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Localization transition

Conventional CA models are defined on particular lattice-networks, the sites of which are populated with discrete-valued dynamic elements evolving under certain local transition functions. Such a network with N sites is simply a general (undirected) graph G of size N and is completely defined by the NxN) connectivity matrix... [Pg.444]

For entirely nonadiabatic transitions, the transition probabilities are so small that the reaction does not disturb the equilibrium distribution in the nuclear subsystems (q9 Q, s), and the calculation of the mean transition probability is reduced to averaging the corresponding local transition probability over the equilibrium distribution of the coordinates q, Q, s ... [Pg.161]

The NBO-based VB-like description of localized transition-metal bonding and hyperbonding (as espoused throughout this chapter) differs significantly from more familiar descriptions of transition-metal complexes in delocalized MO terms. In this... [Pg.563]

Kellman, M. E. (1985), Algebraic Resonance Dynamics of the Normal/Local Transition from Experimental Spectra of ABA Triatomics, J. Chem. Phys. 83,3843. [Pg.229]

Fig. 10.4. Localized transition structure molecular orbital in the Stg2 reaction between Me2CuLi LiCI and MeBr. Fig. 10.4. Localized transition structure molecular orbital in the Stg2 reaction between Me2CuLi LiCI and MeBr.
These tru 5-dioxoruthenium(VI) complexes have characteristic UV-vis absorption spectra. The fj-saturated nature of the macrocyclic tertiary amine ligands enables the high-energy metal-localized transition to be observed. " The weak vibronic structured band at 370-400nm has been assigned to (0 ) —> Ru charge transfer transition that is vibronically coupled to the... [Pg.774]

The energy of the localized transition state for the ortho route (uncatalyzed reaction) is 14 kcal moL higher than that of the meta channel. Therefore, the ortho channel can be excluded. Unlike the uncatalyzed transformation, the TADDOL-catalyzed HDA... [Pg.25]

The request that no ND4 should be within the cube is represented by n = 0. The inter-centre distance increases here so fast with x that the behaviour of the system cannot be explained with ND4 clean cubes. Since the density of nucleation centres should not increase drastically on increasing x, we have either to reduce the clean volume with x, or to allow for some stray ND4 keeping the volume constant. The latter possibility is shown in Fig. 14. The open circles correspond to the values where n is increased by one when x is increased by 0.05, starting with n = 0 for x = 0.15. It should be noted that these points still correspond to Rb-rich areas. This can be seen in Fig. 14 where the minima of the curves indicate the average concentration x = n/32. The spoiling of the nucleation centres has, of course, to be paid with a lower local transition temperature, which is indeed observed in the real system. Going along with this procedure, we would obtain cluster sizes of about 100 formula units for D-RADP-25 and of 80 formula units for D-RADP-30, i.e. of about 2 nm in... [Pg.144]

The energy of the localized transition state for the ortho route (uncatalyzed reaction) is 14kcal/mol higher than that of the meta channel. Therefore, the ortho channel can be excluded. Unlike the uncatalyzed transformation, the TADDOL-catalyzed HDA reaction exhibited a clear energetic preference for the endo- over the exo-approach. Thus, only endo transition states were considered. The number of possible reaction paths/transition states is thus reduced from eight to two, namely endo-approach with re- or si-face attack of the model diene to the activated benzaldehyde. [Pg.39]

The shorter wavelength bands (200-300 mp) could be similar (but less forbidden) charge-transfer transitions or homoannular ring-localized transitions. For instance, Nesmeyanov10 concludes, from an inspection of oscillator strengths, that the strong 200 mp band is a -n -s- tt transition in the ring. [Pg.229]

We have also briefly discussed, that the inclusions of Coulomb interaction may destroy the unpinning (localization) transition at zero temperature. [Pg.115]

The main difference between metals and polymers is related to the fact that transitions from one state to another in polymers occur (as a result of changing of environmental conditions, primarily temperature) not as jumps but continuously. This leads to the absence of a clearly defined line or transition front. Additionally, because of die low heat and temperature conductivity of polymeric materials, a change in material properties may take place over a large volume,or even simultaneously throughout the whole mass of an article, although the local transition rates and degrees of conversion may be different. Thus it is necessary to develop a macrokinetic model of the transition. This model must describe the combined effects of non-stationary heat transfer and reaction kinetics and is used to determine the temperature and conversion fields. [Pg.83]

External stress, locally applied, can have nonlocal static effects in ferroelastics (see Fig. 4 of Ref. [7]). Dynamical evolution of strains under local external stress can show striking time-dependent patterns such as elastic photocopying of the applied deformations, in an expanding texture (see Fig.5 of Ref. [8]). Since charges and spins can couple linearly to strain, they are like internal (unit-cell) local stresses, and one might expect extended strain response in all (compatibility-linked) strain-tensor components. Quadratic coupling is like a local transition temperature. The model we consider is a (scalar) free energy density term... [Pg.141]

Polymers 619 and 620 exhibit two absorption maxima located at 444 and 471 nm for 619 and 473 and 503 nm for 620. These transitions likely correspond to predominantly local transitions of the constituent dibenzosilole and mono/bithiophene copolymer building blocks. The absorption maxima of polymer 618-620 cast as thin films are 401 nm (618), 484 nm (619), and 493 nm (620). The fluorine-based copolymers exhibit maxima at 427 nm in solution and 440 nm as a thin film for 621 and 456 nm in solution (with strong shoulder at 502 nm) and 460 nm as a thin film for 622. Dibenzosilole-based copolymers 619 and 620 exhibit significant bathochromic shifts of ca. 30-50 nm compared to the fluorine-based polymers 621 and 622. [Pg.327]

Carrier, film, matrix Carrier, film, matrix Controlled release Safety for administration Safety for administration Localization, transit rate control Enhancement of transport... [Pg.59]


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See also in sourсe #XX -- [ Pg.91 ]

See also in sourсe #XX -- [ Pg.429 ]

See also in sourсe #XX -- [ Pg.208 , Pg.220 , Pg.340 ]




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Electron localized-delocalized transition

Electronic transitions, local control theory

Ligand localized transitions

Linear Synchronous Transit , Local

Local Dynamics and the Glass Transition

Local phase transitions

Localized to itinerant electronic transition

Localized transition model

Localized transitions

Nucleic acids local conformational transitions

Open shell transition local spin

Phase transitions Anderson localization

Phase transitions localization under very high

Transition from localized to itinerant electronic

Transition from localized to itinerant electronic behavior

Transition localization—delocalization

Transition metal local atomic structure

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