H. Liebermann, IAP Frankfurt Training Course on Particle Accelerator Technology Mol, Belgium, May 10.-11. 2007 Design of the superconducting 350 MHz CH-prototype cavity
H. Liebermann, IAP FrankfurtTraining Course on Particle Accelerator TechnologyMol, Belgium, May 10.-11. 2007
Design of the superconducting 350 MHz
CH-prototype cavity
H. Liebermann, IAP Frankfurt
Institut für Angewandte PhysikLINAC AG
Training Course on Particle Accelerator TechnologyMol, Belgium, May 10.-11. 2007 2
Overview• Introduction• MicroWave Studio Simulations
– Endcell-Design (Radius and Length)– Girder-Height
• Electrical and magnetical peak-fields
H. Liebermann, IAP Frankfurt
Institut für Angewandte PhysikLINAC AG
Training Course on Particle Accelerator TechnologyMol, Belgium, May 10.-11. 2007 3
H-Mode Family
IH-Strukture
4-vane RFQIH-RFQ
CH-Strukture
Interdigital H-Mode (IH)B E
++
-- Interdigital H-Mode (IH)BBB E
++
-- B E
++
++
--
--
Crossbar H-Mode (CH)BBB E
++
++
--
--
Crossbar H-Mode (CH)
H. Liebermann, IAP Frankfurt
Institut für Angewandte PhysikLINAC AG
Training Course on Particle Accelerator TechnologyMol, Belgium, May 10.-11. 2007 4
Copper model
H. Liebermann, IAP Frankfurt
Institut für Angewandte PhysikLINAC AG
Training Course on Particle Accelerator TechnologyMol, Belgium, May 10.-11. 2007 5
Endcell-Radius
0 100 200 300 400 500 600 7000,0
2,0x106
4,0x106
6,0x106
|Ez,
MW
S| [V/
m]
Position Strahlachse [mm]
Radius 170mm Radius 210mm Radius 250mm Radius 290mm
170mm
H. Liebermann, IAP Frankfurt
Institut für Angewandte PhysikLINAC AG
Training Course on Particle Accelerator TechnologyMol, Belgium, May 10.-11. 2007 6
Endcell-Length-Variation(Copper-Model beta=0,2)
1654mm
Endlength=81,3mm
1794mm
Endlength=151,3mm
plus 70mm
H. Liebermann, IAP Frankfurt
Institut für Angewandte PhysikLINAC AG
Training Course on Particle Accelerator TechnologyMol, Belgium, May 10.-11. 2007 7
Endcell-Length
0 200 400 600 8000,0
2,0x106
4,0x106
6,0x106
8,0x106
1,0x107
1,2x107
1,4x107
Ez,
MW
S [V/m
]
Position z-Achse [mm]
Länge 21,3mm Länge 61,3mm Länge 111,3mm Länge 131,3mm Länge 151,3mm
Kupfermodell beta=0,2
0 100 200 300 400 5000,0
5,0x106
1,0x107
1,5x107
2,0x107
E z,M
WS [V
/m]
Position Achse [mm]
Länge 5,65mm Länge 45,65mm Länge 105,65mm Länge 115,65mm Länge 145,65mm
Kupfermodell beta=0,1
Electric fields alongthe beam axis
H. Liebermann, IAP Frankfurt
Institut für Angewandte PhysikLINAC AG
Training Course on Particle Accelerator TechnologyMol, Belgium, May 10.-11. 2007 8
Flatness and Frequency
0 20 40 60 80 100 120 140 160 180
-1
0
1
2
3
4
5
g/l = 0,5
(Een
d-Em
ittel)/E
mitt
el
Endrohrlänge [mm]
Kupfermodell beta 0,1 , r = 140mm Kupfermodell beta 0,2 , r = 170mm
0 20 40 60 80 100 120 140 160 180 200 220280
290
300
310
320
330
340
350
360
370
g/l = 0,5
Freq
uenz
[MH
z]
Endrohrlänge [mm]
Kupfermodell beta 0,1 , r = 140mm Kupfermodell beta 0,2 , r = 170mm
H. Liebermann, IAP Frankfurt
Institut für Angewandte PhysikLINAC AG
Training Course on Particle Accelerator TechnologyMol, Belgium, May 10.-11. 2007 9
Variation of Girder-HeightCopper-model: beta=0,2 and radius=170mm
Girderheight=70mm Girderheight=0mm
H. Liebermann, IAP Frankfurt
