Nick Walker (DESY/GDE) GDE Internal Cost Review FNAL 13.11.12 ILC Design Overview 13.12.12 N. Walker ILC PAC TDR review1.

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Presentation transcript:

Nick Walker (DESY/GDE) GDE Internal Cost Review FNAL ILC Design Overview N. Walker ILC PAC TDR review1

Contents Requirements (from Physics and Detector) Design evolution to the TDR baseline Baseline 500 GeV E cm Parameters Approach to Site-Dependent Design Variants ILC overview (intro to detail talks) –RTML and bunch compressor Emittance preservation (beam dynamics) Low E cm Running Luminosity upgrade TeV energy upgrade N. Walker ILC PAC TDR review2

Requirements from ‘the customers’ Baseline: –Energy range: 200 ≤ E cm ≤ 500 GeV –∫ Ldt ~ 500 fb -1 (in four years) –Ability to make energy scans (about Ecm) –  E/E ≤ 0.1% both pulse ‘jitter’ and bunch/train energy spread –Electron polarisation ≥ 80% –Support for two detectors push-pull –Calibration at Z-pole (~90 GeV) but low lumi. –Beamstrahlung ‘low’ (~few %) Upgrades: –Energy upgrade to ~ 1 TeV  important –Not to exclude e  e  or  collider options –Polarised positrons ≥50% –Giga-Z (Z factory with several cm -2 s -1 ) focus of GDE design efforts conceptual approach considered. acknowledged but not considered in any detail N. Walker ILC PAC TDR review3

ILC in a Nutshell Damping Rings Polarised electron source Polarised positron source Ring to Main Linac (RTML) (inc. bunch compressors) e- Main Linac Beam Delivery System (BDS) & physics detectors e+ Main Linac Beam dump not too scale N. Walker ILC PAC TDR review4

Design Evolution: RDR  TDR 2007 Reference Design Report and cost estimate Technical Design Phase Re-evaluation of baseline layout  updated design Updated value estimate N. Walker ILC PAC TDR review5 RDRSB2009

Scope of Design Changes MV/m average accelerating gradient including ±20% spread 2.Single tunnel for Main Linacs 3.Undulator-based e  source relocation to end of e  Main Linac –RDR: located at nominal 150 GeV point in elec. main linac 4.Reduced beam-power parameter set –2625  1312 bunches per pulse (8.8  5.8mA) –reduced klystron / modulator count (~30%) –and…  3.2km circumference Damping Ring 6.Central region integration (general) –RTML, sources and BDS integration N. Walker ILC PAC TDR review6

ILC Published Parameters Centre-of-mass independent: Luminosity Upgrade Advantage of SCRF technology: long pulses N. Walker ILC PAC TDR review7

ILC Published Parameters Centre-of-mass dependent: N. Walker ILC PAC TDR review8

ILC Published Parameters Centre-of-mass dependent: Focus of design (and cost!) effort N. Walker ILC PAC TDR review9

ILC Footprint Total site length (500 GeV CM)30.5 km SCRF Main Linacs22.2 km RTML (bunch compressors)2.8 km Positron source1.1 km BDS / IR4.5 km Damping Rings (circumference)3.2 km There are the SCRF main linacs…. … and there is everything else N. Walker ILC PAC TDR review10

Site-Dependent Designs Top-level parameters Accelerator layout –lattice –geometry –parameters –etc. CFS requirements –Central region (source, BDS, DR) –RTML (bunch compressors) Civil engineering solutions –topography –geology Main linac layout RF power distribution (  CFS) cost effective tunnelling methods 11

SCRF Linac Technology 1.3 GHz Nb 9-cellCavities16,024 Cryomodules1,855 SC quadrupole pkg MW MB Klystrons & modulators 436 / 471 * Approximately 20 years of R&D worldwide  Mature technology * site dependent  Presentation by A. Yamamoto N. Walker ILC PAC TDR review12

RF Power Source Marx modulator 10MW MB Klystron  Presentation by S. Fukuda Adjustable local power distribution system N. Walker ILC PAC TDR review13

Main Linac Parameters (500 GeV) Average accelerating gradient31.5 (±20%)MV/m Cavity Q 010 (Cavity qualification gradient35 (±20%)MV/m) Beam current5.8mA Number of bunches per pulse1312 Charge per bunch3.2nC Bunch spacing554ns Beam pulse length730 ss RF pulse length (incl. fill time)1.65ms Efficiency (RF  beam)0.44 Pulse repetition rate5Hz Peak beam power per cavity190*kW * at 31.5 MV/m N. Walker ILC PAC TDR review14

