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Compact X-ray & Emittance Measurement by Laser Compton Scattering Zhi Zhao Jan. 31, 2014
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Outline Overview of Compton scattering ERL-based compact x-ray Emittance measurement
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Overview of Compton scattering
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Compton Scattering Scattered photon: longer wavelength ! (h/mc)cos( ); h/mc = 0.024 A
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Inverse Compton Scattering Scattered photon: high-energy, tunable, and compact ! E = 0.511 * (MeV); (1 ^2)^(-1/2) ħ = ħ (1 cos( ))/(1 cos( )) If , and =0; then h = 4 ^2*h Drive laser: 1.2 eV (1.04 m), electron: = 60 (~30 MeV) Photon energy: 17 keV (0.73 A)
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Compton & Thomson Scattering Compton scattering: if Electron recoil is included ! Thomson scattering: if Electron recoil is negligible ! ħ = ħ (1 cos( ))/[(1 cos( )+ħ (1+cos( )cos( )/E 0 ) Including the electron recoil: ħ ~ E 0 ħ << E 0
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Nonlinear Laser-Electron Scattering Electron’s dynamic: Electron oscillating approaching light speed Force of magnetic and electric comparable Nonlinear dynamics, i.e. multi-photon event, figure-8 movement Laser accelerator… Nonlinear parameter, ~ 1 @ I=10^18 W/cm^2
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Linear Laser-Electron Scattering Linear scattering regime Photon flux & brilliance Beam size & emittance 1 uJ, 50 MHz/1.3 GHz & 5 MeV, 80 pC, 2 mJ, 50 MHz/1.3 GHz & 30 Mev, 80 pC, Our focus: Working regimes
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ERL-based Compact X-Ray
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Photon Energy vs Scattering Angle ħ = ħ (1 cos( ))/(1 cos( )) Drive laser: 1.2 eV (1.04 m) Electron: ~ 60 (30 MeV) high-energy photon is concentrated around 1/ !
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Cross-section vs Scattering Angle d /dcos( ) = 3/8* th*(1/ ^2/(1 cos( ))*(1+((cos( )- )/(1 cos( ))^2) th 0.665 barns Small angle: bigger diff. cross-section Total cross-section around 1/ is ~ 0.165 barns
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Key for Photon Flux Flux is the product of electron current and photon flux Flux per bunch, assuming Gaussian profile in electron and laser Key factors: High electron bunch charge High laser pulse energy & High repetition rate Small beam sizes at the interaction point Photon Flux@80 pC, 1 uJ, 50 MHz, beam size of 1 mm X 2 mm: 1 MHz
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Keys for Brightness Keys: Both photon flux and small emittance F is the photon flux per 0.1 % energy bandpass Photon Brightness
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Technical Approaches I: Small Storage Ring Lyncean Technologies, Inc., High repetition rate, small emittance, Cavity-enhanced laser power
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Technical Approaches I: Small Storage Ring Thales/CEA, France High repetition rate, small emittance, Cavity-enhanced laser power Beam emittance and energy spread may grow; long pulse duration
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Technical Approaches II: Linac & SRF Linac High brightness, short pulse duration, High repetition rate, small emittance, Cavity-enhanced laser power Compatible with ERL
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MIT ICS Source: Planned
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Technical Approaches II: ERL-based Cavity-enhanced laser power High-power laser generated by ERL (Jlab & Japan) We can easily generate X-ray and -ray if we reach 5 GeV!
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Emittance Measurement
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Emittance Measurement (I): Intensity Profile Beam size and divergence: can not be directly measured. Measuring beam sizes at three different locations Laser wires: Induced current from secondary emission or flux
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Emittance Measurement (I): Intensity Profile Scanning the beam transversely Monitoring the X-ray yield Fitting to find out the beam size Three locations for determining emittance Copy from exp. of ILC
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Emittance Measurement (II): X-ray Spectrum Two factors: Intensity profile: determining beam size X-ray spectrum: deriving beam divergence Spectrum width and shaping: the function of Spatial and temporal profiles of the electron and laser beams as well as electron angular and energy spread Divergent angle decreasing the x-ray energy Signature, “low energy trail”
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Emittance Measurement (II): X-ray Spectrum Scattering photons: Energy spectrum: Model: The spatial and temporal profiles of the electron and laser beams as well as the electron angular and energy spread.
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Intensity profile determine the beam size.
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Scattered x-ray energy flux: Deriving beam divergence by fitting X-ray spectrum Intensity profile and Energy spectrum determine the emittance.
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Divergent angle: Signature, “low energy trail”
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Photon energy: 100 kV – 1 MeV low energy trail
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Summary Potential X-ray & -Ray sources by ERL LCS for nondestructive beam diagnostic More effort is underway…
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