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JPS6037920B2 - X-ray image storage display element - Google Patents
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JPS6037920B2 - X-ray image storage display element - Google Patents

X-ray image storage display element

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Publication number
JPS6037920B2
JPS6037920B2 JP51069751A JP6975176A JPS6037920B2 JP S6037920 B2 JPS6037920 B2 JP S6037920B2 JP 51069751 A JP51069751 A JP 51069751A JP 6975176 A JP6975176 A JP 6975176A JP S6037920 B2 JPS6037920 B2 JP S6037920B2
Authority
JP
Japan
Prior art keywords
phase
electrode
image storage
display element
insulating liquid
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
JP51069751A
Other languages
Japanese (ja)
Other versions
JPS52153455A (en
Inventor
哲夫 石井
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.)
Fujifilm Business Innovation Corp
Original Assignee
Fuji Xerox 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 Fuji Xerox Co Ltd filed Critical Fuji Xerox Co Ltd
Priority to JP51069751A priority Critical patent/JPS6037920B2/en
Publication of JPS52153455A publication Critical patent/JPS52153455A/en
Publication of JPS6037920B2 publication Critical patent/JPS6037920B2/en
Expired legal-status Critical Current

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  • Conversion Of X-Rays Into Visible Images (AREA)
  • Combination Of More Than One Step In Electrophotography (AREA)
  • Electrochromic Elements, Electrophoresis, Or Variable Reflection Or Absorption Elements (AREA)
  • Apparatus For Radiation Diagnosis (AREA)

Description

【発明の詳細な説明】 本発明は新規なX線画像蓄積表示素子に関する。[Detailed description of the invention] The present invention relates to a novel X-ray image storage and display device.

最近、銀ハラィド乳剤フィルム(以下線塩フィルムとい
う)を用いないX線画像形成方法がいろいろ発表された
いる。
Recently, various X-ray image forming methods that do not use silver halide emulsion films (hereinafter referred to as ray salt films) have been announced.

その代表的なものは光半導体のX線感光性を利用したゼ
ロラジオグラフィ−で、ゼロックス社よりシステム12
5として商品化されている。一方、気体や絶縁性液体の
電磁現象を利用したィオノグラフイーと呼ばれるものが
ある。ゼロラジオグラフイー及びイオノグラフイーはと
もに電子写真法を利用した現像方法で、その特徴である
エッジ効果により従来の銀塩フィルムでは満足な画像を
得られなかった低コントラスト部分の識別性が非常によ
いが、ゼロラジオグラフィーは一般に感度が低く、また
ィオノグラフィ−は絶縁性液体の汚染などによる導電率
変化を防止するのに注意を要し、そのため装置が大がか
りになるといった欠点があった。そこで密閉したチャン
バ−内に絶縁性液体を封入して潜像をチャンバー外部に
形成し、これを直接あるいは転写して現像することが試
みられた。すなわち第1図に示すように、放射線透過性
の高い電極2と平行しかつ間隙を存するようにスベーサ
4を介して対設された高絶縁性フィルム3と、上記電極
2及び高絶縁性フィルム3の間に放射線吸収効率の高い
絶縁性液体5を封入したチャンバー1を、第2図に示す
ような構成で配置し、まず帯電器10で高絶縁性フィル
ム3を帯電し、次いで被検体9を介して放射線を照射し
ながら、帯電器1川こて逆極性帯電して静電潜像をチヤ
ンバー1の表面に形成し、これを従来の電子写真法によ
り現像する方法である。しかし、このチャンバー1を実
用に供するように大型化して胸部撮影等のように垂直近
く立てて使用すると、第3図に示すように高絶縁性フィ
ルム3脚が、絶縁性液体5の重力により下方にかたより
蟹曲突起状に変形して使用不可能となる。またこのよう
な電子写真法による現像では可視化のため現像処理工程
が必要であり、しかもそのため解像力等が低下する廉れ
があった。本発明は上記事情に鑑みなされたものであり
、その目的はX線画像を蓄積し、それを周囲光で観察で
き、しかも自由に消去できるX線画像蓄積表示素子を提
供するものである。
A representative example of this is xeroradiography, which utilizes the X-ray sensitivity of photosemiconductors.
It has been commercialized as 5. On the other hand, there is something called ionography that uses electromagnetic phenomena in gases and insulating liquids. Both xeroradiography and ionography are development methods that utilize electrophotography, and their characteristic edge effect makes it very easy to distinguish low-contrast areas where conventional silver halide films could not obtain satisfactory images. However, xeroradiography generally has low sensitivity, and ionography requires care to prevent changes in conductivity due to contamination of the insulating liquid, resulting in a large-scale apparatus. Therefore, attempts have been made to seal an insulating liquid in a closed chamber, form a latent image outside the chamber, and develop this latent image either directly or by transfer. That is, as shown in FIG. 1, there is a highly insulating film 3 that is parallel to and opposite to the highly radiolucent electrode 2 with a spacer 4 in between, and the electrode 2 and the highly insulating film 3. A chamber 1 filled with an insulating liquid 5 with high radiation absorption efficiency is arranged between the chambers as shown in FIG. In this method, an electrostatic latent image is formed on the surface of the chamber 1 by charging the chamber 1 with reverse polarity while irradiating radiation through the chamber 1, and this is developed by a conventional electrophotographic method. However, when this chamber 1 is enlarged for practical use and used in a nearly vertical position for chest radiography, the three legs of the highly insulating film are pushed downward by the gravity of the insulating liquid 5, as shown in FIG. It deforms into a crab-shaped protrusion and becomes unusable. Further, development by such electrophotography requires a development process for visualization, and this has the disadvantage of lowering resolution and the like. The present invention has been made in view of the above circumstances, and its object is to provide an X-ray image storage/display element that can store X-ray images, observe them in ambient light, and erase them freely.

