JPH0359370B2 - - Google Patents
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- Publication number
- JPH0359370B2 JPH0359370B2 JP57066453A JP6645382A JPH0359370B2 JP H0359370 B2 JPH0359370 B2 JP H0359370B2 JP 57066453 A JP57066453 A JP 57066453A JP 6645382 A JP6645382 A JP 6645382A JP H0359370 B2 JPH0359370 B2 JP H0359370B2
- Authority
- JP
- Japan
- Prior art keywords
- pellet
- pyroelectric
- support
- approximately
- adhesive
- 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.)
- Expired
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Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J5/00—Radiation pyrometry, e.g. infrared or optical thermometry
- G01J5/10—Radiation pyrometry, e.g. infrared or optical thermometry using electric radiation detectors
- G01J5/34—Radiation pyrometry, e.g. infrared or optical thermometry using electric radiation detectors using capacitors, e.g. pyroelectric capacitors
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- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Photometry And Measurement Of Optical Pulse Characteristics (AREA)
- Radiation Pyrometers (AREA)
Description
【発明の詳細な説明】
本発明は入射赤外線変化量に応じて電荷を発生
する焦電体ペレツトを備えた焦電型赤外線検出器
に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a pyroelectric infrared detector equipped with a pyroelectric pellet that generates a charge depending on the amount of change in incident infrared radiation.
通常、入射赤外線変化量に応じて電荷を発生す
る焦電体ペレツトはこの散逸熱が小である程出力
が増大する特性を有しており、従つて従来の検出
器では第1図に示す如く焦電体ペレツト1は断熱
されるように支持台2に金線3,3にて宙吊り状
態に支持されていた。しかし乍ら、焦電体ペレツ
ト1はその厚さが数10μmと極めて薄く且つ形状
も数ミリ角と小さいため、上述のように宙吊りに
する場合取扱いに困難を有し検出器の量産性が低
かつた。 Normally, a pyroelectric pellet that generates electric charge according to the amount of change in incident infrared rays has a characteristic that the smaller the dissipated heat, the greater the output. Therefore, in conventional detectors, as shown in Figure 1, The pyroelectric pellet 1 was supported in a suspended state on a support stand 2 by gold wires 3, 3 so as to be thermally insulated. However, since the pyroelectric pellet 1 is extremely thin with a thickness of several tens of micrometers and has a small shape of several millimeters square, it is difficult to handle when suspended in the air as described above, and the mass productivity of the detector is low. It was.
そこで、最近の検出器では第2図に示す如く、
上面に凹部4を有する支持台5の上面に焦電体ペ
レツト6をエポキシ系接着剤7にて接着すること
により上記ペレツト6を支持する構造となつてい
る。そして、上記凹部4の存在により上記ペレツ
ト6は充分に断熱されているから、ペレツト6の
散逸熱は極めて小さく抑えられている。 Therefore, recent detectors, as shown in Figure 2,
The structure is such that the pellets 6 are supported by adhering the pyroelectric pellets 6 to the upper surface of a support base 5 having a recess 4 on the upper surface using an epoxy adhesive 7. Since the pellets 6 are sufficiently insulated due to the presence of the recesses 4, the heat dissipated from the pellets 6 is suppressed to an extremely low level.
一般に、焦電体ペレツト1および6はそれぞれ
支持台2および5と共に、この種電気業界でPO
−5型と称されている収納缶に収納されている。
即ち、この収納缶は直径8mm、深さ4〜7mm、肉
厚0.2mmの鉄−ニツケル合金製の有底円筒容器で
あり、従つて、この中に収納される焦電体ペレツ
トの面積は約25mm2以下に制限されることになる。
而して、焦電体ペレツト1および6の表面および
裏面電極に金属細線(金、アルミ等)よりなる信
号引出線を接合する場合、通常、その接合方法は
熱溶着、超音波溶着或はそれ等の併用である。し
かるに、これ等のいずれの方法も用いても接合時
の加圧は不可欠である。また、単結晶材料(タン
タル酸リチウム等)およびセラミツク材料
(PZT等)よりなる焦電体ペレツトの厚みは一般
に30〜100μm程度である。このような薄膜上に
この薄膜を破損することなく、電極の引出線の接
合を行うには何等かの工夫が必要である。また、
一般にこの引出線には直径30μmの金属細線が用
いられる。 In general, the pyroelectric pellets 1 and 6, together with the supports 2 and 5, respectively, are commonly used in this type of electrical industry.
