Nigel Watson (Birmingham) LAL, 16-May-2006

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Presentation transcript:

Nigel Watson (Birmingham) LAL, 16-May-2006 ILC Collimator Design spoiler Nigel Watson (Birmingham) LAL, 16-May-2006 Aims Status T-480 beam test Damage studies Plans

Nigel Watson / Birmingham People “Spoiler Wakefield and Mechanical Design” task Details on project web: http://hepunx.rl.ac.uk/swmd/ Birmingham: N.Watson CCLRC: C.Beard,G.Ellwood,J.Greenhalgh,J.O'Dell,L.Fernandez CERN: F.Zimmermann,G.Rumolo,D.Schulte [DESY: I.Zagorodnov] Lancaster: D.Burton,N.Shales,J.Smith,A.Sopczak,R.Tucker Manchester: R.Barlow,A.Bungau,G.Kurevlev,R.Jones,A.Mercer TEMF, Darmstadt: M.Kärkkäinen,W.Müller,T.Weiland For ESA tests, working closely with CCLRC on optics for wakefield and beam damage studies SLAC for all aspects EUROTeV 2nd Workshop, LAL Nigel Watson / Birmingham

Aims Design / optimisation of spoiler jaws (geometry and materials) for wakefield and beam damage performance Development of improved EM modelling methods Benchmarking of wakefield calculations against experiments SLAC ESA beam test / data analysis RF bench tests (training/code comparisons) Tracking simulations with best models of wakefields Simulations of beam damage to spoilers Material studies using beam test Project web: http://hepunx.rl.ac.uk/swmd/ Ongoing: analytic calcs. ECHO-2D/3D Ongoing: Mafia, GdfidL Completed 1st run In preparation Ongoing Ongoing Planning Submitted 7 abstracts to EPAC, several EUROTeV reports/memos EUROTeV 2nd Workshop, LAL Nigel Watson / Birmingham

Collimator Wakefields Improvements to theory (Stupakov et al) Very difficult to calculate analytically - possible for simple, symmetric configurations Resistive wakes (tapered rectangular) Kicks Geometric wakes (tapered, rectangular) collimators Inductive (shallow tapers) Intermediate regime Diffractive (steep tapers) 3 runs with dedicated facility at SLAC, study geometric and resistive wakes, 2000-2004 Analytic calculations used in TRC, assuming  is = Cu No tail folding Near-axis wakes (linear, dipole region) Behaviour on ½ gap, r, predicted ~ 1/r2 – 1/r3/2 EUROTeV 2nd Workshop, LAL Nigel Watson / Birmingham

EUROTeV 2nd Workshop, LAL A C-module for wake fields has been constructed and implemented in PLACET in order to allow full tracking including the collimator wake fields According to the parameters of the problem, the module distinguishes between different regimes for the geometric part of the wake: Inductive regime Intermediate regime Diffractive regime Successfully started benchmarking of GdfidL and for the resistive wall part of the wake: Short-range Intermediate-range Long-range Nigel Watson / Birmingham EUROTeV 2nd Workshop, LAL

EUROTeV 2nd Workshop, LAL Examples of kick calculations in resistive wall wake field in the intermediate-range (left) and long-range (right) regimes. (x 10-7) (x 10-7)  Details of the used approach and first results from actual particle tracking through the CLIC-BDS using PLACET will be presented in EPAC: „Effects of wake fields in the CLIC BDS“, G.Rumolo, A. Latina and D. Schulte Nigel Watson / Birmingham EUROTeV 2nd Workshop, LAL

Nigel Watson / Birmingham T-480 Experiment BPM 2 doublets ~40m BPM Two triplets ~16m Vertical mover Wakefields measured in running machines: move beam towards fixed collimators Problem Beam movement  oscillations Hard to separate wakefield effect Solution Beam fixed, move collimators around beam Measure deflection from wakefields vs. beam-collimator separation Many ideas for collimator design to test… EUROTeV 2nd Workshop, LAL Nigel Watson / Birmingham

Nigel Watson / Birmingham T-480 Experiment BPM 2 doublets ~40m BPM Two triplets ~16m Vertical mover Wakefields measured in running machines: move beam towards fixed collimators Problem Beam movement  oscillations Hard to separate wakefield effect Solution Beam fixed, move collimators around beam Measure deflection from wakefields vs. beam-collimator separation Many ideas for collimator design to test… EUROTeV 2nd Workshop, LAL Nigel Watson / Birmingham

