high gradient performance of clic-designed structures
DESCRIPTION
High Gradient Performance of CLIC-Designed Structures. Chris Adolphsen 10/12/09. CLIC Quad Structure Tests. HDX11 X-Band Damped Quad Structure. Structure Installed in a Vacuum Can for Testing. Visual/SEM Inspection after Processing. Iris Slots. Scattered Dark Spots. Input Coupler Iris. - PowerPoint PPT PresentationTRANSCRIPT
High Gradient Performance ofCLIC-Designed Structures
Chris Adolphsen10/12/09
CLIC Quad Structure Tests
In NLCTA Beamline
Structure Note Performance
11/06 – 2/07 C11vg5Q16First X-band Quad
- Irises Slotted Poor: 57 MV/m, 150 ns, 2e-5 BDR –
grew whiskers on cell walls
2/08 - 4/08C11vg5Q16
Redux Refurbished
Initially good (105 MV/m, 50 ns,1e-5 BDR) but one cell degraded
4/07 – 10/07 C11vg5Q16-MoMolybdenum
Version of AbovePoor: 60 MV/m, 70 ns, 1e-6 BDR
10/08 – 12/08 TD18vg2.6_QuadNo Iris Slots but WG
DampingVery Poor: would not process above 50 MV/m, 90ns – gas spike after BD
Test at KEK
08/09 - presentTD18vg2.6_Quad
50 m Rounded Iris Edges
Very Poor: after 400 hours, only reached 60 MV/m with 50 ns pulses
HDX11 X-Band Damped Quad Structure
Number of Cells 11 + 2 Matching
a/ 16 %
Phase per Cell 60 deg
Es/Ea 1.6
vg/c 5.1%
Iris Thickness 1.4 mm
Q 3760
r/Q 13 kOhm/m
For Eacc = 100 MV/m
Input Power 164 MW
Structure Installed in a VacuumCan for Testing
Scattered Dark Spots
Areas of DiscolorationPatchy breakdown areas along sides of irises
Iris Slots
Input Coupler
Iris
Visual/SEM Inspection after Processing
Iris 7&8(Top Right)
Iris 7(Top Right)
After First Run, Decided To
• Electro-polish surface to smooth pits and whiskers
• Fire at 1050 degC (when brazing on water fittings)
to grow large grains
• Attempt to better align quadrants
• Re-install in the can with the orientation reversed
so the ‘good’ end now sees the input power.
Iris 1 Before and After Electro-Polishing
Before Electropolish After 7-minute Electropolish
Before Braze After Braze
After Brazing on New Water Fittings
Quad 7-8: Iris 1. Grain growth significantly increased
0 50 100 150 200 250 300 350 400 4500
20
40
60
80
100
120
Time w ith RF On: hr
C11g5Q16-orignal 07-Nov-2006--18-Dec-2006 23:59:43
Average gradient: MV/m
Pulse w idth: 10nsec
Trip rate: 10/hr
0 50 100 150 200 2500
20
40
60
80
100
120
Time w ith RF On: hr
C11g5Q16-repolished 03-Mar-2008--19-Mar-2008 22:59:33
Average gradient: MV/m
Pulse w idth: 10nsec
Trip rate: 10/hr
0 50 100 150 200 2500
10
20
30
40
50
60
70
Time w ith RF On: hr
C11g5Q16-repolished 03-Mar-2008--19-Mar-2008 22:59:33
Trip rate: /hr
0 50 100 150 200 250 300 350 400 4500
50
100
150
200
250
300
Time w ith RF On: hr
C11g5Q16-repolished 07-Nov-2006--18-Dec-2006 23:59:43
Trip rate: 1/hr
Damaged at100 MV/m, 70 ns
Second RunFirst Run
SEM Photos after Second Run: Nearly all Damage on Sides of Cell 1 in One Quadrant
