JPH0695048B2 - Infrared detector - Google Patents
Infrared detectorInfo
- Publication number
- JPH0695048B2 JPH0695048B2 JP62049324A JP4932487A JPH0695048B2 JP H0695048 B2 JPH0695048 B2 JP H0695048B2 JP 62049324 A JP62049324 A JP 62049324A JP 4932487 A JP4932487 A JP 4932487A JP H0695048 B2 JPH0695048 B2 JP H0695048B2
- Authority
- JP
- Japan
- Prior art keywords
- infrared
- lens
- condenser lens
- pyroelectric
- infrared detector
- 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 - Lifetime
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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)
Description
【発明の詳細な説明】 産業上の利用分野 本発明は宇宙産業における人工衛星の姿勢制御用に使用
される地球センサ用の赤外検出器に関するものである。Description: FIELD OF THE INVENTION The present invention relates to an infrared detector for an earth sensor used for attitude control of a satellite in the space industry.
従来の技術 地球センサ用赤外検出器としては、サーミスタ、サーモ
パイルあるいは焦電素子を用いたものが知られている。
これらのうちサーミスタを利用したものについては電子
技術総合研究所調査報告第177号第65〜66頁に示されて
いるように赤外検出感度向上のために、赤外集光レンズ
を赤外検出素子と一体化したものが実用化されている。2. Description of the Related Art As an infrared detector for an earth sensor, one using a thermistor, a thermopile or a pyroelectric element is known.
Among them, those using a thermistor detect the infrared condensing lens in order to improve the infrared detection sensitivity as shown in Research Report No. 177, pp. 65-66 of the Electrotechnical Laboratory. A device integrated with an element has been put into practical use.
第3図(a)(b)は焦電素子をレンズに一体化した例
である。図において、11は焦電素子を利用した赤外検出
素子、12は赤外線を透過させるGeなどで形成された集光
レンズ、13は焦電素子11の裏面に形成された信号取出し
電極としての裏面電極、16は赤外受光電極でアース電極
として使用される。14、15は各々信号取出しリード、ア
ースリードである。3 (a) and 3 (b) are examples in which a pyroelectric element is integrated with a lens. In the figure, 11 is an infrared detection element using a pyroelectric element, 12 is a condenser lens formed of Ge or the like that transmits infrared rays, and 13 is a back surface as a signal extraction electrode formed on the back surface of the pyroelectric element 11. Electrodes, 16 are infrared receiving electrodes, which are used as ground electrodes. 14 and 15 are a signal extraction lead and a ground lead, respectively.
このような構成において、集光レンズ12に入射した赤外
線は、集光レンズにて集光されて赤外検出素子12に入射
し、焦電効果によって信号取出し電極13より信号が取り
出される。In such a configuration, the infrared light that has entered the condenser lens 12 is condensed by the condenser lens and enters the infrared detection element 12, and a signal is extracted from the signal extraction electrode 13 by the pyroelectric effect.
赤外検出素子11と集光レンズ12を一体化した効能は次の
通りである。すなわち第3図に示すように赤外検出素子
11を集光レンズ12に密着させることにより光学収差によ
る性能劣化を無視し得る程度に抑えた状態で光学系を明
るくすることができる。従って、赤外線の集光効率が向
上し、赤外検出感度の向上が可能になる。The effects of integrating the infrared detection element 11 and the condenser lens 12 are as follows. That is, as shown in FIG. 3, an infrared detection element
By bringing 11 into close contact with the condenser lens 12, the optical system can be brightened while the performance deterioration due to optical aberration is suppressed to a negligible level. Therefore, the efficiency of collecting infrared rays is improved, and the infrared detection sensitivity can be improved.
発明が解決しようとする問題点 しかし、赤外検出素子11は集光レンズ12に密着している
ので、赤外検出器の重要な特性項目のひとつである熱時
定数が短かくなる。焦電素子の場合、集光レンズ一体形
でない場合熱時定数は数10mSであるが、一体形でレンズ
に密着させた場合0.1mSのオーダーになる。However, since the infrared detection element 11 is in close contact with the condenser lens 12, the thermal time constant, which is one of the important characteristic items of the infrared detector, becomes short. In the case of a pyroelectric element, the thermal time constant is several tens of mS when it is not integrated with a condenser lens, but it is on the order of 0.1 mS when it is closely attached to the lens.
