000941324 001__ 941324
000941324 003__ SzGeCERN
000941324 005__ 20161219094318.0
000941324 0247_ $$2DOI$$a10.5170/CERN-2006-002.105
000941324 0248_ $$aoai:cds.cern.ch:941324$$pDOI$$pINIS$$pcerncds:CERN:FULLTEXT$$pcerncds:FULLTEXT$$pcerncds:CERN
000941324 041__ $$aeng
000941324 100__ $$aPichoff, N$$uCEA/DIF/DPTA/SP2A/LFPA, France
000941324 245__ $$aIntroduction to RF linear accelerators
000941324 250__ $$a2003 ed.
000941324 260__ $$c2006
000941324 260__ $$bCERN
000941324 520__ $$aAfter a short introduction to applications of RF linacs and their advantages and drawbacks as opposed to circular accelerators, the model of RF resonant cavities and their excitation by RF sources or beam is introduced. Then beam dynamics notions, essential to linacs, such as transit-time factor, synchronism, r.m.s. properties, matching and mismatching in linear or nonlinear forces, are presented.
000941324 65017 $$2SzGeCERN$$aAccelerators and Storage Rings
000941324 690C_ $$aARTICLE
000941324 690C_ $$aYELLOWREPCONTRIB
000941324 690C_ $$aCERN
000941324 8564_ $$uhttp://documents.cern.ch/cgi-bin/setlink?base=yellowarticle&categ=2006-002&id=p105$$yPublished version from CERN
000941324 8564_ $$uhttp://cds.cern.ch/record/941324/files/p105.pdf$$yPublished version from CERN
000941324 916__ $$sh$$w200615
000941324 960__ $$a13
000941324 961__ $$c20100203$$h0851$$lCER01$$x20060410
000941324 963__ $$aPUBLIC
000941324 962__ $$b603056$$k105-128$$nzeuthen20030915
000941324 970__ $$a002608519CER
000941324 980__ $$aARTICLE
000941324 980__ $$aConferencePaper