丁基黄药在CuO表面吸附的二维连续在线原位ATR-FTIR光谱研究

运用连续在线原位衰减全反射傅里叶变换红外光谱(ATR-FTIR)技术测定了纳米CuO表面对丁基黄药的吸附行为. 在FTIR 谱图中发现有峰的红移现象,吸收峰由1200 cm^-1偏移到1193 cm^-1,用超纯去离子水脱附,峰强度只有微小的变化,可判断丁基黄药在CuO表面发生了很强的化学吸附. 通过对吸附行为进行二维(2D)红外光谱分析,分辨出吸附过程中光谱强度的变化顺序. 二维异步相关光谱测定结果表明,1265 cm^-1处振动吸收峰最先引起光谱强度的变化,1265 cm^-1处吸收峰可归因为表面反应生成的双黄药和黄药分子聚集体的复合峰. 根据1200 cm^-1处黄药特征吸收峰强度的变化,进行吸附动力学模拟,得出CuO对丁基黄药的最大吸附量为529 mg·g^-1,且吸附符合拟二级吸附动力学过程.     

新型含三氰根的铁(III)配合物作为组装基元所构筑的分子性磁石

由于其潜在的多功能的应用, 以分子为基础的磁性材料引起了广泛的关注. 利用3d六氰金属化合物已成功地合成了一系列的分子磁体. 我们一直在研究和开发一些顺磁性的三价的钌和锇的金属氰化物: 例如, trans- [Ru^III(acac)(CN)₂]^-, trans-[M^III(salen)(CN)₂]^- (M = Ru or Os) 和 [Ru^III(CN-sap)(CN)₃]^2-, 并以此来用作磁性材料的建筑模块. 在本文中, 我们报道一系列的带有三齿希夫碱配体的三氰根铁(III)配合物的合成及表征. 在THF, FeCl₂·4H₂O 和5-取代的sapH₂反应一天生成红褐色固体[Fe^III(5-Xsap)(THF)₂Cl] (1a~1e). 这些化合物的红外光谱都在1600 cm^-1 显示了v(C=N)吸收. 5-位上的取代基团对此吸收没有明显的影响. 然而与sapH₂ 配体相比较, 这些v(C=N)吸收向低波数移动了30 cm^-1 . 在MeOH, 化合物1a 的质谱在m/z = 267显示了一个最显著的峰. 这个峰被指认为[Fe^III(sap)]⁺(源于母体离子在离子化的过程中减除两个THF和一个Cl). 实验与模拟的同位素分布图是非常一致的. 化合物1b~1e的质谱图与1a相似. 化合物1a~1e在室温下的磁矩在6.02~6.12μB范围内(Gouy方法, 固样), 这意味着这些铁化合物都是高自旋态的有5个单电子. 在H2O中, 化合物[Fe^III(5-Xsap)(THF)₂Cl] (X = H, Me, OMe, Cl 或Br)与过量的KCN反应生成一系列三氰铁(III)化物, [Fe^III(5-Xsap)(CN)₃]^2-. 这些化合物都以PPh4+盐的形式2a~2e分离出来(70%产率). 这些化合物的红外光谱在2102~2106 cm^-1 的范围内显示了v(C≡N)吸收. 与未配位的氰根相比较(2080 cm^-1 ), 这些v(C≡N)吸收都移向了高波数. 但是, 这个值又低于[(Tp)Fe^III(CN)₃]^- (v_CN = 2123 cm^-1 ). 在CH₃CN, 化合物2a 的质谱显示了一个单一的峰(m/z = 319). 这个峰被指认为[Fe(sap)(CN)₂]^- (源于母体离子在离子化的过程中减除一个CN^-). 实验与模拟的同位素分布图是非常一致的. 化合物1b~1e的质谱图与1a相似. 在这些化合物的质谱中, 都没有观察到相应的母体离子[Fe(5-Xsap)(CN)₃] ^2-的峰. 然而, 在CH₃CN 中测量的这些化合物的摩尔电导率在232~240Ω^-1·cm²·mol^-1范围内. 这意味着这些化合物是2:1的电解质, 与在溶液中[Fe(5-Xsap)(CN)₃]^2- 为二价的阴离子一致. 此2:1的结构构型进一步通过XRD得到确认. 化合物2a~2e 在293 K的磁矩在2.10~2.20μB范围内(Gouy方法, 固样), 符合低自旋态的d⁵化合物. 这说明通过氰根的配位, 这些铁(III)化合物都从高自旋转变为低自旋态.     

