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Linear Collider AD&I Update

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Linear Collider AD&I Update. N. Walker, E. Paterson, V Kuchler, T. Lackowski, J. A. Osbourne,J . Clarke, A. Wolski, S. Guiducci, N. Solyak,…. 30/08/2009. Norbert Collomb. Linear Collider – AD&I. During the last 2 - 3 WebEx meetings an apparent discrepancy has been noted. - PowerPoint PPT Presentation
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Linear Collider AD&I Update N. Walker, E. Paterson, V Kuchler, T. Lackowski, J. A. Osbourne,J. Clarke, A. Wolski, S. Guiducci, N. Solyak,… Norbert Collomb 30/08/20 09
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Page 1: Linear  Collider AD&I  Update

Linear Collider AD&I Update

N. Walker, E. Paterson, V Kuchler, T. Lackowski, J. A. Osbourne,J. Clarke, A. Wolski, S. Guiducci, N.

Solyak,…

Norbert Collomb30/08/2009

Page 2: Linear  Collider AD&I  Update

30/08/2009

N.Collomb 2

Linear Collider – AD&I

During the last 2 - 3 WebEx meetings an apparent discrepancy has been noted.

The location of the Damping Ring has been shown in two different locations.

Location 1: (work done by U.K. Sources and Damping Ring) places the Damping Rings ’inside’ the ‘V’ shape of the Positron and Electron beam.

Location 2: (work done by CERN/FNAL) places the Damping Rings ‘outside’ the ‘V’ shape of the Positron and Electron beam.

We are at a stage where a decision needs to made in order to feed this info back to N. Solyak to commence work on the RTML.

Page 3: Linear  Collider AD&I  Update

30/08/2009

N.Collomb 3

Linear Collider – Positron Source

-1500 -1000 -500 0 500 1000 15000

200

400

600

800

1000

1200

1400

1600

BDS - RDR Layoutebds1-EBSY1

ebds0-EBDSD

edbs1-EBSY2

ebds1-EFF1

ebsy1-EDL1

pbds1-PBSY1

pbds0-PBSYD

pbds1-PBSY2

pbds1-PFF1

pbds1-PDL1

6.4km Damping RingZ - Axis (m)

X -

Axi

s (m

)

-800.00 -600.00 -400.00 -200.00 0.00 200.00 400.00 600.00 800.00-10.00

0.00

10.00

20.00

30.00

40.00

50.00

60.00

Detail around I.P.

DR Extract Right

DR Extract Left

BDS e- side

BDS e+ side

Z - Axis (m)

X -

Axi

s (m

)

‘U.K.’ AD&I machine layout (I.P. at X:0, Y:0)

Electron Main DumpPositron Main Dump

Page 4: Linear  Collider AD&I  Update

30/08/2009

N.Collomb 4

Linear Collider – AD&I

-1500 -1000 -500 0 500 1000 1500

-1600

-1400

-1200

-1000

-800

-600

-400

-200

0

BDS - RDR Layoutebds1-EBSY1

ebds0-EBDSD

edbs1-EBSY2

ebds1-EFF1

ebsy1-EDL1

pbds1-PBSY1

pbds0-PBSYD

pbds1-PBSY2

pbds1-PFF1

pbds1-PDL1

6.4km Damping Ring (CERN)

Z - Axis (m)

X -

Axi

s (m

)

‘CERN/FNAL’ AD&I machine layout (I.P. at X:0, Y:0)

-800.00 -600.00 -400.00 -200.00 0.00 200.00 400.00 600.00 800.00

-60.00

-50.00

-40.00

-30.00

-20.00

-10.00

0.00

10.00

Detail around I.P.

DR Extract_Right

DR Extract_Left

BDS e- side

BDS e+ side

Z - Axis (m)

X -

Axi

s (m

)

Electron Main DumpPositron Main Dump

Page 5: Linear  Collider AD&I  Update

30/08/2009

N.Collomb 5

Linear Collider – AD&I

Both have advantages and disadvantages concerning the physics and physical aspects.

U.K. modelAdvantages:- Short tunnels,- Share shafts (D.R. + Target Hall, Interaction Point),- Inside ‘V’ shape to avoid any possible radiation from Main Dumps,- Simpler Physics and room for RTML components.Disadvantages:- Service tunnel around Target Hall interference,- To avoid interference, D.R. offset needs to increase to approx. 65m

instead the current 50m,- ‘S’ shape of beam more distinct (larger angles)?

