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J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 1
PITZ Shutdown 2007
J.Bähr
PITZ, DESY
Technisches Seminar 3.Juli 2007
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 2
Outline• Outline
1. Introduction
2. Explanations: PITZ, XFEL, Emittance,…
3. PITZ more detailed
4. Shutdown: Why and what
5. Manpower and coordination
6. Outlook
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 3
1.Introduction- A long shutdown at PITZ is planned starting
from 20/08/2007 until beginning of November
- Most modules of the vacuum beamline will be dismounted and re-mounted in a new scheme
- The Conditioning Test Stand (CTS) will be mounted in the tunnel bearing gun 4.1
- The rf system 1 will be re-organized for the use of a 10 MW klystron
- Many further tasks
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 4
2. Explanations: PITZ, XFEL, Emittance …
• What is that:• PITZ,XFEL,FLASH,emittance, laser, SASE,
space charge, electron gun…• What is the connection between:
– FEL and emittance– Emittance and space charge– A gun and a TV tube– PITZ and the XFEL,FLASH– …
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 5
Setup PITZ1.6 completed !transverse emittance
gunboosterquads
longitudinal phase space masks
Gun
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 6
PITZ• PITZ:“ Photo injector
Test Facility“• Test and optimize
electron sources for FELs: FLASH,XFEL
• X-FEL:
European X-ray FEL project
e-gun
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 7
„FEL-Microscope“• FEL: „Free Electron Laser“:
„Microscope“ Motivation!!!• Resolution R:
about wavelength R~ λ
for microscopes• The higher the beam
energy , the smaller • better) the resolution R of
the „microscope“• c=νλ ,E=hv E=hc/λ
λ~1/E • Resolution ~ λ~1/E
• Resolution of microscopes
Device Energy
Electron/
photon
Resolution Object
Light micro-scope
1 eV (light) 1 µm Biologic cell
Electron micro-scope
~70 keV ~O(10 nm)
Magnifica-tion: 10**5
Big molecules
FLASH 500 MeV/
200eV
~7nm Molecules
XFEL 3 GeV ~1 Angstr. Atoms
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 8
FEL
• FEL: Free electron laser :SASE principle
e-GunLinear accelerator Undulator: Magnetic structure
E-beam
Light/electro-magnradiation
Beam dump
SASE principle:„Self amplified radiation by stimulated emission“
PITZ
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 9
The gun
• The gun:– Laser input port – Cathode– rf coupler– Solenoid magnets– Resonator– Vacuum tubes
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 10
Comparison of an e-gun and a TV tubeGun-TV
TV Gun
Bild Bild
Cathode thermal Photo effect acceleration Electro static Rf Voltage accel. ~4kV ~6 MV Electron energy ~4 keV
W=Q*U=1e*4kV 6 MeV
El. Field strength E=U/d=4kV/0.2m=20kV/m 60MV/m Deflection Electro static Dipole magnet (if
wanted visualisation TV screen + eye Flourescence screen
+ TV camera (no access)
radiation X-rays X-rays Create image deflection Move laser spot
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 11
Comparison between TV tube and an electron gun
Focusing using solenoids
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 12
Mis-unerstanding• If one does not consider the motivation and
the context one could assume:
• PITZ is a not effective designed, rather huge built TV tube with enormous running parameters, where one has no access and the TV program is not interesting for typical citizens and difficult to regard and only remotely because there is no access possible. The screen size is much too low (about 2“).
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 13
FLASH• FLASH: Free electron LASer in Hamburg
• (earlier TTF)
Brilliance: Photons in solid angle and per area unit pro wavelength intervall
Gun
LINAC Undulator
PITZ
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 14
Laser• LASER: „Light Emission by Stimulated Emission of
Radiation“• Characteristics of laser light:
1. High energy density :“parallel“ ray of light instead of divergent bundle
2. Coherence: phase relations between parts of the light ray: possibility of interference Holography
3. Monochromatic light: only one wavelength (visible-invisible)
Resolution R~ λ~1/E
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 15
Electromagnetic spectrum
Resolution R~ λ~1/E
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 16
Emittance• Emittance : Characteristic of electron
beam• For FEL small emittance
necessary!!!• Optimization of e-gun:
Minimalization of transverse emittance
• - EMSY: Emittance measurement system
• Emittance cannot be improved after the source!!
