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JP3846616B2 - Thin film gas sensor - Google Patents
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JP3846616B2 - Thin film gas sensor - Google Patents

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JP3846616B2
JP3846616B2 JP09627499A JP9627499A JP3846616B2 JP 3846616 B2 JP3846616 B2 JP 3846616B2 JP 09627499 A JP09627499 A JP 09627499A JP 9627499 A JP9627499 A JP 9627499A JP 3846616 B2 JP3846616 B2 JP 3846616B2
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Prior art keywords
film
heater
thin film
sio
gas sensor
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JP2000214119A (en
Inventor
眞一 小知和
孝一 津田
克己 小野寺
卓弥 鈴木
文宏 井上
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Fuji Electric FA Components and Systems Co Ltd
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Fuji Electric FA Components and Systems Co Ltd
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Description

【0001】
【発明の属する技術分野】
この発明は、電池駆動に好適な低消費電力型薄膜ガスセンサに関する。
【0002】
【従来の技術】
一般のガスセンサのうち、特に家庭用ガス漏れ警報器等の用途に用いられるものはCO,CH4 ,C3 8 等に選択的に感応するデバイスであり、その性格上、高感度,高選択性,高応答性,高信頼性,低消費電力が必要不可欠である。
ところで、家庭用として普及しているガス漏れ警報器には、都市ガス用やプロパンガス用の可燃性ガス検知を目的とするもの、燃焼機器の不完全燃焼ガス検知を目的とするもの、または、両方の機能を合わせ持ったものなどがあるが、いずれもコストや設置性の問題から普及率はそれほど高くない。このような事情から普及率アップを図るべく設置性の改善、具体的には電池駆動としてコードレス化することが望まれている。
【0003】
電池駆動を実現するためには小型化し、低消費電力化することが不可欠であるが、従来一般的に用いられる接触燃焼式や半導体式のガスセンサは、ガスに感応する感応膜をSnO2 などの粉体を焼結する方法により製造しており、スクリーン印刷等の方法を用いたとしても小型化には限界があった。
一方、比較的小型化が容易である半導体微細加工プロセスを用いたセンサも知られており、これは、基板上に絶縁膜,ヒーター,電極,感応膜などを化学気相法(CVD法)や蒸着法,スパッタ法により積層し、さらにセンサの熱容量を小さくしかつ熱絶縁を図るために、基板をエッチングすることで薄くしたり、または完全に除去するといった方法が採られている。
【0004】
【発明が解決しようとする課題】
上記のような微細加工プロセスを用いたセンサでは、Ptをヒーター層として用いることが多い。
ところで、ヒーター抵抗体の長さLは、次式により制約される。
L≧Vappl/(Jmax×ρ) …(1)
ここに、Vapplは印加電圧、Jmaxは最大電流密度、ρはヒーターの比抵抗(抵抗率)を示す。
【0005】
いま、印加電圧を2V、最大電流密度を5×109 A/m2 とした場合、上式からPt(ρ≒10μΩcm)ではL≧4mmとなる。温度に対する応答性を考慮すると、センサとしては100μm×100μm程度のチップ面積であることが望ましく、その場合のヒーター線幅は約1μmとなる。これを比較的簡便なウェットエッチによるフォトプロセスで実現するのは難しく、少なくともPtの5倍程度の比抵抗を有する材料をヒーターに用いる必要が生じる。
【0006】
また、電池で駆動することを想定すると、パルス電圧印加による間欠駆動が不可欠であるが、SiO2 やSiNなどの絶縁膜の上に一般的なメタルのヒーター層を形成した場合、熱膨張係数の差による変形や応力集中により破壊されやすいという問題もある。