It is stored in a storage can called Type-5.
That is, this storage can is a bottomed cylindrical container made of iron-nickel alloy with a diameter of 8 mm, a depth of 4 to 7 mm, and a wall thickness of 0.2 mm. Therefore, the area of the pyroelectric pellets stored therein is approximately It will be limited to 25mm2 or less.
When joining signal lead wires made of thin metal wires (gold, aluminum, etc.) to the front and back electrodes of the pyroelectric pellets 1 and 6, the joining method is usually thermal welding, ultrasonic welding, or other methods. etc. are used in combination. However, no matter which method is used, pressurization during bonding is essential. Further, the thickness of the pyroelectric pellet made of a single crystal material (such as lithium tantalate) and a ceramic material (such as PZT) is generally about 30 to 100 μm. Some kind of contrivance is required to join the lead wire of the electrode onto such a thin film without damaging the thin film. Also,
Generally, a thin metal wire with a diameter of 30 μm is used for this lead wire.
しかし乍ら、斯る第2図に示す如き検出器では
接着剤層の厚みを均一にしなければ所謂ポツプコ
ーンノイズを発生してしまう。即ち、接着剤層の
厚みが不均一であると、検出器の周囲温度などの
外的環境が変化した場合に接着剤層の各部が不均
一に伸縮し、斯る不均一な伸縮力により焦電体ペ
レツト6に歪が発生する。そして、斯る歪がある
レベル以上になると焦電体ペレツト6は瞬時的に
歪を解消すべく、即ち上記付近一な伸縮力から開
放させるべく元の状態に復帰する。ここに、焦電
体ペレツト6は必ず圧電効果を有するため、印加
される外力が瞬時的に大きく変化すると、即ち上
述の如き歪が解消されるとかなりの電荷を突発的
に、所謂ポツプコーンノイズを発生してしまう。 However, in such a detector as shown in FIG. 2, so-called popcorn noise will occur unless the thickness of the adhesive layer is made uniform. In other words, if the thickness of the adhesive layer is uneven, each part of the adhesive layer will expand and contract unevenly when the external environment such as the ambient temperature of the detector changes, and this uneven stretching force will cause the focus to deteriorate. Distortion occurs in the electric pellet 6. When the strain exceeds a certain level, the pyroelectric pellet 6 instantaneously returns to its original state in order to eliminate the strain, that is, to release itself from the above-mentioned uniform expansion and contraction force. Here, since the pyroelectric pellet 6 always has a piezoelectric effect, when the applied external force changes instantaneously, that is, when the above-mentioned distortion is eliminated, a considerable amount of charge is suddenly generated, forming a so-called popcorn. This will generate noise.
第3図は斯るポツプコーンノイズの発生状態を
示し、ポツプコーンノイズはP1,P2,P3の如く
時間経過につれて外的環境の変化によりホワイト
ノイズの電圧レベルW(±300mV程度)より高レ
ベルにて突発的に発生していることが分る。 Figure 3 shows the generation state of such popcorn noise. Popcorn noise is caused by changes in the white noise voltage level W (approximately ±300 mV) due to changes in the external environment as time passes, such as P 1 , P 2 , and P 3 . ) It can be seen that this occurs suddenly at higher levels.
而して、斯るポツプコーンノイズが発生する
と、検出器のSN比が低下し検出器の信頼性が劣
ると云う欠点がある。 However, when such popcorn noise occurs, there is a drawback that the SN ratio of the detector decreases and the reliability of the detector deteriorates.
本発明は斯る点に鑑みてなされたもので、以下
本発明実施例を、侵入警報器の検知部に用いる焦
電体赤外線検出器について、図面に基づいて詳述
する。 The present invention has been made in view of these points, and embodiments of the present invention will be described below in detail with reference to the drawings, regarding a pyroelectric infrared detector used in a detection section of an intruder alarm.
