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@INPROCEEDINGS{Faatz:1018251,
author = {Faatz, Nicolas and Engels, Ralf W. and Wirtz, Jan and
Lehrach, Andreas and Kannis, Chrysovalantis and Zheng, Chuan
and Soltner, Helmut and Felden, Olaf and Grigoryev, Kirill
and Büscher, Markus and Faatz, Nicolas and Gebel, Ralf and
Pütz, Simon Jakob},
title = {{F}irst test of a polarized $^3${H}e$^+$ ion source},
school = {RWTH Aachen},
reportid = {FZJ-2023-04647},
year = {2023},
abstract = {The use of polarized $^3$He ions in storage rings opens a
new window to investigate nuclear forces, because the
spin-dependent part of the differential cross section of the
observed reactions must stem in first order from the neutron
spin. Thus, nuclear polarized $^3$He$^{2+}$ beams can be
regarded as an ideal substitute for polarized neutron beams.
Polarized $^3$He ions were used in the 1960’s, but either
the nuclear polarization and/or the usable intensity of the
corresponding ion sources was rather small. Since then,
several groups around the world have been working on the
realization of an efficient polarized $^3$He ion source for
injection into storage rings. Current concepts are based on
the rapid ionization of optically-pumped polarized $^3$He
gas with polarization values up to 0.8. Nevertheless, most
of the different ionization processes tested so far result
in large polarization losses.A new approach at the Institute
for Nuclear Physics in the Research Center Jülich promises
to overcome the recent limitations with an intense (>10 μA)
polarized $^3$He$^{1+}$ beam with a polarization up to P ~
0.9 that can be used for stripping injection to feed storage
rings. The method itself is similar to “optical
pumping”, but instead of laser beams single radio-wave
pulses are used to induce transitions within the hyperfine
substates in the Zeeman region of a $^3$He$^{1+}$ beam at 4
keV. The corresponding photons are coherent and
monochromatic, and the induced transitions at an energy
level of 10$^{−8}$ eV interfere with each other. Based on
this phenomenon, the three substates of the F = 1 state can
be pumped into a single substate with $m_F =$ +1 or -1. The
corresponding polarization will be measured after
acceleration to about 100 MeV due to the known analyzing
powers of elastic scattering on protons with an existing
polarimeter behind the cyclotron JULIC. In principle, this
technique can be expanded to other ions, even heavy ions,
and may open the door for a new generation of polarized ion
sources or polarized fuel, thus increasing the energy output
of future fusion reactors.},
month = {Sep},
date = {2023-09-24},
organization = {25th International Spin Symposium,
Durham (USA), 24 Sep 2023 - 29 Sep
2023},
subtyp = {After Call},
cin = {IKP-2 / IKP-4 / PGI-6 / ZEA-1 / IKP-TA},
cid = {I:(DE-Juel1)IKP-2-20111104 / I:(DE-Juel1)IKP-4-20111104 /
I:(DE-Juel1)PGI-6-20110106 / I:(DE-Juel1)ZEA-1-20090406 /
I:(DE-Juel1)VDB521},
pnm = {612 - Cosmic Matter in the Laboratory (POF4-612)},
pid = {G:(DE-HGF)POF4-612},
typ = {PUB:(DE-HGF)6},
doi = {10.34734/FZJ-2023-04647},
url = {https://juser.fz-juelich.de/record/1018251},
}