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Surface Orders

A large number of ordered surface structures can be produced experimentally on single-crystal surfaces, especially with adsorbates [H]. There are also many disordered surfaces. Ordering is driven by the interactions between atoms, ions or molecules in the surface region. These forces can be of various types covalent, ionic, van der Waals, etc and there can be a mix of such types of interaction, not only within a given bond, but also from bond to bond in the same surface. A surface could, for instance, consist of a bulk material with one type of internal bonding (say, ionic). It may be covered with an overlayer of molecules with a different type of intramolecular bonding (typically covalent) and the molecules may be held to the substrate by yet another fomi of bond (e.g., van der Waals). [Pg.1758]

The ability of XPD and AED to measure the short-range order of materials on a very short time scale opens the door for surface order—disorder transition studies, such as the surface solid-to- liquid transition temperature, as has already been done for Pb and Ge. In the caseofbulkGe, a melting temperature of 1210 K was found. While monitoring core-level XPD photoelectron azimuthal scans as a function of increasing temperature, the surface was found to show an order—disorder temperature 160° below that of the bulk. [Pg.249]

LEED is the most powerfiil, most widely used, and most developed technique for the investigation of periodic surface structures. It is a standard tool in the surface analysis of single-crystal surfaces. It is used very commonly as a method to check surface order. The evolution of the technique is toward greater use to investigate surface disorder. Progress in atomic-structure determination is focused on improving calculations for complex molecular surface structures. [Pg.262]

Figure 2.12 A set of parallel, isentropic surfaces ordered so that S, > S2 > S3. The solid curve marked 6 rev = 0 represents a reversible adiabatic path that connects two states that lie on the entropy surface. Si. The dashed curves marked 6qm = 0 are irreversible paths that connect states on different entropy surfaces. Only one of these two paths will be allowed the other will be forbidden. Figure 2.12 A set of parallel, isentropic surfaces ordered so that S, > S2 > S3. The solid curve marked 6 rev = 0 represents a reversible adiabatic path that connects two states that lie on the entropy surface. Si. The dashed curves marked 6qm = 0 are irreversible paths that connect states on different entropy surfaces. Only one of these two paths will be allowed the other will be forbidden.
Because the second harmonic response is sensitive to the polarizability of the interface, it is sensitive to the adsorption and desorption of surface species and is capable of quantifying surface species concentrations. Furthermore, SHG can be used to quantify surface order and determine surface symmetry by measuring the anisotropic polarization dependence of the second harmonic response. SHG can also be used to determine important molecular-level and electrochemical quantities such as molecular orientation and surface charge density. [Pg.501]

Clavilier J, Feliu J, Femandez-Vega A, Aldaz A. 1989a. Electrochemical behaviour of irreversibly adsorbed bismuth on Pt(lOO) with different degrees of crystalline surface order. J Electroanal Chem 269 175-189. [Pg.239]

In chemical vapor deposition (CVD or MOCVD), a film of the desired material is prepared by evaporation of volatile precursor molecules which then decompose to give a film deposited on the substrate. The ordering in the film as it grows is dictated by the surface ordering of the substrate, hence the deposition is epitaxial . The necessary decomposition of the precursor molecules can take place either on the surface of the substrate or in the gas phase close to it. [Pg.702]

In what follows we will discuss systems with internal surfaces, ordered surfaces, topological transformations, and dynamical scaling. In Section II we shall show specific examples of mesoscopic systems with special attention devoted to the surfaces in the system—that is, periodic surfaces in surfactant systems, periodic surfaces in diblock copolymers, bicontinuous disordered interfaces in spinodally decomposing blends, ordered charge density wave patterns in electron liquids, and dissipative structures in reaction-diffusion systems. In Section III we will present the detailed theory of morphological measures the Euler characteristic, the Gaussian and mean curvatures, and so on. In fact, Sections II and III can be read independently because Section II shows specific models while Section III is devoted to the numerical and analytical computations of the surface characteristics. In a sense, Section III is robust that is, the methods presented in Section III apply to a variety of systems, not only the systems shown as examples in Section II. Brief conclusions are presented in Section IV. [Pg.143]

