JPH0228909B2 - - Google Patents
Info
- Publication number
- JPH0228909B2 JPH0228909B2 JP56002459A JP245981A JPH0228909B2 JP H0228909 B2 JPH0228909 B2 JP H0228909B2 JP 56002459 A JP56002459 A JP 56002459A JP 245981 A JP245981 A JP 245981A JP H0228909 B2 JPH0228909 B2 JP H0228909B2
- Authority
- JP
- Japan
- Prior art keywords
- composition
- ceramic
- ferroelectric
- present
- range
- 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
Links
- 239000000919 ceramic Substances 0.000 claims description 27
- 239000000203 mixture Substances 0.000 claims description 26
- 229910052573 porcelain Inorganic materials 0.000 description 8
- 230000008878 coupling Effects 0.000 description 6
- 238000010168 coupling process Methods 0.000 description 6
- 238000005859 coupling reaction Methods 0.000 description 6
- 238000010304 firing Methods 0.000 description 5
- 238000004519 manufacturing process Methods 0.000 description 3
- RTAQQCXQSZGOHL-UHFFFAOYSA-N Titanium Chemical compound [Ti] RTAQQCXQSZGOHL-UHFFFAOYSA-N 0.000 description 2
- 230000000052 comparative effect Effects 0.000 description 2
- 229910002112 ferroelectric ceramic material Inorganic materials 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 230000010287 polarization Effects 0.000 description 2
- 239000002994 raw material Substances 0.000 description 2
- 229910052845 zircon Inorganic materials 0.000 description 2
- GFQYVLUOOAAOGM-UHFFFAOYSA-N zirconium(iv) silicate Chemical compound [Zr+4].[O-][Si]([O-])([O-])[O-] GFQYVLUOOAAOGM-UHFFFAOYSA-N 0.000 description 2
- 229910021193 La 2 O 3 Inorganic materials 0.000 description 1
- BQCADISMDOOEFD-UHFFFAOYSA-N Silver Chemical compound [Ag] BQCADISMDOOEFD-UHFFFAOYSA-N 0.000 description 1
- 229910010413 TiO 2 Inorganic materials 0.000 description 1
- 239000011230 binding agent Substances 0.000 description 1
- 238000004891 communication Methods 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 238000001816 cooling Methods 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 238000001035 drying Methods 0.000 description 1
- 230000005684 electric field Effects 0.000 description 1
- 230000001747 exhibiting effect Effects 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 238000002156 mixing Methods 0.000 description 1
- 239000000843 powder Substances 0.000 description 1
- 238000010298 pulverizing process Methods 0.000 description 1
- 229910052709 silver Inorganic materials 0.000 description 1
- 239000004332 silver Substances 0.000 description 1
- 238000005245 sintering Methods 0.000 description 1
- 238000003878 thermal aging Methods 0.000 description 1
Classifications
-
- C—CHEMISTRY; METALLURGY
- C04—CEMENTS; CONCRETE; ARTIFICIAL STONE; CERAMICS; REFRACTORIES
- C04B—LIME, MAGNESIA; SLAG; CEMENTS; COMPOSITIONS THEREOF, e.g. MORTARS, CONCRETE OR LIKE BUILDING MATERIALS; ARTIFICIAL STONE; CERAMICS; REFRACTORIES; TREATMENT OF NATURAL STONE
- C04B35/00—Shaped ceramic products characterised by their composition; Ceramics compositions; Processing powders of inorganic compounds preparatory to the manufacturing of ceramic products
- C04B35/01—Shaped ceramic products characterised by their composition; Ceramics compositions; Processing powders of inorganic compounds preparatory to the manufacturing of ceramic products based on oxide ceramics
