕える際、
決め手となるのは、(1)できるだけ、自動車に元々設
けである部品(歯付きロータ等)から直接検出可能であ
ること。
On the other hand, the Hall element (Hall IC), the ferromagnetic thin film magnetoresistive element, and the semiconductor magnetoresistive element are all capable of detection from the aforementioned low speed. Each of these elements has advantages and disadvantages, but when used as an automotive rotation sensor,
The deciding factors are: (1) it should be possible to directly detect parts that are originally installed in the car (such as toothed rotors) as much as possible.

(2)素子の動作温度範囲が一50〜+160°Cを満
足すること。
(2) The operating temperature range of the element must be 150 to +160°C.

02点が考えられる。02 points are possible.

(1)に対して、具体的に要求されるのは、例えば、歯
付きロータと素子の間の距離(以降、ギャップと呼ぶ)
の許容度が大きいことで、この為には、ギャップを拡げ
ることに伴う出力の落ちが小さいことが望まれる。この
点で考えれば、ホール素子。
For (1), what is specifically required is, for example, the distance between the toothed rotor and the element (hereinafter referred to as the gap)
To this end, it is desirable that the drop in output due to widening the gap be small, since the tolerance for this is large. If you think about it from this point of view, it is a Hall element.

ホールIC,強磁性薄膜磁気抵抗素子は、出力が小さく
、ギャップが小さい為に、ギヤセンサとしては使いにく
く、一方、半導体磁気抵抗素子は、元々、出力が大きく
、ギャップの許容度も大きく、また、現状の電磁ピック
アップと同じ様な検出方法を用いる為、代替も容易であ
る為、ギヤセンサに適しているものと考えられる。
Hall ICs and ferromagnetic thin-film magnetoresistive elements have low output and small gaps, making them difficult to use as gear sensors. On the other hand, semiconductor magnetoresistive elements have originally large output and large gap tolerance, and Since it uses the same detection method as current electromagnetic pickups, it is easy to replace, so it is considered suitable for gear sensors.

反面(2)の温度特性に関して、現状で、これを満足す
るものは、わずかに、Ga1gホールICのみである。
On the other hand, regarding the temperature characteristic (2), at present, only a Ga1g Hall IC satisfies this.

しかし、このGaAsホールICは、前述した通り、ギ
ャップが小さくなければならず、自動車用ギヤセンサと
しては、必ずしも適当でない。
However, as described above, this GaAs Hall IC must have a small gap and is not necessarily suitable as an automobile gear sensor.

これ等の点を総合すると、結局、自動車用ギヤセンサと
しては、耐温度性を改良することを前提とすれば、半導
体磁気抵抗素子が、最も適当な素子と言える。この半導
体磁気抵抗素子の特性は、衆知の通り、素材の移動度で
決まる。即ち、低磁界での出力は、移動度の自乗に比例
し、高磁界での出力は、移動度に比例する。
Taking all these points together, it can be said that a semiconductor magnetoresistive element is the most suitable element for an automobile gear sensor, provided that the temperature resistance is improved. As is well known, the characteristics of this semiconductor magnetoresistive element are determined by the mobility of the material. That is, the output in a low magnetic field is proportional to the square of the mobility, and the output in a high magnetic field is proportional to the mobility.

従って、半導体磁気抵抗素子の材料としては、半導体中
、移動度が最大であるInSbが多用されている。一方
、衆知の通り、InSbの禁制帯幅は、0.17 eV
と狭く、室温でも、真性伝導を示し、素材の抵抗温度係
数は、−2%/deg、  と大きい。
Therefore, InSb, which has the highest mobility among semiconductors, is often used as a material for semiconductor magnetoresistive elements. On the other hand, as is well known, the forbidden band width of InSb is 0.17 eV
It exhibits intrinsic conduction even at room temperature, and the temperature coefficient of resistance of the material is as large as -2%/deg.

この為、通常、磁気抵抗素子を直列に2個接続し、差動
的に用いることが、一般的で、この際の出力の温度係数
は、−〇、2%/dog、  で、この値は、GaAs
ホールI C+7)出力の温度係数−o、1%/dog
For this reason, it is common to connect two magnetoresistive elements in series and use them differentially, and the temperature coefficient of the output in this case is -〇, 2%/dog, and this value is , GaAs
Hall I C+7) Temperature coefficient of output -o, 1%/dog
.

と比して、大きな遜色はない。There is no big difference compared to.

つまり、InSb磁気抵抗素子を、差動的に用いれば、
室温〜+150°C間の出力の落ちは、高々、20〜3
0%の落ちに過ぎず、デジタル的に用いるのであれば、
問題とならない。
In other words, if InSb magnetoresistive elements are used differentially,
The drop in output between room temperature and +150°C is at most 20-3
If it is only a 0% drop and used digitally,
Not a problem.

