Recent Developments at Diamond Ian Martin On behalf of the Diamond Team Particle Accelerators and Beams Group Meeting Daresbury Laboratory 10th April 2013 Talk Outline Diamond overview ARPES beam line Reduced coupling operation Low alpha with top-up Improved current stability Improved CSR spectral stability Possible future upgrades Diamond II options Modifying a single cell of existing ring Conclusions Ian Martin IOP PAB Group meeting, DL, (April 2013) Overview of Diamond 3rd Generation Synchrotron Light Source 100 MeV Linac 3 GeV booster synchrotron (158.4m) 3 GeV storage ring (561.6m) Mix of BM and ID beamlines (long and standard straight sections) Several modes of operation (all top-up): Standard (900 bunches / 300mA) Hybrid (686 bunches / 300mA + 1 bunch / 3mA) Two low-alpha modes (Short x-ray pulse / THz users) Ian Martin IOP PAB Group meeting, DL, (April 2013) Overview of Diamond Operational (15 ID, 4 Dipole) Optimisation (4 ID) Construction (4 ID, 2 Dipole) Design (3 ID, 1 Dipole) Anticipate all straights assigned and operational by 2017 Ian Martin IOP PAB Group meeting, DL, (April 2013) ARPES (I05) Undulator For the ARPES beamline, a 5m long APPLE-II device was installed in Nov 2012: Long straight section, beta functions larger than standard Large tune-shifts in both planes that need to be compensated Significant impact on the machine (reduction in dynamic aperture, lifetime) Photon Energy Device Period Number of Periods Nominal Length Technology Minimum Gap Peak Field Magnetic Material Ian Martin IOP PAB Group meeting, DL, (April 2013) 18-240 eV 140 mm 34 4.995 m APPLE-II 23.5 mm 0.9T (H) / 0.53T (C) / 0.63T (V) NdFeB y (mm) Dynamic multipole fields compensated using active shim wires 5 5 0 0 -5 -5 -40 -20 0 x (mm) 20 40 -20 0 x (mm) 20 40 0.2 x (mrad) 0.1 Vertical Polarisation Circular Polarisation Horizontal Polarization Uncorrected Corrected Uncorrected Corrected Uncorrected Corrected Tune Shift (ΔQx / ΔQy) -0.043 / 0.032 0.003 / 0.003 -0.030 / 0.026 0.005 / 0.004 -0.003 / 0.015 0.008 / 0.008 Beta Beat (x / y) 33% / 32% 3% / 3% 22% / 23% 2% / 2% 2% / 13% 5% / 6% 0 -0.1 -0.2 -40 Ian Martin IOP PAB Group meeting, DL, (April 2013) Active shim wires Insertion device Residual kick wire current (A) ARPES (I05) Undulator Reduced Vertical Emittance In response to request from Science Division, emittance coupling has been reduced from 1% to 0.3% for user operation (27 pm.rad to 8 pm.rad) Initially confined to machine development periods Two week period from 17th October to 1st November 2012 Standard operational mode since 6th March 2013 Benefits include increased brightness / transverse coherence, smaller spot size 1% coupling -0.15 -0.1 -0.1 -0.05 -0.05 y (mm) y (mm) -0.15 0 0 0.05 0.05 0.1 0.1 0.15 0.15 -0.2 -0.15 -0.1 -0.05 0 0.05 x (mm) 0.1 0.15 0.2 0.3% coupling -0.2 -0.15 Ian Martin IOP PAB Group meeting, DL, (April 2013) -0.1 -0.05 0 0.05 x (mm) 0.1 0.15 0.2 Reduced Vertical Emittance coupling lifetime current Coupling feedback started Ian Martin IOP PAB Group meeting, DL, (April 2013) Reduced Vertical Emittance Reducing vertical emittance leads to small focus on sample Ian Martin IOP PAB Group meeting, DL, (April 2013) Courtesy K. Sawhney Reduced Vertical Emittance Reducing vertical emittance leads to higher spatial coherence Ian Martin IOP PAB Group meeting, DL, (April 2013) Courtesy K. Sawhney Low Alpha The Diamond storage ring is run in a dedicated ‘low alpha’ mode 2-3 times per year Since Oct 2012, this has been in top-up with hourly injection cycles Short pulse mode (NANOSCIENCE beamline I06): Single bunch for time-resolved science Electron bunch length reduced to ~3.5 ps Priority on increased single bunch charge over minimum pulse duration (stable!) THz mode (MIRIAM beamline B22): Above bursting threshold to increase CSR gain in THz region Priority to extend CSR spectrum towards 100cm-1 Momentum Compaction Factor Number of bunches Bunch current Emittance coupling ratio Lifetime Injection efficiency (IDs open) VRF Micro-bunching instability threshold (SB) Bursting threshold (SB) Short Pulse Mode -1×10-5 400 + 1 50 µA (93 pC) 0.3% ~20h 30-40% 3.4MV ~30-35 µA ~55-60 µA Ian Martin IOP PAB Group meeting, DL, (April 2013) THz Mode -4.5×10-6 200 50 µA (93 pC) 1% ~20h 15-20% 3.4MV ~15 µA ~25-30 µA MIRIAM (B22) Spectrum 03/10/2012 04/10/2012 05/10/2012 Courtesy G. Cinque Ian Martin