Institut für Angewandte PhysikLINAC AG
Training Course on Particle Accelerator TechnologyMol, Belgium, May 10.-11. 2007 10
Girder-Height
0 100 200 300 400 500 600 7000,0
2,0x106
4,0x106
6,0x106
|Ez,
MW
S| [
V/m
]
Position z-axis [mm]
Girder 0mm Girder 35mm Girder 70mm Girder 100mm
Copper model beta=0,2 , r = 170mm
0 10 20 30 40 50 60 70 80 90 100
340
345
350
355
360
365Copper model beta=0,2 , r = 170mm
Freq
uenc
y [M
Hz]
girder height [mm]
Electric field along beam axis
Frequency
H. Liebermann, IAP Frankfurt
Institut für Angewandte PhysikLINAC AG
Training Course on Particle Accelerator TechnologyMol, Belgium, May 10.-11. 2007 11
Variation of the Girder-LengthCopper-model: beta=0,2 and Radius=170mm
Girder-Length=91% Girder-Length=100%
(Girderlänge 100% = 1360mm)
H. Liebermann, IAP Frankfurt
Institut für Angewandte PhysikLINAC AG
Training Course on Particle Accelerator TechnologyMol, Belgium, May 10.-11. 2007 12
Girder-Length
0 100 200 300 400 500 600 7000
1x106
2x106
3x106
4x106
5x106
|Ez,
MW
S| [V/
m]
Position z-axis [mm]
91 Prozent 94 Prozent 97 Prozent 100 Prozent
Girderlength 100 Prozent = 1360mmCopper model beta=0,2 , r = 170mm
90 92 94 96 98 100
361,2
361,4
361,6
361,8
362,0
362,2
362,4
362,6
362,8
Freq
uenc
y [M
Hz]
Girderlength [%]
Copper model beta=0,2 , r = 170mm
Girderlength 100 Prozent = 1360mm
H. Liebermann, IAP Frankfurt
Institut für Angewandte PhysikLINAC AG
Training Course on Particle Accelerator TechnologyMol, Belgium, May 10.-11. 2007 13
Endcell-Length-Variation(Prototype beta=0,1)
plus 95mm
928mm 1118mm
Endcell-Length=162,57mmEndcell-Length=67,57mm
H. Liebermann, IAP Frankfurt
Institut für Angewandte PhysikLINAC AG
Training Course on Particle Accelerator TechnologyMol, Belgium, May 10.-11. 2007 14
Endcell-Length
0 100 200 300 400 5000,0
2,0x106
4,0x106
6,0x106
8,0x106
1,0x107
1,2x107
1,4x107
1,6x107
|Ez,
MW
S| [V
/m]
Positon z-axis [mm]
Length 117,57mm Length 137,57mm Length 147,57mm Length 157,57mm
Prototype-configuration beta=0,1
Electric field alongbeam axis
60 80 100 120 140 160 180
-1
0
1
2
3
4
5
Prototype beta 0,1 , r = 140mm
(Een
d-Em
ittel)/E
mitt
el
Endrohrlänge [mm]
g/l = 0,5
Flatness
H. Liebermann, IAP Frankfurt
Institut für Angewandte PhysikLINAC AG
Training Course on Particle Accelerator TechnologyMol, Belgium, May 10.-11. 2007 15
0 2 4 6 8 10 12 14 16 18 200,30
0,35
0,40
0,45
0,50
0,55
0,60
Prototyp beta=0,1
g/l
Gap-Number
Prototype-structure with g/l-variation
Length = 1048mmRadius = 140mmbeta = 0.1
H. Liebermann, IAP Frankfurt
Institut für Angewandte PhysikLINAC AG
Training Course on Particle Accelerator TechnologyMol, Belgium, May 10.-11. 2007 16
On-axis field and flatness
0 100 200 300 400 5000,0
2,0x106
4,0x106
6,0x106
8,0x106
1,0x107
1,2x107
|Ez,
MW
S| [
V/m
]
Positon z-axis [mm]
Length 120,7mm Length 130,7mm Length 140,7mmmit g/l-Variation
(beta=0,1)
120 125 130 135 140
-0,4
-0,2
0,0
0,2
0,4
0,6
0,8
1,0
1,2
(Een
d-Em
ittel)/E
mitt
el
endcell-length [mm]
Prototype beta 0,1 , r = 140mm Prototype beta 0,2 , r = 170mm
with g/l - Variation
H. Liebermann, IAP Frankfurt
Institut für Angewandte PhysikLINAC AG
Training Course on Particle Accelerator TechnologyMol, Belgium, May 10.-11. 2007 17
