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=sμν); it is called *antisymmetric* if it changes sign (aνμ=−aμν).
(a) How many independent elements are there in a symmetric tensor? (Since s12=s21, these would count as only *one* independent element.)
(b) How many independent elements are there in an antisymmetric tensor?
(c) If sμν is symmetric, show that sμν is also symmetric. If aμν is antisymmetric, show that aμν is antisymmetric.
(d) If sμν is symmetric and aμν is antisymmetric, show that sμνaμν=0.
(e) Show that any second-rank tensor (tμν) can be written as the sum of an antisymmetric part (aμν) and a symmetric part (sμν): tμν=aμν+sμν. Construct sμν and aμν explicitly, given tμν.