JPS5928067B2 - charge coupled device - Google Patents
charge coupled deviceInfo
- Publication number
- JPS5928067B2 JPS5928067B2 JP55126793A JP12679380A JPS5928067B2 JP S5928067 B2 JPS5928067 B2 JP S5928067B2 JP 55126793 A JP55126793 A JP 55126793A JP 12679380 A JP12679380 A JP 12679380A JP S5928067 B2 JPS5928067 B2 JP S5928067B2
- Authority
- JP
- Japan
- Prior art keywords
- gate electrode
- charge
- electrodes
- input section
- gate
- 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
Links
Classifications
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10F—INORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
- H10F39/00—Integrated devices, or assemblies of multiple devices, comprising at least one element covered by group H10F30/00, e.g. radiation detectors comprising photodiode arrays
- H10F39/10—Integrated devices
- H10F39/12—Image sensors
- H10F39/15—Charge-coupled device [CCD] image sensors
- H10F39/153—Two-dimensional or three-dimensional array CCD image sensors
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- Light Receiving Elements (AREA)
- Solid State Image Pick-Up Elements (AREA)
Description
【発明の詳細な説明】
本発明は電荷結合装置とくに電極構造を簡易化した電荷
結合装置に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a charge coupled device, and particularly to a charge coupled device with a simplified electrode structure.
光電変換素子と電荷転送素子(以下CTDと略記する)
とを同一の半導体基板に集積した撮像素子が近年提案さ
れた。Photoelectric conversion device and charge transfer device (hereinafter abbreviated as CTD)
Recently, an image sensor has been proposed in which both are integrated on the same semiconductor substrate.
このような撮像素子は通常光電変換素子の一行につき1
系統もしくは2系統のCTDが付属しているとともに、
光電変換素子群とCTDとの間に少なくとも1個のゲー
ト電極が存在している。とくに撮像対象物からの入射光
が微弱な場合、すなわち暗い撮像対象物を撮像する場合
に用いる撮像装置においては光電変換素子群とCTDと
の間に入力ゲート電極、蓄積ゲート電極、移転(Tra
nsfer)ゲート電極の3種の電極が存在し、これら
のゲート電極はたがいに異なる電位をとらなければなら
ないし、またCTDの転送電極とも電気的に独立してい
なければならない。このため電圧印加用母線の数が多く
なるが、さらに各光電変換素子の各行につき1系統ずつ
付属するゲート電極および転送電極の相互接続のための
配線が必要となるため配線層のパターンが大幅に複雑化
し、多くの場合上記相互接続用配線が電極と立体交叉す
るようになる。こうなると製作工程が大幅に繁雑化する
にとどまらず、パルスを伝送する配線が電極と立体交叉
すれば該電極にパルスが誘導されて、装置の動作に悪影
響を及ぼすという問題点がある。とくに入力ゲート電極
は充分に安定した電位に保たれていなければならないた
め、上述のようなパルス誘導は極力防止しなければなら
ない。Such an image sensor usually has one photoelectric conversion element per row.
Comes with one system or two systems of CTD, and
At least one gate electrode exists between the photoelectric conversion element group and the CTD. In particular, in an imaging device used when the incident light from the imaging target is weak, that is, when imaging a dark imaging target, there are input gate electrodes, storage gate electrodes, and transfer (transfer) electrodes between the photoelectric conversion element group and the CTD.
There are three types of gate electrodes, and these gate electrodes must have different potentials and must be electrically independent from the transfer electrode of the CTD. This increases the number of busbars for voltage application, but also requires wiring for interconnecting the gate electrodes and transfer electrodes, which are attached to each row of each photoelectric conversion element, resulting in a significant increase in the pattern of the wiring layer. This increases the complexity, and in many cases, the interconnection wires intersect with the electrodes in three dimensions. This not only greatly complicates the manufacturing process, but also poses a problem in that if the wiring that transmits the pulses intersects with the electrodes, the pulses will be induced into the electrodes, which will adversely affect the operation of the device. In particular, since the input gate electrode must be kept at a sufficiently stable potential, the above-mentioned pulse induction must be prevented as much as possible.
