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1.
利用第一性原理方法研究了一氧化碳分子在本征和硼、氮、铝、磷掺杂的有限尺寸石墨烯上的吸附机理.结果表明,石墨烯作为一氧化碳传感器时的性能依赖于掺杂元素.本征、硼和氮掺杂石墨烯吸附一氧化碳时的吸附能较低,为物理吸附.铝、磷掺杂石墨烯的吸附能显著提高,比本征、硼和氮掺杂时高出约一个数量级,且铝和磷原子从石墨烯中突出,使其发生局部弯曲.铝掺杂石墨烯增强了石墨烯与一氧化碳分子之间的相互作用,可以提高石墨烯的气敏性和吸附能力,是一氧化碳传感器的最佳候选材料之一. 相似文献
2.
摘 要:基于第一性原理的计算方法,建立了本征石墨烯、空位石墨烯及钇( Y)掺杂空位石墨烯模型,并计算了CO、NO在三类石墨烯表面的吸附过程. 从表面能、吸附结构、吸附能和态密度四个方面进行分析讨论,研究掺杂Y对CO、NO气体吸附性能的影响. 结果表明:CO、NO与本征石墨烯之间的吸附为弱的物理吸附,掺杂Y后增强了材料表面对CO、NO的吸附效果,最大吸附能分别为7.414eV、6.702eV,属于化学吸附;掺杂Y使空位石墨烯费米能级附近有了更多的活跃电子,其吸附NO后体系由半金属转变为金属特性,该特性能为开发更加优良的石墨烯气敏材料提供理论支持. 相似文献
3.
表面吸附是石墨烯中质子(H~+)输运的基础步骤.本文基于第一性原理计算研究了B、N、S掺杂对石墨烯表面H~+吸附行为的影响.结果表明,B、N、S掺杂对石墨烯的晶体结构、内聚能及电子性质有重要影响,且影响程度与掺杂元素的性质密切相关,进而导致对石墨烯表面H~+吸附行为产生不同程度的影响.从吸附能的观点看,N、B、S掺杂对石墨烯表面H~+的吸附有利.研究结果对石墨烯在氢贮存、氢同位素分离、燃料电池等领域的应用具有重要的指导意义. 相似文献
4.
孟玲 《原子与分子物理学报》2018,35(5):745-750
采用密度泛函理论(DFT)的第一性原理方法,对Na在本征双层石墨烯(PBLG)和不同掺杂浓度的N掺杂石墨烯(NBLG)表面的吸附性质进行了研究.确定了不同N掺杂浓度时NBLG的最稳定N分布结构,计算了Na在PBLG和不同掺杂浓度的NBLG表面的吸附能.计算结果表明,N原子掺杂倾向于取代对位或次临近位置的C原子,并与下层C原子相对;随着N掺杂浓度的增加,吸附高度逐渐增加,且与掺杂N原子分布相匹配; Na在PBLG表面吸附使平均层间距增加,而在NBLG表面吸附使之减小; Na与C_(27)N_9表面的结合最稳定. 相似文献
5.
孟玲 《原子与分子物理学报》2018,35(4):681-687
采用密度泛函理论(DFT)的第一性原理方法,对Na在本征双层石墨烯(PBLG)和不同掺杂浓度的B掺杂石墨烯(BBLG)表面的吸附性质进行了研究.确定了不同B掺杂浓度时BBLG的最稳定B分布结构,计算了Na在PBLG和不同掺杂浓度的BBLG表面的吸附能.计算结果表明,B原子掺杂倾向于占据上层中对位或次临近位置,并与下层中六边形碳环中心相对,B_4C_(32)的形成能最小;B掺杂浓度的增加使BBLG中上层石墨烯片层结构起伏增大,而对下层影响较小;Na在BBLG表面吸附高度和平均层间距受上层结构起伏影响显著;Na倾向于吸附在B_9C_(27)表面B原子的上方,使原始平面结构产生起伏,Na与B_9C_(27)表面的结合最稳定. 相似文献
6.