したがって、この発明の課題は、低消費電力化を図り間欠動作寿命を延ばすことにある。
【0007】
【課題を解決するための手段】
このような課題を解決すべく、請求項1の発明では、Si基板の一側面中央部がダイアフラム様にくり抜かれた基板面上に、熱酸化SiO2膜,CVD−SiO2膜および窒化Si膜からなる支持膜を介して、薄膜ヒーターをスパッタ法または蒸着法によって形成した後、SiO2膜または窒化Si膜の電気絶縁膜を介して感応膜電極をPt/TaまたはPt/Tiによって形成し、さらに、SnO2を含む感応膜を形成するとともに、前記薄膜ヒーターとして、熱膨張係数が10×10 -6 /℃以下で、かつ、比抵抗が50μΩcm以上のFe−Ni系インバー合金、またはTiB 2 ,ZrB 2 ,HFB 2 を含む金属ホウ化物、若しくはMoSi 2 ,WSi 2 ,TaSi 2 ,TiSi 2 を含む高融点金属シリサイド、或いはSiC,TiN,NbN,Wを2〜16wt%含むPt,Ruを4〜20wt%含むPt,Irを15〜40wt%含むPtのいずれかを用いることを特徴とする。
この請求項1の発明においては、前記薄膜ヒーターは、一定時間毎に極めて短い時間のみ電圧印加を繰り返すパルスにて駆動されることができる(請求項2の発明)。
【0008】
【発明の実施の形態】
図1はこの発明の実施の形態を示す断面構造図である。
すなわち、両面に熱酸化膜が付いたSi基板上に、ダイアフラム構造の支持膜および熱絶縁膜としてのSiNとSiO2 膜を順次プラズマCVD法にて形成する。その上に、この発明によるヒーター層1として、TiSi2 膜を0.5μm形成した。さらに、SiO2 絶縁膜を介してヒータ用と感応膜用の電極2をPt/Taにより形成した後、スパッタ法により感応膜となるSnO2 膜3を形成した。最後に基板裏面からエッチングによりSiを除去し、ダイアフラム構造とした。なお、ダイアフラムとは薄膜状の支持膜の周囲をSi基板により支持し、周囲が厚く中央部が薄く形成されたものをいうこととする。
ヒーター層1であるTiSi2 膜の形成には混晶ターゲットによるスパッタ法を用い、200℃の成膜温度にて実施した。スパッタ後、TiSi2 膜の結晶化を行なうためにN2 雰囲気中にて850℃,3時間の熱処理を実行した。
【0009】
図2にヒーター層の形状例を示す。
これは、10μmの線幅で約500μmの長さを形成した例で、ヒーター層の抵抗値はおよそ200Ωである。
図3にヒーターにおける電圧印加前後での変位の最大値と温度との関係例を示す。実線は材料がNiCrの例、点線はこの発明によるTiSi2 の例である。NiCrを用いた場合、400℃以上では数百万回以下の間欠動作により破壊が生じたのに対し、TiSi2 では450℃においても2000万回の間欠動作後も破壊は認められなかった。ここで、NiCrとTiSi2 の熱膨張係数はそれぞれ18×10-6/℃,7×10-6/℃である。これは、絶縁膜とヒーター材料との熱膨張係数差が大きい程電圧印加前後での変形量が大きく、繰り返し動作による絶縁膜の疲労破壊が生じるためと考えられている。
【0010】
図4はヒーター材料の間欠動作回数に対する抵抗値変化説明図で、上記のようなヒーターを用いた場合と従来のNiCrヒーターの場合とを比較して示している。なお、動作温度は400℃である。
同図からも明らかなように、NiCrヒーターが約200万回程度で破壊しているのに対し、この発明によるTiSi2 ヒーターでは2000万回後も3%程度の抵抗値変化を示すのみで、破壊しないことが分かる。
【0011】
ヒーター層としてPtの比抵抗の3倍、つまり約30μΩcm以上、好ましくはPtの比抵抗の5倍、すなわち約50μΩcm以上の比抵抗を有し、熱膨張係数10×10-6/℃以下の材料として、次のようなものが挙げられる。
比抵抗が50μΩcm以上の材料として、タンタル(Ta),チタン(Ti)またはニオブ(Nb)から選ばれた一成分の窒化物(第1のグループ)、また、比抵抗が30μΩcm以上の材料として、白金(Pt)を主成分とし、これにタングステン(W),ルテニウム(Ru)またはイリジウム(Ir)のうちの一成分を含む合金(第2のグループ)が存在することが判明している。
【0012】
以下、これらについて説明する。なお、第1のグループの窒化物としては、金属と窒素の原子比は1:1のものが使用できるが、金属と窒素の原子比は必ずしも1:1に限定されるものではなく、例えば特開平9−201965号公報にも記載されているように、金属と窒素の比率が1:1以外の窒化物、例えば1:0.8(TaN0.8)のものも使用可能である。