そこで入力ゲート電極と配線との交叉を無くしようとす
ると配線層パターンに無理が生じ、また交叉させてもそ
の影響を極力少なくしようとして入力ゲート電極の形状
をあまりに細密化すると該電極の伝達コンダクタンスが
低下して見掛け上量子効率が低下したかのごとくなると
いうような問題を生ずる。本発明は前述の問題を解決し
たもので、転送電極の少なくとも一部とその前段のゲー
ト電極とを常に同電位に保ちながら電荷堰の形状および
電極下の基板表層の電位制御によつて正常な読み出し動
作を行うことを可能とした新規な電荷結合装置を提供せ
んとするものである。Therefore, if we try to eliminate the crossover between the input gate electrode and the wiring, the wiring layer pattern becomes unreasonable, and if we make the shape of the input gate electrode too fine in an attempt to minimize the influence of crossover, the transfer conductance of the electrode will decrease. A problem arises in that the quantum efficiency decreases and the quantum efficiency appears to decrease. The present invention solves the above-mentioned problem by controlling the shape of the charge weir and the potential of the substrate surface layer under the electrode while always keeping at least a part of the transfer electrode and the gate electrode in the preceding stage at the same potential. It is an object of the present invention to provide a novel charge-coupled device capable of performing read operations.
以下図面を用いて本発明の一実施例について詳細に説明
する。An embodiment of the present invention will be described in detail below with reference to the drawings.
第1図は本発明の一実施例における不純物ドープ層の平
面的パターンを示したもので、便宜上基板はp型シリコ
ンであるとする。FIG. 1 shows a planar pattern of an impurity doped layer in one embodiment of the present invention, and for convenience it is assumed that the substrate is p-type silicon.
理解し易くするため本図において不純物ドープがなされ
た部位に斜線を施し、後述する電極等は除去した状態を
示した。なお第1図においては装置の一部だけを示して
いるが、図からも明らかなようにパターンはすべてX,
y両方向に周期性を有しているから、任意の面積に亘つ
て同一パターンを周期的に配列することができ、単位パ
ターンの数に格別の制限はない。第1図において小さい
正方形領域1,2,3,・・・・・・9は基板と逆の導
電型(すなわちn型)の島状領域で、信号電荷を発生す
る部分である。In order to make it easier to understand, in this figure, regions doped with impurities are shaded, and electrodes and the like, which will be described later, are shown removed. Although only a part of the device is shown in Figure 1, as is clear from the figure, all the patterns are X,
Since it has periodicity in both the y directions, the same pattern can be arranged periodically over any area, and there is no particular restriction on the number of unit patterns. In FIG. 1, small square regions 1, 2, 3, . . . 9 are island-like regions of the opposite conductivity type (ie, n-type) to the substrate, and are portions that generate signal charges.
ゆえに従来の電荷結合装置と同様に上記逆導電型領域1
〜9をソース領域と呼ぶ。上記各ソース領域以外の不純
物ドープ領域はすべて基板と同一導電型であつて、ドナ
ーイオンをイオン注入法でドープすることにより形成さ
れたものである。Therefore, as in the conventional charge-coupled device, the above-mentioned opposite conductivity type region 1
9 is called the source region. All the impurity-doped regions other than the source regions are of the same conductivity type as the substrate and are formed by doping with donor ions by ion implantation.
