JPH0864883A - Piezoelectric ceramic transformer - Google Patents

Piezoelectric ceramic transformer

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Publication number
JPH0864883A
JPH0864883A JP6199756A JP19975694A JPH0864883A JP H0864883 A JPH0864883 A JP H0864883A JP 6199756 A JP6199756 A JP 6199756A JP 19975694 A JP19975694 A JP 19975694A JP H0864883 A JPH0864883 A JP H0864883A
Authority
JP
Japan
Prior art keywords
piezoelectric ceramic
ceramic transformer
polarized
output
input
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.)
Pending
Application number
JP6199756A
Other languages
Japanese (ja)
Inventor
Junichi Toyoda
準一 豊田
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.)
Sony Corp
Original Assignee
Sony Corp
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 Sony Corp filed Critical Sony Corp
Priority to JP6199756A priority Critical patent/JPH0864883A/en
Publication of JPH0864883A publication Critical patent/JPH0864883A/en
Pending legal-status Critical Current

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Abstract

PURPOSE: To obtain a piezoelectric ceramic transformer having a large step-up ratio without increasing the L/T of the length L and the thickness T of a piezoelectric element ceramic assembly. CONSTITUTION: The input electrodes 2 and 3 side of the primary side of a piezoelectric ceramic element assembly 1 of a flat rectangular parallelepiped shape are polarized in a thickness T direction, output electrodes 8A and 8B of secondary side are divided into a plurality, and polarized in the length L direction of the reverse direction thereto.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明はセラミック(磁器)を用
いたコイル不用の圧電セラミックトランスに係わり、特
に圧電セラミック素体の2次側の出力電極を2分割した
圧電セラミックトランスに関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a piezoelectric ceramic transformer using a ceramic (porcelain) that does not require a coil, and more particularly to a piezoelectric ceramic transformer in which an output electrode on the secondary side of a piezoelectric ceramic body is divided into two parts.

【0002】[0002]

【従来の技術】従来から圧電セラミックトランスは高圧
電源を得る方法として広く利用されている。この圧電セ
ラミックトランスは図3に示す様に、長さ2Lmm、幅
Wmm、厚さTmmの偏平な直方体状の圧電セラミック
素体1の上下面(2L×W面)の長さ2L方向の略2L
/2=L位置まで1次側の入力電極2及び3を形成し、
同じく右側面(W×T面)に出力電極6を形成し、入力
側は厚さT方向にP1 の様に分極し、出力側は長さL方
向にP2 の様に分極させる。これら、各電極2及び3並
びに6は夫々入出力端子4及び5並びに7に接続され、
入力端子4及び5間に入力電圧を供給することで出力端
子7及び5間に出力電圧が得られる様に成されている。
2. Description of the Related Art Conventionally, piezoelectric ceramic transformers have been widely used as a method for obtaining a high voltage power supply. As shown in FIG. 3, the piezoelectric ceramic transformer has a length of 2 Lmm, a width of Wmm, and a thickness of Tmm.
/ 2 = form the primary side input electrodes 2 and 3 up to the L position,
Similarly, the output electrode 6 is formed on the right side surface (W × T surface), the input side is polarized in the thickness T direction as P 1 , and the output side is polarized in the length L direction as P 2 . These electrodes 2 and 3 and 6 are connected to input / output terminals 4 and 5 and 7, respectively,
The output voltage is obtained between the output terminals 7 and 5 by supplying the input voltage between the input terminals 4 and 5.

【0003】上述の構成で入力電圧が供給される入力側
を低インピーダンスと成し、出力電圧が得られる出力側
を高インピーダンスにすれば、共振時にはインピーダン
ス比の平方根に等しい変圧比が得られる。
When the input side to which the input voltage is supplied has a low impedance and the output side from which the output voltage is obtained has a high impedance in the above configuration, a transformation ratio equal to the square root of the impedance ratio can be obtained at the time of resonance.

