JPH0483383A - Manufacture of thin film superconducting element - Google Patents

Manufacture of thin film superconducting element

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Publication number
JPH0483383A
JPH0483383A JP2197297A JP19729790A JPH0483383A JP H0483383 A JPH0483383 A JP H0483383A JP 2197297 A JP2197297 A JP 2197297A JP 19729790 A JP19729790 A JP 19729790A JP H0483383 A JPH0483383 A JP H0483383A
Authority
JP
Japan
Prior art keywords
thin film
oxide superconducting
superconducting thin
barrier layer
oxide
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
JP2197297A
Other languages
Japanese (ja)
Inventor
Shigemi Furubiki
古曳 重美
Koichi Mizuno
紘一 水野
Kentaro Setsune
瀬恒 謙太郎
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
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Filing date
Publication date
Application filed by Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP2197297A priority Critical patent/JPH0483383A/en
Publication of JPH0483383A publication Critical patent/JPH0483383A/en
Pending legal-status Critical Current

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  • Crystals, And After-Treatments Of Crystals (AREA)
  • Superconductor Devices And Manufacturing Methods Thereof (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は超伝導応用技術に使用される薄膜超伝導素子の
製造方法に関す4 従来の技術 近If−,La−Sr−Cu−OP、  Y−Ba−C
u−0’if、  B1−3r−Ca−Cu−0系TI
B a−3r−Cu−0系など常伝導状態における電荷
輸送担体が空孔のp型酸化物超伝導材料と、電子を常伝
導状態における電荷輸送担体とするNd−Ce−Cu−
0L  Nd−Cu−OxF系などNd2Cu○4型結
晶構造のn型酸化物超伝導材料が発見され九 これらの
材料の超伝導機構の詳細は明らかではない力(量子干渉
素子など各種エレクトロニクス分野への応用が期待され
ている。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to a method of manufacturing a thin film superconducting element used in superconducting application technology. Ba-C
u-0'if, B1-3r-Ca-Cu-0 system TI
B A p-type oxide superconducting material such as the a-3r-Cu-0 system in which the charge transport carrier in the normal conduction state is a hole, and a Nd-Ce-Cu- material in which the charge transport carrier in the normal conduction state is an electron.
0L N-type oxide superconducting materials with a Nd2Cu○4 type crystal structure such as the Nd-Cu-OxF system have been discovered.9 The details of the superconducting mechanism of these materials are not clear. Applications are expected.

