JPS59202036A - Infrared ray detector - Google Patents

Infrared ray detector

Info

Publication number
JPS59202036A
JPS59202036A JP58076758A JP7675883A JPS59202036A JP S59202036 A JPS59202036 A JP S59202036A JP 58076758 A JP58076758 A JP 58076758A JP 7675883 A JP7675883 A JP 7675883A JP S59202036 A JPS59202036 A JP S59202036A
Authority
JP
Japan
Prior art keywords
infrared
bodies
vibrating
transmitting section
opposing
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.)
Granted
Application number
JP58076758A
Other languages
Japanese (ja)
Other versions
JPH0425485B2 (en
Inventor
Toshiaki Yokoo
横尾 敏昭
Kenichi Shibata
賢一 柴田
Kosuke Takeuchi
孝介 竹内
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
Sanyo Denki Co Ltd
Original Assignee
Sanyo Electric Co Ltd
Sanyo Denki 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, Sanyo Denki 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

    • 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
    • G01J5/02—Constructional details
    • G01J5/08—Optical arrangements
    • G01J5/0803—Arrangements for time-dependent attenuation of radiation signals
    • G01J5/0805—Means 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)

Abstract

PURPOSE:To improve the accuracy in the temperature measurement by arranging first and second vibrators for vibrating first and second opposed bodies each having an infrared rays transmitting section and non-transmitting section so that respective surfaces thereof vertical to the directions of vibration are positioned on the same plane. CONSTITUTION:First and second opposed bodies 16 and 17 are arranged in an infrared rays incident area and each have an infrared rays transmitting section and non-transmitting section. The first and second opposed bodies are vibrated cyclically with first and second vibrators 34 and 35 in such a manner as to repeat the state of the infrared rays transmitting section and the non- transmitting section of the first opposed body overlapping the non-transmitting section and the transmitting section of the second opposed body respectively and the state of the transmitting sections and non-transmitting sections thereof overlapping each other alternately. The first and second vibrators 34 and 35 are arranged on a fixed based 36 so that surfaces A and B of the first and second vibrators 34 and 35 vertical to the directions (a) and (b) of vibration respectively are positioned on the same plane to prevent possible deviation between the first and second opposed bodies 16 and 17.

Description

【発明の詳細な説明】 (イJ 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 Field of the Invention The present invention relates to an infrared detector for detecting, for example, the temperature of a detected part using infrared rays.

(口]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
。
(Example) 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
(LiTa05J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
C二対してシールドするシールド体で、その前面≦二は
検出体(m: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 (LiTa05J 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 a metal support made of phosphor bronze, etc., (5) is a conductive adhesive, and (6) is a shield body that shields the infrared detector (1) from external noise C2, the front surface of which is Detection body (m: Opposed openings (7) are formed.

(8)は金属性のキャップ(9)及びヘッダ(10)か
らなる収納体で、該収納体内の上記ヘッダ<10)上に
二は上記支持台(4)が固定されている。(11)は上
記ヘッダ(10)≦二直接植設され、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は上記へラダ00)に絶縁
材を介して植設され、上記表面電極(2)に電気的g二
連なり、上記検出体(11に発生した電荷を外部へ取出
すための信号端子、a9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ャップ(
9)の前面l二穿設された開口、0釘ま該開口を閉塞す
る赤外線透過フィルタである。
(8) is a storage body consisting of a metal cap (9) and a header (10), and the support stand (4) is fixed on the header (<10) inside the storage body. (11) is directly planted on the header (10)≦2, and the support base (4)
and a ground terminal that is electrically connected to the back electrode (3) via an adhesive (5), (12 is installed on the ladder 00 above) via an insulating material, and is electrically connected to the front electrode (2). g, a signal terminal for extracting the electric charge generated on the detection body (11) to the outside;
9) is an infrared transmission filter that closes the two openings on the front surface and the openings.

(15)は上記収納体(8)内C配置さ几、上記開口α
J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(二おいて
、(L6)、(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)と開口住粉との間に互い
に平行C二して配置された平面状の第1、第2対向体で
ある。
(15) is the container C located inside the storage body (8), and the opening α
This is an intermittent means for intermittent infrared rays from a detected part outside the storage body (8) passing through J. The intermittent means (2, (L6) and (17) are arranged parallel to each other in the incident area of the infrared rays to the detecting body (1), that is, between the detecting body (1) and the open housing powder. The first and second opposing bodies are arranged in a planar shape.

