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FACET MD Plans – 2014 Spring Run. Linac setup based on S20 performance estimates: Choose an R56 chicane setting to use based on simulation performance estimates {0-10mm} R56 config Observables: sig_z fully compressed, 2-bunch parameters notched, sig_x , delta_E
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FACET MD Plans – 2014 Spring Run • Linac setup based on S20 performance estimates: • Choose an R56 chicane setting to use based on simulation performance estimates {0-10mm} • R56 config • Observables: sig_z fully compressed, 2-bunch parameters notched, sig_x, delta_E • Free parameters: stag_chirp, comp_V, R56 • Linac setup procedure: • comp_V on [ LI02 pyro / max(LI02 pyro) ] • stag_chirp on [LI18 pyro / max(LI18 pyro)] OR LI20 pyro • Discrete configs for fully compressed & notched setups • … then LINAC emittance tuning • S20 pencil-beam studies [0.5Q, uncompressed] IP beta = 0.5x5 m • BBA key QUAD BPMs • 2050, 2147, 2235, 2365, 2445 & [3011 – 3156] • Sextupole alignment check • parabolic orbit & dispersion methods • Achieve 100% transmission to S20 dump • ballistic studies with bends @ 20.35 GeV • check individual quads powered (that are not part of above BBA procedure, especially strings) to check for any coarse misalignments • 2-D response-matrix scans • J. Sheppard plan • Beta matching at WS1,2&3 • Sexts OFF high IP beta • Sexts ON, low IP beta • Get beta, emit-limited focus-point beam sizes • Re-check BBA before compressing to assess stability • 0.5Q, Compressed config • Check sig_z, 2-bunch notched params & delta_E against model predictions for chosen R56 config • Waist beam tuning & beta-match check • 1Q, compressed
Choice of LI20 Chicane R56 • Simulation of particle transport LI02-LI20 with Lucretia: • Starting with standard DR extracted bunch assumed • 6mm sig_z, 2E10 charge and usual asymmetry parameters • If bunch length longer, will change setup parameters, this is probably worth studying with measured DR bunch length… • Use a “typical” klystron compliment • Load an LI20 R56 optics [0:10 mm], 10x100 cm IP beta @ MIP • For a given LI02 compressor voltage setting, scan staggered_chirp to minimize bunch length at IP: keep 9GeV @ LI10 and 20.35GeV @ LI20 using LI09 and LI18 energy feedbacks and adding/removing tubes as required
Simulation Results • Bunch density is 1/(sig_x*sig_y*sig_z) based on gaussian fits to x/y/z projected profiles • “Chromatic sensitivity” is relative increase in sig_x when changing centroid bunch energy by 0.5% • In general terms: • Bunch density improves with increasing R56 • Chromatic sensitivity degrades with increasing R56 • Increases below 4mm because chicane betas become too small for sextupoles to sufficiently compensate chromaticity and second-order dispersion, could improve by re-matching with higher beta functions in chicane • Chicane beta-functions increase with increasing R56 • Energy spread does not vary very significantly • 2-bunch notch setup becomes qualitatively easier with higher R56 • For some chicane configurations, the bunch density performance is more sensitive to chirp configuration than others- doesn’t correlate with R56 magnitude • Based on the above observations, an optimal choice for LI20 chicane optics is chosen to be 7mm.
Example 2-Bunch Longitudinal Config, Set – Change staggered_chirp by 0.5 degree (-ve z = head of bunch)
Linac Setup • Set optimal config using LI02 and LI20 PYROs • 55% of max PYRO in LI02 assuming proportional to 1/sig_z using compV • MAX PYRO in LI20 unsignstaggered_chirp LI02 PYRO 55% of max (+ve V from peak) Compressor V = 40.408 MV Staggered_Chirp= -1.742 degrees (*[0 0 1 2 3 3 0 0 0 5] LI sector multipliers ) -> == max PYRO signal in LI20