本文采用基于密度泛函理论的第一性原理方法,研究了气体分子CO、NO、NO_2和SO_2吸附对Ti掺杂石墨烯(Ti G)电子结构和磁性的调制.研究表明:Ti G对CO、NO、NO_2和SO_2分子的吸附作用较强,各分子与Ti原子键合并形成Ti-X键(X代表C、O、N原子);各分子的吸附可导致Gas@Ti G体系电磁性质明显改变:CO分子吸附基底后,虽未能引起CO@Ti G体系电子性质改变和磁性的产生,却能够有效调控该体系的带隙宽度;不同于CO分子,NO、NO_2和SO_2分子的吸附使得半导体性的Ti G基底转变为金属特性,但各体系磁性表征不同:NO@Ti G发生完全自旋极化,即NO分子与基底上均有自旋分布,且二者的自旋方向相同;顺磁性的NO_2分子吸附于Ti G基底时磁性消失;SO_2分子吸附于Ti G基底后自身产生磁性,但基底几乎未发生自旋极化,SO_2@Ti G呈现自旋极化的局域分布特征.由此,依据分子吸附后体系电磁性质特征的不同,可辨识被测气体分子.此项研究结果为高灵敏度和高选择性的石墨烯基气体传感器的设计提供理论参考. 相似文献
7.
采用基于密度泛函理论的第一性原理方法,研究了本征石墨烯(P-graphene)和氧掺杂的石墨烯(O-graphene)吸附钠原子的吸附能、电荷密度、态密度以及储存量.结果表明,两种石墨烯中,钠原子的最佳吸附位置都是H位. O-graphene对钠原子的吸附能是-4.347 eV,比P-graphene对钠原子的吸附能(-0.71 eV)低很多. O-graphene中钠原子与氧原子和碳原子发生轨道杂化,P-graphene中没有杂化现象. O-graphene能够吸附10个钠原子,较P-graphene多.因此,O-graphene更适合储钠. 相似文献
8.
姚利花 《原子与分子物理学报》2017,34(3):569-576
采用基于密度泛函理论的第一性原理方法,研究了本征石墨烯及缺陷石墨烯对Na原子的吸附行为.主要研究了三种石墨烯:本征石墨烯、B掺杂的石墨烯和N掺杂的石墨烯.结果表明,与本征石墨烯相比,B掺杂的石墨烯和N掺杂的石墨烯在吸附能、电荷密度、态密度和储钠量方面表现出很大的差异.B掺杂的石墨烯对Na原子的吸附能是-1.93 e V,约为本征石墨烯对Na原子吸附能的2.7倍;与本征石墨烯相比,N掺杂的石墨烯对Na原子的吸附能明显增大.态密度计算结果表明,Na原子与B掺杂的石墨烯中的B原子发生轨道杂化,而本征石墨烯和N掺杂的石墨烯中不存在轨道杂化现象.B掺杂的石墨烯对Na原子的吸附量是3个,与本征石墨烯相比显著提高.因此,B掺杂的石墨烯有望成为一种新型的储钠材料. 相似文献
9.
姚利花 《原子与分子物理学报》2018,35(6)
采用基于密度泛函理论的第一性原理方法,研究了本征石墨烯及缺陷石墨烯对Na原子的吸附行为。主要研究了三种石墨烯:本征石墨烯、B掺杂的石墨烯和N掺杂的石墨烯。结果表明,与本征石墨烯相比,B掺杂的石墨烯和N掺杂的石墨烯在吸附能、电荷密度、态密度和储钠量方面表现出很大的差异。B掺杂的石墨烯对Na原子的吸附能是-1.93 eV,约为本征石墨烯对Na原子吸附能的2.7倍;与本征石墨烯相比,N掺杂的石墨烯对Na原子的吸附能明显增大。态密度计算结果表明,Na原子与B掺杂的石墨烯中的B原子发生轨道杂化,而本征石墨烯和N掺杂的石墨烯中不存在轨道杂化现象。B掺杂的石墨烯对Na原子的吸附量是3个,与本征石墨烯相比显著提高。因此,B掺杂的石墨烯有望成为一种新型的储钠材料。 相似文献
10.