ところで、現在、市販されているInSb磁気抵抗素子
は、大半が、バルク型を用いており、薄膜型を用いてい
る所は、極めて少ない。この最も大きな理由は、前述し
た様に、半導体磁気抵抗素子の出力は、移動度が大きい
程、大きいという点(通常、半導体磁気抵抗素子として
必要な移動度は、200oOv/Cd以上)である。即
ち、バルク単結晶、多結晶は、薄膜型非エピタキシャル
なものより、常に移動度が大きい為である。しかし、前
述した、−60〜+150’Cの温度範囲を考えた場合
、少し様相が異なる。
By the way, most of the InSb magnetoresistive elements currently on the market are of the bulk type, and very few are of the thin film type. The most important reason for this is that, as described above, the output of a semiconductor magnetoresistive element increases as its mobility increases (normally, the mobility required for a semiconductor magnetoresistive element is 200 oOv/Cd or more). That is, bulk single crystals and polycrystals always have higher mobility than thin film non-epitaxial ones. However, when considering the above-mentioned temperature range of -60 to +150'C, the situation is slightly different.

通常、InSb磁気抵抗素子の動作温度範囲は、−20
〜+80°C程度で、これは、アナログ的な出力を得る
為の動作限界である点および、高温になるのに伴ない、
抵抗が下がり、従って、動作電力が大きくなることに伴
なう自己発熱の増加に依る素子破断を含む劣化に起因す
る。
Typically, the operating temperature range of InSb magnetoresistive elements is -20
~+80°C, which is the operating limit for obtaining analog output, and as the temperature increases,
This results in degradation, including device failure, due to increased self-heating as the resistance decreases and therefore the operating power increases.

通常InSbでは、その移動度は、低温域で、不純物散
乱高温域で、有極性光学散乱に依って支配され、それら
各々の依存する領域の境界に、移動度のピーク値を取る
。ピーク値から高温側では、はぼ移動度は、温度の−1
,7乗に沿って変化する。
Normally, in InSb, its mobility is dominated by polar optical scattering in the low temperature region, impurity scattering in the high temperature region, and the peak value of the mobility is at the boundary of each dependent region. On the high temperature side from the peak value, the mobility is -1 of the temperature.
, changes along the seventh power.

バルク単結晶等では、移動度は、極低温側(70に付近
)で、急峻なピークを持つのに対し、薄膜型での移動度
のピークは、高温側にシフトし、室温付近で幾分ブロー
ドなピークを持つ。従って、高温用途に対しては、薄膜
型の方が好ましく、加えて、薄膜型の方が、高抵抗化が
容易で、この為、素子の低消費電力化、小型化が可能な
為、有利である。これら薄膜型の利点があるにも関わら
ず、それ程、これが普及していない点および、高温用途
で用いられていない原因としては、以下の事柄が考えら
れる。
In bulk single crystals, etc., the mobility has a steep peak at extremely low temperatures (around 70°C), whereas in thin film types, the mobility peak shifts to the high temperature side and decreases somewhat around room temperature. Has a broad peak. Therefore, for high-temperature applications, the thin-film type is preferable, and in addition, the thin-film type is advantageous because it is easier to increase the resistance, and therefore allows for lower power consumption and miniaturization of the element. It is. Despite these advantages of the thin film type, the reasons why it is not widely used and why it is not used in high temperature applications are considered to be as follows.

まず、第1点として、薄膜型非エピタキシャルなもので
、移動度を向上することにおける本質的な難しさ。(エ
ビタキンヤルでは、CdTe、 PbTe基板等を用い
れば、可能と考えられるが、基板コストが、極めて高い
) しかし、これに対しては、東洋通信機技報、應40(1
987)で、線中等が述べている通り、へき開マイカ基
板を用いた場合、単結8並みの移動度が得られることが
、明らかになっている。反面、この方法では、高温用途
で用いることは困難である。それは、InSbとマイカ
基板の密着性が悪い為、このInSbを別の支持基板上
に、エポキシ等の接着層を介して転写するプロセスを用
いている点である。こうしたプロセスを用いる為、どう
しても、でき上った素子においては、高温時に、接着層
とInSb薄膜間の熱膨張係数の相異が大きく、I n
sb薄膜に亀裂が生じる等、特に、前述した一5o〜+
160°Cの温度範囲において、実用に耐え得る信頼性
を有していなかった。
First, there is the inherent difficulty in improving mobility with thin-film non-epitaxial devices. (For Evita Kinyal, it is possible to use a CdTe, PbTe substrate, etc., but the substrate cost is extremely high.)
987), it has been revealed that when a cleaved mica substrate is used, a mobility comparable to that of single bond 8 can be obtained, as stated by Line et al. On the other hand, this method is difficult to use in high-temperature applications. This is because the adhesion between InSb and the mica substrate is poor, so a process is used in which this InSb is transferred onto another support substrate via an adhesive layer such as epoxy. Because such a process is used, it is inevitable that the finished device will have a large difference in thermal expansion coefficient between the adhesive layer and the InSb thin film at high temperatures.
In particular, cracks occur in the sb thin film, etc.
It did not have reliability sufficient for practical use in a temperature range of 160°C.

