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JPH0731367B2 - Radiation image reading method - Google Patents
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JPH0731367B2 - Radiation image reading method - Google Patents

Radiation image reading method

Info

Publication number
JPH0731367B2
JPH0731367B2 JP61055971A JP5597186A JPH0731367B2 JP H0731367 B2 JPH0731367 B2 JP H0731367B2 JP 61055971 A JP61055971 A JP 61055971A JP 5597186 A JP5597186 A JP 5597186A JP H0731367 B2 JPH0731367 B2 JP H0731367B2
Authority
JP
Japan
Prior art keywords
radiation image
conversion panel
light
radiation
image
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
JP61055971A
Other languages
Japanese (ja)
Other versions
JPS62211637A (en
Inventor
久憲 土野
亜紀子 加野
邦昭 中野
幸二 網谷
文生 島田
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.)
Konica Minolta Inc
Original Assignee
Konica Minolta Inc
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 Konica Minolta Inc filed Critical Konica Minolta Inc
Priority to JP61055971A priority Critical patent/JPH0731367B2/en
Publication of JPS62211637A publication Critical patent/JPS62211637A/en
Publication of JPH0731367B2 publication Critical patent/JPH0731367B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Facsimile Scanning Arrangements (AREA)
  • Conversion Of X-Rays Into Visible Images (AREA)
  • Radiography Using Non-Light Waves (AREA)
  • Luminescent Compositions (AREA)

