镁热还原催化合成亚稳态立方相氮化硼e-BN纳米多晶粉

以无水氯化钴(CoCl₂)为催化剂, 采用氧化硼(B₂O₃)和氯化铵(NH₄Cl)为反应原料与镁粉在密闭反应釜内发生镁热还原反应合成了亚稳态立方氮化硼(e-BN)多晶粉. 产物粉末的X光衍射(XRD)分析表明晶格常数a＝0.8304 nm, 红外光谱(FTIR)在500, 650, 797, 1085, 1374和1580 cm^－1有特征吸收峰. 扫描电子显微镜(SEM)观察到产物为近似球状颗粒, 平均直径为70 nm, 粒径均匀. 讨论了化学反应和产物在催化剂作用下的形成机理.     

LnBaB9O16:Eu3+(Ln=La,Y)的结构与荧光性质

利用电子衍射、X射线衍射和荧光光谱等方法研究了LnBaB₉O₁₆(Ln=La,Y)的结构特性.LnBaB₉O₁₆为单斜晶系,其中LaBaB₉O₁₆的晶胞参数a=1.3660nm,b=0.7882nm,c=1.6253nm,β=106.15°;YBaB₉O₁₆的晶胞参数a=1.3476nm,b=0.7776nm,c=1.6040nm,β=106.38°.荧光光谱研究表明,这两种化合物结构不同,Y³⁺在YBaB₉O₁₆结构中处于中心对称格位,而LaBaB₉O₁₆中La³⁺的格位则无中心对称性.Gd³⁺部分取代LaBaB₉O₁₆:Eu³⁺中的La³⁺可改善Eu³⁺离子的发光性质.LaBaB₉O₁₆:Eu³⁺在真空紫外区的吸收比较弱,这可能与硼氧比较小有关.     

2-呋喃甲酸锶的晶体结构

在水溶液中合成并培育了2-呋喃甲酸锐Sr₆(C₅H₃O₃)₁₂单晶。经元素分析、红外光谱、差热热重分析、密度测定以及X射线衍射结构分析确定了该化合物的组成、结构和部分性质。结构分析结果表明:该晶体属单斜晶系,空间群P2₁/n,a=2.3090(7)nm,b=1.3376(4)nm,c=2.3093(6)nm,β=107.06(2)°,Z=4,R=0.0603.D_c=1.82×10³kg/m³,D_m=1.81×10³kg/m³.化合物通过羧氧桥联形成三维网状结构,其中Sr-O键的平均键长为0.2641nm,而Sr-O(羧氧)为0.2535nm,Sr-O(呋喃环氧)为0.2861nm.     

γ-Fe2O3纳米纤维的丙酮敏感特性

采用静电纺丝法制备了PVP/FeC₆H₅O₇复合纳米纤维, 并将复合纤维在500 ℃高温烧结3 h, X射线衍射分析(XRD)表明, 烧结后的产物为正尖晶石结构的γ-Fe₂O₃晶体. 扫描电子显微镜(SEM)观测结果表明, 制得了直径均匀、 连续的复合纳米纤维, 其平均直径约为1000 nm; 烧结后的γ-Fe₂O₃纳米纤维保持了其连续性, 但纤维发生了收缩, 直径较烧结前小, 平均约为600 nm. 比表面积分析表明, γ-Fe₂O₃纳米纤维比表面积为57.18 m²/g. 气敏性能测试结果表明, 230 ℃为γ-Fe₂O₃纳米纤维检测丙酮气体的最佳工作温度. 在此温度下, γ-Fe₂O₃纳米纤维对丙酮气体表现出高响应度[S=6.9, c(Acetone)=7.88×10⁴ mg/m³]和线性度(7.88×10²~1.58×10⁵ mg/m³浓度范围内). 同时, γ-Fe₂O₃纳米纤维气体传感器件还表现出良好的长期稳定性.     

