Beam dump system design for 100 MeV high intensity proton cyclotron

2013 ◽  
Vol 25 (4) ◽  
pp. 977-980
Author(s):  
贾先禄 Jia Xianlu ◽  
张天爵 Zhang Tianjue ◽  
王峰 Wang Feng ◽  
吕银龙 Lü Yinlong ◽  
魏素敏 Wei Sumin ◽  
...  
2021 ◽  
Vol 81 (8) ◽  
Author(s):  
Stefan Ghinescu ◽  
Babette Döbrich ◽  
Elisa Minucci ◽  
Tommaso Spadaro

AbstractThe search for feebly-interacting new-physics particles in the MeV-GeV mass range often involves high-intensity beams dumped into thick heavy targets. The challenge of evaluating the expected backgrounds for these searches from first principles is limited by the CPU time needed to generate the shower induced by the primary beam. We present a Monte Carlo biasing method allowing a three orders of magnitude increase in the efficiency for the simulation of the muon production in a 400 GeV/c proton beam-dump setup. At the same time, this biasing method is maintaining nearly every feature of a simulation from first principles.


1981 ◽  
Vol 28 (3) ◽  
pp. 2774-2776 ◽  
Author(s):  
J. Kidd ◽  
N. Mokhov ◽  
T. Murphy ◽  
M. Palmer ◽  
T. Toohig ◽  
...  
Keyword(s):  

Author(s):  
Sumin Wei ◽  
Yinlong Lv ◽  
Tianjue Zhang ◽  
Zhenghe Zhou ◽  
Zhenguo Li ◽  
...  

Author(s):  
George Christov ◽  
Bolivar J. Lloyd

A new high intensity grid cap has been designed for the RCA-EMU-3 electron microscope. Various parameters of the new grid cap were investigated to determine its characteristics. The increase in illumination produced provides ease of focusing on the fluorescent screen at magnifications from 1500 to 50,000 times using an accelerating voltage of 50 KV.The EMU-3 type electron gun assembly consists of a V-shaped tungsten filament for a cathode with a thin metal threaded cathode shield and an anode with a central aperture to permit the beam to course the length of the column. The cathode shield is negatively biased at a potential of several hundred volts with respect to the filament. The electron beam is formed by electrons emitted from the tip of the filament which pass through an aperture of 0.1 inch diameter in the cap and then it is accelerated by the negative high voltage through a 0.625 inch diameter aperture in the anode which is at ground potential.


2006 ◽  
Vol 175 (4S) ◽  
pp. 86-86
Author(s):  
Makoto Sumitomo ◽  
Junichi Asakuma ◽  
Yasumasa Hanawa ◽  
Kazuhiko Nagakura ◽  
Masamichi Hayakawa

2005 ◽  
Vol 173 (4S) ◽  
pp. 379-380
Author(s):  
James E. Kennedy ◽  
Rowland O. Illing ◽  
Feng Wu ◽  
Gail R. ter Haar ◽  
Rachel R. Phillips ◽  
...  

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