% IMPORTANT: The following is UTF-8 encoded. This means that in the presence
% of non-ASCII characters, it will not work with BibTeX 0.99 or older.
% Instead, you should use an up-to-date BibTeX implementation like “bibtex8” or
% “biber”.
@INPROCEEDINGS{Engels:1040662,
author = {Engels, Ralf and Büscher, Markus and Faatz, Nicolas and
Kannis, Chrysovalantis and Sefzick, Thomas and Soltner,
Helmut and Pütz, Simon},
title = {{N}ew {I}nsights into {S}ona {T}ransitions},
volume = {472},
publisher = {Sissa Medialab Trieste},
reportid = {FZJ-2025-01993},
pages = {005},
year = {2025},
abstract = {The Sona method, described in 1968 by Peter Sona, has been
used in polarized sources of the Lamb-shift type and is
still important at optically pumped ion sources, e.g. at
BNL. The trick of this method is that an electron
polarization of a hydrogen beam, e.g. produced by charge
exchange of a proton beam with optically pumped rubidium
atoms, can be transferred into nuclear polarization. For
this purpose, the electron-polarized hydrogen atoms have to
pass a zero-crossing of a longitudinal magnetic field that
acts as quantization axis. This non-adiabatic passage
exchanges the occupation numbers of the "pure" hyperfine
substates |1> and |3>, but keeps the “mixed” states |2>
and |4>. Thus, the atoms in a hydrogen beam in the states
|1> and |2>, both characterized by $m_J$=+1/2, will end up
in the states |2> and |3> that have both $m_I$=−1/2.Like
other groups operating such a Sona unit for metastable
hydrogen atoms, we observed strong oscillations of the
occupation numbers of the involved hyperfine substates.
These depend on several parameters like the magnetic field
shape and amplitude of the Sona unit or the velocity of the
hydrogen beam. In this proceeding we discussed the
theoretical explanation of this effect and possible
application for future polarized sources.},
month = {Sep},
date = {2024-09-22},
organization = {20th International Workshop on
Polarized Source, Targets, and
Polarimetry, Jefferson Lab (Newport
News), 22 Sep 2024 - 27 Sep 2024},
cin = {IKP-2 / PGI-6 / ITE},
cid = {I:(DE-Juel1)IKP-2-20111104 / I:(DE-Juel1)PGI-6-20110106 /
I:(DE-Juel1)ITE-20250108},
pnm = {612 - Cosmic Matter in the Laboratory (POF4-612) / DFG
project G:(GEPRIS)533904660 - Eine vielseitige
Polarisationsmethode für Teilchen mit einfachen
Hyperfeinstrukturen (533904660)},
pid = {G:(DE-HGF)POF4-612 / G:(GEPRIS)533904660},
typ = {PUB:(DE-HGF)8},
doi = {10.22323/1.472.0005},
url = {https://juser.fz-juelich.de/record/1040662},
}