JPH0795189B2 - Image information recording and reading method - Google Patents
Image information recording and reading methodInfo
- Publication number
- JPH0795189B2 JPH0795189B2 JP62084834A JP8483487A JPH0795189B2 JP H0795189 B2 JPH0795189 B2 JP H0795189B2 JP 62084834 A JP62084834 A JP 62084834A JP 8483487 A JP8483487 A JP 8483487A JP H0795189 B2 JPH0795189 B2 JP H0795189B2
- Authority
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- Japan
- Prior art keywords
- electromagnetic wave
- light
- image information
- panel
- recording
- 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.)
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- Radiography Using Non-Light Waves (AREA)
Description
【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、例えば放射線照射で画像を記録し、これを読
み取る方法に関する。The present invention relates to a method of recording an image by, for example, irradiation with radiation and reading the image.
この種の画像記録読取方法として、輝尽性蛍光体等で構
成されたパネルを記録媒体として使用し、人体等の画像
情報をX線を照射してそこに記録し、その後にその記録
パネルに励起光を走査照射して蛍光体を励起させ、それ
によって輝尽発光した蛍光光を光伝送体で光電変換素子
まで案内して、画像情報を読み取るようにした方法が知
られている。As an image recording / reading method of this kind, a panel made of a stimulable phosphor or the like is used as a recording medium, and image information of a human body or the like is irradiated therewith by X-rays to be recorded there, and then the recording panel is recorded. There is known a method in which excitation light is scan-irradiated to excite a fluorescent substance, and thereby fluorescent light emitted by stimulated emission is guided to a photoelectric conversion element by an optical transmission member to read image information.
ところが、この方法は、輝尽発光光を光ファイバ束等の
端面から集光して光電変換素子に導いているので、その
効率が芳しくない。また、この輝尽発光光はその波長が
約200nm〜500nm程度と短く、集光光学系における伝送効
率も低い。更に光電変換素子における変換効率も低いと
う問題があった。更に、この方法では輝尽発光光に比較
して極めて強力な励起光も一部が集光されるので、輝尽
発光光を励起光から分離して光電変換しなければなら
ず、励起光を遮断するための特殊なフィルタが必要とな
っていた。However, this method is not efficient because the stimulated emission light is condensed from the end face of the optical fiber bundle or the like and guided to the photoelectric conversion element. Further, the wavelength of this stimulated emission light is as short as about 200 nm to 500 nm, and the transmission efficiency in the condensing optical system is also low. Further, there is a problem that the conversion efficiency of the photoelectric conversion element is low. Furthermore, in this method, a part of the excitation light, which is extremely strong as compared with the stimulated emission light, is also collected, so the stimulated emission light must be separated from the excitation light and photoelectrically converted. A special filter to cut off was required.
本発明の目的は、上記したような問題点を一掃した画像
情報記録読取方法を提供することである。It is an object of the present invention to provide an image information recording / reading method that eliminates the above-mentioned problems.
このために本発明は、第1の電磁波を記録パネルに照射
して画像情報を記録し、第2の電磁波で該パネルを主走
査方向に主走査しながら該主走査方向と交差する方向に
相対的に副走査して上記パネルの記録面から第3の電磁
波を発生させ、上記パネルの上記主走査方向に形成され
る走査線に沿うよう配置させたロッド形状の波長変換媒
体を上記第2の電磁波の上記副走査に応じて上記副走査
と同一方向に相対的に移動させ、上記第3の電磁波を上
記波長変換媒体に入射させて第4の電磁波に変換し、該
第4の電磁波を光電変換して得られた電気信号を処理す
ることにより、上記画像情報を得るように構成した。For this reason, the present invention irradiates a recording panel with the first electromagnetic wave to record image information, and relatively scans the panel in the main scanning direction with the second electromagnetic wave in a direction intersecting with the main scanning direction. The sub-scanning to generate a third electromagnetic wave from the recording surface of the panel, and the rod-shaped wavelength conversion medium is arranged along the scanning line formed in the main scanning direction of the panel. In response to the sub-scanning of the electromagnetic wave, the electromagnetic wave is relatively moved in the same direction as the sub-scanning, the third electromagnetic wave is made incident on the wavelength conversion medium and converted into the fourth electromagnetic wave, and the fourth electromagnetic wave is photoelectrically converted. The image information is obtained by processing the electric signal obtained by the conversion.