1 cell 0 cell2 cell3 cell4 cell
5 cell6 cell7 cell8 cell9 cell
Opposing ‘Tips’ on Side Walls
‘Stonehenge’First Iris
above the Damaged Quadrant
Molybdenum HDX11
TD18 Quad Structure
TD18 Quad Processing History
0 5 10 15 20 25 30 35 40 450
50
Ave
rag
e U
nlo
ad
ed
Gra
die
nt:
MV
/m
0 5 10 15 20 25 30 35 40 450
50
100
Time with RF on: hrs
Bre
akd
ow
n R
ate
: 1/h
r
90ns
80ns60ns80ns
Breakdowns Located Throughout Structure
TD18 Quad Post-Run Examination
Not able to take good photos or SEM images, but saw damage similar to CERN 30 GHz HDX-like structures except practically
no pitting on the irises (i.e., all breakdowns near joints)
30 GHz NDS4_vg2.5_thick
30 GHz HDS4_Thick Post Mortem
See similar metal protrusions in the TD Quad structure
Edges rounded (50 micron radius) in TD18 produced at KEK
Recent KEK Results from Testing a TD18 Quad Structure with 50 m Rounded Iris Edges
60 MV/m
Structure a/ (%)P
(MW)
E (MV/m
)
HDS60vg8.0 19 16.1 61
HDS60vg5.1 16 13.3 75
HDS4vg2.6_thick 17.5 7.5 67
NDS4vg2.5_thick 17.5 8.6 75
C30vg4.7 17.5 21.0 94
C40vg7.4_/2 20 19.2 65
C30vg4.7_sb 17.5 20 92
All measured data at 70 ns pulse length and 10-3 breakdown rate
Summary of 30 GHz Structures
Steffen Doebert
In NLCTA Beamline
Structure Note Performance
4/08 – 7/08T18vg2.6-Disk
SLAC_1Cells by KEK,
Assembled at SLAC
Good: 105 MV/m, 230 ns at LC BDR spec of 8e-7/pulse/m but hot cell
developed
7/08 – 10/08T18vg2.6-Disk
SLAC_1Powered from
Downstream EndGood: 163 MV/m, 80 ns, 2e-5 BDR in last cell, consistent with fwd operation
12/08 – 2/09T18vg2.6-Disk
CERN_1CERN Built, Operate
in Vac CanVery Poor: very gassy with soft breakdowns at 60 MV/m, 70 ns
Test at KEK
10/08 – 06/09
T18vg2.6-Disk
KEK_1Cells by KEK,
Assembled at SLACGood: 102 MV/m, 240 ns at LC BDR
spec – no bkd location info
7/09 – 8/09T24vg1.8Disk
CERN_1CERN Built, Cells
Pre-FiredPoor: achieve < 60 MV/m after 100 hours with pulse lengths < 100 ns
5/09 - presentT18vg2.6-Disk
SLAC_2Cells by KEK,
Assembled at SLACGood: after 280 hours, 97 MV/m, 230 ns
at LC DBR spec – one hot cell
CLIC Disk Structure Tests
T18-Disk Structure(First attempt at an optimal CLIC structure)
Field Profile Along the Structure
Cells 18+input+output
Filling Time: ns 36
Length: cm 29
a/λ (%) 15.5 ~ 10.1
vg/c (%) 2.6 - 1.0
S11/ S21 0.035 / 0.8
Phase Advance Per Cell 2/3
Power Needed <Ea> = 100 MV/m 55.5 MW
Unloaded Ea(out)/Ea(in) 1.55
Es/Ea 2
Pulse Heating ΔT: K (75.4MW@200ns)
16.9 - 23.8
95 100 105 110 11510
-7
10-6
10-5
10-4
Unloaded Gradient: MV/m
BK
D R
ate
: 1/p
uls
e/m
BKD Rate for 230ns
250hrs
500hrs
1200hrs
900hrs
500 1000 150095
100
105
110
115
Time with RF on: hrs
Gra
die
nt:
MV
/mGradient at 2e-6/pulse/m for 230ns pulse
Experiment DataPower Fit
Gradient Increase Over Time at a Constant Breakdown Rate
Hot Cell Flare-up
First T18 StructureTested at SLAC
0 5 10 15 200
10
20
30
40
50
Cell No.
