® Backward Error Analysis and Numerical Software Sven Hammarling NAG Ltd, Oxford [email protected].
Optimization of Compact X-ray Free-electron Lasers Sven Reiche May 27 th 2011.
-
Upload
garry-watts -
Category
Documents
-
view
220 -
download
0
Transcript of Optimization of Compact X-ray Free-electron Lasers Sven Reiche May 27 th 2011.
![Page 1: Optimization of Compact X-ray Free-electron Lasers Sven Reiche May 27 th 2011.](https://reader036.fdocuments.us/reader036/viewer/2022062409/5697bf861a28abf838c87ecd/html5/thumbnails/1.jpg)
Optimization of Compact X-ray Free-electron Lasers
Sven ReicheMay 27th 2011
![Page 2: Optimization of Compact X-ray Free-electron Lasers Sven Reiche May 27 th 2011.](https://reader036.fdocuments.us/reader036/viewer/2022062409/5697bf861a28abf838c87ecd/html5/thumbnails/2.jpg)
Free-Electron Lasers
![Page 3: Optimization of Compact X-ray Free-electron Lasers Sven Reiche May 27 th 2011.](https://reader036.fdocuments.us/reader036/viewer/2022062409/5697bf861a28abf838c87ecd/html5/thumbnails/3.jpg)
Electron Beam Parameters
Almost everything scales with the FEL parameter (1D Model):
The characteristic length is the power gain length:
Increasing the current and/or reducing the emittances increase the performance and reduce the overall required length of the FEL.
Impact of energy spread and emittance needs to be small (Both spreads out any bunching and thus act against FEL process):
(Ideal Case)
![Page 4: Optimization of Compact X-ray Free-electron Lasers Sven Reiche May 27 th 2011.](https://reader036.fdocuments.us/reader036/viewer/2022062409/5697bf861a28abf838c87ecd/html5/thumbnails/4.jpg)
Saturation Power and Brilliance Saturation power:
For a given wavelength it favors a higher beam energy and thus a longer undulator period.
Peak Brilliance:
At saturation:
SwissFEL
(transverse coherence)
![Page 5: Optimization of Compact X-ray Free-electron Lasers Sven Reiche May 27 th 2011.](https://reader036.fdocuments.us/reader036/viewer/2022062409/5697bf861a28abf838c87ecd/html5/thumbnails/5.jpg)
Optimizing the Focusing
Decreasing the -function (increase focusing), increases the FEL parameter .
Too strong focusing enhances the emittance effect and increasing the FEL gain length.
From 1D Theory:
3D Optimization for SwissFEL
![Page 6: Optimization of Compact X-ray Free-electron Lasers Sven Reiche May 27 th 2011.](https://reader036.fdocuments.us/reader036/viewer/2022062409/5697bf861a28abf838c87ecd/html5/thumbnails/6.jpg)
Transverse Coherence (2D FEL Theory) Diffraction Parameter:
Assuming electron size as radiation source size:
Rayleigh Length
Char. Scaling of FEL (=2ku in 1 D model)
x
px
Photon Emittance Diffraction LimitedPhoton Emittance
Constraint for emittance to be smaller than photon emittance for all electrons to contribute on the emission process
Electron
![Page 7: Optimization of Compact X-ray Free-electron Lasers Sven Reiche May 27 th 2011.](https://reader036.fdocuments.us/reader036/viewer/2022062409/5697bf861a28abf838c87ecd/html5/thumbnails/7.jpg)
Transverse Coherence (Saldin et al) Growth rates for FEL eigenmodes (r,-decomposition):
Increased gain length due to strong diffraction
Mode competition and reduced coherence
Optimum growth rate of 1D model
Optimum:
Note: fundmental FEL Eigenmode has intrinsic wavefront curvarture and thus correspond to a larger photon emittance
![Page 8: Optimization of Compact X-ray Free-electron Lasers Sven Reiche May 27 th 2011.](https://reader036.fdocuments.us/reader036/viewer/2022062409/5697bf861a28abf838c87ecd/html5/thumbnails/8.jpg)
Growth of transverse coherence = spreading the phase information transversely.
