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Substrate electrified

Why should electricity not modify the formation and properties of crystals 9 [Pg.117]

As we have seen, the chemisorption properties of the substrate depend on its electronic structure, so that changes in the latter are reflected in the former. In the case of electrified substrates, the strength of the applied electric field governs the substrate modification and, thereby, regulates the chemisorption process in a controllable manner. [Pg.117]


The process of chemisorbing an atom onto an electrified substrate is known as electrochemisorption. The initial studies, described here, employed the ANG model (English et al 1997 English and Davison 1998). Later, Davison et al (2001) incorporated the presence of surface states. [Pg.129]

Tao et al. [32] pioneered a technique based on the formation of single molecular junctions between the tip of an STM and a metal substrate. The method was adapted by other groups, modified and applied to a large number of molecular conductance studies at (electrified) solid/liquid interfaces [33, 113-119]. For details we refer to Sect. 2.3. [Pg.126]

Fig. 7.4. Chemisorption of adatom of site (bond) energy a(Pa) onto electrified chain of length m. Substrate has site (bond) energy on(P), where an = a + nT(n = 1,..., m), T being the potential gradient. Fig. 7.4. Chemisorption of adatom of site (bond) energy a(Pa) onto electrified chain of length m. Substrate has site (bond) energy on(P), where an = a + nT(n = 1,..., m), T being the potential gradient.
The ILs interact with surfaces and electrodes [23-25], and many more studies have been done that what we can cite. As one example, in situ Fourier-transform infrared reflection absorption spectroscopy (FT-IRAS) has been utilized to study the molecular structure of the electrified interphase between a l-ethyl-3-methylimidazolium tetrafluoroborate [C2Qlm][BF4] liquid and gold substrates [26]. Similar results have been obtained by surface-enhanced Raman scattering (SERS) for [C4Cilm][PFg] adsorbed on silver [24,27] and quartz [28]. [Pg.309]

A very useful extension of the voltammetric technique is cyclic voltammetry (Adams, 1969 Cauquis and Parker, 1973) in which one scans the potential of the working electrode in an unstirred electrolyte solution in the anodic (cathodic) direction and records one or several peaks due to oxidation (reduction) of the substrate. At some suitable potential, the direction of the scan is reversed and peaks due to reduction (oxidation) of intermediates and/or products formed during the forward scan are observed. In the simplest case a linear increase (decrease) of the potential with time is employed (triangular cyclic voltammetry) with scan rates in the range 0 01-1000 V s 1. It should be noted that cyclic voltammetry at scan rates above 1 Vs"1 requires the use of a differential cell to reduce the residual current due to charging of the electrified interface (see, for example, Peover and White, 1967). The theory of cyclic voltammetry has been... [Pg.7]

See also the main entry -+ underpotential deposition. Refs. [i] Haissinsky M (1933) J Chim Phys 30 27 [ii] Frumkin AN (1934) Zh Fiz Khimii 5 240 [iii] Kolb DM (1978) Physical and electrochemical properties of metal monolayers on metallic substrates. In Gerischer H, Tobias CW (eds) Advances in electrochemistry and electrochemical engineering, vol. 11. Wiley New York, p 125 [iv] Conway B (1984) Progr Surf Sci 16 1 [v] Ye S, Uosaki K (2003) Atomically controlled electrochemical deposition and dissolution of noble metals. In BardAJ, Stratmannn M, Gileadi E, Urbakh M (eds) Thermodynamics and electrified interfaces. Encyclopedia of electrochemistry, vol. 1. Wiley-VCH, p 471 [vi] Adzic R (2003) Electrocatalysis on surfaces modified by metal monolayers deposited at underpotentials. In Bard AJ, Stratmannn M, Gileadi E, Urbakh M (eds) Thermodynamics and electrified interfaces. Encyclopedia of electrochemistry, vol. 1. Wiley-VCH, p 561... [Pg.541]

The technique, electrification assisted controlled particle deposition, is based on the fundamentals of electrophotography. As shown in Fig. 12.11, at first, the electron beam produces an electrified pattern on the substrate surface. Next, positively electrified particles are attracted by electrostatic forces to the electrified pattern and adhere there. By repeating the electron beam drawing and the adhesion steps, using different types of particles, composite deposits can be created. [Pg.521]


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