SnO2掺杂对(Ba0.85Ca0.15)(Ti0.9Zr0.1-xSnx)O3无铅压电陶瓷介电弛豫与电性能的影响

采用固相烧结法制备了(Ba0.85Ca0.15)(Ti09Zr0.1-xSnx) O3(BCZTS)无铅压电陶瓷.研究了不同含量SnO2(x=0,0.02,0.04,0.06,0.08)对BCZT无铅压电陶瓷相结构、压电性能、介电性能和铁电性能的影响,并利用XRD、SEM、准静态d33测试仪等表征样品.结果表明,所有样品均为单一钙钛矿结构.当掺杂x=0.02时,(Ba0.ss Ca0.1s)(Ti0.9 Zr0.1-xSnx) O3无铅压电陶瓷材料的综合性能优异:d33 =553 pC/N,kp=49;,εr～ 7474(l kHz),tanδ～1.5; (lkHz),Pr=6.06 μC/cm2,Ec=2 kV/cm,利用Curie-Weiss定律对该实验结果进行拟合,发现x=0.02的样品的介电弛豫特征更为明显.     

预烧温度对(Ba0.85Ca0.15)(Ti0.9Hf0.1)O3压电陶瓷电性能的影响

采用固相法分别在1100~1250 ℃的预烧温度下制备了(Ba0.85Ca0.15)(Ti0.9Hf0.1)O3(BCHT)无铅压电陶瓷,通过对所制备陶微观结构和电性能的测试,发现:所有样品均具有纯的钙钛矿结构;随预烧温度的增加,室温下样品逐渐由四方相向三方相转变,预烧温度在1150~1250 ℃时两相共存;样品的压电常数d33、剩余极化强度Pr均随预烧温度的升高呈现先减小后增加的趋势,相对介电常数εr、弥散系数γ呈现先增加后减小的趋势,而矫顽场Ec则逐渐降低.样品的综合性能在预烧温度1250 ℃处达到最佳值: d33=525 pC/N,Pr=10.2 μC/cm2,Ec=1.30 kV/cm,εr=17699,γ=1.65,表明该材料具有良好的应用前景.     

烧结温度对(Ba0.85 Ca0.15)(Ti0.9 Hf0.1)O3陶瓷压电性能的影响

采用传统固相反应法在系列烧结温度下制备了(Ba0.85 Ca0.15)(Ti0.9 Hf0.1)O3无铅压电陶瓷,并对陶瓷样品的晶格结构、表面形貌、铁电性能、压电性能和常温介电性能进行了测试与分析.结果表明:样品均具有纯的钙钛矿结构,随着烧结温度的升高,样品的晶体结构由立方相转变为四方相;压电系数和机电耦合系数随之增大,当烧结温度为1340℃时,样品的晶粒尺寸较为均匀,约为2～7μm,并且样品压电系数最大为250 pC·N-1,此时,2Pr=13.33μC·cm-2,2Ec=5.91 kV·cm-1,i=0.05 mA,ε=1803,tanδ≈0.017,Kp=0.32,Qm=116.     

(Ba0.85Ca0.15)(Ti1-xZrx)O3无铅压电陶瓷的性能研究

采用固相法制备了(Ba0.85Ca0.15)(Ti1-xZrx)O3(BCTZ)无铅压电陶瓷,研究Zr含量(x=0～0.15)对BCTZ陶瓷微观结构和电性能的影响。结果表明:所有样品均具有纯的钙钛矿结构;随Zr含量的增加,室温下样品逐渐由四方相向三方相转变,在0.05相似文献   

烧结温度对Cao.9(NaCe)0.05Bi2Nb2O9无铅压电陶瓷性能的影响

采用传统固相反应法制备了Ca0.9(NaCe)0.05Bi2 Nb2 O9铋层状无铅压电陶瓷.采用XRD、SEM、EDS及相关电学性能测试系统表征了样品的晶体结构、断面形貌、元素组成以及介电、压电、铁电等性能,探究不同烧结温度对于陶瓷性能的影响.结果表明:当烧结温度为1150℃时,样品的晶体结构单一均匀,呈现片层状结构,致密性较好,压电常数高达17 pC/N,介电损耗仅为0.42;,居里温度为908℃,并且具有很好的温度稳定性,说明固相反应法制备的Ca0.9(NaCe)0.05Bi2Nb2O9压电陶瓷最佳烧结温度为1150℃.     