锯齿型和扶手椅型六角形石墨烯分别跨接在两Au电极上, 构成分子纳器件, 同时考虑对六角形石墨烯分别进行B, N和BN局部规则掺杂. 利用第一性原理方法, 系统地研究了这些器件的电子输运特性. 计算结果表明: B及BN掺杂到扶手椅型六角形石墨烯, 对其电流有较好的调控效应, 同时发现本征及掺杂后的锯齿型六角形石墨烯均表现为半导体性质, 且N及BN掺杂时, 表现出明显的负微分电阻现象, 特别是N掺杂的情况, 能呈现显著的负微分电阻效应, 这也许对于发展分子开关有重要应用. 通过其透射特性及掺杂诱发的六角形石墨烯电子结构的变化, 对这些结果的内在原因进行了说明. 相似文献
11.
采用密度泛函理论方法研究了不同种类和数量的气体小分子在类石墨烯材料(graphenylene)衬底支撑的金属原子(M=Co, Mo和Pd, gra-M)表面的吸附特性,系统地分析了吸附不同数量的NO和CO分子的稳定构型,吸附能,电荷转移量以及引起的体系电子结构和磁性变化.研究结果表明:1) NO、CO气体小分子的稳定吸附位在金属原子顶位,吸附物与衬底间的电荷转移量表明负载不同的金属原子能够有效地调制类石墨烯材料的气敏特性;2)单个和两个气体分子吸附能够引起gra-M体系的自旋电荷密度分布发生变化,进而使得气体吸附体系表现出不同磁矩大小. 相似文献
12.
The structural, electronic, and magnetic properties of arsenene doped with a series of nonmetals (B, C, F, N, and O) and nonmagnetic metals (Al, Ga, Li, Mg, and Na) are investigated using density functional theory. Magnetism is observed in the case of C. Among all the cases, the C-doped system is the most stable formed system. Hence, we study the ferromagnetic interaction in two-C-doped arsenene. Interestingly, both nonmagnetic (NM) and antiferromagnetic (AFM) states have been observed. As the increasing C?C distance, the magnetic coupling between the moments induced by two C is found to be AFM and the origin of the coupling can be attributed to the p?p hybridization interaction involving polarized electrons. 相似文献
13.
A resonant method based on the phenomenon of electron cyclotron resonance is used to determine the frequency of collisions between electrons and He, Ar atoms and H2S, SO2, H2O, and CsCl molecules. Electron distribution over energy is measured under experimental conditions and the mean electron energy determined therefrom. Existing techniques of collision frequency measurement and calculation are discussed. Experimental dependences of reduced collision frequency on mean electron energy are obtained and the parameter E/N is compared to values presented in the literature. 相似文献
14.
F. Penent P. Lablanquie J. Palaudoux G. Gamblin L. Andric K. Ito Y. Hikosaka T. Kaneyasu J. H.D. Eland 《The European physical journal. Special topics》2009,169(1):73-78
Absorption of one VUV photon by an atom or a molecule can induce the ejection of several electrons through different processes.
Such multiple ionization processes, studied by coincidence electron spectroscopy, provide a wealth of information on electron
correlations. A magnetic bottle electron time of flight spectrometer implemented on synchrotron radiation centers has allowed
the efficient detection in coincidence of two, three and up to five electrons with good energy resolution. The branching ratios
of the different processes are easily extracted from the experimental spectra due to the constant transmission of the spectrometer.
Multiple Auger decay was observed in rare gases atoms after inner-shell ionization, while core-valence and core-core initial
double ionization followed by Auger decay are other pathways to multiple ionization. For molecules, Coulomb explosion with
energy released in ionic fragments may occur after multiple ionization, nevertheless, coincidence electron spectroscopy can
also provide a clear interpretation for peculiar decay channels in molecules. 相似文献
15.
