Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JPH034520B2 - - Google Patents
[go: Go Back, main page]

JPH034520B2 - - Google Patents

Info

Publication number
JPH034520B2
JPH034520B2 JP28844186A JP28844186A JPH034520B2 JP H034520 B2 JPH034520 B2 JP H034520B2 JP 28844186 A JP28844186 A JP 28844186A JP 28844186 A JP28844186 A JP 28844186A JP H034520 B2 JPH034520 B2 JP H034520B2
Authority
JP
Japan
Prior art keywords
single crystal
pbtio
crystal
growing
pbo
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
Application number
JP28844186A
Other languages
Japanese (ja)
Other versions
JPS63144199A (en
Inventor
Masabumi Ofune
Tadashi Kawabe
Chiaki Sakamoto
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.)
Tateho Chemical Industries Co Ltd
Original Assignee
Tateho Chemical Industries Co Ltd
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 Tateho Chemical Industries Co Ltd filed Critical Tateho Chemical Industries Co Ltd
Priority to JP28844186A priority Critical patent/JPS63144199A/en
Publication of JPS63144199A publication Critical patent/JPS63144199A/en
Publication of JPH034520B2 publication Critical patent/JPH034520B2/ja
Granted legal-status Critical Current

Links

Landscapes

  • Crystals, And After-Treatments Of Crystals (AREA)
  • Inorganic Insulating Materials (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