また細幅の部分11,12,13はチヤンネルストツプ
(ChannelstOp)であつて、以下電荷堰と言
う。各電荷堰は文字“h゛を縦方向に連結したものに類
似した形状を有している。そしてその垂直部分から逆L
字状に延びる鉤型電荷堰の中にソース領域1〜9が位置
していて入力部が区画されていることは図を一見すれば
明らかである。上記中間領域内にある不純物ドーブ層2
1,22,23,・・・・・・26は電荷堰および基板
に比べて低い不純物濃度を有する領域で、以下一時蓄積
領域と呼.80また電荷堰11と12との間、および電
荷堰12と13との間にある不純物ドープ層31,32
,33,・・・・・・38は電荷転送の方向を決めるた
めに設けられたものであるから以下案内層と呼メち後述
するように各列において電荷は上記案内層を番号順にた
どるように転送される。これら各案内層31〜38もま
た電荷堰11〜13に比し低不純物濃度である。つぎに
第2図に本実施例による電荷転送装置の電極形状を含め
た平面構成を示す。この第2図において前述の不純物ド
ープ領域は斜線を付して示されている。第2図から一層
明らかなように、垂直方向の帯状電荷堰11,12,1
3の間に列チヤンネルが定められ、各列チヤンネルの中
には、前述のソース領域1,2・・・9を逆L字状に囲
む鉤型電荷堰11a,12a,13aによつて入力部1
1b,12b,13bが区画されている。Further, the narrow portions 11, 12, and 13 are channel stops (ChannelstOps), and are hereinafter referred to as charge weirs. Each charge weir has a shape similar to the letter "h" connected vertically, and from its vertical portion to an inverted L.
It is clear from a glance at the figure that the source regions 1 to 9 are located in the hook-shaped charge weir extending in the shape of a letter and that the input section is partitioned. Impurity doped layer 2 in the intermediate region
1, 22, 23, . . . 26 are regions having a lower impurity concentration than the charge weir and the substrate, and are hereinafter referred to as temporary storage regions. 80 and impurity doped layers 31 and 32 between charge weirs 11 and 12 and between charge weirs 12 and 13.
, 33, . . . , 38 are provided to determine the direction of charge transfer, so they are hereinafter referred to as guide layers, and as will be described later, the charges in each column follow the guide layers in numerical order. will be forwarded to. Each of these guide layers 31-38 also has a lower impurity concentration than the charge weirs 11-13. Next, FIG. 2 shows a planar configuration including the electrode shape of the charge transfer device according to this embodiment. In FIG. 2, the aforementioned impurity-doped regions are shown with diagonal lines. As is clearer from FIG.
A column channel is defined between 3 and 3, and each column channel is provided with an input section by hook-shaped charge weirs 11a, 12a, 13a surrounding the source regions 1, 2, . . . 9 in an inverted L shape. 1
1b, 12b, and 13b are divided.
従つて各列チヤンネル中これら入力部を除く領域が垂直
転送部となる。一方本実施例において基板上に設けられ
る電極はすべて基板と絶縁され、水平方向に細長い帯状
をなしている。Therefore, the area excluding these input sections in each column channel becomes a vertical transfer section. On the other hand, in this embodiment, all the electrodes provided on the substrate are insulated from the substrate and have a horizontally elongated strip shape.
すなわち各行の鉤型電荷堰の下部開放端に隣接して入力
部と転送部を連通するよう水平方向に延びる第1のゲー
ト電極101が設けられ、さらに各行の第1ゲート電極
間には同じく水平方向に延びる第2〜第5のゲート電極
が順次配設されている。各ゲート電極は入力部と転送部
を共通にカバーし、転送部においては第2および第4ゲ
ート電極102,104の下に前述の不純物ドープ領域
が対応し、かつ各電極幅は略等しく設定されている。ま
た入力部においては、第3ゲート電極103aの下に不
純物ドープ領域が対応するようその電極幅が広げられ、
その分第2ゲート電極102aの幅がせばめられている
。第4ゲート電極104aは入力部のソース領域と第3
ゲート電極との間に延びており、第5ゲート電極105
aはソース領域を避けるパターンで水平方向に配列され
ている。便宜上、入力部に対応した電極部分には副号a
を添えて示す。各行5本ずつのゲート電極は、同順位の
もの同志共通に接続してそれぞれ端子Zl,(/T,S
G,G,Z2に導出されている。さて以上の構成におい
て、第3および第4ゲート電極103,104には端子
SG,IGを通して常時所定の直流電圧を印加し、入力
部においては第4ゲート電極104a下よりも不純物を
ドープした第3ゲート電極103a下に深い井戸ができ
、転送部においては第3ゲート電極下よりも不純物をド
ープした第4ゲート電極下に深い井戸ができるようにし
てある。よつて各ソース領域4等で発生した電荷は入力
部の第4ゲート電極104a下の井戸を介して第3ゲー
ト電極103a下の井戸に一時蓄積されることになる。
所定の蓄積時間終了後上記第3ゲート電極下の井戸に溜
まつた電荷を各列チヤンネル転送部に移すのであるが、
これには第2ゲート電極102に端子Ztから電圧を印
加してその下に深い井戸が生ずるょうにし、っいで第1
ゲート電極1旧にも端子Z1から電圧を印加すれば、信
号電荷は入力部における第2ゲート電極102a下を通
