Li吸附对双层α-硼烯功函调控作用的理论研究

硼烯基纳米复合体是一种极具潜力的电极材料，因此硼烯的功函调控对于最大化器件的能量转换效率及性能至关重要.本工作基于第一性原理密度泛函理论，研究了Li吸附对双层α-硼烯（DBBP）的结构、电子性质和功函的影响及影响Li_n/DBBP功函变化的因素（如基底变形、电子转移、真空和费米能级）.结果表明，Li吸附可将DBBP的功函从4.65 eV调低至1.96～4.46 eV，优于文献报道的Li吸附单层BBP （从4.16 eV调至2.31～3.67 eV）、双层石墨烯中插入Li （3.4～3.9 eV）和K （3.3～3.8 eV）的功函调控效果.其中，Li_2（D）/DBBP （3.73 eV）和Li_3（D）/DBBP的功函（2.91 eV）分别与常用的电极材料Mg （3.68 eV）和Ca （2.90 eV）相近，Li_4（D）/DBBP的功函（1.96 eV）甚至低于Ca.本研究表明Li吸附是降低DBBP功函的一种简单而有效的方法，具有金属性和低功函的Li吸附DBBP纳米材料在电子器件中的阴极材料方面具有应用价值.     

磁透镜引起的氯化银谱峰异常位移及其在X射线光电子能谱成象分析中的应用

用X射线光电子能谱（XPS）分析了与样品托有良好电接触的银片及其上面的AgCl。观察到在使用样品磁透镜和非单色化X射线源的实验条件下不导电的AgCl的电子峰产生异常大的谱峰位移,还发现这种异常谱峰位移可以应用于XPS成象分析,以提高化学位移很小的元素化学态（如Ag^0和Ag^ )的XPS象的分辨能力。     

超薄铝/碳酸锂修饰氧化铟锡阴极制备蓝色磷光反转底发光有机发光二极管

在氧化铟锡（ITO）阴极上依次蒸镀2 nm铝和2 nm碳酸锂（Li2CO3）薄膜作为电子注入层,成功制备出器件结构为ITO/Al/Li2CO3/SPPO13/SPPO13∶FIrpic/TCTA/MoO3/Al(SPPO13：2,7-双（二苯基磷）-9,9′-螺二[芴];FIrpic：双(4,6-二氟苯基吡啶-N,C2)吡啶甲酰合铱;TCTA：4,4′,4″-三(咔唑-9-基)三苯胺)的蓝色磷光反转底发光有机发光二极管（IBOLED）。 结果表明,Al/Li2CO3作为电子注入层可以有效降低ITO与有机材料之间的电子注入势垒,蓝色磷光IBOLED的起亮电压由11 V降至4.2 V,器件的发光效率也得到有效提高。 蓝光磷光IBOLED的最大电流效率与功率效率分别达到了28.2 cd/A和19.6 lm/W,制备出的反转结构器件性能可与传统正置结构比美,说明Al/Li2CO3可以作为反转有机发光二极管优良的电子注入层。     

COT-H在金属Ru表面上沉积的光电子能谱分析

采用紫外光电子能谱（UPS），分析了不对称四苯基四苯乙炔基环辛四烯（COT H）有机发光材料与金属之间的界面电子结构，研究了在金属/COT H界面上的逸出功变化.UPS谱中位于费米能级以下5.6、7.9和10.2 eV处的三个谱峰分别来自于COT H材料中苯环的πCC、σCC和σCH轨道.位于3.8 eV处的谱峰反映了八个苯环聚合后具有π轨道特性的C－C键.从UPS谱图中可以看到， COT H材料的最高占有态（HOS：highest occupied state）位于费米能级以下1.8 eV处.COT H材料的逸出功只有3.2 eV，比清洁Ru表面的逸出功小1.0 eV.角分辨紫外光电子能谱（ARUPS）的结果表明,组成COT H分子应该近似平行于衬底表面.     

