JPH0425485B2 - - Google Patents

Info

Publication number
JPH0425485B2
JPH0425485B2 JP58076758A JP7675883A JPH0425485B2 JP H0425485 B2 JPH0425485 B2 JP H0425485B2 JP 58076758 A JP58076758 A JP 58076758A JP 7675883 A JP7675883 A JP 7675883A JP H0425485 B2 JPH0425485 B2 JP H0425485B2
Authority
JP
Japan
Prior art keywords
infrared
bodies
vibrating
opposing
vibrating bodies
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
Application number
JP58076758A
Other languages
Japanese (ja)
Other versions
JPS59202036A (en
Inventor
Toshiaki Yokoo
Kenichi Shibata
Kosuke Takeuchi
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.)
Sanyo Electric Co Ltd
Original Assignee
Sanyo Electric 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 Sanyo Electric Co Ltd filed Critical Sanyo Electric Co Ltd
Priority to JP58076758A priority Critical patent/JPS59202036A/en
Publication of JPS59202036A publication Critical patent/JPS59202036A/en
Publication of JPH0425485B2 publication Critical patent/JPH0425485B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J5/00Radiation pyrometry, e.g. infrared or optical thermometry
    • G01J5/02Constructional details
    • G01J5/08Optical arrangements
    • G01J5/0803Arrangements for time-dependent attenuation of radiation signals
    • G01J5/0805Means for chopping radiation

Landscapes

  • 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】 (イ) 産業上の利用分野 本発明は例えば被検知部の温度を赤外線にて検
知するための赤外線検出器に関する。
DETAILED DESCRIPTION OF THE INVENTION (a) Field of Industrial Application The present invention relates to an infrared detector for detecting, for example, the temperature of a detected part using infrared rays.

(ロ) 従来技術 最近、第1図に示す如き赤外線検出器が提案さ
れている。
(b) Prior Art Recently, an infrared detector as shown in FIG. 1 has been proposed.

1は表、裏面電極2,3を有し、入射赤外線変
化量に応じて電荷を発生する、タンタル酸リチウ
ム(LiTaO3)単結晶からなる焦電型赤外線検出
体、4は燐青銅などからなる金属支持台、5は導
電接着剤、6は上記赤外線検出体1を外来ノイズ
に対してシールドするシールド体で、その前面に
は検出体1に対向して開口7が穿設されている。
1 is a pyroelectric infrared detector made of lithium tantalate (LiTaO 3 ) single crystal, which has front and back electrodes 2 and 3 and generates a charge according to the amount of change in incident infrared rays; 4 is made of phosphor bronze, etc. A metal support, 5 a conductive adhesive, 6 a shield body for shielding the infrared detector 1 from external noise, and an opening 7 facing the detector 1 is bored in its front surface.

8は金属性のキヤツプ9及びヘツダ10からな
る収納体で、該収納体内の上記ヘツダ10上には
上記支持台4が固定されている。11は上記ヘツ
ダ10に直接植設され、上記支持台4及び接着剤
5を介して上記裏面電極3に電気的に連なるアー
ス端子、12は上記ヘツダ10に絶縁材を介して
植設され、上記表面電極2に電気的に連なり、上
記検出体1に発生した電荷を外部へ取出すための
信号端子、13は上記検出体1に表面電極2側か
ら赤外線を入射せしめるべく上記キヤツプ9の前
面に穿設された開口、14は該開口を閉塞する赤
外線透過フイルタである。
Reference numeral 8 denotes a storage body consisting of a metal cap 9 and a header 10, and the support base 4 is fixed on the header 10 inside the storage body. Reference numeral 11 is a ground terminal that is directly implanted in the header 10 and is electrically connected to the back electrode 3 via the support base 4 and adhesive 5; A signal terminal 13 is electrically connected to the surface electrode 2 and is used to take out the electric charge generated in the detection object 1 to the outside. A signal terminal 13 is provided on the front surface of the cap 9 to allow infrared rays to enter the detection object 1 from the surface electrode 2 side. The provided opening 14 is an infrared transmission filter that closes the opening.

