JPH0943357A - Driving method for radiation detector - Google Patents
Driving method for radiation detectorInfo
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- JPH0943357A JPH0943357A JP7189957A JP18995795A JPH0943357A JP H0943357 A JPH0943357 A JP H0943357A JP 7189957 A JP7189957 A JP 7189957A JP 18995795 A JP18995795 A JP 18995795A JP H0943357 A JPH0943357 A JP H0943357A
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- radiation detector
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Abstract
(57)【要約】
【課題】 CdTe等の半導体放射線検出器を、高いX
線光子量領域でも動作させることのできる駆動方法を提
供する。
【解決手段】 高線量のX線が検出器に入射したとき
に、結晶内部に電荷がトラップされ、このトラップ電荷
により空間電荷が形成され、この空間電荷が原因となっ
て結晶にバイパスがかからなくなり、検出器が正常に動
作しなくなるわけであるが、検出器を空間電荷制限電流
で動作させることで、電極から電荷が結晶内部に注入さ
れ、トラップされた電荷と再結合する結果、結晶内部の
電荷空間が解消される。
(57) Abstract: A semiconductor radiation detector such as CdTe has a high X
Provided is a driving method which can be operated even in a line photon amount region. SOLUTION: When a high dose of X-rays enters a detector, charges are trapped inside the crystal, and the trapped charges form space charges, which cause the crystals to bypass. However, by operating the detector with a space charge limited current, the charge is injected from the electrode into the crystal and recombines with the trapped charge. The charge space of is eliminated.
Description
【0001】[0001]
【発明の属する技術分野】本発明は医用X線撮像装置に
利用される放射線検出器の駆動方法に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method for driving a radiation detector used in a medical X-ray imaging apparatus.
【0002】[0002]
【従来の技術】X線検出器としては化合物半導体検出器
が知られており、この半導体検出器のうち、特に、Cd
Te放射線検出器は常温で使用でき、高いエネルギが検
出できる等の利点があることから様々な開発が行われて
きた。2. Description of the Related Art A compound semiconductor detector is known as an X-ray detector, and among these semiconductor detectors, particularly Cd.
Since the Te radiation detector can be used at room temperature and has advantages such as high energy detection, various developments have been made.
【0003】この種の半導体検出器は、一般に、化合物
半導体基板の両面に電極を形成し、これら電極間へのバ
イアス印加により結晶を空乏層化し、この状態の結晶内
部にX線光子が入射した際に発生する電荷を、電極を通
じて外部に取り出す構造となっており、その電荷パルス
の計数により入射したX線光子の量を知ることができ
る。In this type of semiconductor detector, generally, electrodes are formed on both sides of a compound semiconductor substrate, a crystal is depleted by applying a bias between these electrodes, and X-ray photons are incident inside the crystal in this state. The charge generated at that time is taken out to the outside through the electrode, and the amount of the incident X-ray photons can be known by counting the charge pulse.
【0004】[0004]
【発明が解決しようとする課題】ところで、CdTe等
の半導体検出器を医用X線撮像の分野で使用するために
は、高いX線光子量の領域でも作動する検出器であるこ
とが必要となる。By the way, in order to use a semiconductor detector such as CdTe in the field of medical X-ray imaging, it is necessary that the detector be operable even in a high X-ray photon amount region. .
【0005】しかしながら、CdTe放射線検出器等
は、従来、専ら低いX線光子量の領域でのエネルギ分解
つまりスペクトル測定に使用されていることから、検出
器の動作条件(バイアス印加条件)も、結晶が空乏層化
されれば良い程度つまり電流電圧特性でいうところのオ
ーミック領域に設定されている。However, since CdTe radiation detectors and the like are conventionally used exclusively for energy decomposition in the region of low X-ray photon amount, that is, spectrum measurement, the operating conditions (bias application conditions) of the detector are also crystallized. Is set to a depletion layer, that is, the ohmic region in terms of current-voltage characteristics.
