JP2624334B2 - Driving method of solid-state imaging device - Google Patents

Driving method of solid-state imaging device

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Publication number
JP2624334B2
JP2624334B2 JP1151918A JP15191889A JP2624334B2 JP 2624334 B2 JP2624334 B2 JP 2624334B2 JP 1151918 A JP1151918 A JP 1151918A JP 15191889 A JP15191889 A JP 15191889A JP 2624334 B2 JP2624334 B2 JP 2624334B2
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Japan
Prior art keywords
transfer
photoelectric conversion
transfer electrode
charge
electrode
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JP1151918A
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Japanese (ja)
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JPH0316480A (en
Inventor
琢己 山口
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松下電子工業株式会社
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  • Transforming Light Signals Into Electric Signals (AREA)

Description

【発明の詳細な説明】 産業上の利用分野 本発明は固体撮像装置の駆動方法に関するものであ
る。
Description: TECHNICAL FIELD The present invention relates to a driving method of a solid-state imaging device.

従来の技術 近年、固体撮像装置の開発が進み、性能の点から見て
撮像管に匹敵ないし、上回るものがある。そのなかでも
インターライン転送方式CCD固体撮像装置(以下IT−CCD
と略記)は特に優れた特性を持っており実用化されてい
る。
2. Description of the Related Art In recent years, the development of solid-state imaging devices has progressed, and some of them are comparable or superior to imaging tubes in terms of performance. Among them, the inter-line transfer type CCD solid-state imaging device (hereinafter referred to as IT-CCD)
Abbreviations) have particularly excellent properties and have been put to practical use.

以下、図面を参照しながら、IT−CCDの従来の構成に
ついて説明する。
Hereinafter, a conventional configuration of an IT-CCD will be described with reference to the drawings.

第3図はIT−CCDの全体構成図である。第3図におい
て、1は光電変換素子、2は光電変換素子1に蓄積され
た信号電荷を垂直方向に転送する垂直CCD(以下VCCDと
略記)、3はVCCD2により転送された信号電荷を水平方
向に転送する水平転送CCD(以下HCCDと略記)、4はHCC
D3により転送された信号電荷を検知する出力アンプ部、
である。
FIG. 3 is an overall configuration diagram of the IT-CCD. In FIG. 3, 1 is a photoelectric conversion element, 2 is a vertical CCD (hereinafter abbreviated as VCCD) for vertically transferring signal charges stored in the photoelectric conversion element 1, and 3 is a signal for transferring signal charges transferred by VCCD2 in a horizontal direction. Transfer CCD (hereinafter abbreviated as HCCD) to transfer to 4
An output amplifier that detects the signal charge transferred by D3,
It is.

第4図は第3図の破線部Aの拡大図である。この図で
は遮光膜は省略してある。5はVCCD2の転送電極で電荷
を光電変換素子1から読み出した後、転送するφパル
スの加わる転送電極、6は転送のみ行うφパルスの加
わる転送電極、7はφパルスの加わる転送電極と同様
の役割を持つφパルスの加わる転送電極、8は転送の
み行うφパルスの加わる転送電極、9は光電変換素子
1間や、VCCD2と光電変換素子の間を分離する分離領域
であり分離を確実に行うため濃度の高いP形層となって
いる。フィールドモード駆動の固体撮像装置では、光電
変換素子1で発生した電荷は、光電変換素子1から、転
送電極5と7によりVCCD2に読み出され、転送電極5,6,
7,8により、隣り合った2個の光電変換素子1の電荷を
ペアとして混合された後、転送電極5,6,7,8により転送
される。
FIG. 4 is an enlarged view of a broken line portion A in FIG. In this figure, the light shielding film is omitted. 5 after reading from the photoelectric conversion element 1 a charge transfer electrode of VCCD 2, the transfer electrodes applied with phi 1 pulse to be transferred, the transfer electrodes applied with phi 2 pulses to perform only transfer 6, 7 applied with phi 1 pulse transfer electrodes transfer electrodes, applied the phi 3 pulses having the same role as 8 transfer electrodes applied with phi 4 pulses to perform only the transfer, the or between the photoelectric conversion element 1 9, be a separation region separating between VCCD2 the photoelectric conversion element The P-type layer has a high concentration in order to ensure separation. In the solid-state imaging device driven by the field mode, the charge generated in the photoelectric conversion element 1 is read out from the photoelectric conversion element 1 to the VCCD 2 by the transfer electrodes 5 and 7, and is transferred to the transfer electrodes 5, 6,.
After the electric charges of two adjacent photoelectric conversion elements 1 are mixed as a pair by 7, 8, the transfer is performed by the transfer electrodes 5, 6, 7, and 8.