Additional Effects
8
Diffraction Convection Spreading
Phase spread by field
Phase spread by electrons
Beam size variation
Emittance constraints is relaxed when realistic electron motion is included
FEL Theory only treats diffraction effects, but spreading is dominating effect in short wavelength FELs
TEM01 Growth rate
FODO Lattice
Rigid
![Page 9: Optimization of Compact X-ray Free-electron Lasers Sven Reiche May 27 th 2011.](https://reader036.fdocuments.us/reader036/viewer/2022062409/5697bf861a28abf838c87ecd/html5/thumbnails/9.jpg)
Definition of Coherence (Goodman) Coherence is a stochastic quantity and
correlates the phase relation between two transverse location:
In relation to diffraction experiments: A pulse can be fully coherent without
100% contrast in interference pattern (E0(r1) ≠E0(r2)).
The quasi-monochromatic approximation (E0(t)=E0(t+dt)) is not necessarily fulfilled.
Single spike pulse is not a stationary process and would require ensemble average.
Mutual Coherence Function Normalized Coherence Factor
E0(r2,t-dt)
E0(r2,t)
E0(r1,t)
![Page 10: Optimization of Compact X-ray Free-electron Lasers Sven Reiche May 27 th 2011.](https://reader036.fdocuments.us/reader036/viewer/2022062409/5697bf861a28abf838c87ecd/html5/thumbnails/10.jpg)
Example: Coherence for SwissFEL
10
n = 0.43 mm mradSpot Size: 0.0018 mm2
Coherence Area: 0.021 mm2
n = 0.86 mm mradSpot Size: 0.0023 mm2
Coherence Area: 0.015 mm2
=0.86
=0.69
Intensity Mutual Coherence
Intensity
Mutual Coherence
![Page 11: Optimization of Compact X-ray Free-electron Lasers Sven Reiche May 27 th 2011.](https://reader036.fdocuments.us/reader036/viewer/2022062409/5697bf861a28abf838c87ecd/html5/thumbnails/11.jpg)
Towards Compact FELs
Maximize the FEL parameter by maximizing the peak current.
Large FEL parameters allows for relaxed values for energy spread and emittance.
“Conventional” undulator design though with a short undulator period.
Reduce undulator period by using a laser wiggler as radiation device.
Provide a low emittance, low energy spread beam.
Moderate peak current which are consistent with the low emittance and energy spread values.
Approach A Approach B
Plasma InjectorField Emitter Source
![Page 12: Optimization of Compact X-ray Free-electron Lasers Sven Reiche May 27 th 2011.](https://reader036.fdocuments.us/reader036/viewer/2022062409/5697bf861a28abf838c87ecd/html5/thumbnails/12.jpg)
Case Study:
Laser Wiggler
![Page 13: Optimization of Compact X-ray Free-electron Lasers Sven Reiche May 27 th 2011.](https://reader036.fdocuments.us/reader036/viewer/2022062409/5697bf861a28abf838c87ecd/html5/thumbnails/13.jpg)
From XFEL to Laser Wiggler
Due to the scaling, the FEL parameter is always smaller for laser wiggler than for conventional SASE FELs.
In addition, the extreme constraints on the beam quality limits the current to a much smaller value than for SASE FELs.
u: 5 cm 500 nm: 15 GeV 20 MeV
Resonance Condition FEL Parameter
: 5.10-4 5.10-5
![Page 14: Optimization of Compact X-ray Free-electron Lasers Sven Reiche May 27 th 2011.](https://reader036.fdocuments.us/reader036/viewer/2022062409/5697bf861a28abf838c87ecd/html5/thumbnails/14.jpg)
Case Study for Laser Wiggler
Emittance and spread has been artificially chosen to allow the FEL to laser with the given peak current.
Energy spread is way beyond state-of-the-art electron beam sources.
Electron emittance much larger than photon emittance.
Energy 6.5 MeV
Current 500 A
Energy Spread 60 eV (!!!)
Emittance 0.1 mm mrad (!)
Laser Period 500 nm
Laser Field Strength 0.5
FEL Wavelength 2 nm
![Page 15: Optimization of Compact X-ray Free-electron Lasers Sven Reiche May 27 th 2011.](https://reader036.fdocuments.us/reader036/viewer/2022062409/5697bf861a28abf838c87ecd/html5/thumbnails/15.jpg)
Coherence Properties
An estimate of the coherence can be obtained by the fluctuation in the radiation power.
As expected from the high beam emittance value, only a poor degree of coherence is achieved.
Less than 10% coherence
Pulse profile at saturation
![Page 16: Optimization of Compact X-ray Free-electron Lasers Sven Reiche May 27 th 2011.](https://reader036.fdocuments.us/reader036/viewer/2022062409/5697bf861a28abf838c87ecd/html5/thumbnails/16.jpg)
Field stability requirement for all electrons along the interaction length:
Most stringent requirement for transverse dimension over at least 2 of the bunch, assuming a fundamental Gauss mode (alternative is transverse mode stacking):
Required radiation power:
Comments on the Laser Field
Interaction Length
Waist sizeBunch
For the example given the required power is 0.5 PW with a pulse duration of 15 ps !!!!