• Emittance
• Divergent electron beam• ε : diameter * angle• ε = d * α in mm *mrad• Example : • Beam diameter : 1mm• Divergence α =0.05 °=
1mrad ε = 1mm mrad
d
α
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 17
Space charge and emittance• Space charge:• 10,000,000,000 electrons
per bunch (1 nC)• About 1mm³ bunch size strong forces• What is to be done:
– Solenoid magnet: focusing– High acceleration in the gun
40MV/m 60 MV/m /June 2007)
– Laser profiles:long.,transv.– 1nC = 0.000,000,001 As– In 1ps = 0.000,000,000,001s– 1nC in 20 ps: 50A in 20ps
• Longitudinal Laser profile: rectangular
• Transverse Laser profile : rectangular
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 18
Emittance
1. What emittance has been measured by PITZ?
2. What are the goals?
3. World record?
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 19
εx,y ~ (e- beam size) • (e- beam angular divergence)
Why injector so important ?What is emittance ?
Why it must be small ?
n = 1mm mrad
length of the undulator
n = 2 mm mrad
n = 4 mm mrad
Q = 1 nCou
tpu
t p
eak
po
wer
of
th
e V
UV
-FE
L @
6.4
nm
(
GW
)
path length in the undulator (m)
VUV-FEL
peak power
• smaller emittance new horizons: shorter wavelength, higher repetition rate
• XFEL goal: 0.9 mm mrad@injector = 1.4 mm mrad@undulator
n = 1 mm mrad
ou
tpu
t p
eak
po
wer
of
th
e X
FE
L S
AS
E2
@ 0
.1 n
m
(G
W)
path length in the undulator (m)
n = 2 mm mrad
n = 3 mm mrad
peak current: 5 kAenergy spread: 2.5 MeV
XFEL
absolute numbers
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 20
Emittance• Emittance results:
0.8
1.2
1.6
2.0
2.4
2.8
3.2
320 322 324 326 328 330Imain, A
no
rm. e
mit
tan
ce /
mm
mra
d ExEySQRT(Ex*Ey)measured @ PITZ:
p = 5.2 MeV/c
Q = 1 nC = m
Ibuck = Imain * 0.075(100% rms projected emittance)
Results fromPITZ1: 2005 (Gun1) VUV-FEL13nm
XFEL
WR
VUV-FEL 6nm
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 21
Emittance• Results 2006: Gun3.1
0,5
1,0
1,5
2,0
2,5
3,0
278 280 282 284 286 288 290Imain [A]
no
rm. p
roje
cte
d e
mit
tan
ce
[mm
mra
d]
Emitt(x)Emitt(y)
ASTRA simulation
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 22
Setup PITZ1.6 completed !transverse emittance
gunboosterquads
longitudinal phase space masks
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 23
Present layout of PITZ
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 24
PITZ• Simplified scheme
DDC
Rf-coupler
rf
Laser beam
E-gun
Diagnostics
Booster cavityDiagnosticsBeam dump
Not in scale!!
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 25
PITZ diagnostics
Measure Device
Beam:Profile, diameter Screen station (TV), wire scanner
Charge Faraday cup,
ICT (Integrating current transformer)
Beam energy Spectrometer,
dipole magnet
Bunch length Streak camera
Emittance EMSY
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 26
PITZ : Auxiliary system• Auxiliary systems• Vacuum
• Photocathode laser and laser beamline
• Cooling and climatization
• Rf system: 2 Klystrons 5-10 MW, modulators,…
• Electronics
• Controls
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 27
PITZ history
PITZ history Year Gun Project
stage Remarks
1999 Decision directorate 2000 Construction 2001 Gun2 PITZ1 Commissioning 13/01/2002 Gun2 PITZ1 1st photoelectrons 2003 Gun2 PITZ1 Nov.:Gun2: HH 2004 Gun1 Dec.: upgrad 2005 Gun1 PITZ1.5 Upgrade, booster,
10MW klystron 2006 Gun1 PITZ1.6 57MW/m Gun3.1 Conditioning,
Characterization, Gun3.1HH
2007 Gun3.2 PITZ1.6 Cond.,Charact. 2007 PITZ1.7
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 28
PITZ : The shutdown• Why?• Insert HEDA1: High energy
dispersive arm• Move booster downstream
(higher gun gradient)• Space for new CDS booster
(2008)• Minor change of sequence
of diagnostics elements• Prepare for PITZ 2
beamline 2008• Reconstruction of low
energy section (New DDC,..)
• Further tasks• Extension of laser hutch• New laser• New klystron 10MW for rf1• New technical interlock• Many small tasks
– TV system– Exchange YAG screen– EMSYs…– …
• PITZ1.6 PITZ1.7
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 29
PITZ : The shutdown• Major changes in beam
line
GunBooster
Dipole Diagnostics Beam dump
Beam dump
Reconstructed low energy section
HEDA1
New HEDA1
HE diagnostics
modified
PITZ1.6
PITZ1.7
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 30
PITZ 1.6, PITZ 1.7PITZ 1.6
PITZ 1.7
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 31
PITZ : The shutdown• Vacuum work:
– Dismount modules– CTS: Conditioning test stand:
Gun 4.1– Mount modules – Mount HEDA1– Reconstruction Low energy
section:• DDC• Dipole…
– ……– Parallel work of two teams New dipole HEDA1 – 180 grad
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 32
PITZ : The shutdown• RF group:• Reconstruction rf system1• Exchange klystron 5MW10MW• Waveguides to CTS• Investigation of T-combiner • ………
• Electronics:• New technical interlock• Connect all new/moved components, tests• ……….
