992 resultados para Sm~(3 )


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本论文合成了R_1Ba_2Cu_3O_(2-x) (R = La、Nd、Sm、Eu、Gd、Dr、Ho、Er、Tm、Yb)、Y_2Ba_2Cu_3O_(2-x) (x = 0.10~1.17)和Y_1Ba_2Cu_3O_(7-x)S_x (x = 0~2),并对磁性和超导电性进行了较为系统的研究。R_1Ba_2Cu_3O_(2-x)的磁化率在T > Tc的很宽的温度范围内服从Curic-Weiss定律,求得的有效磁矩略大于理论值,差值与Y_1Ba_2Cu_3O_(2-x)中Cu~(2+)磁矩相近,说明Cu~(2+)的磁矩对体系磁性有额外贡献,这贡献随R~(3+)离子中自旋平行的电子权的增多而增大。其高温下的磁化率CT > 700K)相对Curic-Weiss定律发生较大偏离,这偏离可能的来源有三个:高温下稀土离子发生较大的能级反转效应,高温下结构相变对磁性的影响,高温下氧含量减少造成Cu~(2+)磁矩增大。R_1Ba_2Cu_3O_(2-x)磁化率在T < Tc时也服从Curic-Weiss定律,R~(3+)磁矩是定域的,表明超导与磁性相互独立。互不相关,稀土磁矩与传导电子间无相互作用。用Sr取代R_1Ba_2Cu_3O_(2-x)中的Ba,没能使体系产生磁有序的变化,但却使有效磁矩增大,并完全破坏了样品的超导电性。Sm~(3+)磁化率不服从Curic-Weiss定律,在Sm_1Ba_2Cu_3O_(2-x)中Sm~(3+)显示了典型Van VlccK离子的特性。Y_1Ba_2Cu_3O_(2-x)随氧含量减少发生超导体一半导体一绝缘体的转化,当氧含量由6.90减小至6.49时发生由正交到四方的结构相变。当(7-x) = 5.83时有较多杂质相出现,123相开始分解。样品磁化率均服从Curic-Weiss定律,并随氧含量增大磁化率-温度曲线越来越趋于平缓(直线),当(7-x) = 6.90时磁化率基本不随温度变化,这时Pauli顺磁性占主导地位,这说明氧含量增加定域磁矩减少,求得的有效磁矩Peff随氧含量增大总趋势减小。提出了电子“巡游”的观点,较好地解释了上述现象,并推测出Cu(2)的d电子是离域的,对样品磁矩没有贡献,样品Peff来源于部分Cu(1)的定域Cu~(2+)的磁矩,上述推测被EPR结果证实。正交相Y_1Ba_2Cu_3O_(2-x)的EPR谱显示了中心对称成准立方晶场中Cu~(2+)(d~9, S = 1/2, I = 3/2)的EPR物性。而四方相样品的EPR谱却出现了明显的各向异性,说明观察到的为Cu(1)的EPR信号,由Cu(1)~(2+)的写域磁矩产生。Y_1Ba_2Cu_3O_(2-x)的EPR信号束源于本体相,而非Y_2Cu_2O_5、BaCuO_2、Y_2BaCuO_5等杂质相。各样品EPR信号的自旋浓度远小于1spin/cu,并随氧含量减小而增大,当(7-x) = 6.49、6.40时自旋浓度出现陡增,这时伴随由正交到四方的转化,证明了电子“巡游”观点的正确。用硫部分取代Y_1Ba_2Cu_3O_2g中的氧,当Y_1Ba_2Cu_3O_(2-x)Sx中x = 0.11时Tc = 92.6K,比Y_1Ba_2Cu_3O_(7-x)升高2K,但由于杂质相的存在,ΔTc加宽。其他样品多为半导体和绝缘体。硫取代0,当x = 0.04,0.06,0.11和1.20时磁化率服从Curic-Weiss定律,并且x = 0.87,1.2时分别在230K、240K出现反铁磁有序。其他样品由于Cu被还原为+1价而变成抗磁性。x = 0.11 (Tc = 92.6K),EPR谱为正交场中Cu~(2+)的信号。自旋浓度与温度无关。当所有Cu均为Cu~(1+)时,测问的是-s-的EPR信号,而Cu为混合价态(+1和+2时)测问是上述两种信号的叠加。

