JPS60191051A - Pyroelectric type infrared ray decting element - Google Patents

Pyroelectric type infrared ray decting element

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Publication number
JPS60191051A
JPS60191051A JP59042917A JP4291784A JPS60191051A JP S60191051 A JPS60191051 A JP S60191051A JP 59042917 A JP59042917 A JP 59042917A JP 4291784 A JP4291784 A JP 4291784A JP S60191051 A JPS60191051 A JP S60191051A
Authority
JP
Japan
Prior art keywords
pyroelectric
infrared detection
detection element
infrared
decting
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.)
Pending
Application number
JP59042917A
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Japanese (ja)
Inventor
中本 正幸
平尾 洋佐
洋八 山下
岩瀬 暢男
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.)
Toshiba Corp
Original Assignee
Toshiba Corp
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Publication date
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Priority to JP59042917A priority Critical patent/JPS60191051A/en
Publication of JPS60191051A publication Critical patent/JPS60191051A/en
Pending legal-status Critical Current

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Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 〔発明の技術分野〕 本発明は人体の移動、物体の有無などの検知に適する焦
電形赤外線検出素子に関する。
DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to a pyroelectric infrared detection element suitable for detecting the movement of a human body, the presence or absence of an object, etc.

〔発明の技術的背景とその問題点〕[Technical background of the invention and its problems]

所謂るマイクロエレクトロニクスの発達に伴ない9例え
ば赤外線検出素子(赤外線センサ)も人体の存否乃至移
動、物体の有無乃至移動を検知したり或いは非接触温度
測定などへの応用が拡大している。
With the development of so-called microelectronics, for example, infrared detection elements (infrared sensors) are increasingly being applied to detect the presence or absence or movement of a human body, the presence or absence or movement of an object, or non-contact temperature measurement.

ところでとの種赤外線検出素子としては、半導体の光伝
導や光起電力を利用した量子形のもの。
By the way, the type of infrared detection element mentioned above is a quantum type that uses semiconductor photoconduction and photovoltaic force.

例えばHg Cd Te −? Pb Sを本体とした
ものが知られている。この量子形赤外線検出素子は感度
がよく応答性がすぐれている反面、使用に際しては極低
温に冷却する必要があり簡易に取扱い得ないうえ赤外領
域の感度にも波長依存性がある。かくして用途も限定さ
れ実用的にはなを問題がある。
For example, Hg Cd Te −? Those whose main body is PbS are known. Although this quantum infrared detection element has good sensitivity and excellent response, it must be cooled to an extremely low temperature before use, making it difficult to handle, and its sensitivity in the infrared region is also wavelength dependent. Therefore, the application is limited and there are problems in practical use.

一方チタン酸ジルコン酸鉛(PbZr Tl 03)も
しくはチタン酸鉛(PbTi03)の焦電効果を利用し
た所謂る焦電形赤外線検出素子の開発も試みられている
On the other hand, attempts have been made to develop so-called pyroelectric infrared detection elements that utilize the pyroelectric effect of lead zirconate titanate (PbZr Tl 03) or lead titanate (PbTi03).

しかしこれらPb Zr ’I’l 03やPbTl0
3など検出素子の本体を成す焼結体(セラミックス)は
、使用に際して特に冷却を要しないこと、波長依存性も
ないことなどの利点をもつ反面、感度など性能面に劣る
不都合さがある。即ち焦電効果を利用した赤外線検出素
子においては、その性能が焦電効果により発生する電圧
に対する評価指数Fvに大きく影響される。
However, these Pb Zr 'I'l 03 and PbTl0
The sintered body (ceramics) that forms the main body of a detection element such as No. 3 has advantages such as not requiring particular cooling during use and no wavelength dependence, but has the disadvantage of being inferior in terms of performance such as sensitivity. That is, in an infrared detection element using the pyroelectric effect, its performance is greatly influenced by the evaluation index Fv for the voltage generated by the pyroelectric effect.

ここで評価指数ii”vは焦電係数P(C//crIL
2°C)、定積比熱Cv(J/′CrIL3°C)、比
誘電率6としたとき。
Here, the evaluation index ii”v is the pyroelectric coefficient P(C//crIL
2°C), specific heat at constant volume Cv (J/'CrIL3°C), and relative dielectric constant 6.

