CTF3 2014 Operations & Plans Piotr Skowroński for the CLIC Collaboration 27 January 2015 CLIC Workshop 2015 1.

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Presentation transcript:

CTF Operations & Plans Piotr Skowroński for the CLIC Collaboration 27 January 2015 CLIC Workshop

CTF3 experimental program January 2015 CLIC Workshop Phase feed-forward & stability studies Beam Loading / BDR experiment Two-Beam ModuleTBL DeceleratorDiagnostic Tests Commissioning Beam tests (X-box n.a.) TBTS program completion Deceleration to 40% & RF shaping Testing of EO bunch profile monitor, DB BPM, MB BPM 2 3Shut-downRF ConditioningInstallation TBM Installation of new tank Installation 4Commissioning & tests1st runCommissioningDeceleration to 50%tests cont'd + OTR Shut-down + restart 2 Combined beams, femto-second timing 2nd run (shared with normal operation) Complete commissioning & 1st run RF conditioning & testing with drive beam Available beam time Shut-down + restartModule upgrade?Shut-down + restart 2 Transverse feed- forward 3rd run (shared with normal operation) 2nd run RF conditioning & testing with drive beam Available beam time 3 4

2014 Running 1.76 M pules  587h weeks days 3 Dog-leg beam excluded!

2014 Running The plotted data are the CTF3 monitor records of mean values Caveats: there are many reasons data is missing  Blocked control system communication (very often this year, up to 20%)  Short pulses outside the window where the mean is calculated  CTF3 monitor not running or hanging 1.76 M pules  587h of beam  Dog-leg excluded 4

2014 Running With Dog-Leg  1.31 M Dog-Leg pulses  436 hours of beam time 27 January 2015 CLIC Workshop CLEX Beam Efficiency  days * 8 h/day = 1048h  587 h of beam / 1048 h = 0.56 Adding 20% margin: ~75% efficiency  For blocked CO communication, etc. Dog-Leg Beam Efficiency  30d*24h/d + 13d*8h/d = 824h  436h of beam / 1048 h = 0.53

2014 Running One the biggest issues are the klystron trips and the 2-3 minutes recovery that it takes for the pulse compressors to stabilize 7 February 2014 CLIC Workshop

2014 Running One the biggest issues are the klystron trips and the 2-3 minutes recovery that it takes for the pulse compressors to stabilize  Distribution of the time between pulses (CLEX beam only) 7 February 2014 CLIC Workshop e M pules

2014 Running 1.45 M pules one after another 1900 klystron trips  Pause between pulses in range of 111s - 270s  Avg. recovery time ~130s  Total: 130s*1900 = 68h 155 stops from 4.5 to 60 minutes  Includes all operator trips: discussions, meetings, coffees, cigarettes, lunches and other “I have to leave for 5 minutes”  Avg. recovery time ~600s  Total: 600s*155=26h 7 February 2014 CLIC Workshop operator trips and other technical issues klystron trips 1.45e6

1.5 GHz beam setup Setup directly 1.5 GHz beam with switches The setup strategy during previous runs  Start with 3GHz beam, setup factor 4 Easy beam, comfortable for initial measurements  Setup 1.5 GHz, readjust the linac  Add the phase switches However, it is not transparent as we expected  There is above 140 ns transient  Adjusting TWT and pre-buncher phases lets to recover the condition  However, the beam is different  We were ending up with 3 different setups 27 January 2015 CLIC Workshop FWHM 1.5% FWHM 1.75%

3 GHz Beam setup 3 GHz beam is still needed  Orbit setup, optics measurements, some experiments (PFF)  Some BPI’s badly read 1.5 GHz beam Still a puzzle why (I will come back to it)  3 GHz beam is much easier to handle: more stable and smaller Smaller dp/p  Smaller beam size in dispersive regions  Smaller non-linearities and emittance growth  For experiments where moderate power is sufficient Having 1.5 GHz going, the 3 GHz one is immediate to setup  Disable TWTs  Adjust phase of klystron 02 Defines bunching phase -> adjust to the LINAC bucket  Adjust the gun current 27 January 2015 CLIC Workshop

BPI response to 1.5 & 3 GHz beam 2D scans (h/v) with a corrector magnet example: CC.BPI0665 Solid 3GHz Dashed 1.5GHz All should be like this 27 January 2015 CLIC Workshop

