JP2539584B2 - Superconducting quantum interference device - Google Patents

Superconducting quantum interference device

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Publication number
JP2539584B2
JP2539584B2 JP5244258A JP24425893A JP2539584B2 JP 2539584 B2 JP2539584 B2 JP 2539584B2 JP 5244258 A JP5244258 A JP 5244258A JP 24425893 A JP24425893 A JP 24425893A JP 2539584 B2 JP2539584 B2 JP 2539584B2
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Japan
Prior art keywords
layer
superconducting
normal
film
thin film
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JP5244258A
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JPH07106645A (en
Inventor
塚本  晃
良信 樽谷
正一 赤松
一重 今川
宇紀 樺沢
徳海 深沢
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Hitachi Ltd
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Hitachi Ltd
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Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、酸化物超電導体を用い
たジョセフソン接合を含む超電導エレクトロニクス素子
の分野に係り、特に液体窒素温度(77K)以上で動作
可能な超電導量子干渉素子に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to the field of superconducting electronic devices including Josephson junctions using oxide superconductors, and more particularly to a superconducting quantum interference device capable of operating above liquid nitrogen temperature (77K).

【0002】[0002]

【従来の技術】Agを常伝導層としたSNS接合で構成
された従来の素子は、ネイチャー.354巻(1991
年)513頁から515頁(Nature,vol.3
54(1991)pp513−515)に記載されてい
る。上記構造を図1に示す。上記従来技術は、あらかじ
め表面に段差を形成した基板に、左斜め上方から酸化物
超電導体を堆積させることで、堆積した酸化物超電導層
(S層)に数百nmの隙間を形成し、空間的に分離され
た2つの超電導電極を形成する。上記超電導電極を形成
した装置より資料を外に取り出さずに、上記2つの超電
導電極間に右斜め上方から常伝導金属3(N層)として
Agを蒸着することでSNS接合を形成している。ま
た、IEEE トランザクション オン マグネティク
ス.27巻(1991年)3098頁から3101頁
(IEEE TRANSACTIONON MAGNE
TICS,vol.27(1991)pp3098−3
101)でForresterらが図2に示すようなS
NS接合の構造を報告している。上記構造は、酸化物超
電導薄膜上にAu膜5を形成し、微細加工で2つの超電
導電極を形成し、それらをAu膜6でつないだ構造であ
る。
2. Description of the Related Art A conventional element composed of an SNS junction using Ag as a normal conductive layer is a nature. Volume 354 (1991)
Pp. 513-515 (Nature, vol. 3)
54 (1991) pp 513-515). The above structure is shown in FIG. In the above-mentioned conventional technique, by depositing an oxide superconductor from a diagonally upper left direction on a substrate having a step formed on the surface in advance, a gap of several hundred nm is formed in the deposited oxide superconducting layer (S layer), and a space is formed. Form two superconducting electrodes that are electrically separated. The SNS junction is formed by evaporating Ag as normal conductive metal 3 (N layer) from the diagonally right upper side between the two superconducting electrodes without taking out the material from the device in which the superconducting electrode is formed. In addition, IEEE Transaction on Magnetics. Volume 27 (1991) pp. 3098-3101 (IEEE TRANSACTION MAGNE
TICS, vol. 27 (1991) pp3098-3
101) Forrester et al.
The structure of the NS junction is reported. The above structure is a structure in which the Au film 5 is formed on the oxide superconducting thin film, two superconducting electrodes are formed by microfabrication, and they are connected by the Au film 6.

【0003】[0003]

【発明が解決しようとする課題】上記従来技術では、基
板上に形成した段差に沿って素子を配置する必要がある
ため、素子の集積化が困難である、との問題があった。
また、素子の接合部を流れる超電導電流(Ic)や接合
抵抗(Rn)を電極間距離や常伝導層の膜厚などで制御
するためには、常伝導金属自体の抵抗よりも十分に低い
接触抵抗が必要である。しかし、上記従来技術のSNS
接合では、接合抵抗が常伝導体であるAu自体の抵抗よ
りも約2桁大きく、接合抵抗が接触抵抗に支配されてい
る、との問題があった。
The above-mentioned prior art has a problem that it is difficult to integrate the elements because it is necessary to arrange the elements along the steps formed on the substrate.
Further, in order to control the superconducting current (Ic) and the junction resistance (Rn) flowing through the junction of the device by the distance between the electrodes and the film thickness of the normal conductive layer, the contact is sufficiently lower than the resistance of the normal conductive metal itself. I need resistance. However, the above-mentioned conventional SNS
In the joining, there is a problem that the joining resistance is about two orders of magnitude higher than the resistance of Au itself which is a normal conductor, and the joining resistance is dominated by the contact resistance.

