铜族金属与完整及氮掺杂石墨烯的相互作用

基于广义梯度密度泛函理论和周期平板模型,研究了铜族金属单原子和双原子簇与完整及氮掺杂石墨烯的结合情况.结果表明,氮掺杂后石墨烯的电子结构特性由半金属性变为金属性;铜族金属在完整及石墨型氮掺杂石墨烯上的吸附较弱,结合能约为0.5eV,而在吡啶型氮掺杂和吡咯型氮掺杂石墨烯上有较强的化学吸附,结合能一般大于1eV;吡咯型氮掺杂后的构型不稳定,金属原子及簇与包含该结构的石墨烯衬底作用时会使其向吡啶型氮掺杂转变,并最终得到基于吡啶型氮掺杂的稳定吸附构型.Mulliken电荷布居分析显示,吸附在吡啶型氮掺杂石墨烯上的金属单原子与金属双原子簇带电性质相反.态密度及轨道分析表明,Cu与吡啶型氮掺杂石墨烯空位处留有悬挂键的三个原子成键,而Au与其中两个C原子成键.     

衬底上石墨烯制备及改性研究

大面积高质量石墨烯的制备对石墨烯电子特性及石墨烯基纳器件相关研究有重要意义。本文综述了近几年来衬底上制备石墨烯的相关实验以及衬底与石墨烯相互作用研究的重要进展。目前,采用化学气相沉积、外延生长等方法可在衬底表面上制备出较大面积、高质量的石墨烯材料。衬底与石墨烯相互作用和界面间晶格匹配、原子成键及电荷转移等密切相关,其对吸附石墨烯的几何结构、能带结构及电子特性等产生明显影响。实验与理论计算的结合可望加深衬底与石墨烯作用机理的理解,指导衬底上石墨烯制备及改性的进一步研究。     

石墨烯纳米带的可控制备研究进展

石墨烯纳米带是宽度为纳米尺度的石墨烯条带,根据其边缘构型的不同可以分为锯齿型石墨烯纳米带和扶手型石墨烯纳米带.纳米尺度导致的量子限域效应和边缘构型引起的边缘效应能够调节石墨烯纳米带的电子结构,打开石墨烯的带隙.而且,石墨烯纳米带具有极大的长宽比和极高比例的边缘原子,为通过结构裁剪实现功能定制提供了无限可能.这些几何和电子结构特性使得石墨烯纳米带在电子器件等诸多领域比石墨烯具有更大的应用潜力,因此,石墨烯纳米带的相关研究一直是纳米材料领域的热点.基于此,本综述首先介绍了石墨烯纳米带的结构和性质,全面介绍了石墨烯纳米带的制备方法,相应的制备方法可以分为两部分:(1)自上而下法:通过等离子体、离子束、扫描隧道显微镜和金属纳米颗粒对石墨烯和碳纳米管进行刻蚀和切割,制备石墨烯纳米带.该方法面临最大挑战在于如何提高刻蚀和切割精度.(2)自下而上法:利用含碳前驱体,如有机化合物、碳氢化合物气体以及碳化硅等,制备石墨烯纳米带.该方法利于实现原子精度的结构控制,尤其是化学气相沉积法有望实现低成本、规模化制备.最后展望石墨烯纳米带研究的挑战和前景.我们相信,随着材料和技术的创新发展,石墨烯纳米带必将成为一...     

基于石墨烯修饰电极的电化学生物传感

石墨烯是一种具有单原子厚度的二维碳纳米材料,具有大的比表面积、高的导电性和室温电子迁移率,以及优异的机械力学性能.石墨烯还具有电化学窗口宽,电化学稳定性好,电荷传递电阻小,电催化活性高和电子转移速率快等电化学特性.化学修饰石墨烯,特别是氧化石墨烯(GO)和还原氧化石墨烯(rGO),可以被宏量、廉价地制备出来.它们具有可加工性能,可以被组装、加工或复合成具有可控组成和微结构的宏观电极材料.因此,石墨烯及其化学修饰衍生物是用于电化学生物传感的独特而诱人的电极材料.例如,GO是一种化学修饰石墨烯,也是石墨烯的重要前驱体;其边缘具有大量的羧基可用于共价固定酶,从而能实现酶电极的生物检测.在GO上的不可逆蛋白吸附也可以促进蛋白质的直接电子转移以提高其电化学检测性能.但是,GO大量的含氧官能团破坏了石墨烯本征的共轭结构,降低了其电学性能并限制了其实际应用.GO可以通过化学、电化学、热还原等技术转化成rGO,从而能部分修复其共轭结构,提高其导电性与传感性能.另一方面,石墨烯是一种零带隙材料;原子掺杂可以调控其能带结构,提高其电催化性能.石墨烯材料也常常需要通过与其它功能材料的复合进一步改善其可分散与可加工性能,提高其电催化活性和电化学选择性.本文综述了本征石墨烯(包括GO,rGO和掺杂石墨烯)以及石墨烯与生物分子、高分子、离子液体、金属或金属氧化物纳米粒子等复合材料修饰电极在检测各种生物分子方面的研究进展,并对该研究领域进行了展望.     