稀土掺杂La-Al-EU-1分子筛的合成与表征

在HMBr2-Na2O-Al2O3-SiO2-La2O3-H2O体系中,采用水热法合成了高结晶度的La-Al-EU-1分子筛。通过XRD,FT-IR,XPS,TG-DTG和UV-Vis DRS等手段对合成样品进行分析。结果表明:随着原始溶胶中镧的质量分数增加,La-Al-EU-1分子筛晶胞体积膨胀;FT-IR骨架振动频率向低波数方向移动,在约980 cm-1处出现Si-O-La对称伸缩振动谱带;在λ=245 nm分子筛骨架O原子的成键2p电子向骨架四配位的La原子的空d轨道的p-d跃迁产生的特征峰强度增强;La3d3/2和La3d5/2伴峰电子结合能比La2O3高1.0 eV,氧的O1s电子结合能比La2O3高1.1 eV,La3d和O1s的电子结合能同步向高能方向移动,导致La-O键共价性减少,电子云密度降低,La-O键长增加,证明了La原子已经进入了分子筛骨架,并以La3+离子四配位方式存在;当ωLa0.82%,n(SiO2)/n(Al2O3)=50~80时,晶化时间24~41 h,可以合成高结晶度的La-Al-EU-1分子筛。     

LiAlH4与Li3AlH6的成键特性及热力学稳定性

采用基于密度泛函理论(DFT)的平面波赝势(PW-PP)方法, 计算了LiAlH4分解反应中各个产物的晶胞参数、电子结构、生成焓和分解反应的反应焓. 反应中各固态、气态物质的晶胞的结构优化后的晶格参数与相应的实验值均符合得较好. 对LiAlH4与Li3AlH6的电子结构分析均表明, 其中的Al—H键为共价键、Li—H键为离子键. 对各分解反应的反应焓计算结果表明, (1) LiAlH4→1/3Li3AlH6+2/3Al+H2,(2) 1/3Li3AlH6→LiH+1/3Al+1/2H2及(3) LiH+Al→LiAl+1/2H2均为吸热反应, 298 K时计算的反应焓分别为14.3、14.9 与50.9 kJ·mol-1, 与相应的实验值符合得较好.     

硼环平面八配位及九配位的铝和镓

用硼环Bn平面配位金属中心M,两者必须在几何和电子结构上良好匹配.对Al和Ga而言,B8环半径略小,完全平面的D8hAl@B8^-（1）和D8hGa@B8^-（3）均为具有一个虚频的过渡态;金属中心沿体系八重轴轻微向上移动（0.3-0.5）所形成的C8vAl@B8^-（2）和C8vGa@B8^-（4）才是体系的稳定几何构型.轻微畸变的C8v阴离子具有准平面结构,与D8h平面结构在能量上非常接近.广泛的结构搜索表明,B9环与Al和Ga中心良好匹配,D9hAl@B9（5）与D9hGa@B9（6）均为直径约4.45的完美轮状中性分子,它们在得到的所有异构体中能量最低.在D9h5和6中,Al和Ga平面九配位中心携带的净原子电荷分别为＋1.3｜e｜和＋1.5｜e｜,其Wiberg总键级为2.5和2.8;而周边相邻B-B原子间的WBIB-B键级接近1.5,具有明显的双键特征.D9hAl@B9中中心原子的电子组态（Al3s^0.423px^0.343py^0.343pz^0.34）表明,Al在配合物中主要失去3s2价电子,其sp2杂化轨道和3pz原子轨道部分参与了体系的离域σ键和离域π键.结果表明,D9hAl@B9有三个离域的π轨道（简并的HOMO和HOMO-2）和三个离域的σ轨道（简并的HOMO-1和HOMO-4）,分别符合4n＋2休克尔芳香性规则,因而具有σ＋π双重芳香性.M@B8-和M@B9（M=Al,Ga）体系的核独立化学位移（NICS（1））均为较大的负值（介于-17~-26ppm）,进一步确定了体系的芳香性本质. C8vAl@B8^-和C8vGa@B8^-阴离子的计算单电子剥离能分别为ADE=3.41,3.23eV和VDE=3.52,3.32eV,而D9hAl@B9和D9hGa@B9中性分子的计算第一电离势分别为IP=8.51,8.34eV.这些结果为在光电子能谱实验中表征这些分子提供了依据.     

