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![Page 1: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/1.jpg)
The NLC RF Pulse Compression and High Power RF Transport Systems
Sami G. Tantawi, G.Bowden,
K.Fant, Z.D.Farkas, W.R.Fowkes
J.Irwin, N.M.Kroll,
Z.H.Li, R.Loewen, R.Miller,
C.Nantista, J.Rifkin, R.Ruth,
A.Vlieks, P.Wilson.
![Page 2: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/2.jpg)
Outline
• System Requirements • Comparison between Different Pulse Compression
Systems• Single Moded Delay Line Distribution System (DLDS) • Multi-Moded DLDS• Summary• Collaborative work with KEK (Y. H. Chin)
– Development of multi-moded components
– Mode stability experiment
![Page 3: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/3.jpg)
System Requirements and Goals
• Efficiency from klystrons to accelerator structures should exceed 85%.– Limited choice of systems– Component efficiency including copper losses should be better than 99%.
• Output Pulse should be flat for approximately 253 nS with a linear ramp at the beginning for approximately 104 nS. (Again this limits the choice of possible systems)
• The system should be cost effective– Reduced length of vacuum over-moded delay lines– Compact, and mechanically simple components.
• Peak surface field should be less than 40 MV/m at the rated rf power (600 MW for most components)
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The development of various pulse compression systems has been an ongoing program at SLAC for over 10 years.
• Pulse compression systems that have the potential of achieving the NLC requirements and have been studied are:
– Resonant Delay Lines (SLED-II) • Active SLED-II• Multi-moded SLED-II
– Binary Pulse Compression (BPC)• Multi-Moded Reflective BPC
– Delay Line Distribution System (DLDS)• Multi-Moded DLDS• Active DLDS
• For each of these systems we calculated the following:– efficiency– number and cost of components– length and cost of delay lines– cost of klystrons– cost of modulators
![Page 5: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/5.jpg)
Mode Launcher (A set Of 4 hybrids)
~7.4 cm Circular Waveguide
Single-moded DLDS
Klystron
~53 m
~12.7 cm Circular Waveguide Propagating The TE01 mode
Tantawi 8/97
Load
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Single Moded DLDSThis system contains ~260 km of vacuum 4.75”-diameter waveguides
• Propagation of TE01 mode in circular over-moded waveguides, NLCTA experience
• Pump-outs
• Mode Converters
• Hybrids
• Flanges
• Tapers
• 90-Degree Bends
• Power Dividers for the Local Distribution System
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• Experience gained from NLCTA – Propagation of the TE01 mode in highly over-moded waveguides (94
modes in the WC475, and 41 modes in WC293• Effect of Mechanical Tolerances on Circular Waveguides
– Diameter, Offset, Tilt, and Roundness
– Resonant Effects, and Mode Filters
• Design of Flanges
• Assembly Procedures
• Pump-outs
• Tapers
• Mode Converters (Flower Petal)
• Hybrids (Magic Tees)
• Measurement Techniques
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The theoretical losses / 100 ns for a delay line with 4.75” diameter is 0.54%. This is
the delay line size used at the SLED-II pulse compressor at SLAC.
Test Lab
SLED II
NLCTA
Station #0
NLCTA
Station #1
NLCTA
Station#2
Compression Ratio 8 6 6 6
Pulse width (nS) 150 223 245 245
Delay LineLosses/100nS (%)
1.63 0.68 0.58 0.59
Intrinsic Q 4.3x105 1.05x106 1.37x106 1.21x106
Total Delay LineLosses (%)
5.05 3.63 2.34 2.39
External Losses (%) 4.85 6.89 6.36 5.26
Total Efficiency (%) 58.6 67.5 68.6 69.3
Comparison Between the 4 SLED II Systems at SLAC
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0
50
100
150
200
0
1
Pow
er (
MW
)
Relative Pow
er (Cold Test)
2
3
4
-0.1 0.3 0.7 1.1 1.5Time (µs)
SLED IIXL-4
SLED IIInput Pulse
High Power
Cold Test
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Most components have been designed with different concepts, for example:
• Mode Converters– based on the wrap-around concept– based on the Circular to Square Tapers
• Hybrids– Magic Tee– based on wrap around mode converters (Old concept)– based on circular to rectangular tapers (New Concept, presented here)
However, we present here only the most recent developments.