Fe3O4和Zn2+掺杂型Zn1-xFe2+xO4纳米晶的溶剂热合成和电磁性能

利用溶剂热法, 在醋酸钠静电保护剂的辅助下, 成功制备出Fe₃O₄和Zn²⁺掺杂型Zn_0.07Fe_2.93O₄纳米晶. 利用X射线衍射仪和扫描电子显微镜等对样品的晶体结构、粒径、形貌和化学组成进行了分析. 结果表明, 所得纳米晶的粒径均匀, 形貌为球形, 分散度好; Zn_0.07Fe_2.93O₄纳米晶的平均粒径(70 nm)明显小于Fe₃O₄(170 nm). 磁性能测量结果表明, 室温下Zn_0.07Fe_2.93O₄的饱和磁化强度(54.2 A·m²·kg^-1)小于Fe₃O₄ (81.6 A·m²·kg^-1). 利用矢量网络分析仪对样品的电磁性能和吸波性能进行了研究. 结果表明, Zn²⁺掺杂型Zn_0.07Fe_2.93O₄纳米晶的吸波性能优于Fe₃O₄, 前者的最大吸收峰(-19.3 dB)大于后者(-9.8 dB), 且吸收峰低于-10 dB的峰宽达2.5 GHz.     

纳米晶(CeO2)1-x(BiO1.5)x固溶体的水热合成与离子输运性质研究

在240℃水热体系中首次合成出系列纳米晶固溶体(CeO₂)_1-x(BiO_1.5)_x(x=0.0～0.50).产物采用X射线衍射,扫描电子显微镜和X射线光电子能谱仪进行表征.Bi₂O₃在CeO₂中的固溶限约为50%.所有固溶体结晶属立方萤石结构,粒度范围为10～18nm.当Bi₂O₃掺杂量小于固溶限时,于800℃烧结不会导致结构转变.而对于(CeO₂)_0.5(BiO_1.5)_0.5,于800℃在空气中烧结将导致固溶限降低.Bi₂O₃含量低于固溶限时,固溶体只具有体电导,而(CeO₂)_0.6(BiO_1.5)_0.4的总电导可分为体电导和晶界电导.体电导为氧离子,而晶界为来自电极的银离子.     

2-吡咯类酰腙的合成、晶体结构及与小牛胸腺DNA的相互作用

以2-吡咯甲酰肼与2,4-二羟基苯甲醛和2-羟基-3-甲氧基苯甲醛经缩合反应合成2,4-二羟基苯甲醛-2-吡咯甲酰腙C₁₂H₁₁N₃O₃(Ⅰ)和2-羟基-3-甲氧基苯甲醛-2-吡咯甲酰腙C₁₃H₁₅N₃O₄(Ⅱ),并利用红外光谱、元素分析、¹H NMR、X射线单晶衍射和热重分析进行表征,结果表明晶体Ⅰ属单斜晶系,空间群为P2₁/c,Z=4,晶胞参数为a=1.2586(4) nm,b=0.8050(3) nm,c=1.1914(4) nm;晶体Ⅱ为正交晶系,空间群为P2₁2₁2₁,Z=4,晶胞参数为a=0.4756(2) nm,b=1.2491(6) nm,c=2.2145(11) nm。 热重结果显示,化合物Ⅰ和Ⅱ最大热分解峰分别出现在267.59和284.79 ℃,表观活化能分别为176.6和122.9 kJ/mol,表明化合物Ⅰ和Ⅱ具有较高的热稳定性。 利用粘度实验和微量热实验研究了化合物Ⅰ和Ⅱ与CT-DNA的相互作用,均显示两种化合物均与CT-DNA发生了插入作用,且相互作用过程放热,焓变值分别为ΔH(Ⅰ)=4.67 kJ/mol和ΔH(Ⅱ)=4.40 kJ/mol。     

