coupler effects in high energy part of xfel linac

17
Coupler Effects in High Energy Part of XFEL Linac V. Tsakanov CANDLE (Armenia) XFEL Beam Dynamics Group Meeting , 31 March 2008 Laboratory Report

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Coupler Effects in High Energy Part of XFEL Linac. Laboratory Report. V. Tsakanov CANDLE (Armenia). XFEL Beam Dynamics Group Meeting , 31 March 2008. Contents. Coupler RF and Wake field Effects Injector and Linac 1 Low energy Linac -0.5-2 GeV High Energy Linac – 2-20 GeV Summary. - PowerPoint PPT Presentation

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Page 1: Coupler Effects in High Energy Part of XFEL Linac

Coupler Effects in High Energy Part of XFEL Linac

V. Tsakanov

CANDLE (Armenia)

XFEL Beam Dynamics Group Meeting , 31 March 2008

Laboratory Report

Page 2: Coupler Effects in High Energy Part of XFEL Linac

Contents

• Coupler RF and Wake field Effects

• Injector and Linac 1

• Low energy Linac -0.5-2 GeV

• High Energy Linac – 2-20 GeV

• Summary

Page 3: Coupler Effects in High Energy Part of XFEL Linac

rkk(s)r)(s,W D

- Monopole term -Dipole termk Dk

• Beam coherent oscillations

• Head-Tail Relative kick

• Wakefield Emittance dilution (Cavity wake)

• Chromatic Emittance dilution ( Energy spread)

k

rmsk

Introduction Couplers : Wake Field , RF Distortion

Page 4: Coupler Effects in High Energy Part of XFEL Linac

The field potential - linear variation within the bunch

rms0 k3k

0k

3

W(s)

S=0

rσs

kkσs

kkr)(s,W Drms

D0rms0

Monopole term Dipole term

Krf ~ Vcav*σz

• Coupler RF kick –

Scaling with accel grad and bunch length

Model for Transverse Potential

Page 5: Coupler Effects in High Energy Part of XFEL Linac

Beam Model for Particle Tracking

E/E(s)

q(sk),E(sk

)

q(E/E)

sk

x (y)

x’ (y’)

(s, E/E,x,x’,y,y’)

xx, x’x’,xx’

slices subslices

moments

yy, y’y’,yy’

Uncorrelated

Page 6: Coupler Effects in High Energy Part of XFEL Linac

Main Parameters

Bunch Length

μm

Acc. Grad.

MV/m

Wake rms

kick k0

V/nC/cav

RF rms kick k0

V/nC/cav

Wake rms kick k1 (dipole)

V/nC/mm/cav

RF rms kick k1 (dipole)

V/nC/mm/cav

Cavity rms kick k1(dipole)

V/nC/mm/cav

Injector 2000 12 8.2 38.4 1.25 1.8 21.6

Booster 120 16 8.2 3.0 1.25 0.14 3.5

Main Linac

25 20.8 8.2 0.8 1.25 0.04 0.77

5MeV - 500MeV 0.5GeV - 2GeV 2GeV - 20GeV

BC1 BC2

I.Zagorodnov, M. Dohlus

RF kick Wake kick Wake kick

Cavity kick Cavity kick Wake kick

For beam offset < 1mm monopole term k0 dominates

Monopole

Dipole

rmskDrmsk

Monopole

Dipole

For cavity 0k

kk

kk

0

Drms1

rms0

Page 7: Coupler Effects in High Energy Part of XFEL Linac

Injector Part ACCEL15 MeV ~100 MeV

12 MV/m

8 cavities

4 TESLA Modules ~ 12MV/m

~100 MeV ~500 MeVLINAC1

Bunch Charge – 1nC

Bunch rms length – 2mm

Normalized emittance – 1mm*mrad

Page 8: Coupler Effects in High Energy Part of XFEL Linac

Optics ( W. Decking)

Page 9: Coupler Effects in High Energy Part of XFEL Linac

ACCEL 1

ACCEL15 MeV ~100 MeV

12 MV/m

8 cavities

Trajectory Emittance dilution

Coupler RF Field & Wake

Dominate by RF Head –tail kick by monopole term

Cavity wake effect - < 0.1%

Page 10: Coupler Effects in High Energy Part of XFEL Linac

Other Options (??)

β0=2.4

V1: α0=-4.2

V2: α0 =-3.0

V3: α0=-2.3

3.5%

7%

14%

V1- Injector Design

2Δφ

sinLβ

~εΔε 4

cell

av

Page 11: Coupler Effects in High Energy Part of XFEL Linac

LINAC1

4 TESLA Modules ~ 12MV/m

~100 MeV ~500 MeVLINAC1

Coupler Wake Coupler RF

0.25%

~5%

Page 12: Coupler Effects in High Energy Part of XFEL Linac

Summary for Injector

• Coupler RF Field effects

ACCEL1 – 5-100 MeV Emittance growth ~14 %

Linac 1 – 100-500 MeV Emittance growth ~5%

• Other effects

RF Wake Injection Jitter – 1 sigma offset Cavity&Modules misal. -0.5mm Cavity tilts – 0.5 mrad

<1%

Page 13: Coupler Effects in High Energy Part of XFEL Linac

Booster+Main Linac

Booster Linac • Coherent oscillations

uncorrelated 6·10-6 2·10-4

correlated 2·10-3 1.2·10-3

• Cavity Misalignments 5·10-6 3·10-7

• Modules Misalignments 4·10-5 2.5·10-6

• Correlated Misal. (130o) - 7·10-6

• Cavity tilts uncorrelated 5.8·10-5 0.6% correlated 0.6% 1.9%• One-to-One correction uncorrelated 6.3·10-5 0.4% correlated 1.7% 2%

Total Emittance dilution <5% with 2 Modules/Cell

Summary of Emittance Dilution

Page 14: Coupler Effects in High Energy Part of XFEL Linac

Booster Linac

Wake

RF kick

x

x

2Δφ

sinLβ

~εΔε 4

cell

av

• Natural global compensation

• Dominate by RF Head –tail kick - monopole term

2Δφ

sin~ 2

2πΔφ

π/3μ

6 FODO cells

Page 15: Coupler Effects in High Energy Part of XFEL Linac

Main Linac- Coupler Wake

Monopole term - Offset independent wake

52 FODO Cells – Betatron oscillations ~9

Accum. Emittance Dilution

Correlated, Chromatic

Page 16: Coupler Effects in High Energy Part of XFEL Linac

Cavity tilts

0

302

0

2202 ln

2sin3

4

tg

L

Nd

c

cav

F D σtilt=0.5mrad

Uncorrelated

Correlated

Page 17: Coupler Effects in High Energy Part of XFEL Linac

Summary

• Coupler RF Field effects

ACCEL1 – 5-100 MeV Emittance dilution - 14 % (Head Tail kick) Linac 1 – 100-500 MeV Emittance dilution – 5% (Head tail Kick)

• Coupler Wake Effects Booster - 0.5-2 GeV Emittance dilution – 0.02% ( Head tail kick) Main Linac – 2-20 GeV Emittance dilution – 0.025% ( Chromatic)