Abstract:We calculate event rates and demonstrate the observational feasibility of very high energy muons (1 TeV-1000 TeV) in a large mass underground detector operating as a pair-meter. This energy range corresponds to surface muon energies of ∼(5 TeV -5000 TeV) and primary cosmic ray energies of ∼ (50 TeV -5 ×10 4 TeV). Such measurements would significantly assist in an improved understanding of the prompt contribution to ν e , ν µ and µ fluxes in present and future ultra-high energy neutrino detectors. In addition, … Show more
“…The differential pair production cross section can be calculated by taking some approximation of relative energy transfer and threshold energy is given by [4,5,12,13].…”
Section: Pair Production Cross Sectionmentioning
confidence: 99%
“…Uncontrollable fluxes have been produced, which is the major disadvantage of cosmic rays. The study of cosmic ray spectrum enhances our knowledge about both astrophysics and particle physics [1][2][3][4][5], and also gives a signature of the existence of the new particles and some physics behind it, which was confirmed by some accelerator experiments. These experiments provide us to understand the structure of matter and interaction between its building blocks.…”
“…The differential pair production cross section can be calculated by taking some approximation of relative energy transfer and threshold energy is given by [4,5,12,13].…”
Section: Pair Production Cross Sectionmentioning
confidence: 99%
“…Uncontrollable fluxes have been produced, which is the major disadvantage of cosmic rays. The study of cosmic ray spectrum enhances our knowledge about both astrophysics and particle physics [1][2][3][4][5], and also gives a signature of the existence of the new particles and some physics behind it, which was confirmed by some accelerator experiments. These experiments provide us to understand the structure of matter and interaction between its building blocks.…”
“…Its charge identification capability gives it an edge for hierarchy determination and CP, CPT studies. The high Z medium also allows a studies of very high energy cosmic-ray (CR) muons using the pair-meter method, allowing a probe of the CR flux at energies around the "knee" and beyond [20].…”
Abstract. We discuss the physics capabilities of basic types of future atmospheric detectors being considered at present, with their strengths and limitations, and compare them with those of long-baseline (LBL) experiments. We also argue that recent studies signal the importance of synergistically combining complementary features of both these classes of experiments in order to accrue maximum benefit towards furthering our goal of building a complete picture of neutrino properties and parameters.
“…1 Number of the muon events per steradian per year expected at INO detector near direction cos θ = 0.7 is presented in Table III (see details in Ref. [12]). Last three columns in Table III represent the ratio of the conventional muon flux to the prompt muon one due to three charm production models, GGV01, GGV05 and QGSM, respectively.…”
Section: Expected Muon Flux At the Depth Of Pushep Sitementioning
We calculate the zenith-angle dependence of conventional and prompt high-energy muon fluxes at India-Based Neutrino Observatory (INO) depth. This study demonstrates a possibility to discriminate models of the charm hadroproduction including the low-x QCD behaviour of hadronic cross-sections relevant at very high energies.
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