以下、本発明の実施例について説明する。第1図は本発
明を実施するための装置の全体の概略を示す構成図であ
る。本実施例では、人体等の被写体1の背面にX線照射
器2、正面にグリッド3、フォトタイマ4、及び輝尽性
蛍光体パネル5を順次並べて配置し、その輝尽性蛍光体
パネル5に対して被写体1のX線透過画像を蛍光蓄積エ
ネルギーとして記録するようにしている。グリッド3は
X線照射器2の方向から以外の他から入射する(他で反
射若しくは散乱した)X線を遮蔽して正確なX線画像を
得るためのもの、フォトタイマ4はX線の照射蓄積量を
検出してX線照射器2を制御するためのものである。以
上のX線照射器2、グリッド3、フォトタイマ4等が記
録部分を構成する。Examples of the present invention will be described below. FIG. 1 is a block diagram showing an outline of an entire apparatus for carrying out the present invention. In the present embodiment, an X-ray irradiator 2 is provided on the back of a subject 1 such as a human body, a grid 3, a photo timer 4, and a stimulable phosphor panel 5 are sequentially arranged in front, and the stimulable phosphor panel 5 is arranged. On the other hand, the X-ray transmission image of the subject 1 is recorded as fluorescence accumulated energy. The grid 3 shields X-rays incident from other than the direction of the X-ray irradiator 2 (reflected or scattered by others) to obtain an accurate X-ray image, and the photo timer 4 irradiates X-rays. This is for detecting the accumulated amount and controlling the X-ray irradiator 2. The X-ray irradiator 2, the grid 3, the photo timer 4 and the like described above constitute a recording portion.
一方、読取部分は、半導体レーザ等を使用したビーム光
源6から光ビームを偏向器7で偏向(走査)して、ミラ
ー8等を経由して輝尽性蛍光体パネル5を走査し、その
走査光スポット部で発生する輝尽発光光をロッド状の光
変換伝導体9で扱い易い波長に波長変換して、その光変
換伝導体9で発生する光を、他の光を除去するフィルタ
10を介してPMT(フォトマルチプライヤ)11で光電変換
し、増幅器12で増幅した後にA/D変換器13でデジタル信
号に変換して、そのデジタル信号を図示しない画像処理
回路に送り、読取画像を得るようにしている。14は消去
ランプであり、これを点灯して輝尽性蛍光体パネル5を
走査することにより、そのパネル5の読取走査後の残存
したエネルギーが放出・消去される。On the other hand, the reading portion deflects (scans) the light beam from the beam light source 6 using a semiconductor laser or the like by the deflector 7, scans the stimulable phosphor panel 5 via the mirror 8 or the like, and scans the scanning. A filter that converts the stimulated emission light generated in the light spot portion into a wavelength that can be easily handled by the rod-shaped light conversion conductor 9 and removes the light generated in the light conversion conductor 9 from other light.
Photoelectric conversion is performed by PMT (photomultiplier) 11 via 10, amplified by amplifier 12, then converted to digital signal by A / D converter 13, and the digital signal is sent to an image processing circuit (not shown) to read the image. Trying to get. Reference numeral 14 denotes an erasing lamp, which is turned on and the stimulable phosphor panel 5 is scanned, whereby the energy remaining after the reading and scanning of the panel 5 is released and erased.