四氮杂大环化合物在有机电致发光器件中的应用(英文)

合成了四氮杂大环化合物,Tetraazamacrocycliccompound,6,12,19,25 tetramethyl 7,11:20,24 dinitrilo dibenzo［b,m］［1,4,12,15］tetra azacyclo docosine(TMCD).TMCD作为电子传送材料,探讨了它在有机电致发光器件中的应用.制作了结构为:玻璃基板／ITO阳极／NPD／Alq／TMCD／LiF／Al阴极的器件.评价的结果显示:该有机电致发光器件在538nm的绿色发光来源于Alq层.它的最大外部量子效率为0.84%,视感效率为1.30lm／W.最先提出了四氮杂大环化合物做为电子传送材料,可应用于电致发光领域.     

脉冲激光沉积CuF2薄膜的电化学性能

采用脉冲激光沉积法在不锈钢基片上制备了纳米结构的CuF2薄膜,其充放电性能显示该薄膜具有540mAh·g-1可逆容量,对应于每个CuF2可与2.0个Li发生反应.其循环伏安特性显示在2.2和2.8 V(νs Li/Li+)处出现了一对新的氧化还原峰.充放电后薄膜的组成与结构通过非原位高分辨电子显微和选区电子衍射来表征.结果揭示了纳米结构CuF2薄膜的电化学反应机理,LiF在过渡金属Cu的驱动下可以发生可逆的分解和形成.     

氧化铝薄膜表面羰基钼物种的可逆再生

 通过Mo(CO)6的热分解制备了Al2O3薄膜负载的金属钼模型催化剂,并采用热脱附谱(TDS)和X射线光电子能谱(XPS)原位研究了CO在金属态Mo/Al2O3模型催化剂表面的化学吸附. 结果表明,在低温下CO可与Al2O3表面的金属钼纳米粒子发生多重配位形成类似于羰基钼的物种. CO在Mo/Al2O3模型催化剂表面的吸附导致Mo 3d XPS峰向高结合能方向位移,所生成的羰基钼物种表现为TDS谱中在240 K处有脱附峰. 负载的金属钼模型表面与体相金属钼的化学性质完全不同,表现出明显的粒子尺寸效应.     

Excitation energy dependence for the Li 1s X-ray photoelectron spectra of LiMn2O4.

The Li 1s XPS (X-ray Photoelectron Spectroscopy) spectra of LiMn2O4, which is one of the major positive-electrode materials in lithium-ion rechargeable batteries, and MnO2 as a reference material, were measured by a laboratory-type XPS spectrometer. The Li 1s peak was not observed in the spectra excited by the Mg Kalpha line (1253.6 eV), because the Li 1s peak overlapped the background of the Mn 3p peak of LiMn2O4. The photoionization cross section of Mn 3p was larger than that of Li 1s for Mg Kalpha excitation. Therefore, the XPS measurement of LiMn2O4 by soft X-ray synchrotron excitation was carried out at beamline BL-7B on NewSUBARU synchrotron facility. Excitation energies of 110, 120, 130, 140, 150 and 151.4 eV were selected. The Li 1s peak was clearly observed in these XPS spectra. In order to investigate the excitation energy dependence, the area ratio of the Li 1s and Mn 3p peaks in the XPS spectra was plotted against the excitation energy. As a result, when the excitation energy was 110 eV, the area ratio had the maximum value.     

Interface formation of metals and poly(p-phenylene vinylene): surface species and band bending

