多酸-介孔分子筛复合材料的制备、表征及光催化活性

采用浸渍法将具有光催化活性的多金属氧酸盐(polyoxometalate,POM)磷钨酸和硅钨酸负载到介孔分子筛MCM-41,制备了H3PW12O40/MCM-41和H4SiW12O40/MCM-41两种复合材料,以红外光谱(FT-IR)、X射线衍射(XRD)、N2吸附、高分辨透射电镜(HRTEM)等分析手段对所合成的多酸-分子筛复合材料进行了表征,并以农药百草枯的光催化降解考察了复合材料的光催化活性。所合成的复合材料同时保留了母体多酸的Keggin特征结构和载体MCM-41分子筛均匀的六方孔道结构,比表面积超过200m2.g-1。用于农药百草枯的光催化降解实验表明,两种复合材料均具有较高的光催化活性。在365nm紫外光辐照下,以H3PW12O40/MCM-41和H4SiW12O40/MCM-41为催化剂催化反应14h后,百草枯(10mg.L-1)的降解转化率分别达到92.0%和87.6%,反应符合一级化学动力学模型,半衰期分别为3.7和4.6h。     

H_3PW_(12)O_(40)/MCM-48的制备及其光催化降解农药(英文)

以介孔分子筛MCM-48为载体,采用水热法制备了负载磷钨酸H3PW12O40(HPW)的多金属氧酸盐催化剂HPW/MCM-48。利用傅里叶变换红外光谱(FT-IR)、小角度X射线粉末衍射(XRD)、氮气吸附检测和高分辨透射电子显微镜(HRTEM)对其结构进行了表征,并以农药吡虫啉和百草枯为对象,考察了所制备的HPW/MCM-48的光催化降解活性。结果表明,采用水热法制备的催化剂保持了MCM-48的介孔分子筛结构和HPW的Keggin结构,比表面积783.35m2·g-1,孔体积1.46cm3·g-1,平均孔径2.76nm,相比于母体HPW,HPW/MCM-48的比表面积大大增加;在365nm紫外光下反应14h后,20mg剂量HPW/MCM-48催化剂能使50mL,10mg·L-1吡虫啉和百草枯的降解率分别达57.38%和63.79%,而HPW对两种农药的降解率在25%左右,空白组降解率均低于5%,说明负载后HPW对两农药的降解活性显著增强。动力学考察表明,HPW/MCM-48对农药降解过程符合一级动力学方程,对吡虫啉和百草枯这两种农药的降解速率常数Ka分别为0.089和0.117h,半衰期t1/2为7.8和5.9h。     

可见光响应SO_4~(2-)/Ce-TiO_2的光谱特征及催化性能

采用溶胶-凝胶法制备了Ce掺杂TiO_2,经H_2SO_4处理得到酸化Ce掺杂TiO_2。利用X射线衍射(XRD)、傅里叶变换红外光谱(FTIR)、吡啶吸附红外光谱(Py-FTIR)、紫外-可见光漫反射光谱(UV-Vis)及X射线光电子能谱(XPS)技术对样品的性质进行了表征,以罗丹明B(RhB)在样品上的可见光催化降解为模型反应,评价了所制备样品的光催化性能。XRD测试结果表明,铈掺杂使TiO_2产生晶格缺陷、粒径减小,有利于光生电荷的转移,继而提高催化剂的活性;FTIR谱图说明SO_4~(2-)以桥式双齿配位吸附形式存在;PyFTIR谱图显示,酸化铈掺杂TiO_2样品表面同时存在Brnsted和Lewis酸位,但以Lewis酸为主。Lewis酸中心的缺电子性质有利于样品表面的光生电子与光生空穴分离,从而改善催化剂的活性;UV-Vis结果表明,Ce掺杂减小了TiO_2的带隙能,引入的杂能级能够捕获导带上的光生电子和价带上的光生空穴,降低光生电子-空穴对的复合几率;同时还可以使能量较小的光子激发杂能级上捕获的电子,拓宽光响应范围;XPS分析表明SO2-4/Ce-TiO_2样品上同时存在Ce3+/Ce4+的混合价态,Ce~(3+)/Ce~(4+)氧化-还原转换有助于TiO_2受光激发后产生的光生电子和空穴的分离,从而提高光量子效率。酸化Ce掺杂TiO_2对RhB的可见光催化降解反应有很好的活性,实验结果证明,H_2SO_4酸化和Ce掺杂的协同作用改善了样品的可见光响应,促进了其可见光催化反应活性。     