Fe2O3掺杂(Ba0.7Ca0.3)TiO3-Ba(Zr0.2Ti0.8)O3无铅压电陶瓷的制备与性能

采用固相合成法制备了Fe2O3掺杂(Ba0.7Ca0.3)TiO3-Ba(Zr0.2Ti0.8)O3(简称BCZT)无铅压电陶瓷。借助XRD、SEM、阻抗分析仪等对该陶瓷的相组成、显微结构以及压电和介电性能进行了研究。结果表明,Fe2O3掺杂降低了BCZT无铅压电陶瓷的烧结温度并使居里温度Tc从85℃提高到95℃;当Fe2O3掺杂为0.02wt%～0.1wt%时,陶瓷样品均为ABO3型钙钛矿结构;少量Fe2O3掺杂促进了陶瓷晶粒的生长,但随着Fe2O3掺杂量进一步增加,陶瓷晶粒随之细化;当Fe2O3掺杂量为0.04wt%时,陶瓷样品具有最优综合电性能,其压电常数d33、机电耦合系数kp、机械品质因数Qm、介电损耗tanδ和介电常数εr分别为400 pC/N,0.40,51,0.023和3482。     

LiBiO2掺杂的低温烧结PSZT压电陶瓷

采用固相二步合成法,通过在预烧粉料中添加LiBiO2,制备出一种低温烧结的Pb0.95Sr0.05(Zr0.54Ti0.46)O3压电陶瓷材料。LiBiO2的添加具有降低烧结温度同时提高陶瓷性能的优点。实验结果表明:适量的LiBiO2掺杂,可形成过渡液相烧结,使烧结温度降低到950～1050℃,比未添加时的烧结温度低240～340℃。当w(LiBiO2)=1.0%,陶瓷达到最佳压电性能:压电应变常数d33=425 pC/N,平面机电耦合系数kp=57.62%,退极化温度Td=350℃,相对介电常数ε3T3/ε0=1543,介电损耗tanδ=0.0216,剩余极化强度Pr=35.51μC/cm2,体积密度ρ=7.45g/cm3。该材料可应用于低温共烧的叠层压电器件中。     

SiO2对低温烧结压电陶瓷PMNNS的性能影响

在烧结温度为1020℃下,采用固相二步合成法制备了Pb(Ni1/3Nb2/3)0.05(Mn1/3Nb2/3)0.04(Mn1/3Sb2/3)0.01(Zr1/2Ti1/2)0.9O3(PMNNS)压电陶瓷,研究了加入不同掺杂量的SiO2对陶瓷的结构与机电性能的影响。结果表明:加入SiO2可以明显地降低烧结温度;而且当SiO2的掺杂量为0.1%时,陶瓷的性能最佳,其性能如下:d33=331 pC/N,tanδ=0.0041,kp=0.62,Qm=1326,εr=917。     

Y2O3掺杂对(Ba0.85Ca0.15)Zr0.1Ti0.896Sm0.004O3无铅压电陶瓷介电弛豫与电性能的影响

采用固相法制备了(Ba0.85Ca0.15)1-xYxZr0.1Ti0.896Sm0.004O3(BCZTS-Yx)无铅压电陶瓷.研究了Y2O3含量对BCZTS-Yx无铅压电陶瓷相结构、压电与介电性能的影响.结果表明:Y3+作为施主掺杂物占据A位.当0.004≤x≤0.006时,陶瓷存在三方相与四方相共存的准同型相界结构.当x=0.006时,陶瓷具有最佳的电性能,分别为d33=384 pC/N,kp=37.2;,εr～6775,tanδ ～ 2.04;.利用Curie-Weiss定律对该实验结果进行拟合,发现x为0.006的样品的介电弛豫特征更为明显.     