脱质子化1,3环加成石墨烯外在固定位上的贵金属纳米线(英文)

为研究纳米线的形成机理,通过密度泛函理论(DFT)研究了贵金属(铂)在脱质子化1,3-环加成石墨烯上的吸附.研究发现:(1)吸附在1,3-环加成石墨烯上的铂原子引起该结构的脱质子化过程并形成脱质子化1,3-环加成石墨烯;(2)贵金属在脱质子化1,3-环加成石墨烯上的锚定位是氮原子邻位的碳原子,这在邻位碳原子的平均巴德电荷分析(高达1.0e)中得到进一步的证实;(3)铂原子在相邻的脱质子化吡啶炔单元上形成金属纳米线,并且该纳米线比相应的铂团簇稳定得多;(4)电子结构分析表明,铂的吸附并没有从根本上改变脱质子化1,3-环加成石墨烯的电子性质.铂金属的掺杂使得Pt6团簇吸附形成的复合物呈现金属性,而Pt6纳米线形成的复合物则为半金属性.     

CH_4,CO_2和H_2O在非金属原子修饰石墨烯表面的吸附

煤层气(矿井瓦斯)是一种有望替代传统化石燃料,如煤、石油和天然气的非常规气体.作为可得的清洁能源,它的利用被认为是节能和经济的选择.在本工作中,非金属原子X(X=H,O,N,S,P,Si,F,Cl)修饰的石墨烯(Gr)被用来代表具有结构异性的煤表面模型.通过密度泛函理论系统地研究了煤层气组分Y(Y=CH4,CO2,H2O)在非金属原子修饰石墨烯上的吸附作用.结果表明Y在非金属原子修饰石墨烯上的吸附均为物理吸附.态密度和差分电荷密度共同表明了这种弱的相互作用.其中,H和Cl对CH4的作用较大;N、O、F、Cl对CO2的作用较强;N,Cl对H2O的影响不容忽视.总的来说,吸附能大小依次为:H2OCO2CH4.因此,在CH4富集的煤层里注入H2O或CO2可以与CH4形成竞争吸附,进而提高煤层气采收率.本工作提供了在分子水平下煤层气与非金属原子修饰石墨烯之间的相互作用的详情,并为煤层瓦斯的开采与分离提供了有用的信息.     

(Al16Ti)n± (n=0-3)离子团簇中Ti原子对电子结构及其与H2O分子相互作用的显著影响

用密度泛函理论结合全电子自旋极化方法构建并优化出了最稳定的(Al₁₆Ti)^n± (n=0-3)离子团簇, 研究了其几何结构、稳定性和电子结构. 同时研究了水分子在(Al₁₆Ti)^n± (n=0-3)离子团簇表面的吸附结构和吸附能. 研究结果与纯(Al₁₇Ti)^n± (n=0-3)离子团簇的电子结构及其与H₂O分子的相互作用规律做了对比. 通过电子最高占据轨道和最低空轨道的空间分布, 发现大部分的活性电子占据在Ti 原子位置, 少量电子根据曲率从大到小的顺序依次占据. 通过分析最稳定的(Al₁₆TiH₂O)^n± (n=0-3)吸附化合物的几何结构可以看出, 水分子都倾向于吸附在Ti原子上, 并且为亲氧吸附. 在所有的吸附化合物中, (Al₁₆TiH₂O)⁺具有最短的平均O―H键长, 比孤立H₂O分子中的O―H键约长0.0003 nm, 然后随着电子数的增加或减少, O―H键都会进一步被拉长. 研究结果表明, Al 团簇离子中Ti 原子的掺杂可以有效提高H₂O分子的解离效率. 另外, 在金属团簇的几何结构效应与杂质效应共同出现时, 杂质的影响占据了主导地位.     

