Cross Section for Ionization of Alkali Atoms by Collision with Excited Noble Gas Atoms

1966 ◽  
Vol 37 (7) ◽  
pp. 2928-2929 ◽  
Author(s):  
John W. Sheldon
Keyword(s):  
Cross Section ◽  
Noble Gas ◽  
Alkali Atoms

Measurements on the glory structure in the total cross section of noble gas systems I. The beam apparatus and data reduction

1979 ◽  
Vol 99 (1-2) ◽  
pp. 145-165 ◽  
Author(s):  
C.A. Linse ◽  
J.J.H. van den Biesen ◽  
E.H. van Veen ◽  
C.J.N. van den Meijdenberg ◽  
J.J.M. Beenakker
Keyword(s):  
Total Cross Section ◽  
Cross Section ◽  
Data Reduction ◽  
Noble Gas

scholarly journals Cross sections of electron collisions with noble gases atoms

2021 ◽  
pp. 11-16
Author(s):  
Rusudan Golyatina ◽  
Sergei Maiorov
Keyword(s):  
Cross Section ◽  
Cross Sections ◽  
Noble Gas ◽  
Empirical Formulas ◽  
Electron Collisions ◽  
Wide Range ◽  
Analytical Formulas ◽  
The Cross ◽  
Approximation Coefficients ◽  
Ionization Cross Sections

Consideration is given to the analysis of data on the cross sections of elastic and inelastic col-lisions of electrons with noble gas atoms. The transport (diffusion) cross section, the excita-tion and ionization cross sections are studied. For the selected sets of experimental and theo-retical data, optimal analytical formulas are found and approximation coefficients are select-ed for them. The obtained semi-empirical formulas allow us to reproduce the cross section values in a wide range of collision energies from 0.001 to 10000 eV with an accuracy of sev-eral percent.

Theory of excitation transfer in collisions between alkali atoms. I. Identical partners

1969 ◽  
Vol 47 (12) ◽  
pp. 1237-1248 ◽  
Author(s):  
E. I. Dashevskaya ◽  
A. I. Voronin ◽  
E. E. Nikitin
Keyword(s):  
Excitation Energy ◽  
Excited States ◽  
Cross Section ◽  
Electronic Excitation ◽  
Electronic States ◽  
Excitation Transfer ◽  
Electronic Excitation Energy ◽  
Alkali Atoms ◽  
The Cross

A mechanism is derived for nonresonant transfer of electronic excitation energy, induced in the process M*(2P3/2) + M(2S1/2) → M*(2P1/2) + M(2S1/2), where M and M* are identical alkali atoms in the ground and first excited states, respectively. Various types of interactions, responsible for the nonadiabatic combination of electronic states of the quasi molecule M2*, were considered, and their respective contributions to the cross section for excitation transfer were determined.

Measurements on the glory structure in the total cross section of noble gas systems II. Ne and Ar scattered by Ar, Kr and Xe

1979 ◽  
Vol 99 (1-2) ◽  
pp. 166-183 ◽  
Author(s):  
C.A. Linse ◽  
J.J.H. van den Biesen ◽  
E.H. van Veen ◽  
C.J.N. van den Meijdenberg
Keyword(s):  
Total Cross Section ◽  
Cross Section ◽  
Noble Gas

scholarly journals NOBLE GAS, ALKALI AND ALKALINE ATOMS INTERACTING WITH A GOLD SURFACE

2010 ◽  
Vol 25 (11) ◽  
pp. 2337-2344 ◽  
Author(s):  
GRZEGORZ ŁACH ◽  
MAARTEN DEKIEVIET ◽  
ULRICH D. JENTSCHURA
Keyword(s):  
Noble Gas ◽  
Gold Surface ◽  
Perfect Conductor ◽  
Interaction Potentials ◽  
Atomic Systems ◽  
Electromagnetic Interactions ◽  
Alkali Atoms ◽  
Explicitly Correlated ◽  
Realistic Representation ◽  
Dynamic Polarizabilities

The attractive branch of the interaction potentials with the surface of gold have been computed for a large variety of atomic systems: the hydrogen atom, noble gases ( He , Ne , Ar , Kr , Xe ), alkali atoms ( Li , Na , K , Rb , Cs ) and alkaline atoms ( Be , Mg , Ca , Sr , Ba ). The results include highly accurate dynamic polarizabilities for the helium atom calculated using a variational method and explicitly correlated wavefunctions. For other atoms considered we used the data available in the literature. The interaction potentials include both the effects of retardation of the electromagnetic interactions and a realistic representation of the optical response function of gold (beyond the approximation of a perfect conductor). An explicit comparison of our result to the interaction between an atom and a perfect conductor is given.

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