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Evolution of the INDO SCI-calculalcd. splitting between the lowest two oplieal transitions of cofacial dimers formed by two PPV chains as a function of the inverse number of bonds .

Evolution of the INDO SCI-calculated splitting between the lowest two optical transitions of cofacial dimers formed by two PPV chains as a function of the inverse number of bonds .

Evolution of the inert composition PDF for binary mixing.

Evolution of the inicrostruclure after a creep test at I400 C lasting 14 h.

Evolution of the initial reaction rate for the reaction A Q S according to a Langmuir-Hinshelwood Hougen-Watson mechanism as a function of the reactant concentration depending on the RDS

Evolution of the innovation during the recursive estimation process .

Evolution of the insoluble fraction versus the absorbed dose and the fluence for a PVDF and a poly

Evolution of the intensities for transitions from the ground state to two bound excited states coupled by a perturbation, in the vicinity of an avoided crossing. The inner side of the hashed area gives the energies of the perturbed eigenvalues, and the hashed area gives approximate intensities. Note the zero in one of the branches at the point marked X in the figure. It is detuned from the avoided crossing and reveals stabilisation against radiation by the perturbation .

Evolution of the intensities related to the cases of

Evolution of the interfaciai morphoiogy due to crowding of the interface by interfacial copolymers and consequent decrease ofthe interfaciai tension

Evolution of the interior of a thermally pulsing AGB star. Locations of the lower boundary of the convective envelope, the H-burning shell, and lower edge to the He-shell are labelled. Two convective thermal pulses are shown. Key to understanding the s-process are the shaded bars of which the middle one is overwritten with a P and 13C - see text. From Busso, Gallino Wasserburg .

Evolution of the interlamellar distance during the transition L - L L in 20 wt POPC induced by a T-jump of 15 C from an initial temperature of 30 C. For comparison the inset represents the temperature dependence of the lamellar repeat distance of POPC under equilibrium condition. Reproduced from Reference 5 with permission of the Royal Society of Chemistry.

Evolution of the intermediate tetrachloroethylene with temperature in the oxidation of TCE over noble metal-based catalysts, in both the presence and absence of water adapted from

Evolution of the intermediate tetrachloroethylene with temperature in the oxidation of TCE over noble metal-based catalysts, in the absence and presence of water adapted from Gonzalez-

Evolution of the internal resistance

Evolution of the intrinsic catalytic activity of platinized platinum for the hydrogenation of maleic acid .5 Reprinted with permission from Elsevier Science.

Evolution of the inverse of surface resistance with thickness of polyaniline deposits.

Evolution of the ion yield during the optimization experiment plotted for the NajK-signal .

Evolution of the ionic temperature during the FEMD simulations at different electronic temperatures. For low electron excitations below about 2eV, no chemical bond dismption was observed and the net effect is only the creation of phonons induce chemical and topological modifications on the system and the

Evolution of the IR integrated absorption of the C—H stretching modes involving sp carbon atoms. The corresponding absorption band is indicated by the star in the IR spectra reported in the inset during a compression cycle.

Evolution of the IR spectra of

Evolution of the IR spectra of the CH stretching modes of the electrolyte and its residue on MgO-coated DC0O2 cathode charged to different voltages.

Evolution of the island density with growth temperature for Au N Cu

Evolution of the isotropic distribution and of the gain-to-loss ratios in nitrogen.

Evolution of the isotropic integrands s Iais for the computation of Q during tensile testing of PP nanocomposites as a function of the local macroscopic strain e on a logarithmic intensity scale



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