つて第1ゲート電極101下の井戸内に移転する。That is, a first gate electrode 101 is provided adjacent to the lower open end of the hook-shaped charge weir in each row and extends in the horizontal direction so as to communicate the input section and the transfer section. Second to fifth gate electrodes extending in the direction are sequentially arranged. Each gate electrode commonly covers the input section and the transfer section, and in the transfer section, the above-mentioned impurity doped regions correspond under the second and fourth gate electrodes 102 and 104, and each electrode width is set approximately equal. ing. Further, in the input section, the electrode width is widened so that the impurity doped region corresponds to the bottom of the third gate electrode 103a,
The width of the second gate electrode 102a is narrowed accordingly. The fourth gate electrode 104a is connected to the source region of the input section and the third gate electrode 104a.
The fifth gate electrode 105 extends between the gate electrode and the fifth gate electrode 105.
A is arranged in the horizontal direction in a pattern that avoids the source region. For convenience, the electrode part corresponding to the input part is marked with the subtitle a.
Shown with. Five gate electrodes in each row are commonly connected to those of the same rank and connected to terminals Zl, (/T, S, respectively).
G, G, Z2 are derived. Now, in the above configuration, a predetermined DC voltage is always applied to the third and fourth gate electrodes 103 and 104 through the terminals SG and IG, and the third A deep well is formed under the gate electrode 103a, and in the transfer section, a deeper well is formed under the fourth gate electrode doped with impurities than under the third gate electrode. Therefore, charges generated in each source region 4 etc. are temporarily accumulated in the well under the third gate electrode 103a via the well under the fourth gate electrode 104a of the input section.
After a predetermined accumulation time, the charge accumulated in the well under the third gate electrode is transferred to each column channel transfer section.
To do this, a voltage is applied from the terminal Zt to the second gate electrode 102 to form a deep well below it, and then the first
If a voltage is also applied to the gate electrode 1 from the terminal Z1, the signal charge passes under the second gate electrode 102a at the input portion and is transferred into the well under the first gate electrode 101.
すなわち電極102は移転ゲート電極に相当する。しか
るに移転ゲート電極102の、転送部の下の基板表面に
はドナーイオン注入による不純物ドープ領域があるため
この箇所に生ずる井戸はきわめて深い。ゆえに第1ゲー
ト電極101下に一旦移つた電荷はただちに上記不純物
ドープ領域に対応した移転部の第2ゲート電極下の井戸
に流入し、ここに蓄積される。こうなれば移転ゲート電
極としての第2ゲート電極102の井戸は不要であるか
らその電圧を零に戻せば、電荷は第3ゲート電極103
下の井戸に移り、次いで不純物ドープ領域に対応した第
4ゲート電極104下のより深い井戸に自動的に移る。That is, the electrode 102 corresponds to a transfer gate electrode. However, since there is an impurity doped region by donor ion implantation on the substrate surface below the transfer portion of the transfer gate electrode 102, the well formed at this location is extremely deep. Therefore, the charge once transferred under the first gate electrode 101 immediately flows into the well under the second gate electrode in the transfer portion corresponding to the impurity doped region and is accumulated there. In this case, the well of the second gate electrode 102 as a transfer gate electrode is unnecessary, so if the voltage is returned to zero, the charge is transferred to the third gate electrode 103.
The process automatically moves to the lower well and then to the deeper well below the fourth gate electrode 104 corresponding to the impurity doped region.