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は放射線画像変換パネルに蓄積された放射線画
像情報の読取方法に関し,更に詳しくは該放射線画像を
正確に再現する読取方法に関するものである. 〔発明の背景〕 放射線を輝尽性蛍光体に照射すると放射線エネルギーが
蓄積され,この蓄積エネルギーは可視光等で励起すると
輝尽発光を蓄積エネルギーに応じた強さで発光すること
が知られている. 前記輝尽性蛍光体の特性を活かして,人体等の放射線画
像情報を輝尽性蛍光体層を有する放射線画像変換パネル
(以後「変換パネル」と略称する)に潜像として蓄積記
録し,該変換パネルをレーザ光等の輝尽励起光で走査し
て輝尽発光させ,該輝尽発光を光電変換して画像信号と
し,これを可視化する方法が,例えば,米国特許第3,85
9,527号,特開昭55-12144号に提案されている. 次に,前記の如き変換パネルを用いた放射線画像情報読
取方法及び装置を第3図を用いて説明する. レーザ光源302を発した輝尽励起光用レーザ光305がカル
バノメータミラー304で一定振幅で振られながら反射し
て放射線画像情報を潜像として蓄積されている変換パネ
ル301を照射する. この際,変換パネル301は同時に振幅方向に直角に移動
させられる.即ち,前記変換パネル301は振幅方向(X
方向)に主走査されY方向に副走査され,変換パネル30
1の全域が走査され,その走査線上に輝尽発光する. 一方,振幅面と変換パネル表面との交線に近接して平行
に受光面306aを配置した集光体306が設置されており,
該集光体306は細長い平面切口をなす受光面306aから次
第にしぼまり,その終端の伝達面306bにおいてほゞ円筒
状となって光検出器(例えばフォトマルチプライヤー
等)307に輝尽発光と励起用レーザ光とを分離するため
のフィルター308を介して臨接している. 以上の構成によって走査線上に生じた輝尽発光は受光面
306aから集光体306に入り,終端の伝達面306bに到り光
検出器307に入って光電変換を受け,画像表示装置311に
送られ,該画像表示装置311において光電変換された画
像情報が処理され,CRT或いは磁気テープまたは写真感光
材料等を用いて可視像として観察される. ここで注意すべきは,集光体306の受光面306aには該受
光面306aに対して全反射角以内にある点からの光は全て
集光体306の中に入射されることであって走査線上でレ
ーザ光305によって励起された輝尽発光のみならず,装
置外からの迷光或いは変換パネル301の表面からのレー
ザ光の反射光の一部若しくは残光等が全て拾われ,画像
情報を表示する輝尽発光に混和し,これらが正確な画像
情報を混乱させるノイズ光となる. 前記ノイズ光のうち,装置外からの迷光や変換パネル30
1の表面からのレーザ光の反射光は遮光,フィルター等
により排除できるから,ノイズ光としては変換パネル30
1の表面からの残光が問題となる. 前記残光には放射線が変換パネルの輝尽性蛍光体を刺激
することによって発生する蛍光の残光(以後「蛍光残
光」と称す」と,放射線によって輝尽性蛍光体が蓄積し
たエネルギーをレーザ光等の輝尽励起光で励起するとき
に発生する輝尽発光の残光(以後「輝尽残光と称す)と
がある. この前者の蛍光残光は一般に第4図に示すような指数関
数的減衰曲線を示す.即ち,時刻t1からt2までのΔt時
間放射線を照射してt2で停止したとすると,発光強度LO
は直ちに0に減衰することはない.その減衰状況は蛍光
体によって異なり,発光強度が1/eになる時定数はタン
グステン酸塩では10-6秒,希土類元素イオンやマンガン
イオンを含む蛍光体では10-3〜10-1秒に及ぶことがあ
る.また,蛍光残光は第4図の曲線aで表される主の残
光の他に,同図bで表されるような従の残光が重なり合
っている場合が多い.前記従の残光は一般に発光強度は
弱いが減衰の時定数が著しく大きい. 輝尽発光は前記したように輝尽励起光がある時刻に照射
される極く小さな面積(面素相当)から発するのに対
し,蛍光残光は放射線が照射された全面から発光し,第
3図の集光体306の受光面306aの全反射角以内にある点
からの光は全て集光される. この場合,変換パネルの輝尽発光面積に比べて,集光体
306の集光面積が著しく大きいため,一画素当たりの蛍
光残光強度が輝尽発光強度と比較して無視できるほど小
さくなったとしても,光検出器に伝達される光量として
蛍光残光量は無視できなくなる.例えば集光体306の集
光面積を400mm×2mmとし,画素の大きさを200μm×200
μmとすると集光体に集光される画素数は2×104個で
あり,一画素当たりの蛍光残光強度が輝尽発光強度の10
-4程度であったとしても,光検出器に伝達される光量の
うち蛍光残光量と輝尽発光量との比は2:1となってしま
う. このように,従来の放射線画像情報読取方法においては
放射線照射後,螢光残光強度が十分無視できる程度にな
るまで放射線画像情報の読取りまでの時間を待機する必
要があり,迅速,大量に連続して画像情報を読取ること
が困難であった.特に,第4図の曲線aに表される主の
残光の時定数が大きな場合,或いは主の残光の時定数は
小さくても同図曲線bで表される時定数の大きな従の大
きな残光が存在する場合は致命的であった. 〔発明の目的〕 本発明は前述のような従来の放射線画像読取方法の欠点
に鑑みてなされたものであり,本発明の目的は蛍光残光
による影響が少なく,実際の画像に合った正確な画像信
号を得てSN比のよい高品質の再生画像を得ることのでき
る放射線画像情報読取方法を提供することにある. また,本発明の他の目的は放射線の照射から画像の読取
りまでの時間を短縮して,装置のスループットを向上さ
せ,迅速,大量に連続して画像情報を読取ることのでき
る放射線画像情報読取方法を提供することにある. 〔発明の構成〕 上記目的を達成するため,この発明は i)被写体を透過した,或いは被検体から発せられた放
射線を下記一般式で表される輝尽性蛍光体を主成分とし
て含有する放射線画像変換パネルに吸収させる工程; 一般式 MIX・aMIIX′・bMIIIX″3:cA (但し,MIは,Li,Na,K,Rb及びCsから選ばれる少なくとも
一種のアルカリ金属であり,MIIはBe,Mg,Ca,Sr,Ba,Zn,C
d,Cu及びNiから選ばれる少なくとも一種の二価金属であ
る.MIIIはSc,Y,La,Ce,Pr,Nd,Pm,Sm,Eu,Gd,Tb,Dy,Ho,Er,
Tm,Yd,Lu,Al,Ga及びInから選ばれる少なくとも一種の三
価金属である.X,X′及びX″はF,Cl,Br及びIから選ば
れるすくなくとも一種のハロゲンである.AはTm,Dy,Pr,H
o,Nd,Yb,Er,Gd,Lu,Sm,Y,Tl,Na,Ag,Cu及びMgから選ばれ
る少なくとも一種の金属である. また,aは0≦a<0.5の範囲の数値であり,bは0≦b<
0.5の範囲の数値であり,cは0<c<0.2の範囲の数値で
ある.) ii)前記i)の工程終了後,直ちに該放射線画像変換パ
ネルに500〜900nmの波長領域の輝尽励起光を照射するこ
とにより,該放射線画像変換パネルに蓄積・記録されて
いる放射線エネルギーを輝尽発光として放出させる工
程; iii)該輝尽発光を検出する工程を含むことを特徴とす
るものである. 即ち,本発明者らは蛍光残光量が著しく少なく,蛍光残
光による読取りまでの待機時間を設ける必要のない前記
一般式で表されるアルカリハライド輝尽性蛍光体を利用
することにより従来の方法に比較して高SN比で高品位の
画像を与えることができ,かつ,装置のスループットを
向上させ得るようにしたものである. なお,前記ii)でいう「直ちに」とは放射線照射後,長
くとも1分以内,好ましくは30秒以内,より好ましくは
10秒以内を言う. 以下,本発明を第1図及び第2図に基づいて詳細に説明
する. 第1図は前述のような諸特性の向上した本発明の放射線
画像情報読取方法に用いる装置の一例を示す概略図であ
る.本発明に用いる装置はこれに限られることはなく,
第3図に示すような装置でもよいが,本発明の方法によ
る効果を充分発揮させるためにはビルド・インタイプの
装置であった方がより好ましい. 本図において,101は放射線源,102は被写体,103は前記一
般式で表されるアルカリハライド輝尽性蛍光体層104を
有する変換パネルである.変換パネル103の輝尽性蛍光
体層104側の表面に向き合う位置には,例えばレーザ光
等の輝尽励起光を発する輝尽励起光源105と,この輝尽
励起光源105から発せられた輝尽励起光111のみを透過さ
せるフィルター110,該輝尽励起光111を変換パネル103の
幅方向に走査する例えばガルバノメーターミラー等の光
偏光器106,前記輝尽励起光により励起された輝尽性蛍光
体層104から発する輝尽発光を読み取る光検出器107及び
この光検出器107に前記輝尽発光を導く集光体108が共通
の搬送ステージ112上に設けられている.前記光検出器1
07は例えば光電子増倍管,光電子増幅用マイクロチャン
ネルプレート等であり,集光体108で導かれた輝尽発光
は輝尽励起光と輝尽発光とを分離するためのフィルタ10
9で分離された後,該光検出器107で光電的に検出され
る. また,前記輝尽励起光源105は500〜900nmにスペクトル
分布をもつ光を放出する光源の他に,He-Neレーザ,YAGレ
ーザ,Arレーザ,半導体レーザ,LED等が用いられるが,
特に,He-Neレーザや半導体レーザが好ましい. 114は検出された信号の増幅器,115は増幅器114で増幅さ
れた信号を画像として再生するための画像再生装置,116
は画像表示装置である. また,前記変換パネル103の輝尽性蛍光体層104側の表面
に対向する位置には,消去用光源113が設けられ,搬送
ステージ112とともに矢印の方向に搬送される.この消
去用光源113は輝尽性蛍光体層104に該蛍光体の励起波長
領域を含む光を発する光源であり,例えば特開昭56-113
92号に示されているようなハロゲンランプ,タングステ
ンランプ,赤外線ランプ,LED或いはレーザ光源等が任意
に選択使用され得る. 前記構造を有する本実施態様の装置において,被写体10
2が変換パネル103と,放射線源101との間に配された
後,放射線源101が点灯されると,変換パネル104の輝尽
性蛍光体層104上に前記被写体102の透過放射線画像情報
が記録蓄積される.この放射線の照射後直ちに500nm〜9
00nmの波長領域の輝尽励起光を照射することにより,前
記変換パネル103に蓄積・記録されている放射線エネル
ギーは輝尽発光として放出される.この輝尽発光は光検
出器107に集光され光電変換された後,画像再生装置115
によって画像として再生され,画像表示装置116によっ
て可視画像として表示される. なお,前記輝尽励起光の照射において,該励起光の副走
査は搬送ステージ112の移動により行われ,変換パネル1
03の画像記録部分の全域が走査される.また,画像読取
終了後,消去光源113により,残存画像情報が消去され
て初期状態に戻るようになる. 次に,本発明の放射線画像読取方法に用いられる輝尽性
蛍光体について説明する. 本発明に主成分として用いられる下記一般式で表わされ
るアルカリハライド輝尽性蛍光体は従来公知の輝尽性蛍
光体に比較して著しく蛍光残光の少ない及び/または蛍
光残光寿命の短いことが要求される. 一般式 MIX・aMIIX′・bMIIIX″3:cA (但し,MIは,Li,Na,K,Rb及びCsから選ばれる少なくとも
一種のアルカリ金属であり,MIIはBe,Mg,Ca,Sr,Ba,Zn,C
d,Cu及びNiから選ばれる少なくとも一種の二価金属であ
る.MIIIはSc,Y,La,Ce,Pr,Nd,Pm,Sm,Eu,Gd,Tb,Dy,Ho,Er,
Tm,Yd,Lu,Al,Ga及びInから選ばれる少なくとも一種の三
価金属である.X,X′及びX″はF,Cl,Br及びIから選ば
れるすくなくとも一種のハロゲンである.AはTm,Dy,Pr,H
o,Nd,Yb,Er,Gd,Lu,Sm,Y,Tl,Na,Ag,Cu及びMgから選ばれ
る少なくとも一種の金属である. また,aは0≦a<0.5の範囲の数値であり,bは0≦b<
0.5の範囲の数値であり,cは0<c<0.2の範囲の数値で
ある.) 特に,該アルカリハライド輝尽性蛍光体のうち,MIはK,R
b,Csから選ばれる少なくとも一種のアルカリ金属であ
り,AはTl,Naから選ばれる少なくとも一種の金属である
アルカリハライド輝尽性蛍光体が,蛍光残光が少なく及
び/または蛍光残光の寿命が短くて優れている. 前記アルカリハライド輝尽性螢光体は単独で用いる必要
はなく,他の輝尽性螢光体と混合して用いてもよい.た
だし,アルカリハライド輝尽性螢光体を他の輝尽性螢光
体と混合して用いる場合には前記アルカリハライド蛍光
体の混合比は50wt%以上,更には70wt%以上とすること
が好ましい. 前記アルカリハライド蛍光体と混合して用いてもよい輝
尽性螢光体としては,例えば特開昭48-80487号に記載さ
れているBaSO4:Ax(但し,AはDy,Tb及びTmのうちすくな
くとも一種であり,xは0.001≦x<1モル%である.)
で表わされる蛍光体,特開昭48-80488号記載のMgSO4:Ax
(但し,AはHo或いはDyのうちいずれかであり,0.001≦x
≦1モル%である)で表わされる蛍光体,特開昭48-804
89号に記載されているSrSO4:Ax(但し,AはDy,Tb及びTm
のうち少なくとも一種であり,xは0.001≦x<1モル%
である.)で表わされている蛍光体,特開昭51-29889号
に記載されているNa2SO4,CaSO4及びBaSO4等にMn,Dy及び
Tbのうち少なくとも一種を添加した蛍光体,特開昭52-3
0487号に記載されているBeO,LiF,MgSO4及びCaF2等の蛍
光体,特開昭53-39277号に記載されているLi2B4O7:Cu,A
g等の蛍光体,特開昭54-47883号に記載されているLi2O
・(B2O2)x:Cu(但しxは2<x≦3),及びLi2O・
(B2O2)x:Cu,Ag(但し,xは2<x≦3)等の蛍光体,
米国特許第3,859,527号に記載されているSrS:Ce,Sm,Sr
S:Eu,Sm,La2O2S:Eu,Sm及び(Zn,Cd)S:Mn,X(但し,Xは
ハロゲン)で表わされる蛍光体が挙げられる.また,特
開昭55-12142号に記載されているZnS:Cu,Pb蛍光体,一
般式がBaO・xAl2O3:Eu(但し,0.8≦x≦10)で表わされ
るアルミン酸バリウム蛍光体,及び一般式がMIIO・xSiO
2:A(但し,MIIはMg,Ca,Sr,Zn,Cd又はBaであり,AはCe,T
b.Eu,Tm,pb,Tl,Bi及びMnのうち少なくとも一種であり,x
は0.5≦x<2.5である.)で表わされるアルカリ土類金
属珪酸系蛍光体が挙げられる.また,一般式が (Ba1−x−yMgxCay)FX:eEU2+ (但し,XはBr及びClの中の少なくとも一つであり,x,y及
びeはそれぞれ0<x+y≦0.6,xy≠0及び10-6≦e≦
5×10-2なる条件を満たす数である.)で表わされるア
ルカリ土類弗化ハロゲン化物蛍光体,特開昭55-12144号
に記載されている一般式が LnOX:xA (但し,LnはLa,Y,Gd及びLuの少なくとも一つを,XはCl及
び/又はBrを,AはCe及び/又はTbを,xは0<x<0.1を
満足する数を表わす.)で表わされる蛍光体,特開昭55
-12145号に記載されている一般式が (Ba1−xMIIx)FX:yA (但し,MIIはMg,Ca,Sr,Zn及びCdのうちの少なくとも一
つを,XはCl,Br及びIのうち少なくとも一つを,AはEu,T
b,Ce,Tm,Dy,Pr,Ho,Nd,Yb及びErのうちの少なくとも一つ
を,x及びyは0≦x≦0.6及び0≦y≦0.2なる条件を満
たす数を表わす.)で表わされる蛍光体,特開昭55-843
89号に記載されている一般式がBaFX:xCe,yA(但し,XはC
l,Br及びIのうち少なくとも一つを,AはIn,Tl,Gd,Sm及
びZrのうちのすくなくとも一つであり,x及びyはそれぞ
れ0≦x≦2×10-1及び0<y≦5×10-2である.)で
表わされる蛍光体,特開昭55-160078号に記載されてい
る一般式が MIIFX・xA:yLn (但し,MIIはMg,Ca,Ba,Sr,Zn及びCdのうちの少なくとも
一種,AはBeO,MgO,CaO,SrO,BaO,ZnO,Al2O3,Y2O3,La2O3,I
n2O3,SiO2,TiO2.ZrO2,GeO2,SnO2,Nb2O5,Ta2O5及びThO2
のうちの少なくとも一種,LnはEu,Tb,Ce,Tm,Dy,Pr,Ho,N
d,Yb,Er,Sm及びGdのうちの少なくとも一種であり,xはC
l,Br及びIのうちの少なくとも一種であり,x及びyはそ
れぞれ5×10-5≦x≦0.5及び0<y≦0.2なる条件を満
たす数である.)で表わされる希土類元素付活2価金属
フルオロハライド蛍光体,一般式がZnS:A,CdS:A,(Zn,C
d)S:A,ZnS:A,X及びCdS:A,X(但し,AはCu,Ag,Au,又はMn
であり,Xはハロゲンである.)で表わされる蛍光体,特
開昭57-148285号に記載されている下記いずれかの一般
式, xM3(PO4・NX2:yA M3(PO42:yA (式中,M及びNはそれぞれMg,Ca,Sr,Ba,Zn及びCdのうち
の少なくとも一種,XはF,Cl,Br及びIのうち少なくとも
一種,AはEu,Tb,Ce,Tm,Dy,Pr,Ho,Nd,Yb,Er,Sb,Tl,Mn及び
Snのうちの少なくとも一種を表わす.また,x及びyは0
<x≦6,0≦y≦1なる条件を満たす数である.)で表
わされる蛍光体,下記いずれかの一般式 nReX3・mAX′2:xEu nReX3・mAX′2:xEu,ySm (式中,ReはLa,Gd,Y,Luのうち少なくとも一種,Aはアル
カリ土類金属,Ba,Sr,Caのうちの少なくとも一種,X及び
X′はF,Cl,Brのうちの少なくとも一種を表わす.また,
x及びyは1×10-4<x<3×10-1,1×10-4<y<1×1
0-1なる条件を満たす数であり,n/mは1×10-3<n/m<7
×10-1なる条件を満たす.)で表わされる蛍光体等が挙
げられる. 本発明の放射線画像読取方法に用いられる輝尽性蛍光体
の一例として,タリウム付活臭化ルビジウム輝尽性蛍光
体(RbBγ:Tl)はX線照射後第2図(a)に示すような
発光特性を示す. 第2図(a)の曲線は第1図の放射線画像情報読取装置
を用いて求めたもので,第1図における輝尽励起光源10
5は20mWの半導体レーザ,集光体108の受光面108aの形状
は幅400mm,厚さ5mm,交換パネルの大きさは幅350mm,長さ
420mmであった.また,変換パネルに照射したX線量は5
00mRであった.更に,第2図(a)の曲線を求めるに当
たっては副走査は行わず,従って半導体レーザ光による
主走査も一ラインのみであった. 第2図(a)において,aはX線照射による蛍光であり,b
は前記蛍光による残光の減衰曲線,cは輝尽発光強度であ
る.また輝尽発光強度と蛍光残光強度との比(SN比)は
(S1−S2)/S2で求められる.該SN比をX線照射後から
輝尽発光を得るまでの時間を種々変化させて求め,第2
図(b)に示す. 本発明者らの検討によれば,前記SN比は高いことが好ま
しいが,被写体のダイナミックレンジ等を考慮すると,1
03以上あればよく,104〜105程度であることが好まし
い.しかし,SN比を5×105以上とすることは過剰品質で
ある.よって,第2図(a),(b)より明らかなよう
に本発明の放射線画像読取方法に用いられるタリウム付
活臭化ルビジウム輝尽性蛍光体(RbBγ:Tl)は蛍光残光
が少なく,また,その寿命も短いので,X線照射後2秒程
度で充分SN比が高い画像読取が可能となる.また,得ら
れる放射線画像の画質と読取りのスループットの両方か
らX線照射後長くとも1分以内に読取りを開始すること
が好ましく,30秒以内であっても画質の劣化はほとんど
なく,より好ましい.しかし,X線照射後1分以上とする
ことは読取りのスループットが低下してしまい経済的に
不利となる. 一方,第5図(a)は従来公知の二価のユーロピウム付
活弗化臭化バリウム輝尽性蛍光体(BaFBr:Eu2+)の発光
特性を示し,aはX線照射による蛍光であり,bは前記蛍光
による残光の減衰曲線,cは輝尽発光である.第5図
(b)は輝尽励起光源として半導体レーザの代わりにHe
-Neレーザを用いた以外は前記第2図(b)と同様にし
て求めたSN比である. 従来の二価ユーロピウム付活弗化臭化バリウム輝尽性蛍
光体は蛍光残光が多く,その寿命も長いので,SN比を103
以上にするためにはX線照射後少なくとも1分間以上の
後,画像読取を行う必要があり,読取りのスループット
が著しく低下する. 前記輝尽性蛍光体層は例えば次のような方法により支持
体上に形成することができる. まず,前記の輝尽性蛍光体粒子と結着剤とを適当な溶剤
に加え,これを充分混合して結着剤溶液中に輝尽性蛍光
体粒子が均一に分散した塗布液を調整する. 輝尽性蛍光体層の結着剤の例としては,ゼラチン等のタ
ンパク質,デキストラン等のボリサッカライドまたはア
ラビアゴムのような天然高分子物質;及びポリビニルブ
チラール,ポリ酢酸ビニル,ニトロセルロース,エチル
セルロース,塩化ビニリデン・塩化ビニルコポリマー,
ポリメチルメタクリレート,塩化ビニル・酢酸ビニルコ
ポリマー,ポリウレタン,セルロースアセテートブチレ
ート,ポリビニルアルコール,線状ポリエステルなどの
ような合成高分子物質などにより代表される結着剤を挙
げることができる. 塗布液調整用の溶剤の例としては,メタノール,エタノ
ール,n−プロパノール,n−ブタノールなどの低級アルコ
ール:メチレンクロライド,エチレンクロライドなどの
塩素原子含有炭化水素;アセトン,メチルエチルケト
ン,メチルイソブチルケトンなどのケトン:酢酸メチ
ル,酢酸エチル,酢酸ブチルなどの低級脂肪酢と低級ア
ルコールとのエステル;ジオキサン,エチレングリコー
ルエチルエーテル,エチレングリコールモノメチルエー
テルなどのエーテル:そして,それらの混合物を挙げる