【0004】本願発明の目的は、液体窒素温度以上の高
温で動作可能であり、接合特性の安定性、再現性にすぐ
れ、特性の設計と制御および素子の集積化が可能なジョ
セフソン接合、およびそれらを有する超電導量子干渉素
子(SQUID)を提供することを目的とする。
An object of the present invention is a Josephson junction which can be operated at a temperature higher than the liquid nitrogen temperature, has excellent stability and reproducibility of the junction characteristics, and can be designed and controlled for the characteristics and the integration of elements, and It is an object to provide a superconducting quantum interference device (SQUID) having them.

【0005】[0005]

【課題を解決するための手段】上記目的を解決するため
に本願発明は、図3に示すようなプレーナー型のSNS
接合を形成する。上記構造は、酸化物超電導体層、金属
または合金からなる第1の常伝導金属層、および化学的
に安定な金属からなる保護膜層で構成された3層膜を同
一平面上に空間的に分離させ、2つの電極を形成し、そ
の上に一部重なるようにして金属または合金からなる第
2の常伝導金属層を作製することで超電導電極を常伝導
金属でつなぐ、ことによって形成されている。第1の常
伝導金属層と第2の常伝導金属層が異なる材料であって
もかまわない。
In order to solve the above-mentioned object, the present invention is a planar type SNS as shown in FIG.
Form a bond. In the above structure, a three-layer film composed of an oxide superconductor layer, a first normal metal layer made of a metal or an alloy, and a protective film layer made of a chemically stable metal is spatially arranged on the same plane. It is formed by connecting two superconducting electrodes with a normal conducting metal by separating them, forming two electrodes, and forming a second normal conducting metal layer made of a metal or an alloy so as to partially overlap them. There is. The first normal conductive metal layer and the second normal conductive metal layer may be different materials.

【0006】[0006]

【作用】本願発明で用いているAu、Ptなど化学的に
安定な保護膜層9は、微細加工プロセスでの保護膜とし
て作用し、また、第1の常伝導金属層8が微細加工プロ
セスにおいて、変質してしまう事を防止する。従って、
酸化物超電導体と低い接触抵抗で接続できる材料を第1
の常伝導金属層8に用いることができる。
The chemically stable protective film layer 9 such as Au and Pt used in the present invention acts as a protective film in the microfabrication process, and the first normal metal layer 8 is used in the microfabrication process. , Prevent it from changing. Therefore,
First material that can be connected to oxide superconductors with low contact resistance
Can be used for the normal conductive metal layer 8.

【0007】また、空間的に分離した2つの超電導電極
間の距離を一定にする、第2の常伝導金属層の幅を超電
導電極の幅より狭くすることにより、超電導電流を超電
導電極間に均一に流すことができる。これにより、素子
の特性、再現性が向上し、素子の設計、作製が容易にな
る。
Further, by making the width of the second normal-conducting metal layer narrower than the width of the superconducting conductive electrode so that the distance between the two spatially separated superconducting conductive electrodes is constant, the superconducting current can be made uniform between the superconducting conductive electrodes. Can be flushed to. As a result, the characteristics and reproducibility of the element are improved, and the element can be easily designed and manufactured.

【0008】[0008]

【実施例】〔実施例1〕以下、本発明の実施例を示し、
さらに本発明を説明する。
EXAMPLES [Example 1] Examples of the present invention will be shown below.
The present invention will be further described.