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本工作用无水SmCl_3和YbCl_3每二摩尔比的叔丁基环戊二烯基钠在四氢呋喃中反应,合成了二(叔丁基环戊二烯基稀土氧化物(t-C_4H_9C_5H_4)_2Sm(DME)和(t-C_4H_9C_5H_4)_2YbCl(THF),配合物得到元素分析及~1H-NMR的鉴定。通过(t-C_4H_9C_5H_4)_2SmCl(DME)和(t-C_4H_9C_5H_4)_2YbCl(THF)分别每金属钠在四氢呋喃中的还原反应,分离得到了相应的二价稀土络合物(t-C_4H_9C_5H_4)_2Sm(DME)和(t-C_4H_9C_5H_4)_2Yb(THF)_2。络合物经元素分析,~1H-NMR鉴定,并通过对络合物具有弯曲的夹心式结构,中心金属离子Yb~(2+)除每两个五元环络合外,还与两个THF的氧配位,形成稳定的8配位结构。本工作还研究了二价络合物(t-C_4H_9C_5H_4)_2Sm(DME)的还原性,并通过(t-C_4H_9C_5H_4)_2Sm(DME)每phc≡CH在甲苯中反应,证明了(t-C_4H_9C_5H_4)_2Sm(DME)具有很强的还原性,能每phC≡CH发生单电子转移反应,从此瓜体系中分离得到了一个新的三价Sm~(3+)络俣物[(t-C_4H_9C_5H_4)_2Sm(u-C≡Cph)]_2。经X光单晶结构的鉴定,证明此络合物具有双分子结构,中心金属离子Sm~(3+)除了与两个叔丁基环戊二烯基负离子络合外,还与两个桥炔配位,构成八配位的结构。二价Yb~(2+)络合物(t-C_4H_9C_5H_4)_2Yb(THF)_2能与三苯氧膦在甲苯溶液中反应,发生配体交换,使络合物中的一个THF分子被三苯氧膦取代,得到(t-C_4H_9C_5H_4)_2Yb(opph_3)(THF)。此外,我们还研究了(C_tMe)_2Nd(u-Cl)_2Na(DME)_2与甲基萘钠在溶剂DME中的反应,结果表明,在这一体系中,发生了甲基萘钠对溶剂分子CH_3OCH_2CH_2OCH_3中CH_3-O键的断裂反应断裂反应产生的CH_3ONa能与(C_5Me_5)_2Nd(u-Cl)_2Na(DME)_2发生交换反应得到(C_5Me_5)_2Nd(u-Cl)_2Na(DME)_2。络合物经元素分析,水解色质(GC-MC)谱及~1H-NMR鉴定,并通过X光单晶结构的测定证明具有弯曲夹心式结构。

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Thin film phosphors with compositions of RP1-xVxO4: A (R = Y, Gd, La; A = Sm3+, Et3+; x = 0, 0.5, 1) have been prepared by a Pechini sol-gel process. X-Ray diffraction, atomic force microscopy (AFM), photoluminescence excitation and emission spectra were utilized to characterize the thin film phosphors. The results of XRD showed that a solid solution formed in YVxP1-xO4: A film series from x = 0 to x = 1 with zircon structure, which also held for GdVO4: A film. However, LaVO4: A film crystallized with a different structure, monazite. AFM study revealed that the phosphor films consisted of homogeneous particles ranging from 90 to 400 nm depending on the compositions. Upon short ultraviolet excitation, the films exhibit the characteristic Sm(3+ 4)G(5/2)-H-6(J) (J=5/2, 7/2, 9/2) emission in the red region and Er3+ H-2(11/2), S-4(3/2)-I-4(15/2) emission in the green region, respectively With the increase of x values in YVxP1-xO4: SM3+ (Er3+) films, the emission intensity Of SM3+ (Er3+) increases due to the increase of energy transfer probability from VO43- to Sm3+ (Er3+). Due to the structural effects, the Sm3+ (Er3+) shows similar spectral properties in YVO4 and GdVO4 films, which are much different from those in LaVO4 film.

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Nanocrystalline Gd2O3:A (A = Eu3+, Dy3+, Sm3+, Er3+) phosphor films and their patterning were fabricated by a Pechini sol-gel process combined with a soft lithography. X-ray diffraction (XRD), atomic force microscopy (AFM), scanning electron microscopy (SEM) and optical microscopy, UV/vis transmission and photoluminescence (PL) spectra as well as lifetimes were used to characterize the resulting films. The results of XRD indicated that the films began to crystallize at 500 degreesC and that the crystallinity increased with the elevation of annealing temperatures. Uniform and crack free non-patterned phosphor films were obtained by optimizing the composition of the coating sol, which mainly consisted of grains with an average size of 70 nm and a thickness of 550 nm. Using micro-molding in capillaries technique, we obtained homogeneous and defects-free patterned gel and crystalline phosphor films with different stripe widths (5, 10, 20 and 50 mum). Significant shrinkage (50%) was observed in the patterned films during the heat treatment process. The doped rare earth ions (A) showed their characteristic emission in crystalline Gd2O3 phosphor films due to an efficient energy transfer from Gd2O3 host to them. Both the lifetimes and PL intensity of the rare earth ions increased with increasing the annealing temperature from 500 to 900 degreesC, and the optimum concentrations for Eu3+, Dy3+, sm(3+), Er3+ were determined to be 5, 0.25, 1 and 1.5 mol% of Gd3+ in Gd2O3 films, respectively.