ことができる. 塗布液における結着剤と輝尽性蛍光体粒子との混合比は
目的とする変換パネルの特性,輝尽性蛍光体粒子の種類
などによって異なるが,一般には結着剤と輝尽性蛍光体
粒子との混合比は1:1ないし1:100(重量比)の範囲から
選ばれ,そして,特に1:8乃至1:40(重量比)の範囲か
ら選ぶことが好ましい. なお,前記塗布液には該塗布液中における輝尽性蛍光体
粒子の分散性を向上させるための分散剤,また,形成後
の輝尽性蛍光体層中における結着剤と輝尽性蛍光体粒子
との間の結合力を向上させるための可塑剤などの種々の
添加剤が混合されていてもよい.そのような目的に用い
られる分散剤の例としては,フタル酸,ステアリン酸,
カプロン酸,親油性界面活性剤などを挙げることができ
る.そして可塑剤の例としては,燐酸トリフェニル,燐
酸トリクレジル,燐酸ジフェニルなどの燐酸エステル;
フタル酸ジエチル,フタル酸ジメトキシエチルなどのフ
タル酸エステル;グリコール酸エチルフタリルエチル,
グリコール酸ブチルフタリルブチルなどのグリコール酸
エステル:そして,トリエチレングリコールとアジピン
酸とのポリエステル,ジエチレングリコールとコハク酸
とのポリエステルなどのポリエチレングリコールと脂肪
族二塩基酸とのポリエステルなどを挙げることができ
る. 前記のようにして調整された輝尽性蛍光体粒子と結着剤
とを含有する塗布液を,次に支持体の表面に均一に塗布
することにより塗布液の塗膜を形成する.この塗布液の
塗布操作は通常の塗布手段,例えばドクターブレード,
ロールコーター,ナイフコーターなどを用いることによ
り行うことができる. 塗膜形成後,塗膜を徐々に加熱することにより乾燥し
て,支持体上への輝尽性蛍光体層の形成を完了する.輝
尽性蛍光体層の層厚は目的とする変換パネルの特性,輝
尽性蛍光体粒子の種類,結着剤と輝尽性蛍光体粒子との
混合比などによって異なるが,通常は20μmないし1mm
とする.但し,この層厚は50乃至500μmとするのが好
ましい. また,輝尽性蛍光体層は必ずしも前記のように支持体上
に塗布液を直接塗布して形成する必要はなく,例えば別
に保護層などのシート上に塗布液を塗布し,乾燥するこ
とにより蛍光体層を形成した後,これを支持体上に押着
するか,或いは接着剤を用いるなどして支持体と輝尽性
蛍光体層とを接合してもよい. なお,輝尽性蛍光体層は一層だげで構成してもよいが,
二層以上積層してもよい. 輝尽性螢光体層の他の形成方法としては気相堆積法があ
る.該気相堆積法としては真空蒸着法,スパッタリング
法,CVD法等を用いることができる.アルカリハライド輝
尽性螢光体は気相堆積法で前記輝尽性螢光体を形成させ
易く該方法の利用が好ましい. 本発明に係る変換パネルにおいて輝尽性蛍光体層に自己
支持能がない場合には,該輝尽性蛍光体層を支持するた
めの支持体が設けられる.前記支持体としては各種高分
子材料,ガラス,金属等が用いられ,セルロースアセテ
ートフィルム,ポリエステルフィルム,ポリエチレンテ
レフタレートフィルム,ポリアミドフィルム,ポリイミ
ドフィルム,トリアセテートフィルム,ポリカーボネー
トフィルム等のプラスチックフィルム,アルミニウムシ
ート,鉄シート,銅シート等の金属シート或いは該金属
酸化物の被覆層を有する金属シートが好ましい. これらの支持体の表面は滑面であってもよいし,輝尽性
蛍光体層との接着性を向上させる目的でマット面として
もよい.また,支持体の表面は凹凸面としてもよいし,
隔絶されたタイル状板を敷き詰めた構造でもよい.前者
の場合には輝尽性蛍光体層が凹凸面によって細分化され
るので,画像の鮮鋭性が一段と向上する.後者の場合に
は輝尽性蛍光体層が支持体のタイル状板の輪郭を維持し
ながら堆積するので,結果的には輝尽性蛍光体層は亀裂
によって隔絶された輝尽性蛍光体の柱状ブロックからな
るため,画像の鮮鋭性が一段と向上する. さらにこれらの支持体は輝尽性蛍光体層との接着性を向
上させる目的で輝尽性蛍光体層が設けられる面に下引層
を設けてもよい.また,これら支持体の層厚は用いられ
る支持体の材質等によって異なるが,一般的には50〜20
00μmであり,取り扱い上の点から更に好ましくは80〜
1000μmである. 本発明に係る変換パネルにおいては一般的に前記輝尽性
蛍光体層が設けられる面とは反対側の面に,輝尽性蛍光
体層を物理的或いは化学的に保護するための保護層が設
けられてもよい.この保護層は保護層用塗布液を輝尽性
蛍光体層上に直接塗布してもよいし,予め別途形成した
保護層を輝尽性蛍光体層上に接着してもよい.或いは別
途形成した保護層上に輝尽性蛍光体層を形成する手順を
とってもよい.保護層の材料としては酢酸セルロース,
ニトロセルロース,ポリメチルメタクリレート,ポリビ
ニルブチラール,ポリビニルホルマール,ポリカーボネ
ート,ポリエステル,ポリエチレンテレフタレート,ポ
リエチレン,ポリ塩化ビニリデン,ナイロン,ポリ四フ
ッ化エチレン,ポリ三フッ化−塩化エチレン,四フッ化
エチレン−六フッ化プロビレン共重合体,塩化ビニリデ
ン−塩化ビニル共重合体,塩化ビニリデン−アクリロニ
トル共重合体等の通常の保護層用材料が用いられる.ま
た,この保護層は蒸着法,スパッタリング法等によりSi
C,SiO2,SiN,Al2O3などの無機物質を積層して形成しても
よい.これらの保護層の層厚は一般には0.1μm〜100μ
m程度が好ましい. 〔実施例〕 以下,実施例を用いて本発明を説明する. 実施例1 変換パネルはRbBr:Tl+からなる輝尽性蛍光体13重量部
と,ポリビニルプチラール1重量部を溶剤(シクロヘキ
サノン)を用いて分散させ,これをポリエチレンテレフ
タレート基板上に均一に塗布し,一昼夜放置し,自然乾
燥することによって約300μmの輝尽性蛍光体層を形成
して作製した.この変換パネルに管電圧80KVのX線を50
0ミリレントゲン照射し,10秒後に25mWの半導体レーザで
画像信号を読取った.画像信号を読取る直前の螢光残光
信号の大きさと前記画像信号の大きさとの比(SN比)を
求め,第1表に示す. 比較例 輝尽性蛍光体としてRbBr:Tl+の代わりにBaFBr:Eu2+を用
いる以外は実施例1と同様に変換パネルを作製し,X線を
照射し,10秒後にHe-Neレーザで画像信号を読取った.画
像信号を読取る直前の螢光残光信号の大きさと前記画像
信号の大きさとの比(SN比)を求め,第1表に示す. 実施例2 実施例1と同様にRbBr:Tl+輝尽性蛍光体60重量%,BaFB
r:Eu2+40重量%を用いて変換パネルを作製した.次に,
実施例1と同様に前記変換パネルにX線を照射し,10秒
後に半導体レーザで画像信号を読取った.画像信号を読
取る直前の螢光残光信号の大きさと前記画像信号の大き
さとの比(SN比)を求め,第1表に示す. 実施例1乃び比較例より,輝尽性蛍光体としてアルカリ
ハライド輝尽性螢光体であるRbBr:Tl+蛍光体を用いた場
合,X線照射後直ちに画像読取を行っても高SN比の画像が
得られた. また,実施例2よりアルカリハライド蛍光体を添加する
と,螢光残光が少なくなり,X線照射後直ちに画像読取を
行っても十分高いSN比が得られた. 〔発明の効果〕 以上説明したように,この発明の放射線画像情報読取方
法は i)被写体を透過した,或いは被検体から発せられた放
射線を下記一般式で表される輝尽性蛍光体を主成分とし
て含有する放射線画像変換パネルに吸収させる工程; 一般式 MIX・aMIIX′・bMIIIX″3:cA (但し,MIはLi,Na,K,Rb及びCsから選ばれる少なくとも
一種のアルカリ金属であり,MIIはBe,Mg,Ca,Sr,Ba,Zn,C
d,Cu及びNiから選ばれる少なくとも一種の二価金属であ
る.MIIIはSc,Y,La,Ce,Pr,Nd,Pm,Sm,Eu,Gd,Tb,Dy,Ho,Er,
Tm,Yd,Lu,Al,Ga及びInから選ばれる少なくとも一種の三
価金属である.X,X′及びX″はF,Cl,Br及びIから選ば
れるすくなくとも一種のハロゲンである.AはTm,Dy,Pr,H
o,Nd,Yb,Gd,Lu,Sm,Y,Tl,Na,Ag,Cu及びMgから選ばれる少
なくとも一種の金属である. また,aは0≦a<0.5の範囲の数値であり,bは0≦b<
0.5の範囲の数値であり,cは0<c<0.2の範囲の数値で
ある.) ii)前記i)の工程終了後,直ちに該放射線画像変換パ
ネルに500〜900nmの波長領域の輝尽励起光を照射するこ
とにより,該放射線画像変換パネルに蓄積・記録されて
いる放射線エネルギーを輝尽発光として放出させる工
程; iii)該輝尽発光を検出する工程; を含むことを特徴としているから,蛍光残光による影響
が少なく,実際の画像に合った正確な画像信号を得てSN
比のよい高品質の再生画像を得ることのできる. また,本発明によれば蛍光残光量が著しく少なく,蛍光
残光による読取りまでの待機時間を設ける必要のない前
記一般式で表されるアルカリハライド輝尽性蛍光体を利
用しているから,放射線の照射から画像の読取りまでの
時間を短縮して,装置のスループットを向上させ得,迅
速かつ大量に連続して画像情報を読取ることのできるな
どの,各種の優れた効果を奏するものである.
DETAILED DESCRIPTION OF THE INVENTION [Industrial application] The present invention relates to a radiation image stored in a radiation image conversion panel.
Regarding the method of reading image information, more specifically, the radiation image
It relates to a reading method that reproduces accurately. BACKGROUND OF THE INVENTION When irradiating a stimulable phosphor with radiation, the radiation energy
When stored energy is excited by visible light etc.
Emit stimulated emission with intensity according to the stored energy
It has been known. Taking advantage of the characteristics of the stimulable phosphor, the radiation image of the human body, etc.
Radiation image conversion panel having stimulable phosphor layer for image information
Accumulated as a latent image in (hereinafter abbreviated as "conversion panel")
Recorded and scanned the conversion panel with stimulated excitation light such as laser light.
To emit stimulated emission and photoelectrically convert the stimulated emission to produce an image signal.
However, a method for visualizing this is described in, for example, US Pat.
Proposed in 9,527 and JP-A-55-12144. Next, read the radiation image information using the conversion panel as described above.
The taking method and device will be described with reference to FIG. The laser light 305 for stimulated excitation light emitted from the laser light source 302 is
It is reflected by the vanometer mirror 304 while being shaken with a constant amplitude.
Conversion panel that stores radiation image information as a latent image
Irradiate with le 301. At this time, the conversion panel 301 moves simultaneously at a right angle to the amplitude direction.
Be made. That is, the conversion panel 301 has an amplitude direction (X
Direction) and sub-scanning in the Y direction.
The entire area of 1 is scanned, and stimulated emission is emitted on that scanning line. On the other hand, close to and parallel to the line of intersection between the amplitude plane and the conversion panel surface.
A light collector 306 having a light-receiving surface 306a is installed at
The condensing body 306 is located next to the light receiving surface 306a which forms an elongated flat cut surface.
It is narrowed to the end and the transmission surface 306b at the terminal end is almost cylindrical.
Photodetector (eg photomultiplier
Etc.) To separate the stimulated emission and the laser light for excitation into 307
They are in contact with each other through the filter 308 of. With the above structure, the stimulated emission generated on the scanning line is the light receiving surface.
Light enters the condenser 306 from 306a and reaches the transmission surface 306b at the end.
Enters the detector 307, receives photoelectric conversion, and is displayed on the image display device 311.
The image transmitted and photoelectrically converted by the image display device 311.
Image information is processed, CRT or magnetic tape or photographic exposure
It is observed as a visible image using materials. It should be noted here that the light receiving surface 306a of the light collector 306 has the light receiving surface 306a.
All light from points within the total reflection angle with respect to the light surface 306a
The light is incident on the condenser 306, and the
Not only stimulated emission excited by laser light 305
Stray light from outside or rays from the surface of the conversion panel 301.
Some of the reflected light or afterglow is completely picked up, and the image
Accurate images mixed with stimulated emission that displays information
It becomes noise light that confuses information. Of the noise light, stray light from outside the device or the conversion panel 30
The reflected light of the laser light from the surface of 1 is shielded, a filter, etc.
Since it can be eliminated by the conversion panel 30
The afterglow from the surface of 1 is a problem. Radiation in the afterglow stimulates the stimulable phosphor of the conversion panel
Afterglow of fluorescence generated by
It is called "light", and the stimulable phosphor accumulates due to radiation.
The excited energy with stimulated excitation light such as laser light
Afterglow of stimulated emission (hereinafter referred to as "stimulated afterglow")
There is. The former fluorescent afterglow is generally related to the index function as shown in FIG.
The numerical decay curve is shown. That is, at time Δt from time t1 to t2
Assuming that radiation is emitted for a period of time and stopped at t2, the emission intensity LO
Does not immediately decay to 0. The decay situation is fluorescent
Depending on the body, the time constant at which the emission intensity is 1 / e is the tan
10 for gustenoate-6Seconds, rare earth ions and manganese
10 for phosphors containing ions-3~Ten-1It can take up to a second
The The fluorescence afterglow is the main afterglow represented by the curve a in FIG.
In addition to the light, the afterglow of subordinate light as shown in FIG.
In many cases In general, the afterglow of the subordinate light emission intensity is
It is weak, but the damping time constant is extremely large. The stimulated emission is irradiated at the time when the stimulated excitation light is present as described above.
To emit from an extremely small area (equivalent to a surface element)
However, the fluorescent afterglow emits light from the entire surface irradiated with radiation,
Point within total reflection angle of light receiving surface 306a of light collector 306 in FIG.
All the light from is collected. In this case, compared to the stimulated emission area of the conversion panel,
Since the converging area of 306 is extremely large,