第2図は読取部分をより詳細に示した構成ブロック図で
ある。ビーム光源6内にはコリメートレンズを具備し、
そこらの光ビームはビーム整形器15でビーム形状を整形
され、ミラー16、フィルタ17を経由して、偏向器7とし
てのガルバノミラー18で走査される。そして、この走査
されたビームはfθレンズ19を通過してミラー8で光路
を変更して、輝尽性蛍光体パネル5に励起光として入射
する。上記した光変換伝導体9はその励起光の走査方向
に沿った方向で且つ輝尽性蛍光体パネル5上の走査線を
覆うようにそこに平行に配置されたロッド形状でなり、
その両端にフィルタ10を介してPMT11が結合されてい
る。20はPMT11用の電源である。21はPMT11で得られた電
流信号を電圧に変換する電流/電圧変換回路、22は両方
の電流/電圧変換回路21で得られた電圧信号を加算する
加算器である。24は増幅器12の出力を対数増幅する対数
増幅器、25はノイズ成分除去用のフィルタ、26は読取画
像信号を画素単位でサンプリングするサンプリングホー
ルド回路である。また、輝尽性蛍光体パネル5の片端に
は、走査ビーム光を検知するフォトダイオード等の光セ
ンサ27が配置され、その光センサ27からので得られた水
平同期信号(励起光の1回の主走査で1個のパルスが出
る。)が処理のタイミングを決めるタイミング信号発生
回路28に入力している。このタイミング信号発生回路28
からの信号は、サンプリングホールド回路26、A/D変換
器13、光ビーム発生器6を制御するドライバ29、ガルバ
ノミラー・ドライバー30等に出力している。FIG. 2 is a structural block diagram showing the reading portion in more detail. The beam light source 6 has a collimator lens,
The light beam from there is shaped into a beam by a beam shaper 15, passes through a mirror 16 and a filter 17, and is scanned by a galvanometer mirror 18 as a deflector 7. Then, the scanned beam passes through the fθ lens 19, the optical path is changed by the mirror 8, and the beam is incident on the stimulable phosphor panel 5 as excitation light. The above-mentioned light conversion conductor 9 has a rod shape arranged in parallel to the scanning line of the stimulable phosphor panel 5 in the direction along the scanning direction of the excitation light,
A PMT 11 is coupled to both ends of the PMT 11 via a filter 10. 20 is a power supply for PMT11. Reference numeral 21 is a current / voltage conversion circuit that converts the current signal obtained by the PMT 11 into voltage, and 22 is an adder that adds the voltage signals obtained by both current / voltage conversion circuits 21. Reference numeral 24 is a logarithmic amplifier for logarithmically amplifying the output of the amplifier 12, 25 is a filter for removing noise components, and 26 is a sampling and holding circuit for sampling the read image signal in pixel units. Further, an optical sensor 27 such as a photodiode for detecting the scanning beam light is arranged at one end of the stimulable phosphor panel 5, and a horizontal synchronizing signal obtained by the optical sensor 27 (one time of excitation light One pulse is output in the main scan.) Is input to the timing signal generation circuit 28 that determines the processing timing. This timing signal generation circuit 28
The signal from is output to the sampling and holding circuit 26, the A / D converter 13, the driver 29 that controls the light beam generator 6, the galvanometer mirror driver 30, and the like.