Collimator Wakefield Beam Test (T-480) Wakefield beam tests at ESA SLAC Proposal T-480 (Watson, Tenenbaum et al), Apr-2005 Many people involved directly, see proposal Part of evolving programme of ILC tests at ESA Purpose Commision/validate CollWake Expt. at ESA Additional study of resistive wakes in Cu First study of 2-step tapers Development of explicit FDTD code (TEMF) for shallow tapers/short bunches Schedule Commissioning, 4-9 Jan. 2006, 4 (old) collimators Physics, 24-Apr – 8-May 2006, 8 new collimators (CCLRC) Data rate “Real” DAQ, runs 10Hz (not via SCP)  # pulses/scan point ~600 Related activity Implementation of validated/realistic 3D wakefunctions in Merlin Collimator damage studies considered for ESA/TTF EUROTeV 2nd Workshop, LAL Nigel Watson / Birmingham

ESA beamline layout (plan) Wakefield box Beam Measure kick factor using incoming/outgoing beam trajectory, scanning collimator gap through beam Stage 1, 5 rf cavity BPMs, 1 stripline BPM, 2 wire scanners Downstream BPMs themselves R&D project … Wakefield box, proposal for 2 sets of four pairs of spoiler jaws Each set mounted in separate “sandwich” to swap into WF box (Relatively) rapid change over, in situ – ½ shift for access Commissioning run, Jan 4-9, 2006 Physics run, 24-Apr – 8-May, 2006 EUROTeV 2nd Workshop, LAL Nigel Watson / Birmingham

Wakefield box 1500mm Ebeam=28.5GeV ESA sz ~ 300mm – ILC nominal sy ~ 100mm (Frank/Deepa design) Magnet mover, y range = 1.4mm, precision = 1mm EUROTeV 2nd Workshop, LAL Nigel Watson / Birmingham

Nigel Watson / Birmingham Optical design Optical design of A-line for T-480 (F.Jackson/D.Angal-Kalinin) sy~100mm and flat in vicinity of WF box EUROTeV 2nd Workshop, LAL Nigel Watson / Birmingham

Wakefield Box Relocation EUROTeV 2nd Workshop, LAL Nigel Watson / Birmingham

Successful commisioning and Beamline preparation at SLAC - Ray Arnold ESA Test Beam for T-480 sy = 117 mm Wire scanner measurement of vertical spotsize. Successful commisioning and physics runs in 2006 Wakefield box Beamline preparation at SLAC - Ray Arnold EUROTeV 2nd Workshop, LAL Nigel Watson / Birmingham

Energy profile with SLM digitized Physics run, Apr-May 2006 Successful! Energy profile with SLM digitized (saturates at peak) 1.2% dE/E Energy profile with SLM digitized (saturates at peak) 1.2% dE/E Wire scanner measurement, sy = 80 mm Optimised Linac injection phase, compressor voltage for short bunches removes low energy tail (for high energy tail) EUROTeV 2nd Workshop, LAL Nigel Watson / Birmingham

a Side view (“DESY sandwich”) Beam view 1, 1 2, 2 3, 3 4, 4 h=38 mm Collim. #, slot Side view (“DESY sandwich”) Beam view Revised 4-May-2006 1, 1 a=324mrad r=2.0mm 2, 2 r=1.4mm 3, 3 4, 4 a=p/2rad r=4.0mm h=38 mm 38 mm a r=1/2 gap As per last set in Sector 2, commissioning Extend last set, smaller r, resistive WF in Cu L=1000 mm 7mm cf. same r, tapered EUROTeV 2nd Workshop, LAL Nigel Watson / Birmingham

cf. collim. 7, and same step in/out earlier data Collim.#, slot Side view (“SLAC sandwich”) Beam view Revised 4-May-2006 8, 1 r1 =4.0mm r2 =1.4mm a1=289mrad a2=166mrad 7, 2 a1=p/2 rad r1=4.0mm r2=1.4mm 6, 3 a=166mrad r=1.4mm 5, 4 a=p/2rad 133mm cf. collim. 7, and same step in/out earlier data 38 mm h=38 mm 31mm cf. collims. 4 and 6 211mm cf. collim. 2, same r 7 mm cf. collim. 4 smaller r EUROTeV 2nd Workshop, LAL Nigel Watson / Birmingham