Site Dependence I: KCS Klystron Cluster Scheme Novel system 35×10 MW MBK  350 MW Feeds ~1 km of linac via over-moded circular WG ( ∅ 48 cm) ~8 MW ‘tapped-off’ every 26 cavities Special Coxaxial Tap-Offs (CTO) used for both combining and splitting N. Walker ILC PAC TDR review15

Site Dependence I: KCS “Flat” topography site-dependent design  Presentations by M. Ross and V. Kuchler N. Walker ILC PAC TDR review16

Site Dependence II: DKS “Mountainous” Topography site- dependent design “Komoboko” tunnel Reduced surface presence. Horizontal access Most infrastructure underground.  Presentation by A. Enomoto N. Walker ILC PAC TDR review17

Site Dependence II: DKS N. Walker ILC PAC TDR review accelerator cryomodules Distributed Klystron Scheme  presentations by M. Ross and S. Fukuda 18

ILC in a Nutshell Damping Rings Polarised electron source Polarised positron source Ring to Main Linac (RTML) (inc. bunch compressors) e- Main Linac Beam Delivery System (BDS) & physics detectors e+ Main Linac Beam dump not too scale N. Walker ILC PAC TDR review19

Ring To Main Linac (RTML) 5 GeV 15 GeV 5 GeV 15 GeV 5 GeV (FoDo lattice) bunch length: 6 mm0.9 mm0.3 mm beam energy: 5 GeV 4.8 GeV15 GeV  E/E: 0.11% 1.42%1.12% ÷6.7 ÷3 R 56 = -372 mmR 56 = -55 mm N. Walker ILC PAC TDR review DKS also used for flat topography site

RTML / Bunch Compressor Emittance preservation primary challenge –fast ion instability in ~30km long return line –stray time-varying fields (≤2 nT). –spin rotation (solenoids  x-y coupling) –RF and long bunch / large  E/E  wakefields, coupler kicks, cavity tilt effects… –  beam based alignment Tight requirements on phase/amplitude stability –timing at IP  luminosity loss –0.24° / 0.48° stability (correlated/uncorrelated) –LLRF challenge N. Walker ILC PAC TDR review21

Central Region 5.6 km region around IR Systems: –electron source –positron source –beam delivery system –RTML (return line) –IR (detector hall) –damping rings Complex and crowded area Central Region common tunnel N. Walker ILC PAC TDR review22

Central Region Example: Flat Topography The central region beam tunnel remains a complex region. Complete, detailed and integrated lattices are now available Generic design used for geometry and generating component counts and CFS requirements. CFS (particularly CE) solutions are site-dependent! service tunnel N. Walker ILC PAC TDR review23

Damping Rings Circumference3.2km Energy5GeV RF frequency650MHz Beam current390mA Store time200 (100)ms Trans. damping time24 (13)ms Extracted emittancex5.5 mm (normalised)y20nm No. cavities10 (12) Total voltage14 (22)MV RF power / coupler176 (272)kW No.wiggler magnets54 Total length wiggler113m Wiggler field1.5 (2.2)T Beam power1.76 (2.38)MW Values in () are for 10-Hz mode Many similarities to modern 3 rd -generation light sources  presentation by G. Dugan N. Walker ILC PAC TDR review24

Positron Source (central region) located at exit of electron Main Linac 147m SC helical undulator driven by primary electron beam ( GeV) produces ~30 MeV photons converted in thin target into e+e- pairs not to scale! yield = 1.5  Presentation by W. Gai N. Walker ILC PAC TDR review25

Polarised Electron Source Laser-driven photo cathode (GaAs) DC gun Integrated into common tunnel with positron BDS  Presentation by W. Gai N. Walker ILC PAC TDR review26

BDS and MDI e- BDS e+ source electron Beam Delivery System  Presentation by K. Buesser Geometry ready for TeV upgrade N. Walker ILC PAC TDR review27

IR region (Final Doublet) FD arrangement for push pull –different L* –ILD 4.5m, SiD 3.5m Short FD for low E cm –Reduced  x * increased collimation depth –“universal” FD avoid the need to exchange FD conceptual - requires study Many integration issues remain –requires engineering studies beyond TDR –No apparent show stoppers BNL prototype of self shielded quad  Presentation by K. Buesser N. Walker ILC PAC TDR review28

MDI (Detector Hall) Flat-topography detector hall concept  Presentation by K. Buesser N. Walker ILC PAC TDR review29

MDI (Detector Hall) Mountainous-topography detector hall concept  Presentation by K. Buesser N. Walker ILC PAC TDR review30

