Griffiths Introduction to Elementary Particles · Problem 3.8

Symmetries — David J. Griffiths

Physics — QFT · tensors-symmetric-antisymmetric

Problem

A second-rank tensor is called *symmetric* if it is unchanged when you switch the indices (sνμ=sμνs^{\nu\mu} = s^{\mu\nu}); it is called *antisymmetric* if it changes sign (aνμ=−aμνa^{\nu\mu} = -a^{\mu\nu}). (a) How many independent elements are there in a symmetric tensor? (Since s12=s21s^{12} = s^{21}, these would count as only *one* independent element.) (b) How many independent elements are there in an antisymmetric tensor? (c) If sμνs^{\mu\nu} is symmetric, show that sμνs_{\mu\nu} is also symmetric. If aμνa^{\mu\nu} is antisymmetric, show that aμνa_{\mu\nu} is antisymmetric. (d) If sμνs^{\mu\nu} is symmetric and aμνa^{\mu\nu} is antisymmetric, show that sμνaμν=0s_{\mu\nu}a^{\mu\nu} = 0. (e) Show that any second-rank tensor (tμνt^{\mu\nu}) can be written as the sum of an antisymmetric part (aμνa^{\mu\nu}) and a symmetric part (sμνs^{\mu\nu}): tμν=aμν+sμνt^{\mu\nu} = a^{\mu\nu} + s^{\mu\nu}. Construct sμνs^{\mu\nu} and aμνa^{\mu\nu} explicitly, given tμνt^{\mu\nu}.

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