Analysis of ATF EXT/FF Orbit Jitter and extrapolation to IP (Data of 2014.11.18) ATF2 Project Meeting 2015. 2 K. Kubo Data taking • Data taken in November 18 (2014) swing shift. • After IP beam size tuning, observing modulation with IPBSM 174 degree mode. (10x1 optics) – Positions of the BPM reference cavity and OTR2 chanber were optimized. • Data of EXT/FF BPM are saved with several conditions. (See Log Note) • This report used data of – One file (2000 pulses) with bunch intensity intentionally changed by hand. – 3 files (1000 pulses), each is for fixed bunch intensity setting. (N~8.5E9, 4.9E9, 1.8E9) BPM reading vs, pulse number (MQD10BFF: Large beta_y) 600 500 y 400 400 300 200 200 0 100 -200 0 -400 -600 -100 0 500 1000 1500 2000 pulse number In horizontal, drift is larger compare with pulse to pulse jitter. In vertical, pulse to pulse jitter is more significant. (It may be only in this particular case. (?)) y (m) x (m) x Analysis using SVD BPM1x - pulse1 BPM1y - pulse1 BPM2x - pulse1 BPM1x - pulse2 BPM1y - pulse2 BPM2x - pulse2 M BPM1x - pulse3 BPM1y - pulse3 BPM2x - pulse3 monitor (Average is subtracted for each monitor) (Data far from average (>5-sigma) removed. BPM noise, etc.) M UWV W: Diagonal matrix of singular values w1 0 W 0 pulse 0 0 w2 0 0 w3 U_ij represents amplitude of mode j in pulse i V_kl represents response of monitor l to mode k Result of SVD: First 4 modes vs. BPM x,y Circles: amplitude at each BPM, Lines: Fitting by injection orbit + dispersion (model) 150 150 x data y data x fit y fit RMS Amplitude (m) 100 50 x data y data x fit y fit mode 2 100 RMS Amplitude (m) mode 1 0 -50 -100 50 0 -50 -100 -150 -150 0 10 20 30 40 0 10 BPM Number 30 40 BPM Number 40 40 x data y data x fit y fit 20 mode 4 30 RMS Amplitude (m) mode 3 30 RMS Amplitude (m) 20 10 0 -10 -20 x data y data xfit yfit 20 10 Dispersion 0 -10 -20 -30 -30 -40 0 10 20 BPM Number 30 40 0 10 20 BPM Number 30 40 Result of SVD: other 2 modes vs. BPM x,y 25 10 15 RMS Amplitude (m) RMS Amplitude (m) x data y data x fit y fit mode 5 20 10 5 0 -5 x data y data x fit y fit 5 0 -5 -10 -10 -15 0 10 20 30 40 BPM Number Intensity dependence Only seen in data with large intensity change 0 10 20 30 BPM Number y position at IP phase 40 Standard deviation at each BPM in EXT/FF (not from SVD) (High intensity N~8.5E9) 200 x stdv 0.3*sigmax y jitter (m) 150 Horizontal: ~20% of beam size (emittance 2 nm assumed) 100 50 0 0 10 20 30 40 BPM number 140 y stdv 0.3*sigmay y jitter (m) 120 Vertical: ~40% of beam size (emittance 12 pm assumed) 100 80 60 40 20 0 0 10 20 BPM number 30 40 Effect to IP position of some first modes -1 • 3 Different intensities (about 1000 pulses for each) – All BPMs used for fitting Mode 1 2 3 8 4 Total of mode 1 - 10 Vertical Jitter propagation to IP (nm) N~8.5E9 N~4.9E9 N~1.8E9 3.9 12.5 17.3 16.6 9.4 7.1 1.1 4.4 2.0 6.1 7.3 6.6 0.5 0.8 0.1 18.1 17.9 No intensity dependence. 20.3 Effect to IP position of some first 10 modes -2 Compared • Using All BPMs • Using only downstream BPMs Extrapolated to IP Used BPM Vertical Jitter propagation to IP (nm) N changed N~8.5E9 N~4.9E9 N~1.8E9 All 19.9 18.1 17.9 20.3 From QD10AFF 1272 1258 1098 1139 From QF7FF 1000 974 863 882 Too large jitter using downstream BPMs only check waist shift (May be from optics error???) Fitted orbit around IP (s=0) Y (microm) All BPMs used s (m) There is waist shift. (Note different scales) Y (microm) BPM from MQD10AFF used s (m) Effect to position at waist of first 10 modes • Using All BPMs • Using only downstream BPMs Extrapolated to waist (not exactly IP) Used BPM Vertical Jitter propagation to IP (nm) N changed N~8.5E9 N~4.9E9 N~1.8E9 All 8.5 6.4 9.1 8.0 From QD10AFF 233 283 184 183 From QF7FF 251 213 208 210 Still large using BPMs only in downstream region Simulation of SVD analysis • Create sets of EXT-FF BPM data – Orbit jitter is given • At the beginning of the extraction line (injection error) • Or position jitter of QD10BFF magnet • Or position jitter of All Q-magnets – Beam position at every BPM is calculated by SAD – BPM resolution assumed • 1 micron, or 100 nm for cavity BPMs • 10 micron for stlipline BPMs • Apply the same analysis program for the real data. – Look at evaluated (extrapolated) y position jitter at IP by SVD – Compare with “real” jitter