999精品在线视频,手机成人午夜在线视频,久久不卡国产精品无码,中日无码在线观看,成人av手机在线观看,日韩精品亚洲一区中文字幕,亚洲av无码人妻,四虎国产在线观看 ?

CaTiO3∶Zn溶膠-凝膠法制備、結構及介電性能

2012-11-09 09:16:28黃萬群張啟龍申乾宏
無機化學學報 2012年11期

黃萬群 張啟龍 楊 輝 申乾宏

CaTiO3∶Zn溶膠-凝膠法制備、結構及介電性能

黃萬群 張啟龍*楊 輝 申乾宏

(浙江大學材料科學與工程學系,杭州 310027)

采用溶膠-凝膠法制備了CaTiO3∶Zn納米粒子,透射電鏡圖顯示平均粒徑為25 nm。Zn的摻雜位置對于陶瓷相組成和燒結特性有很大影響。Ca1-xZnxTiO3和CaTiO3+zZnO樣品的Zn以Zn2TiO4相形式存在;而CaZnyTi1-yO3-δ(y=0.01)樣品中的Zn進入Ti位形成固溶體,無明顯的降溫效果,當Zn量增至0.05和0.1時,出現ZnO相。ZnO和Zn2TiO4第二相的存在均能明顯促進陶瓷燒結。CaTiO3∶Zn超細粉體可在較低溫度下致密燒結(≤1 250℃)。1 250℃燒結的CaZnyTi1-yO3-δ(y=0.01)陶瓷具有較好的介電性能:介電常數 ε=157,品質因數 Q×f=6 819 GHz,諧振頻率溫度系數 τf=7.51×10-4℃-1。

CaTiO3:Zn;溶膠-凝膠法;納米粉體;介電性能

0 Introduction

The development of microwave dielectric ceramics resonators for communication systems such as cellular telephones and global positioning systems has been rapidly growing in the past decades[1].In order to reduce circuit/device size,many microwave ceramics with high dielectric constant (εr)such as Ca0.6La0.267TiO3,BaONd2O3-TiO2,CaO-Nd2O3-TiO2and BaO-Gd2O3-TiO2[2-8],have been studied.CaTiO3material is usually used as compensators of the temperature coefficient of resonant frequency(τf)due to its high εr(~170)and large τf(~8×10-4℃-1)[9-13].However,the sintering temperature of pure CaTiO3is very high (≥1 400 ℃)and it has relativelylow Q×f value (~3500 GHz)by the traditional solidstate preparation process.

Sol-gel method has been used for the fabrication of microwave ceramic materials with improved compositional homogeneity, lower densification temperatures,and better dielectric properties[14-17].To the best of our knowledge,there has been no report on the preparation and dielectric properties of CaTiO3∶Zn nanoparticles.

In this work,Zn was introduced into CaTiO3(CT)ceramic as a substitution of A site,B site and as sintering additive with the stoichiometry of Ca1-xZnxTiO3(ZCT),CaZnyTi1-yO3-y(CZT)and CaTiO3+zZnO(CTZ).Well dispersed powders were synthesized by sol-gel method.The effect of the Zn substitution site on sintering temperature and dielectric property was investigated.The sintering temperature was decreased and the Q×f value was improved due to the effect of nano-sized particles and the addition of Zn.

1 Experimental

Powders were sy nthesized by a sol-gel method,using calcium nitrate[Ca(NO3)2·4H2O,99.9%],zinc nitrate[Zn(NO3)2·6H2O,99.9%]and tetrabutyl titanium[Ti(C4H9O)4,99%]as raw materials according to the d esiredstoichiometry:CaTiO3,Ca1-xZnxTiO3,CaZnyTi1-yO3-δ,CaTiO3+zZnO (x=y=z=0.01,0.05,0.1, δ presents oxygen vacancy concentration).Ethanol was used as solvent,PEG1000 was added so as to account for 2wt%of the total solution and nitric acid was used to adjust the pH value to about 4.After 1 h stirring,the light yellow solution became viscous sol.The sol was aged for 10 h until it turned completely a gel.The gel was dried and then treated at 500~800 ℃ for 2 h to get the powder.Then the powder was milled by planetmilling and dried.After that,5wt% of Polyvinyl Alcohol(PVA)was added,and the samples were then pressed into disks under about 80 MPa pressure.The disks were sintered at a temperature ranging from 1 100 to 1 300℃.