![Page 11: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/11.jpg)
Old Marie’ Mode Converter
Short Marie’ Mode Converter (GA)
Flower Petal Mode Converter
Wrap-Around Mode Converter. Tested
up to 480 MW
Several Generations of Mode Converter
Development
![Page 12: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/12.jpg)
HFSS simulation results for the wrap around mode converter. The color shades represents the magnitude of the electrical field. a. is a cut plane through the slots, b is a cut plane in the circular guide 2.5 cm away from the slots.
a
b
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Input
Output
Wrap-around Mode Converter
H-Plane Over-moded Hybrid
Iris
Delay Lines
Sled-II Configuration
0
100
200
300
400
500
0 0.5 1 1.5 2
Pulse compressor inputPulse compressor output
Pow
er (
MW
)
Time (micro-seconds)
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-5
-4
-3
-2
-1
0
11.3 11.35 11.4 11.45 11.5 11.55 11.6
Transmission throught the bend plus two TE10
rectangular to TE01
circular mode converters
dB
Frequency (GHz)
New 90-degree BendBased on Circular to Square Waveguide
Tapers
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-40
-35
-30
-25
-20
-15
-10
-5
0
11.174 11.2573 11.3407 11.424 11.5073 11.5907 11.674
Circular TE01
mode Reflection Coefficient
dB
Frequency (GHz)
3.81 cm
3.556 cm
1.905 cm
Type 1: TE01 Circular to Square Taper
Coupling of the TE01 in the circular guide to spurious modes in the square guide. At the design
length for Type 2 taper.
-70
-60
-50
-40
-30
-20
-10
0
11.174 11.2573 11.3407 11.424 11.5073 11.5907 11.674
Transmission from circular TE0 1
to rectangular TE2 2
T ransmission from circular TE0 1
to rectangular TM2 2
dB
Frequency (GHz)
Field pattern of Type 2 taper when coupling from TE12 in the circular guide to TE03 in the square
guide
Type 2: TE01 and TE12 Circular to Square Taper.
10.16 cm
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3.81 cm
A straight section. The cross section shape is given by
)2cos1.01()( 0 rr
2.54 cm
3.286 cm
2.54 cm
3.696 cm3.131 cm
Field Pattern as TE01in the circular guide get converted to TE20in the rectangular guide
-40
-35
-30
-25
-20
-15
-10
-5
0
11.174 11.2573 11.3407 11.424 11.5073 11.5907 11.674
Transmission to TE02
Transmission to TE20
Reflection to TE01
Reflection to TE21
dB
Frequency (GHz)
Type 3: TE01 Circular to TE20 Rectangular Taper.
![Page 17: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/17.jpg)
Accelerator Structure Distribution System
![Page 18: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/18.jpg)
8 Klystrons grouped in pairs
Single-moded DLDS
Mode Launcher (A set Of 4 hybrids)
~7.4 cm Circular
Waveguide
Accelerator Structure (~1.8 m)
~ 6 m~53 m
~12.7 cm Circular Waveguide
TE12 Mode Extractor
TE01
TE12 (Vertical)TE12 (Horizontal)
TE01
TE12 (Vertical)
TE01
TE12 Mode Extractor
Mode Launcher (Fed by four rectangular waveguides)
~7.4 cm Circular Waveguide
Accelerator Structure (~1.8 m)
8 Klystrons grouped in pairs
~ 6 m
TE01 Mode
TE01 Tap-off
Multi-moded DLDS
![Page 19: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/19.jpg)
Multi-Moded Delay Line Distribution System This system contains ~130 km of vacuum 4.75”-diameter waveguides
• Introduction
• Experimental Tools
• Components required to implement the system (Launcher and Extractor)
• Components based on over-moded rectangular waveguides
• Components based on the wrap-around mode converter (will be presented by Y. H. Chin as part of component development at KEK)
• Flanges
• Tapers
• Mode Rotation Problems
![Page 20: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/20.jpg)
0.5
0.6
0.7
0.8
0.9
1
1.1
1.2
4 6 8 10 12 14 16