预烧温度对La0.67Ca0.33MnO3陶瓷结构及电学性能的影响

采用溶胶-凝胶法成功制备了La0.67Ca0.33MnO3粉末,并通过改变预烧温度获取电学性能优异的陶瓷.利用X射线衍射(XRD)、扫描电子显微镜(SEM)、四探针法对不同预烧温度处理后的La0.67Ca0.33MnO3陶瓷的物相、结构、微观形貌和电学性能进行测试,分析预烧温度对材料的晶粒尺寸和电学性能的影响,从而摸索出最佳预烧温度.实验结果表明:样品的结晶性能好物相纯,随着预烧温度的增加,晶粒尺寸、致密度、收缩率和电阻温度系数(TCR)在不断减小,电阻率先减小后增加.在300℃预烧,1450℃烧结得到的样品具有较高的TCR值达到了40.8;·K-1.     

Structure of (chloranilato)bis(tri-n-butylphosphine)palladium(II)

(Chloranilato)bis(tri-n-butylphosphine)palladium(II), [Pd(C₆Cl₂O₄){P(C₄H₉)₃}₂] (chloranilic acid=2,5-dichloro-3,6-dihydroxy-p-benzoquinone): FW=718.02,P2₁/c,a=21.729(6),b=17.293(5),c=21.010(9) Å,=112.62(3)°,V=7287.42 ų,Z=8,D _c=1.309mg m^–3, Mo, =0.710730 Å,=0.76 mm^–1,F(000)=3008, finalR=0.087, 2594 observed reflections. Palladium is ligated by a distorted square planar P₂O₂ coordination sphere in the title compound. The two molecules per asymmetric unit differ in the arrangement of phosphine n-butyl chains, yielding two unique metal centers.     

Crystal structure of triphenylphosphine-(1-(di(trifluoromethyl)-hydroxymethyl)-cyclopentadienyl)-(1,2-di(carboxymethyl) ethylene-1-yl) ruthenium (0)

The structure of triphenylphosphine — (1 — (di(trifluoromethyl) — hydroxymethyl) — cyclopentadienyl) — (1,2 — di(carboxymethyl)ethylene — 1 — yl) — ruthenium (0) has been studied by single-crystal X-ray diffraction techniques. This compound, [C₅ H₄(CF₃)2 COH] Ru(PPh₃)C2(CO₂Me)₂H, crystallizes in the triclinic space groupP¯1 witha =10.131,b= 15.107,c= 10.798 Å, = 102.14, = 107.04, = 89.64° andZ = 2. The structure was refined by block-diagonal least-squares methods to a finalR value of 0.042, including hydrogen atoms. The compound contains a dicarboxymethylethylene ligand coordinated to ruthenium both through a ketonic oxygen and through a metal--carbon -bond. An intramolecular hydrogen bond is observed. Details of the structure are reported, and the structures of several Ru(0) complexes are compared.     

Synthesis, spectroscopy, and X-ray structures of fac-(CO)3(dppe)MnSC(S)H, fac-(CO)3(dppe)ReSC(S)H, fac-(CO)3(dppp)ReSC(S)H, and fac-(CO)3(dppb)ReSC(S)H