Understanding Sensitivity to Long-Range Surface Order... [Pg.42]

As an ex situ technique for structural information on surfaces, STM is an excellent complement to the standard electron and ion diffraction probes of surface order. The STM method can identify both short range order and long range periodicity, as well as disordered surface layers (e.g., images of sorbic acid on Highly Ordered Pyrolitic Graphite (HOPG), vida infra). In contrast,... [Pg.176]

Independently of the technique used to investigate the prise cause of the existence of the adsorption states at the higher potentials on Pt(lll) and Pt(100), the conclusion is they result froa the existence of atoaically flat extended surface doaains with the respective orientation, i.e. existence of long range surface order. These adsorption states appear as an intriguing and a unique property of well-ordered Pt(lll) and Pt(100) surfaces in contact with various electrolyte solutions because no equivalent effects are known with the saae orientations in gas phase experiaents. In this sense, these properties say be considered as a specific aspect of the electrocheaistry of surface processes. [Pg.206]

The same type of voltammogram has been obtained with a Pt (111) electrode after its ordered surface was subjected to argon ion bombardment, introducing structural defects like randomly distributed steps (14). The similar effects of oxygen electrosorption and ion bombardment show clearly that the former perturbs the surface order,... [Pg.207]

A voltammetric characterization of platinum single crystal surfaces produced by these three methods shows that a very similar surface order and cleanliness are obtained in each case. The features embodied by the third method which we use for the radio-electrochemistry work, are as follows ... [Pg.249]

Leermakers, F. A. M. and Cohen Stuart, M. A. (1996). Self-consistent-field lattice gas model for the surface ordering transition of n-hexadecane, Phys. Rev. Lett., 76, 82-85. [Pg.103]

Azz - (1/2 Axx + 1/2 Ayy) is the maximum anisotropy in hyperfine splitting that is possible. The anisotropy observed in Figure 6, and reported in Table 3 below, is much smaller than the maximum. One can quantify the degree of surface ordering by defining an order parameters, 8 ... [Pg.372]

Since the early 1980s, cyclic voltammetry has been used to characterize singlecrystal electrodes in terms of surface order, presence or absence of defects, contaminations, and so on. In some cases, the... [Pg.518]

Electronic structure theory has developed to a point where realistic bond energies and activation barriers can be calculated. Typically the model catalysts used in such calculations are even more idealized than in the surface science experiments (perfect surfaces, ordered overlayers etc.), but the insight into the details of the potential energy surface of the reaction is much greater. [Pg.87]

Bowers, J., Vergara-Gutierrez, M. C., and Webster, J. R. R, Surface ordering of amphiphilic ionic liquids, Langmuir, 20, 309-312, 2004. [Pg.351]

In many cases ordering is no longer observable in the presence of steps. Ordered carbonaceous layers form on the Ir(l 11) crystal face, for example, while ordering is absent on the stepped iridium surface. Ordering is absent on stepped Pt surfaces for most molecules that would order on the low Miller-Index (111) or (100) surfaces. [Pg.15]

Figure 4.1. Calculated adsorption energy for atomic oxygen as a function of distance of the atom above the surface for a range of close-packed transition metal surfaces (ordered according to their position in the periodic table). In the box showing results for Ru, the energy per atom in 02 is shown for comparison. Only metals where the minimum in the adsorption energy function is below this value will be able to dissociate 02 exothermally. Adapted from Ref. [4]. Figure 4.1. Calculated adsorption energy for atomic oxygen as a function of distance of the atom above the surface for a range of close-packed transition metal surfaces (ordered according to their position in the periodic table). In the box showing results for Ru, the energy per atom in 02 is shown for comparison. Only metals where the minimum in the adsorption energy function is below this value will be able to dissociate 02 exothermally. Adapted from Ref. [4].
Despite the range of hydrides present, hydride termination by HF etching stabilizes the surface against oxidation and maintains surface ordering for further wet chemistry. Hydride-terminated germanium shows no oxidation after exposure to ambient... [Pg.338]