ヒーター材料としてTaN(TaNヒーター)を用いたときの、図3に対応する最大変位量とヒーター温度との関係を図5に、また、図4に対応する間欠動作回数に対する抵抗変化の関係を図6にそれぞれ示す。なお、TaNの熱膨張係数は8×10-6/℃である。図5,図6の実線がTaの場合、点線がNiCrの場合である。図5,図6からも明らかなように、その特徴はTiSi2 の場合と殆ど同様であることが分かる。
【0013】
これらの特性はTiN,NbNを用いた場合も全く同様である。なお、TiN,NbNの各熱膨張係数は9.4×10-6/℃,10×10-6/℃である。
表1にTiN,NbNヒーターの場合の、450℃における変位の最大値を、NiCrヒーターと比較して示す。TiN,NbNのいずれも、電圧印加前後の最大変位量はNiCrに比べて小さく、NiCrの変位量の約75%程度となっている。
【表1】

Figure 0003846616
【0014】
TiN,NbNヒーターを、450℃で2000万回間欠動作させたときの抵抗の変化(2000万回間欠動作後/間欠動作前の比)を表2に示す。
【表2】
Figure 0003846616
表2から、TiN,NbNのいずれも、2000万回以上の間欠動作でも、ヒーターの破損は認められなかったことが分かる。
【0015】
次に、第2のグループの例について説明する。
まず、W−Pt膜を図1と同様に形成した例では、Wの含有率を2,4,6,8,12および20wt%(重量百分率)の6種類としたときの比抵抗,熱膨張係数を表3に示す。
【表3】
Figure 0003846616
表3に示すように、W−Pt系合金の熱膨張係数は、個々の熱膨張係数の重量分率の和で表わされるのに対し、比抵抗はWの含有率約6wt%に極大値が見られる。すなわち、20℃での比抵抗が30μΩcm以上の組成範囲は、Wが3〜16wt%であった。
【0016】
表3で比抵抗が極大値を示す6wt%W−Ptヒーターについて、450℃加熱前後の最大変位量と、2000万回間欠動作前後の抵抗の変化を表4に示す。
【表4】
Figure 0003846616
表4から、W−Ptヒーターは第1のグループの窒化物系ヒーターと同等またはそれ以上の間欠動作安定性を示すことが分かる。
【0017】
ヒーター層としてRu−Pt系合金を用いる場合について説明する。
この場合も、Ruの含有率を5,10,20,30wt%の4種類としたときの比抵抗,熱膨張係数を表5に示す。
【表5】
Figure 0003846616
表5から、W−Pt系の場合と同様、熱膨張係数は個々の熱膨張係数の重量分率の和で表わされるのに対し、比抵抗はRuの含有率約10wt%に極大値が見られる。すなわち、20℃での比抵抗が30μΩcm以上の組成範囲は、Ruが4〜20wt%であった。
【0018】
次に、ヒーター層としてIr−Pt系合金を用いる場合について説明する。
この場合も、Irの含有率を10,25,40p55wt%の4種類としたときの比抵抗,熱膨張係数を表6に示す。
【表6】
Figure 0003846616
表6から、W−Pt系の場合と同様、熱膨張係数は個々の熱膨張係数の重量分率の和で表わされるのに対し、比抵抗はIrの含有率約25wt%に極大値が見られる。すなわち、20℃での比抵抗が30μΩcm以上の組成範囲は、Irが15〜40wt%であった。
【0019】
ここで、10wt%Ru−Ptと25wt%Ir−Ptの2種類のヒーターについて、450℃加熱前後の最大変位量と、2000万回間欠動作前後の抵抗の変化を表7に示す。
【表7】
Figure 0003846616
表7に示すように、Ru−Pt,Ir−Pt系ヒーターのいずれも、窒化物系ヒーターと同等またはそれ以上の間欠動作安定性を示すことが分かる。
【0020】
【発明の効果】
この発明によれば、薄膜ヒーター材としてPtの5倍、つまり50μΩcm以上の比抵抗を有し、かつ熱膨張係数が10×10-6/℃以下、望ましくは7×10-6/℃以下の材料を用いることで、従来よりも低消費電力で間欠動作寿命の長い薄膜ガスセンサを得ることが可能となる利点がもたらされる。
【図面の簡単な説明】
【図1】この発明の実施の形態を示す構造断面図である。
【図2】図1で用いられるヒーター層の形状例説明図である。
【図3】ヒーター部の間欠動作回数に対する抵抗変化説明図である。
【図4】ヒーター部の電圧印加前後での変位の最大値と温度との関係説明図である。
【図5】ヒーター部の間欠動作回数に対する抵抗変化の別の例の説明図である。
【図6】ヒーター部の電圧印加前後での変位の最大値と温度との関係の別の例の説明図である。
【符号の説明】
1…ヒーター層、2…電極、3…SnO2 膜(感応膜)。[0001]
BACKGROUND OF THE INVENTION
The present invention relates to a low power consumption thin film gas sensor suitable for battery driving.