斯る第1、第2対向体(L6)、(I7)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l二はぼ平行な方向(第1図1二て扇
形線状に延設された複数の第1亦外線非透過部αa、吐
・・・及び第2赤外線非透過部(11、C1l・・・が
形成され、そして斯る第1赤外線非透過部叫、αa・・
・の各々の間及び第2赤外線非透過部旧e、 C19−
・・の各々の間には夫々第1赤外線透過部(20)、(
201・・・及び第2赤外線透過部(211%(211
・・・が形成されている。上記非透過部αg、(181
・・・及び(19、C9・・・と上記透過部(20)、
t2G・・・及び(21)、 (211・・・は共に同
一寸法形状であり、幅Wl、W2は夫々100/Im、
120.amである。
The first and second opposing bodies (L6) and (I7) are made of an infrared non-transparent material such as aluminum, as shown in FIGS. 2a and 2b, respectively. Second, a plurality of first infrared non-transmissive portions αa, discharge, etc. and second infrared non-transmissive portions (11, C1l, etc.) extending in a fan-shaped linear shape are formed, and the first infrared non-transmissive portions (11, C1l, . Transparent part shout, αa...
・ between each and the second infrared non-transmissive part old e, C19-
The first infrared transmitting portion (20), (
201... and the second infrared transmitting part (211% (211
... is formed. The non-transparent part αg, (181
... and (19, C9... and the above-mentioned transparent part (20),
t2G... and (21), (211... both have the same dimensions and shape, and the widths Wl and W2 are respectively 100/Im,
120. It is am.

(22)は上記第1対向体(L61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
1二示す如く上記第2対向体αのを振動せしめるための
第2振動体(ハ)が配置されている。斯る第1、第2振
動体(2り、(ハ)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なる導電体が中央電極C2勾
となり、斯る電極(24)の両側i二は、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(ホ)が、その分極方向(矢印PJが同一となるよ
うl二装置され、そして上記圧電体(2最の片側表面(
二は銀などからなる表面電極(ハ)が形成されている。
(22) is a first vibrating body for vibrating the first opposing body (L61), and behind the vibrating body (FIG. 1) is a vibrating body for vibrating the second opposing body α as shown in FIG. A second vibrating body (c) is arranged to vibrate the vibration. The structure of the first and second vibrating bodies (c) is as follows. The conductor becomes the central electrode C2, and on both sides of the electrode (24) are polarized piezoelectric materials (e) made of barium titanate, lead zirconate titanate, etc. The piezoelectric body (the uppermost surface of the piezoelectric body) is
Second, a surface electrode (c) made of silver or the like is formed.

上記第1、第2対向体06)、αη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0η、(2紛を介して取着されている。
The first and second opposing bodies 06) and αη are respectively attached to the right ends of the first and second vibrating bodies (22+, (23+) through insulating first and second bases 0η, (2). ing.

(29)、(7)は夫々上記ヘッダ(10)上に二絶縁
層c1υを介して配置され、上記第1、第2振動体(2
4、(ハ)を固定支持し、各振動体(22、關の表面電
極(2e、(2E9と電気的(二連なる金属性の第1、
第2固定台、□□□、田は夫々上記ヘッダaα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(221の中央電極t2(イ)
及び上記第2固定台−が接続され、上記第2振動端子1
33には上記第1固定台C29)及び上記第2振動体の
の中央電極(ハ)が接続されている。
(29) and (7) are respectively arranged on the header (10) via two insulating layers c1υ, and the first and second vibrating bodies (2
4. (c) is fixedly supported, and electrically connected to the surface electrodes (2e, (2E9) of each vibrating body (22,
The second fixed base, □□□, and field are first and second vibration terminals respectively implanted in the header aα via an insulating material, and the first vibration terminal is connected to the center of the first vibrator (221). Electrode t2 (a)
and the second fixed base are connected, and the second vibration terminal 1
33 is connected to the first fixing base C29) and the center electrode (C) of the second vibrating body.