- C04B35/48—Shaped ceramic products characterised by their composition; Ceramics compositions; Processing powders of inorganic compounds preparatory to the manufacturing of ceramic products based on oxide ceramics based on zirconium or hafnium oxides, zirconates, zircon or hafnates
- C04B35/49—Shaped ceramic products characterised by their composition; Ceramics compositions; Processing powders of inorganic compounds preparatory to the manufacturing of ceramic products based on oxide ceramics based on zirconium or hafnium oxides, zirconates, zircon or hafnates containing also titanium oxides or titanates
- C04B35/491—Shaped ceramic products characterised by their composition; Ceramics compositions; Processing powders of inorganic compounds preparatory to the manufacturing of ceramic products based on oxide ceramics based on zirconium or hafnium oxides, zirconates, zircon or hafnates containing also titanium oxides or titanates based on lead zirconates and lead titanates, e.g. PZT
- C04B35/493—Shaped ceramic products characterised by their composition; Ceramics compositions; Processing powders of inorganic compounds preparatory to the manufacturing of ceramic products based on oxide ceramics based on zirconium or hafnium oxides, zirconates, zircon or hafnates containing also titanium oxides or titanates based on lead zirconates and lead titanates, e.g. PZT containing also other lead compounds
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N—ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N30/00—Piezoelectric or electrostrictive devices
- H10N30/80—Constructional details
- H10N30/85—Piezoelectric or electrostrictive active materials
- H10N30/853—Ceramic compositions
Landscapes
- Chemical & Material Sciences (AREA)
- Engineering & Computer Science (AREA)
- Ceramic Engineering (AREA)
- Composite Materials (AREA)
- Manufacturing & Machinery (AREA)
- Materials Engineering (AREA)
- Structural Engineering (AREA)
- Organic Chemistry (AREA)
- Compositions Of Oxide Ceramics (AREA)
- Inorganic Insulating Materials (AREA)
Description
本発明は強誘電性磁器組成物、特に、機械的品
質係数が低く特性の安定性が高い強誘電性磁器組
成物に関する。
近年、AMラジオ、FMラジオ、その他の音声
通信機器などにおいて音質を重視する傾向が一段
と強くなり、これらの機器に適応されるセラミツ
クフイルタとして位相ひずみの非常に少ないもの
が要求されるようになつてきた。このためセラミ
ツクフイルタ用強誘電性磁器材料としては、機械
的品質係数(以下、Qmと記す。)が低く、安定
した特性を持つことが要求されている。
従来、Qmの低い強誘電性磁器材料としては、
ジルコンチタン酸鉛(Pb(Zr、Ti)O3)のPbの
一部をBa、Sr、Ca等、二価の元素で置換したも
の、あるいはジルコンチタン酸鉛にNb2O5、
Sb2O3、La2O3などの酸化物を添加したものなど
が知られている。しかし、これらの磁器材料では
Qmが80〜200の低い値になる組成にすると、電
気機械結合係数Kpおよび比誘電率εT33/ε0がそれ
ぞれ60〜70%、1500〜2500と共に大きな値にな
り、狭帯域のセラミツクフイルタを製造するには
分極のコントロールを行わなければならず、その
結果バラツキが大きくなり、特性の安定したセラ
ミツクフイルタを量産することが困難であるとい
う問題があつた。しかも、中心周波数の安定性が
悪くセラミツクフイルタとしての実用化が困難で
ある他、焼結温度が1250〜1300℃と高いため焼成
時鉛の蒸発量が多く、再現性が悪いという問題が
あつた。
本発明は、かかる問題を解決すべくなされたも
のであつて、Qmが低く特性の安定度が高く、狭
帯域のセラミツクフイルタを製造することができ
る強誘電性磁器組成物を提供することを目的とす
る。
また本発明は超音波振動子、セラミツクデイス
クリミネータ、圧電トランス、圧電着火素子、あ
るいはその他の圧電トランスジユーサに用途を有
する強誘電性磁器組成物を提供することを目的と
する。
本発明に係る強誘電性磁器組成物は、一般式:
xPb(Y1/2Sb1/2)O3−yPbTiO3−zPbZrO3
(ただし、x、y、zは各成分のモル比で、x+
y+z=1.00、0.005≦x≦0.200、0.140≦y≦
0.620、0.350≦z≦0.830を満足する。)で表わさ
れる組成物からなり、第1図に示される多角形
ABCDEFで囲まれた範囲内の組成を有し、前記
多角形の各頂点における組成が次に示される組成
であることを特徴とするものである。
x y z
A 0.200 0.450 0.350
B 0.030 0.620 0.350
C 0.005 0.615 0.380
D 0.005 0.165 0.830
E 0.030 0.140 0.830
F 0.200 0.270 0.530
本発明に係る強誘電性磁器組成物の組成を第1
図の多角形ABCDEFで囲まれた範囲内の組成に
限定したのは、その範囲外の組成では電気機械結
合係数が20%以下になると共に、熱エージングに