The monodentate dithioformato complexes, fac-(CO)₃(dppe)MnSC(S)H (1), fac- (CO)₃(dppe)ReSC(S)H (2), fac-(CO)₃(dppp)ReSC(S)H (3), and fac-(CO)₃ (dppb)ReSC(S)H (4), where dppe is 1,2-bis(diphenylphosphino)ethane, dppp is 1,3-bis(diphenylphosphino)propane, and dppb is 1,4-bis(diphenylphosphino)butane, were synthesized from the treatment of the corresponding hydrides, fac-(CO)₃ (P-P)MSC(S)H with CS₂. Compounds 1–4 crystallize in the monoclinic crystal system: for 1, space group = P2₁/c, a = 15.3139(3) Å, b = 9.7297(4) Å, c = 19.0991(6) Å, = 105.928(1), V = 2736.5 ų, Z = 4; for 2, space group = P2₁/c, a = 15.6395(8) Å, b = 9.8182(5) Å, c = 19.4153(11) Å, = 106.741(1), V = 2854.9(3) ų, Z = 4; for 3, space group = P2₁/n, a = 11.3570(10) Å, b = 19.465(2) Å, c = 15.5702(14) Å, = 104.776(2), V = 3328.3(5) ų, Z = 4; and for 4, space group = C2/c, a = 32.078(2) Å, b = 10.4741(6) Å, c = 19.0608(9) Å, = 94.315(2), V = 6386.1(6) ų, Z = 8.     

Crystal and molecular structures oftrans-dichloro-(ethylene) (4-methylpyridine)platinum(II) andtrans-dichloro(ethylene) (2,4,6-trimethylpyridine)platinum(II)

The crystal and molecular structures oftrans-[PtCl₂(C₂H₄)(4-MeC₅H₄N)] (I) andtrans-[PtCl₂(C₂H₄)(2,4,6-Me₃C₅H₂N)] (II) have been determined by single-crystal x-ray methods.I crystallizes in space groupP2₁/c witha= 4.991(1), b=21.658(3), c=10.675(3) Å, =110.17(2) °,Z=4;II is orthorhombic (Pbca) witha=10.295(6),b=12.393(8),c=20.370(10) Å,Z=8.Full-matrix least-squares refinements have given finalR factors of 0.053 (1520 reflections) forI and 0.042. (1412 reflections) forII. The intensities were recorded by counter methods, and only those reflections havingI>3(I) were used in the analyses.In both complexes, platinum is four-coordinate with the two chlorine atoms, the double bond of the ethylene, and the nitrogen atom of the substituted pyridine. The two structures are discussed in terms of the arrangement of the pyridine ligand with respect to the PtCl₂(C₂H₄) moiety.     

Structure of (N-(2-hydroxyphenyl)-salicylaldiminopiperidino) Ni(II) complex

The crystal and molecular structure of the title complex, C₁₈H₁₉N₂O₂Ni, has been determined by direct methods. The compound crystallizes in the monoclinic crystal system witha=22.973(1),b=5.212(1),c=27.076(1)Å, β=106.46(1)°, space groupC2/c,V=3109.1(6)ų, Z=8, andD _x=1.51g cm^?3. The nickel atom is in a slightly distorted square-planar environment of two oxygens [Ni(1)?O(1) 1.824(3) and Ni(1)?O(2) 1.856(3)Å] and two nitrogens [Ni(1)?N(1) 1.849(3) and Ni(1)?N(2) 1.932(3)Å] with O?Ni?N angles between 85.7(1) and 97.1(1)°. The nickel atom is 0.006 Å out of the plane of its ligands.     

Crystal structure of bis(4-dimethylaminopyridinium) tribromocuprate(I) and bis(4-dimethylaminopyridinium) tetrabromocuprate(II)

The synthesis and crystal structures of two copper bromide salts of the 4-dimethylaminopyridinium (4DMAP⁺) cation are reported. The Cu(I) salt, (4DMAP)₂CuBr₃, crystallizes in the monoclinic space group C2/c, with a = 11.724(2), b = 11.055(3), c = 15.763(3) Å, = 107.64(3)°, and Z = 4. It contains isolated planar 4DMAP⁺ cations and trigonal planar CuBr₃ ^2– anions. Small distortions from idealized D _3h symmetry are observed for the anion. For the Cu(II) salt, (4DMAP)₂CuBr₄, a triclinic cell is observed with a = 8.2373(2), b = 9.2428(2), c = 14.4391(1) Å, = 93.760(1), = 94.576(1), = 105.249(1)°, and Z = 2. This compound contains discrete planar 4DMAP⁺ cations and flattened tetrahedral CuBr₄ ^2– anions. Small distortions are observed for ideal D _2d symmetry.     