で示され、赤外線検出素子の本体を成す焦電材料につい
ては、センサとしての性能面からすれば焦電係数Pが大
きく、安積比熱CVおよび比誘電率εが小さいことが望
まれる。
In terms of performance as a sensor, it is desired that the pyroelectric material forming the main body of the infrared detection element has a large pyroelectric coefficient P and a small Hazumi specific heat CV and dielectric constant ε.

しかるにPb Zr ’r103の場合は、定積比熱C
v−2,42J/CrrL3℃であるが、誘電率g=3
80〜1700と大きく、またPb’l”i03の場合
は定積比熱Cv=3.11J7cm3’(]であるが、
焦電係数% = 1.8 X 10−8C/rx2°C
で評価指数Fy = 0.3 X 10−’QC−am
/Jと値が低く上記の如く性能的に問題がある。特にP
bTs03焦電材料は自発分極を起こすための分極処理
に当っては200°0の高温下で601(■軸以上の電
界を印加する必要があり、この分極処理も実用面で問題
になっている。
However, in the case of Pb Zr 'r103, the specific heat at constant volume C
v-2,42J/CrrL3℃, but dielectric constant g=3
80 to 1700, and in the case of Pb'l"i03, the specific heat at constant volume Cv = 3.11J7cm3' (),
Pyroelectric coefficient % = 1.8 x 10-8C/rx2°C
Evaluation index Fy = 0.3 x 10-'QC-am
/J, which causes performance problems as described above. Especially P
When polarizing the bTs03 pyroelectric material to cause spontaneous polarization, it is necessary to apply an electric field of 601 (■ axis or higher) at a high temperature of 200°0, and this polarization process also poses a practical problem. .

〔発明の目的〕[Purpose of the invention]

本発明は上記の如き事情に対処して、室温で両投 作する高感度の且つ馬用性の高い焦電形赤外線検出素子
を提供しようとするものである。
The present invention addresses the above-mentioned circumstances and provides a pyroelectric infrared detecting element which is highly sensitive and highly usable for horses, and which can be operated at room temperature.

〔発明の要点〕[Key points of the invention]

本発明は一般式 %式% (但し式中fvle = Ba、 Sr、 Ca )う
ちの1種以上。
The present invention uses one or more of the general formula % (where fvle = Ba, Sr, Ca).

X = 0.05〜0.35の数、y=0.01〜0.
10の故)で示される複合ペロブスカイトt1°4造の
ものに。
X = number from 0.05 to 0.35, y = 0.01 to 0.
10) of the composite perovskite t1°4 structure.

MnO,Ni O,I+’e2’03のうちの少なくと
も1棟を0.01〜2重18%添加配合してなる焼結体
を本体として成ることを特徴とする焦電形赤外線検出素
子である。
A pyroelectric infrared detecting element characterized in that its main body is a sintered body containing at least one of MnO, NiO, I+'e2'03 added in an amount of 0.01 to 18%. .

しかして本件発明は、上記一般式で示される複合ペロブ
スカイト構造のものに所定瓜のNiQ、P、400゜F
e203などを添加含有せしめてなる焼結体がf’好な
焦電性を示すとともに赤外線検出素子(センサ)として
実用上すぐれた性能を備えているとの知見に基づくもの
である。
Therefore, the present invention provides a composite perovskite structure represented by the above general formula with a predetermined amount of NiQ, P, 400°F.
This is based on the knowledge that a sintered body containing e203 or the like exhibits f'-favorable pyroelectricity and has excellent practical performance as an infrared detection element (sensor).

〔発明の実施4i1J ) 先ず(Pb+−x Cax) C(COt/2Wl/2
)0.04 ’I”o、 96 ) 03 +0.3.
7ff、Fi’r%〜In O十0.4重hセ%NiO
となるようにPbO。
[Practice of the invention 4i1J] First, (Pb+-x Cax) C(COt/2Wl/2
) 0.04 'I”o, 96 ) 03 +0.3.
7ff, Fi'r%~InO10.4foldhce%NiO
PbO so that

