共查询到18条相似文献,搜索用时 218 毫秒
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用超高真空扫描隧道显微镜(UHV-STM)研究了室温下甘氨酸在Cu(111)表面的吸附行为.实验发现,在低覆盖度下甘氨酸分子在表面表现为二维气体.当覆盖度足够高时,甘氨酸分子最终会形成二维固相结构,为(4×8)超结构.针对这种结构提出了两种可能的结构模型,模型能够很好地解释STM图.当覆盖度介于气相和固相之间时,根据蒸镀条件和退火条件的不同,表面可能出现两种不同的中间相,一种为条纹结构,另一种为六角结构,对于中间相有待于进一步的研究
关键词:
表面吸附
甘氨酸
铜
扫描隧道显微术 相似文献
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在异质纳米结构表面发生的新现象是当前研究的热点.最近发现,尽管甘氨酸在纯Ag表面只 能作物理吸附,蒸镀在Cu表面的单层Ag岛却能在Cu的帮助下,出现对甘氨酸作化学吸附的能力,这种现象是溢流效应的一种反映.蒸镀在Ag表面的Cu岛也能帮助附近裸露的Ag表面获得 化学吸附甘氨酸的能力,虽然这里已不是单原子层的银了.结果说明这种溢流现象来源于CuA g在表面的纳米结构共存,而不只是这种共存的某个结构所特有的.但是,由于Cu的表面能大 于Ag,所以即使是在室温下,Cu岛也会逐渐地被一单层Ag原子完全覆盖,从而失去溢
关键词:
溢流
甘氨酸
Cu
Ag(111) 相似文献
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用扫描隧道显微镜(STM)研究了室温下天冬氨酸在Cu(001)表面的吸附行为.实验发现,在较 低的覆盖度下,天冬氨酸分子在Cu(001)表面存在两种吸附状态.从STM数据估算出两种吸附 状态下天冬氨酸分子在Cu(001)表面的扩散激活能分别为079±001eV,088±005eV. 随着覆盖度的提高,天冬氨酸分子最终在Cu(001)表面形成一均匀衬度的吸附层,但并不形 成有序吸附结构,也不能使台阶发生小面化.天冬氨酸分子的这些吸附特点是迄今研究过的 所有氨基酸在Cu(001)表面吸附时不具有的.
关键词:
表面吸附
扫描隧道显微镜
氨基酸 相似文献
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在超高真空中采用分子束外延(molecular beam epitaxial)技术进行C60分子在硅(111)-7×7表面的生长,并利用扫描隧道显微镜进行原位研究.室温下,相对于无层错半胞(unfaulted half unit cell),C60更易于吸附在有层错半胞(faulted half unit cell).表面台阶处的电子悬挂键密度最高,通过控制温度和时间进行退火处理后,C60分子会向着台阶的方向扩散并聚集.测量分子在不同吸附位
关键词:
60分子')" href="#">C60分子
分子束外延
Si(111)-7×7
超高真空扫描隧道显微镜 相似文献
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采用第一性原理研究了H2O分子在Fe(100),Fe(110),Fe(111)三个高对称晶面上的表面吸附.结果表明,H2O分子在三个晶面上的最稳定结构皆为平行于基底表面的顶位吸附结构.H2O分子与三个晶面相互作用的吸附能及几何结构计算结果表明H2O分子与三个晶面的相互作用程度不同,H2O分子与Fe(111)晶面的相互作用最强,其次是Fe(100),相互作用最弱的是Fe(110)表面,而这与晶面原子
关键词:
第一性原理
Fe单晶表面
2O分子')" href="#">H2O分子
分子吸附 相似文献
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室温下利用磁控溅射在p型Si(111)衬底上沉积了Cu薄膜. 利用X射线衍射和卢瑟福背散射分别对未退火以及在不同温度点退火后样品的结构进行了表征. 在此基础上,研究了Cu/SiO2/Si(111)体系的扩散和界面反应. 实验结果表明:当退火温度高于450℃时出现明显的扩散现象,并且随着温度的升高,体系扩散现象会更加显著. 当退火温度低于450℃时没有铜硅化合物生成,当温度达到500℃时才有铜硅化合物生成.
关键词:
薄膜
扩散
界面反应
硅化物 相似文献
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Adsorption geometry of glycine on Cu(001) determined with low—energy electron diffraction and scanning tunnelling microscopy
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Using low-energy electron diffraction (LEED) and scanning tunnelling microscopy (STM) it has been found that glycine molecules adsorbed on Cu(001) can form but only the (2×4) and c(2×4) superstructures. On the basis of the missing LEED spots of the surface, it has been concluded that: each (2×4) unit cell consists of two molecules, one being the mirror image of the other; the C-C axis of both molecules lies in the mirror plane of the Cu substrate without a significant shift and twist from the plane; and the two O atoms of the carboxylate group of both molecules locate at the same height level without significant buckling. According to these conclusions, a structural model has been proposed for the (2×4) superstructure (a model for the c(2×4) superstructure already exists). We argue that the (2×4) and c(2×4) superstructures must have similar specific surface free energy, that their hydrogen bonds must be of N-H-OII type, and that their local adsorption geometry must be similar or even the same. The advantage of combining STM with LEED to determine surface structures is clearly demonstrated. 相似文献
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在超高真空环境下使用扫描隧道显微镜研究了吸附有双甘氨肽分子的Cu(001)表面.在一定的 偏压条件下,针尖在该表面扫描后会形成纳米尺度的Cu团簇,这些团簇可以根据意愿排列成 字母或图形.团簇的高度同偏压、隧道电流以及时间等条件有密切关系.在室温下可以稳定存 在的团簇为制造纳米器件提供了技术上的可能性.实验结果表明,形成团簇的Cu原子不是来 自Cu衬底表面或是针尖.化学吸附在Cu表面的双甘氨肽分子,受到隧道电场的作用会在Cu表 面形成张应变场,Cu亚表面自间隙原子在张应变场作用下迁移到表面是形成团簇的原因.