基于碳量子点过氧化物模拟酶的肌氨酸比色测定

以果皮为原料制备了水溶性碳量子点(CQDs), 透射电子显微镜分析表明其平均粒径为2.4 nm; 红外光谱分析证实CQDs表面富含含氧官能团. 所得CQDs可催化H₂O₂氧化3,3',5,5'-四甲基联苯胺(TMB)生成蓝色氧化产物(ox-TMB). 基于上述反应, 建立了测定H₂O₂的分析方法, 在pH=3.5, 温度40 ℃, TMB浓度为1.0 mmol/L及孵育时间15 min的条件下, 当H₂O₂浓度在5.0~100 μmol/L范围时, ox-TMB的吸光度随H₂O₂浓度的升高而线 性增强, 方法的检出限为3.0 μmol/L. 鉴于H₂O₂是肌氨酸氧化酶催化肌氨酸氧化的产物之一, 建立了CQDs催化H₂O₂氧化TMB间接测定肌氨酸的分析方法. 结果表明, 当肌氨酸浓度在0.5~350 μmol/L范围内时, 吸光度 与其浓度呈良好的线性关系, 方法的检出限为0.3 μmol/L; 将该方法应用于人体尿样的测定, 回收率为94%~99%.     

磁性介孔纳米粒子的制备及对抗癌药紫杉醇的传输

以十六烷基溴化铵(CTAB)为结构导向剂, 正硅酸乙酯(TEOS)为硅源, 在碱性环境下经过自组装过程对单分散性磁性Fe₃O₄纳米粒子进行包覆, 制备出磁性硅基介孔纳米粒子Fe₃O₄@SiO₂. 结合X射线衍射、 傅里叶变换红外光谱(FTIR)、 透射电子显微镜(TEM)以及氮气吸附-脱附等技术对Fe₃O₄@SiO₂粒子进行表征. 结果表明Fe₃O₄@SiO₂纳米粒子具有球形形貌, 平均直径约为150 nm, 蠕虫状介孔结构, 比表面积为932 m²/g, 孔径为2.5 nm且分布较均匀, 包覆后Fe₃O₄的结构得以保持, 同时材料具有很好的磁响应能力. 以抗癌药紫杉醇(Paelitaxel, TXL)为模型药物进行负载, 实验结果表明, Fe₃O₄@SiO₂对TXL的负载能力为80 mg/g, TXL-Fe₃O₄@SiO₂对TXL的缓释时间持续120 h以上, 累积释放量达到30 mg/g. 通过噻唑蓝比色(MTT)法测量了TXL-Fe₃O₄@SiO₂粒子对体外培养的HeLa细胞的细胞毒性, 与相同浓度的TXL相比, TXL-Fe₃O₄@SiO₂对HeLa细胞的抑制率明显增高.     

SiO2@Fe2O3核-壳结构催化剂的制备及表征

采用优化的Stöber法制备了平均粒径为230 nm的单分散球形SiO₂颗粒,并以此为内核,通过水解沉积法制备了不同壳层厚度的核-壳结构SiO₂@Fe₂O₃催化剂。采用扫描电子显微镜(SEM)、透射电子显微镜(TEM)、N₂物理吸附和X射线衍射分析(XRD)等手段对催化剂进行表征,探讨了不同制备条件对SiO₂@Fe₂O₃催化剂形貌的影响。结果表明,通过水解沉积法制备的SiO₂@Fe₂O₃催化剂具有明显的核-壳结构,并且保持了原始SiO₂核的球形形貌,Fe₂O₃纳米粒子通过-OH的氢键作用连接在SiO₂表面,形成了2~10 nm厚的Fe₂O₃均匀连续包覆层。     

毛刺状竹节结构氮化硼纳米管的合成与生长机理

以非晶硼和氧化镍纳米颗粒为原料,在氨气中1100℃下合成了毛刺状竹节结构的氮化硼纳米管. 利用X射线衍射和透射电镜研究了氮化硼纳米管的结构和形貌. 竹节结构纳米管表面的毛刺是六方氮化硼的纳米薄片. 提出了一种基于固态硼和气态二氧化硼扩散的毛刺形貌生长机理.     

