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Neutrino Interactions
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GEANT4
Geant4 is a toolkit for the simulation of the passage of particles through matter. Its areas of application include high energy, nuclear and accelerator physics, as well as studies in medical and space science. The two main reference papers for Geant4 are published in Nuclear Instruments and Methods in Physics Research A 506 (2003) 250-303,…
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Muon Tomography (cont)
It is the case of an article on Muon Tomography, titled New Muon Detector Could Find Hidden Nukes. The article appeared a few days ago on Wired. It is centered on Lisa Grossman’s interview to Marcus Hohlmann, a colleague from the Florida Institute of Technology. In a nutshell, the article explains how muon particles from…
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Muon Detection
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Neutrino Events in IceCube Strings
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Muon Tomography
The same nuclear reaction described above (i.e. hadron-hadron impacts to produce pion beams, which then quickly decay to muon beams over short distances) is used by particle physicists to produce muon beams, such as the beam used for the muon g − 2 experiment Can you create relationships of Pierre Auger cosmic particle collision’s energy…
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G-2 Experiment
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The Bolshoi simulation
A virtual world? The more complex the data base the more accurate one’s simulation is achieved. The point is though that you have to capture scientific processes through calorimeter examinations just as you do in the LHC. So these backdrops are processes in identifying particle examinations as they approach earth or are produced on earth.…
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first tau-neutrino “appearing” out of several billion of billions muon neutrinos
Layout of the CNGS beam line. The OPERA neutrino experiment [1] at the underground Gran Sasso Laboratory (LNGS) was designed to perform the first detection of neutrino oscillations in direct appearance mode in the νμ→ντ channel, the signature being the identification of the τ− lepton created by its charged current (CC) interaction [2]. See: Measurement…
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Energy Boost From Shock Front
Main Components of CNGS A 400 GeV/c proton beam is extracted from the SPS in 10.5 microsecond short pulses of 2.4×1013 protons per pulse. The proton beam is transported through the transfer line TT41 to the CNGS target T40. The target consists of a series of graphite rods, which are cooled by a recirculated helium…
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Seeing Underlying Structures
There is gap between, “Proton Collision ->Decay to Muons and Muon Neutrinos ->Tau Neutrino ->[gap] tau lepton may travel some tens of microns before decaying back into neutrino and charged tracks.” Use the case of Relativistic Muons? An analysis of four Fermi-detected gamma-ray bursts (GRBs) is given that sets upper limits on the energy dependence…
