Abstract

Measurement and correction of focusing errors is of great importance for performance and machine protection of circular accelerators. Furthermore LHC needs to provide equal luminosities to the experiments ATLAS and CMS. High demands are also set on the speed of the optics commissioning, as the foreseen operation with ${\ensuremath{\beta}}^{*}$-leveling on luminosity will require many operational optics. A fast measurement of the $\ensuremath{\beta}$-function around a storage ring is usually done by using the measured phase advance between three consecutive beam position monitors (BPMs). A recent extension of this established technique, called the N-BPM method, was successfully applied for optics measurements at CERN, ALBA, and ESRF. We present here an improved algorithm that uses analytical calculations for both random and systematic errors and takes into account the presence of quadrupole, sextupole, and BPM misalignments, in addition to quadrupolar field errors. This new scheme, called the analytical N-BPM method, is much faster, further improves the measurement accuracy, and is applicable to very pushed beam optics where the existing numerical N-BPM method tends to fail.

Highlights

  • In recent years the field of optics measurement and correction is growing in interest with the design of pushed optics like the high-luminosity LHC (HL-LHC) upgrade and generation light sources

  • III we incorporate these results in the development of a fully analytical N-beam position monitors (BPMs) method which does not require the splitting of the statistical phase uncertainties and the systematic errors

  • In the post-processing of the data taken during the LHC Machine Development measurement (MD) [13] for testing the Achromatic Telescopic Squeeze (ATS) principle with a βà 1⁄4 10 cm optics, the analytical N-BPM method was used for the first time with filtering of bad phase advances

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Summary

Franchi

ESRF, CS 40220, 38043 Grenoble CEDEX 9, France (Received 10 July 2017; published 10 November 2017). LHC needs to provide equal luminosities to the experiments ATLAS and CMS. High demands are set on the speed of the optics commissioning, as the foreseen operation with βÃ-leveling on luminosity will require many operational optics. We present here an improved algorithm that uses analytical calculations for both random and systematic errors and takes into account the presence of quadrupole, sextupole, and BPM misalignments, in addition to quadrupolar field errors. This new scheme, called the analytical N-BPM method, is much faster, further improves the measurement accuracy, and is applicable to very pushed beam optics where the existing numerical N-BPM method tends to fail

INTRODUCTION
Original N-BPM method
Extension of the N-BPM method
Effect of longitudinal quadrupole misalignments
Effect of BPM misalignments
HL-LHC
CONCLUSION
Error propagation
The generalized least-squares estimator
Full Text
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