T.A.C. FREE ELECTRON LASER FACILITY (T.A.R.L.A.) TURKISH PHYSICAL SOCIETY 5 th INTERNATIONAL PARTICIPATION PARTICLE ACCELERATOR and APPLICATIONS CONGRESS 7-9 September 2013 İSTANBUL - TURKEY Dr. Suat ÖZKORUCUKLU* Vice Director of TAC Project Director of TARLA Istanbul University University *On behalf of TAC Collaboration 1 TURKISH ACCELERATOR and RADIATION LABORATORY in ANKARA (T.A.R.L.A.)
Transcript
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T.A.C. FREE ELECTRON LASER FACILITY (T.A.R.L.A.) TURKISH
PHYSICAL SOCIETY 5 th INTERNATIONAL PARTICIPATION PARTICLE
ACCELERATOR and APPLICATIONS CONGRESS 7-9 September 2013 STANBUL -
TURKEY Dr. Suat ZKORUCUKLU* Vice Director of TAC Project Director
of TARLA Istanbul University University * On behalf of TAC
Collaboration 1 TURKISH ACCELERATOR and RADIATION LABORATORY in
ANKARA (T.A.R.L.A.)
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The First Beam 2
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10-11 June 2012 The TARLA aims to obtain FEL between 2.5-250 m
ranges out of two different optical cavity systems with undulators
of 2.5cm and 9.0cm periods. The electron beam energy is 15-40 MeV.
There is also a Bremsstrahlung line after the second accelerating
module. The electron source is chosen to be a high average current
thermionic DC gun running at up to 250keV, which is in
manufacturing phase at the moment. The injector system will be
completely based on normal conducting technology with two buncher
cavities that operate 260 MHz and 1.3 GHz, respectively The main
acceleration structure will consist of two ELBE modules that each
houses two TESLA 9-cell SC structure. These modules are designed to
operate at 1 mA electron beam current at continuous wave operation
(CW) 3 The Goal
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Glbasi Campus of Ankara University Lake Mogan ANKARA (15km)
Town Glba TARLA 4
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10-11 June 2012 IV. iSAC Meeting 7 He Plant RF &
PowerElectronicsBrems. Exp.Electronics FEL Experiments Clean Room
FEL Experiments Accelerators FELs Layout of TARLA
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Layout of T.A.R.L.A
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Main Components E-Source (Gun) Buncher Cavities Accelerating
units Bunch Compressor Focusing-defocusing magnets Bending magnets
Beam Diagnostic tools .. 9 Overview of TARLA
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To obtain high quality FEL electron source should supply
continuous high bunch charge with lowest emittance We have chosen
thermionic DC gun as the source To obtain 1.0 mA average peak
current we need approximately 80 pC bunch charge with 77 ns bunch
duration 80 pC 10 Electron Gun
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The electron bunches should have short bunch length Therefore
the bunches at the exit of the gun which has approximately 500ps
are needed to be compressed less than 10ps And bunch separation
should maintain same distance as 77 ps. +E drift space standing
electromagnetic wave ~500ps It is possible to use several Buncher
and Buncher frequency should be synchronized with RF frequency in
linac. 11 Buncher Cavities
Slide 12
For having higher current, another equipment which should be on
beam line is bunch compressor. Using Bunch Compressor, bunch length
can be reduced less than 1ps 12 Bunch Compressor
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To achieve 40 MeV electron beam energy we are using two 2
accelerating modules with 2 TESLA (9-cell) cavities To have a large
application area beam should have continuous structure This modules
will able to provide CW electron beam structure 13 Accelerator
Structure
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200-250 keV, 1 mA 9-cell Tesla-cavity 1.3 GHz 1.8 K helium
reservoir 20 MeV. 1mA = 20kW vacuum isolation liquid N 2 shield
solid isolation helium port liquid He @ 1.8K RF ports 10kW 1.3GHz
14 SRF Cavities
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10-11 June 2012 IV. iSAC Meeting ParametersValue Energy
[MeV]15-38.5 Bunch Charge [pC]80 Average Beam Current [mA]1.0 Bunch
Repetition Rate [MHz]13 (16.25) Bunch Length [ps]0.4-6 Norm. RMS
Trans. Emit. [mm mrad]< 16 Norm. RMS Long. Emit. [keV.ps] <