IOP PAB Group meeting, DL, (April 2013) Diamond Upgrade Starting to take a look at possible options for a future upgrade of the Diamond lattice* Initial criteria Reuse tunnel and beamlines Reuse as much hardware as possible Phased installation (avoid long shutdown) Different ‘flavours’ under consideration Evolution of 4 Bend Achromat (BA), 5BA, 7BA, ... More beamlines vs. lower emittance *see poster by T. Pulampong Ian Martin IOP PAB Group meeting, DL, (April 2013) 4 Bend Achromat 10 8 6 4 Original DBA Y[m] 2 0 Modified 4BA3.35m 3.35m -2 4BA -4 -6 -8 0 5 10 15 X[m] Magnet arrangement allows 24 additional short straight sections Natural emittance 275 pm.rad (factor 10 reduction on present lattice) Magnets and vacuum design challenging (high gradients / small apertures) Design utilises gradient bending magnets Harmonic number lowered by 1 to minimize transverse offset for existing beamlines (circumference reduced from 561.6m to 561.0m) Ian Martin IOP PAB Group meeting, DL, (April 2013) 20 5 Bend Achromat 10 8 6 4 Original DBA Y[m] 2 0 5BA -2 -4 -6 -8 0 5 10 15 20 X[m] Length of existing straight sections reduced to accommodate additional magnets Natural emittance 155 pm.rad (factor 17 reduction on present lattice) Phase advance across two cells matched to odd integer to help cancel sextupole driving terms and increase dynamic aperture (~4mm): x , cell 4 . 5 y , cell 2 . 5 Ian Martin IOP PAB Group meeting, DL, (April 2013) 7 Bend Achromat 10 8 6 4 Original DBA Y[m] 2 0 7BA -2 -4 -6 -8 0 5 10 15 20 X[m] Natural emittance 45 pm.rad (factor 58 reduction on present lattice) Basic design includes dispersion bump between dipoles 1-2 and 6-7 to ease correction of natural chromaticity Maximum sextupole strength factor 2 lower as a result Intra-beam scattering places upper limit on beam current that still allows low emittance to be maintained Ian Martin IOP PAB Group meeting, DL, (April 2013) MBA Comparison Existing DBA Modified 4BA 5BA 7BA Circumference (m) 561.6 561 561.6 561.6 Natural Emittance (pm.rad) 2600 276 155 45.7 Tune Point (Qx / Qy) 27.20 / 13.37 50.76/18.36 53.66/28.87 75.42/52.17 Natural Chromaticity (ξx / ξy) -80.4 / -35.6 -128/ -94 -130/-50 -348 / -119 Momentum compaction 1.66×10-4 1.02×10-4 1.30×10-4 0.80×10-4 Max Quad. Strength (m-2) <2 (1.99) <7 <7 < 10 Max Sext. Strength (m-3) <35 (20.0) < 380 < 700 < 326 - 288 192 103 11.3 / 8.3 9.1 / 6.7 / 3.2 9.5/6.5 8.0 / 5.0 Emittance with IBS* (pm.rad) Length of straight sections# (m) *Intra-Beam Scattering calculated using ELEGANT for 450mA / 900 bunches / 10% coup / 3.3MV #Quadrupole to quadrupole separation Ian Martin IOP PAB Group meeting, DL, (April 2013) ‘DIAD’ Beamline Dual Imaging and Diffraction (DIAD) beamline requires high flux in the 4-40keV range Considering replacing existing cell with a modified 4BA 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) modified 4BA cell Additional straight Still work in progress; need to find solution with adequate dynamic aperture and lifetime before it could be considered. Other options include modified DBA cell or replacing second bending magnet with a 3T normal conducting super-bend. Ian Martin IOP PAB Group meeting, DL, (April 2013) Conclusions Work at Diamond is continuing on different fronts, partly by increasing the capacity of the facility by adding new beamlines, but also by upgrading existing beamlines and improving the performance of the accelerator itself (e.g. improving MTBF, reducing coupling, increasing beam current, beam stability, ...) Other current topics not mentioned so far: Low emittance optics for existing lattice Girder re-alignment program ‘COLDDIAG’ – diagnostic device to study head load on cryogenic surfaces Fast polarisation switching during user time (I10) Increasing beam current (350mA tests soon, working towards 500mA) 4th RF cavity Ian Martin IOP PAB Group meeting, DL, (April 2013) Acknowledgements ARPES (I05) S. Mhaskar, E. Longhi, B. Singh, R. Fielder, R. Bartolini Reduced Coupling Studies D. Hicken, M. Abbott, C. Thomas, R. Bartolini, K. Sawhney Low Alpha R. Bartolini, G. Cinque, M. Frogley, P. Karataev, A. Morgun, G. Rehm, W. Shields, C. Thomas, R. Walker Diamond Upgrade R. Bartolini, C. Bailey, M. Cox, N. Hammond, R. Holdsworth, J. Jones, J. Kay, L. Malysheva, N. Marks, S. Mhaskar, T. Pulampong, R. Walker, ... Ian Martin IOP PAB Group meeting, DL, (April 2013)