What is the trace of the second-Rank tensor?

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In Lorentz group in QFT, why the trace of the symmetric second-Rank tensor [tex]S^{\mu\nu}[/tex] is defined as follows?
[tex]S=g_{\mu\nu}S^{\mu\nu}[/tex].
Is it just a definition or the genuine trace of the second-Rank tensor, and why?
 
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my opinion,The trace of [tex]S^{<br /> \mu\nu}[/tex] should be [tex]S^{<br /> 00}+S^{11}+S^{22}+S^{33}[/tex]
, i.e. the sum over the diagonal elements.
Now the metric tensor [tex]g_{<br /> \mu\nu}[/tex] is taken into account, the trace becomes
[tex]S^{<br /> 00}-S^{11}-S^{22}-S^{33}[/tex].
The problem is that I don't know why
 
This seems to be a common point of misunderstanding:

Matrices properly correspond to tensors with one index up and one index down.

The fact that books often just write the metric with all up or all down as a matrix is just confusing.
 
The basic definition of the trace of a matrix is simply the sum of its diagonal elements.
However, in order to make the trace invariant under a generalized rotation, the metric is included.
 
Thank Cristo, genneth, and clem.
You are correct, it is described in general relativity.