【0009】作製プロセスを図4を参照しつつ説明す
る。基板11としてSrTiO3(100)単結晶を用
い、この上にHoBa2Cu3Ox(以下HBCOと略
す)酸化物超電導薄膜12を形成する。成膜は酸素プラ
ズマ中に置いた基板上にHo、Ba、Cuの金属を蒸着
し、基板上で酸素プラズマ中の活性な酸素と金属を反応
させて酸化物薄膜を成長させる反応性蒸着法で行い、成
膜温度は650℃、成膜速度は1.2nm/min、膜
厚は50から200nmとする。また、酸素プラズマと
して圧力0.01Paの純酸素ガスに875gauss
の磁場中で2.45GHzのマイクロ波を照射して放電
させたECR(電子サイクロトロン共鳴)プラズマを用
い、マイクロ波電力は120Wとする。成膜後、酸素プ
ラズマ中、10℃/minの速度で250℃まで冷却す
る。酸素プラズマを止めて、0.0001Pa以下の真
空度まで真空槽を排気し、基板温度250℃で第1の常
伝導金属であるAg薄膜13を超電導薄膜の上に蒸着す
る。上記Ag薄膜の形成は、超電導薄膜を形成した資料
を形成装置より外部に取り出さずに続けて行う。この
際、メタルマスクを用い、試料の中心部にのみAg薄膜
を作製し、Ag膜の膜厚は10から50nmとする。さ
らに、同様にして保護膜であるAu薄膜14をその上に
蒸着する。Au膜の膜厚は50から100nmとする。
資料を外部に取り出さずに、酸化物超電導体上にAgを
蒸着することで常伝導金属/超電導体の界面が後の工程
で汚染されることを防ぐことができる。また、Agの上
に化学的に安定なAuを蒸着する事で後の微細加工プロ
セスでAgが酸化するなどの変質を防ぐことができる。
作製したHBCO薄膜はc軸配向しており、基板面に垂
直にHBCOのc軸が配向した。薄膜のTcは85〜9
0K、Jcは77K、0磁場で約106A/cm2であ
る。次に、試料を成膜装置から取り出し、電子線描画用
レジスト15を300nm塗布し、電子線描画法でパタ
ーンを作製する。この時点での断面構造図を図4(a)に
示す。図4(a)の構造を0.01PaのArガスを用
いたECRプラズマエッチング法を用いてエッチングを
行う。エッチング後の状態を図4(b)に示す。エッチン
グ後、レジスト15はすべて酸素プラズマを照射して除
去する(図4(c))。次に、再び電子線描画用のレジス
ト15を再び塗布し、電子線描画法で第2の常伝導金属
層16を作製するためのリフトオフパターンを作製する
(図4(d))。リフトオフパターン作製後、接合部周辺
に第2の常伝導金属層16であるAu膜を蒸着し(図4
(e))、膜厚は200nmとする。アセトンを用いたリ
フトオフ法を用い余分なAu膜を除去し、接合に必要な
部分のみを残す(図4(f))。完成した接合は図3に示
した構造である。接合部分の酸化物超電導薄膜および第
1の常伝導金属層の横幅(W1)は10μm、電極間距
離(L)は0.2μm、第2の常伝導金属層の横幅(W
2)は5μmである。
The fabrication process will be described with reference to FIG. A SrTiO 3 (100) single crystal is used as the substrate 11, and a HoBa 2 Cu 3 Ox (hereinafter abbreviated as HBCO) oxide superconducting thin film 12 is formed thereon. The film formation is a reactive deposition method in which Ho, Ba, and Cu metals are deposited on a substrate placed in oxygen plasma, and active oxygen in the oxygen plasma reacts with the metal to grow an oxide thin film on the substrate. The film formation temperature is 650 ° C., the film formation rate is 1.2 nm / min, and the film thickness is 50 to 200 nm. Also, as oxygen plasma, pure oxygen gas having a pressure of 0.01 Pa is applied with 875 gauss
ECR (electron cyclotron resonance) plasma discharged by irradiating the microwave of 2.45 GHz in the magnetic field is used, and the microwave power is 120 W. After the film formation, the film is cooled to 250 ° C. in oxygen plasma at a rate of 10 ° C./min. The oxygen plasma is stopped, the vacuum chamber is evacuated to a vacuum degree of 0.0001 Pa or less, and the Ag thin film 13, which is the first normal conductive metal, is vapor-deposited on the superconducting thin film at a substrate temperature of 250 ° C. The formation of the Ag thin film is continuously performed without taking out the material on which the superconducting thin film is formed from the forming apparatus. At this time, using a metal mask, an Ag thin film is formed only in the central portion of the sample, and the thickness of the Ag film is set to 10 to 50 nm. Further, similarly, an Au thin film 14 as a protective film is vapor-deposited thereon. The film thickness of the Au film is 50 to 100 nm.
By depositing Ag on the oxide superconductor without taking out the material to the outside, it is possible to prevent the normal metal / superconductor interface from being contaminated in a later step. Further, by chemically depositing Au which is chemically stable on Ag, it is possible to prevent alteration such as oxidation of Ag in the subsequent fine processing process.
The produced HBCO thin film was c-axis oriented, and the c-axis of HBCO was oriented perpendicular to the substrate surface. Tc of thin film is 85-9
0K and Jc are 77K and about 10 6 A / cm 2 at 0 magnetic field. Next, the sample is taken out from the film forming apparatus, an electron beam drawing resist 15 is applied to 300 nm, and a pattern is formed by an electron beam drawing method. A cross-sectional structure diagram at this point is shown in FIG. The structure of FIG. 4A is etched using the ECR plasma etching method using 0.01 Pa of Ar gas. The state after etching is shown in FIG. After the etching, the resist 15 is entirely removed by irradiation with oxygen plasma (FIG. 4 (c)). Next, a resist 15 for electron beam writing is applied again, and a lift-off pattern for producing the second normal conductive metal layer 16 is produced by the electron beam writing method (FIG. 4 (d)). After forming the lift-off pattern, an Au film, which is the second normal-conducting metal layer 16, is vapor-deposited around the junction (see FIG. 4).
(e)), and the film thickness is 200 nm. Excessive Au film is removed by a lift-off method using acetone, leaving only a portion necessary for bonding (FIG. 4 (f)). The completed joint has the structure shown in FIG. The lateral width (W1) of the oxide superconducting thin film and the first normal-conducting metal layer at the joint portion is 10 μm, the interelectrode distance (L) is 0.2 μm, and the lateral width (W) of the second normal-conducting metal layer (W).
2) is 5 μm.