(産業上の利用分野) 本発明は圧電及び焦電材料に用いられる強誘電
体単結晶の製造方法に関し、特に、PbO−
PbTiO3系融液からPbTiO3単結晶を育成する過
程において、Pbの一部をMgで置換された
(Pb1-xMgx)TiO3(0<x≦0.5)で表される新規
な強誘電体単結晶の製造方法に関する。 (従来技術) 近年来、PbTiO3はペロブスカイト型構造を有
する強誘電体で、キユリー温度が490℃と高く、
ほかの強誘電体(たとえば、BaTiO3)と比較し
て焦電係数(dpr/dT)ならびに性能指数
(dpr/dT)(1/ε)が大きいことから、焦電形
赤外線検出器用材料として注目されいる。 (発明が解決しようとする問題点) しかしながら、これまでのところ、作製された
純粋なPbTiO3結晶は非常に脆く、しかも多くの
空孔や結晶欠陥を有するものしか得られておら
ず、ほとんど電気的な諸定数も測定されるに至つ
ていないのが実情であり、数少ない報告例による
と、室温の抵抗率は高々106Ω・cm程度のものし
か得られていない。 そこで、この抵抗率を改善する目的から、たと
えば、3価の金属酸化物などの不純物質を添加し
た場合に抵抗率は向上するが、これに反して他の
電気特性を劣化させて最終的な材料の焦電係数及
び性能指数を低下させるという問題点があつた。
さらに、従来法で作製したPbTiO3結晶は多くの
双晶構造を有するため、数KV/cmから50KV/
cm程度の強電界処理を施しても容易に単分域化で
きない欠点も有していた。 (問題点を解決するための手段) 本発明は上述の問題にかんがみ、発明されたも
のであつて、弱電界処理で容易に単分域化するこ
とができ、優れた加工性及び電気特性を発揮する
と共に量産性に富み、製造コストも割安となる新
規な強誘電体単結晶(Pb1-xMgx)TiO3(0<x
≦0.5)を得ることができる方法を提供しようと
いうものである。 以下、本発明の構成について説明する。 すなわち、本発明の構成要旨とするところは、
PbO−PbTiO3系融液からPbTiO3単結晶を育成
する過程において、強誘電体単結晶の育成坩堝材
としてマグネシア単結晶を用いることにより、
Pbの一部をMgで置換した一般式(Pb1-xMgx
TiO3(0<x≦0.5)で表される単結晶の育成を
行うことを特徴とする強誘電体単結晶の製造方法
にある。 ここで、上記の本発明製造方法において、マグ
ネシア単結晶の育成坩堝材として用いる理由は高
温のPbO−PbTiO3系融液から徐々に結晶を育成
する過程において、坩堝材からのMgの溶出によ
り、PbTiO3単結晶のPbの一部をMgで置換する
ためである。その結果、育成結晶の抵抗率を改善
するとともにその他の電気特性も向上させて、最
終的に材料の焦電性能を大幅に高められることに
なる。また、育成手段としては好ましくはフラツ
クス法あるいはフラツクス引上げ法によるが、特
に、フラツクス法で行う場合には、坩堝内の出発
原料粉末の上部もしくは下部に1〜2mm程度の厚
さのマグネシア単結晶薄板を置くことにより、融
液状態で融液比重が約8.0、マグネシア単結晶薄
板の比重が約3.585から比重差によつて薄板が融
液の上面に押し上げられ、この結果、高温部での
PbO蒸気の揮散を著しく抑制し、より良質の大型
単結晶が高収率で得られる。なお、このマグネシ
ア単結晶薄板はPbO蒸気の揮散防止以外に、坩堝
材と同様に結晶の育成過程における重要なMgの
供給源として利用されることになる。 さらに、上記育成手段において、Mgの溶出
量、すなわち、PbTiO3単結晶のPbの一部と置換
固溶するMg量は結晶の育成条件である保持温度
ならびに保持時間により制御されるものであり、
これにより所望のMg量を固溶した(Pb1-xMgx
TiO3(0<x≦0.5)単結晶が得られる。ただし、
X=0組成の結晶の走査型顕微鏡写真は第2図に
示すとおり、多孔質でこわれやすい結晶であり、
Xが0.5を超えると組成の結晶は内部に多くの気
泡や異種相が介在し、不透明な結晶であつた。 (実施例) PbO:PbTiO3=80:20(モル%)に調整され
たPbO−PbTiO3系配合物50gをマグネシア単結
晶坩堝(純度99.99%以上、寸法:内径40×高さ
50mm、外径60mm×高さ60mm)に入れ、さらに、そ
の上にマグネシア単結晶薄板(純度99.99%以上、
寸法:直径39mm×厚さ1.7mm)を置いて蓋をした。
これをさらに緻密なアルミナ坩堝(純度99.5%以
上、寸法:外径78mm×高さ125mm)に入れ、電気
炉に装填した後、室温から1100℃まで200℃/時
間で昇温させた。その温度を10時間保持した後、
室温まで10℃/時間で徐冷した。育成結晶の取出
しは2N−HNO3中に坩堝全体を浸漬させ、これ
を加熱しながら、撹拌することで完全にフラツク
スを除去した。得られた結晶の走査型顕微鏡写真
を第1図に、また、原子吸光分析ならびに蛍光X
線分析による結晶の化学組成を第1表に示す。
(Industrial Application Field) The present invention relates to a method for producing ferroelectric single crystals used in piezoelectric and pyroelectric materials, and in particular, to
In the process of growing a PbTiO 3 single crystal from a PbTiO 3 - based melt, a new strong crystal, expressed as (Pb 1-x Mg The present invention relates to a method for manufacturing a dielectric single crystal. (Prior art) In recent years, PbTiO 3 is a ferroelectric material with a perovskite structure and has a high Kyrie temperature of 490°C.
It is attracting attention as a material for pyroelectric infrared detectors due to its large pyroelectric coefficient (dpr/dT) and figure of merit (dpr/dT) (1/ε) compared to other ferroelectric materials (e.g., BaTiO 3 ). It is done. (Problem to be solved by the invention) However, so far, the pure PbTiO 3 crystals that have been produced are extremely brittle and have many vacancies and crystal defects, and they have almost no electrical power. The reality is that the various constants have not yet been measured, and according to the few reports, the resistivity at room temperature is only about 10 6 Ωcm. Therefore, for the purpose of improving this resistivity, for example, when adding impurities such as trivalent metal oxides, the resistivity improves, but on the other hand, it deteriorates other electrical properties and the final There was a problem that the pyroelectric coefficient and figure of merit of the material were reduced.
Furthermore, since the PbTiO 3 crystal produced by the conventional method has many twin crystal structures, it is possible to
It also had the drawback that it could not be easily converted into a single domain even if treated with a strong electric field of about cm. (Means for solving the problems) The present invention was invented in view of the above-mentioned problems. A new ferroelectric single crystal (Pb 1-x Mg x )TiO 3 (0<x