【0006】従って、高いX線光子量領域での動作に関
しては不明ではあるものの、入射X線が高線量になると
空間電荷の発生等の原因により計数率が低下するのは明
らかで、また、実際に、動作条件をオーミック領域に設
定して高X線線量域での検出を行ったところ、計数率が
低下することが判明した。Therefore, although the operation in the high X-ray photon amount region is unknown, it is clear that the count rate decreases when the incident X-ray becomes a high dose due to the generation of space charge, and in fact, Moreover, when the operating condition was set to the ohmic region and the detection was performed in the high X-ray dose range, it was found that the count rate decreased.
【0007】本発明はこのような実情に鑑みてなされた
もので、CdTe等の半導体放射線検出器を、高いX線
光子量領域でも動作させることのできる駆動方法を提供
することにある。The present invention has been made in view of the above circumstances, and an object thereof is to provide a driving method capable of operating a semiconductor radiation detector such as CdTe even in a high X-ray photon amount region.
【0008】[0008]
【課題を解決するための手段】上記の目的を達成するた
め、本発明は、CdTe等の化合物半導体基板の表裏両
面にそれぞれ電極が形成された構造で、その表裏の電極
間にバイアスを印加した状態で放射線が入射したときに
電荷パルスを発生する放射線検出器において、バイアス
印加条件を空間電荷制限電流領域に設定することによっ
て特徴づけられる。In order to achieve the above object, the present invention has a structure in which electrodes are formed on both front and back surfaces of a compound semiconductor substrate such as CdTe, and a bias is applied between the front and back electrodes. In a radiation detector that generates a charge pulse when radiation enters in a state, it is characterized by setting a bias application condition to a space charge limited current region.
【0009】ここで、本発明で言う、空間電荷制限電流
領域とは、この種の検出器の電流電圧特性において、オ
ーミック電流以上で電圧の2乗に比例して変化する電流
の領域をさす(図2参照)。Here, the space charge limited current region referred to in the present invention refers to a region of a current that changes in proportion to the square of the voltage above the ohmic current in the current-voltage characteristics of this type of detector ( See FIG. 2).
【0010】そして、このような空間電荷制限電流領域
で検出器を動作させることで、高線量のX線が検出器に
入射しても正常に動作する。その理由を以下に述べる。
まず、この種の放射線検出器では、X線入射により発生
した電荷は結晶中にトラップされ、このトラップされた
電荷が空間電荷を形成する。この空間電荷は、入射X線
が低線量で入射X線光子の時間間隔が充分に長い場合に
は、その入射間隔内で解消されるので問題はないが、入
射X線が高線量となると、空間電荷が解消されないうち
に次のX線光子が入射するため、結晶にバイアスがかか
らなくなってしまい、このことが、計数率の低下、計数
安定性の低下を引きおこす原因となる。By operating the detector in such a space charge limited current region, the detector operates normally even when a high dose of X-rays enters the detector. The reason is described below.
First, in this type of radiation detector, charges generated by X-ray incidence are trapped in the crystal, and the trapped charges form space charges. If the incident X-rays have a low dose and the time interval of the incident X-ray photons is sufficiently long, this space charge is resolved within the incident intervals, so there is no problem, but when the incident X-rays have a high dose, Since the next X-ray photon is incident before the space charge is eliminated, the crystal is not biased, which causes a decrease in the counting rate and a decrease in the counting stability.
【0011】従って、高X線線量域での正常な検出を可
能とするには、電荷のトラップにより形成された空間電
荷が速やかに解消されるようにすればよく、これを達成
するため、本発明では、空間電荷制限電流領域(図2)
で動作させるといった方法を採っており、このような動
作条件により、電極から結晶内部に電荷が注入され、ト
ラップされた電荷と再結合する結果、結晶内部の空間電
荷が瞬時に解消され、結晶にバイアスがかかるようにな
る。Therefore, in order to enable normal detection in the high X-ray dose range, it is sufficient to promptly eliminate the space charges formed by the charge traps. In the invention, the space charge limited current region (Fig. 2)
Under these operating conditions, charges are injected from the electrodes into the crystal and recombine with the trapped charges.As a result, the space charge inside the crystal is instantly eliminated and Be biased.