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利用高温固相法合成了系列稀土离子掺杂的CdSiO_3:RE~(3+)(RE=Y,La,Ce,Pr,Nd,Sm,Eu,Gd,Tb,Dy,Ho,Er,Tm,Yb,Lu)多光色长余辉磷光体。XRD分析结果表明在1050℃下烧结3小时的产物为单相。稀土掺杂CdSiO_3磷光体具有良好的发光性能。引入Y~(3+),La~(3+),Gd~(3+),Lu~(3+)以及Ce~(3+),Nd~(3+),Ho~(3+),Er~(3+),Tm~(3+),Yb~(3+)可获得一个最大发射中心位于420 nm附近的缺陷发光宽带,引入 Pr~(3+),Sm~(3+),Eu~(3+),Tb~(3+),Dy~(3+)时,除了产生约420 nm的蓝紫色缺陷发光外同时产生很强的稀土离子特征发光,这两种发光混合导致不同的余辉颜色。

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The VUV-UV spectra of rare earth ions activated calcium borophosphate, CaBPO5:RE (RE = Ce3+, sm(3+), Eu2+, Eu3+, Tb3+ and Dy3+) were determined. The bands at about 155 nm in the VUV excitation spectra are attributed to the host lattice absorptions. The bands at 166 and 190 nm for the sample CaBPO5:Sm have been considered as related to the f-d transition and the charge transfer band (CTB) of Sm3+ ions, and the band at 169 nm for the sample CaBPO5:Dy is assumed to be connected with the f-d transition of the Dy3+ ions in CaBPO5. The partial reduction of Eu3+ CaBPO5:Eu prepared by high temperature solid state reaction in air is confirmed by the VUV-UV spectra.

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稀土配合物能使极性和非极性单体聚合[1] .虽然目前已测定了几乎所有的三 (环戊二烯基 )稀土配合物及部分三 (取代环戊二烯基 )稀土配合物的晶体结构 ,但有关三 (茚基 )稀土配合物的报道较少 .第一个三 (茚基 )稀土配合物是无水三氯化稀土与 3倍物质的量的茚基钠 C9H7Na在四氢呋喃中反应而得 ,但未报道其晶体结构[2 ] .后来用同样的反应却分离出以氯为桥的二聚体离子对配合物[Na( THF) 6][Ln( η5- C9H7) 3μ( Cl) Ln( η5- C9H7) 3]( Ln=Nd,Sm) [3] .无水三氯化稀土与 Mg( C9H7) 2 或C9H7K等物质的量反应则生成非溶剂化的 ( C9H7) 3Sm[4 ] ,而与茚基钠和环辛四烯钾 ( C8H8K)以 1∶ 2∶ 1物质的量比反应时 ,则得到 ( C9H7) 3Ln( THF) ( Ln=Nd,Gd) [5] .Bottomley[6] 曾用 ( C9Me7) K(七甲基茚基钾 )与 L n Cl3(物质的量比 3∶ 1 )反应制备 ( C9Me7) 3Nd( THF) 5和 ( C9Me7) 3Er· ( THF) 3,但未报道晶...

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本文利用溶胶-凝胶法合成了Ce_(1-x)Sm_xO_(2-x/2)(x=0-0.4)系列固体电解质,并且系统地研究了其晶体结构随Sm含量的变化关系。XRD表明:该体系从160℃开始即形成了立方萤石结构,且在所研究的组成范围内全部形成了单相固溶体。此温度远低于传统的高温固相合成法所需的温度,同时也较水热合成法的温度低。高温X-ray衍射研究表明直到800℃Ce_(1-x)Sm_xO_(2-x/2)未出现结构相转变,其晶格常数和晶胞体积随温度升高而增大。EPR测试证实了由于Sm~(3+)部分置换Ce~(4+)固溶体中所存在的单电荷缺陷(Sm_(Ce’),V_o~(oo))结构。在固溶体的Raman谱中观察到:纯CeO_2在465cm~(-1)仅有一个Raman振动模式,随着掺杂量的增大,此振动模式向低频方向移动,而且Raman线变宽且在570cm~(-1)附近出现一新的峰,这些变化都是由Sm~(3+)取代Ce~(4+)所产生的氧空位引起的。

