含NiTi阻挡层的硅基(La0.5Sr0.5)CoO3/Pb(Zr0.4Ti0.6)O3/(La0.5Sr0.5)CoO3铁电电容器异质结

应用磁控溅射法制备的非晶NiTi薄膜作阻挡层,在Si (100)衬底上构造了(La0.5Sr0.5)CoO3/ Pb(Zr0.4Ti0.6)O3/(La0.5Sr0.5)CoO3(LSCO/PZT/LSCO)铁电电容器异质结,研究了Pb(Zr0.4Ti0.6)O3铁电薄膜的结构和物理性能.实验发现LSCO/PZT/LSCO铁电电容器具有良好的电学性能,在417kV/cm的驱动场强下,PZT铁电电容器具有较低的矫顽场强(125kV/cm)和较高的剩余极化强度(19.0μC/cm2),良好电容-电压特性(C-V)和保持特性,铁电电容器经过1010次反转后,极化强度没有明显下降,表明了非晶NiTi薄膜可以用作高密度硅基铁电存储器的扩散阻挡层.     

Pb过量对以Ti-Al为阻挡层的硅基铁电电容器极化翻转性能的影响

以射频磁控溅射法生长的La0.5Sr0.5CoO3( LSCO)为电极,采用溶胶-凝胶法在以Ti-Al为导电阻挡层的Si基片上生长了用不同Pb过量前驱体溶液(溶胶)制备的LSCO/Pb( Zro4Ti0.6)O3(PZT)/LSCO电容器,以此构造了Pt/LSCO/PZT/LSCO/Ti-Al/Si异质结.Pb过量对LSCO/PZT/LSCO电容器极化翻转性能的影响表明:不同Pb过量溶胶对电容器的极化翻转性能影响很大,其中Pb过量15;的溶胶制备的样品在550℃常规退火1h后相对具有较好的翻转性能.在5V的外加电场下,LSCO/PZT/LSCO电容器的矫顽电压和剩余极化强度分别为1.25V和24.6μC/cm2.疲劳和电阻率测试分析表明:在经过109翻转后,不同样品的抗疲劳性能均很好,而电阻率随前驱体溶液Pb过量的增加呈现下降的趋势.     

含Ni-Nb阻挡层的硅基Pb(Zr0.4,Ti0.6)O3电容器的制备及铁电性能研究

采用Ni-Nb薄膜作为导电阻挡层,以La0.5Sr0.5CoO3(LSCO)为底电极,构建了LSCO/Pb(Zr0.4,Ti0.6)O3(PZT)/LSCO异质结电容器。使用X射线衍射仪和铁电测试仪对其进行结构表征和性能测试。实验发现:Ni-Nb薄膜为非晶结构,PZT薄膜结晶状况良好。LSCO/PZT/LSCO电容器在5 V外加电压测试下,电滞回线具有良好的饱和趋势,剩余极化强度Pr为35.5μC/cm2,矫顽电压Vc为1.42 V,电容器具有良好的抗疲劳特性和保持特性。     

La0.5Sr0.5CoO3/Pb(Zr0.4Ti0.6)O3/La0.5Sr0.5CoO3铁电电容器的结构和性能研究

采用磁控溅射法和脉冲激光沉积法,在SrTiO3(001)衬底上制备了La0.5Sr0.5CoO3(70 nm)/Pb(Zr0.4Ti0.6)O3(70 nm)/La0.5Sr0.5CoO3(70 nm) (LSCO/PZT/LSCO)铁电电容器异质结.X射线衍射结果表明:LSCO和PZT薄膜均为外延结构.在5 V的外加电压下, LSCO/PZT/LSCO电容器具有较低的矫顽电压(0.49 V),较高的剩余极化强度(41.7 μC/cm2 )和较低的漏电流密度(1.97×10-5 A/cm2),LSCO/PZT/LSCO电容器的最大介电常数为1073.漏电流的分析表明:当外加电压小于0.6 V时,电容器满足欧姆导电机制;当外加电压大于0.6 V时,符合空间电荷限制电流(SCLC)导电机制.     

