  The second (unphysical) critical charge in the 3-body quantum Coulomb system
of a nucleus of positive charge $Z$ and mass $m_p$, and two electrons,
predicted by F~Stillinger has been calculated to be equal to $Z_{B}^{\infty}\
=\ 0.904854$ and $Z_{B}^{m_p}\ =\ 0.905138$ for infinite and finite (proton)
mass $m_p$, respectively. It is shown that in both cases, the ground state
energy $E(Z)$ (analytically continued beyond the first critical charge $Z_c$,
for which the ionization energy vanishes, to $Re Z < Z_c$) has a square-root
branch point with exponent 3/2 at $Z=Z_B$ in the complex $Z$-plane. Based on
analytic continuation, the second, excited, spin-singlet bound state of
negative hydrogen ion H${}^-$ is predicted to be at -0.51554 a.u. (-0.51531
a.u. for the finite proton mass $m_p$). The first critical charge $Z_c$ is
found accurately for a finite proton mass $m_p$ in the Lagrange mesh method,
$Z^{m_p}_{c}\ =\ 0.911\, 069\, 724\, 655$.
