WO2016119157A1 - Method for preparing pyroelectric single crystal - Google Patents

Method for preparing pyroelectric single crystal Download PDF

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WO2016119157A1
WO2016119157A1 PCT/CN2015/071798 CN2015071798W WO2016119157A1 WO 2016119157 A1 WO2016119157 A1 WO 2016119157A1 CN 2015071798 W CN2015071798 W CN 2015071798W WO 2016119157 A1 WO2016119157 A1 WO 2016119157A1
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crystal
hours
mgnb
innbo
crucible
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PCT/CN2015/071798
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Chinese (zh)
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罗豪甦
王升
李晓兵
徐海清
赵祥永
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上海硅酸盐研究所中试基地
中国科学院上海硅酸盐研究所
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Priority to PCT/CN2015/071798 priority Critical patent/WO2016119157A1/en
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    • CCHEMISTRY; METALLURGY
    • C30CRYSTAL GROWTH
    • C30BSINGLE-CRYSTAL GROWTH; UNIDIRECTIONAL SOLIDIFICATION OF EUTECTIC MATERIAL OR UNIDIRECTIONAL DEMIXING OF EUTECTOID MATERIAL; REFINING BY ZONE-MELTING OF MATERIAL; PRODUCTION OF A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; SINGLE CRYSTALS OR HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; AFTER-TREATMENT OF SINGLE CRYSTALS OR A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; APPARATUS THEREFOR
    • C30B29/00Single crystals or homogeneous polycrystalline material with defined structure characterised by the material or by their shape
    • C30B29/10Inorganic compounds or compositions
    • C30B29/16Oxides
    • C30B29/22Complex oxides
    • CCHEMISTRY; METALLURGY
    • C30CRYSTAL GROWTH
    • C30BSINGLE-CRYSTAL GROWTH; UNIDIRECTIONAL SOLIDIFICATION OF EUTECTIC MATERIAL OR UNIDIRECTIONAL DEMIXING OF EUTECTOID MATERIAL; REFINING BY ZONE-MELTING OF MATERIAL; PRODUCTION OF A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; SINGLE CRYSTALS OR HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; AFTER-TREATMENT OF SINGLE CRYSTALS OR A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; APPARATUS THEREFOR
    • C30B11/00Single-crystal growth by normal freezing or freezing under temperature gradient, e.g. Bridgman-Stockbarger method
    • CCHEMISTRY; METALLURGY
    • C30CRYSTAL GROWTH
    • C30BSINGLE-CRYSTAL GROWTH; UNIDIRECTIONAL SOLIDIFICATION OF EUTECTIC MATERIAL OR UNIDIRECTIONAL DEMIXING OF EUTECTOID MATERIAL; REFINING BY ZONE-MELTING OF MATERIAL; PRODUCTION OF A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; SINGLE CRYSTALS OR HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; AFTER-TREATMENT OF SINGLE CRYSTALS OR A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; APPARATUS THEREFOR
    • C30B29/00Single crystals or homogeneous polycrystalline material with defined structure characterised by the material or by their shape
    • C30B29/10Inorganic compounds or compositions
    • C30B29/16Oxides
    • C30B29/22Complex oxides
    • C30B29/30Niobates; Vanadates; Tantalates
    • CCHEMISTRY; METALLURGY
    • C30CRYSTAL GROWTH
    • C30BSINGLE-CRYSTAL GROWTH; UNIDIRECTIONAL SOLIDIFICATION OF EUTECTIC MATERIAL OR UNIDIRECTIONAL DEMIXING OF EUTECTOID MATERIAL; REFINING BY ZONE-MELTING OF MATERIAL; PRODUCTION OF A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; SINGLE CRYSTALS OR HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; AFTER-TREATMENT OF SINGLE CRYSTALS OR A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; APPARATUS THEREFOR
    • C30B29/00Single crystals or homogeneous polycrystalline material with defined structure characterised by the material or by their shape
    • C30B29/10Inorganic compounds or compositions
    • C30B29/16Oxides
    • C30B29/22Complex oxides
    • C30B29/32Titanates; Germanates; Molybdates; Tungstates
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10NELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10N15/00Thermoelectric devices without a junction of dissimilar materials; Thermomagnetic devices, e.g. using the Nernst-Ettingshausen effect
    • H10N15/10Thermoelectric devices using thermal change of the dielectric constant, e.g. working above and below the Curie point

Definitions

  • the invention relates to a preparation method of a large-sized manganese-doped novel pyroelectric single crystal, in particular to a method for preparing a large-sized (diameter ⁇ three inches) manganese-doped lead indium bismuth-bismuth by a modified Bridgman method.
  • the method of lead magnesium titanate-titanate lead ternary pyroelectric single crystal belongs to the technical field of crystal growth.
  • Infrared detectors are mainly divided into photon type infrared detectors and thermal infrared detectors.
  • the common photon-type infrared detector mainly uses a narrow band gap semiconductor material represented by mercury cadmium telluride and an optoelectronic semiconductor material represented by gallium arsenide.
  • semiconductor infrared devices generally require low-temperature refrigeration, which is bulky, costly, and consumes a lot of power.
  • the pyroelectric infrared detector developed by the pyroelectric effect of the material has a flat spectral response in the ultraviolet, visible and infrared bands, and has no need for refrigeration, low power consumption, low noise bandwidth, compact structure and convenience.
  • the advantages of carrying and low cost have become one of the most eye-catching focuses in the field of infrared technology.
  • pyroelectric infrared detectors for low cost, low power consumption and miniaturization, pyroelectric infrared detectors are rapidly expanding from the military market to the civilian market, especially in human body detection, fire warning, gas analysis, infrared spectrometers. And infrared thermal imaging, etc.
  • the field plays an important role and at the same time reflects the huge market potential.
  • the materials currently used in pyroelectric infrared detectors mainly include lead zirconate titanate (PZT), barium titanate (BST) and lead citrate (PST), etc., and the main limitations of materials for pyroelectric unit detectors. Lithium niobate (LiTaO 3 ), triglyceride sulfate (TGS), and the like.
  • PZT lead zirconate titanate
  • BST barium titanate
  • PST lead citrate
  • TGS triglyceride sulfate
  • these traditional materials have shortcomings such as low pyroelectric coefficient, large dielectric loss, and unstable physical properties, which are difficult to meet the application requirements of high-performance pyroelectric infrared detectors and their extended products.