発明が解決しようとする課題 上述した様に、ギヤセンサとしては、InSb磁気抵抗
素子が、最も適切であり、且つ、自動車用等、高温用途
においては、バルク型よりも薄膜型の方が好ましいが、
一方で、薄膜型において、移動度を向上させる目的で用
いられるマイカ基板とInSbの密着性が悪いことに依
る転写プロセスの適用は、高温時、或いは、低温〜高温
の温度サイクル時に、InSb薄膜と、接着層(エポキ
シ等)の間の熱膨張係数の違いに伴なうInSbへの亀
裂の発生を招き、自動車用等の高温用途に供する為の十
分な信頼性を有していなかった。かかる点から本発明は
、自動車用ギヤセンサ等、特に、高温用途においても、
十分な信頼性を有する半導体薄膜磁気抵抗素子の製造方
法を提供することを主たる目的とするものである。
Problems to be Solved by the Invention As mentioned above, an InSb magnetoresistive element is most suitable as a gear sensor, and in high-temperature applications such as automobiles, a thin film type is preferable to a bulk type.
On the other hand, in the thin film type, application of the transfer process due to the poor adhesion between InSb and the mica substrate used for the purpose of improving mobility is due to the fact that the InSb thin film and However, cracks were caused in the InSb due to the difference in thermal expansion coefficient between the adhesive layers (epoxy, etc.), and the InSb did not have sufficient reliability for use in high-temperature applications such as automobiles. From this point of view, the present invention is applicable to gear sensors for automobiles, etc., especially in high-temperature applications.
The main purpose of this invention is to provide a method for manufacturing a semiconductor thin film magnetoresistive element with sufficient reliability.

課題を解決するための手段 本発明は、上記課題を解決する為に、絶縁物もしくは半
導体よりなる基板、或いは、表面絶縁化基板を用い、こ
の上に、アルカリ土類弗化物、特に、CaF2. Sr
F2. BILF2(7)中より選ばれたもの(混晶を
含む)よりなる材料層を形成した後、高移動度半導体材
料薄膜、特に、InSbよりなる薄膜を形成するもので
ある。
Means for Solving the Problems In order to solve the above problems, the present invention uses a substrate made of an insulator or a semiconductor, or a surface-insulated substrate, and coats an alkaline earth fluoride, particularly CaF2. Sr.
F2. After forming a layer of material selected from BILF2(7) (including mixed crystal), a thin film of a high mobility semiconductor material, particularly a thin film of InSb, is formed.

作用 上述した構成において、アルカリ土類金属弗化物よりな
る材料層、特にBaF、、はInSbと格子定数が近く
、下地基板材料との格子定数等の適合性に応じ、CaF
、SrF2等も適宜混合した混晶等も用いることに依り
、これらBaF2. CaF2. SrF、、等は、下
地基板上に特定方位をもって配向し、InSb薄膜の良
好な核形成材となり、かつ密着性も良好である。
Effect In the above structure, the material layer made of alkaline earth metal fluoride, especially BaF, has a lattice constant close to that of InSb, and depending on the compatibility of the lattice constant etc. with the underlying substrate material, CaF
, SrF2, etc., as well as mixed crystals mixed appropriately, these BaF2. CaF2. SrF, etc. are oriented in a specific direction on the base substrate, and serve as a good nucleation material for the InSb thin film, and also have good adhesion.

以上の点から、上述した構成に依り、高温における安定
性と、高移動度を有する半導体薄膜磁気抵抗素子を構成
できる。
From the above points, the above-described configuration makes it possible to construct a semiconductor thin film magnetoresistive element having stability at high temperatures and high mobility.

