Positron-impact direct ionization of lithium, sodium and potassium atoms

2021 ◽  
Vol 75 (10) ◽  
Author(s):  
R. Utamuratov ◽  
D. V. Fursa ◽  
A. S. Kadyrov ◽  
R. I. Campeanu ◽  
I. Bray ◽  
...  
1996 ◽  
Vol 74 (7-8) ◽  
pp. 367-372 ◽  
Author(s):  
J. Moxom ◽  
P. Ashley ◽  
G. Laricchia

The single direct ionization cross sections for positron scattering [Formula: see text] on He, Ar, Kr, and H2 were measured and compared with existing data and the corresponding cross sections for electron impact [Formula: see text]. At most impact energies the present data for He and H2 are in reasonable accord with other measurements and, in the case of He, with some of the available calculations. At low energies, [Formula: see text] is found to increase more slowly than [Formula: see text], probably due to the importance of Ps formation in this energy range.


Atoms ◽  
2021 ◽  
Vol 9 (4) ◽  
pp. 99
Author(s):  
Małgorzata Franz ◽  
Katarzyna Wiciak-Pawłowska ◽  
Jan Franz

We introduce two models for the computation of direct ionization cross sections by positron impact over a wide range of collision energies. The models are based on the binary-encounter-Bethe model and take into account an extension of the Wannier theory. The cross sections computed with these models show good agreement with experimental data. The extensions improve the agreement between theory and experiment for collision energies between the first ionization threshold and the peak of the cross section. The models are based on a small set of parameters, which can be computed with standard quantum chemistry program packages.


A quadrupole mass spectrometric analyser for use in flame ionization is described, together with its application to the ions produced by traces of sodium, added as chloride, in premixed hydrogen-air flames. Negative ions (Cl¯ and OH¯) appear to be of subsidiary importance in the main ionization processes, which rather proceed through direct production of electrons. Nevertheless, it is established that the appearance of Cl¯ ions is consistent with dissociative attachment HCl+ e ¯ → Cl¯+H, rather than by three-body attachment Cl+ e ¯+ M → Cl¯+ M . Hydroxyl ions probably are formed in the same way. The ratios of the amounts of A + (alkali) and A + . H 2 O (alkali monohydrate) ions have been measured in the cases of lithium, sodium and potassium. Equilibrium constants for the reaction A + .H 2 O ⇌ A + + H 2 O are obtained and heats of monohydration of 44, 28 and 17 kcal/mole deduced respectively for A ≡ Li, Na, K. Small amounts of H 3 O + appear in the reaction zone because of traces of hydrocarbon impurities in the flame gas supplies. These are severely reduced by alkali addition, apparently by an exchange reaction A +H 3 O + → A + +H 2 O+H, with a rate constant of 1.1 x 10 -8 cm 3 /s at 2000 °K, rather than by recombination with electrons produced by direct ionization of alkali H 3 O + + e - → H 2 O+H. In contrast with the steady production of A + ions in the burnt gases by reactions of the type A + M → A + + e ¯+ M , there is an anomalously high rate of production in the reaction zone. This appears difficult to explain without introduction of processes involving ‘hot’ electrons.


Sign in / Sign up

Export Citation Format

Share Document