968 resultados para (Ag.) W. Sm.
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RBa2Cu3O7 (R = Pr, Sm, Eu, Gd, Dy, Y, Ho, Er, Tm) has been studied using complex chemical bond theory. The results indicated that with the decreasing of R radius, the ionicities for all considered types of bond decrease. This is in good agreement with the experimental fact that T-c decreases with the decreasing of R radius. PrBa2Cu3O7 with no Ba-site Pr in this calculation is also predicted to be a superconductor. This supports the conclusion obtained by Blackstead et al. The ionicity for each bond obeys the following order: Ba-O > R-O > Cu(2)-O(1) > Cu(2)-O(2,3) > Cu(1)-O(4) similar to Cu(1)-O(1).
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本文生长出了K2Ln(NO3)5.2H2O(Ln=La;Ce;Pr;Nd;Sm的单晶,并对其进行了晶体结构及差热-热重分析研究.结果表明,K2Ln(NO3)5.2H2O(Ln=La;Ce;Pr;Nd)的晶体属正交晶系,Fdd2空间群.首次生长出KPrN单晶并用直接法解出其晶体结构.解得KPrN的晶胞参数为:a=11.2210(10),b=21.411(3),c=12.208(2),Z=6;R=0.0240.对KLnN加热,则依次出现脱水、熔化、不可逆相变和NO的分解过程(K2Ce(NO3)5·2H2O除外)K2Ln(NO3)5·2H2O(Ln=La;Nd;Sm的NO分三步分解,K2Ln(NO3)5·2H。O(Ln=Ce;Pr)的NO分两步分解·KNO3和Ln(NO3)3·nH2O的混合物在225℃左右生成K2Ln(NO3)5
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非线性光学新材料K2Ln(NO3)5·2H2O(Ln=La,Ce,Pr,Nd,Sm)的晶体生长、结构和表征董文庭张洪杰苏锵(中国科学院长春应用化学研究所稀土化学与物理开放实验室,长春130022)Growth,StructureandCharact...
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Reaction of [Ph(4)P]2WS4 With NiCl2 in methanol solution in the presence of NaOCH3 leads to the formation of [Ph(4)P](2) [S2W(mu-S)(2)Ni(S-2)] (I) A Similar reaction between (NH4)(2)WS4 and NiCl2 under O-2 atmosphere in the presence of Ph(4)PCl or (n)Bu(4)NCl affords [Ph(4)P](2)([(S-2)W(O)(mu-S)(2)]Ni-2] (IIa) and [(n)Bu(4)N](2)([(S-2)W(O)(mu-S)(2)]Ni-2} (IIb) Under argon the same reaction gives [Ph(4)P](2)[Ni(WS4)(2)] (IIIa) and [(n)Bu(4)N](2)[Ni(WS4)(2)] (IIIb). [Ph(4)P](2)[Ni(WOS3)(2)] (IV) and [Ph(4)P](2)[Ni(WO2S2)(2)] (V) can be prepared from the reaction of [Ph(4)P]2WOS3 and [Ph(4)P]2WO2S2 with NiCl2. Treatment of (NH4)(2)WS4 with CuCl in the presence of PPh(3) in boiling pyridine produces W(mu-S)(4)Cu-2(PPh(3))(3) (VI), which can further react with excess PPh(3) to give W(mu-S)(4)Cu-2(PPh(3))(4) . py (VII). Complex I crystallizes in the space group P2(1)/n with the cell parameters: a = 20.049(4), b = 17.010(4), c = 14.311(7) Angstrom; beta = 110.24(3)degrees and Z = 4; R = 0.058 for 4267 independent reflections. The structural study confirms that complex I contains two terminal sulfide ligands, two bridging sulfide ligands, a side-on disulfide ligand, and a planar central W(mu-S)(2)Ni four membered ring. Complex VII crystallizes in the space group C2/c with the cell parameters: a = 26.436(8), b = 20.542(6), c = 19.095(8) Angstrom; beta = 125.00(3)degrees and Z = 4; R = 0.080 for 3802 independent reflections. The structural study reveals a perfect linear arrangement of the three metal atoms Cu-W-Cu.