実施例 (実施例1) 第1図に、本発明の半導体薄膜磁気抵抗素子の製造方法
の基本構成を示す。本実施例では、基板1としてCGW
#7059 (−y−ニング社製)を用いた。(CGW
gyo69の線膨張係数は、4.6X10  (K  
))  この基板1を洗浄後、直ちに真空蒸着装置内に
導入し、真空度をlX10’Torr以下にした後、8
00〜900℃で基板1の表面を10分間加熱もしくは
、Ar、H2等のガスプラズマもしくは、イオンビーム
に依り、基板1の表面をスパッタリング効果でたたき、
いずれにしても、基板表面の清浄化を行った後、基板温
度600〜7oo℃、真空度10 ’order(To
rr)以下において、第1図(blに示す様に、アルカ
リ土類金属弗化物よりなる材料層2、本実施例では、B
aF2よりなる材料層2を抵抗加熱方式でBaF2イン
ゴットを蒸発させることにより、基板1上に形成する。
Example (Example 1) FIG. 1 shows the basic configuration of the method for manufacturing a semiconductor thin film magnetoresistive element of the present invention. In this embodiment, CGW is used as the substrate 1.
#7059 (manufactured by -Y-Ning Co., Ltd.) was used. (CGW
The linear expansion coefficient of gyo69 is 4.6X10 (K
)) Immediately after cleaning this substrate 1, it was introduced into a vacuum evaporation apparatus, and after reducing the degree of vacuum to 1 x 10' Torr or less,
The surface of the substrate 1 is heated at 00 to 900° C. for 10 minutes, or the surface of the substrate 1 is hit with a sputtering effect using gas plasma such as Ar or H2, or an ion beam.
In any case, after cleaning the substrate surface, the substrate temperature is 600-700°C and the vacuum degree is 10' order (To
rr) Below, as shown in FIG. 1 (bl), the material layer 2 made of alkaline earth metal fluoride, in this example, B
A material layer 2 made of aF2 is formed on the substrate 1 by evaporating a BaF2 ingot using a resistance heating method.

これら一連の工程において、BaF2でなる材料層2の
基板温度は、600〜700°Cの範囲では、高い程、
その結晶性は、改善され、また、圧力が低い程、結晶性
は、良好となる。また、本実施例で、BaF 2よりな
る材料層2をBaF2インゴットの抵抗加熱に依り、形
成した理由として、他に、電子ビーム等で形成した場合
、BaF 2の一部が構成元素に分解し、BaF2でな
る材料層2でストイキオメトリ−からのずれが生じるの
に対し、抵抗加熱では、良好なストイキオメトリ−性を
保てることにある。
In these series of steps, the substrate temperature of the material layer 2 made of BaF2 is in the range of 600 to 700°C, the higher the
Its crystallinity is improved, and the lower the pressure, the better the crystallinity. In addition, in this example, the material layer 2 made of BaF 2 was formed by resistance heating of a BaF 2 ingot. Another reason is that when it is formed with an electron beam or the like, a part of BaF 2 decomposes into its constituent elements. , a deviation from stoichiometry occurs in the material layer 2 made of BaF2, whereas resistance heating can maintain good stoichiometry.

以上の工程を経て、得られるBaF 2よりなる材料層
2は、鋭く(111)方向に配向する。
Through the above steps, the material layer 2 made of BaF 2 obtained is sharply oriented in the (111) direction.

この後、第1図(C)に示す様に、InSb薄膜3を形
成する。このInSb薄膜3は、基板温度400〜50
00C1真空度10 ’0rder(TOrr)  で
、In、 Sbを各々、個別ソースとしてソース温度を
個別に制御して成膜を行う三温度法に依って行った。こ
れに依って得られたInSb薄膜3の結晶性は、基板温
度400〜500″Cにおいては、温度が高い程、また
、初期核生成に影響を与える初期成膜速度が遅い程、そ
して、その後の成膜速度を速くする程、向−ヒした。こ
の成膜速度の高速化は、通常の結晶成長における様に、
成膜速度を遅くする場合と異なる。それは、通常の薄膜
の結晶成長では、1 o−8Torr以下の高真空を用
いる為、成長面へのガス吸着を考えなくても良いのに対
して、本実施例の成膜時真空度1o ’order(T
orr)では、例えば、酸素ガスの吸着は、はんの数秒
で生じる為、膜の純度を上げることの為に必要とされる
Thereafter, as shown in FIG. 1(C), an InSb thin film 3 is formed. This InSb thin film 3 has a substrate temperature of 400 to 50
The film was formed using a three-temperature method in which In and Sb were each used as separate sources and the source temperatures were individually controlled at a vacuum level of 10'0rder (TOrr). The crystallinity of the InSb thin film 3 obtained in this way changes as the substrate temperature increases from 400 to 500''C, the higher the temperature, the slower the initial deposition rate that affects initial nucleation, and the later The faster the film formation rate, the more the damage was improved.
This is different from the case where the film formation rate is slowed down. This is because, in normal thin film crystal growth, a high vacuum of 1 o-8 Torr or less is used, so there is no need to consider gas adsorption to the growth surface, whereas in this example, the vacuum level during film formation was 1 o' order(T
orr), for example, adsorption of oxygen gas occurs within a few seconds of the electrolyte and is therefore required to increase the purity of the membrane.

