002928181 001__ 2928181
002928181 003__ SzGeCERN
002928181 005__ 20250417230609.0
002928181 0247_ $$2DOI$$9CERN$$a10.23730/CYRSP-2024-003.323
002928181 0248_ $$aoai:cds.cern.ch:2928181$$pcerncds:FULLTEXT$$pcerncds:CERN:FULLTEXT$$pINIS$$pcerncds:CERN
002928181 035__ $$9https://inspirehep.net/api/oai2d$$aoai:inspirehep.net:2901991$$d2025-03-27T10:04:43Z$$h2025-03-28T05:00:12Z$$mmarcxml
002928181 035__ $$9Inspire$$a2901991
002928181 041__ $$aeng
002928181 100__ $$aCarmignani, Nicola$$uESRF, Grenoble
002928181 245__ $$9CERN$$aI.7 — Injection and extraction
002928181 260__ $$c2024
002928181 300__ $$a17 p
002928181 520__ $$9CERN$$aA particle accelerator has limited dynamic range, so a chain of accelerators is required to reach high energies. A combination of septa and kicker magnets is used to extract and inject beam from one ring to the next. Injections can be performed on-axis in a single turn or off-axis in many turns. Off-axis injections are very different in the heavy-particle accelerators and in the electron/positron rings, where there is synchrotron radiation damping. The extraction from a intermediate stage of the accelerator chain is usually done in a single turn, but multi-turn slow extractions can be required for different applications. Different injection and extraction methods are explained in this chapter.
002928181 540__ $$aCC-BY-4.0$$bCERN$$uhttps://creativecommons.org/licenses/by/4.0/
002928181 542__ $$dCERN$$g2024
002928181 65017 $$2SzGeCERN$$aAccelerators and Storage Rings
002928181 690C_ $$aARTICLE
002928181 690C_ $$aCERN
002928181 690C_ $$aYELLOWREPCONTRIB
002928181 700__ $$aPerron, Thomas$$uESRF, Grenoble
002928181 773__ $$02902634$$c323$$pCERN Yellow Rep. School Proc.$$v3$$wC24-11-27$$y2024
002928181 8564_ $$82722149$$s5314723$$uhttps://cds.cern.ch/record/2928181/files/document.pdf$$yFulltext
002928181 960__ $$a13
002928181 962__ $$b2927974$$k323$$ngeneva20241117
002928181 980__ $$aARTICLE
002928181 980__ $$aConferencePaper
002928181 980__ $$aBookChapter