【0004】即ち、変圧比(Vout /Vin)は次の
(1)式の様に表される。 Vout /Vin∝k31・k33・Qm ・L/T ‥‥ (1) ここで、K31:横効果の結合係数、k33:縦効果の結合
係数、Qm :機械品質係数、L及びTは圧電セラミック
素体1の長さ及び厚さである。
That is, the transformation ratio (Vout / Vin) is expressed by the following equation (1). Vout / Vin ∝k 31 · k 33 · Q m · L / T (1) where K 31 : lateral effect coupling coefficient, k 33 : longitudinal effect coupling coefficient, Q m : machine quality coefficient, L And T are the length and thickness of the piezoelectric ceramic body 1.

【0005】[0005]

【発明が解決しようとする課題】上述の従来構成で説明
した圧電セラミックトランスは上述の(1)式から解る
様に変圧比を大きく(或は入力電圧を低減)するにはk
31,k33,Qm 等の各係数が一定であるためL/Tを大
きくすればよい。然し、L/Tを大きくするためにはL
を大きくするかTを小さくすることになり、Lを大きく
すれば当然圧電セラミックトランスが大型化する、又、
Tを小さくすれば当然薄くなり、機械的強度出力で問題
があった。
In the piezoelectric ceramic transformer described in the above-mentioned conventional configuration, k can be obtained by increasing the transformation ratio (or reducing the input voltage) as can be seen from the above equation (1).
Since the coefficients of 31 , k 33 , Q m, etc. are constant, L / T should be increased. However, to increase L / T, L
Is increased or T is decreased, and if L is increased, the piezoelectric ceramic transformer is naturally increased in size.
If T is made smaller, it naturally becomes thinner, and there is a problem in mechanical strength output.

【0006】本発明は叙上の問題点を解消するために成
されたもので、その目的とするところは従来構成と同一
形状でもより高い変圧比(昇圧比)が得られる圧電セラ
ミックトランスを得ようとするものである。
The present invention has been made in order to solve the above problems, and an object thereof is to obtain a piezoelectric ceramic transformer which can obtain a higher transformation ratio (step-up ratio) with the same shape as the conventional configuration. It is something to try.

【0007】[0007]

【課題を解決するための手段】本発明の圧電セラミック
トランスはその例が図1に示されている様に偏平な直方
体状の圧電セラミック素体1の上下主面に対向して1次
側の入力電極2及び3が形成され、該入力電極2及び3
が形成された側の側面と反対の側面に2次側の出力電極
が形成された圧電セラミックトランスに於いて、上記上
下主面1a及び1bに対向形成した1次側入力電極2及
び3の厚み方向Tに分極P1 すると共に上記反対の側面
1dに形成した2次側の出力電極8A及び8Bを複数分
割し、上記直方体の圧電セラミック素体1の長手方向L
に互に逆方向に分極P2 及びP3して成るものである。
As shown in FIG. 1, the piezoelectric ceramic transformer of the present invention has a primary side facing the upper and lower main surfaces of a flat rectangular parallelepiped piezoelectric ceramic body 1. Input electrodes 2 and 3 are formed, and the input electrodes 2 and 3 are formed.
In the piezoelectric ceramic transformer in which the secondary side output electrode is formed on the side surface opposite to the side surface on which is formed, the thickness of the primary side input electrodes 2 and 3 formed to face the upper and lower main surfaces 1a and 1b. the opposite output electrodes 8A and 8B of the secondary side that is formed on the side surface 1d along with polarized P 1 in the direction T by dividing into plural, the longitudinal direction L of the piezoelectric ceramic body 1 of the rectangular
And P 2 and P 3 are polarized in opposite directions.

【0008】[0008]

【作用】本発明によればトランスの二次側の出力電極を
例えば2分割8A及び8Bして逆方向に分極P2 及びP
3 することでL/Tを大きくすることなく高い変圧比
(昇圧比)の圧電セラミックトランスが得られる。
According to the present invention, the output electrode on the secondary side of the transformer is divided into, for example, two sections 8A and 8B, and polarizations P 2 and P are applied in opposite directions.
By doing so, a piezoelectric ceramic transformer with a high transformation ratio (step-up ratio) can be obtained without increasing L / T.