(La0.5Sr0.5)CoO3为电极的Pb(Zr0.4Ti0.6)O3和Pb(Zr0.2Ti0.8)O3铁电电容器结构及电学性能

分别采用磁控溅射法和溶胶-凝胶法(Sol-gel)制备了(La0.5Sr0.5)CoO3(LSCO)和Pb(Zr1-xTix)O3(PZT)薄膜,在Pt(111)/Ti/SiO2/Si基片上构架了LSCO/Pb(Zr0.4Ti0.6)O3(PZT(40/60))/LSCO和LSCO/Pb(Zr0.2Ti0.8)O3(PZT(20/80))/LSCO铁电电容器,研究了两种铁电电容器的结构和性能。XRD结构分析表明:两种四方相的不同Zr/Ti比例的PZT薄膜均为结晶良好的多晶钙钛矿结构。在5 V测试电压下,LSCO/PZT(40/60)/LSCO和LSCO/PZT(20/80)/LSCO两种铁电电容器的剩余极化强度(Pr)和矫顽场(Ec)分别为:28μC/cm2和1.2 V以及32μC/cm2和2 V。相对于PZT(40/60),PZT(20/80)具有较大的剩余极化强度和矫顽场,是由于其矩形度(c/a)较大。两种电容器都具有较好的脉宽依赖性和抗疲劳性。在5 V的测试电压下,LSCO/PZT(40/60)/LSCO电容器的漏电流密度为3.2×10-5A/cm2,LSCO/PZT(20/80)/LSCO电容器的漏电流密度为3.11×10-4A/cm2,经拟合分析发现:在0～5 V的范围内,两种电容器都满足欧姆导电机制。     

La_(1-x)Sr_xMnO_3电极的制备及其对Ba_(1-x)Sr_xTiO_3薄膜介电性能的影响

采用溶胶-凝胶法在Si(100)基底上制备了La_(1-x)Sr_xMnO_3电极材料.采用XRD、SEM对材料的晶体结构、表面形貌、薄膜厚度进行了表征,研究了退火温度对薄膜结构及电阻率的影响,以及介电常数与介电损耗随频率变化的关系.结果表明:在x=0.5,退火温度为800 ℃时,La_(0.5)Sr_(0.5)MnO_3薄膜的电阻率为1.2×10~(-2) Ω·cm.La_(0.5)Sr_(0.5)MnO_3薄膜与Ba_(1-x)Sr_xTiO_3匹配性较好,实现了BST薄膜的外延生长,其介电性能比在Pt上制备的Ba_(1-x)Sr_xTiO_3得到了明显的改善.     

非晶Ni-Al阻挡层对快速退火制备的硅基Ba0.6Sr0.4TiO3薄膜结构及物性影响的研究

应用非晶Ni-Al薄膜作为扩散阻挡层,采用磁控溅射法和溶胶-凝胶法在Pt/TiO2/SiO2/Si(001)衬底上制备了Pt/Ni-Al/Ba0.6Sr0.4TiO3/Ni-Al/Pt电容器结构,研究了在650～800 ℃温度范围内快速退火(RTA)工艺对电容器结构和物理性能的影响.结果表明:在外加电场为-100 kV/cm时,700 ℃和750 ℃退火样品的介电常数达到最大,分别为150和170.非晶Ni-Al薄膜的应用可以有效地降低BST薄膜的漏电流密度.650 ℃退火样品在整个测试电场范围内满足欧姆导电机制;700 ℃、750 ℃和800 ℃退火样品分别在电压低于-3.67 V、-2.65 V和-2.14 V时满足欧姆导电机制,在电压高于-3.67 V、-2.65 V和-2.14 V时满足普尔-弗兰克导电机制.     