この中には その超伝導遷移温度(Tc)が液体窒素温
度(77,3ケルビン)を越えるものもあり、超伝導体
の応用分野を大きく広げることとなった その実用化の
一つである超伝導素子について、酸化物超伝導体を二つ
に割り、再びわずかに接触させたジョセフソン素子、酸
化物超伝導体を薄膜にし 小さなくびれをつけたブリッ
ジ型ジョセフソン素子、酸化物超伝導体間をAu、Ag
などの貴金属で接続したジョセフソン素子が従来試作さ
れてき連 発明が解決しようとする課題 しかしながら従来試作されてきた素子のう板ポイントコ
ンタクト型と呼ばれる酸化物超伝導薄膜どうしを接触さ
せるタイプでは再現性が得られ哄 また特性が非常に不
安定であっμ さらに酸化物超伝導薄膜にくびれをつけ
たり、貴金属で接続したブリッジ型素子ではわずかな静
電的ショックで破損するという欠点があった そこで酸化物超伝導薄膜を用いた接合型の構造を持つ超
伝導素子が望まれている力丈 酸化物超伝導薄膜の成膜
温度が約600℃以上必要なため上部に形成にする酸化
物超伝導薄膜の成膜時にバリア層成分が拡散したり、酸
化物超伝導薄膜に用いた材料とバリア層の材料の熱膨張
係数が違うため室温に戻したときに薄膜にストレスが入
り、上部に形成した酸化物超伝導薄膜の超伝導性が著し
く損なわれム バリア層にピンホールが存在するなどの
問題があった さらに 酸化物超伝導薄膜とバリア層の
結晶構造の違いによる格子定数のミスマツチによって上
部に形成した酸化物超伝導薄膜の結晶性が悪く、その超
伝導性が基板上の酸化物超伝導薄膜に比べて劣るという
問題点があったすなわ板 従来の酸化物超伝導薄膜の形
成過程で得られる薄膜の結晶性やそれに取り込まれる酸
素の量の制御は良好な超伝導特性を得るには必ずしも十
分ではなく、最良の超伝導特性を持たせるには 結晶性
の更なる向上と十分な酸素の離脱のための処理を施す必
要があった 本発明はこのような上記の課題を解決するもので、結晶
性の良いp型またはn型の薄膜超伝導素子の製造方法の
提供を目的とすも 課題を解決するための手段 上記の課題を解決するために本発明の薄膜超伝導素子の
製造方法法 基板上に酸化物超伝導薄膜バリア層および
酸化物超伝導薄膜をこの順序で形成して三層の薄膜積層
体とし 薄膜堆積中または薄膜堆積後にX線を照射し 
薄膜のC軸を基板に対して垂直に配向させ、酸化物薄膜
がp型の場合にはひき続き酸化処理を施し薄膜超伝導素
子とし薄膜がn型の場合にはそのまま薄膜超伝導素子と
すム ここて p型の薄膜超伝導素子における酸化物超
伝導薄膜およびバリア層はBi、アルカリ土類金属およ
びCuを主成分とする酸化物力\ BiyPbyアルカ
リ土類金属およびCuを主成分とする酸化物であム ま
た n型の薄膜超伝導素子における酸化物超伝導薄膜の
主成分はF−G−Cu−Xで表わされ バリア層の主成
分はH−Cu−0で表わされる。ここ’+’=  Fは
ネオジウム(Nd)、サマリウム(Sm)、プルトニウ
ム(Pr)のうちの一種以上の元iGはセリウム(Ce
)、 トリウム(Th)のうちの一種以上の元魚Xは酸
素(O)または弗素(F)のうちの一種以上の元素であ
ム 作用 本発明は上記の構成により、 p型酸化物を用いた薄膜
超伝導素子の製造において1よ 薄膜堆積中または薄膜
堆積後にX線を照射することにより結晶中の陰イオンで
ある酸素イオンなどを結晶中から離脱させたり、ポテン
シャルエネルギーの開放により陽イオンを再配列させて
、 C軸配向の薄膜を成長させLp型型化化物場合には
X線照射後酸化処理を施すと結晶性が向上する。
Some of these superconducting transition temperatures (Tc) exceed the liquid nitrogen temperature (77.3 Kelvin), greatly expanding the field of application of superconductors. Concerning conduction elements, there is a Josephson device in which an oxide superconductor is split in half and they are brought into slight contact again, a bridge-type Josephson device in which the oxide superconductor is made into a thin film and a small constriction is formed, and an oxide superconductor interlayer. Au, Ag
Previously, Josephson devices connected with precious metals such as In addition, the characteristics were very unstable.Furthermore, bridge-type devices connected by constricting the oxide superconducting thin film or connected with precious metals had the disadvantage of being damaged by a slight electrostatic shock. A superconducting element with a junction type structure using a superconducting thin film is desired.Since the deposition temperature of the oxide superconducting thin film must be approximately 600°C or higher, the temperature of the oxide superconducting thin film formed on the top is The barrier layer components may diffuse during film formation, or the thermal expansion coefficients of the material used for the oxide superconducting thin film and the material for the barrier layer may be different, which may cause stress to the thin film when it is returned to room temperature, causing the oxide formed on the top to There were problems such as the superconductivity of the superconducting thin film being significantly impaired and the presence of pinholes in the barrier layer.Furthermore, there were problems such as the presence of pinholes in the barrier layer.Furthermore, there were problems such as the presence of pinholes in the barrier layer.Furthermore, pinholes formed on the top due to the mismatch in lattice constant due to the difference in the crystal structure of the oxide superconducting thin film and the barrier layer. The problem is that the crystallinity of the oxide superconducting thin film is poor, and its superconductivity is inferior to that of the oxide superconducting thin film on the substrate. Controlling the crystallinity of a thin film and the amount of oxygen taken into it is not necessarily sufficient to obtain good superconducting properties, and in order to obtain the best superconducting properties, it is necessary to further improve crystallinity and release sufficient oxygen. The present invention solves the above-mentioned problems, and aims to provide a method for manufacturing a p-type or n-type thin film superconducting element with good crystallinity. Means for Solving the Problems In order to solve the above problems, a method for manufacturing a thin film superconducting element according to the present invention. An oxide superconducting thin film barrier layer and an oxide superconducting thin film are formed in this order on a substrate to form three layers. A thin film stack is formed, and X-rays are irradiated during or after thin film deposition.
The C-axis of the thin film is oriented perpendicular to the substrate, and if the oxide thin film is p-type, it is subsequently subjected to oxidation treatment to become a thin-film superconducting element, and if the thin film is n-type, it is directly used as a thin-film superconducting element. The oxide superconducting thin film and barrier layer in a p-type thin film superconducting element are oxides containing Bi, alkaline earth metals, and Cu as main components. In addition, the main component of the oxide superconducting thin film in an n-type thin film superconducting element is represented by F-G-Cu-X, and the main component of the barrier layer is represented by H-Cu-0. Here, '+' = F is one or more elements of neodymium (Nd), samarium (Sm), and plutonium (Pr); iG is cerium (Ce);
), one or more elements of thorium (Th) are one or more elements of oxygen (O) or fluorine (F). In the production of thin film superconducting devices, 1. By irradiating X-rays during or after thin film deposition, oxygen ions, which are anions in the crystal, can be removed from the crystal, and cations can be released by releasing potential energy. Crystallinity is improved by rearranging, growing a thin film with C-axis orientation, and performing an oxidation treatment after X-ray irradiation in the case of an Lp-type compound.