Thermal analysis for the dried gel was carried out using a TG-DTA analyzer (German Netzsch Co.STA449C)from room temperature to 1 000℃in air at a heating rate of 10 ℃·min-1.Crystal phases of the nanoparticlesand ceramicswere investigated by Shimadzu XRD-6000 X-raydiffractometerwith a graphite diffracted-beam monochromator for Cu-Kα radiation(λ=0.154 18 nm)at 40 kV and 40 mA,using 0.15 mm receiving slit and scintillation counter as the detector.The 2θ region was in the range of 10°~70°with a step of 0.02°and a scanning speed of 4°·min-1.Transmission electron microscopy (TEM)images were performed on JEM-1230 TEM with an acceleration voltage of 200 kV.Scanning electron microscopy(SEM)was performed on HitachiS4800 SEM atan accelerating voltage of 5 kV.Dielectric constant(εr)and quality factor value(Q×f)at microwave frequency were measured using Hakki-Coleman method and cavity method by vector network analysis (Agilent 8719ET,USA),respectively.

2 Results and discussion

Fig.1 shows the TG and DTA curves of the CaZnyTi1-yO3-δ(y=0.01)xerogel.The appearance of endothermic peaks at 130℃,associated with weight loss between 30 and 150℃in the TG curve is possibly due to the evaporation of residual water and organics absorbed on the surface of the xerogel.A sharp exothermic peak at 160℃accompanied by a sharp weightlossisobserved in theTG curve.This corresponds to the combustion of the xerogel.In this process,it is concluded that decomposition of butoxy,PEG400 and nitrate acid produces a lot of oxygen.The oxygen could accelerate the combustion process and generate a great amount of heat.The second exothermic peak at about 370℃is attributed to the combustion of remaining organics.The endothermic peak at 620 ℃associated with a weight loss of 20%might be due to the decomposition of NO3-.A small endothermic peak appeared at 730℃accompanied with a weight loss of 5%is assigned to the decomposition of CaCO3,which is demonstrated by the analysis of XRD in Fig.2.

XRD patterns of the CaZnyTi1-yO3-δ(y=0.01)xerogel calcined at 500~800 ℃ for 2 h are illustrated in Fig.2.Fig.2(a)shows the presence of orthorhombic perovskite CaTiO3phase as the major phase,along with small peaks corresponding to CaCO3and Ca2Ti2O6.With increasing the temperature from 500℃ to 700℃,the diffraction intensities of CaTiO3and Ca2Ti2O6increase,but the diffraction intensities of CaCO3gradually decrease.At 800 ℃ ,CaCO3and Ca2Ti2O6nearly disappear while intense peaks of CaO appear along with small peaks of Ca2Zn4Ti15O36.Complex reactions happen in this stage including the decomposing of CaCO3,Ca2Ti2O6,and the forming of Ca2Zn4Ti15O36:[18-19]

TEM shows that all the samples have similar particle size and shapes.Fig.3 shows the transmission electron micrograph (TEM)of the CaZnyTi1-yO3-δ(y=0.01)xerogel calcined at 500 ℃ for 2 h.It can be seen that the most probable particle size is about 20~30 nm.

Fig.4 illustratesXRD patternsforceramics prepared by nanopowders.Single phase CaTiO3with orthorhombic space group Pmna is obtained in the undoped sample.Except for the orthorhombic perovskite CaTiO3phase as the major phase,the Zn2TiO4phase is formed in the ZCT and CTZ samples,however,a small diffraction peaks from ZnO can be identified in the CZT sample (y≥0.05).There is no evidence of any secondary phases in CaZnyTi1-yO3-δ(y=0.01).

Table 1 shows the unit cell parameters of sintered ceramics.There are no obvious changes on the unit cells of Ca1-xZnxTiO3and CaTiO3+zZnO (x=z=0.05),compared with the pure CaTiO3.However,for CaZnyTi1-yO3-δ,the lattice parameters,especially c and the unit cell volume,show a small increase and there issome indication that the maximum values are obtained at y=0.01.It is clear that a solid solution forms,therefore;possibly the solid solution limit is at y=0.01,which agrees with the reference[20].From the size consideration,it is assumed that Zn substitutes for Ti associated with oxygen vacancies for charge compensation.It also indicates that,for ZCT and CTZ,the ZnO does not obviously substitute for A site or other site,the reaction between the ZnO and TiO2forms the Zn2TiO4phase,which is demonstrated by the analysis of XRD in Fig.4(b)and(d).

