si d in 14mrad/14mrad/z=0 ilc t. markiewicz/slac sid advisory group 14 august 2006

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Si D in 14mrad/14mrad/z=0 ILC T. Markiewicz/SLAC SiD Advisory Group 14 August 2006

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Page 1: Si D in 14mrad/14mrad/z=0 ILC T. Markiewicz/SLAC SiD Advisory Group 14 August 2006

Si D in 14mrad/14mrad/z=0 ILC T. Markiewicz/SLAC

SiD Advisory Group

14 August 2006

Page 2: Si D in 14mrad/14mrad/z=0 ILC T. Markiewicz/SLAC SiD Advisory Group 14 August 2006

Tom Markiewicz2 / 18

Change Requested

• Current– 2mrad/20mrad layout with IPs separated by x=21m,

z=138m– Linacs point at 20mrad IP– Soft bend to 2mrad IP

• Request– 14mrad/14mrad layout with IPs separated by x=28m,z=0– Linacs point at one of the 14mrad IPs– Soft bend to the other

Page 3: Si D in 14mrad/14mrad/z=0 ILC T. Markiewicz/SLAC SiD Advisory Group 14 August 2006

Tom Markiewicz3 / 18

Crossing Angle

• 20mrad14mrad is good for e+e- in every respect– upgrade to >=25mrad will require digging new extraction line tunnels

• Arguments surrounding low (0,2) vs high (14,20,25) are well documented– Low Crossing Angle

• Increased hermiticity at low angles– SUSY search for stau will low m

• Lower (x2) backgrounds from backscattered e+e- beamstrahlung-produced pairs• Larger aperture magnets and required to support diagnostic chicanes lead to

62MW power req.• Separate photon dump and high power (>250kW, depending on parameter set)

collimators required• Longer extraction line• Crab cavity not essential

– High Crossing Angle• Cleaner extraction, especially at higher energy, higher disruption beam

parameters with modest magnets, minimal collimation, & shorter beamlines• Cleaner measurements of Energy and Polarization of disrupted beam• Crab cavity essential• DID desirable for polarization compensation & orbit correction, (anti-DID) for

directing e+e- to exit aperture to avoid backscattered e+e- debris– Symmetric 14/14 vs. low/high

• Matter of taste• Increased emittance dilution at IP protected by the 14 mrad “Big Bend”

Page 4: Si D in 14mrad/14mrad/z=0 ILC T. Markiewicz/SLAC SiD Advisory Group 14 August 2006

Tom Markiewicz4 / 18

IPs at a Common z

Advantages– Remove “Stretch” in linac introduced to accommodate timing

constraints required by z=138m

– PRESUMED cost savings due to shared facilities

Disadvantages– Interference between detector construction, installation, operations

and maintenance

Confusions– CURRENT Baseline not well described to detector community

• Underground hall designs are regional (and therefore different)

• Above ground cost model is CMS at LHC

– No design of common z halls & structures available yet

– Future change request to mandate CMS style above ground assemble has been advertised

Page 5: Si D in 14mrad/14mrad/z=0 ILC T. Markiewicz/SLAC SiD Advisory Group 14 August 2006

Tom Markiewicz5 / 18

2005.10.11 Discussion of Si D Underground Hall Space Requirements shown 2005-12-16

Talk at Si D Collaboration Meeting

• SiD Dimensions from 2005-05 files– Barrel radius=6.450m

– Barrel half-length=2.775m

– EC Yoke=3.12m thick

– EC Yoke ends at 5.895m=2.775+3.120m

• Garage assembly requirements– 3m shielding wall between beamline position & garage

• Assuming self-shielding [which seems OK: see L. Keller, 2005.12.13 SLAC BDS mtg.] wall needed for commissioning only

– 5m free space between shield wall & rotated barrel yoke3

• 2m free + 2m assembly fixture+1m free

– 4m free space between rotated barrel yoke & rotated barrel HCAL

• 1m free + 2m assembly fixture+1m free

– 5m free space between rotated barrel HCAL & pit wall

• 2m free + 2m assembly fixture+1m free

Page 6: Si D in 14mrad/14mrad/z=0 ILC T. Markiewicz/SLAC SiD Advisory Group 14 August 2006

Tom Markiewicz6 / 18

Detector Access Guesstimates

• Door support leg overhang=– 3.2m~25% door height (=barrel diameter=12.9m)

• Door opening=– 3.0m

• Free space to walk around door ends=– 1.9m

• Reserved radius = – 8.0m (6.45 iron +1.55m services)

