Wakefields in XFEL undulator intersections Igor Zagorodnov Beam Dynamics Group Meeting 26.02.07.

22
Wakefields in XFEL undulator intersections Igor Zagorodnov Beam Dynamics Group Meeting 26.02.07

Transcript of Wakefields in XFEL undulator intersections Igor Zagorodnov Beam Dynamics Group Meeting 26.02.07.

Page 1: Wakefields in XFEL undulator intersections Igor Zagorodnov Beam Dynamics Group Meeting 26.02.07.

Wakefields in XFEL undulator intersections

Igor Zagorodnov

Beam Dynamics Group Meeting

26.02.07

Page 2: Wakefields in XFEL undulator intersections Igor Zagorodnov Beam Dynamics Group Meeting 26.02.07.
Page 3: Wakefields in XFEL undulator intersections Igor Zagorodnov Beam Dynamics Group Meeting 26.02.07.

Aluminium

7 -1 -13.66 10 [Ω m ]

-157.1 10 sec

600 nmrough

5 nmoxid

Elliptical chamber length = 5122 mm

Page 4: Wakefields in XFEL undulator intersections Igor Zagorodnov Beam Dynamics Group Meeting 26.02.07.

Absorber :length 3mmTapers 2*9.5 mm width 9mmheigh 8mm

Copper

7 -1 -15.8 10 [Ω m ]

-142.46 10 sec

0 nmrough

0 nmoxid

Absorber length = 22 mm

Page 5: Wakefields in XFEL undulator intersections Igor Zagorodnov Beam Dynamics Group Meeting 26.02.07.

Cavity BPM design, Dirk Lipka

elliptical pipe

round pipe

absorber

Round pipe length = 690mm

Copper

7 1 15.8 10 m

-142.46 10 sec

0 nmrough

0 nmoxid

Cavity BPM = 2 Pillbox cavities with gap 10mm and distance 45 mm between them

Page 6: Wakefields in XFEL undulator intersections Igor Zagorodnov Beam Dynamics Group Meeting 26.02.07.

Elements

Elliptical chamber = 5122 mm

Absorber = 22 mm

Round pipe = 690 mm

Cavity BPM = 2 Pillbox cavities with gap 10mm and distance 45 mm between them

Not considered (see TESLA FEL 2005-10)

216 mm

(5000+1100)-5884=266

Pumping slots = 2*25=50 mm

Flange gaps?Belows?

???

5122+22+690+50==5884 mm

Page 7: Wakefields in XFEL undulator intersections Igor Zagorodnov Beam Dynamics Group Meeting 26.02.07.

Absorber

4 mm

5 mm4 mm

9.5 mm 3 mm

0.4 mm

15mm

3mm

8.8mm

5 mm

Page 8: Wakefields in XFEL undulator intersections Igor Zagorodnov Beam Dynamics Group Meeting 26.02.07.

Absorber. Effect of Tapering

4 mm

5 mm4 mm

9.5 mm

3 mm

5 mmg = 4 mm

3 mm

-5 -4 -3 -2 -1 0 1 2 3 4 5-150

-100

-50

0

50

4.5 mm

9.5 mm

5 mm4 mm

6o

~ 0.4og

3o

90o

6o 3o

Loss,

V/pC

Spread,

V/pC

step 89 35

taper 48 39

taper +step 52 26

Page 9: Wakefields in XFEL undulator intersections Igor Zagorodnov Beam Dynamics Group Meeting 26.02.07.

Absorber. Effect of Tapering

7.5 mm4.5 mm

9.5 mm 3 mm

0.4 mm

15mm

3mm

8.8mm

~ 3o

17.5o

5 mm

9.5 mm

7.5 mm4.5 mm

This taper has no effect.

The taper angle should be about 3 grad.

17.5o

2.4o

Page 10: Wakefields in XFEL undulator intersections Igor Zagorodnov Beam Dynamics Group Meeting 26.02.07.

Absorber. Long Elliptical Step Collimator

0.4 mm

2 15w mm

3mm

2 8.8g mm

0

0 0 0 0

0 2 20 0 0 0

0 01

Re Re Im Im( , , , ) 4 ln ( ) ( )

cosh( ) sinh( )

nu n n n n

n

x iy x iyx iy x iyT T T T

e d d d dG x y x y x x y y

n nu nu

0 00 0 0 0 0 0( , , , ) ( , , , ) (0, , , )G x y x y G x y x y G g x y

G.Stupakov, K.L.F.Bane, I.Zagorodnov „Optical approximation in the theory of geometric impedance“, in preparation

The semi-analytical approach developed in the paper allows to calculate high-frequency impedance of any short transition.

Loss=86 V/pC

Page 11: Wakefields in XFEL undulator intersections Igor Zagorodnov Beam Dynamics Group Meeting 26.02.07.

Elliptical 15mm*8.8mm

Absorber 9mm*8mm

Round R=?

Absorber+Round Pipe

Page 12: Wakefields in XFEL undulator intersections Igor Zagorodnov Beam Dynamics Group Meeting 26.02.07.

