SLAC Summer School on Electron and Photon Beams · PDF fileSLAC Summer School on Electron and...
Transcript of SLAC Summer School on Electron and Photon Beams · PDF fileSLAC Summer School on Electron and...
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SLAC Summer School onElectron and Photon Beams
Tor RaubenheimerLecture #3: High Gain FEL’s
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Outline
• Synchrotron radiation• Bending magnets• Wigglers and undulators• Inverse Compton scattering• Free Electron Lasers• FEL Oscillators• High gain X-ray FEL’s• Coherence and Seeding
SSSEPB, July 22-26, 2013
Lecture #1
Lecture #2
Lecture #3
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Types of FEL’s
SSSEPB, July 22-26, 2013
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High Gain Free Electron Laser Principle
• Due to sustained interaction, some electrons lose energy, while others gain energy modulation at 1
• e losing energy slow down, and e gaining energy catch up density modulation at 1 (microbunching)
• Microbunched beam radiates coherently at 1, enhancing the process exponential growth of radiation power
uu
ee11
xx--rayray
• Electrons slip behind EM wave by 1 per undulator period ( u)
+ + +
+ + +
KK//
vvxxEExx < < 00 vvxxEExx > 0…> 0…
+
SSSEPB, July 22-26, 2013 4
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Early LCLS Gain Measurements
SSSEPB, July 22-26, 2013
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1-D Wave Equation
Allowing the field to change slowly (>> u) along the undulator, the wave equation in 1-D is
whereand
In the 1-D approximation, we ignored the self-fields (space charge) from the beam and diffraction effects of the radiation as well as the matching of the beam and radiation fields.To solve this, we drop the 2nd derivatives because the field is assumed to be changing slowly where J1 is the component of thecurrent at the radiation wavelength
tJtzE
tczx
x 02
2
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),(1
)](exp[),(),( tkzitzEtzEx )cos(),( zkKJtzJ uzx
1
~0
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4),(1 JKctzE
tcz r
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1-D FEL Equations
Now we have the pendulum equations for the motion of the particles within the radiation bucket which depends on a varying electric field but the field and current equations depend on the particle distribution
2N+2 equations
SSSEPB, July 22-26, 2013
~
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)exp(2
)exp(
... 1 where2
JcKEkz
iN
JJ
imc
EeKdz
d
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ru
n
N
nz
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#2, p. 23
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1-D Solution (I)
Introduce dimensionless variables:
then neglect and linearize in terms of collective variablesa
SSSEPB, July 22-26, 2013
3/12
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/ˆ and 2ˆ
KJJK
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zkz
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)exp(21
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)exp(ˆˆ
ˆˆ
n
nn
nn
iaz
cciazd
dzd
d
)exp(ˆ)exp(
nn
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iP
ibCompex field
Bunching parameter
Collective momentum iPzd
db
bzd
da
ˆ
ˆ
ˆa
zddP
and
R. Bonifacio, C. Pellegrini, and L.M. Narducci, “Collective instabilities and high-gain regime in a free-electron laser,” Opt. Commun., 50, 373 (1984).
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1-D Solution (II)
This has a general solution of the form withhas three roots: one oscillatory, one damped and one growing.
The equation can be futher generalized to include the detuning and energy spread
where is the fractional detuning ( - r)/ r and is the width of a uniform energy spread in units of
The high gain FEL differs from the small signal gain in that the highest gain occurs on resonance
SSSEPB, July 22-26, 2013
)ˆ exp(~ zia 13
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Evolution of the FEL Microbunching
FEL bucket grows rapidly asthe beam begins to bunch andradiate coherently. After a ¼ synchrotron oscillation the bunching begins to decreaseagain and the FEL saturates
SSSEPB, July 22-26, 2013 From P. Schmuser et al.
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Gain Length and Lethargy
After some initial mode competition, the exponentially mode will grow.The 1-D power gain length is given in terms of
At the beginning, the growingmode is competing with theoscillatory and the dampedmodes field is roughlydivided between modes andit takes 1 ~ 2 gain lengths to get started
SSSEPB, July 22-26, 2013
34
uG0L
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Gain versus Detuning
In the low gain FEL the maximum gain arises when the FEL is slightly detuned and the beam energy is higher than the amplified signal.
