LMC tune perturbation and stability, 1 2010-03-10 LHC Machine Committee Status of the Investigations.

Slides:



Advertisements
Similar presentations
M.Gasior, CERN-AB-BIBase-Band Tune (BBQ) Measurement System 1 Base-Band Tune (BBQ) Measurement System Marek Gasior Beam Instrumentation Group, CERN.
Advertisements

8:16 SB 25ns dumped by RF; integrated lumi 0.6 nb-1. 9:14 BIC problem in TI8 and CMS recovering their tracker 10:09 Abort gap cleaning commissioning. 16:29.
Beam commissioning strategy Global machine checkout Essential 450 GeV commissioning System/beam commissioning Machine protection commissioning.
Impedance measurements at SLS E. Koukovini-Platia CERN, EPFL TIARA mid-term meeting, Madrid, 13 th June 2012 Many thanks to M. Dehler, N. Milas, A. Streun.
Bunch Flattening with RF Phase Modulation T. Argyropoulos, C. Bhat, A. Burov, J. F. Esteban Müller, S. Jakobsen, G. Papotti, T. Pieloni, T. Mastoridis,
MG - MTE Workshop 24/09/20101 Measurements’ analysis S. Gilardoni, M. Giovannozzi, M. Newman Introduction Techniques, tools Results (selected) Outlook.
LHC progress with beam & plans. Of note since last time Transverse damper Beta beating in the ramp Collimation set-up at 450 GeV & validation LBDS – systematic.
AB-ABP/LHC Injector Synchrotrons Section CERN, Giovanni Rumolo 1 Final results of the E-Cloud Instability MDs at the SPS (26 and 55 GeV/c) G.
First measurements of longitudinal impedance and single-bunch effects in LHC E. Shaposhnikova for BE/RF Thanks: P. Baudrenghien, A. Butterworth, T. Bohl,
:00: Prepared new fill B1: Q X =0.293, Q Y =0.269; lifetime = 25h ✔ B2: Q X =0.297, Q Y =0.267; lifetime = 5h ✗ Strong 50Hz and 100hz lines.
BBQ system Tatiana and Benoit, thanks to a lot of help from Christian Boccard, Marek Gasior and Ralph Steinhagen (BE/BI-QP)
The HiLumi LHC Design Study is included in the High Luminosity LHC project and is partly funded by the European Commission within the Framework Programme.
Managed by UT-Battelle for the Department of Energy Analysis of 2008 Beam Instability Data S. Cousineau, V. Danilov, M. Plum HB2008.
Nominal intensity bunches ● First ramp with nominal intensity bunches suffered from an instability appearing around 1.8 TeV. ● Nominal intensity bunches.
4 th Order Resonance at the PS R. WASEF, S. Gilardoni, S. Machida Acknowledgements: A. Huschauer, G. Sterbini SC meeting, 05/03/15.
ADT Tune Measurement F. Dubouchet, W. Hofle, D. Valuch Acknowledgement: R. Calaga, F. Roncarolo, E. Bravin, shift crews New developments and tests on August.
Shortened program (2 days), as decided in LMC. MD program worked very well  all MD’s on plan with ~foreseen beam time. LHC in very good shape with excellent.
Damping of Coupled-bunch Oscillations with Sub-harmonic RF Voltage? 1 H. Damerau LIU-PS Working Group Meeting 4 March 2014.
Saturday 11.9 ● From Friday – Minimum required crossing angle is 100  rad in 2010 – Plenty of aperture at triplets: > 13  (n1 > 10) – Can stay with 170.
Progress with Beam Report to LMC, Machine Coordination W10: Mike Lamont – Ralph Assmann Thanks to other machine coordinators, EIC’s, operators,
Summary slides on orbit, Q/Q' instrumentation diagnostics, Status of Orbit, Q/Q' & Coupling Diagnostics and FB Systems Main message: All systems.
Collimation Aspects for Crab Cavities? R. Assmann, CERN Thanks to Daniel Wollmann for presenting this talk on my behalf (criticism and complaints please.
Benchmarking Headtail with e-cloud observations with LHC 25ns beam H. Bartosik, W. Höfle, G. Iadarola, Y. Papaphilippou, G. Rumolo.
AGS FY11 Summary RHIC Spin Collaboration Meeting 5/6/11.
AB-ABP/LHC Injector Synchrotrons Section CERN, Giovanni Rumolo 1 Preliminary results of the E-Cloud Instability MDs at the SPS G. Rumolo, in.
Tuesday 7 th August - morning 07:10 Reinjection after loss of fill 2920 to UFO near ALICE  26 pb -1 in 1h16m; peak lumi 6.4e33 cm -2 s -1 08:10 dump at.
LHC Beam Commissioning, LHC Q Stability Revisited M. Gasior & Ralph J. Steinhagen,
Ralph Assmann, Giulia Papotti, Frank Zimmermann 25 August 2011
MD Planning Fri – Sat (26. – 27.8.)
1st LHC MD Period Started
Cryo Problem MD Planning Tue (1.11.) C B Day Time MD MP Tue 01:00
LEIR IMPEDANCE AND INSTABILITY MEASUREMENTS
MD #453 Effect of low frequency noise
Wire, flat beams and beam-beam MDs in 2017
Saturday 21st April 00:33 Interlock during ramp on BLM HV
Monday :00 Stable beams 9_6_6_6 13:40 Access.
Results of the LHC Prototype Chromaticity Measurement
MD Report 24 June 2012 Machine coordinators: Barbara Holzer, Mike Lamont MD Coordinators: Ralph Assmann, Giulia Papotti, Frank Zimmermann MD#2 News & Plan.
Monday h00: Ramp 10 A/s (chromaticity, crossing angle non-closure, beta-beating): At 7m and 3.5m, put in one by one crossing angles, calculated.
MD2490: Measurement of the TMCI Threshold at Flat-Top
M. Gasior, A. Boccardi, S. Jackson, O. R. Jones, R. J
LHC Beam Commissioning WG Meeting
LHC Status Wed Morning 13-April R. Assmann, B. Holzer et al
Status of LHC Operations
Thursday morning – optics correction
Monday 18 October : Collimation system
Wednesday Morning 8: :30 end of fill study - octupole polarity inversion (Elias, Tatiana, Alexey, Georges, …): Goal: study the effect of the.
Alice solenoid – orbit distortion
MD#4 Progress MD Coordinators: Giulia Papotti, Frank Zimmermann
Mon 22/8 – Tue 23/8 00:07 stable beams #2040. Initial luminosities: 2.1x1033 cm-2s-1 18:00 Programmed dump. End of physics #2040. ~83 pb-1 in ~18 hours.
Tuesday 20 March 2012.
Tuesday 28th September Fill 1375 ongoing 09:00 Move in Roman Pots
Planning at 5 o’clock meeting Friday
Thursday :00: Physics fill from the night shift
450 GeV Initial Commissioning with Pilot Beam - Beam Instrumentation
Global aperture measurements at 450 GeV with 170 mrad crossing angle
Saturday 7th May Sat – Sun night
LHC Morning Meeting - G. Arduini
(on behalf of the LHC team)
Machine Tolerances in Cleaning Insertions
Summary of week 19 Machine Coordinators: G. Arduini, M. Lamont Main aim: Luminosity production.
LHC impedance: Comparison between phase 1 and IR3MBC – follow-up
Thursday Fill 1364 (24 bunch) dumped at 07h
Monday 8th December Morning used for RF work (IP z, injection), damper noise checks. Stable beams period with LHCb spectrometer OFF – lost beam after.
Monday :00 – 15:00 : Stable beams 15:30 : Recover…
LHC Morning Meeting - G. Arduini
Mon 2/4 08:00-13:00: Access for: Experiments Power converters BBQ
Another Immortal Fill….
Saturday 15th May One bunch 1 e11 per beam 09:57: start ramp
31/3/2010 Difficult day… but at the end stable beams.
Presentation transcript:

LMC tune perturbation and stability, LHC Machine Committee Status of the Investigations related to The Broad-Band Perturbation Source(s) in the Vicinity of the Nominal Tune Working Points Or 'The Hump' Ralph J. Steinhagen, BE-BI Special thanks to: M. Gasior, G. Arduini and the OP crew

LMC tune perturbation and stability, 2 Overview and Summary Beam spectrum issues affecting beam diagnostics and operation –UPS' 8 kHz line et Co. → W. Höfle et al. –Residual tune stability (Q' and other higher-order diagnostics) contribution of RQT[D/F] circuits only 10% further investigation pending... –Broad frequency “hump” driven beam excitation Better/more systematic understanding of symptoms Could eliminate some circuits as pot. source by switching them 'off'. No single source responsible for this effect has been identified Collimator at nominal settings will make the effect more apparent

LMC tune perturbation and stability, 3 Effects seen so far I There are at least three++ 'humps', with approx. base-band frequencies: ~ f rev, ~ f rev (vertical tune), > f rev, and –#4 & ~0.25 & ~ 0.37 f rev (much smaller and possible harmonic of #) Example: Q v set below 'hump' (red) and after Q v trim on top of 'hump' #2 (blue): –Driving of the tune resonance clearly visible → beam size growth → losses #1#1 #4#4 #2#2 #3#3 #5#5 vertical tune

LMC tune perturbation and stability, 4 Effects seen so far II - Absolute Amplitude Hump #2 400 nm Assuming single dipolar pertubation → kick ~ 1 nRad kick only –a non-issue if the present tune working point wouldn't be exactly on it