SrRuO3导电层对快速退火制备Pb(Zr,Ti)O3薄膜结构和性能的影响

采用溶胶-凝胶法在Pt/Ti/SiO2/Si基片上,制备了Pt/Pb(Zr,Ti)O3(PZT)/Pt和SrRuO3(SRO)/PZT/SrRuO3(SRO)异质结电容器,并研究了快速退火条件下SRO导电层对PZT结构和性能的影响.XRD测试表明,两种结构电容器中的PZT薄膜均为钙钛矿结构,SRO/PZT/SRO、Pt/PZT/Pt均具有较好的铁电性和脉宽依赖性,5 V电压下两电容器的剩余极化强度Pr和矫顽电压Vc分别为28.3 μC/cm2、1.2 V和17.4 μC/cm2、2.1 V.在经过1010次翻转后,SRO/PZT/SRO铁电电容器疲劳特性相对于Pt/PZT/Pt电容器有了较大的改善,但SRO导电层的引入也带来了漏电流增大的问题.     

含Ni-Al阻挡层硅基BiFe0.95Mn0.05O3铁电电容器的结构及物理性能

以Ni-Al为阻挡层,在Si衬底上构架了SrRuO3(SRO)/BiFe0.95Mn<0.05O3(BFMO)/SRO异质结电容器.x射线衍射(XRD)分析表明:Ni-Al阻挡层为非晶结构,BFMO薄膜为具有良好结晶质量的多晶结构.在5 kHz测试频率下,SRO/BFMO/SRO电容器呈现饱和的电滞回线.实验发现,SRO/BFMO/SRO铁电电容器具有良好的抗疲劳性能.漏电机制研究表明,外加电场小于210 kV/cm时,SRO/BFMO/SRO电容器满足欧姆导电机制,在电场大于210kV/cm时,满足空间电荷限流传导机制.     

非晶 Ti-Al 过渡层对 Pt/Ba0.6Sr0.4TiO3/Pt电容器结构和性能的影响

应用磁控溅射法在 Pt/Ti/SiO2/Si(001)衬底上制备 5 mm 厚超薄非晶 Ti-Al 薄膜作为过渡层,利用脉冲激光沉积法制备 Ba0.6 Sr0.4TiO3 薄膜,构造了 Pt/Ba0.6Sr0.4TiO3/Pt(Pt/BST/Pt)和 Pt/Ti-Al/Ba0.6Sr0.4TiO3/Ti-Al/Pt(Pt/Ti-Al/BST/Ti-Al/Pt)结构的电容器,研究了 Ti-Al 过渡层对 Pt/BST/Pt 电容器结构及其性能的影响.实验表明,过渡层的引入有效地阻止了 Pt 电极和 BST 薄膜的互扩散,降低了 BST 薄膜氧空位的浓度,提高了铁电电容器的介电性能.当测试频率为 1 kHz、直流偏压为0 V时,介电常数由引入过渡层前的 530 增大到引入后的 601,介电损耗则由0.09减小到0.03.而且过渡层的引入有效地降低了 BST 薄膜的漏电流,使正负向漏电流趋于对称,在测试电压为5 V 时,漏电流密度由3.8×10-5 A/cm2 减小到 8.25 ×10-6 A/cm2.     

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.     

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.     

Molecular structure and spectral characteristics of bis(S-methyl-N-(2-pyridyl)methylendithiocarbazato)nickel(II), (Ni(NNS)2)

A nickel(II) complex of the pyridine-2-aldehyde Schiff base of S-methyldithiocarbazate (HNNS) has been synthesized and characterized by means of elemental analysis, IR and UV-vis spectra. The crystal structure of the complex has been determined by single-crystal X-ray diffraction. The complex crystallizes in the monoclinic, space P2₁/c, with a = 14.092(2), b = 16.886(2), c = 8.857(2)Å; = 105.78(3) °, V = 2028.2(6) ų, and Z = 4. The nickel atom is octahedrally coordinated by two uninegatively charged tridentate Schiff base in a mer-configuration via the pyridine nitrogen atom, azomethine nitrogen atom, and mecaptide sulfur atom.     

