Cooper pairing in two dimensions is analyzed with a set of renormalized equ
ations to determine its binding energy for any fermion number density and a
ll coupling assuming a,generic pairwise residual interfermion interaction.
Also considered are Cooper pairs (CP's) with nonzero center-of-mass momentu
m (CMM) and their binding energy is expanded analytically in powers of the
CMM up to quadratic terms. A Fermi-sea-dependent linear term in the CMM dom
inates the pair excitation energy in weak coupling (also called the BCS reg
ime) while the more familiar quadratic term prevails in strong coupling (th
e Bose regime). The crossover, though strictly unrelated to BCS theory per
se, is studied numerically as it is expected to play a central role in a mo
del of superconductivity as a Bose-Einstein condensation of CPs where the t
ransition temperature vanishes for all dimensionality d less than or equal
to 2 for quadratic dispersion, but is nonzero for all d greater than or equ
al to 1 for linear dispersion.