上記した光変換伝導体9は、第3図に示すように、側面
から入射する光により、内部から別の波長の光を端面方
向に発生する性質を有するもので、輝尽性螢光体パネル
5に面して配置することにより、そのパネル5の輝尽発
光点からの立体受光角度が極めて大きくなり、集光効率
が大きくなる。この光変換伝導体9は、蛍光オプトコレ
クタ(商品名)とも呼ばれ、アクリライト、ポリカーボ
ネイト、特定条件下のポリスチレン等の透明プラスチッ
クに特殊蛍光物質を分散混入したものである。外部から
の光入射により内部で発生する蛍光は、その内部で大部
分(80%)が全反射の法則に従って両方の端面部分に誘
導され、濃密化された状態で放出される。本実施例で
は、励起光λ2(=500nm〜2,000nm、半導体レーザの光
では700nm〜800nm)により励起されて輝尽性蛍光体パネ
ル5から発生する輝尽発光光λ3(=200nm〜500nm)を
側面から受けて別の波長λ4(=400nm〜2,000nm)の光
に変換して両方の端面から出射し、フィルタ10を介して
PMT11に入射させる。第4図はこの光変換伝導体9の波
長変換の特性を示す図であり、第4図(a)は入射光の
スペクトル、(b)は出射光のスペクトルの一例であ
る。輝尽性螢光体パネル5に面してこの光変換伝導体9
を配置した場合、励起光の成分はその光変換伝導体9を
通り抜けるので、PMT11に入射することはなく、S/Nが良
好となる。As shown in FIG. 3, the above-mentioned light conversion conductor 9 has a property of generating light of another wavelength from the inside in the end face direction by the light incident from the side surface, and is a stimulable phosphor panel. By arranging the panel 5 so as to face it, the stereoscopic light receiving angle from the stimulated emission point of the panel 5 becomes extremely large, and the light collection efficiency becomes large. The light conversion conductor 9 is also called a fluorescent optocollector (trade name), and is made by mixing and mixing a special fluorescent substance in a transparent plastic such as acrylite, polycarbonate, polystyrene under specific conditions. Most (80%) of the fluorescence generated inside due to light incident from the outside is guided to both end face portions according to the law of total internal reflection, and is emitted in a dense state. In this embodiment, the excitation light lambda 2 emitted light lambda 3 generated from the stimulable phosphor panel 5 is excited by (= 500nm~2,000nm, 700nm~800nm in light of the semiconductor laser) (= 200 nm to 500 nm ) Is received from the side surface, converted into light of another wavelength λ 4 (= 400 nm to 2,000 nm), emitted from both end surfaces, and passed through the filter 10.
It is incident on PMT11. FIG. 4 is a diagram showing wavelength conversion characteristics of the light conversion conductor 9, FIG. 4 (a) is an example of the spectrum of incident light, and FIG. 4 (b) is an example of the spectrum of emitted light. Facing the photostimulable phosphor panel 5, this light conversion conductor 9
, The excitation light component passes through the light conversion conductor 9, so that it does not enter the PMT 11 and the S / N is improved.
なお、第5図に示すように、この光変換伝導体9の片端
面に銀メッキ等によりミラー31を形成すれば、他端側に
取り付けた1個のPMT11だけで、第2図に示す場合と同
様な効率でそこで変換された出射光λ4の集光を行うこ
とができる。As shown in FIG. 5, if a mirror 31 is formed on one end surface of the light conversion conductor 9 by silver plating or the like, only one PMT 11 attached to the other end side can be used as shown in FIG. It is possible to collect the emitted light λ 4 converted there with the same efficiency as.
この光変換伝導体9としては、第6図に示すように、内
部を高屈折率のコア9aとし、その外部に低屈折率のクラ
ッド9bを設けて、その内部コア9a側に蛍光物質を混入さ
せた異種媒体の複合構成とすれば、クラッド9bの外被の
汚れや傷等の影響を受けることなく第7図に示すよう
に、変換後の出射光λ4を両端に導出することができ、
その集光効率が格段に向上する。第7図中、9cは螢光物
質である。As shown in FIG. 6, the light converting conductor 9 has a high-refractive index core 9a inside and a low-refractive index clad 9b provided outside the inner core 9a. With the composite structure of the different media, the output light λ 4 after conversion can be led out to both ends without being affected by dirt or scratches on the outer cover of the cladding 9b, as shown in FIG. ,
The light collection efficiency is significantly improved. In FIG. 7, 9c is a fluorescent substance.
この場合、コア9aの屈折率をn1、クラッド9bの屈折率を
n2とすると、開口数N.A.と受光及び出射角度は、 N.A.=(n1 2−n2 2)1/2 受光及び出射角度=2sin-1(N.A.) となる。In this case, the refractive index of the core 9a is n 1 and the refractive index of the clad 9b is
Assuming n 2 , the numerical aperture NA and the light receiving and emitting angles are NA = (n 1 2 −n 2 2 ) 1/2 light receiving and emitting angles = 2 sin −1 (NA).