可见光响应SO2－4／Ce-TiO2的光谱特征及催化性能

采用溶胶‐凝胶法制备了Ce掺杂 T iO2,经 H2 SO4处理得到酸化Ce掺杂 T iO2。利用X射线衍射（XRD）、傅里叶变换红外光谱（FTIR）、吡啶吸附红外光谱（Py‐FTIR）、紫外‐可见光漫反射光谱（UV‐Vis）及X射线光电子能谱（XPS）技术对样品的性质进行了表征,以罗丹明B（RhB）在样品上的可见光催化降解为模型反应,评价了所制备样品的光催化性能。XRD测试结果表明,铈掺杂使 TiO2产生晶格缺陷、粒径减小,有利于光生电荷的转移,继而提高催化剂的活性;FTIR谱图说明SO2－4以桥式双齿配位吸附形式存在;Py‐FTIR谱图显示,酸化铈掺杂TiO2样品表面同时存在Br?nsted和Lewis酸位,但以Lewis酸为主。Lewis酸中心的缺电子性质有利于样品表面的光生电子与光生空穴分离,从而改善催化剂的活性;UV‐Vis结果表明,Ce掺杂减小了TiO2的带隙能,引入的杂能级能够捕获导带上的光生电子和价带上的光生空穴,降低光生电子‐空穴对的复合几率;同时还可以使能量较小的光子激发杂能级上捕获的电子,拓宽光响应范围;XPS分析表明SO2－4／Ce‐TiO2样品上同时存在Ce3＋／Ce4＋的混合价态,Ce3＋／Ce4＋氧化‐还原转换有助于TiO2受光激发后产生的光生电子和空穴的分离,从而提高光量子效率。酸化Ce掺杂TiO2对RhB的可见光催化降解反应有很好的活性,实验结果证明,H2 SO4酸化和Ce掺杂的协同作用改善了样品的可见光响应,促进了其可见光催化反应活性。     

CuO/Cu2(OH)3Cl的制备及其光催化降解染料光谱性能研究

以CuCl2和NaOH为原料、微波液相加热法制得CuO/Cu2(OH)3Cl粉体作为光催化剂,XRD和FTIR进行了表征.用光度分析法测定了不同光源、溶液的酸度、催化剂的用量、光照时间等条件对染料脱色率的影响.结果表明,用太阳光作为光源照射4h,溶液的酸度为pH8,CuO/Cu3(OH)3 Cl的用量为40 mg/50 mL,氨基黑、靛蓝二磺酸钠等染料脱色率达到90%以上.加入Fe3 ,H2O2等其他物质可提高染料的脱色率.通过红外光谱和紫外光谱分析,表明染料分子在催化剂和光照条件下发生了降解.     

Mn_2[V_(12)B_(16)O_(52)(OH)_6](en)_2(H_3O)_6(H_2O)_5(en=ethylenediamine)的结构及谱学研究

采用水热合成法合成了一种结构新颖的多硼钒氧簇化合物Mn2[V12B16O52(OH)6](en)2(H3O)6(H2O)5(en=ethylenediamine)1,通过单晶X射线衍射确定该化合物的结构。化合物1中,在ab平面上,簇单元之间通过[Mn(H2O)2]2+连接成二维层状结构,另外,层与层之间在c方向上通过氢键连接成三维空间结构。此外,对化合物1的谱学性质进行了红外光谱、磁和热微扰下的二维红外相关光谱、紫外-可见固体漫反射光谱分析,探讨了其结构与谱学性质的关系。磁微扰的二维红外相关光谱表明B—O,V—O—V和Mn—O—B的伸缩振动对于磁场的变化比较敏感,热微扰的二维红外相关光谱表明B—OH,B—O,V—O—V和Mn—O—B的伸缩振动对热微扰比较敏感。     

微波场辅助银掺杂TiO2薄膜光催化降解甲基橙溶液的实验研究

用紫外-可见吸收光谱仪和原子力显微镜(AFM)表征了制备的TiO2和Ag/TiO2薄膜的光谱特性和表面形貌,研究了掺杂改性、微波场辅助作用以及两者相结合的光催化降解方法的薄膜催化活性.结果表明:催化剂的掺杂改性与微波场辅助作用相结合的光催化降解效果优于微波场辅助光催化方法和银掺杂光催化方法.     

