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Reconstruction phases

Figure Bl.23.8. Scattering intensity of 2 keV Ne versus azimuthal angle 6 scans for Pt 110] in the (1 x 2) and (1 X 3) reconstructed phases. Scattering angle 0 = 28° and incident angle a = 6°. Figure Bl.23.8. Scattering intensity of 2 keV Ne versus azimuthal angle 6 scans for Pt 110] in the (1 x 2) and (1 X 3) reconstructed phases. Scattering angle 0 = 28° and incident angle a = 6°.
Figure 7. Proposed structure model of the cne-dlnEnsicaially ordered streak jhase, the second reconstructed phase observed with the H/Ni(110) system. Again, shaded circles represent Ni atoms of the second layer. Figure 7. Proposed structure model of the cne-dlnEnsicaially ordered streak jhase, the second reconstructed phase observed with the H/Ni(110) system. Again, shaded circles represent Ni atoms of the second layer.
Reconstructive phase transitions Chemical bonds are broken and rejoined the reconstruction involves considerable atomic movements. Such conversions are always first-order transitions. [Pg.33]

The coordination numbers of the atoms increase from 6 to 8 in the NaCl —> CsCl type conversion therefore, it is a reconstructive phase transition which can only be a first-order transition. [Pg.256]

It is noteworthy that prior to the advent of scanning probe microscopy electrochemically driven reconstruction phenomena had been identified and studied using traditional macroscopic electrochemical measurements [210,211], However, STM studies have provided insight as to the various atomistic processes involved in the phase transition between the reconstructed and unreconstructed state and promise to provide an understanding of the macroscopically observed kinetics. An excellent example is provided by the structural evolution of the Au(lOO) surface as a function of potential and sample history [210,211,216-223], Flame annealing of a freshly elec-tropolished surface results in the thermally induced formation of a dense hexagonal close-packed reconstructed phase referred to as Au(100)-(hex). For carefully annealed crystals a single domain of the reconstructed phase... [Pg.256]

Figure 5 shows the 3-dimensional reconstructed attractors and their projections on canonical planes. The reconstructed phase portraits do not exhibit a defined structure, i.e., it is not toroidal or periodic. As matter of fact, the oscillatory structure is only observed in the Poincare map. The Poincare map is often used to observe the oscillatory structure in dynamical systems. The... [Pg.295]

In a single HRTEM image, it is difficult to measure atomic positions with a high accuracy especially next to an interface due to contrast delocalization. However, the delocalization is removed in the exit wave function and the maxima in the reconstructed phase directly correspond to the center of the atomic positions. The atomic positions can, therefore, be measured with a... [Pg.390]

Figure 4 (a) A clockwise step up followed by a clockwise step down generates a shift in the reconstruction order R. and R+ indicate the two possible reconstructed phases, (b) As a consequence of this a closed clockwise step must be accompanied by domain boimdaries between the two phases R. and R+. [Pg.220]

Figure 9 (a) The network of crossing steps, and (b) a combination of two step arrays of different orientation, after the phase separation, predicted by (5) for e > 0, has occurred. The + and - indicate the opposite reconstruction phases induced by the clockwise steps. [Pg.225]

Changing the bond graph—reconstructive phase transitions... [Pg.172]

Reconstructive phase transitions occur when major changes are made in the topology, i.e. when the bond graph is reorganized. The transitions usually observed in structures with lattice-induced strain are displacive and often second order (no latent heat). Reconstructive transitions arise when two quite different structures with the same composition have similar free energies. Unlike the displacive transitions they involve the dissolution of one structure and the recrystallization of a quite different structure. These phase transitions possess a latent heat and often display hysteresis. [Pg.172]

The steady state reaction of NO with H2 and NH3 on Pt(l 0 0) has been studied using REMPI detection of the N2 product state distributions [134]. These reactions show very complex kinetics, with strongly coverage dependent reaction rates which lead to kinetic oscillations [135] and explosive desorption [136]. This surface also shows a phase transition between the clean surface hex reconstructed phase and... [Pg.171]

Although the detailed features of the interactions involved in cortisol secretion are still unknown, some observations indicate that the irregular behavior of cortisol levels originates from the underlying dynamics of the hypothalamic-pituitary-adrenal process. Indeed, Ilias et al. [514], using time series analysis, have shown that the reconstructed phase space of cortisol concentrations of healthy individuals has an attractor of fractal dimension dj = 2.65 0.03. This value indicates that at least three state variables control cortisol secretion [515]. A nonlinear model of cortisol secretion with three state variables that takes into account the simultaneous changes of adrenocorticotropic hormone and corticotropin-releasing hormone has been proposed [516]. [Pg.335]

In the disillusionment phase, however, depression and hopelessness may become more prominent, as the reality of how life has changed postdisaster becomes ever more apparent. The enormous drain of reserves— physical, financial, and emotional—takes its toll. Adults may experience physical reactions such as headaches, increased blood pressure, ulcers, gastrointestinal problems, and sleep disorders. Emotional reactions may vacillate between emotional numbness and expressions of intense emotion. Anxiety and depression are common emotional reactions, as are anger and frustration— sometimes displaced onto relief workers when anger about the disaster seems less rational. The reconstruction phase gradually becomes more apparent as intense emotions are replaced by a sense of acceptance, increasing independence, and emotional reinvestment in relationships and activities of daily life. [Pg.85]

Thus if we know the moduli (amplitudes) and the phase angles of X-ray reflections, we can calculate the distribution of electron density in the unit cell, that is, find the atomic positions. Finding Fhki from fu is straightforward, but the values of ahu are lost in all usual diffraction experiments. Determining (reconstructing) phase angles remains the most difficult part of the structure solution. [Pg.1106]


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Changing the bond graph—reconstructive phase transitions

Maximum-likelihood phase reconstruction

Phase reconstructive

Phase reconstructive

Phase space reconstruction

Phase transformation reconstructive

Reconstruction of Phase Portraits

Reconstruction of the Phase Space

Reconstructive phase transition

Soft phonons reconstructions structural phase transitions

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