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  Persuing geometrical meaning of Wald (7.1.20) to (7.2.21)

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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)(dtw(ρ,z)dϕ)2+V1ρ2dϕ2+Ω(ρ,z)2(dρ2+Λ(ρ,z)dz2)

it can be checked by some direct calculation and the two are equal to Λ,zρΩ2Λ, 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=axicc(Ai)a

for a antisymmetric (2,0) tensor, the covariant derivative is,

cAca=1|g|(Aca|g|)Xc

applying to (???),

cc(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,ngnxi,c)=gacgcxi,n=haihixi,n

(notice: the non-vanishing components of the connection are Γx xy, Γy xx, Γy yy.)

substitute it into (???),

cc(Ai)a=1|g|(kmnhaihixi,n|g|)ym

axi is to pick out the xi term of the index a, thus summing up (???) over xis, 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=hhijymhij

asked Jan 25, 2016 in Theoretical Physics by Reiko Liu (15 points) [ revision history ]
edited Jan 25, 2016 by Reiko Liu

It is the first time I ask question and I'm not sure it's appropriate to put it here, so feel free to give suggestions or vote.

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