【0009】[0009]

【実施例】以下、本発明の圧電セラミックトランスを図
1及び図2によって説明する。図1は本発明の圧電セラ
ミックトランスの一実施例を示す全体的な斜視図であ
り、図2A〜Dは本発明の圧電セラミックトランスの入
出力電極の形成手順並びに分極手順を説明するための説
明図である。尚、従来構成で説明した圧電セラミックト
ランスとの対応部分には同一符号を付して示してある。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS The piezoelectric ceramic transformer of the present invention will be described below with reference to FIGS. FIG. 1 is an overall perspective view showing an embodiment of the piezoelectric ceramic transformer of the present invention, and FIGS. 2A to 2D are explanations for explaining a forming procedure of an input / output electrode and a polarization procedure of the piezoelectric ceramic transformer of the present invention. It is a figure. The parts corresponding to those of the piezoelectric ceramic transformer described in the conventional configuration are designated by the same reference numerals.

【0010】図1で圧電セラミック素体1は長さ2Lm
m、幅Wmm、厚さTmmの薄板状の偏平な略々直方体
状と成される。その材料としては機械品質係数の大きい
PZTセラミックスが選択される。
In FIG. 1, the piezoelectric ceramic body 1 has a length of 2 Lm.
m, width Wmm, and thickness Tmm is a flat, substantially rectangular parallelepiped shape. As the material, PZT ceramics having a large mechanical quality factor is selected.

【0011】この圧電セラミック素体1の上下主面(2
L×W面)1a及び1bに長さ2L方向の略2L/2=
L位置まで全幅に亘って圧電セラミックトランス10の
1次側の主面に入力電極2及び3を形成する。同様に圧
電セラミック素体1の左右側面1c及び1dの主面の入
力電極2及び3が形成されている側の例えば左側面1c
と反対側の右側面1dに圧電セラミックトランス10の
2次側の出力電極8A及び8Bを形成する。この出力電
極8A及び8Bは図3で示した従来の出力電極6の様に
右側面に一様に全面に形成するのではなく、所定のギャ
ップ幅を有する空隙部から成るギャップ9を設けて出力
電極8A及び8Bを2分割する様に形成する。これら入
出力電極2,3並びに8A及び8BはAgベースト等が
焼付けられる。
The upper and lower main surfaces (2
(L × W surface) 1a and 1b have a length of 2L, approximately 2L / 2 =
The input electrodes 2 and 3 are formed on the primary side main surface of the piezoelectric ceramic transformer 10 over the entire width up to the L position. Similarly, for example, the left side surface 1c on the side where the input electrodes 2 and 3 are formed on the main surfaces of the left and right side surfaces 1c and 1d of the piezoelectric ceramic body 1.
The output electrodes 8A and 8B on the secondary side of the piezoelectric ceramic transformer 10 are formed on the right side surface 1d on the opposite side. The output electrodes 8A and 8B are not formed uniformly on the entire surface on the right side like the conventional output electrode 6 shown in FIG. 3, but are provided with a gap 9 consisting of a void having a predetermined gap width. The electrodes 8A and 8B are formed so as to be divided into two. These input / output electrodes 2, 3 and 8A and 8B are baked with Ag base or the like.

【0012】更に1次側は厚さT方向にP1 の様に分極
し、二次側は長さL方向に互に逆方向にP2 及びP3
様に分極する。これら各電極2及び3並びに8A及び8
Bは入出力端子4及び5並に6及び7に接続され、出力
端子6及び7は負荷抵抗R等を介して直列接続され、入
力端子4及び5間にAC5V〜12V程度の入力電圧を
供給することで出力端子6及び7間に昇圧された高電圧
が出力される様に成されている。
Further, the primary side is polarized in the thickness T direction like P 1 , and the secondary side is polarized in the length L direction opposite to each other like P 2 and P 3 . These respective electrodes 2 and 3 and 8A and 8
B is connected to input / output terminals 4 and 5 as well as 6 and 7, and output terminals 6 and 7 are connected in series via a load resistor R or the like to supply an input voltage of about AC5V to 12V between input terminals 4 and 5. By doing so, the boosted high voltage is output between the output terminals 6 and 7.