以下第4図以降を参照して本発明の実施例を説明する。Embodiments of the present invention will be described below with reference to FIG. 4 and subsequent figures.

本発明のX線画像蓄積表示素子は第4図に示すように、
X線透過性の高い電極11、X線吸収効率の高い絶縁性
液体12、誘電性鏡面層13、強議電層と反強議電層あ
るいは常議電層が組成変態相境界を有して共存する電気
光学セラミック固溶体14、透明電極.15を積層し、
上記絶縁性液体12はスべ−サ16にて電極11と誘電
性鏡面層13の間に封入されている。本発明に用いるセ
ラミック固熔体14、例えばPLZTについて説明する
。PLZTとはPb(Zr・Ti)03系固溶体にLa
を添加したセラミックスPb(,★)Lax(ZrくQ
−y)Tiy),奪03の略称である。
As shown in FIG. 4, the X-ray image storage and display element of the present invention has the following features:
The electrode 11 with high X-ray transparency, the insulating liquid 12 with high X-ray absorption efficiency, the dielectric mirror layer 13, the strong electrolytic layer and the anti-strong electrolytic layer or the normal electrolytic layer have a compositional transformation phase boundary. Coexisting electro-optic ceramic solid solution 14, transparent electrode. 15 are stacked,
The insulating liquid 12 is sealed between the electrode 11 and the dielectric mirror layer 13 at a spacer 16. The ceramic solid body 14 used in the present invention, for example, PLZT, will be explained. PLZT is a Pb(Zr・Ti)03 solid solution containing La.
Ceramics Pb(,★)Lax(ZrkuQ
-y)Tiy), is an abbreviation for 03.

その製法‘まPb0’TiQ’Zr02,la203等
の酸化粉をボールミル内で蒸留水を加えて約2時間混合
し、ほぼ90ooで乾燥させて固め、次に800〜90
0qCで約1時間かけて仮焼のPはTを作り、均一のた
めこれを粉砕して乾燥、二次仮煉させる。そして、水分
添加後50〜60メッシュのナイロン製ふるいでふるい
にかけ圧粉体を成形した後、約120倣siの圧力を印
加するホットプレス法で焼結させ透明なセラミックを得
る。このようにして得られたPLZTは、強議題相(F
enaelectric、Phase)と反強議電相(
価tilerroeleccmcPhase)あるいは
常誘電相(ParaelectricPhase)とが
相成変化に対し、温度に対しては変化の少ない組成変態
相境界(Morphotropic、PhaseBo肌
船ry)を持ち、この転移が一次の場合は熱履歴が大き
く、高温から冷却した場合と、低温から加熱した場合と
では組成変態相境界は温度または組成に対し異つた場所
に生じ、降温組成変態境界と昇温組成変態境界にはさま
れや領域では一方の相は安定で、他方の相は準安定とな
り、両相とも共存可能である。
Its manufacturing method: Oxidized powders such as Pb0'TiQ'Zr02 and LA203 are mixed in a ball mill with distilled water for about 2 hours, dried at about 90 oo to solidify, and then 800 to 90 oo
P and T are calcined at 0qC for about 1 hour, and to make them uniform, they are ground, dried, and subjected to secondary calcining. After adding water, the powder is sieved through a 50 to 60 mesh nylon sieve to form a green compact, and then sintered by a hot press method applying a pressure of about 120 mm to obtain a transparent ceramic. The PLZT obtained in this way is
enaelectric, Phase) and Anti-Strong Telephone Minister (
The compositional transformation phase (Morphotropic, PhaseBo) has a phase boundary (Morphotropic, PhaseBo) that does not change much with respect to temperature, and if this transition is primary, the thermal history is large, and when cooling from a high temperature and heating from a low temperature, the composition transformation phase boundary occurs at a different location with respect to temperature or composition, and there is a region sandwiched between the cooling composition transformation boundary and the heating composition transformation boundary. One phase is stable and the other phase is metastable, and both phases can coexist.

