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Isolated line approximation

The RC is an ideal system to test theoretical ideas (memory effect, coherence effect, etc.), fundamental approximations (isolated line approximation, Markov approximation, etc.), and techniques (generalized linear response theory, Forster-Dexter theory, Marcus theory, etc.) for treating ultrafast phenomena. As mentioned above, this ideality is mainly due to the fact that the electronic energy level spacing in RC is small (typically from 200 to 1500 cm-1), and the interactions between these electronic states are weak. [Pg.212]

If visual inspection of the most suspect joints or stopcocks fails to reveal the leak, a systematic isolation of parts of the vacuum system is in order. For a vacuum line of conventional design (e.g., a line approximating that in Fig. 5.2), it is generally best to turn off all stopcocks which interconnect the various parts of the vacuum system. As a result, the high-vacuum manifold is isolated from the pumps and the rest of the line, and it is checked by determining if there is a steady pressure rise in that section. If this section appears to be intact, but it... [Pg.78]

No isolated lines are present in this spectrum, preventing a precise analysis of the lineshape. The linewidth of 5 GHz FWHM exceeds, however, substantially the spectral resolution and clearly indicates the fragment recoil. As shown in Fig. 3b, the lines may be approximated by a Gaussian profile so that the width of 5 GHz can be related to a most probable recoil speed v= 1430 m/s of C2(a II ) in a respective vibrational -rotational level, v corresponds to an average kinetic recoil energy of —2 CO2 photons of 10.591 pm, compared to 0.4 photons obtained in the previous experiment with the time-of-flight technique. [Pg.139]

January 10, 1987 (UN-lOO-N-23) - External corrosion caused a leak in the diesel oil supply line. Approximately 760 L (200 gal) of diesel oil was released to the soil. The line was isolated, excavated, and repaired. Groundwater Monitoring Well 199-N-16 was sampled and oil was found. Residual oil was recovered from the well (WHC 1989b). [Pg.144]

The NMR characteristics of the bromonium ion triflate prove to be interesting in that the proton NMR spectrum of a 1 1 mixture of parent olefin and bromonium ion at room temperature is an average of those of the two isolated species. This suggests that there is a rapid site exchange of the Br+ between the ion and olefin. The phenomenon can be most simply studied by NMR spectroscopy. An approximately 100 mM solution of the ion in CD2C12 held at - 80°C was treated with small aliquots of Ad=Ad, the NMR spectrum was monitored after each addition. At zero added Ad=Ad, the spectrum of the ion consists of a seven line pattern indicative of a species (eqn. 3, 5a) having two perpendicular planes of symmetry that pass, respectively, through the three heavy atoms of the bromonium... [Pg.116]

There is an approximation implicit in the final line. The subscript zero implies an average for an isolated system (i.e., on an adiabatic or bare Hamiltonian trajectory), whereas the actual trajectory used to obtain this result is the modified one, ry(f r,) ro(f r,). In so far as these are the same to leading order, this difference may be neglected. [Pg.72]

The Caco-2 cell line was isolated from a human colon carcinoma, and has been characterized as one of the best in vitro models of intestinal epithelium. Indeed, in contrast to other intestinal cell lines, Caco-2 cells are able to constitute a homogenous monolayer and to spontaneously differentiate into polarized cells, highly similar to human mature enterocytes, after approximately 2 weeks of culture. Furthermore, the Caco-2 cells present microvillosities at the apical side and have a high transmembrane resistivity, which confirms the fact that the cells are confluent and link to one another via gap junctions. Finally, they can absorb different compounds, express many enzymes involved in intestinal metabolic pathways (Pinto et al. 1983, Musto et al. 1995, Salvini et al. 2002), and give reproducible in vitro results consistent with results obtained in in vivo studies (Artursson and Karlsson 1991). [Pg.381]

The catalyst preparation area is positioned between the two polyethylene production units with 60 feet separating each one. The aluminum alkyls storage canopy and isopentane horizontal storage tank are located at a remote area at an approximate distance of 250 feet away from the production and utility areas. The isopentane is transported to the catalyst preparation area through a 3-inch pipeline. A remote actuated isolation valve on this supply line that fails closed is located at the isopentane storage tank. This control valve and an associated isopentane feed pump are managed by the operator in the control room. [Pg.369]

Whereas absorption spectra can be obtained at a given temperature via Monte-Carlo t q)e simulations, the reach of equilibrium in an excited state of an isolated cluster is less obvious, and even less is the definition of a relevant temperature. In any case, the final state may be strongly dependent on the excitation process. Here we will ignore the vibrations of the Na(3p)Arn cluster. We assume a Franck-Condon type approximation and that emission takes place from relaxed equilibrium geometry structures on the Na(3p)Arn excited PES. The Einstein coefficients of the lines of emission towards the ground state at energy AE are given by... [Pg.380]

To consider gas molecules as isolated from interactions with their neighbors is often a useless approximation. When the gas has finite pressure, the molecules do in fact collide. When natural and collision broadening effects are combined, the line shape that results is also a lorentzian, but with a modified half-width at half maximum (HWHM). Twice the reciprocal of the mean time between collisions must be added to the sum of the natural lifetime reciprocals to obtain the new half-width. We may summarize by writing the probability per unit frequency of a transition at a frequency v for the combined natural and collision broadening of spectral lines for a gas under pressure ... [Pg.39]

External noise denotes fluctuations created in an otherwise deterministic system by the application of a random force, whose stochastic properties are supposed to be known. Examples are a noise generator inserted into an electric circuit, a random signal fed into a transmission line, the growth of a species under influence of the weather, random loading of a bridge, and most other stochastic problems that occur in engineering. In all these cases clearly (4.5) holds if one inserts for A(y) the deterministic equation of motion for the isolated system, while L(t) is approximately but never completely white. Thus for external noise the Stratonovich result (4.8) and (4.9) applies, in which A(y) represents the dynamics of the system with the noise turned off. [Pg.233]


See other pages where Isolated line approximation is mentioned: [Pg.143]    [Pg.308]    [Pg.178]    [Pg.1042]    [Pg.104]    [Pg.17]    [Pg.143]    [Pg.232]    [Pg.975]    [Pg.329]    [Pg.91]    [Pg.328]    [Pg.400]    [Pg.107]    [Pg.234]    [Pg.7]    [Pg.184]    [Pg.352]    [Pg.33]    [Pg.139]    [Pg.169]    [Pg.466]    [Pg.68]    [Pg.74]    [Pg.170]    [Pg.639]    [Pg.211]    [Pg.164]    [Pg.162]    [Pg.231]    [Pg.492]    [Pg.87]    [Pg.146]    [Pg.301]    [Pg.94]    [Pg.284]    [Pg.90]    [Pg.347]    [Pg.442]   
See also in sourсe #XX -- [ Pg.212 ]




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