【0013】この様な圧電セラミックトランス10の電
極形成手順及び分極手順を図2を用いて説明する。
An electrode forming procedure and a polarization procedure of such a piezoelectric ceramic transformer 10 will be described with reference to FIG.

【0014】先ずセラミック素体1の原料としては機械
品質係数Qm の高いPZTセラミックスが選択される。
このPZTセラミックは例えばPbZrO3 (ジルコン
酸鉛)にPbTiO3 (チタン酸鉛)を加えて固溶体結
晶を作る際に菱面体晶系を経て正方晶系に移る相境界近
傍となる組成比で機械品質係数Qm の最大値が現われ、
温度に対しても安定なものが得られている。
First, as the raw material of the ceramic body 1, PZT ceramics having a high mechanical quality factor Q m is selected.
This PZT ceramic, for example, has a mechanical ratio of PbZrO 3 (lead zirconate) added to PbTiO 3 (lead titanate) to form a solid solution crystal. The maximum value of the coefficient Q m appears,
It is stable with respect to temperature.

【0015】この様なPZTに所定のバインダ(成形助
剤)を混合して流込み法、押出し法、プレス法等の成形
型に入れ、偏平な長さ2L=24mm、幅W=6mm、
厚さT=1.5mmの偏平な直方体(板体)に形成、焼
結して圧電セラミック素体1を得る。
Such PZT is mixed with a predetermined binder (molding aid) and put into a molding die such as a pouring method, an extrusion method, a pressing method, etc., and a flat length 2L = 24 mm, width W = 6 mm,
The piezoelectric ceramic body 1 is obtained by forming and sintering a flat rectangular parallelepiped (plate) having a thickness T = 1.5 mm.

【0016】次に、この圧電セラミック素体1の上下主
面1a及び1bの長手方向2Lの略々2L/2=Lの全
幅Wに亘って図2Aの様に入力電極2及び3を形成す
る。この電極はAgペーストを焼付けて用いることが出
来る。更に同図に示す様に圧電セラミック素体1の左側
面1dに所定のギャップ9を介して2分割した電極8A
及び8BがAgペーストを焼付けて形成される。
Next, as shown in FIG. 2A, the input electrodes 2 and 3 are formed over the entire width W of approximately 2L / 2 = L in the longitudinal direction 2L of the upper and lower main surfaces 1a and 1b of the piezoelectric ceramic body 1. . This electrode can be used by baking Ag paste. Further, as shown in the figure, an electrode 8A divided into two via a predetermined gap 9 on the left side surface 1d of the piezoelectric ceramic body 1.
And 8B are formed by baking Ag paste.

【0017】次に圧電セラミック素体1の長さ方向に2
次側の分極を行なう。即ち、1次側の入力電極2及び3
を共通に接続して一端を接地させた図2Bの接続状態に
する。そして、100℃のシリコン油槽中に圧電セラミ
ック素体1を浸し、先ず2分割させた一方の出力電極8
Aに直流プラス30KVを1時間印加させて、圧電セラ
ミック素体1の長さ方向LにP3 で示す様に分極を行な
い。同様に他の出力電極8Bにも直流マイナス30KV
を1時間印加させてP3 とは逆向きのP2 方向に長さ方
向Lに分極を施す。この場合の分極電圧は25KV/c
mである。
Next, the piezoelectric ceramic body 1 is separated by 2 in the length direction.
Polarize the next side. That is, the input electrodes 2 and 3 on the primary side
Are connected in common and one end is grounded to obtain the connection state of FIG. 2B. Then, the piezoelectric ceramic body 1 was dipped in a silicon oil bath at 100 ° C., and first divided into two output electrodes 8
A direct current plus 30 KV is applied to A for 1 hour to polarize the piezoelectric ceramic body 1 in the length direction L as indicated by P 3 . Similarly, the other output electrode 8B has a DC of -30 KV.
Is applied for 1 hour to polarize in the length direction L in the P 2 direction opposite to P 3 . The polarization voltage in this case is 25 KV / c
m.

