PPT-The High-Power-Target System
Author : aaron | Published Date : 2018-01-07
of a Muon Collider or Neutrino Factory K McDonald Princeton U August 29 2014 NuFact14 U Glasgow The Target System Concept A M uon Collider needs muon beams
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The High-Power-Target System: Transcript
of a Muon Collider or Neutrino Factory K McDonald Princeton U August 29 2014 NuFact14 U Glasgow The Target System Concept A M uon Collider needs muon beams of both signs. Context: Muon Collider and Neutrino Factory. 1997. : Colin . Johnson argued . that the next step after the ACOL antiproton production target should be a mercury jet target. . [U. Miss. Workshop, Jan 1997; my introduction to Muon Collider . Yongjoong. Lee. ESS, Materials. , Target Division. 5. th. High Power . Targetry. Workshop. May 20, 2014. Spallation Target at ESS. 5 MW spallation source. 5 MW (2.0 GeV/2.5 mA) proton beam . 2.86 ms long beam pulse with 14 Hz repetition rate. Muon. Source. K. McDonald. Princeton U.. . (December . 5. , 2014). MAP Winter Meeting. SLAC. The Target System Concept. A . M. uon. Collider needs . muon. beams of both signs.. A Neutrino Factory based on neutrinos from . Robert Wham, Ph.D.. Presented to. Future in Space Operations. April 20, 2016. You Tube. . . https://www.youtube.com/watch?v=9YmkxGdp-b0. . Why Pu-238 as a Heat Source?. Long half-life- 87.7 years. Yongjoong. Lee. ESS, Materials. , Target Division. 5. th. High Power . Targetry. Workshop. May 20, 2014. Spallation Target at ESS. 5 MW spallation source. 5 MW (2.0 GeV/2.5 mA) proton beam . 2.86 ms long beam pulse with 14 Hz repetition rate. Context: Muon Collider and Neutrino Factory. 1997. : Colin . Johnson argued . that the next step after the ACOL antiproton production target should be a mercury jet target. . [U. Miss. Workshop, Jan 1997; my introduction to Muon Collider . of a . Muon. Collider or Neutrino Factory. K. McDonald. Princeton U.. . (August . 29, 2014). NuFact’14. U Glasgow. The Target System Concept. A . M. uon. Collider needs . muon. beams of both signs.. Tony Gabriel. University of Tennessee. April 19, 2013. Acknowledgements: A very strong thank you to the staff of the SNS for providing many of the slides. Special thanks to Phil Ferguson, Bernie . Riemer. in Smart Grids. Jue. . Tian. 1,2. . . Rui. Tan. 2. . Xiaohong. Guan. 1,3. Ting Liu. 1,4. 1. Xi’an . Jiaotong. University, P.R. . China . 2. Nanyang . Technological University, . Singapore. Stuart Henderson. Fermilab. January 13, 2012. Accelerator Driven Systems. High-power, highly reliable proton accelerator. ~1 . GeV. beam energy. ~1 MW of beam power for demonstration. Tens of MW beam power for Industrial-Scale System. Flow, and Control. Jeff . Dagle. Pacific Northwest National . Laboratory. April . 2016. The "System Operations, Power Flow, and Control" focus area has . four. . main activities designed to support innovation and advancements in these technologies. Innovative. . Ideas. and New R&D. Session 5 Chair: Markus Nordberg. Thursday . February. 9, 2017. Status. of . Accelerator-. Driven. . Systems. . Research. and . Technology. . Development. Mark Wendel. Transformative Hadron . Beamlines. Workshop . 21-23 July . 2014 . Brookhaven National Laboratory. SNS – running since 2006. Mission is focused on neutron science. 1.4 MW . on target, 1 . ESS RF Group Unit Leader for Spoke . Power and RF Distribution. FREIA Group Unit Leader . 2. ESS: Superconducting 5 MW Linac. Frequency = 352.21 MHz. Number of spoke resonators = 28. Maximum power to beam = 240 kW.
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