15は上記収納体8内に配置され、上記開口1
3を通過する収納体8外の被検知部からの赤外線
を断続するための断続手段である。該断続手段に
おいて、16,17は上記検出体1への赤外線の
入射域、即ち上記検出体1と開口13との間に互
いに平行にして配置された平面状の第1、第2対
向体である。斯る第1、第2対向体16,17は
夫々第2図a及びbに示す如く、アルミニウムな
どの赤外線非透過材料からなり紙面にほぼ平行な
方向(第1図)にて扇形線状に延設された複数の
第1赤外線非透過部18,18…及び第2赤外線
非透過部19,19…が形成され、そして斯る第
1赤外線非透過部18,18…の各々の間及び第
2赤外線非透過部19,19…の各々の間には
夫々第1赤外線透過部20,20…及び第2赤外
線透過部21,21…が形成されている。上記非
透過部18,18…及び19,19…と上記透過
部20,20…及び21,21…共に同一寸法形
状であり、幅W1、W2は夫々100μm、120μmであ
る。
15 is arranged in the storage body 8, and the opening 1
3 is an intermittent means for intermittent infrared rays from a detected portion outside the storage body 8 that passes through the infrared rays. In the disconnection means, 16 and 17 are planar first and second opposing bodies arranged in parallel to each other in the incident area of the infrared rays to the detection body 1, that is, between the detection body 1 and the opening 13. be. As shown in FIGS. 2a and 2b, these first and second opposing bodies 16 and 17 are made of an infrared opaque material such as aluminum, and are arranged in a fan-shaped linear shape in a direction substantially parallel to the plane of the paper (FIG. 1). A plurality of extended first infrared non-transmissive parts 18, 18... and second infrared non-transmissive parts 19, 19... are formed, and between each of the first infrared non-transparent parts 18, 18... A first infrared transmitting section 20, 20... and a second infrared transmitting section 21, 21... are formed between each of the two infrared non-transmitting sections 19, 19.... The non-transmissive parts 18, 18, . . . and 19, 19 , . . . and the transparent parts 20, 20, .

22は上記第1対向体16を振動せしめるため
の第1振動体で、該振動体の後方(第1図)には
第3図に示す如く上記第2対向体17を振動せし
めるための第2振動体23が配置されている。斯
る第1、第2振動体22,23の構成は次の通り
である。即ち、燐青銅、ステンレスなどから導電
体が中央電極24となり、斯る電極24の両側に
は、チタン酸バリウム、ジルコン酸チタン酸鉛な
どからなり分極された圧電体25が、その分極方
向(矢印P)が同一となるように配置され、そし
て上記圧電体25の片側表面には銀などからなる
表面電極26が形成されている。上記第1、第2
対向体16,17は夫々第1、第2振動体22,
23の右端に絶縁性の第1、第2基台27,28
を介して取着されている。
Reference numeral 22 denotes a first vibrating body for vibrating the first opposing body 16, and behind the vibrating body (FIG. 1) there is a second vibrating body for vibrating the second opposing body 17 as shown in FIG. A vibrating body 23 is arranged. The configurations of the first and second vibrating bodies 22 and 23 are as follows. That is, a conductor made of phosphor bronze, stainless steel, etc. serves as the central electrode 24, and on both sides of the electrode 24, polarized piezoelectric materials 25 made of barium titanate, lead zirconate titanate, etc. are placed in the direction of polarization (arrow). P) are arranged to be the same, and a surface electrode 26 made of silver or the like is formed on one surface of the piezoelectric body 25. 1st and 2nd above
The opposing bodies 16 and 17 are the first and second vibrating bodies 22,
Insulating first and second bases 27 and 28 are placed on the right end of 23.
It is attached via.

29,30は夫々上記ヘツダ10上に絶縁層3
1を介して配置され、上記第1、第2振動体2
2,23を固定支持し、各振動体22,23の表
面電極26,26と電気的に連なる金属性の第
1、第2固定台、32,33は夫々上記ヘツダ1
0に絶縁材を介して植設された第1、第2振動端
子で、該第1振動端子には上記第1振動体22の
中央電極24及び上記第2固定台30が接続さ
れ、上記第2振動端子33には上記第1固定台2
9及び上記第2振動体23の中央電極24が接続
されている。
29 and 30 are insulating layers 3 on the header 10, respectively.
1 and the first and second vibrating bodies 2
2, 23, and are electrically connected to the surface electrodes 26, 26 of each vibrating body 22, 23.
The center electrode 24 of the first vibrating body 22 and the second fixing base 30 are connected to the first vibrating terminal, and the first vibrating terminal is connected to the first vibrating terminal 24 and the second fixing base 30. 2. The first fixed base 2 is attached to the second vibration terminal 33.
9 and the center electrode 24 of the second vibrating body 23 are connected.