よつて特性が著しく変動するからである。また、
Pb(Y1/2Sb1/2)O3のモル比xが0.005より小さく
なると、焼成温度が1270〜1300℃と高くなるとと
もに、電気機械結合係数(Kp)、比誘電率
(εT33/ε0)、Qm、周波数定数(frD)などの電気
的特性の再現性が悪くなり、0.200を越えると、
体積固有抵抗が減少し、分極処理が困難となる。
また、PbTiO3のモル比yが0.140未満又は0.620
を越えると、電気機械結合係数(Kp)が20%未
満となり、実用上十分な値のものが得られない。
PbZrO3のモル比zが0.350未満又は0.830を越える
と、電気機械結合係数(Kp)が20%未満となり、
実用上十分な値のものが得られない。
前記強誘電性磁器組成物は従来公知の方法によ
つて製造することができるが、1210〜1250℃と従
来より比較的低い焼成温度で焼結するので、焼成
中の鉛の蒸発量が少なく配合比のずれが制御され
るため再現性がよく、従つて量産性に優れてい
る。また、前記多角形の範囲内で組成を選定する
ことにより、90〜300の範囲内の任意の低いQm
値を示すと同時に、電気機械結合係数(Kp)お
よび比誘電率(εT33/ε0)がそれぞれ20〜55%、
300〜1500の範囲の低い値を示す磁器を得ること
ができる。従つて、同一組成の磁器で種々の帯域
のセラミツクフイルタを製造することができ、工
業的に極めて有用である。また、この磁器でセラ
ミツクフイルタを製造した場合、磁器の特性の安
定性がよいので、中心周波数の安定性が非常によ
いものが得られる。
以下、本発明の実施例について説明する。
実施例
素原料としてPbOまたはPb3O4、Y2O3、
Sb2O3、TiO2およびZrO2を用い、第1表に示す
組成になるように秤量調合し、ポツトミルにて約
20時間湿式混合した後、乾燥させ、次いで、850
〜950℃で2時間仮焼する。仮焼した原料を粉砕
した後、適当量の公知バインダを加えてポツトミ
ルにて約10時間湿式混合し、80メツシユのふるい
を通して造粒する。このようにして得た粉粒体を
直径22mm、厚さ1.1mmの円板に700〜1000Kg/cm2の
圧力で成形し、第1表に示す焼成温度で2時間焼
成し、強誘電性磁器の試料を得る。
この試料の両平面に銀電極を焼付け、80℃の絶
縁油中にて1.0〜3.0KV/mmの直流電界を印加し
て分極させ、その電気的特性を測定した。得られ
た結果を第1表に示す。なお、試料の圧電的特性
はIRE標準回路を用いて測定し、比誘電率はキヤ
パシタンスブリツジを用いて測定した。第1表
中、*は本発明の範囲外の組成のものを示し、記
号A、B、C、D、E、Fはそれぞれ第1図中の
同記号のものに対応する。
第1表の結果から、本発明に係る強誘電性磁器
はQmが90〜300と低く、Kpは20〜55%、比誘電
率は300〜1500の各範囲内で任意の値をもつもの
が得られることがわかる。
The present invention relates to a ferroelectric ceramic composition, and particularly to a ferroelectric ceramic composition having a low mechanical quality factor and high stability of properties. In recent years, there has been a growing tendency to emphasize sound quality in AM radio, FM radio, and other audio communication equipment, and ceramic filters with extremely low phase distortion are now required to be used in these equipment. Ta. Therefore, ferroelectric ceramic materials for ceramic filters are required to have a low mechanical quality factor (hereinafter referred to as Qm) and stable characteristics. Conventionally, ferroelectric ceramic materials with low Qm are
Lead zircon titanate (Pb(Zr,Ti)O 3 ) in which part of the Pb is replaced with divalent elements such as Ba, Sr, Ca, etc., or lead zircon titanate with Nb 2 O 5 ,
Those to which oxides such as Sb 2 O 3 and La 2 O 3 are added are known. However, these porcelain materials
When the composition has a low value of Qm of 80 to 200, the electromechanical coupling coefficient Kp and the relative dielectric constant ε T33 /ε 0 become large values of 60 to 70% and 1500 to 2500, respectively, making it possible to create a narrow band ceramic filter. In manufacturing, polarization must be controlled, resulting in large variations, making it difficult to mass-produce ceramic filters with stable characteristics. Moreover, the stability of the center frequency was poor, making it difficult to put it to practical use as a ceramic filter, and the high sintering temperature of 1,250 to 1,300°C caused a large amount of lead to evaporate during firing, resulting in poor reproducibility. . The present invention was made to solve this problem, and an object of the present invention is to provide a ferroelectric ceramic composition that has a low Qm and high stability of characteristics and can be used to manufacture a narrow band ceramic filter. shall be. Another object of the present invention is to provide a ferroelectric ceramic composition that has applications in ultrasonic vibrators, ceramic disc liminators, piezoelectric transformers, piezoelectric ignition elements, and other piezoelectric transducers. The ferroelectric ceramic composition according to the present invention has the general formula: xPb(Y 1/2 Sb 1/2 )O 3 −yPbTiO 3 −zPbZrO 3 (where x, y, and z are the molar ratios of each component, x+
