JPS60182703A - Method of producing thin film resistor - Google Patents

Method of producing thin film resistor

Info

Publication number
JPS60182703A
JPS60182703A JP3932984A JP3932984A JPS60182703A JP S60182703 A JPS60182703 A JP S60182703A JP 3932984 A JP3932984 A JP 3932984A JP 3932984 A JP3932984 A JP 3932984A JP S60182703 A JPS60182703 A JP S60182703A
Authority
JP
Japan
Prior art keywords
thin film
gas
film resistor
producing thin
resistance
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
JP3932984A
Other languages
Japanese (ja)
Inventor
篤 中村
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.)
Rohm Co Ltd
Original Assignee
Rohm 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 Rohm Co Ltd filed Critical Rohm Co Ltd
Priority to JP3932984A priority Critical patent/JPS60182703A/en
Publication of JPS60182703A publication Critical patent/JPS60182703A/en
Pending legal-status Critical Current

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  • Physical Vapour Deposition (AREA)
  • Adjustable Resistors (AREA)
  • Apparatuses And Processes For Manufacturing Resistors (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】 この発明は薄膜抵抗の製造法に関する。[Detailed description of the invention] This invention relates to a method for manufacturing thin film resistors.

たとえばサーマルプリント用の発熱抵抗、ショットキー
FET成’v−hlよ超LSIの配線等にMO−81の
スパッタ111方からなる薄腓ガ使用されている。
For example, thin filaments made of sputtered MO-81 are used for heating resistors for thermal printing, Schottky FET formation, V-HL wiring, ultra-LSI wiring, and the like.

このような薄lIケの生成法はすでによ(知られてbる
。たとえば直流2極スパッタ蒸着の場合にνよ第1図に
原理的に示しであるように真空ジャー1内にMo −S
iからなるI−ゲット2と陽画となる基板3とを配IP
Fシー両冒嘆間で異常ゲロー放γ1fを起させる、4は
真空排檗口である。通常は放電ガスとl−てArガスを
用いる。へrイオン7′I;ターゲット2に衝突して原
子を叩き出し−これ75;基板3に付着する。、とれに
よってMO−Si、薄膜カ5形成されるようになる。第
2図はターゲット2の一例を示し、MO−h−らなふ基
体5の表1奮にSi 6を付着して構成される。)、(
体5の表面積に対するSi6の表面積を変更することに
よってMOに対してSlの含有率の異なる薄11りを生
成することができる。もちろんl−ゲットとしてこのよ
うな構成のものに限らf15ず、Siの含有率の異なる
焼結合金。
The method for producing such a thin film is already well known. For example, in the case of direct current bipolar sputter deposition, Mo-S is deposited in a vacuum jar 1 as shown in principle in FIG.
Arrange the I-get 2 consisting of i and the substrate 3 which is a positive image.
4 is a vacuum evacuation hole which causes an abnormal gelatin emission γ1f between the F sea and the air. Usually, Ar gas is used as the discharge gas. Herium ion 7'I; collides with target 2 and knocks out atoms - this 75; adheres to substrate 3; , a MO-Si thin film 5 is formed due to the cracking. FIG. 2 shows an example of the target 2, which is constructed by depositing Si 6 on the top surface of a MO-h-rough substrate 5. ), (
By changing the surface area of Si6 relative to the surface area of body 5, thin films 11 with different contents of Sl relative to MO can be produced. Of course, the l-get is not limited to f15 having such a configuration, but also sintered alloys with different Si contents.

混合粉末であってもよい。It may be a mixed powder.

第8図に示す特性曲線ダは比抵抗#(μΩ−c!x)と
抵抗温度係数TCP(PPM/lll:)で、横軸はタ
ーゲット中の一8j−含有率(mo71!%)である。
The characteristic curve DA shown in Fig. 8 is the specific resistance # (μΩ-c! .