【0010】この様にして作製したSNS接合の電流−
電圧特性(77K)を図5に示す。Icは170μAで
ある。また、10GHzのマイクロ波を照射した時のI
−V特性は、シャピロステップが10ステップ以上まで
明瞭に観測することができる。さらに、外部磁場を加え
ることで、ジョセフソン接合に特有なフラウンホーファ
ーパターンも観察でき、均一な接合を持つジョセフソン
接合を作製できる。また、20%Agを含むAuを第2
の常伝導金属層16として同じ構造のSNS接合を作製
した所、Icが約1/3に減少した。よって、常伝導金属
層を合金化することで接合の特性を制御できることが確
認できた。また、基板にSrTiO3(110)を用い
た場合でも、上記のプロセスを用いてジョセフソン接合
を作製することができる。
The current of the SNS junction manufactured in this way-
The voltage characteristic (77K) is shown in FIG. Ic is 170 μA. In addition, I when irradiated with a microwave of 10 GHz
The -V characteristic can be clearly observed up to 10 or more Shapiro steps. Furthermore, by applying an external magnetic field, the Fraunhofer pattern peculiar to the Josephson junction can also be observed, and the Josephson junction having a uniform junction can be manufactured. In addition, the second Au containing 20% Ag is used.
When an SNS junction having the same structure as that of the normal conductive metal layer 16 was prepared, Ic was reduced to about 1/3. Therefore, it was confirmed that the joining characteristics can be controlled by alloying the normal conductive metal layer. Further, even when SrTiO 3 (110) is used for the substrate, the Josephson junction can be manufactured using the above process.

【0011】次に、この様にして作製したSNS接合を
用いてdcSQUIDを作製する。上に述べたSNS接
合作製プロセスと同じ条件で、図6に示すように10m
m×10mmのSrTiO3(100)基板上に保護
膜層/常伝導金属層/酸化物超電導層の3層膜を作製し
た後、電子線描画法とドライエッチング法で3層膜を正
方形のワッシャーリングの形状に加工する。その後、上
に述べたSNS接合作製プロセスと同じ条件で、ワッシ
ャーリングの3層膜を2か所で基板1まで到達する溝で
分断し、分断された三層膜の上面を接続する常伝導金属
層を設けてSNS接合18を形成し、dcSQUIDを
作製する。ワッシャーリング17の外径、内径はそれぞ
れ300μm、100μmとし、接合幅は10μm、接
合距離は0.2μmとする。
Next, a dcSQUID is produced using the SNS junction produced in this way. Under the same conditions as the SNS junction manufacturing process described above, as shown in FIG.
After forming a three-layer film of protective film layer / normal conductive metal layer / oxide superconducting layer on a SrTiO 3 (100) substrate 1 of m × 10 mm, the three-layer film was formed into a square film by electron beam drawing and dry etching. Process into a washer ring shape. Then, under the same conditions as SNS junction fabrication processes mentioned above, Wasshi
In the groove that reaches the substrate 1 in two places,
Normal metal that divides and connects the upper surface of the divided three-layer film
And a layer forming the SNS junction 18 to produce a d cSQUID. The outer diameter and the inner diameter of the washer ring 17 are 300 μm and 100 μm, respectively, and the joining width is 10 μm and the joining distance is 0.2 μm.