We used X-ray photoemission spectroscopy (XPS) to investigate the surface species of poly(p-phenylene vinylene) (PPV) and its interface formation with Ca and Al. PPV surfaces compositions varied with sample preparation. For relatively "clean'' surfaces with 4–5% O, analysis of the O 1s peak revealed four types of oxygen species, namely carbonyl (C=O), hydroxyl (C–OH), ether (C–O–C) and the carboxylic groups (HO–C=O). The oxygen groups, excluding ether, reacted with Al or Ca to form the corresponding metal oxides. Chemical interactions between the metals and the phenylene and vinylene units to yield new species were not detected. For sulfur-free surfaces, a C 1s peak shift of +0.5 eV followed the deposition of 15–30 Å of Ca on PPV. For sulfur-containing surfaces, the C 1s peak shift was −0.5 eV. We attribute this difference to the interaction of metal atoms with the sulfur impurities. For Al/PPV, a C 1s peak shift occurred at <2 Å of Al deposition and reached a constant value of about +0.4 eV after ⪅8 Å of Al. Again, the direction of the peak shift depended on the presence of sulfur impurities. We attribute the C 1s peak shifts to surface band bending and to Schottky barrier formation. Since surface oxidation of PPV can inhibit band-bending, our overall results suggest that the barrier height at the metal/PPV interface is highly sensitive to the surface preparation and relatively insensitive to the work function of the metals. The shift seen by XPS in the C 1s core level spectra of PPV points clearly to charge transfer and Schottky barrier formation at the interface as a result of metal deposition. These results imply that the metal/polymer interface is not rigid and that triangular barrier tunneling fails to take into account the effect of barrier formation. We propose a band-bending modified tunneling (BBMT) model to explain charge transfer at the Ca/polymer interface. © 1997 John Wiley & Sons, Ltd.     

Interfacial interaction between ZnO thin film and polyimide substrate investigated by XPS and DFT calculation

The interfacial interaction between the ZnO film and the polyimide substrate was investigated by XPS and density functional theory (DFT) calculation, for the ZnO thin films deposited on polyimide (PI) substrates using cathodic vacuum arc deposition technique. The XPS results showed that a shoulder peak was present for the ZnO film with the thickness of about 15 nm, used for depth profiling, at the binding energy 1 eV higher than that of the Zn2p3 core level for bulk ZnO. Such a shoulder peak is attributed to the interaction between the ZnO and the polyimide. This agrees with the results of DFT calculation. Furthermore, the difference in adsorption energy between the polyimide monomer and the ZnO molecule at different adsorption sites showed that the carbonyl (C?O) plays an important role in the interfacial strength. Copyright © 2011 John Wiley & Sons, Ltd.     

甲烷氧化偶联催化剂Li/MgO的结构及表面性质的研究

本文用XRD、TEM、XPS和荧光光谱等方法研究了一组不同Li~+含量的Li/MgO催化剂的结构及表面性质,并与它们的氧化偶联甲烷的催化性能相关联。结果表明,低配位O~(2-)(O_(3c)~(2-))是使甲烷活化的活性中心。O_(1s)结合能为531.9eV的氧物种是对甲烷氧化偶联反应的C_2选择性起作用的活性氧物种。     

HREELS, STM, and STS study of CH(3)-terminated Si(111)-(1x1) surface

An ideally (1x1)-CH(3)(methyl)-terminated Si(111) surface was composed by Grignard reaction of photochlorinated Si(111) and the surface structure was for the first time confirmed by Auger electron spectroscopy, low energy electron diffraction, high-resolution electron energy loss spectroscopy (HREELS), scanning tunneling microscopy (STM), and scanning tunneling spectroscopy (STS). HREELS revealed the vibration modes associated to the CH(3)-group as well as the C-Si bond. STM discerned an adlattice with (1x1) periodicity on Si(111) composed of protrusions with internal features, covering all surface terraces. The surface structure was confirmed to be stable at temperatures below 600 K. STS showed that an occupied-state band exists at gap voltage of -1.57 eV, generated by the surface CH(3) adlattice. This CH(3):Si(111)-(1x1) adlayer with high stability and unique electronic property is prospective for applications such as nanoscale lithography and advanced electrochemistry.     

