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Line-patterning

It turns out that many surfaces (and many line patterns such as shown in Fig. XV-7) conform empirically to Eq. VII-20 (or Eq. VII-21) over a significant range of r (or a). Fractal surfaces thus constitute an extreme departure from ideal plane surfaces yet are amenable to mathematical analysis. There is a considerable literature on the subject, but Refs. 104-109 are representative. The fractal approach to adsorption phenomena is discussed in Section XVI-13. [Pg.275]

You will find It revealing to construct a splitting diagram similar to that of Figure 13 20 for the case in which the CIS and trans H—C=C—H coupling con stants are equal Under those circumstances the four line pattern simplifies to a triplet as It should for a proton equally coupled to two vici nal protons... [Pg.543]

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]

The 1-chloro- and 2-chlorodibenzo-p-dioxins, which readily dissolved in TFMS acid, formed cation radicals without UV irradiation or the addition of oxidizing agents. With the exception of broader resonance lines. Figure 3 shows that the five-line pattern observed with 1-chloro-dibenzo-p-dioxin is similar to that of the unsubstituted dibenzo-p-dioxin. Apparently, protons at the 2, 3, 7, and 8 positions became less equivalent... [Pg.37]

Bertrand et al. [90] isolated red crystals of radical VI, which were stable under inert atmosphere. The FPR signal of a THF solution of VI displayed a five-line pattern with an intensity ratio 1 3 4 3 1 due to coupling to two equivalent phosphorus (ap=0.94 mT) and one nitrogen (%=0.99 mT) nucleus. [Pg.69]

Salomon and Shirley [296] have performed Mossbauer-source experiments on Fe( Os) alloys with less than 0.1 at% osmium against a metallic Ir absorber. Their spectra were well-resolved magnetic eight-line patterns, which the authors could satisfactorily analyze using the Hamiltonian... [Pg.333]

We have a limited selection of line patterns or symbols. For example, we can try 3... [Pg.219]

The SEM photograph of the double-layer resist pattern thus obtained is shown in Figure 5. In this way, submicron level line patterns where the minimum line width is 0.5 ym and the aspect ratio is above 3.0 could readily be obtained. [Pg.221]

If you ever run a sample which is contaminated with an ammonium salt, in DMSO, you will see 14N-proton coupling, as shown in Spectrum 6.14. Note that the three lines of the multiplet are of equal intensity (the middle line is a little bit taller than the outer ones, but this is because of the width of the peaks at their bases. The central signal is reinforced because it stands on the tails of the outer two). This is because 14N has a spin of 1=1, and the allowed states are therefore -1, 0 and +1. This three line pattern with its 51 Hz splitting is highly characteristic and once seen, should never be forgotten. [Pg.89]

The relative intensities of the seven-line pattern then is expected to be approximately 1 12 49 84 49 12 1. With luck, all seven lines might be observable. Patterns like this are more complicated to analyze, but they also provide a fingerprint, identifying the number of equivalent nuclei involved in... [Pg.39]

Equation 10.2 affords a single, isotropic line split into a triplet by the 14N nucleus and a further splitting into doublets by the II nucleus, altogether resulting in a pattern of six-lines of equal width and intensity. For particular magnitudes of AN and AH the lines may partly, or completely overlap as is the case for the HO adduct of DMPO, which has AN AH, resulting in a four-line pattern with 1 2 2 1 intensities (Figure 10.2). [Pg.170]