第5図は第4図のB−C間の断面図である。10は基板
のn形層、11は光電変換素子のn形層、12はVCCDのn形
層、13は分離のP形層、14はVCCDの空乏層、15は発生電
荷、16は遮光膜、17は光である。
FIG. 5 is a sectional view taken along the line B-C in FIG. 10 is an n-type layer of a substrate, 11 is an n-type layer of a photoelectric conversion element, 12 is an n-type layer of VCCD, 13 is a separate P-type layer, 14 is a depletion layer of VCCD, 15 is generated charge, and 16 is a light shielding film. , 17 is light.

光電変換素子のn形層11とVCCDのn形層12にはさまれ
た領域は、電荷を低電圧で光電変換素子のn形層11から
VCCDのn形層12に読み出せるように低濃度となってい
る。したがってφパルスの加わる転送電極5に高い電
圧が加わった場合、その領域にVCCDの空乏層14が広が
り、入射した光17による発生電荷15がVCCDのn形層12に
入り易くなり、よってスミア信号の増加をもたらす。そ
れをなくすために、VCCDの転送パルスのうち、電荷を光
電変換素子のn形層11からVCCDのn形層12へ読み出す役
割を持つ転送電極5と7は転送パルスの大部分の期間は
低い電圧が加わるようになっている。
The region sandwiched between the n-type layer 11 of the photoelectric conversion element and the n-type layer 12 of the VCCD is used to transfer electric charges at a low voltage from the n-type layer 11 of the photoelectric conversion element.
It has a low concentration so that it can be read out to the n-type layer 12 of VCCD. Therefore, when the high voltage applied to the transfer electrode 5 applied with phi 1 pulse, the depletion layer 14 of VCCD is spread in the region, generating charge 15 by the light 17 which is incident is likely to enter the n-type layer 12 of VCCD, thus smear This leads to an increase in the signal. In order to eliminate this, among the transfer pulses of the VCCD, the transfer electrodes 5 and 7, which have the role of reading out the charge from the n-type layer 11 of the photoelectric conversion element to the n-type layer 12 of the VCCD, are low during most of the transfer pulse period. The voltage is applied.

第6図は固体撮像装置の駆動タイミング図である。φ
は垂直ブランキングパルスである。18は垂直ブランキ
ング期間、19は有効走査期間、20は光電変換素子1から
VCCD2に電荷を読み出す読み出しパルス、21は電荷を転
送する転送パルス振幅である。光電変換素子1で発生し
た電荷は垂直ブランキング期間18に読み出しパルス20に
よりVCCD2に読み出され、転送パルス振幅21により転送
される。φとφの加わるパルスは、VCCDの空乏層が
広がりをおさえスミアの増加を防ぐため、有効走査期間
19の大部分の期間はLowレベルの電位となっている。
FIG. 6 is a drive timing chart of the solid-state imaging device. φ
5 is a vertical blanking pulse. 18 is the vertical blanking period, 19 is the effective scanning period, 20 is the photoelectric conversion element 1
A read pulse for reading charges to VCCD2, and 21 is a transfer pulse amplitude for transferring charges. The charge generated in the photoelectric conversion element 1 is read out to the VCCD 2 by the readout pulse 20 during the vertical blanking period 18 and is transferred by the transfer pulse amplitude 21. phi 1 and phi 3 of applied pulses, in order to prevent an increase of the smear suppressing a depletion layer expands in the VCCD, effective scanning period
Most of the period of 19 is a low-level potential.

第7図は第6図の垂直ブランキング期間18に転送電極
に加わるパルスタイミング図である。t1,t2,t3,t4,t5
各々時刻を示す。
FIG. 7 is a pulse timing chart applied to the transfer electrodes during the vertical blanking period 18 in FIG. t 1 , t 2 , t 3 , t 4 , and t 5 each indicate time.