而して、上記第1振動端子32には−20Vの一
定電圧が印加され、上記第2振動端子33には±
10Vの電圧が交互に周期的に印加される。
A constant voltage of -20V is applied to the first vibration terminal 32, and a voltage of ±20V is applied to the second vibration terminal 33.
A voltage of 10V is applied alternately and periodically.

斯る+10Vの電圧の印加時には、上記第1振動
体22においては外側の圧電体25が縮むと共に
内側の圧電体25が伸び、従つて第1振動体22
は、矢印a方向に撓む。又、上記第2振動体23
においては内側の圧電体25が伸びると共に外側
の圧電体25が縮み、従つて第2振動体23は矢
印b方向に撓む。
When such a voltage of +10V is applied, the outer piezoelectric body 25 of the first vibrating body 22 contracts and the inner piezoelectric body 25 expands, so that the first vibrating body 22
is bent in the direction of arrow a. Moreover, the second vibrating body 23
In this case, the inner piezoelectric body 25 expands and the outer piezoelectric body 25 contracts, so that the second vibrating body 23 bends in the direction of arrow b.

一方、第2振動端子33に−10Vの電圧が印加
されると、第1、第2振動体22,23は夫々上
述とは逆にb、a方向に撓む。
On the other hand, when a voltage of -10V is applied to the second vibrating terminal 33, the first and second vibrating bodies 22 and 23 bend in directions b and a, respectively, contrary to the above description.

これにより、上記第1、第2振動体22,23
は互いに逆方向に周期的に振動し、斯る振動に基
づいて、第1対向体16の第1赤外線透過部2
0,20…及び第1赤外線非透過部18,18…
と第2対向体17の第2赤外線非透過部19,1
9…及び第2赤外線透過部21,21…が夫々重
畳する状態と、赤外線透過部20,20…,2
1,21…どうし及び赤外線非透過部18,18
…,19,19…どうしが重畳する状態とが、交
互に繰返され、即ち開口13を通過した外部の被
検知部からの赤外線が検出体1に断続的に入射
し、従つて検出体1は入射赤外線量が変化し、被
検知部の温度に応じた電荷を発生する。
As a result, the first and second vibrating bodies 22, 23
vibrate periodically in opposite directions, and based on such vibrations, the first infrared transmitting portion 2 of the first opposing body 16
0, 20... and the first infrared non-transmissive portions 18, 18...
and the second infrared opaque portion 19,1 of the second opposing body 17.
9... and the second infrared transmitting sections 21, 21... overlap each other, and the infrared transmitting sections 20, 20..., 2
1, 21... and infrared non-transmissive parts 18, 18
..., 19, 19... are repeated alternately, that is, the infrared rays from the external detected part that has passed through the opening 13 are intermittently incident on the detection object 1, and therefore the detection object 1 is The amount of incident infrared rays changes, generating a charge depending on the temperature of the detected part.

ところで、上記第1、第2振動体22,23は
中央電極24に対して完全に対称構造となるもの
が最も好ましい。即ち、この様な構造の場合、中
央電極24両側の夫々の構造の平均熱膨脹係数が
同一となり、これにより周囲温度が変化しても斯
る変化に基づいて第1、第2振動体22,23が
同様に伸縮するから不所望に撓むことがない。そ
して、この様な撓みのない状態においては、第
1、第2振動体22,23の振動に際し上述の2
つの重畳が確実に繰返されて、赤外線断続が確実
に行なわれ、これにより検出体1から被検知部の
温度に応じた所望の電荷が発生され、精度良い温
度測定が行なえるのである。
By the way, it is most preferable that the first and second vibrating bodies 22 and 23 have a completely symmetrical structure with respect to the center electrode 24. That is, in the case of such a structure, the average coefficient of thermal expansion of the respective structures on both sides of the center electrode 24 is the same, so that even if the ambient temperature changes, the first and second vibrating bodies 22, 23 Since it expands and contracts in the same way, it will not bend undesirably. In such a state where there is no deflection, when the first and second vibrating bodies 22 and 23 vibrate, the above-mentioned two
The two superimpositions are reliably repeated, and infrared rays are reliably switched on and off, thereby generating a desired charge from the detection object 1 in accordance with the temperature of the detected part, allowing highly accurate temperature measurement.