実施例 以下、本発明の実施例を図面と共に説明すも実施例1 本発明の薄膜超伝導体の製造に1よ 例えば 第1図に
示すような薄膜形成槽1内!ミ 薄膜堆積のための蒸着
源2、結晶性向上と還元処理のための装置3とマイクロ
波電源で駆動する酸化処理装置12を備えたものを使用
すム 第1図の例では蒸着源2としては 高周波電源で
駆動する高周波マグネトロンスパッタ装置を、結晶性向
上と還元処理のための装置としては高圧電源で駆動する
RhX線管球を用いてい4 本実施例では四元酸化物薄
膜4を基板5上にスパッタリング法で形成した第2図は
本発明の実施例を示す工程図である。
EXAMPLES Hereinafter, examples of the present invention will be described with reference to the drawings. Example 1 To manufacture the thin film superconductor of the present invention, for example, inside a thin film forming tank 1 as shown in FIG. M. Use a vapor deposition source 2 for thin film deposition, a device 3 for improving crystallinity and reduction treatment, and an oxidation treatment device 12 driven by a microwave power source. In this example, a high-frequency magnetron sputtering device driven by a high-frequency power source is used, and a Rh X-ray tube driven by a high-voltage power source is used as the device for crystallinity improvement and reduction treatment. FIG. 2, which was formed by sputtering on the top, is a process diagram showing an embodiment of the present invention.

MgO単結晶を基板5に用1.z  X線照射を行ない
つxRFマグネトロンスパッタリング法によって、結晶
相が主として2212相で、化学式が(B i 5−I
IP bII) 2−8 rs−Cat−Cua−Ox
 (但し0≦y< 0.5)の厚さ300 nmの酸化
物超伝導薄膜Aを6として薄膜を形成し九 ひき続き同一薄膜形成槽】内において結晶相が主として
2201相で、化学式がBiz−Sr2−Ca2  O
X%  のバリア層7を厚さ3nm堆積させ[第2図工
程(a)]、その上に酸化物超伝導薄膜Bを8として形
成した この薄膜は結晶相が主として2212相で、化学式が (B i +−−P bv) e−Sr2−Cat−C
a2−Ox(但し0≦y< 0.5)の厚さ200 n
mである[第2図工程(b)]。
Using MgO single crystal as the substrate 51. z X-ray irradiation and xRF magnetron sputtering method revealed that the crystal phase was mainly 2212 phase and the chemical formula was (B i 5-I
IP bII) 2-8 rs-Cat-Cua-Ox
(however, 0≦y<0.5), a 300 nm thick oxide superconducting thin film A was formed as 6, and in the same thin film formation tank for 9 consecutive times, the crystal phase was mainly 2201 phase, and the chemical formula was Biz. -Sr2-Ca2O
A barrier layer 7 of 3 nm thick is deposited with a thickness of 3 nm [step (a) in Figure 2], and an oxide superconducting thin film B is formed thereon as 8. The crystal phase of this thin film is mainly 2212, and the chemical formula is ( B i +--P bv) e-Sr2-Cat-C
Thickness of a2-Ox (0≦y<0.5) 200 n
m [Fig. 2, step (b)].

以上三層の薄膜はいずれも基板温度500tで形成し九 その抵 ネガレジスト9を用いたフォトリソグラフィー
およびイオンミリングによりバリア層7および酸化物超
伝導薄膜Bをトンネル接合形状にパターニングしたU第
211ilJ工程(C)]。
The above three thin films were all formed at a substrate temperature of 500 t, and the barrier layer 7 and the oxide superconducting thin film B were patterned into a tunnel junction shape by photolithography using a resistor resist 9 and ion milling. (C)].

その徽 ネガレジスト9を除去せずく 電極間分離層1
0として250nmのCaFsを真空蒸着により堆積後
[第2図工程(d)〕、 トリクロロエタンによる超音
波洗浄および第1図に示す酸化処理装置(E CR酸素
(O)ガスプラズマ装置)12  (ITorr、  
13. 56MHz、400W>によるリフトオフ法で
酸化物超伝導薄膜Bの表面を露出させた[第2図工程(
e)]。
The result is that without removing the negative resist 9, the inter-electrode separation layer 1
After depositing 250 nm of CaFs as 0 by vacuum evaporation [Step (d) in Figure 2], ultrasonic cleaning with trichloroethane and oxidation treatment equipment (ECR oxygen (O) gas plasma equipment) 12 (ITorr,
13. The surface of the oxide superconducting thin film B was exposed by a lift-off method using 56 MHz, 400 W [Step in Figure 2 (
e)].

最後へ メタルマスクを用い酸化物超伝導薄膜Bの一部
に接触させコンタクト電極11として200nmの白金
(Pt)をRFマグネトロンスパッタリング法により堆
積させ薄膜超伝導素子14を完成させた[第2図工程(
f)]。
To the end Platinum (Pt) with a thickness of 200 nm was deposited by RF magnetron sputtering method as a contact electrode 11 in contact with a part of the oxide superconducting thin film B using a metal mask to complete the thin film superconducting element 14 [Steps in Figure 2] (
f)].

