free-electron laser “sacla” and its basicpf...free-electron laser “sacla” and its basic yuji...
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![Page 1: Free-electron laser “SACLA” and its basicpf...Free-electron laser “SACLA” and its basic Yuji Otake, on behalf of the members of XFEL R&D division RIKEN SPring-8 Center Light](https://reader035.vdocuments.us/reader035/viewer/2022081611/5f0b55ac7e708231d430013e/html5/thumbnails/1.jpg)
Free-electron laser “SACLA” and its basic
Yuji Otake, on behalf of the members of XFEL R&D division
RIKEN SPring-8 Center
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Light and Its Wavelength, Sizes of Material �
Bacteria
Energy
Microwave
Laser
Virus
Protein
Atom・Molecule
Mosquito
X-rayVisible light
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Ordinal Laser, e.g. Helium Neon Laser• Excite the orbital electrons of an atom by external light. • Change an orbital energy level (Pump) to make a inverted
distribution of the electrons. • Generate stimulated emission by returning the electrons to the
original energy level. • The special features of this laser are monochromatic,
coherent, pointing stability and small spot size. • Fixed wavelength (Energy), pulse width and intensity (Pulse
energy).
Excitation by Light
Light (Electric Magnetic Wave) Emission
Nucleolus
Electron
Orbit(Energy Level)
E1E2
Thermal Equilibrated Distribution
Inverted Distribution
E2
E1
Orbit(Energy Level)
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Principle of Mode-locked Laser
Cut by an optical filter
Pump Light: make the inverted energy level distribution of the orbital electrons of the atom.
ModulationSignal Generator
Optical Cavity
Input Output
Electro Optic ModulatorLase Light
MirrorMirror
n = 1n = 2n = 3n = 5n = 6
f (Hz)
Optical Amplitude
time
FrequencyPump Light
Lase Amplification MediumTi-Sapphire Crystal
Suchas400nm(Green)Light
e.g. Ti-Sapphire :800 nm(Infrared) Light
Optical Comb Pulse Train
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Radiation When Moving an Electron (Electromagnetic Wave Radiation)
Electrons
Incoherent light
Intensity Spectrum of Radiation
Radiation by Curved Obit Electron
Bending Magnet
Electron
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Undulator Principle
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Electron Movement by Its Radiation (SASE)
Retarded Potential
Generation Wave Length Electron
ForceLorenz Factor
Electron Beam Electron Velocity V = c Relativistic Condition
Electric Field of Undulator
Deflection Parameter
Undulator & Permanent Magnet
Period of Magnetic Field
Undulated Orbit
|E|2= (ρ/ε)12+(ρ/ε)2
2+ --- |E|2= (Σn(ρ/ε))2ρ : Electron Chargeε : Dielectric Constant
P : Electron Charge
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Electron Radiation Angle in Undulator
The radiations form the behind electrons modulates the transvers motion of the advanced electron.
The straightness of the electron orbits are within 1.6 x 10E-4 rad, 1/γ @8 GeV.
γ : Lorenc Factor
The radiation angle from the electrons is 1/γ.
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RefernceSpringer Tracts in Modern Physics Volume 258 2014 Free-Electron Lasers in the Ultraviolet and X-Ray Regime, 2nd Ed, Physical Principles, Experimental Results, Technical Realization
Laser Brightness and Photon Energies of XFELs and Synchrotrons
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Feature of FEL
• Electrons passing Undulated with the undulators emit the free-electron laser, FEL.
• T h e s p e c i a l f e a t u r e s o f F E L a r e monochromatic, coherent, pointing stability and small spot size.
• Variable wavelength (Energy), pulse width and intensity (Pulse energy) by the electron energy, the bunch compress, the K value (Magnetic field strength) of the undulator and the electron peak current.
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SPring-8 Campus�
14
SACLA
SPring-8 SR Ring
New Subaru
1 Gev Linac & Synchrotron
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SACLA Accelerator Main Components
~700m
500 kV low-emittance pulsed thermionic electron-gun
C-band acceleration structures (37MV/m @SACLA)
Short-period in-vacuum undulators (K〜2.1)
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Machine Configuration of SACLA
22
18
3
We have 2 laser sources, which are SACLA and SCSS+. They mainly comprise thermionic electron-guns, C-band acceleration structures, and in-vacuum undulators.
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Magnetic Bunch Compression
Low Energy
Acceleration Structure
4 Bending Magnets Chicane
Low Energy
High Energy
Electron BeamElectron Bunch
High Energy
Acceleration RF
Acceleration
Deceleration
Time
The low-energy part of the bunch takes the detour.The high-energy part of the bunch takes the shortcut.