Pe
rce
nt o
f BK
D E
ven
ts
394 BKDs within 0~250hrs193 BKDs within 250~500hrs298 BKDs within 500~750hrs57 BKDs within 750~900hrs74 BKDs within 900~1000hrs34 BKDs within 1000~1200hrs24 BKDs within 1200~1400hrs
BKD Distribution Along Structure at Different Stages of Processing
Did not find visual evidence related to the hot cell in a post-run boroscope exam – typical of NLC/GLC structures, many of which had hot cells
First T18 StructureTested at KEK
Operated 3900 hours
0 50 100 150 200 250 3000
20
40
60
80
100
120
BKD Rate (hr-1)Average gradient (MV/m)
50 ns 100 ns 150 ns 200 ns
This time, processed structure by progressively lengthening the pulse at constant gradient (110 MV/m)
Second T18 Structure Tested at SLAC
95 100 105 110 115
10-7
10-6
10-5
10-4
Unloaded Gradient: MV/m
BK
D R
ate
: 1/p
uls
e/m
BKD Rate for 230ns
250hrs
500hrs
1200hrs
900hrs
Comparison of current BDR rate (blue circle) with the rate curves from the First SLAC T18 structure at different processing times
T18_SLAC_2
-150 -100 -50 0 50 100 150-5
0
5
10
15
20
25
30
35
40
Reflected Phase: Deg
Fill
ing
tim
e fo
r d
iffe
ren
t ce
ll: n
sRF Breakdown LocationsBlue dots: T18_SLAC_2 after 250 hrs running
Red squares: T18_SLAC_1 after 1200 hrs running
0.5
1
1.5
30
210
60
240
90
270
120
300
150
330
180 0
Reflected Power -vs- Reflected Phase
T18_SLAC_2
CERN Built T18Cells made by Kugler, no etch, 820 degC vacuum braze at CERN,
installed in a vacuum can at SLAC
Copper grain size small due to ‘low’
braze temperature
Photo of Iris
0 10 20 30 40 50 60 70 80 900
50
100
Ave
rag
e U
nlo
ad
ed
Gra
die
nt: M
V/m
0 10 20 30 40 50 60 70 80 900
50
100 Bre
akd
ow
n R
ate
: 1
/hr70ns 230ns 200ns70ns
CERN T18 Processing History
Time (hr)
Breakdown Characteristics T18_Disk_1 during last 500 hrs, ~ 115 MV/m, 220 ns
T18_Disk_CERN during last 40 hrs, ~ 50 MV/m, 200 ns
-100 0 100-5
0
5
10
15
20
25
30
35
40
Reflected Phase: Deg
Fill
ing
tim
e fo
r d
iffe
ren
t ce
ll: n
s
0 10 20 300
0.2
0.4
0.6
0.8
1Missing Energy -vs- Breakdown Position (cell #)
-100 0 10010
-2
10-1
100Reflected Power -vs- Reflected Phase (deg)
0 50 100 150 200 250
0
0.2
0.4
0.6
0.8
1Missing Energy -vs- Time of Breakdown (ns)
Time of Breakdown (ns)
Fra
ctio
nal M
issi
ng E
nerg
y
Loca
tion
of B
reak
dow
n (n
s)
Iris 12 Autopsy
A 200 micron long calcium and carbon rich object that appears to have caused surface melting over a 1 mm wide area on this iris
4 6 8 10 12 14
0
0.05
0.1
0.15
0.2
0.25
0.3
0.35
Position (a.u.)
E fie
ld (
a.u
.)
11.427 GHz FROM INPUT
CERN T24 Disk Structure
Cells 24+input+output
Filling Time: ns 61
Length: cm 30 (wg2wg)23 (24+2 cells)
a/λ (%) 12.6 - 9.4
vg/c (%) 1.8 - 0.9
S11/ S21 0.016 / 0.715
Phase Advance Per Cell 2/3
Power Needed <Ea> = 100 MV/m 42.4 MW
Unloaded Ea(out)/Ea(in) 108/90
Es/Ea 2
Pulse Heating ΔT: K (<100MV/m>@100ns)
7.5 – 8.4
Field Profile Along the Structure
T24 Fabrication• Manufactured
at VDL, Q4 ‘08 • Assembly at CERN with
“new” procedure (following T18 task force ) Apr-Jun 09
• Pre-fire of disks at 1040 ˚C. Resulting uneven surface caused braze leaks
• Cells oxidized at one point but it was removed with 650 ˚C bake
• Now back at CERN for evaluation
0 10 20 30 40 50 60 70 80 90 1000
10
20
30
40
50
60
Time with RF On (hr)
Average Unloaded Gradient (MV/m)BKD Rate (1/hr)
T24 Processing History at 100 ns and Shorter Pulse Lengths
0.2
0.4
0.6
0.8
30
210
60
240
90
270
120
300
150
330
180 0
Reflected Phase -vs- Relfected Power (max)
0 10 20 30 40 50 60-10
0
10
20
30
40
50
Bkd Event Number
BK
D P
ositi
on (
ns)
Breakdown Locations
Summary• With strong dependence on structure fabrication
technique, cannot evaluate performance dependence
on structure geometry (a,vg,phi)
• Quad approach does not appear viable
– Need to improve quad ‘z’ alignment and reduce virtual leaks
– Probably cannot allow irises to touch nor have a low phase advance per cell
(which lowers Es/Ea)
– Should do a final test of a 2/3, brazed version with slots
• T18 design is very promising, but not optimal for CLIC
– Three versions have operated at CLIC-like parameters although they take
> 1000 hours of operation to achieve low breakdown rates
• Future
– CERN adopting SLAC-like structure assembly techniques
– Verify T24 with HOM damping meets CLIC specs (will test TD18_disk first)
LC