LMC tune perturbation and stability, 5 Effects seen so far III – Correlation between Humps I/II If structure '#5' is a true second harmonic of '#1' → width difference would give an indication on the base-band origin of the effect –Central frequency #1: f rev or ~2 kHz –Shifting the tune out this region would help for the diagnostics #1#1 #3#3 #5#5 #2#2 #4#4

LMC tune perturbation and stability, 6 Effects seen so far III – Correlation between Humps II/II Detailed correlation between Hump #1 & #5: –likely second harmonic –Perturbation #2 (~0.3, vertical tune) could be the fourth harmonic? Would also explain why it is much broader than the others need to move tune off the present tune working point for further studies f hump#5 &2 * f Hump#1 f Hump#1 4 * f Hump#1 f hump# 5 f hump# 1

LMC tune perturbation and stability, 7 Effects seen so far IV Structure of the perturbation depends on the observation time-scale, e.g. –0.1 Hz b→ broad 'hump', or –10 Hz acquisition BW → narrow-bandwidth line with shifting mean frequency Here, 'Hump' at 0.16 f rev :

LMC tune perturbation and stability, 8 Effects seen so far V – B1/B2 Correlation Hump on Beam 1 is correlated with the one in Beam 2: correlation factor = frequency change spectra 1/f reference BBQ frequency res. limit for 1024

LMC tune perturbation and stability, 9 Effects seen so far IV – Energy Scaling Amplitude seems to approximately scale with energy (-8dB reduction) –excludes some effects (e.g quad. vibration)... … but not all (e.g. quad. current noise) –tune spectra before (450 GeV) and after (1.18 TeV) the ramp #6:

LMC tune perturbation and stability, 10 Vertical Tune Scan across 'Hump Domain' The observed excitation frequency are real and cause a blow-up of the vertical emittance –10 % beam size blow-up within about 5 minutes –beam is eventually intercepted at an aperture bottlenecks (e.g. TDI or TCDQ) → later collimator would intercept this at an earlier stage vertical tune frequency Vertical tune amplitude Vertical beam size (BSRT)

LMC tune perturbation and stability, 11 Beam Size Growth and Effect of Power Converter Verified effect on the hump for following circuits: –Both MSI's, transfer lines, RSS, RCO, RCD and vertical 60A orbit correctors → No effect! However, whilst effect is visible on both beams, the vertical plane of B2 seems to be more affected: vertical beam size B2 vertical beam size B1

LMC tune perturbation and stability, 12 Effect on Beam Life-Time Each transient causes some short term beam-life loss but eventually recovers –Again: B2 beam-life time much poorer than for B1 FastBCT based beam life-times with minimal collimation: –Be aware: these life-times tell you how much intensity is kept in the LHC but not in which shape (e.g. transverse/long. bunch sizes)!! Beam 1 vs. Beam 2

LMC tune perturbation and stability, 13 Facts and Figures of 'Hump' Investigations Not one but at family (at least 3) of different perturbations Seen already in 2009 (and 2010) –Amplitudes are in the few hundred nanometre range –Effect scales down with energy (2009 ramps) –Either 'hump' or 'fast shifting line' depending on observation time-scale –Correlated between Beam 1 & 2, – however – while seen on both beams, hump effect on beam-life time is more apparent for B2 Additional studies in 2010 revealed no effect on 'hump' regardless of: –Tune or chromaticity changes –Single or two beam operation –Switching 'off'/'on' circuits: MSI's, transfer lines, RSS, RCO, RCD and vertical 60A orbit correctors –If B1/B2 RF frequencies are unlocked –If B1/B2 RF frequencies are set apart –If damper (ADT) power driver being switched 'off'

LMC tune perturbation and stability, 14 How to proceed? Two options the LMC should decide whether: A)Find and mitigate the perturbation source – the “clean solution” Other circuits/systems: RCS, MS, RF, effects of He flow-rates/orbit More exotic sources: triplet vibrations, beam screen, vacuum pumps → mechanical vibrations in the > 3 kHz range?!? However, we may need soon to move to effective operation with higher intensities B)Shift the tunes to another working point (e.g..45/.46) – the “practical approach” Hump Domain

LMC tune perturbation and stability, 15 Reserve Slides

LMC tune perturbation and stability, 16 Impact The “clean solution” (if hump not identified soon) This does probably not impact 3.5 TeV ramps/operation with a few bunches, However: Poor life-time with closed collimators Limits the intensity we can store and accelerate nominal beam safely The “practical solution” (provided beam is stable at 0.45/0.46) Buys us some time until we found the 'true' hump source Tune/Orbit not an issue with the given diagnostics and controls Non-local beta-beating correction may need to be redone

LMC tune perturbation and stability, 17 Enlarged Tune Diagram up to 10 th order Hump Domain

LMC tune perturbation and stability, 18 Effect of trimming RF voltage from 8MV → 4MV → 8MV –Only preliminary observations → need to redo these more systematically