【0012】図7に、作製したSQUIDの出力電圧−
磁場特性を示す。100Hz以上では実用可能な特性を
得ることができる。また、上記工程で0.5×0.5m
2の面積に、接合幅10μm、電極間距離0.2μm
のSNS接合を100個直列に並べる。これらの特性を
調べたところ、全ての接合がジョセフソン特性を示して
いることが確認出来た。このように、本発明の素子構造
では、素子の集積化が容易である。なお、本実施例にお
いて、酸化物超電導薄膜12はHBCO薄膜に限らず、
YBa2Cu30xやBi系、Tl系など他の高温超電導
体薄膜を使用できることは勿論であり、常伝導金属につ
いてもAu−Ag合金以外にAu,Ag,Pt,Rh,
Re,Ir,Ruおよびこれらを含む合金を使用でき
る.第1の常伝導金属層と第2の常伝導金属層で材料が
異なっていてもかまわない。また、基板1に関しても、
良好な特性を有する超電導薄膜が形成可能であれば、M
gOやNdGaO3など他の材料も使用でき、また、面
方位についても(100)面以外でもかまわない。
FIG. 7 shows the output voltage of the produced SQUID--
The magnetic field characteristics are shown. Practical characteristics can be obtained at 100 Hz or higher. Also, in the above process, 0.5 × 0.5 m
an area of m 2, bonding width 10 [mu] m, the inter-electrode distance 0.2μm
100 SNS junctions are arranged in series. When these characteristics were examined, it was confirmed that all the junctions exhibited Josephson characteristics. Thus, the device structure of the present invention facilitates device integration. In this embodiment, the oxide superconducting thin film 12 is not limited to the HBCO thin film,
Of course, other high-temperature superconductor thin films such as YBa 2 Cu 3 0x, Bi-based, Tl-based, etc. can be used, and as for the normal conductive metal, Au, Ag, Pt, Rh,
Re, Ir, Ru and alloys containing them can be used. The first normal conductive metal layer and the second normal conductive metal layer may be made of different materials. Also regarding the substrate 1,
If a superconducting thin film with good characteristics can be formed, M
Other materials such as gO and NdGaO 3 can also be used, and the plane orientation may be other than the (100) plane.

【0013】〔実施例2〕次に、本発明の実施例2を図
8を用いて説明する。
[Second Embodiment] Next, a second embodiment of the present invention will be described with reference to FIG.