Fig. 29. STM image of a Au(l 11) electrode in 0.5 M H2SO4 + 0.4 mM CuS04 + 0.1 sodium dodecyl sulfate (SDS) at +0.27 vs. Cu/Cu++. SDS adsorbs at this potential on Au(lll) as hemimicelles, forming a line pattern on the surface [97, 98],... Fig. 29. STM image of a Au(l 11) electrode in 0.5 M H2SO4 + 0.4 mM CuS04 + 0.1 sodium dodecyl sulfate (SDS) at +0.27 vs. Cu/Cu++. SDS adsorbs at this potential on Au(lll) as hemimicelles, forming a line pattern on the surface [97, 98],...
Figure 4.105 A schematic perturbative-analysis diagram for occupied valence MOs (center) of PtH42 (B3LYP/LANL2DZ level), showing tie-lines for analysis in terms of AO basis functions (left) versus NAOs (right). (A tie-line is shown when the AO or NAO contributes at least 5% to the connected MO.) Note the much smaller number of contributing orbitals, the sparser tie-line patterns, and the more realistic physical range of atomic orbital energies for NAOs than for standard Gaussian-basis AOs. Figure 4.105 A schematic perturbative-analysis diagram for occupied valence MOs (center) of PtH42 (B3LYP/LANL2DZ level), showing tie-lines for analysis in terms of AO basis functions (left) versus NAOs (right). (A tie-line is shown when the AO or NAO contributes at least 5% to the connected MO.) Note the much smaller number of contributing orbitals, the sparser tie-line patterns, and the more realistic physical range of atomic orbital energies for NAOs than for standard Gaussian-basis AOs.
The remaining step (d) in Fig. 4.106 (NLMO— MO) involves more complex tie-line patterns, but fortunately these are all superfluous and can be ignored as having no physical consequence This remark follows from the general (unitary) equivalence of MO determinantal wavefunctions formed either from NLMOs or... [Pg.569]

The conversion of iron catalysts into iron carbide under Fischer-Tropsch conditions is well known and has been the subject of several studies [20-23], A fundamentally intriguing question is why the active iron Fischer-Tropsch catalyst consists of iron carbide, while cobalt, nickel and ruthenium are active as a metal. Figure 5.9 (left) shows how metallic iron particles convert to carbides in a mixture of CO and H2 at 515 K. After 0.5 and 1.1 h of reaction, the sharp six-line pattern of metallic iron is still clearly visible in addition to the complicated carbide spectra, but after 2.5 h the metallic iron has disappeared. At short reaction times, a rather broad spectral component appears - better visible in carburization experiments at lower temperatures - indicated as FexC. The eventually remaining pattern can be understood as the combination of two different carbides -Fe2.2C and %-Fe5C2. [Pg.143]

The 193 nm light from a Questek ArF excimer laser was used to obtain sensitivity data by exposing 1 cm2 areas. Fine line patterning with 193 nm light was done on a Leitz IMS exposure apparatus with either 15X or 36X reflective objectives. The fluence was varied from 0.1 to 100 mJ/cm2/pulse. All exposures at 248 nm were conducted on a deep-UV stepper(12) with a NA = 0.38 lens, 5X reduction, a minimum feature size of 0.4 pm and a fluence of -0.3 mJ/cm2/pulse. [Pg.193]

Figure 38 shows the angular dependence of the ENDOR transitions of the amino protons in Cu(II)-doped TGS for B0 normal to a m The observed eight-line pattern... [Pg.75]

The generally multi-colored background is printed by various methods such as offset litho, indirect letterpress (letterset) and offset gravure (gravure via a rubber cylinder). Using special guilloche screens, wavy or curved line patterns are produced, which are an important security feature. [Pg.153]

If the alloy is quenched so as to preserve some of the high temperature gamma phase which is not ferromagnetic, one observes a single peak at the center in addition to the six-line pattern from the disordered solid... [Pg.28]

It is also interesting to look at alloys in this system at and near the equiatomic composition. Figure 4 shows just two lines of the six-line pattern—the two on the far right. At 50% rhodium every iron is completely surrounded by rhodium neighbors, and the lines are perfectly... [Pg.29]

Figure 6 illustrates a more complicated situation. The sample was a plain iron-carbon steel—an iron foil carburized to about 5 atomic % carbon and then quenched. One sees a rather complex pattern. There is a large central peak from some untransformed high temperature face-centered phase of iron containing carbon in solid solution, retained austenite. There is a strong six-line pattern coming from martensite, a distorted body-centered solid solution of carbon in iron. We also see a... [Pg.30]


See other pages where Line-patterning is mentioned: [Pg.446]    [Pg.145]    [Pg.211]    [Pg.324]    [Pg.506]    [Pg.58]    [Pg.343]    [Pg.65]    [Pg.66]    [Pg.464]    [Pg.192]    [Pg.94]    [Pg.108]    [Pg.241]    [Pg.194]    [Pg.99]    [Pg.286]    [Pg.87]    [Pg.164]    [Pg.207]    [Pg.44]    [Pg.140]    [Pg.567]    [Pg.952]    [Pg.312]    [Pg.407]    [Pg.21]    [Pg.77]    [Pg.230]   
See also in sourсe #XX -- [ Pg.566 , Pg.768 ]




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