Cu掺杂SnO_2/TiO_2复合薄膜的制备及性能研究

制备Cu掺杂的纳米Sn O2/Ti O2溶胶,采用旋涂法在载玻片上镀膜,经干燥、煅烧制得Cu掺杂的Sn O2/Ti O2薄膜,通过对比实验探讨掺杂比例、条件、复合形式等对结构和性能的影响。采用XRD、SEM、EDS、UVVis等测试手段对样品进行表征,并以甲基橙为探针考察了其光催化降解性能。XRD测试结果显示薄膜的晶型为锐钛矿型,结晶度较高。SEM谱图显示薄膜表面无明显开裂,粒子分布均匀,粒径约为20 nm。EDS测试结果表明薄膜材料中含有Cu元素,谱形一致。UV-Vis吸收光谱表明Cu掺杂以及Sn O2/Ti O2的复合使得在近紫外区的光吸收比纯Ti O2明显增强。光催化实验表明Cu掺杂后使得Sn O2/Ti O2复合薄膜对甲基橙的光催化降解效率进一步提高,Sn O2/Ti O2复合薄膜的光催化活性在10%Cu掺杂时达到最高。     

一种新型钼磷酸盐杂多化合物(NH3CH2CH2NH3)7H2[NaMo12O30(PO4)2(HPO4)5(H2PO4)]·7H2O的合成和光谱研究

本文采用水热反应条件 ,合成得到一种新型的含五价钼原子的杂多化合物 :(NH3CH2 CH2 NH3) 7H2[NaMo1 2 O30 (PO4 ) 2 (HPO4 ) 5(H2 PO4 ) ]·7H2 O ,在晶体结构测定的基础上对其进行红外、拉曼和紫外 可见漫反射光谱研究。结果表明 :较长的Mo(Ⅴ )—O键键长和分子内大量的氢键造成化合物红外光谱特征的红移。     

Visible-Light Activities of Erbium Doped BiVO4 Photocatalysts

采用水热合成法,制备出Er掺杂的BiVO₄复合光催化剂,并采用XRD、SEM、XPS和紫外-可见漫反射光谱技术对其进行分析表征．通过可见光下降解水溶液中甲基橙分子来考察其光催化性能,结果显示掺杂组份以氧化物Er₂O₃形式存在于的复合光催化剂中;且掺杂复合光催化剂的可见光吸收和催化活性都比纯BiVO₄有所增强．     

The magnetic structure of Cs0.4 Mn0.4 Fe1.6 F6 and of Cs0.4 Ni0.4 Fe1.5 F6

The magnetic structure of the two compounds as determined by neutron diffraction is reported. Both compounds are antiferromagnetic with Néel-temperatures of 115 and 100 K respectively. Both compounds show a very pronounced diffuse scattering.     

Lithium motion in Li0.33 TiS2 and Li0.94 TiS2

We have studied the motion of lithium ions in Li_xTiS₂ (x = 0.33, 0.94) using pulsed NMR techniques. The temperature dependences of the spin lattice relaxation in the rotating frame (T_1?) suggest comparable activation energies for lithium ion diffusion for both samples, 3370 K, but an appreciably longer hopping time for the x = 0.94 sample. Low temperature values of T₂ agree with calculated and measured second moments for both materials.     

