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Budker INP, Novosibirsk, Russia Novosibirsk Free Electron Laser Unique Source of the Terahertz and Infrared Coherent Radiation Presented by O.A. Shevchenko, BINP SFR-2016, 47 July 2016, Novosibirsk, Russia Budker INP, Novosibirsk,


  1. Budker INP, Novosibirsk, Russia Novosibirsk Free Electron Laser Unique Source of the Terahertz and Infrared Coherent Radiation Presented by O.A. Shevchenko, BINP SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  2. Budker INP, Novosibirsk, Russia Project participants V.S.Arbuzov, N.A.Vinokurov, P.D.Vobly, V.N.Volkov, Ya.V.Getmanov, I.V.Davidyuk, O.I.Deychuly, E.N.Dementyev, B.A.Dovzhenko, B.A.Knyazev, E.I.Kolobanov, A.A.Kondakov, V.R.Kozak, E.V.Kozyrev, V.V.Kubarev, G.N.Kulipanov, E.A.Kuper, I.V.Kuptsov, G.Ya.Kurkin, S.A.Krutikhin , L.E.Medvedev, S.V.Motygin, V.K.Ovchar, V.N.Osipov, V.M.Petrov, A.M.Pilan, V.M.Popik, V.V.Repkov, T.V.Salikova, I.K.Sedlyarov, S.S.Serednyakov, A.N.Skrinsky, S.V.Tararyshkin, A.G.Tribendis, V.G.Tcheskidov, K.N.Chernov, M.A.Scheglov, O.A. Shevchenko 2/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  3. Budker INP, Novosibirsk, Russia Outline • Brief introduction to the FEL physics • The NovoFEL accelerator design and operation • NovoFEL as three FELs based source of radiation • The third FEL commissioning and first experiments • Nearest and far future plans for the conclusion 3/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  4. FEL principle of operation  +  λ 2 K   λ ≈ w 1   γ 0 2   2 2 synchronisme condition which is necessary for the energy transfer γ ε d e = x V x 3 dz mc 4/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  5. FEL principle of operation FEL oscillator Equivalent scheme 0,3 0,2 ( ) ω G 0,1 noise Gain, a.u. 0,0 -0,1 -0,2 -0,3 -3 -2 -1 0 1 2 3 δω/ω ◊ , 1/N w 5/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  6. NovoFEL Accelerator Design Energy Recovery Linac 1 – injector, 2 – linac, 3 – bending magnets, 4 – undulator, 5 –dump Accelerator is the most important part of any FEL . ERL is the best choice for high power FEL . 6/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  7. NovoFEL Accelerator Design Energy Recovery Linac 1 – injector, 2 – linac, 3 – bending magnets, 4 – undulator, 5 –dump Accelerator is the most important part of any FEL . ERL is the best choice for high power FEL . 7/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  8. NovoFEL Accelerator Design Gun Injector 8/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  9. NovoFEL Accelerator Design Gun Injector Main linac Dump 9/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  10. NovoFEL Accelerator Design Gun Injector Main linac The first THz FEL Dump undulator sections 10/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  11. NovoFEL Accelerator Design Gun The second FEL Injector undulator Main linac The first THz FEL Dump undulator sections 11/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  12. NovoFEL Accelerator Design The third IR FEL Gun undulator sections The second FEL Injector undulator Main linac The first THz FEL Dump undulator sections 12/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  13. Horizontal tracks 1 st stage FEL 2 nd stage FEL undulator undulator Main linac