熱履歴の温度範囲において強議鰭相と反強議略3相が共
存している場合は第5図に示すような二重ヒステリシス
曲線を示す。前述のPはTにおいてx,yの値に対して
PはTIO瓜/10W/100(1一y)と記して区別
すると0.05ミxミ0.1,0.6ミyミ0.8が一
般に熱履歴の温度範囲が広く、とく子にPWT7.6/
70/30では約15qoにも及ぶ。しかもこのセラミ
ック固溶体14は光を敬乱しない反強謎電体であるが、
電圧を印加すると結晶構造の異なる強謎電相が誘起され
光を激しく散乱する。そこで、第4図に示すような本発
明に係るX線画像蓄積表示素子に第6図に示されるよな
構成で鰭極11と透明電極15の間に電圧を印放しなが
らX線源8から被検体9を介してX線を照射すると、被
検体9を通過したX線量に応じて絶縁性液体12で正、
負イオン対または正イオンと電子が発生し、それぞれ対
応する電極側へ移動する。絶縁性液体としてはCCそ3
,CC夕3Br,CC夕31やその他原子番号17以上
の元素を含む分子混合化合0物であれば良い。すなわち
、X線照射を受けた絶縁性液体12は後様に導電状態と
なったのと同じでセラミック固溶体層14の両側の電界
強度を後様に変化させ強議電相を誘起する。この像様の
分極は第5図の二重ヒステリシス曲線から判るよう5に
電圧印加を停止しても残っており、これに透明電極15
側から光を照射すると、強譲電相のところは強く散乱さ
れ、反強誘電相の部分は散乱されない。それ故散乱像と
して画像が識別できる。この画像を消去するには、この
素子を加熱して、強議電相を無くせばよい。短時間で消
去したい場合は、第8図に示すように透明電極15の両
端に電極16,17を設け、それぞれNPN形トランジ
スター18,19のェミッタに接続すると共に、抵抗2
0,21を介して接地し、電極11を接地した構成でゲ
ートA,Bを周期数ミリ〜数10ミリ秒で交互に開閉し
、数10Vのパルス亀圧を印加する。このようにすれば
透明電極15内に電流が交互に流れ、透明電極15上の
電位は時間的、場所に変動するが時間平均をとると、両
電極間に一様な逆電圧として作用し、同時にジュール熱
で強譲電性のなくある温度以上に加熱できるので画像は
数分の1秒で完全に消去される。本発明に係るX線画像
蓄積表示素子は上述したごと〈、X線吸収率の高い絶縁
性液体12を電極11、誘電性鏡面層13、スベーサ1
6等の固い物質内に封入しており、大型化して垂直に立
てて使用してもその一部分が絶縁性液体12の重さで鴬
曲突起状に変形することもなく、しかも撮影後画像を任
意時間蓄積することができ、その画像は周囲光で見るこ
とができ、不必要になれば自由に消去できる。
When the strong fin phase and the anti-strong fin phase coexist in the temperature range of the thermal history, a double hysteresis curve as shown in FIG. 5 is shown. The above-mentioned P is 0.05 mm x 0.1, 0.6 mm y 0.0. 8 generally has a wide temperature range of thermal history, and PWT7.6/
At 70/30, it reaches about 15 qo. Moreover, this ceramic solid solution 14 is an anti-strong mysterious electric material that does not disturb light;
When a voltage is applied, a strong mysterious electric phase with a different crystal structure is induced and light is scattered violently. Therefore, the X-ray image storage/display element according to the present invention as shown in FIG. 4 is configured as shown in FIG. When X-rays are irradiated through the object 9, the insulating liquid 12 is applied to the
Negative ion pairs or positive ions and electrons are generated and each moves to the corresponding electrode side. CC So3 is an insulating liquid.
, CC-3Br, CC-31, and other molecular mixed compounds containing elements with an atomic number of 17 or more may be used. That is, the insulating liquid 12 that has been irradiated with X-rays becomes conductive, and changes the electric field strength on both sides of the ceramic solid solution layer 14 to induce a strong electromagnetic phase. As can be seen from the double hysteresis curve in FIG. 5, this image-like polarization remains even after the voltage application to the transparent electrode 15 is stopped.
When light is irradiated from the side, the ferroelectric phase is strongly scattered, and the antiferroelectric phase is not scattered. Therefore, the image can be identified as a scattering image. To erase this image, the element can be heated to eliminate the strong electromagnetic phase. If erasing is desired in a short time, electrodes 16 and 17 are provided at both ends of the transparent electrode 15 and connected to the emitters of NPN transistors 18 and 19 respectively, as shown in FIG.
0 and 21, and the electrode 11 is grounded, gates A and B are alternately opened and closed at a period of several milliseconds to several tens of milliseconds, and a pulse voltage of several tens of volts is applied. In this way, current flows alternately in the transparent electrode 15, and the potential on the transparent electrode 15 varies over time and location, but when averaged over time, it acts as a uniform reverse voltage between the two electrodes, At the same time, the image can be completely erased in a fraction of a second because it can be heated to a certain temperature using Joule heat without strong transference. As described above, the X-ray image storage display element according to the present invention includes an insulating liquid 12 having a high X-ray absorption rate, an electrode 11, a dielectric mirror layer 13, and a substrate 1.
It is enclosed in a hard material such as No. 6, so even if it is enlarged and used vertically, a part of it will not deform into a curved shape due to the weight of the insulating liquid 12, and furthermore, the image after shooting is It can be stored for any length of time, the image can be viewed in ambient light, and it can be erased at will when no longer needed.

