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Sign reversal

Figure 2 Flow diagram of the DHT with N=8, P=3. Broken lines represent transfer factors -1 while full lines represent unity transfer factor. The crossover boxes perform the sign reversal called for by the shift theorem which also requires the sine and cosine factors Sn, Cn. Figure 2 Flow diagram of the DHT with N=8, P=3. Broken lines represent transfer factors -1 while full lines represent unity transfer factor. The crossover boxes perform the sign reversal called for by the shift theorem which also requires the sine and cosine factors Sn, Cn.
Finally, following Mead and Truhlar [10], it may be seen that an interchange of A and B is equivalent to a sign reversal of <() followed by a rotation perpendicular to the AB bond, under the latter of which Aab) is invariant and Fab) changes sign. The net effect is therefore to induce the tiansitions... [Pg.31]

Its charge density distribution is like that of the cation (with sign reversal) because the added electron goes into the nonbonded orbital with a node at the central carbon atom. The probability of finding that electron precisely at the central carbon atom is zero. [Pg.212]

Thns the strain energy release rate is effectively an instantaneous value of Dupre s energy of adhesion, with 6 = 0(0 instead of the equilibrium value. The sign reversal in the left-hand side of Eq. (18) when compared to Eq. (15) is due simply to the fact that we have a closing crack with a spreading liquid. [Pg.295]

Fig. 12. Derivative curves of EPR in a highly dislocated As-doped germanium crystal grown in a H2 atmosphere. The magnetic field is oriented along the [100] direction. T= 2 K, /= 25.16 GHz. Note the sign reversal of the new lines as compared to the As-donor hyperfine structure. Dislocation density 2 x 104 cm 2. (Courtesy Pakulis and Jeffries, reprinted with permission from the American Physical Society, Pakulis, E.J., Jeffries, C D. Phys. Rev. Lett. (1981). 47, 1859.)... Fig. 12. Derivative curves of EPR in a highly dislocated As-doped germanium crystal grown in a H2 atmosphere. The magnetic field is oriented along the [100] direction. T= 2 K, /= 25.16 GHz. Note the sign reversal of the new lines as compared to the As-donor hyperfine structure. Dislocation density 2 x 104 cm 2. (Courtesy Pakulis and Jeffries, reprinted with permission from the American Physical Society, Pakulis, E.J., Jeffries, C D. Phys. Rev. Lett. (1981). 47, 1859.)...
Cell name Mutagens Selective agents Mutating frequency Phenotype sign Reverse frequency... [Pg.214]

Thus, it clearly appears that sign reversal occurs in this coupling system. As will be seen later, this is partly dependent upon molecular geometry and upon nature of substituents, but the main factor is the... [Pg.28]

A positive sign has also been found for P-O-CH involving a pentaco-ordinated phosphorus (in phosphonitrilics).(1969,68) As no J(P-O-CH) values are in the vicinity of zero it is unlikely that this coupling experiences sign reversal it may be taken as positive in all cases. As a consequence, this is not so for J(P-0-C-CH), especially for the above mentioned phosphites. [Pg.40]

Similar behaviour is found in the variously substituted vinylic systems. In Pm fluorinated vinyl compounds, for which Cowley and Taylor have obtained the relative signs, <1969.54>55) s founcj that sign reversal may occur in gem couplings and that the trans couplings generally have the lowest values (Table XX). [Pg.50]

It should be pointed out that sign reversals are likely to occur when the hybridisation of phosphorus, or the nature of the substituents, change in systems such as <1988,62)... [Pg.52]

The interest in considering such couplings in relation to the nature of P-P bonds has been discussed by Cowley in an earlier review.<1965,26) Since then a considerable amount of experimental data has been obtained and sign determination on typical compounds has revealed another interesting fact, namely that sign reversal occurs in this one-bond coupling depending upon the hybridisation of phosphorus and possibly upon the substituents. As mentioned earlier (Section III.A) this has prompted some theoreticians to consider this problem in detail. [Pg.60]

The observed trend may be interpreted on the basis of changes of s character but again sign reversal is present. [Pg.68]

Fig. 10. This feature undoubtedly reflects that there are similar factors effecting these couplings. Another observation which warrants mention is that geminal HPH couplings which have recently been investigated also demonstrate the same sign reversal, without any clear correlation with the H-P-H bond angle, but are very dependent upon the hybridisation of the phosphorus. (1969 41>... Fig. 10. This feature undoubtedly reflects that there are similar factors effecting these couplings. Another observation which warrants mention is that geminal HPH couplings which have recently been investigated also demonstrate the same sign reversal, without any clear correlation with the H-P-H bond angle, but are very dependent upon the hybridisation of the phosphorus. (1969 41>...
Table 3 Orbital energies of the 111 anion (a.u., signs reversed). Table 3 Orbital energies of the 111 anion (a.u., signs reversed).
To check (13.13) we can invoke the solution to the scattering problem for an optically active sphere. Such a sphere is symmetric under all rotations, but the off-diagonal elements of its scattering matrix (13.7) do not vanish identically. As required by symmetry and the matrices (13.12) and (13.13), (13.7) is invariant with respect to interchange and sign reversal of its off-diagonal elements. [Pg.411]

In crystalline semiconductors, the most common technique for the measurement of carrier mobility involves the Hall effect. However, in noncrystalline materials, experimental data are both fragmentary and anomalous (see, for example. Ref. [5]). Measured HaU mobility is typically of the order of 10 - 10 cm A /s and is frequently found to exhibit an anomalous sign reversal with respect to other properties providing information concerning the dominant charge carrier. Thus, apart from some theoretical interest, the Hall effect measurements are of minimal value in the study of macroscopic transport in amorphous semiconductors. [Pg.39]

W. M. Latimer, Oxidation Potentials. 2nd edn.. Prentice-Hall. New York, 1952. As its title implies, this book contains oxidation potentials (i.e. reduction potentials with their signs reversed, as was the convention at the time of its publication) for all the elements. This is a classic book, full of good chemistry, written by the inventor of Latimer diagrams and still available in libraries. [Pg.122]


See other pages where Sign reversal is mentioned: [Pg.4]    [Pg.10]    [Pg.336]    [Pg.336]    [Pg.384]    [Pg.232]    [Pg.85]    [Pg.106]    [Pg.261]    [Pg.282]    [Pg.108]    [Pg.114]    [Pg.442]    [Pg.442]    [Pg.391]    [Pg.135]    [Pg.142]    [Pg.258]    [Pg.21]    [Pg.50]    [Pg.12]    [Pg.13]    [Pg.14]    [Pg.68]    [Pg.290]    [Pg.218]    [Pg.220]    [Pg.373]    [Pg.23]    [Pg.42]    [Pg.384]   
See also in sourсe #XX -- [ Pg.7 , Pg.60 ]

See also in sourсe #XX -- [ Pg.290 ]

See also in sourсe #XX -- [ Pg.358 ]




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