≦0.5). The configuration of the present invention will be explained below. That is, the gist of the present invention is as follows:
In the process of growing PbTiO 3 single crystal from PbO-PbTiO 3 system melt, by using magnesia single crystal as a crucible material for growing ferroelectric single crystal,
General formula in which part of Pb is replaced with Mg (Pb 1-x Mg x )
A method for producing a ferroelectric single crystal, characterized by growing a single crystal represented by TiO 3 (0<x≦0.5). Here, in the production method of the present invention described above, the reason why it is used as a growth crucible material for magnesia single crystals is that in the process of gradually growing crystals from a high-temperature PbO-PbTiO 3 system melt, Mg is eluted from the crucible material. This is to replace part of the Pb in the PbTiO 3 single crystal with Mg. The result is improved resistivity of the grown crystal as well as other electrical properties, ultimately significantly increasing the material's pyroelectric performance. The growth method is preferably a flux method or a flux pulling method, but in particular, when the flux method is used, a magnesia single crystal thin plate with a thickness of about 1 to 2 mm is placed above or below the starting material powder in the crucible. By placing , the specific gravity of the melt in the melt state is about 8.0, and the specific gravity of the magnesia single crystal thin plate is about 3.585, so the thin plate is pushed up to the top surface of the melt due to the difference in specific gravity, and as a result, the thin plate is pushed up to the top of the melt.
The volatilization of PbO vapor is significantly suppressed, and larger single crystals of better quality can be obtained in high yield. In addition to preventing the volatilization of PbO vapor, this magnesia single crystal thin plate will be used as an important source of Mg in the crystal growth process, similar to the crucible material. Furthermore, in the above growth means, the amount of Mg eluted, that is, the amount of Mg that replaces a part of the Pb of the PbTiO 3 single crystal and forms a solid solution, is controlled by the holding temperature and holding time, which are the crystal growth conditions.
As a result, the desired amount of Mg was dissolved in solid solution (Pb 1-x Mg x )
A TiO 3 (0<x≦0.5) single crystal is obtained. however,
As shown in Figure 2, a scanning micrograph of a crystal with a composition of X=0 shows that it is a porous and fragile crystal.
When X exceeds 0.5, the crystal with the composition has many bubbles and foreign phases interposed inside, and is an opaque crystal. (Example) 50 g of PbO-PbTiO 3 -based compound adjusted to PbO:PbTiO 3 = 80:20 (mol%) was placed in a magnesia single crystal crucible (purity 99.99% or more, dimensions: inner diameter 40 x height
50mm, outer diameter 60mm x height 60mm), and on top of that, a magnesia single crystal thin plate (purity of 99.99% or more,
Dimensions: 39 mm diameter x 1.7 mm thickness) was placed and the lid was placed.
This was placed in a denser alumina crucible (99.5% purity or higher, dimensions: outer diameter 78 mm x height 125 mm), loaded into an electric furnace, and then heated from room temperature to 1100 °C at a rate of 200 °C/hour. After holding that temperature for 10 hours,
It was slowly cooled to room temperature at a rate of 10°C/hour. To take out the grown crystals, the entire crucible was immersed in 2N-HNO 3 and the flux was completely removed by stirring while heating the crucible. A scanning micrograph of the obtained crystal is shown in Figure 1, and atomic absorption analysis and fluorescence
The chemical composition of the crystals determined by line analysis is shown in Table 1.

