PPT-CLIC Spectrometer Magnet Interference

Computation of transversal Bfield on primary beam CLIC main parameters 9252009 Detlef Swoboda 2 Center of mass energy 3 TeV Peak Luminosity 2 10 34 cm 2 s 1 Repetition rate. Scheme. in the (80 km) TOE: Tunnel Of . Everything. Lucio Rossi, Attilio Milanese and Davide Tommasini. CERN. Work. of H. . Piekarz. (FNAL) . widely. . used. HE-LHC . c. ost. : . rough . evalution. Engineering Development update. Norbert Collomb, STFC Daresbury Laboratory. 1. N. Collomb. 13/09/2012. CLIC Permanent Magnet Quadrupole. First part of presentation:. Progress since last meeting. Assembly images. MICO 230. Steve Virostek. LBNL. August 7, 2013. Status of SS1. The magnet was cooled down to LHe temperature two weeks ago.. Iron shield with 60 cm hole has been mounted.. Low current testing (up to 50 A) revealed resistive behavior in the E2 coil 500 A HTS lead – worse than previous failed HTS lead.. Solenoid magnet funding. Brisbane magnet. Some logistics. Status of detector system design. Robert Page. 1. Solenoid magnet funding. Funding approved for:. Brisbane magnet. Power supplies. Shipping. David Townsend. President of CLIC. Chair, Save the Dam Working Group. Who is CLIC ?. Chiputneticook Lakes International Conservancy (CLIC). Founded in 1992. Non-Profit incorporated under laws of Maine. muon. beam. A pair of identical, 3-m long spectrometer solenoids will provide a 4-tesla uniform field region at each end of the cooling channel. The . emittance. of the beam as it enters and exits the cooling channel will be measured within the 400 mm diameter magnet bores. The magnets incorporate a three-coil spectrometer magnet section and a two-coil section that matches the solenoid uniform field into the MICE cooling channel. The cold mass, radiation shield and leads are kept cold by means of a series of two-stage . G. Riddone, 02/02/2010. 1. Content. Introduction to RF . structures and . components. Fabrication baseline procedure for accelerating structures . Application to CERN ac. structure fabrication. Fabrication of PETS . 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 . Hiroyuki Sako (ASRC, JAEA / U. Tsukuba) for J-PARC-HI Collaboration. Outline. Overview of J-PARC-HI. Experimental design and simulations. Summary and Prospect. 1. J-PARC Heavy-Ion Project (J-PARC-HI). And. Proposal for a short term R&D effort. Recent Events. Conventional Facility Design for NLC · Stanford Linear Accelerator Center, March 10 to 28, 2003. CARE/ELAN meeting @ CERN November 23 - 25 2005.. 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. 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:. Staging. , . early. science and . upgrade. . path. Rasmus Toft-Petersen. Technical University of Denmark. Calibration. . normalization. Gold . foil. for flux (tricky with . white. beam). Vanadium line .