一方、地球センサ設計の立場からは、地球端検出時の赤
外入力信号を効率よく検出するため、入力信号の主要周
波数帯60〜300Hzに対応した周波数特性が要求される。
焦電素子においては、熱時定数を短かくすれば、それに
比例して感度が低下するので、(1)式で与えられる12
0Hz相当の熱時定数以上に設定することが必要である。On the other hand, from the standpoint of earth sensor design, in order to efficiently detect the infrared input signal when detecting the earth's edge, frequency characteristics corresponding to the main frequency band 60 to 300 Hz of the input signal are required.
In the pyroelectric element, if the thermal time constant is shortened, the sensitivity decreases in proportion to it.
It is necessary to set the thermal time constant equal to or higher than 0 Hz.
設計の余裕も考慮するとGT2mSが地球センサ側の要求
条件になる。 Considering the design margin, GT2mS will be a requirement on the earth sensor side.
以上のように集光効率を上げるために、レンズと一体化
した赤外検出器においては熱時定数が地球センサ設計で
要求する値より短かくなる。そして、感度が低下し、し
かも集光効率向上によって得られた入力信号の増大分よ
りもこの低減率の方がはるかに大きな影響を与え、総合
的には感度向上どころか低下してしまうという問題があ
る。As described above, in order to increase the light collection efficiency, the thermal time constant of the infrared detector integrated with the lens becomes shorter than the value required for the earth sensor design. Then, there is a problem that the sensitivity is lowered, and the reduction rate has a far greater effect than the increase of the input signal obtained by the improvement of the light collection efficiency, and the sensitivity is lowered rather than the overall improvement. is there.
本発明はこのような問題点を解決するもので、赤外検出
素子と集光レンズとを一体化し、かつ熱時定数の大きい
赤外検出器を得ることを目的とするものである。The present invention solves such problems, and an object thereof is to obtain an infrared detector having a large thermal time constant by integrating an infrared detection element and a condenser lens.
問題点を解決するための手段 上記問題を解決するために、本発明は集光レンズと赤外
検出素子間をその有効受光面において、検出すべき赤外
線の波長の1/4以下の間隔をあけ、熱時定数が地球セン
サ設計要求条件を満すようにしようとするものである。Means for Solving the Problems In order to solve the above problems, the present invention provides a space between the condensing lens and the infrared detection element on the effective light receiving surface thereof, which is 1/4 or less of the wavelength of infrared rays to be detected. , The thermal time constants try to satisfy the earth sensor design requirements.
作用 上記構成において、赤外検出素子と集光レンズ間に間隔
があるので、赤外検出素子から集光レンズへの熱拡散が
小さくなるので熱時定数は大きくなる。また、この間隔
がλ/4以下であるため光学収差はほとんど無視すること
ができる。Action In the above configuration, since there is a space between the infrared detection element and the condenser lens, thermal diffusion from the infrared detection element to the condenser lens becomes small, and the thermal time constant becomes large. Further, since this distance is λ / 4 or less, the optical aberration can be almost ignored.
実施例 地球センサにおいては、炭酸ガスの放射帯である14〜16
μm帯あるいは水蒸気の放射帯である17〜35μm帯の赤
外線が観測の対象になる。このような長波長の赤外線を
検出する場合、光学収差が地球センサの性能に悪影響を
与えない条件を保ちながら集光レンズと赤外検出素子間
に間隔を設けて、熱時定数を地球センサの設計要求値ま
で長くすることが可能である。光学設計によるとその間
隔はλ/4以下であればよい。ここで、λは検出すべき赤
外線の最短波長である。従って、λ=14μmであれば、
集光レンズと赤外検出素子との間隔は3.5μmまで広げ
られる。Example In the earth sensor, the emission band of carbon dioxide gas is 14 to 16
Infrared rays in the μm band or 17 to 35 μm band, which is the radiation band of water vapor, are the targets of observation. When detecting such long-wavelength infrared rays, the thermal time constant of the earth sensor is set by providing a space between the condenser lens and the infrared detecting element while maintaining the condition that optical aberration does not adversely affect the performance of the earth sensor. It is possible to increase to the design required value. According to the optical design, the distance may be λ / 4 or less. Here, λ is the shortest wavelength of infrared rays to be detected. Therefore, if λ = 14 μm,
The distance between the condenser lens and the infrared detection element can be increased to 3.5 μm.
熱時定数τTは次式で与えられる。The thermal time constant τ T is given by the following equation.
ここで、Hは赤外検出素子有効感熱部の熱容量(J/
℃),Gは赤外検出素子有効感熱部からヒートシンク部
(集光レンズはヒートシンクとして作用する。)までの
熱放散能(J/℃・S)である。 Here, H is the heat capacity of the infrared sensing element effective heat-sensitive part (J /
℃), G is the heat dissipation capacity (J / ℃ ・ S) from the effective heat-sensitive part of the infrared detection element to the heat sink (the condenser lens acts as a heat sink).