y+z=1.00, 0.005≦x≦0.200, 0.140≦y≦
Satisfies 0.620, 0.350≦z≦0.830. ), and the polygon shown in Figure 1
It has a composition within a range surrounded by ABCDEF, and is characterized in that the composition at each vertex of the polygon is as shown below. x y z A 0.200 0.450 0.350 B 0.030 0.620 0.350 C 0.005 0.615 0.380 D 0.005 0.165 0.830 E 0.030 0.140 0.830 F 0.200 0.270 0 .530 The composition of the ferroelectric ceramic composition according to the present invention is
The reason why we limited the compositions to those within the range surrounded by the polygon ABCDEF in the figure is because compositions outside this range would have an electromechanical coupling coefficient of 20% or less, and the characteristics would change significantly due to thermal aging. . Also,
When the molar ratio x of Pb(Y 1/2 Sb 1/2 ) O 3 becomes smaller than 0.005, the firing temperature increases to 1270-1300℃, and the electromechanical coupling coefficient (Kp) and relative dielectric constant (ε T33 / The reproducibility of electrical characteristics such as ε 0 ), Qm, and frequency constant (frD) deteriorates, and when it exceeds 0.200,
Volume resistivity decreases and polarization becomes difficult.
In addition, the molar ratio y of PbTiO 3 is less than 0.140 or 0.620
If it exceeds , the electromechanical coupling coefficient (Kp) will be less than 20%, making it impossible to obtain a value sufficient for practical use.
If the molar ratio z of PbZrO 3 is less than 0.350 or more than 0.830, the electromechanical coupling coefficient (Kp) will be less than 20%,
Practically sufficient values cannot be obtained. The ferroelectric ceramic composition can be manufactured by a conventionally known method, but since it is sintered at a firing temperature of 1210 to 1250°C, which is relatively lower than conventional methods, the amount of lead evaporated during firing is small. Since the ratio deviation is controlled, reproducibility is good, and therefore mass production is excellent. In addition, by selecting the composition within the range of the polygon, any low Qm within the range of 90 to 300 can be obtained.
At the same time, the electromechanical coupling coefficient (Kp) and relative permittivity (ε T33 /ε 0 ) are 20 to 55%, respectively.
It is possible to obtain porcelain exhibiting low values in the range 300-1500. Therefore, ceramic filters of various bands can be manufactured using porcelain of the same composition, which is extremely useful industrially. Furthermore, when a ceramic filter is manufactured using this porcelain, the stability of the characteristics of the porcelain is good, so a filter with very good center frequency stability can be obtained. Examples of the present invention will be described below. Examples PbO or Pb 3 O 4 , Y 2 O 3 as raw materials,
Sb 2 O 3 , TiO 2 and ZrO 2 were weighed and mixed to have the composition shown in Table 1, and then mixed in a pot mill to approx.
