JPH0556470B2 - - Google Patents

Info

Publication number
JPH0556470B2
JPH0556470B2 JP58201739A JP20173983A JPH0556470B2 JP H0556470 B2 JPH0556470 B2 JP H0556470B2 JP 58201739 A JP58201739 A JP 58201739A JP 20173983 A JP20173983 A JP 20173983A JP H0556470 B2 JPH0556470 B2 JP H0556470B2
Authority
JP
Japan
Prior art keywords
layer
amorphous semiconductor
ray
conductive layer
window
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
Application number
JP58201739A
Other languages
Japanese (ja)
Other versions
JPS6093372A (en
Inventor
Tokuzo Komai
Tomomi Katayama
Tatsuo Hashizume
Yasuyoshi Doi
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.)
Shimadzu Corp
Original Assignee
Shimadzu Corp
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 Shimadzu Corp filed Critical Shimadzu Corp
Priority to JP58201739A priority Critical patent/JPS6093372A/en
Publication of JPS6093372A publication Critical patent/JPS6093372A/en
Publication of JPH0556470B2 publication Critical patent/JPH0556470B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01TMEASUREMENT OF NUCLEAR OR X-RADIATION
    • G01T1/00Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation
    • G01T1/16Measuring radiation intensity
    • G01T1/20Measuring radiation intensity with scintillation detectors
    • G01T1/2018Scintillation-photodiode combinations

Landscapes

  • Physics & Mathematics (AREA)
  • Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • High Energy & Nuclear Physics (AREA)
  • Molecular Biology (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • Measurement Of Radiation (AREA)
  • Light Receiving Elements (AREA)

Description

【発明の詳細な説明】 (イ) 産業上の利用分野 この発明は、X線自動露出制御装置等に用いる
のに最適な半導体X線検出器に関する。
DETAILED DESCRIPTION OF THE INVENTION (a) Field of Industrial Application This invention relates to a semiconductor X-ray detector that is most suitable for use in automatic X-ray exposure control devices and the like.

(ロ) 従来技術 X線自動露出制御装置に用いる場合、X線検出
器は、通常、被検体とX線フイルムとの間に配置
される。ところで近年、単結晶半導体を用いてX
線検出器が使用され始めている。しかし、従来の
単結晶半導体を用いたX線検出器は、半導体とそ
の支持具材とのX線吸収差によつてX線フイルム
に濃度差が生じ、X線写真の読影時に障害となる
という欠点があつた。この濃度差が生じないよう
な構造の半導体X線検出器も提案されている(特
開昭55−146071号公報参照)が、X線検出器全体
の構造が複雑になつている。
(b) Prior Art When used in an automatic X-ray exposure control device, an X-ray detector is usually placed between the subject and the X-ray film. By the way, in recent years, X
Ray detectors are beginning to be used. However, with conventional X-ray detectors using single-crystal semiconductors, differences in X-ray absorption between the semiconductor and its supporting material cause density differences in the X-ray film, which poses an obstacle when interpreting X-ray photographs. There were flaws. A semiconductor X-ray detector with a structure that does not cause this concentration difference has also been proposed (see Japanese Patent Laid-Open No. 146071/1983), but the overall structure of the X-ray detector is complicated.

まだ、X線検出器は、特定の臓器等の診断部位
に対応した形状の大きな面積のものが好ましい
が、従来の半導体X線検出器では任意の大きさの
ものや任意の形状のものを製作することは非常に
困難である。
It is still preferable for an X-ray detector to have a large area and a shape that corresponds to the diagnostic site of a specific organ, etc., but conventional semiconductor X-ray detectors can be manufactured to any size or shape. It is very difficult to do so.

(ハ) 目的 この発明は、簡単な構造でありながら半導体と
その支持具材とのX線吸収差による陰影を取り除
き、しかもX線に対する有感部を診断部位に対応
した形状・大きさとすることが容易な半導体X線
検出器を提供することを目的とする。
(C) Purpose This invention has a simple structure, yet eliminates shadows due to the difference in X-ray absorption between the semiconductor and its supporting material, and also makes the X-ray sensitive part have a shape and size that corresponds to the diagnosis site. An object of the present invention is to provide a semiconductor X-ray detector that is easy to operate.

