Baseline BDS Design Updates Glen White, SLAC Sept. 4, 2014 Ichinoseki, MDI/CFS Meeting.

Slides:



Advertisements
Similar presentations
Background studies Takashi Maruyama SLAC GDE Baseline Assessment Workshop SLAC, January 18-21, 2011.
Advertisements

Ideas and Speculations for the Headon Extraction Line L. Keller Oct. 19, Give up the 3.5 m Separation between the Charged Dump and the Incoming.
EXTRACTION BEAM LOSS AT 1 TEV CM WITH TDR PARAMETERS Y. Nosochkov, G. White August 25, 2014.
4.1/9.1m L* Optics & Performance Glen White, SLAC SiD Meeting, SLAC Jan 13, 2015.
BDS Change Request: Support of Single L* Optics Configuration Shared by both Detectors Glen White, Nick Walker Sept MDI/CFS Ichinoseki.
Zero Degree Extraction using an Electrostatic Separator Take another look at using an electrostatic separator and a weak dipole to allow a zero degree.
Overview of Beam Delivery System Final Focus Optics Collimator Final Doublet Extraction/Dump Others S.Kuroda ( KEK ) MDI meeting at SLAC 1/6/2005.
Summary of wg2a (BDS and IR) Deepa Angal-Kalinin, Shigeru Kuroda, Andrei Seryi October 21, 2005.
NLC - The Next Linear Collider Project  IR background issues and plans for Snowmass Jeff Gronberg/LLNL Linear Collider Workshop October 25, 2000.
NLC - The Next Linear Collider Project NLC IR Layout and Background Estimates Jeff Gronberg/LLNL For the Beam Delivery Group LCWS - October 25, 2000.
NLC - The Next Linear Collider Project Backgrounds Update Tom Markiewicz SLAC LCWS Cornell 15 July 2003.
1 August 12, 2005 Running 2mrad IR in e-e- mode: BDS constraints A.Seryi August 12, 2005.
Status of ongoing studies for comparing 2-mrad and 20-mrad IRs T. Maruyama SLAC.
IR Beamline and Sync Radiation Takashi Maruyama. Collimation No beam loss within 400 m of IP Muon background can be acceptable. No sync radiations directly.
Beam Delivery System Review of RDR(draft) 1.Overview 2.Beam parameters 3.System description 3.1 diagnostic, tune-up dump, machine protection MPS.
NLC - The Next Linear Collider Project NLC Backgrounds What’s New? Tom Markiewicz LC’99, Frascati, Italy October 1999.
November 07, 2006 Global Design Effort 1 Beam Delivery System updates BDS Area leaders Deepa Angal-Kalinin, Hitoshi Yamamoto, Andrei Seryi Valencia GDE.
Overview of Extraction Line Designs and Issues
Ground Motion + Vibration Transfer Function for Final QD0/SD0 Cryomodule System at ILC Glen White, SLAC ALCPG11, Eugene March 21, 2011.
1 Status of EMMA Shinji Machida CCLRC/RAL/ASTeC 23 April, ffag/machida_ ppt & pdf.
October 31, BDS Group1 ILC Beam Delivery System “Hybrid” Layout 2006e Release Preliminary M. Woodley.
January 10, 2007M. Woodley (SLAC)1 ILC Beam Delivery System “Interim Working Assumption” 2006e Release European LC Workshop, January , Daresbury.
Backgrounds in the NLC BDS ISG9 December 10 – Takashi Maruyama SLAC.
October 4-5, Electron Lens Beam Physics Overview Yun Luo for RHIC e-lens team October 4-5, 2010 Electron Lens.
CASA Collider Design Review Retreat HERA The Only Lepton-Hadron Collider Ever Been Built Worldwide Yuhong Zhang February 24, 2010.
Status of ILC BDS Design Deepa Angal-Kalinin ASTeC/Cockcroft Institute, Daresbury Laboratory Andrei Seryi SLAC National Accelerator Laboratory ILC-CLIC.
ILC Beam Delivery System / MDI Issues for LCC-phase (~
