The second-quantized form of the Laughlin states for the fractional qu
antum Hall effect is discussed by decomposing the Laughlin wavefunctio
ns into the N-particle Slater basis. A general formula is given for th
e expansion coefficients in terms of the characters of the symmetric g
roup, and the expansion coefficients are shown to possess numerous int
eresting symmetries. For expectation values of the density operator it
is possible to identify individual dominant Slater states of the corr
ect uniform bulk density and filling fraction in the physically releva
nt N --> infinity limit.