关键词:
扫描隧道显微镜
纳米尺度Cu团簇
自间隙原子 相似文献
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《Surface science》2002,496(1-2):69-76
We study tip-adsorbate–substrate interactions in scanning tunneling microscopy (STM) manipulation and imaging, and the influence of impurities on the images. Thence, we perform molecular dynamics simulations and calculate qualitative STM images for oxygen on Pt(1 1 1) surface. The adsorption site of the oxygen molecule is found to be in accordance with ab initio calculations. The calculated STM image has a good resemblance to the experimental ones. The contamination of the tip by oxygen or water alters the STM image strongly. Molecular dynamics simulations on manipulations of oxygen on the surface reveal several mechanisms of how molecular oxygen can be either produced or decomposed with STM tip. Finally, we find out that transfer of oxygen from the surface to an STM tip is not very probable. 相似文献
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Ch. Loppacher M. Bammerlin M. Guggisberg E. Meyer H.-J. Güntherodt R. Lüthi R. Schlittler J.K. Gimzewski 《Applied Physics A: Materials Science & Processing》2001,72(7):S105-S108
Combined STM/AFM experiments were performed on monolayer islands of Cu-TBPP molecules on Cu(100). Pulling of single molecules on the substrate was observed and the imaging parameters were compared to STM studies. Local frequency shift vs. distance curves reveal three types of curves, which can be related to the interaction of the tip above the Cu(100) substrate, the centre of the molecule and the leg of the molecule. The frequency vs. distance curves above the legs reveal two minima, which are associated with the bending of the legs above a certain threshold value. Quantitative analysis yields force values of about 0.4 nN. 相似文献
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We report on the first successful lateral manipulation of molecules and controlled formation of nanostructures with the Scanning Tunneling Microscope (STM) at temperatures above 4 K as used by Eigler and collaborators. Among the first structures, we built the letters F and U forming the logo of our university at 30 K with CO molecules on a Cu(211) substrate. Our method to manipulate the molecules is analogous to that employed successfully up to now only by Eigler and co-workers. First experiences concerning the manipulation of the CO molecules on the highly anisotropic substrate are presented and the crucial role of the tip composition in imaging the CO molecules is demonstrated. 相似文献
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《Superlattices and Microstructures》1999,25(1-2):463-471
We briefly survey our recent studies on the ‘soft’lateral manipulation of atoms and small molecules with the scanning tunneling microscope (STM), whereby mainly the tip–surface forces are employed. Repulsive (pushing) as well as discontinuous (pulling) and continuous (sliding)attractive manipulation modes could be distinguished on Cu(211) for CO molecules and metal atoms, respectively. In the case of pulling of Cu atoms on Cu(111) even finer details could be discerned: the adparticle may show various movement patterns visiting different surface sites upon applying different tip forces. Lateral manipulation also allows modifications of the Cu(211) substrate itself in an atom-by-atom manner by releasing atoms from sixfold coordinated kink sites and even sevenfold coordinated regular step sites. Furthermore, investigations concerning controled vertical manipulation with emphasis on ‘picking-up’ single CO molecules are reported. The mechanism behind vertical transfer of CO molecules relates to ultrafast chemical processes. Vertical manipulation implies, besides extending the possibilities for the build-up of nanostructures, the important possibility of creating structurally and compositionally well-defined tips, which may eventually lead to chemical sensitivity with the STM. 相似文献
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《Surface science》1996,349(1):L139-L145
We report on a quantitative investigation of the structure and morphology of ultrathin films of Co deposited on Cu(111) by an in situ combination of real space (STM) and diffraction (LEED) techniques. The film grows initially as bilayer islands with strict fcc stacking. part of them are covered by Cu. The lateral distribution of Co- and Cu-terminated domains as well as of uncovered patches is both quantitatively determined by intensity analysis and visualized by STM images. Their simultaneous presence correlates nicely to known magnetic properties of ultrathin films, in particular with the observed magnetic anisotropy. 相似文献
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Metal-free phthalocyanine (Pc) molecules adsorbed on the Au(110) surface have been studied both experimentally (STM, LEED) and with density functional calculations. A strong interaction between substrate and adsorbate is observed. On the one hand, a clear template effect of the anisotropic substrate is observed: already at low coverages, the Pc molecules adsorb in various typical row patterns. On the other hand, the molecular adsorption modifies the substrate: at coverages higher than 0.25 monolayers, the usual (1 × 2) reconstruction is converted to a (1 × 3) reconstruction. First principle DFT calculations yield adsorption geometries that agree with the measured STM images and adsorption energies in the range of 2–3 eV. The adsorption leads to covalent and van der Waals interactions between adsorbate and substrate and is accompanied by a considerable charge transfer. 相似文献