Abstract
For a uniform electron gas of density n=n+n=3/4πrs3ks6/192 and spin polarization ζ=(n-n)/n, we study the Fourier transform ρ¯c(k,rs,ζ) of the correlation hole, as well as the correlation energy ɛc(rs,ζ)=F0dk ρ¯c/π. In the high-density (rs→0) limit, we find a simple scaling relation ksρ¯cg2f(z,ζ), where z=k/gks, g=[(1+ζ)2/3+(1-ζ)2/3]/2, and f(z,1)=f(z,0). The function f(z,ζ) is only weakly ζ dependent, and its small-z expansion -3z/π2+4 √3 z2/π2+... is also the exact small-wave-vector (k→0) expansion for any rs or ζ. Motivated by these considerations, and by a discussion of the large-wave-vector and low-density limits, we present two Padé representations for ρ¯c at any k, rs, or ζ, one within and one beyond the random-phase approximation (RPA). We also show that ρ¯ cRPA obeys a generalization of Misawa’s spin-scaling relation for