  This work continues \cite{bib1} where the construction of Hamiltonian $H$ for
the system of three quantum particles is considered. Namely the system consists
of two fermions with mass $1$ and another particle with mass $m>0$. In the
present paper, like in \cite{bib1}, we study the part $T_{l=1}$ of auxilliary
operator $T = \oplus_{l=0}^{\infty} T_l$ involving the construction of the
resolvent for the operator $H$. In this work together with the previous one two
constants $0<m_1<m_0<\infty$ were found such that: 1) for $m>m_0$ the operator
$T_{l=1}$ is selfadjoint but for $m \leqslant m_0$ it has the deficiency
indexes $(1,1)$; 2) for $m_1<m<m_0$ any selfadjoint extension of $T_{l=1}$ is
semibounded below; 3) for $0<m<m_1$ any selfadjoint extension of $T_{l=1}$ has
the sequence of eigenvalues $\{\lambda_n <0, n> n_0\}$ with the asymptotics \[
\lambda_n = \lambda_0 e^{\delta n} + O(1),\quad n\to\infty, \] where $\lambda_0
<0$, $\delta >0$, $n_0>0$ and there is'nt other spectrum on the interval
$\lambda < \lambda_{n_0}$.
