Beam Delivery System: status and plans of R&D until CDR R. Tom - - PowerPoint PPT Presentation

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Beam Delivery System: status and plans of R&D until CDR R. Tom - - PowerPoint PPT Presentation

Beam Delivery System: status and plans of R&D until CDR R. Tom as, D. Angal-Kalinin, B. Dalena, L. Fernandez, F . Jackson, J. Resta, G. Rumolo, A. Seryi, P . Schuler and D. Schulte CLIC ACE 2009 Rogelio Tom as Garc a Beam


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SLIDE 1

Beam Delivery System: status and plans of R&D until CDR

  • R. Tom´

as, D. Angal-Kalinin, B. Dalena,

  • L. Fernandez, F

. Jackson, J. Resta, G. Rumolo,

  • A. Seryi, P

. Schuler and D. Schulte CLIC ACE 2009

Rogelio Tom´ as Garc´ ıa Beam Delivery System: status and plans of R&D until CDR – p.1/23

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SLIDE 2

Contents

  • New instrumentation: The polarimeter
  • Preservation of emittances:
  • Transport aberrations
  • Failure to tune the FFS
  • .
  • ATF2
  • Collective effects

   Resistive wall Fast ion instability Collimator wakefields

  • Machine protection:
  • Collimation systemm
  • Plans towards CDR

Rogelio Tom´ as Garc´ ıa Beam Delivery System: status and plans of R&D until CDR – p.2/23

slide-3
SLIDE 3

Contents

  • New instrumentation: The polarimeter
  • Preservation of emittances:
  • Transport aberrations
  • Failure to tune the FFS
  • ′′
  • ATF2
  • Collective effects

   Resistive wall Fast ion instability Collimator wakefields

  • Machine protection:
  • Collimation systemm
  • Plans towards CDR

Rogelio Tom´ as Garc´ ıa Beam Delivery System: status and plans of R&D until CDR – p.2/23

slide-4
SLIDE 4

Contents

  • New instrumentation: The polarimeter
  • Preservation of emittances:
  • Transport aberrations
  • Failure to tune the FFS
  • ′′
  • ATF2
  • Collective effects

   Resistive wall Fast ion instability Collimator wakefields

  • Machine protection:
  • Collimation systemm
  • Plans towards CDR

Rogelio Tom´ as Garc´ ıa Beam Delivery System: status and plans of R&D until CDR – p.2/23

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SLIDE 5

The BDS

100 200 300 400 500 600 0.5 1 1.5 2 2.5 3

  • 0.05

0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 β1/2 [m1/2] D [m] Longitudinal location [km] Diagnostics Energy collimation Transverse collimation Final Focus system βx

1/2

βy

1/2

Dx

Rogelio Tom´ as Garc´ ıa Beam Delivery System: status and plans of R&D until CDR – p.3/23

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SLIDE 6

Polarimeter location & performance

  • 2
  • 1.5
  • 1
  • 0.5

0.5 500 1000 1500 2000 2500 3000 x[m] Longitudinal location [m] BDS layout IP directions (0.6mrad)

Laser IP at 742 m and detector at 907 m. Relative polarization measurement error is 0.61% (for 1s).

Rogelio Tom´ as Garc´ ıa Beam Delivery System: status and plans of R&D until CDR – p.4/23

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SLIDE 7

BDS emittance “spoilers” by design

  • CLIC BDS transport aberrations have been

extensively minimized (MAPCLASS, extra non-linear elements, etc)

  • Aberrations increase vertical IP beam size by

15%

  • Synchrotron radiation reduces luminosity by

20%

  • (in ILC these effects are below the 1%)

Rogelio Tom´ as Garc´ ıa Beam Delivery System: status and plans of R&D until CDR – p.5/23

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SLIDE 8

Vertical IP beam sizes and chromaticities

Project Status σ∗

y [nm]

ξy FFTB Measured 70 17000 ATF2 Commissioning 37 19000 ILC Design 6 15000 ILC low power Proposed 4 30000 CLIC Design 1 63000 CLIC, the most challenging.

