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A DDBA lattice upgrade of the Diamond ring. R. Bartolini, C. Bailey*, M. Cox*, N. Hammond*, R. Holdsworth*, J. Kay*, J. Jones**, E. Longhi*, S. Mhaskar*, T. Pulampong, G. Rehm*, R. Walker* John Adams Insititute and *Diamond Light Source ** ASTeC/Cockcroft Institute. - PowerPoint PPT Presentation
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A DDBA lattice upgrade of the Diamond ringA DDBA lattice upgrade of the Diamond ring
R. Bartolini, C. Bailey*, M. Cox*, N. Hammond*, R. Holdsworth*, J. Kay*, J. Jones**, E. Longhi*, S. Mhaskar*, T. Pulampong, G.
Rehm*, R. Walker*
John Adams Insitituteand
*Diamond Light Source** ASTeC/Cockcroft Institute
3rd Low Emittance Ring WorkshopOxford, 8 July 2013
OutlineOutline
• Diamond upgrade plansMBAs options consideredTools used for optimisationDDBA lattice and its evolution
• Cell2 modification for VMX beamlineAP and ID performanceDesign issues targeting VMX
• Technical subsystems (requirements, challenges and WIP)magnets (see C. Bailey’s talk on Tuesday)engineering integration (see N. Hammond’s talk on Wednesday)vacuum, RF, diagnostics, …
• Future work
3rd Low Emittance Ring WorkshopOxford, 8 July 2013
Emittance in 3Emittance in 3rdrd GLS, DR and B-factories GLS, DR and B-factories
Transverse coherence requires small emittanceDiffraction limit at 0.1 nm requires 8 pm
4
~ 2013
'yy'xx24
fluxbrilliance
2ph
2exx ,
2ph
2exx ',''
2xxxx )D(
2xxxx D )'('
4
Luph
uph L
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?
MAX IV 7BA 3 GeV 320 pm 500 mA SS length 5m DA 7mm w/errors
Sirius 5BA w/superbend
3 280 500 5m & 6m 5 mm w/errors
Spring-8 6BA 6 67.5 300 4.5m & 27m 3 mm w/errors
APS 7BA 6 147 100
Pep-X 7BA 4.5 11 200 5 m 10 mm w/errors
ESRF Phase II
7BA 6 130 200 5m 10 mm
SOLEIL QBA w/longit.. gradient dipole
2.75 980 (220)
500 Robins. Wiggler + beam adapter
Diamond mod. 4BA, 5BA, 7BA
3 45-300 300 5m & 7 m 2 mm
ALS 5BA - 7BA 2 50-100 500 5 m 2-3 mm
BAPS 7BA-15BA 5 50 150 10m & 7m 10 mm w/errors
tUSR 7BA 9 3 100 TEV tunnel 0.8 mm
Survey of low emittance lattices (Beijing Nov. 2012)
Lattice design at DiamondLattice design at Diamond
• Initial criteria
Reuse tunnel and beamlinesReuse as much hardware as possiblePhased installation (avoid long shutdown)
• Evolution of MBA design
Initial low emittance lattice design used standard MBA cells M = 7, 6, 5 and 4
It transpired that a 4BA cell can be modified to introduce an additional straight in the middle of an arc (a generalisation of SOLEIL’s approach*)
while keeping the dispersion small and the emittance small
3rd Low Emittance Ring WorkshopOxford, 8 July 2013
Lattice design at DiamondLattice design at Diamond
Early studies with MBAs
3rd Low Emittance Ring WorkshopOxford, 8 July 2013
Original DBA
0 5 10 15 20X[m]
-8
-6
-4
-2
0
2
4
6
8
10
Y[m]
5BA
5BA and 7BA fitting Diamond cell length5BA and 7BA fitting Diamond cell length
Original DBA
0 5 10 15 20X[m]
-8
-6
-4
-2
0
2
4
6
8
10
Y[m]
7BA
5BA optimisation5BA optimisation
Driving term compensation after 4 cells
Fourth order and detuning terms much harder to compensate
MOGA sumDiff + sumRDTs using harmonic sextupoles; chromaticity (2,2)
DA optimisationDA optimisation
3rd Low Emittance Ring WorkshopOxford, 8 July 2013
The optimisation of the DA and lifetime is an iterative process that involves
Linear optic matching and working point selectionRDT analysis, FM and detuning curve checkMOGA