  • the more mature commercial LiTaO 3 infrared detectors have a detection level of only 1 ⁇ 10 8 cm (Hz) 1/2 /W to 4 ⁇ 10 8 cm (Hz) 1/2 /W. Therefore, at the same time, overcoming the shortcomings of the above materials, exploring new pyroelectric materials with high detection value has become an urgent need for the development of uncooled infrared devices.
  • the size of the single crystals prepared using the Bridgman method is less than 2 inches. In order to reduce the cost of the device, detector design and other factors, more and more larger wafers are needed.
  • the increase in the thickness of the crucible causes the internal stress of the crystal to increase, causing the crystal to crack, so that the crystal can not be subsequently applied, and the preparation cost is further Also greatly increased.
  • Patent literature
  • Patent Document 1 Chinese patent CN 1080777C;
  • the present invention provides a large-sized manganese-doped pyroelectric single crystal prepared by the modified Bridgman method to solve the defects in the prior art that large-sized Mn-doped pyroelectric single crystals are difficult to grow in batches.
  • An aspect of the present invention provides a method for preparing a single crystal, which is an improved method.
  • the Bridgman method includes the following specific steps:
  • Step 1 Obtain high-purity Pb(Mn 1/3 Nb 2/3 )O 3 , MgNb 2 O 6 , InNbO 4 , TiO 2 and PbO for 20 to 30 hours, then pre-burn at 6 to 1300 ° C for 6 to 10 Hour as the starting material for crystal growth;
  • Step 2 Fixing the bottom of the crucible with PMNT (lead magnesium niobate-lead titanate) or PIMNT (lead antimony lead indium niobate-lead magnesium niobate-lead titanate) or its Mn-doped crystal as a seed crystal
  • PMNT magnesium niobate-lead titanate
  • PIMNT lead indium niobate-lead magnesium niobate-lead titanate
  • Mn-doped crystal as a seed crystal
  • the starting material is charged and closed, and the crucible is placed in a crystal growth furnace, and the crystal growth furnace adopts a melting zone width of 10 to 25 mm, and the crucible is used for storing the original material.
  • the diameter is greater than three inches.
  • the ruthenium material is platinum, and the ruthenium has a thickness of 0.6 to 1.5 mm.
  • the seed crystal has a length of 50 to 70 mm, and the seed crystal diameter is less than or equal to the diameter of the grown crystal, and preferably the seed crystal diameter is 30 to 40 mm.
  • the crystallographic direction of the seed crystal is [001].
  • the furnace temperature is controlled at 1350 to 1400 °C.
  • the solid-liquid interface temperature gradient is 50 to 100 ° C / cm.
  • the falling speed is 7.0 to 10. mm/day.
  • the second aspect is also a method for providing high purity Pb(Mn 1/3 Nb 2/3 )O 3 , MgNb 2 O 6 and InNbO 4 as follows:
  • Step a preparing Pb(Mn 1/3 Nb 2/3 )O 3 : mass ratio 1:1 weighs MnO 2 and Nb 2 O 5 , mixes for 20-30 hours, and then in a vacuum atmosphere 900-1000 degrees Celsius The calcination was carried out for 12 to 16 hours to obtain MnNb 2 O 6 .
  • Preparation of Pb(Mn 1/3 Nb 2/3 )O 3 The MnNb 2 O 6 prepared in the step a is ground into a powder, and the MnNb 2 O 6 and PbO are weighed at a molar ratio of 1:5, and mixed 20-30. After an hour, it is pre-fired at 1100 to 1300 ° C for 12 to 16 hours to obtain Pb(Mg 1/3 Nb 2/3 )O 3 .
  • step b MgNb 2 O 6 is prepared: MgO and Nb 2 O 5 are weighed in a molar ratio of 1:1, and after mixing for 20 to 30 hours, calcination is carried out at 900 to 1100 ° C for 12 to 16 hours to obtain MgNb 2 O 6 .
  • Step c preparing InNbO 4 : In 2 O 3 and Nb 2 O 5 are weighed in a molar ratio of 1:1, mixed for 20 to 30 hours, and then calcined at 1100 to 1350 ° C for 10 to 13 hours to obtain InNbO 4 .
  • the inventors of the present application specifically improve that through the step a, the Mn element can exist in the +2 valence state, thereby achieving the purpose of reducing the dielectric properties such as dielectric loss of the material; b, may be such that Mn element occupies a perovskite structure ABO B bit 3 of the material according to the design requirements, to avoid lead and manganese free state of erosion of the crucible material during melting; preparation of starting materials combined step b and step 1 Can avoid free lead and manganese.
  • the raw material is prepared by the synthesis method of the present application, so that the Mn element occupies the B position of the perovskite structure ABO 3 according to the material design requirement, and exists in the +2 valence state, thereby achieving the purpose of reducing the dielectric property loss and the like.
  • the raw material is completely present in the form of a pure perovskite phase, which avoids the erosion of free lead and manganese during the melting of the raw material.
  • the inventors of the present application found that another advantage of selecting a narrow melting zone is that it can increase the temperature gradient of the growth interface, since Mn needs to be bonded to the Mg, Ti, and Nb of the B site. More heat is released, so the narrow melting zone, that is, the large temperature gradient, facilitates the Mn ions to bond to the solid-liquid interface and enter the crystal, thereby avoiding the erosion of the free manganese during the melting of the raw material.
  • the conventional helium-down method growth relaxation ferroelectric crystal adopts the [111] direction seed crystal.
  • This method uses the [001] direction seed crystal growth tetragonal phase relaxation ferroelectric single crystal.
  • the optimal pyroelectric performance direction of the tetragonal phase relaxation ferroelectric single crystal for pyroelectric devices is the [001] direction, and the seed crystal growth in this direction can obtain large wafer uniformity, and the heat of the tetragonal phase large-sized crystal. The application of electricity is necessary.
  • Mn doping to eliminate defects caused by [001] direction growth and improve crystal integrity.
  • crystal growth in the [001] direction is advantageous for obtaining a wafer having uniform performance, point defects are generated to cause blackening of the crystal as compared with the conventional growth in the [111] direction.
  • the Mn doping regulates the dot defect structure in the crystal, inhibits crystal blackening, and improves wafer integrity.