CaCO3,Ti(J2. coo、 wo3. Mn
CO3、l’+5 ヨびNiOを所定−5tそれぞれ秤
取し、アルミナボットミルを用いてそれぞれ湿式混合し
た。これらの混合物を900 ’0で2時間仮焼した後
アルミナボンドミルにて粉砕〔で原料粉末をii”l 
4’Jした。次いでこれらの原料粉末をプレスによりシ
ート化し、このシートから打抜き力1ぼにより径20 
mzの円板をそれぞれ得、この円板をマグネシア製容器
に入れ1100〜1180”Oで0.5〜4時間焼成し
て厚さ1=@4μm 、径20朋の薄い円板を得たつ れぞれ被着形成して一対の電極とした。この電極性は後
100’Qのシリコーン油中に浸漬し+ 40〜50k
V/CnLのIよ圧金印加し5分間分極処理を施してか
ら100℃、24時間エージング処理し2次いで精密カ
ッタにて3 X a mz片に切り出して焦電形赤外検
出素子(センサ)をそれぞれ得た。
CaCO3, Ti (J2. coo, wo3. Mn
A predetermined amount of -5 tons of CO3, l'+5 and NiO were each weighed out and wet-mixed using an alumina bot mill. After calcining these mixtures at 900'0 for 2 hours, they were pulverized with an alumina bond mill to obtain raw material powder.
I did 4'J. Next, these raw material powders are pressed into a sheet, and punched from this sheet with a diameter of 20 mm using a force of 1 mm.
mz discs were obtained, and the discs were placed in a magnesia container and fired at 1100 to 1180"O for 0.5 to 4 hours to obtain thin discs with a thickness of 1 = @ 4 μm and a diameter of 20 mm. A pair of electrodes was formed by adhering to each other.The polarity was determined by immersing it in silicone oil for 100 minutes and then heating it for +40 to 50K.
Apply a pressure of V/CnL to I, polarize for 5 minutes, age at 100°C for 24 hours, and then cut into 3 x a mz pieces with a precision cutter to form a pyroelectric infrared detection element (sensor). were obtained respectively.

上記によって得た各焦電形赤外線検出素子について、そ
の検出素子の本体をなす焦′i材料の組成比(PbのC
a If換量X)と、焦電係数P、比誘電率ε、評価指
数(゛を1圧感度)ドVとの関係を測定したところ第1
図に示す如くであった。第1図において曲線(1)は焦
電係数Pを2曲線(2)は比誘電率εを2曲m* (3
)は評価指数1・vをそれぞれ示し、また比較のためチ
タン酸鉛(Pb Tr 03 )の焦電係数Pを◎印、
評価指数FVを目印で夫々示した。
Regarding each pyroelectric infrared detection element obtained as described above, the composition ratio of the pyroelectric material (Pb to C
When we measured the relationship between a If conversion amount
It was as shown in the figure. In Figure 1, curve (1) represents the pyroelectric coefficient P and curve (2) represents the relative permittivity ε and represents the two curves m* (3
) indicate the evaluation index 1·v, respectively, and for comparison, the pyroelectric coefficient P of lead titanate (Pb Tr 03 ) is marked ◎,
The evaluation index FV is indicated with a mark.

第1図から明らかのようにXの値、即ちCaによるPb
の置換比が0.05〜o、35の範囲で焦電係数Pは高
い値を示し、また比誘電率εは180〜360の値を示
し、この比誘電率εの値はPb ZrTr 03の場合
の380より低い。さらに評価指数FVもXの値カ0.
05〜0.35で高い値を有しており、しかモg2図に
示す如く、キュリ一点も200 ’0以上で赤外線検出
素子として実用上の不都合さも全く認められなかった。
As is clear from Fig. 1, the value of X, that is, Pb due to Ca
The pyroelectric coefficient P shows a high value when the substitution ratio of lower than 380 in case. Furthermore, the evaluation index FV also has a value of X of 0.
However, as shown in the Mog2 diagram, even a single Curie point had a value of 200'0 or more, and no practical inconvenience was observed as an infrared detecting element.

一方上記本発明に係る焦電形赤外線検出素子について実
用面から評価したところ次のσ「1くであった。即し」
二り己ilJ成の3x3im片の一面側の電)取金一部
除去して素子面を蕗出式せた焦’1g形赤外検出素子に
ついて+;t′写3図示の検出回路として1L圧感度I
(vおよび比(・、冒り能りをそれぞれ測定したところ
On the other hand, when the pyroelectric infrared detection element according to the present invention was evaluated from a practical standpoint, the following σ was "1".
Regarding the 1g type infrared detection element, which is made by removing a part of the metal handle on one side of the 3x3im piece made by two people and making the element surface exposed. Pressure sensitivity I
(v and ratio (·, Flow performance were measured respectively.