また、この光変換伝導体9としては、第8図に示すよう
に、輝尽性蛍光体パネル5の励起光の走査方向に沿った
方向に配置する部分を直線状とし、その両端を1個のPM
T11に導くように折り曲げた形状にすることも、また第
9図に示すように、複数の小径の光変換伝導体を束ねた
集束光変換伝導体9′として同様に配置することもでき
る。In addition, as shown in FIG. 8, the light conversion conductor 9 has a linear portion at a position along the scanning direction of the excitation light of the stimulable phosphor panel 5, and has one end at each end. PM
It may be bent so as to lead to T11, or, as shown in FIG. 9, it may be similarly arranged as a focused light conversion conductor 9'in which a plurality of small diameter light conversion conductors are bundled.
一方、励起光λ2の入射方法としては、第10図(a)〜
(d)に示すように斜め方向から入射させる方法の他
に、同部(e)〜(h)に示すように真上から入射せる
方法がある。前者の場合は必要に応じて光変換伝導体
9、9′の一部に励起光λ2の通過用のギャップを形成
する。また、後者の場合は2個並べたの光変換伝導体9
或いは9′の真上の隣接間を励起光が通過するようにす
る。On the other hand, as an incident method of the excitation light λ 2 , there are
In addition to the method of obliquely entering the light as shown in (d), there is a method of making the light incident directly from above as shown in the parts (e) to (h). In the former case, a gap for passing the excitation light λ 2 is formed in a part of the light conversion conductors 9 and 9 ′, if necessary. In the latter case, two light conversion conductors 9 are arranged.
Alternatively, the excitation light is allowed to pass between the adjacent portions immediately above 9 '.
また、輝尽性蛍光体パネル5から発生する輝尽発光光の
光変換伝導体への入射効率を向上させるためには、第11
図に示すように、その光変換伝導体の背面(輝尽性蛍光
体パネル5に面する側と反対側)に密着して或いは離し
て輝尽発光光反射部材32を取り付ける。この反射部材32
は、複数の小径の集束光変換伝導体9′に密着させれ
ば、その伝導体9′の束ねの機能も果たすようになる。
またこの反射部材32は、励起光に対して透過性能を有す
る材質とし、その励起光がそこで反射されて輝尽性蛍光
体パネル5に戻ることを防止して、読み取った画質が励
起光の妨害を受けて劣化しないようにする。第12図はこ
のような反射部材32を取り付けた光変換伝導体の例を示
す図である。In addition, in order to improve the incidence efficiency of the photostimulated luminescent light generated from the stimulable phosphor panel 5 to the light conversion conductor,
As shown in the figure, the photostimulable luminescent light reflecting member 32 is attached to the back surface (the side opposite to the side facing the stimulable phosphor panel 5) of the photoconversion conductor so as to be in close contact with or away from it. This reflective member 32
When brought into close contact with a plurality of small-diameter focused light conversion conductors 9 ', they also function as a bundle of the conductors 9'.
The reflecting member 32 is made of a material having a transmissivity for the excitation light, and prevents the excitation light from being reflected there and returning to the stimulable phosphor panel 5 to prevent the read image quality from disturbing the excitation light. So that it will not be deteriorated. FIG. 12 is a diagram showing an example of a light conversion conductor to which such a reflecting member 32 is attached.
第13図は輝尽性蛍光体パネル5の表裏両面に光変換伝導
体9或いは9′を配置した例を示す図である。輝尽性蛍
光体パネル5は励起光により照射した側のみならず、そ
の反対面からも輝尽発光光を発生するので、その反対側
にも光変換伝導体を配置することにより、集光効率が大
幅に向上するようになるのである。FIG. 13 is a view showing an example in which the photoconversion conductors 9 or 9'are arranged on both front and back surfaces of the stimulable phosphor panel 5. Since the stimulable phosphor panel 5 generates stimulated emission light not only from the side irradiated with the excitation light but also from the opposite side, the light conversion conductor is also arranged on the opposite side to collect light. Will be greatly improved.
以上のように本発明は、波長変換を行っているので、集
光光学系の扱いやすい波長に変換することにより、その
光学系のコスト低下、光電変換素子の最適化、フィルタ
の選定の容易化等を実現できる。As described above, the present invention performs wavelength conversion. Therefore, by converting the wavelength into a wavelength that can be easily handled by the condensing optical system, cost reduction of the optical system, optimizing photoelectric conversion elements, and facilitating selection of filters are possible. Etc. can be realized.
