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Simulations for LEP3/TLEP Marco Zanetti (MIT) 1 Introduction - PowerPoint PPT Presentation

Simulations for LEP3/TLEP Marco Zanetti (MIT) 1 Introduction Beams are squeezed at the IP to push for high luminosity. Similar to ILC but in this case beams cannot be disrupted after the collision. Beamstrahlung effects must be mild


  1. Simulations for LEP3/TLEP Marco Zanetti (MIT) 1

  2. Introduction • Beams are squeezed at the IP to push for high luminosity. • Similar to ILC but in this case beams cannot be disrupted after the collision. • Beamstrahlung effects must be mild enough to allow a reasonable lifetime – At least larger than burn-out lifetime • Additional key ingredient is the enhanced momentum acceptance – we aim at 4% (by increasing RF voltage) • LEP3/TLEP parameters already chosen accordingly to analytical formulation and full beam-beam simulation – V. Telnov, http://arxiv.org/abs/1203.6563, based on analytic formulation of the problem – MZ at 1 st LEP3 workshop, http://tinyurl.com/8lzdad2 2

  3. Simulation – Analytic form • Analytic functional form (red in the plot): • Constants not checked yet 3

  4. Outlook • BS lifetime results (TLEP) • Luminosity profile • Power dissipation • Multi-turn simulation 4

  5. Energy spectrum • Single crossing guinea-pig based simulation – Simulate 360M macroparticles around the working point • Lifetime features exponential dependency on energy acceptance TLEP-T TLEP-H Lifetime>4h h =3% • As for LEP3, TLEP BS lifetime well above required threshold • In particular some margin (x2 ?) is there for TLEP-H 5

  6. Luminosity profile • Look at the how much luminosity is delivered within 1% of nominal √s (L 0.01 ) – Key quantities for Physics – ISR not included, single crossing simulation • Beamstrahlung effects much smaller than at ILC • Almost monochromatic luminosity profile – Very similar performances for all circular collider options • To be confirmed by multi-turn simulation 6

  7. Power dissipation • The photon flux could be problematic for machine and detector instrumentation • Run the simulation to estimate the photon rate and energy • Use that to compute how much power is dissipated as a function of the polar angle LEP3 7

  8. Power dissipation • Similar dissipation for LEP3 and TLEP (O(10) kW integrated) • Should be manageable, most of the power dissipated at very small angle – No harm to experiments – Beam pipe needs protection – Flux on quadrupoles rather limited TLEP 8

  9. Multi-turn simulation • Goal is to check the beam parameters at equilibrium – Assume TLEP-H parameters • Integrate beam-beam simulation with simple longitudinal and transverse dynamics • Transverse motion: – Qx,Qy>0.5 • Synchrotron motion: • Radiation damping: 9

  10. H plane: effect of collision • A correlation is introduced – Linear in the bulk, non-linear in the tails • Correct it by means of a rotation matrix (quad): – a determined empirically from the fit of the bulk 10

  11. H plane: effect of correlation Colliding once and then transporting the beams around w/o further collision (divergent otherwise) 11

  12. H plane: compensating correlation • Collide only once, then transport • Correct right after the collision • Rotation of the tails not fully corrected 12

  13. H plane: full simulation • Collide at every turn in 1 IP • Still some beating 13

  14. V plan: full simulation • Small correlation also here • No compensation applied, still beam is not diverging 14

  15. Z plane: full simulation • Strong damping • Not totally clear to me.. 15

  16. Summary • Analytic computation verified by simulation – Very short lifetime for original beam parameters – Negligible effect on energy spread – Number of gammas <1 (0.6) • First implementation of multi-pass simulation is encouraging – Need to cope with large a in the H plane • Long to do list: – Understand/debug features – Compute relevant quantities at equilibrium – Implement 4 IPs – .. 16

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