Cold Cavity BPM R&D for the ILC

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November 30, 200 6 CA RE Workshop Global Design Effort 1 Cold Cavity BPM R&D for the ILC Manfred Wendt Fermilab

description

Cold Cavity BPM R&D for the ILC. Manfred Wendt Fermilab. The International Linear Collider. ILC Beam Parameters (nominal):. ILC Beam Instrumentation. ~ 2000 Button/stripline BPM’s ~ 1800 Cavity BPM’s (warm) 770 Cavity BPM’s (cold, part of the cryostat) 21 LASER Wirescanners - PowerPoint PPT Presentation

Transcript of Cold Cavity BPM R&D for the ILC

Page 1: Cold Cavity BPM R&D for the ILC

November 30, 2006 CARE Workshop Global Design Effort 1

Cold Cavity BPM R&Dfor the ILC

Manfred Wendt

Fermilab

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The International Linear Collider

beam energy = 2 x 250 GeV

luminosity L = 2 x 1034

rep. frequency frep = 5 Hz

macro pulse length tpulse = 800 µs

# of bunches per pulse = 2820

bunch spacing Δtb = 308 ns

bunch charge = 3.2 nC

bunch length σz ≈ 300 µm

vert. emittance γ εy* = 0.04 mm mrad

RMS energy spread = 0.1 %

βx* (IP) = 21 mm

βy* (IP) = 0.4 mm

hor. beamsize (IP) σx = 500 nm

vert. beamsize (IP) σy = 5 nm

ILC Beam Parameters (nominal):

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ILC Beam Instrumentation

• ~ 2000 Button/stripline BPM’s• ~ 1800 Cavity BPM’s (warm)• 770 Cavity BPM’s (cold, part of the cryostat)• 21 LASER Wirescanners• 20 Wirescanners (traditional)• 15 Deflecting Mode Cavities (bunchlenght)• ~ 1600 BLM’s• Many other beam monitors, including toroids, beam

phase monitors, wall current monitors, faraday cups, OTR & other screen monitors, sync light monitors, streak cameras, feedback systems, etc.

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Cold BPM Requirements• BPM location in the cryostat, at the SC-quad• Every 3rd cryostat is equipped with a BPM/quad:

650x cold BPM’s total.– Real estate: ~ 170 mm length, 78 mm beam pipe

diameter (???).– Cryogenic environment (~ 4 K)– Cleanroom class 100 certification (SC-cavities nearby!)– UHV certification

• < 1 µm single bunch resolution, i.e. measurement (integration) time < 300 ns.

• < 200 µm error between electrical BPM center and magnetic center of the quad.

• Related issues:– RF signal feedthroughs.– Cabling in the cryostat– Read-out System

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Possible Cold BPM Solutions

• Dedicated, high resolution BPM (baseline design):

Cavity BPM, based on the characterization of beam excited dipole eigenmodes, also requires the measurement of the monopole modes for normalization and evt. sign of the beam displacement.

• Combination of dedicated, lower resolution BPM’s and HOM coupler signal BPM’s (alternative design):– Simple, button style BPM’s (~ 50 µm resolution) for

machine tune-up and single bunch orbit measurements.– HOM coupler BPM signal processor as high resolution

BPM

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Cavity BPM PrincipleProblems with simple“Pill-Box” Cavity BPM’s• TM010 monopole

common mode (CM)• Cross-talk (xy-axes,

polarization)• Transient response

(single-bunch measurements)

• Wake-potential (heat-load, BBU)

• Cryogenic and cleanroom requirements

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CM-free Cavity BPM• uses waveguide ports to

suppress the monopole mode (no hybrid-junction required)

+ very high resolution potential (~ 20 nm)!

– complicated mechanics, i.e. cleanroom and cryogenic issues

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KEK ATF nanoBPM CollaborationBINP cavity BPM:• C-Band (6426 MHz)• 20 mm aperture• Selective dipole-

mode waveguide couplers

• 3 BPM’s in a LLBL hexapod spaceframe (6 degrees of freedom for alignment)

• Dual-downconversion electronics (476 & 25 MHz)

• 14-bit, 100 MSPS digitizer

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Cavity BPM Resolution at ATF• 10 minute run• 800 samples• σ ≈ 24 nm

Move BPM in 1 µm steps

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SLAC Cavity BPM

+ S-Band design for 35 mm beam-pipe aperture

+ Waveguide cut to beam-pipe (better cleaning)

+ Successful beam measurements at SLAC-ESA (~ 0.8 µm resolution)

– No cryogenic temperature tests so far.

