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1 Accelerator R&D for Future Large Colliders at IFIC Scientific Staff: A. Faus-Golfe, C. Alabau, J.J. García, S. Verdu, J. Alabau Technical Staff: J.V.

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Presentation on theme: "1 Accelerator R&D for Future Large Colliders at IFIC Scientific Staff: A. Faus-Golfe, C. Alabau, J.J. García, S. Verdu, J. Alabau Technical Staff: J.V."— Presentation transcript:

1 1 Accelerator R&D for Future Large Colliders at IFIC Scientific Staff: A. Faus-Golfe, C. Alabau, J.J. García, S. Verdu, J. Alabau Technical Staff: J.V. Civera, C. Blanch ILC Spain 09

2 2 Capabilities - CALCULATION BEAM DYNAMICS EXPERTISE:  Electromagnetic analysis Electric circuits & electronics  Mechanical analysis  Optics design  Non-linear dynamics studies  New instrumentation techniques  Commissioning 3-D modelling of BPM - PROTOTYPING  Design: tooling, drawings  Fabrication follow-up  Assembly  Testing and Calibration BEAM INSTRUMENTATION : ILC Spain 09 Emittance simulations and measuremts in ATF

3 3 Main ongoing projects  ILC and its Test Facility ATF-ATF2: Beam dynamic studies and commissioning of the ATF EXT line (LAL, KEK, SLAC) Multi-OTR system for ATF2 (SLAC, KEK) BPM supports with micromovers for FONT4 in (KEK, JAI) BDS instrumentation studies  CLIC and its Test Facility CTF3: BPM’s for the TBL in CTF3 (UPC, CERN, Applied Physics-UV) Drive Beam BPM’s for CLIC module (CERN) ILC Spain 09  Super Large Hadron Collider: Beam dynamics studies and measurements on beam halo, intensity reach and collimation efficiency (CERN-EUCARD)

4 4 ATF was built in KEK (Japan) to create small emittance beams. The Damping Ring of ATF has a world record of the normalized emittance of 3x10 -8 m rad at 1.3 GeV. ATF2 has been built to study the feasibility of focusing the beam into a nanometer spot (~40 nm) and nanometer stability in a future linear collider. Extraction line drives the beam from ATF to ATF2 ILC and its Test Facility ATF/ATF2: ILC Spain 09

5 5 (OTR) extraction diagnostic section wire scanners OTR monitor ATF and ATF2: Emittance growth Since several years, the vertical emittance measured in the diagnostic section of the EXT line is significantly larger than the emittance measured in the DR. The simulations and the measurements of the effect of non- linear magnetic fields (mainly QM7R) show an emittance growth with a strong dependence with the extraction position. But still there must be another source for the emittance growth since the extracted beam was significantly larger than expected in three of the data sets. Recently, the QM7R magnet was replaced by a similar one with larger aperture, for which magnetic measurements and simulations indicate that non-linear fields are negligible at the extraction position. The beam passes horizontally off-axis through the shared magnets with the DR ILC Spain 09 Beam size at the OTR/XSR

6 6 Emittance measurements with the wire scanners located in the diagnostic section of the EXT line are very slow. (OTR) extractiondiagnostic section wire scanners OTR monitor Multi-OTR (4 units) beam dynamics studies, design, construction, and characterization including associated software control and electronics ATF and ATF2: Multi-OTR System ILC Spain 096

7 7 ATF and ATF2: Multi-OTR System OTR1X OTR0OTR1 OTR2 OTR3OTR4 extraction diagnostic section The location of the OTR’s has to be optimized such that the phase advances be apropiate to allow emittance measurements ILC Spain 097

8 8 ATF and ATF2: Multi-OTR System ILC Spain 09 Beam dynamics calculated with MAD to study the beam sizes in order to place the OTR’s. MW0X MW1X y vs x x’ vs xy’ vs y 8ILC Spain 09

9 9 ATF and ATF2: Multi-OTR System Current OTR installed in the ATF2 EXT line target CCD camera beam The current OTR was updated with a new target and target actuator, calibrated and tested with beam during November ´09. Beam spot measurement with OTR 9ILC Spain 09

10 10 ATF and ATF2: Multi-OTR System New design of the OTR for ATF-ATF2 - Target actuator relocated to the top (no interference with the girder) and smaller design  greater flexibility in the OTR placement - Thinner target  reduce radiation damage - CCD camera parallel to the target (before it was not parallel, which meant that the beam spot was in focus on only a small portion of the target)  greater depth of field. - 12 bit camera for more dynamic range with smaller pixel size for more resolution. New OTRs will have same controls and motion capabilities as current OTR with the following improvements: Focus adjuster slide X and Y target position viewing adjusters Mitutoyo 10X lens And 1x tube lens 90deg mirror Newport Vertical mover Newport Horizontal mover Target inserter Prosilica camera Installation planned on March´10 10ILC Spain 09

