Three two-component fermions with contact interactions: correct formulation and energy spectrum

Properties of two identical particles of mass $m$ and a distinct particle of mass $m_1$ in the universal low-energy limit of zero-range two-body interaction are studied in different sectors of total angular momentum $L$ and parity $P$. For the unambiguous formulation of the problem in the interval $\mu_r(L^P) < m/m_1 \le \mu_c(L^P)$($\mu_r(1^-) \approx 8.619$and$\mu_c(1^-) \approx 13.607$,$\mu_r(2^+) \approx 32.948$and$\mu_c(2^+) \approx 38.630$,~etc.) in each $L^P$ sector an additional parameter $b$ determining the wave function near the triple-collision point is introduced; thus, a one-parameter family of self-adjoint Hamiltonians is defined. Within the framework of this formulation, dependence of the bound-state energies on $m\mathrm{/}{m}_1$ and $b$ in the sector of angular momentum and parity $L^P$ is calculated for $L\le 5$ and analysed with the aid of a simple model. A number of the bound states for each $L^P$ sector is analysed and presented in the form of `phase diagrams’ in the plane of two parameters $m\mathrm{/}{m}_1$ and $b$.