html5-img
1 / 23

Beam Halo Monitoring using Optical Diagnostics

Beam Halo Monitoring using Optical Diagnostics. Hao Zhang University of Maryland/University of Liverpool/Cockcroft Institute. Outline. Introduction Motivation to Study Beam Halo Method Adaptive Method Using Digital Micro-mirror Device Experiment

mercer
Télécharger la présentation

Beam Halo Monitoring using Optical Diagnostics

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript

  1. Beam Halo Monitoring using Optical Diagnostics Hao Zhang University of Maryland/University of Liverpool/Cockcroft Institute

  2. Outline • Introduction • Motivation to Study Beam Halo • Method • Adaptive Method Using Digital Micro-mirror Device • Experiment • University of Maryland Electron Ring (UMER) • JLAB FEL • Injection of SPEAR3 storage ring

  3. Motivation for Beam Halo Studies Halo can be regarded as small fraction of particles out a well defined beam core. • Beam Halo has many negative effects • Nuclear Activation of The Transport Channel • Emittance Growth • Emission of Secondary Electrons • Increasing Noise in The Detectors Halo Picture credit: Kishek, Stratakis

  4. Imaging Halos Problems: 1) Need High Dynamic Range ( DR >105 - 106) 2) Core Saturation with conventional CCD’s: blooming, possible damage 3) Diffraction and scattering associated with high core intensity contaminate halo 4) Adaptability when the beam core shape change. Solutions: 1) Passive spatial filtering, e.g. solar corography applied to beam imaging by T. Mitsuhashi of KEK DR = 106-107achieved 2) Spectra-Cam CID , DR ~ 106measured with laser by J. Egberts, C. Welsch, T. Lefevre and E. Bravin 3) Adaptive Mask based on Digital Micromirror Array; DR ~ 105 measured with laser and 8 bit CCD camera by Egberts, Welsch

  5. 120 Digital Micro-mirror arrayDevice* *DLPTM TexasInstruments Inc. Micro-mirror architecture: • Mirror size: 13.68 um x 13.68 um • Resolution: 1024 X 768 pixels 450

  6. Adaptive Method for Halo Measurement Source Source Mirror Mirror L1 L1 Computer Computer L2 L2 L3 L3 L4 L4 Halo Light Core Light Image 2 Camera Sensor Camera Sensor 32mm Mask Image 1 DMD DMD

  7. Quadrupole Screen UMER Experiment

  8. Testing filtering ability of DMD Beam on, DMD all on Beam on, DMD all off 32mm Average readout of the core region 49616 21

  9. Dynamic Range Test of DMD with intense beam and circular mask* 32mm Integration Frames: 20 275 1000 Integration Frames: 2000 3000

  10. Circular Mask Data line profile 32mm 1 0

  11. Demonstration of Adaptive Masking on UMER Quadrupole Current IQ 82.9%IQ 66.3%IQ 49.7%IQ 32mm (a) y x 70 45 45 60 (b) 280 640 660 250

  12. Halo Experiment with OSR in JLab FEL Bending Magnet Beam pipe

  13. Masking OSR Image of JLAB FEL Beam y 1 3 2 4 mm X 4 mm 1.2 s No mask Integration Time Mask Level 2.2 s 25000 35000 1.5 s 6 5 4 14 s 4 s 15000 80 s 2000 5000

  14. Measurement of Dynamic Range for OSR DMD System 100 Normalized Counts 10-2 10-4 10-6 pixel

  15. DMA/DMD Configuration M=0.14 M=4 M=1

  16. More Details… Mechanical Shutter (5ms) Filter wheel f=+125mm f=+100mm, 2” dia 1000x1000 DMD Scheinflug angle Diffraction pattern

  17. Data acquisition Injector Gate Injected beam READOUT BTS M3=1 f=+100mm PiMax 24° DMD Stored beam SPEAR3 f=+125mm Filter wheel M2=3.55 M = M1*M2*M3 = 0.4 Aperture & Cold finger OSR Source M1=0.138 9.6m 7.14m f=+2m

  18. PSF measurement of the stored beam • 2 ms shutter mode • Increase the mask size by changing the intensity threshold level • ND filter from ND =5 to ND = 0 No Mask 18 mm ND 3 ND 4 ND 5 Mask ND 0 ND 1 ND 2

  19. Injected 18 mm Stored beam beam Current /bunch 0.42 mA 1.52 mA 3.05 mA 6.11 mA Injected beam with presence of stored beam with different currents (a) (b)

  20. Three matching condition by altering the quads in the BTS

  21. Evolution of Beam centroid and beam size

  22. Conclusion • Applied a adaptive optics to detect small image signals from either beam halo or Injected beam compared with beam core or stored beam. • Achieve a high dynamic range with this method.

  23. Discussion • How can we apply this method to other existing machines? • What is the limitation of dynamic range? • For Proton machine, since the beam is destructive, are there any usable screens?

More Related