[0002]
[Prior art]
Among general gas sensors, those used for applications such as household gas leak alarms are devices that are selectively sensitive to CO, CH 4 , C 3 H 8, etc. Performance, high responsiveness, high reliability, and low power consumption are indispensable.
By the way, the gas leak alarms that are widely used for household use include those for the purpose of detecting flammable gases for city gas and propane gas, those for the purpose of detecting incomplete combustion gases in combustion equipment, or There are things that have both functions, but the penetration rate is not so high due to cost and installation problems. Under such circumstances, it is desired to improve the installation property, specifically, to be cordless as battery driving in order to increase the diffusion rate.
[0003]
In order to realize battery driving, it is indispensable to reduce the size and reduce the power consumption. However, conventionally used catalytic combustion type and semiconductor type gas sensors have a sensitive film sensitive to gas such as SnO 2 . The powder is manufactured by sintering, and there is a limit to downsizing even if a method such as screen printing is used.
On the other hand, a sensor using a semiconductor microfabrication process that is relatively easy to downsize is also known. This is because an insulating film, a heater, an electrode, a sensitive film, etc. are formed on a substrate by a chemical vapor deposition (CVD) method or the like. In order to reduce the heat capacity of the sensor and to achieve thermal insulation, the substrate is thinned by etching or completely removed in order to reduce the heat capacity of the sensor and to achieve thermal insulation.
[0004]
[Problems to be solved by the invention]
In a sensor using the microfabrication process as described above, Pt is often used as a heater layer.
By the way, the length L of the heater resistor is restricted by the following equation.
L ≧ Vappl / (Jmax × ρ) (1)
Here, Vappl is the applied voltage, Jmax is the maximum current density, and ρ is the specific resistance (resistivity) of the heater.
[0005]
Now, assuming that the applied voltage is 2 V and the maximum current density is 5 × 10 9 A / m 2 , L ≧ 4 mm at Pt (ρ≈10 μΩcm) from the above equation. Considering responsiveness to temperature, the sensor preferably has a chip area of about 100 μm × 100 μm, and the heater line width in that case is about 1 μm. This is difficult to realize by a relatively simple wet etching photo process, and it is necessary to use a material having a specific resistance of at least about 5 times Pt for the heater.
[0006]
In addition, assuming driving with a battery, intermittent driving by applying a pulse voltage is indispensable. However, when a general metal heater layer is formed on an insulating film such as SiO 2 or SiN, the coefficient of thermal expansion is There is also a problem that it is easily broken by deformation or stress concentration due to the difference.
Accordingly, an object of the present invention is to reduce power consumption and extend the intermittent operation life.
