Keyword: quadrupole
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MOP004 Design and Study of Cavity Quadrupole Moment and Energy Spread Monitor cavity, simulation, framework, linac 37
 
  • Q. Wang, Q.Y. Dong, L.T. Huang
    DICP, Dalian, Liaoning, People’s Republic of China
  • Q. Luo
    USTC/NSRL, Hefei, Anhui, People’s Republic of China
 
  A nondestructive method to measure beam energy spread using the quadrupole modes within a microwave cavity is proposed. Compared with a button beam position monitor (BBPM) or a stripline beam position monitor (SBPM), the cavity monitor is a narrow band pickup and therefore has better signal-to-noise ratio (SNR) and resolution. In this study, a rectangular cavity monitor is designed. TM220 mode operating at 4.76 GHz in the cavity reflects the quadrupole moment of the beam. The cavity plans to be installed behind a bending magnet in Dalian Coherent Light Source (DCLS), an extreme ultraviolet FEL facility. In this position, the beam has a larger dispersion, which is beneficial to measure the energy spread. A quadrupole magnet, a fluorescent screen, and a SBPM with eight electrodes is installed near the cavity for calibration and comparison. The systematic framework and simulation results are also discussed in this paper.  
poster icon Poster MOP004 [0.882 MB]  
DOI • reference for this paper ※ doi:10.18429/JACoW-IBIC2023-MOP004  
About • Received ※ 13 July 2023 — Revised ※ 08 September 2023 — Accepted ※ 13 September 2023 — Issue date ※ 28 September 2023
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MOP037 Tune Feedback at the Canadian Light Source feedback, injection, operation, storage-ring 106
 
  • W.A. Wurtz, C.K. Baribeau, A.M. Duffy
    CLS, Saskatoon, Saskatchewan, Canada
 
  In order to maintain good injection efficiency for top-up operation at the Canadian Light Source, we must keep the betatron tunes constant even as changes in insertion device fields cause the tunes to vary. To meet this requirement, we implemented a tune feedback system. We measure the tunes at a rate of 1 Hz using Dimtel bunch-by-bunch systems. The transverse feedback function of the bunch-by-bunch systems provides tune measurements without disturbing the electron beam. We adjust two quadrupole families at a rate of 0.25 Hz to control the horizontal and vertical tunes. In this article we describe the tune feedback system, its development and its performance. The system has proven to be very robust, enabling reliable top-up operation.  
poster icon Poster MOP037 [1.284 MB]  
DOI • reference for this paper ※ doi:10.18429/JACoW-IBIC2023-MOP037  
About • Received ※ 24 August 2023 — Revised ※ 07 September 2023 — Accepted ※ 14 September 2023 — Issue date ※ 21 September 2023
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MOP045 Robust Emittance Measurements emittance, focusing, solenoid, experiment 127
 
  • I. Pinayev
    BNL, Upton, New York, USA
 
  Funding: Work supported by Brookhaven Science Associates, LLC under Contract No. DE-SC0012704 with the U.S. Department of Energy
The quadrupole scan is commonly used for measurement of beam emittance. The found dependence of the beam size vs. quadrupole strength is fitted with parabola, which coefficients are used for emittance calculations. The measurement errors can cause substantial variations in the emittance value. Sometimes the fitted parabola has negative minimum value, making impossible emittance calculation. We propose more robust data processing using weighted fit for parabola or modifying the quadrupole scan procedure. The experimental results are presented.
 
poster icon Poster MOP045 [0.255 MB]  
DOI • reference for this paper ※ doi:10.18429/JACoW-IBIC2023-MOP045  
About • Received ※ 25 August 2023 — Revised ※ 11 September 2023 — Accepted ※ 13 September 2023 — Issue date ※ 28 September 2023
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MOP046 Measurement of Slice Emittance with Deflecting Cavity and Slit emittance, cavity, experiment, electron 129
 
  • I. Pinayev
    BNL, Upton, New York, USA
 
  Funding: Work supported by Brookhaven Science Associates, LLC under Contract No. DE-SC0012704 with the U.S. Department of Energy
Coherent Electron Cooling experiment carried out at RHIC requires small slice emittance of 15 MeV electron beam with high peak current. In this paper we describe the system for slice emittance measurement utilizing transverse deflecting cavity and slit. The image of the beam passing through the slit is used to measure slice intensity and angular divergence. Beam size at slit location is measured using scan of the beam across the slit with trim. The angular kick by the trim is taken into the account during calculations. Data processing and the experimental results are presented.
 