いずれも従東知られているチタン酸鉛(Pbi”i 0
3 )を本体としてなる焦′tl;:形赤外線検出素子
の場合に較へ20〜100%もすぐれた性能を示した。
Both lead titanate (Pbi”i 0
3) The performance was 20 to 100% superior to that of the infrared detecting element having the main body.

ここで、Eも負イijiで、−(>rけ4画、i:、+
(に発生した′「に圧を負荷抵抗(dllO〜121(
ΩのF J、Th ’11’ (%界効果形トランジス
タ)のソースフォロアでインピーダンス変換した値と、
入射赤外線のパワー値との比で表したものである。
Here, E is also negative iji, -(>r ke 4 strokes, i:, +
(The pressure generated at '' is applied to the load resistance (dllO ~ 121 (
The value obtained by impedance conversion with the source follower of F J, Th '11' (% field effect transistor) of Ω,
It is expressed as a ratio to the power value of incident infrared rays.

尚第3図において(e)は電源端子を、(f)は出力端
子を、(g)はアースを示す。燻た比検出能■)は赤外
線検出素子(alの雑tf出力”Ne ’jに圧感度I
Q bよび赤外線検出系子(a)の表面積Aとし 次式
%式% にてめた値である。
In FIG. 3, (e) shows a power supply terminal, (f) shows an output terminal, and (g) shows a ground. The smoke ratio detection ability (■) is the infrared detection element (al's miscellaneous tf output "Ne'j" and the pressure sensitivity I
This value is calculated using the following formula, where Q b and the surface area A of the infrared detection system (a) are expressed as %.

このように本発明に係る焦電形赤外検出素子は赤外線セ
ンサとして実用上正視される電圧感度1(V。
As described above, the pyroelectric infrared detection element according to the present invention has a voltage sensitivity of 1 (V) which can be viewed directly as an infrared sensor in practical use.

比検出能■Nなどすぐれているばかりでなく9例えば9
5%相対湿度、40°Cの葵囲気下にて100 (1時
間連続動作させても特性の劣化はほとんど認められず、
長期間に亘って赤外線検出素子としてのイ虎11目を十
分にX(fj を青するととも確認された。
Ratio detection ability■ Not only is it excellent such as N, but also 9 For example, 9
100 at 5% relative humidity and 40°C (with almost no deterioration in characteristics even after continuous operation for 1 hour,
It was also confirmed that the X (fj) of the 11th eye of the tiger as an infrared detection element was sufficiently blue over a long period of time.

尚上記にオSいては焦電形赤外線検出素子の本体の主成
分をなすゼJ合ペロブスカイト桔造を採る( Pb C
a ) [I (Co I/2 W)/2)’I”l 
〕03系においてTi及び(COl、/2W、/2)の
比を一定にし、 PbとCaO比を変えた例を示したが
、CaO代りにBa、Srを用いた」ハ合も。
In the case of the above, the main component of the main body of the pyroelectric infrared detection element is a perovskite (PbC).
a) [I (Co I/2 W)/2)'I”l
] In the 03 system, an example was shown in which the ratio of Ti and (COl, /2W, /2) was kept constant and the ratio of Pb and CaO was changed, but it is also possible to use Ba and Sr instead of CaO.

また′1゛1と(Cot/2 Wl/2 )の比を0.
01〜0.10の範囲に変えた場合もほぼ同様の性能を
ボした。
Also, the ratio of '1゛1 and (Cot/2 Wl/2) is 0.
Almost the same performance was obtained when the value was changed to a range of 0.01 to 0.10.