第4図及び第5図において、8は入射赤外線変
化量に応じて電荷を発生するタンクル酸リチウム
(LiTaO3)結晶等で形成された焦電体ペレツト、
9および10は夫々ニクロム(Ni−Cr)の真空
蒸着により形成された上記ペレツト8の表、裏面
電極で、表面電極9は互いに分離され且つ同形状
を有する第1及び第2表面電極9a,9bからな
つており、裏面電極10は上記ペレツト8の裏面
全面に施されている。11a及び11bは夫々第
1及び第2引出線12a,12bを上記第1及び
第2表面電極9a,9bに超音波ボンデイングす
るための第1及び第2パツドで、該第1及び第2
パツドは夫々アルミニウム等の真空蒸着膜から成
り上記第1及び第2表面電極9a,9bの角部に
設けられている。尚、上記第1引出線12は接地
され、上記第2引出線12bから信号が出力され
る。13は燐青銅などからなり、上記ペレツト8
を裏面電極10側にてエポキシ系接着剤14で上
面に装着支持する支持台である。 In FIGS. 4 and 5, reference numeral 8 indicates a pyroelectric pellet made of lithium tanchlorate (LiTaO 3 ) crystal, etc., which generates an electric charge according to the amount of change in incident infrared rays;
Reference numerals 9 and 10 are front and back electrodes of the pellet 8 formed by vacuum evaporation of nichrome (Ni-Cr), respectively, and the front electrodes 9 are first and second front electrodes 9a and 9b that are separated from each other and have the same shape. The back electrode 10 is applied to the entire back surface of the pellet 8. 11a and 11b are first and second pads for ultrasonic bonding the first and second lead wires 12a and 12b to the first and second surface electrodes 9a and 9b, respectively;
The pads are each made of a vacuum-deposited film of aluminum or the like and are provided at the corners of the first and second surface electrodes 9a, 9b. Note that the first leader line 12 is grounded, and a signal is output from the second leader line 12b. 13 is made of phosphor bronze, etc., and the pellet 8 is
This is a support stand that is attached and supported on the upper surface with an epoxy adhesive 14 on the back electrode 10 side.
そして、上記焦電体ペレツト8の前面におい
て、人体が矢印Aの如く通過すると、まずペレツ
ト8の第1の表面電極9a側にてに人体から放射
された赤外線に基づいて入射赤外線量に変化す
る。すると、ペレツト8の第1表面電極9a側に
て電荷が発生し、斯る電荷による信号が裏面電極
10、第2表面電極9bを介して第2引出線12
bから外部へ導出される。次いでペレツト8の第
2表面電極9b側にて入射赤外線量が変化する。
斯る場合も同様にして信号が第2引出線12bか
ら外部へ導出される。そして、これらの信号に基
づいて侵入警報器さら警報が発せられる。 When a human body passes through the front surface of the pyroelectric pellet 8 as shown by arrow A, the amount of incident infrared rays changes based on the infrared rays emitted from the human body on the first surface electrode 9a side of the pellet 8. . Then, a charge is generated on the first surface electrode 9a side of the pellet 8, and a signal due to the charge is transmitted to the second lead line 12 via the back surface electrode 10 and the second surface electrode 9b.
b to the outside. Next, the amount of incident infrared rays changes on the second surface electrode 9b side of the pellet 8.
In such a case, the signal is similarly led out from the second leader line 12b. Then, based on these signals, an intruder alarm is issued.
尚、上記ペレツト8は太陽光などからも同様に
赤外線を入射するが、この場合は何ら信号を出力
しない。即ち、太陽光などからの赤外線は等量に
してペレツト8全面に亘つて同時に入射して、ペ
レツト8の第1及び第2表面電極9a,9b側に
は等量の電荷が同時に発生し、従つて斯る電荷に
互いに相殺するので第2引出線12bからの信号
出力はない。 Incidentally, the pellet 8 receives infrared rays from sunlight as well, but in this case it does not output any signal. That is, an equal amount of infrared rays from sunlight etc. is simultaneously incident on the entire surface of the pellet 8, and equal amounts of charges are simultaneously generated on the first and second surface electrodes 9a and 9b of the pellet 8. Since the charges cancel each other out, there is no signal output from the second leader line 12b.