0.4 0.5 0.6 0.7

0

50

100

150

200Loss [V/pC]

R [cm]

Elliptical 15mm*8.8mm

Round R=?

Elliptical 15mm*8.8mmER

RE

ER RE

Total

Let us forget about absorber and suggest that we want to have a round pipe. Why do not take a round absorber with R=5mm?

Elliptical+Round Pipe

Page 13: Wakefields in XFEL undulator intersections Igor Zagorodnov Beam Dynamics Group Meeting 26.02.07.

0.4 0.5 0.6 0.7

0

50

100

150

200

250Loss [V/pC]

R [cm]

Elliptical 15mm*8.8mm

Round R=?

Elliptical 15mm*8.8mmAR

RE

AR RE

Total

EA

Absorber 9mm*8mm

Absorber+Round Pipe+Elliptical Pipe

Page 14: Wakefields in XFEL undulator intersections Igor Zagorodnov Beam Dynamics Group Meeting 26.02.07.

0.35 0.4 0.45 0.5 0.55 0.60

50

100

150

200Loss [V/pC]

R [cm]

OldType I

Geometric Wakes

Page 15: Wakefields in XFEL undulator intersections Igor Zagorodnov Beam Dynamics Group Meeting 26.02.07.

0.4 0.45 0.5 0.55 0.6 0.650

20

40

60

80

100

120

140

160

180

200Loss [V/pC]

R [cm]

Old

Type I

Type II

40%

Geometric Wakes

Page 16: Wakefields in XFEL undulator intersections Igor Zagorodnov Beam Dynamics Group Meeting 26.02.07.

0.4 0.5 0.6 0.70

50

100

150

200

250

4 5 6 70

20

40

60

80

100

120

Loss [kV/nC] Spread [kV/nC]

R [cm] R [cm]

resistive

geom.

L=690mm

Geometric+Resistive Wakes

Page 17: Wakefields in XFEL undulator intersections Igor Zagorodnov Beam Dynamics Group Meeting 26.02.07.

-5 0 5-200

-150

-100

-50

0

50

resistive

geom.

/s

|| /W V pC

total

R=4.5mm

Loss,

V/pC

Spread,

V/pC

res. 22 27

geom. 87 34

total 109 55

L=690mm

Geometric+Resistive Wakes

Page 18: Wakefields in XFEL undulator intersections Igor Zagorodnov Beam Dynamics Group Meeting 26.02.07.

-5 0 5-600

-400

-200

0

200

400

Aluminium

7 -1 -13.66 10 [Ω m ]

5122mmL

1 4.4 mmb

resistive total

Loss 225 241

Spread 238 310

kV/nC

|| kV/nCW

ms

Main Pipe (resistive+oxid layer+roughness)

resistive

-157.1 10 sec 600 nmrough

5 nmoxid

(T.Wohlenberg)

Page 19: Wakefields in XFEL undulator intersections Igor Zagorodnov Beam Dynamics Group Meeting 26.02.07.

-5 -2.5 0 2.5 5

-80

-60

-40

-20

0

|| kV/nCW

ms

only first

pillbox

total

Loss 25 48

Spread 10 19

kV/nC

BPM

2*pillbox

4.5 mm 38.58 mm26.29 mm

45 mm

10 mm

10 mm

BPM

Page 20: Wakefields in XFEL undulator intersections Igor Zagorodnov Beam Dynamics Group Meeting 26.02.07.

7.5mm

7.5mm

3.8mm7.5mm

7.5mm

7.5mm

Old geometry!

Loss 9*2=18

Spread 4*2=8

kV/nC

Pumping Slots

2 items?

Page 21: Wakefields in XFEL undulator intersections Igor Zagorodnov Beam Dynamics Group Meeting 26.02.07.

Impedance BudgetUndulator pipe

Pump

(2 items)

BPM

(2 pillboxes)

Round pipe in intersection with absorber

15mm*

8.8mm (5122 mm)

Old geometry

2*10mm pipe R=4.5

absorber 8mm*9mm

(690+22=712mm)

pipe R=5mm

absorber R=5mm

(712mm)

Loss, kV/nC 241 18 48 109 74

Spread, kV/nC 310 8 25 55 41

Loss,

V/pC

Spread,

V/pC

Total geom.

pro section 70 25

resistive (Al)

6.1m 303 325

Old budget from TESLA-FEL 2005-10 (elliptical pipe 15*7.6 mm)

0

50

100

150

200

250

300

350

400

pipe intersection total

new

old

Energy SpreadV/pC

Page 22: Wakefields in XFEL undulator intersections Igor Zagorodnov Beam Dynamics Group Meeting 26.02.07.

Conclusion In new budget the energy spread is larger by 14 %.

Intersection causes about 25 % of the energy spread.

Round pipe with R=4.5 mm does not increase longitudinal wake.

To suppress the geometric wake the tapers should be less than 3 grad.

Why do not take a round absorber with R=5mm?

A description of 216 mm? (bellows, flange gaps, etc)

0

50

100

150

200

250

300

350

400

pipe intersection total

new

old

pipe93%

intersection7%

pipe77%

intersection23%

Energy SpreadV/pC