PPT-Two beam power loss: how to compute it

F Giordano B Salvant N Biancacci L Teofili and C Zannini Many thanks to G Rumolo and the CST team Outline Background Two beam power loss computation with CST Filling scheme generator script introduction. Tatiana Rijoff, Frank Zimmermann . ColUSM. #19 - 01/03/2013. long-range beam-beam collisions . perturb motion at large betatron amplitudes. , where particles come close to opposing beam. cause . ‘diffusive aperture’. Yue Hao. Collider-Accelerator Department. Brookhaven National Laboratory. Jan 10, 2009 EIC Meeting at Stony Brook. Outline. Beam-beam effect on the Electron beam. Beam distribution disruption. Mismatch with the design lattice. M. . Fitterer. , R. De Maria,. S. . Fartoukh. ,. M. . Giovannozzi. Acknowledgments: G. . Arduini. , A. . Ballarino. , R. Bruce, J.-P. Burnet, E. McIntosh, F. . . Schmidt, H. . Thiesen. , E. . Todesco. Team Members: . . David Sierra . . Erwin . Holzhauser. . . Matt . Faller. Project Sponsors: . . Mangesh. . Nijasure. Todd Martin. Saad. . Arrabi. The need for tessellation:. The industry demands a higher graphical fidelity. Ziam Ghaznavi. CHE 384T Lithography. November 30. th. , 2017. 1. Outline/Agenda. Motivation. Ion – Solid Interactions. Overview of IBL Systems . Future Outlook. 2. Motivation. SEMATECH and the ITRS. Gianluca Valentino. University of Malta, . Msida. , Malta. Belen . Salvachua. CERN, Geneva, Switzerland. Thanks also to the LHC . collimation team for support in measurements and analysis. ICFA Mini-Workshop: Machine Learning Applications for Particle Accelerators. for circular accelerators. Rüdiger . Schmidt, CERN. U.S. Particle Accelerator School January . 2017. Programme for the school. What can go wrong?. What are the consequences?. Mitigation. Are the protection systems efficient and reliable?. Tuning the beam (from Andy’s slides). SLAC can provide (and you can control) . between single electrons – 200 electrons per bunch as its output. 5 bunches a second (5Hz). Beam size between 30 microns and 1cm. T. Southern, Oak Ridge National Lab. 02 October 2018 . CCL. SCL. . b. =. 0.61. SCL. . b. =0.81. DTL. RFQ. Source. MEBT. SNS Accelerator. 945 ns. Current. 1 ms macro-pulse. Linac. Target. Current. 1ms. M Väänänen. , B . Lindström. , D . Wollmann. , P. Belanger. CERN. Technical meeting – 25 April 2019. UFO observations in the LHC. LHC first proton accelerator to suffer from their impact. Still many unknowns, impact expected to increase in future (higher beam energy, higher beam intensity...). W. Farabolini . on behalf of all the CALIFES beam users. 01/121/2015. CLIC Project Meeting #23. 1. Studies repartition with CALIFES and TBM. Test Beam Module : 21 days W. Farabolini. Wake Field Monitors : 48 days R. Lillestol et al.. Bunch currentBeam energyRepetition frequency Number of bunches 4 per beamHorizontal emittanceVertical emittanceMax luminosity2 BEAM DIAGNOSTICSThe BEUV telescopes detect the synchrotron light emit-te Bunch currentBeam energyRepetition frequency Number of bunches 4 per beamHorizontal emittanceVertical emittanceMax luminosity2 BEAM DIAGNOSTICSThe BEUV telescopes detect the synchrotron light emit-te Chandra Bhat. Fermilab. Acknowledgements. W. . Pellico. , B. Chase, S. . Chaurize. , . C. . Drennan. , F. Garcia, B. . Hendrick. , . J. Nelson*, K. . . Seiya. , . T. . Sullivan, C. Y. Tan. , . K. Triplett, M.-J. Yang.