002290464 001__ 2290464
002290464 003__ SzGeCERN
002290464 005__ 20241025033822.0
002290464 0247_ $$2DOI$$9JACoW$$a10.18429/JACoW-IPAC2017-MOPAB108
002290464 0248_ $$aoai:inspirehep.net:1626382$$pcerncds:CERN:FULLTEXT$$pcerncds:FULLTEXT$$pcerncds:CERN$$qINSPIRE:HEP$$qForCDS
002290464 035__ $$9http://inspirehep.net/oai2d$$aoai:inspirehep.net:1626382$$d2017-10-24T11:07:03Z$$h2017-10-25T04:00:06Z$$mmarcxml
002290464 035__ $$9Inspire$$a1626382
002290464 041__ $$aeng
002290464 084__ $$2CERN Library$$aCLIC-Note-01114
002290464 088__ $$aCERN-ACC-2017-106
002290464 088__ $$aCLIC-Note-1114
002290464 100__ $$aÖgren, [email protected]$$uUppsala U. (main)
002290464 245__ $$9JACoW$$aBeam-Based Alignment Studies at CTF3 Using the Octupole Component of CLIC Accelerating Structures
002290464 260__ $$c2017
002290464 300__ $$a3 p
002290464 520__ $$9JACoW$$aThe Compact Linear Collider (CLIC) uses normal-conducting accelerating structures that are sensitive to wakefield effects and therefore their alignment is extremely important. Due to the four-fold symmetry of the structures, they allow for an octupole component of the rf fields. By scanning the beam transversely we can determine the center of the structures from the shifts in beam position due to the kicks from the octupole field. We present some initial results from measurements at the CLIC test facility 3 at CERN.
002290464 540__ $$9JACoW$$aCC-BY-3.0$$uhttp://creativecommons.org/licenses/by/3.0/
002290464 595__ $$aCLIC-Note
002290464 595__ $$aCLICARCHIVE
002290464 65017 $$2SzGeCERN$$aAccelerators and Storage Rings
002290464 6531_ $$2JACoW$$aoctupole
002290464 6531_ $$2JACoW$$awakefield
002290464 6531_ $$2JACoW$$aexperiment
002290464 6531_ $$2JACoW$$aalignment
002290464 6531_ $$2JACoW$$acollider
002290464 690C_ $$aCERN
002290464 693__ $$eCERN CTF3
002290464 700__ $$aBhattacharyya, [email protected]$$uUppsala U. (main)
002290464 700__ $$aFarabolini, [email protected]$$uIRFU, Saclay
002290464 700__ $$aHolz, [email protected]$$uUppsala U. (main)
002290464 700__ $$aRuber, [email protected]$$uUppsala U. (main)
002290464 700__ $$aZiemann, Volker$$iINSPIRE-00138549$$jJACoW-00001528$$kORCID:0000-0002-6229-5620$$uUppsala U. (main)
002290464 773__ $$cMOPAB108$$qIPAC2017$$wC17-05-14$$y2017
002290464 8564_ $$81362414$$s199548$$uhttp://cds.cern.ch/record/2290464/files/mopab108.pdf
002290464 8564_ $$81362414$$s1532494$$uhttp://cds.cern.ch/record/2290464/files/mopab108.pdf?subformat=pdfa$$xpdfa
002290464 960__ $$a13
002290464 962__ $$b2263434$$kMOPAB108$$ncopenhagen20170514
002290464 980__ $$aARTICLE
002290464 980__ $$aConferencePaper
002290464 980__ $$aCLICNOTE
002290464 999C6 $$a0-0-0-1-0-0-1$$t2017-09-28 23:43:33$$vcontent.pdf;1$$vInvenio/1.1.2.1260-aa76f refextract/1.5.44
002290464 999C5 $$hS. Stapnes (Ed.$$mThe CLIC Programme: Towards a Staged e+e- Linear Collider Exploring the Terascale Geneva$$o1$$rCERN-2012005$$y2012
002290464 999C5 $$hR. L. Lillestol, et al.$$min Proc. IPAC’16, pp.-2101$$o2$$y2099
002290464 999C5 $$hR. Ruber, et al.$$mThe CTF3 Two-beam Test Stand, Nucl. Inst. and Methods A 729 546$$o3$$y2013
002290464 999C5 $$hW. Farabolini and A. Grudiev$$mat the CLIC RF Development Meeting$$o4$$uhttp://indico.cern.ch/event/245687/$$y2013
002290464 999C5 $$hW. Farabolini et al.$$min Proc. IPAC’14, pp. 1880-1882$$o5
002290464 999C5 $$01382451$$hJ. Ögren, R. Ruber, V. Ziemann, W. Farabolini$$mMeasuring the full transverse beam matrix using a single octupole$$o6$$sPhys.Rev.ST Accel.Beams,18,072801$$y2015
002290464 999C5 $$hJ. Ögren and V. Ziemann$$min Proc. IPAC’16, pp. 280-282$$o7
002290464 999C5 $$9CURATOR$$hJ. Ögren and V. Ziemann$$mAligning the Compact Linear Collider accelerating structures using a co-propagating octupolar mode, in manuscript.$$o8$$y2017