The afterglow intensity is negligibly small compared to the stimulated emission intensity
Even if it becomes low, the amount of light transmitted to the photodetector
The amount of fluorescence afterglow cannot be ignored. For example, a collection of light collectors 306
Light area is 400mm × 2mm, pixel size is 200μm × 200
Assuming μm, the number of pixels focused on the light collector is 2 × 10FourIn pieces
Yes, the fluorescence afterglow intensity per pixel is 10 times the stimulated emission intensity.
-FourThe amount of light transmitted to the photodetector
The ratio of the amount of fluorescent afterglow to the amount of stimulated emission is 2: 1.
U. Thus, in the conventional radiation image information reading method,
After the irradiation, the intensity of the afterglow of the fluorescent light becomes sufficiently negligible.
It is necessary to wait until the reading of the radiation image information
There is a need to read image information in large quantities in rapid succession.
Was difficult. In particular, the main part represented by the curve a in FIG.
If the afterglow time constant is large, or if the main afterglow time constant is
Even if it is small, it has a large time constant represented by curve b in the figure.
It was fatal if there was a strong afterglow. [Object of the Invention] The present invention is a drawback of the conventional radiation image reading method as described above.
In view of the above, the object of the present invention is to provide a fluorescent afterglow.
Accurate image signal matching the actual image
It is possible to obtain high quality reconstructed images with good signal to noise ratio.
The purpose is to provide a radiation image information reading method. Another object of the present invention is to read an image from irradiation of radiation.
Time to improve equipment throughput.
In addition, it is possible to read image information in rapid succession in large quantities.
The purpose is to provide a radiation image information reading method. [Structure of the Invention] In order to achieve the above-mentioned object, the present invention is: i) A radiation transmitted through a subject or emitted from a subject.
The ray is mainly composed of a stimulable phosphor represented by the following general formula
Absorbed in the radiation image conversion panel contained as a general formula MIX ・ aMIIX ′Two・ BMIIIX ″3: cA (However, MIIs at least selected from Li, Na, K, Rb and Cs
A kind of alkali metal, MIIIs Be, Mg, Ca, Sr, Ba, Zn, C
At least one divalent metal selected from d, Cu and Ni
MIIIIs Sc, Y, La, Ce, Pr, Nd, Pm, Sm, Eu, Gd, Tb, Dy, Ho, Er,
At least one of three selected from Tm, Yd, Lu, Al, Ga and In
It is a valent metal. X, X'and X "are selected from F, Cl, Br and I
It is at least a kind of halogen. A is Tm, Dy, Pr, H
selected from o, Nd, Yb, Er, Gd, Lu, Sm, Y, Tl, Na, Ag, Cu and Mg
Is at least one metal. Also, a is a numerical value in the range of 0 ≦ a <0.5, and b is 0 ≦ b <
It is a numerical value in the range of 0.5, and c is a numerical value in the range of 0 <c <0.2.
is there. Ii) Immediately after the step i), the radiation image conversion pattern is
The channel is irradiated with stimulated excitation light in the wavelength range of 500 to 900 nm.
By, it is stored and recorded in the radiation image conversion panel.
The technology to emit the radiant energy as stimulated emission
Iii) comprising a step of detecting the stimulated luminescence
It is something. That is, the present inventors have remarkably small amount of fluorescence afterglow and
There is no need to set a waiting time until reading with light.
Uses an alkali halide stimulable phosphor represented by the general formula
The high SN ratio and high quality compared to the conventional method
Image can be given and the throughput of the device can be increased.
This is something that can be improved. The term "immediately" in ii) above means that after irradiation
Within at least 1 minute, preferably within 30 seconds, more preferably
Say within 10 seconds. Hereinafter, the present invention will be described in detail with reference to FIGS. 1 and 2.
Do. FIG. 1 shows the radiation of the present invention having improved characteristics as described above.
FIG. 3 is a schematic diagram showing an example of an apparatus used in the image information reading method.
The The device used in the present invention is not limited to this,
Although the apparatus shown in FIG. 3 may be used, the method of the present invention
Build-in type
A device is more preferable. In this figure, 101 is a radiation source, 102 is a subject, and 103 is the above-mentioned one.
The alkali halide stimulable phosphor layer 104 represented by the general formula
It is a conversion panel that has. Photostimulable fluorescence of conversion panel 103
At the position facing the surface on the body layer 104 side, for example, laser light
Excitation light source 105 that emits excitation light such as
Only the stimulated excitation light 111 emitted from the excitation light source 105 is transmitted.
A filter 110 for making the stimulated excitation light 111 of the conversion panel 103
Light that scans in the width direction, such as a galvanometer mirror
Polarizer 106, stimulable fluorescence excited by the stimulated excitation light
A photodetector 107 for reading the stimulated emission emitted from the body layer 104 and
The photodetector 107 has a common condenser 108 for guiding the stimulated emission.
It is provided on the transfer stage 112 of. The photo detector 1
07 is, for example, a photomultiplier tube and a photomultiplier microchannel.
Photostimulated luminescence that is guided by the condenser 108, such as a flannel plate
Is a filter 10 for separating stimulated excitation light and stimulated emission light.
After being separated at 9, it is photoelectrically detected at the photodetector 107.
The The stimulated excitation light source 105 has a spectrum of 500 to 900 nm.
In addition to a light source that emits light with a distribution, a He-Ne laser and a YAG laser
Laser, Ar laser, semiconductor laser, LED, etc. are used,
Especially, He-Ne laser and semiconductor laser are preferable. 114 is an amplifier of the detected signal, 115 is an amplifier 114
An image reproducing device for reproducing the captured signal as an image, 116
Is an image display device. Further, the surface of the conversion panel 103 on the stimulable phosphor layer 104 side
An erasing light source 113 is provided at a position facing the
It is conveyed along with the stage 112 in the direction of the arrow. This erase
The leaving light source 113 is the excitation wavelength of the phosphor in the stimulable phosphor layer 104.
A light source that emits light including a region, for example, Japanese Patent Application Laid-Open No. 56-113
Halogen lamps such as those shown in No. 92
Lamp, infrared lamp, LED or laser light source is optional
Can be used selectively. In the apparatus of this embodiment having the above structure, the subject 10
2 was placed between the conversion panel 103 and the radiation source 101
After that, when the radiation source 101 is turned on, the conversion panel 104 is stimulated.
Radiation image information of the subject 102 on the fluorescent phosphor layer 104
Is recorded and stored. Immediately after irradiation with this radiation, 500 nm-9
By irradiating stimulated excitation light in the wavelength region of 00 nm,
Radiation energy stored and recorded in the conversion panel 103
Ghee is emitted as stimulated emission. This stimulated emission is an optical inspection
After being collected by the output device 107 and photoelectrically converted, an image reproducing device 115
Is reproduced as an image by the image display device 116.
Is displayed as a visible image. In the irradiation of the stimulated excitation light, the excitation light is run by side.
The inspection is performed by moving the transfer stage 112, and the conversion panel 1
The entire image recording area of 03 is scanned. Also, image reading
After the end, the erasing light source 113 erases the residual image information.
Will return to the initial state. Next, the photostimulability used in the radiation image reading method of the present invention
The phosphor will be explained. It is represented by the following general formula used as the main component in the present invention.
Alkali halide stimulable phosphors are
The fluorescence afterglow is significantly less than that of the phosphor and / or the firefly.
Short afterglow life is required. General formula MIX ・ aMIIX ′Two・ BMIIIX ″3: cA (However, MIIs at least selected from Li, Na, K, Rb and Cs
A kind of alkali metal, MIIIs Be, Mg, Ca, Sr, Ba, Zn, C
At least one divalent metal selected from d, Cu and Ni
MIIIIs Sc, Y, La, Ce, Pr, Nd, Pm, Sm, Eu, Gd, Tb, Dy, Ho, Er,
At least one of three selected from Tm, Yd, Lu, Al, Ga and In
It is a valent metal. X, X'and X "are selected from F, Cl, Br and I
It is at least a kind of halogen. A is Tm, Dy, Pr, H
selected from o, Nd, Yb, Er, Gd, Lu, Sm, Y, Tl, Na, Ag, Cu and Mg
Is at least one metal. Also, a is a numerical value in the range of 0 ≦ a <0.5, and b is 0 ≦ b <
It is a numerical value in the range of 0.5, and c is a numerical value in the range of 0 <c <0.2.
is there. ) In particular, among the alkali halide stimulable phosphors, MIIs K, R
At least one alkali metal selected from b and Cs
, A is at least one metal selected from Tl and Na
Alkali halide stimulable phosphor has low afterglow
And / or fluorescence afterglow has a short life and is excellent. The alkali halide stimulable phosphor must be used alone