DA achieved (WIP) 4BA DA 5 mm5BA DA 3.5 mm7BA DA 1 mm
IBS emittance blow-up as a function of stored current coupling 10% 900 bunches – computed with elegant
4BA H emittance
IBS emittance increaseIBS emittance increase
3rd Low Emittance Ring WorkshopOxford, 8 July 2013
5BA H emittance 7BA H emittance
4BA lattice 265 pm 280 pm @ 300 mA relative increase 6%
5BA lattice 140 pm 180 pm @ 300 mA relative increase 29%
7BA lattice 45 pm 90 pm @ 300 mA relative increase 100%
300 mA 300 mA 300 mA
Lattice design at DiamondLattice design at Diamond
4BA
3rd Low Emittance Ring WorkshopOxford, 8 July 2013
• Increase dispersion at chromatic sextupoles• Optimize magnets positions and length leaving more distance between dipoles
(no coil clash)• removed sextupoles in the new straight• Longer mid-cell straight section from 3m to 3.4 m – longer is unmanageable
A 4BA lattice for Diamond-IIA 4BA lattice for Diamond-II
0 5 10 15 20X[m]
-8
-6
-4
-2
0
2
4
6
8
10
Y[m]
original DBA cell
3rd Low Emittance Ring WorkshopOxford, 8 July 2013
This lattice combines the ideas of doubling the capacity of the ring with the low emittance
Parameters Modified 4BA
Circumference [m] 561.0
Emittance [pm.rad] 275
Tune Point [Qx / Qy] 50.76/18.36
Chromaticity(ξx / ξy) -128/ -94
straight sections [m] 9.1 / 6.7 / 3.2
Momentum compaction 1.02e-04
Bunch length [mm] 1.77
Energy spread (rms) 7.94e-4
Damping time h/v/s [ms] 14.78/19.60/11.70
Energy loss/turn [MeV] 0.573
A 4BA lattice for Diamond-IIA 4BA lattice for Diamond-II
3rd Low Emittance Ring WorkshopOxford, 8 July 2013
Optimisation (I): driving termsOptimisation (I): driving terms
Qx: 4.5 /cellQy: 0.775*2 /cell
1 superperiod i.e. 4 cells give (2n)pi
All first terms cancellation within 1 super period
Cell phase advance adjusted to compensate 1st order RDTsChromaticity set to (2,2): detuning terms still large; higher order resonances still large
3rd Low Emittance Ring WorkshopOxford, 8 July 2013
DA still below 5 mm – under optimisation
Optimisation (II): Multi-objective GA for DAOptimisation (II): Multi-objective GA for DA
3rd Low Emittance Ring WorkshopOxford, 8 July 2013
Lattice design at DiamondLattice design at Diamond
One (or more) modified 4BA cells in the present lattice
(to be called DDBA)
3rd Low Emittance Ring WorkshopOxford, 8 July 2013
One DDBA cell in the existing latticeOne DDBA cell in the existing lattice
DDBA cell
Replacing the existing cell2 with a DDBA cell
Introduces an additional straight section (bending magnet beamline upgraded to ID beamline)
Serves as a prototype for low emittance lattice upgrade
In line with phased upgrade Lots of R&D required (magnet design
challenging, vacuum with small apertures, engineering integration, etc)
Additional straight
3rd Low Emittance Ring WorkshopOxford, 8 July 2013
Cell 2 upgrade for VMXi-VMXmCell 2 upgrade for VMXi-VMXm
VMXm VMXi
3rd Low Emittance Ring WorkshopOxford, 8 July 2013
ID performanceID performance
(courtesy EL)
VMXi moved from the side branch to the middle of the straight 2
2 m U21 in-vac0.7 m U30 ex-vac
3rd Low Emittance Ring WorkshopOxford, 8 July 2013
Ring optics with and without the DDBA cell in cell2Ring optics with and without the DDBA cell in cell2
3rd Low Emittance Ring WorkshopOxford, 8 July 2013
Parameters
Emittance [m-rad]
Tune x Tune y ChromaticityLifetime [h]
2.5e-9 28.18 13.29
2,227 (29)
