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Undulator-Based Positron Source: Optimizing the Photon Spectrum

Undulator-Based Positron Source: Optimizing the Photon Spectrum. Mike Jenkins and Ian Bailey. Positron Requirements of a New Collider. SLC. 6.0x10 12 e + /s. ILC. 3.9x10 14 e + /s. CLIC. 1.1x10 14 e + /s. LHeC. 4.0x10 16 e + /s. Undulator-Based Positron Source.

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Undulator-Based Positron Source: Optimizing the Photon Spectrum

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  1. Undulator-Based Positron Source: Optimizing the Photon Spectrum Mike Jenkins and Ian Bailey

  2. Positron Requirements of a New Collider SLC 6.0x1012 e+/s ILC 3.9x1014 e+/s CLIC 1.1x1014 e+/s LHeC 4.0x1016 e+/s

  3. Undulator-Based Positron Source

  4. Undulator-Based Positron Source Based on OPERA 3D model created by Jim Rochford Image of ILC Undulator Prototype at RAL

  5. Undulator-Based Positron Source

  6. Efficiency of Positron Production

  7. Efficiency of Positron Production

  8. Ideal Helical Undulator Spectrum

  9. Simulating Undulator Photon Spectra In order to test a non ideal helical undulator photon spectrum we need to be able to generate a photon spectrum from an arbitrary magnetic field map. HUSR developed at Cockcroft Institute by David Newton FluxCalc developed at Cockcroft Institute by Duncan Scott

  10. HUSR: Particle Tracking HUSR utilizes Lie maps in the tracking of particles through a magnetic field z(m) y(m) x(m)

  11. HUSR: Photon Spectra • HUSR calculates the synchrotron radiation produced from a particle track at a number of observation points • The electric field at each observation point is calculated using the retarded potential • This field is then Fourier transformed to give the frequency spectrum of the observed radiation

  12. Benchmarking HUSR

  13. Benchmarking HUSR

  14. Optimising the Photon Spectrum

  15. Optimising the Photon Spectrum

  16. Short Undulators • The possibility of using a number of short undulators has been investigated • Number of periods is 15 rather than 155 for ILC TDR Undulator module

  17. Short Undulators @ 150 GeV

  18. Short Undulators @ 250 GeV

  19. Summary • Undulator-based positron sources could provide the positron flux required by ILC and CLIC • Further optimisation of positron source is possible • Using new software tools we can now optimise the undulator • Possibility to design an undulator to provide the required light for an experiment

  20. Acknowledgements • David Newton – University of Liverpool and Cockcroft Institute • Duncan Scott – ASTeC and Cockcroft Institute • Sabine Riemann, Andreas Schaelicke and AndriyUshakov - PPS-Sim Group at DESY • Jim Clarke and the HeLiCal collaboration

  21. Thank You. Are there any questions?

  22. Additional Slides

  23. Photon Requirements LCLS CLIC LHeC ILC

  24. NbTi Helical Undulator * *Equation 1.9 From Klaus Flottmann’s Thesis Images of ILC Undulator Prototype at RAL

  25. Nb3Sn Helical Undulator Z Based on OPERA 3D model created by Jim Rochford

  26. ‘Realistic’ Undulator Photon Spectra Analytic Expression for Undulator Photon Spectrum*: *From Paper by B.M. Kincaid 1976, Eq 25

  27. Growing Period Undulators z(m) y(m) x(m)

  28. Off Axis Injection into Undulators y(m) y(m) x(m) x(m) z(m) z(m)

  29. Summary • Investigations into growing period undulators and effect of off axis electron trajectories is on going • Photon and positron polarisation studies have been carried out • Paper on undulator studies currently being written • Positron source thesis to be submitted in Feb 2013

  30. Thank You. Are there any questions?

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