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Ionization energy 184 Subject

Figures 8.7 and 8.8 illustrate the point that there are two ways in which we can define the ionization energy. One is the adiabatic ionization energy which is defined as the energy of the v = 0 — v" = 0 ionization. This quantity can be subject to appreciable uncertainty if the... Figures 8.7 and 8.8 illustrate the point that there are two ways in which we can define the ionization energy. One is the adiabatic ionization energy which is defined as the energy of the v = 0 — v" = 0 ionization. This quantity can be subject to appreciable uncertainty if the...
The He(Ia) photoelectron spectra of the parent heterocycles have been the subject of much study. Initially the assignment of the ionization energies to appropriate occupied molecular orbitals was confused by the unexpected reversal in the sequence of the two highest occupied MOs in tellurophene relative to the other heterocycles. The reported values are compared in Table 24. The assignments are based upon comparisons with the spectra... [Pg.24]

Indazoles have been subjected to certain theoretical calculations. Kamiya (70BCJ3344) has used the semiempirical Pariser-Parr-Pople method with configuration interaction for calculation of the electronic spectrum, ionization energy, tt-electron distribution and total 7T-energy of indazole (36) and isoindazole (37). The tt-densities and bond orders are collected in Figure 5 the molecular diagrams for the lowest (77,77 ) singlet and (77,77 ) triplet states have also been calculated they show that the isomerization (36) -> (37) is easier in the excited state. [Pg.175]

The advantages and disadvantages of most of the techniques dealt with in this report have already been discussed in their respective sections. However, it is perhaps useful to compare their relative utilities in determining certain useful quantities, such as, e.g., impurity concentrations, or ionization energies. The discussion in this section will be brief and mostly qualitative, and it must be remembered that some of the conclusions drawn may be more subjective than hard and firm. [Pg.121]

Again, t is the coupling between the two orbitals that are located at 1 in our distance units, 2A is the relative ionization potential of the donor and acceptor orbitals and the c s are the orbital coefficients. Solutions of this equation for E are the variationally minimized energies subject to the polarization constraint. The A dependent wave functions give the energy of the polarized state and its polarization P(A). We will define a unitless polarization V as (-c2D + c ). The analytical result for the energy as a function of polarization is... [Pg.103]

The hetero atom parameters have been obtained in various ways, for example by striving for a best correlation of HOMO values with ionization energies, or of polarographic reduction potentials with LUMO values. The whole subject of SHM parameters and best heteroatom parameters is now of little practical importance, since much better quantitative molecular orbital methods are now readily available. [Pg.614]

The small number of fundamental mass spectrometric studies on Ge, Sn and Pb derivatives also accounts for our poor knowledge of their thermochemistry. Heats of formation, ionization energies, bond energies and electron affinities of even simple Ge, Sn and Pb species are still scarce and subject to considerable uncertainty, as illustrated in the most recent NIST database5. [Pg.360]


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Ionization Subject

Ionization energy

Ionizing energy

Subject energy

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