KarateMan
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I have questions about the infinitesimal Lorentz transformation. but specifically about index manipulations.
\Lambda^{\mu}_{}_{\nu}=\delta^{\mu}_{\nu}+\delta\omega^{\mu}_{}_{\nu}
where \delta\omega^{\mu}_{}_{\nu} << 1
as found in many textbooks, we substitute this into
g_{\mu\nu}\Lambda^{\mu}_{}_{\alpha}\Lambda^{\nu}_{}_{\beta}=g_{\alpha\beta}
and do the tedious(?) algebra...
g_{\mu\nu}(\delta^{\mu}_{\alpha}\delta^{\nu}_{\beta}+\delta^{\mu}_{\alpha}\delta\omega^{\nu}_{}_{\beta}+\delta\omega^{\mu}_{}_{\alpha}\delta^{\nu}_{\beta}+\delta\omega^{\mu}_{}_{\alpha}\delta\omega^{\nu}_{}_{\beta})=g_{\alpha\beta}
and the last term is negligible because it too small (correct me if wrong!)
my question is the second and third terms. they are supposed to become...
...\delta\omega_{\mu\nu}+\delta\omega_{\nu\mu}...
why is that? because \delta^{\mu}_{\nu}'s are identity matrices, so whichever order we multiply, we get the same result.
and I look up some articles and found something about "abstract index notation". but is this the one?
\Lambda^{\mu}_{}_{\nu}=\delta^{\mu}_{\nu}+\delta\omega^{\mu}_{}_{\nu}
where \delta\omega^{\mu}_{}_{\nu} << 1
as found in many textbooks, we substitute this into
g_{\mu\nu}\Lambda^{\mu}_{}_{\alpha}\Lambda^{\nu}_{}_{\beta}=g_{\alpha\beta}
and do the tedious(?) algebra...
g_{\mu\nu}(\delta^{\mu}_{\alpha}\delta^{\nu}_{\beta}+\delta^{\mu}_{\alpha}\delta\omega^{\nu}_{}_{\beta}+\delta\omega^{\mu}_{}_{\alpha}\delta^{\nu}_{\beta}+\delta\omega^{\mu}_{}_{\alpha}\delta\omega^{\nu}_{}_{\beta})=g_{\alpha\beta}
and the last term is negligible because it too small (correct me if wrong!)
my question is the second and third terms. they are supposed to become...
...\delta\omega_{\mu\nu}+\delta\omega_{\nu\mu}...
why is that? because \delta^{\mu}_{\nu}'s are identity matrices, so whichever order we multiply, we get the same result.
and I look up some articles and found something about "abstract index notation". but is this the one?