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W-183 NMR spectra were obtained for [La(AsW11O39)(2)](11-), [La(As2W17O61)(2)](17-), [La(SiW9Mo2O39)(2)](13-), [LaSb9W21O86](16-), [LaAs4W40O140](25-) and alpha-, beta-[(CeO)(3) . (SiW9O34)(2)](14-) complexes, Tungsten NMR studies showed that the C-s symmetry of the square antiprism for [La(ASW(11)O(39))(2)](11-) and [La(As2W17O61)(2)](17-) anions keep constant in aqueous solution; the lanthanide accupied the central S-1 site in [LnSb(9)W(21)O(86)](16-) and [LnAs(4)W(40)O(140)](25-) complexes, respectively, and lanthanide metal cations gave [(CeO)(3) . (SiW9O34)(3)](14-) type of complexes with SiW9O3410-.
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The compounds O(CH2CH2C5H4)(2)Ln(THF)(2) [Ln = Sm(1), Yb(2)] were synthesized by the reduction of O(CH2CH2C5H4)(2)LnCl with sodium metal in tetrahydrofuran (THF) at room temperature. Recrystallization of 2 from dimethoxyethane (DME) produced the single-crystal O(CH2CH2C5H4)(2)Yb(DME) (3) whose structure has been determined by an X-ray diffraction study. The crystals are orthorhombic, space group Pcab, with a = 14.168(4), b = 13.541(6), c = 19.314(8) Angstrom, Z = 8, D-calc. = 1.66 g cm(-3).
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~(183)W核磁共振研究确认,La(AsW_(11))_2、Lam(As_2W_(17))_2在溶液中仍保持其四方反棱柱的C_3结构,La(SiW_9MO_2)_2阴离子中,2个Mo原子取代了2个等价的W原子,在穴状杂多阴离子LnAs_4W_(10)和LnSb_9W_(21)中,稀土离子占据中心S_1位置,SiW_9与稀土离子生成(LnO)_3(SiW_9)_2型杂多阴离子。
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多组分氧化物Ag-Bi-V-Mo-O催化作用的光电子能谱研究宋伟,李静,窦伯生(中国科学院长春应用化学研究所长春130022)关键词 钼钒酸铋,助剂Ag,XPS,Ar~+刻蚀,氧化还原对于烃类选择氧化反应中复合氧化物的催化作用,普遍认为是Redox机...
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Three new oxides Sm2SrCo2O7, Sm2BaCo2O7 and Gd2SrCo2O7 have been synthesized successfully by solid state reaction mathod. The X-Ray diffraction spectra show that they are all isostructural with Sr3Ti2O7, and Ln(2)SrCo(2)O(7)(Ln=Sm,Gd) crystallized in tetragonal system, Sm2BaCo2O7 in orthrhombic system. The Co-O bonds in CoO2 planes of Ln(2)SrCo(2)O(7) are shorter than those of LnSrCoO(4)(Ln=Sm, Gd), and so their delectrons are more delocalized and their electrical resistivities are smaller. The electrical resistivities versus temperature in the range 300 similar to 1100K showed that the five brides show the characters of weakly localized systems. In the lower temperature range, the magnetic behaviors of Gd2SrCo2O7 and GdSrCoO4 fit Curie-Weiss law well, and the magnetic exchange reaction in CoO2 sublattices of Gd2SrCo2O7 is ferromagnetic, but that of GdSrCoO4 is antiferromagnetic. The other three oxides with Sm3+ showed complex magnetic behaviors which is perhaps related with the complexity of Sm3+.
