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MDI Planning for ILC (What should we do if Project Approval & Funding occur?) MDI Planning for ILC (What should we do if Project Approval & Funding occur?)

MDI Planning for ILC (What should we do if Project Approval & Funding occur?) - PowerPoint Presentation

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MDI Planning for ILC (What should we do if Project Approval & Funding occur?) - PPT Presentation

T MarkiewiczSLAC Snowmass 2021 Community Planning Mtg 20201006 2 Preparing for the Preparatory Phase of ILC List the fundamental shared MDI design choices made in the long process of bringing the ILC to a reality ID: 930891

ilc amp markiewicz mdi amp ilc mdi markiewicz 2021 cpm detector design snowmass beam crossing degrees energy angle line

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Slide1

MDI Planning for ILC(What should we do if Project Approval & Funding occur?)

T. Markiewicz/SLAC

Snowmass 2021 Community Planning Mtg.

2020-10-06

Slide2

2

Preparing for the Preparatory Phase of ILC

List the fundamental shared MDI design choices made in the long process of bringing the ILC to a reality

What was chosen and why

There IS a complete solution: see RDR & TDR & Detector BaselinesWhich choices, if any, should be re-evaluatedThis partly so that the next generation who will see the project to completion “own” those choicesWhich choices have been so “baked-into” the design that they should not be questionedDocumentation for choices made tends to be scattered over time & spaceList MDI Engineering Issues and R&D required before construction begins

Snowmass 2021 CPM-Markiewicz-MDI at ILC

Slide3

3

List of Issues usually part of “MDI” Discussions

Understanding/Mitigating Beam-Beam Backgrounds

Proportional to Luminosity; Function of IP beam parameters

Guinea Pig & CAIN generators calculate pairs & disrupted beamEstimating Mitigating Machine Related BackgroundsSynchrotron Radiation from bendsMuons from collimation systemBackscattered neutrons from the beam dumpMaximizing Luminosity and AcceptanceFinal Doublet Position Stability, Physical Size, Energy FlexibilitySlow and Very Fast FeedbackPrecision Luminosity, Energy & Polarization MeasurementsOptimization for performance, cost, etc.Mechanical Issues Arising from 2-Detector Hypothesis, Detector Assembly & ShieldingTechnical R&D on Final Doublet, Crab Cavity, BeamCal

,…

Snowmass 2021 CPM-Markiewicz-MDI at ILC

Slide4

4

Pair Background Calculations

Snowmass 2021 CPM-Markiewicz-MDI at ILC

Slide5

5

Engineering & Integration of the R<=25cm region

Snowmass 2021 CPM-Markiewicz-MDI at ILC

Slide6

6

List of Design Choices

Crossing Angle

L*

Common L*QD0 TechnologyExtraction line chicaneIncoming line polarimeterMuon Walls and BackgroundsSelf-ShieldingAnti-Detector-Integrated-DipoleOne or Two DetectorsPlatform Under the Detector, or notUnderground versus Above Ground AssemblyMagnetic Fringe Field RequirementsSnowmass 2021 CPM-Markiewicz-MDI at ILC

Slide7

7

Crossing Angle

History

0 degrees TESLA

2 degrees 30 degrees Gamma-Gamma compatible20 degrees CLIC compatible14 degrees Current ILC14 degrees chosen for ILC as it is thought to be the smallest crossing angle compatible with a minimum radius (30cm) compact SC Final Focus Cryostat housing both incoming and extraction QD and QF quadsCouples to L* choiceAssumed to minimize risk associated with crab cavityAssumed that package would be mounted in endcap and of minimal diameter to maximize detector acceptance

Snowmass 2021 CPM-Markiewicz-MDI at ILC

Slide8

8

L*

Current compromise value of 4.1m

Naïve assumption that smaller L* maximizes luminosity

Not necessarily born out by detailed studies where control of higher order optical effects dominate spot size3.5m was consistent with smallest 14mrad crossing angle and compact SC technology developed by Parker at BNL4.5m advocated for ILD with TPCCLIC studies show no loss of luminosity at larger L*Mounting QD0 outside detector simplifies detector swapManagement decision (Walker, ~2014) to have common L*Snowmass 2021 CPM-Markiewicz-MDI at ILC