熱放散能Gは、熱輻射、対流、熱伝導の3種類の要因を
含むが熱伝導が主要因なので、これを抑えればGが小さ
くなり、熱時定数τTが長くなる。The heat dissipation capability G includes three types of factors of heat radiation, convection, and heat conduction, but since heat conduction is the main factor, if this is suppressed, G will decrease and the thermal time constant τ T will increase.
集光レンズと赤外検出素子間に数μmの間隔があれば、
その間の熱放散は気体による対流と熱輻射によるものと
なり大巾に低減する。また、この間隔における気圧が減
圧されれば、対流も減少する。残る要因は、赤外検出素
子周辺から支持台を経由してヒートシンク体であるレン
ズに伝導で逃げる熱である。これは、赤外検出素子の構
造、レンズへの固定法に左右されるが、設計で制御し得
る要因であり、赤外検出器の設計に積極的に利用でき
る。If there is a space of several μm between the condenser lens and the infrared detection element,
The heat dissipation during that time is largely due to the convection due to the gas and the heat radiation. Also, if the atmospheric pressure in this interval is reduced, convection is also reduced. The remaining factor is heat that escapes by conduction from the periphery of the infrared detection element to the lens, which is the heat sink body, via the support base. This depends on the structure of the infrared detection element and the method of fixing it to the lens, but it is a factor that can be controlled by design and can be positively used for designing the infrared detector.
以下、本発明の実施例について図面とともに説明する。Embodiments of the present invention will be described below with reference to the drawings.
第1図は本発明の一実施例におけるレンズ一体形焦電赤
外検出素子22の構造を示す図である。FIG. 1 is a view showing the structure of a lens-integrated pyroelectric infrared detection element 22 in one embodiment of the present invention.
赤外集光レンズ12はゲルマニウム製で、直径3mmφの片
凸レンズで、凸面の曲率半径2.5mm、厚さ2mmであり、両
面に波長14μmの赤外光の1/4波長の光学的厚さの硫化
亜鉛膜が蒸着され、これが14〜16μm帯の赤外線に対し
て反射防止膜となっている。The infrared condensing lens 12 is made of germanium, is a single-convex lens with a diameter of 3 mmφ, and has a convex surface with a radius of curvature of 2.5 mm and a thickness of 2 mm. A zinc sulfide film is vapor-deposited, which serves as an antireflection film for infrared rays in the 14 to 16 μm band.
上記の赤外集光レンズの光学設計条件は、これと組合せ
る主レンズ(対物レンズ)との組合せにおいて決定され
たもので本発明の本質に関係するものではない。The optical design conditions of the above infrared condensing lens are determined in combination with the main lens (objective lens) to be combined therewith and are not related to the essence of the present invention.
焦電素子11は、寸法1mm×1mm×10μm厚のチタン酸鉛セ
ラミックで、有効受光面すなわち有感部は、1mm×1mmの
中央部0.3mmφとする。この部分に赤外入射面すなわち
集光レンズ12に向う面にアース電極16としてニクロム電
極をシート抵抗が1cm巾、1cm間隔で300〜400Ωになるよ
うに蒸着する。このニクロム電極膜16は、0.2mm巾で一
方向にリード取り出しのため1mm×1mmの焦電素子の縁部
まで延ばして蒸着しておく。裏面も同様に信号取出し電
極13としてアルミ蒸着膜を1〜2μmの厚さで蒸着す
る。The pyroelectric element 11 is a lead titanate ceramic having a size of 1 mm × 1 mm × 10 μm, and an effective light receiving surface, that is, a sensitive portion has a central portion of 0.3 mmφ of 1 mm × 1 mm. A nichrome electrode as a ground electrode 16 is vapor-deposited on this portion on the infrared incident surface, that is, the surface facing the condenser lens 12 so that the sheet resistance is 1 cm wide and 300 cm to 400 Ω at 1 cm intervals. This nichrome electrode film 16 is 0.2 mm wide and is vapor-deposited by extending it to the edge of a 1 mm × 1 mm pyroelectric element for taking out the lead in one direction. Similarly, on the back surface, an aluminum vapor deposition film is vapor-deposited with a thickness of 1 to 2 μm as the signal extraction electrode 13.
一方集光レンズ12の平面部に素子支持枠17として厚さ2
μmのアルミ膜を蒸着しておく。蒸着部分は、集光レン
ズ中央0.6mm□を除いて、約1mm×1mmとし、更に赤外受
光面電極16を引き出すために第1図(b)に示すように
0.3mmだけリード取付部を追加しておく。尚、集光レン
ズ12と焦電素子11間の空間が密閉状態にならないよう、
少くとも2ケ所以上アルミ蒸着素子支持枠17に蒸着なし
の部分を設けておく。On the other hand, the thickness of the element support frame 17 is 2 on the flat surface of the condenser lens 12.