Central Region Integration e- BDS e- BDS muon shield e+ main beam dump detector RTML return line e+ source Damping Rings 3D CAD has been used to developed beamline layouts and tunnel requirements. Complete model of ILC available N. Walker ILC PAC TDR review31

Where are we? Requirements (from Physics and Detector) Design evolution to the TDR baseline Baseline 500 GeV E cm Parameters Approach to Site-Dependent Design Variants ILC overview (intro to detail talks) –RTML and bunch compressor Emittance preservation (beam dynamics) Low E cm Running Luminosity upgrade TeV energy upgrade N. Walker ILC PAC TDR review32

Emittance Preservation Damping Ring:  y = 20nm –~30km RTML return line –Turn around and spin rotation –Bunch compressor (two-stages) –Acceleration (10km main linac) –Positron production (e- only) –Beam delivery system (non-linear optics) –Final Doublet and collision! Budget 15 nm   y = 35 nm at IP N. Walker ILC PAC TDR review33

Emittance Budgets Mean90% level Damping ring extraction20 RTML (Return line, turn-around, spin rotation) RTML (Bunch compressors) Main Linac End of Main Linac (total)3137 BDS (budgeted)+4 IP (effective):35>40 Results of extensive simulations (over 10 years) Standard alignment (survey) errors assumed Several beam-based alignment techniques studied (most notably DFS) ‘Realistic’ simulation (including wakefields, non-linear fields etc.) Tuning algorithms (dispersive closed bumps, final focus tuning etc.) Dynamic errors included (ground motion, vibration, beam-based feedback etc.)  IP looks OK on average (in simulation!) N. Walker ILC PAC TDR review34

Low Ecm Running (<300 GeV) Positron production (yield) drops with <150 GeV Low E cm running (≤250 GeV)  10Hz mode Alternate pulses for e+ production: –150 GeV e- pulse to generate positrons –E cm /2 e- pulse for luminosity Ramifications: –100ms store time in DR  shorter damping times –Need to dump 150 GeV production pulse after undulator (new beamline, pulsed-magnet system) –Pulsed trajectory-correction system before undulator for 150 GeV production beam. Electron Main Linac requires no modification –Installed AC power sufficient for ~½ energy operation at 10Hz N. Walker ILC PAC TDR review35

Luminosity Upgrade Concept: increase n b from 1312 → 2625 –Reduce linac bunch spacing 554 ns → 336 ns –Increase pulse current 5.8 → 8.8 mA –Increase number of klystrons by ~50% Doubles beam power  ×2 L (3.6×10 34 cm -2 s -1 ) Damping ring: –Electron ring doubles current (389mA  778mA) –Positron ring: possible 2 nd (stacked) ring (e-cloud limit) AC power: 161 MW  204 MW (est.) –AC power increased by ×1.5 –shorter fill time and longer beam pulse results in higher RF-beam efficiency (44%  61%) N. Walker ILC PAC TDR review36

Luminosity Upgrade Adding klystrons (and modulators) Flat Topography (KCS) MountainTopography (DKS) KCS Building Damping Ring: N. Walker ILC PAC TDR review37

TeV Upgrade 2.2 km 1.3 km 10.8 km 1.1 km BDS Main Linac e+ src bunch comp. <26 km ? (site length <52 km ?) Main Linac = 31.5 MV/m G eff ≈ 22.7 MV/m (fill fact.= 0.72) IP central region <10.8 km ? Snowmass 2005 baseline recommendation for TeV upgrade: G cavity = 36 MV/m ⇒ 9.6 km (VT≥ 40 MV/m) Based on use of low-loss or re- entrant cavity shapes Assume Higher Gradient N. Walker ILC PAC TDR review38

TeV upgrade: Construction Scenario BDS Main Linac e+ src IP BC BDS Main Linac e+ src IP BC BDS Main Linac e+ src IP BC BDS Main Linac e+ src IP BC start civil construction 500GeV operations Installation/upgrade shutdown civil construction + installation final installation/connection removal/relocation of BC Removal of turnaround etc. Installation of addition magnets etc. Commissioning / operation at 1TeV N. Walker ILC PAC TDR review39

TeV Parameters (2 sets) low and high beamstrahlung horizontal focusing main difference shorter bunch length (within BC range) P AC constrained ≤300 MW N. Walker ILC PAC TDR review40

Detailed Presentations SCRF Tech: Cavities and CryomodulesA. Yamamoto afternoon: Main linac layouts (incl. design variants)M. Ross RF power generation / distributionS. Fukuda Electron and positron sourcesW. Gai Damping RingsG. Dugan Beam delivery system and MDIK. Buesser CFSV. Kuchler A. Enomoto N. Walker ILC PAC TDR review41