After wet mixing for 20 hours, drying and then 850
Calcinate at ~950℃ for 2 hours. After pulverizing the calcined raw material, an appropriate amount of a known binder is added, wet-mixed in a pot mill for about 10 hours, and granulated through an 80-mesh sieve. The powder thus obtained was molded into a disk with a diameter of 22 mm and a thickness of 1.1 mm at a pressure of 700 to 1000 Kg/cm 2 and fired at the firing temperature shown in Table 1 for 2 hours to produce ferroelectric porcelain. Obtain a sample of Silver electrodes were baked on both surfaces of this sample, and a DC electric field of 1.0 to 3.0 KV/mm was applied in insulating oil at 80° C. to polarize the sample, and its electrical characteristics were measured. The results obtained are shown in Table 1. The piezoelectric properties of the sample were measured using an IRE standard circuit, and the dielectric constant was measured using a capacitance bridge. In Table 1, * indicates a composition outside the scope of the present invention, and symbols A, B, C, D, E, and F correspond to the same symbols in FIG. 1, respectively. From the results in Table 1, the ferroelectric ceramics according to the present invention have a low Qm of 90 to 300, a Kp of 20 to 55%, and a specific dielectric constant of any value within the range of 300 to 1500. You can see what you can get.
【表】【table】
【表】【table】
【表】【table】
【表】【table】
【表】
次に、0.04Pb(Y1/2Sb1/2)O3−0.53PbZrO3−
0.43PbTiO3、および0.02Pb(Y1/2Sb1/2)O3−
0.51PbZrO3−0.47PbTiO3の各組成を有する試料、
141および142と、それと比較のため(Pb0.96
Sr0.04)(Zr0.05Ti0.46)O3+0.03モル%Sb2O3およ
び(Pb0.92Sr0.08)(Zr0.52Ti0.48)O3+0.03モル%
Nb2O5の各組成を有する比較試料1および2を実
施例と同様にして用意し、得られた各磁器を用い
て中心周波数10.7MHzのエネルギとじ込型セラミ
ツクフイルタを得た。試料141のフイルタの減衰
特性を第2図に示す。得られた各フイルタについ
て−55℃〜+85℃の温度範囲で熱サイクルテスト
をくり返し、中心周波数および3dB通過帯域幅並
びに20dB通過帯域幅の変化を調べた。この熱サ
イクルテストは、各フイルタをまず−55℃に冷却
して数分間保持した後、+85℃まで数秒で昇温さ
せて同温度で数分間保持し、次いで数秒で−55℃
まで冷却する工程を1サイクルとしてくり返した
ものである。それらの結果を第3図〜第5図に示
す。
第3図〜第5図の結果からわかるように、本発
明に係る磁器を用いたものでは熱サイクルテスト
を100回くり返しても、従来の比較例の磁器を用
いたものより中心周波数および3dB通過帯域幅並
びに20dB通過帯域幅の変化が著しく小さく、特
性の安定性において非常に優れている。[Table] Next, 0.04Pb(Y 1/2 Sb 1/2 )O 3 −0.53PbZrO 3 −
0.43PbTiO3 , and 0.02Pb(Y1 / 2Sb1 /2 ) O3−
Samples with each composition of 0.51PbZrO3 −0.47PbTiO3 ,
141 and 142 and for comparison (Pb 0.96
Sr 0.04 ) (Zr 0.05 Ti 0.46 ) O 3 + 0.03 mol% Sb 2 O 3 and (Pb 0.92 Sr 0.08 ) (Zr 0.52 Ti 0.48 ) O 3 + 0.03 mol%
Comparative samples 1 and 2 having respective compositions of Nb 2 O 5 were prepared in the same manner as in the examples, and each of the obtained ceramics was used to obtain an energy trapping type ceramic filter with a center frequency of 10.7 MHz. Figure 2 shows the attenuation characteristics of the filter of sample 141. Thermal cycle tests were repeated for each of the obtained filters in the temperature range of -55°C to +85°C, and changes in the center frequency, 3 dB pass band width, and 20 dB pass band width were examined. In this thermal cycle test, each filter was first cooled to -55°C and held for several minutes, then heated to +85°C in a few seconds, held at the same temperature for several minutes, and then cooled to -55°C in a few seconds.
The cooling process is repeated as one cycle. The results are shown in FIGS. 3 to 5. As can be seen from the results shown in Figures 3 to 5, even after repeating the thermal cycle test 100 times, the product using the porcelain according to the present invention has a higher center frequency and 3 dB passthrough than the conventional comparative example using porcelain. Changes in bandwidth and 20dB passband width are extremely small, and the characteristics are extremely stable.
