1 / 44

Prajwal T. Mohan Murthy Laboratory for Nuclear Science , MIT ν DM Group

Spin-Light Polarimeter for the Electron Ion Collider. Prajwal T. Mohan Murthy Laboratory for Nuclear Science , MIT ν DM Group. EIC Users Meeting 2014 Jun 2014 Story Brook , NY. Outline (CHANGE). Synchrotron Radiation (SR) “Spin-Light” Wiggler Magnets Collimators Ionization Chambers

derica
Télécharger la présentation

Prajwal T. Mohan Murthy Laboratory for Nuclear Science , MIT ν DM Group

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. Spin-Light Polarimeter for theElectron Ion Collider Prajwal T. Mohan Murthy Laboratory for Nuclear Science, MITνDM Group EIC Users Meeting 2014 Jun 2014Story Brook, NY

  2. Outline (CHANGE) Synchrotron Radiation (SR) “Spin-Light” Wiggler Magnets Collimators Ionization Chambers Geant4 Simulations Topic by Topic Case Studies (Only a Few Presented) Summary

  3. Outline (CHANGE) • Quick parts, for details, please refer to: • arXiv:1401.6744 • arXiv:1309.6711 • arXiv:1309.2988 Synchrotron Radiation (SR) “Spin-Light” Wiggler Magnets Collimators Ionization Chambers Geant4 Simulations Topic by Topic Case Studies (Only a Few Presented) Possible Location at mEIC Summary

  4. Outline (CHANGE) • Quick parts, for details, please refer to: • arXiv:1401.6744 • arXiv:1309.6711 • arXiv:1309.2988 Latest Updates Synchrotron Radiation (SR) “Spin-Light” Wiggler Magnets Collimators Ionization Chambers Geant4 Simulations Topic by Topic Case Studies (Only a Few Presented) Possible Location at mEIC Summary

  5. Comparative Introduction

  6. What is Synchrotron Radiation? First seen in General Electric Lab, 1947 Angular Distribution

  7. So where is spin dependence? With QED Correctionsby A.A.Sokolov and I.M.Ternov (1960s) Spin dependent term Spin flip dependent term Verified at VEPP-4 storage ring in Novosibirsk Belomesthnykh et. al., NIM 227, 173 (1984)

  8. Longitudinal Spin Light

  9. What are Spin-Light Characteristics? Spin light characteristics A=

  10. Conceptual Design

  11. Won’t all the fans of SR merge? The SR fans may be selected out after each dipole and collimated before being fed into the DIC. Notice only 2 fans are required for polarimetry, 4 fans are for statistics.

  12. What are Spin-Light Characteristics? A differential ionization chamber can be used to measure the asymmetry. SR (+ SpinLight) • The ionization chamber can use Xenon • A split plane IC can pick out small up-down asymmetries in SR - influx. • At the IC, the collimated SR beam spots shall be about 1cm. • Notice: Figure on left is only one half of the actual IC. The middle plate is held at an intermediate potential.

  13. Detecting the Collimated SR A schematic for detection of SR (alternative arrangements are a possible)

  14. What will be the signal?

  15. Geant 4 Simulation

  16. Geant 4 Simulation Results Simulation reproduces photon spectrum and asymmetry Only a single DIC is being simulated along with collimators

  17. What about Background Simulations? Background events are mostly Bremsstrahlung events from the collimators

  18. SR Spots from GEANT4? Notice only 2 fans are required for polarimetry, 4 fans are for statistics. Note: The Geant4 simulation plots are all for just one split plane IC, on one side of beamline.

  19. How does this scale with EBeam and IBeam? Number Spectra

  20. How does this scale with EBeam and IBeam? Power Spectra

  21. How does this scale with Ebeamand Ibeam? Asymmetry • Power output remains to be a challenge for high energy EIC • Spin-Light Polarimeter is best suited for: • E(e) = [2,20]GeV • I(e) < 10mA

  22. Where could this be accommodated in mEIC? Ample real-estate near the 8 dipoles and the fact that the magnets are of 20mrad bend angle (twice as much as initial proposal design) allows for convenient sized collimators.

  23. Updated Geant4 Results Theory Plots: Updated Spectra and Corresponding Asymmetry

  24. Updated Characteristic Plots Theory Plots: Updated Spectra and Corresponding Asymmetry The spectra now is completely in the hard X-ray Spectrum

  25. Updated Geant4 Results Number Spectra for beam energy of 5GeV, magnet pole strength of 0.22T

  26. Updated Geant4 Results Power Spectra for beam energy of 5GeV, magnet pole strength of 0.22T

  27. Updated Geant4 Results Number Spectra for beam energy of 12GeV, magnet pole strength of 0.5T

  28. Updated Geant4 Results Power Spectra for beam energy of 12GeV, magnet pole strength of 0.5T

  29. Updated Geant4 Results But the Geant4 asymmetry for both the energy configurations (12GeV @ 0.5T and 5GeV @ 0.22T) match within about 5%

  30. Slit Width Effects For 5GeV @ 0.22T

  31. Slit Width Effects For 12GeV @ 0.5T: Completely resolved even if the e-beam is allowed a 4cm wide passage.

  32. Uncertainties Background and background asymmetry has to be measured with the wiggler on/off Simulation was used to estimate background

  33. 3 dipole magnet: .1m dipoles separated by 1m. DIC 10m away • Asymmetry in SR gives spin light component -> Polarization • A non invasive and continuous method • Possible location at mEICzeroed on SUMMARY Acknowledgements This work is supported by the U.S. Department of Energy under contract number DE-FG02-07ER41528 ‘10 – ’13 and MIT Frank Fellowship.

  34. Backup

  35. How does the dipole field look like? Magnet Face BEAM Edge fringe field Conceptual Design Central Uniform field Beam Pipe

  36. How does the dipole field look like? Magnet Face BEAM Central Uniform field Edge fringe field Simulated using LANL Poisson EM Code Beam Pipe

  37. Does the asymmetry in B field change anything? For each dipole Magnet: There is a reduction in both the total events and spin-light events (Plot: Events vs. E(MeV) of the light emitted)

  38. Does the asymmetry in B field change anything? For each dipole Magnet: Even though there was a decrease in SR and SpinLight events, the asymmetry remains the same.

  39. Does the Gaussian Beam profile change anything? Beam Pipe Point Beam SR Profile for Point Cross section of Beam The graph shows events as seen at the DIC For a point beam cross section, the SR profile is “box” like. 2inch

  40. Does the Gaussian Beam profile change anything? Finite Beam size Beam Pipe SR Profile for Gaussian Beam Profile The graph shows events as seen at the DIC For a Gaussian beam profile, the SR profile is “box” with smooth edges. Notice the asymmetry has not changed. 200μ Note: Has been scaled to make it visible 2inch

  41. Do the B field and dimensions affect? YES! B field was chosen to be 4T And the corresponding pole length of 10cm. This corresponds to a 10mrad angular beam bend.

  42. What are Spin-Light Characteristics? Beam Energy dependence

  43. How does this scale inclusion of Beam Halo? Asymmetry

  44. Collaboration

More Related