Timeline Very short winter break No shutdown, restarted the beam in January (Jan 30) Initial problems with the gun  Very slow “heating” process, up to 4 hours Problems with timing, controls (large “LS1 upgrade”), cooling stations Vacuum problems in Linac girder 15 after a power cut  Took more than a week Problem with MKS14 CLIC Workshop February 2014 CLIC Workshop

Timeline 27 January 2015 CLIC Workshop Janfirst beam from the gun CLIC Workshop Febfirst beam in the injector Injector setup 3rd TWT (the brand new one) added 17 Febfirst beam in spectrometer 10 (3 GHz) Linac rematch 18 Febfirst 3 GHz beam in CR, first 1.5 GHz beam in linac 19 Febfirst CALIFES beam 20 Febfirst 1.5 GHz beam to CR Optimization of dp/p in CTS, Transverse rematch after the Stretcher 24 Febfirst combination 4 beam (1.5 GHz with phase switches) 26 Feb14 A (factor 4) extracted from CR 27 Febfirst drive beam in CLEX (uncombined) 4 Marfirst beam (3 GHz) to – and through – DL 5 Mar full combination factor 2 in DL (7 A) Dispersion, closure, emittance, ring length optimizations 13 Marbeam (uncombined) end of TBL / 3 GHz factor 4 optimized, 16 A

Timeline 27 January 2015 CLIC Workshop Marfirst drive beam to TBTS for Uppsala beam tests (factors 1 to 4) 20 Marconditioning of the new TBL tank 21 Marfirst factor 8 recombination ~ 20 A 25 Margood factor 8, ~ 25 A ~1% stability CALIFES, start of EOS tests 1 Aprstart of BLM tests in CALIFES 9 Aprtransport to TBTS, > 20 A Tuning of Factor 8: closure, dispersion emittance 25 Aprlossless factor 8, 28 A ~ 0.7% stability after CR, 28 A end of TL2, 25A in CLEX 28 Marstreak camera measurements of CALIFES beam for EOS crosscheck 29 Apr 26 A in CLEX, measured emittance 550/ Aprleak in TBL, RF load, new one outgassing for very long time (weeks) 7 May23 A end of TBTS 8 May24 A end of TBTS Tuning of Factor 8: closure of Twiss parameters, 2 nd order corrections 13 MayEOS experiment on the CALIFES beam 20 MayTBL conditioning after the vacuum issue

Timeline 27 January 2015 CLIC Workshop JunMKS15 died, one week reparation 15 JunWake Field Monitor Tests on CALIFES 17 Jun PFF the first tests of a complete system slow phase correction tests (Phase Feed-Back) 20 JunShutdown Jun-SepTBM installation Alignment

Timeline 27 January 2015 CLIC Workshop AugDog-Leg run start 30 SepFirst DB of run 2 Until Oct 16running DB Mon-Wedn, Dog-Leg Thu-Sun 7 OctLinac rematch 16 OctDispersion Tuning in CT 17 OctPower Cut causing many problems MKS14 Many power converters Coil Temperature probes on CR bends to be changed 21 OctRecovered the power cut Octdp/p optimization in CTS (RF phase tuning) 22 OctDispersion Tuning in CT 29 OctBeam through DL 30 OctIncrease the gun current and lower the beam energy 31 Oct-10 Nov Re-tuning optics, dispersion, dp/p 10 NovFirst beam in CALIFES, probe beam goes through TBM 11 NovFirst beam in the Combiner Ring 12 NovStraight beam through TBL 13 NovFirst beam through DL 14 NovCT quad scans and re-matching 19 NovFirst drive beam through TBM (uncobined)

Timeline 27 January 2015 CLIC Workshop NovDL recombination 19 NovDB in TBM, some acceleration seen on the probe Record beam charge in CALIFES 1.4 nC for single bunch 21 NovStart of PFF beam 25 NovPFF beam through, start of PFF commissioning 26 NovVarying TL1 R56, very easy (surprise) 1 DecBack to recombination factor DecCombiner Ring closure, 28 NovCALIFES beam for OTRI commissioned DecOTRI tests 3 DecFactor 8 combination re-established 4-5 DecPFF 8 DecFactor 2 Circulating in CR, ring length measurements 9 DecRecombination 8, Straight beam to TBM 9 DecProblem with TBM phasing confirmed DecPFF 11 DecStart of WFM commissioning in TBM 12 DecHalf a day for TBM 17 DecBeam based alignment checks in TBM and CALIFES 18 DecShutdown

