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The existence of bound states of the system in a magnetic field is studied using the variational method. It is shown that for $B \gtrsim 0.13,{\rm a.u.}(\al,e,e)^-$ atomic ion. Its ground state is a spin-doublet at $0.74, {\rm a.u.} \gtrsim B \gtrsim 0.13, {\rm a.u.}^4(-3)^{+}$ for larger magnetic fields. For $0.8, {\rm a.u.} \gtrsim B \gtrsim 0.7, {\rm a.u.}^-^2(-1)^{+}^4(-3)^{+}$.

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