【0018】勿論、上述の様に別々に分極を施さずに一
方の出力電極8Aを直流プラス30KV電源に接続し、
他方の出力電極8Bに直流マイナス30KV電源を接続
し、1次側の電極2及び3を共通接続させて接地させて
同時に長さ方向Lに対し逆方向に分極させてもよい。
Of course, as described above, one output electrode 8A is connected to a DC plus 30 KV power source without being separately polarized,
A DC minus 30 KV power source may be connected to the other output electrode 8B, the primary side electrodes 2 and 3 may be commonly connected and grounded, and at the same time polarized in the opposite direction to the length direction L.

【0019】更に、上述とは逆に出力電極8A側に直流
マイナス30KVを印加し、出力電極8B側に直流プラ
ス30KVを印加すれば図2Cの分極P3 及びP2 方向
とは逆の方向に分極された圧電セラミック素子1が得ら
れることは明らかである。
Further, contrary to the above, if DC minus 30 KV is applied to the output electrode 8A side and DC plus 30 KV is applied to the output electrode 8B side, the directions are opposite to the polarization P 3 and P 2 directions of FIG. 2C. It is clear that a polarized piezoceramic element 1 is obtained.

【0020】次に図2Cに示す様に圧電セラミック素体
1の1次側の入力電極2及び3間に直流3.75KVの
電圧を印加する。即ち、入力電極3側を接地し、他方の
入力電極2に厚さ1.5mmとしてDC3.75KV、
(25KV/cm)を100℃のシリコン油中で1時間
印加することで圧電セラミック素体1の厚さT方向にP
1 の様に分極が行なわれる。
Next, as shown in FIG. 2C, a DC voltage of 3.75 KV is applied between the input electrodes 2 and 3 on the primary side of the piezoelectric ceramic body 1. That is, the input electrode 3 side is grounded and the other input electrode 2 has a thickness of 1.5 mm and DC 3.75 KV,
By applying (25 KV / cm) in silicon oil at 100 ° C. for 1 hour, P is applied in the thickness T direction of the piezoelectric ceramic body 1.
Polarization is performed in 1 of the way.

【0021】この様に電極形成及び分極の行なわれた夫
々の電極2及び3並びに8A及び8Bに図2Dの様に1
次及び2次側のリード線11及び12を接続し、入力端
子4及び5にACの1次電圧を供給することで出力端子
6及び7間に接続された負荷抵抗Rに2次電圧とし昇圧
された高電圧が得られる。
As shown in FIG. 2D, the electrodes 2 and 3 and the electrodes 8A and 8B, which have been formed and polarized as described above, have a number 1 as shown in FIG.
By connecting the lead wires 11 and 12 on the secondary and secondary sides and supplying the primary voltage of AC to the input terminals 4 and 5, the load resistor R connected between the output terminals 6 and 7 is boosted to a secondary voltage. High voltage is obtained.

【0022】即ち本例では圧電セラミック素子1の長さ
2L方向は従来に比べて2L×2=4Lと成されるため
従来同一長さの圧電セラミック素体1と比較して略々4
倍の昇圧比が得られることになる。
That is, in the present example, the length 2L of the piezoelectric ceramic element 1 is 2L × 2 = 4L as compared with the conventional one, so that it is approximately 4 as compared with the piezoelectric ceramic element body 1 having the same conventional length.
A double boosting ratio will be obtained.

【0023】上記した圧電セラミック素体1の偏平な直
方体の長さL=24mm、幅W=6mm、厚さT=1.
5mmとし2次側の出力電極を2分割させない図3の構
成の従来の圧電セラミックトランスに1次電圧としてA
C5V〜12Vを印加した時の2次電圧はAC500V
〜AC1200Vであるのに対し、本例の2次電圧はA
C1900〜AC2200Vと略々4倍の値を示した。
The flat rectangular parallelepiped of the piezoelectric ceramic body 1 described above has a length L = 24 mm, a width W = 6 mm, and a thickness T = 1.
In the conventional piezoelectric ceramic transformer of the structure shown in FIG. 3 in which the output electrode on the secondary side is not divided into two, the primary voltage is A
The secondary voltage when applying C5V-12V is AC500V
~ AC1200V, the secondary voltage of this example is A
The value was about four times as large as C1900 to AC2200V.