  • FIG. 2 is a schematic view showing the structure of a melting zone of a Mn-doped relaxation ferroelectric single crystal growth furnace
  • Example 3 is a photograph of a three-inch manganese-doped pyroelectric crystal prepared in Example 1;
  • Example 4 is a graph showing the relationship between the dielectric constant ⁇ r of the ⁇ 001> oriented single crystal prepared in Example 1 after the polarization treatment at 1, 10, and 100 kHz, respectively.
  • MnO 2 and Nb 2 O 5 were weighed at a molar ratio of 1:1, and after mixing for 20 hours, they were calcined at 1000 ° C for 12 hours in a vacuum atmosphere (step a).
  • the obtained agglomerated MnNb 2 O 6 was ground into a powder, and MnNb 2 O 6 and PbO were weighed at a molar ratio of 1:5, mixed for 20 hours, and then calcined at 1200 ° C for 15 hours to obtain Pb (Mn 1/3 Nb). 2/3 ) O 3 (step a).
  • MgO and Nb 2 O 5 were weighed in a molar ratio of 1:1, and after mixing for 20 hours, calcination was carried out at 1000 ° C for 15 hours to obtain MgNb 2 O 6 (step b).
  • In 2 O 3 and Nb 2 O 5 were weighed in a molar ratio of 1:1, mixed for 20 hours, and then calcined at 1200 ° C for 12 hours to obtain InNbO 4 (step c).
  • a PMNT crystal having a diameter of 40 mm and a length of 50 mm in the [001] direction is used as a seed crystal, and is placed in a platinum crucible.
  • the crystal growth portion has a crucible diameter of 77 mm and a thickness of 1 mm; and the pre-fired starting material is further used. Load and close the ⁇ . Then, it is placed in a crystal growth furnace as shown in Fig. 2, the furnace temperature is controlled at 1350 to 1400 ° C, and the melting zone width is 15 mm. Crystal growth is achieved by adjusting the inoculation position to a predetermined inoculation temperature and temperature gradient and then starting to fall. The temperature gradient of the solid-liquid interface was controlled to be 60 ° C / cm, and the rate of decline was 0.7 mm / hr. The crystal shown in Figure 3 is finally obtained.
  • Line 4 in Figure 1 represents the valence state of the crystal prepared in Example 1 of the present application
  • lines 1, 2, 3, and 5 are the valence states of the material containing Mn element known in the prior art
  • the line 1 is the absorption edge of Mn in (Sr 0.97 Mn 0.03 )TiO 3
  • lines 2, 3 are absorption edges of Mn in Sr(Ti 0.97 Mn 0.03 )O 3 purchased from different companies
  • line 5 is Pb (Mn 1/2 Mn in Nb 1/2 )O 3
  • Line 4 is the absorption edge of Mn in the Mn-doped relaxed ferroelectric crystal obtained by the present method.
  • the structure of the crystal prepared by the present application is a pure perovskite structure in which the doped Mn is +2 valence and occupies the B site of the perovskite structure ABO 3 .
  • Figure 4 is a graph showing the dielectric constant ⁇ r of a Mn-doped PIMNT 29/29/42 single crystal at a frequency of 0.1 kHz, 1.0 kHz, and 10.0 kHz as a function of temperature.
  • the inner point is 258 degrees Celsius and the crystal is a tetragonal phase crystal.
  • the average dielectric constant of the same film is 240, and the dielectric constant fluctuation of different parts is ⁇ 4.0%, indicating that the crystal has high uniformity.

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  • Inorganic Chemistry (AREA)
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Abstract

Disclosed is a method for preparing a large-size high-homogeneity manganese-doped pyroelectric single crystal. The chemical composition of the manganese-doped pyroelectric single crystal is as follows: Mn-(1-x-y)Pb(In1/2Nb1/2)O3-yPb(Mg1/3Nb2/3)O3-xPbTiO3, wherein x=0.35-0.42, y=0.30-0.45, and 1-x-y=0.20-0.29. The doping amount of Mn is 0-5%. The preparation method for the material is an improved Bridgman method, which comprises raw material synthesis, seed crystal selection, growth process control, defect regulation and control, etc. The present invention overcomes the disadvantages in the prior art that it is difficult to dope the Mn element, the crucible easily leaks, and a defect is easily generated in the [001] direction, and provides an implementation method for the industrial growth of large-size pyroelectric single crystals.

Description

一种热释电单晶的制备方法Method for preparing pyroelectric single crystal 技术领域Technical field
本发明涉及一种大尺寸锰掺杂新型热释电单晶的制备方法,具体说,是涉及一种采用改进的Bridgman法制备大尺寸(直径≥三英寸)锰掺杂铌铟酸铅-铌镁酸铅-钛酸铅三元系热释电单晶的方法,属于晶体生长技术领域。The invention relates to a preparation method of a large-sized manganese-doped novel pyroelectric single crystal, in particular to a method for preparing a large-sized (diameter ≥ three inches) manganese-doped lead indium bismuth-bismuth by a modified Bridgman method. The method of lead magnesium titanate-titanate lead ternary pyroelectric single crystal belongs to the technical field of crystal growth.
技术背景technical background
当今世界各国竞相发展红外探测和成像技术,其应用遍及军事、航天、科研、医疗、工业等众多领域。红外探测器主要分为光子型红外探测器和热型红外探测器两大类。目前常见的光子型红外探测器主要采用以碲镉汞为代表的窄禁带半导体材料和以砷化镓为代表的光电子半导体材料。但半导体红外器件一般需要低温致冷工作,体积大、成本高、功耗大。In the world today, countries are competing to develop infrared detection and imaging technology, which is used in many fields such as military, aerospace, scientific research, medical, industrial and so on. Infrared detectors are mainly divided into photon type infrared detectors and thermal infrared detectors. At present, the common photon-type infrared detector mainly uses a narrow band gap semiconductor material represented by mercury cadmium telluride and an optoelectronic semiconductor material represented by gallium arsenide. However, semiconductor infrared devices generally require low-temperature refrigeration, which is bulky, costly, and consumes a lot of power.