この製造方法による薄膜超伝導素子14は液体窒素温度
において良好な超伝導トンネル特性およびジョセフソン
効果を示すことを確認し九第3図は本薄膜超伝導素子の
三層膜のX線回折パターン図である。これによると、 
500℃の成膜温度において各層はC軸配向を示してお
り、RHEED観察などよりエピタキシャル成長してい
ることが確認された この薄膜超伝導素子の特性は15
0マイクロアンペアの超伝導電流が流れ(直流ジョセフ
ソン効果)、またヒステリシスを持つ動作をした −古
本実施例に用いたものと同様な三層膜に対し700℃以
下の酸素中でのアニル処理をしても結晶性を保ったまま
であり、かつA、  B両酸化物超伝導薄膜の超伝導性
が向上二この三層膜を用いた接合型の超伝導素子の特性
の向上ができることを確認した X線照射による結晶性
向上と還元処理は 成膜後では常温の温度で一定時間行
うことによって効率的かつ簡便に行えも この効果ζよ 結晶性向上並びに還元処理を薄膜堆積を
中断して行う、すなわ杖 薄膜堆積工程と結晶性向上並
びに還元処理とを成膜温度において交互に繰り返す場合
にも見られることを本発明者らは確認した これらの結
晶性向上並びに還元処理を施すべき温度&よ 薄膜の粗
砥 表面状態によっても異なるた八 各場合について最
適なものを選ぶ必要がある力丈 本発明者らは900℃
以下500℃以上の温度範囲にあることを確認したな抵
 処理時間についてL 薄膜の粗砥 膜尾表面状態に応
じて必要最小限の値が存在すム結晶性向上並びに還元処
理を施すという点からだけで(よ この処理を薄膜堆積
と同時に行うのが最も望ましい力(薄膜堆積過程の種類
によって(表処理温度が堆積基板温度に限定されるため
に十分な効果が得られない場合もあることが確認された
本発明者ら&よ むしろ結晶性向上並びに還元処理を薄
膜堆積を中断して行う、すなわち薄膜堆積工程と結晶性
向上並びに還元処理を交互に繰り返しながら行なった場
合の方に同等もしくはそれ以上の効果が得られることを
確認し九 ごれら薄膜堆積過程においては 堆積直後の各構成元素
は励起状態にあり、場合によっては 安定化するのに数
分のオーダーの時間を要するものも多(、特に積層構造
をとるものについて4i  1周期構造分堆積させる毎
に堆積を中断して安定化が図られている場合もあa この様な堆積中断時間に結晶性向上並びに還元処理を施
せば 短時間で理想的な結晶性向上並びに還元処理を施
せると考えられも 本発明者らは 適当な堆積時間毎に中断し 結晶性向上
並びに還元処理を施すことによって、優れた特性を有す
る超電導薄膜を得ることが出来ることを確認した 更に その堆積時間間隔として、その間に堆積される被
膜の厚みが10Å以上100Å以下とするものが有効で
あることを確認した 本発明者ら41  結晶性向上処理と酸化処理を薄膜堆
積と同時に行う場合、あるいは 薄膜堆積を中断して打
う、すなわ板 薄膜堆積工程と結晶性向上処理と酸化処
理行程とを交互に繰り返す場合に用いる酸化処理の方法
としてζよ 少なくとも酸素を含むガスの放電により生
成される酸素イオンにより処理す4 あるいは励起状態
にある中性酸素原子を照射することが効果的かつ簡便で
あることを発見し九 例えは 第1図に示す酸化処理装置12を用t、に薄膜
形成槽1に連結されたプラズマ生成室13内に酸素ガス
あるいは酸素を含む混合ガスを導入しこのガスにマイク
ロ波を照射して放電プラズマを発生させ、これにマグネ
ット15によって磁場を印加し イオン化の確率を上げ
ることにより高エネルギーの酸素イオンおよび中性酸素
原子がp型超伝導薄膜を効率的に酸化することを見いだ
したなかでL 酸化物超伝導薄膜Aおよび酸化物超伝導
薄膜Bが主として(B i +−,P tz) 2−8
 r2Ca+−Cu2−Ox(但しO≦y< 0.5)
なる2212結晶相、 バリア層が主としてBlp−S
ra−Cu+−0つなる2201結晶相である薄膜超伝
導素子および酸化物超伝導薄膜Aおよび酸化物超伝導薄
膜Bが主として(B i +−,P b M) 2− 
S r 2−Ca2−Cus−OX (但しO≦y<0
.5)なる2223結晶相、 バリア層が主として(B
 i +−,P bν)2−Srs−Cae  Cus
  OXなる2201結晶相である薄膜超伝導素子は優
れた超伝導特性を示しへ実施例2 次に本発明の他の実施例を図面と共に説明する。
It was confirmed that the thin film superconducting device 14 produced by this manufacturing method exhibits good superconducting tunneling properties and the Josephson effect at liquid nitrogen temperatures. Figure 3 is an X-ray diffraction pattern diagram of the three-layer film of this thin film superconducting device. It is. according to this,
At a film formation temperature of 500°C, each layer showed C-axis orientation, and RHEED observation confirmed epitaxial growth.The characteristics of this thin film superconducting element are 15
A superconducting current of 0 microampere flowed (DC Josephson effect), and the operation had hysteresis. -An annealing treatment in oxygen at a temperature below 700°C was applied to a three-layer film similar to that used in the old book example. It was confirmed that the superconductivity of both A and B oxide superconducting thin films was improved, and the properties of junction-type superconducting devices using these three-layer films could be improved. Crystallinity improvement and reduction treatment by X-ray irradiation can be efficiently and easily carried out by performing the film at room temperature for a certain period of time after film formation. In other words, the present inventors confirmed that this phenomenon also occurs when the thin film deposition process, crystallinity improvement, and reduction treatment are alternately repeated at the film formation temperature. Rough polishing of a thin film varies depending on the surface condition, and the strength must be selected optimally for each case.
