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50 ns Back-up Solution - Summary

50 ns Back-up Solution - Summary. V. Kain, B. Salvant , B. Goddard, W. Hofle , G. Iadarola , T. Pieloni , G. Arduini , M. Meddahi , G. Rumolo , J. Wenninger. Résumé of 25 ns possible issues. Machine protection due to increased energy density: probably solvable

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50 ns Back-up Solution - Summary

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  1. 50 ns Back-up Solution - Summary V. Kain, B. Salvant, B. Goddard, W. Hofle, G. Iadarola, T. Pieloni, G. Arduini, M. Meddahi, G. Rumolo, J. Wenninger

  2. Résumé of 25 ns possible issues • Machine protection due to increased energy density: probably solvable • Beam inducedheating: similar for 25 ns and 50 ns • UFOs: to be seen in LHC run 2 • Possible only real threat: e-cloud RLIUP workshop - Archamp

  3. The only real threat: E-Cloud • Significant increase of heat load (~ factor 4) in arcs during ramp • Coming only from e-cloud in the dipoles • Does not decrease over time at flattop (no scrubbing at flattop ?) • Underlying mechanism to be understood • Assuming 2012 scrubbing situation: • Limited to 50 % of nominal number of bunches for 25 ns spacing • Mitigation: • Remove e-cloud “completely”in dipoles: doublet beam scrubbing • To be tried in 2015 • HL era: Cryo cooling power upgrade? RLIUP workshop - Archamp

  4. 50 ns alternative RLIUP workshop - Archamp

  5. Integrated luminosity estimate - assumptions • Physics Efficiency = time in stable beams / total available time • Use 2012 physics efficiency: 0.37 • Pessimistic/realistic fill length distribution: exponential distribution • Average fill length ~ 6 h (2012) • Remark: uniform distribution: ~ 15 % more performance • Assume luminosity lifetime = 9 h (const.) • Simplistic assumption • 160 days of physics operation • Pile-up limit 140  50 ns leveled to half the 25 ns leveled luminosity Exponential fill length distribution 2012. J. Wenninger RLIUP workshop - Archamp

  6. Efficiency – 50 ns HL parameters 2012 efficiency For 50 ns crab cavities NOT big impact on performance (for small efficiencies). Efficiency is key. Target 25 ns meets target at ~ 47 % efficiency. 50 ns would need ~ 80 % !!! RLIUP workshop - Archamp

  7. Upgrades for 50 ns in injectors? Does anything else help? Status August 2013 • Sdf • Consider performance with post-LS2 50 ns parameters • Same assumptions as before for physics efficiency, average fill length • But assume 40 % emittance growth in LHC due to higher brightness Full HL-LHC 50 ns scenario & crab: yearly Lint≈ 123 fb-1 50 ns post-LS2 with planned injector upgrades & crab: ≈ 113 fb-1 Only 10 % difference  50 ns parameters after planned upgrades & crab cavities give (almost) as good results as proposed HL parameters… RLIUP workshop - Archamp

  8. Conclusion • 25 ns preferred but still to be proven in operation – still some unknowns • E-cloud could still be a show-stopper for this beam in the LHC. • 2015 will tell us • 50 ns could be an alternative – worked at 4 TeV to 1.8×1011 ppb…but… • Efficiency is key – to become comparable to 25 ns performance, an efficiency in the range of 70-80 % needed (which is totally unrealistic) • 50 ns means less integrated luminosity: ~ 60 % of 25 ns performance • No clear-cut additional upgrades identified for 50 ns • Efficiency and crab cavities in LHC more important than 'stretching’ injector performance • Beam stability with high bunch intensities might be an issue • Need to understand 2012 instability mechanism 2015 beam tests • Input for damping requirements or impedance reduction RLIUP workshop - Archamp

  9. RLIUP workshop - Archamp

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