The non-Abelian Stokes theorem in its original operator form roughly claims that the holonomy around a closed curve C = 05 equals a surface-ordered... [Pg.438]

As with all surface analytical methods, surface preparation is critical to obtaining reproducible SHG from metallic surfaces and single crystals in particular. For surfaces prepared in UHV and then transferred to an electrochemical cell, sputtering and heating or annealing followed by Auger analysis of impurities should proceed inert transfer. Low energy electron diffraction (LEED) can also be used to check surface order. Metal electrode surfaces, particularly for the rotational anisotropy ex-... [Pg.159]

Wajnberg, E. El-Jaick, L.J. Linhares, M.P. Esquivel, D.M. Ferromagnetic resonance of horse spleen ferritin core blocking and surface ordering temperatures. J. Magn. Reson. 2001, 153(1), 69-74. [Pg.67]

Monoenergetic beams of atoms are scattered from ordered surfaces and detected as a function of scattering angle. This gives structural information on the outermost layer of the surface. Atom diffraction is extremely sensitive to surface ordering and defects. [Pg.511]

First we want to know the interaction with the bare substrate does the molecule become physisorbed, chemisorbed, dissociate or react with the surface atoms, what is the interaction time To answer these questions we have to prepare a clean MgO surface, which is obtained by cleavage under UHV (the cleanliness and the perfect surface order are checked by diffraction of He atoms and AES [23]). Then, a pulsed beam of NO is directed to the MgO clean surface and the (possible) desorbed products (NO, N2, N20, N02, 02) are simultaneously detected by the mass spectrometer. [Pg.258]


See other pages where Surface Orders is mentioned: [Pg.464]    [Pg.71]    [Pg.225]    [Pg.78]    [Pg.182]    [Pg.60]    [Pg.51]    [Pg.250]    [Pg.6]    [Pg.435]    [Pg.449]    [Pg.410]    [Pg.28]    [Pg.179]    [Pg.181]    [Pg.142]    [Pg.158]    [Pg.165]    [Pg.57]    [Pg.61]    [Pg.598]    [Pg.224]   
See also in sourсe #XX -- [ Pg.260 ]




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Alloy surface ordering

Contents 1 First-order Energy Surfaces

Copolymer, block surface-induced ordering

Filler surface modifier structural ordering

First-order reactions surface reaction

Higher-order models, response surface

Interfacial Phenomena at Surfaces of Structurally Ordered Silicas

Lateral ordered surface alloy

Liquid crystal, surface-induced ordering

Long-range surface order, sensitivity

Microscopic surface order, nematics

Nth-order surface reaction

Order parameter at the surface

Order parameter surfaces

Ordered alloys, surface segregation

Ordering on Surfaces

Orders of surfaces

Phase transition, surface first-order

Polyimide surface ordering

Polymers ordered, periodic surfaces

Possible Mechanisms of Defects-Induced Ferromagnetic Order Near the Surface

Potential energy surface first-order derivatives

Potential energy surface second-order derivatives

Potential-energy surfaces first order

Potential-energy surfaces zero order

Properties ordered surface alloy

Range Surface Order

Reaction second-order surface

Response Surface Methodology second-order designs

Second order surface perturbation

Second-order surface polarization

Single-surface nuclear dynamics, vibronic multiplet ordering

Surface Modification and Ordered Monolayers

Surface Orientational Order

Surface chemical ordering

Surface excess order parameter

Surface first order

Surface layer order parameter

Surface magnetic ordering

Surface order-disorder transition

Surface ordered alloys

Surface ordering

Surface ordering

Surface ordering parameter

Surface orientational order, nematics

Surface reaction first-order

Surface reactions unimolecular, first-order

Surface structure ordered

Surface-Induced Changes in the Orientational Order Parameter

Surface-Induced Smectic Ordering

Surface-enhanced order

Surface-induced order

Surface-induced ordering

Surface-order forces

The Effect of Surface Irregularities on Ordering

Transition, first-order surface effects)

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