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000192510 0247_ $$2doi$$a10.18429/JACoW-IPAC2014-THPME116
000192510 0247_ $$2datacite_doi$$a10.3204/PUBDB-2014-04107
000192510 0247_ $$2openalex$$aopenalex:W2187319960
000192510 020__ $$a978-3-95450-132-8
000192510 037__ $$aPUBDB-2014-04107
000192510 041__ $$aEnglish
000192510 1001_ $$0P:(DE-H253)PIP1014786$$aMayet, Frank$$b0$$eCorresponding Author
000192510 1112_ $$0C14-06-16$$2inspire$$a5th International Particle Accelerator Conference$$cDresden$$d2014-06-15 - 2014-06-20$$gIPAC2014$$wGermany
000192510 245__ $$aStudies on a Diagnostic Pulse for FLASH
000192510 260__ $$aGeneva$$bJACoW, Geneva, Switzerland$$c2014
000192510 29510 $$aProceedings of the 5th Int. Particle Accelerator Conf., IPAC2014, Dresden, Germany
000192510 300__ $$a3
000192510 3367_ $$2ORCID$$aCONFERENCE_PAPER
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000192510 3367_ $$0PUB:(DE-HGF)8$$2PUB:(DE-HGF)$$aContribution to a conference proceedings$$bcontrib$$mcontrib$$s1646829778_5366
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000192510 520__ $$aThe long-term stability of the beam optics at FLASH is crucial for all connected experiments and the operation of the new second beamline FLASH2. It is therefore desirable to have a simple procedure to monitor the beam optics rou- tinely and at the same time minimally invasive. This way user operation is not disturbed. An automated procedure, which has been successfully employed at the SLAC linac is presented in the context of FLASH. The betatron oscilla- tions of selectively kicked pulses are recorded using BPMs at a fixed time interval. An online algorithm is then used to extract the betatron phase advance, as well as potential growth of the betatron oscillation amplitude and the Twiss parameters beta and alpha. Using this method, the long-term beam optics stability can be monitored in order to identify potential sources of drifts.
000192510 536__ $$0G:(DE-H253)POF2-XFEL-20130405$$aFacility (machine) XFEL (POF2-XFEL-20130405)$$cPOF2-XFEL-20130405$$x0
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000192510 650_7 $$2Other$$aAccelerator Physics
000192510 650_7 $$2Other$$a06 Instrumentation, Controls, Feedback & Operational Aspects
000192510 650_7 $$2Other$$aT03 Beam Diagnostics and Instrumentation
000192510 693__ $$0EXP:(DE-H253)FLASH(machine)-20150101$$1EXP:(DE-H253)FLASH-20150101$$5EXP:(DE-H253)FLASH(machine)-20150101$$aFLASH$$eFacility (machine) FLASH$$x0
000192510 693__ $$0EXP:(DE-H253)XFEL(machine)-20150101$$1EXP:(DE-H253)XFEL-20150101$$5EXP:(DE-H253)XFEL(machine)-20150101$$aXFEL$$eFacility (machine) XFEL$$x1
000192510 7001_ $$0P:(DE-H253)PIP1017739$$aAssmann, Ralph$$b1$$udesy
000192510 7001_ $$0P:(DE-H253)PIP1001613$$aSchreiber, Siegfried$$b2$$udesy
000192510 7001_ $$0P:(DE-H253)PIP1003368$$aVogt, Mathias$$b3$$udesy
000192510 773__ $$a10.18429/JACoW-IPAC2014-THPME116
000192510 7870_ $$0PUBDB-2017-144829$$aPetit-Jean-Genaz, Christine et.al.$$dGeneva : JACoW, 2014$$iIsParent$$tParticle accelerator
000192510 8564_ $$yRestricted
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000192510 9141_ $$y2014
000192510 9101_ $$0I:(DE-HGF)0$$6P:(DE-H253)PIP1014786$$aExternes Institut$$b0$$kExtern
000192510 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1017739$$aDeutsches Elektronen-Synchrotron$$b1$$kDESY
000192510 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1001613$$aDeutsches Elektronen-Synchrotron$$b2$$kDESY
000192510 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1003368$$aDeutsches Elektronen-Synchrotron$$b3$$kDESY
000192510 9131_ $$0G:(DE-HGF)POF2-54G17$$1G:(DE-HGF)POF2-540$$2G:(DE-HGF)POF2-500$$9G:(DE-H253)POF2-XFEL-20130405$$aDE-H253$$lForschung mit Photonen, Neutronen und Ionen (PNI)$$vDESY-participation in XFEL$$x0
000192510 9132_ $$0G:(DE-HGF)POF3-631$$1G:(DE-HGF)POF3-630$$2G:(DE-HGF)POF3-600$$aDE-HGF$$bForschungsbereich Materie$$lMaterie und Technologie$$vAccelerator R & D$$x0
000192510 9201_ $$0I:(DE-H253)MPY-20120731$$kMPY$$lBeschleunigerphysik$$x0
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