[0007]
[Means for Solving the Problems]
To solve such problems, in the invention of claim 1, on the substrate surface which one side central portion is hollowed out in the diaphragm-like Si substrate, a thermal oxide SiO 2 film, CVD-SiO 2 film and the Si nitride film A thin film heater is formed by a sputtering method or a vapor deposition method through a support film made of, and then a sensitive film electrode is formed by Pt / Ta or Pt / Ti through an electric insulating film of a SiO 2 film or a Si nitride film, Further, a sensitive film containing SnO 2 is formed , and as the thin film heater, a Fe—Ni-based invar alloy having a thermal expansion coefficient of 10 × 10 −6 / ° C. or less and a specific resistance of 50 μΩcm or more, or TiB 2 , ZrB 2 , metal boride containing HFB 2 , refractory metal silicide containing MoSi 2 , WSi 2 , TaSi 2 , TiSi 2 , or SiC, TiN, NbN Pt containing 2 to 16 wt% of W, Pt containing 4 to 20 wt% of Ru, or Pt containing 15 to 40 wt% of Ir.
In this invention of Claim 1, the said thin film heater can be driven by the pulse which repeats a voltage application only for a very short time for every fixed time (Invention of Claim 2).
[0008]
DETAILED DESCRIPTION OF THE INVENTION
FIG. 1 is a cross-sectional structural view showing an embodiment of the present invention.
That is, a SiN and SiO 2 film as a support film having a diaphragm structure and a thermal insulating film are sequentially formed on a Si substrate having a thermal oxide film on both sides by a plasma CVD method. A TiSi 2 film of 0.5 μm was formed thereon as the heater layer 1 according to the present invention. Furthermore, after the electrodes 2 for the heater and the sensitive film were formed of Pt / Ta through the SiO 2 insulating film, the SnO 2 film 3 serving as the sensitive film was formed by sputtering. Finally, Si was removed from the back surface of the substrate by etching to form a diaphragm structure. In addition, the diaphragm means that the periphery of the thin film-like support film is supported by the Si substrate and the periphery is thick and the central portion is thin.
The TiSi 2 film as the heater layer 1 was formed by sputtering using a mixed crystal target at a film forming temperature of 200 ° C. After sputtering, heat treatment was performed at 850 ° C. for 3 hours in an N 2 atmosphere in order to crystallize the TiSi 2 film.
[0009]
FIG. 2 shows an example of the shape of the heater layer.
This is an example in which a line width of 10 μm and a length of about 500 μm are formed, and the resistance value of the heater layer is about 200Ω.
FIG. 3 shows an example of the relationship between the maximum displacement value and temperature before and after voltage application in the heater. The solid line is an example where the material is NiCr, and the dotted line is an example of TiSi 2 according to the present invention. When NiCr was used, destruction occurred due to intermittent operation of several million times or less at 400 ° C. or more, whereas TiSi 2 did not show destruction even at 450 ° C. after 20 million times of intermittent operation. Here, the thermal expansion coefficients of NiCr and TiSi 2 are 18 × 10 −6 / ° C. and 7 × 10 −6 / ° C., respectively. This is considered to be because the larger the difference in thermal expansion coefficient between the insulating film and the heater material, the larger the deformation amount before and after voltage application, and the fatigue failure of the insulating film due to repeated operations.
[0010]
FIG. 4 is an explanatory diagram of changes in resistance value with respect to the number of intermittent operations of the heater material, and shows a comparison between the case of using the heater as described above and the case of a conventional NiCr heater. The operating temperature is 400 ° C.
As is clear from the figure, the NiCr heater broke down about 2 million times, whereas the TiSi 2 heater according to the present invention only showed a resistance value change of about 3% after 20 million times. You can see that it wo n’t break.
[0011]
A material having a specific resistance of 3 times the specific resistance of Pt, that is, about 30 μΩcm or more, preferably 5 times the specific resistance of Pt, that is, about 50 μΩcm or more, and having a thermal expansion coefficient of 10 × 10 −6 / ° C. or less as the heater layer The following may be mentioned.
As a material having a specific resistance of 50 μΩcm or more, a one-component nitride (first group) selected from tantalum (Ta), titanium (Ti) or niobium (Nb), or a material having a specific resistance of 30 μΩcm or more, It has been found that there is an alloy (second group) containing platinum (Pt) as a main component and containing one component of tungsten (W), ruthenium (Ru) or iridium (Ir).
