Suppose the metric g with respect to coordinate Xa=(xi,ym) has the form g=hij(y)dxidxj+kmn(y)dymdyn, and Rxixi=Rx1x1+....+Rxnxn=0, then the square root of det of hij is harmonic in the metric kmn, ie,
DmDm√|h|=0
where D is the connection of kmn.
Motivation:
in the page 166 Wald says: the equation (7.1.20) yields (7.1.21),
here the two equations are,
0=Rtt+Rϕϕ=(∇at)Rabξb+(∇aϕ)Rabψb
and,
DaDaρ=0
where the metric ansatz is,
ds2=−V(ρ,z)(dt−w(ρ,z)dϕ)2+V−1ρ2dϕ2+Ω(ρ,z)2(dρ2+Λ(ρ,z)dz2)
it can be checked by some direct calculation and the two are equal to √Λ,zρΩ2√Λ, up to a factor, and certainly it holds not accidentally, which motivites the foregoing results.
Question:
Can it be derived more geometrically using something like foliation?
And what is the intuitive picture?
Here is a proof I got. It's direct, but with less intuition.
Proof:
There are n Killing vector fields (Ai)a wrt xi for g is independent of xi, which leads to, (notice: no summation here, and xi is a scalar function)
Rxixi=∇axi⋅∇c∇c(Ai)a
for a antisymmetric (2,0) tensor, the covariant derivative is,
∇cAca=1√|g|∂(Aca√|g|)∂Xc
applying to (???),
∇c∇c(Ai)a=1√|g|∂(∇m(Ai)a√|g|)∂ym
we need to calculate ∇m(Ai)a,
∇m(Ai)a=gmbΓa bd(Ai)d=kmnΓa nxi
and,
Γa nxi=gac(gcn,xi+gcxi,n−gnxi,c)=gacgcxi,n=haihixi,n
(notice: the non-vanishing components of the connection are Γx xy, Γy xx, Γy yy.)
substitute it into (???),
∇c∇c(Ai)a=1√|g|∂(kmnhaihixi,n√|g|)∂ym
∇axi⋅ is to pick out the xi term of the index a, thus summing up (???) over xi−s, the vanishment of partial trace of Ricci tensor is equivalent to,
1√|g|∂(kmnhjihij,n√|g|)∂ym=0
while for DmDm√|h|=1√|k|∂∂ym(kmn√|k|∂∂yn(√|h|)), the last ingrediant left is,
∂∂ymh=hhij∂∂ymhij