さて、斯る検出器にてポツプコーンノイズが発
生すると侵入警報器からは人体が侵入したものと
みなされて誤報が発せられる。そこで斯るポツプ
コーンノイズを抑制するるための実験及びその検
討を種々行なつた。その結果、ポツプコーンノイ
ズの発生は焦電体ペレツト8の表面電極9の総面
積(S1とする)に対する支持台13の接着支持部
の総面積(S2とする)の比率R(=S2/S1・100%)
に大きく起因することが分つた。 Now, if popcorn noise is generated in such a detector, the intruder alarm will assume that a human body has invaded and will issue a false alarm. Therefore, various experiments and studies were conducted to suppress such popcorn noise. As a result, the generation of popcorn noise is determined by the ratio R (= It was found that this was largely caused by S 2 /S 1・100%).
即ち、ポツプコーンノイズの電圧レベルは第6
図に示す通り、上記比率Rが8%以下の場合は略
第3図に示す如きホワイトノイズの電圧レベルW
(±300mV程度)以下で一定となり、8%を超え
ると漸次大きくなる。 That is, the voltage level of popcorn noise is 6th
As shown in the figure, when the ratio R is 8% or less, the white noise voltage level W is approximately as shown in FIG.
(approximately ±300 mV) or less, it becomes constant, and when it exceeds 8%, it gradually increases.
そこで、上記比率Rを略8%以下に抑えればポ
ツプコーンノイズの電圧ノベルはホワイトノイズ
の電圧レベル内に入り、実質的にポツプコーンノ
イズの発生を抑制できることが判明した。 Therefore, it has been found that if the ratio R is suppressed to approximately 8% or less, the voltage level of popcorn noise falls within the voltage level of white noise, and the generation of popcorn noise can be substantially suppressed.
一方、上記比率Rを余り小さくするとペレツト
8の接着支持が困難になる。更に、ペレツト8を
断熱してペレツト8の出力を増大するために、支
持台13の接着支持部以外においてペレツト8の
裏面電極10側と支持台13との間を空間とする
必要がある。この場合、上記第1及び第2引出面
12a,12bの超音波ボンデイング時の圧力
は、第1、第2パツド11a,11bを支持台1
3の接着支持部に対向して設けることにより、接
着剤14の介して支持台13にて受けるようにす
ればよい。ここに、上記比率Rが小さ過ぎると
(表面電極9の総面積S1を一定とする)、支持台1
3の接着支持部が小さくなるため、第1、第2パ
ツド11a,11bと接着支持部との位置を精度
良く合すことが困難となり、従つてボンデイング
時の圧力が上記空間部に伝わつてペレツト8が割
れてしまう場合が生じる。 On the other hand, if the ratio R is too small, it becomes difficult to adhesively support the pellets 8. Further, in order to increase the output of the pellet 8 by insulating the pellet 8, it is necessary to provide a space between the back electrode 10 side of the pellet 8 and the support 13 except for the adhesive support portion of the support 13. In this case, the pressure at the time of ultrasonic bonding of the first and second extraction surfaces 12a and 12b is such that the first and second pads 11a and 11b are
By providing it opposite to the adhesive support section 3, it may be received by the support base 13 via the adhesive 14. Here, if the ratio R is too small (assuming the total area S 1 of the surface electrode 9 is constant), the support base 1
Since the adhesive support part 3 becomes smaller, it becomes difficult to align the first and second pads 11a, 11b with the adhesive support part with high precision, and therefore the pressure during bonding is transmitted to the space part and the pellet is 8 may be broken.
而して、上記比率Rの最小限度を種々実験、検
討した結果、上記比率Rを略0.8%以上に確保す
るとペレツト8の接着支持を確実に行なうことが
できると共に、第1、第2引出線12a,12b
のボンデイング時にペレツト8が割れる危険性を
顕著に解消できることが判明した。 As a result of various experiments and studies on the minimum value of the ratio R, we found that if the ratio R is maintained at approximately 0.8% or more, the adhesive support of the pellet 8 can be reliably achieved, and the first and second leader lines 12a, 12b
It has been found that the risk of the pellets 8 breaking during bonding can be significantly eliminated.
故に、上記比率Rは略0.8〜8%の範囲に保た
ねばならない。 Therefore, the ratio R must be maintained within the range of approximately 0.8 to 8%.