100 Macro pulse Duration [s] 40 - CW Macro pulse Reputation Rate
[Hz] 10 CW 15 Main Electron Beam Parameters
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16 Obtaining FEL
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10-11 June 2012 IV. iSAC Meeting ParametersU1U2 Undulator
Magnet MaterialNdFe Undulator Period [cm]2.59 Magnetic Gap [cm]1.54
Effective Field [T]0.350.42 Undulator Strength0.25-0.70.7-2.5
Number of Period6040 Roll-off-field @ 5mm (%)0.03 0.11 Rayleigh
Length [m] 0.972.08 Resonator length [m]11.53 1st Mirror Radius of
Curvature [m]5.926.51 2nd Mirror Radius of Curvature [m]5.926.51
Radius of Out Coupling Hole [mm]0.5/2 17 Main Und. and
Res.Parameters
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T.H.M. T.A.R.L.A. Demet Parametreleri Some Calculations 18
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T.H.M. T.A.R.L.A. Demet Parametreleri Some Calculations 19
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T.H.M. T.A.R.L.A. Demet Parametreleri Some Calculations 20
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10-11 June 2012 IV. iSAC Meeting UndulatorsU1U2 Wavelength [m]3
- 1918-250 Micro pulse Repetition Rate [MHz]13 Max Peak Power
[MW]~5~2.5 Average Power [W]0.1-400.1-30 Max. Pulse Energy [J]~10~8
Pulse Length [ps]1-10 21 Main FEL Parameters
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10-11 June 2012 IV. iSAC Meeting The injector consists of a
250kV DC Gun a 260 MHz S.H.B a 1.3GHz F.B., Solenoids, Diagnostics
vacuum equipment's 22 Status of Injector
Slide 23
Gun mechanical manufacturing completed Clean room and cleaning
station obtained Vacuum components obtained Test stand and
shielding cover manufactured Control units for vacuum and HV
devices obtained Bias and filament heater power supply are obtained
HV platform holder and isolator legs obtained Selenoid magnet
ordered 150 kV HV Power Supply and Pulse Generator 350 kV High
Voltage Isolation Transformer High Voltage Cable, Shielded,
isolation voltage >350 kV dc. FCT/ ICT current transformer
obtained 23 Status of Injector
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Control software Control electronics Steerer magnet View ports
and cameras Emittance measurement systems designed Other diagnostic
tools from NTG company ordered Faraday Cup with feed through
Faraday Cup as a beam dump BPM (2) Feed through (3) Different
lengths beam pipes 24 Status of Injector
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10-11 June 2012 High Voltage Divider: 37 HV resistors in series
10Meg each resistor 15cm each resistor Each resistor has 8kV and
6.4W @300KV 0.8mA 150kV output @ 300kV 8mA input Since mechanical
design is modular, electrical parameters can be modified easily 25
Technical: Voltage Divider
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10-11 June 2012 1.High Voltage Divider 2.Custom Design Devices
inside Faraday Cup: Remote Controller for Pulser 13MHz Trigger and
Macropulser for Pulser RF Mixer 3.Cathode and connections 4.6
Channel Temperature Controller 5.1.3 GHz Master Oscillator 6.I/O
Protection Circuit 7.8 Channel PLL Divider 8.Motor Drivers 26
Technical: Electronics
10-11 June 2012 IV. iSAC Meeting EPICS Extensions: MEDM, Probe,
Visual CT Soft Module: ASYN Protocols: RS232, TCP LAB VIEW 29
Technical: Software Development
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Technical: LabView 30
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E-PERM System 50 LT detectors 6 ST detectors 1 Water test kit 1
Reader EPD response: 0.01mSv-10 Sv Energy range: 50keV-6 MeV (for
gamma and X-rays) 2 Portable Survey meters Individual Monitoring 55
EPDs 2 Access control readers database & utility software's
respond to gamma and X-rays uses Electret Ion Chambers as a passive
device suitable for long term and short term atmospheric radon
measurements, as well as radon in water error < %8 For alpha,
beta, gamma, X-ray radiations Max dose rate 100 mSv/h Overload
indication up to 10 Sv/h Linearity error 10% in the measuring range
31 Technical: Radiation Safety
Average Beam Current Measurement : Electron beam enegry was 165
keV Grid Voltage was -165 kV + -20V Voltage was 0.035 mV Beam Dump
IeIe 0.1 ohm Shunt Resistance Average beam current has measured 350