连续在线原位ATR-FTIR技术测定介孔CuAl2O4对黄药的吸附

以丁胺和正十二醇为混合模板剂, 采用共沉淀法制备了介孔纳米CuAl₂O₄. 用X射线粉末衍射(XRD)、傅里叶变换红外(FTIR)光谱、N₂吸附-脱附对产物的结构进行了表征. 采用连续在线原位衰减全反射傅里叶变换红外(ATR-FTIR)光谱技术研究了水溶液中丁基和辛基黄药在介孔CuAl₂O₄表面的吸附. 随着吸附时间的延长,1200 和1040 cm^-1两处黄药特征峰的高度逐渐增加, 根据1200 cm^-1处C-O-C伸缩振动峰的变化来评价黄药在CuAl₂O₄表面的吸附动力学过程. 结果表明, 介孔纳米CuAl₂O₄对黄药有很强的吸附能力, 在100 min 的时间内, CuAl₂O₄样品对丁基和辛基黄药的吸附量分别达到了236 和300 mg·g^-1, 且属于化学吸附. 对实验数据进行理论模拟, 发现吸附过程更接近于拟二级吸附动力学方程.     

枝晶状Pt 薄膜的制备及其特殊红外效应

采用方波电位, 在10×10^-3 mol·L^-1 K₂PtCl₆+3×10^-4 mol·L^-1 PbAc₂+0.5 mol·L^-1 HClO₄溶液中, 于本体Pt 电极上电沉积制备出枝晶状Pt 薄膜. 随着沉积时间的增加, 枝晶长度逐渐由400 nm增加到900 nm, 且枝晶上的小晶粒(~10 nm大小)变得密集. 根据循环伏安(CV)曲线中氢吸脱附电量可得出Pt 薄膜具有中等粗糙度(C_r=9-36), 且电极表面的粗糙度随着沉积时间增加而增大. 观察到Pt 薄膜上吸附态CO的原位红外光谱具有明显的增强吸收效应, 当沉积时间为6 min 时所制得的枝晶Pt 电极的红外增强效应最大. CO呈现多种谱峰形状, 随着沉积时间的增加, 谱峰形状依次为左高右低的双极峰(类Fano 红外效应), 单极向下(表面增强红外吸收), 左高右低的双极峰, 单极向上(异常红外效应), 左低右高的双极峰和单极向下. 这表明纳米材料薄膜所呈现出的特殊红外性能, 与纳米材料的尺度和聚集状态等密切相关. 所制备的枝晶状Pt 薄膜有望为深入认识纳米材料的特殊红外性能提供一个良好的模型材料.     

纳米CaCO3微晶的晶格畸变和反常红外特性

利用TEM、SEM、X射线衍射(XRD)和Voigt函数单峰分析法讨论了纳米CaCO₃微晶结构,解释了纳米CaCO₃微晶的反常红外吸收特性,并认为微结构中的尺寸效应使得纳米CaCO₃晶格中存在较大的畸变应力,从而引起了碳酸钙微晶的红外ν₃吸收峰有约40 cm^-1的蓝移和明显窄化。     