この様にして成膜を行うことに依り、InSb薄膜3の
厚さ1μm程度で、十分膜面方向(横方向)にグレイン
サイズが大きく、室温での移動度が、aooooV/d
程度のものが得られた。
By forming the film in this way, the InSb thin film 3 with a thickness of about 1 μm has a sufficiently large grain size in the film plane direction (lateral direction), and the mobility at room temperature is aoooooV/d.
I got something of a certain degree.

これに対して、第1図(kl)に示すBaF2よりなる
材料層2を形成せず、基板1上にInSb薄膜3を前述
したと同様の条件にて成膜したものでは、グレインサイ
ズは、高々膜厚程度のオーダーに過ぎず、InSb薄膜
3の厚さ1μm程度で、室温における移動度は、高々、
100oOv/c−程度に過ぎなかった。
On the other hand, in the case where the InSb thin film 3 is formed on the substrate 1 under the same conditions as described above without forming the material layer 2 made of BaF2 shown in FIG. 1(kl), the grain size is At most, the mobility at room temperature is only on the order of the film thickness, and the thickness of the InSb thin film 3 is about 1 μm.
It was only about 100oOv/c-.

これら、BaF2よりなる材料層2の有無に依る移動度
の相異は、結局、InSb薄膜3の格子定数(o、e+
snm  )と、BaF 2層2の格子定数(0,62
nm)は、比較的接近しており、また、InSbは立方
晶ZnS  形、BaF2は蛍石形で、結晶構造が似通
っている点、加えて、Ba72層2の配向面に沿って、
InSb薄膜3が成長し、即ち、Ba72層2がInS
b薄膜3の核形成材としての役割りを果しているのに対
し、BIL72層2がない場合は、均質核生成が行われ
にくく、InSb薄膜3を構成する粒子の成長方向がラ
ンダムになり、従って、グレインサイズが高々膜厚方向
オーダーの多結晶膜となり、移動度は、グレインバウン
ダリーでの散乱を受け、これに依る規制を受ける。また
、本実施例に示す様にCGW#7059ガラス(線膨張
係数4.6X10  (K  ))基板1は、InSb
薄膜3の線膨張係数(5,04X10 ’(K ’))
より小さく、InSb薄膜3へ、引張り応力が入る。
These differences in mobility depending on the presence or absence of the material layer 2 made of BaF2 are ultimately due to the lattice constants (o, e+
snm ) and the lattice constant of BaF 2 layer 2 (0,62
nm) are relatively close to each other, and InSb has a cubic ZnS type and BaF2 has a fluorite type, and their crystal structures are similar.In addition, along the orientation plane of the Ba72 layer 2,
An InSb thin film 3 is grown, that is, the Ba72 layer 2 is InS
In contrast, in the absence of the BIL72 layer 2, homogeneous nucleation is difficult to occur, and the growth direction of the particles constituting the InSb thin film 3 becomes random. , the grain size becomes a polycrystalline film whose grain size is at most on the order of the film thickness direction, and the mobility is subject to scattering at the grain boundary and is regulated thereby. Further, as shown in this example, the CGW#7059 glass (linear expansion coefficient 4.6X10 (K)) substrate 1 is made of InSb
Linear expansion coefficient of thin film 3 (5,04X10'(K'))
The tensile stress is smaller and enters the InSb thin film 3.

衆知の通り、移動度は、引張り応力時の方が、良好な結
果が得られる。こうした点で、基板1として、他に、石
英基板(5,4X10  (K  ))。
As is well known, better mobility results can be obtained under tensile stress. In this respect, the substrate 1 may also be a quartz substrate (5.4×10 (K)).

CGW#7740(3,25X10   (K   )
)。
CGW#7740 (3,25X10 (K)
).

CGW$79oo(a×1o  (K  ))等を用い
ても、移動度の大きいInSb薄膜3を得ることができ
る。まだ、本実施例における基板1BaF2層2、In
5b薄膜3の各々の眉間における密着性は、いずれも良
好であり、−60〜+160°C間の温度サイクルを繰
り返しても、剥離は生じなかった。
The InSb thin film 3 with high mobility can be obtained even by using CGW$79oo (a×1o (K )) or the like. Still, in this example, the substrate 1 BaF2 layer 2, In
The adhesion between the eyebrows of each of the 5b thin films 3 was good, and no peeling occurred even after repeated temperature cycles between -60 and +160°C.