at IP Simulation result of SVD analysis -1 injection jitter Extrapolated y jitter at IP by SVD (nm) Evaluated jitter (all BPMs used) vs. Real jitter at IP Real jitter was changed by changing amplitude of injection jitter. Evaluated jitter include 10 SVD modes 40 Resolution CavBPM: 1 um Stlipline: 10 um 35 30 25 20 15 10 Good resolution for injection jitter, using all BPMs 5 0 0 5 10 15 20 25 30 real y jitter at ip (nm) 35 40 Simulation result of SVD analysis -2 jitter induced at QD10BFF 160 140 Fitted y jitter at IP (nm) Evaluated jitter vs. Real jitter at IP “Real” jitter amplitude was changed by changing position jitter amplitude of QD10BFF. Evaluated jitter include 10 SVD modes 6 cases of used BPMs (and resolution) Use All BPMs from QD10AFF (1 um and 100 nm) from QF7FF (1 um and 100 nm) Good estimation using BPMs downstream of jitter source only All BPM used BPM from QD10AFF (resolution 1m) BPM from QD10AFF (resolution 100nm) BPM from QF7FF (resolution 1m) BPM from QF7FF (resolution100 nm) 120 100 80 60 simulation, orbit by QD10BFF offset 40 100 nm BPM resolution: good estimation 1 um BPM resolution: over estimate jitter at IP by several x 10 nm. 20 0 0 20 40 60 80 100 Real y jitter at IP (nm) 120 140 Simulation result of SVD analysis -3 jitter induced at all Quads 140 120 Fitted y jitter at IP (nm) Evaluated jitter vs. Real jitter at IP “Real” jitter amplitude was changed by changing position jitter amplitude of all Quads in EXT-FF. Evaluated jitter include 10 SVD modes All BPM, CavBPM rtesolution 100 nm All BPM, CavBPM resolution 1 m BPM from MQD10A, resolution 100 nm BPM from MQD10A, resolution 1 m 100 80 Use All BPMs and use from MQD10AFF CavBPM resolution 100 nm and 1 um Orbit by all Quads' vibration 60 Always underestimate jitter at IP 40 Bad BPM resolution makes estimated jitter large 20 0 0 20 40 60 80 100 Real y jitter at IP (nm) 120 140 Fitted jitter depends on BPM resolution jitter induced at all Quads Fitted y jitt at IP (nm) 1000 Orbit by vobration of all Q 20 nm Real jiier at IP = 35 nm use BPMs from MQD10AFF 100 10 0.1 1 10 Cav BPM resolution (m) BPM resolution about 5 um may explain the large fitted jitter using BPMs in downstream part of FF line only. (about 200 nm at waist) Extrapolated position jitter at IP • About 20 nm (RMS) vertical jitter at IP using all BPMs (57% of beam size) • • Using BPMs in downstream part of FF line only, large extrapolated position jitter (about 1 um at IP, 200 nm at waist) – Orbit jitter induced in FF line so large? (But measured beam size was ~60nm a few hours before these data taken.) – Or, misunderstood BPM data, or assumed wrong optics in FF, , , , , ,? Simulations were performed to check the analysis. – If BPMs downstream of jitter source are used, the analysis can reproduce jitter at IP. – Including BPMs upstream of jitter source, the analysis tends to underestimate jitter at IP. (This is reasonable.) – Bad BPM resolution overestimate jitter at IP (This is reasonable too.) • 200 nm jitter from the analysis of the experimental data may be explained if BPM resolution is about 5 um. But it seems too large. No clear conclusion on jitter induced in the beam line NOTE: BPMs in downstream FF line is not so sensitive to Position-at-IP phase orbit 4 5 10 1000 orbit y-at-IP phase y = 37 nm, y' = 0 IP orbit y-at-IP phase y = 37 nm, y' = 0 IP IP IP y (nm) y (nm) 500 0 0 -500 4 -5 10 -1000 0 20 40 s (m) 60 80 50 55 60 65 70 75 80 85 s (m) Using IPBPM will be probably necessary for reliable estimation of orbit difference induced in the FF line. 90 SUMMARY • • • • • Data of EXT/FF BPM taken in November 18 (2014) swing shift were analyzed using Singular Value Decomposition method. Vertical jitter at FF line BPMs (angle-at-IP phase) is a bout 40% of beam size. Position jitter at IP (or waist) estimated extrapolating orbits calculated from SVD modes. – About 20 nm jitter from injection (or from upstream part of EXT) jitter. – No intensity dependence. – Estimation of jitter induced in FF beam line was tried without any clear results. With more data, better optics information and careful BPM calibration, some improved results may be possible. But, Using IPBPM is simple for reliable estimation of position jitter at IP.
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