而利用材料热释电效应研制的热释电红外探测器由于其在紫外波段、可见波段、红外波段具有平坦的光谱响应,同时具有无需致冷、功耗低、噪声带宽小、结构紧凑、便于携带、成本低等优点,已经成为当前红外技术领域中最引人瞩目的焦点之一。随着热释电红外探测器向低成本、低功耗及小型化发展,热释电红外探测器正从军用市场向民用市场快速拓展,尤其是在人体探测、火灾预警、气体分析、红外光谱仪以及红外热成像等 领域发挥了重要作用,同时体现了巨大的市场潜力。The pyroelectric infrared detector developed by the pyroelectric effect of the material has a flat spectral response in the ultraviolet, visible and infrared bands, and has no need for refrigeration, low power consumption, low noise bandwidth, compact structure and convenience. The advantages of carrying and low cost have become one of the most eye-catching focuses in the field of infrared technology. With the development of pyroelectric infrared detectors for low cost, low power consumption and miniaturization, pyroelectric infrared detectors are rapidly expanding from the military market to the civilian market, especially in human body detection, fire warning, gas analysis, infrared spectrometers. And infrared thermal imaging, etc. The field plays an important role and at the same time reflects the huge market potential.
目前用于热释电红外探测器的材料主要包括锆钛酸铅(PZT),钛酸锶钡(BST)和钽钪酸铅(PST)等,用于热释电单元探测器件的材料主要局限于钽酸锂(LiTaO3)、硫酸三甘酞(TGS)等。但是,这些传统材料有着热释电系数低、介电损耗大以及物理性能不稳定等缺点,很难满足高性能热释电红外探测器及其延伸产品的应用要求。例如,比较成熟的商用LiTaO3红外探测器的探测率水平仅为1×108cm(Hz)1/2/W至4×108cm(Hz)1/2/W。因此同时克服以上材料的缺点,探索获得高探测优值的新型热释电材料成为目前发展非制冷红外器件的迫切需求。The materials currently used in pyroelectric infrared detectors mainly include lead zirconate titanate (PZT), barium titanate (BST) and lead citrate (PST), etc., and the main limitations of materials for pyroelectric unit detectors. Lithium niobate (LiTaO 3 ), triglyceride sulfate (TGS), and the like. However, these traditional materials have shortcomings such as low pyroelectric coefficient, large dielectric loss, and unstable physical properties, which are difficult to meet the application requirements of high-performance pyroelectric infrared detectors and their extended products. For example, the more mature commercial LiTaO 3 infrared detectors have a detection level of only 1 × 10 8 cm (Hz) 1/2 /W to 4 × 10 8 cm (Hz) 1/2 /W. Therefore, at the same time, overcoming the shortcomings of the above materials, exploring new pyroelectric materials with high detection value has become an urgent need for the development of uncooled infrared devices.
1996年开始,罗豪甦等人率先用布里奇曼(Bridgman)方法成功生长出弛豫铁电单晶(1-x)Pb(Mg1/3Nb2/3)O3–xPbTiO3铌镁钛酸铅(简称PMNT)(专利文献1)以来。自2003年开始,罗豪甦等人又首先发现了PMNT的优异热释电性能,并开展了大量的相关热释电性能优化和材料工艺研究,陆续制备出具有更低损耗的掺锰PMNT单晶及具有更高使用温度的掺锰PIMNT单晶。Beginning in 1996, Luo Haosu and others first succeeded in the growth of relaxed ferroelectric single crystal (1-x)Pb(Mg 1/3 Nb 2/3 )O 3 -xPbTiO 3铌magnesium titanium by Bridgman method. Lead acid (abbreviated as PMNT) (patent document 1). Since 2003, Luo Haosu and others have first discovered the excellent pyroelectric performance of PMNT, and carried out a large number of related pyroelectric performance optimization and material process research, and successively prepared a manganese-doped PMNT single crystal with lower loss and A manganese-doped PIMNT single crystal having a higher use temperature.
但是,通过在现有技术中,使用布里奇曼(Bridgman)方法制备得到的单晶的尺寸均小于2英寸。而出于降低器件成本、探测器设计等因素的考虑,需要越来越多尺寸更大的晶圆。However, by the prior art, the size of the single crystals prepared using the Bridgman method is less than 2 inches. In order to reduce the cost of the device, detector design and other factors, more and more larger wafers are needed.
如前所述,大尺寸晶圆是降低器件成本的重要途径和发展趋势,此外 热释电探测器阵列也对晶片的大小提出了要求。但是尺寸的增大和Mn的加入使得在晶体生长之前,原料需要更加长时间的保温才能熔化,这使得铂金坩埚更容易发生渗漏而导致晶体生长失败。在本领域中,现有的解决方式为增加坩埚厚度,以避免渗漏的发生。As mentioned earlier, large-size wafers are an important way and trend to reduce device costs. Pyroelectric detector arrays also impose requirements on the size of the wafer. However, the increase in size and the addition of Mn make it necessary for the raw material to be melted for a longer period of time before crystal growth, which makes the platinum crucible more likely to leak and cause crystal growth failure. In the art, the existing solution is to increase the thickness of the crucible to avoid the occurrence of leakage.
然而,增加坩埚厚度虽可改善渗漏,但同时带来两个新问题,一是坩埚厚度的增加导致晶体内部的应力加大使得晶体开裂,从而这样的晶体事实上无法后续应用,另外制备成本也大大增加。However, increasing the thickness of the crucible can improve the leakage, but at the same time brings two new problems. First, the increase in the thickness of the crucible causes the internal stress of the crystal to increase, causing the crystal to crack, so that the crystal can not be subsequently applied, and the preparation cost is further Also greatly increased.
故,迄今为止,行业内针对如何提高掺Mn热释电单晶尺寸这一技术问题,尚未有适宜工业应用的解决方法。Therefore, so far, there is no suitable solution for industrial application in the industry for how to improve the size of the Mn pyroelectric single crystal.
专利文献:Patent literature:
专利文献1:中国专利CN 1080777C;Patent Document 1: Chinese patent CN 1080777C;
发明概要Summary of invention
本发明的提供一种采用改进的Bridgman法制备的大尺寸掺锰热释电单晶,以解决现有技术中的大尺寸掺Mn热释电单晶难以批量生长的缺陷。The present invention provides a large-sized manganese-doped pyroelectric single crystal prepared by the modified Bridgman method to solve the defects in the prior art that large-sized Mn-doped pyroelectric single crystals are difficult to grow in batches.
适用于本发明提供方法的单晶体的化学组成为:Mn-(1-x-y)Pb(In1/2Nb1/2)O3-yPb(Mg1/3Nb2/3)O3-xPbTiO3,其中x=0.35~0.42,y=0.30~0.45,1-x-y=0.20~0.29,Mn的掺杂量为摩尔百分比0~5.0%。The chemical composition of a single crystal suitable for use in the method of the present invention is: Mn-(1-xy)Pb(In 1/2 Nb 1/2 )O 3 -yPb(Mg 1/3 Nb 2/3 )O 3 -xPbTiO 3 Wherein x = 0.35 to 0.42, y = 0.30 to 0.45, 1-xy = 0.20 to 0.29, and the doping amount of Mn is 0 to 5.0% by mole.