(実施例2) 本実施例では、基板として、(111)Siウェハーを
用いるものとする。第2図(a)に示す様に、(111
)Siウェハー4を洗浄し、その上に、同図(b)に示
す様に酸化膜5in2tsを、熱酸化法に依り形成し、
この後、真空蒸着装置内に導入し、実施例1と同様の作
成条件に依り、アルカリ土類金属弗化物、特にBaF2
でなる材料層6、InSb薄膜7を順次積層形成しても
、実施例1と同様、移動度が大きく、層間の密着性が良
好ガものを得ることができる。一方、(111)S1ウ
エハー4上に、酸化膜5in25を形成せずに、直接ア
ルカリ土類金属弗化物6を、直接、(111)Siウェ
ハー4上に形成し、その上に、InSb薄膜7を形成す
ることも可能である。この場合に留意を要するのは、ア
ルカリ土類金属弗化物6を形成する際の真空度(I X
1o8Torr  以下)と、形成前(111)Si基
板の清浄化処理および、アルカリ土類金属弗化物6の選
択である。(111)Siウェハー4上に直接、アルカ
リ土類金属弗化物6を形成する際は、格子定数として、
CaF 2が、0.548 nm 、 SrF2が、0
.580 nm 、 BaF2が0.620 nm 、
 Siが0.543 nm 、 InSbが、0.64
8 nmの関係よ抄、アルカリ土類金属弗化物6の形成
初期には、(111)Siウェハー4に格子定数の近い
CaF2を形成し、次いで、徐々に(ljaF2にSr
F 2を混ぜた混晶組成をSrF2!Jッチにし、次い
で徐々にSrF2にBaF 2を混ぜた混晶組成を、B
ILF2!Jッチにし、最終的にIn8b薄膜7と接す
る界面は、BaF 2にすることで、(111)面に配
向した、InSbエピタキシャル成長膜を得ることも可
能である。この場合も、各層間の密着性は、良好である
(Example 2) In this example, a (111) Si wafer is used as the substrate. As shown in Figure 2(a), (111
) The Si wafer 4 was cleaned, and an oxide film of 5 in 2 ts was formed thereon by a thermal oxidation method as shown in FIG.
Thereafter, the alkaline earth metal fluoride, especially BaF2
Even if the material layer 6 and the InSb thin film 7 are sequentially laminated, it is possible to obtain a material with high mobility and good interlayer adhesion, as in Example 1. On the other hand, an alkaline earth metal fluoride 6 is directly formed on the (111) Si wafer 4 without forming an oxide film 5 in 25 on the (111) S1 wafer 4, and an InSb thin film 7 is formed thereon. It is also possible to form In this case, it is important to pay attention to the degree of vacuum (I
108 Torr or less), cleaning treatment of the (111) Si substrate before formation, and selection of alkaline earth metal fluoride 6. When forming the alkaline earth metal fluoride 6 directly on the (111) Si wafer 4, the lattice constant is
CaF2 is 0.548 nm, SrF2 is 0
.. 580 nm, BaF2 is 0.620 nm,
Si is 0.543 nm, InSb is 0.64 nm
8 nm relationship, at the initial stage of formation of the alkaline earth metal fluoride 6, CaF2 with a similar lattice constant was formed on the (111) Si wafer 4, and then Sr was gradually added to the (ljaF2).
The mixed crystal composition mixed with F2 is SrF2! Then, gradually change the mixed crystal composition of SrF2 and BaF2 to
ILF2! It is also possible to obtain an InSb epitaxially grown film oriented in the (111) plane by making a J-touch and making BaF 2 the interface that finally contacts the In8b thin film 7. Also in this case, the adhesion between each layer is good.

以上述べた実施例1.2では、高移動度半導体材料薄膜
として、InSbを用いたが、この他に、InAs (
格子定数o、soanm)、 InGaSb  (格子
定数InSb : o、e 48 nm 〜Garb 
: o、61onm)もCaF2. SrF2. Ba
F2  でなる適当な混晶を用い、格子定数を合わせて
、成膜すれば、良好な結晶性が得られ、従って移動度が
大きく、また、層間密着性も良好なものが得られる。
In Example 1.2 described above, InSb was used as the high mobility semiconductor material thin film, but InAs (
Lattice constant o, soanm), InGaSb (Lattice constant InSb: o, e 48 nm ~Garb
: o, 61 onm) is also CaF2. SrF2. Ba
By forming a film using a suitable mixed crystal of F2 and matching the lattice constant, a film with good crystallinity, high mobility, and good interlayer adhesion can be obtained.

また、第3図に示す様に実施例1.2のいずれの方法に
依って形成されたInSb薄膜B上に、Cu/Tl二層
、Cu−層、Ag−層1人l−層等、電極9を形成し、
短絡電極10のパターン形成を行った後、素子間を分離
する為のフォトレジストパターン11を形成し、ウェッ
ト方式では、HF。
Further, as shown in FIG. 3, on the InSb thin film B formed by any method of Example 1.2, Cu/Tl double layer, Cu layer, Ag layer, single layer, etc. forming an electrode 9;
After patterning the shorting electrode 10, a photoresist pattern 11 for separating the elements is formed, and in the wet method, HF is used.

