pbg structure experiments, aac 2008 photonic bandgap accelerator experiments roark a. marsh, michael...
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PBG Structure Experiments, AAC 2008
Photonic Bandgap Accelerator Experiments
Roark A. Marsh, Michael A. Shapiro, Richard J. Temkin
Massachusetts Institute of Technology,Plasma Science and Fusion Center
Work supported by DOE HEP
PBG Structure Experiments, AAC 2008
Collaborators
Continuing collaboration with Jake Haimson and HRC
6 Cell structure was designed, built, and tested by Evgenya Smirnova, now at LANL
Wakefield simulations in collaboration with Kwok Ko at SLAC, and John DeFord at STAAR, Inc.
Breakdown experiments were designed to be tested, and in collaboration with Sami Tantawi and Valery Dolgashev at SLAC
PBG Structure Experiments, AAC 2008
Outline
17.14 GHz Experimental Results Lab 6 Cell Traveling Wave Structure Wakefield Simulations Wakefield Measurements
11.424 GHz Planned Experiments Single Cell Breakdown Structures Design of PBG Breakdown Structure
Future PBG Improvements and Experiments
PBG Structure Experiments, AAC 2008
Outline
17.14 GHz Experimental Results Lab 6 Cell Traveling Wave Structure Wakefield Simulations Wakefield Measurements
11.424 GHz Planned Experiments Single Cell Breakdown Structures Design of PBG Breakdown Structure
Future PBG Improvements and Experiments
PBG Structure Experiments, AAC 2008
HRC Relativistic beam Klystron:
Microwave PowerSource 25 MW @ 17.14 GHz
25 MeV Linac:0.5 m long
94 cells
Structure Test
Stand
MIT 17 GHz Accelerator
700 kV500 MW
Modulator
Photonic Bandgap
Accelerator
PBG Structure Experiments, AAC 2008
Motivation
Acceleration demonstrated but what about HOMs?
2D Theory predicts all HOMs in propagation band
PBG HOM Damping in practice is more complicated 3D Structure with disk loading (irises/plates) Propagation band means damping, but how much?
HOM Simulations need to be backed by experiments
Beam excitation of wakefields using 6 Cell structure
PBG Structure Experiments, AAC 2008
Experimental Setup
Structure is unpowered DC injector produces a train
of bunches Matched load on input port Diode detector observations
made through output port and vacuum chamber windows
1/17GHz = 60ps
100ns
Diode
Horn & Diode
Load
PBG Structure Experiments, AAC 2008
Experimental Setup Pictures
ChamberWindow
MatchedLoad
OutputPort
Window
View from Below
PBG Structure Experiments, AAC 2008
Bunch train with 1 mm rms bunch length and 17.5 mm spacing driven through structure
PBG Multi-Bunch SimulationMatched Load Output Port
Chamberwindow
PBG Structure Experiments, AAC 2008
Bunch train with 1 mm rms bunch length and 17.5 mm spacing driven through structure
PBG Multi-Bunch SimulationMatched Load Output Port
Chamberwindow
PBG Structure Experiments, AAC 2008
Bunch train with 1 mm rms bunch length and 17.5 mm spacing driven through structure
PBG Multi-Bunch SimulationMatched Load Output Port
Chamberwindow
PBG Structure Experiments, AAC 2008
Bunch train with 1 mm rms bunch length and 17.5 mm spacing driven through structure
PBG Multi-Bunch SimulationMatched Load Output Port
Chamberwindow
PBG Structure Experiments, AAC 2008
Bunch train with 1 mm rms bunch length and 17.5 mm spacing driven through structure
PBG Multi-Bunch SimulationMatched Load Output Port
Chamberwindow
PBG Structure Experiments, AAC 2008
16 18 20 22 24 26-100
-80
-60
-40
-20
0S21
[dB
]
Frequency [GHz]
Your text
Cold Test of PBG HOMs
17.14 GHz Q = 4000 group velocity = 0.0109
c
Lattice HOMs Q < 250
Low Q Lattice HOMs
PBG Structure Experiments, AAC 2008
Simulation of PBG Lattice HOMs Electric field from HFSS simulations of PBG Train of bunches means harmonics of 17.14 GHz Dipole mode not observed
Fundamental: 17 GHz, Q = 4000 Lattice HOM: 34 GHz, Q = 100
PBG Structure Experiments, AAC 2008
Measured 17 GHz Beam Loading Output Port diode measurement No fitting parameters, excellent agreement
vg 0.0109c
Q 4000
I 1.04 dB/m
r 98 MΩ/m
L 29.15 mm
Pb (Theory)
PBG Structure Experiments, AAC 2008