本发明的一方面,在于提供一种单晶的制备方法,是一种改进的 Bridgman法,包括如下具体步骤:An aspect of the present invention provides a method for preparing a single crystal, which is an improved method. The Bridgman method includes the following specific steps:
步骤1:取得高纯度的Pb(Mn1/3Nb2/3)O3、MgNb2O6、InNbO4、TiO2、PbO混合20~30小时后,在1100~1300摄氏度预烧6~10小时作为晶体生长的起始物料;Step 1: Obtain high-purity Pb(Mn 1/3 Nb 2/3 )O 3 , MgNb 2 O 6 , InNbO 4 , TiO 2 and PbO for 20 to 30 hours, then pre-burn at 6 to 1300 ° C for 6 to 10 Hour as the starting material for crystal growth;
步骤2:以PMNT(铌镁酸铅-钛酸铅)或PIMNT(铌铟酸铅-铌镁酸铅-钛酸铅)或其Mn掺杂晶体作为籽晶固定于坩埚底部,再将所述起始物料装入并封闭坩埚,并将所述坩埚放入晶体生长炉中,且所述晶体生长炉采的熔区宽度10~25毫米,且所述坩埚中用于存放所述原始物料处的直径大于三英寸。Step 2: Fixing the bottom of the crucible with PMNT (lead magnesium niobate-lead titanate) or PIMNT (lead antimony lead indium niobate-lead magnesium niobate-lead titanate) or its Mn-doped crystal as a seed crystal The starting material is charged and closed, and the crucible is placed in a crystal growth furnace, and the crystal growth furnace adopts a melting zone width of 10 to 25 mm, and the crucible is used for storing the original material. The diameter is greater than three inches.
其中,坩埚材料为铂金,坩埚厚度0.6~1.5毫米。Among them, the ruthenium material is platinum, and the ruthenium has a thickness of 0.6 to 1.5 mm.
其中,所述籽晶长度为50~70毫米,籽晶直径小于或等于生长晶体的直径,优选籽晶直径为30~40毫米。Wherein, the seed crystal has a length of 50 to 70 mm, and the seed crystal diameter is less than or equal to the diameter of the grown crystal, and preferably the seed crystal diameter is 30 to 40 mm.
其中,当所述晶体的晶体结构为四方相时,所述籽晶的晶体学方向为[001]。Wherein, when the crystal structure of the crystal is a tetragonal phase, the crystallographic direction of the seed crystal is [001].
其中,所述炉温控制在1350~1400℃。Wherein, the furnace temperature is controlled at 1350 to 1400 °C.
其中,所述固液界面温度梯度为50~100℃/cm。Wherein, the solid-liquid interface temperature gradient is 50 to 100 ° C / cm.
其中,所述下降速度为7.0~10.毫米/天。 Wherein, the falling speed is 7.0 to 10. mm/day.
其中,为了保证晶体的生长,Pb(Mn1/3Nb2/3)O3、MgNb2O6、Pb(Mn1/3Nb2/3)O6、TiO2、PbO的纯度要求是必须的。一般而言,其纯度需达到99.99%。Among them, in order to ensure the growth of crystals, the purity requirements of Pb(Mn 1/3 Nb 2/3 )O 3 , MgNb 2 O 6 , Pb(Mn 1/3 Nb 2/3 )O 6 , TiO 2 and PbO are necessary. of. In general, its purity needs to reach 99.99%.
对于TiO2、PbO一般市售可得,而对于Pb(Mn1/3Nb2/3)O3、MgNb2O6以及InNbO4,由于在市场上并未成熟的制备工艺,故本申请的第二方面,还在于一种提供高纯度Pb(Mn1/3Nb2/3)O3、MgNb2O6以及InNbO4的方法,具体如下:For TiO 2 , PbO is generally commercially available, and for Pb(Mn 1/3 Nb 2/3 )O 3 , MgNb 2 O 6 and InNbO 4 , due to the unprepared preparation process on the market, the present application The second aspect is also a method for providing high purity Pb(Mn 1/3 Nb 2/3 )O 3 , MgNb 2 O 6 and InNbO 4 as follows:
步骤a,制备Pb(Mn1/3Nb2/3)O3:按摩尔比1:1称取MnO2和Nb2O5,混合20~30小时后,再在真空气氛下900~1000摄氏度预烧12~16小时得到MnNb2O6Step a, preparing Pb(Mn 1/3 Nb 2/3 )O 3 : mass ratio 1:1 weighs MnO 2 and Nb 2 O 5 , mixes for 20-30 hours, and then in a vacuum atmosphere 900-1000 degrees Celsius The calcination was carried out for 12 to 16 hours to obtain MnNb 2 O 6 .
Figure PCTCN2015071798-appb-000001
Figure PCTCN2015071798-appb-000001
制备Pb(Mn1/3Nb2/3)O3:将步骤a中制备得到的MnNb2O6研磨成粉,再按摩尔比1:5称取MnNb2O6和PbO,混合20~30小时,然后在1100~1300摄氏度预烧12~16小时得到Pb(Mg1/3Nb2/3)O3Preparation of Pb(Mn 1/3 Nb 2/3 )O 3 : The MnNb 2 O 6 prepared in the step a is ground into a powder, and the MnNb 2 O 6 and PbO are weighed at a molar ratio of 1:5, and mixed 20-30. After an hour, it is pre-fired at 1100 to 1300 ° C for 12 to 16 hours to obtain Pb(Mg 1/3 Nb 2/3 )O 3 .
Figure PCTCN2015071798-appb-000002
Figure PCTCN2015071798-appb-000002
步骤b,制备MgNb2O6:按摩尔比1:1称取MgO和Nb2O5,混合20~30小时后,再在900~1100摄氏度预烧12~16小时得到MgNb2O6In step b, MgNb 2 O 6 is prepared: MgO and Nb 2 O 5 are weighed in a molar ratio of 1:1, and after mixing for 20 to 30 hours, calcination is carried out at 900 to 1100 ° C for 12 to 16 hours to obtain MgNb 2 O 6 .