Instead, it may be mixed with other stimulable phosphors. Was
However, an alkali halide photostimulable phosphor is used as another photostimulable phosphor.
When used as a mixture with the body, the above-mentioned alkali halide fluorescence
The body mixing ratio should be 50 wt% or more, and further 70 wt% or more
Is preferred. Brightness that may be used by mixing with the alkali halide phosphor
Exhaustible fluorescent materials are described, for example, in JP-A-48-80487.
BaSOFour: Ax (However, A is one of Dy, Tb, and Tm
It is at least one, and x is 0.001 ≤ x <1 mol%. )
And the MgSO 4 described in JP-A-48-80488Four: Ax
(However, A is either Ho or Dy, and 0.001 ≦ x
≦ 1 mol%), JP-A-48-804
SrSO listed in No. 89Four: Ax (where A is Dy, Tb and Tm
At least one of the above, x is 0.001 ≦ x <1 mol%
Is. ), The phosphor represented by JP-A-51-29889
Na listed in2SOFour, CaSOFourAnd BaSOFourEtc. to Mn, Dy and
Phosphor to which at least one of Tb is added, JP-A-52-3
BeO, LiF, MgSO described in No. 0487FourAnd CaF2Firefly
Optical body, Li described in JP-A-53-392772BFourO7: Cu, A
g and other phosphors, Li described in JP-A-54-478832O
・ (B2O2) X: Cu (where x is 2 <x ≦ 3), and Li2O
(B2O2) X: Cu, Ag (where x is 2 <x ≦ 3), etc.,
SrS: Ce, Sm, Sr described in U.S. Pat.No. 3,859,527
S: Eu, Sm, La2O2S: Eu, Sm and (Zn, Cd) S: Mn, X (where X is
Examples include phosphors represented by halogen. In addition, special
ZnS: Cu, Pb phosphors described in KAISHO 55-12142,
General formula is BaOxAl2O3: Eu (however, 0.8 ≦ x ≦ 10)
Barium aluminate phosphor with general formula MIIO ・ xSiO
2: A (However, MIIIs Mg, Ca, Sr, Zn, Cd or Ba, A is Ce, T
b. at least one of Eu, Tm, pb, Tl, Bi and Mn, x
Is 0.5 ≦ x <2.5. ) Alkaline earth gold
Examples include genus silicate phosphors. Also, the general formula is (Ba1-X-yMgxCay) FX: eEU2+ (However, X is at least one of Br and Cl, and x, y and
And e are 0 <x + y ≦ 0.6, xy ≠ 0 and 10 respectively.-6≤e≤
5 x 10-2Is a number that satisfies the condition. )
Lucari earth fluorohalide phosphor, JP-A-55-12144
The general formula described in LnOX: xA (where Ln is at least one of La, Y, Gd and Lu, and X is Cl and
And / or Br, A is Ce and / or Tb, and x is 0 <x <0.1
Represents a satisfied number. ), A phosphor represented by
The general formula described in -12145 is (Ba1−xMIIx) FX: yA (However, MIIIs at least one of Mg, Ca, Sr, Zn and Cd.
X, at least one of Cl, Br and I, A is Eu, T
At least one of b, Ce, Tm, Dy, Pr, Ho, Nd, Yb and Er
X and y satisfy the conditions of 0 ≦ x ≦ 0.6 and 0 ≦ y ≦ 0.2.
Represents the number to add. ), A phosphor represented by
The general formula described in No. 89 is BaFX: xCe, yA (where X is C
At least one of l, Br and I, A is In, Tl, Gd, Sm and
And at least one of Zr, where x and y are
0 ≤ x ≤ 2 x 10-1And 0 <y ≦ 5 × 10-2Is. )so
Phosphors represented, described in JP-A-55-160078
General formula is MIIFX ・ xA: yLn (However, MIIIs at least one of Mg, Ca, Ba, Sr, Zn and Cd.
A, BeO, MgO, CaO, SrO, BaO, ZnO, Al2O3, Y2O3, La2O3, I
n2O3, SiO2, TiO2.ZrO2, GeO2, SnO2, Nb2OFive, Ta2OFiveAnd ThO2
, Ln is Eu, Tb, Ce, Tm, Dy, Pr, Ho, N
at least one of d, Yb, Er, Sm, and Gd, and x is C
at least one of l, Br and I, and x and y are
5 × 10 each-FiveSatisfies the conditions of ≦ x ≦ 0.5 and 0 <y ≦ 0.2
It is the number to add. ) Divalent metal with activated rare earth element
Fluorohalide phosphor, the general formula is ZnS: A, CdS: A, (Zn, C
d) S: A, ZnS: A, X and CdS: A, X (where A is Cu, Ag, Au, or Mn
And X is halogen. ) Phosphor represented by
General one of the following listed in Kaisho 57-148285
Expression, xM3(POFour)Two・ NX2: yA M3(POFour)2: yA (where M and N are Mg, Ca, Sr, Ba, Zn and Cd, respectively)
At least one of X, at least one of F, Cl, Br and I
A is Eu, Tb, Ce, Tm, Dy, Pr, Ho, Nd, Yb, Er, Sb, Tl, Mn and
Represents at least one of Sn. Also, x and y are 0
It is a number that satisfies the condition of <x ≦ 6,0 ≦ y ≦ 1. )
Fluorescent substance, one of the following general formulas nReX3・ MAX ′2: xEu nReX3・ MAX ′2: xEu, ySm (where Re is at least one of La, Gd, Y, Lu, A is
Potassium earth metal, at least one of Ba, Sr, Ca, X and
X'represents at least one of F, Cl and Br. Also,
x and y are 1 × 10-Four<X <3 × 10-1, 1 × 10-Four<Y <1 × 1
0-1Is a number that satisfies the following condition, and n / m is 1 × 10-3<N / m <7
× 10-1Satisfy the condition ) Phosphors, etc.
It is possible. Photostimulable phosphor used in the radiation image reading method of the present invention
As an example, thallium-activated rubidium bromide stimulable fluorescence
The body (RbBγ: Tl) is as shown in Fig. 2 (a) after X-ray irradiation.
The luminescence characteristics are shown. The curve of FIG. 2 (a) is the radiation image information reading apparatus of FIG.
The excitation light source 10 in FIG.
5 is a 20 mW semiconductor laser, the shape of the light receiving surface 108a of the condensing body 108
Width 400mm, thickness 5mm, replacement panel size is width 350mm, length
It was 420 mm. Also, the X-ray dose applied to the conversion panel is 5
It was 00mR. Furthermore, to obtain the curve in Fig. 2 (a),
Since sub-scanning is not performed, the semiconductor laser light is used.
The main scan was only one line. In Fig. 2 (a), a is fluorescence due to X-ray irradiation, and b
Is the decay curve of the afterglow due to the fluorescence, and c is the stimulated emission intensity.
The Also, the ratio of the stimulated emission intensity and the fluorescence afterglow intensity (SN ratio) is
(S1-S2) / S2Can be obtained with. From the S / N ratio after X-ray irradiation
The time required to obtain stimulated emission was changed variously, and the second
Shown in Figure (b). According to the study by the present inventors, it is preferable that the SN ratio is high.
However, considering the dynamic range of the subject, 1
03Greater than 10Four~TenFivePreferred to be degree
Yes. However, the SN ratio is 5 × 10FiveThe above is excess quality
is there. Therefore, as is clear from FIGS. 2 (a) and 2 (b).
With thallium used in the radiation image reading method of the present invention
Rubidium bromide stimulable phosphor (RbBγ: Tl) is fluorescent afterglow
Is less and has a shorter life, so about 2 seconds after X-ray irradiation
It is possible to scan images with a sufficiently high SN ratio. Also got
Both the quality of the radiographic image and the read throughput
Start reading within 1 minute at the longest after X-ray irradiation
Is preferable, and there is almost no deterioration in image quality even within 30 seconds.
None, more preferable. However, 1 minute or more after X-ray irradiation
That reduces read throughput and is economical
It will be a disadvantage. On the other hand, FIG. 5 (a) shows a conventionally known divalent europium
Active barium fluorobromide stimulable phosphor (BaFBr: Eu2+) Emission
Shows the characteristics, a is the fluorescence by X-ray irradiation, b is the fluorescence
The decay curve of the afterglow due to, c is the stimulated emission. Fig. 5
(B) shows He as a stimulated excitation light source instead of a semiconductor laser.
-The same as in Fig. 2 (b) except that a Ne laser was used.
Is the SNR obtained by Conventional divalent europium activated barium fluorobromide stimulable firefly
Since the optical body has a lot of fluorescent afterglow and has a long life, the SN ratio is 103
To achieve the above, at least 1 minute after X-ray irradiation
After that, it is necessary to perform image reading, and the reading throughput
Is significantly reduced. The stimulable phosphor layer is supported by, for example, the following method.
It can be formed on the body. First, the stimulable phosphor particles and the binder are mixed with a suitable solvent.
In addition to this, it is thoroughly mixed and stimulable fluorescent in the binder solution.
Prepare a coating solution in which body particles are uniformly dispersed. Examples of the binder for the stimulable phosphor layer include gelatin and the like.
Bolisaccharides such as protein and dextran or
Natural polymeric substances such as labia gum; and polyvinyl
Chiral, polyvinyl acetate, nitrocellulose, ethyl
Cellulose, vinylidene chloride / vinyl chloride copolymer,
Polymethylmethacrylate, vinyl chloride / vinyl acetate
Polymer, polyurethane, cellulose acetate butyre
Sheets, polyvinyl alcohol, linear polyester, etc.
Binders represented by such synthetic polymer substances are listed.
You can get it. Examples of the solvent for adjusting the coating solution include methanol and ethanol.
Alcohol, n-propanol, n-butanol, etc.
: Methylene chloride, ethylene chloride, etc.
Hydrocarbons containing chlorine atoms; acetone, methyl ethyl keto
And ketones such as methyl isobutyl ketone: Methyl acetate
Lower fatty acid vinegar and lower alcohol such as
Esters with rucor; dioxane, ethylene glycol
Ruethyl ether, ethylene glycol monomethyl ester
Ethers such as ter: and list their mixtures
be able to. The mixing ratio of the binder and the stimulable phosphor particles in the coating liquid is
Target conversion panel characteristics, types of stimulable phosphor particles
Generally, a binder and a photostimulable phosphor
Mixing ratio with particles is from 1: 1 to 1: 100 (weight ratio)
Selected, and especially in the range 1: 8 to 1:40 (weight ratio)
It is preferable to choose from It should be noted that the coating liquid is a stimulable phosphor in the coating liquid.
Dispersant for improving the dispersibility of particles, and also after formation
Binder and stimulable phosphor particles in the stimulable phosphor layer
Various plasticizers to improve the bond strength between
Additives may be mixed. Used for such purposes
Examples of dispersants that can be used include phthalic acid, stearic acid,