An aluminum film of μm is vapor-deposited. Evaporation portion, except for the condenser lens center 0.6 mm □, of about 1 mm × 1 mm, as further shown in FIG. 1 (b) to derive the infrared light-receiving surface electrode 16
Add 0.3mm of lead mounting part. It should be noted that the space between the condenser lens 12 and the pyroelectric element 11 should not be sealed.
At least two or more locations are provided on the aluminum vapor deposition element support frame 17 without vapor deposition.
この素子支持枠17上に前記焦電素子11を接着剤にて接着
する。赤外入射面電極引出し側(第1図の焦電素子11の
左側)は導電性接着剤で接着し電気的導通をとりアース
電極とした。一方第1図の焦電素子11の右側は、絶縁性
接着剤で接着する。しかる後、微細金線(30μ中)を各
々のリード取付部に超音波ボンダーにて接続し、信号取
出リード14、アースリード16を取り付ける。The pyroelectric element 11 is bonded onto the element supporting frame 17 with an adhesive. The infrared incident surface electrode extraction side (the left side of the pyroelectric element 11 in FIG. 1) was bonded with a conductive adhesive to establish electrical continuity and used as a ground electrode. On the other hand, the right side of the pyroelectric element 11 in FIG. 1 is bonded with an insulating adhesive. After that, a fine gold wire (in 30μ) is connected to each lead mounting portion with an ultrasonic bonder, and the signal extraction lead 14 and the ground lead 16 are attached.
以上で、集光レンズ付焦電赤外検出素子が作成できた。
これを用いて第2図に示すような構造の地球センサ用赤
外検出器を作製した。第2図は、2素子形赤外検出器の
一例を示すもので、14〜16μm又は17〜35μmの赤外線
のみを透過する赤外干渉フィルタを窓板18に用いてい
る。マウントベース20に集光レンズ付の赤外検出素子22
が組入まれ、キャップ19にて真空封止されている。信号
及び電源については、ピン端子21を用いて、信号が取出
されあるいは電源が印加される。ピン端子21はアースピ
ン、ケースピンを含め4ピンとした。With the above, a pyroelectric infrared detection element with a condenser lens was produced.
Using this, an infrared detector for earth sensor having a structure as shown in FIG. 2 was produced. FIG. 2 shows an example of a two-element infrared detector, in which an infrared interference filter which transmits only infrared rays of 14 to 16 μm or 17 to 35 μm is used for the window plate 18. Infrared detector 22 with a condenser lens on the mount base 20
Are assembled and vacuum-sealed with a cap 19. Regarding the signal and the power source, the signal is taken out or the power source is applied using the pin terminal 21. The pin terminal 21 has four pins including a ground pin and a case pin.
この赤外検出器の熱時定数は3mSであり、十分地球セン
サの設計要求条件を満している。The thermal time constant of this infrared detector is 3mS, which satisfies the design requirements of the earth sensor.
第2の実施例として、素子支持枠17をアルミ蒸着膜のか
わりにレンズの反射防止膜材料である硫化亜鉛とした。
厚さは2μmで、寸法は同じであるが、赤外入射面電極
取出し側に0.2mm巾のアルミ蒸着膜を硫化亜鉛枠上に蒸
着し、そこからアースリードをとった。この実施例で
は、真空封止せず、乾燥窒素ガス封止とした。In the second embodiment, the element supporting frame 17 is made of zinc sulfide which is a material for the antireflection film of the lens instead of the aluminum vapor deposition film.
Although the thickness was 2 μm and the dimensions were the same, a 0.2 mm wide aluminum vapor-deposited film was vapor-deposited on the zinc sulfide frame on the side from which the infrared incident surface electrode was taken out, and the earth lead was taken therefrom. In this example, dry nitrogen gas sealing was performed without vacuum sealing.
熱時定数は2mSで地球センサの要求値を満たした。The thermal time constant was 2 mS, which satisfied the required value of the earth sensor.