Table 1 Unit cell parameters calculated from the XRD

Fig.5 showsthe XRD patternsofceramics CaZnyTi1-yO3-δ(y=0.01)sintered at the different temperatures.Thereisno obviousphase change with increasing the sintering temperature.SEM micrographs of dense CaTiO3∶Zn ceramics are shown in Fig.6(a)~(d).CaZnyTi1-yO3-δ(y=0.01)specimens sintered at 1 150 ℃are not completely dense and a small amount of porosity can be observed (SEM is not shown here).At 1 250 ℃,well-sintered dense ceramics are obtained;the grain size is increased with increasing the sintering temperature.However too high sintering temperature causes the abnormal grain growth,samples sintered at 1 300℃has abnormal grain growth,and parts of the abnormal grain size are larger than 4 μm (SEM is not shown here).Dense ceramics are also obtained for ZnxCa1-xTiO3(x=0.01)and CaTiO3+zZnO (z=0.01)ceramics.However,pure CaTiO3ceramics sintered at 1 250℃is not as dense;pores are obvious as seen from Fig.6(a).It indicates that the dense temperature of ZCT,CZT,and CTZ,is about 1 150℃,1250℃and 1150℃,respectively.The sintering temperature of pure CaTiO3ceramics synthesized by the solid-state reaction method is higher than 1 400℃.In contrast to that,the CaTiO3and CaTiO3∶Zn nanopowders synthesized by the sol-gel method could be densified at lower than 1 250℃.The result indicates that the nanoparticles with high ratio of specific surface area and surface energy contribute to promotethesinteringpropertiesand reduce the sintering temperature.Moreover,the CaTiO3∶Zn has a lower dense temperature than pure CaTiO3.For the ZCT and CTZ ceramics,the added Zn acts as sintering aid,melting at a relatively lower temperature and forms the Zn2TiO4.Zn2TiO4could be sintered at temperatures lower than 1 000℃[21-23],which further improves the sintering characterization.

Table 2 illustrates the dielectric properties of ceramics.For all the samples,the εrachieves the maximum value at the highest relative densities.The εrof CaTiO3doped with Zn is lower than that of pure CaTiO3,and decreases with increasing the Zn content,which is due to the appearance of Zn2TiO4or ZnO with lower εrvalue (≤30)[24-26].Although the Zn2TiO4exhibits a relatively high Q×f value,the ZCT ceramics with dense structure (at 1 150℃)still achieve the lowest Q×f value.The reason for this is not clear at present and will be further studied.For CaZnyTi1-yO3-δ(y=0.01)samples,the εrfirstly increases with the sintering temperatures,reaches the maximum value(~158)at1 200 ℃ ,and then decreaseswith increasing the sintering temperature.The maximum εrvalue of CaZnyTi1-yO3-δ(y=0.01)is lower than CaTiO3duetotheTi siteby Zn substitution and the appearance of oxygen vacancy.It is interesting that the Q×f value increases with the increase of the sintering temperature.The Q×f value can be affected by porosity and grain size[27].Generally,a larger grain size and a smaller grain boundary indicate reduction in dielectric loss.Sample sintered at 1 150 ℃ with low dielectric constant and Q×f value are attributed to a low bulk density.As the sintering temperature increase from 1 150℃ to 1 300℃,the Q×f value increasesdue to grain size augmentand grain boundary reduction.For all samples doped with Zn,the τfvalues are decreased compared with CaTiO3.CaZnyTi1-yO3-δ(y=0.01)ceramics sintered at 1 250 ℃possesses a dielectric constant of 157,a Q×f value of 6 819 GHz and a τfvalue of+7.5×10-4℃-1.

