Carminati–McLenaghan invariants

In general relativity, the Carminati–McLenaghan invariants or CM scalars are a set of 16 scalar curvature invariants for the Riemann tensor. This set is usually supplemented with at least two additional invariants.

Mathematical definition

The CM invariants consist of 6 real scalars plus 5 complex scalars, making a total of 16 invariants. They are defined in terms of the Weyl tensor $C_{{abcd}}$ and its right (or left) dual ${{}^{\star }C}_{ijkl}=(1/2)\epsilon _{klmn}C_{ij}{}^{mn}$ , the Ricci tensor $R_{ab}$ , and the trace-free Ricci tensor

S_{ab}=R_{ab}-{\frac {1}{4}}\,R\,g_{ab}

In the following, it may be helpful to note that if we regard ${S^{a}}_{b}$ as a matrix, then ${S^{a}}_{m}\,{S^{m}}_{b}$ is the square of this matrix, so the trace of the square is ${S^{a}}_{b}\,{S^{b}}_{a}$ , and so forth.

The real CM scalars are:

$R={R^{m}}_{m}$ (the trace of the Ricci tensor)
$R_{1}={\frac {1}{4}}\,{S^{a}}_{b}\,{S^{b}}_{a}$
$R_{2}=-{\frac {1}{8}}\,{S^{a}}_{b}\,{S^{b}}_{c}\,{S^{c}}_{a}$
$R_{3}={\frac {1}{16}}\,{S^{a}}_{b}\,{S^{b}}_{c}\,{S^{c}}_{d}\,{S^{d}}_{a}$
$M_{3}={\frac {1}{16}}\,S^{bc}\,S_{ef}\left(C_{abcd}\,C^{aefd}+{{}^{\star }C}_{abcd}\,{{}^{\star }C}^{aefd}\right)$
$M_{4}=-{\frac {1}{32}}\,S^{ag}\,S^{ef}\,{S^{c}}_{d}\,\left({C_{ac}}^{db}\,C_{befg}+{{{}^{\star }C}_{ac}}^{db}\,{{}^{\star }C}_{befg}\right)$

The complex CM scalars are:

$W_{1}={\frac {1}{8}}\,\left(C_{abcd}+i\,{{}^{\star }C}_{abcd}\right)\,C^{abcd}$
$W_{2}=-{\frac {1}{16}}\,\left({C_{ab}}^{cd}+i\,{{{}^{\star }C}_{ab}}^{cd}\right)\,{C_{cd}}^{ef}\,{C_{ef}}^{ab}$
$M_{1}={\frac {1}{8}}\,S^{ab}\,S^{cd}\,\left(C_{acdb}+i\,{{}^{\star }C}_{acdb}\right)$
$M_{2}={\frac {1}{16}}\,S^{bc}\,S_{ef}\,\left(C_{abcd}\,C^{aefd}-{{}^{\star }C}_{acdb}\,{{}^{\star }C}^{aefd}\right)+{\frac {1}{8}}\,i\,S^{bc}\,S_{ef}\,{{}^{\star }C}_{abcd}\,C^{aefd}$
$M_{5}={\frac {1}{32}}\,S^{cd}\,S^{ef}\,\left(C^{aghb}+i\,{{}^{\star }C}^{aghb}\right)\,\left(C_{acdb}\,C_{gefh}+{{}^{\star }C}_{acdb}\,{{}^{\star }C}_{gefh}\right)$

The CM scalars have the following degrees:

$R$ is linear,
$R_{1},\,W_{1}$ are quadratic,
$R_{2},\,W_{2},\,M_{1}$ are cubic,
$R_{3},\,M_{2},\,M_{3}$ are quartic,
$M_{4},\,M_{5}$ are quintic.

They can all be expressed directly in terms of the Ricci spinors and Weyl spinors, using Newman–Penrose formalism; see the link below.

Complete sets of invariants

In the case of spherically symmetric spacetimes or planar symmetric spacetimes, it is known that

R,\,R_{1},\,R_{2},\,R_{3},\,\Re (W_{1}),\,\Re (M_{1}),\,\Re (M_{2})

{\frac {1}{32}}\,S^{cd}\,S^{ef}\,C^{aghb}\,C_{acdb}\,C_{gefh}

comprise a complete set of invariants for the Riemann tensor. In the case of vacuum solutions, electrovacuum solutions and perfect fluid solutions, the CM scalars comprise a complete set. Additional invariants may be required for more general spacetimes; determining the exact number (and possible syzygies among the various invariants) is an open problem.

References

Carminati J.; McLenaghan, R. G. (1991). "Algebraic invariants of the Riemann tensor in a four-dimensional Lorentzian space". J. Math. Phys. 32: 3135–3140. Bibcode:1991JMP....32.3135C. doi:10.1063/1.529470.

External links

The GRTensor II website includes a manual with definitions and discussions of the CM scalars.
Implementation in the Maxima computer algebra system

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Carminati–McLenaghan invariants

Mathematical definition

Complete sets of invariants

See also

References

External links