步骤c,制备InNbO4:按摩尔比1:1称取In2O3和Nb2O5,混合20~30小时后再在1100~1350摄氏度预烧10~13小时得到InNbO4Step c, preparing InNbO 4 : In 2 O 3 and Nb 2 O 5 are weighed in a molar ratio of 1:1, mixed for 20 to 30 hours, and then calcined at 1100 to 1350 ° C for 10 to 13 hours to obtain InNbO 4 .
在以上这一制备方法中,本申请的发明人具体做出的改进有:通过步骤a,可使得Mn元素以+2价状态存在,从而达到降低材料介电损耗等性能调控的目的;通过步骤b,可使得Mn元素按照材料设计要求占据钙钛矿结构ABO3的B位,避免了游离态的铅和锰在原料熔化过程中对坩埚的侵蚀;结合步骤b以及步骤1中起始物料的制备,可以避免游离态的铅和锰。In the above preparation method, the inventors of the present application specifically improve that through the step a, the Mn element can exist in the +2 valence state, thereby achieving the purpose of reducing the dielectric properties such as dielectric loss of the material; b, may be such that Mn element occupies a perovskite structure ABO B bit 3 of the material according to the design requirements, to avoid lead and manganese free state of erosion of the crucible material during melting; preparation of starting materials combined step b and step 1 Can avoid free lead and manganese.
与现有技术相比,本发明的改进之外在于:The improvement of the present invention is in addition to the prior art:
1)采用本申请的合成法制备原料,使得Mn元素按照材料设计要求占据钙钛矿结构ABO3的B位,并且以+2价状态存在,从而达到降低材料介电损耗等性能调控的目的。此外,使得原料完全以纯钙钛矿相的形式存在,避免了游离态的铅和锰在原料熔化过程中对坩埚的侵蚀。1) The raw material is prepared by the synthesis method of the present application, so that the Mn element occupies the B position of the perovskite structure ABO 3 according to the material design requirement, and exists in the +2 valence state, thereby achieving the purpose of reducing the dielectric property loss and the like. In addition, the raw material is completely present in the form of a pure perovskite phase, which avoids the erosion of free lead and manganese during the melting of the raw material.
2)不同于现有技术中增大坩埚厚度以防止渗漏,从而达成生长尺寸提高的方法。本申请的发明人选择窄熔区,以实现增大晶体尺寸的效果。本申请的发明人发现,将熔区宽度设置为10~25毫米,可既防止渗漏,又可获得大尺寸晶体所需温度梯度从而达到提高晶体尺寸的效果。2) Different from the prior art method of increasing the thickness of the crucible to prevent leakage, thereby achieving an increase in growth size. The inventors of the present application selected a narrow melting zone to achieve the effect of increasing the crystal size. The inventors of the present application have found that setting the width of the melt zone to 10 to 25 mm can prevent leakage and obtain a temperature gradient required for a large-sized crystal to achieve an effect of increasing the crystal size.
3)同时,本申请的发明人发现,选择窄熔区的另一优势在于,其可使得生长界面温度梯度增加,由于Mn相对于B位的Mg、Ti、Nb成键需 放出更多热量,所以窄熔区即大的温度梯度有利于Mn离子成键于固液界面而进入晶体,避免了游离态的锰在原料熔化过程中对坩埚的侵蚀。3) At the same time, the inventors of the present application found that another advantage of selecting a narrow melting zone is that it can increase the temperature gradient of the growth interface, since Mn needs to be bonded to the Mg, Ti, and Nb of the B site. More heat is released, so the narrow melting zone, that is, the large temperature gradient, facilitates the Mn ions to bond to the solid-liquid interface and enter the crystal, thereby avoiding the erosion of the free manganese during the melting of the raw material.
4)传统的坩埚下降法生长弛豫铁电晶体采用[111]方向籽晶,本方法采用[001]方向籽晶生长四方相弛豫铁电单晶。热释电器件用的四方相弛豫铁电单晶的最优热释电性能方向是[001]方向,采用此方向籽晶生长能够获得大的晶片均匀性,对于四方相大尺寸晶体的热释电应用是必要的。4) The conventional helium-down method growth relaxation ferroelectric crystal adopts the [111] direction seed crystal. This method uses the [001] direction seed crystal growth tetragonal phase relaxation ferroelectric single crystal. The optimal pyroelectric performance direction of the tetragonal phase relaxation ferroelectric single crystal for pyroelectric devices is the [001] direction, and the seed crystal growth in this direction can obtain large wafer uniformity, and the heat of the tetragonal phase large-sized crystal. The application of electricity is necessary.
5)利用Mn掺杂消除[001]方向生长带来的缺陷,提高晶体完整性。虽然[001]方向生长晶体有利于获得性能均匀的晶片,但是与传统沿[111]方向生长相比,会产生点缺陷,使晶体发黑。通过Mn掺杂调控了晶体中点缺陷结构,抑制了晶体发黑,提高了晶片完整性。5) Use Mn doping to eliminate defects caused by [001] direction growth and improve crystal integrity. Although crystal growth in the [001] direction is advantageous for obtaining a wafer having uniform performance, point defects are generated to cause blackening of the crystal as compared with the conventional growth in the [111] direction. The Mn doping regulates the dot defect structure in the crystal, inhibits crystal blackening, and improves wafer integrity.
附图说明DRAWINGS
图1是Mn掺杂的弛豫铁电单晶中Mn元素的吸收边,从而表示同步辐射X射线吸收谱测量Mn掺杂PMNT单晶中Mn的价态;1 is an absorption edge of Mn element in a Mn-doped relaxed ferroelectric single crystal, thereby indicating a synchrotron radiation X-ray absorption spectrum for measuring a valence state of Mn in a Mn-doped PMNT single crystal;
图2是Mn掺杂的弛豫铁电单晶生长炉熔区结构示意图;2 is a schematic view showing the structure of a melting zone of a Mn-doped relaxation ferroelectric single crystal growth furnace;
图3是实施例1制备出的三英寸掺锰热释电晶体照片;3 is a photograph of a three-inch manganese-doped pyroelectric crystal prepared in Example 1;
图4是实施例1制备的<001>取向的单晶在极化处理后的介电常数εr分别在1、10、100kHz下随温度变化的关系曲线。 4 is a graph showing the relationship between the dielectric constant ε r of the <001> oriented single crystal prepared in Example 1 after the polarization treatment at 1, 10, and 100 kHz, respectively.