Table 2 Dielectric properties of ceramics

3 Conclusions

The sol-gel method was adopted to synthesize the nano-sized CaTiO3∶Zn particles.The average particle size calculated from TEM micrograph is 25 nm.Zn substitution site has a great influence on phase composition and sintering temperature.The added Zn exists as Zn2TiO4phase for Ca1-xZnxTiO3and CaTiO3+zZnO.However,for CaZnyTi1-yO3-δ(y=0.01),Zn substitutes for Ti site and forms a solid solution,which has no obvious effect on sintering characteristics.As the y value is increased to 0.05 and 0.1,ZnO phase is formed.The existence of ZnO or Zn2TiO4phase can decrease sintering temperature.The ultrafine CaTiO3∶Zn powders can be sintered at relatively lower temperatures (≤1250 ℃)and most of them possess high Q ×f values.CaZnyTi1-yO3-δ(y=0.01)ceramics sintered at 1250℃exhibits good dielectric properties with a dielectric constant of 157 and a Q×f value of 6819 GHz.

[1]Wersing W.Curr.Opin.Solid State Mater.Sci.,1996,1(5):715-731

[2]Li J M,Qiu T,Fan C G,et al.J.Sol-Gel Sci.Technol.,2011,59(3):525-531

[3]Lee W H,Lee Y C.Ceram.Int.2010,36(1):181-185

[4]Fu M S,Liu X Q,Chen X M.J.Eur.Ceram.Soc.,2008,28(3):585-590

[5]Zhang Q L,Sun H P,Yang H.J.Alloys Compd.,2011,509(42):9986-9991

[6]Liang B L,Zheng X H,Tang D P.J.Alloys Compd.,2009,488(1):409-413

[7]Jacob K S,Satheesh R.Mater.Res.Bull.,2009,44(10):2022-2026

[8]Bindra N S,Dalveer K,Singh T K.J.Ceram.Process Res.,2009,10(5):595-599

[9]Wang S F,Wang Y R,Hsu J C.J.Phys.Chem.Solids,2011,72(9):1011-1014

[10]Huang C L,Tseng Y W.J.Am.Ceram.Soc.,2011,94(6):1824-1828

[11]Zhu H,Lu W Z,Lei W.Ceram.Int.,2011,37(5):1515-1519

[12]Huang C L,Chen J Y,Huang G S.J.Alloys Compd.,2010,499(1):48-52

[13]Hsu C H,Ho H A.Mater.Lett.,2010,64(3):396-398

[14]Zhang Q L,Wu F,Yang H.Scripta Mater.,2011,65(9):842-845

[15]Pang L X,Wang H,Zhou D,et al.Mater.Chem.Phys.,2010,123(2/3):727-730

[16]Yue Z,Zhang Y,Gui Z,et al.Appl.Phys.A,2005,80(8):1757-1761

[17]Zhang Q L,Wu F,Yang H,et al.J.Alloys Compd.,2010,508:610-615

[18]ZHANG Qi-Long(張啟龍),WANG Huan-Ping(王煥平),YANG Hui(楊輝).Chinese J.Inorg.Chem.(Wuji Huaxue Xuebao),2009,22(9):1657-1662

[19]Pang L X,Wang H,Chen Y H,et al.J.Mater.Chem.,2009,20(6):528-533

[20]Zhang Q L,Maso N,Liu Y,et al.J.Mater.Chem.,2011,21(34):12894-12900

[21]Ahn C W,Song H C,Nahm S.J.Am.Ceram.Soc.,2006,89(3):921-925

[22]Zhang Q L,Yang H,Zou J L,et al.Mater.Lett.,2005,59(8/9):880-884

[23]Kim H T,Kim S H,Nahm S,et al.J.Am.Ceram.Soc.,1999,82(11):3043-3048

[24]Kim H T,Byun J D,Kim Y.Mater.Res.Bull.,1998,33(6):963-973

[25]Li B,Tang B,Zhang S R,et al.J.Mater.Sci.,2010,45(23):6461-6466

[26]Kim H T,Kim Y.J.Am.Ceram.Soc.,2001,84(5):1081-1086

[27]Perm S J,Alford N M,Templeton A,et al.J.Am.Ceram.Soc.,1997,80(7):1885-1888

Preparation,Structure and Dielectric Properties of CaTiO3∶Zn Ceramics Based on Sol-Gel Technology