而して、上記第1振動端子に)には−20Vの一定電圧
が印加され、上記第2振動端子時には+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, and a voltage of +10V is alternately and periodically applied to the second vibration terminal.

斯る+10Vの電圧の印加時Cは、上記第1振動体(2
21においては外側の圧電体(2■が縮むと共に内側の
圧電体(2四が伸び、従って第1振動体(2鼾マ、矢印
a方向≦二撓む。又、上記$2振動体(Zii二おいて
は内側の圧電体(ハ)が伸びると共に外側の圧電体12
5)が縮み、従って第2振動体(ハ)は矢印す方向C撓
む。
When a voltage of +10V is applied, C is applied to the first vibrating body (2).
In 21, the outer piezoelectric body (2) contracts and the inner piezoelectric body (24) expands, so the first vibrating body (2 snores, direction of arrow a≦2 deflections. Also, the above $2 vibrating body (Zii) In the second case, the inner piezoelectric body (c) extends and the outer piezoelectric body 12
5) is contracted, and therefore the second vibrating body (C) is bent in the direction of the arrow C.

一方、第2振動端子に)に−1ovの電圧が印加される
と、第1、第2振動体(2力、(ハ)は夫々上述とは逆
にす、a方向に撓む。
On the other hand, when a voltage of -1 ov is applied to the second vibrating terminal, the first and second vibrating bodies bend in the direction a, where (c) is the opposite of the above.

これにより、上記第1、第2振動体(2り、(ハ)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aeの第1赤外線透過部(2o)、翰・・・及
び第1赤外線非透過部(181,(1s・・・と第2対
向体(17)の第2赤外線非透過部(L■、翰・・・及
び第2赤外線透過部(21)、(7!D・・・が夫々重
畳する状態と、赤外線透過部(2U)、(2■・・・、
圓、(21)・・・どうし及び赤外線非透過部(2)、
αa・・・、α■、0・・・どうしが重畳する状態とが
、交互C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(111=断続的に入射し
、従って検出体(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 (2, (c) vibrate periodically in opposite directions to each other, and based on such vibrations, the first infrared transmitting part (2o) of the first opposing body ae , Kanji... and the first infrared non-transmissive part (181, (1s...) and the second infrared non-transmissive part (L) of the second opposing body (17), Kanji... and the second infrared transmissive part ( 21), (7!D... are superimposed on each other, and the infrared transmitting part (2U), (2■...,
En, (21)... and infrared non-transparent part (2),
The state in which αa..., α■, 0... are superimposed is repeated alternately C, that is, the infrared rays from the external detected part that have passed through the aperture (13) are intermittently incident on the detection object (111 = Therefore, the amount of incident infrared rays on the detecting body (1) changes, and an electric charge is generated depending on the temperature of the detected part.

ところで、上記第1、第2振動体(221,Q:4t−
x中央電極(2狛二対して完全に対称構造となるのが最
も好ましい。即ち、この様な構造の場合、中央電極04
)両側の夫々の構造の平均熱膨張係数が同一となり、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振動体の、(2(至)が同様【二伸縮するから不
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+、困の振動に
際し上述の2つの重畳が確実C二繰返さ几て、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, the first and second vibrating bodies (221, Q: 4t-
x central electrode (2. It is most preferable to have a completely symmetrical structure with respect to 2. In other words, in such a structure, the central electrode 04
) The average coefficient of thermal expansion of the respective structures on both sides is the same, so that even if the ambient temperature changes, the first
, of the second vibrating body (2 (to)) similarly expands and contracts, so it does not bend undesirably.In a state where there is no such deflection, the first and second vibrating bodies (22+, When the vibration occurs, the above-mentioned two superpositions are reliably repeated twice, and infrared rays are reliably interrupted, thereby generating a desired charge from the detection object (1) according to the temperature of the detected part, with high accuracy. Temperature measurements can be performed.

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04)両側の圧電体C
251及び表面電極(26)の厚みを積置良く一致させ
ることが困難であり、すると中央電極(2)両側の構造
の平均熱膨張係数が異なることとなり、この場合法1、
第2振動体器、(ハ)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 extremely difficult to obtain a completely symmetrical structure as described above.
It is difficult to match the thicknesses of 251 and the surface electrode (26) well, and the average coefficient of thermal expansion of the structures on both sides of the center electrode (2) will be different.
The second vibrating body (c) undesirably bends due to changes in ambient temperature.