Orthonitridoborate ions [BN3]6- in oxonitridosilicate cages: synthesis, crystal structure, and magnetic properties of Ba4Pr7[Si12N23O][BN3], Ba4Nd7[Si12N23O][BN3], and Ba4Sm7[Si12N23O][BN3

The isotypic title compounds Ba4Pr7[Si12N23O][BN3], Ba4Nd7[Si12N23O][BN3], and Ba4Sm7[Si12N23O][BN3] were prepared by reaction of Pr, Nd, or Sm, with barium, BaCO3, Si(NH)2, and poly(boron amide imide) in nitrogen atmosphere in tungsten crucibles using a radiofrequency furnace at temperatures up to 1650 C. They were obtained as main products (approximately 70%) embedded in a very hard glass matrix in the form of intense dark green (Pr), orange-brown (Sm), or dark red (Nd) large single crystals, respectively. The stoichiometric composition of Ba4Sm7[Si12N23O][BN3] was verified by a quantitative elemental analysis. According to the single-crystal X-ray structure determinations (Ba4Ln7[Si12N23][BN3], Z= , P6 with Ln = Pr: a = 1225.7(1), c = 544.83(9) pm, R1 = 0.013, wR2 = 0.030; Ln = Nd: a = 1222.6(1), c = 544.6(1) pm, R1 = 0.017, wR2 = .039; Ln = Sm: a = 1215.97(5), c = 542.80(5) pm, R1 = 0.047, wR2 = 0.099) all three compounds are built up by a framework structure [Si12N23O]23- of corner-sharing SiX4 tetrahedrons (X = O, N). The oxygen atoms are randomly distributed over the X positions. The trigonal-planar orthonitridoborate ions [BN3]6- and also the Ln(3)3+ are situated in hexagonal cages of the framework (bond lengths Si-(N/O) 169-179 pm for Ln=Pr). The remaining Ba2+ and Ln3- ions are positioned in channels of the large-pored network. The trigonal-planar [BN3]6- ions have a B-N distance of 147.1(6) pm (for Ln = Pr). Temperature-dependent susceptibility measurements for Ba4Nd7[Si12N23O][BN3] revealed Curie-Weiss behavior above 60 K with an experimental magnetic moment of muexp = 3.36(5) microB/Nd. The deviation from Curie-Weiss behavior below 60 K may be attributed to crystal field splitting of the J = 9/2 ground state of the Nd3+ ions. No magnetic ordering is evident down to 4.2 K.     

高温高压Li3N-hBN体系cBN转变的热力学分析

以经典热力学第二定律ΔG<0为依据,分析了静态高温高压触媒法合成立方氮化硼(cBN)过程中发生的可能反应.考虑温度和压强对反应物相体积的影响,计算了六方氮化硼(Li3N-hBN)体系中hBN+Li3N→Li3BN2,h BN→cBN及Li3BN2→Li3N+cBN反应在高温高压条件下的ΔG.结果证实,Li3BN2由Li3N与hBN在高温高压(T>1300 K,P>3.0 GPa)条件下反应得到,在cBN的合成(T=1600～1800 K,P=4.6～6.0 GPa)条件下,hBN和Li3BN2都有向cBN转化的倾向,但由hBN向cBN直接转变的反应自由能比Li3BN2分解生成cBN的反应自由能更负,反应的可能性更大.探讨了高温高压条件下立方氮化硼的转变机理。     