しかるに、上述の如き完全な対称構造を得るこ
とは実際甚だ困難であり、例えば中央電極24両
側の圧電体25及び表面電極26の厚みを精度良
く一致させることが困難であり、すると中央電極
24両側の構造の平均熱膨脹係数が異なることと
なり、この場合第1、第2振動体22,23は周
囲温度の変化に基づいて不所望に撓んでしまう。
However, it is actually extremely difficult to obtain a completely symmetrical structure as described above. For example, it is difficult to match the thickness of the piezoelectric body 25 and the surface electrode 26 on both sides of the center electrode 24 with high accuracy. The average coefficients of thermal expansion of the structures will be different, and in this case, the first and second vibrating bodies 22 and 23 will undesirably flex due to changes in ambient temperature.

而して、上記赤外線検出器においては、第1、
第2振動体22,23が周囲温度変化により撓ん
でも、第1、第2対抗体16,17の相互関係が
上述の如き撓みがない場合と較べてあまり変わら
ないように、第1、第2振動体22,23は周囲
温度変化に伴なつて同一方向a又はbに同程度に
撓むようなものが選択されている。しかし乍ら、
周囲温度変化による第1、第2振動体22,23
の撓みにおいて、第1、第2対向体16,17の
相互関係は実際は第4図に詳細に示す如くずれ
る。
Therefore, in the above-mentioned infrared detector, the first,
Even if the second vibrating bodies 22 and 23 are deflected due to changes in ambient temperature, the mutual relationship between the first and second opposing bodies 16 and 17 does not change much compared to the case where there is no deflection as described above. The two vibrating bodies 22 and 23 are selected so that they bend to the same extent in the same direction a or b as the ambient temperature changes. However,
The first and second vibrating bodies 22, 23 due to changes in ambient temperature
In this deflection, the mutual relationship of the first and second opposing bodies 16, 17 actually shifts as shown in detail in FIG.

即ち、第1、第2振動体22,23は夫々その
支点としての第1、第2固定台29,30がヘツ
ダ10上で離間しているために、第1、第2振動
体22,23が周囲温度変化により例えばa方向
に実線の位置から破線の位置に撓むと、第1、第
2対向体16,17はその中央線C,C′を参照す
ると寸法lだけずれてしまう。
That is, since the first and second fixed bases 29 and 30 serving as fulcrums of the first and second vibrating bodies 22 and 23 are spaced apart on the header 10, the first and second vibrating bodies 22 and 23 When the first and second opposing bodies 16, 17 are deflected by a dimension l when referring to their center lines C and C', for example, if the deflection occurs in the direction a from the position indicated by the solid line to the position indicated by the broken line due to a change in ambient temperature.

ここに、斯るずれが生じた状態においては、第
1、第2振動体22,23の振動に際し、上述の
如き2つの重畳が確実に行なわれないので、赤外
線断続が確実に行なわれず、これにより検出体1
から被検知部の温度に応じた所望とする電荷が発
生されず、精度良い温度測定が行なえない。
In a state where such a deviation occurs, the above-mentioned two superpositions cannot be reliably performed when the first and second vibrating bodies 22 and 23 vibrate, so the infrared rays cannot be intermittent reliably. Detected object 1
Therefore, a desired charge corresponding to the temperature of the detected part is not generated, and accurate temperature measurement cannot be performed.

(ハ) 発明の目的 本発明は、赤外線断続が確実に行なわれるよう
にして、例えば温度測定においては斯る温度測定
が精度良く行なえる様にすることを目的とする。
(C) Object of the Invention The object of the present invention is to ensure that infrared rays are intermittent, so that, for example, in temperature measurement, such temperature measurement can be performed with high accuracy.