HNO3の混合液等、ドライ方式では、CF4と02の
混合ガス等で、InSb薄膜8をエツチング除去する。
In a dry method such as a mixed solution of HNO3, the InSb thin film 8 is etched away using a mixed gas of CF4 and 02.

この際、アルカリ土類金属弗化物12は、これらetc
hantには侵食されず、良好なエツチング防止材とな
る。この後、吸湿防止等の観点から5iON膜等のパッ
シベーション膜を施し、素子が完成する。こうして完成
した素子において、60〜+150°Cの温度サイクル
、耐湿試験等を繰り返したが、従来生じた様な素子劣化
は生じず、極めて高い信頼性を有することが、確認され
た。
At this time, the alkaline earth metal fluoride 12 is
It is not eroded by etching and becomes a good etching prevention material. Thereafter, a passivation film such as a 5iON film is applied to prevent moisture absorption, and the device is completed. The device thus completed was subjected to repeated temperature cycles of 60 to +150° C., moisture resistance tests, etc., but it was confirmed that the device did not suffer from the deterioration that occurred in the past, and had extremely high reliability.

発明の効果 以上述べてきた様に、本発明は、絶縁物もしくは、半導
体よりなる基板或いは、表面絶縁化基板上に、アルカリ
土類金属弗化物よりなる材料層を形成するし、この材料
層−ヒに、高移動度半導体材料薄膜を形成するものであ
るので、アルカリ土類金属弗化物の配向性を利用し、こ
れを核形成材として、高移動度半導体材料薄膜の結晶性
を改善し、移動度が向上すると共に、層間の密着性も良
好で、これに依り、従来生じていた様な、膜亀裂等に依
る特性劣化は生じず、−60〜+160°Cの温度範囲
で十分な信頼性を有する半導体薄膜磁気抵抗素子となる
Effects of the Invention As described above, in the present invention, a material layer made of an alkaline earth metal fluoride is formed on a substrate made of an insulator or a semiconductor, or a surface insulated substrate, and this material layer - First, since a thin film of high mobility semiconductor material is to be formed, the orientation of alkaline earth metal fluoride is utilized and this is used as a nucleation material to improve the crystallinity of the thin film of high mobility semiconductor material. In addition to improved mobility, the adhesion between layers is also good, and as a result, there is no characteristic deterioration due to film cracks, etc., which occurs in the past, and it is fully reliable in the temperature range of -60 to +160°C. This results in a semiconductor thin-film magnetoresistive element with properties.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図(&)〜(0)は、本発明の半導体薄膜磁気抵抗
素子の製造方法の基本例を示す断面図、第2図(a3〜
((13は、本発明の一実施例の断面図、第3図(&)
〜((ilは本発明の他の実施例の斜視図である。 1.4.13・・・・・・基&、2,6.12・・・・
・・アルカリ土類金属弗化物よりなる材料層、3,7.
8・・・・・高移動度半導体材料薄膜(InSb)。 代理人の氏名 弁理士 中 尾 敏 男 ほか1名第 図
FIGS. 1(&) to (0) are cross-sectional views showing a basic example of the method for manufacturing a semiconductor thin film magnetoresistive element of the present invention, and FIGS.
((13 is a sectional view of one embodiment of the present invention, FIG. 3(&)
~((il is a perspective view of another embodiment of the present invention. 1.4.13...Group &, 2,6.12...
... Material layer made of alkaline earth metal fluoride, 3, 7.
8... High mobility semiconductor material thin film (InSb). Name of agent: Patent attorney Toshio Nakao and one other person

Claims (6)