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本文研究了铽(Tb~(3-))对钐(Sm~(3-))-2-噻吩甲酰三氟丙酮(TTA)-氯代甲基三烷基铵(N_(263))-Triton X-100荧光体系的共发光效应,结果表明:Tb~(3-)的浓度1×10~(-5)~5×10~(-5)mol/L范围内体系的荧光强度最大.Sm~(3-)的浓度在1.0×10~(-9)~1.0×10~(-7)mol/L范围内与荧光强度呈线性关系,检测限为1.0X10~(-11)mol/L,方法灵敏,简便,用于混合稀土样品中痕量Sm~(3-)的测定,结果满意。

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一定条件下钐离子、铕离子、镱离子等都具有明显的变价特性。钐离子通常以+3价形式存在,Sm~(3+)电子构型为[Xe]4f~5,基态光谱项为~6H_(5/2),4f能级最低激发态为~4G_(5/2)。Sm~(2+)在溶液中很不稳定,极易被氧化,但在某些固态化合物中Sm~(2+)能够比较稳定存在。通过适当的还原方法可以制得+2价钐的化合物。Sm~(2+)电子构型为[Xe]4f~6,基态光谱项为~7F_0,4f能级最低激发态光谱项为~5D_0。通常~5D_0能级位置较其4f~5d激发态能级下限位置低,因此室温

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报道了合成二价钐激活的复合氟化物的简单方法。用H_2作还原剂,用高温固相反应直接制得8m~(2+)激活磷光体:KMgF_3,LiBaF_3,BaBeF_4,SrMgF_4和BaMgF_4等,其中BaBeF_4,SrMgF_4和BaMgF_4中掺入Sm~(2+)为首次报道。在KCaF_3,CaBeF_4,SrBeF_4和CaMgF_4中只观察到Sm~(3+)发射而无Sm~(2+)发光。分析了钐离子价态与基质组成结构间关系,讨论了钐离子(8m~(2+)和Sm~(3+))的光谱特征。

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标题化合物SmCl_3(THF)_4(M_r=545.2)晶体属正交晶系,空间群为Pdd 2。晶胞参数为a=9.211(4),6=16.436(6),c=29.666(12);V=4491(3) ~3;Z=8,D_c=1.61g.cm~(-3),F(000)=2184,μ_c=30.3cm~(-1)。最终的偏因子R=0.063,R_(to)=0.062。Sm~(3+)与三个Cl~-及四个四氢呋喃分子中氧原子配位,形成一个五角双锥的空间结构,其中二个氯原子分别位于二个顶点位置。分子中有一个通过Sm~(3+)及Cl~-的C_2轴。Sm-Cl及Sm-0的平均键长分别为2.683(5)及2.469(11)。

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利用极谱,Ⅲ利用电位阶跃研究了轻稀土离子在碱金属氯化物熔盐中的阴极还原。本文作者研究过Sm~(3+)在NaCl-KCl熔盐中的电还原。上述工作分别提出了稀土离子一步还原和分步还原的结论。本文采用线性扫描伏安法和恒电位电解,并配以扫描电子显微镜X射线能谱分析,对Nd~(3+)在Pt电极上的阴极还原过程进行了研究,利

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本文用脉冲衰减法和时间分辨荧光光谱法测量了六种不同稀土离子浓度的Sm_xLa_(1-x)P_5O_4晶体的~4G_(5/2)→~6H_J(J=5/2,7/2,9/2,11/2)四个能级和七种不同稀土离子浓度的Dy_xY_(1-x)P_5O_(14)晶体的~4F_(9/2)→~6H_J(J=15/2,13/2,11/2,9/2)四个能级的荧光寿命和荧光强度。结果指出,在这类晶体中,Sm~(3+)和Dy~(3+)的荧光寿命随着离子的浓度增加而变短,存在着严重的荧光浓度猝灭现象。最后还讨论了浓度与寿命,寿命与荧光强度的关系。

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Ce(0.8)SM(0.2)O(1.9) and CeO(2) nanomaterials were prepared by a solution technique to produce an ultrafine particulate material with high sinterability. In this work, the structural characteristics, the photoluminescent behavior and the ionic conductivity of the synthesized materials are focused. The thermally decomposed material consists of less than 10 nm in diameter nanoparticles. The Raman spectrum of pure CeO(2) consists of a single triple degenerate F(2g) model characteristic of the fluorite-like structure. The full width at half maximum of this band decreases linearly with increasing calcination temperature. The photoluminescence spectra show a broadened emission band assigned to the ligand-to-metal charge-transfer states O -> Ce(4+). The emission spectra of the Ce(0.8)Sm(0.2)O(1.9) specimens present narrow bands arising from the 4G(5/2) -> (6)H(J) transitions (J = 5/2, 7/2, 9/2 and 11/2) of Sm(3+) ion due to the efficient energy transfer from the O -> Ce(4+) transitions to the emitter 4G(5/2) level. The ionic conductivity of sintered specimens shows a significant dependence on density. (C) 2009 Elsevier B.V. All rights reserved.