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.     

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 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.     

B位四价Sn4+, Zr4+取代对Ba(Zn1/3Nb2/3)O3系统微观结构的影响

采用传统的固相陶瓷烧结工艺,利用四价正离子Sn4+、Zr4+取代Ba(Zn1/3Nb2/3)O3陶瓷的B位Zn2+、Nb5+,研究其对Ba(Zn1/3Nb2/3)O3系统微观结构的影响.四价Sn4+、Zr4+取代B位Zn2+、Nb5+可以形成固溶体,系统的主晶相仍为立方相.系统晶格常数a随着Sn4+取代量的增加而呈线性增大,相同Sn4+取代量下随着烧结温度的增加,晶格常数a增大.BaZrO3(BZ)的加入可减少第二相的生成.Sn4+、Zr4+均可改善系统烧结特性,加快致密化形成.     

Crystal of catena-(μ2-terephthalato)-bis (N-methylimidazole)-copper(II)

A new one-dimensional chain complex [Cu(ta) (N-MeIm)₂]n (where ta = terephthalic acid dianion,N-MeIm =N-methylimidazole) has been synthesized and structurally characterized by single-crystal X-ray diffraction. The compound crystallizes in the Monoclinic space groupP2₁/c with the parameters:a = 5.2930(11)Å,b = 14.679(3)Å,c = 11.007(3)Å, β = 104.84(3)^°,V = 826.7(3)ų, withZ = 4 formula units. In the structure, each Cu atom is coordinated by a pair ofN-methylimidazole ligands and a pair of monodentate carboxylate groups, affording a square planar N₂O₂ geometry. Both carboxylate groups of the terephthalate dianion coordinate in a monodentate mode bridging two Cu(II) ions with formation of 1D zigzag chain along thec axis. This supramolecular compound exhibits a three-dimensional solid state structure constituted by hydrogen bonds and C–H–π stacking interactions.     

Crystal structure of aquo (hydroxo) (ethylenediaminetetraacetato) sodium(I) tin(IV), NaSn(OH)(edta)(H2O)

NaSn(OH)(edta)(H₂O) is monoclinic, space groupP2₁/c, witha=9.747(3)Å,b=9.121(3)Å,c=16.430(6)Å, =98.69(4)°, ų, andZ=4. The coordination environment of Sn(IV) is a capped octahedron. Sn–O distances range from 1.990(6)Å to 2.351(7)Å. Na(I) is five coordinated to three different edta molecules. Na–O distances range from 2.283(9)Å to 2.414(7)Å. The edta ligand presents the E, G/R conformation. The crystal structure is composed of sheets parallel to (001): inside a sheet Sn(OH)(edta) molecules are connected to each other by the Na(I) interactions.     

Structure of trans-aqua-bis(pyridine)dibenzoatocopper(II)

Crystals oftrans-aqua-bis(pyridine)dibenzoatocopper(II), Cu(NC₅H₅)₂(C₇H₅O₂)₂(H₂O), are monoclinic,P2₁/n, witha=5.9847(10),b=18.874(5),c=19.728(10)A,=92.97(4)°,Z=4, andV=2225.5(13)A³. The full-matrix least-squares refinement used 3030 reflections withI> 2.5(I) and converged toR=0.067. The benzoate ions bond as monodentate ligands in this five-coordinate complex. The copper ion is in a square pyrimidal environment with trans pyridine groups and benzoate ions in a slightly distorted square planar arrangement and a water ligand in the axial position. The Cu-O distance to the water molecule is significantly longer (2.273(4) Å) than the distances to the O atoms of the carboxyl groups (1.934(3) and 1.930(4)Å).