Binary peak

The whole spectrum is dominated by the ECC peak, which, in accordance with theory, extends much higher than the experimental data. The cusp itself shows the usual asymmetry, with cross sections after the peak falling off more steeply than before it. The binary peak is negligibly small at this projectile energy because the projectile velocity is of the same magnitude as the velocity spread associated with the target electron. 

Switch on X-rays and search for a peak by scaiming the axis. The binary peak search described in section 2.6.1.1 is the most efficient if the position is unknown. An intense peak is easily seen, therefore the scan can be fast, with short detector counting times. 

Figure 3-19. Photodissociation of HI monomers and clusters. The solid traces indicate the substantial discrimination available when using polarized photolysis radiation note the high S/N. Under conditions of such minimal clustering, it is reasonable to assume that most of the clusters are binary. Peaks labeled v = 1 and v = 2 are due to inelastic H + HI collisions within the cluster. The superelastic peak ft is assigned tentatively to secondary photolysis of I HI complexes, in which the escaping hydrogen deactivates the nearby I, (a) Vertical and (b) horizontal polarization of the photolysis radiation relative to the molecular beam. The plenum pressure is 1900 torr.

Concept of molecular ratio of iron oxides. Why does the activity show hump)-type curve (binary peak) with the ratio of Fe +/Fe + At first, someone suggested that it is possible the result of the increasing contents of iron in the catalysts. However, it is seen from Fig. 3.28 that the activity displays the hump-type curve along with the increasing Fe +/Fe + and this kind of difference of activity is not caused by the changing contents of the iron. Because the contents of the iron increase monotonicaUy with the increasing Fe /Fe " ", while the activity does not. 

The limits of lifetime detection and resolution in on-the-flight fluorescence lifetime detection in hplc were evaluated for simple, binary systems of polycycHc hydrocarbons (70). Peak homogeneity owing to coelution was clearly indicated for two compounds having fluorescence lifetime ratios as small as 1.2 and the individual peaks could be recovered using predeterrnined lifetimes of the compounds. Limits of lifetime detection were deterrnined to be 6 and 0.3 pmol for benzo[b]fluoranthene and benzo[k]fluoranthene, respectively. 

The thermal, mechanical, and morphological behaviors of two binary blends, HDPE-E-plastomer (Engage 8200) and iPP-E-plastomer (Engage 8200) have been investigated to compare the compatibility and molecular mechanistic properties of the blends. Both systems are thermodynamically immiscible but mechanically compatible. Thermal studies indicate that both blends exhibit two distinct melting peaks and there is depression of the HDPE melting peak in the blend with high... 

The experiments showing the influence of lateral interaction on coelution of the two species were discussed in Subsection 2.4.2. Figure 2.18 and Figure 2.19 give a comparison of single profiles of acid and ketone or of alcohol and ketone with those attained for the binary mixture. Very similar peak profiles can be obtained upon solving Equation 2.21 separately for the alcohol, acid, and ketone with isotherms (Equation 2.4 and Equation 2.7a), and for the binary mixture with the isotherms (Equation 2.9 and Equation 2.10). 

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