【0014】NdGaO3(100)単結晶基板上に
マルチターゲットのレーザーアブレーション法で膜厚2
00nmのYBa2Cu3Ox(YBCO)超電導薄膜、
膜厚300nmのSrTiO3薄膜を順次作製する。作
製条件はYBCO、SrTiO 3 ともに以下の条件とす
るターゲットはYBa2Cu3Ox焼結体およびSrTi
3単結晶を用いる。波長248nmのKrFエキシマ
レーザーを周波数5Hz、エネルギー密度1.1J/c
2で用いる。基板温度は700℃、成膜時の酸素分圧
は100mTorrとする。このYBCO薄膜はグラン
ドプレーン21として使用し、SrTiO3薄膜はグラ
ンドプレーン21とワッシャーリング17間の層間絶縁
20aとして使用する。このようにして作製したSr
TiO3/YBCOの2層膜上に、実施例1で示した方
法で保護膜層/常伝導金属層/酸化物超電導層の3層膜
23を作製し、電子線描画法による微細加工を行いワッ
シャーリング17とSNS接合18(保護膜層22上面
間を第2の常伝導金属層10で接続してなる)を形成
し、dcSQUIDを作製する。グランドプレーン21
を作製することで、ワッシャーリング17の中心を通過
した磁束が必ずグランドプレーン21とワッシャーリン
17の間のSrTiO3薄膜部分を通るため、均一に
dcSQUIDに磁場が加わる。この結果、SQUID
の感度と安定性が向上し、また設計が容易になる。さら
に、このワッシャーリング上にインプットコイル19を
作製するため、膜厚200nmのSrTiO3層間絶縁膜20
を作製し、その上に膜厚100nmのHBCO薄膜を作製
する。このHBCO薄膜を電子線描画法とECRプラズ
マエッチングで線幅10μmのコイルに加工する。この
際、接合部分の上は結晶性が低下するため、SNS接合
18を避けるようにHBCO薄膜を加工してインプット
コイル19を形成する。さらに、このうえに膜厚100nm
のSrTiO3層間絶縁膜20c、膜厚100nmのHBCO
膜を作製し、これらを同様にして加工し、インプットコ
イルの中心から端子24を取り出した。図にインプッ
トコイルを備えたSQUID素子の平面図と断面図をし
めす。インプットコイル19を作製しても、SQUID
素子の特性は特に劣化しない。また、インプットコイル
19とSQUID素子は磁気的に結合している。なお、
本実施例において、酸化物超電導薄膜とグランドプレー
ンはYBCO薄膜やHBCO薄膜に限らず、他の高温超
電導体薄膜を使用できることは勿論である。また、基板
に関しても、良好な特性を有する超電導薄膜が形成可能
であれば、MgOやNdGaO3など他の材料でも使用
でき、また、面方位についても、(100)面以外でも
かまわない。本実施例では層間絶縁膜としてSrTiO
3を用いたが,酸化物超電導体と格子の整合性が良く,
超伝導体と反応しにくい材料であれば、NdGaO3
LaAlO3、YAlO3、MgO、Y23、PrBa2
Cu3Oxなど他の材料を用いても、上記実施例と同じ
効果を得ることができる。
A film thickness of 2 is formed on the NdGaO 3 (100) single crystal substrate 1 by a multi-target laser ablation method.
00 nm YBa 2 Cu 3 Ox (YBCO) superconducting thin film,
SrTiO 3 thin films having a film thickness of 300 nm are sequentially manufactured. The manufacturing conditions are as follows for both YBCO and SrTiO 3. The targets are YBa 2 Cu 3 Ox sintered body and SrTi.
O 3 single crystal is used. A KrF excimer laser with a wavelength of 248 nm is used at a frequency of 5 Hz and an energy density of 1.1 J / c.
Used at m 2 . The substrate temperature is 700 ° C., and the oxygen partial pressure during film formation is 100 mTorr. This YBCO thin film is used as the ground plane 21, and the SrTiO 3 thin film is used as the interlayer insulating film 20a between the ground plane 21 and the washer ring 17. Sr produced in this way
On the two-layer film of TiO 3 / YBCO, the three- layer film of protective film layer / normal conductive metal layer / oxide superconducting layer by the method shown in Example 1.
23 is formed, and fine processing is performed by an electron beam drawing method, and the washer ring 17 and the SNS junction 18 (the upper surface of the protective film layer 22).
The second normal metal layer 10 is connected between the two) to form a dcSQUID. Ground plane 21
By producing the magnetic field, the magnetic flux that has passed through the center of the washer ring 17 always passes through the SrTiO 3 thin film portion between the ground plane 21 and the washer ring 17 , so that a magnetic field is uniformly applied to the dcSQUID. As a result, SQUID
Improves sensitivity and stability, and simplifies design. Further, in order to form the input coil 19 on this washer ring, the SrTiO 3 interlayer insulating film 20 with a film thickness of 200 nm is formed.
b is formed, and an HBCO thin film having a film thickness of 100 nm is formed thereon. This HBCO thin film is processed into a coil having a line width of 10 μm by electron beam drawing and ECR plasma etching. At this time, since the crystallinity is lowered on the joint portion, the HBCO thin film is processed so as to avoid the SNS junction 18 to form the input coil 19. Furthermore, a film thickness of 100 nm
SrTiO 3 interlayer insulating film 20c , HBCO with a film thickness of 100 nm
A film was prepared and processed in the same manner, and the terminal 24 was taken out from the center of the input coil. FIG. 8 shows a plan view and a cross-sectional view of the SQUID element having the input coil. Even if the input coil 19 is manufactured, the SQUID
The characteristics of the element are not particularly deteriorated. The input coil 19 and the SQUID element are magnetically coupled. In addition,
In this embodiment, the oxide superconducting thin film and the ground plane are not limited to the YBCO thin film and the HBCO thin film, and needless to say, other high temperature superconductor thin films can be used. Regarding the substrate, other materials such as MgO and NdGaO 3 can be used as long as a superconducting thin film having good characteristics can be formed, and the plane orientation may be other than the (100) plane. In this embodiment, SrTiO 3 is used as the interlayer insulating film.
3 was used, but the compatibility between the oxide superconductor and the lattice was good,
If the material does not easily react with the superconductor, NdGaO 3 ,
LaAlO 3 , YAlO 3 , MgO, Y 2 O 3 , PrBa 2
Even if another material such as Cu 3 Ox is used, the same effect as in the above embodiment can be obtained.

