actividades del grupo de aceleradores del ciemat en los grandes aceleradores lineales en proyecto
DESCRIPTION
Actividades del grupo de aceleradores del CIEMAT en los grandes aceleradores lineales en proyecto. David Carrillo en nombre de la Unidad de Aceleradores. Índice. Contribución a CLIC–CTF3 (PETS, quads, kicker) PETS TBL Diseño y fabricación Medidas Contribución a XFEL Linac CIEMAT. - PowerPoint PPT PresentationTRANSCRIPT
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David Carrillo en nombre de la Unidad de Aceleradores
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Contribución a CLIC–CTF3 (PETS, quads, kicker)◦ PETS TBL
Diseño y fabricación Medidas
Contribución a XFEL
Linac CIEMAT
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* In 2004, CIEMAT joined the CTF3 experiment to test the feasibility of CLIC(CERN). Our contribution consists of the delivery of different components for the Combiner Ring and also for the Transfer Lines and the Test Beam Line. In this participation, with an overall budget of around 1,5M€, we had an important industrial contribution.
33 Horizontal/Vertical Correctors
Tail Clipper Kicker16 TBL quad Movers
Fast Kicker
Septa
4 TBL PETS
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Previous design30 GHz PETS (4 waveguide extractor)
Final version:12 GHz PETS(2 waveguide extractor)
Electron
beam
Electric field produced when The electrons are “decelerated”
RF optimization
Power extracted
Power extracted
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Copper rods
Power extractor Vacuum port
WR90 waveguide
Supports
Fiducials
Cooling pipes
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Each PETS was made of eight OFE copper rods (800 mm) These were the most difficult parts to fabricate: overall tolerance is
+/- 0.02 mm and roughness should be better than 0.4 micron The coupling cell is smaller: two different tools were necessary Two intermediate thermal treatments for stress relaxation
8
Copper rod
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Waveguides brazed in Spanish company AIMEN
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•Brazing consists of the joining of metals through the use of heat and a filler metal – one whose melting temperature is above 450°C but below the melting point of the metals being joined
•There have been some problems: •Furnace has not view port •It has graphite heating elements•Copper machining (flatness, roughness)
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Courtesy Serge Mathot, CERN
•Copper parts were polished at CERN, because they were not flat enough
•Copper parts were cleaned by ultrasonic bath, and at CERN, they were also etched and passivated
•Power extractor was successfully brazed at CERN
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Contribución a CLIC (PETS, quads, kicker..)◦ PETS TBL
Diseño y fabricación Medidas
Contribución a XFEL
Linac CIEMAT
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A special test bench has been designed to do RF measurements on each rod It consisted of two side blocks put together with a single PETS bar in order to
create inside a mode with same properties as decelerating mode Results agree with 3-D measurements
Mode TE10
HFSS model
E field and probe
Phase S31 vs position
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Mode launcher was needed to produce working mode in order to do RF measurements on PETS before final assembly
Two mode launchers were manufactured and measured and they were ok for measuring PETS final assembly
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Input couplers manufactured
HFSS input coupler model
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InputCoupler
InputCoupler
Coax to
WR90
Power Extractor
Absorber
Absorber
Port1
Port4Port2
Port3
Choke
Absorber
Coax to
WR90
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No visible change in S11 when removing wire, or absorber from port 4
Both S21 and S31 are aprox. -3dB at 12 GHz
S11 HFSS Simulation
S11 Experimental results
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•A special test bench was designed to measure the assembly of rods•A coaxial antenna was used to measure the field through the slots between the rods
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11944 MHz 50 MHz detuning
In the worst case a 10% power loss extraction is expected
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m
MHz
dRa
df
2.0
m
MHz
dIncRb
df
1.1
Distance from PETS cell peak to axis
Radius of curvature
deg2MHz
edRcurvatur
df
Distance from peak to valley
R curvature
Beam
axis
Ra
IncRb
A sensitivity analysis is ongoing to understand the cause of this detuning
In principle frequency looks quite sensitive to the profile flatness and to the distance from peak to valley
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0 50 100 150 200 250 300 350 400 450 500-100
-80
-60
-40
-20
0
20
40
60
80
100
Time (ns)
RF
pha
ses
(deg
)
Pout left
Pout right
0 100 200 300 400 500 600-16
-14
-12
-10
-8
-6
-4
-2
0
2
Time (ns)
Bea
m c
urre
nt (
A)
BPM0150
BPS0210
BPS0250BPS0310
BPM0310
-100 0 100 200 300 400 500-1
0
1
2
3
4
5
6
7
8
9
Time (ns)
RF
pow
er (
MW
)
Pout left
Pout right
Pref leftPref right
P predict
TBL PETS Contribution TBL Commissioning Status
RF power producedRF pulse phase
Beam current along the line
Courtesy Steffen Doebert, CERN
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up to 10 A through PETS
20 MW max produced at a pulse length of 280 ns
Power production consistent assuming a form factor of 0.9
PETS series production launched together wit CIEMAT(series of 8)
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TBL prototype beam line spring 2009
BPM, Quad Mover, Quad, PETS-tank
Courtesy Steffen Doebert, CERN
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TBL PETS Contribution
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Contribución a CLIC (PETS, quads, kicker..)◦ PETS TBL
Diseño y fabricación Medidas
Contribución a XFEL
Linac CIEMAT
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XFEL CONTRIBUTION
LASER LIGHT SOURCES:XFEL (1)
• CIEMAT is collaborating since 2004 in the international project XFEL (X-Ray Free Electron Laser) to be installed in DESY (Hamburg).