poster icon Poster MOP046 [0.997 MB]  
DOI • reference for this paper ※ doi:10.18429/JACoW-IBIC2023-MOP046  
About • Received ※ 28 August 2023 — Revised ※ 11 September 2023 — Accepted ※ 14 September 2023 — Issue date ※ 19 September 2023
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WEP007 Beam Profile Measurement using Helium Gas Light Emission and BEPM for Superheavy Element Search Experiment target, controls, experiment, optics 343
 
  • T. Watanabe, O. Kamigaito, T. Nishi, A. Uchiyama
    RIKEN Nishina Center, Wako, Japan
  • T. Adachi, B. Brionnet, K.M. Morimoto
    RIKEN, Saitama, Japan
  • A. Kamoshida
    National Instruments Japan Corporation, MInato-ku, Tokyo, Japan
  • K. Kaneko, R. Koyama
    SHI Accelerator Service Ltd., Tokyo, Japan
 
  The newly constructed superconducting linear accelerator (SRILAC) is now in operation with the aim of discovering new superheavy elements and advancing the production of medical radiation isotopes. Because it is crucial to extend the durability of the expensive Cm target for as long as possible, these experiments require the accelerated V beam to be sufficiently widened. To this end, a helium gas light emission monitor (HeLM) has been introduced to measure the beam profile. Because He gas flows within the target chamber, by capturing the light emitted from He gas with a CCD camera, the beam profile can be obtained nondestructively and continuously. These measurements are handled through programming in LabVIEW, with analyzed data integrated into an EPICS control system. A method to estimate the beam envelope has been recently developed by leveraging the measured quadrupole moments with beam energy position monitors (BEPMs), and incorporating calculations of the transfer matrix. The synergistic use of HeLM and BEPM plays a useful role in accurately controlling the beam size at the Cm target.  
poster icon Poster WEP007 [4.168 MB]  
DOI • reference for this paper ※ doi:10.18429/JACoW-IBIC2023-WEP007  
About • Received ※ 04 September 2023 — Revised ※ 09 September 2023 — Accepted ※ 13 September 2023 — Issue date ※ 22 September 2023
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WEP014 Measuring Electromagnet Polarity Using Magnetic Remanence power-supply, MMI, dipole, booster 354
 
  • K.P. Wootton
    ANL, Lemont, Illinois, USA
 
  Funding: This research used resources of the Advanced Photon Source, operated for the U.S. Department of Energy Office of Science by Argonne National Laboratory under Contract No. DE-AC02-06CH11357.
Large accelerator systems typically include many individually powered electromagnets. An important activity prior to commissioning with beam is verifying that the polarity of the installed magnets matches the design lattice. In the present work, we motivate the measurement of magnet polarity in a manner that is electrically safe, by measuring the magnetic remanence of iron yokes of normal conducting electromagnets. This has been used to confirm the polarities of iron-dominated dipole and quadrupole electromagnets at the Linac Extension Area at the Advanced Photon Source.
 
poster icon Poster WEP014 [0.504 MB]  
DOI • reference for this paper ※ doi:10.18429/JACoW-IBIC2023-WEP014  
About • Received ※ 24 July 2023 — Revised ※ 08 September 2023 — Accepted ※ 14 September 2023 — Issue date ※ 29 September 2023
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WEP036 Study of Non-destructive BPM-Based Energy Measurement of the Canadian Light Source Linac linac, electron, focusing, survey 438
 
  • H. Shaker, A. Bertwistle, E.J. Ericson, Y. Yousefi Sigari
    CLS, Saskatoon, Saskatchewan, Canada
  • E. Soltan, Y. Yousefi Sigari
    University of Saskatchewan, Saskatoon, Canada
 
  There is a plan in the Canadian Light Source (CLS) to replace the current Linac with a new one from Research Instruments GmbH in mid-2024. The first straight section of LTB (Linac-To-Booster) was upgraded to have two BPMs with a 4.79m drift between them, and two phosphor screens were replaced by YAG screens. A new BPM and a YAG-based screen station upgraded the following 90-degree achromat beamline. These upgrades help us to measure the current and future Linac beam parameters, including the beam twiss parameters, energy, and energy spread. In this paper, we discussed how we could use these three BPMs for non-destructive energy measurement, which will be a part of the active energy correction system.  
DOI • reference for this paper ※ doi:10.18429/JACoW-IBIC2023-WEP036  
About • Received ※ 29 August 2023 — Revised ※ 09 September 2023 — Accepted ※ 27 September 2023 — Issue date ※ 28 September 2023
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