第1図は本発明の強誘電性磁器組成物の組成範
囲を示す三角図、第2図は本発明に係る強誘電性
磁器を用いたセラミツクフイルタの減衰特性を示
すグラフ、第3図は本発明に係る強誘電性磁器お
よび従来の強誘電性磁器を用いたセラミツクフイ
ルタの中心周波数の熱サイクルテストによる変化
を示すグラフ、第4図および第5図はそれぞれそ
の3dB通過帯域幅および20dB通過帯域幅の熱サ
イクルテストによる変化を示すグラフである。
FIG. 1 is a triangular diagram showing the composition range of the ferroelectric ceramic composition of the present invention, FIG. 2 is a graph showing the attenuation characteristics of a ceramic filter using the ferroelectric ceramic according to the present invention, and FIG. 3 is a graph showing the composition range of the ferroelectric ceramic composition of the present invention. Graphs showing changes in center frequencies of ceramic filters using ferroelectric ceramics according to the invention and conventional ferroelectric ceramics due to thermal cycle tests. Figures 4 and 5 show their 3 dB passband width and 20 dB passband, respectively. It is a graph showing a change in width due to a thermal cycle test.
Claims (1)
y+z=1.00、0.005≦x≦0.200、0.140≦y≦
0.620、0.350≦z≦0.830を満足する。) で表わされる組成物からなり、第1図に示される
多角形ABCDEFで囲まれた範囲内の組成を有し、
前記多角形の各頂点における組成が次に示される
組成である強誘電性磁器組成物。 x y z A 0.200 0.450 0.350 B 0.030 0.620 0.350 C 0.005 0.615 0.380 D 0.005 0.165 0.830 E 0.030 0.140 0.830 F 0.200 0.270 0.530[Claims] 1 General formula: xPb(Y 1/2 Sb 1/2 )O 3 −yPbTiO 3 −zPbZrO 3 (where x, y, and z are the molar ratios of each component, and x+
y+z=1.00, 0.005≦x≦0.200, 0.140≦y≦
Satisfies 0.620, 0.350≦z≦0.830. ) and has a composition within the range surrounded by the polygon ABCDEF shown in Figure 1,
A ferroelectric ceramic composition in which the composition at each vertex of the polygon is as shown below. x y z A 0.200 0.450 0.350 B 0.030 0.620 0.350 C 0.005 0.615 0.380 D 0.005 0.165 0.830 E 0.030 0.140 0.830 F 0.200 0.270 0 .530
Priority Applications (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56002459A JPS57115888A (en) | 1981-01-09 | 1981-01-09 | Porcelain composition with strong dielectric property |
| DE19823200339 DE3200339A1 (en) | 1981-01-09 | 1982-01-08 | Ferroelectric ceramic |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56002459A JPS57115888A (en) | 1981-01-09 | 1981-01-09 | Porcelain composition with strong dielectric property |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS57115888A JPS57115888A (en) | 1982-07-19 |
| JPH0228909B2 true JPH0228909B2 (en) | 1990-06-27 |
Family
ID=11529878
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP56002459A Granted JPS57115888A (en) | 1981-01-09 | 1981-01-09 | Porcelain composition with strong dielectric property |
Country Status (2)
| Country | Link |
|---|---|
| JP (1) | JPS57115888A (en) |
| DE (1) | DE3200339A1 (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE4223186A1 (en) * | 1992-07-15 | 1994-01-20 | Hoechst Ceram Tec Ag | Sinterable offset at low temperatures for the production of piezoelectric, ceramic shaped bodies and shaped bodies produced therefrom by sintering |
| DE102006035569B4 (en) * | 2006-07-26 | 2017-06-08 | Michael Hörauf Maschinenfabrik GmbH & Co. KG | Device and method for transporting a sleeve |
-
1981
- 1981-01-09 JP JP56002459A patent/JPS57115888A/en active Granted
-
1982
- 1982-01-08 DE DE19823200339 patent/DE3200339A1/en not_active Withdrawn
Also Published As
| Publication number | Publication date |
|---|---|
| JPS57115888A (en) | 1982-07-19 |
| DE3200339A1 (en) | 1982-09-16 |
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