Page 6: Linear  Collider AD&I  Update

30/08/2009

N.Collomb 6

Linear Collider – AD&I

CERN/FNAL model

Advantages:- Shallow ‘S’ shape beam can be achieved,- Target Hall design can remain as is,- Offset can remain at 50m,- Service Tunnel does not have to come ‘up and over’.

Disadvantages:- Longer Tunnels and more of them,- More shafts required,- Complexity increases for beam line,- Radiation risk from Main Beam Dumps(crossover?),- Eliminates option to combine BDS Dumps?

Page 7: Linear  Collider AD&I  Update

30/08/2009

N.Collomb 7

Linear Collider – AD&I

Can we make a decision soon as to the side of the Damping Ring.

Since we are assembled here, we can investigate the physical aspects.

The work done by Tom (see next slide) is of great help in determining the Physical constraints.

N. Solyak can aid in the decision for Physics reasons.

Also noted was the inversion of the ‘V’ on drawings (T. Lackowski). Although not detrimental at this stage, HOWEVER bad habits tend to stick and lead to confusion later on. Please inform and update Tom about this.

Page 8: Linear  Collider AD&I  Update

30/08/2009

N.Collomb 8

Linear Collider – AD&I

Tom’s LayoutIncorrect Information.Discuss lengths, position of systems and quantity.

Update required.Discuss spatial requirements on info available.

Page 9: Linear  Collider AD&I  Update

30/08/2009

N.Collomb 9

Linear Collider – AD&I

I love this sketch!It helps immensely when explaining the basics of the ILC.Thank you Tom.

Page 10: Linear  Collider AD&I  Update

J.Osborne CERN

1000m?

Next Slide

Page 11: Linear  Collider AD&I  Update

30/08/2009

N.Collomb 11

Linear Collider – AD&I

2 D Layout for Option1 Positron Source region.

Positron Source length currently at approx. 920m.

Booster length fixed.Position relative to Positron Source can vary in steps of 16.8m either direction.

BDS Chicane, Collimation and Fast Abort Extraction (350m).

Converting this 2 D data into 3 D has taken place as depicted in the following slides.

Page 12: Linear  Collider AD&I  Update

30/08/2009

N.Collomb 12

Linear Collider – AD&I

3 D Overall Layout for Option1 Positron Source region.

Spin Rotation added in the last few days. Some guesswork to be confirmed via lattice design Booster

Option 1:BDS Chicane + Collimation + Fast Abort

AUX Source added recently.Some guesswork to be confirmed via lattice design.Area of optimisation!

Page 13: Linear  Collider AD&I  Update

30/08/2009

N.Collomb 13

Linear Collider – AD&I

3 D Layout Positron Source BDS Fast Abort region.

Kicker Magnets

Quadrupole,Sextupole and Dipole Magnets

BDS Chicane + Collimators

11 MW?? Dump

RTML

Undulator Section(20 off 1 off Quad + 3 SC Undulators = 302m)

Pre – Undulator Quads (48m)

I.P. Direction

Page 14: Linear  Collider AD&I  Update

30/08/2009

N.Collomb 14

Linear Collider – AD&I3 D Layout Positron Source BDS Fast Abort region.

Is an Alcove like this feasible?(9.5° off axis)

Sufficient clearance between Fast Abort Magnets and Undulator Modules

Interleaved Fast Abort and Undulator Magnets

RTML

I.P. Direction

I.P. Direction

Page 15: Linear  Collider AD&I  Update

30/08/2009

N.Collomb 15

Linear Collider – AD&I

3 D Layout Positron Source ‘BDS Dogleg’ region.

AUX Source

BDS ‘Dogleg’1.5m ML-Axis offset

RTML

40m Drift to clear Remote Handling and Dump shielding

I.P. Direction

Page 16: Linear  Collider AD&I  Update

30/08/2009

N.Collomb 16

Linear Collider – AD&I

3 D Layout Positron Source ‘AUX Source’ region.

Thermionic Gun, Bunchers,Diagnostics, 2 off Standing Wave Accelerators (12 MeV/m),Diagnostic Section and Tune-Up Dumps.

