Abstract
At very high energies, pair production formation (γ + N → e+e-) exhibits a variety of intriguing properties. Analytically and quantitatively, the formation of Electron-Positron pairs in the Electro-Magnetic field of light nuclei has been calculated. In Ultra-Relativistic (UR) areas of incident photon energy, applying the resulting formulas to the energy distribution of the (e-, e+) operation. When we compare the results, we can observe that the Magnetic field of the target nucleus is more efficacious than the Electric field of the nucleus in the (e-, e+) operation. Furthermore, we can show that in Pair Production operation, the Differential Cross Section (DCS) owing to the target nucleus’s Electric Quadrupole (EQ) and Magnetic Octupole (MO) are bigger than the Differential Cross Section (DCS) attributable to the target nucleus’s Electric Charge (EC) distribution and Magnetic Dipole (MD).
Highlights
There are numerous particles in nature, each of which is accompanied by its field as it moves
When we compare the results, we can observe that the Magnetic field of the target nucleus is more efficacious than the Electric field of the nucleus
( ) Magnetic dM Differential Cross Section(DCS) for the e−, e+ using formulas for the energy distribution are obtained for the nucleus N174 and for different values of incident photon energies εγ = (2 GeV, 4 GeV, 6 GeV), where
Summary
There are numerous particles in nature, each of which is accompanied by its field as it moves. They are split into Pheromones and Bosons. The Electron, Muon, and Tau are three charged Leptons, and neutrinos are three neutral Leptons [1]. Both the Electron and the Positron will be studied. The Electron was discovered in 1897 by J.J. The Electron was discovered in 1897 by J.J Thomson, and it is still the prototypical elementary particle. Anderson saw Pair Production for the first time in 1932 when he exploited the operation to find the Positron [2]. Bethe and Heitler’s work shaped our present theoretical understanding of Pair
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