Ti-MWW分子筛正弦孔道内骨架钛物种的结构和红外振动光谱的理论计算

应用密度泛函理论计算,研究了Ti-MWW分子筛10元环正弦孔道内骨架钛物种的结构和振动光谱。计算采用基于36T簇模型的B3LYP/6-31G(d,p)方法,确定了[Ti(OSi)₄]物种优先落位于T3位,在924~987cm^-1区域内存在3个振动峰,都属于以Ti为正四面体中心分布的4个Ti-O-Si键的协同伸缩振动,其中958cm^-1的振动强度较大,属于[Ti(OSi)₄]的特征频率。T2和T8位上钛物种不出现该特征峰。Ti(Ⅳ)中心上吸附一个水分子形成五配位配合物,其特征振动频率没有变化。[Ti(OSi)₄]物种进一步水解形成[Ti(OSi)₃OH]物种,其Ti-O-Si的特征振动蓝移到969cm^-1。此外,还考察了Ti-MWW分子筛中可能存在的骨架硼以及羟基巢的结构和振动光谱,计算频率与已有文献数据相符。     

多孔纳米Ce-M-O (M＝Pr, La)粉末的微波诱导燃烧合成及其表征

使用Ce(NO₃)₃•6H₂O, Pr(NO₃)₃•6H₂O, La(NO₃)₃•6H₂O, 尿素为原料, 利用微波引诱燃烧法合成了多孔纳米Ce-M-O (M＝Pr, La)固溶体. 使用XRD, X光电子能谱仪(XPS), Raman光谱仪, 红外光谱仪(FT-IR), 透射电镜(TEM), 场发射扫描电镜(FE-SEM)等仪器对纳米粉体进行了表征. XRD分析显示Ce-M-O粉体的粒径在20～50 nm之间, 且所有样品均具有萤石结构. XPS证明在Ce-Pr-O固溶体中Pr以＋3和＋4两种形式存在. Raman光谱表明随着M^3＋的掺杂, 在CeO₂晶格中产生氧缺陷, 且缺陷浓度随掺杂量增加不断提高. 红外光谱证明Ce—O键的吸收峰在1400 cm^－1左右, 且由于M^3＋的掺杂在2346 cm^－1的吸收峰消失. TEM照片说明样品具有类盘状的网络纳米微晶结构. 扫描图像说明产物具有多孔的外貌特征, 且孔径分布在2～40 nm之间.     

反式N-3-炔丁烯基咔唑的合成及其齐聚行为

在65 ℃、氮气保护下, 往咔唑钠的四氢呋喃溶液中缓慢滴加1,4-二氯-2-丁炔. 反应9 h后, 在苯和石油醚混合溶剂中重结晶, 分离得到反式N-3-炔丁烯基咔唑. 在加热, BPO, BF₃, FeCl₃, P₂O₅, 紫外或可见光的引发作用下, 反式N-3-炔丁烯基咔唑发生齐聚反应. 通过元素分析, IR, ¹H NMR, MS, UV等方法对反应产物进行分析表征. IR和¹H NMR图谱显示单体聚合后炔基及其相连氢原子的特征吸收峰(ν: 3278, 2099 cm^－1; : 2.8～3.0)消失, VPO法测得齐聚物分子量在8.3×10²至1.9×10³之间(聚合度4～9).     

桥头碳上氮杂芳基功能化的双吡唑甲烷与羰基钨反应

研究了(氮甲基咪唑-2-基)双(3,5-二甲基吡唑)甲烷(L¹),2-吡啶基双(3,5-二甲基吡唑)甲烷(L²)及4-吡啶基双(3,5-二甲基吡唑)甲烷(L³)与羰基钨的反应,合成了一系列以单齿,双齿及三齿氮配位的羰基金属衍生物LW(CO)₅ (L=L¹或L³),LW(CO)₄ (L=L¹,L²或L³)和LW(CO)₃ (L=L¹或L²).核磁,红外及X-射线单晶衍射分析表明这3种配体表现出了可变的配位方式.在LW(CO)₅中,当配体为L¹时,其倾向于通过咪唑氮与金属配位,而为L³则倾向于利用吡啶氮与金属作用;在LW(CO)₄中,配体L¹表现为通过咪唑氮和吡唑氮原子配位的[N,N']双齿配体,而L²和L³表现为通过吡唑氮原子配位的[N,N]双齿配体;在LW(CO)₃中,L¹和L²起着[N,N,N']三齿螯合配体的作用.     