• It is a Laser Light Pulsed Source of 100ns duration pulses in the band from 0.085 to 6 nm.
• It consists of a Superconducting LINAC ( cavities and magnets) up to 20 GeV plus an array of undulators based on permanent magnets.
Our contribution is valued in about 12 M€ and our commitment consist of the delivery of the following systems:
•120 Superconducting Magnets plus their Power Supplies.
• 91 Intersections between undulators made from different elements
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* Within the first contribution, our group has developed a short series of four superconducting combined magnets (one quadrupole + two dipoles) while the remaining 100 magnets will be developed by industry. The design is being reviewed to decrease the magnetization effects.
LASER LIGHT SOURCES:XFEL (2)
Combined Superconducting Magnet for XFEL (2006)
Combined Superconducting Magnet for XFEL
Installed in the “XFEL String” (2007)
fname "HH_10052007_0949"
60 40 20 0 20 40 600.114
0.116
0.118
0.12
0.122
0.124
0.126
0 - 5050 - 00- -50-50 - 00 - 50
I [A]
gdl/I
60 40 20 0 20 40 600.94
0.96
0.98
1
1.02
1.04
1.06
0 - 5050 - 00- -50-50 - 00 - 50
I [A]
gdl/I/.1
223
Magnetization Measurements for the
Combined Superconducting Magnet for XFEL (2007)
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* Within the second contribution, CIEMAT must deliver some main components of the intersections between undulators, as well as its full assembly (optional). These components are:
* The Phase Shifter Magnet (including a magnetic measuring table to measure its field quality)
* The MOVERS for the quadrupoles
* The base structure for the full Intersection
LASER LIGHT SOURCES:XFEL (3)
General Scheme for the XFEL Interseccions
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LASER LIGHT SOURCES:XFEL (4)
Phase Shifter 3D Model by CIEMAT
Measurement bench 3D Model
by CIEMAT
Mover 3D Model by CIEMAT
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Contribución a CLIC (PETS, quads, kicker..)◦ PETS TBL
Diseño y fabricación Medidas
Contribución a XFEL
Linac CIEMAT
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MULTIPURPOSE: THE CIEMAT LINACCIEMAT is considering to install a multipurpose accelerator to study some of the applications presented in this table. A first analysis has been performed at Bevatech and there an existing proposal based on IH cavities
APLICACION Partículas Energía (Mev)
Corriente (µA)
TRANSMUTACION p,d 200 100-1500 INSTRUMENTACION NUCLEAR
p,d 15-30 100
MATERIALES p,He 5-50 10 FUSION p,d,He 20-60 1-10 DOSIMETRIA p 100 1 MEDICINA NUCLEAR p,d,He 7-200 0,01-100 ELECTRONICA p 5-60 0,01-1 Proposal for a LINAC-CIEMAT based on IH Cavities at room
temp.
ION SOURCE Parameter
Ion Species H,D,He A/q=2
Beam Current Up to 1 mA
Beam Emittance 0.4-0.8
Extraction voltage 3-20 kV
RFQ Parameter
Input Energy 3-10 (AkeV)
Output Energy 300-1000 (AkeV)
Operation RF Frequency 175 MHz
Duty cucle >1% (possibility cw)
DTL Parameter
Input Energy 300-1000 (AkeV)
Output Energy 30 (AMeV)
Operation RF Frequency 175 MHz
Upgrade option Yes, up to 50 (AMeV)
Energy variability Yes in 5 steps