Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA,...
Transcript of Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA,...
![Page 1: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/1.jpg)
Overview of FETS
Alan Letchford
Proton Accelerators for Science and Innovation
Fermi National Accelerator Laboratory
11-13 November 2015
![Page 2: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/2.jpg)
• FETS will demonstrate front end technologies for
future high power proton drivers
• High power means 20 kW @ 3 MeV
= 1 MW @ 180 MeV
• FETS is at RAL because infrastructure and
support services are available
• FETS is generic – many possible applications
Motivation for FETS
![Page 3: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/3.jpg)
FETS Collaboration
![Page 4: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/4.jpg)
![Page 5: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/5.jpg)
What is FETS?
High brightness H– ion source
• 4 kW peak-power arc discharge
• 60 mA, 0.25 π mm mrad beam
• 2 ms, 50 Hz pulsed operation
Radio Frequency Quadrupole
• Four-vane, 324 MHz, 3 MeV
• 4 m bolted construction
• High power efficiency
Low Energy Beam Transport
• Three-solenoid configuration
• Space-charge neutralisation
• 5600 Ls-1 total pumping speed
Medium Energy Beam Transport
• Re-buncher cavities and EM quads
• Novel ‘fast-slow’ perfect chopping
• Low emittance growth
Diagnostics
• Non-interceptive
• Well distributed
• Laser-based
Beam Dumps
• Defocussing quads
• Water cooled cones
• Pure Al
![Page 6: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/6.jpg)
• High brightness Penning Surface Plasma
Source (SPS)
• Very high emission current density >1Acm-2
• Based on ISIS operational source
H– Ion Source
![Page 7: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/7.jpg)
60 mA 1ms 50 Hz
Maximum LEBT output:
![Page 8: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/8.jpg)
60 mA 2ms 25 Hz
OR
![Page 9: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/9.jpg)
This appears to be a fundamental limit of the present source design.
In order to fully meet the FETS beam requirements we must modify the
plasma geometry.
This has led to the VESPA experiment - Vessel for Extraction and
Source Plasma Analyses.
Ion source status and research is covered in Dan Faircloth’s WG1 talk
‘H- Ion Source Development at RAL’
![Page 10: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/10.jpg)
Low Energy Beam Transport (LEBT)
![Page 11: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/11.jpg)
Solenoid Design
![Page 12: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/12.jpg)
Solenoid magnets and 300 A
solenoid power supplies supplied
as part of our collaboration with
ESS Bilbao.
![Page 13: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/13.jpg)
LEBT Beam Transport Studies Although good
transmission was
achieved, a major concern
was significant
misalignment of the beam:
Configuring the LEBT for a pencil beam coupled with
particle tracking has allowed this to be almost
completely corrected:
![Page 14: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/14.jpg)
LEBT Matching Following successful realignment of the ion source beam and reliability
improvements to hardware, further parametric studies of the LEBT have been
performed to demonstrate the ability to match into the RFQ.
The LEBT beam can be taken
through a focus at the RFQ
matching plane. Although the
emittance is still a little large
this result gives us confidence
of being able to achieve a
reasonable match.
![Page 15: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/15.jpg)
The FETS RFQ
324 MHz, 3 MeV, 4 vane, 4m long
![Page 16: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/16.jpg)
RFQ Construction Sections made of 2 major and 2 minor vanes
3D o-ring
4 x 1 m long sections
bolted together
Vanes bolted together to
make 1 m sections
![Page 17: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/17.jpg)
Machining of all 4 sections is essentially complete except for a skim to their
final length following alignment.
![Page 18: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/18.jpg)
RFQ sections have been
surveyed at the manufacturer and
by RAL metrology.
Modelling the RFQ with as measured
errors demonstrates that we can
achieve the desired RF and beam
properties.
![Page 19: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/19.jpg)
Some RFQ sections have undergone
RF measurement in an attempt to
confirm the surveying results.
![Page 20: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/20.jpg)
RF distribution system design is complete and assembly of
delivered components has begun.
![Page 21: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/21.jpg)
The klystron, modulator and
circulator have been tested at
full power into dummy loads.
The LLRF systems for FETS
are being supplied by the
University of the Basque
Country in Bilbao.
![Page 22: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/22.jpg)
RFQ Power Coupler
The high power RFQ coupler
engineering design is complete and
its performance confirmed by
simulation. It will soon go for
manufacture.
![Page 23: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/23.jpg)
Medium Energy Beam
Transport Lattice Requirements:
• Perfect chopping
• Low beam loss: 3 MeV causes activation
• Low emittance growth
• Space for diagnostics
• Minimize cost i.e. reduce:
Number of components
Magnet & RF power
Achieving all of the lattice requirements simultaneously proved to be
challenging and time consuming.
