There might be some extra bits feel free to remove
ClearAll["Global`*"];
n = 4;
coord = {t, x, y, z};
(*For raising/lowering latin indices like a, b, ...*)
\[Eta] = {{-1, 0, 0, 0}, {0, 1, 0, 0}, {0, 0, 1, 0}, {0, 0, 0, 1}};
\[Eta] // MatrixForm;
inveta = Inverse[\[Eta]];
inveta // MatrixForm;
(*"e-Metric";*)
e = {{\[ScriptCapitalN][t], 0, 0, 0}, {0, \[ScriptA][t], 0, 0}, {0,
0, \[ScriptA][t], 0}, {0, 0, 0, \[ScriptA][t]}};
\[ScriptCapitalN][t] = -1;
e // MatrixForm;
dete = Det[e];
(*Inverse e-Metric*)
inve = Inverse[e];
inve // MatrixForm;
detinve = Det[inve];
g := g = Simplify[Table[
ParallelSum[ \[Eta][[a, b]]*e[[a, \[Mu]]]*e[[b, \[Nu]]]
, {a, 1, n}, {b, 1, n}]
, {\[Mu], 1, n}, {\[Nu], 1, n}]]
g // MatrixForm;
(*g is used to LOWER indices for Greek indices \[Mu], \[Nu]*)
invg = Inverse[g];
invg // MatrixForm;
(*invg is used to RAISE indices for Greek indices \[Mu], \[Nu]*)
(* In the form \[CapitalGamma]^{x}_{xx}*)
affine := affine = Simplify[Table[(1/2)*Sum[(invg[[i, s]])*
(D[g[[s, j]], coord[[k]] ] +
D[g[[s, k]], coord[[j]] ] - D[g[[j, k]], coord[[s]] ]), {s,
1, n}],
{i, 1, n}, {j, 1, n}, {k, 1, n}] ];
listaffine :=
Table[If[UnsameQ[affine[[i, j, k]],
0], {ToString[\[CapitalGamma][i, j, k]],
affine[[i, j, k]]}] , {i, 1, n}, {j, 1, n}, {k, 1, j}];
TableForm[Partition[DeleteCases[Flatten[listaffine], Null], 2],
TableSpacing -> {2, 2}];
(* In the form R^{x}_{xxx} *)
riemann := riemann = Simplify[Table[
D[affine[[i, j, l]], coord[[k]] ] -
D[affine[[i, j, k]], coord[[l]] ] +
Sum[
affine[[s, j, l]] affine[[i, k, s]] -
affine[[s, j, k]] affine[[i, l, s]],
{s, 1, n}],
{i, 1, n}, {j, 1, n}, {k, 1, n}, {l, 1, n}] ];
listriemann :=
Table[If[UnsameQ[riemann[[i, j, k, l]], 0], {ToString[R[i, j, k, l]],
riemann[[i, j, k, l]]}] , {i, 1, n}, {j, 1, n}, {k, 1, n}, {l, 1,
k - 1}]
TableForm[Partition[DeleteCases[Flatten[listriemann], Null], 2],
TableSpacing -> {2, 2}];
(* In the form R_{xxxx} *)
riemann1 := riemann1 = Simplify[Table[
Sum[
g[[\[Mu], \[Mu]1]]*riemann[[\[Mu]1, \[Nu], \[Rho], \[Sigma]]]
, {\[Mu]1, 1, n}]
, {\[Mu], 1, n}, {\[Nu], 1, n}, {\[Rho], 1, n}, {\[Sigma], 1, n}]]
listriemann1 :=
Table[If[UnsameQ[riemann1[[\[Mu], \[Nu], \[Rho], \[Sigma]]],
0], {ToString[R1[\[Mu], \[Nu], \[Rho], \[Sigma]]],
riemann1[[\[Mu], \[Nu], \[Rho], \[Sigma]]]}] , {\[Mu], 1,
n}, {\[Nu], 1, n}, {\[Rho], 1, n}, {\[Sigma], 1, \[Rho] - 1}];
TableForm[Partition[DeleteCases[Flatten[listriemann1], Null], 2],
TableSpacing -> {2, 2}];
(* In the form R^{xxxx} *)
riemann2 := riemann2 = Simplify[Table[
Sum[
Sum[
Sum[
invg[[\[Nu]1, \[Nu]]]*invg[[\[Rho]1, \[Rho]]]*
invg[[\[Sigma]1, \[Sigma]]]*
riemann[[\[Mu], \[Nu]1, \[Rho]1, \[Sigma]1]]
, {\[Nu]1, 1, n}]
, {\[Rho]1, 1, n}]
, {\[Sigma]1, 1, n}]
, {\[Mu], 1, n}, {\[Nu], 1, n}, {\[Rho], 1, n}, {\[Sigma], 1, n}]]
listriemann2 :=
Table[If[UnsameQ[riemann2[[\[Mu], \[Nu], \[Rho], \[Sigma]]],
0], {ToString[R2[\[Mu], \[Nu], \[Rho], \[Sigma]]],
riemann2[[\[Mu], \[Nu], \[Rho], \[Sigma]]]}] , {\[Mu], 1,
n}, {\[Nu], 1, n}, {\[Rho], 1, n}, {\[Sigma], 1, \[Rho] - 1}];
TableForm[Partition[DeleteCases[Flatten[listriemann2], Null], 2],
TableSpacing -> {2, 2}];
KretschmannScalar = Simplify[
Sum[riemann1[[a, b, c, d]]*riemann2[[a, b, c, d]], {a, 1, n}, {b, 1,
n}, {c, 1, n}, {d, 1, n}]]
With that input metric I got this answer:
$\frac{12 \left(\mathit{a}(t)^2 \mathit{a}''(t)^2+\mathit{a}'(t)^4\right)}{\mathit{a}(t)^4}$