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The Injector Design C.Y. Tan 01 Sep 2011 1 The Injector BNL - - PowerPoint PPT Presentation
The Injector Design C.Y. Tan 01 Sep 2011 1 The Injector BNL - - PowerPoint PPT Presentation
The Injector Design C.Y. Tan 01 Sep 2011 1 The Injector BNL (2009 line) FNAL Proposed 1 x 35 keV H- source (round 2 x 35 keV H- sources (round type) type) on a slide LEBT (~ 4 m) For redundancy Short LEBT (~118 cm)
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The Injector
- 2 x 35 keV H- sources (round
type) on a slide
- For redundancy
- Short LEBT (~118 cm)
- 2 solenoids for focusing
- Xe gas for neutralization
- Einzel lens chopper
- RFQ 201.25 MHz, 1.2 m long
- Short MEBT (1 m)
- 2 sets of doublets
- 1 BNL style buncher
- 1 x 35 keV H- source (round
type)
- LEBT (~ 4 m)
- 2 x solenoids
- Xe gas for neutralization
- 1 Einzel lens
- 1 electrostatic chopper.
- RFQ 201.25 MHz, 1.5 m long
- Short MEBT (0.73 m)
- 1 set of triplets
- 1 buncher
FNAL Proposed BNL (2009 line)
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H- Source
- BNL style round (dimpled) magnetron source.
- More discussion in D. Bollinger's talk.
- BNL has very good experience with this type of
- sources. Very reliable.
- FNAL has a lot of experience with slit type
magnetron sources. Easier transition to round type.
- Good choice because it can use the same type of
hardware FNAL already has.
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LEBT
46.55”
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LEBT (cont'd)
- BNL source emit-
tance numbers
- RFQ input numbers
from manufacturer
- Assume beam is
neutralized.
Edge of beam pipe
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Solenoid Settings in Trace2D
Focal length is consistent with as built solenoid set to 500 A.
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FNAL Solenoids
Solenoids run DC. Water cooled. Settings probably > 500A. Designed by A. Makarov and V. Kashikhin.
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B field Measurements
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Small x-offset (~ 0.2 mm) in position and angle when current is changed from 500 A to 600 A. Do not expect to work below 500A. No change in y. Should be correctable with dipole correctors.
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Neutralization using N2 in test stand
N2 used. Good vacuum 1e-6 torr. Bad vacuum 1e-4 torr. Note: pressure gauge quite far from beam in test stand. Faraday cup measurement
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Chopper
- Einzel lens is used as a chopper
- Suggested by D. Raparia
- Lens placed close to the entrance of the RFQ
– Keep de-neutralization region to a minimum. – Beam is already tightly focused by the solenoid at this
- location. So neutralization is probably at a minimum here.
- Einzel lens as chopper experiments in the test
stand have verified that method works.
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Einzel Lens Chopper
- Simulation using SIMION
- Optimized lens
- 2” long
- 1.75” diameter
- -37 kV to stop 35keV
beam.
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Einzel Lens as Built
Designed by A. Makarov
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Chopper Timings
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Einzel Lens Test
Note there is scraping at the beginning of the pulse in the test stand. This is a different Einzel lens than the one that we will be using. This Einzel lens is 2” in diameter and 2.5” long. Note: injector lens is 1.75” diameter and 2” long.
- F. Cup
Toroid
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Einzel Lens Test (cont'd)
Rise time on Faraday cup is bet- ter than 50ns. Con- sistent with thyrat- ron turn on of 35 ns. Ringing from finite bw of Faraday cup.
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LEBT Corrector Dipoles
Designed to fit over 4” beam pipe. Corrects drop in integrated Bdl when placed close to iron. 10A corrects 1 deg. H+V in one < 1.5” package.
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RFQ
Designed by A. Schempp. Tuned by J. Schmidt and B. Koubek. Rod type RFQ.
>
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As found RFQ parameters. Note frequency is 190 kHz too low.To be cor- rected with tuner.
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PARMTEQM Simulations
Transmission effi- ciency > 99% for 60mA beam.
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PARMTEQM Simulations (cont'd)
Input Output
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MEBT
Doublet – Buncher – Doublet (30 cm longer compared to BNL MEBT)
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MEBT Simulations
PARMILA shows 95.1% of the beam is captured at the end
- f DTL 1.
Note: Lattice of DTL not well understood! Using “as found” DTL lattice from M. Popovic. Note: Quads are very strong
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Before doublet After Buncher Before Tank 1 End of Tank 1
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Buncher
Same as BNL (except FNAL buncher is made of copper while BNL buncher is made of aluminium) Designed by M. Okamura. Must have grids to get transit time factor correct. Low power test without grids are complete at FNAL. With grid has been done in Japan.
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Grids
Grids to correct transit time factor. Picture is BNL grids.
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Bead Pull Data
FNAL Japan Full width half height ~ 30mm gap. With grid effectively re- duces gap or increases transit time by 40%
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Doublets (Quads with embedded corrector dipoles)
Quadrupole runs DC and water cooled. Iron core. Has embedded corrector dipoles. Overall length of doublet is 7”, 1.5” beam pipe.
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Quadrupole Design
Single quad. 4.4 kA/pole Doublet 4.4 kA/pole 400A and 11 turns per pole Field inhomogeneity is 1.7% @ 1 cm with F/D at 4.4kA/pole.
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Sextupole Component from Dipole
Integrated vertical dipole field at centre And 1 cm
The dipole contributes a sextupole component
- f Sint=0.56410-4 Tm when powered to de-
flected beam 0.2 deg. (gives 1mm deflection from last corrector to the DTL, Bdl = 0.4510-3 Tm) If integrated sextupole field A3 < 0.5% of integ- rated quadrupole field, transverse emittance blow up < 1%.
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Coupling
If quad random rolls < |0.5| deg for all 4 quadrupoles, emittance growth is < 1% at the start of DTL 1.
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Performance Goals
At minimum, must perform as well as present system.
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Conclusion
- Nothing in the design is technically
unachievable.
- Not pushing any envelopes!
- However, there are some concerns. See
“Outstanding Issues and Contingencies Talk”
- Copying as much as possible BNL design has
helped the injector design.
- There will be a lot of work to validate design in
the test set up.
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Acknowledgements
- D. Raparia, J. Alessi, M. Okamura (BNL)
- Generous hosts when we visited.
- Shared drawings of solenoid and quadrupoles.
- Allowed us to copy BNL buncher (Okamura)
– Fixes to BNL buncher that were incorporated into FNAL buncher.
- Discussions with D. Raparia
– Supplied initial input files to Trace, Parmila and Parmteqm.
- A. Makarov, V. Kashikhin, G. Velev (FNAL, TD)
- Designed and built solenoids, einzel lens and quads.
- All the personnel in Proton source, Mech. Support, EE Support.
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Backup Slides
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Test Stand
Einzel lens is 2” in diameter and 2.5” long. Note: injector lens is 1.75” diameter and 2” long.
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