BC, Bunch Compressor
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Measurement of Beam Bunch Length by the RF Deflector System
t
~ 100 fs FWH
M
100 fs
Q magnet
t
~20 fs FWH
M
100 fs
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Temporal Electron Bunch Structures of BL3 and BL2
10000
8000
6000
4000
2000
0
Current (A)
350300250200150100500Time (fs)
High current bunch
Low current bunch
(230 pC)
(170 pC)
• Red: A peak current of the BL3 is ~10 kA at 8.0 GeV. • Blue: A peak current of the BL2用 is ~1 kA at 6.3 GeV.
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Specifications of BL3 and BL2
Number of undulators 22@BL3, 18@BL2Undulator length 5 mNumber of period (undulator) 277Minimum magnetic gap (undulator)
< 3.5 mm
Maximum K value (undulator) < 2.85Effective length of the beam line ~ 90 mOutput wave length ~ 0.08 nm@BL3
~ 0.12nm@BL2Electron beam energy ~ 8.5 GeVSelf seeding function BL3
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Present Laser Performance (BL3)
SASE Intensity Stability for 24 Hours
V10 um, H20 um in rms ~ several % of beam size
Pointing stability @Experiment Hutch 10 keV
10 10.049.96Size : 2~3 mmFWHM
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Simultaneous Double Electron Beam Energies Operation at the BL3 and BL2
Electron Peak Current: 1.2 kA, Pulse Width: ~150 fs FWHM, Repetition: 30 Hz at both Bl2 and BL3.
BL3Electron 7.8 GeVPhoton 10.09 keV15 HzK=2.1
1.0
0.8
0.6
0.4
0.2
0.0
Intensity (a.u.)
4.124.084.04Photon energy (keV)
(a) BL2
1.0
0.8
0.6
0.4
0.2
0.0
Intensity (a.u.)
10.1210.0810.04Photon energy (keV)
(b) BL3
Laser Spectra at BL2 and BL3BL2Electron 6.3 GeVPhoton 4.09 keV15 HzK=2.85
200
150
100
50
0
Pulse energy (µJ)
80006000400020000Pulse number
(b) BL3 (10.09 keV)Relative stability 9.1 % (STD)
200
150
100
50
0
Pulse energy (µJ)
80006000400020000Pulse number
(a) BL2 (4.09 keV)Relative stability 10.5 % (STD)
Laser intensity time trends
~ 600 s
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FWHM 15 fs
Projection
X-ray Pulse Energy• An X-ray nominal pulse energy value is 0.6 ~ 0.7
mJ. @ 10 keV• Possible X-ray energies are from 5 keV ~ 15 keV. • An electron bunch length is <15 fs (FWHM)
measured with RF deflector. (A measurement accuracy is ~12 fs limited by the natural emittance of the electron beam.)
C-OTR noise
Electron beam (deflector-ON)
ßhe
ad
Temporal Structure of Electron Beam observed with RF Deflector.
250
fs
Tail→
K value are from 1.5 to 2.15 at the individual electron energy.
X-ray Laser Intensity Map
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SCSS+ Configuration
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Specifications Comparison between SCSS and SCSS+
SCSS SCSS+Operation period 2005 ~ 2013 2015 ~
AcceleratorBeam energy 250 MeV 400 ~ 800 MeVBunch charge ~0.3 nC ~0.3 nCPeak current ~300 A ~500 ARepetition 60 pps (max.) 60 pps (max.)
UndulatorPeriodic length 15 mm 18 mm
K parameter 1.5 (max.) 2.1 (max.)Photon Beamline
Wavelength 50 - 60 nm 13 - 40 nmPulse energy 10-30 µJ/pulse 100 µJ/pulse
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Temporal Bunch Structure Measurements by the RF Zero-cross Method and the Streak Camera
• We give energy modulation along the bunch at the RF zero-crossing point in the acceleration unit, CB1-3, and measure the energy distribution of the bunch at the BC2.
RF Amplitude
Bunch
Beam Charge: 0.28 nC
Set the RF zero-cross phase
Streak Camera Case using OTR.
Streak camera
RF Zero-cross Method Case
1.6 ps 1.5 ps
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Laser Intensity Time Trend of the BL1
Laser profile in the experimental hutch
Shot by shot fluctuation is 30%(σ).
Acceptance of Beamline: ~45%
4.8
mm
, 2σ
4.2 mm, 2σ
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Laser Spectra of the BL1
Spectrum width is ~1 eV in FWHM.Center photon energy is ~42.5 eV. Center photon energy is ~98 eV.
Spectrum width is ~2 eV in FWHM.
12.6 nm
29nm
~ 0.8 GeV Electron
~ 0.5 GeV Electron
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Summary
• The variable wavelength (Energy), pulse width and intensity of FEL , as which I already show you, is very important characteristics for users.
Thank you for your aoention.