The effect of fluorine on the electronic spectra and ionization potentials of molecules

The effect of substituents on the spectra and ionization potentials of electrons in chromophoric groups can in a general way be divided into two major contributions, namely, ( a ) inductive effects which act mainly by changing the binding of electrons in the ground state, and ( b ) resonance effects which stabilize the molecular ion. When the substituent is a fluorine atom these effects are large but of opposite sign. The magnitude of the inductive effect is shown to be in some cases as much as several electron volts by considering sets of molecules where resonance stabilization of the molecular ion is negligible, for example, hydrocarbons and their perfluoroderivatives, NH 3 and NF 3 , the perfluoromethyl halides, etc. In other classes of molecules, such as the trifluoromethyl radicals, the fluorinated ethylenes and aromatics, large resonance stabilization of the molecular ion occurs along with the inductive effect and as these are of opposite sign, relatively small changes of ionization potential result from the substitution. The study of the dependence of increases of ionization potential due to inductive effects on the distance of the substituted fluorine from a chromophore shows how this is reduced as the separation increases. Many of the longer wavelength bands of various chromophores show shifts on substitution which are in the opposite direction to the changes which occur in the ionization potential. It is suggested that these can in many cases be attributed to the different spatial dependence of resonance and inductive effects. The interplay of this spatial variation and the dimensions of the upper orbital, especially when this has a large overlap with the substituting group, can produce energy changes in the excited orbitals which make the bands appear to behave anomolously on substitution. New values for the ionization potentials of the fluorinated ethylenes, aromatics and alkyl halides are given.

1972 ◽  
Vol 50 (7) ◽  
pp. 692-699 ◽  
Author(s):  
F. Ackermann ◽  
H. Lefebvre-Brion ◽  
A. L. Roche

The Rydberg States of the PO molecule, converging to the ground state of the PO+ ion, are calculated using the LCAO–MO SCF orbitals of the molecular ion core. An adjustment between the observed and calculated values for the energy of the first Rydberg A2Σ+ state gives a value of about 66 400 cm−1 for the ionization potential of PO. The agreement between the experimental and calculated values is very good for the other observed Rydberg states. In the 5300–3800 Å region, no more than four 2Σ+ Rydberg states are expected, which supports the "deperturbation" procedure carried out by Verma. A comparison is made between the p, d, and ƒ complexes in PO and NO. The B2Σ+ state appears to be a valence state corresponding to the electron excitation from an antibonding (vπ)* orbital to a weakly antibonding (uσ)* orbital.


Theoretical justification for a relationship between ionization potential ( I ) and electronegativity ( x ) rests in the equation derived by Mulliken (1934, 1949), viz.: X = I + E / 2 where E is the electron affinity. Elements situate on the left-hand side of the Periodic Table have small E values, so that in these cases a direct relationship between x and I might be anticipated. On the right-hand side of the Periodic Table, the electron affinities may be appreciable, and for example in the halogens, are of the order 3 to 4 eV. The neglect of the term in E in these instances represents a serious departure from Mulliken’s equation. It is furthermore important to stress that the values of I which apply in the Mulliken equation are ‘valence-state’ ionization potentials, and are not in general to be identified with the first ionization potentials of the elements, which Walsh has employed. The relationships observed by Walsh might, in consequence, be misleading in cases where the ionization potential of the ground-state of an atom is far removed (in energy) from the ionization potential of the atom in its appropriate valence-state (e.g. Zn, Cd, Hg).


Molecules ◽  
2021 ◽  
Vol 26 (6) ◽  
pp. 1615
Author(s):  
Amy Boylan ◽  
Thien S. Nguyen ◽  
Brian J. Lundy ◽  
Jian-Yuan Li ◽  
Ravikrishna Vallakati ◽  
...  

Two key factors bear on reaction rates for the conjugate addition of alkenyl boronic acids to heteroaryl-appended enones: the proximity of inductively electron-withdrawing heteroatoms to the site of bond formation and the resonance contribution of available heteroatom lone pairs to stabilize the developing positive charge at the enone β-position. For the former, the closer the heteroatom is to the enone β-carbon, the faster the reaction. For the latter, greater resonance stabilization of the benzylic cationic charge accelerates the reaction. Thus, reaction rates are increased by the closer proximity of inductive electron-withdrawing elements, but if resonance effects are involved, then increased rates are observed with electron-donating ability. Evidence for these trends in isomeric substrates is presented, and the application of these insights has allowed for reaction conditions that provide improved reactivity with previously problematic substrates.


2013 ◽  
Vol 117 (39) ◽  
pp. 10119-10128 ◽  
Author(s):  
A. V. Turbiner ◽  
J. C. Lopez Vieyra
Keyword(s):  

2016 ◽  
Vol 94 (8) ◽  
pp. 705-711
Author(s):  
Wessameldin S. Abdelaziz

Energy levels of 249 excited levels in nickel-like erbium are calculated using the 3s23p63d10 as a ground state and the single electron excited states from n = 3 to n = 4, 5 orbitals, calculations have been performed using FAC code (Gu. Astrophys. J. 582, 1241 (2003). doi:10.1086/344745 ). The populations are calculated over electron densities from 1020 to 1023 cm−3 and electron temperatures 1/2, 3/4 of the ionization potential of Ni-like Er. The gain coefficients of the transitions are calculated.


An analysis of the 1650-1350 Å band system of nitrogen dioxide has been carried out. A pattern of band spacings and intensities is found that is complex but regular. It is shown that this pattern is qualitatively, and to a large extent quantitatively, just what would be expected for a transition in which the shape of the molecule changes from bent to linear. The transition is a parallel one and the upper state has 2 Σ + u symmetry. The symmetrical stretching frequency is increased from its ground-state value to ca. 1420 cm -1 in the upper state. The upper-state bending frequency is ca. 600 cm -1 . The N — O length is decreased from its groundstate value, probably to 1·1(3) Å. The upper state resembles closely the ground state of NO + 2 . The transition is to be classed as one of the Rydberg transitions leading to the first ionization potential of NO 2 ; and the orbital to which the odd electron is transferred in the transition is (pσ) in type. The anharmonic constant g 22 for the linear upper state is found to be 2·(3) cm -1 . Other Rydberg transitions may well be present in the region, but have not been definitely identified.


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