HUANG Wan-QunZHANG Qi-Long*YANG HuiSHEN Qian-Hong
(Department of Materials and Engineering,Zhejiang University,Hangzhou,310027,China)

Nano-sized CaTiO3∶Zn particles were synthesized by a sol-gel technique.The average particle size of the powder calculated from TEM micrograph is 25 nm.Zn substitution site has great influence on the phase composition and the sintering temperature of the ceramics.The added Zn exists as Zn2TiO4phase for Ca1-xZnxTiO3and CaTiO3+zZnO.However,for Ca(Zny,Ti1-y)O3-δ(y=0.01),Zn substitutes for Ti site and forms a solid solution,which has no obvious effect on sintering characteristics.When the y value is 0.05 and 0.1,ZnO phase is formed.The existence of ZnO or Zn2TiO4phase can improve the sintering properties.The ultrafine CaTiO3∶Zn powders can be sintered at relatively lower temperatures (≤1250 ℃).CaZnyTi1-yO3-δ(y=0.01)sintered at 1 250 ℃ possesses a dielectric constant εrof 157,a Q×f value of 6819 GHz and a τfvalue of 7.51×10-4℃-1.

CaTiO3:Zn;sol-gel processes;nanoparticles;dielectric properties

TQ174

A

1001-4861(2012)11-2379-06

2011-12-16。收修改稿日期:2012-03-14。

國家科技支撐計劃(No.2009BAG12A07);浙江省創新團隊(No.2011R09010)資助項目。*

。 E-mail:mse237@zju.edu.cn

主站蜘蛛池模板: 久久国产热| 扒开粉嫩的小缝隙喷白浆视频| 精品国产aⅴ一区二区三区| 欧美综合中文字幕久久| 欧美亚洲欧美区| 99久久亚洲综合精品TS| 精品国产欧美精品v| 亚洲欧美一区二区三区蜜芽| 超清人妻系列无码专区| 中文字幕人妻无码系列第三区| 五月天福利视频| A级毛片高清免费视频就| 亚洲中文精品人人永久免费| 久久福利网| 亚洲成AV人手机在线观看网站| 视频在线观看一区二区| 国产91特黄特色A级毛片| 日韩在线2020专区| 日本在线视频免费| 国产精品福利在线观看无码卡| 国产91高清视频| 性视频久久| 四虎影视库国产精品一区| 国产剧情国内精品原创| 极品私人尤物在线精品首页 | 欧美午夜视频| 色噜噜狠狠色综合网图区| 欧美激情第一区| 国产内射在线观看| 伊人成人在线视频| 欧美黑人欧美精品刺激| 91在线激情在线观看| 美女无遮挡拍拍拍免费视频| 无码一区18禁| 亚洲AV电影不卡在线观看| 亚洲国产成人久久77| 亚洲色偷偷偷鲁综合| 日韩精品一区二区三区大桥未久| 玖玖免费视频在线观看| 黑人巨大精品欧美一区二区区| 国产亚洲精品97AA片在线播放| 被公侵犯人妻少妇一区二区三区| 97成人在线视频| 美女毛片在线| 亚洲综合中文字幕国产精品欧美| 亚洲综合九九| 国产欧美日韩综合在线第一| 无码丝袜人妻| 国产成人无码久久久久毛片| 五月综合色婷婷| 亚洲欧美色中文字幕| 亚洲性日韩精品一区二区| 熟女日韩精品2区| 亚洲中文字幕无码爆乳| 中日韩一区二区三区中文免费视频 | 永久天堂网Av| 亚洲欧美另类中文字幕| 国产区成人精品视频| 午夜电影在线观看国产1区| 天天色综合4| 久久无码免费束人妻| 日韩免费毛片| 亚洲女人在线| 欧美区日韩区| 992tv国产人成在线观看| 久视频免费精品6| 在线欧美a| 女人毛片a级大学毛片免费| 国内丰满少妇猛烈精品播| 波多野吉衣一区二区三区av| 国产精品xxx| 91福利国产成人精品导航| 欧美激情成人网| 高h视频在线| 国产精品视频a| 久久影院一区二区h| 国产女人在线视频| 欧美中出一区二区| a色毛片免费视频| 波多野结衣一区二区三区四区 | 国产一在线观看| 全部无卡免费的毛片在线看|