【0012】[0012]
【発明の実施の形態】図1は本発明の実施の形態を示す
図である。この図1に示す放射線検出器は、化合物半導
体基板1の一面に、Auを一様に蒸着してなる共通電極
2が形成され、その反対側の面には、複数個の分割電極
(Niメッキ製)3・・3が行列状に形成された構造の検
出器で、その共通電極2に逆バイアス(−V)が印加さ
れ、この状態で、放射線が入射したときに電荷パルスを
発生するように構成されている。FIG. 1 is a diagram showing an embodiment of the present invention. In the radiation detector shown in FIG. 1, a common electrode 2 formed by uniformly depositing Au is formed on one surface of a compound semiconductor substrate 1, and a plurality of split electrodes (Ni plating) are formed on the opposite surface. 3 ... 3 is a detector having a structure formed in a matrix, and a reverse bias (-V) is applied to the common electrode 2 thereof, and in this state, a charge pulse is generated when radiation is incident. Is configured.
【0013】なお、この図1の構造において分割電極3
・・3は接地側に置かれ、また、各分割電極3・・3には、
それぞれ前置増幅器3a・・3aが接続されている。そし
て、この実施の形態においては、動作条件つまりバイア
ス印加条件を、図2に示す電圧電流特性においてオーミ
ック電流以上となる空間電荷制限電流領域に設定する点
と、化合物半導体基板1として、垂直ブリッジマン法あ
るいは温度勾配法など、自然固化によって作製された塩
素ドープCdTe単結晶を用いている点に特徴がある。In the structure of FIG. 1, the split electrode 3
..3 is placed on the ground side, and each split electrode 3 ...
Preamplifiers 3a ... 3a are connected to each. Further, in this embodiment, the operating condition, that is, the bias applying condition is set to a space charge limited current region in which the ohmic current is equal to or higher than the ohmic current in the voltage-current characteristics shown in FIG. Is characterized by using a chlorine-doped CdTe single crystal produced by natural solidification, such as the method or temperature gradient method.
【0014】このように放射線検出器を空間電荷制限電
流領域で動作させると、先に述べたように、高線量のX
線が入射した際の計数率が低下することがなく、さら
に、高X線線量域での計数安定性も良くなる。When the radiation detector is operated in the space charge limited current region in this manner, as described above, a high dose of X
The counting rate when a ray is incident does not decrease, and the counting stability in the high X-ray dose range is improved.
【0015】また、化合物半導体基板1に塩素ドープC
dTe単結晶を用いると、図2に示す電流電圧特性にお
いて、オーミック領域から空間電荷制限電流領域へと変
化する点Cpを、他のドーパントを用いた場合よりも低
い値とすることができ、これにより、結晶に高いバイア
スを印加することにより生じる弊害・影響を軽減するこ
とができる。Further, chlorine-doped C is added to the compound semiconductor substrate 1.
When the dTe single crystal is used, in the current-voltage characteristics shown in FIG. 2, the point Cp at which the ohmic region changes to the space charge limited current region can be set to a lower value than when other dopants are used. As a result, it is possible to reduce the adverse effects and effects caused by applying a high bias to the crystal.
【0016】なお、以上の実施の形態のように、化合物
半導体基板1をCdTe単結晶とする場合、そのドーパ
ントとして塩素に代えて、例えばIn,Ge等の他の元
素を用いてもよいし、あるいはノンドープの単結晶を用
いてもよい。ただし、前記したように、空間電荷制限電
流領域で動作させるためのバイアス条件Cpを低く設定
できる点を考慮すると、塩素ドープCdTeを用いるこ
とが好ましい。When the compound semiconductor substrate 1 is made of CdTe single crystal as in the above-mentioned embodiments, other elements such as In and Ge may be used instead of chlorine as the dopant. Alternatively, a non-doped single crystal may be used. However, as described above, considering that the bias condition Cp for operating in the space charge limited current region can be set low, it is preferable to use chlorine-doped CdTe.
【0017】また、以上の実施の形態では、化合物半導
体基板1としてCdTe単結晶を用いた検出器に、本発
明を適用した例を示したが、これに限られることなく、
本発明は、例えばGaAsまたはHgI2 の結晶等の他
の化合物半導体を用いた放射線検出器にも適用できる。Further, in the above-mentioned embodiments, the example in which the present invention is applied to the detector using the CdTe single crystal as the compound semiconductor substrate 1 is shown, but the present invention is not limited to this.
The present invention can be applied to a radiation detector using other compound semiconductor such as GaAs or HgI 2 crystal.
