1. Emanuel Karantzoulis– ESLS XXIII, 24-25 November, 2015 - PSI 1 Elettra Status and upgrades Emanuel Karantzoulis

2. Emanuel Karantzoulis– ESLS XXIII, 24-25 November, 2015 - PSI 2 Elettra Sincrotrone Trieste in brief: 2 complementary Light Sources FERMI Elettra

3. Emanuel Karantzoulis– ESLS XXIII, 24-25 November, 2015 - PSI FERMI 3  50 m Experim. Hall  100 m Undulator Hall  200 m Linac Tunnel + Injector Extension Seeded FEL, 1.5 (1.8 ) GeV, 10 Hz (50 Hz) – First Lasing Dec.13, 2010 Open to external users since 2012 (FEL-1), Courtesy A. Fabris

4. Emanuel Karantzoulis– ESLS XXIII, 24-25 November, 2015 - PSI FERMI Layout 4 FEL1 FEL2 I/O mirrors & gas cells PADReS EIS DIPROI LDM Photon Beam Lines slits experimental hall undulator hall Transfer Line FEL1 FEL2 L1 X-band BC1 L2 L3 L4 BC2 Electron linear accelerator tunnel PI Laser Heater Pump&Probe Autocorrelator Pump&Probe Autocorrelator Courtesy A. Fabris

5. Emanuel Karantzoulis– ESLS XXIII, 24-25 November, 2015 - PSI FERMI Overview 5  FERMI is a single-pass FEL user facility, based on the high gain harmonic generation scheme HGHG  Two FEL lines are available (externally seeded – single and double stage HGHG -> XUV spectral range characterized by a very high degree of coherence both in the longitudinal and transverse )  Three beam lines presently in operation: DiProi, EIS-TIMEX, LDM 320 - 62 eV 62 - 12 eV

6. Emanuel Karantzoulis– ESLS XXIII, 24-25 November, 2015 - PSI FERMI – electron/photon beam parameters 6

7. Emanuel Karantzoulis– ESLS XXIII, 24-25 November, 2015 - PSI Some results / future experiments Echo-Enabled Harmonic Generation (EEHG) at FERMI FEL-2 Feasibility study (E. Alaria et al.) 7 Multiple pulses are generated by double pulse seeding in different ways, depending on the requirements on the output radiation. Typical temporal separation between 250-300 and 700- 800 fs. (L. Gianessi et al.) Pulse compression in Chirped Pulse Amplification experiment (G. De Ninno et al.)

8. Emanuel Karantzoulis– ESLS XXIII, 24-25 November, 2015 - PSI FERMI – Status 8  FEL-1: open to external users since December 2012.  Nominal performance of FEL -2 reached in September 2014  FEL-2 open to external from the first users period of 2015. OPERATING HOURS DISTIBUTION Total operating hours6640 User operation284843 % Machine tuning112017 % Commissioning267240 %  Four calls from 2012 so far: 193 proposal, 76 on DiProI, 55 on EIS-TIMEX and 62 on LDM  At the last call for proposal deadline in January 2015, 68 proposals were submitted, 30% of them on FEL-2.  The oversubscription factor is about 3.5 (was 3.1 for the 3 rd call). M / Svandrlik et al., “The FERMI Seeded FEL Facility: Operational Experience and Future Plans”, IPAC 2015, Richmond, May 2015

9. Emanuel Karantzoulis– ESLS XXIII, 24-25 November, 2015 - PSI  Third generation light source, open to external users since 1994  The machine complex initially made of a 1 GeV linac and a storage ring operating at 2.0 and since 1998 also at 2.4 GeV, in 2008 built a full energy injector (2.5 GeV booster plus 100 MeV linac) and since 2010 operates in top-up mode. Elettra 9 Linac + Booster (114 m) Storage Ring (259 m) Operate also a storage ring FEL and superconducting systems ( a 3.5 T wiggler and a third harmonic cavity )

10. Emanuel Karantzoulis– ESLS XXIII, 24-25 November, 2015 - PSI Elettra in brief 10 Operating modes for users:  Operates for 6400 hours per year (24h, 7/7 ), 5016 hours for users  Top-up 2.0 GeV, 310 mA for 75 % of users time  Top-up 2.4 GeV, 160 mA for 25 % of users time  Filling patterns: multi-bunch 95 % filling or hybrid. Other filling patterns, as single bunch, few bunches or other multi-bunch fillings can be provided.  28 beam lines  In 2014: 947 proposals (10 % increase with respect to 2013)  Oversubscription rate from 1.5 to 3 depending on the beamline.