Surface peak fields (prototype)
electric
magnetic
H. Liebermann, IAP Frankfurt
Institut für Angewandte PhysikLINAC AG
Training Course on Particle Accelerator TechnologyMol, Belgium, May 10.-11. 2007 18
Stem-variation
b
a1 0 1 2 1 4 1 6 1 8 2 0 2 2 2 4 2 6 2 8
5 ,6
5 ,8
6 ,0
6 ,2
6 ,4
8 ,0
8 ,5
9 ,0
9 ,5
1 0 ,0
1 0 ,5
1 1 ,0
1 1 ,5
1 2 ,0
E peak
/Eac
c
s te m w id th b [m m ] (a = 2 1 .4 m m )
Bpe
ak/E
acc [m
T/M
V/m
]prototype: a=12.5mm , b=20mm
H. Liebermann, IAP Frankfurt
Institut für Angewandte PhysikLINAC AG
Training Course on Particle Accelerator TechnologyMol, Belgium, May 10.-11. 2007 19
Drifttube-thickness
R1
R2 0 20 40 60 80 1000.0
5.0x106
1.0x107
1.5x107
2.0x107
2.5x107
3.0x107
E abs [
V/m
]
Position [mm]
R2 - R1
5 mm 7 mm 9 mm 11 mm
electrical field at the aperture fordifferent drifttube-thicknesses
H. Liebermann, IAP Frankfurt
Institut für Angewandte PhysikLINAC AG
Training Course on Particle Accelerator TechnologyMol, Belgium, May 10.-11. 2007 20
electrical field at the surface of the drifttube with different thicknesses (5mm (left) und 11mm (right)) (ηpeak=0.9)
H. Liebermann, IAP Frankfurt
Institut für Angewandte PhysikLINAC AG
Training Course on Particle Accelerator TechnologyMol, Belgium, May 10.-11. 2007 21
sc prototype gap
23.87max.13.94min.gaplength [mm]
mm857.422
=βλ
2mm
4βλ
R2-R1
y
H. Liebermann, IAP Frankfurt
Institut für Angewandte PhysikLINAC AG
Training Course on Particle Accelerator TechnologyMol, Belgium, May 10.-11. 2007 22
min. & max. prototype gap
0,0 2,5 5,0 7,5 10,0 12,5 15,0 17,5 20,0 22,5 25,01,50x107
2,00x107
2,50x107
3,00x107
3,50x107
4,00x107
E abs [V
/m]
Position [mm]
R2 - R1
4 mm 5 mm 7 mm
Gap=13.94148mm
y0,0 2,5 5,0 7,5 10,0 12,5 15,0 17,5 20,0 22,5 25,0
1,50x107
2,00x107
2,50x107
3,00x107
3,50x107
E abs [V
/m]
Position [mm]
R2 - R1
4 mm 5 mm 7 mm
Gap=23.87280mm
y
Electrical field along y.
Variation of the drifttube-thickness
H. Liebermann, IAP Frankfurt
Institut für Angewandte PhysikLINAC AG
Training Course on Particle Accelerator TechnologyMol, Belgium, May 10.-11. 2007 23
The prototype
178000(Ra/Q)G (Ω2)
155W (mJ/(MV/m)2)
352Frequency (MHz)
3.8E0 (MV/m)
3.7x108Q0 (total Rs=150 nΩ)
56G=RsQ0 (Ω)
3180Ra/Q (Ω) (T incl.)
3.0Ea=ET (MV/m)
19Ep (MV/m) @ Ea=3 MV/m
21Bp (mT) @ Ea=3 MV/m
1.5x109Q0 (BCS, 4.5K, 352 MHz)
0.1β
1048Length (mm)
19Gap number
H. Liebermann, IAP Frankfurt
Institut für Angewandte PhysikLINAC AG
Training Course on Particle Accelerator TechnologyMol, Belgium, May 10.-11. 2007 24
Parts of the structure
H. Liebermann, IAP Frankfurt
Institut für Angewandte PhysikLINAC AG
Training Course on Particle Accelerator TechnologyMol, Belgium, May 10.-11. 2007 25
H. Liebermann, IAP Frankfurt
Institut für Angewandte PhysikLINAC AG
Training Course on Particle Accelerator TechnologyMol, Belgium, May 10.-11. 2007 26
H. Liebermann, IAP Frankfurt
Institut für Angewandte PhysikLINAC AG
Training Course on Particle Accelerator TechnologyMol, Belgium, May 10.-11. 2007 27
at
H. Liebermann, IAP Frankfurt
Institut für Angewandte PhysikLINAC AG
Training Course on Particle Accelerator TechnologyMol, Belgium, May 10.-11. 2007 28
superconductingCH-Prototype
RealCST MicroWaveStudio