第8図は第7図の各時間における第4図,D−E間の断
面ポテンシャル図である。なお22は電荷である。t1のポ
テンシャル図は、φパルスの加わる転送電極5により
光電変換素子1からVCCD2に電荷22が読み出された後の
様子を示す。t2のポテンシャルは、さらに、φパルス
の加わる転送電極7により光電変換素子1からVCCD2へ
電荷22が読み出された後の様子を示す。t3のポテンシャ
ル図は、フィールドモード駆動時に転送電極5と7の下
の電荷22が混合された様子を示す。t4のポテンシャル図
は転送電極5と7をLowレベルにしてスミアの増加を防
いだ時の様子を示す。t5のポテンシャル図は、転送電極
8がHighレベルの電位になった様子を示す。このとき第
4図からわかるように、転送電極8の両側は濃度の高い
分離領域9となっているため、転送電極8がHighレベル
の電位になった場合でも、光電変換素子1側へVCCDの空
乏層14が広がらずスミアの大きな増加はない。
FIG. 8 is a sectional potential diagram between D and E in FIG. 4 at each time in FIG. 22 is a charge. potential diagram t 1 shows a state after the charge 22 is read out from the photoelectric conversion element 1 to VCCD2 by the transfer electrode 5 applied with phi 1 pulse. potential of t 2 further shows a state after the charge from the photoelectric conversion element 1 to the VCCD 2 22 is read by the transfer electrode 7 applied the phi 3 pulses. potential t 3 diagram illustrates how the charge 22 under the transfer electrode 5 when the field mode drive 7 are mixed. potential diagram t 4 shows a state in which prevented the increase of the smear to the transfer electrodes 5 and 7 to the Low level. potential diagram t 5 illustrates how the transfer electrodes 8 becomes a High level potential. At this time, as can be seen from FIG. 4, since both sides of the transfer electrode 8 are the separation regions 9 having a high concentration, even if the transfer electrode 8 becomes the high level potential, the VCCD is transferred to the photoelectric conversion element 1 side. The depletion layer 14 does not spread and there is no large increase in smear.

発明が解決しようとする課題 しかしながら、上記のような構成では、電荷22はφ
パルスの加わる転送電極6の下のみに蓄積されていて、
φパルスの加わる転送電極8の下には電荷22がない状
態となっており、VCCD2の電荷を転送できる容量が、転
送電極6の容量だけで決まってしまうためVCCD2の電荷
を転送できる容量が小さくなってしまう。
However, in the above configuration, the charge 22 is φ 2
Accumulated only under the transfer electrode 6 to which the pulse is applied,
Under the transfer electrodes 8 exerted a phi 4 pulse has a state where there is no electric charge 22, capacity to transfer the charges of VCCD2 is, capacity to transfer the charges of VCCD2 for thus determined only by the capacity of the transfer electrodes 6 It will be smaller.

課題を解決するための手段 上記問題を解決するために、本発明の固体撮像装置の
駆動方法は、行列状に配列された複数個の光電変換素子
と前記光電変換素子で発生した電荷を読み出し、転送す
る複数個の転送電極を持つ転送部を備えた固体撮像装置
において、前記転送電極の下へ、ひとつの出力信号とな
る電荷を分割して蓄積する期間を有する駆動方法となっ
ている。
Means for Solving the Problems In order to solve the above problems, a method for driving a solid-state imaging device according to the present invention reads a plurality of photoelectric conversion elements arranged in a matrix and electric charges generated in the photoelectric conversion elements, In a solid-state imaging device including a transfer unit having a plurality of transfer electrodes for transferring, a driving method has a period in which a charge serving as one output signal is divided and accumulated below the transfer electrode.

作用 この構成によって、転送部の多数の転送電極下へ、ひ
とつの出力信号となる電荷を分割して蓄積することで転
送部の蓄積できる容量を増やすことができる。
Operation With this configuration, it is possible to increase the capacity that can be accumulated in the transfer unit by dividing and accumulating the charge serving as one output signal under a number of transfer electrodes of the transfer unit.

実施例 以下、本発明の実施例について、図面を参照しながら
説明する。第1図は本発明の実施例における垂直ブラン
キング期間の転送電極に加わるパルスタイミング図であ
る。時刻t6,t7,t8でのパルスタイミングは第7図の従来
のパルスタイミング図のt1,t2,t3と同じであるが、t9,t
10,t11のパルスタイミングで、一度、混合した電荷を2
つの転送電極の下に分割して蓄積することとなる。
Embodiments Hereinafter, embodiments of the present invention will be described with reference to the drawings. FIG. 1 is a pulse timing chart applied to a transfer electrode during a vertical blanking period in an embodiment of the present invention. Time t 6, the pulse timing at t 7, t 8 is the same as t 1, t 2, t 3 of a conventional pulse timing diagram of Figure 7, t 9, t
At the pulse timing of 10 , t 11 ,
It is divided and accumulated under one transfer electrode.