Measured 34 GHz Wakefields
Output Port diode measurement Awaiting theory, please help…
Quadratic fit
PBG Structure Experiments, AAC 2008
Experimental Results Summary
Summary of measurements for 100 mA average current
Observations made on Chamber window as well as Output Port
Multiples of 17.14 GHz observed up to 85.7 GHz with heterodyne receiver
PBG Structure Experiments, AAC 2008
Outline
17.14 GHz Experimental Results Lab 6 Cell Traveling Wave Structure Wakefield Simulations Wakefield Measurements
11.424 GHz Planned Experiments Single Cell Breakdown Structures Design of PBG Breakdown Structure
Future PBG Improvements and Experiments
PBG Structure Experiments, AAC 2008
SLAC Setup
TM01 Mode Launcher
Single Cell SW Cavity Input and end cells for matching Central test cell New design uses PBG as
central test cell
PBG Structure Experiments, AAC 2008
X Band PBG Structure Test
SLAC test stand with reusable TM01 mode launchers MIT designed PBG structure for high power testing Under construction
Tuning Parameters
Input Cell Radius 11.627 mm
PBG Cell Radius 38.87 mm
End Cell Radius 11.471 mm
Coupling Iris Radius 5.132 mm
PBG Rod Radii 2.176 mm
PBG Rod Spacing 12.087 mm
PBG Structure Experiments, AAC 2008
Design Results
Designed to have ½ field in each pillbox coupling cell, only full field region is in PBG “test” cell
Coupling optimized by minimizing S11 reflection from TM01 Mode launcher
Field on axis S11 Coupling reflection
PBG Structure Experiments, AAC 2008
X Band PBG Single Cell Structure Central PBG test cell Pillbox matching cells
First iris radius varied to optimize coupling
PBG Structure Experiments, AAC 2008
½ Field Full Field
PBG Structure Experiments, AAC 2008
Electric Field Plots
Electric field plots: top and side views 6.6 MW in = 100 MV/m gradient = 180 MV/m
surface field on iris
PBG Structure Experiments, AAC 2008
Magnetic Field Plots
Magnetic field plots: top and side views 6.6 MW in = 100 MV/m gradient = 0.8 MA/m
surface field on inner rod
PBG Structure Experiments, AAC 2008
Outline
17.14 GHz Experimental Results Lab 6 Cell Traveling Wave Structure Wakefield Simulations Wakefield Measurements
11.424 GHz Planned Experiments Single Cell Breakdown Structures Design of PBG Breakdown Structure
Future PBG Improvements and Experiments
PBG Structure Experiments, AAC 2008
PBG Structures, The Next Generation
1st PBG structure test made using: a/b = 0.18 Triangular lattice of cylindrical rods 3 rows of rods
Relatively high pulsed heating on inner row of rods
Next generation: PBG with low pulsed heating, high gradient, low lattice HOMs
Planned additional tests of improved PBG structures at 11.424 GHz, at SLAC and at 17.14 GHz, at MIT
PBG Structure Experiments, AAC 2008
Summary and Conclusions
Measured beam loading in PBG structure Excellent agreement with theory Measured HOMs at 34 GHz (waiting for theory…)
X-band standing wave PBG structure designed for SLAC, under fabrication
First high gradient, breakdown tested PBG structure
Future Plans Better PBG structures Testing at SLAC, and MIT
PBG Structure Experiments, AAC 2008
Any Questions?
Thank You
PBG Structure Experiments, AAC 2008
AbstractDamping wakefields is a critical issue in the next generation of high gradient accelerators. Photonic bandgap (PBG) structures have unique properties that offer significant wakefield damping. Experimental measurements of wakefields excited by an 18 MeV electron beam in a 6 cell, 17.14 GHz metallic PBG traveling wave accelerator structure are reported. Theory calculations including traveling wave beam coupling, and wakefield simulations using T3P and Analyst are discussed. Good agreement is obtained between theory and experiment. Design and status of an 11.424 GHz standing waves PBG breakdown experiment to be performed at SLAC are discussed. Current status and future plans for design work including future X-band PBG breakdown structures, and improved pulsed heating performance PBGs will be discussed.
Work supported by DOE HEP, under contract DE-FG02-91ER40648