【0015】[0015]

【発明の効果】本発明により、以下の効果が得られる。According to the present invention, the following effects can be obtained.

【0016】Au/常伝導金属/超電導体の3層膜をあ
らかじめ作製し、Auを常伝導金属の保護膜に用いるこ
とで反応しやすい常伝導金属を用いた接合を作製でき
る。さらに、常伝導層にAu、Ag、Pt、Rh、R
e、Ir、Ruおよびこれらを含む合金を用いること
で、常伝導層の抵抗(Rn)を変えることができ、これ
により、接合特性を電極間距離や常伝導金属そのものの
抵抗値で制御、設計できる。その結果、SNS接合の特
性、SQUIDの特性を設計、最適化でき、SQUID
素子を集積化できた。
By forming a three-layered film of Au / normal conductive metal / superconductor in advance and using Au as a protective film for the normal conductive metal, it is possible to manufacture a bond using a normal conductive metal which is easy to react. Furthermore, Au, Ag, Pt, Rh, R are added to the normal conductive layer.
By using e, Ir, Ru, and alloys containing these, the resistance (Rn) of the normal conductive layer can be changed, whereby the bonding characteristics can be controlled and designed by the distance between the electrodes or the resistance value of the normal conductive metal itself. it can. As a result, the characteristics of the SNS junction and the characteristics of the SQUID can be designed and optimized.
The device could be integrated.

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

【図1】基板上に作製した段差を用いたSNS接合の断
面構造図である。
FIG. 1 is a cross-sectional structure diagram of an SNS junction using a step formed on a substrate.

【図2】従来技術で作製されたプレーナー形SNS接合
の断面構造図である。
FIG. 2 is a cross-sectional structural diagram of a planar type SNS junction manufactured by a conventional technique.

【図3】本発明のプレーナー形SNS接合の構造図であ
る。
FIG. 3 is a structural diagram of a planar SNS junction of the present invention.

【図4】本発明のプレーナー形SNS接合の作製プロセ
ス表わしている。
FIG. 4 illustrates a fabrication process for a planar SNS junction of the present invention.

【図5】作製したプレーナー形SNS接合の電流−電圧
特性である。
FIG. 5 is a current-voltage characteristic of the manufactured planar SNS junction.

【図6】本発明のプレーナー形SNS接合を用いたdc
SQUIDの平面図である。
FIG. 6 dc using the planar SNS junction of the present invention
It is a top view of SQUID.

【図7】作製したdcSQUIDの出力電圧−磁場特性
(77K)である。
FIG. 7 is an output voltage-magnetic field characteristic (77K) of the produced dcSQUID.

【図8】インプットコイルを備えたdcSQUIDの
(a)平面図と(b)断面図である。
FIG. 8: dcSQUID with input coil
(a) A plan view and (b) a cross-sectional view.