• Free space between dressed barrel & pit walls=– 2.0m

• PACMAN annulus=– 3.0m [1m Fe, 2m concrete]

• Other– Tunnel diameter 3.2m– Assumed beam height=Barrel radius + 1m

Page 7: Si D in 14mrad/14mrad/z=0 ILC T. Markiewicz/SLAC SiD Advisory Group 14 August 2006

Tom Markiewicz7 / 18

-10

-8

-6

-4

-2

0

2

4

6

8

10

0 2 4 6 8 10 12 14 16

SiD closed, on beamline, in 20m x 28m

3.0 m

Foot

Foot

Mobile PAC1

Fixed PAC2

5.105 m

Pit Wall

Tunnel

Shield Wall

Door

Barrel

Page 8: Si D in 14mrad/14mrad/z=0 ILC T. Markiewicz/SLAC SiD Advisory Group 14 August 2006

Tom Markiewicz8 / 18

Half SiD in 48m x 28m IRanamorphic scale

-40

-35

-30

-25

-20

-15

-10

-5

0

5

10

0 2 4 6 8 10 12 14 16

5.00 m

6.45 m

6.45 m

3.00 m

4.00 m

5.00 m

Barrel Yokerotated

HCALrotated

Shield Wall

Page 9: Si D in 14mrad/14mrad/z=0 ILC T. Markiewicz/SLAC SiD Advisory Group 14 August 2006

Tom Markiewicz9 / 18

SiD (open) in 48m x 18m IRX scale = y scale

-40 -35 -30 -25 -20 -15 -10 -5 0 5 10

01

23

45

67

89

10

Page 10: Si D in 14mrad/14mrad/z=0 ILC T. Markiewicz/SLAC SiD Advisory Group 14 August 2006

Tom Markiewicz10 / 18

GLD

14.9x14.0x14.0 m3 in 32m (z) x 72m (x) x 40m (y) cavern with 15m ϕ access shaft

Assembly from “bottoms-up” in “garage”

Repair access by transverse door motion

TPC slides along beam line to access VXD

Page 11: Si D in 14mrad/14mrad/z=0 ILC T. Markiewicz/SLAC SiD Advisory Group 14 August 2006

Tom Markiewicz11 / 18

Americas CF&S conceptual layout

Page 12: Si D in 14mrad/14mrad/z=0 ILC T. Markiewicz/SLAC SiD Advisory Group 14 August 2006

Tom Markiewicz12 / 18

Americas CF&S conceptual layout

Page 13: Si D in 14mrad/14mrad/z=0 ILC T. Markiewicz/SLAC SiD Advisory Group 14 August 2006

Tom Markiewicz13 / 18

Americas CF&S conceptual layout

Page 14: Si D in 14mrad/14mrad/z=0 ILC T. Markiewicz/SLAC SiD Advisory Group 14 August 2006

Tom Markiewicz14 / 18

Americas CF&S conceptual layout

Page 15: Si D in 14mrad/14mrad/z=0 ILC T. Markiewicz/SLAC SiD Advisory Group 14 August 2006

Tom Markiewicz15 / 18

CERN Underground Cavern Scheme

Page 16: Si D in 14mrad/14mrad/z=0 ILC T. Markiewicz/SLAC SiD Advisory Group 14 August 2006

Tom Markiewicz16 / 18

Above Ground Footprints

Baseline: Footprint Aboveground equals

footprint belowground

This Change Request: Double Up

Assembly Hall

Extension

15m shaft

~5m shielding

Page 17: Si D in 14mrad/14mrad/z=0 ILC T. Markiewicz/SLAC SiD Advisory Group 14 August 2006

Tom Markiewicz17 / 18

Comments to Si D Exec regarding reply to WWS on 14mr/14mr/z=0 Baseline Change

Request• By allowing CF&S to cost 32x72x40m caverns high cost

was guaranteed• By designing 2mrad magnets for 1 TeV high disruption

beam parameters WITH diagnostic chicanes high power dipoles were guaranteed

• Reducing either of these design constraints and keeping 2mrad would also be a possibility

• Nontheless, from an SLC experience point of view, 14mrad should result in a more robust and cost effective machine

• I would recommend supporting the 14/14mr part of the CR• The experimental community has NOT been told exactly

what is in/not in the design so it is hard to comment quantitatively on z=0 part of CR. Nonetheless you are meant to think that, relative to baseline, you will not lose anything at this stage, so why not.– Next CR regarding CMS style installation and any efforts to

reduce costs by sharing facilities between detectors needs to be looked at.