(ニ) 構成 この発明による半導体X線検出器は、X線吸収
の少ない均一な基板と、該基板上の全面に形成さ
れた第1の導電層と、該導電層上の全面に形成さ
れた非晶質半導体層と、該非晶質半導体層上の全
面に、所定領域の窓部を残して形成された絶縁層
と、該絶縁層の全面および上記窓部の上に形成さ
れ、窓部において上記非晶質半導体層に接触する
透明な第2の導電層と、該第2の導電層上の全面
に形成された蛍光層とを有することによつて構成
されている。
(d) Structure The semiconductor X-ray detector according to the present invention includes a uniform substrate with low X-ray absorption, a first conductive layer formed on the entire surface of the substrate, and a first conductive layer formed on the entire surface of the conductive layer. an amorphous semiconductor layer, an insulating layer formed on the entire surface of the amorphous semiconductor layer leaving a window in a predetermined region, and an insulating layer formed on the entire surface of the insulating layer and on the window, and an The device includes a transparent second conductive layer in contact with the amorphous semiconductor layer, and a fluorescent layer formed on the entire surface of the second conductive layer.

(ホ) 実施例 第1図A,Bにおいて、基板11はX線吸収の
少ない均一な薄いシート状物、たとえばポリイミ
ドフイルムなどの樹脂フイルムからなり、その大
きさはX線フイルムのサイズと同等若しくはそれ
より大きいものとする。そしてこの基板11の表
面に電極をなすアルミニウムなどの蒸着層(図示
しない)が設けられており、さらにその上に全面
にわたつて非晶質半導体層(アモルフアス半導体
層)12が数十〜数百μmの厚さに一様に形成さ
れている。この非晶質半導体層12は、たとえ
ば、Si、AsGa、Geに必要なドープ剤を混入した
ものまたはこれらの混合物あるい化合物を用いた
PIN(P層−絶縁層−N層)構造とする。この非
晶質半導体層12の全面上に設けられた図示しな
い透明電極の上に、必要な大きさ・形状の孔が切
り抜かれている遮光シートを貼り付けるかあるい
は蒸着などの手段により透明窓部14を有する遮
光層13が形成されている。さらにこの遮光層1
3上には蛍光層15が設けられている。この蛍光
層15はX線を可視光に変換するものであり、遮
光層13はこの可視光を遮るもので、透明窓部1
4は可視光に対して透明な部分である。なお、基
板11は非晶質半導体層12の一方の電極を兼ね
たアルミニウム板で構成することもできる。
(E) Embodiment In FIGS. 1A and 1B, the substrate 11 is made of a uniform thin sheet-like material with low X-ray absorption, for example, a resin film such as a polyimide film, and its size is equal to or equal to the size of the X-ray film. It shall be larger than that. A vapor deposited layer (not shown) of aluminum or the like is provided on the surface of this substrate 11 to form an electrode, and several tens to hundreds of amorphous semiconductor layers 12 are formed over the entire surface. It is formed uniformly to a thickness of μm. This amorphous semiconductor layer 12 is made of, for example, Si, AsGa, Ge mixed with a necessary dopant, or a mixture or compound of these.
It has a PIN (P layer-insulating layer-N layer) structure. A transparent window is formed by pasting a light-shielding sheet in which holes of the required size and shape are cut out on the transparent electrode (not shown) provided on the entire surface of the amorphous semiconductor layer 12, or by vapor deposition. A light shielding layer 13 having 14 is formed. Furthermore, this light shielding layer 1
A fluorescent layer 15 is provided on 3. The fluorescent layer 15 converts X-rays into visible light, and the light shielding layer 13 blocks this visible light.
4 is a portion transparent to visible light. Note that the substrate 11 can also be formed of an aluminum plate that also serves as one electrode of the amorphous semiconductor layer 12.

こうして形成される半導体X線検出器は、その
蛍光層15の前面端よりX線が入射するようにし
て使用される。入射したX線は蛍光層15により
可視光に変換される。この可視光は遮光層13の
透明窓部14のみを通過し、非晶質半導体層12
に入射し、この非晶質半導体層12によつて電気
量に変換される。この非晶質半導体層12はX線
に対してはほとんど感度を有さないが、可視光に
対しては良好な感度を持つているので、蛍光層1
5でX線を一旦可視光に変換してこの可視光に感
応させるようにしているのである。
The semiconductor X-ray detector thus formed is used so that X-rays are incident on the front end of the fluorescent layer 15. The incident X-rays are converted into visible light by the fluorescent layer 15. This visible light passes only through the transparent window section 14 of the light shielding layer 13 and passes through the amorphous semiconductor layer 12.
and is converted into an electrical quantity by this amorphous semiconductor layer 12. This amorphous semiconductor layer 12 has almost no sensitivity to X-rays, but has good sensitivity to visible light, so the fluorescent layer 12
In step 5, the X-rays are first converted into visible light, and the device is made to be sensitive to this visible light.

そして、透明窓部14以外は遮光層13で遮光
されるため、この透明窓部14の部分がX線に対
する有感部となる。
Since the light shielding layer 13 blocks light except for the transparent window section 14, the transparent window section 14 becomes a sensitive section for X-rays.