J.E. Müller 《Applied Physics A: Materials Science & Processing》2007,87(3):433-434
I propose that an interpretation of the interaction of noble gas atoms with metal surfaces as predominantly physisorbing provides
the best explanation for the systematics of their binding energies and surface dipoles, as well as for the tendency of noble
gas atoms to bind in low coordinated sites. In the present context physisorption is defined as a process driven by the overlap
of the electrostatic atomic potentials of the interacting species.
PACS 68.43.Fg; 68.47.De 相似文献
16.
Penning electron distributions arising from the ionization of Na and K by He (1s 2s 1,3 S)-metastables in thermal collisions, as well as the absolute cross section for Penning ionization of Na by He (23 S) and relative cross sections for ionization of Na and K by He(21 S) and He(23 S) are measured. It is shown that under fairly general conditions the well depth ε* of the interaction potential between the metastable and the target particle can be obtained directly from the measured electron distributions. ε*-values are reported for the moleules He(1s 2s 1,3 S)-Na(2 S), K(2 S) (2,2Ω), and for He(1s 2s 1,3 S)-Hg(1 S)(1,3Ω). These latter values are obtained from previously published measurements and are to be considered preliminary. Further, additional evidence is given, that Penning ionization with metastables is an electron exchange process. 相似文献
17.
From a He-beam excited by electron impact we eliminated the He(21 S) component to better than 0.5% by irradiating light from a He discharge. The quenching process ishv(21 P→21 S)+He(21 S)→He(21 P)→He(11 S +hv) (21 P 1)1 S. By measuring the ions produced in collisions of the He-metastables with various target gases in a mass spectrometer, singlet to triplet Penning-cross section ratios were obtained. These ratios are without exception close to one, which is taken as evidence for the previously proposed electron exchange mechanism of the Penning ionization. In the case that more ions are produced in the collision of He (21 S) and He(23 S) with a target gas, separate relative production cross sections are obtained for the two metastables. For the rare gases the measurements are performed at two temperatures of the He-beam, 320 and 90 °K. It is found that the cross section ratio of associative — to Penning ionization increases considerably as the temperature is decreased for both, He(21 S) and He(23 S), the effect being much more pronounced for He(21 S). The results of this work are found to confirm conclusions drawn from measured energy distributions of the electrons ejected in the Penning process. 相似文献
18.
Ionizing collisions of long lived excited particles with atoms and molecules are studied by a cross beam technique. For the first time reactions of atoms in high Rydberg states are included in the investigation. In this paper we report relative cross sections for the production of the ions RH+, RH 2 + , and H 2 + by collisions of excited rare gas atoms R* with H2. With HD as the target molecule the isotope effect for the production of RD+ and RH+ has been determined. In the case of argon and krypton, ions are produced only by the high Rydberg states, whereas in the case of helium and neon only the metastable states contribute to a measurable extent. The data indicate, that the reaction mechanism is different in principle for metastable and highly excited atoms. Simple models are proposed to explain the experimental results. 相似文献
19.
The adsorption kinetics of CO2, NO, H2, D2, and H2O on a selenium foil were characterized by thermal desorption spectroscopy. In addition, Auger electron spectroscopy and X-ray diffraction were used to characterize the surface. With the exception of H/D, rather strong interactions were present, including the formation of Se hydrate. 相似文献
20.
Recent advances in the scattering of electrons by free atoms and molecules are considered with an emphasis on the interface between experiment and theory. A survey is made of the theory and methods of measurement and their trend towards the perfect scattering experiment. For atomic targets a detailed coverage is given of the various theoretical models and the results compared with experimental data. For elastic and excitation collisions, the low and high energy regions are reasonably well understood. In the medium energy region, extending from a few times the ionization threshold down to about the ionization threshold there are still difficulties arising from the infinite number of open channels. For ionizing collisions, the three body Coulomb interaction still presents unanswered theoretical problems but has inspired some elegant experimental studies. For molecular targets the additional complexities arising from the nuclear motion, the lack of a centre of symmetry and the evaluation of multicentre integrals are considered. A brief discussion of some current problems and possible future developments is given. 相似文献