Single Moded DLDSMulti-Moded DLDS (number of modes=3)Active DLDSMulti-Moded BPC (A high power circulator and 3 modes)Multi-Moded SLED II (A high power circulator and 3 modes) Active SLED II (One time Switching [7])Multi-Moded DLDS (n
k=4, number of modes =3)
Single-Moded DLDS (nk=4)
Rel
ativ
e C
ost
Compression Ratio
nk=8
![Page 21: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/21.jpg)
TE21
TE01 Mode Extractor
TE01
TE12 (Vertically Polarized)
TE01
TE12 (Vertically Polarized)TE12 (Horizontally Polarized)
Accelerator Structure (~1.8 m)
~7.4 cm Circular Waveguide
TE01
Mode Launcher (Fed by Four Rectangular Waveguides)
Klystrons
~ 6 m
TE12 to TE01 Mode Converter
~53 m
~12.7 cm Circular Waveguide
TE01 Tap-Off TE01 Mode Converter (Fed by Four Rectangular Waveguides)
TE21-TE01 Mode Converter
TE01 Mode Extractor(Power is Extracted Evenly Between Four Waveguides)
![Page 22: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/22.jpg)
~7.4 cm Circular Waveguide
TE01 Mode Extractor(Power is Extracted Evenly Between Four Waveguides)
TE01
TE12 (Vertically Polarized)TE12 (Horizontally Polarized)
TE01
TE12 (Vertically Polarized)
TE01
TE01 Mode Extractor
Mode Launcher (Fed by Four Rectangular Waveguides)
TE21
TE21-TE01 Mode Converter
Klystrons
~ 6 mTE01 Mode Converter (Fed by Four Rectangular Waveguides)
TE12 to TE01 Mode Converter
~12.7 cm Circular Waveguide
TE01 Tap-Off
SLAC
KEK
![Page 23: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/23.jpg)
Multi-Moded Structure test Setup
Mode Launcher (TE11 and TE01)Mode Pre-launcher, for testing launchers. The output phase of the four-waveguide output is controlled by the choice between the two inputs
![Page 24: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/24.jpg)
TE11 (Vertical)TE12 (Horizontal)TE01
TE11 (Vertical)TE11 (Horizontal)
TE11 (Vertical)TE01
TE01
TE01 Extractor
To Accelerator Structures
TE01 Launcher
Extractor Schematic Diagram
![Page 25: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/25.jpg)
TE12-TE11 Mode Converter TE12-TE11 Mode ConverterTE11-TE01 Mode Converter
TE01 Mode Extractor5”
![Page 26: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/26.jpg)
Modular Launcher
TE11 Launcher TE01 LauncherTE01 Launcher
Both Polarizations of T
E 11
TE 01
TE 01
”
![Page 27: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/27.jpg)
0.75
0.8
0.85
0.9
0.95
1
1.05
1.1
3 4 5 6 7 8 9
Single-Moded DLDSMulti-Moded DLDS
Rel
ativ
e C
ost o
f th
e rf
Sys
tem
Compression Ratio
Compression Ratio=WidthPulserAccelerato
WidthPulseKlystron
![Page 28: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/28.jpg)
Cost Model
)1(max rm Ct
rC
T
2max r
gm
Cvtl
crkk
aac CnP
PNN
2
1max gm
k
aa
ck
vt
P
PN
nL
k
aa
crk P
PN
CN
1
rkk
aakmk SA
P
PNSSSS 0
![Page 29: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/29.jpg)
000
0
1111 m
r
sm
r
sm
k
aa
cr
rsmmkm A
C
k
C
k
P
PN
C
CkANS
cc
r
pl
vll
rg
ckk
aaccc
pl
vlc nA
CDAAR
Cv
Pn
PNnANLDAAS
1
2
)1(
ka
r
rkk C
CAA
00
r
cpl
vll
r
k
c
r
sm
r
sm
m
a
r
r
rc
smc
vl
plmlkrr
C
nDkkR
C
n
k
C
k
C
kk
C
C
C
kkkkkRnDCS
k
2
)1(111
),,,,;,,,(
00
c
gvlv
lk
cc
k
mm A
vAk
A
Ak
A
Ak
,,
00
c
gp
lpl A
vAk
![Page 30: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/30.jpg)
Single Moded DLDS
3
771.46901DTE dB/S;
itc 9.0
rk Cn
5.0lR
1i
3
3
456.8
456.8
101
101
Dr
CD
t
C
r
T h e s y s t e m r e q u i r e s t h e f o l l o w i n g c o m p o n e n t s :
i . )( rk Cn h y b r i d s ( e a c h h y b r i d i s c o u n t e d a s o n e c o m p o n e n t )
i i . )( rk Cn l o a d s ( e a c h l o a d i s c o u n t e d a s o n e c o m p o n e n t )
i i i . rC2 T E 0 1 b e n d ( e a c h b e n d i s c o u n t e d a s o n e c o m p o n e n t )
i v . )1(log2 2 r
r CC
h i g h p o w e r h y b r i d s , e a c h h y b r i d i s c o u n t e d a s t w o c o m p o n e n t s .