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 33
PITZ : The shutdown• Controls
• Control and data aquisition of elements of reconstructed beam line and CTS
• Control for new laser
• Control of rf1
• …..
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 34
PITZ : The shutdown• Technical infrastructure• Second crane in tunnel• Reconstruction laser hutch• New climatisation and cooling for laser and
laser hutch• Extension of cooling in tunnel new elements
and CTS• Upgrade of cooling systems• ……• Partially done by external firms
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 35
PITZ : The shutdown• Laser hutch and laser• Extension of Laser: longitudinal profile: flat top with
rise and fall time of 1-2ps(10**-12)• Dismount laser• Extension of laser hutch• Climatisation, cooling , network, electric power• Cleaning• Mount new laser table• Mount new laser• Commissioning of laser: Beginning of November
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 36
PITZ : The shutdown• To do: Preparation and during shutdown
• Sequence of work
• Coordination between technical groups
• Delivery of components
• End of shutdown
• Start running with new laser in test mode: Beginning of November
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 37
PITZ : The shutdown• Flow chart
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 38
PITZ : Outlook• Outlook
• PITZ1.7 PITZ 2 : 2008• HEDA2 :July 2008• Tomography module (March 2008)• Magnets• Rf deflector as option• CDS Booster (Jan. 2008) • Beam dump : 2m³ concreteJuly 2008
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 39
Comparison: PITZ1.6 ↔ PITZ2.0PITZ1.6:
PITZ2.0:
TESLA
CDS
• dipole is ready and tested,• technical design of dispersive arm ready,• parts in fabrication• installation starting August 20
• preliminary dispersive arm and beam dumps have to be replaced by final components• physics design is ongoing• sweeper under fabrication
tomography module + RF deflector are realized depending on EU contracts,basic design available for both devices
tomography module + RF deflector are realized depending on EU contracts,basic design available for both devices
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 40
Acknowledgement• Thanks to F.Stephan, S. Rimjaem and S.
Khodyachykh for providing transparencies and photos
• Thanks to S.Niedworok and Chr. Iezzi for the poster
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 41
PITZ shutdown 2007
• The end
J.Bähr, PITZ, Technisches Seminar, 3.Juli, 2007يح- 42
0,8
1,2
1,6
2,0
2,4
2,8
3,2
320 322 324 326 328 330
Imain, A
norm
. em
ittan
ce /
mm
mra
d ExEySQRT(Ex*Ey)measured @ PITZ:
p = 5.2 MeV/c
Q = 1 nC = m
Ibuck = Imain * 0.075(100% rms projected emittance)
Results from PITZ1:
Particularities, Results from PITZ1• PITZ source must drive super conducting linac long pulse trains, i.e. high average power, good stability
• XFEL goes to very short wavelength very good emittance required
0.2
0.3
0.4
0.5
0.6
0.7
800 1000 1200 1400 1600 1800 2000 2200
t / sec
a.u. Forw ard pow er
R eflected pow er
e.g. 800 µs
~ log(power)long RF pulse:
amplified output train
pulse train from the oscillator
10 Hz, 800µs, 1 MHz
long laser pulse train:
VUV-FEL, 6nm
XFEL
C
WR
measured @ VUV-FEL:
p = 127 MeV/c
Q = 1 nC
• regularly obtain 2.1 mm mrad (100% rms projected emittance)
• minimum 1.1 mm mrad (90% rms projected emittance)
PITZ gun installed at VUV-FEL in 2004
first preliminary emittance results (not optimized yet !)
in operation: gun + booster 13.7 MeV/c
current booster: TESLA prototype
3,5
4
4,5
5
5,5
6
6,5
7
7,5
2 3 4 5 6 7 8
gun peak power, MW
Pm
ean
, MeV
/c
38,4 44,3 49,6 54,3 58,7 62,7Ecath, MV/m
max. mean momentum ↔ gun power
goal: 60 MV/m
measured at PITZ2 (momentum of dark
current edge)
p = 12.8 MeV/c, Q = 1 nC,gun = max_p, booster = min_dp
obtained at PITZ1
0
1
2
3
4
5
6
7
8
262 264 266 268 270 272 274 276 278 280 282
Imain, A
Em
itta
nce
, [m
m-m
rad
]
Xemittance, measured
Yemittance, measured
Simulation (ASTRA)
First Results from PITZ2
Status: • new gun cavity (#3) installed and under conditioning now• upgrade of beamline ongoing