Supercritically charged objects and electron-positron pair creation

preprint2020arXivOpen access

Abstract

We investigate the stability and e+e−e^+e^- pair creation of supercritically charged superheavy nuclei, ududQM nuggets, strangelets, and strangeon nuggets based on Thomas-Fermi approximation. The model parameters are fixed by reproducing their masses and charge properties reported in earlier publications. It is found that ududQM nuggets, strangelets, and strangeon nuggets may be more stable than 56{}^{56}Fe at A≳315A\gtrsim 315, 5×1045\times10^4, and 1.2×1081.2\times10^8, respectively. For those stable against neutron emission, the most massive superheavy element has a baryon number ∼\sim965, while ududQM nuggets, strangelets, and strangeon nuggets need to have baryon numbers larger than 3939, 433, and 2.7×1052.7\times10^5. The e+e−e^+e^- pair creation will inevitably start for superheavy nuclei with charge numbers Z≥177Z\geq177, ududQM nuggets with Z≥163Z\geq163, strangelets with Z≥192Z\geq 192, and strangeon nuggets with Z≥212Z\geq 212. A universal relation Q/Re=(me−μˉe)/αQ/R_e = \left(m_e - \barμ_e\right)/α is obtained at a given electron chemical potential μˉe\barμ_e, where QQ is the total charge and ReR_e the radius of electron cloud. This predicts the maximum charge number by taking μˉe=−me\barμ_e=-m_e. For supercritically charged objects with μˉe<−me\barμ_e<-m_e, the decay rate for e+e−e^+e^- pair production is estimated based on the JWKB approximation. It is found that most positrons are emitted at t≲10−15t\lesssim 10^{-15} s, while a long lasting positron emission is observed for large objects with R≳1000R\gtrsim 1000 fm. The emission and annihilation of positrons from supercritically charged objects may be partially responsible for the short γγ-ray burst during the merger of binary compact stars, the 511 keV continuum emission, as well as the narrow faint emission lines in X-ray spectra from galaxies and galaxy clusters.

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