Showing posts with label photoelectron. Show all posts
Showing posts with label photoelectron. Show all posts

Tuesday, 23 May 2023

Atomic Photoionization Dependence on the Light Polarization: Application to Hydrogenoid Atom | Chapter 6 | Fundamental Research and Application of Physical Science Vol. 4

 The characteristic or total cross-sections are fundamental limits in physics to understand the matter structure. These limits provide appropriate information on the interplay process probability. They are secondhand in various application in the way that laser physics, healing radiation care and nuclear requests. In the case of atoms or complex molecules photoionization, the analytical judgment of cross section is dull and very complex because we should use poly-electronic wave function. In this case it is troublesome to solve the problem utilizing the Schrodinger's equation. In order to fool these difficulties, we apply mathematical approximations. This item provides a general study of the photoionization by seeing atom assign electromagnetic radiation accompanying photon energy nearly the upper ionization threshold and utilizing also individual active energized matter model. A general and particularized calculation of the differential representative sample as a function of photon polarization in uninterrupted case and the circular case has been acted. Moreover, we made case of an unpolarized wave and deducted the oval-shaped polarization component the keeping in mind that unpolarized light is principally composed by an elliptically reverse wave. Then, a study of the angular classification of the photoelectrons according to the β irregularity parameter was made. A particular use was made on hydrogenoid bit considered as of highest quality-electron method. From this study it appears in the vicinity of the above photoionization threshold, the characteristic cross section decreases accompanying the incident photon strength in the linear and circular polarization cases while it increases in the oval-shaped polarization case. So, In the undeviating polarization case, a suggestion of correction the circular and elliptical case, the maximum photoelectron signal (peak) is acquired witch the ejection photoelectron angle θ = 0 (forwards expulsion electron) or θ = π (backscattering).

Author(s) Details:

Issoufou Arzika Alio,
Climate, Environment and Materials Radiation Laboratory (LCEMR), Physics Department, Faculty of Sciences and Techniques, Abdou Moumouni University, Niamey, Niger.

Almoustapha Aboubacar,
Climate, Environment and Materials Radiation Laboratory (LCEMR), Physics Department, Faculty of Sciences and Techniques, Abdou Moumouni University, Niamey, Niger.

Please see the link here: https://stm.bookpi.org/FRAPS-V4/article/view/10590


Tuesday, 8 June 2021

Doubly-charged Negative Ion of C60 Molecule | Chapter 10 | Newest Updates in Physical Science Research Vol. 5

 An electronic structure of the doubly-charged negative ion is depicted in the Dirac- and Lorentz-bubble potential models C60 A variational method was used to investigate it. The overall energy of the system is negative even in the first approximation of this method when a trial wave function of the two electrons is represented as a product of one-electron functions, indicating the existence of a stable state of the doubly-charged negative ion in these models. According to estimates, C60 second electron affinity is around ε2 ≈ 1 eV. This ion's photodetachment cross sections σ(ω) have also been determined. Near the threshold σ(ω), strange and intriguing behaviour is observed. Near the process threshold, the first cross section accompanied by the transition of the doubly-charged negative ion into a singly-charged one is exponentially small. The photodetachment of a singly-charged ion is represented by the second cross section, which increases as a power function of the photoelectron's kinetic energy near the threshold. The photodetachment cross sections of atomic ions with the same electron affinity are of the same order as these cross sections.

Author (s) Details

A. S. Baltenkov
Arifov Institute of Ion-Plasma and Laser Technologies Tashkent, 100125, Uzbekistan.

A. Z. Msezane
Center for Theoretical Studies of Physical Systems, Clark Atlanta University, Atlanta, Georgia 30314, USA.

View Book :- https://stm.bookpi.org/NUPSR-V5/article/view/1405