而して、上記赤外線検出器(二おいては、第1、第2振
動体(22)、(23)が周囲温度変化g:より撓んで
も、第1、第2対向体(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(2L (23+は周囲温度変
化C伴なって同一方向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l二よ
る第1、第2振動体(22+、(23)の撓み5二おい
て、第1、第2対向体u6)、0ηの相互関係は実際は
第4図に詳細に示す如くずれる。
Therefore, even if the first and second vibrating bodies (22), (23) of the infrared detector (2) are bent due to changes in the ambient temperature, the first and second opposing bodies (16), The first and second vibrating bodies (2L (23+) are to the same extent in the same direction a or b due to the ambient temperature change However, due to the change in ambient temperature l2, the first and second vibrating bodies (22+, (23) are deflected at 52, and the first and second opposing bodies u6) , 0η actually shifts as shown in detail in FIG.

即ち、第1、第2振動体の、Q暗よ夫々その支点として
の第1、第2固定台I29)、例がヘッダα0)上で離
間しているためf二、第1、第2振動体az、@が周囲
温度変化(二より例えばa方向C二実線の位置から破線
の位置に撓むと、第1、第2対向体(1ta、anはそ
の中央線a、dを参照すると寸法lだけずれてしまう。
That is, since the first and second vibrating bodies are spaced apart on the first and second fixed bases I29), which serve as their fulcrums, respectively, and the header α0), the first and second vibrations are When the body az, @ bends due to a change in ambient temperature (for example, from the position of the solid line C2 in the a direction to the position of the broken line), the first and second opposing bodies (1ta, an are the dimensions l when referring to their center lines a, d) It's just off.

ここに、斯るずれが生じた状態においては、第1 、m
 2 振動体(27J、(ハ)の振動≦二際し、上述の
如き2つの重畳が確実に二行なわれないので、赤外線断
続が確実に行なわれず、これ2二より検出体(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。
Here, in a state where such a shift occurs, the first, m
2. When the vibration of the vibrating body (27J, (c) ≦ 2, the two superpositions described above are not performed reliably, the intermittent infrared rays cannot be reliably performed, and due to this 22, the detection object (1) The desired charge according to the temperature of the detection part is not generated,
Accurate temperature measurement cannot be performed.

し1 発明の目的 本発明は、赤外線断続が確実≦二行なわれるように二し
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C二することを目的とする。
1. OBJECTS OF THE INVENTION It is an object of the present invention to ensure that infrared rays are intermittent ≦2 times, so that, for example, when measuring temperature, such temperature measurement can be performed with high precision.

に)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振動体に二おける
各々の振動方向に垂直な面が同一平面上(二位置するよ
うに、上記第1、第2振動体を配置したことを特徴とす
る。
B) Structure of the Invention In order to achieve the above object, the infrared detector of the present invention includes 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, and an infrared transmitting part disposed in the infrared incident area to the detecting body. first and second opposing bodies both having non-transparent parts; a state in which the infrared transparent part and the infrared non-transparent part of the first opposing body overlap with the infrared non-transmissive part and the infrared transparent 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. The first and second vibrating bodies are arranged such that the two surfaces perpendicular to the respective vibration directions of the first and second vibrating bodies are on the same plane (two positions). .

(ホ)実施例 以1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 1 An infrared detector according to an embodiment of the present invention will be explained based on 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.

(至)、(至)は夫々右側の下端及び上端c二取付けら
れた第1、第2対向体ル、卸を周期的C二振動せしめる
ための第1、第2振動体で、該第1、第2−振動体はそ
の圧′心体輯ω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。卿は、上記第1、第2振
動体例、(至)における各々の振動方向a、bl二垂直
な面、A、Bが同一平面上g二位置するようC;、上記
第1、第2振動体■、田を固定支持するための金属性の
固定台であり、上記第1振動端子柊には第1、第2振動
体(ロ)、c’sの中央電極(財)が接続され、上記?
J&2撒動端子□□□には上記固定台(7)が接続され
ている。
(to) and (to) are first and second vibrating bodies for causing periodic vibration of the first and second opposing bodies attached to the lower end and upper end of the right side, respectively; , the second vibrating body is the same as the conventional one except that its pressure's core body curve ω is polarized in the p and p' directions, respectively. In the above first and second vibrating body examples, the respective vibration directions a and bl in (to) and two perpendicular planes, A and B, are located on the same plane g; The body is a metal fixing base for fixedly supporting the body, and the first and second vibrating bodies (b) and the central electrode (goods) of c's are connected to the first vibrating terminal. the above?
The fixed base (7) is connected to the J&2 swing terminal □□□.