Au@g-C3N4支架的制备及其光催化性能

以三聚氰胺、甲醛、尿素等原料合成具有可塑性的三聚氰胺树脂,通过发泡法构建前驱体支架,并通过磁控溅射法在支架表面沉积金,550℃下热聚合后,成功制备得到负载Au的石墨相氮化碳(Au@g-C₃N₄)支架,其比表面积可达1 480 m²·g^-1。负载6%Au后,Au@g-C₃N₄支架的紫外吸收光谱在550nm处出现了新的吸收峰,吸收带边红移至507nm,禁带宽度缩小至2.45eV,Au@g-C₃N₄支架荧光强度和阻抗显著降低,光电流从0.28μA·cm^-2提升至0.62μA·cm^-2。负载Au既拓宽了Au@g-C₃N₄支架可见光吸收性能,又抑制了电子-空穴对的复合,光催化性能稳定,光催化降解罗丹明B的降解率提高近1倍。此外,Au@g-C₃N₄支架强度适中,具有一定韧性,在光催化领域应用中便于回收和再利用。     

CoPt纳米空心球甲醇电催化氧化和原位电化学傅里叶变换红外光谱研究

采用化学还原和电位置换法制备了CoPt 纳米空心球, 该催化剂对甲醇氧化表现出较好的电催化活性.透射电镜(TEM)、能量散射光谱(EDS)和电化学循环伏安实验结果表明, 在0.1 mol·L^-1 H₂SO₄+0.1 mol·L^-1CH₃OH中进行测试时, CoPt 纳米空心球发生了去合金化过程, 催化剂表面Co元素溶解, 形成了富Pt 表面, 表现出更好的电催化活性, 同时表现出较好的结构稳定性. 采用原位电化学红外光谱在分子水平研究了CoPt 纳米空心球上甲醇氧化过程, 发现甲醇在CoPt 纳米空心球氧化中间产物主要为CO, 且CO表现出异常红外效应, 与CO为探针分子在CoPt纳米空心球上得到的红外光谱结果一致. 研究结果表明, 去合金化方法是一种有效调节催化剂表面组成和性能的手段, 原位电化学红外光谱是潜在的原位研究有机小分子氧化机理的方法, 在燃料电池中将得到广泛的应用.     

FTIR study of the Cl-atom initiated oxidation of methylglyoxal

The kinetics and mechanism of Cl-atom initiated reactions of CH₃C(O)CHO were studied using the FTIR detection method in the photolysis (λ < 300 nm) of Cl₂? CH₃C(O)CHO mixtures in 700 torr of N₂? O₂ diluent at 298 ± 2 K. The observed product distribution over the O₂ pressure range from 0–700 torr, combined with relative rate measurements, provided evidence that: (1) the primary step is Cl + CH₃C(O)CHO → HCl + CH₃C(O)CO with a rate constant of (4.8 ± 1.1) × 10^?11 cm³ molecule^?1 s^?1; and (2) the predominant fate of the primary radical CH₃C(O)CO under atmospheric conditions is unimolecular dissociation to CH₃C(O) radicals and CO, rather than O₂-addition to yield the corresponding carbonylperoxy radical CH₃C(O)C(O)OO.     

New N-nitrosoamines. 1. Synthesis and nitrosative cleavage of the Mannich bases derived from nitrogen-containing heterocycles and primary aliphatic amines

The reactions of isatin, benzotriazole, and succinimide with formaldehyde and methylamine yield monoamines RCH₂N(Me)CH₂R and methylenediamines RCH₂N(Me)CH₂N(Me)CH₂R. The use of ethylenediamine as the amino component affords N,N"-disubstituted imidazolidines, while the reactions with 3-aminopropan-1-ol give N-substituted tetrahydro-1,3-oxazines. RCH₂NBuⁱ ₂ was obtained from succinimide, formaldehyde, and diisobutylamine. Nitrosative cleavage of the amines obtained was studied; it was shown that monoamines and methylenediamines give N-nitrosoamines RCH₂N(NO)Me, which were structurally characterized by X-ray diffraction analysis. RCH₂NBuⁱ ₂ affords diisobutylnitrosamine, while imidazolidines transform into dinitroso compounds RCH₂N(NO)CH₂CH₂N(NO)CH₂R.     