Caproic acid, lipophilic surfactant, etc. can be mentioned.
The Examples of plasticizers include triphenyl phosphate and phosphorus.
Phosphates such as tricresyl acid and diphenyl phosphate;
For example, diethyl phthalate or dimethoxyethyl phthalate
Talic acid ester; Ethyl glycolate Phthalylethyl ester,
Glycolic acid such as butyl phthalyl butyl glycolate
Esters: And triethylene glycol and adipine
Polyester with acid, diethylene glycol and succinic acid
Polyethylene glycol such as polyester and fat
Examples include polyesters with group dibasic acids
The Photostimulable phosphor particles and binder prepared as described above
Then, the coating solution containing and is uniformly applied to the surface of the support.
By doing so, a coating film of the coating liquid is formed. Of this coating liquid
The coating operation is carried out by a conventional coating means such as a doctor blade,
By using a roll coater, knife coater, etc.
Can be done. After forming the coating film, dry it by gradually heating the coating film.
The formation of the stimulable phosphor layer on the support is completed. Kagayaki
The thickness of the exhaustive phosphor layer depends on the characteristics of the target conversion panel and the brightness.
Of the type of stimulable phosphor particles, the binder and the stimulable phosphor particles
Normally 20 μm to 1 mm, depending on the mixing ratio
And However, it is preferable that this layer thickness is 50 to 500 μm.
Good. Further, the stimulable phosphor layer is not always on the support as described above.
It is not necessary to directly apply the coating solution to the
Apply the coating solution on a sheet such as a protective layer and dry it.
After forming the phosphor layer with, press it onto the support.
Or stimulable with the support by using an adhesive
It may be joined to the phosphor layer. The stimulable phosphor layer may be composed of a single layer,
Two or more layers may be laminated. Another method of forming the photostimulable phosphor layer is vapor deposition.
The As the vapor deposition method, vacuum vapor deposition method, sputtering
Method, CVD method, etc. can be used. Alkali halide Kagayaki
The photostimulable phosphor is formed by the vapor deposition method to form the photostimulable phosphor.
It is easy to use this method. In the conversion panel according to the present invention, the stimulable phosphor layer has a self
When it has no supporting ability, it supports the stimulable phosphor layer.
Support is provided. As the support, various types
Child material, glass, metal, etc. are used.
Film, polyester film, polyethylene film
Rephthalate film, Polyamide film, Polyimide
Film, triacetate film, polycarbonate
Film such as plastic film, aluminum film
Sheet, metal sheet such as iron sheet, copper sheet or the like
A metal sheet having an oxide coating layer is preferred. The surface of these supports may be smooth or stimulable.
As a matte surface for the purpose of improving the adhesiveness with the phosphor layer
Good. Also, the surface of the support may be an uneven surface,
It may be a structure in which tiled boards that are isolated are spread. former
In the case of, the photostimulable phosphor layer is subdivided by the uneven surface.
Therefore, the sharpness of the image is further improved. In the latter case
The photostimulable phosphor layer maintains the contours of the support tile plate.
However, as a result, the stimulable phosphor layer cracks.
The columnar block of photostimulable phosphor isolated by
Therefore, the sharpness of the image is further improved. In addition, these supports have an improved adhesiveness with the stimulable phosphor layer.
Undercoat layer on the surface where the stimulable phosphor layer is provided for the purpose of raising
May be provided. Also, the layer thickness of these supports is
It depends on the material of the support, etc.
00 μm, and more preferably 80 to 80 from the viewpoint of handling.
It is 1000 μm. In the conversion panel according to the present invention, the photostimulability is generally
On the surface opposite to the surface on which the phosphor layer is provided, stimulable fluorescent
A protective layer is provided to physically or chemically protect the body layer.
You may be kicked. This protective layer stimulates the coating liquid for protective layer
It may be applied directly on the phosphor layer, or it may be formed separately in advance.
A protective layer may be adhered on the stimulable phosphor layer. Or another
The procedure for forming a stimulable phosphor layer on the protective layer that has been formed
Very good. As a material for the protective layer, cellulose acetate,
Nitrocellulose, polymethylmethacrylate, polybi
Nylbutyral, polyvinyl formal, polycarbonate
Sheet, polyester, polyethylene terephthalate, polyethylene
Polyethylene, polyvinylidene chloride, nylon, polytetrafluoroethylene
Ethylene fluoride, polytrifluoride-ethylene chloride, tetrafluoride
Ethylene-hexafluoropropylene copolymer, vinylidene chloride
-Vinyl chloride copolymer, vinylidene chloride-acryloni
Ordinary protective layer materials such as toll copolymers are used. Well
In addition, this protective layer is made of Si by vapor deposition, sputtering, etc.
C, SiO2, SiN, Al2O3Even if it is formed by laminating inorganic substances such as
Good. The thickness of these protective layers is generally 0.1 μm to 100 μm.
About m is preferable. [Examples] Hereinafter, the present invention will be described using examples. Example 1 The conversion panel is RbBr: Tl+13 parts by weight of stimulable phosphor
And 1 part by weight of polyvinyl butyral as a solvent (cyclohexene
Sanon) to disperse and
Apply evenly on the tarate substrate, let stand overnight and let it dry naturally.
A stimulable phosphor layer of about 300 μm is formed by drying.
I made it. 50 X-rays with a tube voltage of 80KV are applied to this conversion panel.
After irradiating 0 milli-roentgen and 10 seconds later, with a 25mW semiconductor laser.
The image signal was read. Fluorescent afterglow just before reading the image signal
The ratio of the signal size to the image signal size (SN ratio)
The results are shown in Table 1. Comparative example RbBr: Tl as stimulable phosphor+Instead of BaFBr: Eu2+For
A conversion panel was prepared in the same manner as in Example 1 except that
The image signal was read with a He-Ne laser 10 seconds after irradiation. Picture
The magnitude of the fluorescence afterglow signal and the image just before reading the image signal
Table 1 shows the ratio (SN ratio) to the signal magnitude. Example 2 As in Example 1, RbBr: Tl+Photostimulable phosphor 60% by weight, BaFB
r: Eu2+A conversion panel was prepared using 40% by weight. next,
The conversion panel was irradiated with X-rays for 10 seconds as in Example 1.
Later, we read the image signal with a semiconductor laser. Read image signal
Magnitude of fluorescence afterglow signal and magnitude of the image signal just before taking
The ratio (SN ratio) to and is shown in Table 1.From Example 1 and Comparative Example, alkali was used as the stimulable phosphor.
RbBr: Tl, a halide photostimulable phosphor+When using a phosphor
In this case, even if the image is read immediately after X-ray irradiation, an image with a high SN ratio is obtained.
It was obtained. In addition, the alkali halide phosphor is added from Example 2.
The afterglow of the fluorescent light decreases, and the image is read immediately after X-ray irradiation.
Sufficiently high SN ratio was obtained even if it went. As described above, the radiation image information reading method of the present invention
The methods are: i) Emissions transmitted through the subject or emitted from the subject.
The ray is mainly composed of a stimulable phosphor represented by the following general formula
Absorbed in the radiation image conversion panel contained as a general formula MIX ・ aMIIX ′Two・ BMIIIX ″3: cA (However, MIIs at least selected from Li, Na, K, Rb and Cs
A kind of alkali metal, MIIIs Be, Mg, Ca, Sr, Ba, Zn, C
At least one divalent metal selected from d, Cu and Ni
MIIIIs Sc, Y, La, Ce, Pr, Nd, Pm, Sm, Eu, Gd, Tb, Dy, Ho, Er,
At least one of three selected from Tm, Yd, Lu, Al, Ga and In
It is a valent metal. X, X'and X "are selected from F, Cl, Br and I
It is at least a kind of halogen. A is Tm, Dy, Pr, H
o, Nd, Yb, Gd, Lu, Sm, Y, Tl, Na, Ag, Cu and Mg
At least it is a kind of metal. Also, a is a numerical value in the range of 0 ≦ a <0.5, and b is 0 ≦ b <
It is a numerical value in the range of 0.5, and c is a numerical value in the range of 0 <c <0.2.
is there. Ii) Immediately after the step i), the radiation image conversion pattern is
The channel is irradiated with stimulated excitation light in the wavelength range of 500 to 900 nm.
By, it is stored and recorded in the radiation image conversion panel.
The technology to emit the radiant energy as stimulated emission
Iii) The step of detecting the stimulated luminescence;
There is little noise, and an accurate image signal that matches the actual image is obtained and SN
It is possible to obtain a high quality reconstructed image with good ratio. Further, according to the present invention, the amount of fluorescent afterglow is extremely small, and
Before there is no need to set a waiting time until reading with afterglow
The alkali halide stimulable phosphor represented by the general formula
Since it is used, from the irradiation of radiation to the reading of images
It can shorten the time and improve the throughput of the device.
It is not possible to read image information in rapid succession in large quantities.
Which has various excellent effects.