Correlation between hydroxyl fraction and O/Al atomic ratio as determined from XPS spectra of aluminium oxide layers

A set of five different aluminium oxide layers has been investigated using XPS. The oxide layers were made by oxidizing aluminium in a vacuum, with an alkaline and acidic pretreatment and in boiling water. Hydroxyl fractions of the aluminium oxide layers ranging from 0.0 to 0.5 were determined by constrained curve-fitting of the O 1s peak. The O/Al atomic ratios of the aluminium oxide layers, ranging from 1.5 to 2.0, were determined from the O 1s and Al 2p photoelectron intensities. A method is presented to account for the attenuation of the photoelectron intensities by the contamination overlayer. For the studied oxide layers, a linear relation is observed between the hydroxyl fraction and the O/Al atomic ratio of the aluminium oxide layers. It is concluded that the results obtained by the curve-fitting procedure are reliable. Furthermore, a linear relation is observed between the hydroxyl fraction and the O 1s peak width. The O 1s binding energies of the O²⁻ and OH⁻ components of the oxide layers correspond to 531.0 ± 0.1 eV and 532.4 ± 0.1 eV, respectively. Only pseudoboehmite showed 0.5 eV lower binding energies for these components. Angle-resolved XPS analysis showed that most of the studied oxides are enriched in hydroxyl groups at their outermost surface. Copyright © 2004 John Wiley & Sons, Ltd.     

HREELS to identify electronic structures of organic thin films

The electronic structure of alpha-oligothiophene (alphanT) thin films has been investigated for increasing chain lengths of n= 4-8 thiophene units with high resolution electron energy loss spectroscopy (HREELS) in the specular reflection geometry at a primary energy of 15 eV. The great advantage of this technique in contrast to UV/VIS absorption spectroscopy results from the fact, that the impact scattering mechanism of HREELS makes it possible to also detect optically forbidden electronic transitions. On the other hand, the electrons used as probes in HREELS have a wavelength which is two orders of magnitudes smaller if compared to those of photons used in UV/VIS absorption spectroscopy. Therefore individual molecules are excited by HREELS independent from each other and hence the excitation of collective excitons is not possible. As a result, information about the orientation of the molecules cannot be achieved with HREELS, which, however, is possible in polarization-dependent UV/VIS spectroscopy.     

Functionalization of a self-assembled monolayer driven by low-energy electron exposure

Self-assembled monolayers (SAMs) of 10-undecene-1-thiol on Au were functionalized with nitrogen-containing groups using an approach in which multilayer ammonia (NH(3)) films were deposited at low temperature onto the SAMs and subsequently exposed to 15 eV electrons. The result of this process was investigated after removal of the remaining NH(3) by annealing to room temperature using high-resolution electron energy loss spectroscopy (HREELS) and X-ray photoelectron spectroscopy (XPS). HREELS shows that the CC double bonds disappear during electron exposure, while XPS gives evidence that about 25% of the terminal double bonds of the SAM were functionalized. Also, XPS shows that a sufficiently thick NH(3) layer protects the underlying SAM from electron-induced damage. The process suggested here thus represents a particularly gentle approach to the functionalization of ultrathin molecular layers. Thermal desorption spectrometry (TDS) and electron-stimulated desorption (ESD) experiments on condensed layers of NH(3) reveal production of N(2) but show that significant amounts of the initial NH(3) as well as N(2) produced during electron exposure desorb. Hydrogen released upon formation of N(2) is held responsible for the reduction of double bonds and protection of the SAMs from damage.     

A [4+2]-like cycloaddition of methyl methacrylate on Si(100)-2 x 1

The attachment of methyl methacrylate (MMA) on Si(100)-2x1 was investigated using high-resolution electron energy loss spectroscopy (HREELS), X-ray photoelectron spectroscopy (XPS), ultraviolet photoelectron spectroscopy (UPS), and density functional theory (DFT) calculations. The HREELS spectra of chemisorbed MMA show the disappearance of characteristic vibrations of C=O (1725 cm(-1)) and C(sp(2))-H (3110, 1400, and 962 cm(-1)) coupled with the blue shift of the C=C stretching mode by 34 cm(-1) compared to those of physisorbed molecules. These results clearly demonstrate that both C=C and C=O in MMA directly participate in the interaction with the surface to form a SiCH(2)C(CH(3))=C(OCH(3))OSi species via a [4+2]-like cycloaddition. This binding configuration was further supported by XPS, UPS, and DFT studies.