CLIC Crab Cavity and Wakefields Praveen Ambattu CLIC crab group - - PowerPoint PPT Presentation

clic crab cavity and wakefields
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CLIC Crab Cavity and Wakefields Praveen Ambattu CLIC crab group - - PowerPoint PPT Presentation

ICFA Beam Dynamics Workshop 2010, Daresbury CLIC Crab Cavity and Wakefields Praveen Ambattu CLIC crab group Cockcroft Institute / Lancaster University / University of Manchester / ASTeC Crab Cavity Operation BDS chapter of the CLIC CDR,


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SLIDE 1

CLIC Crab Cavity and Wakefields

ICFA Beam Dynamics Workshop 2010, Daresbury Praveen Ambattu CLIC crab group Cockcroft Institute / Lancaster University / University of Manchester / ASTeC

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SLIDE 2

Crab Cavity Operation

BDS chapter of the CLIC CDR, http://clicr.web.cern.ch/CLICr/MainBeam/BDS/CDR/TEX/

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SLIDE 3

Technology choice

 High group velocity / TW cavity:

  • beam-loading correction
  • phase control , than SW cavity
  • a = 5 mm, vgr = 2.95 %

 12 GHz cavity:

  • availability of X-band Klystron
  • kick per cavity
  • phase tolerance

 Heavily damped or moderately damped-detuned cavity:

  • Transverse and longitudinal wakefield
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SLIDE 4

16 cell Crab Cavity

Vcav=2.55 MV Etr=18 MV/m Pcav=1.19 MW Pbeam=117 kW Pin=7.3 MW Pout=6 MW

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SLIDE 5

Wakefield effects in crab cavity

  • Lower order mode  energy spread inefficient focus
  • Crab / operating mode beamloading amplitude error
  • Same order mode  vertical deflection  bunches miss at IP
  • Higher order modes (HOMs)  both monopole and dipole contributions

The most dangerous in the group is the SOM which has the same frequency and kick as the operating mode but in the vertical plane. Bunch(es) can excite a variety of modes with different properties

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SLIDE 6

 Since the multi-bunch transverse wake field is a sum of sinusoidal oscillations, there are frequencies where the wakefield is essentially zero  This happens at harmonics of half bunch frequency (n.1GHz, n=1,3, 5..), no need of any SOM damping iff the bunches are coming at the same offset from the axis

Multibunch wakefield in the undamped cavity, Q=6000

b

N 1 m,t m,t m b b d n 1

W 2rK sin(n T )exp( nT / T )

 

  

1) Fixed offset for all bunches

11 GHz 13 GHz 1 MHz off Single mode-Multibunch-Transverse wake:

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SLIDE 7

2) Fixed offset and sign alternation bunch-to-bunch 3) Random offset and random sign Damping is essential !

10 GHz 12 GHz 14 GHz

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SLIDE 8

Fixed offset and sign alternation bunch-to-bunch , Q=30 Random offset and random sign, Q=30

Tolerance

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SLIDE 9
  • The maximum longitudinal wake occurs at the bunch harmonic
  • In the 12 GHz dipole cavity, the LOM occurs between 8.3 and 8.8 GHz

which are far off-resonance

b

N 1 m,z m,z m b b d n 1

W K 1 2 cos(n T )exp( nT / T )

 

         

  • However, geometry modifications for damping dipole modes may shift the

LOM also to resonance. So LOM damping is also essential

Single mode-Multibunch-Longitudinal wake:

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SLIDE 10

Damping tolerances

  • Transverse wake: Luminosity loss is under 2 %

Tolerance: 0.3 V/pC, for a 16 cell cavity

  • Longitudinal wake: Bunch energy spread is under 1e-4%,

Tolerance: 2500 V/pC for a 16 cell CC

  • Worst case Qs: Calculated at the frequency of maximum kick / loss factor

mode Freq., GHz df for max wake, MHz Qext(x) Qext(y) Dipole modes (offset = 35 mm) Dip1 11.9942 1

  • 33

Dip3 24.0663 2 225 211 Dip4 25.634 2.14 457 429 Dip6 32.8852 2.74 611 572 Monopole modes (offset = 0) Mon1 8.6683 668 665 Mon2 20.854 854 1229 Mon3 28.7514 751 1111

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SLIDE 11

Waveguide damping

WR112 WR42 SiC load (10-j3)

Crab SOM Dip3x Dip3y LOM

Dip3x SOM

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SLIDE 12

Choke-mode damping

eRx Rx eRx Rx w/2

Shape Qext Crab SOM LOM Basic choke mode cavity 1.906E+04 1.906E+04 218 Elliptical cavity 1.554E+04 240 15 Elliptical choke 1.557E+04 587 172 Slotted Choke 1.557E+04 172 67

The basic choke-mode cavity can’t damp the SOM, so we need to device asymmetric choke-mode dampers

Elliptical cavity Elliptical choke Slotted choke

SiC load

SOM

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SLIDE 13

Detuning to decohere SOM wake

  • Detuning assisted by moderate damping already in progress for the CLIC main

linac

  • Detuning the SOM to have a spread of frequencies by changing the equator

ellipticity downstream

  • This allows the SOM wake to decay with Gaussian profile over a few bunch

times

y = 11.99x-0.45 10.5 11 11.5 12 12.5 13 13.5 0.7 0.8 0.9 1 1.1 1.2 1.3 Freq, GHz Rx/Ry

Dip1 Dip2 Power (Dip2)

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SLIDE 14

Uncoupled calculation

Q Sum wake (V/pC) 6500 2.443 500 0.165 100 0.028

  • V. Khan, R.M. Jones, CI / UMAN
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SLIDE 15

2.4 2.5 2.6 2.7 2.8 2.9 3

  • 5
  • 4
  • 3
  • 2
  • 1

1 2 3 4 5 Group velocity, %c Frequency split, GHz

  • SOM spread for detuning is limited by the group velocity of operating mode

f = 11.9942 GHz

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SLIDE 16

RF properties

Cavity Trans R/Q, W Trans Rsh, MW/m Vgr, %c Es/Etr Hs/Etr Undamped 53.92 41.4 2.93 3.57 0.012 Choke mode (Qsom~50) 47.46 (-12 %) 26.5 (-36 %) 2.84 3.55 0.024 (+100 %) Waveguide (Qsom~50) 52.86 37.8 2.63 (-10 %) 3.55 0.012 Detuned

(df=4.2 GHz)

50.2 37 2.48 (-15 %) 3.39 0.01

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SLIDE 17

Conclusions

1) Waveguide damping:  Meets the required wakefield tolerance (Q~30)  Group velocity concern  Fabrication difficulty 2) Choke mode cavity:

  • Moderate damping (Q~200)
  • Higher surface magnetic field

2) SOM detuning:

  • Meets required wakefield tolerance, combined with moderate

damping (Q~500)

  • Group velocity reduction restricts achievable SOM spread
  • Choke-mode-detuned cavity is a good option for a possible

prototype