第2図は第1図の各時間における転送電極下の断面ポ
テンシャル図である。t6,t7,t8までのポテンシャル図は
第8図のポテンシャル図のt1,t2,t3のポテンシャル図と
同じてある。t9,t10により、t8の時刻に、転送電極5,6,
7の下に蓄積されていた電荷22が、転送電極6,7,8の下へ
転送される。この後、t11の時刻には、スミアの増加を
防ぐため転送電極7がLowレベルの電位となり、この時
蓄積されていたひとつの信号となる電荷を2つの転送電
極6,8へと分割して蓄積できることとなる。
FIG. 2 is a sectional potential diagram under the transfer electrode at each time of FIG. The potential diagrams up to t 6 , t 7 and t 8 are the same as the potential diagrams at t 1 , t 2 and t 3 in the potential diagram of FIG. According to t 9 and t 10 , at the time of t 8 , the transfer electrodes 5, 6,
The electric charge 22 accumulated under 7 is transferred to below the transfer electrodes 6, 7, 8. Thereafter, the time t 11, the transfer electrode 7 to prevent the increase of the smear becomes the Low level potential, divides the charge as a single signal that has been the case accumulated into two transfer electrodes 6 and 8 Can be accumulated.

発明の効果 以上のように、本発明は、ひとつの信号として出力さ
れる電荷を転送中に一度、読み出し転送を行う転送電極
をLowレベルの電位にし、転送を行う2つの転送電極の
下へ分割して蓄積できる転送電極のタイミングとなって
おり、スミアの増加を防止し垂直転送部の転送できる電
荷の容量を増加でき、その実用的効果は大なるものがあ
る。
Effect of the Invention As described above, according to the present invention, once a charge output as one signal is transferred, the transfer electrode performing the read transfer is set to the low-level potential, and divided below the two transfer electrodes performing the transfer. This is the timing of the transfer electrodes that can be accumulated and stored, so that an increase in smear can be prevented and the capacity of the charges that can be transferred by the vertical transfer unit can be increased, and the practical effect is large.

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

第1図は本発明の実施例における垂直ブランキング期間
の転送電極に加わるパルスタイミング図、第2図は第1
図の各時間における転送電極下の断面ポテンシャル図、
第3図はIT−CCDの全体構成図、第4図は第3図の破線
部Aの拡大図、第5図は第4図のB−C間の断面図、第
6図は固体撮像装置の駆動タイミング図、第7図は第6
図の垂直ブランキング期間に転送電極に加わるパルスタ
イミング図、第8図は第7図の各時間における第4図,D
−E間の断面ポテンシャル図である。 1……光電変換素子、2……垂直転送CCD(VCCD)、3
……水平転送CCD(HCCD)、4……出力アンプ部、5…
…φパルスの加わる転送電極、6……φパルスの加
わる転送電極、7……φパルスの加わる転送電極、8
……φパルスの加わる転送電極、9……分離領域、10
……基板のn形層、11……光電変換素子のn形層、12…
…VCCDのn形層、13……分離のP形層、14……VCCDの空
乏層、15……発生電荷、16……遮光膜、17……光、18…
…垂直ブランキング期間、19……有効走査期間、20……
読み出しパルス、21……転送パルス振幅、22……電荷。
FIG. 1 is a pulse timing chart applied to a transfer electrode during a vertical blanking period in an embodiment of the present invention, and FIG.
Sectional potential diagram under the transfer electrode at each time in the figure,
3 is an overall configuration diagram of the IT-CCD, FIG. 4 is an enlarged view of a broken line portion A in FIG. 3, FIG. 5 is a cross-sectional view between B and C in FIG. 4, and FIG. FIG. 7 is a drive timing chart of FIG.
FIG. 8 is a timing chart of the pulse applied to the transfer electrode during the vertical blanking period shown in FIG.
It is sectional electric potential diagram between -E. 1 ... photoelectric conversion element, 2 ... vertical transfer CCD (VCCD), 3
…… horizontal transfer CCD (HCCD), 4 …… Output amplifier section, 5…
... Transfer electrode to which φ 1 pulse is applied, 6... Transfer electrode to which φ 2 pulse is applied, 7... Transfer electrode to which φ 3 pulse is applied, 8
...... phi 4 pulses applied transfer electrodes 9 ...... isolation region 10
... n-type layer of substrate, 11 ... n-type layer of photoelectric conversion element, 12 ...
... n-type layer of VCCD, 13 ... p-type layer of isolation, 14 ... depletion layer of VCCD, 15 ... generated charge, 16 ... light shielding film, 17 ... light, 18 ...
... vertical blanking period, 19 ... effective scanning period, 20 ...
Read pulse, 21: transfer pulse amplitude, 22: electric charge.