【0024】尚、上述の実施例では2次側の出力電極を
2分割した例を説明したがn分割することでより高い2
n倍の昇圧比の圧電セラミックトランスが得られること
が明らかである。
In the above embodiment, the secondary side output electrode is divided into two, but it is possible to obtain a higher number by dividing the output electrode into n.
It is clear that a piezoelectric ceramic transformer having an n-fold boost ratio can be obtained.

【0025】[0025]

【発明の効果】本発明の圧電セラミックトランスによれ
ば従来の圧電セラミックトランスと同一形状寸法即ちL
/Tを有していながら二次電圧は略々4倍の昇圧比のも
のが得られ、圧電セラミック素子の長さLを大きくした
り厚さTを薄くする必要がないので機械的強度を下げず
に高出力電圧の圧電セラミックトランスを得ることがで
きる。
According to the piezoelectric ceramic transformer of the present invention, the same shape dimension as the conventional piezoelectric ceramic transformer, that is, L
A secondary voltage having a step-up ratio of about 4 times is obtained while having / T, and it is not necessary to increase the length L or the thickness T of the piezoelectric ceramic element, thereby lowering the mechanical strength. It is possible to obtain a piezoelectric ceramic transformer having a high output voltage without using it.

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

【図1】本発明の一実施例を示す圧電セラミックトラン
スの斜視図である。
FIG. 1 is a perspective view of a piezoelectric ceramic transformer showing an embodiment of the present invention.

【図2】本発明の圧電セラミックトランスの電極及び分
極手順を示す説明図である。
FIG. 2 is an explanatory diagram showing electrodes and polarization procedures of the piezoelectric ceramic transformer of the present invention.

【図3】従来の圧電セラミックトランスの原理的説明図
である。
FIG. 3 is a principle explanatory diagram of a conventional piezoelectric ceramic transformer.

【符号の説明】[Explanation of symbols]

1 圧電セラミック素子 2,3 入力電極 8A,8B 出力電極 P1 ,P2 ,P3 分極方向1 Piezoelectric ceramic element 2, 3 Input electrode 8A, 8B Output electrode P 1 , P 2 , P 3 Polarization direction

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 偏平な直方体状の圧電セラミック素体の
上下主面に対向して1次側の入力電極が形成され、該入
力電極が形成された側の側面と反対の側面に2次側出力
電極が形成された圧電セラミックトランスに於いて、 上記上下主面に対向形成した1次側入力電極の厚み方向
に分極すると共に上記反対の側面に形成した2次側の出
力電極を複数分割し、上記直方体の圧電セラミック素体
の長手方向に互に逆方向に分極して成ることを特徴とす
る圧電セラミックトランス。
1. A primary side input electrode is formed so as to face upper and lower main surfaces of a flat rectangular parallelepiped piezoelectric ceramic body, and a secondary side is provided on a side surface opposite to a side surface on which the input electrode is formed. In a piezoelectric ceramic transformer having an output electrode formed thereon, the primary side input electrode formed opposite to the upper and lower main surfaces is polarized in the thickness direction, and the secondary side output electrode formed on the opposite side surface is divided into a plurality of parts. A piezoelectric ceramic transformer, wherein the rectangular parallelepiped piezoelectric ceramic body is polarized in mutually opposite directions in a longitudinal direction.
JP6199756A 1994-08-24 1994-08-24 Piezoelectric ceramic transformer Pending JPH0864883A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6199756A JPH0864883A (en) 1994-08-24 1994-08-24 Piezoelectric ceramic transformer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6199756A JPH0864883A (en) 1994-08-24 1994-08-24 Piezoelectric ceramic transformer

Publications (1)

Publication Number Publication Date
JPH0864883A true JPH0864883A (en) 1996-03-08

Family

ID=16413108

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6199756A Pending JPH0864883A (en) 1994-08-24 1994-08-24 Piezoelectric ceramic transformer

Country Status (1)

Country Link
JP (1) JPH0864883A (en)

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