Rogelio Tom´ as Garc´ ıa Beam Delivery System: status and plans of R&D until CDR – p.6/23

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SLIDE 9

Imperfections as emittance “spoilers”

  • 10µm transverse misalignments can

decrease lumi by 10−6

  • 10−5 relative gradient error in QD0

decreases lumi by 0.94

  • Tuning algorithms are fundamental!
  • Can we tune the FFS using the Simplex to

maximize lumi?

Rogelio Tom´ as Garc´ ıa Beam Delivery System: status and plans of R&D until CDR – p.7/23

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SLIDE 10

Current status of FFS tuning

2 4 6 8 10 12 14 0.6 0.8 1 1.2 Counts Relative final luminosity [L0]

Pre-alignment is 10µm 80% of the cases reach 80% of the lumi in 18000 iterations.

Rogelio Tom´ as Garc´ ıa Beam Delivery System: status and plans of R&D until CDR – p.8/23

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SLIDE 11

How to improve tuning performance?

  • Use of more clever algorithms than the

Simplex (presently on-going)

  • Tune in a beta-squeeze sequence (like

colliders)

  • Relax the optics
  • Andrei Seryi proposed a new optics with

double L* to ease QD0 stabilization, let’s see what happens

Rogelio Tom´ as Garc´ ıa Beam Delivery System: status and plans of R&D until CDR – p.9/23

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SLIDE 12

Comparing Andrei’s FFS to CLIC nominal

100 200 300 400 500 600 700 800 900 100 200 300 400 500 600 700 800 βy [km] Longitudinal location [m] Andrei’s proposal CLIC nominal

Andrei’s prop: L*=8.0m, β∗

y=0.10mm

CLIC nominal: L*=3.5m, β∗

y=0.07mm

Rogelio Tom´ as Garc´ ıa Beam Delivery System: status and plans of R&D until CDR – p.10/23

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SLIDE 13

Sensitivity to misalignments

10-12 10-10 10-8 10-6 10-4 10-2 100 2 4 6 8 10 Relative luminosity (L/L0) Transverse misalignments (σx,y) [µm] L*=3.5m L*=8.0m

Doubling L* increases sensitivity to misalign- ments by a factor of 4

Rogelio Tom´ as Garc´ ıa Beam Delivery System: status and plans of R&D until CDR – p.11/23

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SLIDE 14

Sensitivity to QD0 gradient error

0.9 0.92 0.94 0.96 0.98 1 1.02

  • 0.15
  • 0.1
  • 0.05

0.05 0.1 0.15 Luminosity (L/L0) QD0 relative gradient error [10-4] 0.05 0.03 L*=8.0m L*=3.5m fits

Doubling L* increases sensitivity to gradient error by a factor of 2

Rogelio Tom´ as Garc´ ıa Beam Delivery System: status and plans of R&D until CDR – p.12/23

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SLIDE 15

QD0 specifications

L*=3.5m L*=8.0m Gradient 575T/m 211T/m Aperture (radius) 3.5mm 8.5mm Outer radius 35mm 70mm QD0 jitter 0.15nm 0.18nm QD0 support detector ground QD0 technology PM PM QD0 grad tol. 5×10−6 3×10−6 A superconducting QD0 adds the extra challenge

  • f stabilizing coils.

Rogelio Tom´ as Garc´ ıa Beam Delivery System: status and plans of R&D until CDR – p.13/23

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SLIDE 16

Tuning longer L* with better pre-alignment

2 4 6 8 10 12 14 16 18 0.5 0.6 0.7 0.8 0.9 1 Counts Relative final luminosity L/L0

Pre-alignment is 2µm Same tuning performance as for nominal by re- ducing pre-alignment a factor 5

Rogelio Tom´ as Garc´ ıa Beam Delivery System: status and plans of R&D until CDR – p.14/23

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SLIDE 17

ATF2 ultra-low β proposal

  • CARE/ELAN-2008-002 proposed a squeeze
  • f the ATF2 IP β-functions by a factor of 4
  • σy ≈20 nm, ξy ≈76000
  • ATF2 ultra-low β will experimentally prove

CLIC-like aberrations and tuning algorithms.

  • Beneficial for the ILC project, more in

particular for the ILC low power option.

