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Even-electron

The symmetry argument actually goes beyond the above deterniination of the symmetries of Jahn-Teller active modes, the coefficients of the matrix element expansions in different coordinates are also symmetry determined. Consider, for simplicity, an electronic state of symmetiy in an even-electron molecule with a single threefold axis of symmetry, and choose a representation in which two complex electronic components, e ) = 1/v ( ca) i cb)), and two degenerate complex nuclear coordinate combinations Q = re " each have character T under the C3 operation, where x — The bras e have character x. Since the Hamiltonian operator is totally symmetric, the diagonal matrix elements e H e ) are totally symmetric, while the characters of the off-diagonal elements ezf H e ) are x. Since x = 1, it follows that an expansion of the complex Hamiltonian matrix to quadratic terms in Q. takes the form... [Pg.7]

The concept of biradicals and biradicaloids was often used in attempts to account for the mechanism of photochemical reactions [2,20,129-131]. A biradical (or diradical) may be defined as [132] an even-electron molecule that has one bond less than the number permitted by the standard rules of valence. [Pg.388]

In practice side reactions intervene to reduce the efficiency of the propagation steps The chain sequence is interrupted whenever two odd electron species combine to give an even electron product Reactions of this type are called chain terminating steps Some commonly observed chain terminating steps m the chlorination of methane are shown m the following equations... [Pg.173]

Even-electron ion. An ion containing no unpaired electrons, e.g., CHj in its ground state. [Pg.441]

Consider now the behaviour of the HF wave function 0 (eq. (4.18)) as the distance between the two nuclei is increased toward infinity. Since the HF wave function is an equal mixture of ionic and covalent terms, the dissociation limit is 50% H+H " and 50% H H. In the gas phase all bonds dissociate homolytically, and the ionic contribution should be 0%. The HF dissociation energy is therefore much too high. This is a general problem of RHF type wave functions, the constraint of doubly occupied MOs is inconsistent with breaking bonds to produce radicals. In order for an RHF wave function to dissociate correctly, an even-electron molecule must break into two even-electron fragments, each being in the lowest electronic state. Furthermore, the orbital symmetries must match. There are only a few covalently bonded systems which obey these requirements (the simplest example is HHe+). The wrong dissociation limit for RHF wave functions has several consequences. [Pg.111]

Processes occurring upon ionization and notations used for odd-electron ions (4) and even-electron ions ( + ) are illustrated in Equations 1, 2, and 3. [Pg.211]

It can be determined from the higher effect of the p-substitution compared with the 7-substitution and the high donor ability of the stilbene (ECT = 200 kJ mol-1 x(HOMO) = 0.504 qa = qp = 1.000), that an even electron distribution in the n-system of the donor causing a high electron density in the vicinity of the monomer double bond is important for the strength of the EDA interaction between 71-donor and 7t-acceptor. [Pg.202]

Section III.C). Using a rotational temperature to characterize an ion source can be misleading, as the reactions used to form the ions of interest can be quite exothermic, producing vibrationally and even electronically excited ions. These degrees of freedom are more difficult to cool than rotations. Transitions from vibrationally excited molecules provide very useful information, if they can be identified and analyzed. Hot FeO (produced using 3% N2O in helium) has a... [Pg.337]

The product ions generated by chemical ionisation are stable even-electron species with relatively little excess energy compared to those generateg electron impact. The chemical ionization mass... [Pg.989]

DI methods tend to produce even-electron ions such as protonated molecules [M + H]+, or cationised molecules such as [M + Na]+ these stable ions undergo only a minimum amount of fragmentation. Desorption/ionisation mass-spectral methods (in particular FD, EH and LD) may be used for determining molecular... [Pg.384]

Poor understanding of fragmentation of even-electron ions... [Pg.498]

The case of interaction between an even-electron molecule A and an odd-electron molecule B can be discussed in a similar manner. Eq. (3.20) is modified to be... [Pg.22]

As seen in the previous section, one characteristic of the triplet state is its paramagnetism. This alone would of course not suffice as a definition of the triplet since there are many odd-electron species that also exhibit paramagnetism but do not exist as triplets. Thus we might state that a triplet is a paramagnetic even-electron species. This still does not constitute a limiting definition since compounds containing even numbers of electrons may exhibit two, three, or even five distinct electronic levels. For example, when in a biradical the radical centers are separated by several carbon atoms as below, no interaction between the electron spins occurs and the radicals appear as two doublet states ... [Pg.410]