The ν3 and 2ν3 bands of SO3, SO3, SO3, and SO3

This sixth of a series of publications on the high-resolution rotation-vibration spectra of sulfur trioxide reports the results of a systematic study of the ν₃ and 2ν₃ infrared bands of the four symmetric top isotopomers ³²S¹⁶O₃, ³²S¹⁸O₃, ³⁴S¹⁶O₃, and ³⁴S¹⁸O₃. An internal coupling between the l=0(A₁^′) and l=2(E^′) levels of the 2ν₃ states was observed. This small perturbation results in a level crossing between |k−l|=9 and 12, in consequence of which the band origins of the A₁^′,l=0 “ghost” states could be determined to a high degree of accuracy. Ground and upper state rotational constants as well as vibrational anharmonicity constants are reported. The constants for the center-of-mass substituted species ³²S¹⁶O₃ and ³⁴S¹⁶O₃ vary only slightly, as do the constants for the ³²S¹⁸O₃, ³⁴S¹⁸O₃ pair. The S-O bond lengths for the vibrational ground states of the species ³²S¹⁶O₃, ³⁴S¹⁶O₃, ³²S¹⁸O₃, and ³⁴S¹⁸O₃ are, respectively, 141.981 99(1), 141.979 38(6), 141.972 78(8), and 141.969 93(8) pm, where the uncertainties, given in parentheses, are two standard deviations and refer to the last digits of the associated quantity.     

Wing profile measurements of the Na-doublet lines in C2H2/O2/N2, H2/O2/N2 and H2/O2/Ar frames at 1 atm

Fluorescence-excitation (wing) profiles of the Na-D doublet lines were measured over a wavelength range extending from 0.3 to 200 Å from the line center for the red D₁ and blue D₂ wings and from 0.3 to 3 Å for the red D₂ and the blue D₁ wings, respectively. The line profiles were determined with the aid of a tunable CW dye-laser as a background source by measuring the total fluorescence intensity observed on detuning the laser wavelength. The flames were premixed, laminar, shielded flames at 1 atm, with temperatures ranging from 1860 to 2270 K; N₂ and Ar served as diluent gases. The line core and near-wing profiles (i.e. the region covering 0.3<Δλ<7 Å for the outer wings and 0.3<Δλ<3 Å for the inner ones) in all of the flames studied appeared to have the same frequency dependence, regardless of the nature and concentrations of the gases used. The blue D₂-line profile followed an unexpected (-2.2) law, while the other three profiles obeyed the theoretically expected (-2) law (the dispersion profile function). The line profile in the Δλ range between the impact and quasistatic regions was found to depend on the main perturbers involved. We found that the far blue D₂- and red D₁-wings in the Ar-diluted H₂/O₂ flame obeyed the (-$\text{5}\text{4}$) and (-$\text{3}\text{2}$) laws, respectively, as predicted by the quasi-static theory for the Lennard-Jones interaction. For the N₂-diluted C₂H₂/O₂ and H₂/O₂ flames, we did not find these wing dependences in the Δλ range investigated.     

The ν9 + ν11 − ν11, ν10 + ν11 − ν11 hot band system in allene-d4

The hot band system ν₉ + ν₁₁ ? ν₁₁, ν₁₀ + ν₁₁ ? ν₁₁ in allene-d₄ was studied at a resolution near 0.010 cm^?1. About 1500 partly overlapped hot band rotational lines were assigned and fitted to a model taking into account z-Coriolis resonance between the combination levels ν₉ + ν₁₁ and ν₁₀ + ν₁₁ as well as vibrational l-type resonances within these levels. Upperstate constants have been derived from an analysis in which the constants for the ν₁₁ level were constrained. A detailed study of rotational as well as vibrational l-type doublings occurring in the KΔK = ?1 subband is presented, and the sign of vibrational l-type doubling constants for the ν₁₀ + ν₁₁ level is determined. A localized (x, y)-Coriolis resonance between ν₁₀ + ν₁₁ and ν₄(B₁) + ν₁₁ is discussed and the interaction parameter is obtained as well as some constants for ν₄ + ν₁₁.     

Magnetic susceptibility studies of (CH2)3(NH3)2FeCl2Br2 and (CH2)6(NH3)2FeCl2Br2

The magnetic susceptibility of the layered compounds (CH₂)₃(NH₃)₂FeCl₂Br₂ and (CH₂)₆(NH₃)₂FeCl₂Br₂ has been measured in the range 80 < T < 300 K. The results follow a Curie-Weiss behavior in the range 120 < T < 300 K but are field dependent for T < 120 K. The results are interpreted in terms of a two-dimensional antiferromagnetic interaction which is canted. A comparison with the corresponding pure chloride compounds is given.     

