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

Physics Letters A

Collision rates of optically oriented potassium atoms

P. Geittner

Published Dec 1, 1971• 2 citations
Publisher
DOI
10.1016/0375-9601(71)90698-0

Related papers

Collision ionization processes in the optical excitation of Rydberg states of potassium

Andrey N. Klyucharev, A. V. Lazarenko

OptSp•Feb 1, 1980•0 citations

Penning-Trap Technique for Studying Electron-Atom Collisions at Low Energy

Michael D. McGuire, E. Norval Fortson

In a new technique for studying electron collisions, the electrons are confined by electromagnetic fields and exposed to a known low density of atoms or molecules. Collisions rates are measured by electron diffusion in the trap. The use of spin-oriented atoms allows triplet and singlet contributions to be separated. Results of such studies are reported for room-temperature collisions of electrons with potassium atoms and with nitrogen molecules.

Physical Review Letters•Sep 23, 1974•11 citations

Collisional transfer of population and orientation in sodium potassium

Christopher M. Wolfe

•Jan 1, 2010•0 citations

Magnetic Resonance Frequency Shift of Na Atoms during Collisions in a Mixture of Potassium and Sodium Atoms

Victor A. Kartoshkin

Collisions between sodium and potassium atom in the conditions of optical orientation of potassium atoms are considered. Because of collisions, the spin exchange occurs between colliding atoms, which leads to a magnetic resonance frequency shift of Na atoms. Calculations reveal that the magnetic resonance frequency shift of Na atoms in the upper hyperfine state (F = 2) changes its sign from negative to positive upon an increase in the temperature in the absorption chamber from 300 to 500 K and passes through zero near temperature T ~ 450 K, while the frequency shift of the lower hyperfine state (F = 1) remains negative in the entire range of investigated temperatures. An analogous effect is observed for the first time in the case in which the main contribution to the magnetic resonance frequency shift comes from the spin exchange.

Technical Physics•Nov 1, 2021•3 citations

mJ Mixing in Oriented 4P122 Potassium Atoms, Induced by Collisions with Inert Gases

W. Berdowski, L. Krause

A modified Zeeman scanning method was used to excite selectively the magnetic substates of the $4^{2}P_{\frac{1}{2}}$ potassium atoms mixed with inert gases and placed in a strong magnetic field. The resulting potassium-inert-gas atomic collisions induced ${m}_{J}$ mixing in potassium, which manifested itself by the depolarization of the potassium resonance fluorescence. The polarization measurements yielded the following disorientation cross sections: K-He: 46 ${\mathrm{\AA{}}}^{2}$; K-Ne: 39 ${\mathrm{\AA{}}}^{2}$; K-A: 52 ${\mathrm{\AA{}}}^{2}$; K-Kr: 80 ${\mathrm{\AA{}}}^{2}$; K-Xe: 107 ${\mathrm{\AA{}}}^{2}$.

Physical Review•Jan 5, 1968•32 citations

Photoassociation of laser-cooled Potassium atoms

Eite Tiesinga, Paul S. Julienne, Xiaotian Wang +3 more

APS•May 1, 1998•0 citations
Collisions between sodium and potassium atom in the conditions of optical orientation of potassium atoms are considered. Because of collisions, the spin exchange occurs between colliding atoms, which leads to a magnetic resonance frequency shift of Na atoms. Calculations reveal that the magnetic resonance frequency shift of Na atoms in the upper hyperfine state (F = 2) changes its sign from negative to positive upon an increase in the temperature in the absorption chamber from 300 to 500 K and passes through zero near temperature T ~ 450 K, while the frequency shift of the lower hyperfine state (F = 1) remains negative in the entire range of investigated temperatures. An analogous effect is observed for the first time in the case in which the main contribution to the magnetic resonance frequency shift comes from the spin exchange.
A modified Zeeman scanning method was used to excite selectively the magnetic substates of the 42P124^{2}P_{\frac{1}{2}}42P21​​ potassium atoms mixed with inert gases and placed in a strong magnetic field. The resulting potassium-inert-gas atomic collisions induced mJ{m}_{J}mJ​ mixing in potassium, which manifested itself by the depolarization of the potassium resonance fluorescence. The polarization measurements yielded the following disorientation cross sections: K-He: 46 A˚2{\mathrm{\AA{}}}^{2}A˚2; K-Ne: 39 A˚2{\mathrm{\AA{}}}^{2}A˚2; K-A: 52 A˚2{\mathrm{\AA{}}}^{2}A˚2; K-Kr: 80 A˚2{\mathrm{\AA{}}}^{2}A˚2; K-Xe: 107 A˚2{\mathrm{\AA{}}}^{2}A˚2.