氮化硼负载的高分散Au-CuOx纳米颗粒用于低温CO氧化

负载型金催化剂显示出高的低温CO氧化活性,其催化性能与载体的性质密切相关.近年来,六方氮化硼作为一种新型催化材料引起了极大关注.已有研究表明,二维结构的氮化硼纳米片有利于传质扩散,并且暴露出大量的表面和边缘,作为新型非金属催化剂在烷烃氧化脱氢中表现出优异的活性.同时,CO氧化反应是强放热过程,氮化硼具有优良的导热性能,能够减少反应过程中热点的形成.然而氮化硼是非还原性载体,与活性组分金之间的相互作用较弱,需要通过改性来加强金与氮化硼载体间的相互作用.基于此,本文首先通过球磨处理来获得具有高比表面积和富缺陷的氮化硼纳米片载体,采用浸渍法在氮化硼纳米片上引入铜物种,实现对载体的改性,然后采用传统的沉积-沉淀法制备Au-CuO_x/BN催化剂.经氧化性气氛预处理后,Au-CuO_x/BN催化剂表现出良好的低温CO氧化活性,80℃下即可实现CO的完全转化.采用X射线衍射(XRD),高分辨透射电镜(HRTEM),氢气程序升温还原(H₂-TPR),X射线光电子能谱(XPS),CO吸附原位漫反射红外光谱(CO-DRIFT)等表征手段深入分析了Au-CuO_x/BN的结构与催化活性的关系.XRD测试结果未观察到明显的金和铜物种衍射峰,表明二者在氮化硼载体上高度分散.HRTEM和元素分析面扫描结果进一步表明,氧化铜主要分布于BN边缘的官能团和缺陷位上,金纳米粒子与铜物种的空间分布位置一致,表明BN通过稳定CuO_x物种进而实现了金纳米粒子(2.0 nm)的高分散,且反应后的金纳米粒子未发生明显团聚.H₂-TPR结果表明金和铜物种间的相互作用可促进铜物种的还原,XPS分析进一步证实了金和铜物种之间存在电子转移.CO-DRIFT结果表明,Au-CuO_x/BN催化剂对CO的吸附能力和提供活性氧物种的能力显著强于Au/BN催化剂,从而促进了CO氧化反应.综上,铜物种作为连接金和氮化硼载体之间的桥梁,促进了金纳米粒子在氮化硼载体上的分散和稳定,同时增强了CO的吸附和氧的活化.本文拓展了氮化硼在多相催化中的应用,为发展新型二维催化材料提供新的思路.     

Synthesis of highly crystalline rhombohedral BN triangular nanoplates via a convenient solid state reaction

Highly crystalline rhombohedral boron nitride (r-BN) with regular triangular shapes were synthesized on a large scale in a stainless steel autoclave using B₂O₃ and NaNH₂ as reactants at 600 °C for 6 h. The as-prepared BN triangular nanoplates have an average edge length of 400 nm and the thickness of about 60 nm. The photoluminescence measurements reveal that the r-BN products show strong yellow-green emission. The as-prepared r-BN has potential optical and optoelectronic applications in high temperature devices due to its excellent thermal stability and anti-oxidation properties.     

Functionalization and Dispersion of Hexagonal Boron Nitride (h‐BN) Nanosheets Treated with Inorganic Reagents

A mixture of bulk hexagonal boron nitride (h‐BN) with hydrazine, 30 % H₂O₂, HNO₃/H₂SO₄, or oleum was heated in an autoclave at 100 °C to produce functionalized h‐BN. The product formed stable colloid solutions in water (0.26–0.32 g L ^?1) and N,N‐dimethylformamide (0.34–0.52 g L ^?1) upon mild ultrasonication. The yield of “soluble” h‐BN reached about 70 wt %. The dispersions contained few‐layered h‐BN nanosheets with lateral dimensions in the order of several hundred nanometers. The functionalized dispersible h‐BN was characterized by IR spectroscopy, X‐ray photoelectron spectroscopy (XPS), Raman spectroscopy, UV/Vis spectroscopy, X‐ray diffraction (XRD), dynamic light scattering (DLS), scanning electron microscopy (SEM), transmission electron microscopy (TEM), and atomic force microscopy (AFM). It is shown that h‐BN preserves its hexagonal structure throughout the functionalization procedure. Its exfoliation into thin platelets upon contact with solvents is probably owing to the attachment of hydrophilic functionalities.     