X-ray crystal structure of trans-bis(monoethanolamine) bis(saccharinato)nickel(II)

The crystal structure of trans-bis(monoethanolamine)bis(saccharinato)nickel(II), [Ni(C₇H₄NO₃S)₂(C₂H₇NO)₂], has been determined from X-ray diffraction data. The metal complex is monoclinic, with a = 11.0555(5), b = 8.9103(4), c = 11.3890(5) Å, = 105.0230(10)°, Z = 2, and space group P2_1/c . The structure consists of individual molecules. Two monoethanolamine molecules and two saccharinate anions coordinate the nickel atom forming a distorted octahedron. The monoethanolamine molecules act as a bidentate ligand and form five-membered trans chelate rings, which constitute the plane of the coordination octahedron, while two saccharinate ions behave as a monodentate ligand occupying the axial positions. Intermolecular hydrogen bonds link the molecules to form a three-dimensional infinite structure.     

Crystal and molecular structures of trans-bis(acetonitrile)bis(bipyridine)ruthenium(II) perchlorate and trans-diamminebis(bipyridine)ruthenium(II) perchlorate

The structures of trans-[(MeCN)₂(bpy)₂Ru](ClO₄)₂(I) andtrans-[(NH₃)₂(bpy)₂Ru](ClO₄)₂(II) have been determined by single crystal X-ray diffraction methods. (I) forms monoclinic crystals in the space groupP2₁/c witha=8.399(2),b=10.406(2),c=15.590(3) Å,=93.78(2)° andZ=2 atT=293 K. The final refinement gaveR=0.040 for 2448 reflections withF _o ² >3(F _o ² ). (II) crystallizes in the triclinic space groupP¯1 witha=1.702(1),b=8.439(2),c=10.525(2) Å,=107.56(2),=104.63(1), =100.89(2)° andZ=1 atT=293 K. Refinement using 1878 reflections withF _o ² >3(F _o ² ) produced a finalR value of 0.036. Both of these structures have the ruthenium atom located on a crystallographic inversion center. The bipyridine ligands in both structures are in the bowed conformation as a means of circumventing the steric problems associated with the trans arrangement of the bipyridine ligands. The Ru-N(monodentate) distance is longer for the ammonia complex (2.106(3) Å) than for the acetonitrile complex (2.008(4) Å); there are no significant differences in the distances and angles of the two Ru(bpy)₂ frameworks.     

X-ray structures of tris(0-cyclohexyl-dithiocarbonato)bismuth(III) and tris(0-benzyl-dithiocarbonato)bismuth(III)

The crystal structures of two Bi tris xanthates are reported, namely [Bi(S₂CO-c-C₆H₁₁)₃ J and [Bi(S₂COCH₂C₆H₅)₃]. They exist as centrosymmetric dimers, owing to the presence of bridging xanthate ligands, with seven-coordinate Bi atoms. The presence of a stereochemically active lonepair of electrons in each structure distorts the coordination geometry defined by seven S atoms and causes the elongation of some of the Bi-S bond distances. Crystals of both compounds are triclinic, space groupP¯1 with unit cell dimensions for [Bi(S₂CO-c-C₆H₁₁)₃]:a=12.417(3),b=13.571(3),c=9.681(4) Å;=102.30(2),=109.21(2), =66.23(2)° andZ=2; and for [Bi(S₂COCH₂C₆H₅)₃]:a=14.747(2),b=15.966(2),c=5.991(1) Å;=95.08(1),=98.51(1), =104.92(1)° andZ=2. The structures were refined by a full-matrix least-squares procedure to finalR=0.045 using 4274 reflections for [Bi(S₂CO-c-C₆H₁₁)₃] and toR=0.027 using 3993 reflections for [Bi(S₂COCH₂C₆H₅)₃].