Concept of PERLE, a High Intensity Energy Recovery Linac Facility Erk Jensen presenting a team effort of a growing collaboration (so probably I missed.

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Presentation transcript:

Concept of PERLE, a High Intensity Energy Recovery Linac Facility Erk Jensen presenting a team effort of a growing collaboration (so probably I missed some – sorry): Alex Bogacz (JLAB), Oliver Brüning, Rama Calaga, Nuria Catalan, Vera Chetvertkova, Rhodri Jones, Max Klein, Frank Marhauser (JLAB), Attilio Milanese, Dario Pellegrini, Juri Pupkov (BINP), Robert Rimmer (JLAB), Roberto Torres, Alessandra Valloni, Daniel Wollmann, Fabien Zomer (LAL) and special thanks to: Kurt Aulenbacher (U Mainz), Ilan Ben-Zvi (BNL), Ralf Eichhorn, Georg Hoffstaetter (Cornell), Andrew Hutton (JLAB) filo di PERLE

What are we talking about? Let’s call it PERLE for now (Powerful ERL for Experiments) – please propose a better name! Construction in stages: ◦ Initially: Injector – Cryomodule – Beam dump, ◦ add arcs ◦ add CM’s ◦ … later use as user facility … 24 June 2015 LHeC Workshop 2015 E. Jensen: Concept of PERLE2 900 MeV Up to sixteen 5-cell cavities in four cryomodules, 802 MHz, 19 MV/cavity

Why study ERL? Because it’s a great idea – accelerate, use the beam, decelerate and recover beam energy! This saves energy! For all large future accelerators we have an obligation to optimize their energy efficiency! Recovering energy or increasing efficiency one gains twice – since needing less energy also means smaller installation, less irradiation and less cooling. Look at the 50-year-old concept of Maury Tigner – can you see the TeV-range linear collider with energy recovery? To prepare technology for any future accelerator: it’s accelerator R&D at its best! 24 June 2015 LHeC Workshop 2015 E. Jensen: Concept of PERLE3 From M. Tigner: “A Possible Apparatus for Electron Clashing-Beam Experiments”, Il Nuovo Cimento Series 10, Vol. 37, issue 3, pp ,1 Giugno 1965

Why at CERN? CERN is intensifying R&D on SRF, getting ready for the next generation of HEP accelerators: LHC, HL-LHC, SPL, LHeC, FCC ◦ SRF needed for: LHC, HL-LHC, HIE-ISOLDE, SPL, LHeC, FCC see next pages. ◦ … the highlighted can directly take advantage of this facility It is important that the next generation of accelerator physicists, engineers and technicians can work and train with a real beam facility without risking interruption of LHC Physics! PERLE is above all a facility for SRF R&D! With it we can complement the SRF testing – typical sequence of tests: ◦ Sample tests in quadrupole resonator, ◦ low power tests of bare cavity in vertical cryostat, ◦ high power tests of dressed cavity in horizontal cryomodule, ◦ tests with beam (HOM excitation!) 24 June 2015 LHeC Workshop 2015 E. Jensen: Concept of PERLE4

SRF at CERN 1: LHC LHC: In operation: 4 cryomodules with 4 single-cell cavities each Recently, one module was swapped with the only spare module We are in the process to build another spare to guarantee LHC availability! Parameters: 401 MHz, 2 MV/cavity, 4 cavities/CM Nb sputtered on Cu 24 June 2015 LHeC Workshop 2015 E. Jensen: Concept of PERLE5 Nb-sputtered Cu cavity

SRF at CERN 2: HL-LHC Crab cavities are part of baseline for HL-LHC – w/o crab cavities, the available luminosity cannot be fully exploited. Prototypes have been built, CM’s are in construction, tests with proton beams are foreseen in SPS in 2018, production phase for 32 cavities plus spares: 2019 … 2024 Parameters: 401 MHz, 3.4 MV/cavity, 2 cavities/CM Also in HL-LHC: Study of harmonic cavities for LHC : 200 MHz and 802 MHz. 24 June 2015 LHeC Workshop 2015 E. Jensen: Concept of PERLE6 DQW: concept and prototype for vertical x-ing (IP1) RFD: concept for horizontal x-ing (IP5) CM concept (common)

SRF at CERN 3: HIE-ISOLDE 24 June 2015 LHeC Workshop 2015 E. Jensen: Concept of PERLE7 before … … and after sputtering Cavity preparation First completely assembled cryomodule