1.5 GHz sources End of 2013 got brand new amplifier from PIT-RADWAR (former Bumar Electronika) that works flawlessly (almost)  Next one is expected to arrive in 2 week This gave us finally 3 TWTs + 1 spare However  One of TMD’s broke again  Another one started dropping in power, which made factor 8 operation difficult again 27 January 2015 CLIC Workshop PIT-RADWAR TMD

Drive Beam Generation Factor 8 Finally reached lossless full recombination  0.4 – 0.5 A in satellites  Still need some improvement Emittance:  H = 350 µm  V = 120 µm, target < 150 µm Stability: 1%, target < 0.1% 27 January 2015 CLIC Workshop Pulse recombination in Combiner Ring

Combined beam transport -28 A at the CLEX wall- 25 A in CLEX -Issue with BPMs calibration 27 January 2015 CLIC Workshop

Reproducibility We were able to maintain the current, I think, quite well taking into account a TWT that was continuously dropping in power  Although other parameters were forfeited  Naturally, continuous readjustments took quite a lot of beam time from the experiments and fine tuning procedures 27 January 2015 CLIC Workshop

Charge stability at end of the LINAC better than CLIC requirements to S [m] Drive Beam stability Charge stability – Factor 4 (2013) 27 January 2015 CLIC Workshop

Drive Beam stability 27 January 2015 CLIC Workshop Charge stability – Factor 8 (on a good day)

Drive Beam stability 27 January 2015 CLIC Workshop Charge stability – Factor 8 (a usual day)

Beam control Orbit Fully automatic tools for steering and orbit closure of the combined beams (see Devide talk after the following one)  Automatic response matrix learning, including “correct and learn” mode The improvement is huge, both in resulting quality and correction speed However, even this did not help to get orbit of a required quality  Large feed-down effects leading to large spurious dispersion and big difficulties in chromatic corrections 27 January 2015 CLIC Workshop CR Horizontal DL Vertical

Alignment Complete alignment campaign started during summer stop  Started with measurements  Only few magnets could have been realigned right away Availability of surveyors during LS1 combined with finite length of shutdown  It is being completed during this shutdown  Measured BPM offsets set in the control system 27 January 2015 CLIC Workshop CR: orbit kicks due to misalignments SpringAutumn

Alignment Beam chamber alignment  Up to +/- 1cm on a 4 cm chamber  There is no proper alignment system provisioned  Tremendous help from surveyors who did ad-hoc measurements such that OP team could correct the misalignments  Several locations still to be fixed Alignment is also an issue for the probe beam 27 January 2015 CLIC Workshop

Beam control Dispersion Large progress in dispersion control  Fully automatic tool for fast and precise dispersion measurements by Davide (*)  A key instrument for quick dispersion corrections It enabled Dispersion Free and Dispersion Target Steering  Fully automatic tool (prepared also by Davide (*)) Satisfactory control of horizontal dispersion  Despite of the large misalignments present 27 January 2015 CLIC Workshop (*) see the one after following talk by Davide

Beam control Dispersion This year we discovered problem with vertical dispersion in TL1  Dispersion Free Steering did not manage to take it out Not enough correctors  Alignment in the suspicious region is being checked  It seems that it plays important role in issues with TL2 transport Only a small change in vertical orbit leads to losses, while the vertical should be “easy” 27 January 2015 CLIC Workshop

Beam control Model Improved model of TL2  Much easier setup of beams this Plus magnets and chamber alignment helped Still, can be much improved There is a large error in TL2’, both TBTS and TBL lines affected  Optics Measurements using phase space painting were planned, but finally did not find any time slot for this 27 January 2015 CLIC Workshop TL2 model vs measured Response Matrix

Beam control Non-linearities Delay Loop and TL2 dog-leg optics shows large emittance growth due to induced higher order dispersion  Need of sextupole corrections Tricky, see next slide  Need for a smoother optics in DL and TL2 And always isochronous and achromatic Not straight forward to get, needs some deeper study  And not sure that it can be found See Davide’s presentation today & LCWS’15 presentation: contribution/111/material/slides/0.pdf 27 January 2015 CLIC Workshop

