PPT-CLIC Permanent Magnet Quadrupole

Engineering Development update Norbert Collomb STFC Daresbury Laboratory 1 N Collomb 13092012 CLIC Permanent Magnet Quadrupole First part of presentation Progress since last meeting Assembly images. 4 HP Kollmorgen B 802 PM Brushless Servomotor at 1 5 HP Kollmorgen M 828 PM Brush less Rotor Kollmorgen B 808 PM Brushless Rotor brPage 2br Permanent Magnet Servomotor and Induction Motor Considerations Having a lower inertia typically will allow for Magnets. Shashikant . Manikonda. Taylor . Model Methods . VII, . Dec. 14. th. -17. th. , 2011, Key West, Florida. S3 device at SPIRAL2. 2. SHE / VHE - Fusion-evaporation in direct kinematics . SHE / VHE. F. Richard LAL/Orsay. PAC Eugene October 2010. 1. Introduction .  . The . Joint working group on CLIC/ILC general detector issues. , up to now mostly informative since collaborations takes place in a spontaneous fashion, has identified areas which need improvements . and Final Focus Stabilisation. CERN, 27-Mar-2009. 1. EuCARD NCLinac Task 9.3. 27/3/2009. Task 9.3. Task 3 in . DoW. :. Task3. . Linac. & FF Stabilisation. Design, build and test for stabilisation a CLIC . Helena Khazdozian. WESEP. Major Department: Electrical Engineering. Major Professor: Dr. David . Jiles. Outline. Problem Definition. Commercial Wind Turbines. Permanent Magnet Generators. Magnetic Materials. Cryogen Free Splittable Quadrupole. (. Technical Design). . V. . Kashikhin. . for . Superconducting Magnet . Team. Splittable. Quad Review, March 2, 2010, FNAL. 2. Splittable. . Quadrupole. . Milestones . Allen R. . Majewski. Department of Physics. University of Florida . February 2015. NiCl. 2. - [SC(NH. 2. ). 2. ]. 4. . dichloro. -. tetrakis. -. thiourea. -nickel. Overview. The . value of nuclear quadrupole resonance . Possible improvement of the CLIC accelerating structure. From CLIC_G to CLIC_K. 2 .07.2009 Alexej Grudiev CERN Outline Current CLIC accelerating structure: CLIC_G Compact coupler design with damping Transverse Landau Damping. in Circular Accelerators. IPAC’17, Copenhagen, Denmark. . 17. May 2017. M. Schenk. , . X. . Buffat. , L. R. Carver, A. . . Grudiev. , K. Li, . A. . . Maillard. , E. . Métral. 3 . TeV. Many new agreements for X-band development and machines recently . One new coll. inst. (Canadian Light Source, Saskatoon) . WEB pages . Nikos . Kokkinis. has taken over as . responsible from . CIEMAT: . AC structures and Dipoles magnets. CELLS - ALBA: . Stripline. kickers, Impedance and Collective effects, Beam size measurements and 1.5GHz RF system. IFIC (CSIC-UV): . HG-RF and BPMs. 09/06/15. )=0.3B(T)p(GeV/c GeV/crad !8 FODO cells!Dipole length = 5 m!Maximum dipole 25 September 2009. Role of the MDI. The MDI is the part of the CLIC facility (approximately) inside the detector cavern, i.e. the area in which there is a strong coupling of technical subsystems of the machine and of the physics detectors. The lines for the spent beams shall also be considered part of the MDI. accelerating structure design. 21/10/2010. A.Grudiev. (CERN). RF design constraints for CLIC. Beam dynamics (BD) constraints based on the simulation of the main . linac. , BDS and beam-beam collision at the IP:.