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2 degree observer

Can we increase the efficiency of exciton transport in amphi-PIC J-aggregates We have to take into consideration a large disorder degree observed in amphi-PIC J-aggregates that leads to different localization effects which influence exciton dynamics in amphi-PIC J-aggregates [5]. One of the... [Pg.162]

Each vehicle must be assigned a sector of fire. Vehicle crew maintains a 360-degree observation and an air guard. [Pg.139]

Figure 7.3. Vertical distributions of electron density observed during daytime at Wallops Island, Virginia, during different seasons, for a zenith angle of 60 degrees. Observations in April 1964, June 1965, September 1965, and December 1965. From Mechtly and Smith (1968). Figure 7.3. Vertical distributions of electron density observed during daytime at Wallops Island, Virginia, during different seasons, for a zenith angle of 60 degrees. Observations in April 1964, June 1965, September 1965, and December 1965. From Mechtly and Smith (1968).
Adsorbant functionality Contact angle H2O (degree) Contact angle HD (degree) Observed thickness (nm) Expected thickness (nm)... [Pg.100]

The following weather conditions were observed in the locally confined area of technological work wind direction 25°, speed 11 knots current direction 50°, speed 0.9 knots wave direction 300° degrees, observed significant wave height 1 m. [Pg.30]

A first approach to testing, ASTM D 1094, is to create, using a potassium phosphate reagent, a separation between two layers, hydrocarbon and aqueous. The degree of separation of the two phases is estimated by attributing a grade from 1 to 3 and the appearance of the interface by five levels of observation 1, lb, 2, 3, and 4. The specifications establish both the quality of separation (2 is the maximum) and the appearance of the interface (lb maximum). [Pg.250]

The parameters of equivalent planar OSD are then obtained by iterative minimization of a specifie dissimilarity eriterion measuring the degree of matching between the parametric descriptions of the observed segmented Bscan image Y° = s" = n = 1,..,jV and... [Pg.173]

The main disadvantage of Feldkamp s approaeh is the fact, that it is mathematically correct only in tire midplane of the beam. With larger Cone-Beam angles the error grows and over 30 degrees severe artefacts can be observed In the reconstruction. [Pg.494]

In principle, nucleation should occur for any supersaturation given enough time. The critical supersaturation ratio is often defined in terms of the condition needed to observe nucleation on a convenient time scale. As illustrated in Table IX-1, the nucleation rate changes so rapidly with degree of supersaturation that, fortunately, even a few powers of 10 error in the preexponential term make little difference. There has been some controversy surrounding the preexponential term and some detailed analyses are available [33-35]. [Pg.335]

The effect of temperature on contact angle is seldom very great, as a practical observation. Some values of d0/dTare included in Table X-2 a common figure is about -0.1 degrees/K (but note the case of CS2 on ice also rather large temperature changes may occur in L1-L2-S systems (see Ref. 160). [Pg.369]

Chemical properties of deposited monolayers have been studied in various ways. The degree of ionization of a substituted coumarin film deposited on quartz was determined as a function of the pH of a solution in contact with the film, from which comparison with Gouy-Chapman theory (see Section V-2) could be made [151]. Several studies have been made of the UV-induced polymerization of monolayers (as well as of multilayers) of diacetylene amphiphiles (see Refs. 168, 169). Excitation energy transfer has been observed in a mixed monolayer of donor and acceptor molecules in stearic acid [170]. Electrical properties have been of interest, particularly the possibility that a suitably asymmetric film might be a unidirectional conductor, that is, a rectifier (see Refs. 171, 172). Optical properties of interest include the ability to make planar optical waveguides of thick LB films [173, 174]. [Pg.560]

Infrared Spectroscopy. The infrared spectroscopy of adsorbates has been studied for many years, especially for chemisorbed species (see Section XVIII-2C). In the case of physisorption, where the molecule remains intact, one is interested in how the molecular symmetry is altered on adsorption. Perhaps the conceptually simplest case is that of H2 on NaCl(lOO). Being homo-polar, Ha by itself has no allowed vibrational absorption (except for some weak collision-induced transitions) but when adsorbed, the reduced symmetry allows a vibrational spectrum to be observed. Fig. XVII-16 shows the infrared spectrum at 30 K for various degrees of monolayer coverage [96] (the adsorption is Langmuirian with half-coverage at about 10 atm). The bands labeled sf are for transitions of H2 on a smooth face and are from the 7 = 0 and J = 1 rotational states Q /fR) is assigned as a combination band. The bands labeled... [Pg.634]

One might expect the frequency factor A for desorption to be around 10 sec (note Eq. XVII-2). Much smaller values are sometimes found, as in the case of the desorption of Cs from Ni surfaces [133], for which the adsorption lifetime obeyed the equation r = 1.7x 10 exp(3300// r) sec R in calories per mole per degree Kelvin). A suggested explanation was that surface diffusion must occur to desorption sites for desorption to occur. Conversely, A factors in the range of lO sec have been observed and can be accounted for in terms of strong surface orientational forces [134]. [Pg.709]

Figure A3.4.4 summarizes these steps in one scheme. Different theories of elementary reactions represent different degrees of approximations to certain averages, which are observed in experiments. Figure A3.4.4 summarizes these steps in one scheme. Different theories of elementary reactions represent different degrees of approximations to certain averages, which are observed in experiments.
In extensively deionized suspensions, tliere are experimental indications for effective attractions between particles, such as long-lived void stmctures [89] and attractions between particles confined between charged walls [90]. Nevertlieless, under tliese conditions tire DLVO tlieory does seem to describe interactions of isolated particles at tire pair level correctly [90]. It may be possible to explain tire experimental observations by taking into account explicitly tire degrees of freedom of botli tire colloidal particles and tire small ions [91, 92]. [Pg.2687]

Figure C3.2.12. Experimentally observed electron transfer time in psec (squares) and theoretical electron transfer times (survival times, Tau a and Tau b) predicted by an extended Sumi-Marcus model. For fast solvents tire survival times are a strong Emction of tire characteristic solvent relaxation dynamics. For slower solvents tire electron transfer occurs tlirough tire motion of intramolecular degrees of freedom. From [451. Figure C3.2.12. Experimentally observed electron transfer time in psec (squares) and theoretical electron transfer times (survival times, Tau a and Tau b) predicted by an extended Sumi-Marcus model. For fast solvents tire survival times are a strong Emction of tire characteristic solvent relaxation dynamics. For slower solvents tire electron transfer occurs tlirough tire motion of intramolecular degrees of freedom. From [451.

See other pages where 2 degree observer is mentioned: [Pg.118]    [Pg.67]    [Pg.216]    [Pg.4]    [Pg.268]    [Pg.184]    [Pg.128]    [Pg.334]    [Pg.315]    [Pg.288]    [Pg.27]    [Pg.257]    [Pg.467]    [Pg.652]    [Pg.72]    [Pg.74]    [Pg.177]    [Pg.265]    [Pg.927]    [Pg.1078]    [Pg.1263]    [Pg.2061]    [Pg.2109]    [Pg.2363]    [Pg.2488]    [Pg.2500]    [Pg.2538]    [Pg.2618]    [Pg.2785]    [Pg.2841]    [Pg.3033]    [Pg.513]    [Pg.50]   
See also in sourсe #XX -- [ Pg.4 ]




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