Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Springer eBooks

Probing The Collective and Independent-Particle Character of Atomic Electrons

R. Stephen Berry

Published Jan 1, 1995• 0 citations
Publisher
DOI
10.1007/978-94-011-0263-6_6

Related papers

From independent particle towards collective motion for two polarized electrons on a square lattice

Moises Martinez-Mares, J.‐L. Pichard

arXiv:cond-mat/0203579•The European Physical Journal B•Nov 1, 2002•3 citations

Collective oscillations of atomic electrons

B.Kh. Ishmukhametov, Yu. A. Babanov

Physics Letters A•Jul 1, 1967•4 citations

Atomic Electron Shells Formation Laws

Oleg G. Verin

The analysis based on experimental characteristics of atoms shows, that the theory of electron movement in atom in its modern state is essentially erroneous. It is impossible to consider electrons in atoms as separate particles because in each electron shell they form a Bose-condensate. Therefore real electron collectives absolutely not resemble drawn by the theory stochastic orbital spread in space. In the article physical characteristics data of atoms repeatedly confirmed by experiments are used. Therefore disclosed laws, undoubtedly, have objective character and will be a reliable basis for further researches.

•Aug 1, 2016•2 citations

Atomic- and electron-beam spectroscopy of rarefied semiquantum media

Eugene P. Bashkin, Sergey B. Stepaniants

The quantum-mechanical collective effects accompanying the propagation of a low-energy atomic or electron beam through a rarefied medium are discussed. An unusual dissipation mechanism due to the inelastic scattering of a test particle with thermal collective modes is considered. The phenomenon in question comes into effect even in a thin target at distances less than the mean free path calculated for direct atomic collisions. This effect provides the possibility to study the collective many-body properties of the medium by means of traditional atomic (electron) spectroscopy. The differential cross sections for the inelastic scattering of a probe particle with fluctuations of density, macroscopic magnetization, and entropy in the target are expressed in terms of the corresponding structure functions and calculated both in the hydrodynamic and collisionless regimes. The spin-flip transitions as well as the nonflip scattering are considered in detail. Possible applications of the theory to semiquantum systems such as gaseous H\ensuremath{\downarrow}, D\ensuremath{\downarrow}, and dilute $^{3}\mathrm{\ensuremath{-}}^{4}$He mixtures as well as some aspects of neutron optics and atomic (electron) spectroscopy are briefly discussed.

Physical review. B, Condensed matter•Feb 1, 1995•2 citations

Independent Operators for Interacting Electrons

Roger Haydock

Bulletin of the American Physical Society•Mar 7, 2018•0 citations

Collective Processes At Nonlinear Atom Ionization

Nikolai B. Delone

The experimental results on multicharged ion formation at nonlinear atom ionization are analyzed. A presence of data referring to a collective character of interaction of the atomic electrons with radiation field is clarified.

Proceedings of SPIE, the International Society for Optical Engineering/Proceedings of SPIE•Oct 21, 1986•0 citations
The analysis based on experimental characteristics of atoms shows, that the theory of electron movement in atom in its modern state is essentially erroneous. It is impossible to consider electrons in atoms as separate particles because in each electron shell they form a Bose-condensate. Therefore real electron collectives absolutely not resemble drawn by the theory stochastic orbital spread in space. In the article physical characteristics data of atoms repeatedly confirmed by experiments are used. Therefore disclosed laws, undoubtedly, have objective character and will be a reliable basis for further researches.
The quantum-mechanical collective effects accompanying the propagation of a low-energy atomic or electron beam through a rarefied medium are discussed. An unusual dissipation mechanism due to the inelastic scattering of a test particle with thermal collective modes is considered. The phenomenon in question comes into effect even in a thin target at distances less than the mean free path calculated for direct atomic collisions. This effect provides the possibility to study the collective many-body properties of the medium by means of traditional atomic (electron) spectroscopy. The differential cross sections for the inelastic scattering of a probe particle with fluctuations of density, macroscopic magnetization, and entropy in the target are expressed in terms of the corresponding structure functions and calculated both in the hydrodynamic and collisionless regimes. The spin-flip transitions as well as the nonflip scattering are considered in detail. Possible applications of the theory to semiquantum systems such as gaseous H\ensuremath{\downarrow}, D\ensuremath{\downarrow}, and dilute $^{3}\mathrm{\ensuremath{-}}^{4}$He mixtures as well as some aspects of neutron optics and atomic (electron) spectroscopy are briefly discussed.