  • This proposal was accepted
  • Presently a CERN PhD working on this

Rogelio Tom´ as Garc´ ıa Beam Delivery System: status and plans of R&D until CDR – p.15/23

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SLIDE 18

Collective effects: Resistive wall

  • 25
  • 20
  • 15
  • 10
  • 5

5 10 15 20 25 0.5 1 1.5 2 2.5 3 Last bunch vertical excursion [µm] Longitudinal location [km] Resistive wall effect (Cu beam pipe) Initial batch offset=0.2µm radius=2mm radius=3mm radius=4mm radius=6mm

8mm Cu beam-pipe is enough to neglect resistive

  • wall. Only QD0 has a smaller aperture.

Rogelio Tom´ as Garc´ ıa Beam Delivery System: status and plans of R&D until CDR – p.16/23

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SLIDE 19

Collective effects: Fast ion

Two sources:

  • Scattering ionization
  • Field ionization

10 nTorr seem enough to avoid fast ion instabili- ties.

Rogelio Tom´ as Garc´ ıa Beam Delivery System: status and plans of R&D until CDR – p.17/23

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SLIDE 20

Collective effects: Collimator wakefields

5 10 15 20 25 0.05 0.1 0.15 0.2 0.25 ∆L/L0 coll wakefield no coll wakefield

10σx,44σy Assuming an initial jitter of 0.2σ wakefields peak lumi reduction is 20%. Open the collimator gaps?

Rogelio Tom´ as Garc´ ıa Beam Delivery System: status and plans of R&D until CDR – p.18/23

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SLIDE 21

Energy collimator (Be) survivability

50 100 150 200 250 300 350 50 100 150 200 250 300 350 400 450 500 550 Distance [mm] Temperature increment [K] Temperature increment in a Be spoiler with tapers and a 0.5 rad. lengths body hit by a full CLIC train

Temperature raise after impact of a full train below melting level. (different philosophy than ILC)

Rogelio Tom´ as Garc´ ıa Beam Delivery System: status and plans of R&D until CDR – p.19/23

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SLIDE 22

Collimator gap scan

x

σ N

10 20 30 40 50 60

y

σ N

20 40 60 80 100

a

x

σ N

10 20 30 40 50 60

y

σ N

20 40 60 80 100

b

Good particles for QF1 and QD0 Bad particles for QF1 or QD0

x

σ N

10 20 30 40 50 60

y

σ N

20 40 60 80 100

c

x

σ N

10 20 30 40 50 60

y

σ N

20 40 60 80 100

d

x

σ N

10 20 30 40 50 60

y

σ N

20 40 60 80 100

e

x

σ N

10 20 30 40 50 60

y

σ N

20 40 60 80 100

f

Acceptable collimation depths are between 10- 15σx and 44-55σy.

Rogelio Tom´ as Garc´ ıa Beam Delivery System: status and plans of R&D until CDR – p.20/23

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SLIDE 23

Plans towards CDR

  • CLIC 500 GeV lattice optimization (new

CERN student on August)

  • New tuning algorithms and knobs (help from

SLAC, LAL, ATF2...)

  • ATF2 ultra-low β progress (new CERN PhD

since March and ILC)

  • Review and optimization of collimation:
  • wakefields with new parameters (UK)
  • simulations including secondaries (UK)
  • QD0 review (Detlef)
  • Global feedback studies (new CERN fellow

since May)

Rogelio Tom´ as Garc´ ıa Beam Delivery System: status and plans of R&D until CDR – p.21/23

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SLIDE 24

Some bonus points

  • Luminosity measurement, fast and precise

(?)

  • Crab cavity phase specifications review

(0.025◦ for 12 GHz) (A. Dexter ?)

  • Post-IP polarization measurement (help from

ILC?)

  • 15mW beam dump (help from ILC?)

Rogelio Tom´ as Garc´ ıa Beam Delivery System: status and plans of R&D until CDR – p.22/23

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SLIDE 25

Stabilization to the 0.13nm

Ground isolation and resonance rejection works.

Rogelio Tom´ as Garc´ ıa Beam Delivery System: status and plans of R&D until CDR – p.23/23