In the high gain case, this differs and maximum gain arises on resonance however it takes somelength for this exponential modeto dominate
SSSEPB, July 22-26, 2013
Growing mode
Damped mode
Low Gain
High Gain
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Small Gain Limit of High Gain FEL
SSSEPB, July 22-26, 2013 From P. Schmuser et al.
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Energy Spread and Emittance Effects
Energy spread needs to be small compared to the width of the gain curve
Tranverse emittance has two effects:
1. Increase the longitudinal slipage.
where x and y are the acceleratoroptical functions NOT velocity and Jx andJy are the particle transverse amplitudes
2. Match the beam to the radiation size and minimize diffraction
SSSEPB, July 22-26, 2013
y
y
x
xz
JJK2
2
22/11
)1( 2, Kyxeff
4
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3-D Parametrization
Many effects increase the 1-D gain length: energy spread, emittance, diffraction, finite bunch length, … These effects can be approximated as LG = LG0 (1 + ) where:
SSSEPB, July 22-26, 2013
Xie, M.: Exact and variational solutions of 3D eigenmodes in high gain FELs.Nucl. Instr. Meth. A 445, 59 (2000) 92, 93
andFinally, the saturationpower is estimated toscale as:
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SASE FEL Micro-Bunching Along Undulator
UCLAUCLA
S. ReicheSASE* FEL starts up from noise
log log (radiation power)(radiation power)
distancedistance
electron beam
photon beam
beam dumpbeam dumpundulatorundulator
* Self* Self--Amplified Amplified Spontaneous Spontaneous EmissionEmission
Power comes from last gainlength Lg
SSSEPB, July 22-26, 2013 16
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SASE Pulse Evolution
Starts from noise but as the beam propagates, thespectrum narrows. However, the light is still temporally chaotic unless the correlation length iscomparable to the bunchlength
SCSSspectrum
LCLS Simulation
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Initial measurements of e-beam and x-ray temporal profiles using the XTCAV
Data taken on June 4th, 2013.Beam energy 3.5GeV, 150pC.Temporal resolution is about 1.7fs rms in this test.
Preliminary results.
FEL Off FEL On
SSSEPB, July 22-26, 2013
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SASE Temporal Coherence
Single pass SASE FEL starts from noise
Slippage length is ~ (Lg * u)
• No phase correlation between portions
Would like to have transform limited pulsesfor many experiments Y. DingY. Ding
Z. HuangZ. Huang15 Å15 Å,2.42.4 10101111 photons,photons,IIpkpk = 2.6 kA,= 2.6 kA,
0.4 µm0.4 µm 1.2 fs1.2 fs
Simulation at 15 Å based on measured injector &linac beam & Elegant tracking, with CSR & 20 pC.
Y. DingY. DingZ. HuangZ. Huang
Simulation at 1.5 Å based on measured injector &linac beam & Elegant tracking, with CSR, at 20 pC.
1.5 Å1.5 Å,,3.63.6 10101111 photonsphotonsIIpkpk = 4.8 kA= 4.8 kA
0.4 µm0.4 µm
SIMULATED FEL PULSESSIMULATED FEL PULSES
SSSEPB, July 22-26, 2013
SASE
Seeded
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Transverse Coherence
Radiation can be decomposed into transverse modes. The TEM00 has the highest intensity on axis while other modes extend out radially. The fundemental TEM00 mode grows fastestand rapidly dominates although the othermodes can catch up once into saturation
SSSEPB, July 22-26, 2013
In the LCLS
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Slide 21
SSSEPB, July 22-26, 2013
Linac Coherent Linac Coherent Light Source FacilityLight Source Facility
Injector at 2-km point
Existing Linac (1 km)(with modifications)
First Light April 2009, CD-4 June 2010First Light April 2009, CD-4 June 2010
New e Transfer Line (340 m)
X-ray Transport Line (200 m)
UCLAUCLA
Undulator (130 m)
Near Experiment HallNear Experiment Hall
Far Experiment HallFar Experiment Hall
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LCLS Concept: Fourth Generation Workshop21 Years Ago
C. Pellegrini, A 4 to 0.1 nm FEL Based on the SLAC Linac,Workshop on Fourth Generation Light Sources, February, 1992
Herman Winick’s Study GroupClaudio Pellegrini Herman Winick
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Engaged Bjorn Wiik andGerd Materlik duringsabbaticals at SLAC