It has been confirmed that the temperature range is 500℃ or higher.Regarding treatment time L Rough polishing of thin film There is a minimum value required depending on the surface condition of the film.From the point of view of improving crystallinity and performing reduction treatment. However, it is most desirable to perform this treatment simultaneously with thin film deposition (depending on the type of thin film deposition process, sufficient effects may not be obtained because the surface treatment temperature is limited to the deposition substrate temperature). The present inventors and others have confirmed that the results are equivalent to or similar to the case where the crystallinity improvement and reduction treatment are performed by interrupting the thin film deposition, that is, the thin film deposition process, the crystallinity improvement and reduction treatment are alternately repeated. We have confirmed that the above effects can be obtained.In the thin film deposition process, each constituent element is in an excited state immediately after deposition, and in some cases it often takes several minutes to stabilize. (Especially for those with a laminated structure, there are cases where stabilization is achieved by interrupting the deposition every time one periodic structure is deposited. If the crystallinity is improved and the reduction treatment is performed during such a deposition interruption time, Although it is thought that ideal crystallinity improvement and reduction treatment can be performed in a short period of time, the present inventors succeeded in creating a superconducting thin film with excellent properties by interrupting the deposition at appropriate intervals and performing crystallinity improvement and reduction treatment. Furthermore, the present inventors confirmed that it is effective to set the thickness of the film deposited between 10 Å and 100 Å during the deposition time interval.41 Crystallinity Improvement Treatment and Oxidation The oxidation treatment method used when the treatment is performed simultaneously with thin film deposition, or when the thin film deposition is interrupted, that is, when the thin film deposition process, crystallinity improvement treatment, and oxidation treatment process are repeated alternately, is ζ. We discovered that it is effective and simple to treat with oxygen ions generated by the discharge of oxygen-containing gas, or to irradiate neutral oxygen atoms in an excited state. When using the apparatus 12, oxygen gas or a mixed gas containing oxygen is introduced into the plasma generation chamber 13 connected to the thin film forming tank 1, and this gas is irradiated with microwaves to generate discharge plasma, which is then attached to a magnet. 15 found that high-energy oxygen ions and neutral oxygen atoms efficiently oxidize p-type superconducting thin films by applying a magnetic field and increasing the probability of ionization. Superconducting thin film B is mainly (B i +-, P tz) 2-8
r2Ca+-Cu2-Ox (O≦y<0.5)
2212 crystal phase, the barrier layer is mainly Blp-S
The thin film superconducting element, oxide superconducting thin film A and oxide superconducting thin film B, which are 2201 crystal phases consisting of ra-Cu+-0, are mainly (B i +-, P b M) 2-
S r 2-Ca2-Cus-OX (O≦y<0
.. 5) 2223 crystal phase, the barrier layer is mainly (B
i +-, P bν)2-Srs-Cae Cus
A thin film superconducting element having a 2201 crystal phase called OX exhibits excellent superconducting properties.Example 2 Next, another example of the present invention will be described with reference to the drawings.

