Aperture Considerations in the FEL Upgrade • Accepted design process – generate design known – set aperture = N + W • N typically 4 to 6 • W is “beam handling allowance” example: IR Demo has A = 6+ 4 cm – “Other restrictions may apply” • constraints imposed by FEL - optical mode size • Here, programmatic considerations force deviation from accepted practice risk escalates • Can reduce risk by using all available information – previous design studies – experience with IR Demo What Do We Know? • No design unknown • Injector not quantitatively understood N135 pC unknown unknown • FEL optical mode larger 3” aperture needed unless we can compress e- beam transport What Can We Reasonably Surmise? • N135 pC > N60 pC • upgrade > demo – larger machine larger and/or more quads • more quads undesirable – higher cost – increased chromatic aberration (in turn a limit on larger required momentum acceptance) 2 • 1st iteration linac optics (actually, 2nd - 1st was UV Demo design study) has larger beam envelopes – ’s “same” in modules 2” may be okay for modules provided emittance does not increase too much – ’s 2 x larger in warm regions » triplet focussing needed to handle longer linac, higher RF focussing from increased module gradient for same emittance, need 2 bigger aperture 50 40 30 20 10 0 0 -10 -20 10 20 30 r e c i r c u l a t o r beta x 10*eta x beta y 40 50 60 70 Geometric Emittance Comparison to Demo accelerate 150 MeV 100 MeV 50 MeV 10 MeV 10 MeV 50 MeV 100 MeV 150 MeV energy recover • upgrade > demo with upgradegeometric > demogeometric larger spots • upgradegeometric > demogeometric with upgrade ~ demo larger spots • N135 pC > N60 pC likely, upgrade > demo certain • Injector setup required for high FEL gain (tapered wiggler tests) limited to 1.5 mA by BLM hits 2” aperture inadequate even at 60 pC when high gain configuration required? Conclusion #1 Though 2” possibly (probably?) adequate in modules, peak ’s in upgrade are in warm regions and will drive increase in aperture there Recommendation(s) #1 • Make effort to understand injector quantitatively and run 5 mA CW at 135 pC – helps define if 2” injector chamber allows reliable operation – characterized normalized emittance at elevated charge • 3” warm region in linac Linac-to-FEL Transport at 100-200 MeV • It is possible geometricupgrade < geometricdemo in the module to FEL transport even with space-charge driven degradation (higher energy) – upgrade > demo is washed out in spot size in full energy transport – note that at same energy (mid linac in upgrade, end of linac in demo) spot sizes are larger in upgrade – at low end of energy range (~100 MeV) spots may be same or larger in upgrade due to increased normalized emittance and larger beam envelopes Conclusion #2 2” tube may be adequate for full energy beam from end of linac to start of FEL insertion Recommendation(s) #2 100-200 MeV beam start 2” 10 MeV beam optical cavity chicane end 2” to wiggler Component Reuse Larger aperture requirements limit component reuse to regions such as linac-to-FEL transport • Diagnostics reusable without modification • QB quads probably reusable without modification – 48 MeV IR Demo QB maximum current ~2 A – QBs spec’d to 10 A with LCW can get to ~200 MeV with 20% headroom for matching • Correctors may prove useful under similar analysis FEL Insertion Region • Optical mode significantly larger than in IR Demo: – either use 3” aperture (including dipoles) – or restrict matching regions to ~ 5 m length • Current “existence proof” uses ~10 m match – manages aberrations at 5% momentum offsets by adjusting phase advances amongst telescopes/arc components • causes destructive interference of chromatic effects – y~ ds/ if L reduced, must reduce • good for small apertures, but, smaller quads stronger • stronger quads aberrations larger – higher order chromatics ~quadratic in quad strength, halving lengths doubles quads, quadruples aberrations Conclusion #3 10 m match “meets spec”5 m match “4 x out of spec” - go with 3” Recommendation(s) #3 • FEL insertion region: optical cavity chicane 3” wiggler end 2” – basic optimization for matching telescope length must balance keeping small - for good performance and acceptance while keeping L large - to limit quad strength – ~10 m match in this machine • Choose magnet families to keep construction simple – fringe models developed for spectrometer magnets; 3” is not “large” so predictive capability likely okay – match magnet gaps in “similar” families – p-bends probably tolerate 2” because , (and h) “smaller” – power requirements dominated by p-bends (180o out of 300o bending per end loop, so draw most of power) – IR Demo successful matching magnets within and across families; should anticipate similar results in upgrade Conclusion(s) #4 To avoid undue risk must make FEL insertion 3” “Little” additional cost in making all reverse bends 3” • moderate additional DC power (most in p-bends) • no overhead in “lost” magnets – no dipoles “lost” as none upgrade – need new trim quads, 6-poles, 8-poles due to horizontal aperture increase necessary to accommodate 10% dp/p • significant risk reduction, especially for lower energy operation at higher space charge (can tolerate ~2x larger emittance) Injection/Reinjection Region - 2” or 3”? upgrade ~2 or 3 x demo at reinjection Nupgrade > Ndemo (space charge) geo.upgrade~ 1/2 to 1/3 geo.demo (adiabatic damping) it will not get better How good is it now? • Cavity 8 tunes a fair bit ( losses) • ILM0F062 hits have been limitation • ILM0F06 hits are a limit when running injector for high wiggler gain Conclusion #5 3” prudent risk reduction at modest incremental cost • new injection/extraction dipoles needed to increase available dynamic range of injection/final energy – “small” magnets (~DU/DV) minor power impact • QJ quads/associated correctors support 3” • need additional quads for recirculator – not enough QBs to populate reinjection region – at very least, need to re-coil some QGs (~4 for linac to FEL transport, this region would require an additional 6 or 7) – could build an additional half-dozen 3” quads