本発明に係る焦電形赤外線検出素子の本体主栄、y部を
構成する上記一般式 %式% の一部をなすPb(Co□/2 Wl/2)03は焼結
過程において、焼成Yn度の低下、結晶粒の異常成長抑
制に寄与する役目を果し、その組成比、即ち上記一般式
におけるyの値は0.01〜0.10の範囲内に選ぶ必
要がある。その叩出は0.01未満では上述の焼成温度
低下などの効果がなく9寸だ0.10を超えると誘電率
が大きくなり過き、実用面で、・電圧に対する評価指数
が低下し、赤外線センサとして性能が良好でな力1つた
っ ′ さ′)に上記(J”)+−x N1ex)〔(COI/
2 Wl/2 ) y ”1−y ) 03に添加含有
するLin0.NiOおよびFe 203の群から選ば
れた少なくとも1柿の酸化物は得られた焦電形焼結体の
分体処理の?や易化に寄与する役目を果す。しかしてこ
の(’fQ加合有14が重量比で001%未’li’B
でも、゛ま/こ2%を超えても、焦電性の急激な低下を
招来するとともに焼結性や分極処理性が損なわれる仙向
があるため、添加含有量・は常に001〜2重袖%の範
囲内に選択する必要がある。
In the sintering process, Pb(Co□/2 Wl/2)03, which is a part of the general formula % formula %, which constitutes the main body and y part of the pyroelectric infrared detecting element according to the present invention, is The composition ratio, that is, the value of y in the above general formula, must be selected within the range of 0.01 to 0.10. If the knock-out is less than 0.01, there will be no effect such as lowering the firing temperature mentioned above, and if it exceeds 0.10, the dielectric constant will become too large, and from a practical point of view, the evaluation index for voltage will decrease, and the infrared The performance as a sensor is good, and the above (J") + - x N1ex) [(COI/
At least one persimmon oxide selected from the group of Lin0.NiO and Fe203 added to 2Wl/2)y''1-y)03 was added to the resulting pyroelectric sintered body during the separation treatment. However, this ('fQ addition 14 is not 001% by weight)
However, even if it exceeds 2%, the pyroelectricity will drop sharply and the sinterability and polarization properties will be impaired. It is necessary to select within the range of sleeve percentage.

〔発明の効果〕〔Effect of the invention〕

上記の如く9本発明によれば、一般式(PJ−8Mex
)〔(CO1/2Xへ’+/2)y’l”t−y:]0
3で示される複合ペロブスカイト構造のものK N4n
O,Neo、 Fe203 ノうちから選んだ少なくと
も1種を重量比で0.01〜2%添加含有してなるセラ
ミック焼結体を赤外線検出素子本体としている。しかし
て前記セラミック焼結体は、大きな焦電係数を有する川
5niffる焦″に形で。
As described above, according to the present invention, the general formula (PJ-8Mex
) [(CO1/2X'+/2)y'l"t-y:]0
K N4n with a composite perovskite structure shown in 3
The main body of the infrared detecting element is a ceramic sintered body containing at least one selected from O, Neo, and Fe203 in an amount of 0.01 to 2% by weight. Therefore, the ceramic sintered body is in the form of a pyroelectric material having a large pyroelectric coefficient.

低い誘電率を有しており、赤外検出素子としてもすぐれ
た特性を備えている。
It has a low dielectric constant and has excellent characteristics as an infrared detection element.

即ちこの種赤外検出素子として要求される評価指数F■
に大きく寄与する焦電係数P(C/crn2−(3)が
大で、また比誘電率εが小さいと云う特長がある。
In other words, the evaluation index F■ required for this type of infrared detection element
It is characterized by a large pyroelectric coefficient P(C/crn2-(3)) that greatly contributes to the , and a small relative dielectric constant ε.

しかしt実用面からみては赤外線照射に対する応答とし
ての電圧感度Ityが高く、一方り1(音出力は低いの
で、高い比検出能りを発揮する。換言すれば高い感度を
もって、信頼性高く、赤外線を113:易に検出できる
。しかも経時特性も良好で長>uJ間に亘って所妥の赤
外線検出機能を保持発揮する。かくして本発明に係る赤
外線検出素子は焼結し易くまた分極処理も高々100°
C程度の温度40〜5QkV/信の分極′1圧で足り、
製造もし易い点などと相俟って実用に好適する焦電形赤
外線検出素子と云える。
However, from a practical point of view, the voltage sensitivity Ity as a response to infrared irradiation is high, while the sound output is low, so it exhibits high specific detection ability. In other words, it has high sensitivity, high reliability, and 113: can be easily detected.Furthermore, the aging characteristics are also good, and the desired infrared detection function is retained and exhibited over a long period of time > uJ.Thus, the infrared detection element according to the present invention is easy to sinter and can be easily polarized. 100°
A temperature of about 40 to 5 QkV/cm and a polarization pressure of 1 is sufficient.
Coupled with the fact that it is easy to manufacture, it can be said that it is a pyroelectric infrared detection element suitable for practical use.