(ニ) 発明の構成 本発明赤外線検出器は、上記目的を達成すべ
く、入射赤外線変化量に応じて電荷を発生する赤
外線検出体、該検出体への赤外線入射域に配置さ
れ赤外線透過部及び赤外線非透過部を共に有する
第1、第2対向体、該第1対向体の赤外線透過部
及び赤外線非透過部と上記第2対向体の赤外線非
透過部及び赤外線透過部が夫々重畳する状態と、
上記第1、第2対向体の赤外線透過部どうし及び
赤外線非透過部どうしが重畳する状態とを交互に
繰返せしめるべく、上記第1、第2対向体を各々
振動せしめる第1、第2振動体を備え、該第1、
第2振動体における各々の振動方向に垂直な面が
同一平面上に位置するように、上記第1、第2振
動体を配置したことを特徴とする。
(d) Structure of the Invention In order to achieve the above object, the infrared detector of the present invention comprises: an infrared detecting body that generates an electric charge according to the amount of change in incident infrared light; an infrared transmitting part disposed in the infrared incident area to the detecting body; first and second opposing bodies both having an infrared non-transmissive part; a state in which the infrared transparent part and the infrared non-transmissive part of the first opposing body overlap with the infrared non-transmissive part and the infrared transmissive part of the second opposing body, respectively; ,
First and second vibrations that vibrate the first and second opposing bodies, respectively, in order to alternately repeat a state in which the infrared transmitting parts and the non-infrared transmitting parts of the first and second opposing bodies overlap each other. comprising a body, the first;
The first and second vibrating bodies are arranged such that the surfaces perpendicular to the vibration directions of the second vibrating bodies are located on the same plane.

(ホ) 実施例 以下本発明実施例赤外線検出器を第5図及び第
6図に基づいて説明する。尚、従来例と同一部分
には同一符号を記してその説明を省略する。
(e) Embodiment An infrared detector according to an embodiment of the present invention will be described below with reference to FIGS. 5 and 6. Incidentally, the same parts as in the conventional example are denoted by the same reference numerals, and the explanation thereof will be omitted.

34,35は夫々右側の下端及び上端に取付け
られた第1、第2対向体16,17を周期的に振
動せしめるための第1、第2振動体で、該第1、
第2振動体はその圧電体25が各々P,P′方向に
分極されている以外は従来のものと同様である。
36は、上記第1、第2振動体34,35におけ
る各々の振動方向a,bに垂直な面、A,Bが同
一平面上に位置するように、上記第1、第2振動
体34,25を固定支持するための金属性の固定
台であり、上記第1振動端子32には第1、第2
振動体34,35の中央電極24が接続され、上
記第2振動端子33には上記固定台36が接続さ
れている。
Reference numerals 34 and 35 denote first and second vibrating bodies for periodically vibrating the first and second opposing bodies 16 and 17 attached to the lower and upper ends of the right side, respectively;
The second vibrating body is similar to the conventional one except that its piezoelectric body 25 is polarized in the P and P' directions, respectively.
36 is a plane perpendicular to the vibration directions a and b of the first and second vibrating bodies 34 and 35, respectively, so that A and B are located on the same plane. 25, and the first vibration terminal 32 has first and second vibration terminals.
The center electrodes 24 of the vibrating bodies 34 and 35 are connected, and the second vibration terminal 33 is connected to the fixing base 36.

而して、第1振動端子32には−20Vの一定電
圧が印加され、上記第2振動端子33には±10V
の電圧が交互に印加される。
Thus, a constant voltage of -20V is applied to the first vibration terminal 32, and a voltage of ±10V is applied to the second vibration terminal 33.
voltages are applied alternately.

斯る+10Vの電圧印加時には、第1、第2振動
体34,35は各々a,b方向に撓み、−10Vの
電圧印加時には、第1、第2振動体34,35は
各々b,a方向に撓み、これにより第1、第2振
動体34,35は従来と同様に周期的に振動し、
赤外線断続が行なわれる。
When a voltage of +10V is applied, the first and second vibrating bodies 34 and 35 bend in directions a and b, respectively, and when a voltage of -10V is applied, the first and second vibrating bodies 34 and 35 bend in directions b and a, respectively. As a result, the first and second vibrating bodies 34 and 35 vibrate periodically as in the conventional case,
Infrared intermittent is performed.

ここに、第1、第2振動体34,35は夫々そ
の支点が固定台36にて同一直線上に存在し縦に
重なつているから、第1、第2振動体34,35
が周囲温度変化により撓んでも、それにより第
1、第2対向体16,17の両者間にずれが生じ
ることはない。
Here, since the fulcrums of the first and second vibrating bodies 34 and 35 are on the same straight line at the fixed base 36 and are vertically overlapped, the first and second vibrating bodies 34 and 35
Even if the first and second facing bodies 16 and 17 are bent due to a change in ambient temperature, this will not cause any misalignment between the first and second opposing bodies 16 and 17.