发明内容Summary of the invention
实施例1:Example 1:
按摩尔比1:1称取MnO2和Nb2O5,混合20小时后,在真空气氛下1000摄氏度预烧12小时(步骤a)。将获得的结块的MnNb2O6研磨成粉,再按摩尔比1:5称取MnNb2O6和PbO,混合20小时,然后在1200摄氏度预烧15小时得到Pb(Mn1/3Nb2/3)O3(步骤a)。按摩尔比1:1称取MgO和Nb2O5,混合20小时后,再在1000摄氏度预烧15小时得到MgNb2O6(步骤b)。按摩尔比1:1称取In2O3和Nb2O5,混合20小时后,再在1200摄氏度预烧12小时得到InNbO4(步骤c)。最后,按照Mn-(1-x-y)Pb(In1/2Nb1/2)O3-yPb(Mg1/3Nb2/3)O3-xPbTiO3,其中x=0.42,y=0.29,1-x-y=0.29,Mn的掺杂量的摩尔百分比为1.0%的化学式将MgNb2O6、InNbO4、PbO、TiO2和Pb(Mn1/3Nb2/3)O3混合24小时后1100度预烧10小时作为晶体生长的起始物料。MnO 2 and Nb 2 O 5 were weighed at a molar ratio of 1:1, and after mixing for 20 hours, they were calcined at 1000 ° C for 12 hours in a vacuum atmosphere (step a). The obtained agglomerated MnNb 2 O 6 was ground into a powder, and MnNb 2 O 6 and PbO were weighed at a molar ratio of 1:5, mixed for 20 hours, and then calcined at 1200 ° C for 15 hours to obtain Pb (Mn 1/3 Nb). 2/3 ) O 3 (step a). MgO and Nb 2 O 5 were weighed in a molar ratio of 1:1, and after mixing for 20 hours, calcination was carried out at 1000 ° C for 15 hours to obtain MgNb 2 O 6 (step b). In 2 O 3 and Nb 2 O 5 were weighed in a molar ratio of 1:1, mixed for 20 hours, and then calcined at 1200 ° C for 12 hours to obtain InNbO 4 (step c). Finally, according to Mn-(1-xy)Pb(In 1/2 Nb 1/2 )O 3 -yPb(Mg 1/3 Nb 2/3 )O 3 -xPbTiO 3 , where x=0.42, y=0.29, 1-xy=0.29, a chemical formula of Mn doping amount of 1.0% is mixed with MgNb 2 O 6 , InNbO 4 , PbO, TiO 2 and Pb(Mn 1/3 Nb 2/3 )O 3 for 24 hours. It was calcined at 1100 degrees for 10 hours as a starting material for crystal growth.
以[001]方向的直径为40毫米、长度为50毫米的PMNT晶体作为籽晶,置于铂金坩埚中,晶体生长部分的坩埚直径77毫米,厚度1毫米;再将预烧好的起始物料装入并封闭坩埚。然后放入如图2所示的晶体生长炉中,炉温控制在1350~1400℃,熔区宽度为15毫米。调节接种位置达到预定的接种温度和温度梯度后开始下降实现晶体生长。控制固液界面温度梯度为60℃/cm,下降速率为0.7mm/hr。最终获得如图3所示晶体。 A PMNT crystal having a diameter of 40 mm and a length of 50 mm in the [001] direction is used as a seed crystal, and is placed in a platinum crucible. The crystal growth portion has a crucible diameter of 77 mm and a thickness of 1 mm; and the pre-fired starting material is further used. Load and close the 坩埚. Then, it is placed in a crystal growth furnace as shown in Fig. 2, the furnace temperature is controlled at 1350 to 1400 ° C, and the melting zone width is 15 mm. Crystal growth is achieved by adjusting the inoculation position to a predetermined inoculation temperature and temperature gradient and then starting to fall. The temperature gradient of the solid-liquid interface was controlled to be 60 ° C / cm, and the rate of decline was 0.7 mm / hr. The crystal shown in Figure 3 is finally obtained.
图1中的线条4,代表本申请实施例1制备得到的晶体的价态,而线条1、2、3、5则是现有技术中已知的含有Mn元素的材料的价态,其中线条1是(Sr0.97Mn0.03)TiO3中Mn的吸收边,线条2,3是购买自不同公司的Sr(Ti0.97Mn0.03)O3中Mn的吸收边,线条5是Pb(Mn1/2Nb1/2)O3中的Mn。线条4是本方法得到的Mn掺杂弛豫铁电晶体中Mn的吸收边。从图1中可知,本申请所制备得到的晶体的结构是纯的钙钛矿结构,其中掺杂的Mn为+2价,占据钙钛矿结构ABO3的B位。 Line 4 in Figure 1 represents the valence state of the crystal prepared in Example 1 of the present application, and lines 1, 2, 3, and 5 are the valence states of the material containing Mn element known in the prior art, wherein the line 1 is the absorption edge of Mn in (Sr 0.97 Mn 0.03 )TiO 3 , lines 2, 3 are absorption edges of Mn in Sr(Ti 0.97 Mn 0.03 )O 3 purchased from different companies, and line 5 is Pb (Mn 1/2 Mn in Nb 1/2 )O 3 . Line 4 is the absorption edge of Mn in the Mn-doped relaxed ferroelectric crystal obtained by the present method. As can be seen from FIG. 1, the structure of the crystal prepared by the present application is a pure perovskite structure in which the doped Mn is +2 valence and occupies the B site of the perovskite structure ABO 3 .
图4为极化处理后的Mn掺杂PIMNT 29/29/42单晶在0.1kHz、1.0kHz、10.0kHz三个频率下介电常数εr在随温度变化曲线,由图可以得到晶体的居里点为258摄氏度,显示晶体为四方相晶体。由同一个片子的平均介电常数为240,不同部位的介电常数波动<4.0%,表明晶体具有较高的均匀性。 Figure 4 is a graph showing the dielectric constant ε r of a Mn-doped PIMNT 29/29/42 single crystal at a frequency of 0.1 kHz, 1.0 kHz, and 10.0 kHz as a function of temperature. The inner point is 258 degrees Celsius and the crystal is a tetragonal phase crystal. The average dielectric constant of the same film is 240, and the dielectric constant fluctuation of different parts is <4.0%, indicating that the crystal has high uniformity.

