Abstract
The Eliashberg equation is solved in both frequency and momentum variables to obtain the superconducting transition temperature Tc in the multivalley electron gas without phonons. Both the one-particle Green’s function and irreducible two-electron interaction are evaluated in the random-phase approximation which provides exact results in the limit of large valley degeneracy gv and is known to give sufficiently accurate ones even for gv as small as 3 or 4. Among s-, p-, and d-waves, the s-wave pairing is most stable for gv≥2 with a fairly high Tc. For gv>>1, our solution is reduced to “bipolaronic superconductivity”. We discuss implications of the present results to the exotic superconductors with relatively low carrier concentration.