【表】 第1表より明らかなように、得られた結晶は
(Pb0.978 Mg0.022TiO3単結晶であることが確認で
きる。 つぎに、育成した結晶を2.0×2.0×1.0mmの寸法
に研磨加工した後、電気炉に入れ、600℃から室
温までの温度域で電場冷却を行つた。この時の印
加電界は100V/cmで育成結晶は容易に単分域化
された。 これを測定試料として、誘電率(ε)、誘電損
失(tan δ)、抵抗率(ρ)及び焦電係数
(dpr/dT)を測定した。測定結果を第2表に示
す。
[Table] As is clear from Table 1, it can be confirmed that the obtained crystal is a (Pb 0.978 Mg 0.022 TiO 3 single crystal.) Next, the grown crystal was polished to a size of 2.0 x 2.0 x 1.0 mm. After processing, it was placed in an electric furnace and cooled in an electric field at a temperature range from 600°C to room temperature.The applied electric field at this time was 100V/cm, and the grown crystal was easily made into a single domain.This was used as the measurement sample. The dielectric constant (ε), dielectric loss (tan δ), resistivity (ρ), and pyroelectric coefficient (dpr/dT) were measured.The measurement results are shown in Table 2.

【表】 さらに、誘電率の温度特性から測定試料はキユ
リー温度Tc=489℃、キユリーワイス温度To=
465℃、キユリー定数c=2.1×105℃を有する優
れた強誘電体単結晶であつた。なお、実施例では
育成方法としてフラツクス法を用いた例を上げた
が、ほかにフラツクス引上げ法により育成された
結晶が(Pb1-xMgx)TiO3(0<x≦0.5)で表さ
れる強誘電体単結晶であれば、上述のごとく、優
れた特性を発揮することはいうまでもない。 (発明の効果) 以上、説明したとおり、本発明による製造方法
によれば、PbO−PbTiO3系融液からPbTiO3
結晶を育成する過程において、Pbの一部をMgで
置換した(Pb1-xMgx)TiO3(0<x≦0.5)単結
晶を工業的規模で比較的容易に得ることができる
メリツトがある。また、得られた(Pb1-xMgx
TiO3(0<x≦0.5)単結晶はこれまでの多孔質
で脆いPbTiO3結晶に比べ、切断・研磨の際の加
工性に優れているので、たとえば、約1×1×
0.5mm程度まで容易に精密加工できるなど加工精
度がきわめて優れている。さらに、弱電界処理で
簡単に単分域化し、キユリー温度をほとんど低下
させることなく、大幅に抵抗率ならびにそのほか
の電気特性も改善できることから、その優れた焦
電性を利用した各種センサへの応用が期待され
る。
[Table] Furthermore, from the temperature characteristics of the dielectric constant, the measurement sample has a Curie temperature Tc = 489℃ and a Currie-Weiss temperature To =
It was an excellent ferroelectric single crystal with a temperature of 465°C and a Curie constant c=2.1×10 5 °C. In addition, although the example uses the flux method as the growth method, crystals grown by the flux pulling method are also expressed as (Pb 1-x Mg x )TiO 3 (0<x≦0.5). It goes without saying that a ferroelectric single crystal that is made of ferroelectric material exhibits excellent characteristics as described above. (Effects of the Invention) As explained above, according to the manufacturing method of the present invention, in the process of growing a PbTiO 3 single crystal from a PbO-PbTiO 3 system melt, a part of Pb is replaced with Mg (Pb 1 -x Mg x ) TiO 3 (0<x≦0.5) single crystals have the advantage of being relatively easy to obtain on an industrial scale. Also obtained (Pb 1-x Mg x )
TiO 3 (0<x≦0.5) single crystal has excellent workability during cutting and polishing compared to conventional porous and brittle PbTiO 3 crystals.
The machining accuracy is extremely high, allowing for easy precision machining down to around 0.5 mm. Furthermore, it can be easily made into a single domain by weak electric field treatment, and the resistivity and other electrical properties can be significantly improved with almost no drop in the Curie temperature, so it can be applied to various types of sensors that take advantage of its excellent pyroelectricity. There is expected.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は本発明製造方法によつて製造される
(Pb0.978 Mg0.022)TiO3単結晶の走査型電子顕微
鏡写真を示すものであり、また、第2図は
PbTiO3結晶の走査型電子顕微鏡写真を示してい
る。
FIG. 1 shows a scanning electron micrograph of a (Pb 0.978 Mg 0.022 ) TiO 3 single crystal produced by the production method of the present invention, and FIG.
A scanning electron micrograph of a PbTiO3 crystal is shown.

Claims (1)

【特許請求の範囲】 1 PbO−PbTiO3系融液からPbTiO3単結晶を
育成する過程において、強誘電体単結晶の育成坩
堝材としてマグネシア単結晶を用いることによ
り、Pbの一部をMgで置換した 一般式; (Pb1-xMgx)TiO3(0<x≦0.5)で表される
単結晶の育成を行うことを特徴とする強誘電体単
結晶の製造方法。 2 特許請求の範囲第1項に記載の方法におい
て、PbO−PbTiO3系融液からの結晶育成をフラ
ツクス法あるいはフラツクス引上げ法により行う
ことを特徴とする強誘電体単結晶の製造方法。 3 特許請求の範囲第1項に記載の方法におい
て、フラツクス法により結晶を育成させる際に坩
堝内の出発原料の上部もしくは下部にマグネシア
単結晶薄板を置くことにより、融液状態でのPbO
蒸気の揮散を抑制することを特徴とす強誘電体単
結晶の製造方法。
[Claims] 1. In the process of growing a PbTiO 3 single crystal from a PbO-PbTiO 3 system melt, by using a magnesia single crystal as a crucible material for growing a ferroelectric single crystal, a part of Pb can be replaced with Mg. A method for producing a ferroelectric single crystal, which comprises growing a single crystal represented by the substituted general formula: (Pb 1-x Mg x )TiO 3 (0<x≦0.5). 2. A method for producing a ferroelectric single crystal according to claim 1, characterized in that crystal growth from a PbO-PbTiO 3 melt is carried out by a flux method or a flux pulling method. 3 In the method described in claim 1, when growing crystals by the flux method, by placing a magnesia single crystal thin plate above or below the starting material in the crucible, PbO in the melt state can be grown.
A method for producing a ferroelectric single crystal characterized by suppressing volatilization of vapor.
JP28844186A 1986-12-02 1986-12-02 Production of ferroelectric single crystal Granted JPS63144199A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP28844186A JPS63144199A (en) 1986-12-02 1986-12-02 Production of ferroelectric single crystal

