Abstract

This paper presents measurements of the GeV-scale electron beam energy for the storage rings at the synchrotron light source facilities Australian Synchrotron (AS) and SPEAR3 at SLAC. Resonant spin depolarization was employed in the beam energy measurement, since it is presently the highest precision technique and an uncertainty of order ${10}^{\ensuremath{-}6}$ was achieved at SPEAR3 and AS. Using the resonant depolarization technique, the beam energy was measured at various rf frequencies to measure the linear momentum compaction factor. This measured linear momentum compaction factor was used to evaluate models of the beam trajectory through combined-function bending magnets. The main bending magnets of both lattices are rectangular, horizontally defocusing gradient bending magnets. Four modeling approaches are compared for the beam trajectory through the bending magnet: a circular trajectory, linear and nonlinear hyperbolic cosine trajectories, and numerical evaluation of the trajectory through the measured magnetic field map. Within the uncertainty of the measurement the momentum compaction factor is shown to agree with the numerical model of the trajectory within the bending magnet, and disagree with the hyperbolic cosine approximation.

Highlights

  • This paper presents measurements of the momentum compaction factor using resonant spin depolarization, to calibrate the model of horizontal defocusing rectangular gradient bending magnets

  • Within the uncertainty of the measurement the momentum compaction factor is shown to agree with the numerical model of the trajectory within the bending magnet, and disagree with the hyperbolic cosine approximation

  • Linear and numerical models of the trajectory are compared, as the linear method is commonly implemented in accelerator tracking codes, and elements commonly included in accelerator tracking codes can be used to yield the numerically evaluated trajectory

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Summary

INTRODUCTION

This paper presents measurements of the momentum compaction factor using resonant spin depolarization, to calibrate the model of horizontal defocusing rectangular gradient bending magnets. We present experimental results in the storage rings of light sources SPEAR3 [1] and the Australian Synchrotron (AS) [2], which are modern light sources of intermediate energy with rectangular defocusing gradient dipoles in the double-bend achromat lattices [3]. The technique is used because it is the highest precision energy measurement presently available, and the typical measurement accuracy is of order 10À5–10À6 This is one of very few methods for measurement of the momentum compaction factor, which can be calculated from measurements of the synchrotron frequency [9]. The electron trajectory through the gradient dipoles is modeled using trajectories that are circular, linear hyperbolic cosine, nonlinear hyperbolic cosine, or numerical integration of the measured magnetic field [21]

POLARIZATION THEORY
Radiative polarization
Resonant spin depolarization
Current fundamental and experimental uncertainties
Depolarizing effects
Lattice and beam parameters
Polarization time
GRADIENT BENDING MAGNET MODELING
Coordinates and parameters
Circular arc trajectory
Linear hyperbolic cosine trajectory
Nonlinear hyperbolic cosine trajectory
Numerically integrated trajectory using measured magnetic field data
Evaluation of modeling approaches
DISCUSSION
CONCLUSION
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