次に第5ゲート電極105に電圧を印加して、該電極下
に電荷を移す。このようにして電荷は上記電荷堰の間を
電極番号順に、すなわち図の矢印イの方向に転送されて
行く。ここまでの説明から理解されるように、第2図の
各電極は一時蓄積、移転等の役割と、従来これらの役割
を有する電極と分離されていたCTDの転送電極の役割
とを兼ねている。Next, a voltage is applied to the fifth gate electrode 105 to transfer charge under the fifth gate electrode. In this way, charges are transferred between the charge weirs in the order of electrode numbers, that is, in the direction of arrow A in the figure. As can be understood from the explanation up to this point, each electrode in Figure 2 has the roles of temporary storage, transfer, etc., as well as the role of the CTD transfer electrode, which was conventionally separated from the electrodes that had these roles. .
しかも従来光電変換素子の一列または一行ごとに少なく
とも1系統が必要であつたCTDも、すべて本実施例に
おいては区分されていない。換言すれば各電極は各CT
Dの転送電極と、異なる系統のCTDの電極どうしを結
ぶ接続線とを兼ねている。以上の動作と、電極の機能は
すべての電極について電極101〜105と同様である
。Furthermore, all CTDs, which conventionally required at least one system for each column or row of photoelectric conversion elements, are not classified in this embodiment. In other words, each electrode corresponds to each CT
It also serves as the transfer electrode of D and a connection line that connects the electrodes of CTDs of different systems. The above operations and functions of the electrodes are the same for all electrodes as for electrodes 101 to 105.
よつて第2図の実施例が従来の2次元光電変換装置と本
質的に同等の動作をなすことがわかる。しかも電極およ
び配線の形状および構造はきわめて簡単である。すなわ
ち電極どうしの接続線が不要なため電極と接続線との交
叉が実質上皆無となり、さらに入力ゲート電極、一時蓄
積電極、移転ゲート電極等が転送電極と一体化され、結
局全部の電極が、部分的に幅狭い箇所と幅広い箇所とが
あることを別にすれば全体としてほぼ帯状のものだけで
構成され、きわめて簡易な構造となつている。なお以上
は埋込みチヤンネルの場合につき説明したが、表面チヤ
ンネルにも本発明の適用は容易である。Therefore, it can be seen that the embodiment shown in FIG. 2 operates essentially the same as the conventional two-dimensional photoelectric conversion device. Furthermore, the shapes and structures of the electrodes and wiring are extremely simple. In other words, since there is no need for connection lines between electrodes, there is virtually no crossover between electrodes and connection lines, and furthermore, the input gate electrode, temporary storage electrode, transfer gate electrode, etc. are integrated with the transfer electrode, and in the end, all the electrodes are Apart from the fact that there are some narrow and wide sections, the structure as a whole is made up almost entirely of band-shaped parts, making it an extremely simple structure. Although the above description has been made regarding the case of a buried channel, the present invention can easily be applied to a surface channel as well.
また井戸の深さを調整するには、周知のごとく電極下の
絶縁被膜の厚さの調整によつてもよい。本発明の電荷結
合装置は上述した構造の簡易さに加えて、雑音誘導によ
つて悪影響を受ける入力部の電極に接続線の交叉がない
ため、安定した低雑音動作が可能であり、その他構造の
簡易さに基づく生産コスト低減、歩留まり向上等の多種
の利点を有するもので、撮像装置、信号処理装置等に適
用してきわめて有利である。Further, the depth of the well may be adjusted by adjusting the thickness of the insulating film under the electrode, as is well known. In addition to the simple structure described above, the charge-coupled device of the present invention is capable of stable, low-noise operation because there is no crossing of connection wires at the electrodes of the input section, which are adversely affected by noise induction. It has various advantages such as reduced production cost and improved yield based on the simplicity of the process, and is extremely advantageous when applied to imaging devices, signal processing devices, etc.
第1図は本発明の一実施例における電荷堰および不純物
ドープ領域のパターンを示す平面図、第2図は上記実施
例における電極の形状を示す平面図である。
1〜9:ソース領域、11〜13:電荷堰、21〜26
:ー時蓄積領域、31〜38:案内層。FIG. 1 is a plan view showing a pattern of a charge weir and an impurity doped region in one embodiment of the present invention, and FIG. 2 is a plan view showing the shape of an electrode in the above embodiment. 1-9: Source region, 11-13: Charge weir, 21-26
:-Time accumulation area, 31-38: Guide layer.