【0018】ここで、本発明において検出器を空間電荷
制限電流で動作させるための条件、すなわち、図2に示
した点Cpは、基板に用いる化合物半導体の種類、ドー
パントの元素種、電極の材質(例えばAu,Ni,P
t,Ir,Se,In,CuまたはAl等)、並びに基
板と電極のコンタクト法、等のパラメータによって決ま
るので、それらの各パラメータを適当に選定することに
より、適正なバイアス印加条件つまり図2の点Cpが最
小値となる条件を決定することができる。Here, in the present invention, the condition for operating the detector with the space charge limited current, that is, the point Cp shown in FIG. 2 is the kind of compound semiconductor used for the substrate, the kind of dopant element, the material of the electrode. (For example, Au, Ni, P
t, Ir, Se, In, Cu or Al, etc., and the contact method between the substrate and the electrode, etc., so that appropriate bias application conditions, that is, as shown in FIG. The condition that the point Cp becomes the minimum value can be determined.
【0019】[0019]
【実施例】図1に示した構造のCdTe(塩素ドープ)
放射線検出器において、バイアス印加条件を、空間電荷
制限電流領域とした場合と、オーミック領域とした場合
について、それぞれ、入射X線線量を変化させて計数率
を測定したところ、図3に示すような計数特性が得られ
た。EXAMPLES CdTe (chlorine-doped) having the structure shown in FIG.
In the radiation detector, the incident X-ray dose was changed and the count rate was measured when the bias application conditions were the space charge limited current region and the ohmic region, respectively. Counting characteristics were obtained.
【0020】この図3から明らかなように、オーミック
領域での動作条件では、高線量のX線入射において計数
率が低下するのに対し、空間電荷制限電流領域では、そ
のような計数率の低下が現れないことが確認できた。As is apparent from FIG. 3, under the operating conditions in the ohmic region, the count rate decreases at high dose X-ray incidence, whereas in the space charge limited current region, the count rate decreases. It was confirmed that did not appear.
【0021】また、同じくバイアス印加条件を、空間電
荷制限電流領域とした場合と、オーミック領域とした場
合について、それぞれ、高X線線量域と低いX線線量域
の二つの領域で計数率の時間安定性についての測定を行
ったところ、図4(A) と(B)に示す結果が得られた。Similarly, when the bias application condition is set to the space charge limited current region and the ohmic region, the count rate time is set in two regions, a high X-ray dose region and a low X-ray dose region, respectively. When the stability was measured, the results shown in FIGS. 4 (A) and 4 (B) were obtained.
【0022】この測定結果から明らかなように、空間電
荷制限電流領域で放射線検出器を動作させることで、高
X線線量域でも計数安定性が良くなることが確認でき
た。As is clear from the measurement results, it was confirmed that the counting stability was improved even in the high X-ray dose region by operating the radiation detector in the space charge limited current region.
【0023】[0023]
【発明の効果】以上説明したように、本発明方法では、
放射線検出器に印加するバイアスの条件を、空間電荷制
限電流領域としているので、結晶内部で形成される空間
電荷の問題が解消され、これにより高線量のX線が入射
した場合でも検出器が正常に動作する。その結果、高い
X線光子量領域でも安定した計数測定が可能になり、例
えばCdTe放射線検出器を医用X線撮像の分野で使用
することが可能となる。As described above, according to the method of the present invention,
Since the bias condition applied to the radiation detector is the space charge limited current region, the problem of space charge formed inside the crystal is solved, which allows the detector to operate normally even when a high dose of X-rays is incident. To work. As a result, stable count measurement is possible even in a high X-ray photon amount region, and for example, the CdTe radiation detector can be used in the field of medical X-ray imaging.
【図1】本発明の実施の形態を示す図FIG. 1 is a diagram showing an embodiment of the present invention.
【図2】放射線検出器の電流電圧特性を示すグラフFIG. 2 is a graph showing a current-voltage characteristic of a radiation detector.
【図3】本発明の実施例の説明図で計数率特性の測定結
果を示すグラフFIG. 3 is a graph showing measurement results of count rate characteristics in an explanatory diagram of an example of the present invention.