v . 2
rC s u p e r - h i g h p o w e r h y b r i d s , e a c h i s c o u n t e d a s f o u r c o m p o n e n t s
H e n c e , t h e t o t a l n u m b e r o f c o m p o n e n t s i s g i v e n b y :
)1(log2 2 rrkc CCnn .
![Page 31: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/31.jpg)
Single Moded DLDS3
771.46901DTE dB/S;
itc 9.0
rk Cn
5.0lR
1i
3
3
456.8
456.8
101
101
Dr
CD
t
C
r
T h e s y s t e m r e q u i r e s t h e f o l l o w i n g c o m p o n e n t s :
i . )( rk Cn h y b r i d s
i i . )( rk Cn l o a d s
i i i . rC2 T E 0 1 b e n d
i v . )1(log2 2 r
r CC
h i g h p o w e r h y b r i d s
v . 2
rC s u p e r - h i g h p o w e r h y b r i d s
v i . 4
3 rC t a p - o f f s
systemunitKlystronsofNumbern
RationCompressioC
k
r
/
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T h e s y s t e m r e q u i r e s t h e f o l l o w i n g c o m p o n e n t s :
i . )( rk Cn h y b r i d s
i i . )( rk Cn l o a d s
i i i . rC2 T E 0 1 b e n d
i v . )1(log2 2 r
r CC
h i g h p o w e r h y b r i d s
v . 2
rC s u p e r - h i g h p o w e r h y b r i d s
v i . 4
3 rC t a p - o f f s
systemunitKlystronsofNumbern
RationCompressioC
k
r
/
Single-Moded DLDS
![Page 33: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/33.jpg)
Multi-Moded DLDS ;5.01
m
rp n
Cn
)1(
)1(2/1(
rr
pmrpl CC
nnCnR
m
pmrj
mj
pmjn
j
nnjC
n
nn
rt C 1
120
20
20
10
101
1011
1
T h e s y s t e m r e q u i r e t h e f o l l o w i n g c o m p o n e n t s :
i . )( rk Cn h y b r i d s
i i . )( rk Cn l o a d s
i i i . )( pr nC T E 0 1 b e n d
i v . pn m o d e l a u n c h e r .
v . )( pr nC m o d e e x t r a c t o r s .
systemunitKlystronsofNumbern
RationCompressioC
k
r
/
DDTE
67185.1336.909312 dB/S
3
771.46901DTE dB/S;
![Page 34: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/34.jpg)
rl C
R1
r
rCoff
sonsoff
s
Coffs
r
tC
1
111
3
456.8
10 D
T h e s y s t e m r e q u i r e t h e f o l l o w i n g c o m p o n e n t s :
i . )( rk Cn h y b r i d s ( e a c h h y b r i d i s c o u n t e d a s o n e c o m p o n e n t )
i i . )( rk Cn l o a d s ( e a c h l o a d i s c o u n t e d a s o n e c o m p o n e n t )
i i i . rC T E 0 1 b e n d ( e a c h b e n d i s c o u n t e d a s o n e c o m p o n e n t )
i v . O n e T E 0 1 m o d e l a u n c h e r , ( c o u n t e d a s t w o c o m p o n e n t s ) .
v . )1( rC s w i t c h e s ( e a c h c o u n t e d a s s i x c o m p o n e n t s ) .
T h e t o t a l n u m b e r o f c o m p o n e n t s i s g i v e n b y
452 rkc Cnn .