Nigel Watson / Birmingham All jaws 1000mm OFE Cu, ½ gap 1.4mm EUROTeV 2nd Workshop, LAL Nigel Watson / Birmingham

First glimpse of data Preliminary, one run only BPM calibrations, systematics, etc…. Short collimator #2 Expect per pulse resolution ~mrad Angular deflection (arbitrary units) Beam-collimator center /mm EUROTeV 2nd Workshop, LAL Nigel Watson / Birmingham

First glimpse of data Preliminary, one run only BPM calibrations, systematics, etc…. Long collimator #3 Angular deflection (arbitrary units) Beam-collimator center /mm EUROTeV 2nd Workshop, LAL Nigel Watson / Birmingham

Details in EUROTeV Reports 2006-015, -021 Nigel Watson / Birmingham Damage Studies Considered steady state heating, and bunch impacts Energy deposition profile from Fluka/Geant4 Study transient effects, fracture, etc. Using CCLRC expertise from NF target studies as necessary Beam tests to be designed following simulations Could use ESA, TTF? Quantify damage detection also? Consider using new collimators in these tests – assess impact on measured wakefields [G.Ellwood] Details in EUROTeV Reports 2006-015, -021 EUROTeV 2nd Workshop, LAL Nigel Watson / Birmingham

Nigel Watson / Birmingham Preliminary 2 mm deep from top Full Ti alloy spoiler 405 K 270 K 135 K ∆Tmax = 420 K per a bunch of 2E10 e- at 250 GeV σx = 111 µm, σy= 9 µm [L.Fernandez, ASTeC] EUROTeV 2nd Workshop, LAL Nigel Watson / Birmingham

Nigel Watson / Birmingham Preliminary 2 mm deep from top Full Ti alloy spoiler 810 K 405 K 270 K 135 K ∆Tmax = 870 K per a bunch of 2E10 e- at 500 GeV σx = 79.5 µm, σy= 6.36 µm [L.Fernandez, ASTeC] EUROTeV 2nd Workshop, LAL Nigel Watson / Birmingham

Spoilers considered include… 250, 500 GeV e- 2 mm, 10mm Ti/C 0.6 Xo of Ti alloy leading taper (gold), graphite (blue), 1 mm thick layer of Ti alloy 0.3 Xo of Ti alloy each side, central graphite part (blue). EUROTeV 2nd Workshop, LAL Nigel Watson / Birmingham

Nigel Watson / Birmingham Preliminary 10 mm deep from top Ti alloy and graphite spoiler beam Ti C Temperature data in the left only valid the Ti-alloy material. Top increase of temp. in the graphite ~200 K. Dash box: graphite region. Peak at the exit 405 K 270 K 200 K 135 K ∆Tmax = 295 K per a bunch of 2E10 e- at 250 GeV σx = 111 µm, σy= 9 µm [L.Fernandez, ASTeC] EUROTeV 2nd Workshop, LAL Nigel Watson / Birmingham

Nigel Watson / Birmingham Preliminary 2 mm deep from top Ti alloy and graphite spoiler Temperature data in the left only valid the Ti-alloy material. Top increase of temp. in the graphite ~400 K. Dash box: graphite region. 540 K 405 K 400 K 270 K ∆Tmax = 575 K per a bunch of 2E10 e- at 500 GeV σx = 79.5 µm, σy= 6.36 µm [L.Fernandez, ASTeC] EUROTeV 2nd Workshop, LAL Nigel Watson / Birmingham

Nigel Watson / Birmingham Preliminary 10 mm deep from top Ti alloy and graphite spoiler Temperature data in the left only valid the Ti-alloy material. Top increase of temp. in the graphite ~400 K. Dash box: graphite region. 540 K 405 K 400 K 270 K ∆Tmax = 580 K per a bunch of 2E10 e- at 500 GeV σx = 79.5 µm, σy= 6.36 µm [L.Fernandez, ASTeC] EUROTeV 2nd Workshop, LAL Nigel Watson / Birmingham

Nigel Watson / Birmingham 2 ILC bunches [Ellwood/RAL] beam ANSYS for transient mechanical stress, temperature rise Peak stress from bunch 1 ~ arrival time of bunch 2 Time structure important for tests Realistic spoiler energy depostion from FLUKA Consistent results from G4/EGS EUROTeV 2nd Workshop, LAL Nigel Watson / Birmingham