SRF at CERN 4: SPL 24 June 2015 LHeC Workshop 2015 E. Jensen: Concept of PERLE8 EP finish diagnostics HPR Preparing insert tuner test lowering into cryostat Pure SRF R&D project! Presently 704 MHz (ESS), but we’re considering change to 802 MHz. Bulk Nb, 5-cell SS He-vessel, alternative CM design

SRF at CERN 5: LHeC LHeC is presently not a high priority at CERN – but of course it was the LHeC study (Linac-Ring option) that triggered the study of an ERL and of PERLE. A cavity/cryomodule design is identical to that of PERLE. 802 MHz, bulk Nb, 5-cell cavities. 24 June 2015 LHeC Workshop 2015 E. Jensen: Concept of PERLE9 R. Calaga, M. Karppinen, K. Schirm, R. Torres-Sanchez (CERN) F. Marhauser, R. Rimmer (JLAB)

SRF at CERN 6: FCC Study FCC-hh: RF system approximately LHC system x5, 401 MHz (plus harmonic system 802 MHz), Nb on Cu FCC-ee: Huge RF system, 100 MW RF power in CW! ◦ 401 MHz and 802 MHz, maximum efficiency (including cryogenics) – challenging SRF R&D, Nb sputtered and bulk, new materials? More on next slide FCC-he: baseline is 60 GeV ERL identical to that of LHeC. 24 June 2015 LHeC Workshop 2015 E. Jensen: Concept of PERLE10

FCC-ee: 4 different machines! 24 June 2015 LHeC Workshop 2015 E. Jensen: Concept of PERLE11 ParameterHiggs st stage: 1.9 GV 401 MHz, RF power 12 MW nd stage: MHz, RF power 30 MW rd stage Z “Z-peak exploration”: MHz, RF power 50 MW rd stage top: MHz MHz, RF power 50 MW (baseline) Credits: U. Wienands

SRF at CERN: Summary 24 June 2015 LHeC Workshop 2015 E. Jensen: Concept of PERLE12 The CERN SRF R&D has to cover many areas, accelerators, technologies. Where possible, choices were made to exploit synergies! ProgrammeFrequency (MHz) LHC, spare and more401 MHz LHC upgrade200 MHz, 802 MHz HIE-ISOLDE101 MHz HL-LHC crab cavities401 MHz Linac4 (NC)352 MHz SPL (ESS)704 MHz LHeC, FCC-he, PERLE802 MHz FCC-ee, FCC-hh401 MHz & 802 MHz ProgrammeFrequency (MHz) ILC, X-FEL, LCLS-2, …1,300 MHz PIP-II650 MHz SNS805 MHz ESS352 MHz, 704 MHz eRHIC422 MHz JLAB MEIC953 MHz JAERI500 MHz CERNInternational

Motivation for PERLE: 24 June 2015 LHeC Workshop 2015 E. Jensen: Concept of PERLE13

Parameters of PERLE ParameterValue injection energy RF frequency acc. voltage per cavity # cells per cavity 5 # cavities per cryomodule 4 RF power per cryomodule # cryomodules 4 max. acceleration per pass injected beam current nominal bunch charge number of passes 23 top energy duty factor CW 24 June 2015 LHeC Workshop 2015 E. Jensen: Concept of PERLE14 With a photo-injector, other frequencies are possible – see next page!

Operation at different frequencies 24 June 2015 LHeC Workshop 2015 E. Jensen: Concept of PERLE15 ProgrammeFrequency (MHz) CERN frequencies200 MHz, 401 MHz, 704 MHz, 802 MHz ILC, X-FEL, LCLS-2, …1,300 MHz PIP-II650 MHz SNS805 MHz CERN Linac4, ESS352 MHz ESS704 MHz eRHIC422 MHz JLAB MEIC953 MHz JAERI500 MHz

Conceptual Layout 24 June 2015 LHeC Workshop 2015 E. Jensen: Concept of PERLE16 ARC 1 – 155 MeV ARC 3 – 455 MeV ARC 5 – 755 MeV Spreader/combiner Linac 1 Linac 2 “Odd” arcs“Even” arcs CM2 CM4 CM1CM2 Linac 1 CM1CM2

Staged construction 24 June 2015 LHeC Workshop 2015 E. Jensen: Concept of PERLE17 Stage 1 – 2 CMs, test installation – injector, cavities, beam dump. Stage 2 – 2 CMs, set up for energy recovery, 2…3 passes Stage 3 – 4 CMs, set up arcs for higher energies – reach up to 900 MeV 900 MeV