IncidentLaser
![Page 17: Optimization of Compact X-ray Free-electron Lasers Sven Reiche May 27 th 2011.](https://reader036.fdocuments.us/reader036/viewer/2022062409/5697bf861a28abf838c87ecd/html5/thumbnails/17.jpg)
Case Study:
High Current Electron Beam and Short Period
Undulator
![Page 18: Optimization of Compact X-ray Free-electron Lasers Sven Reiche May 27 th 2011.](https://reader036.fdocuments.us/reader036/viewer/2022062409/5697bf861a28abf838c87ecd/html5/thumbnails/18.jpg)
Basic Strategy
Very high peak currents yield a very large FEL parameter, which allows relaxed constraints for the electron beam quality (energy spread, emittance).
The beam energy is still reasonable large (>100 MeV) to allow for short wavelength while fulfilling the coherence condition.
Possible sources are plasma injector with an ultra short drive laser to drive a non-linear trapping mechanism of electrons.Currently an active field of research (LOA, LMU, LBNL etc.)
![Page 19: Optimization of Compact X-ray Free-electron Lasers Sven Reiche May 27 th 2011.](https://reader036.fdocuments.us/reader036/viewer/2022062409/5697bf861a28abf838c87ecd/html5/thumbnails/19.jpg)
Electron Beam Parameters
Ambitious beam parameters, though the lower end has been successful demonstrated at LOA.
Energy 0.1 - 2 GeV
Current 10 - 150 kA (!)
Emittance 1 mm mrad
Energy spread <1%
Charge 10 – 1000 pC
C. Rechatin et al, Phys. Rev. Lett., 102, 164801 (2009)
Most critical parameter is the energy spread, which requires a FEL parameter on the same order or larger.
![Page 20: Optimization of Compact X-ray Free-electron Lasers Sven Reiche May 27 th 2011.](https://reader036.fdocuments.us/reader036/viewer/2022062409/5697bf861a28abf838c87ecd/html5/thumbnails/20.jpg)
Case Study Overly optimistic case (LMU Munich, courtesy of A. Maier/A.
Meseck). E = 2 GeV E/E = 0.04 % (!!!) n = 0.5 mm mrad (!) I = 100 kA (!) Undulator: u = 5 mm, K = 0.65
= 2.5 Å
FEL parameter is ~10-3, thus requiring good beam parameters to make the FEL work. Also coherence is reduced.
![Page 21: Optimization of Compact X-ray Free-electron Lasers Sven Reiche May 27 th 2011.](https://reader036.fdocuments.us/reader036/viewer/2022062409/5697bf861a28abf838c87ecd/html5/thumbnails/21.jpg)
A More Reasonable Case
Energy 1 GeV
Current 10 kA
Emittance 1 mm mrad
Energy spread 5 MeV
Effective FEL Parameter 0.1%
Gain Length 0.23 m
Saturation Length 4.8 m
Saturation Power 9 GW
Bandwidth 0.23 % FWHM
Results for = 1 nm
Larger spread and emittance, less current
![Page 22: Optimization of Compact X-ray Free-electron Lasers Sven Reiche May 27 th 2011.](https://reader036.fdocuments.us/reader036/viewer/2022062409/5697bf861a28abf838c87ecd/html5/thumbnails/22.jpg)
Optimization for Very High Energy Spreads
Use dispersion to stretch the bunch. Reduces bunch current and energy spread
Energy spread conditions improves due to the I1/3
dependence of the FEL parameter. Helps for very large energy spreads:
Current 10 kA 1 kA
Energy Spread 20 MeV 2 MeV
Sat. Power 1 GW 0.4 GW
Sat. Length 19 m 14 m
![Page 23: Optimization of Compact X-ray Free-electron Lasers Sven Reiche May 27 th 2011.](https://reader036.fdocuments.us/reader036/viewer/2022062409/5697bf861a28abf838c87ecd/html5/thumbnails/23.jpg)
Summary
Coherence and peak brightness favors GeVs electron beams with high peak currents.
Plasma injectors are promising candidates for compact x-ray FELs, though the performance seems to be feasible only down to 1 nm
Laser wigglers yield only poor performance (poor coherence) even if the unrealistic beam and laser parameters could be met.
Laser Wiggler
Plasma Beam