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP28844186A JPS63144199A (en) 1986-12-02 1986-12-02 Production of ferroelectric single crystal

Publications (2)

Publication Number Publication Date
JPS63144199A JPS63144199A (en) 1988-06-16
JPH034520B2 true JPH034520B2 (en) 1991-01-23

Family

ID=17730252

Family Applications (1)

Application Number Title Priority Date Filing Date
JP28844186A Granted JPS63144199A (en) 1986-12-02 1986-12-02 Production of ferroelectric single crystal

Country Status (1)

Country Link
JP (1) JPS63144199A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR20250108012A (en) * 2024-01-05 2025-07-15 한국재료연구원 DOPED PbTiO3 PEROVSKITE SINGLE CRYSTAL SEEDS AND MNUFACTURING METHOD FOR THE SAME

Also Published As

Publication number Publication date
JPS63144199A (en) 1988-06-16

Similar Documents

Publication Publication Date Title
Kanuru et al. Synthesis, structural, morphological and electrical properties of NBT–BT ceramics for piezoelectric applications
Mulvihill et al. The role of processing variables in the flux growth of lead zinc niobate-lead titanate relaxor ferroelectric single crystals
Harada et al. Crystal growth and electrical properties of Pb ((Zn1/3Nb2/3) 0.91 Ti0. 09) O3 single crystals produced by solution Bridgman method
Yohachi Yamashita Piezoelectric Properties of Niobium-Doped [P b (S c 1/2 N b 1/2) 1-x T ix] O 3 Ceramics Material near the Morphotropic Phase Boundary
KR102698322B1 (en) Polar nano-stationary engineering-relaxed-PbTiO3 ferroelectric crystals
CN101985775A (en) Ternary system relaxation ferroelectric single crystal material and preparation method thereof
CN103541014A (en) Lead-free high-voltage active crystal material and preparation method thereof
Luo et al. Progress in lead-based ferroelectric and antiferroelectric single crystals: composition modification, crystal growth and properties
CN103774228B (en) Lead scandate columbate-PMN-PT ferro-electricity single crystal and preparation method thereof
CN102560617A (en) Method for preparing ferroelectric single crystal lead indium niobate-lead titanate
Zeng et al. Growth and characterization of lead-free Ba (1− x) CaxTi (1− y) ZryO3 single crystal
Ruiz-Valdés et al. Glass–ceramic materials with regulated dielectric properties based on the system BaO–PbO–TiO2–B2O3–Al2O3
CN102383189B (en) Preparation method for lead zinc niobate-lead titanate monocrystal
CN102644114A (en) Ferroelectric monocrystal lead lutecium niobate-lead titanate and preparation method thereof
Grabmaier PbTiO3 grown from the melt
JPH034520B2 (en)
Karaki et al. Top-seeded solution growth of Pb [(In1/2Nb1/2),(Mg1/3Nb2/3), Ti] O3 single crystals
Sun et al. Growth of large PbTiO3 crystals by a self-flux technique
CN102492991A (en) Lead niobate zincate-lead titanate (PZNT) single crystal material and pyroelectric application thereof
CN103172377B (en) Reaction solid state growth prepares the method for high performance piezoelectric pottery
JP4272830B2 (en) Method for producing BaTiO3-PbTiO3-based piezoelectric single crystal
JP4878607B2 (en) Manufacturing method of full-rate solid solution type piezoelectric single crystal ingot, full-rate solid solution type piezoelectric single crystal ingot, and piezoelectric single crystal element
JP6635366B2 (en) Piezoelectric material, manufacturing method thereof, piezoelectric element and combustion pressure sensor
CN1138870C (en) A kind of antimony-doped strontium titanate thin film and preparation method thereof
JPH034519B2 (en)

Legal Events

Date Code Title Description
LAPS Cancellation because of no payment of annual fees