二维TiC 层表面H2的化学吸附与物理吸附

第一性原理计算研究发现由于二维TiC单原子层具有高的比表面积与大量的暴露在表面的Ti原子,其是一种非常有潜力的储氢材料.计算结果显示H2可以在二维TiC单原子层表面进行物理吸附与化学吸附.其中化学吸附能为每个氢分子0.36 eV,物理吸附能是每个氢分子0.09 eV.覆盖度为1和1/4层(ML)时,H2分子在二维TiC单原子层表面的离解势垒分别为1.12和0.33 eV.因此,除了物理吸附与化学吸附,TiC表面还存在H单原子吸附.最大的H2储存率可以达到7.69%(质量分数).其中,离解的H原子、化学吸附的H2、物理吸附的H2的储存率分别为1.54%、3.07%、3.07%.符合Kubas吸附特征的储存率为3.07%.化学吸附能随覆盖度的变化非常小,这有利于H2分子的吸附与释放.     

二维TiC层表面H2的化学吸附与物理吸附

第一性原理计算研究发现由于二维TiC单原子层具有高的比表面积与大量的暴露在表面的Ti原子,其是一种非常有潜力的储氢材料.计算结果显示H2可以在二维TiC单原子层表面进行物理吸附与化学吸附.其中化学吸附能为每个氢分子0.36 eV,物理吸附能是每个氢分子0.09 eV.覆盖度为1和1/4层(ML)时,H2分子在二维TiC单原子层表面的离解势垒分别为1.12和0.33 eV.因此,除了物理吸附与化学吸附,TiC表面还存在H单原子吸附.最大的H2储存率可以达到7.69％(质量分数).其中,离解的H原子、化学吸附的H2、物理吸附的H2的储存率分别为1.54％、3.07％、3.07％.符合Kubas吸附特征的储存率为3.07％.化学吸附能随覆盖度的变化非常小,这有利于H2分子的吸附与释放.     

NO分子在金表面吸附的理论研究

气体分子在过渡族金属表面吸附是异相催化过程中的一个重要步骤.研究其在金属表面的吸附特性是了解其催化性能的基础,多年来一直是表面科学领域的研究热点.理论研究在解释吸附机理、实验现象以及证实实验结论的可靠性方面发挥着越来越重要的作用.本文使用密度泛函理论(DFT)研究了NO分子在中性及带正、负电荷的Au(111),Au(100),Au(310)和Au/Au(111)表面的吸附行为.研究结果表明,NO倾斜地吸附在金表面.在这种吸附构型中,Au原子的dz2轨道和NO分子的2π*轨道对称性匹配,并达到最大重叠.中性及带正、负电荷的Au(111),Au(100),Au(310)和Au/Au(111)表面不同吸附位对NO的反应活性不同,NO易吸附于各个金表面的顶位.计算结果显示,NO分子在Au(111)面几乎不吸附,而在Au/Au(111)的吸附能高达0.89eV.对表面金原子d态电子分波态密度分析表明,金表面对NO分子的吸附活性随着金原子配位数的减少而增强,这是由于低配位数的金原子的d态电子更靠近费米能级.当金表面增加或减少一个电子时,金表面对NO的吸附能有明显变化.正电荷的金表面对NO吸附的活性比中性的表面活性高,而带...     

Intercalation-etching of graphene on Pt(111) in H_2 and O_2 observed by in-situ low energy electron microscopy

Graphene layers are often exposed to gaseous environments in their synthesis and application processes, and interactions of graphene surfaces with molecules particularly H_2 and O_2 are of great importance in their physico-chemical properties. In this work, etching of graphene overlayers on Pt(111) in H_2 and O_2 atmospheres were investigated by in-situ low energy electron microscopy. Significant graphene etching was observed in 10~(-5) Torr H_2 above 1023 K, which occurs simultaneously at graphene island edges and interiors with a determined reaction barrier at 5.7 eV. The similar etching phenomena were found in 10.7 Torr O_2 above 973 K, while only island edges were reacted between 823 and 923 K. We suggest that etching of graphene edges is facilitated by Pt-aided hydrogenation or oxidation of edge carbon atoms while intercalation-etching is attributed to etching at the interiors at high temperatures. The different findings with etching in O_2 and H_2 depend on competitive adsorption, desorption, and diffusion processes of O and H atoms on Pt surface, as well as intercalation at the graphene/Pt interface.     