11. Emanuel Karantzoulis– ESLS XXIII, 24-25 November, 2015 - PSI IDs and brilliance 11 22 ID segments + 1 SCW installed -> 18 beam lines ( planar, elliptical, canted, electromagnetic) 6 bending magnet source points serving 9 beam lines + 1 IR = 10 beam lines

12. Emanuel Karantzoulis– ESLS XXIII, 24-25 November, 2015 - PSI 12 Uptime Statistics Mean fault duration ~ 0.9 hour No downtime from the injectors Maximum running without a beam dump: 603 hours, the average of maxima is about 300 hours

13. Emanuel Karantzoulis– ESLS XXIII, 24-25 November, 2015 - PSI 13 2010:4720 h scheduled, 94.6/96.1% uptime, MTBF = 42/52 h 2011:5000 h scheduled, 95.7/96.8% uptime, MTBF = 45/53 h 2012:5016 h scheduled, 96.1/97.1% uptime, MTBF = 57/71 h 2013: 5016 h scheduled, 96.9/98.0% uptime, MTBF = 60/77 h 2014: 5016 h scheduled 97.1/98.5 % uptime, MTBF = 63/80 h 2015 (at 79% of UT) : 5016 h scheduled 96.7/97.6 % uptime, MTBF= 63/67 h

14. Emanuel Karantzoulis– ESLS XXIII, 24-25 November, 2015 - PSI 14 Top-up statistics During top-up systems run well and the top-up % of user beam- time is high ~ 98%. The remaining 2% is due to failures that, however, do not impact on the availability. Orbit stability requirements met most of the time provided that ambient temperature is within the defined limits, i.e., ± 0.5oC ≤ ± The long term (>24 h) is ≤ ± 5  m ptp (max value for >120 h). Short term stability (< 24 hours) is at 2% of the beam size

15. Emanuel Karantzoulis– ESLS XXIII, 24-25 November, 2015 - PSI 15 Note: those failures did not produce downtime, however they could give a downtime if intensity dropped below 50% of the nominal. Considered when the intensity is less than 99.5% of the nominal Top-up downtime

16. Emanuel Karantzoulis– ESLS XXIII, 24-25 November, 2015 - PSI Elettra short term developments 16  Elettra has been upgraded during the years to keep the performance competitive to the new light sources being built in the recent years. Some current upgrades include:  RF upgrade (booster Solid State Amplifier )  PS-controls upgrade  Build new bpm electronics (detectors)  Upgrade vacuum system electronics  Studies are going on to exploit the margins for other relatively low impact upgrades to extend the performance to the ultimate limits allowed by the present machine also in terms of operability and stability. Some possibilities ( and actualities) include :  Increasing the energy to 2.5 GeV, 140 mA  Reduce the coupling by installing skew quadrupoles  Reduction of the emittance, presently closest to the theoretical limit for a DBA, with a new optics (60 % reduction if SCW not include, 20 if included at full field).  Unifying space in the arcs, to integrate the two separated shorter straight section in a 2.5 m straight to provide possibilities for new insertion devices.  Low alpha optics for short bunches ( coherent infrared – papers published ) E. Karantzoulis et al, “Elettra Status and Future Prospect”, IPAC 2015, Richmond, May 2015

17. Emanuel Karantzoulis– ESLS XXIII, 24-25 November, 2015 - PSI 17 At 1950 A out of a max of 2000 A of the dipole power supply. To reach 2.5 GeV a small additional power supply is needed. Energy upgrade

18. Emanuel Karantzoulis– ESLS XXIII, 24-25 November, 2015 - PSI 18 Low emittance optics (LEO) and SCW WP (14.3,8.2) E=7 nm rad at 2 GeV WP (16.3,7.2) E=2.6 nm rad at 2 GeV

19. Emanuel Karantzoulis– ESLS XXIII, 24-25 November, 2015 - PSI Independent check with elegant Including errors ref. S. Di Mitri Dynamic apertures Nominal Low emit. 19

20. Emanuel Karantzoulis– ESLS XXIII, 24-25 November, 2015 - PSI A.Carniel, E. Karantzoulis, S. Krecic Injecting and accumulating in the LEO Interesting result also for injection studies 20

21. Emanuel Karantzoulis– ESLS XXIII, 24-25 November, 2015 - PSI Elettra 2.0 21  Conceptual design study to investigate a successor to the machine, Elettra 2.0  Based on latest trends in this field, i.e. next generation, ultimate light sources (ULS):  Much higher brilliance (more than one order of magnitude at lower photon energies, e.g. 1 keV),  High level of coherence in both planes (3rd generation sources have only high vertical coherence),  Smaller spot size and divergence,  Higher flux and a variety of insertion devices. E. Karantzoulis, “Evolution of Elettra towards an Ultimate Light Source”, IPAC 2014, Dresden, June 2014, p. 258 (2014); http://www.JACoW.org