薄膜形成装置および基板は前記実施例と同じであム 薄膜堆積中にX線照射を行ないつzRFマグネトロンス
パッタリング法によってl’J d e−wCe xC
u 04(x=0.15)を主成分とする酸化物薄膜を
厚さ300 nm堆積させ九 ひき続き同一薄膜形成槽
I内においてN d e−tc e *C,u Oa 
(X=0)からなるバリア層7として厚さ3nm堆積さ
せた「第2図工程(a)]。
The thin film forming apparatus and substrate were the same as those in the previous example.
An oxide thin film containing u 04 (x=0.15) as a main component was deposited to a thickness of 300 nm.9 Subsequently, in the same thin film forming tank I, N de-tc e *C, u Oa
In step (a) of FIG. 2, a barrier layer 7 of (X=0) was deposited to a thickness of 3 nm.

次にN da−CeXCu 04 (X=0.15)の
酸化物超伝導薄HDを8として200 nm堆積させた
[第2図工程(b)コ。
Next, an oxide superconducting thin HD of N da-CeXCu 04 (X=0.15) was deposited to a thickness of 200 nm (step (b) in FIG. 2).

基板温度はいずれの場合も500℃である。The substrate temperature was 500° C. in both cases.

その後、ネガレジスト9を用いたフォトリソグラフィー
およびイオンミリングによりバリア層7および酸化物超
伝導薄膜りである8をトンネル接合形状に、パターニン
グした[第2図工程(C)]。
Thereafter, the barrier layer 7 and the oxide superconducting thin film 8 were patterned into a tunnel junction shape by photolithography using a negative resist 9 and ion milling [Step (C) in FIG. 2].

その抵 ネガレジスト9を除去せずく 電極間分離層1
0として250nmのCaFeを真空蒸着法により堆積
後[第2図工程(d)]、 トリクロロエタンによる超
音波洗朱 および第1図に示す酸化処理装置12  (
ITorr、 13.56MHz、400W)によるリ
フトオフ法で酸化物超伝導薄膜りである8を露出させた
【第2図工程(e)コ。
Interelectrode separation layer 1 without removing the resistor 9
After depositing 250 nm of CaFe as 0 by vacuum evaporation [step (d) in FIG. 2], ultrasonic cleaning with trichloroethane and oxidation treatment apparatus 12 (
The oxide superconducting thin film 8 was exposed by a lift-off method using ITorr, 13.56 MHz, 400 W (Step (e) in Figure 2).

最後く メタルマスクを用い酸化物超伝導薄膜りである
8の一部に接触させてコンタクト電極として200nm
のPtをRFマグネトロンスパッタリング法により堆積
させ超伝導素子14を完成させた[第2図工程(f)コ
Finally, use a metal mask to contact a part of 8, which is an oxide superconducting thin film, to form a contact electrode of 200 nm.
The superconducting element 14 was completed by depositing Pt by RF magnetron sputtering method [Step (f) in FIG. 2].

この製造方法による超伝導素子は液体窒素温度において
良好な超伝導トンネル特性およびジョセフソン効果を示
すことを確認しな 第4図は本実施例におけるの薄膜超伝導素子の三層膜の
X線回折パターン図であa これによると、 500℃の成膜温度において各層はC
軸配向を示しており、RHEED観察などによりエピタ
キシャル成長していることが確認され九 な抵 基板5として(友 結晶性の高い酸化物薄膜を堆
積させるためには単結晶の基板が有効であり、Mgへ 
LaAl0a  LaGaO3、チタン酸ストロンチウ
ムなどの単結晶を用いも またコンタクト電極としては
Ptを用いた力<、Au、Ag、Pd、Cuなどの金属
でもより℃発明の効果 以上のように 本発明の薄膜超伝導素子の製造方法によ
れば次の効果が得られも (イ)基板上にp型の薄膜超伝導素子を製造する場合に
(よ 薄膜堆積中または薄膜堆積後にX線を照射しその
後酸化処理を施し薄膜をC軸配向させ、結晶性を向上さ
せるので良好な超伝導特性をもつ薄膜超伝導素子が得ら
れる。
It was confirmed that the superconducting device produced by this manufacturing method shows good superconducting tunneling properties and Josephson effect at liquid nitrogen temperature. Pattern diagram a According to this, each layer has a C
It has been confirmed that epitaxial growth has occurred through RHEED observation, etc. As a resistive substrate 5, a single-crystal substrate is effective for depositing a highly crystalline oxide thin film, and Mg fart
Single crystals such as LaAl0a, LaGaO3, and strontium titanate may be used.Furthermore, metals such as Au, Ag, Pd, and Cu may be used as contact electrodes. The following effects can be obtained according to the method for manufacturing a conductive element: (a) When manufacturing a p-type thin film superconducting element on a substrate, Since the thin film is subjected to C-axis orientation and crystallinity is improved, a thin film superconducting element with good superconducting properties can be obtained.