発明の効果 以上のように、本発明は焦電形赤外検出素子を赤外集光
レンズに対して検出される赤外線の波長の1/4以下の間
隔をもたせて固定し、これを赤外透過窓を有する容器内
に収納した地球センサ用の赤外検出器で、熱時定数2mS
以上にし、集光効率向上による感度改善を維持し、集光
レンズと一体化しない素子に比較して、約2.5倍の電圧
感度向上を達成することができた。なお、本実施例にお
いては、雑音が1.6倍強増大したが、感度向上がそれを
上まわりS/Nは1.5倍改善される。また素子厚を薄くすれ
ば雑音は低減され、例えば素子の厚さを1/3にすること
で、雑音は に低減できるのでS/Nとして2.5倍の改善が達成できる。As described above, according to the present invention, the pyroelectric infrared detection element is fixed to the infrared condensing lens with an interval of 1/4 or less of the wavelength of infrared rays detected, and the infrared detection element An infrared detector for earth sensors housed in a container with a transparent window, with a thermal time constant of 2 mS
As described above, it was possible to maintain the sensitivity improvement due to the improvement of the light collection efficiency and achieve the voltage sensitivity improvement of about 2.5 times as compared with the element not integrated with the light collection lens. It should be noted that in the present embodiment, the noise increased slightly more than 1.6 times, but the improvement in sensitivity exceeded it, and the S / N was improved by 1.5 times. Noise can be reduced by reducing the element thickness. For example, reducing the element thickness to 1/3 reduces the noise. The S / N ratio can be improved 2.5 times.
第1図(a)、(b)は各々本発明による赤外検出器の
要部であるレンズ一体形焦電赤外検出素子の実施例にお
ける側面図および平面図、第2図は本発明による地球セ
ンサ用赤外検出器の実施例における構成を示す断面側面
図、第3図(a)、(b)は各々従来のレンズ一体形焦
電赤外検出素子の側面図および平面図である。 11……焦電素子、12……集光レンズ、13……信号取出し
電極、14……信号取出しリード、15……アースリード、
16……アース電極、17……素子支持枠、18……窓板、19
……キャップ、20……マウントベース1 (a) and 1 (b) are a side view and a plan view of an embodiment of a pyroelectric infrared detection element integrated with a lens, which is a main part of an infrared detector according to the present invention, and FIG. 2 is a view according to the present invention. FIG. 3A and FIG. 3B are a side view and a plan view of a conventional lens-integrated pyroelectric infrared detection element, respectively, showing a sectional side view showing a configuration in an embodiment of an infrared detector for an earth sensor. 11 ... Pyroelectric element, 12 ... Condensing lens, 13 ... Signal extraction electrode, 14 ... Signal extraction lead, 15 ... Ground lead,
16 …… Ground electrode, 17 …… Element support frame, 18 …… Window plate, 19
...... Cap, 20 ...... Mount base
───────────────────────────────────────────────────── フロントページの続き (72)発明者 中村 邦雄 神奈川県川崎市多摩区東三田3丁目10番1 号 松下技研株式会社内 (72)発明者 山香 英三 神奈川県横浜市緑区藤が丘2丁目28番地2 ─────────────────────────────────────────────────── ─── Continuation of front page (72) Kunio Nakamura Inventor Kunio Nakamura 3-10-1 Higashisanda, Tama-ku, Kawasaki City, Kanagawa Matsushita Giken Co., Ltd. (72) Inventor Eizo Yamaka 2-chome Fujigaoka, Midori-ku, Yokohama Address 2
Claims (3)
して検出される赤外線の最短波長の1/4以下の間隔で固
定され赤外フィルタ窓を具備した容器に収納されたこと
を特徴とする赤外検出器。1. A pyroelectric infrared detecting element is fixed at an interval of 1/4 or less of the shortest wavelength of infrared rays detected by an infrared condenser lens and is housed in a container equipped with an infrared filter window. An infrared detector characterized in that
1項記載の赤外検出器。2. The infrared detector according to claim 1, wherein the inside of the container is sealed under reduced pressure.
μm帯の赤外光を選択的に透過する赤外干渉フィルタで
構成された特許請求の範囲第1項記載の赤外検出器。3. An infrared filter window having a band of 14 to 16 μm or 17 to 35
The infrared detector according to claim 1, comprising an infrared interference filter that selectively transmits infrared light in the μm band.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62049324A JPH0695048B2 (en) | 1987-03-04 | 1987-03-04 | Infrared detector |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62049324A JPH0695048B2 (en) | 1987-03-04 | 1987-03-04 | Infrared detector |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS63215922A JPS63215922A (en) | 1988-09-08 |
| JPH0695048B2 true JPH0695048B2 (en) | 1994-11-24 |
Family
ID=12827799
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP62049324A Expired - Lifetime JPH0695048B2 (en) | 1987-03-04 | 1987-03-04 | Infrared detector |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0695048B2 (en) |
-
1987
- 1987-03-04 JP JP62049324A patent/JPH0695048B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS63215922A (en) | 1988-09-08 |
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