ここに、上記第4図及び第5図に再び戻つて説
明するに、15,15,…は上記支持台13の上
面を酸エツチングすることにより4隅に形成され
た高さ約0.1〜0.2mmの1/4状支柱である。そして、
該支柱は上面だけ接着剤14を塗布した状態にし
て上記ペレツト8を接着支持していると共に、斯
る接着支持部以外においては上記ペレツト8の裏
面電極10側と支持台13との間に空間16が形
成されている。又、上記第1、第2パツド11
a,11bは2つの支柱15,15に対向してい
る。 Returning to FIGS. 4 and 5, 15, 15, ... are formed at the four corners by acid etching the upper surface of the support base 13, and have a height of approximately 0.1 to 0.2 mm. It is a quarter-shaped support. and,
The pillars adhesively support the pellets 8 with adhesive 14 applied only to their upper surfaces, and there is no space between the back electrode 10 side of the pellets 8 and the support base 13 except for the adhesive support portion. 16 are formed. In addition, the first and second pads 11
a, 11b are opposed to two pillars 15, 15.
即ち、上述の如き薄膜の焦電体ペレツト8上の
第1および第2パツド11a,11bに、この薄
膜を破損することなく、電極の引出線12a,1
2bの結合を行うには焦電体ペレツト8の裏面側
の引出線の接合部と対向する部分に、接合時の圧
力を十分支えるだけの支柱が必要であり、その役
割を支柱15,15が行つている。前述の如く引
出線12a,12bには直径30μmの金属細線が
用いられる。それ故、支柱15上面の面積は、後
述の如く半径0.1mmの円の面積の1/4(即ち、1/4
円弧の扇形)程度が最低必要である。 That is, the lead wires 12a, 1 of the electrodes are attached to the first and second pads 11a, 11b on the thin film pyroelectric pellet 8 as described above without damaging the thin film.
In order to perform the bonding as shown in FIG. 2b, it is necessary to have a support on the back side of the pyroelectric pellet 8 facing the connection part of the lead wire, which is sufficient to support the pressure during bonding. I'm going. As mentioned above, thin metal wires with a diameter of 30 μm are used for the lead wires 12a and 12b. Therefore, the area of the top surface of the support column 15 is 1/4 of the area of a circle with a radius of 0.1 mm (i.e., 1/4
The minimum required degree is the shape of a sector of a circular arc.
而して、上記第1、第2表面電極9a,9bの
縦寸法a及び横寸法bは夫々例えば2mm及び1mm
で、その総面積S1は4mm2であり、一方上記各支柱
15,15,…の半径rは例えば0.1mmで、接着
支持部の総面積S2はS2=4×(πr2×1/4)=4×
(π×0.1mm×0.1mm×1/4)=0.0314mm2、即ち、略
0.0314mm2である。従つて上記比率R(=S2/S1・100
%)は略0.8%となり上述の範囲(略0.8%〜8
%)に入つている。 The vertical dimension a and the horizontal dimension b of the first and second surface electrodes 9a and 9b are, for example, 2 mm and 1 mm, respectively.
The total area S 1 is 4 mm 2 , and the radius r of each of the pillars 15, 15, ... is, for example, 0.1 mm, and the total area S 2 of the adhesive support part is S 2 = 4 x (πr 2 x 1 /4)=4×
(π×0.1mm×0.1mm×1/4)=0.0314mm 2 , that is, approximately
It is 0.0314mm2 . Therefore, the above ratio R (=S 2 /S 1・100%) is approximately 0.8% and falls within the above range (approximately 0.8% to 8%).
%).
以上の説明から明らかな如く、本発明によれ
ば、表、裏面電極を有し入射赤外線変化量に応じ
て電荷を発生する焦電体ペレツト、該ペレツトを
上記裏面電極側にて接着支持台を備えた焦電型赤
外線検出器において、上記表面電極の総面積に対
する上記支持台の接着支持総面積の比率略0.8〜
8%の範囲とすると共に、上記支持台の接着支持
部以外にて上記ペレツトの裏面電極側と上記支持
台との間に空間を形成したから、ポツプコーンノ
イズの発生を実質的に抑制でき、且つ出力の増大
を図ることができ、更に上記ペレツト接着支持を
確実に行なうことができると共に、上記表面電極
上に引出線をボンデイングする場合に上記ペレツ
トが割れる危険性も殆どなく、よつて極めて信頼
性の高い焦電型赤外線検出器を提供できる。 As is clear from the above description, the present invention provides a pyroelectric pellet that has front and back electrodes and generates electric charge in accordance with the amount of change in incident infrared rays, and an adhesive support for attaching the pellet to the back electrode side. In the pyroelectric infrared detector equipped with the above, the ratio of the total adhesive support area of the support base to the total area of the surface electrode is approximately 0.8 to
8% range, and a space was formed between the back electrode side of the pellet and the support at a point other than the adhesive support part of the support, so the generation of popcorn noise could be substantially suppressed. Moreover, the output can be increased, the pellet can be reliably bonded and supported, and there is almost no risk of the pellet breaking when bonding a lead wire onto the surface electrode. A highly reliable pyroelectric infrared detector can be provided.