uA Technical: First Beam Measurment 34
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10-11 June 2012 IV. iSAC Meeting Research Instruments offers a
Super conducting RF accelerating module with 2 TESLA cavities for
continuous RF operation. This module is compact and houses two
TESLA cavities and is designed for continuous operation at
accelerating fields in the range of 15 to 20 MV/m. The cryostat
design has been developed by ELBE group (Forschungszentrum
Rossendorf) and is used under a license agreement. June 21st, 2012
Tuning range120 kHz External Q of HOM couplers > 5x10 11 Total
accelerating voltage of the module > 20 MV Total cryogenic
losses at 20 MV cw operation < 75W 35 Delivery December 2014
3.88 M Status of SRFs
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10-11 June 2012 IV. iSAC Meeting The supplier is responsible
about the subjects and components listed below The supplier should
manufacture the SRF modules based on the original ELBE design with
some minor changes which are summarized as following: The HOM
couplers will use sapphire feed-through suited for CW operation and
will be thermally anchored to the helium vessel The thermal shield
will be reviewed and eventually produced from copper instead of
aluminum The instrumentation will be updated slightly. The surface
treatment of the cavities after manufacturing and before cold RF
test will be done in accordance with the recipe developed at DESY
for the XFEL cavities. 36 Status of SRFs
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10-11 June 2012 Resonance frequency260 MHz Theoretical Q5800
Tuning range1 KHz Bakeable up to200C Leakage rate< 1E -9 mbar
l/s Weight121 kg MaterialCu OFHC / Stainless Steel 1.4429 Resonance
frequency1300 MHz Theoretical Q13.600 Tuning range2.2 MHz Bakeable
up to200C Leakage rate< 1E -9 mbar l/s Weight16.2 kg MaterialCu
OFHC / Stainless Steel 1.4429 37 Status of Bucher Cavities
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10-11 June 2012 The supplier is responsible about the subjects
and components listed below Design, material and manufacturing of
260 MHz SHB and 1.3 GHz FB cavities Manufacturing of SHB and FB
Vacuum brazing and final surface preparation and delivery of SHB
and FB Leak checking for SHB and FB RF layout for SHB and FB -
including cavities and drive line Complete assembly of buncher
cavities - cavities, tuner, input coupler, field probe Complete
instrum. Of buncher cavities Factory acceptance tests Shipment and
installation at TARLA Acceptance testing Reports of acceptance
tests 38 Status of Bucher Cavities
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10-11 June 2012 Kick-off Meeting: October 2 nd - 4 th 2012
Second Meeting for Payment: May 29 th 30 th, 2013 June 15 th, 2012
39 Delivery Novemver 2014 4.359 M Status of He Plant
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10-11 June 2012 Helium compression system (water cooled) Oil
removal system Gas controlling panel Refrigeration cold boxes 1 -2
Transfer line from cold box to Dewar 2 transfer lines from box 2 to
cryostats Dewar ( 500 l) and Buffer Tank Control system with
additional remote monitoring unit as an option The refrigeration
plant has to (alternatively) fulfill the following tasks: A1-
Cooling of the super conducting cavities from ambient temperature
down to the operation temperature of 1.8 K A2- Cooling of the
cavities during full load operation at 1.8 K A3- Warm up of the
cavity up to ambient temperature B -Cooling of the cavities at 4.5
K in the standby-operation mode and liquefying The Task A2 is the
main purpose of the plant - 220 W at 1.8 K (16 mbar) 40 Status of
He Plant
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10-11 June 2012 IV. iSAC Meeting UnitCyromodule ICyromodule II
HeliumHeat LoadDynamicW80 StaticW15 ContingencyW10 TotalW105
TemperatureMaximumK2.1 MinimumK1.8 Pressure Stabilitymbar 0.2
Liquid Level StabilityL LHe 2 InventoryL70 LN2Total Heat LoadW35
TemperatureK70-80 He Plant Parameters 41
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10-11 June 2012 16 kW solid state power amplifiers (SSPA) were
planned for high power RF (HPRF). We have been in contact with both
Bruker and Thomson Broadcast for the solid state amplifiers.