第1図は本発明の原理を示す画像情報記録読取装置の概
略構成図、第2図は読取装置部分のより詳細なブロック
図、第3図は光変換伝導体の説明図、第4図(a)、
(b)はその光変換の特性図、第5図は光変換伝導体か
らの光の別の集光方法の説明図、第6図は光変換伝導体
を複合構造とした説明図、第7図は第6図に示した光変
換伝導体の作用説明図、第8図と第9図は1つのPMTに
光変換伝導体の両端を結合する説明図、第10図(a)〜
(h)は励起光照射の説明図、第11図(a)、(b)は
輝尽発光光の集光効率向上のために光変換伝導体に反射
部材を取り付けた説明図、第12図(a)〜(h)はその
各場合の説明図、第13図は輝尽性蛍光体パネルの上下面
に光変換伝導体を配置した説明図である。 1…被写体、2…X線発生器、3…グリッド、4…フォ
トタイマ、5…輝尽性蛍光体パネル、6…光ビーム発生
器、7…偏向器、8…ミラー、9…光変換伝導体、10…
フィルタ、11…PMT、12…増幅器、13…A/D変換器、14…
消去ランプ、15…ビーム整形器、16…ミラー、17…フィ
ルタ、18…ガルバノミラー、19…fθレンズ、20…PMT
用電源、21…電流/電圧変換回路、22…加算器、24…対
数増幅器、25…フィルタ、26…サンプリングホールド回
路、27…水平同期信号センサ、28…タイミング発生回
路、29…光ビーム発生器ドライバ、30…ガルバノミラー
・ドライバー、31…ミラー、32…光反射部材。FIG. 1 is a schematic configuration diagram of an image information recording / reading device showing the principle of the present invention, FIG. 2 is a more detailed block diagram of a reading device portion, FIG. 3 is an explanatory view of a light conversion conductor, and FIG. a),
(B) is a characteristic diagram of the light conversion, FIG. 5 is an explanatory diagram of another method of condensing light from the light conversion conductor, FIG. 6 is an explanatory diagram of a composite structure of the light conversion conductor, and FIG. The figure is an explanatory view of the operation of the light conversion conductor shown in FIG. 6, and FIGS. 8 and 9 are illustrations of connecting both ends of the light conversion conductor to one PMT, and FIGS.
11 (a) and 11 (b) are explanatory views of the excitation light irradiation, FIG. 11 (a) and FIG. 11 (b) are explanatory views in which a reflection member is attached to the light conversion conductor for improving the efficiency of concentrating stimulated emission light, and FIG. (A) to (h) are explanatory views in each case, and FIG. 13 is an explanatory view in which a photoconversion conductor is arranged on the upper and lower surfaces of the stimulable phosphor panel. 1 ... Subject, 2 ... X-ray generator, 3 ... grid, 4 ... photo timer, 5 ... stimulable phosphor panel, 6 ... light beam generator, 7 ... deflector, 8 ... mirror, 9 ... light conversion conduction Body, 10 ...
Filter, 11 ... PMT, 12 ... Amplifier, 13 ... A / D converter, 14 ...
Erase lamp, 15 ... Beam shaper, 16 ... Mirror, 17 ... Filter, 18 ... Galvano mirror, 19 ... f.theta. Lens, 20 ... PMT
Power supply, 21 ... Current / voltage conversion circuit, 22 ... Adder, 24 ... Logarithmic amplifier, 25 ... Filter, 26 ... Sampling hold circuit, 27 ... Horizontal sync signal sensor, 28 ... Timing generation circuit, 29 ... Optical beam generator Driver, 30 ... Galvano mirror driver, 31 ... Mirror, 32 ... Light reflecting member.