次に第2の実施例について第2図A,Bを参照
しながら説明する。この第2図A,Bにおいて、
基板21、非晶質半導体層22および蛍光層25
は第1の実施例の基板11、非晶質半導体層12
および蛍光層15と同様なものからなる。この第
2図Bでは導電層26が描かれているが、この導
電層26は蒸着などによつて基板21の全面に設
けられ、非晶質半導体層22の一方の電極および
引き出し線を兼ねたものとして機能する。非晶質
半導体層22の他方(図では上方)の面上には窓
部24を有するよう絶縁層27が形成される。こ
の絶縁層27は蒸着などの手段によつて形成して
もよいし、あるいは必要な位置に必要な大きさ・
形状の孔を有する薄い絶縁シートを貼り付けて形
成してもよい。この絶縁層27および窓部24の
上には全面にわたつて蒸着などにより透明導電層
28が形成されており、この透明導電層28は窓
部24においてのみ非晶質半導体層22と接触し
ている。そしてこのような構造の全体は遮光膜2
9で完全に覆われている。
Next, a second embodiment will be described with reference to FIGS. 2A and 2B. In this Figure 2 A and B,
Substrate 21, amorphous semiconductor layer 22 and fluorescent layer 25
are the substrate 11 and the amorphous semiconductor layer 12 of the first embodiment.
and is made of the same material as the fluorescent layer 15. A conductive layer 26 is depicted in FIG. 2B, and this conductive layer 26 is provided over the entire surface of the substrate 21 by vapor deposition or the like, and also serves as one electrode and lead wire of the amorphous semiconductor layer 22. function as a thing. An insulating layer 27 is formed on the other (upper side in the figure) surface of the amorphous semiconductor layer 22 so as to have a window 24 . This insulating layer 27 may be formed by means such as vapor deposition, or it may be formed in the required position and in the required size.
It may also be formed by pasting a thin insulating sheet having shaped holes. A transparent conductive layer 28 is formed over the entire surface of the insulating layer 27 and the window 24 by vapor deposition, and this transparent conductive layer 28 is in contact with the amorphous semiconductor layer 22 only at the window 24. There is. The entire structure is covered with a light shielding film 2.
9 is completely covered.

この場合、非晶質半導体層22は面方向には導
電性が非常に悪いので、電極が接触している窓部
24の部分で生じた光電流出力が2つの導電層2
6,28より取り出される。したがつて、X線が
入射して蛍光層25が発光すると、絶縁層27が
なく透明導電層28が直接接触している窓部24
の部分での光電流出力が得られるので、この窓部
24の部分がX線に対する有感部ということにな
る。
In this case, since the amorphous semiconductor layer 22 has very poor conductivity in the plane direction, the photocurrent output generated at the window portion 24 where the electrodes are in contact is transferred to the two conductive layers 2.
6,28. Therefore, when X-rays are incident and the fluorescent layer 25 emits light, the window portion 24 where there is no insulating layer 27 and the transparent conductive layer 28 is in direct contact with
Since a photocurrent output is obtained at the portion, this window portion 24 is a sensitive portion for X-rays.

なお、窓部24は1箇所だけに限らず、必要な
ら第2図Aに示すように複数個設けて複数個の有
感部を形成することも可能である。この場合透明
導電層28を第2図Aに示すように分割してそれ
ぞれの有感部からの出力を別個独立に取り出して
それらを加算したり平均したりまたは最大値や最
小値を求めるなどしてX線フイルム濃度をよりき
め細かに制御することもできるし、分割しなけれ
ば複数個の有感部の出力の総和に対応する出力を
取り出すことができる。第1の実施例ではこのこ
とについて触れなかつたが、第1の実施例でも同
様であることは勿論である。
Note that the window portion 24 is not limited to one location, and if necessary, a plurality of window portions 24 may be provided as shown in FIG. 2A to form a plurality of sensitive portions. In this case, the transparent conductive layer 28 is divided as shown in FIG. 2A, and the outputs from each sensitive part are taken out separately and independently, and they are added or averaged, or the maximum and minimum values are determined. The density of the X-ray film can be controlled more precisely by using the X-ray film, and if it is not divided, an output corresponding to the sum of the outputs of a plurality of sensitive parts can be extracted. Although this was not mentioned in the first embodiment, it goes without saying that the same applies to the first embodiment.