11 11 ATF and ATF2: BPM’s supports with micromovers for FONT4 Last line of defence against relative beam misalignment Measure vertical position of outgoing beam and hence beam-beam kick angle Use fast amplifier and kicker to correct vertical position of beam incoming to IR FONT – Feedback On Nanosecond Timescales IP intra-train feedback system ILC Spain 0911ILC Spain 09

12 12 ATF and ATF2: BPM’s supports with micromovers for FONT4 design, construction, and characterization including associated electronics and software development of 3 sets Range: ±1 mm Step size: 10 μm Stability better than 1 μm Time response ~ sec ILC Spain 09 Realignment of BPM to increase the resolution Labview Software development Movers & holding structure 12ILC Spain 09

13 13 ATF and ATF2: BPM’s supports with micromovers for FONT4 ILC Spain 09 One set has been assembled and installed in ATF2. At the moment it’s under modification by magnetic problems. Other two sets in construction. Software already finished. Realistic simulations of the beam dynamics including the FONT feedback system are being made at the moment. Mover installed at ATF2 13ILC Spain 09

14 14 The TBL is designed to study and validate the drive beam stability during deceleration in CTF3. The TBL consists of a series of FODO lattice cells and a diagnostic section at the beginning and end of the line. Each cell is comprised of a quadrupole, a BPM (labeled as BPS) and a Power Extraction and Transfer Structure (PETS). 3D View of a TBL cell with the PETS tanks, the BPS’s and the quadrupoles 2.25 cm BPS Prototype Inductive Pick-up (IPU) TBL beam time structure Inductive sensors PCB The CLIC and its Test Facility CTF3: ILC Spain 09

15 15 CTF3: BPM’s for the Test Beam Line BPS Prototypes, Series Production and Calibration  A set of two prototypes of the BPS's labeled as BPS1 and BPS2 with its associated electronics has been designed, constructed and characterized by the IFIC team with the collaboration of the CTF3 team at CERN (May 2008). BPS1 and its support installed in the TBL line Measurements of the BPS1 with beam in the TBL line ILC Spain 09  BPS1, jointly with its support and its amplifier, was installed successfully at TBL; BPS2 remained at IFIC as spare (July 2008).  BPS1 first beam measurements were carried out (August 2008). Wire set-up for BPS prototype characterization tests at CERN Labs Low-frequency wire set-up 3D view design Control and DAQ equipment for all the setup signals Overview of the new wire test bench for BPS series characterization tests at IFIC labs  A new wire test bench for BPS series characterization tests was designed and built at IFIC (March 2009).  The BPS series production (15 units) started at IFIC labs (November 2008).

16 CTF3: BPM’s for the Test Beam Line BPS Prototypes, Series Production and Calibration  Tests for BPS2 and BPS3 carried out with the new wire set-up at IFIC. Less than 50um accuracy (March 2009).  Two more BPS units was delivered and installed, BPS2 and BPS3 both with new improved electronic PCBs (May 2009).  14 BPS units construction and assembly process finished (August 2009).  A LabVIEW application (SensAT v1.0) is developed for automatize the BPS series characterization tests in the new wire test bench (September 2009).  The 14 BPS units tests finishes, they are delivered to CERN and finally installed in TBL (October 2009).  All the BPS are validated successfully in TBL after first calibration tests (October 2009).  Beam tests in TBL for the full installed BPS series. Measurements at high beam current (30A) and checking of the BPS’ resolution and performances. All BPS units jointly with its supports and amplifiers installed in TBL (CLEX area, CERN). Calibration test in TBL shows good BPS performance with flat-top pulse response. 16ILC Spain 09

17 CTF3: BPM’s for the Test Beam Line BPS High Frequency Test 3D views of the High frequency set-up design for measuring the BPS longitudinal coupling impedance To determine the BPS longitudinal coupling impedance at more than 12GHz, affecting beam stability. Development of HF set-up has been carried out in parallel of the BPS series production. Electromagnetic simulation of HF set- up design (until 30GHz) with specialized software FEST3D HF set-up manufacturing and BPS HF tests to be performed next January Simulation results of last HF set-up design. S11 reflection parameter from 0 to 30GHz. Simulation SW: FEST3D Simulation SW: HFSS -40dB 17ILC Spain 09

18 18 CLIC: Drive Beam BPM for the 1st CLIC module DB BPM The drive beam quadrupole and BPM are mounted on the drive beam girders. BPMs cannot be moved independently of the PETS, the quadrupoles will either be on movers, or equipped with dipole corrector coils. The BPMs are mounted before quadrupoles. The acceptable level of wake field needs to be determined. AccuracyResolutionStabilityRangeBandwidth Beam tube aperture Available length Intercepting device? How many? Used in RT Feedback? Machine protection Item? CommentsRef BPM 20µ m 2µ m ?<5mm35MHz23mm104/74mmNo41480Yes Inductive ? Strip line ? CLIC note 764 Nominal beam parameters: Charges/bunch: 5.2 10 10 Nb of Bunches: 2922 Bunch length: 1mm Train length: 243.7ns

19 19ILC Spain 09


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