Claims (6)
情報を記録し、第2の電磁波で該パネルを主走査方向に
主走査しながら該主走査方向と交差する方向に相対的に
副走査して上記パネルの記録面から第3の電磁波を発生
させ、上記パネルの上記主走査方向に形成される走査線
に沿うよう配置させたロッド形状の波長変換媒体を上記
第2の電磁波の上記副走査に応じて上記副走査と同一方
向に相対的に移動させ、上記第3の電磁波を上記波長変
換媒体に入射させて第4の電磁波に変換し、該第4の電
磁波を光電変換して得られた電気信号を処理することに
より、上記画像情報を得るように構成したことを特徴と
する画像情報記録読取方法。1. A recording panel is irradiated with a first electromagnetic wave to record image information, and a second electromagnetic wave is used to perform main scanning in the main scanning direction while relatively scanning the panel in a direction intersecting the main scanning direction. A sub-scanning is performed to generate a third electromagnetic wave from the recording surface of the panel, and a rod-shaped wavelength conversion medium arranged along a scanning line formed in the main scanning direction of the panel is used to generate a second electromagnetic wave. In response to the sub-scanning, it is relatively moved in the same direction as the sub-scanning, the third electromagnetic wave is made incident on the wavelength conversion medium to be converted into a fourth electromagnetic wave, and the fourth electromagnetic wave is photoelectrically converted. An image information recording / reading method, characterized in that the image information is obtained by processing an electric signal obtained as described above.
ることを特徴とする特許請求の範囲第1項記載の画像情
報記録読取方法。2. The image information recording / reading method according to claim 1, wherein the first electromagnetic wave is radiation such as X-rays.
起する500nm〜2,000nmの波長の励起光であることを特徴
とする特許請求の範囲第1項又は第2項記載の画像情報
記録読取方法。3. The image information recording according to claim 1 or 2, wherein the second electromagnetic wave is excitation light having a wavelength of 500 nm to 2,000 nm that excites the recording panel. How to read.
起する700nm〜800nmの波長の励起光であることを特徴と
する特許請求の範囲第1項乃至第3項記載の画像情報記
録読取方法。4. The image information recording / reading according to claim 1, wherein the second electromagnetic wave is excitation light having a wavelength of 700 nm to 800 nm that excites the recording panel. Method.
0nm〜500nmの波長の輝尽発光光であることを特徴とする
特許請求の範囲第1項乃至第4項記載の画像情報記録読
取方法。5. The third electromagnetic wave is applied to the recording panel 20.
5. The image information recording / reading method according to claim 1, wherein the stimulated emission light has a wavelength of 0 nm to 500 nm.
長であることを特徴とする特許請求の範囲第1項乃至第
5項記載の画像情報記録読取方法。6. The image information recording / reading method according to any one of claims 1 to 5, wherein the fourth electromagnetic wave has a wavelength of 400 nm to 2,000 nm.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62084834A JPH0795189B2 (en) | 1987-04-08 | 1987-04-08 | Image information recording and reading method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62084834A JPH0795189B2 (en) | 1987-04-08 | 1987-04-08 | Image information recording and reading method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS63250634A JPS63250634A (en) | 1988-10-18 |
| JPH0795189B2 true JPH0795189B2 (en) | 1995-10-11 |
Family
ID=13841812
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP62084834A Expired - Lifetime JPH0795189B2 (en) | 1987-04-08 | 1987-04-08 | Image information recording and reading method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0795189B2 (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP3636579B2 (en) * | 1997-11-04 | 2005-04-06 | キヤノン株式会社 | Photoelectric conversion device, method for driving photoelectric conversion device, and system having the photoelectric conversion device |
| JP3717685B2 (en) * | 1998-09-22 | 2005-11-16 | 日本原子力研究所 | Radiation image readout device for imaging plate and readout method thereof |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6284836A (en) * | 1985-10-08 | 1987-04-18 | Toyota Motor Corp | Double action type press machine |
| JPH0618415B2 (en) * | 1987-01-16 | 1994-03-09 | 富士写真フイルム株式会社 | Radiation image information reader |
-
1987
- 1987-04-08 JP JP62084834A patent/JPH0795189B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS63250634A (en) | 1988-10-18 |
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