Disproportionation reactions of the acetonitrile derivatives of group VI hexacarbonyls

The disproportionation reactions of [M(CO)₆-n_-n(CH₃CN)n_n] (M = Cr,Mo, W; n = 1—3) proceed in solution according to the sequence M(CO)₃(CH₃CN)₃ → M(CO)₄(CH₃CN)₂ → M(CO)₅(CH₃CN) → M(CO)₆.Rapid changes are observed in Nujol and acetone at ambient temperature, but in acetonitrile comparable changes require higher temperatures. Additional carbon monoxide groups are provided by the complete decomposition of part of the sample of the complex but free carbon monoxide is not detected in solution. The observed disproportionation reaction enabble the use of M(CO)₃(CH₃CN)₃ complexes for the synthesis of M(CO)₄ derivatives to be rationalised. The nature of an intermediate absorbing at 1996 cm^-1 in the IR spectrum is discussed.     

Temperature-dependent kinetics of the simplest Criegee intermediate reaction with dimethyl sulfoxide

Criegee intermediates are thought to play roles in atmospheric chemistry, including OH radical formation, oxidation of SO₂, NO₂, etc. CH₂OO is the simplest Criegee intermediate, of which the reactivity has been a hot topic. Here we investigated the kinetics of CH₂OO reaction with dimethyl sulfoxide (DMSO) under 278–349 K and 10–150 Torr. DMSO is an important species formed in the oxidation of dimethyl sulfide in the biogenic sulfur cycle. The concentration of CH₂OO was monitored in real-time via its mid-infrared absorption band at about 1,286 cm⁻¹ (Q branch of the ν₄ band) with a high-resolution quantum cascade laser spectrometer. The 298 K bimolecular rate coefficient was determined to be k₂₉₈ = (2.3 ± 0.3) × 10⁻¹² cm³/s at 30 Torr with an Arrhenius activation energy of −3.9 ± 0.2 kcal/mol and a weak pressure dependence for pressures higher than 30 Torr (k₂₉₈ = (2.8 ± 0.3) × 10⁻¹² cm³/s at 100 Torr). The reaction is speculated to undergo a five-membered ring intermediate, analogous to that of CH₂OO with SO₂. The negative activation energy indicates that the rate-determining transition state is submerged. The magnitude of the reaction rate coefficient lies in between those of CH₂OO reactions with (CH₃)₂CO and with SO₂.     

Infrared molecular beam depletion spectroscopy of size-selected methanol clusters

Molecular beam depletion spectroscopy has been employed to study the dissociation of small methanol clusters in the spectral region between 1000 and 1100 cm^?1 which covers thev ₈ CO stretch (1033.5 cm^?1) and thev ₇ CH₃ rock (1074.5 cm^?1) monomer vibrations. Size selection has been achieved by dispersing the (CH₃OH) _n cluster beam by a secondary He beam. Aside from the recently published CH₃OH dimer absorption bands at 1026.5 and 1051.6 cm^?1 which are assigned to the excitation of the CO stretching vibrations in the non-equivalent subunits of the hydrogen-bonded complex, a previously unobserved band was found at 1071.3 cm^?1. This absorption band is attributed to the excitation of the CH₃ rocking vibration in the dimer. It appears that this transition which is very weak in the free methanol monomer receives substantial oscillator strength due to the intermolecular interaction in the complex. A splitting of this band could not be observed. The trimer and tetramer spectra feature single peaks for the CO stretching vibration being centered at 1042.2 cm^?1 and 1044.0 cm^?1, respectively. This observation is consistent with the cyclic structures of these species. The trimer and tetramer rocking vibrations are observed near 1060.5 cm^?1 but cannot be localized exactly, due to a gap in the CO₂ laser tuning range.     