Linac and arc optics Arc optics (e.g. “odd” arcs) Linac optics 24 June 2015 LHeC Workshop 2015 E. Jensen: Concept of PERLE18 Linac 1 Linac 2 Arc 1 Arc 3 Arc 5

Arc Layout 24 June 2015 LHeC Workshop 2015 E. Jensen: Concept of PERLE m m 42.8 cm 98.5 cm 6.8 cm m 13.66

Injector & injector R&D 24 June 2015 LHeC Workshop 2015 E. Jensen: Concept of PERLE20 Materialwork functionobserved Q.E. laser power fo 20 mA observed maximum current observed lifetime Sb-based family, unpolarised 532 nm eV4-5%4.7 W** 65 mA [Cornell] No deterioration reported GaAs-based family, polarised 780 nm1.2 eV* %31.8 W*** 5-6 mA [JLAB] to be checked *- at NEA state, ** - at Q.E.=1%, *** - at Q.E.=0.1%

RF power 250 kW 50 kW 25 kW RF Power 24 June 2015 LHeC Workshop 2015 E. Jensen: Concept of PERLE21 New CERN 802 MHz, 60 kW CW IOT TX 9 units received & tested

Cavity and Cryomodule Design 24 June 2015 LHeC Workshop 2015 E. Jensen: Concept of PERLE22 JLAB design (based on SNS 805 MHz)CERN design (based on SPL 704 MHz) R. Calaga, M. Karppinen, K. Schirm, R. Torres-Sanchez (CERN) F. Marhauser, R. Rimmer (JLAB)

Development of digital LLRF system (Cornell type ?) Amplitude and phase stability at high Q 0 ~ 1 x 10 8 Reliable operation with high beam currents + piezo tuners In case of failure scenarios: cavity trips, arcs etc.. 9-cell cavities at HoBiCaT, Liepe et al. Rms amplitude stability Proportional Gain RF Controls 24 June 2015 LHeC Workshop 2015 E. Jensen: Concept of PERLE23

Further uses of PERLE Test facility for SCRF cavities and cryomodules (described above) Test facility for multi-pass, multiple-cavity ERL, reliability and operational aspects, Injector studies, Beam diagnostics developments and testing with beam, Possible use for detector development and experiments suggests ~1 GeV as final stage energy, Test facility for controlled SC magnet quench tests, Facility for gamma-ray generation via Compton backscattering, It may become the injector to LHeC ERL and to FCC-he. 24 June 2015 LHeC Workshop 2015 E. Jensen: Concept of PERLE24

Beam diagnostics application 24 June 2015 LHeC Workshop 2015 E. Jensen: Concept of PERLE25

Controlled quench & damage tests 24 June 2015 LHeC Workshop 2015 E. Jensen: Concept of PERLE26

Intensity for controlled quench 24 June 2015 LHeC Workshop 2015 E. Jensen: Concept of PERLE27

Goal: generation of high-energy, monochromatic, polarized photons via Compton scattering (for nuclear physics research) 24 June 2015 LHeC Workshop 2015 E. Jensen: Concept of PERLE28 Incident laser beam Incident electron beam Scattered laser beam

24 June 2015 LHeC Workshop 2015 E. Jensen: Concept of PERLE29 ELECTRON BEAM PARAMETERS Energy900 MeV Charge320 pC Bunch Spacing25 ns Spot size30 um Norm. Trans. Emittance5 um Energy Spread0.1 % LASER BEAM PARAMETERS Wavelength515 nm nm Average Power300kW kW Pulse length3 ps Pulse energy7.5mJ - 15 mJ Spot size30 um Bandwidth0.02 % Repetition Rate40 MHz Incident electron beam Incident laser beam

24 June 2015 LHeC Workshop 2015 E. Jensen: Concept of PERLE30 GAMMA BEAM PARAMETERS Energy30 MeV Spectral density9*10 4 ph/s/eV Bandwidth< 5% Flux within FWHM bdw7*10 10 ph/s ph/e - within FWHM bdw10 -6 Peak Brilliance3*10 21 ph/s*mm 2 *mrad 2 0.1% bdw e-beam energy 1 GeV

Summary 24 June 2015 LHeC Workshop 2015 E. Jensen: Concept of PERLE31