Active DLDS
![Page 35: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/35.jpg)
Single-Moded BPC
hC
CR rh
rl 1log
2
11
1
22
rk
r
rkk
Cn
PC
Cn
P
n
P
h
75
2log
75
2
75
2log
max2
maxmax2
3
3
9.16
9.16
101
101
Dr
CD
t
C
r
T h e s y s t e m r e q u i r e t h e f o l l o w i n g c o m p o n e n t s :
i . )2( kn h y b r i d s ( e a c h h y b r i d i s c o u n t e d a s o n e c o m p o n e n t )
i i . )2( kn l o a d s ( e a c h l o a d i s c o u n t e d a s o n e c o m p o n e n t )
i i i . 2 rC T E 0 1 b e n d ( e a c h b e n d i s c o u n t e d a s o n e c o m p o n e n t )
i v .
1
22
hrC
h h i g h p o w e r h y b r i d s , ( c o u n t e d a s f o u r c o m p o n e n t s ) .
v .
1
22
hrC
s p l i t t e r s ( e a c h c o u n t e d a s t h r e e c o m p o n e n t s ) .
T h e t o t a l n u m b e r o f c o m p o n e n t s i s g i v e n b y :
1842
1422
hCnn
hrkc .
![Page 36: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/36.jpg)
Multi-Moded BPC
hC
CnR rh
rml 1log
2
11
1
22
mn
i m
i
r
mn
i m
i
n
r
Cn
t
C 1
1
10
10
101
101
T h e s y s t e m r e q u i r e t h e f o l l o w i n g c o m p o n e n t s :
i . )2( kn h y b r i d s ( e a c h h y b r i d i s c o u n t e d a s o n e c o m p o n e n t )
i i . )2( kn l o a d s ( e a c h l o a d i s c o u n t e d a s o n e c o m p o n e n t )
i i i . 2 rC T E 0 1 b e n d ( e a c h b e n d i s c o u n t e d a s o n e c o m p o n e n t )
i v .
1
22
hrC
h h i g h p o w e r h y b r i d s , ( c o u n t e d a s f o u r c o m p o n e n t s ) .
v .
1
22
hrC
s p l i t t e r s ( e a c h c o u n t e d a s t h r e e c o m p o n e n t s ) .
v i . mhr n
Ch
1
22 m o d e c o n v e r t e r s , ( e a c h i s c o u n t e d a s o n e c o m p o n e n t )
T h e t o t a l n u m b e r o f c o m p o n e n t s i s g i v e n b y
mmhm
rkc nhnn
Cnn 21842
21422
![Page 37: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/37.jpg)
~7.4 cm Circular Waveguide
TE01 Mode Extractor(Power is Extracted Evenly Between Four Waveguides)
TE01
TE12 (Vertically Polarized)TE12 (Horizontally Polarized)
TE01
TE12 (Vertically Polarized)
TE01
TE01 Mode Extractor
Mode Launcher (Fed by Four Rectangular Waveguides)
TE21
TE21-TE01 Mode Converter
Klystrons
~ 6 mTE01 Mode Converter (Fed by Four Rectangular Waveguides)
TE12 to TE01 Mode Converter
~12.7 cm Circular Waveguide
TE01 Tap-Off
SLAC
KEK
![Page 38: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/38.jpg)
Eight 75-megawatt klystrons
RF
e+ or e- A Cluster of 9 Multi-Moded DLDS Sections
RF Power Sources
A Single Multi-Moded Delay Line RF Distribution System
Accelerator Structures
Delay Lines
![Page 39: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/39.jpg)
Relative Cost
Efficiency
Relative Cost
Efficiency
Waveguide Diameter (cm)
Waveguide Diameter (cm)
Single-moded System
Multi-Moded System
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C o m p n en t D e ve lo p m e nt
S in g le -M o d e d D L D S M u lti-M o de d D L DS E xp erim e n ta l S e tu ps(S L E D -II)
A p p lica tion
O ve r-m o d ed C ircu la r W a ve gu id esC o m p o ne n ts B a se d o n the W ra p-A rou n d M o de C o n ve rte r
T a p e rs
O ve r-M od e d R e cta n gu la r W ave g u id e C o m p o ne n tsC o m p o ne n ts b a se d o n H -p lan e d iscon tinu ties
A d ia b a tic T ap e rs Fro m R e c ta ng u la r T o C ircu la r G u id esT E 2 0 -----> T E 0 1T E 3 0 -----> T E 1 2
O ve r-M o de d R e c tan g u la r W a ve gu id esM ixe d w ith O ve r-M o d e d C ircu la r w a veg u id es
T yp e
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Mode Launcher (A set Of 4 hybrids)
~7.4 cm Circular Waveguide
Single-moded DLDS
Klystron
~53 m
~12.7 cm Circular Waveguide Propagating The TE01 mode
Tantawi 8/97
Load
![Page 42: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/42.jpg)
Wrap-Around Mode Converter for Tap-off, and extraction, tested to 320MW