Claims (1)
し、該ソース領域の各行間に垂直方向に延びる帯状電荷
堰を設けて複数の列チャンネルを定め、各列チャンネル
中には一方の帯状電荷堰から水平に延びて上記各ソース
領域を逆L字状に囲む鉤型電荷堰を形成して下端の開放
した入力部を区画し、各行の入力部の開放端部に隣接し
て各列ごとの入力部と列チャンネルとを連通する第1の
帯状ゲート電極を水平方向に配設し、該第1ゲート電極
と各行のソース領域との間には同じく各列の入力部と列
チャンネルを共通にカバーして水平方向に延びる第2、
第3および第4の帯状ゲート電極を順次隣接配置すると
ともに、該第4のゲート電極と隣接した行の第1ゲート
電極との間には上記ソース領域を避けたパターンで第5
の帯状ゲート電極を水平方向に配設し、さらに上記第2
、第3および第4のゲート電極下に形成される電位の井
戸が、入力部においては第2、第4、第3ゲート電極の
順に深くなり、チャンネル部においては第2、第3、第
4ゲート電極の順に深くなるよう表面電位を設定し、ソ
ース領域から入力部の第4ゲート電極下を経て第3ゲー
ト電極下に蓄積された信号電荷を、第2ゲート電極の制
御により、チャンネル部に連通した第1ゲート電極下の
井戸と当該チャンネル部における第2、第3ゲート電極
下の井戸を介して第4ゲート電極下の井戸まで自動的に
転送するようにしたことを特徴とする電荷結合装置。1 A plurality of source regions are arranged in a matrix on the surface of a semiconductor substrate, and a plurality of column channels are defined by providing a strip-shaped charge weir extending vertically between each row of the source regions, and one strip-shaped charge is provided in each column channel. A hook-shaped charge weir is formed that extends horizontally from the weir and surrounds each of the source regions in an inverted L shape to define an input section with an open bottom end. A first band-shaped gate electrode communicating between the input section and the column channel is disposed horizontally, and between the first gate electrode and the source region of each row, the input section of each column and the column channel are also shared. a second extending horizontally covering the
The third and fourth strip-shaped gate electrodes are successively arranged adjacent to each other, and a fifth gate electrode is formed between the fourth gate electrode and the first gate electrode of the adjacent row in a pattern that avoids the source region.
A strip gate electrode is arranged horizontally, and the second strip gate electrode is arranged horizontally.
, the potential wells formed under the third and fourth gate electrodes become deeper in the order of the second, fourth, and third gate electrodes in the input section, and become deeper in the order of the second, third, and fourth gate electrodes in the channel section. The surface potential is set so that it becomes deeper in the order of the gate electrode, and the signal charge accumulated from the source region, under the fourth gate electrode of the input section, and under the third gate electrode is transferred to the channel section by controlling the second gate electrode. A charge coupling characterized in that the charge is automatically transferred to the well under the fourth gate electrode via the well under the first gate electrode and the well under the second and third gate electrodes in the channel portion, which are connected to each other. Device.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP55126793A JPS5928067B2 (en) | 1980-09-11 | 1980-09-11 | charge coupled device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP55126793A JPS5928067B2 (en) | 1980-09-11 | 1980-09-11 | charge coupled device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5750470A JPS5750470A (en) | 1982-03-24 |
| JPS5928067B2 true JPS5928067B2 (en) | 1984-07-10 |
Family
ID=14944079
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP55126793A Expired JPS5928067B2 (en) | 1980-09-11 | 1980-09-11 | charge coupled device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5928067B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0488968A (en) * | 1990-07-31 | 1992-03-23 | Tatsuo Tokuno | Tsukudani (kind of preserved food cooked in soy source) |
-
1980
- 1980-09-11 JP JP55126793A patent/JPS5928067B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5750470A (en) | 1982-03-24 |
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