PPT-The Mu2e Experiment at FNAL

A precision window into physics beyond the standard model Andrew Norman University of Virginia For the Mu2e amp g2 Collaborations DPF 2009 Detroit MI Wayne State University Why Precision . ,. Fermilab. . (on behalf of the team: N. . Solyak. A. . Lunin. , I. . Gonin. , and V. . Yakovlev. ) . Coupler kick and wake simulations upgrade. 1. LCWS2010 & ILC10. March 26-30, 2010. N.Solyak, RTML. Copy these questions to your paper, skipping 2 lines between each question.. What is the problem?. What is the hypothesis?. What are the basic steps in the experiment?. What is the independent variable?. Michael . Lamm. For the Mu2e Solenoids. RESMM’12. February 13, 2011. Outline. Introduction. Scope. Key Design issues. Conclusions. L2 Solenoid. Feb. 13, 2012. Power Supply/Quench Protection. Cryoplant (actually off project). Douglas . L. . Tucker. (. FNAL). DES Collaboration Meeting. ICG, Portsmouth. PreCam Parallel . Session. 29 June 2011. Data Processing. DES. -. Brazil Effort. The official data processing.. Uses a PreCam-specific version of the Quick Reduce Pipeline.. Eric . Prebys. , FNAL. Goals of this course. I hope this course will provide you with…. a rigorous foundation of the underlying physics of particle accelerators, . Fairly sophisticated understanding of . Current status. Arkadiy Klebaner. November . 21. , . 2012. Scope. Compressor system. Refrigeration system. Cryogenic storage and inventory management. Muon g-2 cryogenic distribution system. Mu2e cryogenic distribution system. Pg. 477 - 484. Interference. We now know that the experiments failed for two simple but important reasons:. 1. Atoms send out a burst of light energy about every 10. -8 . s so the probability that the atoms in each source would emit their light waves in phase is nearly zero – the result is an interference pattern that changes in an irregular fashion and is impossible to see. Eric Prebys. Extinction. October 21-24, 2014. WBS 475.02.08 Extinction. The Mu2e experiment has very stringent limits on the amount of beam that appears between pulses. The extinction task is comprised of. Cryogen Free Splittable Quadrupole. (. Technical Design). . V. . Kashikhin. . for . Superconducting Magnet . Team. Splittable. Quad Review, March 2, 2010, FNAL. 2. Splittable. . Quadrupole. . Milestones . Arkadiy . Klebaner. January 23, 2012. Scope. Compressor system. Refrigeration system. Cryogenic storage and inventory management. Muon g-2 cryogenic distribution system. Mu2e cryogenic distribution system. N.2 . C.T.E.R. .. N.1 tecnico a tempo determinato (art.15). N.2 borse da tecnologi (scadenza novembre 2012). N.1 borsa da tecnico (scadenza Marzo 2013). N.1 borsa da tecnico (scadenza Giugno 2014). Attrezzature officina meccanica. st. , 2017. FNAL. SBN – Far Detector . Installation Plans for Warm Vessel. ICARUS-T600 Installation and Integration. Mar 1, 2017. WA104 Meeting - SBN-FD Installation . 2. Overview. Warm vessel steel structure on-site. Aaron Smith under the mentorship of Joseph . Dey. Accelerator . Devision. /RF Department. Beam Bunches. Aaron Smith. 2. RF systems cause the beam to form . bunches. The bunch size (width/time) is determined by the. R. Rivera. Mu2e TDAQ L2 Manager. 4/20/16. TDAQ Management Team. Ryan Rivera – L2 Manager, L3 Manager (Project Management, System Design & Test). Group Leader - Real-time Systems Engineering, Detector .