![Page 43: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/43.jpg)
Instead of using a cutoff section to allow the extraction of the TE01 mode, one can use two mode converters cascaded together
![Page 44: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/44.jpg)
A short circuit
Y0=1 Y0=1
Y0=1 Y0=1
Y0=1
Y0=1
Y0=1Y0=1
5
1
5
2
5
4
5
25
2
5
1
5
2
5
45
4
5
2
5
1
5
25
2
5
4
5
2
5
1
jj
jj
jj
jj
S
4/
4/
Port 1
Port 2
Port 3
Port 4
If a signal is injected in port 1, it will all appear in port 3.
![Page 45: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/45.jpg)
TE12-TE01 Mode Converter
TE01 Mode Extractor
Compact Mode Extractor
![Page 46: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/46.jpg)
Compact Launcher
![Page 47: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/47.jpg)
Mode Pre-launcher, for testing launchers. The output phase of the four-waveguide output is controlled by the choice between the two inputs
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1.5”~7”
A bend based on transition from an over-moded rectangular waveguide to a circular waveguide
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TIMING
Because the rf power is being injected at different times into different modes that have different group velocities, one must pay a special attention to timing. The set of equation that need to be satisfied so that the each accelerator structure set get an rf pulse for a duration at the appropriate time are:
(1)
where L is the distance between accelerator structure sets, L1 is the distance between the launcher and first extractor, L2 is the distance between first and second extractor, L3 is the length of the delay line after the second extractor, vTE01 and vTE12 are the group velocities of the TE01 and TE12 modes respectively, and through are the delays due to the transmission of power from the main rf delay line system to the accelerator structure sets, i.e., the delay through and after the extractors.There are several choices for the lengths L, L1 through L3, and through that satisfy the above set of equations. An attractive choice is to set L1 through L3 equal to L, == and
(2)
This would lead to a fairly symmetric system.
);11
()()(
),11
()()(
),()(
0112234
01
3
0112123
01
2
1201
1
TETETE
TETETE
TE
vvL
c
L
v
L
vvL
c
L
v
L
c
L
v
L
)11
(0112
12TETE vv
L
![Page 50: The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,](https://reader035.fdocuments.us/reader035/viewer/2022062309/5697c0281a28abf838cd685d/html5/thumbnails/50.jpg)
LAUNCHER
Several ideas for the launcher have been proposed (8-9). In all of them a fundamental property of the launcher has been preserved: the launcher has only four inputs and the launcher has to launch four and only four modes. If this is preserved and the launcher is matched for all four different input conditions, because of unitarity and reciprocity the scattering matrix representing the launcher has to take the following form:
(3)
This form forces the isolation between inputs; i.e., if one of the four power supplies drops out or fails, the rest of the power supplies will not receive any reflected power.
00002/12/12/12/100002/12/12/12/100002/12/12/12/100002/12/12/12/12/12/12/12/100002/12/12/12/10000
2/12/12/12/100002/12/12/12/10000
S
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Advanced Concepts
• Distributed Elements
• Circulators
• Switches
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Summary• We have a design for all components required to
implement the Single Moded DLDS, and the Multi-Moded DLDS.
• Going from single-moded to multi-moded systems will be decided after the KEK-SLAC experiment which will study the propagation properties of the TE12 mode (Details of the experiment described by Y. H. Chin).
• High power experimental setups are being prepared to demonstrate these systems.
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