而して、$1倣動端子図【二は一20Vの一定電圧が印
加され、上記第2伽動端子■Cは±10Vの電圧が交互
に印加さ肚る。
Thus, a constant voltage of 20 V is applied to the $1 moving terminal diagram [2], and a voltage of ±10 V is alternately applied to the second moving terminal C.

斯る+IOVの電圧印加時(二は、第1、第2振動体図
、(至)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■、(至)は各々b、a方向
に撓み、これにより第1、第2振動体図、(至)は従来
と同様【二周期的に振動し、赤外線断続が行なわれる。
When a voltage of +IOV is applied, the first and second vibrating bodies (2) are bent in the a and b directions, respectively, and when a voltage of -10V is applied, the first and second vibrating bodies (2) are bent in the a and b directions, respectively. ) are deflected in directions b and a, respectively, and as a result, the first and second vibrator diagrams (to) vibrate periodically as in the conventional case, and infrared rays are intermittent.

ここC二、第1、第2振動体図、C伺は夫々その支点が
固定合一にて同一直線上に存在し縦に重なっているから
、第1、第2倣動体G転□□□が周囲fA度変化により
婉んでも、それにより第1、第2対向体α6ノ、ul)
の両者間にずれが生じることはない。
Here, the fulcrums of C2, the first and second vibrating bodies, and C, respectively, are on the same straight line with a fixed union and overlap vertically, so the first and second moving bodies G are rotated □□□ Even if it decreases due to the change in the surrounding fA degree, the first and second opposing bodies α6, ul)
There will be no discrepancy between the two.

従って、斯る撓みが生じた状態において、第1、第2振
動体例、(至)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 vibrate, the infrared rays are reliably intermittent, and the desired signal is transmitted from the detecting body (1) to the detected part according to the temperature. A charge is generated.

(へ)発明の効果 以上の説明から明らかな如く、本発明(=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 when ambient temperature changes, so for example, in temperature measurement, it can be done with high precision. be able to.

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

第1図は最近提案された赤外線検出器の断面図、$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図は同検出器士 6図は同検出器を矢印■方向から見た要部棲面図である
。 (11・・・焦電型赤外線検出体、 (Le、αD・・
・第1、第2対向体、 (ロ)、(至)・・・第1、第
2振動体。 0θ473 ライト動作制御目y8.−
Figure 1 is a cross-sectional view of a recently proposed infrared detector, Figures a 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 of the detector as seen from the direction of the arrow (■), and FIG. 6 is a plan view of the main part of the detector as seen from the direction of the arrow (■). (11...pyroelectric infrared detector, (Le, αD...
・First and second opposing bodies, (b), (to)...first and second vibrating bodies. 0θ473 Light operation control eye y8. −

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g二繰返せしめるべく、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g二垂直な面が同一平
面上に位置するように二、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 detector 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 region to the detector and have both an infrared transmitting part and an infrared non-transmissive part, and the second opposing body. The state in which the infrared transmitting part and the infrared non-transmitting part of the first opposing body overlap with the infrared non-transmitting part and the infrared transmitting part of the second opposing body, and the infrared transmitting part and the infrared non-transmitting part of the first and second opposing bodies overlap, respectively. In order to alternately repeat the state in which the transparent parts overlap each other, first and second vibrating bodies are provided which respectively vibrate the first and second facing bodies, and each of the first and second vibrating bodies vibrates. 2. An infrared detector characterized in that the first and second vibrating bodies are arranged so that surfaces perpendicular to the vibration direction g 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 true JPS59202036A (en) 1984-11-15
JPH0425485B2 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
JPH0425485B2 (en) 1992-05-01

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