Error Determination in Sextupole Magnet Calibration and Alignment Measurements and Application to Horizontal Beam Size Calculations at the Cornell Electron-positron Storage Ring
We report on measurements and modeling studies performed from 2021 to 2024 on the 76 sextupole magnets in the Cornell Electron-positron Storage Ring CESR. Beam-based, magnet-specific calibrations ($K_2$ value versus excitation current) were measured. It was found that the new calibrations differ fro...
Gespeichert in:
Hauptverfasser: | , , |
---|---|
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext bestellen |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
Zusammenfassung: | We report on measurements and modeling studies performed from 2021 to 2024 on
the 76 sextupole magnets in the Cornell Electron-positron Storage Ring CESR.
Beam-based, magnet-specific calibrations ($K_2$ value versus excitation
current) were measured. It was found that the new calibrations differ from
those previously in use by an average of 3.1% with an RMS spread of 12%. The
uncertainties in the calibration correction factors average 1.7% with an RMS
spread of 1.0%.
Sextupole alignment values relative to the reference orbit were measured by
combining the measured beam position with the quadrupole and skew quadrupole
terms caused by a sextupole strength change $\Delta K_2$. High accuracy was
achieved by fitting to difference phase and coupling functions as $K_2$ was
varied. The horizontal (vertical) average offset values were found to be -0.01
(0.03)~mm with RMS spread of 1.1 (0.9)~mm with some exceptionally large values
of a few millimeters. Typical uncertainties are 0.01-0.02~mm.
The above measurements were motivated by the precision required in measuring
horizontal beam size at each sextupole. A precision of 10\% for a \mbox{1-mm}
beam size requires uncertainties of better than 0.1~$\mu$radian in the
horizontal angle change produced in the sextupole for a typical strength change
of \mbox{$\Delta K_2 \, L$ = 1 m$^{-2}$}, where $L$ is the length of the
sextupole, as well as 10\% in the difference of the squared horizontal and
vertical beam positions relative to the center of the sextupole. These
precision values were achieved by the analysis of difference functions.
However, a small source of horizontal angle change of unknown origin,
independent of the sextupole strength, requires a sextupole strength range
larger than now available to measure accurately the typical horizontal beam
size at CESR. |
---|---|
DOI: | 10.48550/arxiv.2409.19728 |