Diagnostics overview and FB for the XFEL bunch compressors

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Presentation transcript:

Diagnostics overview and FB for the XFEL bunch compressors Holger Schlarb, Christopher Gerth, Michael Röhrs, … DESY 22607 Hamburg 12/7/2018 Holger Schlarb, DESY

Diagnostics overview BC1 proposed beam line design: SRF 1.3 GHz SRF 3.9 GHz Bunch compressor TDS X&Y Diagnostic section SRF 1.3GHz Will be discussed by Ch. Gerth in details Spectrometer Dump Matching sections Diagnostics elements 12/7/2018 Holger Schlarb, DESY

Diagnostics overview BC1 proposed beam line design: SRF 1.3 GHz Bunch compressor TDS X&Y Diagnostic section 3.9 GHz SRF 1.3GHz Spectrometer Dump BPM beam position monitor ~ 20 (not yet determined … every quad?) purpose: orbit correction, transfer measurements, dispersion correction TOR toroid system for transmission measurements (1,3&4 for interlock) OTR optical transition screen (with wire scanners WS?) DC dark current monitors (upstream BC1, downstream BC1) Standard diagnostics: 12/7/2018 Holger Schlarb, DESY

Diagnostics overview BC1 proposed beam line design: SRF 1.3 GHz Bunch compressor TDS X&Y Diagnostic section 3.9 GHz SRF 1.3GHz Spectrometer Dump BCM bunch compression monitors (CSR at D4 and CDR/CTR) BAM beam arrival time monitor TDS transverse deflecting structure X & Y EO electro-optic longitudinal beam profile monitor SR synchrotron radiation monitor (energy and energy spread) Special diagnostics: -> B Schmidt 12/7/2018 Holger Schlarb, DESY

Diagnostics overview BC1 proposed beam line design: SRF 1.3 GHz Bunch compressor TDS X&Y Diagnostic section 3.9 GHz SRF 1.3GHz BLM beam loss monitors (about 8-10 sufficient) Spectrometer Dump COL collimators (1st & 2nd to remove dark current, 3nd & 4th for kicked e-) Align laser for optics alignment KIC fast kicker to off-axis screens (2 x and 2 y) Additional devices: 12/7/2018 Holger Schlarb, DESY

Diagnostics overview BC2 proposed beam line design: SRF 1.3 GHz Bunch compressor BC2 TDS X Diagnostic section SRF 1.3GHz Will be discussed by Ch. Gerth in details TDS transverse deflecting structure (only X <-dump line in Y) ORS optical replica synthesizer Spectrometer Dump Matching sections Diagnostics elements Remaining diagnostics/devices are basically the same as for BC1 12/7/2018 Holger Schlarb, DESY

Longitudinal Feedback most challenges for BC1 SRF 1.3 GHz SRF 3.9 GHz Bunch compressor SRF 1.3GHz E z A1,1   Intra train |S()|2 Pulse to pulse A3,3 Problem: 4 regulation parameter A1,1, A3, 3 +  arrival time of beam into acceleration module (=-rf) Direct measurement: <> beam arrival time  (<30fs) <dE/E> beam energy (after orbit correction) (<10-5) <z2> bunch length (integral pyro signal) (<0.01°) more difficult |S()|2 spectral content of compressed bunch  profile (limit resolution!!!) Ideal operation point: where 2 of 4 parameter have relaxed tolerance (e.g. A3,3) 12/7/2018 Holger Schlarb, DESY

Longitudinal Feedback most challenges for BC1 SRF 1.3 GHz SRF 3.9 GHz Bunch compressor SRF 1.3GHz  |S()|2  E A1,1, 3 Intra train Pulse to pulse z A3 Problem: 4 regulation parameter A1,1, A3, 3 +  arrival time of beam into acceleration module (=-rf) Direct measurement: <> beam arrival time  (<30fs) <dE/E> beam energy (after orbit correction) (<10-5) <z2> bunch length (integral pyro signal) (<0.01°) more difficult |S()|2 spectral content of compressed bunch  profile (limit resolution!!!) Ideal operation point: but typically only 1 can be made insensitive 12/7/2018 Holger Schlarb, DESY

Next steps at FLASH 2007 installation of optical replica synthesizer (< 5fs resolution) in cooperation with Uppsala & Uni. Stockholm preparation of longitudinal feedback system (mainly new monitor systems) allow for laser based beam manipulation and external seeding option: requires ~ 30-60 fs rms arrival time stability incoming orbit energy exiting orbit time compression Fast FB A/ ACC1 Tarrial, A/ ACC1 12/7/2018 Holger Schlarb, DESY

Potential upgrades normal conducting acceleration cavities for large bandwidth longitudinal FB => upstream of BC1 2 * 1 m fast kicker for orbit feedback at BC1 or at BC2 => downstream chicanes 4 * 1m E-SASE operation (laser launched after BC2) => ORS can be used (to be confirmed) Laser? Beam manipulation in BC1 => requires addition space! g 12/7/2018 Holger Schlarb, DESY

Laser manipulation BC1 R54 Most suited in bunch compressor chicane due to large R16 ~ 600mm Longitudinal space is mapped to spatial components (Y) LCLS insertion of slotted foil to increase emittance for macropulse not possible But laser based energy manipulation provides similar option! Z ~ 8m Z ~ 4m Z ~ 8m Z ~ 1.5m Laser pulse ~ mJ Spatial mask imaging optics Z ~ 4m undulator inducing energy spread particle migration due to R54 (y’ smears out E(z)) in BC2 the energy distribution induced 2.5 larger peak current requires 2m space ín BC1 g R54 12/7/2018 Holger Schlarb, DESY

Beam manipulation BC1 - simple simulation - Laser off Single gap Two gaps x=4mm z~6.5m z~1m 2.5 * Ipeak 12/7/2018 Holger Schlarb, DESY

Beam manipulation BC1 spike width and peak current increase tunable via initial energy spread (laser heater) allows more complex longitudinal pattern using different masks requires more detailed simulation concerning laser launch condition and laser parameters collective effects BC1 & particular at BC2 (micro bunch inst.) FEL simulation to verify possibilities and limitation currently not baseline of XFEL design but: space should be reserved for future upgrade Space requirements (approximately): 1.5 m for undulator 2 m total including screens optical table for laser launching laser beam line injector building to BC1 ?! BC2 ?: not so interesting since lower compression (2.5) and much high laser power required g 12/7/2018 Holger Schlarb, DESY