同1ノにおりてA、B11−1−前記した従来の方法に
よって生成したMO−8i薄暎の特性曲線を示す。これ
から理解されるよつに81含有率がeomo/%8彦ま
では抵抗IIFn窄係数’L’ORはリニヤに変化し、
熱的に安定してbることがうかがわれる。このとア きの比抵抗桑は200〃Ω−α以下の比較的低し範囲内
にある。しかしとの種薄;漠の使用目的によつてけ比抵
抗の高いものたとえば400〜1000μΩ−C1n程
度のものを必要とするとき−81の含有率を高めればよ
りとしても−この含有率−1)+6(1rr1077%
を越マると、抵抗温肴係数力f上−ドに太き(f動する
ようになり、熱的に不安定となる。或すけ所望の比抵抗
のものを再現性よ(生成するとと一/J(極めて内鍵と
なる。
A, B11-1 - Characteristic curves of MO-8i thin film produced by the conventional method described above are shown. As can be understood from this, the resistance IIFn narrowing coefficient 'L'OR changes linearly until the 81 content rate reaches eomo/%8hiko.
It can be seen that it is thermally stable. The specific resistance of this case is within a relatively low range of 200 Ω-α or less. However, if you need something with a high specific resistance, for example about 400 to 1000 μΩ-C1n, depending on the purpose of use, it may be better to increase the content of -81. )+6(1rr1077%
If the resistivity is exceeded, the resistance/temperature coefficient force (f) will move significantly (f) and become thermally unstable. 1/J (very internal key).

この発明は高比抵抗の薄膜を熱的に安定に及び再現性よ
(製造することを目的とする。
The object of the present invention is to produce a thin film with high resistivity in a thermally stable and reproducible manner.

この発明はM*−8i からなるターゲットを用いてス
パッタリングする点は従来と同じであるが、放電ガスと
してその一部又は全部にNilガスを用することを特徴
とする。このようにN9ガス全使用した場合、MnけN
llと反応しに(論のに対して、Slは反応しゃす因の
で、これによりSiN又け5iRN4等の化合物の形で
、MO−81,−Nの三元素力)らなる薄膜が形成され
るようになる。
This invention is the same as the conventional method in that sputtering is performed using a target made of M*-8i, but is characterized in that Nil gas is used as part or all of the discharge gas. In this way, when all N9 gas is used, Mn ke N
(Contrary to theory, since Sl is the cause of the reaction, a thin film consisting of three elements of MO-81, -N is formed in the form of compounds such as SiN and 5iRN4). It becomes like this.

そしてSl、N、 Sj*N4は熱的に安定して訃り、
又比抵抗を高めるのに貢献する。
And Sl, N, Sj*N4 die thermally stable,
It also contributes to increasing specific resistance.

第81♂の特性曲線C,Dはこの発明による比抵抗、抵
抗渇仰係数を示す。た七えは比抵抗が8o。
Characteristic curves C and D of the 81st model show the specific resistance and resistance thirst coefficient according to the present invention. Tanae has a specific resistance of 8o.

μΩ−m以上のものを得ようとするとき+ Siの含有
率が20rrl○ρ%以上七すればよ(、し九も抵抗濡
彦係数け2Sj−含有率を増j、て謁つでもほとんど安
定したIiaを呈して因る、この場合スパッタ装置aの
ガス導入系が2系統以上あればAr力゛スと〜9 ガス
とを切担えて編入するようにすると−同じ81含有率の
ターゲットを用すても、高低画比抵45Tの薄11ψを
選択的に形成するとと力;できて有利である。
When trying to obtain a resistance of μΩ−m or more, the Si content should be increased to 20rrl○ρ% or more (and the resistance wettability coefficient should be increased by 2Sj− content, so that almost no In this case, if there are two or more gas introduction systems in the sputtering apparatus a, the Ar gas and the ~9 gas can be combined to handle the target with the same 81 content. It is advantageous to selectively form a thin 11ψ with a high and low image resistivity of 45T even when used for various purposes.