– No clean-room certification– Needs a reference cavity or

signal– Reduced beam-pipe

aperture (nominal: 78 mm)

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Cold L-Band Cavity BPM Design• Waveguide-loaded pillbox with slot coupling.• Dimensioning for f010 and f110 symmetric to fRF,

fRF = 1.3 GHz, f010 ≈ 1.1 GHz, f110 ≈ 1.5 GHz.• Dipole- and monopole ports, no reference cavity for

intensity signal normalization and signal phase (sign).• Qload ≈ 600 (~ 10 % cross-talk at 300 ns bunch-to-

bunch spacing).• Minimization of the X-Y cross-talk (dimple tuning).• Simple (cleanable) mechanics.• Iteration of EM-simulations for optimizing all

dimensions.• Vacuum/cryo tests of the ceramic slot window.• Copper model for bench measurements.

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Scaling of the SLAC Cavity BPM

General viewPorts

Discrete port (current) x=10 mmy=30 mm

Excitation signal

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SLAC BPM (scaled): Eigen Modes

Mode Frequency

1 1.017 – Parasitic E11-like 2 1.023 – Parasitic E21-like3 1.121 – Monopole E01 4 1.198 - Waveguide5 1.465 - Dipole E11

6 1.627

Dipole

Parasitic mode. Coupling throughhorizontal slots is clearly seen

Parasitic modeEz distribution

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Pillbox with WG Slot Coupling

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Optimization of the Slot Dimensions

• EM: Eigen-mode solver• FD: Frequency-domain solver• Slot-L = 55 mm & Slot-W = 5 mm Qload = 678

Q external and Q loaded vs slot length

0

1000

2000

3000

4000

5000

6000

7000

8000

9000

30 40 50 60 70 80

Slot length, mm

Q

Q ext EM

Q load EM

Q load FD

Qload (EM) vs Slot_W (Slot_L=55)

0

200

400

600

800

1000

1200

1400

1 2 3 4 5 6 7 8 9

Width, mm

Q

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Ceramic Windows in the Coupling Slots

Frequency, GHz 1.46

Loaded Q ~ 600

Beam pipe radius, mm 39

Cell radius, mm 114

Cell gap, mm 10

Waveguide, mm 122x110x25

Coupling slot, mm 47x5x3

Window –Ceramic brick of alumina 96%

r ≈ 9.4

Size: the same as slot

N type receptacle,50 Ohm,D=9.75 mmd=3.05 mm

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Matched WG-to-Coaxial Transition

47.03.mm

2

1

Diam. 4.46 mm

11.13 mm 8.9 mm

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Dipole Mode Sensitivity (Resolution)

x

q

Q

R

QQZfxxV

x

sh

11000110110

11)(

GHzxf 46.1)(110 500Z

600Q

141

110

mmx

sh

Q

R

20000 Q

nCq 1

with:

nCVxxV /10145.4)( 3110

mnCmVV /4110 VBWTkZV seThermalNoi 7.00

500Z

KJk /1038.1 23

KT 300

MHzQ

fBW 4.2

110

110

with:

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Monopole-Mode Investigation

Monopole mode damping using simple pin-antennas

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Unmatched Transmission-line Combiner

In-phase signal combining for the monopole-mode signal

• 180 degrees for dipole-mode. Standing wave with some frequency detuning.

• lTL~ 200 mm to avoid resonances around 1.46 GHz (SW eigenmodes for lTL~ 200 mm at: f3 ~1.1 GHz, f5 ~1.9 GHz)

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Combiner-induced Frequency-shift

BPM spectrum vs length of combiner (one leg)

0

0.5

1

1.5

2

2.5

3

0 50 100 150 200 250 300 350

mm

GH

z

Quadrupole

Dipole

Monopole

Appropriate length of combiner – reasonable length and non-resonantInteraction with dipole mode

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Test Model for N2 Temperature Cycles

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L-Band Cavity Assembly

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Next Steps…

• N2 temperature cycles with the test model.

• Drafting of the complete assembly.• EM modeling and fine tuning of the

dimensions.• Investigation of the tolerances.• Prototype manufacturing.• RF measurements and characterization.

Thanks for your patience!