(ロ)基板上にn型の薄膜超伝導素子を製造する場合に
は 薄膜堆積中または薄膜堆積後にX線を照射し薄膜を
C軸配向させ、結晶性を向上させるので良好な超伝導特
性をもつ薄膜超伝導素子が得られも (ハ)本発明の製造方法による薄膜超伝導素子は良好な
超伝導特性をもつので超伝導量子干渉計、計算機メモリ
ー 計算機ロジックなどに応用でき実用的効果が犬であ
(b) When manufacturing an n-type thin film superconducting device on a substrate, X-rays are irradiated during or after thin film deposition to orient the thin film along the C axis, improving crystallinity and ensuring good superconducting properties. (c) Since the thin film superconducting device produced by the manufacturing method of the present invention has good superconducting properties, it can be applied to superconducting quantum interferometers, computer memory, computer logic, etc., and has practical effects. Deam

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

第1図は本発明の薄膜超伝導体素子の製造方法を実施す
るために使用する製造装置の基本構成文第2図(a)〜
(f)は本発明による薄膜超伝導素子の製造方法の工程
医 第3図は本発明による薄膜超伝導素子の第一の実施
例の三層膜のX線回折パターンは 第4図は同じく第二
の実施例の三層膜のX線回折パターン図であも 4・・・酸化物薄11U5・・・基板 6、8・・・酸
化物超伝導薄ji、7・・・バリア凰 9・・・フォト
レジスト、10・・・電極間分離層 11・・・コンタ
クト電極 14・・・薄膜超伝導素り 代理人の氏名 弁理士 粟野重孝 はか1名亀
Figure 1 shows the basic configuration of the manufacturing equipment used to carry out the method for manufacturing thin film superconductor elements of the present invention.
(f) is a process diagram of the method for manufacturing a thin film superconducting device according to the present invention. This is an X-ray diffraction pattern diagram of the three-layer film of Example 2. 4... Oxide thin 11U5... Substrate 6, 8... Oxide superconducting thin ji, 7... Barrier film 9. ... Photoresist, 10 ... Inter-electrode separation layer 11 ... Contact electrode 14 ... Thin film superconducting material Name of agent Patent attorney Shigetaka Awano

Claims (7)