Claims (2)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】行列状に配列された複数個の光電変換素子
と前記光電変換素子に蓄積された信号電荷を読み出し、
転送する複数の転送電極を持つ転送部を備えた固体撮像
装置の駆動方法において、隣り合う前記光電変換素子に
蓄積されたそれぞれの信号電荷を前記転送電極により読
み出した後に前記転送電極の下で混合して混合電荷を作
り、ついで前記混合電荷を、前記信号電荷の読み出しに
用いた転送電極以外の複数の転送電極の下に分割して蓄
積する期間を有することを特徴とする固体撮像装置の駆
動方法。
A plurality of photoelectric conversion elements arranged in a matrix and signal charges stored in the photoelectric conversion elements are read;
In the method for driving a solid-state imaging device including a transfer unit having a plurality of transfer electrodes for transferring, each signal charge stored in an adjacent photoelectric conversion element is read out by the transfer electrode and then mixed under the transfer electrode. A period in which the mixed charge is divided and accumulated under a plurality of transfer electrodes other than the transfer electrode used for reading out the signal charge. Method.
【請求項2】列方向に隣接する第1、第2の光電変換素
子が二次元状に配列された光電変換部と、前記光電変換
部に蓄積された信号電荷を垂直方向に転送する複数の転
送電極を持つ垂直転送部とを備え、前記複数の転送電極
のうち、前記第1の光電変換素子に対応させて第1の転
送電極と第2の転送電極を配置し、前記第2の光電変換
素子に対応させて第3の転送電極と第4の転送電極を配
置し、かつ第3の転送電極を前記第2の転送電極に隣接
するように配置し、前記第1、第3の転送電極はそれぞ
れ前記第1、第2の光電変換素子から信号電荷を読み出
し転送を行い、前記第2、第4の転送電極は信号電荷の
転送を行う固体撮像装置の駆動方法において、前記第
1、第2の光電変換素子からそれぞれ前記第1、第3の
転送電極の下へそれぞれ第1、第2の信号電荷を読み出
し、ついで前記第1、第2、第3の転送電極下で前記第
1、第2の信号電荷を混合して混合電荷を作り、ついで
前記混合電荷を前記第2、第3、第4の転送電極下に転
送後、前記混合電荷を前記第2、第4の転送電極下へ分
割して蓄積する期間を有することを特徴とする固体撮像
装置の駆動方法。
2. A photoelectric conversion unit in which first and second photoelectric conversion elements adjacent to each other in a column direction are arranged two-dimensionally, and a plurality of signal transfer units for vertically transferring signal charges accumulated in the photoelectric conversion unit. A vertical transfer unit having a transfer electrode, wherein a first transfer electrode and a second transfer electrode are arranged among the plurality of transfer electrodes in correspondence with the first photoelectric conversion element; A third transfer electrode and a fourth transfer electrode arranged corresponding to the conversion element, and a third transfer electrode arranged so as to be adjacent to the second transfer electrode; An electrode for reading and transferring a signal charge from each of the first and second photoelectric conversion elements; and a second and fourth transfer electrode for driving the solid-state imaging device that transfers the signal charge. From the second photoelectric conversion element to below the first and third transfer electrodes respectively Reading the first and second signal charges, and then mixing the first and second signal charges under the first, second and third transfer electrodes to form a mixed charge; Driving the solid-state imaging device having a period in which the mixed charge is divided and stored under the second and fourth transfer electrodes after being transferred under the second, third, and fourth transfer electrodes. Method.
JP1151918A 1989-06-14 1989-06-14 Driving method of solid-state imaging device Expired - Fee Related JP2624334B2 (en)

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JP1151918A JP2624334B2 (en) 1989-06-14 1989-06-14 Driving method of solid-state imaging device

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Application Number Priority Date Filing Date Title
JP1151918A JP2624334B2 (en) 1989-06-14 1989-06-14 Driving method of solid-state imaging device

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JPH0316480A JPH0316480A (en) 1991-01-24
JP2624334B2 true JP2624334B2 (en) 1997-06-25

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS604380A (en) * 1983-06-22 1985-01-10 Matsushita Electric Ind Co Ltd Solid-state image pickup device

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