MG13 - Talk detail |
Participant |
Xue, She-Sheng | |||||||
Institution |
ICRANet, Phys. Department, University of Rome, La Sapienza - ICRANet, P.zza della Repubblica 10 - Pescara - I--65122 Pescara - Italy | |||||||
Session |
SF3 |
Accepted |
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Order |
Time |
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Talk |
Oral abstract |
Title |
Electron and positron pair production in gravitational collapse | |||||
Co-authors | ||||||||
Abstract |
Neutral stellar core at or over nuclear densities is described by positive charged baryon core and negative charged electron fluid since they possess different masses and interactions. Based on a simplified model of gravitationally collapsing or pulsating baryon core, we approximately integrate the Einstein-Maxwell equations and the equations for the number and energy-momentum conservation of complete degenerate electron fluid. We show possible electric processes that lead to the production of electron-positron pairs in the boundary of baryon core, and calculate electron-positron pair energy. This might be important for understanding the energy source of gamma-ray bursts. |
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Session |
SN1 |
Accepted |
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Order |
Time |
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Talk |
Oral abstract |
Title |
Neutrinos decoupled from $\beta$-processes and supernova explosion | |||||
Co-authors | ||||||||
Abstract |
Based on the gravitational collapse time-scale is larger than the weak interaction time-scale at core densities $\rho > 10^{11} {\rm gr}/ {\rm cm}^{3}$, we approximately use the $\beta$-equilibrium condition and particle number conservations to calculate the number and energy densities of neutrino sphere in the process of gravitational core collapse towards the formation of a proto-neutron star. We find that at core densities $\rho_{\rm dec} > 10^{12} {\rm gr}/ {\rm cm}^{3}$, the $\beta$-equilibrium condition cannot be satisfied consistently with charge, baryon and lepton number conservations, leading to the presence of excess neutrinos decoupling from the $\beta$-equilibrium. These excess neutrinos interact with nucleons and electrons via the neutral current channel only and their diffusion time is about $10^{-2}\,$ sec. The excess neutrino flux could play an important role in an Supernova explosion, provided the fraction of excess neutrinos over all neutrinos is at least one present. |
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