[0012]
Hereinafter, these will be described. As the first group of nitrides, those having a metal / nitrogen atomic ratio of 1: 1 can be used, but the metal / nitrogen atomic ratio is not necessarily limited to 1: 1. As described in Japanese Utility Model Laid-Open No. 9-201965, nitrides having a metal to nitrogen ratio other than 1: 1, for example, 1: 0.8 (TaN0.8) can be used.
FIG. 5 shows the relationship between the maximum displacement corresponding to FIG. 3 and the heater temperature when TaN (TaN heater) is used as the heater material, and FIG. 5 shows the relationship between the resistance change and the number of intermittent operations corresponding to FIG. 6 respectively. The thermal expansion coefficient of TaN is 8 × 10 −6 / ° C. 5 and 6, the solid line is Ta, and the dotted line is NiCr. As is apparent from FIGS. 5 and 6, the characteristics are almost the same as those of TiSi 2 .
[0013]
These characteristics are exactly the same when TiN or NbN is used. The thermal expansion coefficients of TiN and NbN are 9.4 × 10 −6 / ° C. and 10 × 10 −6 / ° C.
Table 1 shows the maximum value of displacement at 450 ° C. in the case of TiN and NbN heaters in comparison with NiCr heaters. For both TiN and NbN, the maximum displacement before and after voltage application is smaller than that of NiCr, and is about 75% of the displacement of NiCr.
[Table 1]
Figure 0003846616
[0014]
Table 2 shows the change in resistance when the TiN and NbN heaters are intermittently operated 20 million times at 450 ° C. (ratio after 20 million times intermittent operation / before intermittent operation).
[Table 2]
Figure 0003846616
From Table 2, it can be seen that neither TiN nor NbN was found to be damaged by the heater even in intermittent operation of 20 million times or more.
[0015]
Next, an example of the second group will be described.
First, in the example in which the W—Pt film is formed in the same manner as in FIG. 1, the specific resistance and thermal expansion when the W content is six types of 2, 4, 6, 8, 12 and 20 wt% (weight percentage). The coefficients are shown in Table 3.
[Table 3]
Figure 0003846616
As shown in Table 3, the thermal expansion coefficient of the W-Pt alloy is expressed by the sum of the weight fractions of the individual thermal expansion coefficients, whereas the specific resistance has a maximum value at a W content of about 6 wt%. It can be seen. That is, in the composition range where the specific resistance at 20 ° C. was 30 μΩcm or more, W was 3 to 16 wt%.
[0016]
Table 4 shows the maximum displacement amount before and after heating at 450 ° C. and the change in resistance before and after 20 million intermittent operations for the 6 wt% W-Pt heater having the maximum specific resistance in Table 3.
[Table 4]
Figure 0003846616
It can be seen from Table 4 that the W-Pt heater exhibits an intermittent operation stability equivalent to or higher than that of the first group of nitride heaters.
[0017]
The case where a Ru—Pt alloy is used as the heater layer will be described.
Also in this case, Table 5 shows the specific resistance and the thermal expansion coefficient when the Ru content is 4, 10, 20, and 30 wt%.
[Table 5]
Figure 0003846616
From Table 5, as in the case of the W-Pt system, the thermal expansion coefficient is represented by the sum of the weight fractions of the individual thermal expansion coefficients, whereas the specific resistance has a maximum value at a Ru content of about 10 wt%. It is done. That is, in the composition range where the specific resistance at 20 ° C. is 30 μΩcm or more, Ru was 4 to 20 wt%.
[0018]
Next, a case where an Ir—Pt alloy is used as the heater layer will be described.
Also in this case, Table 6 shows specific resistance and thermal expansion coefficient when the Ir content is 10, 25, and 40 p55 wt%.
[Table 6]
Figure 0003846616
From Table 6, as in the case of the W-Pt system, the thermal expansion coefficient is expressed as the sum of the weight fractions of the individual thermal expansion coefficients, whereas the specific resistance has a maximum value at an Ir content of about 25 wt%. It is done. That is, in the composition range where the specific resistance at 20 ° C. is 30 μΩcm or more, Ir was 15 to 40 wt%.
