2-[2-(5-溴喹啉)-偶氮]-5-二乙氨基苯酚固相萃取光度法测定环境样品中镉的研究

合成了新试剂2-[2-(5-溴喹啉)-偶氮]-5-二乙氨基苯酚(5-Br-QADEAP),试剂结构通过元素分析,红外光谱和核磁共振氢谱鉴定。研究了5-Br-QADEAP与镉的显色反应,在pH 8.0的硼酸-氢氧化钠缓冲介质中,Triton X-100存在下,5-Br-QADEAP与镉反应生成2∶1稳定络合物,体系最大吸收波长λ_max=595 nm,摩尔吸光系数ε=1.60×105 L·mol-1·cm-1,样品中的镉用强阴离子交换固相萃取柱固相萃取预分离和富集后用该方法测定,方法相对标准偏差在2.5%～3.2%之间,标准回收率在96%～105%,结果令人满意。     

2-(2-喹啉偶氮)-5-二甲氨基酚固相萃取光度法测定锌的研究

研究了新试剂2-(2-喹啉偶氮)-5-二甲氨基酚(QADMAP)与锌的显色反应,在pH 8.5的硼酸-氢氧化钠缓冲介质中,Triton X-100存在下,QADMAP与锌反应生成2∶1稳定络合物,体系最大吸收波长λ_max=590 nm,摩尔吸光系数ε=1.22×105 L·moL-1·cm-1,样品中的锌用强阴离子交换固相萃取柱固相萃取预分离和富集后用该方法测定,结果令人满意。     

2-(2-喹啉偶氮)-1,5-苯二酚固相萃取光度法测定银的研究

研究了新试剂 2 (2 喹啉偶氮 ) 1,5 苯二酚 (QADHB)与银的显色反应 ,在 pH =5 0柠檬酸 氢氧化钠 (内含 0 0 1mol·L- 1 Na2 EDTA)缓冲介质中 ,十二烷基磺酸钠 (SDS)存在下 ,QADHB与银反应生成摩尔比为 2∶1的稳定络合物 ,该络合物可被WatersSep ParkC1 8固相萃取小柱萃取富集。富集在小柱上的络合物用乙醇 (含 1%乙酸 )洗脱后 ,在乙醇介质中 ,其吸收光谱的λmax=5 5 0nm ,ε=6 99× 10 4 L·mol- 1 ·cm- 1 。银含量在 0～ 1 2 μg·mL- 1 范围内符合比尔定律。方法用于环境水样中痕量银的测定 ,结果令人满意     

2-(2-喹啉偶氮)-5-二乙氨基苯胺固相萃取光度法测定痕量钯的研究

根据2-(2-喹啉偶氮)-5-二乙氨基苯胺(QADEAA)与钯的显色反应及MCI-GEL反相固相萃取小柱对显色络合物的固相萃取,建立了一种测定痕量钯的方法。在0.2～2.0 mol·L-1的盐酸介质中,溴化十六烷基三甲胺 (CTMAB) 存在下,QADEAA与钯反应生成2∶1稳定络合物,该络合物可被MCI-GEL 反相固相萃取小柱萃取富集,富集的络合物用丙酮洗脱后用光度法测定,在丙酮介质中体系λ_max＝615 nm,ε＝1.37×105 L·mol-1·cm-1。钯含量在0.01～1.5 mg·L-1内符合比尔定律,方法用于痕量钯的测定,结果令人满意。     

7-(苯并噻唑-2-偶氮)-8-羟基喹啉-5-磺酸与镉显色反应的研究和应用

在 p H4 .8的邻苯二甲酸氢钾 - Na OH介质中 ,非离子表面活性剂 Tween- 80存在下 ,7- (苯并噻唑 - 2 -偶氮 ) - 8-羟基喹啉 - 5 -磺酸 (BTAQS)与镉形成 2∶ 1的紫红色配合物 ,其最大吸收波长 λmax=5 6 0 nm,表观摩尔吸光系数为 8.71× 10 4L· mol-1·cm-1,镉含量在 0— 6 μg/ 10 m L范围内服从比耳定律。用于矿样中镉的测定 ,相对误差小于 3% ,相对标准偏差小于 2 .5 % (n=5 )。     

2-(2-喹啉偶氮)-5-二甲氨基苯胺光度法测定铜

在pH=4.0的磷酸盐缓冲介质中,CTMAB存在下,2-(2-喹啉偶氮)-5-二甲氨基苯胺(QADMAA)与铜反应生成2:1稳定络合物,络合物λmax=580nm,ε=1.14×105L·mol-1·cm-1.铜含量在0.01-0.6μg/mL内符合比耳定律,方法用于环境样品中铜的测定,结果令人满意.     