  14. 3 d stage FEL undulator

  15. Budker INP, Novosibirsk, Russia Siberian Center of Photochemical Research 120 m }S-0 1st 990 680 G 5450+15 kran-balki Zona 1200 2577 2880 Pol sohranit[ 725 1150 1150 625 1100 AM@S0 2000 900 1100 280 2000 2090 AM@S2 SP-111 1300 3000 %%c180 700 L}3 L}4 349 0@R@F@DR @R@F@G1 %%c110 @L@VR@S2 3x725=2175 71 1175 @L@VR@S4 71 SP-111A ЩПР1-3 B 3210 71 @L@VR@S0 1175 100 235 71 1450 1@R@F@DR 0@R@FS@R1 L}5 0@R@F@GS@R 700 @L@VR@S1 825 @R@F@G5 @L@VR@S6 @R@F@G4 2@R@F@DR 800 1250 @R@F@G0 @R@F@G2 @R@F@G3 900 1100 900 1100 2100 OU-5 OU-5 OU-5 stem Control room Beamlines for r) (ground floor) radiation transport r-recuperator and User Stations ron laser (basement level) (ground and first floors) 15/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  16. Layout of Injector, Main Linac and Vertical Beamline (the First ERL) 7 – magnetic mirror 1 – electron gun 8 – undulator 2 – bunching cavity 3 – focusing solenoids 9 – phase shifter 10 – optical cavity 4 – merger 5 – main linac 11 – calorimeter 12 – beam dump 6 – focusing quadrupoles 16/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  17. Electrostatic Gun Power supply: U max = 300 kV I max = 50 mA 17/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  18. RF Gun Test Setup 575 пс Dr. Vladimir Volkov “New RF gun for Novosibirsk ERL FEL” 05 July, 16:00-17:00, Board 059 Measured beam parameters Energy, KeV 100 ÷ 320 Pulse duration(FWHM), ns ≤ 0.6 Bunch charge, nQ 0.3 ÷ 1.5 Repetition rate, MHz 0.01 ÷ 90 Average current, mA 102 max 18/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  19. Injector 19/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  20. RF Gun Installation Layout 20/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  21. Main Linac 21/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  22. RF Power Supply Frequency, MHz 180.4 Power, MW 2 x 0.6 22/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  23. New Amplifier for the Bunching Cavity f = 180 MHz, efficiency = 52 % P IN = 1 W, P OUT = 5 kW 8 transistors NXP BLF188XR water cooling 23/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  24. Layout of Horizontal Beamlines (the Second and the Third ERLs) Injector Beam dump 22 May 2012 – the first time the beam reached the dump after four accelerations and four decelerations 12 MeV 22 MeV 90% of beam current comes to the dump, the working repetition rate 3.75 MHz and average current 3.2 mA are obtained 32 MeV Only about 3% of beam current is lost with energy > 12 MeV 42 MeV Less than 1% of beam current is lost at the last track 24/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  25. Magnets and Vacuum Chamber of Bends 25/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  26. Beam trajectory can be adjusted only before this point 26/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  27. Compact 13.5-nm free-electron laser for extreme ultraviolet lithography Y.Socol, G.N.Kulipanov, A.N.Matveenko, O.A.Shevchenko and N.A.Vinokurov, FEL10 RF1 AB AB Booster Injector Dump RF2 40 m With 10-T superconducting magnet it may be used to generate 20-fs periodic x-ray pulses, which are necessary for time-resolved experiments, which use femtoslicing technique at storage rings now. But, the number of useful photons is thousands times more. 27/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  28. NovoFEL as Radiation Source NovoFEL X-ray FELs The most attractive ranges for FELs are at very short and at very long wavelength, where there are no other lasers 28/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  29. One of the main FEL advantages is the ability to adjust the wavelength Variation of magnetic field λ = λ = 6 cm 12 cm u u  +  2 K 1   λ = λ 1   Electromagnetic Variable gap γ u 2   2 2 undulator undulator K ~ 0…1.5 K ~ 0.4…2.5 E1 ~ 10…13 MeV Variation of beam energy E2 ~ 20…24 MeV E3 ~ 40…46 MeV Variable period Variation of undulator period undulator λ ~ 4 . 8 ... 9 . 6 cm K ~ 0.42…1.79 u 29/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  30. Electromagnetic Undulators 1-st FEL 2-d FEL Period, cm 12 12 Maximum current, кА 2.4 2.4 Maximum K 1.25 1.47 30/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  31. Variable Period Undulator (for the 2-d FEL) The tunability range of the 2-d FEL will be increased from 37 - 80 to 15 - 80 microns 31/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  32. Variable Period Undulator (for the 2-d FEL) 32/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  33. FEL Optical Cavities 1-st FEL 5.64 MHz ~ 100 ps 2- d FEL 7.52 MHz ~ 50 ps 3- d FEL 3.76 MHz ~ 15 ps 33/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  34. Optical beamlines and user stations Prof. Boris Knyazev “Novosibirsk free electron laser as a user facility” Wednesday, 06 July, 09:40 34/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  35. The 1 st stage FEL radiation parameters • Radiation wavelength, microns 90 - 240 • Minimum pulse duration, ps 70 • Repetition rate , MHz 5.6 / 11.2 / 22.4 • Maximum average power, kW 0.5 • Minimum relative linewidth (FWHM) 3 ⋅ 10 -3 • Maximum peak power, MW 1 The obtained radiation parameters are still the world record in terahertz region. 35/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  36. The Third FEL Design and Commissioning Injector Beam dump FEL radiation Undulator 3 Undulator 2 (power limitation) e - Undulator 1 e - (radiation) (energy modulation) Q1 B2 B1 Q2 ~ 40 m Electron outcoupling scheme may be used here 36/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  37. The third FEL undulator 37/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

  38. The third stage FEL undulator λ w 6 cm K 0.4 – 2.5 38/50 SFR-2016, 4–7 July 2016, Novosibirsk, Russia

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