[0019]
Table 7 shows the maximum displacement before and after heating at 450 ° C. and the change in resistance before and after 20 million intermittent operations for two types of heaters of 10 wt% Ru—Pt and 25 wt% Ir—Pt.
[Table 7]
Figure 0003846616
As shown in Table 7, it can be seen that any of the Ru-Pt and Ir-Pt heaters exhibits an intermittent operation stability equivalent to or higher than that of the nitride heater.
[0020]
【The invention's effect】
According to the present invention, the thin film heater material has a specific resistance of 5 times Pt, that is, 50 μΩcm or more, and a thermal expansion coefficient of 10 × 10 −6 / ° C. or lower, preferably 7 × 10 −6 / ° C. or lower. By using the material, there is an advantage that it is possible to obtain a thin film gas sensor with lower power consumption and longer intermittent operation life than in the past.
[Brief description of the drawings]
FIG. 1 is a structural sectional view showing an embodiment of the present invention.
FIG. 2 is an explanatory diagram of a shape example of a heater layer used in FIG. 1;
FIG. 3 is an explanatory diagram of resistance change with respect to the number of intermittent operations of a heater unit.
FIG. 4 is a diagram for explaining the relationship between the maximum value of displacement before and after voltage application to the heater and the temperature.
FIG. 5 is an explanatory diagram of another example of a resistance change with respect to the number of intermittent operations of the heater unit.
FIG. 6 is an explanatory diagram of another example of the relationship between the maximum value of displacement before and after voltage application to the heater and the temperature.
[Explanation of symbols]
1 ... heater layer, 2 ... electrode, 3 ... SnO 2 film (sensitive film).

Claims (2)

Si基板の一側面中央部がダイアフラム様にくり抜かれた基板面上に、熱酸化SiO2膜,CVD−SiO2膜および窒化Si膜からなる支持膜を介して、薄膜ヒーターをスパッタ法または蒸着法によって形成した後、SiO2膜または窒化Si膜の電気絶縁膜を介して感応膜電極をPt/TaまたはPt/Tiによって形成し、さらに、SnO2を含む感応膜を形成するとともに、前記薄膜ヒーターとして、熱膨張係数が10×10 -6 /℃以下で、かつ、比抵抗が50μΩcm以上のFe−Ni系インバー合金、またはTiB 2 ,ZrB 2 ,HFB 2 を含む金属ホウ化物、若しくはMoSi 2 ,WSi 2 ,TaSi 2 ,TiSi 2 を含む高融点金属シリサイド、或いはSiC,TiN,NbN,Wを2〜16wt%含むPt,Ruを4〜20wt%含むPt,Irを15〜40wt%含むPtのいずれかを用いることを特徴とする薄膜ガスセンサ。A thin film heater is formed by sputtering or vapor deposition on a substrate surface in which one side central portion of a Si substrate is hollowed out like a diaphragm through a support film made of a thermally oxidized SiO 2 film, a CVD-SiO 2 film, and a Si nitride film. Then, a sensitive film electrode is formed of Pt / Ta or Pt / Ti through an electric insulating film of SiO 2 film or Si nitride film, and further, a sensitive film containing SnO 2 is formed , and the thin film heater As follows: Fe—Ni-based Invar alloy having a thermal expansion coefficient of 10 × 10 −6 / ° C. or less and a specific resistance of 50 μΩcm or more, or a metal boride containing TiB 2 , ZrB 2 , HFB 2 , or MoSi 2 , Refractory metal silicide containing WSi 2 , TaSi 2 , TiSi 2 , or Pt and Ru containing 2 to 16 wt% of SiC, TiN, NbN, and W 4 to 20 wt% A thin film gas sensor using any one of Pt containing 15% and Pt containing 15 to 40 wt% Ir . 前記薄膜ヒーターは、一定時間毎に極めて短い時間のみ電圧印加を繰り返すパルスにて駆動されることを特徴とする請求項1に記載の薄膜ガスセンサ。2. The thin film gas sensor according to claim 1, wherein the thin film heater is driven by a pulse that repeats voltage application for a very short time every predetermined time .
JP09627499A 1998-11-17 1999-04-02 Thin film gas sensor Expired - Lifetime JP3846616B2 (en)

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