High-pressure Raman spectroscopic studies on orthophosphates Ba3(PO4)2 and Sr3(PO4)2

By using diamond anvil cell (DAC), high-pressure Raman spectroscopic studies of orthophosphates Ba₃(PO₄)₂ and Sr₃(PO₄)₂ were carried out up to 30.7 and 30.1 GPa, respectively. No pressure-induced phase transition was found in the studies. A methanol:ethanol:water (16:3:1) mixture was used as pressure medium in DAC, which is expected to exhibit nearly hydrostatic behavior up to about 14.4 GPa at room temperature. The behaviors of the phosphate modes in Ba₃(PO₄)₂ and Sr₃(PO₄)₂ below 14.4 GPa were quantitatively analyzed. The Raman shift of all modes increased linearly and continuously with pressure in Ba₃(PO₄)₂ and Sr₃(PO₄)₂. The pressure coefficients of the phosphate modes in Ba₃(PO₄)₂ range from 2.8179 to 3.4186 cm⁻¹ GPa⁻¹ for ν₃, 2.9609 cm⁻¹ GPa⁻¹ for ν₁, from 0.9855 to 1.8085 cm⁻¹ GPa⁻¹ for ν₄, and 1.4330 cm⁻¹ GPa⁻¹ for ν₂, and the pressure coefficients of the phosphate modes in Sr₃(PO₄)₂ range from 3.4247 to 4.3765 cm⁻¹ GPa⁻¹ for ν₃, 3.7808 cm⁻¹ GPa⁻¹ for ν₁, from 1.1005 to 1.9244 cm⁻¹ GPa⁻¹ for ν₄, and 1.5647 cm⁻¹ GPa⁻¹ for ν₂.     

正磷酸盐晶体Ba3(PO4)2和Sr3(PO4)2高温拉曼光谱研究

测量了碱土金属正磷酸盐Ba₃(PO₄)₂和Sr₃(PO₄)₂常温及高温拉曼光谱, 对拉曼振动模式进行指认, 并分析了晶体拉曼振动光谱及晶体结构在高温下的变化. 在温度升高的过程中, 拉曼振动频率向低频移动且振动峰宽度展宽, 晶体中的P-O平均键长随温度升高而变长, 但O-P-O的键角并未发生变化. 晶体在900 ℃以下无结构相变发生. 关键词： 3(PO₄)₂和Sr₃(PO₄)₂')" href="#">Ba₃(PO₄)₂和Sr₃(PO₄)₂ 高温拉曼光谱 振动模式 高温结构     

The ν2, 2ν2, 3ν2, ν4, and ν2 + ν4 bands of 15NH3

The ir absorption of gaseous ¹⁵NH₃ between 510 and 3040 cm^?1 was recorded with a resolution of 0.06 cm^?1. The ν₂, 2ν₂, 3ν₂, ν₄, and ν₂ + ν₄ bands were measured and analyzed on the basis of the vibration-rotation Hamiltonian developed by V. ?pirko, J. M. R. Stone, and D. Papou?ek (J. Mol. Spectrosc.60, 159–178 (1976)). A set of effective molecular parameters for the ν₂ = 1, 2, 3 states was derived, which reproduced the transition frequencies within the accuracy of the experimental measurements. For ν₄ and ν₂ + ν₄ bands the standard deviation of the calculated spectrum is about four times larger than the measurements accuracy: a similar result was found for ν₄ in ¹⁴NH₃ by ?. Urban et al. (J. Mol. Spectrosc.79, 455–495 (1980)). This result suggests that the present treatment takes into account only the most significant part of the rovibration interaction in the doubly degenerate vibrational states of ammonia.     

合成反铁磁Ni81Fe19/Co90Fe10/Ru/Co90Fe10/Ni81Fe19的研究

采用直流磁控溅射方法制备了一系列的合成反铁磁及以其为自由层的自旋阀.研究发现,在Ni₈₁Fe₁₉与Ru层之间插入适当厚度的Co₉₀Fe₁₀层后,可有效地提高合成反铁磁两磁性层间的反铁磁耦合强度,得到具有饱和场H_s更高、饱和磁化强度M_s更低、热稳定性更好的合成反铁磁.另外,以这种合成反铁磁作自旋阀的自由层时,可有效提高自旋阀的稳定性. 关键词： 合成反铁磁 退火 自旋阀