【図面の簡単な説明】[Brief description of drawings]

第1図は本発明の方法を実施する装置の一例を示す略示
的断面図,第2図は本発明の放射線画像読取方法に用い
られる輝尽性蛍光体の一例としてタリウム付活臭化ルビ
ジウム輝尽性蛍光体の発光特性を示す図,第3図は従来
の放射線画像情報読取方法を実施する装置の略示的斜視
図,第4図は蛍光残光の減衰曲線を示す図,第5図は従
来公知の二価のユーロピウム付活弗化臭化バリウム輝尽
性蛍光体の発光特性を示す図である. 101……放射線源 102……被写体 103……変換パネル 104……アルカリハライド輝尽性螢光体層 105……輝尽励起光源 108……集光体
FIG. 1 is a schematic cross-sectional view showing an example of an apparatus for carrying out the method of the present invention, and FIG. 2 is an example of a stimulable phosphor used in the radiation image reading method of the present invention, which is thallium-activated rubidium bromide. FIG. 3 is a diagram showing the emission characteristics of a stimulable phosphor, FIG. 3 is a schematic perspective view of an apparatus for carrying out a conventional radiation image information reading method, and FIG. 4 is a diagram showing a decay curve of fluorescence afterglow. The figure shows the emission characteristics of a conventionally known divalent europium-activated barium fluorobromide stimulable phosphor. 101 …… Radiation source 102 …… Subject 103 …… Conversion panel 104 …… Alkali halide stimulable phosphor layer 105 …… Stimulated excitation light source 108 …… Concentrator