Synergic nitrogen source route to inorganic fullerene-like boron nitride with vessel, hollow sphere, onion, and peanut nanostructures

In this paper we describe the large-scale synthesis of inorganic fullerene-like (IF-like) hexagonal boron nitride with vessel, hollow sphere, peanut, and onion structures by reacting BBr(3) with the synergic nitrogen sources NaNH(2) and NH(4)Cl at 400-450 degrees C for 6-12 h. The composition of products could be confirmed to be pure boron nitride with hexagonal structures by the XRD patterns and FT-IR, XPS, and EDXA spectra. The representative HRTEM images clearly reveal the layerlike features of the products. Here, the peanut-like structure of the IF-like BN is reported for the first time, and added to the list as one kind of new morphology of BN nanomaterials. The similarity in the structure between h-BN and graphite is responsible for the formation of IF-like BN with nanostructures of vessels, hollow spheres, peanuts, and onions.     

二次锂电池正极材料Li_xNi_（0．3）Co_（0．7）O_2的XPS与XRD

结果表明，ＬｉｘＮｉ０．３Ｃｏ０．７Ｏ２具有六方晶系Ｒ３－ｍ空间群结构。当Ｘ＝１，０．３１５时，其晶胞参数分别为ａ＝２．８２６ｎｍ，ｃ＝１４．１３０ｎｍ和ａ＝０．２８０８ｎｍ，ｃ＝１．４２５３ｎｍ；ＭＯ６（Ｍ＝Ｎｉ，Ｃｏ）八面体中Ｍ－Ｏ平均距离分别为０．１９４１ｎｍ和０．１９３３ｎｍ。ＸＰＳ分析结果表明ＬＩｘＮｉ０．３ＣＯ０．７Ｏ２表面存在Ｌｉ２Ｏ，同时探讨了其中过渡金属离子的３ｄ电子结构变化。     

Shape-controlled synthesis of gold icosahedra and nanoplates using Pluronic P123 block copolymer and sodium chloride

Gold icosahedra with an average diameter of about 600 nm were easily prepared by heating an aqueous solution of the amphiphilic block copolymer, poly(ethylene oxide)₂₀-poly(propylene oxide)₇₀-poly(ethylene oxide)₂₀ (Pluronic P123), and hydrogen tetrachloroaurate(III) trihydrate (HAuCl₄·3H₂O) at 60 °C for 25 min. When sodium chloride (NaCl:HAuCl₄ molar ratio=10:1) was added to this aqueous solution, gold nanoplates were produced. The chloride ion was found to be a key component in the formation of the gold nanoplates by facilitating the growth of {111} oriented hexagonal/triangular gold nanoplates, because similar gold nanoplates were produced when LiCl or KCl was added to the aqueous solution instead of NaCl, while gold nanocrystals having irregular shapes were produced when NaBr or NaI was added.     

Chemical Route to Twisted Graphene,Graphene Oxide and Boron Nitride

The recently discovered twisted graphene has attracted considerable interest. A simple chemical route was found to prepare twisted graphene by covalently linking layers of exfoliated graphene containing surface carboxyl groups with an amine-containing linker (trans-1,4-diaminocyclohexane). The twisted graphene shows the expected selected area electron diffraction pattern with sets of diffraction spots out with different angular spacings, unlike graphene, which shows a hexagonal pattern. Twisted multilayer graphene oxide could be prepared by the above procedure. Twisted boron nitride, prepared by cross-linking layers of boron nitride (BN) containing surface amino groups with oxalic acid linker, exhibited a diffraction pattern comparable to that of twisted graphene. First-principles DFT calculations threw light on the structures and the nature of interactions associated with twisted graphene/BN obtained by covalent linking of layers.