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We present the synthesis of AgLnMo(2)O(8) compounds with Ln = La-Nd and Sm. These compounds represent a scheelite-type structure characterized by MoO4- tetrahedrons. IR spectra show five absorption peaks in the region of 1000-400cm(-1), around 800cm(-1) and 400cm(-1), which correspond to the modes of the tetrahedral MoO42- groups. All of AgLnMo(2)O(8) (Ln = La-Nd and Sm) oxides are dielectric materials at room temperature. The temperature dependence of the magnetic susceptibility ofAgLnMo(2)O(8) (Ln = Ce-Nd and Sm) shows Curie-Weiss law behavior from 100K to 300K. This indicates that both Ce and Pr exist in +3 oxidation state in AgLnMo(2)O(8). For AgLaMo2O8, diamagnetic properties are found as expected.
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Three new oxides Ln(2)MCo(2)O(7) (Ln = Sm, Gd; M = Sr, Ba) have been synthesized in solid state reaction method. The powder X-ray diffraction spectra show that they are all isostructural with Sr3Ti2O7. The electrical resistivities in the temperature range 300-1100 K show that they are all semiconductors, and a transition to metals is observed at 1053, 1053, and 573 K for Sm2SrCo2O7, Gd2SrCo2O7, and Sm2BaCo2O7, respectively. The magnetic suspectivities of Gd2SrCo2O7 in the temperature range 300-673 K fit the Curie-Weiss law well. A plateau is observed in the curves of Sm(2)MCo(2)O(7) (M = Sr, Ba) which is attributed to the configuration state change of Co(III) from low spin to high spin. (C) 1995 Academic Press, Inc.
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用固相反应法合成了三个新的交生相氧化物:Sm_2SrCo_2O_7,Gd_2SrCO_2O_7和Sm_2BaCo_2O_7.它们均具有Sr_3Ti_2O_7型的结构,其中Sm_2BaCo_2O_7属于正交晶系,其它属于四方晶系.与LnSrCoO_4相比,Ln_2SrCo_2O_7(Ln=Sm,Gd)中CoO_2平面上的Co-O键缩短,电子离域化趋势增强,导电能力提高.在300~1100K之间,电阻率与温度关系表明,五个氧化物均表现弱定域系统的特性. 300~1100K之间的磁化率与温度关系表明,在较低温度下,GdSrCoO_4和Gd_2SrCo_2O_7符合Curie-Weiss定律,但前者的CoO_2平面上的磁交换作用是反铁磁性的,而后者是铁磁性的;含Sm~(3+)的三个氧化物表现出较为复杂的磁性质,这可能与Sm~(3+)离子磁性质的复杂性有关.
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本文研究了Dawson结构取代原子数与相应的183WNMR谱中“极位’W原子的化学位移值间的关系,预测广α-1,2-[P2W16Nb2O62]8-α-1-2,3-[P2W15MoNb2O62]8-“极位”W原子183WNMR谱化学位移们,结果α-1,2-[P2W16Nb2O62]8-中与取代Nb相连“极位”W原子的化学位移值为-88ppm,与取代Nb书对称“极位”W原了的化学位移值为-144.7ppm,与取代Nb不对称“极位”W原子的化学位移值为-130.5ppm,α-1-2,3-[P2W15MoNb2O62]8-中与取代Mo对称“极位”W原子的化学位移值为-134.7ppm,与取代Nb对称“极位”W原子的化学位移值为-145.6ppm.
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The title complex, bis(2,6-di-tert-butyl-4-methyl-phenolato-O)tris(tetrahydrofuran-O)samarium tetrahydrofuran solvate, [Sm(C15H23O)2(C4H8O)3].C4H8O, has distorted trigonal bipyramidal geometry around the Sm(II) atom. The 0(2), 0(3) and 0(4) atoms of the
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Three new oxides Sm2SrCo2O7, Sm2BaCo2O7 and Gd2SrCo2O7 have been successfully synthesized by a solid state reaction method.The X - Ray diffraction spectra show that they are all isostructural with Sr8Ti 2O7, Ln2SrCo2O7(Ln=Sm, Gd) crystallized in the tetra