One DDBA: dynamic aperture and lifetime with MOGAOne DDBA: dynamic aperture and lifetime with MOGA
3rd Low Emittance Ring WorkshopOxford, 8 July 2013
Fight for space Fight for space
A constant priority in the AP design has been the safeguard of the maximum length in the new mid-cell straight section
• Mid-cell length increased from 3m to 3.2m to 3.4m – 3.5m proved unworkable
• pushing magnets apart, merging quads
• corrector magnets with special design
• coil overhang of magnets
• Shortening of ID vessel to maximise ID length: e.g. flexible taper length
3rd Low Emittance Ring WorkshopOxford, 8 July 2013
Saving space: merging quads Saving space: merging quads
0 5 10 15 20X[m]
-6
-4
-2
0
2
4
Y[m]
3m3.35m3.35m
4BA_1
OriginalDBA
0 5 10 15 20X[m]
-8
-6
-4
-2
0
2
4
6
8
10
Y[m]
3.35m3 m
3.35m4BA_2
4BA_33.2m
3.4m 3.35m3.35m
3rd Low Emittance Ring WorkshopOxford, 8 July 2013
Fight for space: Fight for space: 9cm H/V embedded correctors
3rd Low Emittance Ring WorkshopOxford, 8 July 2013
Saving space: reducing flexible taper length Saving space: reducing flexible taper length
3rd Low Emittance Ring WorkshopOxford, 8 July 2013
(half) DDBA cell(half) DDBA cell
3.4m mid-cell straight
55 T/m 15 cm
65 T/m 20 cm
-14 T/m 66cm
-15 T/m 96cm
55 T/m 15 cm50 T/m2
20 cm
Challenging magnets which require a small bore radius (15mm)but no showstoppers !
Other projects have much more agressive requirements
Even if the minimisation of the emittance is not a primary target, the tight control of dispersion and beta functions requires very strong quads
3rd Low Emittance Ring WorkshopOxford, 8 July 2013
Magnets for USR (Beijing November 2012)Magnets for USR (Beijing November 2012)
Diffraction limited emittance requires magnets with unprecedented strength in storage ring. High gradient and high precision required
quadrupole gradient MAX IV has 40.0 T/mESRF 100 T/mSpring8-II 80 T/mBAPS 50 T/m USR 90 T/m
quadrupoles in dipoles MAX IV has 9 T/m ESRF 30 T/m
sextupoles MAX IV has 4000 T/m2ESRF- USR 7000 T/m2
Spring-8 II 13000 T/m2)
BAPS 7500 T/m2
space between magnets (hard edge) 10 cm MAX IV has 2.5 cmApertures = 20-26 mm diameter in arcs MAX IV inner diam. 22 mm
3rd Low Emittance Ring WorkshopOxford, 8 July 2013
Ring optics with and without two DDBA cellsRing optics with and without two DDBA cells
3rd Low Emittance Ring WorkshopOxford, 8 July 2013
Parameters
Emittance [m-rad]
Tune x Tune y ChromaticityLifetime [h]
2.55e-9 29.1813.30
2,28.2 (23.h)
Two DDBAs: dynamic aperture and lifetime with Two DDBAs: dynamic aperture and lifetime with MOGAMOGA
3rd Low Emittance Ring WorkshopOxford, 8 July 2013
ConclusionsConclusions
Diamond is investigating a full ring upgrade for Diamond – II
Various MBA options are under analysis. We concentrated on a modified 4BA (DDBA) that doubles the capacity and reduces the emittance by a factor 10.
Feasibility studies for the cell2 upgrade to a DDBA cell are promising
• AP-wise the design is feasible• Many technical subsystems prove challenging but no showstoppers have been identified (magnets, vacuum, engineering integration, diagnostics,. …)• Benefit for ID performance are noticeable
Underpins R&D for the full upgrade. Significant further detailed design is needed, as well as R&D for vacuum vessel fabrication and NEG coating
Costing exercise is underway but the project has been fully supported from a technical point of view.
3rd Low Emittance Ring WorkshopOxford, 8 July 2013