(ヘ) 効果 この発明による半導体X線検出器は、X線吸収
の少ない均一な基板上に非晶質半導体層を形成
し、さらにその上に蛍光層を形成してなるので、
構造がきわめて簡単であり大面積のものが容易に
製造できる。また、非晶質半導体を用いているの
で、単結晶半導体を用いた場合に比べて1/10程度
の厚さで済み、X線吸収が少なく、X線フイルム
上に陰影を生じることがない。しかも第2の導電
層と非晶質半導体層との間に、窓部を有する絶縁
層を介在させるというきわめて簡単な構成であ
り、さらに、その絶縁層の窓部の面積・形状を所
望のものにするだけで、X線に対する有感部を診
断部位に応じた形状とすることが簡単にできると
ともに、このようにしてもフイルム上に陰影が現
われることがない。
(f) Effects The semiconductor X-ray detector according to the present invention is formed by forming an amorphous semiconductor layer on a uniform substrate with low X-ray absorption, and further forming a fluorescent layer on top of the amorphous semiconductor layer.
The structure is extremely simple, and large-area products can be manufactured easily. Furthermore, since an amorphous semiconductor is used, the thickness is approximately 1/10 that of a single-crystal semiconductor, and X-ray absorption is low, so no shadows are formed on the X-ray film. Moreover, it has an extremely simple structure in which an insulating layer having a window is interposed between the second conductive layer and the amorphous semiconductor layer, and the area and shape of the window in the insulating layer can be adjusted as desired. By simply doing this, it is possible to easily shape the X-ray sensitive area in accordance with the diagnostic site, and even with this, no shadows appear on the film.

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

第1図A,Bはこの発明の第1の実施例に係る
もので、第1図Aは平面図、第1図Bは第1図A
のB−B線で断面した断面図、第2図A,Bはこ
の発明の第2の実施例に係るもので、第2図Aは
平面図、第2図Bは第2図AのB−B線で断面し
た断面図である。 11,21……基板、12,22……非晶質半
導体層、13……遮光層、14,24……窓部、
15,25……蛍光層、26……導電層、27…
…絶縁層、28……透明導電層、29……遮光
膜。
1A and 1B relate to the first embodiment of the present invention, FIG. 1A is a plan view, and FIG. 1B is a plan view of FIG. 1A.
A cross-sectional view taken along the line B-B of FIG. 2A and FIG. - It is a cross-sectional view taken along the B line. 11, 21... Substrate, 12, 22... Amorphous semiconductor layer, 13... Light shielding layer, 14, 24... Window section,
15, 25... Fluorescent layer, 26... Conductive layer, 27...
... Insulating layer, 28 ... Transparent conductive layer, 29 ... Light shielding film.

Claims (1)

【特許請求の範囲】[Claims] 1 X線吸収の少ない均一な基板と、該基板上の
全面に形成された第1の導電層と、該導電層上の
全面に形成された非晶質半導体層と、該非晶質半
導体層上の全面に、所定領域の窓部を残して形成
された絶縁層と、該絶縁層の全面および上記窓部
の上に形成され、窓部において上記非晶質半導体
層に接触する透明な第2の導電層と、該第2の導
電層上の全面に形成された蛍光層とを有してなる
半導体X線検出器。
1. A uniform substrate with low X-ray absorption, a first conductive layer formed on the entire surface of the substrate, an amorphous semiconductor layer formed on the entire surface of the conductive layer, and a first conductive layer formed on the entire surface of the conductive layer, and an insulating layer formed on the entire surface of the insulating layer leaving a window in a predetermined region, and a transparent second layer formed on the entire surface of the insulating layer and on the window and in contact with the amorphous semiconductor layer at the window. A semiconductor X-ray detector comprising: a conductive layer; and a fluorescent layer formed entirely on the second conductive layer.
JP58201739A 1983-10-27 1983-10-27 semiconductor x-ray detector Granted JPS6093372A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58201739A JPS6093372A (en) 1983-10-27 1983-10-27 semiconductor x-ray detector

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58201739A JPS6093372A (en) 1983-10-27 1983-10-27 semiconductor x-ray detector

Publications (2)

Publication Number Publication Date
JPS6093372A JPS6093372A (en) 1985-05-25
JPH0556470B2 true JPH0556470B2 (en) 1993-08-19

Family

ID=16446131

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58201739A Granted JPS6093372A (en) 1983-10-27 1983-10-27 semiconductor x-ray detector

Country Status (1)

Country Link
JP (1) JPS6093372A (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6271881A (en) * 1985-09-26 1987-04-02 Toshiba Corp Radiation detector
NL8503153A (en) * 1985-11-15 1987-06-01 Optische Ind De Oude Delft Nv DOSEMETER FOR IONIZING RADIATION.
JPS63243781A (en) * 1987-03-30 1988-10-11 Kanegafuchi Chem Ind Co Ltd X-ray detector
JP2638914B2 (en) * 1988-04-22 1997-08-06 富士通株式会社 X-ray intensity measurement method for exposure

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS55146071A (en) * 1979-05-02 1980-11-14 Toshiba Corp Radiant ray detector of semiconductor
JPS57172273A (en) * 1981-04-17 1982-10-23 Toshiba Corp Radiation detector

Also Published As

Publication number Publication date
JPS6093372A (en) 1985-05-25

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