また、画像蓄積には電圧印加を必要としないから持ち運
ぶことができ透視の場合のみならず。診断、観察用にも
利用できる。また、画像をハードコピーとして保存した
い場合は鏡面等を利用して従釆の電子複写機でコピーし
ておけば良い。
In addition, since no voltage is required for image storage, it can be carried around not only for fluoroscopy. It can also be used for diagnosis and observation. Furthermore, if you wish to save the image as a hard copy, you can copy it using a mirror surface or the like using a secondary electronic copying machine.

【図面の簡単な説明】 第1図は従来のィオノグラフィーに用いられるチャンバ
ーの断面図、第2図はその動作説明図、第3図はその不
具合説明図、第4図は本発明の実施例を示す断面図、第
5図は本発明に用いられるセラミック固溶体の二重ヒス
テリシス曲線、第6図、第7図、第8図はその動作説明
図である。 11は電極、12は絶縁性液体、13は譲電性鏡面層、
14は電気光学セラミック固熔体、15は透明電極、1
6はスベーサ。 第1図 第2図 第3図 第4図 第6図 第7図 第5図 第8図
[Brief Description of the Drawings] Figure 1 is a sectional view of a chamber used in conventional ionography, Figure 2 is a diagram explaining its operation, Figure 3 is a diagram explaining its defects, and Figure 4 is a diagram showing the implementation of the present invention. A sectional view showing an example, FIG. 5 is a double hysteresis curve of the ceramic solid solution used in the present invention, and FIGS. 6, 7, and 8 are diagrams explaining its operation. 11 is an electrode, 12 is an insulating liquid, 13 is a conductive specular layer,
14 is an electro-optic ceramic solid melt, 15 is a transparent electrode, 1
6 is subesa. Figure 1 Figure 2 Figure 3 Figure 4 Figure 6 Figure 7 Figure 5 Figure 8

Claims (1)

【特許請求の範囲】[Claims] 1 X線透過性の高い電極11、X線吸収効率の高い絶
縁性液体12、誘電性鏡面層13、強誘電相と反対誘電
相あるいは常誘電相が組成変態相境界を有して共存する
電気光学セラミツク固溶体層14、透明電極15を積層
し、上記絶縁性液体12をスペーサ16にて電極11と
誘電性鏡面層13の間に封入したことを特徴とするX線
画像蓄積表示素子。
1 An electrode 11 with high X-ray transparency, an insulating liquid 12 with high X-ray absorption efficiency, a dielectric mirror layer 13, an electric current in which a ferroelectric phase and an opposite dielectric phase or a paraelectric phase coexist with a compositional transformation phase boundary. An X-ray image storage and display element characterized in that an optical ceramic solid solution layer 14 and a transparent electrode 15 are laminated, and the insulating liquid 12 is sealed between the electrode 11 and the dielectric mirror layer 13 with a spacer 16.
JP51069751A 1976-06-16 1976-06-16 X-ray image storage display element Expired JPS6037920B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP51069751A JPS6037920B2 (en) 1976-06-16 1976-06-16 X-ray image storage display element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP51069751A JPS6037920B2 (en) 1976-06-16 1976-06-16 X-ray image storage display element

Publications (2)

Publication Number Publication Date
JPS52153455A JPS52153455A (en) 1977-12-20
JPS6037920B2 true JPS6037920B2 (en) 1985-08-29

Family

ID=13411802

Family Applications (1)

Application Number Title Priority Date Filing Date
JP51069751A Expired JPS6037920B2 (en) 1976-06-16 1976-06-16 X-ray image storage display element

Country Status (1)

Country Link
JP (1) JPS6037920B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5480469U (en) * 1977-11-17 1979-06-07

Also Published As

Publication number Publication date
JPS52153455A (en) 1977-12-20

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