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Structural tunnels

Scanning tunnelling microscopy (STM) Composition/topo-graphy and atomic structure Tunneling current scans a conducting surface... [Pg.168]

The development of scanning probe microscopies and x-ray reflectivity (see Chapter VIII) has allowed molecular-level characterization of the structure of the electrode surface after electrochemical reactions [145]. In particular, the important role of adsorbates in determining the state of an electrode surface is illustrated by scanning tunneling microscopic (STM) images of gold (III) surfaces in the presence and absence of chloride ions [153]. Electrodeposition of one metal on another can also be measured via x-ray diffraction [154]. [Pg.203]

PTM Photon tunneling microscopy [12] An interface is probed with an evanescent wave produced by internal reflection of the illuminating light Surface structure... [Pg.313]

STM Scanning tunneling microscopy [9, 19, 31] Tunneling current from probe scans a conducting surface Surface structure... [Pg.313]

We have considered briefly the important macroscopic description of a solid adsorbent, namely, its speciflc surface area, its possible fractal nature, and if porous, its pore size distribution. In addition, it is important to know as much as possible about the microscopic structure of the surface, and contemporary surface spectroscopic and diffraction techniques, discussed in Chapter VIII, provide a good deal of such information (see also Refs. 55 and 56 for short general reviews, and the monograph by Somoijai [57]). Scanning tunneling microscopy (STM) and atomic force microscopy (AFT) are now widely used to obtain the structure of surfaces and of adsorbed layers on a molecular scale (see Chapter VIII, Section XVIII-2B, and Ref. 58). On a less informative and more statistical basis are site energy distributions (Section XVII-14) there is also the somewhat laige-scale type of structure due to surface imperfections and dislocations (Section VII-4D and Fig. XVIII-14). [Pg.581]

At a surface, not only can the atomic structure differ from the bulk, but electronic energy levels are present that do not exist in the bulk band structure. These are referred to as surface states . If the states are occupied, they can easily be measured with photoelectron spectroscopy (described in section A 1.7.5.1 and section Bl.25.2). If the states are unoccupied, a teclmique such as inverse photoemission or x-ray absorption is required [22, 23]. Also, note that STM has been used to measure surface states by monitoring the tunnelling current as a fiinction of the bias voltage [24] (see section BT20). This is sometimes called scamiing tuimelling spectroscopy (STS). [Pg.293]

Schneir J, Harary H H, Dagata J A, Hansma P Kand Sonnenfeld R 1989 Scanning tunneling microscopy and fabrication of nanometer scale structure at the liquid-gold interface Scanning Microsc. 3 719... [Pg.320]

Figure Bl.4.9. Top rotation-tunnelling hyperfine structure in one of the flipping inodes of (020)3 near 3 THz. The small splittings seen in the Q-branch transitions are induced by the bound-free hydrogen atom tiiimelling by the water monomers. Bottom the low-frequency torsional mode structure of the water duner spectrum, includmg a detailed comparison of theoretical calculations of the dynamics with those observed experimentally [ ]. The symbols next to the arrows depict the parallel (A k= 0) versus perpendicular (A = 1) nature of the selection rules in the pseudorotation manifold. Figure Bl.4.9. Top rotation-tunnelling hyperfine structure in one of the flipping inodes of (020)3 near 3 THz. The small splittings seen in the Q-branch transitions are induced by the bound-free hydrogen atom tiiimelling by the water monomers. Bottom the low-frequency torsional mode structure of the water duner spectrum, includmg a detailed comparison of theoretical calculations of the dynamics with those observed experimentally [ ]. The symbols next to the arrows depict the parallel (A k= 0) versus perpendicular (A = 1) nature of the selection rules in the pseudorotation manifold.
Hamers R J and Kohler U K 1989 Determination of the local electronic structure of atomic-sized defects on Si(OOI) by tunnelling spectroscopy J. Vac. Sc/. Technol. A 7 2854... [Pg.1721]

Maaloum M, Chretien D, Karsenti E and FIdrber J K FI 1994 Approaching microtubule structure with the scanning tunnelling microscope (STM) J. Ceii Sc/. 107 part II 3127... [Pg.1722]

Shiv]i A P, Brown F, Davies M C, Jennings K H, Roberts C J, Tendler S J B, Wilkinson M J and Williams P M 1995 Scanning tunnelling microscopy studies of p-amyloid fibril structure and assembly FEBS Lett. 371 25-8... [Pg.1724]

Matsumoto H, Inukai J and Ito M 1994 Structures of copper and halides on Pt(111), Pt(IOO) and Au(111) electrode surfaces studied by in situ scanning tunneling microscopy J. Eiectroanai. Chem. 379 223-31... [Pg.2759]

Daizadeh I, Guo J-X and Stuchebrukhov A 1999 Vortex structure of the tunneling flow in long-range electron transfer reactions J. Chem. Phys. 110 8865-8... [Pg.2996]

Fig. 8. (a) Structure of a typical resonant tunneling diode (RTD) (b) conduction band diagram for the barrier stmcture where (-------) represents the... [Pg.375]

The maximum voltage drop in the tunnel is approximately (neglecting current flow from the tunnel structure into the surrounding soil) [6] ... [Pg.352]

The coherent tunneling case is experimentally dealt with in spectroscopic studies. For example, the neutron-scattering structure factor determining the spectral line shape is... [Pg.24]

The fine structure of torsion-vibration spectra of small symmetric molecules and groups such as CH3, CH4, NH3, and NH4 is one of the most illustrative manifestations of tunneling. This problem has been discussed in detail in several reviews and books (see, e.g., Press [1981], Heidemann et al.[1987]). [Pg.114]

Among numerous examples of the role of the chemical structure in tunneling rotation we select just one, connected with the effect of intramolecular hydrogen bond. In acetyl acetone in stable enol form... [Pg.120]

Fig. 57. The INS structure factor at different temperatures for rotational tunneling in a (CH3)2SnCl2 crystal. Fig. 57. The INS structure factor at different temperatures for rotational tunneling in a (CH3)2SnCl2 crystal.

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