【特許請求の範囲】[Claims] (1)絶縁物もしくは、半導体よりなる基板、或いは、
表面絶縁化基板上に、アルカリ土類金属弗化物よりなる
材料層を形成し、この材料層上に、高移動度半導体材料
薄膜を形成した半導体薄膜磁気抵抗素子。
(1) A substrate made of an insulator or a semiconductor, or
A semiconductor thin film magnetoresistive element in which a material layer made of alkaline earth metal fluoride is formed on a surface-insulated substrate, and a high mobility semiconductor material thin film is formed on this material layer.
(2)アルカリ土類金属弗化物よりなる材料層が、Ba
F_2、SrF_2、CaF_2の中より選ばれたもの
(混晶を含む)よりなる材料層で、高移動度半導体材料
薄膜が、InSb、InAs、InGaSbのいずれか
よりなる薄膜である特許請求の範囲第1項に記載の半導
体薄膜磁気抵抗素子。
(2) The material layer made of alkaline earth metal fluoride is Ba
A material layer made of a material selected from F_2, SrF_2, and CaF_2 (including a mixed crystal), and the high mobility semiconductor material thin film is a thin film made of InSb, InAs, or InGaSb. The semiconductor thin film magnetoresistive element according to item 1.
(3)アルカリ土類金属弗化物よりなる材料層が、Ba
F_2、SrF_2、CaF_2の中より選ばれたもの
(混晶を含む)よりなる材料層で、高移動度半導体材料
薄膜が、InSbよりなる薄膜である特許請求の範囲第
1項に記載の半導体薄膜磁気抵抗素子。
(3) The material layer made of alkaline earth metal fluoride is Ba
The semiconductor thin film according to claim 1, wherein the high mobility semiconductor material thin film is a thin film made of InSb, which is a material layer made of a material selected from F_2, SrF_2, and CaF_2 (including mixed crystal). Magnetoresistive element.
(4)絶縁物もしくは、半導体よりなる基板、或いは、
表面絶縁化基板上に、アルカリ土類金属弗化物よりなる
材料層を形成する工程と、この材料層上に、高移動度半
導体材料薄膜を形成する工程を有する半導体薄膜磁気抵
抗素子の製造方法。
(4) A substrate made of an insulator or a semiconductor, or
A method for manufacturing a semiconductor thin film magnetoresistive element, comprising the steps of forming a material layer made of an alkaline earth metal fluoride on a surface-insulated substrate, and forming a high mobility semiconductor material thin film on this material layer.
(5)アルカリ土類金属弗化物よりなる材料層が、Ba
F_2、SrF_2、CaF_2の中より選ばれたもの
(混晶を含む)よりなる材料層で、高移動度半導体材料
薄膜が、InSb、InAs、InGaSbのいずれか
よりなる薄膜である特許請求の範囲第4項に記載の半導
体薄膜磁気抵抗素子の製造方法。
(5) The material layer made of alkaline earth metal fluoride is Ba
A material layer made of a material selected from F_2, SrF_2, and CaF_2 (including a mixed crystal), and the high mobility semiconductor material thin film is a thin film made of InSb, InAs, or InGaSb. 4. A method for manufacturing a semiconductor thin film magnetoresistive element according to item 4.
(6)アルカリ土類金属弗化物よりなる材料層が、Ba
F_2、SrF_2、CaF_2の中より選ばれたもの
(混晶を含む)よりなる材料層で、該高移動度半導体材
料薄膜が、InSbよりなる薄膜である特許請求の範囲
第4項に記載の半導体薄膜磁気抵抗素子の製造方法。
(6) The material layer made of alkaline earth metal fluoride is Ba
The semiconductor according to claim 4, wherein the high mobility semiconductor material thin film is a thin film of InSb, in which the material layer is made of a material selected from among F_2, SrF_2, and CaF_2 (including mixed crystal). A method for manufacturing a thin film magnetoresistive element.
JP63161718A 1988-06-29 1988-06-29 Semiconductor thin film magnetoresistance element and manufacture thereof Pending JPH0210882A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63161718A JPH0210882A (en) 1988-06-29 1988-06-29 Semiconductor thin film magnetoresistance element and manufacture thereof

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63161718A JPH0210882A (en) 1988-06-29 1988-06-29 Semiconductor thin film magnetoresistance element and manufacture thereof

Publications (1)

Publication Number Publication Date
JPH0210882A true JPH0210882A (en) 1990-01-16

Family

ID=15740561

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63161718A Pending JPH0210882A (en) 1988-06-29 1988-06-29 Semiconductor thin film magnetoresistance element and manufacture thereof

Country Status (1)

Country Link
JP (1) JPH0210882A (en)

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57196546A (en) * 1981-05-27 1982-12-02 Hiroshi Ishihara Material for electronic element having multilayer structure of semiconductor and insulator
JPS58166781A (en) * 1982-03-26 1983-10-01 Pioneer Electronic Corp Magnetoelectricity converting element
JPS595620A (en) * 1982-07-02 1984-01-12 Asahi Chem Ind Co Ltd Manufacture of indium-gallium-antimony compound thin film
JPS6299456A (en) * 1985-10-25 1987-05-08 Hitachi Ltd Method for forming metal fluoride thin film

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57196546A (en) * 1981-05-27 1982-12-02 Hiroshi Ishihara Material for electronic element having multilayer structure of semiconductor and insulator
JPS58166781A (en) * 1982-03-26 1983-10-01 Pioneer Electronic Corp Magnetoelectricity converting element
JPS595620A (en) * 1982-07-02 1984-01-12 Asahi Chem Ind Co Ltd Manufacture of indium-gallium-antimony compound thin film
JPS6299456A (en) * 1985-10-25 1987-05-08 Hitachi Ltd Method for forming metal fluoride thin film

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