───────────────────────────────────────────────────── フロントページの続き (72)発明者 網谷 幸二 東京都日野市さくら町1番地 小西六写真 工業株式会社内 (72)発明者 島田 文生 東京都日野市さくら町1番地 小西六写真 工業株式会社内 ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Koji Amitani No. 1 Sakura-cho, Hino-shi, Tokyo Photo Konishi Roku Photo Industry Co., Ltd. (72) Inventor Fumio Shimada No. 1 Sakura-cho, Hino-shi, Tokyo Photo Photo Roku Konishi In the company

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】i)被写体を透過した,或いは被検体から
発せられた放射線を下記一般式で表される輝尽性蛍光体
を主成分として含有する放射線画像変換パネルに吸収さ
せる工程; 一般式 MIX・aMIIX′・bMIIIX″3:cA (但し,MIはLi,Na,K,Rb及びCsから選ばれる少なくとも
一種のアルカリ金属であり,MIIはBe,Mg,Ca,Sr,Ba,Zn,C
d,Cu及びNiから選ばれる少なくとも一種の二価金属であ
る.MIIIはSc,Y,La,Ce,Pr,Nd,Pm,Sm,Eu,Gd,Tb,Dy,Ho,Er,
Tm,Yd,Lu,Al,Ga及びInから選ばれる少なくとも一種の三
価金属である.X,X′及びX″はF,Cl,Br及びIから選ば
れるすくなくとも一種のハロゲンである.AはTm,Dy,Pr,H
o,Nd,Yb,Er,Gd,Lu,Sm,Y,Tl,Na,Ag,Cu及びMgから選ばれ
る少なくとも一種の金属である.また,aは0≦a<0.5
の範囲の数値であり,bは0≦b<0.5の範囲の数値であ
り,cは0<c<0.2の範囲の数値である.) ii)前記i)の工程終了後,直ちに該放射線画像変換パ
ネルに500〜900nmの波長領域の輝尽励起光を照射するこ
とにより,該放射線画像変換パネルに蓄積・記録されて
いる放射線エネルギーを輝尽発光として放出させる工
程; iii)該輝尽発光を検出する工程; を含むことを特徴とする放射線画像読取方法.
1. A step of: i) a radiation image conversion panel containing a stimulable phosphor represented by the following general formula as a main component, which absorbs radiation transmitted through a subject or emitted from a subject; M I X · aM II X ' 2 · bM III X "3: cA ( where, M I is at least one alkali metal selected Li, Na, K, from Rb and Cs, M II is be, Mg, Ca, Sr, Ba, Zn, C
d, Cu and at least one divalent metal selected from Ni. M III is Sc, Y, La, Ce, Pr, Nd, Pm, Sm, Eu, Gd, Tb, Dy, Ho, Er,
It is at least one trivalent metal selected from Tm, Yd, Lu, Al, Ga and In. X, X ′ and X ″ are at least one halogen selected from F, Cl, Br and I. A is Tm, Dy, Pr, H
It is at least one metal selected from o, Nd, Yb, Er, Gd, Lu, Sm, Y, Tl, Na, Ag, Cu and Mg. Also, a is 0 ≦ a <0.5
Is a numerical value in the range of, b is a numerical value in the range of 0 ≦ b <0.5, and c is a numerical value in the range of 0 <c <0.2. Ii) Immediately after completion of the step i), the radiation image conversion panel is irradiated with stimulated excitation light in the wavelength region of 500 to 900 nm so that the radiation energy stored and recorded in the radiation image conversion panel is irradiated. A radiation image reading method comprising: a step of releasing as stimulated emission; iii) a step of detecting the stimulated emission.
【請求項2】前記輝尽励起光が,半導体レーザ光である
特許請求の範囲第1項記載の放射線画像読取方法.
2. The radiation image reading method according to claim 1, wherein the stimulated excitation light is a semiconductor laser light.
JP61055971A 1986-03-13 1986-03-13 Radiation image reading method Expired - Lifetime JPH0731367B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61055971A JPH0731367B2 (en) 1986-03-13 1986-03-13 Radiation image reading method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61055971A JPH0731367B2 (en) 1986-03-13 1986-03-13 Radiation image reading method

Publications (2)

Publication Number Publication Date
JPS62211637A JPS62211637A (en) 1987-09-17
JPH0731367B2 true JPH0731367B2 (en) 1995-04-10

Family

ID=13013960

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61055971A Expired - Lifetime JPH0731367B2 (en) 1986-03-13 1986-03-13 Radiation image reading method

Country Status (1)

Country Link
JP (1) JPH0731367B2 (en)

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6046166A (en) * 1983-08-23 1985-03-12 Fuji Photo Film Co Ltd Reader of radiation picture information
JPS60111568A (en) * 1983-11-21 1985-06-18 Fuji Photo Film Co Ltd Radiation picture information reader
JPH0644080B2 (en) * 1984-08-08 1994-06-08 コニカ株式会社 Radiation image conversion method

Also Published As

Publication number Publication date
JPS62211637A (en) 1987-09-17

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