Claims (9)

  1. 一种热释电单晶的制备方法,所述单晶的化学组成为:A method for preparing a pyroelectric single crystal, wherein the chemical composition of the single crystal is:
    Mn-(1-x-y)Pb(In1/2Nb1/2)O3-yPb(Mg1/3Nb2/3)O3-xPbTiO3,其中x=0.35~0.42,y=0.30~0.45,1-x-y=0.20~0.29,Mn的掺杂量的摩尔百分比为0~5.0%,其特征在于,所述方法包括:Mn-(1-xy)Pb(In 1/2 Nb 1/2 )O 3 -yPb(Mg 1/3 Nb 2/3 )O 3 -xPbTiO 3 , where x=0.35~0.42, y=0.30~0.45 , 1-xy=0.20-0.29, the molar percentage of the doping amount of Mn is 0-5.0%, characterized in that the method comprises:
    步骤1:获得高纯度的Pb(Mn1/3Nb2/3)O3、MgNb2O6、InNbO4、TiO2、PbO,混合20~30小时后,在1100~1300摄氏度预烧6~10小时作为晶体生长的起始物料;Step 1: Obtain high purity Pb(Mn 1/3 Nb 2/3 )O 3 , MgNb 2 O 6 , InNbO 4 , TiO 2 , PbO, mix for 20 to 30 hours, and pre-fire at 1100 to 1300 ° C for 6~ 10 hours as the starting material for crystal growth;
    步骤2:以PMNT或PIMNT或其Mn掺杂晶体作为籽晶固定于坩埚底部,再将所述起始物料装入并封闭坩埚,并将所述坩埚放入晶体生长炉中,其特征在于,所述晶体生长的熔区宽度为10~25毫米,且所述坩埚中用于存放所述原始物料处的直径大于等于三英寸。Step 2: Fixing the PMNT or PIMNT or its Mn-doped crystal as a seed crystal to the bottom of the crucible, loading and closing the crucible, and placing the crucible into a crystal growth furnace, wherein The crystal growth has a melt zone width of 10 to 25 mm, and the diameter of the crucible for storing the original material is greater than or equal to three inches.
  2. 如权利要求1所述的制备方法,其中,The production method according to claim 1, wherein
    所述高纯度的Pb(Mn1/3Nb2/3)O3、MgNb2O6、InNbO4、TiO2、PbO的纯度为99.99%。The purity of the high-purity Pb(Mn 1/3 Nb 2/3 )O 3 , MgNb 2 O 6 , InNbO 4 , TiO 2 , and PbO was 99.99%.
  3. 如权利要求1所述的制备方法,其中,The production method according to claim 1, wherein
    其中所述步骤1中取得高纯度的Pb(Mn1/3Nb2/3)O3、MgNb2O6、InNbO4的方法分为如下步骤:The method for obtaining high-purity Pb(Mn 1/3 Nb 2/3 )O 3 , MgNb 2 O 6 , and InNbO 4 in the step 1 is divided into the following steps:
    步骤a,制备Pb(Mn1/3Nb2/3)O3:按摩尔比1:1称取MnO2和Nb2O5,混 合20~30小时后,再在真空气氛下900~1000摄氏度预烧12~16小时得到MnNb2O6。然后制备Pb(Mn1/3Nb2/3)O3,将以上制备得到的MnNb2O6研磨成粉,再按摩尔比1:5~6称取MnNb2O6和PbO,混合20~30小时,然后在1100~1300摄氏度预烧12~16小时得到Pb(Mn1/3Nb2/3)O3Step a, preparing Pb(Mn 1/3 Nb 2/3 )O 3 : mass ratio 1:1 weighs MnO 2 and Nb 2 O 5 , mixes for 20-30 hours, and then in a vacuum atmosphere 900-1000 degrees Celsius The calcination was carried out for 12 to 16 hours to obtain MnNb 2 O 6 . Then, Pb(Mn 1/3 Nb 2/3 )O 3 is prepared, and the MnNb 2 O 6 prepared above is ground into a powder, and then MnNb 2 O 6 and PbO are weighed by a molar ratio of 1:5 to 6, and mixed 20~. After 30 hours, it was pre-fired at 1100 to 1300 ° C for 12 to 16 hours to obtain Pb(Mn 1/3 Nb 2/3 )O 3 .
    步骤b,制备MgNb2O6:按摩尔比1:1称取MgO和Nb2O5,混合20~30小时后,再在900~1100摄氏度预烧12~16小时得到MgNb2O6In step b, MgNb 2 O 6 is prepared: MgO and Nb 2 O 5 are weighed in a molar ratio of 1:1, and after mixing for 20 to 30 hours, calcination is carried out at 900 to 1100 ° C for 12 to 16 hours to obtain MgNb 2 O 6 .
    步骤c,制备InNbO4:按摩尔比1:1称取In2O3和Nb2O5,混合20~30小时后再在1100~1350摄氏度预烧10~13小时得到InNbO4Step c, preparing InNbO 4 : In 2 O 3 and Nb 2 O 5 are weighed in a molar ratio of 1:1, mixed for 20 to 30 hours, and then calcined at 1100 to 1350 ° C for 10 to 13 hours to obtain InNbO 4 .
  4. 如权利要求1所述的方法,其中,所述坩埚材料为铂金,坩埚总厚度为0.6~1.5毫米。The method of claim 1 wherein said niobium material is platinum and the total thickness of tantalum is from 0.6 to 1.5 mm.
  5. 如权利要求1所述的方法,其中,所述籽晶长度为50~70毫米,籽晶直径小于或等于生长晶体的直径,优选为30~40毫米。The method of claim 1, wherein the seed crystal has a length of 50 to 70 mm and the seed crystal diameter is less than or equal to the diameter of the grown crystal, preferably 30 to 40 mm.
  6. 如权利要求1所述的方法,其中,当所述晶体的晶体结构为四方相时,所述籽晶的晶体学方向为[001]。The method according to claim 1, wherein when the crystal structure of the crystal is a tetragonal phase, the crystallographic direction of the seed crystal is [001].
  7. 如权利要求1所述的方法,其中,所述炉温控制在1350~1400摄氏度。The method of claim 1 wherein said furnace temperature is controlled between 1350 and 1400 degrees Celsius.
  8. 如权利要求1所述的方法,其中,所述固液界面温度梯度为50~100℃/cm。 The method of claim 1 wherein said solid-liquid interface temperature gradient is from 50 to 100 ° C/cm.
  9. 如权利要求1所述的方法,其中,所述下降速度为7.0~10.0毫米/天。 The method of claim 1 wherein said descending speed is from 7.0 to 10.0 mm/day.
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