Chemistry at the Edge of Graphene

The selective functionalization of graphene edges is driven by the chemical reactivity of its carbon atoms. The chemical reactivity of an edge, as an interruption of the honeycomb lattice of graphene, differs from the relative inertness of the basal plane. In fact, the unsaturation of the p_z orbitals and the break of the π conjugation on an edge increase the energy of the electrons at the edge sites, leading to specific chemical reactivity and electronic properties. Given the relevance of the chemistry at the edges in many aspects of graphene, the present Review investigates the processes and mechanisms that drive the chemical functionalization of graphene at the edges. Emphasis is given to the selective chemical functionalization of graphene edges from theoretical and experimental perspectives, with a particular focus on the characterization tools available to investigate the chemistry of graphene at the edge.     

Intercalation-etching of graphene on Pt(111) in H<Subscript>2</Subscript> and O<Subscript>2</Subscript> observed by <Emphasis Type="Italic">in-situ</Emphasis> low energy electron microscopy

Graphene layers are often exposed to gaseous environments in their synthesis and application processes, and interactions of graphene surfaces with molecules particularly H₂ and O₂ are of great importance in their physico-chemical properties. In this work, etching of graphene overlayers on Pt(111) in H₂ and O₂ atmospheres were investigated by in-situ low energy electron microscopy. Significant graphene etching was observed in 10^-5 Torr H₂ above 1023 K, which occurs simultaneously at graphene island edges and interiors with a determined reaction barrier at 5.7 eV. The similar etching phenomena were found in 10^-7 Torr O₂ above 973 K, while only island edges were reacted between 823 and 923 K. We suggest that etching of graphene edges is facilitated by Pt-aided hydrogenation or oxidation of edge carbon atoms while intercalation-etching is attributed to etching at the interiors at high temperatures. The different findings with etching in O₂ and H₂ depend on competitive adsorption, desorption, and diffusion processes of O and H atoms on Pt surface, as well as intercalation at the graphene/Pt interface.     

Position effects of single vacancy on transport properties of single layer armchair h-BNC heterostructure

Based on certain single layer armchair h-BNC heterostructures, six molecular devices with different positions of single vacancy atoms are investigated to explain the modulating process of negative differential resistance (NDR) behaviors and rectifying performance. The results show that NDR behaviors can be observed clearly with vacancy atoms near the interface of graphene nano-ribbon and BN nano-ribbon, and rectifying performance can be enhanced obviously when there are vacancy atoms in the moiety of the BN nano-ribbon. The first-principles analysis of the microscopic nature reveals that strength of electronic transmission, evolutions of molecular orbitals and distributions of molecular states are the intrinsic responses to these transport properties.     

Pt(3) and Pt(4) clusters on graphene monolayers supported on a Ni(111) substrate: Relativistic density-functional calculations

Density-functional theory including spin-orbit coupling and corrections for dispersion forces has been used to investigate the structural and magnetic properties of Pt(3) and Pt(4) clusters deposited on a graphene layer supported on a Ni(111) substrate. It is shown that the strong interaction of the Pt atoms with the Ni-supported graphene stabilizes a flat triangular and a slightly bent rhombic structure of the clusters. Pt atoms are located nearly on top of the C atoms of the graphene layer, slightly shifted towards the bridge positions because the Pt-Pt distances are larger than the C-C distances of the graphene sheet lattice-matched to the Ni support. The strong interaction with the substrate leads to a substantial reduction of both the spin and orbital moments of the Pt atoms, not only compared to the clusters in the gas-phase, but also compared to those adsorbed on a freestanding graphene layer. The trends in the magnetic moments and in the magnetic anisotropy of the cluster/substrate complex have been analyzed and it is demonstrated that the anisotropy is dominated by the Ni support.     