第1図及び第2図は従来の焦電型赤外線検出器
の正面図、第3図は第2図の検出器におけるポツ
プコーンノイズの発生状態を示す特性図、第4図
は本発明実施例焦電型赤外線検出器の斜視図、第
5図は同要部斜視図、第6図はポツプコーンノイ
ズレベルの変化状態を示す特性図である。
8……焦電体ペレツト、9a,9b……第1,
第2表面電極、10……裏面電極、13……支持
台。
Figures 1 and 2 are front views of a conventional pyroelectric infrared detector, Figure 3 is a characteristic diagram showing the popcorn noise generation state in the detector shown in Figure 2, and Figure 4 is a diagram showing the state of occurrence of popcorn noise in the detector of Figure 2. FIG. 5 is a perspective view of an example of a pyroelectric infrared detector, FIG. 5 is a perspective view of the main part thereof, and FIG. 6 is a characteristic diagram showing changes in the popcorn noise level. 8...Pyroelectric pellet, 9a, 9b...1st,
2nd surface electrode, 10... Back electrode, 13... Support stand.
Claims (1)
変化量に応じて電荷を発生するタンタル酸リチウ
ム等よりなり面積25mm2以下で厚さ約30〜100μm
の焦電体ペレツト8と、該ペレツトを上記裏面電
極10側にて接着支持する支持台13を備えた焦
電型赤外線検出器において、該支持台に複数個の
支柱15を設けると共に該支柱に対向する表面電
極10上の位置に信号引出線11a,11bを設
け、前記表面電極9の総面積S1と前記支持台に設
けられた複数個の支柱15上の接着支持総面積S2
(S2は0.03mm2以上)との比率(S2/S1)を略0.8〜
8%の範囲とすると共に、前記支柱上の接着支持
部以外にて前記ペレツトの裏面電極側と前記支持
台との間に空間16を形成したことを特徴とする
焦電型赤外線検出器。1 It has front and back electrodes 9 and 10 and is made of lithium tantalate, etc., which generates electric charge according to the amount of change in incident infrared rays, and has an area of 25 mm 2 or less and a thickness of approximately 30 to 100 μm.
In a pyroelectric infrared detector equipped with a pyroelectric pellet 8 of Signal lead lines 11a and 11b are provided at opposing positions on the surface electrodes 10, and the total area S1 of the surface electrodes 9 and the total adhesive support area S2 on the plurality of pillars 15 provided on the support base are
(S 2 is 0.03mm 2 or more) and the ratio (S 2 /S 1 ) is approximately 0.8 ~
8% range, and a space 16 is formed between the back electrode side of the pellet and the support base in a region other than the adhesive support portion on the pillar.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57066453A JPS58182522A (en) | 1982-04-20 | 1982-04-20 | Pyroelectric type infrared detector |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57066453A JPS58182522A (en) | 1982-04-20 | 1982-04-20 | Pyroelectric type infrared detector |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS58182522A JPS58182522A (en) | 1983-10-25 |
| JPH0359370B2 true JPH0359370B2 (en) | 1991-09-10 |
Family
ID=13316202
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP57066453A Granted JPS58182522A (en) | 1982-04-20 | 1982-04-20 | Pyroelectric type infrared detector |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS58182522A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| GB2174224B (en) * | 1985-04-15 | 1988-07-13 | Philips Electronic Associated | Infra-red intruder detection system |
| WO2006009174A1 (en) * | 2004-07-20 | 2006-01-26 | Murata Manufacturing Co., Ltd. | Infrared sensor and method for manufacturing same |
-
1982
- 1982-04-20 JP JP57066453A patent/JPS58182522A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS58182522A (en) | 1983-10-25 |
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