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2006.10.04 –10.06 Milan Italy LUCX system and dark current (1) LUCX project (2) Phase Ⅰ and...
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Transcript of 2006.10.04 –10.06 Milan Italy LUCX system and dark current (1) LUCX project (2) Phase Ⅰ and...
2006.10.04 –10.06 Milan Italy
LUCX system and dark current
• (1) LUCX project
• (2) PhaseⅠand results
• (3) Phase Ⅱ and dark current
Liu shengguang and LUCX group
2006.10.04 –10.06 Milan Italy
(1) Purpose of LUCX
• LUCX ( Laser Undulator Compton X ray source) is for generation x-ray photon by inverse Compton scattering.
• X-ray is for medical application ----K-edge digital subtraction angiography. In this application, 33KeV X ray photons are required.
• Collision angle between electron beams and the laser beams is 20 degree.
• The detector size is 4cm×4cm, 2m away from the collision point. Acceptance angle of the detector is 10mrad.
2006.10.04 –10.06 Milan Italy
(1) Main parameters of LUCX
Electron beam Laser pulse
Energy 43MeV 1064nm (1.17eV)
Intensity 2nC/bunch (5nC/bunch)
1.25*10^10electron/bunch
17µJ/pulse
9.1*10^13photon/pulse
Width (FWHM) 10ps 10ps
Bunch number 100bunches/train
Beam size σx =64um σy =32um σ= 100um
Repetition rate 12.5Hz
Expected X ray photon number on the detector :
21024102
5105.2
/bunch
/train/sec
2006.10.04 –10.06 Milan Italy
(2) Phase Ⅰ
Until the end of 2005, RF gun study had been finished and multi bunch beams had been generated.
2006.10.04 –10.06 Milan Italy
(2) Cs2Te cathode system
MoverMover
Preparation system
RF gunCathode load system
Transport system
Oct. 2005, we prepared a cathode and loaded it.
At the beginning, QE is 3.7% offline by Xe light
One years later, QE become 0.7% online by laser in gun
2006.10.04 –10.06 Milan Italy
(2) RF-gun Cavity
Cu
Beam
Mo Cathode plug
RF gun cavity (1.6cells)
UV laser
For LUCX gun, space charge effect is severe. In order to decrease it, field distribution be tuned into not balanced distribution. Eh/Ef =1.3
2006.10.04 –10.06 Milan Italy
(2) Chicane
A chicane composed of 4 dipole magnets kicks the beam off the main beam line in order to inject laser on the cathode perpendicularly
2006.10.04 –10.06 Milan Italy
(2) Laser system
266nm 11µJ/pulse 13ps(FWHM) Gaussian
Now we have installed a shaper to convert gaussian laser---> Uniform laser (transverse distribution)
2006.10.04 –10.06 Milan Italy
(2) Experimental results
Because of high charge and multi bunch, we must consider beam loading effect and try to compensate it. We apply ΔT method.
Injection time is 1.703µs
with 2.05µs RF pulse
Injection time is 0.908µs
with 2.05µs RF pulse
2006.10.04 –10.06 Milan Italy
(2) Experimental results
Momentum and momentum spread:
220nC/100bunch : 4.65MeV/c 1.3% bunch to bunch
one bunch : 0.9%
Normalized emittance: 49nC/100 bunch 15πmm.mrad
220nC/100bunch 48 π mm.mrad
High charge: 300nC/100bunch has been generated
2006.10.04 –10.06 Milan Italy
(3) Phase Ⅱ
2006.10.04 –10.06 Milan Italy
(3) RF pulse compressor
3dB CouplerKlystron
GUN
ACC
Dummy Load
RRCS
Phase Shifter
0.7
0.3
1.5dB Coupler
Traveling wave type RF compressor
3.7µs flat ---> 1.0µs
2006.10.04 –10.06 Milan Italy
(3) Dark current
Dark current comes from field emission.
In a RF period, dark current occurs at phase region nearby 90 degree (red shadow) .
During a RF pulse, dark current occurs at the time region that blue shadow shows. If RF pulse width increase, the blue region expands lots, dark current increase much .
2006.10.04 –10.06 Milan Italy
(3) Dark current data 1
1917.4
735.5
116.90
200400600800
100012001400160018002000
0.0 2.0 4.0 6.0 8.0 10.0 12.0 14.0 16.0
Forward RF power to Gun (MW)
dark
cur
rent
in a
RF
puls
e (p
C)
2us1.5us1us
RF pulse Forward power Field at cathode surface
1.0us 8.3MW 81.8MV/m
1.5us 7.0MW 83.8MV/m
2.0us 6.1MW 81.54MV/m
If we regard the value of field gradient at cathode surface as a marker. For LUCX gun, if it is less than 80MV/m, no dark current occurs
2006.10.04 –10.06 Milan Italy
0
20
40
60
80
100
120
140
160
0 10 20 30 40 50 60
solenoid current (A)
dark
cur
rent
(pC
)
(3) Dark current data 2
Dark current is maximum at solenoid current 50A, corresponding maximum magnetic field is about 1.90KGauss
1.0µs 13.8MW
2006.10.04 –10.06 Milan Italy
(3) Dark current data 3
dark current (1.5us)
735.5
20833.3
0
5000
10000
15000
20000
25000
0.0 2.0 4.0 6.0 8.0 10.0 12.0 14.0 16.0forward power to Gun (MW)
dark
cur
rent
(pC
)/RF
pulse 1.5us(now)
1.5us(2 years ago)
20833.3pC / 735.5pC = 28
2006.10.04 –10.06 Milan Italy
Summary
• LUCX has generated 300nC/100bunch electrons• Comparing to dark current from the RF gun two
years ago, dark current level decrease greatly, gun condition improves greatly.
• Now the dark current is not big problem on our operation conditions.
• QE of the cathode decrease from 3.7% to 0.7% during one year
2006.10.04 –10.06 Milan Italy
END
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2006.10.04 –10.06 Milan Italy
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