上記特性曲線C,Dは、N、とArとの混合ガスのガス
圧f 5.0 mTorr 、 N9分圧1.5 m’
rorrでスパッタリングした結果である。N、+Aで
のガス圧としては、1.+1〜5 n m Torr 
、 N、分圧1、n 〜10 m’rorrが適当であ
る。1.0 m’rOrr以下では放電[7に((なる
し、r−、nmTorr以上では比抵抗の再現性が悲(
なる6 以上詳述L−たχらにこの発明によれば、放電ガスの一
部又は全部にN9ガスを用すて−MO−8iターゲット
によりスパッタリングして薄膜を生成するようにしたの
で、その薄膜は−MO−3i−Nの化合物となり−これ
によって比抵抗が 2QOμΩ−a以上の薄膜抵抗を作
る場合でも抵抗温彦係数が比較的安定した特性を有する
ものとなり一しかも単にN、ガスを使用すればよいので
−その卵造は極めて簡単であるといった効果を奏する−
The above characteristic curves C and D have a gas pressure of a mixed gas of N and Ar, f 5.0 mTorr, and a N9 partial pressure of 1.5 m'.
This is the result of sputtering with RORR. The gas pressure at N and +A is 1. +1~5 nm Torr
, N and a partial pressure of 1,n to 10 m'rorr are suitable. Below 1.0 m'rOrr, the discharge becomes [7((), and above nmTorr, the reproducibility of resistivity is poor (
According to the present invention, N9 gas is used as part or all of the discharge gas to generate a thin film by sputtering with a -MO-8i target. The thin film becomes a compound of -MO-3i-N, and as a result, even when making a thin film resistor with a specific resistance of 2QOμΩ-a or more, the resistance temperature coefficient remains relatively stable. It's so easy to make eggs that it's extremely simple to make.

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

第11図はスパッタリングの原理説明図I−槙21却は
ターゲットの斜親図1g3図はこの発明による薄膜抵抗
の特性曲線−である。 2・・・・・・ターゲット、3・・・・・・基板、5・
・・・・・Mo動基体−6・・・・・・Sl 第1図 第3図
FIG. 11 is a diagram illustrating the principle of sputtering.Maki 21 is a diagonal diagram of a target.FIG. 2...Target, 3...Substrate, 5.
...Mo moving base-6...Sl Fig. 1 Fig. 3

Claims (1)

【特許請求の範囲】[Claims] Mo−8iからなるターゲットをもって、一部又は全部
がNzガスである放電ガス中でスパッタリングして基板
上にMo −Si −Nの薄膜抵抗を生成してなるIN
 K’J抵抗のり借方法。
An IN produced by sputtering a target made of Mo-8i in a discharge gas partially or entirely composed of Nz gas to produce a Mo-Si-N thin film resistor on a substrate.
How to use K'J resistance.
JP3932984A 1984-02-29 1984-02-29 Method of producing thin film resistor Pending JPS60182703A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3932984A JPS60182703A (en) 1984-02-29 1984-02-29 Method of producing thin film resistor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3932984A JPS60182703A (en) 1984-02-29 1984-02-29 Method of producing thin film resistor

Publications (1)

Publication Number Publication Date
JPS60182703A true JPS60182703A (en) 1985-09-18

Family

ID=12550057

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3932984A Pending JPS60182703A (en) 1984-02-29 1984-02-29 Method of producing thin film resistor

Country Status (1)

Country Link
JP (1) JPS60182703A (en)

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5325442A (en) * 1976-08-20 1978-03-09 Matsushita Electric Ind Co Ltd Thermal print head
JPS5420676A (en) * 1977-07-15 1979-02-16 Mitsubishi Electric Corp Production of semiconductor heat-sensitive switching elements
JPS59143305A (en) * 1983-02-03 1984-08-16 沖電気工業株式会社 Method of producing resistor thin film

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5325442A (en) * 1976-08-20 1978-03-09 Matsushita Electric Ind Co Ltd Thermal print head
JPS5420676A (en) * 1977-07-15 1979-02-16 Mitsubishi Electric Corp Production of semiconductor heat-sensitive switching elements
JPS59143305A (en) * 1983-02-03 1984-08-16 沖電気工業株式会社 Method of producing resistor thin film

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