When spin-orbit coupling is introduced the symmetry states in the double group CJ are found from the direct products of the orbital and spin components. Linear combinations of the C"V eigenfunctions are then taken which transform correctly in C when spin is explicitly included, and the space-spin combinations are formed according to Ballhausen (39) so as to be diagonal under the rotation operation Cf. For an odd-electron system the Kramers doublets transform as e ( /2)a, n =1, 3, 5,... whilst for even electron systems the degenerate levels transform as e na, n = 1, 2, 3,. For d1 systems the first term in H naturally vanishes and the orbital functions are at once invested with spin to construct the C functions. [Pg.54]

For the odd electron systems, tf3 4Z andc 5 6Z+, measurements of the average susceptibility at very low temperatures are not likely to prove as informative as for the even electron, d 32 species. This is because whereas the latter yield a limiting value of 1 as T -+ 0, from which D/g2 can be directly estimated, the former lead only to a limiting value of the (x)-1 vs. T slope, which except for large values of D will be difficult to determine. Nevertheless calculation shows that even in cases for which only very small deviations from the spin-only behaviour are to be expected, e.g. V(Cp)2, the susceptibility may yet show very considerable anisotropy. Thus, with the parameters of Prim and Van Voorst (47), V(Cp)2 is predicted to show an anisotropy, (x — X )Kx of some 5% at liquid nitrogen temperatures, whilst Ni(Cp)2, with the much larger/) value, should show an anisotropy of about 30% at 77K, which is reduced only to some 12% even at room temperature. There is thus considerable scope for the measurement of anisotropic susceptibilities, and although this technique would probably not be applicable to the d8 bis-arenes (97,... [Pg.108]

Whilst for a molecule it is enough to specify its molecular weight (MW), this is not true for ions. In fact, an ion is defined by its mass (m) and by its charge (z). Both even-electron ions, like H30+, and radical ions, i.e. radicals that carry an electric charge, like CH4+", can be formed in a mass spectrometer. With MS it is possible to study positive or negative ions molecules with basic properties are easily protonated, while those having acidic character are more easily deprotonated. [Pg.39]

In soft ionization methods the excess energy deposited onto the ionized molecule is very small and stable even-electron ions are formed. This leads to easy determination of the molecular weight of the analyte, but as fragmentation is absent or it occurs to a very low extent, structural information is missing in the mass spectrum. However, one can obtain structural information by causing ion fragmentation out of the source by means of tandem mass spectrometry experiments (see below). [Pg.47]

The term desorption ionization indicates those ionization techniques in which the production of ions is based on a desorption process. This consists of the rapid addition of energy to a sample in a condensed phase (i.e. liquid or solid) with subsequent production and emission of stable ions in the gas phase. These are generally even electron species that fragment only to a limited extent. The development of desorption methods has amplified the impact and utility of MS in a lot of fields, such as biology, biochemistry and proteomics. [Pg.51]


See other pages where Even-electron is mentioned: [Pg.6]    [Pg.376]    [Pg.441]    [Pg.268]    [Pg.16]    [Pg.455]    [Pg.50]    [Pg.50]    [Pg.19]    [Pg.180]    [Pg.667]    [Pg.990]    [Pg.1003]    [Pg.360]    [Pg.540]    [Pg.228]    [Pg.308]    [Pg.45]    [Pg.45]    [Pg.45]    [Pg.45]    [Pg.48]    [Pg.66]    [Pg.101]    [Pg.110]    [Pg.561]    [Pg.177]    [Pg.324]    [Pg.170]    [Pg.5]   
See also in sourсe #XX -- [ Pg.130 ]




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Electrons, 176 even number

Even-electron ion

Even-electron ligand

Even-electron molecular species

Even-electron rule

Fragmentation mechanisms of even electron anions (EE

Neutral Dienes and Even-electron Reagent Ions

Odd- and Even-Electron Ions

Odd-even electron numbers and energy level statistics in cluster assemblies

Ortho Elimination from Even-Electron Ions

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