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Missing line

Muns ENDOR mvolves observation of the stimulated echo intensity as a fimction of the frequency of an RE Ti-pulse applied between tlie second and third MW pulse. In contrast to the Davies ENDOR experiment, the Mims-ENDOR sequence does not require selective MW pulses. For a detailed description of the polarization transfer in a Mims-type experiment the reader is referred to the literature [43]. Just as with three-pulse ESEEM, blind spots can occur in ENDOR spectra measured using Muns method. To avoid the possibility of missing lines it is therefore essential to repeat the experiment with different values of the pulse spacing Detection of the echo intensity as a fimction of the RE frequency and x yields a real two-dimensional experiment. An FT of the x-domain will yield cross-peaks in the 2D-FT-ENDOR spectrum which correlate different ENDOR transitions belonging to the same nucleus. One advantage of Mims ENDOR over Davies ENDOR is its larger echo intensity because more spins due to the nonselective excitation are involved in the fomiation of the echo. [Pg.1581]

The n — 1 multiplet rule states that nuclei i and j will exhibit only Ji] and Wj lines. The two missing lines are the high field line of the low field multiplet and the low field line of the high field multiplet. In addition the intensity of emission and absorption over both multiplets balances as would be expected. For example, a high field E/A multiplet would at zero-field exhibit E and A n — 1 multiplets for nuclei i and j respectively. [Pg.77]

The spectra of a number of triatomic radicals with 15 valence electrons are now known for elements of the first period they are B02, N3, and NCO. In addition, the isoelectronic ions C02+ and N20+ have been investigated. The spectrum of B02 was observed by Johns41 in the flash photolysis of a mixture of BCI3 and 02, but later was found to be identical to the green bands observed in most flames and arcs containing boron.42 Isotope shifts (B1X-B10) and alternate missing lines in the spectrum immediately identify the carrier as... [Pg.15]

The remaining data could be fitted to two additional parallel lines of different slope but with a mole fraction separation essentially twice that observed for the primary family. Indeed, point 280 may well lie on a missing line between these latter lines. The slope of the lines for the primary family is similar to that for lines A and B in Figure 1, and the slope for the secondary family is close to that for lines C and D. [Pg.164]

Figure 9 Scanning tunneling microscopy (STM) image of a SAM of dodecanethiolate on Au(l 11) that shows a gold step, a screw dislocation, and depressed lines in the monolayer due to the accommodation of missing lines of thiols by vicinal molecules. The inset shows five pits in gold that were 0.24 nm deep and linked by domain boundaries. The monolayer packing corresponds to a phase of the c(4 2) rectangular superlattice. These images were provided by Biebuyck and coworkers [62]... Figure 9 Scanning tunneling microscopy (STM) image of a SAM of dodecanethiolate on Au(l 11) that shows a gold step, a screw dislocation, and depressed lines in the monolayer due to the accommodation of missing lines of thiols by vicinal molecules. The inset shows five pits in gold that were 0.24 nm deep and linked by domain boundaries. The monolayer packing corresponds to a phase of the c(4 2) rectangular superlattice. These images were provided by Biebuyck and coworkers [62]...
Propose a structure or structures consistent with the proton nmr spectrum of Fig. 17. Numbers adjacent to groups of peaks refer to relative peak areas. Account for missing lines. [Pg.231]

Since the absorbed photon carries one unit of angular momentum, a pure vibrational transition is not possible. This accounts for the missing line labelled... [Pg.283]

The correct choice is b. Fill in the missing line, based on your judgment ... [Pg.319]

Relative intensities can also be useful in confirming transitions in highly ionized species. Tech et al. (1984) examined the 4d -4d 5p transition array in La XIII (which occurs in the region 90-110 A) and they were able to correlate 31 missing lines with low predicted intensities. The 25 known levels of La XIII 4d 5p were fit with nine adjustable parameters to an RMS error of 154cm" . This is only 0.1% of the energy spread of the configuration. [Pg.169]

Chemical identification of unknowns by XRD relies in the accurate determination of a set of ii-spacings for the various crystallographic orientations. The data are screened against database of reference materials which are typically powder data with no preferred orientation. Accuracy of XRD identification of unknown species depends on the careful preparation of the samples, if powder form is required. On the other hand, if samples are not in powder form, care must be taken to account for missing lines in the XRD pattern and for abnormal intensity ratio in the observed peaks due to preferred orientation (texture). Detection limits in this case are within 0.1-1 wt%, which is worse than the ppm or ppb levels provided by surface analysis methods such as XPS or SIMS (discussed in this book). Chemical determination by XRD is limited to crystalline phases rally, but compounds can be identified down to their polymorphic phases. [Pg.40]

Figure 4 Simulated rotational spectrum of the NO ground state (X n) - note that the first rotational line is missing due to the electronic angular momentum A = 1 (n-state) such missing lines aid the assignment of electronic states. Figure 4 Simulated rotational spectrum of the NO ground state (X n) - note that the first rotational line is missing due to the electronic angular momentum A = 1 (n-state) such missing lines aid the assignment of electronic states.

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See also in sourсe #XX -- [ Pg.97 , Pg.111 ]




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