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The Q-value of the continuum-state β - decays we calculate as Qβc-=(Δm-Δd)Ö+ (εTF(Z+1)-εTF(Z))Ö= (-22304+23835)+(-521.826+506.560) keV=1515.734ÖkeV for Hg20580+Ö→ Tl20581++e-Ö+ ν~e and Qβc-=(Δm-Δd)Ö+ (εTF(Z+1)-εTF(Z))Ö= (-21044+22467)+(-537.355+521.826) keV=1407.471ÖkeV for Tl20781+Ö→ Pb20782+++e-+ν~e, where εTF(Z)=-Ö14.33ÖZ2.39ÖeV is the binding energy of electrons in the atom with Z electrons.
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The Q-value of the continuum-state β - decays we calculate as Qβc-=(Δm-Δd)Ö+ (εTF(Z+1)-εTF(Z))Ö= (-22304+23835)+(-521.826+506.560) keV=1515.734ÖkeV for Hg20580+Ö→ Tl20581++e-Ö+ ν~e and Qβc-=(Δm-Δd)Ö+ (εTF(Z+1)-εTF(Z))Ö= (-21044+22467)+(-537.355+521.826) keV=1407.471ÖkeV for Tl20781+Ö→ Pb20782+++e-+ν~e, where εTF(Z)=-Ö14.33ÖZ2.39ÖeV is the binding energy of electrons in the atom with Z electrons.
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The Q-value of the bound-state β - decay is defined by Qns=Qβc-+me(1-n+γn2+2(n-1)γ).
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The Q-value of the bound-state β - decay is defined by Qns=Qβc-+me(1-n+γn2+2(n-1)γ).
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