Cobalt‐catalyzed alternating and nonalternating copolymerization of carbon monoxide with aziridine

Catalysts CH₃COCo(CO)₃PPh₃ ( 1 ) and HCo(CO)₃PPh₃ ( 2 ) catalyze the copolymerization of aziridine and carbon monoxide. Catalyst 2 can be conveniently generated in situ via reaction of Na⁺Co(CO)₄, N,N‐dimethylanilinium chloride, and PPh₃. The copolymerization alternates at high catalyst loadings to produce poly(β‐alanine). The end groups of the poly(β‐alanine) product are characterized by matrix‐assisted laser desorption/ionization time‐of‐flight mass spectrometry and by comparison of the ¹H NMR spectra of the polymer and a stepwise synthesized model compound. At low catalyst loadings, the polymer product contains both the β‐alanine units and amine units because of nonalternating enchainment of the comonomers. The characterization of the amine units is again supported by comparison of the ¹H NMR spectra of the polymers and the stepwise synthesized model compounds. The molecular weights of the polymers are determined by gel permeation chromatography. The thermal stability of the polymers is probed by differential scanning calorimetry and thermogravimetric analysis. © 2002 Wiley Periodicals, Inc. J Polym Sci Part A: Polym Chem 41: 376–385, 2003     

The chemistry of electrogenerated transition metals species - the insertion of olefins into a nickelcarbon bond

The nickel(1) complex, Ni(teta)⁺, formed by cathodic reduction of the corresponding nickel(11) complex, reacts rapidly with alkyl bromides to form an unstable intermediate containing a nickelcarbon bond. When the electrolysis medium also contains an activated olefin an insertion reaction occurs. The new metalcarbon bond is cleaved by further reduction and overall the reduction of Ni(teta)²⁺ in the presence of RBr and CH₂CHY leads to high yiels of RCH₂CH₂Y.     

Some observations on molecular complexes of carbon monoxide in argon and oxygen nutrices

Aggregates of CO were generated in Ar and O₂ matrices by several methods, including deposition of concentrated samples, warming experiments, and photolysis of H₂CO and H₂C₂O₂. The IR absorption frequencies of the CO species were measured by an FTIR spectrometer. In solid Ar, the CO monomer was seen to absorb at 2138.5 cm^?1 and (CO)₂ at 2136.6 cm^t-1. In systems containing only CO and Ar, no distinct peak was observed at 2140 cm^?1 in contrast to previously reported results. The difference may be due to effects of H₂O on CO frequencies and intensities. In solid O₂, the CO monomer absorbed at 2136.6 cm^?1, but it was not possible to assign a structure to (CO)₂ because of a more complicated absorption spectrum than in solid Ar. The spectral data suggest that the CO dimer absorbing at 2136.6 cm^?1 in solid Ar may have a side-by-side antiparallel geometric structure.     

Synthesis and Reactivity of Organometallic Intermediates Relevant to Cobalt-Catalyzed Hydroformylation

Intermediates relevant to cobalt-catalyzed alkene hydroformylation have been isolated and evaluated in fundamental organometallic transformations relevant to aldehyde formation. The 18-electron (R,R)-(^iPrDuPhos)Co(CO)₂H has been structurally characterized, and it promotes exclusive hydrogenation of styrene in the presence of 50 bar of H₂/CO gas (1:1) at 100 °C. Deuterium-labeling studies established reversible 2,1-insertion of styrene into the Co−D bond of (R,R)-(^iPrDuPhos)Co(CO)₂D. Whereas rapid β-hydrogen elimination from cobalt alkyls occurred under an N₂ atmosphere, alkylation of (R,R)-(^iPrDuPhos)Co(CO)₂Cl in the presence of CO enabled the interception of (R,R)-(^iPrDuPhos)Co(CO)₂C(O)CH₂CH₂Ph, which upon hydrogenolysis under 4 atm H₂ produced the corresponding aldehyde and cobalt hydride, demonstrating the feasibility of elementary steps in hydroformylation. Both the hydride and chloride derivatives, (X=H⁻, Cl⁻), underwent exchange with free ¹³CO. Under reduced pressure, (R,R)-(^iPrDuPhos)Co(CO)₂Cl underwent CO dissociation to form (R,R)-(^iPrDuPhos)Co(CO)Cl.