Scaling VFFAG eRHIC Design Progress Report 4 July 15, 2013Stephen Brooks, eRHIC FFAG meeting1.

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Scaling VFFAG eRHIC Design Progress Report 4 July 15, 2013 Stephen Brooks, eRHIC FFAG meeting 1

Transcript of Scaling VFFAG eRHIC Design Progress Report 4 July 15, 2013Stephen Brooks, eRHIC FFAG meeting1.

Page 1: Scaling VFFAG eRHIC Design Progress Report 4 July 15, 2013Stephen Brooks, eRHIC FFAG meeting1.

Scaling VFFAG eRHIC Design

Progress Report 4

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Last time:

• Found FODO lattices rated for 9.4 and 9.5GeV– Extrapolation suggests both allow orbit excursions

of less than 7cm (k=30m^-1) with <10^-6 losses• But this is without alignment errors

– Location relative to resonances understood

• 9.5GeV/80% packing factor lattice became baseline for scaling VFFAG arc magnet design

• Synchrotron radiation ~10MW to first order

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I. Macroparticle Weighting

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Greater accuracy for tail losses

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• Generate macroparticles roughly uniformly as a function of normalised radius out to >10

• Weights are w = f(r)/g(r) where:– f(r) is desired real phase space density function– g(r) is density of generated macroparticles

• Details available in the note on distributions: http://stephenbrooks.org/ral/report/2013-9/4ddist.pdf

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Comparison: 9.5GeV FODO lattice

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Zoom: ‘resonance’ features remain

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Comparison: 8GeV FODO lattice

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Comparison: 9.4GeV FODO lattice

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Comparison: 10GeV FODO lattice

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II. Error Studies of FODO Lattice

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Tracking with translational errors

• Random offsets were generated for each magnet in 500 cells (then reused)

• Error in each axis a normal distribution with mean 0 and standard deviation – RMS 3D distance offset = sqrt(3) ~ 1.73– 99% single axis offset ~ 2.58– 99% 3D distance offset ~ 3.37

• Tracked 2 turns at 1.2GeV, disrupted beam

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Beam loss vs. error sigma

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Loss vs. k and for 9.5GeV lattice

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=100um transmission

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=100um beam centroid

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=100um norm. RMS emittances

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=10um transmission

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=10um beam centroid

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=10um norm. RMS emittances

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=2.5um transmission

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=2.5um beam centroid

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=2.5um norm. RMS emittances

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=1um transmission

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=1um beam centroid

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=1um norm. RMS emittances

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=0 transmission

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=0 beam centroid

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=0 norm. RMS emittances

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III. Synchrotron Radiation Losses

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Compensation-free designs

• FFAG arcs transmit a continuum of energies so don’t strictly speaking need compensation of synchrotron energy losses– All examples given for “9.5GeV” FODO lattice– Assumed FFAG straights radiate same rate as arcs

• Constraints:– My FFAG arcs won’t transmit beam below 1.2GeV– Assumed ring linac won’t transmit below 100MeV

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Schematic changes

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Before

Source, 10?MeV dump 100MeV

ERL1.1GeV

ERL

Compensation RF

After

~200MeVlinac

1.xGeVERL

100MeVERL?

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9-pass 10GeV (worst)

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9-pass 9GeV

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6-pass 10GeV

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6-pass 9GeV (<10MW)

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6-pass 9GeV to 13.5GeV, 6.1mA

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6-pass 9GeV to 14.9GeV, 3.3mA

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This may or may not be practical?

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Source, dump

Overdrive mode

197MeVlinac

1.474GeVnot quite

ERL

100MeVERL

RF

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4-pass 10GeV (~10MW, long linac)

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IV. VFFAG Options Comparison

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FFAG type Synchrotron radiation

Dynamic aperture / error tolerance

Time of flight Energy range / multiple rings

Vertical (nonlinear) scaling** #

10MW at 9-10GeV

Not impossible but difficult

1-beta effect only Infinite / one ring

Vertical linear nonscaling * ##

Potentially to 20GeV 50mA

Better?

Unknown but better than horizontal FFAG

Probably factor 3x / two rings for 10GeV, three rings for 20-30

Vertical nonlinear nonscaling *** ###

Potentially to 20GeV 50mA

Also bad?

At least as good as linear nonscaling VFFAG

At least as good as linear nonscaling VFFAG

Horizontal linear nonscaling * ##

20GeV OK Linear magnets Problematic Two/three rings

Non-FFAG 20GeV OK Presumably good Each ring exact Too many rings

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*, **, *** indicate complexity of magnets and correction#, ##, ### indicate conceptual difficulty

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V. Future Work

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Next steps (if scaling VFFAG)

• Develop “straight” cell for full ring lattice• Work with magnet and FFAG splitter designers• Decide on RF/linac energies• Open issues:

– Emittance growth from SR photon emission– Coherent synchrotron radation?

• “End-to-end” tracking of full ring– Eventually track with fieldmaps from magnet

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Next steps (if non-scaling VFFAG)

• Try linear field NS-VFFAG first (“Davidtron”)– Much less synchrotron radiation– Expect better dynamic aperture– Easier to build (correct and understand!) magnets– Will likely need a cascade of rings 1-3, 3-10 etc.

• Develop quadrupole field models for Muon1 and/or VFFAG tracker code

• Try to search and understand lattice space

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