Mechanic and thermal studies of SRF Power couplers (input &
HOM) are completed (CST), Design Simulation (CST), Production
studies (if it is possible in TURKEY) are ongoing 42 Status of
RF
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10-11 June 2012 Conceptual design of waveguide is finished and
components for transmission lines are determined. HPRF transmission
line simulations (HFSS) are finished. The procurement process has
been planned to complete by the end of 2013. 43 Status of RF
Transmition Lines
Slide 44
FEL Pervin Arkan FEL Pervin Arkan HV B. Ko . ara HV B. Ko . ara
Infrastructure E. Kazanc . ara M. Yldz Infrastructure E. Kazanc .
ara M. Yldz Diagnostic . Kaya A.Aksoy .Polat Diagnostic . Kaya
A.Aksoy .Polat RF . Karsl A. Aksoy Z.Sali B.Dursun .Polat RF .
Karsl A. Aksoy Z.Sali B.Dursun .Polat Control Y.Barutu S. Kuday
E.Kazanc Control Y.Barutu S. Kuday E.Kazanc Electronic B. Ko G.
Kalayc Electronic B. Ko G. Kalayc Vacuum . Kaya E. Kazanc M. Yldz
Vacuum . Kaya E. Kazanc M. Yldz Beamline A.Aksoy . Kaya Beamline
A.Aksoy . Kaya Cryogenics A.Aksoy .Kaya Cryogenics A.Aksoy .Kaya
Resonators A.Aksoy H. Tugay Resonators A.Aksoy H. Tugay 44 Status
of Personel
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10-11 June 2012 IV. iSAC Meeting FEL Pervin Arkan Diagnostic
.Tapan Diagnostic .Tapan Gen. IR Lab. A.Aydinl Gen. IR Lab.
A.Aydinl Ultrafast PAL H. Altan O. Esentrk Ultrafast PAL H. Altan
O. Esentrk Bio-Micro SL F. Severcan. Bio-Micro SL F. Severcan.
Material PL . lday Material PL . lday BREMSSTRAHLUNG skender Akkurt
Detector M.Do ru S. ahin Detector M.Do ru S. ahin Photon Dump H.O.
Tekin Photon Dump H.O. Tekin e. Dump G. Ye in S.Sariaydin e. Dump
G. Ye in S.Sariaydin Radiator N. Demir Z.Demirci Radiator N. Demir
Z.Demirci Simulation N. Karpuzcu Simulation N. Karpuzcu 45
Experimental Groups
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46 IR FEL Stations (5): Photon science and diagnostics
Ultrafast photonics applications General IR spectroscopy Material
characterization Bio-micro spectroscopy and biomedicine
Bremsstrahlung station (1): Nuclear spectroscopy Commissioning of
TARLA accelerator is expected in 2016 TARLA is an official member
of EU-FP7 Project named as CALIPSO for training of users in any 20
European Light Source Facilities 46 Planned Experiments
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Peter MICHEL (HZDR-ELBE, Germany) (Head) Hideaki OHGAKI (Kyoto
University, Japan) Dieter TRINES (DESY, Germany) Ernst WEIHRETER
(HZB-BESSY, Germany) Jean R. DELAYEN (JLab, USA) 1st Meeting:
December 4-5, 2009 Ankara University 2nd Meeting: September 2-3,
2010 Bodrum, Mugla 3rd Meeting: May 12-13, 2011 IAT, Ankara
University 2010 4th Meeting: March 8-9, 2012 IAT, Ankara University
47 5th Meeting: April 22-23 2013 IAT, Ankara University iMAC
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TARLA WBS 48
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10-11 June 2012 IV. iSAC Meeting http://tarla.ankara.edu.tr
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