Slide9

9

QD0 Technology

Direct wind compact SC magnets developed by Brett Parker at BNL

Introduced to LC Community at Snowmass 2005

Used at HERA , KEK and ??ILC prototype begun but not completed due to funding issuesConcerns about vibration due to fluidOther technologies researched by CLICSnowmass 2021 CPM-Markiewicz-MDI at ILC

Slide10

10

Extraction Line Chicane for Polarimeter & Energy Spectrometer

Pros

Advocated by SLC experience

Measures beam after beam-beam interaction has occurredConsLarge aperture dipoles with large power requirementsRadiation shielding required to handle off-energy disrupted beamIncreased size of dump windowSuperfluous according to advocates of Energy/Polarization in incoming beamline

Snowmass 2021 CPM-Markiewicz-MDI at ILC

Slide11

11

Incoming Polarimeter & Energy Spectrometer

Pros

Cleaner measurements made on non-disrupted beam

Advocated by proponents coming from 0 crossing angle TESLA designConsBeam line lengthSuperfluous if you believe advocates of extraction line solutionSnowmass 2021 CPM-Markiewicz-MDI at ILC

Slide12

12

Muon Walls and Backgrounds

Historic SLC experience that muons can be a problem

Gaseous tracking chambers more sensitive

Design & leave space in tunnel but do not implement at t=0ExpensiveSnowmass 2021 CPM-Markiewicz-MDI at ILC

Slide13

13

Self-Shielded Detectors

Probably required in any model where a “garaged” detector is being worked on while 2

nd

detector is taking dataBaked into design in 2-Detector push/pull modelToo long to demountStrong push from SLD people as SLC design had shallow tunnelMay be somewhat similar situation to the “2-tunnel” original ILC design or the Kamaboko tunnel with thick shielding wall“No access during beam operation” is current modelSnowmass 2021 CPM-Markiewicz-MDI at ILC

Slide14

14

Anti-Detector-Integrated-Dipole

“DID” conceived to improve beam spot by cancelling transverse component of solenoid due to crossing angle

Can be done in other ways (QD0 offsets)

Realized “Anti-DID” will direct soft pairs from r=0 where they hit BeamCal & splatter to extraction lineProbably a detector risk/benefit choiceSnowmass 2021 CPM-Markiewicz-MDI at ILC

Slide15

15

One or Two Detectors

Much less expensive, simplified IR design if powers that be descope to one detector

Snowmass 2021 CPM-Markiewicz-MDI at ILC

Slide16

16

Platform

Underground versus Above Ground Assembly

Motivated by CMS experience and CMS-like nature of ILD design

Above vs. Below ground motivated by “timing” arguments that may need to be re-evaluated once funding profiles for ILC construction are knownSnowmass 2021 CPM-Markiewicz-MDI at ILC

Slide17

17

Scope of R&D

Crab Cavity

EM design

Warm & Cold prototypesLLRF system with adequate phase jitterQD0Complete QD0 prototypePrototype with incoming & extraction line quads & all windingsField measurementsVibration measurementsVibration & Vibration Suppression

Design & prototype Mover system with Feedback

SC Cable Design

SiD and ILD based on 25-year-old CMS cable design

He Distribution

The He II system from the 4k cold box to the FFS is not trivial and should be identical for the two detectors.

A  joint R&D opportunity, which very likely is tied to the one for QD0.

Snowmass 2021 CPM-Markiewicz-MDI at ILC

Slide18

18

Scope of R&D

Feedback (FONT-Feedback on Nanosecond Timescale)

Spot Size (ATF2 at KEK)

DiagnosticsPolarimetersEnergy SpectrometersCollimators & Dumps: Probably beyond scope of MDISnowmass 2021 CPM-Markiewicz-MDI at ILC