従つて、斯る撓みが生じた状態において、第
1、第2振動体34,35の振動に際し、確実な
赤外線断続が行なわれ、検出体1から被検知部の
温度に応じた所望とする電荷が発生される。
Therefore, in a state where such deflection occurs, when the first and second vibrating bodies 34 and 35 vibrate, infrared rays are reliably interrupted, and a desired charge is emitted from the detecting body 1 according to the temperature of the detected part. is generated.

(ヘ) 発明の効果 以上の説明から明らかな如く、本発明によれ
ば、周囲温度変化が生じても赤外線断続を確実に
行なうことができるから、例えば温度測定におい
ては、それを精度良く行なうことができる。
(f) Effects of the Invention As is clear from the above explanation, according to the present invention, infrared rays can be reliably interrupted even if the ambient temperature changes, so that it can be performed with high accuracy, for example, in temperature measurement. I can do it.

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

第1図は最近提案された赤外線検出器の断面
図、第2図a,bは夫々同検出器の第1、第2対
向体の平面図、第3図は同検出器を第1図におい
て矢印方向から見た要部平面図、第4図は同検
出器の断続手段の動作を説明するための要部平面
図、第5図は本発明実施例赤外線検出器の断面
図、第6図は同検出器を矢印方向から見た要部
平面図である。 1……焦電型赤外線検出体、16,17……第
1、第2対向体、34,35……第1、第2振動
体。
Figure 1 is a cross-sectional view of a recently proposed infrared detector, Figures 2a and b are plan views of the first and second opposing bodies of the detector, respectively, and Figure 3 shows the same detector as in Figure 1. FIG. 4 is a plan view of the main part as seen from the direction of the arrow; FIG. 4 is a plan view of the main part for explaining the operation of the disconnection means of the detector; FIG. 5 is a sectional view of the infrared detector according to the embodiment of the present invention; FIG. is a plan view of the main part of the same detector as seen from the direction of the arrow. 1... Pyroelectric infrared detector, 16, 17... First and second opposing bodies, 34, 35... First and second vibrating bodies.

Claims (1)

【特許請求の範囲】[Claims] 1 入射赤外線変化量に応じて電荷を発生する赤
外線検出体、該検出体への赤外線入射域に配置さ
れ赤外線透過部及び赤外線非透過部を共に有する
第1、第2対向体、該第1対向体の赤外線透過部
及び赤外線非透過部と上記第2対向体の赤外線非
透過部及び赤外線透過部が夫々重畳する状態と、
上記第1、第2対向体の赤外線透過部どうし及び
赤外線非透過部どうしが重畳する状態とを交互に
繰返せしめるべく、上記第1、第2対向体を各々
振動せしめる第1、第2振動体を備え、該第1、
第2振動体における各々の振動方向に垂直な面が
同一平面上に位置するように、上記第1、第2振
動体を配置したことを特徴とする赤外線検出器。
1. An infrared detecting body that generates a charge according to the amount of change in incident infrared rays, first and second opposing bodies that are arranged in an infrared incident area to the detecting body and have both an infrared transmitting part and an infrared non-transmitting part, and the first opposing body. a state in which the infrared transparent part and the infrared non-transparent part of the body and the infrared non-transparent part and the infrared transparent part of the second opposing body overlap, respectively;
First and second vibrations that vibrate the first and second opposing bodies, respectively, in order to alternately repeat a state in which the infrared transmitting parts and the non-infrared transmitting parts of the first and second opposing bodies overlap each other. comprising a body, the first;
An infrared detector characterized in that the first and second vibrating bodies are arranged so that surfaces perpendicular to the vibration directions of the second vibrating bodies are located on the same plane.
JP58076758A 1983-04-30 1983-04-30 Infrared ray detector Granted JPS59202036A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58076758A JPS59202036A (en) 1983-04-30 1983-04-30 Infrared ray detector

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58076758A JPS59202036A (en) 1983-04-30 1983-04-30 Infrared ray detector

Publications (2)

Publication Number Publication Date
JPS59202036A JPS59202036A (en) 1984-11-15
JPH0425485B2 true JPH0425485B2 (en) 1992-05-01

Family

ID=13614483

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58076758A Granted JPS59202036A (en) 1983-04-30 1983-04-30 Infrared ray detector

Country Status (1)

Country Link
JP (1) JPS59202036A (en)

Also Published As

Publication number Publication date
JPS59202036A (en) 1984-11-15

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