【特許請求の範囲】[Claims] (1)基板上に酸化物超伝導薄膜Aを形成し、その酸化
物超伝導薄膜Aの上にバリア層を形成し、そのバリア層
の上に酸化物超伝導薄膜Bを形成L前記酸化物超伝導薄
膜A、バリア層および酸化物超伝導薄膜BにX線を照射
しc軸配向させ、酸化処理を施し、その後前記酸化物超
伝導薄膜Bの上にフォトレジスト膜を形成し、パターニ
ングを施し、その上に前記バリア層より厚い電極間分離
層を形成し、リフトオフ法で酸化物超伝導薄膜Bを露出
させ、その露出させた酸化物超伝導薄膜Bの上にコンタ
クト電極を形成する薄膜超伝導素子の製造方法。 ここで、酸化物超伝導薄膜A、バリア層および酸化物超
伝導薄膜Bはビスマス(Bi)、アルカリ土類金属およ
び銅(Cu)を主成分とする酸化物またはBi、鉛(P
b)、アルカリ土類金属および銅(Cu)を主成分とす
る酸化物である。
(1) Form an oxide superconducting thin film A on a substrate, form a barrier layer on the oxide superconducting thin film A, and form an oxide superconducting thin film B on the barrier layer L. The superconducting thin film A, the barrier layer, and the oxide superconducting thin film B are irradiated with X-rays to align the c-axis and subjected to oxidation treatment, and then a photoresist film is formed on the oxide superconducting thin film B and patterned. forming an interelectrode separation layer thicker than the barrier layer thereon, exposing the oxide superconducting thin film B by a lift-off method, and forming a contact electrode on the exposed oxide superconducting thin film B. Method for manufacturing superconducting elements. Here, the oxide superconducting thin film A, the barrier layer, and the oxide superconducting thin film B are oxides containing bismuth (Bi), alkaline earth metals, and copper (Cu) as main components, or Bi, lead (Pb).
b) is an oxide whose main components are an alkaline earth metal and copper (Cu).
(2)酸化物超伝導薄膜Aおよび酸化物超伝導薄膜Bが
主として(Bi_1_−_yPb_y)_2−Sr_2
−Ca_1−Cu_2−O_x、0≦y<0.5なる2
212結晶相、バリア層が主としてBi_2−Sr_2
−Cu_1−O_xなる2201結晶相である請求項1
記載の薄膜超伝導素子の製造方法。
(2) Oxide superconducting thin film A and oxide superconducting thin film B are mainly (Bi_1_-_yPb_y)_2-Sr_2
-Ca_1-Cu_2-O_x, 2 where 0≦y<0.5
212 crystal phase, barrier layer is mainly Bi_2-Sr_2
-Cu_1-O_x 2201 crystal phase Claim 1
A method for manufacturing the thin film superconducting device described above.
(3)酸化物超伝導薄膜Aおよび酸化物超伝導薄膜Bが
主として(Bi_1_−_yPb_y)_2−Sr_2
−Ca_2−Cu_3−O_x、0≦y<0.5なる2
223結晶相、バリア層が主として(Bi_1_−_y
Pb_y)_2−Sr_2−Ca_2−Cu_3−O_
xなる2201結晶相である請求項1記載の薄膜超伝導
素子の製造方法。
(3) Oxide superconducting thin film A and oxide superconducting thin film B are mainly (Bi_1_-_yPb_y)_2-Sr_2
-Ca_2-Cu_3-O_x, 2 where 0≦y<0.5
223 crystal phase, the barrier layer is mainly (Bi_1_-_y
Pb_y)_2-Sr_2-Ca_2-Cu_3-O_
2. The method for manufacturing a thin film superconducting device according to claim 1, wherein the thin film superconducting device has a 2201 crystal phase of x.
(4)酸素イオンまたは励起状態にある準安定酸素原子
を照射して、X線照射後の薄膜を酸化処理する請求項1
記載の薄膜超伝導素子の製造方法。
(4) Claim 1, wherein the thin film after X-ray irradiation is oxidized by irradiating oxygen ions or metastable oxygen atoms in an excited state.
A method for manufacturing the thin film superconducting device described above.
(5)基板上に酸化物超伝導薄膜Cを形成し、その酸化
物超伝導薄膜Cの上にバリア層を形成し、そのバリア層
の上に酸化物超伝導薄膜Dを形成し、前記酸化物超伝導
薄膜C、バリア層および酸化物超伝導薄膜DにX線を照
射しc軸配向させ、、その後前記酸化物超伝導薄膜Dの
上にフォトレジスト膜を形成し、パターニングを施し、
その後、前記バリア層より厚い電極間分離層を形成し、
リフトオフ法で酸化物超伝導薄膜Dを露出させ、その露
出させた酸化物超伝導薄膜Dの上にコンタクト電極を形
成する薄膜超伝導素子の製造方法。 ここで、酸化物超伝導薄膜Cおよび酸化物超伝導薄膜D
は主としてF−G−Cu−Xで表わされ、バリア層は主
としてH−Cu−Oで表わされる。 ここに、Fはネオジウム(Nd)、サマリウム(Sm)
、プルトニウム(Pr)のうちの一種以上の元素、Gは
セリウム(Ce)、トリウム(Th)のうちの一種以上
の元素、Xは酸素(O)または弗素(F)のうちの一種
以上の元素である。
(5) Forming an oxide superconducting thin film C on a substrate, forming a barrier layer on the oxide superconducting thin film C, forming an oxide superconducting thin film D on the barrier layer, and forming the oxide superconducting thin film C on the substrate. The oxide superconducting thin film C, the barrier layer and the oxide superconducting thin film D are irradiated with X-rays to align the c-axis, and then a photoresist film is formed on the oxide superconducting thin film D and patterned,
After that, forming an interelectrode separation layer thicker than the barrier layer,
A method for manufacturing a thin film superconducting element, in which an oxide superconducting thin film D is exposed by a lift-off method, and a contact electrode is formed on the exposed oxide superconducting thin film D. Here, oxide superconducting thin film C and oxide superconducting thin film D
is mainly represented by FG-Cu-X, and the barrier layer is mainly represented by H-Cu-O. Here, F is neodymium (Nd), samarium (Sm)
, one or more elements of plutonium (Pr), G is one or more elements of cerium (Ce) or thorium (Th), X is one or more elements of oxygen (O) or fluorine (F) It is.
(6)酸化物超伝導薄膜C、バリア層および酸化物超伝
導薄膜DがNd_2_−_xCe_xCuO_4(x=
0−0.2)である請求項5記載の薄膜超伝導素子の製
造方法。
(6) The oxide superconducting thin film C, the barrier layer and the oxide superconducting thin film D are Nd_2_-_xCe_xCuO_4 (x=
6. The method for manufacturing a thin film superconducting element according to claim 5.
(7)酸化物超伝導薄膜とバリア層の形成工程中、薄膜
堆積とX線照射を交互に繰り返すことを特徴とする請求
項1または5記載の薄膜超伝導素子の製造方法。
(7) The method for manufacturing a thin film superconducting device according to claim 1 or 5, characterized in that during the step of forming the oxide superconducting thin film and the barrier layer, thin film deposition and X-ray irradiation are alternately repeated.
JP2197297A 1990-07-25 1990-07-25 Manufacture of thin film superconducting element Pending JPH0483383A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2197297A JPH0483383A (en) 1990-07-25 1990-07-25 Manufacture of thin film superconducting element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2197297A JPH0483383A (en) 1990-07-25 1990-07-25 Manufacture of thin film superconducting element

Publications (1)

Publication Number Publication Date
JPH0483383A true JPH0483383A (en) 1992-03-17

Family

ID=16372120

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2197297A Pending JPH0483383A (en) 1990-07-25 1990-07-25 Manufacture of thin film superconducting element

Country Status (1)

Country Link
JP (1) JPH0483383A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04111369A (en) * 1990-08-31 1992-04-13 Hitachi Ltd Method for producing multilayer films including superconductor films
JPH0715049A (en) * 1993-06-23 1995-01-17 Nec Corp Superconducting multilayered thin film

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04111369A (en) * 1990-08-31 1992-04-13 Hitachi Ltd Method for producing multilayer films including superconductor films
JPH0715049A (en) * 1993-06-23 1995-01-17 Nec Corp Superconducting multilayered thin film

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