Tune-Up Dump and Diagnostics Section

2 off Cryomodules at 12.6m with Quad, in Line with Photon Beam, approx. 30MeV/m

Photon Beam Pipe

BDS ‘Dogleg’

RTML

Remote Handling

I.P. Direction

Page 17: Linear  Collider AD&I  Update

30/08/2009

N.Collomb 17

Linear Collider – AD&I3 D Layout Positron Source ‘Target Area’.

Capture Chicane

Pre-Acceleration moved downstream. On ML-Axis.

Remote Handling (R. H.)(Vertical Extraction)

I.P. Direction

RTML clears R.H. ‘Box’

R.H. Extraction Shaft?

BDS ‘Dogleg’

Page 18: Linear  Collider AD&I  Update

30/08/2009

N.Collomb 18

Linear Collider – AD&I

3 D Layout Positron Source ‘Spin Rotation’ region.

Spin RotationPositron Transfer start

Pre – Accelerator (to 400 MeV).

Page 19: Linear  Collider AD&I  Update

30/08/2009

N.Collomb 19

Linear Collider – AD&I

3 D Layout for Positron Source ‘Booster region’.

Booster Endbox

1st of 2 Booster periods (141.6m).11 off Cryomodules at 12.6m length + 1 off Endbox (2.5m).

PTRAN end

Page 20: Linear  Collider AD&I  Update

30/08/2009

N.Collomb 20

Linear Collider – AD&I

The Positron Source overall layout can be considered complete (Booster Position and remaining Positron Transfer will require update).

The purpose of this meeting is to update all relevant Workgroups and discuss feasibility of proposal.

CAD models can be distributed now or after update.

Based on the above discussions, new or modified layout needs to be created.

Note, certain system lengths (Cryomodules) and positions ought to be near a sufficiently large access shaft.

Remote Handling change over process and space requirement investigation/development is high on priority list.

Individual systems need to be developed further (are we at a stage where we can go into more detail?)

Summary

Page 21: Linear  Collider AD&I  Update

AD&I e+ layout Option2

Pro

pose

d Fa

st A

bort

Lay

out

(Fea

sibi

lity

Inve

stig

atio

n in

prog

ress

)

Need to check Remote Handling Area for clearance.Can RTML magnets and abort beam line magnets coexist in close proximity?

Preliminary Beam Studies (Deepa and James) indicate that this solution may increase length of machine by approx. 300m.This solution could further increase cost in terms of equipment required (virtually duplicating part of the BDS).Maintenance cost will increase the running cost of the ILC.Starting to look expensive.

250 GeV Beam from Main Linac to be taken to ceiling (diagonally up and towards I.P).Lattice design is complex and Beam acceptance is governing this.Installation and maintenance could be difficult!!

Plenty of room for access (cautious maybe)0.8m Approx. 2m

Approx. 1.8m

Last not least for the observant, there is an Option2 currently under investigation. This where the Fast Abort is taken downstream to the original location (approximately) to combine it with the Diagnostics Dump.

30/08/2009 21

Page 22: Linear  Collider AD&I  Update

03/09/2009 N.Collomb22

Linear Collider – AD&I

Discussion details (refer to slide number):

The Damping Rings are on the opposite side as the Main Beam Dumps (slide 3).

The orientation of the Main Linac has been clarified by Nick Walker (misconception to RDR Fig. 2.3-2).

The I.P. is the Datum. The ‘Z – Axis’ points to the ‘right’ and the ‘X – Axis’ to the top in the Plan View (as was). See sketch 1 below.

The Lattice files do NOT have a rotation. The person converting the data into Excel format for engineering purposes must adopt the convention as follows:The Main Linac angle has been defined with a –ve 7 mrad to the horizontal Z-Axis giving a crossing angle of 14 mrad.

Discussion Summary

I.P.

+ve Z-Axis

+ve X-Axis

+ve Y-AxisComing out of Page

Sketch 1

E- Main Linac

E+ Main Linac

Z-Axis

X-Axis

I.P.

14 mrad-ve 7 mrad

Main Dumps

Page 23: Linear  Collider AD&I  Update

03/09/2009

N.Collomb 23

Linear Collider – AD&IDiscussion Summary

E+ Main LinacE- M

ain Linac

Z-Axis

X-Axis

I.P.

14 mrad +ve 7 mrad

E+ Wiggler E- Wiggler

E+ RF Modules

E- RF Modules

RF Cavern

Target Hall

E+ Injection E+ Extraction

50m???

Target Hall Annex??

NOT TO SCALE

Option 1 adopted


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