22. Emanuel Karantzoulis– ESLS XXIII, 24-25 November, 2015 - PSI Elettra 2.0 requirements 22  The requirements for the new machine have been developed based on the interaction with the users’ community and considering costs optimization.  A dedicated workshop on the future of Elettra was held in April 2014 to examine the different scenarios Design boundary conditions  keep the same building and the same ring circumference (259-260 m),  beam energy: 2 GeV,  keep the same beam intensity  keep the same filling patterns: multibunch, hybrid, single bunch, few bunches,  emittance: to be reduced by more than 1 order of magnitude,  electron horizontal beam size: less than 60 µm,  existing ID beam lines and their position should be maintained,  free space available for IDs: not less than that of Elettra  keep the existing bending magnets beam lines  use the existing injectors, that means off-axis injection. E. Karantzoulis, “Elettra2.0-The Next Machine”, IPAC 2015, Richmond, May 2015

23. Emanuel Karantzoulis– ESLS XXIII, 24-25 November, 2015 - PSI 23 M-bend achromat studies 2 GeV 100 mA, period 46mm, Np=98, L=4.5m 0.1 KeV Elettra 22% Elettra2.0 87% 1 keV Elettra 2% Elettra2.0 38%

24. Emanuel Karantzoulis– ESLS XXIII, 24-25 November, 2015 - PSI Elettra 2.0 Lattice 24 E. Karantzoulis, “Elettra2.0-The Next Machine”, IPAC 2015, Richmond, May 2015 Best configuration satisfying all user requests is based on a six-bend achromat. Three versions are examined for minimal position shift of the dipole beam lines. Possible new beam lines from central dipoles All dipoles at about 0.8T Emit: 0.25 nm-rad, WP 33.2, 9.3 Nat. chrom -63,-50, dE/turn: 162 keV Another solution with the 2 and 4 th dipole at 1.4 T PM + 2 quads Emit: 0.28 nm-rad, WP 33.2,9.3 Nat.chrom -81,-44, dE/turn: 202 keV A third solution with the 2 and 4 th dipole at 0.8 +1.2 T with a series of short PMs Emit: 0.25 nm-rad, WP 33.2,9.3, Nat.chrom -77,-55, dE/turn: 196 keV

25. Emanuel Karantzoulis– ESLS XXIII, 24-25 November, 2015 - PSI 3 new concepts 1.Series of short permanent magnets for bending and focusing (bend-wiggler) 2.Electromagnets with physical length = magnetic length 3.3D girders 25 Important issues Important issues 1. Physical (inter-magnet) space 2. Injection in a small dynamic aperture (shortly we’ll start injection simulations (shortly we’ll start injection simulations and (sextupole) optimizations (modeFRONTIER) and (sextupole) optimizations (modeFRONTIER) Issues and concepts

26. Emanuel Karantzoulis– ESLS XXIII, 24-25 November, 2015 - PSI 26 The bend – “wiggler” combination concept Substitute the 2&5 dipole with a series of small PM dipoles: 0.13 m, 1.51 deg, 1.4 T, k=0 0.13 m, 1.51 deg, 1.4 T, k=0 0.13 m, 0.86 deg, 0.8 T, k=-2.9 0.13 m, 0.86 deg, 0.8 T, k=-2.9 0.13 m, -0.86 deg, 0.8 T, k=-2.9 sum angle 5.6 deg Issues: Temperature dependence Opening – closing the magnet PM with gradients Longitudinal gradient

27. Emanuel Karantzoulis– ESLS XXIII, 24-25 November, 2015 - PSI 27 A PM scaled prototype (Ref. Bruno Diviacco)

28. Emanuel Karantzoulis– ESLS XXIII, 24-25 November, 2015 - PSI 28 Ref. D. Castronovo (Opera) Magnets Not final but important to see the feasibility and the dimensions. Use of new materials such as Cobalt – Iron alloys will also be considered The bending integrated quadrupole component will be done by only the pole profile geometry. In order to optimize space and performances, different coil and frame geometries must be evaluated. Space between the pole terminations will be employed in order to obtain the requested frame stiff. Different quadrupole designs have been started in order to cover all the optic and layout specifications. The quadrupole designs must be developed with the vacuum chamber in order to resolve all the possible transversal interferences (beam lines). Asymmetric poles geometry has been opted. The sextupole magnets have the higher design issue. The transversal interferences between coils and vacuum chamber must be resolved. Not classical coils distributions are under study.

29. Emanuel Karantzoulis– ESLS XXIII, 24-25 November, 2015 - PSI 29 Magnets with Lp=Lm (Ref. D. Castronovo)

30. Emanuel Karantzoulis– ESLS XXIII, 24-25 November, 2015 - PSI Comparison 30

31. Emanuel Karantzoulis– ESLS XXIII, 24-25 November, 2015 - PSI Elettra 2.0 brilliance 31

32. Emanuel Karantzoulis– ESLS XXIII, 24-25 November, 2015 - PSI 32 Conclusions Elettra is running well, many small projects contribute to this. Replacement of old / obsolete hardware is ongoing A conceptual design project for Elettra 2.0 is ongoing. Some new concepts are being tested. FERMI@Elettra is very successful giving unique opportunities to experimentalists. Many new ideas are used / will be tested.

33. Emanuel Karantzoulis– ESLS XXIII, 24-25 November, 2015 - PSI 33 Thank you for your attention