Reactivity of Graphene and Hexagonal Boron Nitride In‐Plane Heterostructures with Oxygen: A DFT Study

A density‐functional study has been undertaken to investigate the chemical properties of in‐plane heterostructures of graphene and hexagonal boron nitride. The interactions of armchair and zigzag linking edges with oxygen are looked at in detail. The results of the calculations indicate that the linking edges are highly reactive to oxygen atoms and predict that oxygen molecules can accordingly be adsorbed dissociatively. Furthermore, because oxygen atoms cooperatively interact with the heterostructures, the process can lead to opening of the linking edges, thus splitting the two materials.     

Graphene nanodots with intrinsically magnetic protrusions

The three step auf bau of a triangular polyaromatic protrusion attached to a larger parent hexagonal shaped graphene nanodot (GND) is described and the dichotomy between intrinsic protrusion localized magnetism and parent extended zigzag edge magnetism is explored using ab initio density functional theory calculations of spin and charge distributions and geometry. Comparison of a three ring with a ten-ring protrusion-GND establishes a pattern for the magnetization of GNDs with larger protrusions and different morphology. The magnetism of the isolated protrusions arises from the mismatch in numbers of sublattice (alternant hydrocarbon) carbon atoms. In the parent, the sublattices are equivalent providing a singlet ground state and the magnetization appears only on long zigzag edges due to exchange interactions operating in a regime of reduced coulombic interactions. We demonstrate that a small protrusion can quench the magnetism of the edge to which it is attached. Concomitantly, the adjacent edges exhibit a small magnetic enhancement, while the remote edges are unperturbed. With size the protrusion can dominate its edge and exert control over the magnetization of other edges. Different multiplicities of the parent moiety were not found. These calculations provide guidance in understanding how the magnetism changes with system shape and in designing nanodots with a specific magnetization.     

Magnetism and bonding in graphene nanodots with H modified interior, edge, and apex

Ab initio density functional theory calculations of hexagonal shaped zigzag edged graphene nanodot molecules, modified by the addition of atomic H to interior and perimeter sites, predict significant changes to the hexagonally sectored spin distribution and chemical bonding of the originals. The redistribution of Kohn-Sham levels at the top of the valence manifold from parent to derivative hint at large changes in the electronic structure. A centrally added H atom creates an occupied level in the middle of the 0.3 eV band gap of the parent molecule and is surrounded by an island of spins. The latter is isolated enough from the perimeter to provide a calibration of the edge spins of the modified parent. Mid-edge addition of a H atom "quenches" the spin on the edge by drawing a p(z)-electron into the C-H bond without reducing the spin on the other edges. Addition of H to an apex carbon atom results in a localized spin freed from the double bond that coexists with the parent spin on the same edge. Saturating the apex double bond by adding two H atoms, returns π-levels shifted in energy and index and parent-like spin patterns on all edges, intact except for small changes on the edges joined at the apex. Taken in unison these results demonstrate how atomic hydrogen and other groups could be used to engineer the magnetism of graphene nanodots.     

Half metallicity and electronic structures in armchair BCN-hybrid nanoribbons

We study magnetism and electronic structures of armchair BCN-hybrid nanoribbons from density functional theory. Different from armchair graphene nanoribbons, armchair BCN-hybrid nanoribbons are found to present magnetism along the edges of the nanoribbons if B and N atoms are unpaired in the nanoribbons. Intriguing spin-polarized bands, including magnetic semiconductors, half metals, and magnetic metals, are obtained in the armchair nanoribbons with both the edges composed of C and N atoms. The spin polarization in these armchair nanoribbons is ascribed to the appearance of the unsaturated electronic states in the systems. The magnetic metallicity can be tuned further to half metallicity by adsorbing O atoms at appropriate positions in the ribbons. The electronic structures of the nanoribbons without spin polarization are also analyzed. Our studies provide understanding of the magnetism mechanisms and the electronic properties and most importantly, how to achieve half metallicity in low-dimensional BCN-hybrid systems.     

Optical Properties of CdS Quantum Dots on Graphene

Hybrid systems based on graphene and semiconductor quantum dots are prospective materials for optoelectronics and photonics. In this work, electronic structure and dielectric properties of small particles of cadmium sulfide on the surface of graphene were studied using the density functional theory. The optical spectrum of this hybrid structure depends on the orientation of the nanoparticle relative to graphene due to the interaction between electrons of sulfur atoms on the surface of the CdS particle and π-orbitals of carbon atoms.