【符号の説明】[Explanation of symbols]

1・・・基板、2・・・超電導電極、3・・・常伝導金
属、4・・・段差、5・・・Au膜、6・・・Au膜、
7・・・酸化物超電導体層、8・・・第1の常伝導金属
層、9・・・保護膜層、10・・・第2の常伝導金属
層、11・・・基板、12・・・酸化物超電導薄膜、1
3・・・Ag薄膜、14・・・Au薄膜、15・・・レ
ジスト、16・・・第2の常伝導金属層、17・・・ワ
ッシャーリング、18・・・SNS接合、19・・・イ
ンプットコイル、20・・・層間絶縁膜、21・・・グ
ランドプレーン。
1 ... Substrate, 2 ... Superconducting electrode, 3 ... Normal conductive metal, 4 ... Step, 5 ... Au film, 6 ... Au film,
7 ... Oxide superconductor layer, 8 ... 1st normal conductive metal layer, 9 ... Protective film layer, 10 ... 2nd normal conductive metal layer, 11 ... Substrate, 12 ... ..Oxide superconducting thin films, 1
3 ... Ag thin film, 14 ... Au thin film, 15 ... Resist, 16 ... Second normal conductive metal layer, 17 ... Washer ring, 18 ... SNS junction, 19 ... Input coil, 20 ... Interlayer insulating film, 21 ... Ground plane.

───────────────────────────────────────────────────── フロントページの続き (72)発明者 今川 一重 東京都国分寺市東恋ケ窪1丁目280番地 株式会社日立製作所中央研究所内 (72)発明者 樺沢 宇紀 東京都国分寺市東恋ケ窪1丁目280番地 株式会社日立製作所中央研究所内 (72)発明者 深沢 徳海 東京都国分寺市東恋ケ窪1丁目280番地 株式会社日立製作所中央研究所内 (56)参考文献 特開 平2−298085(JP,A) 特開 平2−46781(JP,A) 特開 平5−55646(JP,A) ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Ippei Imagawa 1-280 Higashi Koikeku, Kokubunji, Tokyo Inside the Central Research Laboratory, Hitachi, Ltd. (72) Inventor, Uki, 1-280 Higashi Koikeku, Kokubunji, Tokyo Hitachi, Ltd. Central Research Laboratory (72) Inventor Tokumi Fukasawa 1-280 Higashi Koigokubo, Kokubunji City, Tokyo Central Research Laboratory, Hitachi, Ltd. (56) Reference JP-A-2-298085 (JP, A) JP-A-2-46781 ( JP, A) JP-A-5-55646 (JP, A)

Claims (3)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 基板上に酸化物超電導体層と第1の常伝導
金属層と常伝導金属からなる保護膜層とをこの順に積層
させた第1及び第2の三層膜を相互に対向し且つ離間し
て形成し、上記第1及び第2の三層膜を夫々の保護膜層
の上面に接続された第2の常伝導金属膜でつないで形成
された超電導−常伝導−超電導接合部を有し、上記保護
膜層の常伝導金属はAu又はPtからなり、上記第1の
常伝導金属層は該保護膜層より低い接触抵抗で上記酸化
物超電導体層と接続できる材料からなることを特徴とす
る超電導量子干渉素子。
1. A facing the first and second three-layered film in which an oxide on a substrate superconductor layer and the first normal metal layer and the protective layer made of normal metal are laminated in this order to each other Superconducting-normal conducting-superconducting junction formed by connecting the first and second three-layer films with a second normal conducting metal film connected to the upper surface of each protective film layer. Part, and the normal conductive metal of the protective film layer is made of Au or Pt, and the first normal conductive metal layer is made of a material that can be connected to the oxide superconductor layer with lower contact resistance than the protective film layer. A superconducting quantum interference device characterized in that
【請求項2】 上記第1の常伝導金属層は、Ag又はAg
を含む合金であることを特徴とする請求項1記載の超電
導量子干渉素子。
2. The first normal metal layer is Ag or Ag.
The superconducting quantum interference device according to claim 1, wherein the superconducting quantum interference device is an alloy containing.
【請求項3】 上記超電導−常伝導−超電導接合部が超電
導ループに2つ形成されていることを特徴とする請求項
1記載の超電導量子干渉素子。
3. The superconducting quantum interference device according to claim 1, wherein two superconducting-normal-conducting-superconducting junctions are formed in a superconducting loop.
JP5244258A 1993-09-30 1993-09-30 Superconducting quantum interference device Expired - Fee Related JP2539584B2 (en)

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JP2539584B2 true JP2539584B2 (en) 1996-10-02

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CN115835768B (en) * 2023-02-10 2023-05-30 材料科学姑苏实验室 Protective layer for preparing superconducting quantum chip and superconducting quantum chip

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