Sextupolar corrections Tried to correct the 2 nd and 3 rd order dispersion in the Delay Loop It helped to reduce the emittance On the other hand, it spoiled the combined beam transport  Not being able to recover recombination in time, correction was dropped 27 January 2015 CLIC Workshop Bypassing DL DL beam with correction DL beam without correction

Beam control Beam phase propagation The drive beam phase measured in CLEX was never good  However, the measurement with IQ demodulators of the RF produced in PETS was never fully trusted In August the 12 GHz PFF monitor was installed, and it agrees well with the PETS measurements The wiggling of the phase was traced to the imperfect gun pulse flattening Wave Form Generator  There is a static wiggle from the gun pulser  It is corrected by WFG  10MHz only, the correction is imperfect  Not synchronized with CTF clock  changes pulse to pulse  New 120MHz WFG acquired 27 January 2015 CLIC Workshop

Beam control Beam phase propagation During the Feed-Forward tests it was found that the phase jitter increases more than twice between CT and CLEX  The part related to energy was removed by tuning R 56 of TL1  Correlation ~50%  additional source of phase jitter  The gun current ripple strongly reflected on the phase Launch of dedicated study  Correlation plots with beam current, position and RF signals Modified read-out of the phase monitor in the combiner ring  Its measurements were useless because the signal level was too small It was setup to measure the fully recombined beam of 30 A 27 January 2015 CLIC Workshop

Controls During LS1 the Control System infrastructure was upgraded CTF3 served as the guinea-pig – it was the only operating acc. Renovated the crates for RF that made operation much easier  Modulators control  Amplitude and phase measurements  Wave-form generators and their read-back The new driver had a bug which triggered additional klystrons trips  Took a month until realized the reason for this large increase  And another month to fix it Reloading waveform during beam pulse  no waveform  no pulse compression  produced RF in phase with the beam Troubles with Xeneric Sampler driver (BPMs and RF measurements) after upgrade to FESA 3  Server dying very often, for some crates every 2-3 hours  Should be fixed after the shutdown 27 January 2015 CLIC Workshop

Disturbing AD cycle Certain RF signals showed regular oscillation It was traced to the anti-proton decelerator cycle  It creates fluctuations on 230V line, which influences, e.g. TWTs Fortunately, the net effect on the beam was not big Stabilization 230V is being installed for the most important devices 27 January 2015 CLIC Workshop

Conclusions Very good Run1, at least its first part Good Run 2 Big improvement in control of dispersion and orbit Stability – large improvement, still a lot of space for more  And it is a must if we want to complete all the challenging program Reproducibility – improving every year, but we have to do better  More discipline in sticking to the reference Computer program supporting it  Optimize the setup procedures Improved model, easier and faster beam setup 27 January 2015 CLIC Workshop

27 January 2015 CLIC Workshop

27 January 2015 CLIC Workshop

CTF3 experimental program January 2015 CLIC Workshop Still many things to achieve !!! Phase feed-forward & stability studies Beam Loading / BDR experiment Two-Beam ModuleTBL DeceleratorDiagnostic Tests Shut-down + restart 2 tests with 32 & 64kW phase propagation tuning 2nd run (shared with normal operation) Complete commissioning & 1st run RF conditioning & testing with drive beam Available beam time Shut-down + restartModule upgrade?Shut-down + restart 2 combined beams 3rd run (shared with normal operation) 2nd run RF conditioning & testing with drive beam Available beam time 3 4

Backup slides 27 January 2015 CLIC Workshop

ClicWS’14 Presentation  Davides presentation LCWS’14  Automatic closure, dispersion measuremens 3/material/slides/ 27 January 2015 CLIC Workshop

Drive Beam Generation 2013 Factor 4 Routine, well controlled, with nominal specs  Lossless: 4 A from the linac combined to 16A Allows for higher repletion rate where needed  Emittance:  H = 170 µm  V = 120 µm  Stability around 0.1% Stable enough to have machine running over-night with remote supervision only by PS operators from CCC 27 January 2015 CLIC Workshop

first beam from gun beam in linac beam in CALIFES 16 A in CR – factor 4 7 A in DL factor 2 25 A in CR factor 8 23 A in CLEX factor 8

CTF3 Schedule 2014 Installation TBM / Maintenance klystrons