# Phase locking the spin precession in a storage ring

**Authors:** N. Hempelmann, V. Hejny, J. Pretz, E. Stephenson, W. Augustyniak, Z., Bagdasarian, M. Bai, L. Barion, M. Berz, S. Chekmenev, G. Ciullo, S. Dymov,, F.-J. Etzkorn, D. Eversmann, M. Gaisser, R. Gebel, K. Grigoryev, D. Grzonka,, G. Guidoboni, T. Hanraths, D. Heberling, J. Hetzel, F. Hinder, A. Kacharava,, V. Kamerdzhiev, I. Keshelashvili, I. Koop, A. Kulikov, A. Lehrach, P. Lenisa,, N. Lomidze, B. Lorentz, P. Maanen, G. Macharashvili, A. Magiera, D., Mchedlishvili, S. Mey, F. M\"uller, A. Nass, N.N. Nikolaev, A. Pesce, D., Prasuhn, F. Rathmann, M. Rosenthal, A. Saleev, V. Schmidt, Y. Semertzidis, V., Shmakova, A. Silenko, J. Slim, H. Soltner, A. Stahl, R. Stassen, H., Stockhorst, H. Str\"oher, M. Tabidze, G. Tagliente, R. Talman, P. Th\"orngren, Engblom, F. Trinkel, Yu. Uzikov, Yu. Valdau, E. Valetov, A. Vassiliev, C., Weidemann, A. Wro\'nska, P. W\"ustner, P. Zupra\'nski, M. \.Zurek

arXiv: 1703.07561 · 2017-07-12

## TL;DR

This paper demonstrates a feedback control method to precisely lock and manipulate the spin precession phase and rate in a storage ring, enabling advanced experiments like electric dipole moment searches.

## Contribution

It introduces a real-time feedback technique to control spin precession phase and rate in a storage ring using polarization measurements and RF solenoid synchronization.

## Key findings

- Achieved phase control within 0.21 radians.
- Demonstrated frequency adjustments as small as 3.7 mHz.
- Controlled spin precession to facilitate electric dipole moment experiments.

## Abstract

This letter reports the successful use of feedback from a spin polarization measurement to the revolution frequency of a 0.97 GeV/$c$ bunched and polarized deuteron beam in the Cooler Synchrotron (COSY) storage ring in order to control both the precession rate ($\approx 121$ kHz) and the phase of the horizontal polarization component. Real time synchronization with a radio frequency (rf) solenoid made possible the rotation of the polarization out of the horizontal plane, yielding a demonstration of the feedback method to manipulate the polarization. In particular, the rotation rate shows a sinusoidal function of the horizontal polarization phase (relative to the rf solenoid), which was controlled to within a one standard deviation range of $\sigma = 0.21$ rad. The minimum possible adjustment was 3.7 mHz out of a revolution frequency of 753 kHz, which changes the precession rate by 26 mrad/s. Such a capability meets a requirement for the use of storage rings to look for an intrinsic electric dipole moment of charged particles.

## Full text

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## Figures

5 figures with captions in the complete paper: https://tomesphere.com/paper/1703.07561/full.md

## References

10 references — full list in the complete paper: https://tomesphere.com/paper/1703.07561/full.md

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Source: https://tomesphere.com/paper/1703.07561