![Page 24: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/24.jpg)
Parameter 2011 2013 Parameter 2011 2013
Beam Loss 2.5% 0.8% MEBT Length (m) 3.8 4.4
Quad Strength(T/m) 6-30 5.3-18.3 Emittance Growth(x-y-z) 20% 37% / 15% / -
3.5%
Cavity Voltage (kV) 50-150 <100 Extinction 99% 99.2%
Chopper Length
(mm)
450 604
MEBT Performance evolution
Chopper
off
Fast
chopper
on
Slow
chopper
on
MEBT Design Optimisation
![Page 25: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/25.jpg)
MEBT Elements
Fast chopper
Fast chopper
beam dump
Slow chopper
Slow chopper
beam dump
7 small bore quads
Vacuum manifold
3 rebunching
cavities
![Page 26: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/26.jpg)
MEBT Quadrupoles Small Bore
• 80 mm total length
• 20 Tm-1 gradient
• Integrated steering
• PSUs ordered
• Manufactured by Danfysik
Large Bore
• 160 mm total length
• 20 Tm-1 gradient
• Currently being manufactured
by Danfysik
![Page 27: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/27.jpg)
MEBT Rebunching Cavities
Re-bunching cavities:
• Re-entrant type cavities
• 324 MHz, ~8 kW peak power
• 100 kV effective voltage
• Copper plated stainless steel for lower cost
• Cavities are manufactured and in final plating.
• Dimensions and RF properties have been measured at various
stages to confirm modelling results.
![Page 28: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/28.jpg)
FETS Chopper
‘Perfect’ Electrostatic Chopping
Specification:
• No partially chopped bunches
• <2 ns rise time: between bunches
• ~150 μs gap in bunch train
• 6 kW dumped beam power
‘Fast-slow’ chopping scheme:
![Page 29: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/29.jpg)
3 Fast Chopper Designs
Helical
design
Planar
design
Suspended
micro-strip
design
![Page 30: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/30.jpg)
9 x Pulse generator cards
High peak power loads
Control and interface
Combiner
9 x Pulse generator cards
Power supply
9 x Pulse generator cards
9 x Pulse generator cards
1.7 m
Chopper Power Supply
![Page 31: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/31.jpg)
Slow Chopper The slow chopper deflector and feed-through design is nearing completion.
Design of the complete assembly with drivers is well underway.
![Page 32: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/32.jpg)
MEBT Diagnostics FETS will use toroids to measure beam current.
Both CERN shorted stripline BPMs and an in-house designed compact
button BPM will be used for position and bunch timing measurements. 6' ))-NA$*B WK* 6B *9$)-. " )*
! "#$%&' ( ) *+ &, *$- . $' / 012"1$( , %$( 1*) - , - + 0$! "#$%&' ( ) *+ &, *$- . $' / 012"1$( , %$( 1*) - , - + 0$
g*
^$@4 *@0$(&2($\ *ag*4 4 *WA$%&(' 9$*A$" . &, \ *aH*4 4 *8&@-"A$))*)&$$A*N' 9>*[ F ' *@" . A$*S2AA>*)-4 2A@&$9*-"*Q8K*] ' (;fh$(&;*($)' A2C' "*i *Ej 4 *
R!T 7Q[ *), ' (&$"$9*)&(-0A-"$*9$)-. "*
T Kk *N2e ' "*9$)-. "*
^$@4 *@0$(&2($\ *I H*4 4 *WA$%&(' 9$*A$" . &, \ *[ H*4 4 *8&@-"A$))*)&$$A*N' 9>*[ F ' *@" . A$*
![Page 33: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/33.jpg)
Laser Photo-detachment Diagnostic
FETS diagnostics is
covered in Stephen
Gibson’s WG1 talk
‘Diagnostics in FETS’
![Page 34: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/34.jpg)
• Every effort has been made to exclude
radiologically ‘bad’ materials from FETS.
• Even so significant shielding is required
to protect personnel from the expected
mSv/h levels of neutrons and gammas.
Radiation Protection
![Page 35: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/35.jpg)
Radiation shielding
• A shielding concept has
been developed and
approved by RAL RPA
• Most of the concrete except
the roof is in place.
• Roof design complete and
procurement underway.
![Page 36: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/36.jpg)
Cooling Plant
The unstabilised demin circuit is
commissioned.
The high stability demin circuit is
installed and awaiting commissioning.
Most of the plumbing is complete.
![Page 37: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/37.jpg)
• Primary equipment:
ISIS Control System
CompactPCI crates
X-windows/Exceed user interface
• Experiments and diagnostics:
PXI crates
Labview user interface
• Personnel Interlocks:
Hardwired relays and PLC systems
Compliant with relevant safety standards
Control Systems
![Page 38: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/38.jpg)
FETS is funded until the end of 2017.
By then we have to install all the rest of the
equipment, commission a 3 MeV beam, measure
the beam parameters and demonstrate chopping.
Discussions have started with interested parties on
potential future exploitation. Possibilities include
material irradiation or development of a low energy
neutron source based around FETS.
Outlook
![Page 39: Overview of FETS · High brightness H– ion source • 4 kW peak-power arc discharge • 60 mA, 0.25 π mm mrad beam • 2 ms, 50 Hz pulsed operation Radio Frequency Quadrupole •](https://reader036.fdocuments.net/reader036/viewer/2022080718/5f78c46adca2297e9b04544d/html5/thumbnails/39.jpg)
Thank you for your attention.