2-(2-喹啉偶氮)-5-二甲氨基苯酚固相萃取光度法测定铀的研究

合成了新试剂2-(2-喹啉偶氮)-5-二甲氨基苯酚(QADMAP),用红外光谱、核磁共振氢谱、质谱、可见吸收光谱和元素分析鉴定了其结构。研究了QADMAP与铀的显色反应,在pH 7.8的三乙醇胺-盐酸缓冲介质中,Triton X-100和氟离子存在下,QADMAP与铀(Ⅵ)和氟离子反应生成1∶1∶1紫色三元稳定络合物,络合物的λ_max＝590 nm,ε＝1.05×105 L·mol-1·cm-1,铀含量在0～20 μg·10 mL-1内符合比尔定律。环境水样中的铀用TBP萃淋树脂固相萃取柱分离和富集后用该方法测定,方法相对标准偏差在2.2%～3.6%之间,标准回收率在94%～105%。     

2-(2-喹啉偶氮)-4-甲基-1,3-二羟基苯分光光度法测定钒

在 p H为 3.5的柠檬酸 -氢氧化钠缓冲介质中 ,溴化十六烷基三甲基铵 (CTMAB)存在下 ,新试剂 2 -(2 -喹啉偶氮 ) - 4-甲基 - 1,3-二羟基苯 (QAMDHB)与钒发生显色反应 ,生成 2∶ 1稳定络合物 ,最大吸收波长为 5 5 2 nm,摩尔吸光系数 ε=8.0 5× 10 4L· mol-1· cm-1,钒含量在 0— 0 .6 μg/ m L内符合比耳定律。用于几种合金样品中钒的分析 ,结果令人满意。     

微波消化-固相萃取光度法测定生物样品中的钴

根据 2 - (2 -喹啉偶氮 ) - 1,5 -苯二酚 (QADHB)与钴的显色反应及 C18固相萃取小柱对显色络合物的固相萃取 ,建立了一种测定生物样品中痕量钴的新方法。在 p H=4 .0的 HAc- Na Ac缓冲介质中 ,溴化十六烷基三甲基铵 (CTMAB)存在下 ,QADHB与钴反应生成 2∶ 1稳定络合物 ,该络合物可用 C18固相萃取小柱富集 ,小柱上富集的络合物用乙醇 (内含 2 %乙酸 )洗脱后用光度法测定 ,络合物最大吸收波长为5 80 nm,钴含量在 0— 0 .8μg/m L范围内符合比耳定律 ,摩尔吸光系数 ε=5 .6× 10 4L· mol-1·cm-1。本方法用于几种生物样品的分析 ,结果令人满意。     

2-羟基-4-磺酰氨基苯重氮氨基偶氮苯的合成及与锌的显色反应

在 Triton X- 10 0表面活性剂存在下 ,p H=9.5— 11.5的 Na2 B4O7- Na OH缓冲溶液中 ,2 -羟基 - 4-磺酰氨基苯重氮氨基偶氮苯 (HSDAA)与锌 ( )生成 2∶ 1型深红色配合物。最大吸收峰为 λ=5 30 nm处 ,表观摩尔吸光系数为 1.2 4× 10 5L· mol-1· cm-1。 Zn2 的浓度在 0— 4 80μg/L范围内符合比耳定律。用于测定样品中的微量锌 ,结果满意。     

Magnetic ordering in HoRu2Si2, HoRh2Si2, TbRh2Si2 and TbIr2Si2 by neutron diffraction

Neutron diffraction study of polycrystalline HoRu₂Si₂, HoRh₂Si₂, TbRh₂Si₂, and TbIr₂Si₂ was performed in the temperature range between 4.2 and 300 K. For HoRu₂Si₂ the magnetic spin alignment of a linear transverse wave mode below the Néel temperature 19 K is observed. This static moment wave is propagating along the b-axis with k=(0, 0.2, 0) and is polarized in the c-axis. The root-mean-square and maximum saturation moments per Ho atom are 9.26 and 13.09μ_B, respectively. HoRh₂Si₂, TbRh₂Si₂ an TbIr₂Si₂ are simple collinear antiferromagnets of +-+- type with Néel temperatures of (27±1), (98±2) and (72±3) K, respectively. For TbRh₂Si₂ and TbIr₂Si₂ magnetic moments are localized on RE ions only and are aligned along the tetragonal axis, while for HoRh₂Si₂ they form an angle ø = (28±3)°.     