【図4】同じく実施例の説明図で計数率の時間安定性の
高X線線域での測定(A) と低X線線域での測定(B) の各
測定結果を示すグラフFIG. 4 is a graph showing the measurement results of the time stability of counting rate in the high X-ray region (A) and the low X-ray region (B), which are also explanatory views of the embodiment.
1 化合物半導体基板(塩素ドープCdTe単結晶) 2 共通電極 3 分割電極 1 Compound semiconductor substrate (chlorine-doped CdTe single crystal) 2 Common electrode 3 Split electrode
Claims (1)
ぞれ電極が形成された構造で、その表裏の電極間にバイ
アスを印加した状態で放射線が入射したときに電荷パル
スを発生する放射線検出器において、バイアス印加条件
を空間電荷制限電流領域に設定することを特徴とする放
射線検出器の駆動方法。1. A radiation detector, which has a structure in which electrodes are formed on both front and back surfaces of a compound semiconductor crystal substrate, and which generates a charge pulse when radiation is incident with a bias applied between the front and back electrodes, A method of driving a radiation detector, characterized in that a bias application condition is set in a space charge limited current region.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP18995795A JP3520613B2 (en) | 1995-07-26 | 1995-07-26 | Driving method of radiation detector |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP18995795A JP3520613B2 (en) | 1995-07-26 | 1995-07-26 | Driving method of radiation detector |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0943357A true JPH0943357A (en) | 1997-02-14 |
| JP3520613B2 JP3520613B2 (en) | 2004-04-19 |
Family
ID=16250029
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP18995795A Expired - Fee Related JP3520613B2 (en) | 1995-07-26 | 1995-07-26 | Driving method of radiation detector |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP3520613B2 (en) |
Cited By (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| FR2793954A1 (en) * | 1999-05-19 | 2000-11-24 | Commissariat Energie Atomique | Semiconductor radiation detector, useful in radiography for medical applications or non-destructive examination, has at least one electrode sub-divided into individually voltage-biased zones |
| JP2007525812A (en) * | 2003-11-10 | 2007-09-06 | トゥー‐シックス・インコーポレイテッド | Radiation detector |
| JP2016505827A (en) * | 2012-12-04 | 2016-02-25 | コーニンクレッカ フィリップス エヌ ヴェKoninklijke Philips N.V. | Photon counting X-ray detector |
| JP2016198493A (en) * | 2015-04-07 | 2016-12-01 | 東芝メディカルシステムズ株式会社 | X-ray detector apparatus and X-ray CT apparatus |
| CN109888051A (en) * | 2019-03-08 | 2019-06-14 | 中国科学院物理研究所 | An X-ray detector and its manufacturing method |
-
1995
- 1995-07-26 JP JP18995795A patent/JP3520613B2/en not_active Expired - Fee Related
Cited By (9)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| FR2793954A1 (en) * | 1999-05-19 | 2000-11-24 | Commissariat Energie Atomique | Semiconductor radiation detector, useful in radiography for medical applications or non-destructive examination, has at least one electrode sub-divided into individually voltage-biased zones |
| WO2000072386A1 (en) * | 1999-05-19 | 2000-11-30 | Commissariat A L'energie Atomique | High dynamic radiation detection device |
| US6734431B1 (en) | 1999-05-19 | 2004-05-11 | Commissariat A L'energie Atomique | High dynamic radiation detection device |
| JP2007525812A (en) * | 2003-11-10 | 2007-09-06 | トゥー‐シックス・インコーポレイテッド | Radiation detector |
| JP2016505827A (en) * | 2012-12-04 | 2016-02-25 | コーニンクレッカ フィリップス エヌ ヴェKoninklijke Philips N.V. | Photon counting X-ray detector |
| US10422892B2 (en) | 2012-12-04 | 2019-09-24 | Koninklijke Philips N.V. | Photon counting X-ray detector |
| JP2016198493A (en) * | 2015-04-07 | 2016-12-01 | 東芝メディカルシステムズ株式会社 | X-ray detector apparatus and X-ray CT apparatus |
| CN109888051A (en) * | 2019-03-08 | 2019-06-14 | 中国科学院物理研究所 | An X-ray detector and its manufacturing method |
| CN109888051B (en) * | 2019-03-08 | 2020-11-27 | 中国科学院物理研究所 | An X-ray detector and its manufacturing method |
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