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

第1図は本発明に係る焦電形赤外線検出素子の一ド・り
について焦[iN係数、比誘’lJj率および評価指数
と組成との関係をそれぞれ示す曲線図、第2図は同じく
本発明に係る焦r4(形赤外線検出素子の一例について
組成とキュリー輻度との関係を示す曲線し:(、第3図
は本発明に係る焦電形赤外線検出素子についての特性測
定回路図である。 (al・・・赤外線検出素子、(Ill・・赤外4碌。 (Cl・・・高抵抗負荷、(e)・・・1h源端子。 (fl・・・出力端子、(g)・・アース代理人 弁J
jp士 則 近 憲 佑 (ほか 1名) 第1図 Ca ffl x (mol) −
Figure 1 is a curve diagram showing the relationship between the pyroelectric coefficient, dielectric constant, evaluation index, and composition for one pulse of the pyroelectric infrared detecting element according to the present invention. A curve showing the relationship between the composition and the Curie intensity for an example of the pyroelectric infrared detecting element according to the invention: (al... Infrared detection element, (Ill... Infrared 4-pin. (Cl... High resistance load, (e)... 1h source terminal. (fl... Output terminal, (g)...・Earth Agent Ben J
Kensuke Chika (and 1 other person) Fig. 1 Ca ffl x (mol) −

Claims (1)

【特許請求の範囲】 一般式 %式%) (式中MeはBa、 8r、 Caのうちから選ばれた
少なくとも1種の元素、Xは0.05〜0.35の数値
、yは0.01〜0.10の数値) で示される複合ペロプスカイト構造のものにMnO。 Nip、 Fe2 o3のうちから選ばれた少なくとも
1種をit比で0.01〜2%添加配合してなる焼結体
K。 対をなす電極を設けて成ることを特徴とする焦電形赤外
線検出素子。
[Claims] General formula %) (In the formula, Me is at least one element selected from Ba, 8r, and Ca, X is a numerical value of 0.05 to 0.35, and y is 0. 01 to 0.10) MnO has a composite perovskite structure. A sintered body K formed by adding and blending at least one selected from Nip and Fe2O3 in an IT ratio of 0.01 to 2%. A pyroelectric infrared detection element characterized by comprising a pair of electrodes.
JP59042917A 1984-03-08 1984-03-08 Pyroelectric type infrared ray decting element Pending JPS60191051A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59042917A JPS60191051A (en) 1984-03-08 1984-03-08 Pyroelectric type infrared ray decting element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59042917A JPS60191051A (en) 1984-03-08 1984-03-08 Pyroelectric type infrared ray decting element

Publications (1)

Publication Number Publication Date
JPS60191051A true JPS60191051A (en) 1985-09-28

Family

ID=12649367

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59042917A Pending JPS60191051A (en) 1984-03-08 1984-03-08 Pyroelectric type infrared ray decting element

Country Status (1)

Country Link
JP (1) JPS60191051A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0608948A2 (en) * 1993-01-26 1994-08-03 Minister Of Agriculture, Fisheries And Food In Her Britannic Majesty's Gov. Of The U.K. Of Great Britain And Northern Ireland Activity monitors
JP2020007198A (en) * 2018-07-11 2020-01-16 日本セラミック株式会社 Pyroelectric porcelain material for pyroelectric infrared sensor compatible with surface mounting

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0608948A2 (en) * 1993-01-26 1994-08-03 Minister Of Agriculture, Fisheries And Food In Her Britannic Majesty's Gov. Of The U.K. Of Great Britain And Northern Ireland Activity monitors
EP0608948A3 (en) * 1993-01-26 1995-01-18 Mini Agriculture & Fisheries Activity monitors.
JP2020007198A (en) * 2018-07-11 2020-01-16 日本セラミック株式会社 Pyroelectric porcelain material for pyroelectric infrared sensor compatible with surface mounting

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