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Zero sum rule

A negative long-period peak is always accompanied by two positive satellite peaks with each half the area (simplified zero-sum rule). Remember the alternating signs of the 5-functions in Fig. 8.24 and have a look at p. 158. [Pg.167]

A third effect that has been encountered [185] is a structure that is made from a mixture of different kinds of clusters which are all finite stacks and vary by the number of their members. At the first glance such a material looks as if the zero-sum rule were violated - but for each individual cluster it is not. Figure 8.45 shows a sketch of the probability of different clusters in such a structure. In the study [ 185] the parallel fit using three finite stacks (solos, duos, trios of lamellae) yielded a peculiar coupling of cluster fractions according to the relation... [Pg.194]

The General Series Expansion for Stacks. In practice, ID scattering intensities can always be modeled by programming the obvious series expansion of such a structural entity every correlated distance along the stack axis is producing an attenuated oscillation according to Hk (5) that is weighted by the probability of its occurrence under consideration of the zero-sum rule and the related correlation-construction principle (p. 158, Fig. 8.30)... [Pg.195]

At a first glance this subtraction appears to be a violation of the zero-sum rule. However, here an exception has to be made, because particles merge upon direct contact of adjacent structural entities, and thus the number of particles is reduced — just by the amount deduced by RULAND. [Pg.196]

As mentioned above, LSD yields a reasonable description of the exchange-correlation hole, because it satisfies several exact conditions. However, since the correlation hole satisfies a zero sum rule, the scale of the hole must be set by its value at some value of . The local approximation is most accurate at points near the electron. In fact, while not exact at m = 0, LSD is highly accurate there. Thus the on-top hole provides the missing link between the uniform electron gas and real atoms and molecules [18]. [Pg.13]

We now consider the locality of the antiparallel-spin contribution to the correlation energy, relative to the total correlation energy. The holes corresponding to both these contributions obey the zero sum rule, Eq. (17). However, the parallel-spin on-top correlation hole vanishes, suggesting that this hole will... [Pg.24]

You can use valences to write chemical formulas. This method is faster than using Lewis structures to determine chemical formulas. As well, you can use this method for both ionic and covalent compounds. In order to write a chemical formula using valences, you need to know which elements (or polyatomic ions) are in the compound, and their valences. You also need to know how to use the zero sum rule For neutral chemical formulas containing ions, the sum of positive valences plus negative valences of the atoms in a compound must equal zero. [Pg.98]

What is the formula of a compound that consists of magnesium and chlorine You know that the valence of magnesium, Mg, is +2. The valence of chlorine, Cl, is -1. The formula MgCl is not balanced, however, because it does not yet obey the zero sum rule. How can you balance this formula You might be able to see, at a glance, that two chlorine atoms are needed for every magnesium atom. If it is not obvious how to balance a formula, you can follow these steps ... [Pg.99]

Unnormalized FE-NBMO amplitudes are found by a zero-sum rule identical to that of Longuet-Higgins (II) for Hiickel coefficients. Consequently, the unnormalized FEMO amplitudes precisely coincide with the unnormalized Hiickel coefficients. However, to obtain correct normalization, the contributions to the density have to be integrated along the three bonds converging to a joint, whereas only two bonds converge to a nonjoint. Thus, the different 0 values are somewhat compensated by the differences in the coefficients, as shown in the following equations ... [Pg.293]

Cob is the nonbonding MO (NBMO) coefficient on the carbon atom where the oxirane ring is opened. It is calculated according to the Longuet-Higgins zero sum rule for odd alternant aromatic hydrocarbons [36,65], Incidentally, the first authors to try such NBMO coefficients of exocyclic atoms of odd-alternant PAH derivatives were Dipple, Lawley and Brookes [66] in 1968. [Pg.453]

NBMO is equai to the number No in the Hnckel spectrum [56]. Thus, the enumeration of No is reduced to a determination of the number of independent parameters in NBMO which satisi the zero-sum rule. The application of this method is illustrated for 8>indacene (Figure 4). The procedure is as follows eq. (58) is stepwise satisfied for ea< vertex of a graph G Vertices for which the zero-sum rule is executed are denoted by bla dots (a). [Pg.238]

Figure 4. The enumeration of NBMO s in s-indacene (1) Stepwise application of the zero-sum rule (58)... Figure 4. The enumeration of NBMO s in s-indacene (1) Stepwise application of the zero-sum rule (58)...

See other pages where Zero sum rule is mentioned: [Pg.167]    [Pg.171]    [Pg.189]    [Pg.193]    [Pg.195]    [Pg.198]    [Pg.611]    [Pg.107]    [Pg.95]    [Pg.107]    [Pg.679]    [Pg.152]    [Pg.152]    [Pg.156]    [Pg.174]    [Pg.178]    [Pg.180]    [Pg.183]    [Pg.294]    [Pg.373]    [Pg.37]    [Pg.37]   
See also in sourсe #XX -- [ Pg.98 ]




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