Global Design Effort ILC Crab Cavity Overview and requirements Andrei Seryi SLAC on behalf of ILC Beam Delivery and Crab-Cavity design teams Joint BNL/US-LARP/CARE-HHH.
SINGLE-STAGE BUNCH COMPRESSOR FOR ILC-SB2009 Nikolay Solyak Fermilab GDE Baseline Assessment Workshop (BAW-2) SLAC, Jan , 2011 N.Solyak, Single-stage.
17 th November, 2008 LCWS08/ILC08 1 BDS optics and minimal machine study Deepa Angal-Kalinin ASTeC & The Cockcroft Institute Daresbury Laboratory.
1 O. Napoly ECFA-DESY Amsterdam, April 2003 Machine – Detector Interface : what is new since the TDR ? O. Napoly CEA/Saclay.
ILC-GDE Meeting Beijing Feb Effect of MDI Design on BDS Collimation Depth Frank Jackson ASTeC Daresbury Laboratory Cockcroft Institute.
ILC EXTRACTION LINE TRACKING Y. Nosochkov, E. Marin September 10, 2013.
BDS Lattice Design : EDR plans GWP03 Meeting 04/12/2007.
Beam Dynamics IR Stability Issues Glen White / SLAC September IRENG07 Vibration tolerances for final doublet cryomodules Settlement of detector.
COMPENSATION OF DETECTOR SOLENOID FIELD WITH L*=4.1M Glen White, SLAC April 20, 2015 ALCW2015, KEK, Japan.
IWLC10, 18 th -22 nd October10, CERN/CICG 1 Global Design Effort Updates to ILC RDR Beam Delivery System Deepa Angal-Kalinin & James Jones ASTeC, STFC.
BDS/MDI Deepa Angal-Kalinin Andrei Seryi AD&I Meeting, DESY, May 29, 2009.
1 O. Napoly ECFA-DESY Amsterdam, April 2003 Machine – Detector Interface : what is new since the TDR ? O. Napoly CEA/Saclay.
BDS Status Update Glen White, SLAC July ADI Fuze Meeting.
ILC BDS Commissioning Glen White, SLAC AWLC 2014, Fermilab May 14 th 2014.
MAIN DUMP LINE: BEAM LOSS SIMULATIONS WITH THE TDR PARAMETERS Y. Nosochkov E. Marin, G. White (SLAC) LCWS14 Workshop, Belgrade, October 7, 2014.
Design challenges for head-on scheme Deepa Angal-Kalinin Orsay, 19 th October 2006.
The design of the 2mrad extraction line Rob Appleby Daresbury Laboratory On behalf of the SLAC-BNL-UK-France task force ILC European Regional Meeting and.
1 April 1 st, 2003 O. Napoly, ECFA-DESY Amsterdam Design of a new Final Focus System with l* = 4,5 m J. Payet, O. Napoly CEA/Saclay.
JLEIC MDI Update Michael Sullivan Apr 4, 2017.
Collimation Simulations and Optimisation
M. Sullivan International Review Committee November 12-13, 2007
LHeC interaction region
The Interaction Region
Beam-beam effects in eRHIC and MeRHIC
Large Booster and Collider Ring
The small crossing angle layout - where are we and what do we do now?
AD & I : BDS Lattice Design Changes
ILC Baseline BDS Collimation Depth Calculations
Luminosity Optimization at 250GeV
The PEP-II Interaction e+e- Factories Workshop
The 2mrad horizontal crossing angle IR layout for the ILC
Progress of SPPC lattice design
CEPC main ring magnets’ error effect on DA and MDI issues
S.Kuroda ( KEK ) Final Focus Optics Collimeter Final Doublet
Muon Collider Magnet Technologies/Challenges
Muon Collider SR and IR Magnets
Beam-Beam Effects in High-Energy Colliders:
Yuri Nosochkov Yunhai Cai, Fanglei Lin, Vasiliy Morozov
JLEIC Main Parameters with Strong Electron Cooling
G.H. Wei, V.S. Morozov, Fanglei Lin Y. Nosochkov (SLAC), M-H. Wang
ILC Beam Switchyard: Issues and Plans
Fanglei Lin JLEIC R&D Meeting, August 4, 2016
CLIC luminosity monitoring/re-tuning using beamstrahlung ?
Presentation transcript:

Baseline BDS Design Updates Glen White, SLAC Sept. 4, 2014 Ichinoseki, MDI/CFS Meeting

Update of Design SLAC Lattices – Some changes to existing BDS decks Split QF7 for beam profile diagnostics SQFF added u/s SF6 Add 4 skew-sextupoles Move FFB correctors d/s QD0 to between QD0/QF1 to match TDR description – Lattice admin tasks Tidy decks & remove re-definition errors – Lattice description issues LW chicane too long by ~35m? (See MDW talk) Length of BDS used for matching incorrect (historical QF1 position move related) Tune-up dump e- vs. e+ - need DC or pulsed extraction? Length of system… – e+ system needs to match e- BDS optics – Optics matching for baseline L*=3.5 & 4.5m – Collimation design work started for baseline Beam dynamics – Beam losses calculated for baseline & 1TeV optics – Work ongoing for BDS tuning simulations

Lattice Modifications 4 Skew-sextupoles (red) QF7 split (cyan) SQFF (black)

Comments on Optics Matching Bandwidth/tolerances also calculated (see separate talk). Need to fix 1.69m length mismatch to TDR lattice & re-do lattice – QF1 moved in lattice but u/s space not reduced Alternate single-L* optics?

Calculate Collimation Depth to Set Betatron Collimator Apertures SR from particles covering all QF1 phase-space – Rays not hitting apertures shown IP = 14mm (SiD), 16mm (ILD) radius inner vertex detector layer (L=125mm) SiD (L * =3.5m) ILD (L * =4.5m)

3.5m vs. 4.5m L* IR Geometry Difference in detector and extraction system design for 2 IR’s – No simple scaling for collimation depth SiD (L * =3.5m) ILD (L * =4.5m) 6.3m 5.5m

Betatron Spoiler Apertures Nam e L * =3.5mL * =4.5mExisting Lattice X / mm (Nσ x )Y / mm (Nσ y )X / mm (Nσ x )Y / mm (Nσ x )X / mm (Nσ x )Y / mm (Nσ y ) SP (15)0.25 (250) SP (11)0.2 (24)0.3 (2.7)0.2 (24) SP (25)0.22 (219)0.3 (15)0.25 (250) SP (5.4)0.22 (26)0.3 (2.7)0.2 (24) SP (11)0.25 (250) “-” = no collimation needed at this location to prevent IR SR hits. – (L*=3.5m optics completely shielded by magnet apertures) Tightest aperture: SP2/SP4 (X) – 2.7σ = 0.7% Beam loss = 36kW for existing lattice TDR calls for 1-2E-5 main beam loss => 4.3σ tightest collimation aperture. (Max with all muon spoiler space filled = 1E-3 beam loss => 3.3σ) – Tightest L*=4.5m aperture = SP4 = 5.4σ

Summary of extraction loss (baseline 500 GeV Optics) L*=4.5m September 10, 2013 MagnetsDetectorsCollimators SC Warm (max) Synch- rotron Cheren- kov Energy Cheren- kov Dump-1Dump-2Dump-3 TDR W/m30 W130 W22 W0.3 kW2.8 kW1.9 kW3.0 kW Nominal00.6 W/m4 W26 W2 W37 W0.3 kW0.2 kW Low-P0130 W/m0.5 kW0.6 kW0.4 kW2.2 kW14.8 kW9.0 kW10.3 kW Extraction losses with the TDR 2013 IP parameters are a factor of 10 higher than in the RDR 2007 nominal option, but a factor of 5 lower than in the low-P option. The TDR losses on magnets and collimators look acceptable. Losses on the Synchrotron and Cherenkov detectors may need an expert opinion to evaluate the impact of background. The TDR beamstrahlung photon losses are small. Note: The calculations were done assuming ideal collision conditions. Non-ideal conditions, such as large vertical beam-to-beam separation at IP, will increase the disruption and the extraction beam loss. Evaluation of this effect requires a special study.

Summary of beam loss (1 TeV) L*=4.5m 08/25/ Beam loss in option A1 may be manageable (expert opinion is needed). The much higher losses with the y-offset are expected to be only for short periods of time. The IP offsets are expected to be continuously corrected in operation. Beam losses in option B1b are rather high due to the longer beam energy tail and larger angular spread at IP. Of particular concern are the losses on magnets and diagnostic. A better collimation may reduce the losses on magnets and diagnostic. Losses of photons generated in the collision are negligible (compared to electron losses) and limited to two dump collimators. Parameter option MagnetsDetectorsCollimators SC Warm (max per magnet) Synch- rotron Cheren- kov Energy Cheren- kov Dump-1Dump-2Dump-3 A1085 W0.28 kW0.64 kW88 W1.8 kW5.9 kW2.5 kW1.5 kW A1 y-offset0294 W0.56 kW6.3 kW0.9 kW4.0 kW42 kW17 kW11 kW B1b01.6 kW4.0 kW4.6 kW3.5 kW17 kW43 kW18 kW15 kW B1b y-offset01.9 kW3.0 kW37 kW9.8 kW17 kW184 kW56 kW35 kW

Future Work Plan Decision on 1 vs. 2 L* – Decision on L* if single L* Fix lattice irregularities Fine-tune matching Set collimator gaps, calculate beam losses, backgrounds & muon flux Demonstrate BDS tuning and calculate expected luminosities