13C-selective IRMPD of CBr2F2/Cl2 and CCl2F2/Br2 systems

The CO₂ TEA laser irradiation of CBr₂F₂ in the presence of Cl₂ yielded ¹³C-enriched CBrClF₂ and ¹³C-enriched CCl₂F₂ under selected experimental conditions. As the photolysis proceeded, the ¹³C concentration of CBrClF₂ decreased gradually and that of CCl₂F₂ increased up to 90% or higher. These results can be explained by the mechanism involving the secondary ¹³C-selective IRMPD of the primary product CBrClF₂. On the other hand, the carbon-containing product for a CCl₂F₂/Br₂ system was only CBrClF₂; the further IRMPD of which probably regenerated CBrClF₂ in the presence of Br₂. The decomposition probabilities of ¹²C- and ¹³C-containing molecules in both systems were measured as functions of laser line, laser fluence, and reactant pressures.     

μ+SR study of LaNi2As2, URh2Si2 and CeRh2Si2

Muon spin relaxation experiments have been carried out in the paramagnetic and magnetically ordered states of URh₂Si₂ and CeRh₂Si₂. As the magnetic structure of these compounds is well known, these measurements can help to characterise their magnetic properties probed by μSR and to understand the μSR results of the heavy fermion compounds of the same crystallographic family. Our measurements show that the muons occupy two different crystallographic sites. The spectra of URh₂Si₂ and CeRh₂Si₂ in the magnetically ordered states are very different, probably reflecting their different magnetic structures. The spectra obtained on CeRh₂Si₂ are similar to the published spectra of the heavy fermion compound CeCu_2.1 Si₂. Muon spin rotation measurements on LaNi₂As₂ indicate that the muon is diffusing at 150 K.     

Eu2+掺杂CaSi2O2N2荧光粉发光性能

采用固相反应法合成了组成为Ca_1-xEu_xSi₂O₂N₂的Eu²⁺掺杂CaSi₂O₂N₂荧光粉.通过荧光光谱对样品的发光性能进行了研究,发现Eu²⁺掺杂CaSi₂O₂N₂荧光粉发射光谱为宽波段的单峰结构,主要包含绿光和黄光区,发射峰在556~568 nm.从发射光谱的宽带特征来看,CaSi₂O₂N₂:Eu²⁺的发射主要对应着Eu²⁺离子4f⁶5d→4f⁷跃迁.从激发光谱所覆盖的范围还可以看到,样品可以有效的被UV蓝-光激发,这意味着该类荧光粉在白光LED方面有可能得到广泛的应用.另外,样品的发光性能与激发离子的浓度有着很大关系.激发离子浓度增大时,发射光谱会发生明显红移.利用这一性质,可以通过改变Eu²⁺浓度来调节荧光粉的发光范围,从而满足不同场合的需要.同时,Eu²⁺浓度提高,样品发射光谱的强度也会随之增强,在x=0.06时发射强度达到最大值,之后继续增加Eu²⁺浓度,强度不仅没有增加反而降低,即出现浓度猝灭现象.     

Magnetostriction of SmMn2Ge2 and GdMn2Ge2 intermetallic compounds

Longitudinal and transverse magnetostrictions of polycrystalline samples of intermetallic compounds RMn₂Ge₂ (R=Sm or Gd) are measured in pulsed magnetic fields up to 250 kOe. It is found that linear magnetostrictive strains of about 10^?3 arise in a temperature range in which the magnetic field causes a change in the magnetic state of a manganese magnetic subsystem. The results obtained are described within the model of a two-sublattice ferrimagnet with a negative exchange interaction in the manganese subsystem in terms of a strong dependence of this interaction on interatomic distances.     

Polar optic phonons in Hg2Cl2 and Hg2Br2

Far infrared (30–430 cm^?1) reflectivity measurements of Hg₂Cl₂ and Hg₂Br₂ single crystals have been performed in polarized light. The spectra, which are in agreement with group-theoretical predictions, were analyzed by the oscillator fitting procedure and Kramers-Kronig method. The results are compared with the existing data from other measurements and the large anisotropy of polar modes is briefly discussed. The polarization vectors of all long-wavelength symmetry modes were determined group-theoretically.     

Superconductivity in LaPd_2Bi_2 with CaBe_2Ge_2-type structure

正Since the discovery of superconductivity in LaFeAsO_(1-x)F_x,the high-T_c iron-based superconductors have been extensively studied from both experimental and theoretical viewpoints [1-8]. However, the mechanism of the unconventional superconductivity is still to be resolved. To     

X-ray photoemission spectra measurements of CeNi2Sb2 and CeCu2Sb2

X-ray photoemission spectra, resistivity and susceptibility of CeNi₂Sb₂ and CeCu₂Sb₂ were measured and are discussed. The results indicate that these alloys are Kondo systems. For comparison of the valence band properties, the spectra of the isostructural alloys of RT₂X₂-type with R = La, Gd, T = Cu, Ni and X = Sn, Sb were investigated, too.